A model class for new physics in the form of the dimension-six effective Lagrangian. More...

#include <NPSMEFTd6General.h>

Inheritance diagram for NPSMEFTd6General:

Detailed Description

A model class for new physics in the form of the dimension-six effective Lagrangian.

Author: HEPfit Collaboration

Copyright: GNU General Public License

This is a Model class containing parameters and functions associated with the general dimension-six effective Lagrangian. (Use the model "NPSMEFTd6_LFU_QFU" to assume lepton and quark flavour universality)

In this class we consider the dimension-six effective Lagrangian

\[ \mathcal{L}_\mathrm{eff} = \mathcal{L}_\mathrm{SM} + \sum_i \frac{C_i}{\Lambda^2} \mathcal{O}_i. \]

The implementation is written in the basis of [Grzadkowski:2010es]. For convenience, the parameterization also includes operators appearing in other common bases. In particular, the complete set of parameters contains 4 redundancies, given by the coefficients $C_{2B,2W,DHB,DHW,DB,DW} $, which correspond to operators not included in the basis of [Grzadkowski:2010es]. For meaningful physical results one must make sure to include only a complete set of interactions in a given analysis.

Initialization

After creating an instance of the current class with the constructor NPSMEFTd6General(), it is required to call the initialization method InitializeModel(). In the Monte Carlo run, the constructor as well as the initialization method are called in InputParser::ReadParameters().

Model parameters

The model parameters of NPSMEFTd6General are summarized below:

Label	LaTeX symbol	Description
g1_LNP	$g_1(\Lambda_\mathrm{NP})$	The hypercharge coupling constant at the New Physics scale.
g2_LNP	$g_2(\Lambda_\mathrm{NP})$	The SU(2) $_L$ coupling constant at the New Physics scale.
g1_LNP	$g_3(\Lambda_\mathrm{NP})$	The QCD coupling constant at the New Physics scale.
lambdaH_LNP	$\lambda_H(\Lambda_\mathrm{NP})$	The coefficient of the $(H^\dagger H)^2$ term at the New Physics scale.
muH_LNP	$\mu_H(\Lambda_\mathrm{NP})$	The square root of the coefficient of the $(H^\dagger H)$ term at the New Physics scale.
Ye_LNP	$Y_e(\Lambda_\mathrm{NP})$	The electron Yukawa coupling at the New Physics scale.
Ymu_LNP	$Y_\mu(\Lambda_\mathrm{NP})$	The muon Yukawa coupling at the New Physics scale.
Ytau_LNP	$Y_\tau(\Lambda_\mathrm{NP})$	The tau Yukawa coupling at the New Physics scale.
Yu_LNP	$Y_u(\Lambda_\mathrm{NP})$	The up quark Yukawa coupling at the New Physics scale in the up basis.
Yc_LNP	$Y_c(\Lambda_\mathrm{NP})$	The charm quark Yukawa coupling at the New Physics scale in the up basis.
Yt_LNP	$Y_t(\Lambda_\mathrm{NP})$	The top quark Yukawa coupling at the New Physics scale in the up basis.
Yd_LNP	$Y_d(\Lambda_\mathrm{NP})$	The down quark Yukawa coupling at the New Physics scale in the down basis.
Ys_LNP	$Y_s(\Lambda_\mathrm{NP})$	The strange quark Yukawa coupling at the New Physics scale in the down basis.
Yb_LNP	$Y_b(\Lambda_\mathrm{NP})$	The bottom quark Yukawa coupling at the New Physics scale in the down basis.
s12CKM_LNP	$s_{12}(\Lambda_\mathrm{NP})$	The sine of the $\theta_{12}$ angle parameterizing the relative orientation of up and down Yukawa couplings at the New Physics scale.
s13CKM_LNP	$s_{13}(\Lambda_\mathrm{NP})$	The sine of the $\theta_{13}$ angle parameterizing the relative orientation of up and down Yukawa couplings at the New Physics scale.
s23CKM_LNP	$s_{23}(\Lambda_\mathrm{NP})$	The sine of the $\theta_{23}$ angle parameterizing the relative orientation of up and down Yukawa couplings at the New Physics scale.
dCKM_LNP	$\delta(\Lambda_\mathrm{NP})$	The CP-violating phase of the matrix describing the relative orientation of up and down Yukawa couplings at the New Physics scale.
CG	$C_{G} $	The coefficient of the operator ${\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}$.
CW	$C_{W} $	The coefficient of the operator ${\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}$.
CHG	$C_{HG} $	The coefficient of the operator ${\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}$.
CHW	$C_{HW} $	The coefficient of the operator ${\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}$.
CHB	$C_{HB} $	The coefficient of the operator ${\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}$.
CHWB	$C_{HWB} $	The coefficient of the operator ${\cal O}_{HWB}=\big(H^\dagger\sigma^a H\big)W_{\mu\nu}^a B^{\mu\nu}$.
CHD	$C_{HD}$	The coefficient of the operator ${\cal O}_{HD}=\big\|H^\dagger D_\mu H\big\|^2$.
CHbox	$C_{H\Box}$	The coefficient of the operator ${\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)$.
CH	$C_{H}$	The coefficient of the operator ${\cal O}_{H}=\big(H^\dagger H\big)^3$.
CHl1_kk, CHl1_klr, CHl1_kli	$ (C_{HL}^{(1)})_{kk}, \mbox{Re}\big[(C_{HL}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(1)})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{HL}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^j\big)$, for $i,j=1,2,3$.
CHl3_kk, CHl3_klr, CHl3_kli	$ (C_{HL}^{(3)})_{kk}, \mbox{Re}\big[(C_{HL}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(3)})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{HL}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \sigma^a L^j\big)$, for $i,j=1,2,3$.
CHe_kk, CHe_klr, CHe_kli	$ (C_{He})_{kk}, \mbox{Re}\big[(C_{He})_{kl}\big], \mbox{Im}\big[(C_{He})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^j\big)$, for $i,j=1,2,3$.
CHq1_kk, CHq1_klr, CHq1_kli	$ (C_{HQ}^{(1)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(1)})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{HQ}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^j\big)$, for $i,j=1,2,3$.
CHq3_kk, CHq3_klr, CHq3_kli	$ (C_{HQ}^{(3)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(3)})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{HQ}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \sigma^a Q^j\big)$, for $i,j=1,2,3$.
CHu_kk, CHu_klr, CHu_kli	$ (C_{Hu})_{kk}, \mbox{Re}\big[(C_{Hu})_{kl}\big], \mbox{Im}\big[(C_{Hu})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{Hu})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^j\big)$, for $i,j=1,2,3$.
CHd_kk, CHd_klr, CHd_kli	$ (C_{Hd})_{kk}, \mbox{Re}\big[(C_{Hd})_{kl}\big], \mbox{Im}\big[(C_{Hd})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{Hd})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^j\big)$, for $i,j=1,2,3$.
CHud_klr, CHud_kli	$\mbox{Re}\big[(C_{Hud})_{kl}\big], \mbox{Im}\big[(C_{Hud})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{Hud})_{ij} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^j\big)$, for $i,j=1,2,3$.
CeH_klr, CeH_kli	$\mbox{Re}\big[(C_{eH})_{kl}\big], \mbox{Im}\big[(C_{eH})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{eH})_{ij} =\big(H^\dagger H\big) \big(\overline{L^i}\,H E^j\big)$, for $i,j=1,2,3$.
CuH_klr, CuH_kli	$\mbox{Re}\big[(C_{uH})_{kl}\big], \mbox{Im}\big[(C_{uH})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{uH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,\widetilde{H} U^j\big)$, for $i,j=1,2,3$.
CdH_klr, CdH_kli	$\mbox{Re}\big[(C_{dH})_{kl}\big], \mbox{Im}\big[(C_{dH})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{dH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,H D^j\big)$, for $i,j=1,2,3$.
CuG_klr, CuG_kli	$\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A$, for $i,j=1,2,3$.
CuW_klr, CuW_kli	$\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a U^j\big)\widetilde{H} W_{\mu\nu}^a$, for $i,j=1,2,3$.
CuB_klr, CuB_kli	$\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}$, for $i,j=1,2,3$.
CdG_klr, CdG_kli	$\mbox{Re}\big[(C_{dG})_{kl}\big], \mbox{Im}\big[(C_{dG})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{dG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A D^j\big)H G_{\mu\nu}^A$, for $i,j=1,2,3$.
CdW_klr, CdW_kli	$\mbox{Re}\big[(C_{dW})_{kl}\big], \mbox{Im}\big[(C_{dW})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{dW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a D^j\big)H W_{\mu\nu}^a$, for $i,j=1,2,3$.
CdB_klr, CdB_kli	$\mbox{Re}\big[(C_{dB})_{kl}\big], \mbox{Im}\big[(C_{dB})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{dB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} D^j\big)H B_{\mu\nu}$, for $i,j=1,2,3$.
CeW_klr, CeW_kli	$\mbox{Re}\big[(C_{eW})_{kl}\big], \mbox{Im}\big[(C_{eW})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{eW})_{ij} =\big(\overline{L^i}\sigma^{\mu\nu} \sigma_a E^j\big)H W_{\mu\nu}^a$, for $i,j=1,2,3$.
CeB_klr, CeB_kli	$\mbox{Re}\big[(C_{eB})_{kl}\big], \mbox{Im}\big[(C_{eB})_{kl}\big] $	The real and imaginary parts of the coefficient of the operator $({\cal O}_{eB})_{ij} =\big(\overline{L^i}\sigma^{\mu\nu} E^j\big)H B_{\mu\nu}$, for $i,j=1,2,3$.
Cll_1221, Cll_2112	$(C_{LL})_{1221,2112}$	The coefficient of the operator $({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)$, for $ijkl=1221,2112$.
Clq1	$C_{LQ}^{(1)}$	The coefficient of the operator $({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)$.
Clq3	$C_{LQ}^{(3)}$	The coefficient of the operator $({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \sigma_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)$.
Cee	$C_{EE}$	The coefficient of the operator $({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)$.
Ceu	$C_{EU}$	The coefficient of the operator $({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)$.
Ced	$C_{ED}$	The coefficient of the operator $({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)$.
Cle	$C_{LE}$	The coefficient of the operator $({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)$.
Clu	$C_{LU}$	The coefficient of the operator $({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)$.
Cld	$C_{LD}$	The coefficient of the operator $({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)$.
Cqe	$C_{QE}$	The coefficient of the operator $({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)$.
Cqq1_1133, Cqq1_1331, Cqq1_3333	$C_{QQ}^{(1)}$	The coefficient of the operator $({\cal O}_{QQ}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)$.
Cqq3_1133, Cqq3_1331, Cqq3_3333	$C_{QQ}^{(3)}$	The coefficient of the operator $({\cal O}_{QQ}^{(3)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu \sigma_a Q^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)$.
Cuu_1133, Cuu_1331, Cuu_3333	$C_{uu}$	The coefficient of the operator $({\cal O}_{uu})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu u^j\big) \big(\overline{u^k}\,\gamma_\mu u^l\big)$.
Cud1_3311, Cud1_3333	$C_{ud}^{(1)}$	The coefficient of the operator $({\cal O}_{ud}^{(1)})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu u^j\big) \big(\overline{d^k}\,\gamma_\mu d^l\big)$.
Cud8_3311, Cud8_3333	$C_{ud}^{(8)}$	The coefficient of the operator $({\cal O}_{ud}^{(8)})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu T^A u^j\big) \big(\overline{d^k}\,\gamma_\mu T^A d^l\big)$.
Cqu1_1133, Cqu1_3311, Cqu1_3333	$C_{Qu}^{(1)}$	The coefficient of the operator $({\cal O}_{Qu}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{u^k}\,\gamma_\mu u^l\big)$.
Cqu8_1133, Cqu8_3311, Cqu8_3333	$C_{Qu}^{(8)}$	The coefficient of the operator $({\cal O}_{Qu}^{(8)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu T^A Q^j\big) \big(\overline{u^k}\,\gamma_\mu T^A u^l\big)$.
Cqd1_3311, Cqd1_3333	$C_{Qd}^{(1)}$	The coefficient of the operator $({\cal O}_{Qd}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{d^k}\,\gamma_\mu d^l\big)$.
Cqd8_3311, Cqd8_3333	$C_{Qd}^{(8)}$	The coefficient of the operator $({\cal O}_{Qd}^{(8)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu T^A Q^j\big) \big(\overline{d^k}\,\gamma_\mu T^A d^l\big)$.
Cquqd1_3333	$C_{QuQd}^{(1)}$	The coefficient of the operator $({\cal O}_{QuQd}^{(1)})_{ijkl}=\big(\overline{Q^i}\, u^j\big) i\sigma_2 \big(\overline{Q^k}^T\, d^l\big)$.
Cquqd8_3333	$C_{QuQd}^{(8)}$	The coefficient of the operator $({\cal O}_{QuQd}^{(8)})_{ijkl}=\big(\overline{Q^i}\, T^A u^j\big) i\sigma_2 \big(\overline{Q^k}^T\, T^A d^l\big)$.
Lambda_NP	$\Lambda $	The new physics scale.
BrHinv	Br $(H\to invisible)$	The branching ratio of invisible Higgs decays. Only the absolute value of this parameter is considered.(Not part of the EFT. Only for tests.)
BrHexo	Br $(H\to exotic)$	The branching ratio of exotic Higgs decays. Only the absolute value of this parameter is considered. (Not part of the EFT. Only for tests.)
dg1Z	$\delta g_{1Z}$	Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)
dKappaga	$\delta \kappa_{\gamma}$	Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)
lambZ	$\lambda_{Z}$	Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)

Where the hermitian derivatives are defined as

\[ H^\dagger i \overset{\leftrightarrow}{D}_\mu H\equiv H^\dagger i(D_\mu - \overset{\leftarrow}{D}_\mu)H \]

and

\[ H^\dagger i \overset{\leftrightarrow}{D^a_\mu} H\equiv H^\dagger i (\sigma^a D_\mu - \overset{\leftarrow}{D}_\mu \sigma^a)H. \]

Model flags

The Flags of NPSMEFTd6General are summarized below:

Label	Value	Description
MWinput	TRUE / FALSE	This auxiliary flag is used for setting the W mass as a SM input, instead of the electromagnetic constant parameter dAle5Mz. The default value is FALSE. This flag will override the flag of the same name in StandardModel
QuadraticTerms	TRUE / FALSE	This flag is set to TRUE if the quadratic terms in Higgs cross sections and widths are switched on. The default value is FALSE; new physics contributions are linearized.
HiggsSM	TRUE / FALSE	This flag is set to TRUE if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. The default value is FALSE.
LoopHd6	TRUE / FALSE	This flag is set to TRUE if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. The default value is FALSE.
LoopH3d6Quad	TRUE / FALSE	This flag is set to TRUE if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. Works independently of the flag QuadraticTerms (the quadratic contributions are also added if the latter is true). The default value is FALSE.
RGEci	TRUE / FALSE	This flag is set to TRUE if including the SMEFT RGE effects. The default value is TRUE.
finiteNLO	TRUE / FALSE	This flag is set to TRUE if including SMEFT finite NLO terms (where available). The default value is FALSE.
matchLEFT	TRUE / FALSE	This flag is set to TRUE if the matching between SMEFT and LEFT needs to be computed. The default value is TRUE.

Important member functions

See the base classes of the current class.

Definition at line 593 of file NPSMEFTd6General.h.

Public Member Functions
virtual const double	A_f (const Particle f) const
	The left-right asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $\mathcal{A}_f$.

virtual const double	AFB (const Particle f) const
	The forward-backward asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $A^f_{FB}$.

virtual const double	alphaMz () const
	The electromagnetic coupling at the $Z$-mass scale.

virtual const double	aPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	the angular parameter $a$ from $\mu_{e^+e^- \to ZH}$ (arXiv:1708.09079 [hep-ph]).

virtual const double	bPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	the angular parameter $b$ from $\mu_{e^+e^- \to ZH}$ (arXiv:1708.09079 [hep-ph]).

virtual const double	Br_H_exo () const
	The branching ratio of the of the Higgs into exotic particles.

virtual const double	Br_H_inv () const
	The branching ratio of the of the Higgs into invisible particles.

virtual const double	Br_H_inv_NP () const
	The branching ratio of the of the Higgs into invisible particles (only invisible new particles).

virtual const double	BrH2d2dRatio () const
	The ratio of the Br $(H\to 2d2d)$ in the current model and in the Standard Model.

virtual const double	BrH2e2muRatio () const
	The ratio of the Br $(H\to 2e 2\mu)$ in the current model and in the Standard Model.

virtual const double	BrH2e2vRatio () const
	The ratio of the Br $(H\to 2e2v)$ in the current model and in the Standard Model.

virtual const double	BrH2evRatio () const
	The ratio of the Br $(H\to 2ev)$ in the current model and in the Standard Model.

virtual const double	BrH2L2dRatio () const
	The ratio of the Br $(H\to 2L2d)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

virtual const double	BrH2L2LRatio () const
	The ratio of the Br $(H\to 2L2L')$ ( $L,L'=e,\mu,\tau$) in the current model and in the Standard Model.

virtual const double	BrH2L2uRatio () const
	The ratio of the Br $(H\to 2L2u)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

virtual const double	BrH2L2v2Ratio () const
	The ratio of the Br $(H\to 2L2v)$ ( $L=e,\mu$) in the current model and in the Standard Model.

virtual const double	BrH2L2vRatio () const
	The ratio of the Br $(H\to 2L2v)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

virtual const double	BrH2l2vRatio () const
	The ratio of the Br $(H\to 2l2v)$ ( $l=e,\mu$) in the current model and in the Standard Model.

virtual const double	BrH2Lv2Ratio () const
	The ratio of the Br $(H\to 2Lv)$ ( $L=e,\mu$) in the current model and in the Standard Model.

virtual const double	BrH2LvRatio () const
	The ratio of the Br $(H\to 2Lv)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

virtual const double	BrH2mu2vRatio () const
	The ratio of the Br $(H\to 2\mu 2v)$ in the current model and in the Standard Model.

virtual const double	BrH2muvRatio () const
	The ratio of the Br $(H\to 2ev)$ in the current model and in the Standard Model.

virtual const double	BrH2u2dRatio () const
	The ratio of the Br $(H\to 2u2d)$ in the current model and in the Standard Model.

virtual const double	BrH2u2uRatio () const
	The ratio of the Br $(H\to 2u2u)$ in the current model and in the Standard Model.

virtual const double	BrH2udRatio () const
	The ratio of the Br $(H\to 2ud)$ in the current model and in the Standard Model.

virtual const double	BrH2v2dRatio () const
	The ratio of the Br $(H\to 2v2d)$ in the current model and in the Standard Model.

virtual const double	BrH2v2uRatio () const
	The ratio of the Br $(H\to 2v2u)$ in the current model and in the Standard Model.

virtual const double	BrH2v2vRatio () const
	The ratio of the Br $(H\to 2v2v)$ in the current model and in the Standard Model.

virtual const double	BrH4dRatio () const
	The ratio of the Br $(H\to 4d)$ in the current model and in the Standard Model.

virtual const double	BrH4eRatio () const
	The ratio of the Br $(H\to 4e)$ in the current model and in the Standard Model.

virtual const double	BrH4fCCRatio () const
	The ratio of the Br $(H\to 4f, CC)$ in the current model and in the Standard Model.

virtual const double	BrH4fNCRatio () const
	The ratio of the Br $(H\to 4f, NC)$ in the current model and in the Standard Model.

virtual const double	BrH4fRatio () const
	The ratio of the Br $(H\to 4f)$ in the current model and in the Standard Model.

virtual const double	BrH4L2Ratio () const
	The ratio of the Br $(H\to 4L)$ ( $L=e,\mu$) in the current model and in the Standard Model.

virtual const double	BrH4LRatio () const
	The ratio of the Br $(H\to 4L)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

virtual const double	BrH4lRatio () const
	The ratio of the Br $(H\to 4l)$ ( $l=e,\mu$) in the current model and in the Standard Model.

virtual const double	BrH4muRatio () const
	The ratio of the Br $(H\to 4\mu)$ in the current model and in the Standard Model.

virtual const double	BrH4uRatio () const
	The ratio of the Br $(H\to 4u)$ in the current model and in the Standard Model.

virtual const double	BrH4vRatio () const
	The ratio of the Br $(H\to 4v)$ in the current model and in the Standard Model.

virtual const double	BrHbbRatio () const
	The ratio of the Br $(H\to b\bar{b})$ in the current model and in the Standard Model.

virtual const double	BrHccRatio () const
	The ratio of the Br $(H\to c\bar{c})$ in the current model and in the Standard Model.

virtual const double	BrHevmuvRatio () const
	The ratio of the Br $(H\to e\nu \mu\nu)$ in the current model and in the Standard Model.

virtual const double	BrHgagaRatio () const
	The ratio of the Br $(H\to \gamma\gamma)$ in the current model and in the Standard Model.

virtual const double	BrHggRatio () const
	The ratio of the Br $(H\to gg)$ in the current model and in the Standard Model.

virtual const double	BrHll_vvorjjRatio () const
	The ratio of the Br $(H\to l l \nu\nu, l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model.

virtual const double	BrHlv_lvorjjRatio () const
	The ratio of the Br $(H\to l \nu l \nu, l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model.

virtual const double	BrHlvjjRatio () const
	The ratio of the Br $(H\to l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model.

virtual const double	BrHLvudRatio () const
	The ratio of the Br $(H\to Lvud)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

virtual const double	BrHLvvLRatio () const
	The ratio of the Br $(H\to LvvL)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

virtual const double	BrHmumuRatio () const
	The ratio of the Br $(H\to \mu^+\mu^-)$ in the current model and in the Standard Model.

virtual const double	BrHssRatio () const
	The ratio of the Br $(H\to s\bar{s})$ in the current model and in the Standard Model.

virtual const double	BrHtautauRatio () const
	The ratio of the Br $(H\to \tau^+\tau^-)$ in the current model and in the Standard Model.

virtual const double	BrHtoinvRatio () const
	The ratio of the Br $(H\to invisible)$ in the current model and in the Standard Model.

virtual const double	BrHudduRatio () const
	The ratio of the Br $(H\to uddu)$ in the current model and in the Standard Model.

virtual const double	BrHvisRatio () const
	The ratio of the Br $(H\to visible)$ in the current model and in the Standard Model.

virtual const double	BrHVVRatio () const
	The ratio of the Br $(H\to VV)$ in the current model and in the Standard Model.

virtual const double	BrHWffRatio () const
	The ratio of the Br $(H\to W f f)$, with $f$ any fermion, in the current model and in the Standard Model.

virtual const double	BrHWjjRatio () const
	The ratio of the Br $(H\to W j j)$ in the current model and in the Standard Model.

virtual const double	BrHWlvRatio () const
	The ratio of the Br $(H\to W l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model.

virtual const double	BrHWW2l2vRatio () const
	The ratio of the Br $(H\to WW^*\to l\nu l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model.

virtual const double	BrHWW4fRatio () const
	The ratio of the Br $(H\to WW^*\to 4f)$, with $f$ any fermion, in the current model and in the Standard Model.

virtual const double	BrHWW4jRatio () const
	The ratio of the Br $(H\to WW^*\to 4j)$ in the current model and in the Standard Model.

virtual const double	BrHWWRatio () const
	The ratio of the Br $(H\to WW)$ in the current model and in the Standard Model.

virtual const double	BrHZddRatio () const
	The ratio of the Br $(H\to Z d d)$ ( $d=d,s,b $) in the current model and in the Standard Model.

virtual const double	BrHZffRatio () const
	The ratio of the Br $(H\to Zff)$, with $f$ any fermion, in the current model and in the Standard Model.

virtual const double	BrHZgaeeRatio () const
	The ratio of the Br $(H\to Z\gamma\to ee\gamma)$ in the current model and in the Standard Model.

virtual const double	BrHZgallRatio () const
	The ratio of the Br $(H\to Z\gamma\to ll\gamma)$ ( $l=e,\mu $) in the current model and in the Standard Model.

virtual const double	BrHZgamumuRatio () const
	The ratio of the Br $(H\to Z\gamma\to \mu\mu\gamma)$ in the current model and in the Standard Model.

virtual const double	BrHZgaRatio () const
	The ratio of the Br $(H\to Z\gamma)$ in the current model and in the Standard Model.

virtual const double	BrHZllRatio () const
	The ratio of the Br $(H\to Zll)$ ( $l=e,\mu $) in the current model and in the Standard Model.

virtual const double	BrHZuuRatio () const
	The ratio of the Br $(H\to Z u u)$ ( $u=u,c $) in the current model and in the Standard Model.

virtual const double	BrHZvvRatio () const
	The ratio of the Br $(H\to Z\nu\nu)$ in the current model and in the Standard Model.

virtual const double	BrHZZ2e2muRatio () const
	The ratio of the Br $(H\to ZZ* \to 2e 2\mu)$ in the current model and in the Standard Model.

virtual const double	BrHZZ4dRatio () const
	The ratio of the Br $(H\to ZZ* \to 4 d)$ ( $d=d,s,b $) in the current model and in the Standard Model.

virtual const double	BrHZZ4eRatio () const
	The ratio of the Br $(H\to ZZ* \to 4e)$ in the current model and in the Standard Model.

virtual const double	BrHZZ4fRatio () const
	The ratio of the Br $(H\to ZZ* \to 4f)$, with $f$ any fermion, in the current model and in the Standard Model.

virtual const double	BrHZZ4lRatio () const
	The ratio of the Br $(H\to ZZ* \to 4l)$ ( $l=e,\mu $) in the current model and in the Standard Model.

virtual const double	BrHZZ4muRatio () const
	The ratio of the Br $(H\to ZZ* \to 4\mu)$ in the current model and in the Standard Model.

virtual const double	BrHZZ4uRatio () const
	The ratio of the Br $(H\to ZZ* \to 4 u)$ ( $u=u,c $) in the current model and in the Standard Model.

virtual const double	BrHZZ4vRatio () const
	The ratio of the Br $(H\to ZZ* \to 4\nu)$ in the current model and in the Standard Model.

virtual const double	BrHZZRatio () const
	The ratio of the Br $(H\to ZZ)$ in the current model and in the Standard Model.

virtual const double	BrW (const Particle fi, const Particle fj) const
	The branching ratio of the $W$ boson decaying into a SM fermion pair, $Br(W\to f_i f_j)$.

virtual const double	cbW_TWG (const double mu) const

const double	CeeLL_bottom (const double mu) const

const double	CeeLL_charm (const double mu) const

const double	CeeLL_down (const double mu) const

const double	CeeLL_e (const double mu) const

const double	CeeLL_mu (const double mu) const

const double	CeeLL_strange (const double mu) const

const double	CeeLL_tau (const double mu) const

const double	CeeLL_top (const double mu) const

const double	CeeLL_up (const double mu) const

const double	CeeLR_bottom (const double mu) const

const double	CeeLR_charm (const double mu) const

const double	CeeLR_down (const double mu) const

const double	CeeLR_e (const double mu) const

const double	CeeLR_mu (const double mu) const

const double	CeeLR_strange (const double mu) const

const double	CeeLR_tau (const double mu) const

const double	CeeLR_top (const double mu) const

const double	CeeLR_up (const double mu) const

const double	CeeRL_bottom (const double mu) const

const double	CeeRL_charm (const double mu) const

const double	CeeRL_down (const double mu) const

const double	CeeRL_e (const double mu) const

const double	CeeRL_mu (const double mu) const

const double	CeeRL_strange (const double mu) const

const double	CeeRL_tau (const double mu) const

const double	CeeRL_top (const double mu) const

const double	CeeRL_up (const double mu) const

const double	CeeRR_bottom (const double mu) const

const double	CeeRR_charm (const double mu) const

const double	CeeRR_down (const double mu) const

const double	CeeRR_e (const double mu) const

const double	CeeRR_mu (const double mu) const

const double	CeeRR_strange (const double mu) const

const double	CeeRR_tau (const double mu) const

const double	CeeRR_top (const double mu) const

const double	CeeRR_up (const double mu) const

virtual const double	CEWHd11 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hd})_{11}$.

virtual const double	CEWHd22 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hd})_{22}$.

virtual const double	CEWHd33 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hd})_{33}$.

virtual const double	CEWHe11 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{He})_{11}$.

virtual const double	CEWHe22 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{He})_{22}$.

virtual const double	CEWHe33 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{He})_{33}$.

virtual const double	CEWHL111 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(1)})_{11}$.

virtual const double	CEWHL122 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(1)})_{22}$.

virtual const double	CEWHL133 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(1)})_{33}$.

virtual const double	CEWHL311 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(3)})_{11}$.

virtual const double	CEWHL322 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(3)})_{22}$.

virtual const double	CEWHL333 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(3)})_{33}$.

virtual const double	CEWHQ111 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(1)})_{11}$.

virtual const double	CEWHQ122 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(1)})_{22}$.

virtual const double	CEWHQ133 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(1)})_{33}$.

virtual const double	CEWHQ311 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(3)})_{11}$.

virtual const double	CEWHQ322 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(3)})_{22}$.

virtual const double	CEWHQ333 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(3)})_{33}$.

virtual const double	CEWHQd33 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(d)})_{33}$.

virtual const double	CEWHQu33 (const double mu) const
	Combination of coefficients of the Warsaw basis not constrained by EWPO (at LO) $(\hat{C}_{HQ}^{(u)})_{33}$.

virtual const double	CEWHu11 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hu})_{11}$.

virtual const double	CEWHu22 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hu})_{22}$.

virtual const double	CEWHu33 (const double mu) const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hu})_{33}$.

virtual const double	cgaga_HB (const double mu) const
	The Higgs-basis coupling $c_{\gamma\gamma}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	cgg_HB (const double mu) const
	The Higgs-basis coupling $c_{gg}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	cggEff_HB (const double mu) const
	The effective Higgs-basis coupling $c_{gg}^{Eff}$. (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	cHb_TWG (const double mu) const

virtual const double	cHQ3_TWG (const double mu) const

virtual const double	cHQm_TWG (const double mu) const

virtual const double	cHQp_TWG (const double mu) const

virtual const double	cHt_TWG (const double mu) const

virtual const double	cHtb_TWG (const double mu) const

virtual const double	computeGammaTotalRatio () const
	The ratio of the $\Gamma(H)$ in the current model and in the Standard Model.

virtual const double	cQd1_TWG (const double mu) const

virtual const double	cQd8_TWG (const double mu) const

virtual const double	cQe_TWG (const double mu) const

virtual const double	cQl3_TWG (const double mu) const

virtual const double	cQlM_TWG (const double mu) const

virtual const double	cQlP_TWG (const double mu) const

virtual const double	cQq11_TWG (const double mu) const

virtual const double	cQq18_TWG (const double mu) const

virtual const double	cQQ1_TWG (const double mu) const

virtual const double	cQq31_TWG (const double mu) const

virtual const double	cQq38_TWG (const double mu) const

virtual const double	cQQ8_TWG (const double mu) const

virtual const double	cQt1_TWG (const double mu) const

virtual const double	cQt8_TWG (const double mu) const

virtual const double	cQu1_TWG (const double mu) const

virtual const double	cQu8_TWG (const double mu) const

virtual const double	ctd1_TWG (const double mu) const

virtual const double	ctd8_TWG (const double mu) const

virtual const double	cte_TWG (const double mu) const

virtual const double	ctG_TWG (const double mu) const

virtual const double	ctH_TWG (const double mu) const

virtual const double	ctl_TWG (const double mu) const

virtual const double	ctlS_TWG (const double mu) const

virtual const double	ctlT_TWG (const double mu) const

virtual const double	ctq1_TWG (const double mu) const

virtual const double	ctq8_TWG (const double mu) const

virtual const double	ctt1_TWG (const double mu) const

virtual const double	ctu1_TWG (const double mu) const

virtual const double	ctu8_TWG (const double mu) const

virtual const double	ctW_TWG (const double mu) const

virtual const double	ctZ_TWG (const double mu) const

virtual const double	cZBox_HB (const double mu) const
	The Higgs-basis coupling $c_{z\Box}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	cZga_HB (const double mu) const
	The Higgs-basis coupling $c_{z\gamma}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	cZZ_HB (const double mu) const
	The Higgs-basis coupling $c_{zz}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	Dalpha5hMz () const
	The 5-quark contribution to the running of the em constant to the $Z$ pole. $\Delta\alpha_{had}^{(5)}(M_Z)$.

virtual const double	del_A_mu (const double mu) const
	Correction to photon WF.

virtual const double	del_e_mu (const double mu) const
	Correction to electric charge.

virtual const double	del_sW2_mu (const double mu) const
	Correction to (sin squared of) weak mixing angle.

virtual const double	del_Z_mu (const double mu) const
	Correction to Z WF.

virtual const double	del_ZA_mu (const double mu) const
	Correction to Z-A mixing.

virtual const double	delQ_gNC (const double mu) const
	Separate, charge-proportional, indirect correction to EW neutral currents.

virtual const double	delta2sBRH3 (const double C1prod, const double C1Hxx) const
	Quadratic contribution from the Higgs self-couplings modifications to the signal strength for $\sigma \times BR(H\to xx)$ in the current model.

virtual const double	delta2sH3 (const double C1) const
	Quadratic contribution from the Higgs self-couplings modifications to the signal strength for an observable $\sigma$ in the current model.

virtual const double	delta_AFB_ee (const double pol_e, const double pol_p, const double s) const

virtual const double	delta_AFB_f (const Particle f, const double pol_e, const double pol_p, const double s) const

virtual const double	delta_alrmoller (const double q2, const double y) const
	The computation of the parity violating asymmetry in Moller scattering.

virtual const double	delta_amuon () const
	The computation of the anomalous magnetic moment of the muon $a_\mu=(g_\mu-2)/2$.

virtual const double	delta_Dsigma_f (const Particle f, const double pol_e, const double pol_p, const double s, const double cos) const

virtual const double	delta_gAnue () const
	The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gAnue.

virtual const double	delta_gLnuN2 () const
	The computation of the correction to the effective neutrino nucleon LH coupling: delta_gLnuN2.

virtual const double	delta_gRnuN2 () const
	The computation of the correction to the effective neutrino nucleon RH coupling: delta_gRnuN2.

virtual const double	delta_gVnue () const
	The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gVnue.

virtual const double	delta_mubbH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{bbH}$ between the bbH production cross-section in the current model and in the Standard Model.

virtual const double	delta_mubbH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{bbH}$ between the bbH production cross-section in the current model and in the Standard Model.

virtual const double	delta_muggH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{ggH}$ between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.

virtual const double	delta_muggH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{ggH}$ between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.

virtual const double	delta_mutH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{tH}$ between the t-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	delta_mutH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{tH}$ between the t-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	delta_muttH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{ttH}$ between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	delta_muttH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{ttH}$ between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	delta_muVBF_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{VBF}$ between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.

virtual const double	delta_muVBF_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{VBF}$ between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.

virtual const double	delta_muVH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{VH}$ between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	delta_muVH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{VH}$ between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	delta_muWH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{WH}$ between the W-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	delta_muWH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{WH}$ between the W-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	delta_muZH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{ZH}$ between the Z-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	delta_muZH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{ZH}$ between the Z-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	delta_Qwemoller (const double q2, const double y) const
	The computation of the electron's weak charge.

virtual const double	delta_Qwn () const
	The computation of the neutron weak charge: Qwn.

virtual const double	delta_Qwp () const
	The computation of the proton weak charge: Qwp.

virtual const double	delta_sigma_ee (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const

virtual const double	delta_sigma_f (const Particle f, const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const

virtual const double	delta_sigma_had (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const

virtual const double	delta_sigmaTot_ee (const double pol_e, const double pol_p, const double s) const

virtual const double	delta_sigmaTot_f (const Particle f, const double pol_e, const double pol_p, const double s) const

virtual const double	delta_TauLFU_gmuge () const
	The computation of the correction to the LFU ratio $g_\mu/ g_e $.

virtual const double	delta_TauLFU_gtauge () const
	The computation of the correction to the LFU ratio $g_\tau/ g_e $.

virtual const double	delta_TauLFU_gtaugmu () const
	The computation of the correction to the LFU ratio $g_\tau/ g_\mu $.

virtual const double	delta_TauLFU_gtaugmuK () const
	The computation of the correction to the LFU ratio $\left(g_\tau/ g_\mu\right)_K $.

virtual const double	delta_TauLFU_gtaugmuPi () const
	The computation of the correction to the LFU ratio $\left(g_\tau/ g_\mu\right)_\pi $.

virtual const double	deltaa0 () const
	The relative correction to the electromagnetic constant at zero momentum, $\delta \alpha(0)/\alpha(0)$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltaa02 () const
	The relative correction to the electromagnetic constant at zero momentum, $(\delta \alpha(0)/\alpha(0))^2$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltaA_f (const Particle f) const
	The new physics contribution to the left-right asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $\delta \mathcal{A}_f$.

virtual const double	deltaAFB (const Particle f) const
	The new physics contribution to the forward-backward asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $\delta A^f_{FB}$.

virtual const double	deltaaMZ () const
	The relative correction to the electromagnetic constant at the Z pole, $\delta \alpha(M_Z^2)/\alpha(M_Z^2)$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltaaMZ2 () const
	The relative correction to the electromagnetic constant at the Z pole, $(\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltaaSMZ () const
	The relative correction to the strong coupling constant at the Z pole, $\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltaaSMZ2 () const
	The relative correction to the strong coupling constant at the Z pole, $(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltacZ_HB (const double mu) const
	The Higgs-basis coupling $\delta c_z$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	deltadxsdcoseeWWlvjjLEP2 (const double sqrt_s, const int bin) const
	The new physics contribution to the differential cross section in pb for $e^+ e^- \to W^+ W^- \to lv jj $, with $ l= e,\mu $ for the 4 $ cos{\theta}$ bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph].

virtual const double	deltaeNP (const double mu) const
	The new physics relative contribution to the EW coupling constant $e$.

virtual const double	deltaG1_hWW () const
	The new physics contribution to the coupling of the effective interaction $H W_{\mu\nu}^\dagger W^{\mu\nu}$.

virtual const double	deltaG1_hWW_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H W_{\mu\nu}^\dagger W^{\mu\nu}$.

virtual const double	deltaG1_hZA () const
	The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} F^{\mu\nu}$.

virtual const double	deltaG1_hZA_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} F^{\mu\nu}$.

virtual const double	deltaG1_hZARatio () const
	The full new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} F^{A \mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value.

virtual const double	deltaG1_hZARatio_mu (const double mu) const
	The full new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} F^{A \mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value.

virtual const double	deltaG1_hZZ () const
	The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} Z^{\mu\nu}$.

virtual const double	deltaG1_hZZ_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} Z^{\mu\nu}$.

virtual const double	deltag1gaNP (const double mu) const
	The new physics contribution to the anomalous triple gauge coupling $g_{1,\gamma}$.

virtual const double	deltag1ZNP (const double mu) const
	The new physics contribution to the anomalous triple gauge coupling $g_{1,Z}$.

virtual const double	deltag1ZNPEff () const
	The new physics contribution to the effective anomalous triple gauge coupling $g_{1,Z}^{Eff}$ from arXiv: 1708.09079 [hep-ph].

virtual const double	deltaG2_hWW () const
	The new physics contribution to the coupling of the effective interaction $H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}$.

virtual const double	deltaG2_hWW_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}$.

virtual const double	deltaG2_hZA () const
	The new physics contribution to the coupling of the effective interaction $H Z_{\nu} \partial^\mu F^{\mu\nu}$.

virtual const double	deltaG2_hZA_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H Z_{\nu} \partial^\mu F^{\mu\nu}$.

virtual const double	deltaG2_hZZ () const
	The new physics contribution to the coupling of the effective interaction $H Z_{\nu} \partial^\mu Z^{\mu\nu}$.

virtual const double	deltaG2_hZZ_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H Z_{\nu} \partial^\mu Z^{\mu\nu}$.

virtual const double	deltaG3_hWW () const
	The new physics contribution to the coupling of the effective interaction $H W_{\mu}^\dagger W^{\mu}$.

virtual const double	deltaG3_hWW_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H W_{\mu}^\dagger W^{\mu}$.

virtual const double	deltaG3_hZZ () const
	The new physics contribution to the coupling of the effective interaction $H Z_{\mu} Z^{\mu}$.

virtual const double	deltaG3_hZZ_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H Z_{\mu} Z^{\mu}$.

const double	deltag3G () const
	The new physics contribution to the coupling of the effective interaction $f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C$.

gslpp::complex	deltaG_Aff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$.

gslpp::complex	deltaG_Gff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $G_{\mu\nu}^A \bar{f}\sigma^{\mu\nu} T_A f$.

virtual const double	deltaG_hAA () const
	The new physics contribution to the coupling of the effective interaction $H F_{\mu\nu} F^{\mu\nu}$.

virtual const double	deltaG_hAA_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H F_{\mu\nu} F^{\mu\nu}$.

virtual const double	deltaG_hAARatio () const
	The full new physics contribution to the coupling of the effective interaction $H F_{\mu\nu} F^{\mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value.

virtual const double	deltaG_hAARatio_mu (const double mu) const
	The full new physics contribution to the coupling of the effective interaction $H F_{\mu\nu} F^{\mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value.

gslpp::complex	deltaG_hAff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$.

virtual gslpp::complex	deltaG_hff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H f\bar{f}$.

virtual gslpp::complex	deltaG_hff_mu (const Particle p, const double mu) const
	The new physics contribution to the coupling of the effective interaction $H f\bar{f}$.

gslpp::complex	deltaG_hGff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H G_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$.

virtual const double	deltaG_hgg () const
	The new physics contribution to the coupling of the effective interaction $H G_{\mu\nu}^AG^{A \mu\nu}$.

virtual const double	deltaG_hgg_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H G_{\mu\nu}^AG^{A \mu\nu}$.

virtual const double	deltaG_hggRatio () const
	The full new physics contribution to the coupling of the effective interaction $H G_{\mu\nu}^AG^{A \mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value.

virtual const double	deltaG_hggRatio_mu (const double mu) const
	The full new physics contribution to the coupling of the effective interaction $H G_{\mu\nu}^AG^{A \mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value.

virtual const double	deltaG_hhhRatio () const
	The new physics contribution to the Higgs self-coupling $ H H H$. Normalized to the SM value.

virtual const double	deltaG_hhhRatio_mu (const double mu) const
	The new physics contribution to the Higgs self-coupling $ H H H$. Normalized to the SM value.

gslpp::complex	deltaG_hZff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$.

gslpp::complex	deltaG_Zff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$.

virtual const double	deltaGA_f (const Particle p) const
	New physics contribution to the neutral-current axial-vector coupling $g_A^f$.

virtual const double	deltaGamma_W () const
	The new physics contribution to the total decay width of the $W$ boson, $\delta \Gamma_W$.

virtual const double	deltaGamma_Wff (const Particle fi, const Particle fj) const
	The new physics contribution to the decay width of the $W$ boson into a given fermion pair, $\delta \Gamma_Z^{f}$.

virtual const double	deltaGamma_Z () const
	The new physics contribution to the total decay width of the $Z$ boson, $\delta \Gamma_Z$.

virtual const double	deltaGamma_Zf (const Particle f) const
	The new physics contribution to the decay width of the $Z$ boson into a given fermion pair, $\delta \Gamma_Z^{f}$.

const double	deltaGammaH2d2dRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2d2d)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2d2dRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2d2d)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2e2muRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2e 2\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2e2muRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2e 2\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2e2vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2e2v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2e2vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2e2v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2evRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2ev)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2evRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2ev)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2L2dRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2d)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2L2dRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2d)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2L2LRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2L')$ ( $L,L'=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2L2LRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2L')$ ( $L,L'=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2L2uRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2u)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2L2uRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2u)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2L2v2Ratio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2L2v2Ratio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2L2vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2l2vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2l2v)$ ( $l=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2L2vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2l2vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2l2v)$ ( $l=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2Lv2Ratio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2Lv2Ratio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2LvRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2LvRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2mu2vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2\mu 2v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2mu2vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2\mu 2v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2muvRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2\mu v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2muvRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2\mu v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2u2dRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2u2d)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2u2dRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2u2d)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2u2uRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2u2u)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2u2uRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2u2u)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2udRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2ud)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2udRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2ud)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2v2dRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2v2d)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2v2dRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2v2d)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2v2uRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2v2u)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2v2uRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2v2u)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH2v2vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2v2v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH2v2vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2v2v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH4dRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4d)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH4dRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4d)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH4eRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4e)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH4eRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4e)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH4fCCRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4f, CC)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH4fCCRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4f, CC)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH4fNCRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4f, NC)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH4fNCRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4f, NC)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH4fRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4f)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH4fRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4f)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH4L2Ratio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH4L2Ratio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH4LRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH4lRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4l)$ ( $l=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH4LRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH4lRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4l)$ ( $l=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH4muRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH4muRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH4uRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4u)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH4uRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4u)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaH4vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaH4vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHbbRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to bb)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHbbRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to bb)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHccRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to cc)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHccRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to cc)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHevmuvRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to e\nu \mu\nu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHevmuvRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to e\nu \mu\nu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHffRatio1 (const double mf, const double CifH) const
	The ratio of the $\Gamma(H\to ff)$ in the current model and in the Standard Model.

const double	deltaGammaHffRatio2 (const double mf, const double CifH) const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the ratio of the $\Gamma(H\to ff)$ in the current model and in the Standard Model at order Lambd.

const double	deltaGammaHgagaRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to \gamma\gamma)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHgagaRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to \gamma\gamma)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHggRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to gg)$ in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.

const double	deltaGammaHggRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to gg)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHll_vvorjjRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to l l \nu\nu, l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHll_vvorjjRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to l l \nu\nu, l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHlv_lvorjjRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to l \nu l \nu, l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHlv_lvorjjRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to l \nu l \nu, l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHlvjjRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHlvjjRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHLvudRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Lvud)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHLvudRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Lvud)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHLvvLRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to LvvL)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHLvvLRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to LvvL)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHmumuRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to \mu\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHmumuRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to \mu\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHssRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ss)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHssRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ss)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHtautauRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to \tau\tau)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHtautauRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to \tau\tau)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHudduRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to uddu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHudduRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to uddu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHWffRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to W f f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHWffRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to W f f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHWjjRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to W j j)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHWjjRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to W j j)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHWlvRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Wl\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHWlvRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Wl\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHWW2l2vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to l\nu l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHWW2l2vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to l\nu l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHWW4fRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHWW4fRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHWW4jRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to 4j)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHWW4jRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to 4j)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHWWRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHWWRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZddRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z d d)$ ( $d=d,s,b $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZddRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z d d)$ ( $d=d,s,b $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZeeRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Zee)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZeeRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Zee)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZffRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z ff)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZffRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z ff)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZgaRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z\gamma)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZgaRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z\gamma)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZllRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Zll)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZllRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Zll)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZmumuRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z\mu\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZmumuRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z\mu\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZuuRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z u u)$ ( $u=u,c $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZuuRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z u u)$ ( $u=u,c $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZvvRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z\nu\nu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZvvRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z\nu\nu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ2e2muRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 2e2\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ2e2muRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 2e2\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4dRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4 d)$ ( $d=d,s,b $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4dRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4 d)$ ( $d=d,s,b $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4eRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4e)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4eRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4e)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4fRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4fRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4lRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4l)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4lRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4l)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4muRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4muRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4uRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4 u)$ ( $u=u,c $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4uRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4 u)$ ( $u=u,c $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4\nu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZZ4vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4\nu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

const double	deltaGammaHZZRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

const double	deltaGammaHZZRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

virtual const double	deltaGammaTotalRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H)$ in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.

virtual const double	deltaGammaTotalRatio1noError () const
	The new physics contribution to the ratio of the $\Gamma(H)$ in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors.

virtual const double	deltaGammaTotalRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H)$ in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients.

virtual const double	DeltaGF () const
	New physics contribution to the Fermi constant.

const double	deltaGL_f (const Particle p) const
	New physics contribution to the neutral-current left-handed coupling $g_L^f$.

const double	deltaGL_f_mu (const Particle p, const double mu) const
	New physics contribution to the neutral-current left-handed coupling $g_L^f$.

virtual gslpp::complex	deltaGL_Wff (const Particle pbar, const Particle p) const
	New physics contribution to the charged current coupling $W_\mu \bar{f_L}\gamma^mu f_L$.

virtual gslpp::complex	deltaGL_Wff_mu (const Particle pbar, const Particle p, const double mu) const
	New physics contribution to the charged current coupling $W_\mu \bar{f_L}\gamma^mu f_L$.

gslpp::complex	deltaGL_Wffh (const Particle pbar, const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H W_\mu \bar{f_L}\gamma^mu f_L$.

const double	deltaGL_Zffh (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H Z_\mu \bar{f_L}\gamma^mu f_L$.

virtual const double	deltaGmu () const
	The relative correction to the muon decay constant, $\delta G_\mu/G_\mu$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltaGmu2 () const
	The relative correction to the muon decay constant, $(\delta G_\mu/G_\mu)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

const double	deltaGR_f (const Particle p) const
	New physics contribution to the neutral-current right-handed coupling $g_R^f$.

const double	deltaGR_f_mu (const Particle p, const double mu) const
	New physics contribution to the neutral-current right-handed coupling $g_R^f$.

virtual gslpp::complex	deltaGR_Wff (const Particle pbar, const Particle p) const
	New physics contribution to the charged current coupling $W_\mu \bar{f_R}\gamma^mu f_R$.

virtual gslpp::complex	deltaGR_Wff_mu (const Particle pbar, const Particle p, const double mu) const
	New physics contribution to the charged current coupling $W_\mu \bar{f_R}\gamma^mu f_R$.

gslpp::complex	deltaGR_Wffh (const Particle pbar, const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H W_\mu \bar{f_R}\gamma^mu f_R$.

const double	deltaGR_Zffh (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H Z_\mu \bar{f_R}\gamma^mu f_R$.

virtual const double	deltaGV_f (const Particle p) const
	New physics contribution to the neutral-current vector coupling $g_V^f$.

virtual const double	deltaGwd6 () const
	The relative NP corrections to the width of the $W$ boson, $\delta \Gamma_W/\Gamma_W$.

virtual const double	deltaGwd62 () const
	The relative NP corrections to the width of the $W$ boson squared, $(\delta \Gamma_W/\Gamma_W)^2$.

virtual const double	deltaGzd6 () const
	The relative NP corrections to the width of the $Z$ boson, $\delta \Gamma_Z/\Gamma_Z$.

virtual const double	deltaGzd62 () const
	The relative NP corrections to the width of the $Z$ boson squared, $(\delta \Gamma_Z/\Gamma_Z)^2$.

virtual const double	deltaH3L1 (double C1) const
	The coefficient of the 1-loop linear term in the Higgs selfcoupling.

virtual const double	deltaH3L2 (double C1) const
	The coefficient of the 1-loop quadratic term in the Higgs selfcoupling.

virtual const double	deltaKgammaNP (const double mu) const
	The new physics contribution to the anomalous triple gauge coupling $\kappa_{\gamma}$.

virtual const double	deltaKgammaNPEff () const
	The new physics contribution to the effective anomalous triple gauge coupling $\kappa_{\gamma}^{Eff}$ from arXiv: 1708.09079 [hep-ph].

virtual const double	deltaKZNP (const double mu) const
	The new physics contribution to the anomalous triple gauge coupling $\kappa_{Z}$.

virtual const double	deltamb () const
	The relative correction to the mass of the $b$ quark, $\delta m_b/m_b$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltamb2 () const
	The relative correction to the mass of the $b$ quark squared, $(\delta m_b/m_b)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltamc () const
	The relative correction to the mass of the $c$ quark, $\delta m_c/m_c$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltamc2 () const
	The relative correction to the mass of the $c$ quark squared, $(\delta m_c/m_c)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltaMh () const
	The relative correction to the mass of the $H$ boson, $\delta M_H/M_H$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltaMh2 () const
	The relative correction to the mass of the $H$ boson squared, $(\delta M_H/M_H)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

const double	deltaMLL2_f (const Particle f, const double s, const double t) const

const double	deltaMLR2_f (const Particle f, const double s) const

const double	deltaMLR2t_e (const double s, const double t) const

const double	deltaMRL2_f (const Particle f, const double s) const

const double	deltaMRL2t_e (const double s, const double t) const

const double	deltaMRR2_f (const Particle f, const double s, const double t) const

virtual const double	deltamt () const
	The relative correction to the mass of the $t$ quark, $\delta m_t/m_t$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltamt2 () const
	The relative correction to the mass of the $t$ quark squared, $(\delta m_t/m_t)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltamtau () const
	The relative correction to the mass of the $\tau$ lepton, $\delta m_\tau/m_\tau$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltamtau2 () const
	The relative correction to the mass of the $\tau$ lepton squared, $(\delta m_\tau/m_\tau)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltaMw () const
	The relative correction to the mass of the $W$ boson, $\delta M_W/M_W$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltaMw2 () const
	The relative correction to the mass of the $W$ boson squared, $(\delta M_W/M_W)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltaMwd6 () const
	The relative NP corrections to the mass of the $W$ boson, $\delta M_W/M_W$.

virtual const double	deltaMwd62 () const
	The relative NP corrections to the mass of the $W$ boson squared, $(\delta M_W/M_W)^2$.

virtual const double	deltaMz () const
	The relative correction to the mass of the $Z$ boson, $\delta M_Z/M_Z$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	deltaMz2 () const
	The relative correction to the mass of the $Z$ boson squared, $(\delta M_Z/M_Z)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

virtual const double	DeltaOalphtoW (const double dOSMdalpha, const double mu) const
	Difference in prediction in $\alpha$ scheme and W mass scheme, computed from observable in $\alpha$ scheme. Difference at tree level.

virtual const double	DeltaOWtoalph (const double dOSMdMW, const double mu) const
	Difference in prediction in $\alpha$ scheme and W mass scheme, computed from observable in W mass scheme. Difference at tree level.

virtual const double	deltaR0_f (const Particle f) const
	The new physics contribution to the ratio $R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell$, $R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}$ and $R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}$, for charged leptons, quarks and neutrinos, respectively.

virtual const double	deltaSigmaHadron () const
	The new physics contribution to the cross section for the process $e^+ e^-\to Z\to \mathrm{hadrons}$ at the $Z$ pole, $\delta \sigma_h^0$.

virtual const double	deltaxseeWW4fLEP2 (const double sqrt_s, const int fstate) const
	The new physics contribution to the cross section in pb for $e^+ e^- \to W^+ W^- \to 4f $, with $ 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) $ the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].

virtual const double	deltaxseeWWtotLEP2 (const double sqrt_s) const
	The new physics contribution to the total cross section in pb for $e^+ e^- \to W^+ W^-$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].

virtual const double	deltayb_HB (const double mu) const
	The Higgs-basis coupling $\delta y_b$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	deltayc_HB (const double mu) const
	The Higgs-basis coupling $\delta y_c$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	deltaymu_HB (const double mu) const
	The Higgs-basis coupling $\delta y_\mu$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	deltays_HB (const double mu) const
	The Higgs-basis coupling $\delta y_s$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	deltayt_HB (const double mu) const
	The Higgs-basis coupling $\delta y_t$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	deltaytau_HB (const double mu) const
	The Higgs-basis coupling $\delta y_\tau$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	delU_gCC (const double mu) const
	Universal indirect correction to EW charged currents.

virtual const double	delU_gNC (const double mu) const
	Universal indirect correction to EW neutral currents.

virtual const double	dxsdcoseeWWlvjjLEP2 (const double sqrt_s, const int bin) const
	The differential cross section in pb for $e^+ e^- \to W^+ W^- \to lv jj $, with $ l= e,\mu $ for the 4 $ cos{\theta}$ bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph].

virtual const double	dxseeWWdcos (const double sqrt_s, const double cos) const
	The differential distribution for $e^+ e^- \to W^+ W^- \to jj \ell \nu$, with $\ell= e, \mu$, as a function of the $W$ polar angle.

virtual const double	dxseeWWdcosBin (const double sqrt_s, const double cos1, const double cos2) const
	The integral of differential distribution for $e^+ e^- \to W^+ W^- \to jj \ell \nu$, with $\ell= e, \mu$ in a given bin of the $W$ polar angle.

virtual const double	Gamma_Z () const
	The total decay width of the $Z$ boson, $\Gamma_Z$.

virtual const double	Gamma_Zf (const Particle f) const
	The decay width of the $Z$ boson into a given fermion pair, $\Gamma_Z^{f}$.

const double	GammaH2d2dRatio () const
	The ratio of the $\Gamma(H\to 2d2d)$ in the current model and in the Standard Model.

const double	GammaH2e2muRatio () const
	The ratio of the $\Gamma(H\to 2e 2\mu)$ in the current model and in the Standard Model.

const double	GammaH2e2vRatio () const
	The ratio of the $\Gamma(H\to 2e2v)$ in the current model and in the Standard Model.

const double	GammaH2evRatio () const
	The ratio of the $\Gamma(H\to 2ev)$ in the current model and in the Standard Model.

const double	GammaH2L2dRatio () const
	The ratio of the $\Gamma(H\to 2L2d)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

const double	GammaH2L2LRatio () const
	The ratio of the $\Gamma(H\to 2L2L')$ ( $L,L'=e,\mu,\tau$) in the current model and in the Standard Model.

const double	GammaH2L2uRatio () const
	The ratio of the $\Gamma(H\to 2L2u)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

const double	GammaH2L2v2Ratio () const
	The ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu$) in the current model and in the Standard Model.

const double	GammaH2L2vRatio () const
	The ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

const double	GammaH2l2vRatio () const
	The ratio of the $\Gamma(H\to 2l2v)$ ( $l=e,\mu$) in the current model and in the Standard Model.

const double	GammaH2Lv2Ratio () const
	The ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu$) in the current model and in the Standard Model.

const double	GammaH2LvRatio () const
	The ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

const double	GammaH2mu2vRatio () const
	The ratio of the $\Gamma(H\to 2\mu 2v)$ in the current model and in the Standard Model.

const double	GammaH2muvRatio () const
	The ratio of the $\Gamma(H\to 2\mu v)$ in the current model and in the Standard Model.

const double	GammaH2u2dRatio () const
	The ratio of the $\Gamma(H\to 2u2d)$ in the current model and in the Standard Model.

const double	GammaH2u2uRatio () const
	The ratio of the $\Gamma(H\to 2u2u)$ in the current model and in the Standard Model.

const double	GammaH2udRatio () const
	The ratio of the $\Gamma(H\to 2ud)$ in the current model and in the Standard Model.

const double	GammaH2v2dRatio () const
	The ratio of the $\Gamma(H\to 2v2d)$ in the current model and in the Standard Model.

const double	GammaH2v2uRatio () const
	The ratio of the $\Gamma(H\to 2v2u)$ in the current model and in the Standard Model.

const double	GammaH2v2vRatio () const
	The ratio of the $\Gamma(H\to 2v2v)$ in the current model and in the Standard Model.

const double	GammaH4dRatio () const
	The ratio of the $\Gamma(H\to 4d)$ in the current model and in the Standard Model.

const double	GammaH4eRatio () const
	The ratio of the $\Gamma(H\to 4e)$ in the current model and in the Standard Model.

const double	GammaH4fCCRatio () const
	The ratio of the $\Gamma(H\to 4f)$ via CC in the current model and in the Standard Model.

const double	GammaH4fNCRatio () const
	The ratio of the $\Gamma(H\to 4f)$ via NC in the current model and in the Standard Model.

const double	GammaH4fRatio () const
	The ratio of the $\Gamma(H\to 4f)$ in the current model and in the Standard Model.

const double	GammaH4L2Ratio () const
	The ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu$) in the current model and in the Standard Model.

const double	GammaH4LRatio () const
	The ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

const double	GammaH4lRatio () const
	The ratio of the $\Gamma(H\to 4l)$ ( $l=e,\mu$) in the current model and in the Standard Model.

const double	GammaH4muRatio () const
	The ratio of the $\Gamma(H\to 4\mu)$ in the current model and in the Standard Model.

const double	GammaH4uRatio () const
	The ratio of the $\Gamma(H\to 4u)$ in the current model and in the Standard Model.

const double	GammaH4vRatio () const
	The ratio of the $\Gamma(H\to 4v)$ in the current model and in the Standard Model.

const double	GammaHbbRatio () const
	The ratio of the $\Gamma(H\to bb)$ in the current model and in the Standard Model.

const double	GammaHccRatio () const
	The ratio of the $\Gamma(H\to cc)$ in the current model and in the Standard Model.

const double	GammaHevmuvRatio () const
	The ratio of the $\Gamma(H\to e\nu \mu\nu)$ in the current model and in the Standard Model.

const double	GammaHgagaRatio () const
	The ratio of the $\Gamma(H\to \gamma\gamma)$ in the current model and in the Standard Model.

const double	GammaHggRatio () const
	The ratio of the $\Gamma(H\to gg)$ in the current model and in the Standard Model.

const double	GammaHll_vvorjjRatio () const
	The ratio of the $\Gamma(H\to l l \nu\nu, l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model.

const double	GammaHlv_lvorjjRatio () const
	The ratio of the $\Gamma(H\to l \nu l \nu, l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model.

const double	GammaHlvjjRatio () const
	The ratio of the $\Gamma(H\to l l j j)$ ( $l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. @return $\Gamma(H\to l l j j) $/$\Gamma(H\to l l j j)_{\mathrm{SM}} $ / const double GammaHlljjRatio() const; /* @brief The new physics contribution to the ratio of the $\Gamma(H\to l l j j) $ ($l=e,\mu,~~j\not=b $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) @return $\delta \Gamma(H\to l l j j) $/$\Gamma(H\to l l j j)_{\mathrm{SM}} $ / const double deltaGammaHlljjRatio1() const; /* @brief The new physics contribution to the ratio of the $\Gamma(H\to l l j j) $ ($l=e,\mu,~~j\not=b $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) @return $\delta \Gamma(H\to l l j j) $/$\Gamma(H\to l l j j)_{\mathrm{SM}} $ / const double deltaGammaHlljjRatio2() const; /* @brief The ratio of the Br$(H\to l l j j) $ ($l=e,\mu,~~j\not=b $) in the current model and in the Standard Model. @return Br$(H\to l l j j) $/Br$(H\to l l j j)_{\mathrm{SM}} $ / virtual const double BrHlljjRatio() const; /* @brief The ratio of the $\Gamma(H\to l \nu j j) $ ($l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model.

const double	GammaHLvudRatio () const
	The ratio of the $\Gamma(H\to Lvud)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

const double	GammaHLvvLRatio () const
	The ratio of the $\Gamma(H\to LvvL)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

const double	GammaHmumuRatio () const
	The ratio of the $\Gamma(H\to \mu\mu)$ in the current model and in the Standard Model.

const double	GammaHssRatio () const
	The ratio of the $\Gamma(H\to ss)$ in the current model and in the Standard Model.

const double	GammaHtautauRatio () const
	The ratio of the $\Gamma(H\to \tau\tau)$ in the current model and in the Standard Model.

const double	GammaHudduRatio () const
	The ratio of the $\Gamma(H\to uddu)$ in the current model and in the Standard Model.

const double	GammaHWffRatio () const
	The ratio of the $\Gamma(H\to W f f)$, with $f$ any fermion, in the current model and in the Standard Model.

const double	GammaHWjjRatio () const
	The ratio of the $\Gamma(H\to W j j)$ in the current model and in the Standard Model.

const double	GammaHWlvRatio () const
	The ratio of the $\Gamma(H\to W l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model.

const double	GammaHWW2l2vRatio () const
	The ratio of the $\Gamma(H\to WW^*\to l\nu l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model.

const double	GammaHWW4fRatio () const
	The ratio of the $\Gamma(H\to WW^*\to 4f)$, with $f$ any fermion, in the current model and in the Standard Model.

const double	GammaHWW4jRatio () const
	The ratio of the $\Gamma(H\to WW^*\to 4j)$ in the current model and in the Standard Model.

const double	GammaHWWRatio () const
	The ratio of the $\Gamma(H\to WW)$ in the current model and in the Standard Model.

const double	GammaHZddRatio () const
	The ratio of the $\Gamma(H\to Zd d)$ ( $d=d,s,b $) in the current model and in the Standard Model.

const double	GammaHZeeRatio () const
	The ratio of the $\Gamma(H\to Zee)$ in the current model and in the Standard Model.

const double	GammaHZffRatio () const
	The ratio of the $\Gamma(H\to Zff)$, with $f$ any fermion, in the current model and in the Standard Model.

const double	GammaHZgaRatio () const
	The ratio of the $\Gamma(H\to Z\gamma)$ in the current model and in the Standard Model.

const double	GammaHZllRatio () const
	The ratio of the $\Gamma(H\to Zll)$ ( $l=e,\mu $) in the current model and in the Standard Model.

const double	GammaHZmumuRatio () const
	The ratio of the $\Gamma(H\to Z\mu\mu)$ in the current model and in the Standard Model.

const double	GammaHZuuRatio () const
	The ratio of the $\Gamma(H\to Zu u)$ ( $u=u,c $) in the current model and in the Standard Model.

const double	GammaHZvvRatio () const
	The ratio of the $\Gamma(H\to Z\nu\nu)$ in the current model and in the Standard Model.

const double	GammaHZZ2e2muRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 2e2\mu)$ in the current model and in the Standard Model.

const double	GammaHZZ4dRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4 d)$ ( $d=d,s,b $) in the current model and in the Standard Model.

const double	GammaHZZ4eRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4e)$ in the current model and in the Standard Model.

const double	GammaHZZ4fRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4f)$, with $f$ any fermion, in the current model and in the Standard Model.

const double	GammaHZZ4lRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4l)$ ( $l=e,\mu $) in the current model and in the Standard Model.

const double	GammaHZZ4muRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4\mu)$ in the current model and in the Standard Model.

const double	GammaHZZ4uRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4 u)$ ( $u=u,c $) in the current model and in the Standard Model.

const double	GammaHZZ4vRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4\nu)$ in the current model and in the Standard Model.

const double	GammaHZZRatio () const
	The ratio of the $\Gamma(H\to ZZ)$ in the current model and in the Standard Model.

virtual const double	GammaW () const
	The total width of the $W$ boson, $\Gamma_W$.

virtual const double	GammaW (const Particle fi, const Particle fj) const
	A partial decay width of the $W$ boson decay into a SM fermion pair.

void	GenerateSMInitialConditions ()
	Generates the initial condition for the Standard Model parameters.

double	getCG_LNP () const
	Return CG_LNP.

double	getLambda_NP () const
	Return Lambda_NP.

virtual NPSMEFTd6GeneralMatching &	getMatching () const
	A method to get the Matching object for this model.

virtual const double	IctW_TWG (const double mu) const

virtual const double	IctZ_TWG (const double mu) const

virtual const double	intDMLL2eus2 (const double s, const double t0, const double t1) const

virtual const double	intDMLR2etildest2 (const double s, const double t0, const double t1) const

virtual const double	intDMLR2ets2 (const double s, const double t0, const double t1) const

virtual const double	intDMRL2etildest2 (const double s, const double t0, const double t1) const

virtual const double	intDMRL2ets2 (const double s, const double t0, const double t1) const

virtual const double	intDMRR2eus2 (const double s, const double t0, const double t1) const

virtual const double	kappaAeff () const
	The effective coupling $\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}$.

virtual const double	kappabeff () const
	The effective coupling $\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}$.

virtual const double	kappaceff () const
	The effective coupling $\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}$.

virtual const double	kappaGeff () const
	The effective coupling $\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}$.

virtual const double	kappamueff () const
	The effective coupling $\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}$.

virtual const double	kappaseff () const
	The effective coupling $\kappa_{s,eff}=\sqrt{\Gamma_{Hss}/\Gamma_{Hss}^{SM}}$.

virtual const double	kappataueff () const
	The effective coupling $\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}$.

virtual const double	kappaW4feff () const
	The effective coupling $\kappa_{W4f,eff}=\sqrt{\Gamma_{H4f, CC}/\Gamma_{H4f, CC}^{SM}}$.

virtual const double	kappaWeff () const
	The effective coupling $\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}$.

virtual const double	kappaZ4feff () const
	The effective coupling $\kappa_{Z4f,eff}=\sqrt{\Gamma_{H4f, NC}/\Gamma_{H4f, NC}^{SM}}$.

virtual const double	kappaZAeff () const
	The effective coupling $\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}$.

virtual const double	kappaZeff () const
	The effective coupling $\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}$.

virtual const double	lambdaZNP (const double mu) const
	The new physics contribution to the anomalous triple gauge coupling $\lambda_{Z}$.

virtual const double	lambz_HB (const double mu) const
	The Higgs-basis coupling $\lambda_{z}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

virtual const double	mubbH (const double sqrt_s) const
	The ratio $\mu_{bbH}$ between the bbH production cross-section in the current model and in the Standard Model.

virtual const double	mueeHee (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{e^+e^- \to He^+e^-}$ between the $ e^+e^- \to H e^+e^- $ associated production cross-section in the current model and in the Standard Model.

virtual const double	mueeHvv (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{e^+e^- \to H\nu\bar{\nu}}$ between the $ e^+e^- \to H\nu\bar{\nu} $ associated production cross-section in the current model and in the Standard Model.

virtual const double	mueettH (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eettH}$ between the $ e^{+}e^{-}\to t\bar{t} H $ production cross-section in the current model and in the Standard Model.

virtual const double	mueeWBF (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeWBF}$ between the $ e^{+}e^{-}\to \nu\bar{\nu} H $ production cross-section in the current model and in the Standard Model.

virtual const double	mueeWW (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeWW}$ between the $ e^{+}e^{-}\to W^{+}W^{-} $ production cross-section in the current model and in the Standard Model.

virtual const double	mueeZBF (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeZBF}$ between the $ e^{+}e^{-}\to e^{+}e^{-} H $ production cross-section in the current model and in the Standard Model.

virtual const double	mueeZH (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeZH}$ between the $e^{+}e^{-}\to ZH$ associated production cross-section in the current model and in the Standard Model.

virtual const double	mueeZHGen (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeZH}$ between the $ e^{+}e^{-}\to ZH $ associated production cross-section in the current model and in the Standard Model.

virtual const double	mueeZHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeZH}$ between the $ e^{+}e^{-}\to ZH $ associated production cross-section in the current model and in the Standard Model.

virtual const double	mueeZllH (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}$ between the $ e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- $ associated production cross-section in the current model and in the Standard Model.

virtual const double	mueeZllHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}$ between the $ e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- $ associated production cross-section in the current model and in the Standard Model.

virtual const double	mueeZqqH (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeZH, Z \to q \bar{q}}$ between the $ e^{+}e^{-}\to ZH, Z \to q \bar{q} $ associated production cross-section in the current model and in the Standard Model.

virtual const double	mueeZqqHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeZH, Z \to q \bar{q}}$ between the $ e^{+}e^{-}\to ZH, Z \to q \bar{q} $ associated production cross-section in the current model and in the Standard Model.

virtual const double	muepWBF (const double sqrt_s) const
	The ratio $\mu_{epWBF}$ between the $ e^{-} p\to \nu j H $ production cross-section in the current model and in the Standard Model.

virtual const double	muepZBF (const double sqrt_s) const
	The ratio $\mu_{epZBF}$ between the $ e^{-} p\to e^{-} j H $ production cross-section in the current model and in the Standard Model.

virtual const double	muggH (const double sqrt_s) const
	The ratio $\mu_{ggH}$ between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.

virtual const double	muggHbb (const double sqrt_s) const
	The ratio $\mu_{ggH,bb}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

virtual const double	muggHgaga (const double sqrt_s) const
	The ratio $\mu_{ggH,\gamma\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

virtual const double	muggHH (const double sqrt_s) const
	The ratio $\mu_{ggHH}$ between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].)

virtual const double	muggHmumu (const double sqrt_s) const
	The ratio $\mu_{ggH,\mu\mu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

virtual const double	muggHpttH (const double sqrt_s) const
	The ratio $\mu_{ggH+ttH}$ between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	muggHtautau (const double sqrt_s) const
	The ratio $\mu_{ggH,\tau\tau}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

virtual const double	muggHWW (const double sqrt_s) const
	The ratio $\mu_{ggH,WW}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

virtual const double	muggHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{ggH,WW\to 2l2\nu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

virtual const double	muggHZga (const double sqrt_s) const
	The ratio $\mu_{ggH,Z\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

virtual const double	muggHZZ (const double sqrt_s) const
	The ratio $\mu_{ggH,ZZ}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

virtual const double	muggHZZ4l (const double sqrt_s) const
	The ratio $\mu_{ggH,ZZ\to 4l}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

virtual const double	mummH (const double sqrt_s) const
	The ratio $\mu_{\mu\mu H}$ between the $\sigma(\mu \mu \to H)}$ production cross-section in the current model and in the Standard Model.

virtual const double	mummHmm (const double sqrt_s) const
	The ratio $\mu_{\mu\mu H\mu\mu}$ between the $\sigma(\mu \mu \to H \mu \mu)}$ production cross-section in the current model and in the Standard Model.

virtual const double	mummHNWA (const double sqrt_s) const
	The ratio $\mu_{\mu\mu H}$ between the $\sigma(\mu \mu \to H)}$ production cross-section in the current model and in the Standard Model, in the narrow width approximation.

virtual const double	mummHvv (const double sqrt_s) const
	The ratio $\mu_{\mu\mu H\nu\nu}$ between the $\sigma(\mu \mu \to H \nu \nu)}$ production cross-section in the current model and in the Standard Model.

virtual const double	mummttH (const double sqrt_s) const
	The ratio $\mu_{\mu\mu ttH}$ between the $\sigma(\mu \mu \to t\bar{t} H )}$ production cross-section in the current model and in the Standard Model.

virtual const double	mummZH (const double sqrt_s) const
	The ratio $\mu_{\mu\mu ZH}$ between the $\sigma(\mu \mu \to Z H)}$ production cross-section in the current model and in the Standard Model.

virtual const double	mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const
	The number of events in $ p p \to WZ$ in a given $p_{TV}$ bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6General class.

virtual const double	mutH (const double sqrt_s) const
	The ratio $\mu_{tH}$ between the t-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	mutHq (const double sqrt_s) const
	The ratio $\mu_{tHq}$ between the t-q-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	muTHUggHbb (const double sqrt_s) const
	The ratio $\mu_{ggH,bb}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

virtual const double	muTHUggHgaga (const double sqrt_s) const
	The ratio $\mu_{ggH,\gamma\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

virtual const double	muTHUggHmumu (const double sqrt_s) const
	The ratio $\mu_{ggH,\mu\mu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

virtual const double	muTHUggHtautau (const double sqrt_s) const
	The ratio $\mu_{ggH,\tau\tau}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

virtual const double	muTHUggHWW (const double sqrt_s) const
	The ratio $\mu_{ggH,WW}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

virtual const double	muTHUggHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{ggH,WW\to 2l2\nu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

virtual const double	muTHUggHZga (const double sqrt_s) const
	The ratio $\mu_{ggH,Z\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

virtual const double	muTHUggHZgamumu (const double sqrt_s) const
	The ratio $\mu_{ggH,Z\gamma\to \gamma 2\mu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z \gamma\to \gamma 2\mu$ in the current model and in the Standard Model.

virtual const double	muTHUggHZZ (const double sqrt_s) const
	The ratio $\mu_{ggH,ZZ}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

virtual const double	muTHUggHZZ4l (const double sqrt_s) const
	The ratio $\mu_{ggH,ZZ\to 4l}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

virtual const double	muTHUggHZZ4mu (const double sqrt_s) const
	The ratio $\mu_{ggH,ZZ\to 4\mu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*\to 4\mu$ in the current model and in the Standard Model.

virtual const double	muTHUttHbb (const double sqrt_s) const
	The ratio $\mu_{ttH,bb}$ between the ttH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

virtual const double	muTHUttHgaga (const double sqrt_s) const
	The ratio $\mu_{ttH,\gamma\gamma}$ between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

virtual const double	muTHUttHmumu (const double sqrt_s) const
	The ratio $\mu_{ttH,\mu\mu}$ between the ttH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

virtual const double	muTHUttHtautau (const double sqrt_s) const
	The ratio $\mu_{ttH,\tau\tau}$ between the ttH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

virtual const double	muTHUttHWW (const double sqrt_s) const
	The ratio $\mu_{ttH,WW}$ between the ttH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

virtual const double	muTHUttHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{ttH,WW\to 2l2\nu}$ between the ttH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

virtual const double	muTHUttHZga (const double sqrt_s) const
	The ratio $\mu_{ttH,Z\gamma}$ between the ttH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

virtual const double	muTHUttHZZ (const double sqrt_s) const
	The ratio $\mu_{ttH,ZZ}$ between the ttH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

virtual const double	muTHUttHZZ4l (const double sqrt_s) const
	The ratio $\mu_{ttH,ZZ\to 4l}$ between the ttH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

virtual const double	muTHUVBFBRinv (const double sqrt_s) const
	The ratio $\mu_{VBF}$ between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.

virtual const double	muTHUVBFHbb (const double sqrt_s) const
	The ratio $\mu_{VBF,bb}$ between the VBF Higgs production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

virtual const double	muTHUVBFHgaga (const double sqrt_s) const
	The ratio $\mu_{VBF,\gamma\gamma}$ between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

virtual const double	muTHUVBFHinv (const double sqrt_s) const
	The ratio $\mu_{VBF,inv}$ between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.

virtual const double	muTHUVBFHmumu (const double sqrt_s) const
	The ratio $\mu_{VBF,\mu\mu}$ between the VBF Higgs production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

virtual const double	muTHUVBFHtautau (const double sqrt_s) const
	The ratio $\mu_{VBF,\tau\tau}$ between the VBF Higgs production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

virtual const double	muTHUVBFHWW (const double sqrt_s) const
	The ratio $\mu_{VBF,WW}$ between the VBF Higgs production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

virtual const double	muTHUVBFHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{VBF,WW\to 2l2\nu}$ between the VBF Higgs production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

virtual const double	muTHUVBFHZga (const double sqrt_s) const
	The ratio $\mu_{VBF,Z\gamma}$ between the VBF Higgs production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

virtual const double	muTHUVBFHZZ (const double sqrt_s) const
	The ratio $\mu_{VBF,ZZ}$ between the VBF Higgs production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

virtual const double	muTHUVBFHZZ4l (const double sqrt_s) const
	The ratio $\mu_{VBF,ZZ\to 4l}$ between the VBF Higgs production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

virtual const double	muTHUVHbb (const double sqrt_s) const
	The ratio $\mu_{VH,bb}$ between the VH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

virtual const double	muTHUVHBRinv (const double sqrt_s) const
	The ratio $\mu_{VH}$ between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.

virtual const double	muTHUVHgaga (const double sqrt_s) const
	The ratio $\mu_{VH,\gamma\gamma}$ between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

virtual const double	muTHUVHinv (const double sqrt_s) const
	The ratio $\mu_{VH,inv}$ between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.

virtual const double	muTHUVHmumu (const double sqrt_s) const
	The ratio $\mu_{VH,\mu\mu}$ between the VH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

virtual const double	muTHUVHtautau (const double sqrt_s) const
	The ratio $\mu_{VH,\tau\tau}$ between the VH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

virtual const double	muTHUVHWW (const double sqrt_s) const
	The ratio $\mu_{VH,WW}$ between the VH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

virtual const double	muTHUVHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{VH,WW\to 2l2\nu}$ between the VH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

virtual const double	muTHUVHZga (const double sqrt_s) const
	The ratio $\mu_{VH,Z\gamma}$ between the VH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

virtual const double	muTHUVHZZ (const double sqrt_s) const
	The ratio $\mu_{VH,ZZ}$ between the VH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

virtual const double	muTHUVHZZ4l (const double sqrt_s) const
	The ratio $\mu_{VH,ZZ\to 4l}$ between the VH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

virtual const double	muTHUWHbb (const double sqrt_s) const
	The ratio $\mu_{WH,bb}$ between the WH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

virtual const double	muTHUWHgaga (const double sqrt_s) const
	The ratio $\mu_{WH,\gamma\gamma}$ between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

virtual const double	muTHUWHmumu (const double sqrt_s) const
	The ratio $\mu_{WH,\mu\mu}$ between the WH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

virtual const double	muTHUWHtautau (const double sqrt_s) const
	The ratio $\mu_{WH,\tau\tau}$ between the WH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

virtual const double	muTHUWHWW (const double sqrt_s) const
	The ratio $\mu_{WH,WW}$ between the WH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

virtual const double	muTHUWHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{WH,WW\to 2l2\nu}$ between the WH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

virtual const double	muTHUWHZga (const double sqrt_s) const
	The ratio $\mu_{WH,Z\gamma}$ between the WH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

virtual const double	muTHUWHZZ (const double sqrt_s) const
	The ratio $\mu_{WH,ZZ}$ between the WH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

virtual const double	muTHUWHZZ4l (const double sqrt_s) const
	The ratio $\mu_{WH,ZZ\to 4l}$ between the WH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

virtual const double	muTHUZHbb (const double sqrt_s) const
	The ratio $\mu_{ZH,bb}$ between the ZH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

virtual const double	muTHUZHgaga (const double sqrt_s) const
	The ratio $\mu_{ZH,\gamma\gamma}$ between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

virtual const double	muTHUZHmumu (const double sqrt_s) const
	The ratio $\mu_{ZH,\mu\mu}$ between the ZH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

virtual const double	muTHUZHtautau (const double sqrt_s) const
	The ratio $\mu_{ZH,\tau\tau}$ between the ZH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

virtual const double	muTHUZHWW (const double sqrt_s) const
	The ratio $\mu_{ZH,WW}$ between the ZH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

virtual const double	muTHUZHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{ZH,WW\to 2l2\nu}$ between the ZH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

virtual const double	muTHUZHZga (const double sqrt_s) const
	The ratio $\mu_{ZH,Z\gamma}$ between the ZH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

virtual const double	muTHUZHZZ (const double sqrt_s) const
	The ratio $\mu_{ZH,ZZ}$ between the ZH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

virtual const double	muTHUZHZZ4l (const double sqrt_s) const
	The ratio $\mu_{ZH,ZZ\to 4l}$ between the ZH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

virtual const double	muttH (const double sqrt_s) const
	The ratio $\mu_{ttH}$ between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	muttHbb (const double sqrt_s) const
	The ratio $\mu_{ttH,bb}$ between the ttH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

virtual const double	muttHgaga (const double sqrt_s) const
	The ratio $\mu_{ttH,\gamma\gamma}$ between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

virtual const double	muttHgagaZeeboost (const double sqrt_s) const
	The ratio $\sigma(ttH)/\sigma(ttZ)$ in the $H\to b\bar{b}$, $Z\to e^+e^-$ channel channel in the current model and in the Standard Model.

virtual const double	muttHmumu (const double sqrt_s) const
	The ratio $\mu_{ttH,\mu\mu}$ between the ttH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

virtual const double	muttHtautau (const double sqrt_s) const
	The ratio $\mu_{ttH,\tau\tau}$ between the ttH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

virtual const double	muttHWW (const double sqrt_s) const
	The ratio $\mu_{ttH,WW}$ between the ttH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

virtual const double	muttHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{ttH,WW\to 2l2\nu}$ between the ttH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

virtual const double	muttHZbbboost (const double sqrt_s) const
	The ratio $\sigma(ttH)/\sigma(ttZ)$ in the $H,Z\to b\bar{b}$ channel in the current model and in the Standard Model.

virtual const double	muttHZga (const double sqrt_s) const
	The ratio $\mu_{ttH,Z\gamma}$ between the ttH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

virtual const double	muttHZZ (const double sqrt_s) const
	The ratio $\mu_{ttH,ZZ}$ between the ttH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

virtual const double	muttHZZ4l (const double sqrt_s) const
	The ratio $\mu_{ttH,ZZ\to 4l}$ between the ttH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

virtual const double	muVBF (const double sqrt_s) const
	The ratio $\mu_{VBF}$ between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.

virtual const double	muVBFgamma (const double sqrt_s) const
	The ratio $\mu_{VBF+\gamma}$ between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model.

virtual const double	muVBFHbb (const double sqrt_s) const
	The ratio $\mu_{VBF,bb}$ between the VBF Higgs production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

virtual const double	muVBFHgaga (const double sqrt_s) const
	The ratio $\mu_{VBF,\gamma\gamma}$ between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

virtual const double	muVBFHmumu (const double sqrt_s) const
	The ratio $\mu_{VBF,\mu\mu}$ between the VBF Higgs production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

virtual const double	muVBFHtautau (const double sqrt_s) const
	The ratio $\mu_{VBF,\tau\tau}$ between the VBF Higgs production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

virtual const double	muVBFHWW (const double sqrt_s) const
	The ratio $\mu_{VBF,WW}$ between the VBF Higgs production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

virtual const double	muVBFHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{VBF,WW\to 2l2\nu}$ between the VBF Higgs production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

virtual const double	muVBFHZga (const double sqrt_s) const
	The ratio $\mu_{VBF,Z\gamma}$ between the VBF Higgs production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

virtual const double	muVBFHZZ (const double sqrt_s) const
	The ratio $\mu_{VBF,ZZ}$ between the VBF Higgs production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

virtual const double	muVBFHZZ4l (const double sqrt_s) const
	The ratio $\mu_{VBF,ZZ\to 4l}$ between the VBF Higgs production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

virtual const double	muVBFpVH (const double sqrt_s) const
	The ratio $\mu_{VBF+VH}$ between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model.

virtual const double	muVH (const double sqrt_s) const
	The ratio $\mu_{VH}$ between the WH+ZH associated production cross-section in the current model and in the Standard Model.

virtual const double	muVHbb (const double sqrt_s) const
	The ratio $\mu_{VH,bb}$ between the VH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

virtual const double	muVHgaga (const double sqrt_s) const
	The ratio $\mu_{VH,\gamma\gamma}$ between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

virtual const double	muVHmumu (const double sqrt_s) const
	The ratio $\mu_{VH,\mu\mu}$ between the VH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

virtual const double	muVHpT250 (const double sqrt_s) const
	The ratio $\mu_{VH}$ between the WH+ZH associated production cross-section in the current model and in the Standard Model, with $p_{T,H}>250$ GeV.

virtual const double	muVHtautau (const double sqrt_s) const
	The ratio $\mu_{VH,\tau\tau}$ between the VH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

virtual const double	muVHWW (const double sqrt_s) const
	The ratio $\mu_{VH,WW}$ between the VH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

virtual const double	muVHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{VH,WW\to 2l2\nu}$ between the VH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

virtual const double	muVHZga (const double sqrt_s) const
	The ratio $\mu_{VH,Z\gamma}$ between the VH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

virtual const double	muVHZZ (const double sqrt_s) const
	The ratio $\mu_{VH,ZZ}$ between the VH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

virtual const double	muVHZZ4l (const double sqrt_s) const
	The ratio $\mu_{VH,ZZ\to 4l}$ between the VH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

virtual const double	muWH (const double sqrt_s) const
	The ratio $\mu_{WH}$ between the W-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	muWHbb (const double sqrt_s) const
	The ratio $\mu_{WH,bb}$ between the WH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

virtual const double	muWHgaga (const double sqrt_s) const
	The ratio $\mu_{WH,\gamma\gamma}$ between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

virtual const double	muWHmumu (const double sqrt_s) const
	The ratio $\mu_{WH,\mu\mu}$ between the WH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

virtual const double	muWHpT250 (const double sqrt_s) const
	The ratio $\mu_{WH}$ between the W-Higgs associated production cross-section in the current model and in the Standard Model, with $p_{T,H}>250$ GeV.

virtual const double	muWHtautau (const double sqrt_s) const
	The ratio $\mu_{WH,\tau\tau}$ between the WH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

virtual const double	muWHWW (const double sqrt_s) const
	The ratio $\mu_{WH,WW}$ between the WH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

virtual const double	muWHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{WH,WW\to 2l2\nu}$ between the WH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

virtual const double	muWHZga (const double sqrt_s) const
	The ratio $\mu_{WH,Z\gamma}$ between the WH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

virtual const double	muWHZZ (const double sqrt_s) const
	The ratio $\mu_{WH,ZZ}$ between the WH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

virtual const double	muWHZZ4l (const double sqrt_s) const
	The ratio $\mu_{WH,ZZ\to 4l}$ between the WH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

virtual const double	muZH (const double sqrt_s) const
	The ratio $\mu_{ZH}$ between the Z-Higgs associated production cross-section in the current model and in the Standard Model.

virtual const double	muZHbb (const double sqrt_s) const
	The ratio $\mu_{ZH,bb}$ between the ZH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

virtual const double	muZHgaga (const double sqrt_s) const
	The ratio $\mu_{ZH,\gamma\gamma}$ between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

virtual const double	muZHmumu (const double sqrt_s) const
	The ratio $\mu_{ZH,\mu\mu}$ between the ZH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

virtual const double	muZHpT250 (const double sqrt_s) const
	The ratio $\mu_{ZH}$ between the Z-Higgs associated production cross-section in the current model and in the Standard Model, with $p_{T,H}>250$ GeV.

virtual const double	muZHtautau (const double sqrt_s) const
	The ratio $\mu_{ZH,\tau\tau}$ between the ZH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

virtual const double	muZHWW (const double sqrt_s) const
	The ratio $\mu_{ZH,WW}$ between the ZH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

virtual const double	muZHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{ZH,WW\to 2l2\nu}$ between the ZH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

virtual const double	muZHZga (const double sqrt_s) const
	The ratio $\mu_{ZH,Z\gamma}$ between the ZH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

virtual const double	muZHZZ (const double sqrt_s) const
	The ratio $\mu_{ZH,ZZ}$ between the ZH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

virtual const double	muZHZZ4l (const double sqrt_s) const
	The ratio $\mu_{ZH,ZZ\to 4l}$ between the ZH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

virtual const double	Mw () const
	The mass of the $W$ boson, $M_W$.

	NPSMEFTd6General ()
	Constructor.

virtual const double	obliqueS () const
	The oblique parameter $S$. (Simplified implementation. Contribution only from $O_{HWB}$.)

virtual const double	obliqueT () const
	The oblique parameter $T$. (Simplified implementation. Contribution only from $O_{HD}$.)

virtual const double	obliqueU () const
	The oblique parameter $U$.

virtual const double	obliqueW () const
	The oblique parameter $W$. (Simplified implementation. Contribution only from $O_{2W}$.)

virtual const double	obliqueY () const
	The oblique parameter $Y$. (Simplified implementation. Contribution only from $O_{2B}$.)

virtual bool	PostUpdate ()
	The post-update method for NPSMEFTd6General.

virtual const double	ppZHprobe (const double sqrt_s) const
	The direction constrained by $ p p \to Z H$ in the boosted regime, $g_p^Z$. From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6General class.

virtual bool	PreUpdate ()
	The pre-update method for NPSMEFTd6General.

virtual const double	R0_f (const Particle f) const
	The ratio $R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell$, $R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}$ and $R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}$, for charged leptons, quarks and neutrinos, respectively.

virtual const double	RWc () const
	The ratio $R_{W,c)=\Gamma(W\to c + X)/\Gamma(W\to had)$.

virtual const double	RWlilj (const Particle li, const Particle lj) const
	The lepton universality ratio $R_{W,l_i/l_j)=\Gamma(W\to l_i \nu_i)/\Gamma(W\to l_j \nu_j)$.

virtual const double	RZlilj (const Particle li, const Particle lj) const
	The lepton universality ratio $R_{Z,l_i/l_j)=\Gamma(Z\to l_i^+ l_i^-)/\Gamma(Z\to l_j^+ l_j^-)$.

virtual bool	setFlag (const std::string name, const bool value)
	A method to check if all the mandatory parameters for NPSMEFTd6General have been provided in model initialization.

virtual bool	setFlagStr (const std::string name, const std::string value)
	A method to set a flag of NPSMEFTd6General.

virtual const double	sigma0_had () const
	The cross section for the process $e^+ e^-\to Z\to \mathrm{hadrons}$ at the $Z$ pole, $\sigma_h^0$.

virtual const double	STXS0_qqH (const double sqrt_s) const
	The STXS0 bin $pp \to H qq$.

virtual const double	STXS12_BrH4lRatio () const
	The STXS BR $ H \to 4l $, $l=e,\mu$.

virtual const double	STXS12_BrHbbRatio () const
	The STXS BR $ H \to bb $.

virtual const double	STXS12_BrHevmuvRatio () const
	The STXS BR $ H \to e\nu \mu\nu $.

virtual const double	STXS12_BrHgagaRatio () const
	The STXS BR $ H \to \gamma \gamma $.

virtual const double	STXS12_ggH_mjj0_350_pTH0_60_Nj1 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 1,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60$.

virtual const double	STXS12_ggH_mjj0_350_pTH0_60_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60$.

virtual const double	STXS12_ggH_mjj0_350_pTH120_200_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~m_{jj}[GeV]<350,~120<p_{TH} [GeV]<200$.

virtual const double	STXS12_ggH_mjj0_350_pTH60_120_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~m_{jj}[GeV]<350,~60<p_{TH} [GeV]<120$.

virtual const double	STXS12_ggH_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~<p_{TH} [GeV]<200$.

virtual const double	STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25$.

virtual const double	STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]$.

virtual const double	STXS12_ggH_mjj700_Inf_pTH0_200_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200$.

virtual const double	STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25$.

virtual const double	STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]$.

virtual const double	STXS12_ggH_pTH0_10_Nj0 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j=0,~p_{TH} [GeV]<10$.

virtual const double	STXS12_ggH_pTH0_60_Nj1 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j = 1,~p_{TH} [GeV]<60$.

virtual const double	STXS12_ggH_pTH10_200_Nj0 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j=0,~p_{TH} [GeV]<10$.

virtual const double	STXS12_ggH_pTH10_Inf_Nj0 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j=0,~10<p_{TH} [GeV]$.

virtual const double	STXS12_ggH_pTH120_200_Nj1 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j = 1,~120<p_{TH} [GeV]<200$.

virtual const double	STXS12_ggH_pTH200_300 (const double sqrt_s) const
	The STXS bin $gg \to H$, $,200<~p_{TH} [GeV]<300$.

virtual const double	STXS12_ggH_pTH200_300_Nj01 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j\leq 1,~200<p_{TH} [GeV]<300$.

virtual const double	STXS12_ggH_pTH300_450 (const double sqrt_s) const
	The STXS bin $gg \to H$, $,300<~p_{TH} [GeV]<450$.

virtual const double	STXS12_ggH_pTH300_450_Nj01 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j\leq 1,~300<p_{TH} [GeV]<450$.

virtual const double	STXS12_ggH_pTH450_650 (const double sqrt_s) const
	The STXS bin $gg \to H$, $450<~p_{TH} [GeV]<650$.

virtual const double	STXS12_ggH_pTH450_650_Nj01 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j\leq 1,~450<p_{TH} [GeV]<650$.

virtual const double	STXS12_ggH_pTH450_Inf (const double sqrt_s) const
	The STXS bin $gg \to H$, $,450<~p_{TH} [GeV]$.

virtual const double	STXS12_ggH_pTH60_120_Nj1 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j = 1,~60<p_{TH} [GeV]<120$.

virtual const double	STXS12_ggH_pTH650_Inf (const double sqrt_s) const
	The STXS bin $gg \to H$, $~p_{TH} [GeV]>650$.

virtual const double	STXS12_ggH_pTH650_Inf_Nj01 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j\leq 1,650<p_{TH} [GeV]$.

virtual const double	STXS12_ggHll_pTV0_75 (const double sqrt_s) const
	The STXS bin $gg \to H\ell\ell$, $p_{TV}[GeV]<75$.

virtual const double	STXS12_ggHll_pTV150_250_Nj0 (const double sqrt_s) const
	The STXS bin $gg \to H\ell\ell$, $N_j = 0,~150<p_{TV}[GeV]<250$.

virtual const double	STXS12_ggHll_pTV150_250_Nj1 (const double sqrt_s) const
	The STXS bin $gg \to H\ell\ell$, $N_j = 1,~150<p_{TV}[GeV]<250$.

virtual const double	STXS12_ggHll_pTV250_Inf (const double sqrt_s) const
	The STXS bin $gg \to H\ell\ell$, $250 < p_{TV}[GeV]$.

virtual const double	STXS12_ggHll_pTV75_150 (const double sqrt_s) const
	The STXS bin $gg \to H\ell\ell$, $75<p_{TV}[GeV]<150$.

virtual const double	STXS12_qqHll_pTV0_150 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $0<p_{TV}<150[GeV]$.

virtual const double	STXS12_qqHll_pTV0_75 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $p_{TV}[GeV]<75$.

virtual const double	STXS12_qqHll_pTV150_250_Nj0 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $N_j = 0,~150<p_{TV}[GeV]<250$.

virtual const double	STXS12_qqHll_pTV150_250_Nj1 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $N_j \geq 1,~150<p_{TV}[GeV]<250$.

virtual const double	STXS12_qqHll_pTV250_400 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $250<p_{TV}<400[GeV]$.

virtual const double	STXS12_qqHll_pTV250_Inf (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $250<p_{TV}[GeV]$.

virtual const double	STXS12_qqHll_pTV400_Inf (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $400<p_{TV}[GeV]$.

virtual const double	STXS12_qqHll_pTV75_150 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $75<p_{TV}[GeV]<150$.

virtual const double	STXS12_qqHlv_pTV0_150 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $0<p_{TV}<150[GeV]$.

virtual const double	STXS12_qqHlv_pTV0_75 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $p_{TV}[GeV]<75$.

virtual const double	STXS12_qqHlv_pTV150_250_Nj0 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $N_j = 0,~150<p_{TV}[GeV]<250$.

virtual const double	STXS12_qqHlv_pTV150_250_Nj1 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $N_j \geq 1,~150<p_{TV}[GeV]<250$.

virtual const double	STXS12_qqHlv_pTV250_400 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $250<p_{TV}<400[GeV]$.

virtual const double	STXS12_qqHlv_pTV250_Inf (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $250<p_{TV}[GeV]$.

virtual const double	STXS12_qqHlv_pTV400_Inf (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $400<p_{TV}[GeV]$.

virtual const double	STXS12_qqHlv_pTV75_150 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $75<p_{TV}[GeV]<150$.

virtual const double	STXS12_qqHqq_mjj0_60_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~m_{jj}[GeV]<60$.

virtual const double	STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~1000<m_{jj}[GeV]<1500,~p_{TH}[GeV]<200$.

virtual const double	STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~1000<m_{jj}[GeV],~p_{TH}[GeV]>200$.

virtual const double	STXS12_qqHqq_mjj120_350_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~120<m_{jj}[GeV]<350$.

virtual const double	STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~1500<m_{jj}[GeV],~p_{TH}[GeV]<200$.

virtual const double	STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV]<1000,~p_{TH}[GeV]>200$.

virtual const double	STXS12_qqHqq_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200$.

virtual const double	STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25$.

virtual const double	STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]$.

virtual const double	STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV],~200<p_{TH}[GeV]$.

virtual const double	STXS12_qqHqq_mjj60_120_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~60<m_{jj}[GeV]<120$.

virtual const double	STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~700<m_{jj}[GeV]<1000,~p_{TH}[GeV]<200$.

virtual const double	STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25$.

virtual const double	STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]$.

virtual const double	STXS12_qqHqq_Nj0 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j = 0$.

virtual const double	STXS12_qqHqq_Nj1 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j = 1$.

virtual const double	STXS12_qqHqq_VH_veto_Nj01 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j = 0,1$ VH-veto Ref. 2402.05742.

virtual const double	STXS12_tH (const double sqrt_s) const
	The STXS bin $pp \to tH$.

virtual const double	STXS12_ttH_pTH0_60 (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $p_{TH}[GeV]<60$.

virtual const double	STXS12_ttH_pTH120_200 (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $120<p_{TH}[GeV]<200$.

virtual const double	STXS12_ttH_pTH200_300 (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $200<p_{TH}[GeV]<300$.

virtual const double	STXS12_ttH_pTH300_450 (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $300<p_{TH}[GeV]<450$.

virtual const double	STXS12_ttH_pTH300_Inf (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $300<p_{TH}[GeV]$.

virtual const double	STXS12_ttH_pTH450_Inf (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $450<p_{TH}[GeV]$.

virtual const double	STXS12_ttH_pTH60_120 (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $60<p_{TH}[GeV]<120$.

virtual const double	STXS_ggH0j (const double sqrt_s) const
	The STXS bin $gg \to H$.

virtual const double	STXS_ggH1j_pTH_0_60 (const double sqrt_s) const
	The STXS bin $gg \to H$.

virtual const double	STXS_ggH1j_pTH_120_200 (const double sqrt_s) const
	The STXS bin $gg \to H$.

virtual const double	STXS_ggH1j_pTH_200 (const double sqrt_s) const
	The STXS bin $gg \to H$.

virtual const double	STXS_ggH1j_pTH_60_120 (const double sqrt_s) const
	The STXS bin $gg \to H$.

virtual const double	STXS_ggH2j_pTH_0_200 (const double sqrt_s) const
	The STXS bin $gg \to H$.

virtual const double	STXS_ggH2j_pTH_0_60 (const double sqrt_s) const
	The STXS bin $gg \to H$.

virtual const double	STXS_ggH2j_pTH_120_200 (const double sqrt_s) const
	The STXS bin $gg \to H$.

virtual const double	STXS_ggH2j_pTH_200 (const double sqrt_s) const
	The STXS bin $gg \to H$.

virtual const double	STXS_ggH2j_pTH_60_120 (const double sqrt_s) const
	The STXS bin $gg \to H$.

virtual const double	STXS_ggH_VBFtopo_j3 (const double sqrt_s) const
	The STXS bin $gg \to H$.

virtual const double	STXS_ggH_VBFtopo_j3v (const double sqrt_s) const
	The STXS bin $gg \to H$.

virtual const double	STXS_qqHll_pTV_0_150 (const double sqrt_s) const
	The STXS bin $qq \to H \ell \ell$.

virtual const double	STXS_qqHll_pTV_150_250 (const double sqrt_s) const
	The STXS bin $qq \to H \ell \ell$.

virtual const double	STXS_qqHll_pTV_150_250_0j (const double sqrt_s) const
	The STXS bin $qq \to H \ell \ell$.

virtual const double	STXS_qqHll_pTV_150_250_1j (const double sqrt_s) const
	The STXS bin $qq \to H \ell \ell$.

virtual const double	STXS_qqHll_pTV_250 (const double sqrt_s) const
	The STXS bin $qq \to H \ell \ell$.

virtual const double	STXS_qqHlv_pTV_0_150 (const double sqrt_s) const
	The STXS bin $qq \to H \ell \nu$.

virtual const double	STXS_qqHlv_pTV_0_250 (const double sqrt_s) const
	The STXS bin $qq \to H \ell \nu$.

virtual const double	STXS_qqHlv_pTV_150_250_0j (const double sqrt_s) const
	The STXS bin $qq \to H \ell \nu$.

virtual const double	STXS_qqHlv_pTV_150_250_1j (const double sqrt_s) const
	The STXS bin $qq \to H \ell \nu$.

virtual const double	STXS_qqHlv_pTV_250 (const double sqrt_s) const
	The STXS bin $qq \to H \ell \nu$.

virtual const double	STXS_qqHqq_nonVHtopo (const double sqrt_s) const
	The STXS bin $qq \to H qq$.

virtual const double	STXS_qqHqq_pTj_200 (const double sqrt_s) const
	The STXS bin $qq \to H qq$.

virtual const double	STXS_qqHqq_Rest (const double sqrt_s) const
	The STXS bin $qq \to H qq$.

virtual const double	STXS_qqHqq_VBFtopo_j3 (const double sqrt_s) const
	The STXS bin $qq \to H qq$.

virtual const double	STXS_qqHqq_VBFtopo_j3v (const double sqrt_s) const
	The STXS bin $qq \to H qq$.

virtual const double	STXS_qqHqq_VBFtopo_Rest (const double sqrt_s) const
	The STXS bin $qq \to H qq$.

virtual const double	STXS_qqHqq_VHtopo (const double sqrt_s) const
	The STXS bin $qq \to H qq$.

virtual const double	STXS_ttHtH (const double sqrt_s) const
	The STXS bin $ ttH + tH $.

virtual const double	STXS_WHqqHqq_pTj1_200 (const double sqrt_s) const
	The STXS bin $ qq \to WH \to H qq $.

virtual const double	STXS_WHqqHqq_Rest (const double sqrt_s) const
	The STXS bin $ qq \to WH \to H qq $.

virtual const double	STXS_WHqqHqq_VBFtopo_j3 (const double sqrt_s) const
	The STXS bin $ qq \to WH \to H qq $.

virtual const double	STXS_WHqqHqq_VBFtopo_j3v (const double sqrt_s) const
	The STXS bin $ qq \to WH \to H qq $.

virtual const double	STXS_WHqqHqq_VH2j (const double sqrt_s) const
	The STXS bin $ qq \to WH \to H qq $.

virtual const double	STXS_ZHqqHqq_pTj1_200 (const double sqrt_s) const
	The STXS bin $ qq \to ZH \to H qq $.

virtual const double	STXS_ZHqqHqq_Rest (const double sqrt_s) const
	The STXS bin $ qq \to ZH \to H qq $.

virtual const double	STXS_ZHqqHqq_VBFtopo_j3 (const double sqrt_s) const
	The STXS bin $ qq \to ZH \to H qq $.

virtual const double	STXS_ZHqqHqq_VBFtopo_j3v (const double sqrt_s) const
	The STXS bin $ qq \to ZH \to H qq $.

virtual const double	STXS_ZHqqHqq_VH2j (const double sqrt_s) const
	The STXS bin $ qq \to ZH \to H qq $.

const double	tovers2 (const double cosmin, const double cosmax) const

const double	uovers2 (const double cosmin, const double cosmax) const

virtual const double	xseeWW (const double sqrt_s) const
	Total $e^+ e^- \to W^+ W^- \to jj \ell \nu$ cross section in pb, with $\ell= e, \mu$.

virtual const double	xseeWW4fLEP2 (const double sqrt_s, const int fstate) const
	The cross section in pb for $e^+ e^- \to W^+ W^- \to 4f $, with $ 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) $ the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].

virtual const double	xseeWWtotLEP2 (const double sqrt_s) const
	The total cross section in pb for $e^+ e^- \to W^+ W^-$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].

Public Member Functions inherited from NPbase
virtual const double	BR_Zf (const Particle f) const
	The Branching ratio of the $Z$ boson into a given fermion pair, $BR_Z^{f}$.

virtual const double	BrHlljjRatio () const
	The ratio of the Br $(H\to l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model.

virtual const double	C1eeHvv (const double sqrt_s) const
	The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.

virtual const double	C1eettH (const double sqrt_s) const
	The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.

virtual const double	C1eeWBF (const double sqrt_s) const
	The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.

virtual const double	C1eeZBF (const double sqrt_s) const
	The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.

virtual const double	C1eeZH (const double sqrt_s) const
	The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.

virtual const double	cbminuscc () const

virtual const double	cbminusctau () const

virtual const double	ccminusctau () const

virtual const double	cgaplusct () const

virtual const double	cgminuscga () const

virtual const double	cgplusct () const

virtual const double	cVpluscb () const

virtual const double	cVplusctau () const

virtual const double	deltaA_f_2 (const Particle f) const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the left-right asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $\Delta \mathcal{A}_f^{(2)}$.

virtual const double	deltaAFB_2 (const Particle f) const
	The $\mathcal{O}(\Lambda^{-4})$ new physics to the forward-backward asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $\Delta A^f_{FB}$.

virtual const double	deltaGA_f_2 (const Particle f) const

virtual const double	deltaGamma_Z_2 () const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the total decay width of the $Z$ boson, $\Delta \Gamma_Z^{(2)}$.

virtual const double	deltaGamma_Zf_2 (const Particle f) const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the decay width of the $Z$ boson into a given fermion pair, $\Delta \Gamma_{Z,f}^{(2)}$.

virtual const double	deltaGamma_Zhad () const
	The new physics contribution to the hadronic decay width of the $Z$ boson, $\delta \Gamma_{Z,had}$.

virtual const double	deltaGamma_Zhad_2 () const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the hadronic decay width of the $Z$ boson, $\Delta \Gamma_{Z,had}^{(2)}$.

const double	deltaGL_f_mu (const Particle p, const double mu) const
	New physics contribution to the neutral-current left-handed coupling $g_L^f$.

const double	deltaGR_f_mu (const Particle p, const double mu) const
	New physics contribution to the neutral-current right-handed coupling $g_R^f$.

virtual const double	deltaGV_f_2 (const Particle f) const

virtual const double	deltaN_nu () const
	The new physics contribution to the number of neutrinos dervied from the $Z$ pole measurements.

virtual const double	deltaR0_f_2 (const Particle f) const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the ratio $R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell$, $R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}$ and $R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}$, for charged leptons, quarks and neutrinos:

virtual const double	deltaR_inv () const
	The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the $Z$ boson, $\delta R_{inv}$.

virtual const double	deltaRuc () const
	The new physics contribution to the ratio of the $Z\to u\bar{u} + Z\to c\bar{c}$ width to the $Z$-boson hadronic width:

virtual const double	deltaRuc_2 () const
	The $\mathcal{O}(1/\Lambda^4)$ new physics contribution to the ratio of the $Z\to u\bar{u} + Z\to c\bar{c}$ width to the $Z$-boson hadronic width:

virtual const double	deltaSigmaHadron_2 () const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the cross section for the process $e^+ e^-\to Z\to \mathrm{hadrons}$ at the $Z$ pole, $\Delta \sigma_h^{0,(2)}$.

virtual const double	deltaSin2thetaEff_e () const
	The new physics contribution to the effective electron/leptonic weak angle $\delta \sin^2\theta_{\rm eff}^{\rm lept}$ at the $Z$ pole.

virtual const double	deltaSin2thetaEff_e_2 () const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the effective electron weak angle $\Delta \sin^2\theta_{eff,e}^{(2)}$ at the $Z$ pole.

virtual const double	deltaSin2thetaEff_mu () const
	The new physics contribution to the effective muonic weak angle $\delta \sin^2\theta_{\rm eff}^{\mu\mu}$ at the $Z$ pole.

virtual const double	deltaSin2thetaEff_mu_2 () const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the effective muonic weak angle $\Delta \sin^2\theta_{eff, \mu}^{(2)}$ at the $Z$ pole.

virtual const double	deltaxseeWWhadLEP2 (const double sqrt_s) const
	The new physics contribution to the cross section in pb for $e^+ e^- \to W^+ W^- \to j j j j$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.

virtual const double	deltaxseeWWleptLEP2 (const double sqrt_s) const
	The new physics contribution to the cross section in pb for $e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.

virtual const double	deltaxseeWWsemilLEP2 (const double sqrt_s) const
	The new physics contribution to the cross section in pb for $e^+ e^- \to W^+ W^- \to \ell \nu j j$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.

virtual const gslpp::complex	gA_f (const Particle f) const
	The total (SM+NP) contribution to the neutral-current axial-vector coupling $g_A^f$.

virtual const double	Gamma_had () const
	The hadronic decay width of the $Z$ boson, $\Gamma_{Z,had}$.

virtual const StandardModel &	getTrueSM () const
	A method to return a StandardModel object from NPbase.

virtual const gslpp::complex	gV_f (const Particle f) const
	The total (SM+NP) contribution to the neutral-current vector coupling $g_V^f$.

virtual const gslpp::complex	kappaZ_f (const Particle f) const
	The effective neutral-current coupling $\kappa_Z^f$ including SM plus NP contributions.

virtual const double	muggHgagaInt (const double sqrt_s) const
	The ratio $\mu_{ggH,\gamma\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259.

virtual const double	muggHpbbH_Hgaga (const double sqrt_s) const

virtual const double	muggHpbbH_Htautau (const double sqrt_s) const

virtual const double	muggHpbbH_HWW (const double sqrt_s) const

virtual const double	muggHpbbH_HZZ (const double sqrt_s) const

virtual const double	muggHpttHptHpbbH_Hmumu (const double sqrt_s) const

virtual const double	muggHpttHptHpbbH_HZga (const double sqrt_s) const

virtual const double	muggHpVBFpbbH_Hbb (const double sqrt_s) const

virtual const double	muppHmumu (const double sqrt_s) const

virtual const double	muppHZga (const double sqrt_s) const

virtual const double	mutHgaga (const double sqrt_s) const

virtual const double	muttHptH_Hbb (const double sqrt_s) const

virtual const double	muttHptH_Hgaga (const double sqrt_s) const

virtual const double	muttHptH_Hmumu (const double sqrt_s) const

virtual const double	muttHptH_Htautau (const double sqrt_s) const

virtual const double	muttHptH_HWW (const double sqrt_s) const

virtual const double	muttHptH_HZZ (const double sqrt_s) const

virtual const double	muVBFpVH_Hmumu (const double sqrt_s) const

virtual const double	muVBFpVH_HZga (const double sqrt_s) const

virtual const double	muVHcc (const double sqrt_s) const

virtual const double	N_nu () const
	The number of neutrinos dervied from the $Z$ pole measurements, $N_{\nu}$.

	NPbase ()
	The default constructor.

virtual const double	R_inv () const
	The ratio of the invisible and leptonic (electron) decay widths of the $Z$ boson, $R_{inv}$.

virtual const gslpp::complex	rhoZ_f (const Particle f) const
	The effective neutral-current coupling $\rho_Z^f$ including SM plus NP contributions.

virtual const double	Ruc () const
	The ratio of the $Z\to u\bar{u} + Z\to c\bar{c}$ width to the $Z$-boson hadronic width.

virtual const double	sin2thetaEff (const Particle f) const
	The leptonic effective weak mixing angle $\sin^2\theta_{\rm eff}^{\rm lept}$ at the the $Z$ pole.

virtual bool	Update (const std::map< std::string, double > &DPars)
	The update method for NPbase.

virtual const double	UpperLimitZgammaA (const double sqrt_s) const

virtual const double	UpperLimitZgammaA13 (const double sqrt_s) const

virtual const double	UpperLimitZgammaC (const double sqrt_s) const

virtual const double	UpperLimitZgammaC13 (const double sqrt_s) const

virtual const double	xseeWWhadLEP2 (const double sqrt_s) const
	The cross section in pb for $e^+ e^- \to W^+ W^- \to j j j j$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.

virtual const double	xseeWWleptLEP2 (const double sqrt_s) const
	The cross section in pb for $e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.

virtual const double	xseeWWsemilLEP2 (const double sqrt_s) const
	The cross section in pb for $e^+ e^- \to W^+ W^- \to \ell \nu j j$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.

Public Member Functions inherited from StandardModel
gslpp::complex	AH_f (const double tau) const
	Fermionic loop function entering in the calculation of the effective $Hgg$ and $H\gamma\gamma$ couplings.

gslpp::complex	AH_W (const double tau) const
	W loop function entering in the calculation of the effective $H\gamma\gamma$ coupling.

gslpp::complex	AHZga_f (const double tau, const double lambda) const
	Fermionic loop function entering in the calculation of the effective $HZ\gamma$ coupling.

gslpp::complex	AHZga_W (const double tau, const double lambda) const
	W loop function entering in the calculation of the effective $HZ\gamma$ coupling.

const double	Ale (double mu, orders order, bool Nf_thr=true) const
	The running electromagnetic coupling $\alpha_e(\mu)$ in the $\overline{MS}$ scheme.

const double	ale_OS (const double mu, orders order=FULLNLO) const
	The running electromagnetic coupling $\alpha(\mu)$ in the on-shell scheme.

virtual const double	alrmoller (const double q2, const double y) const
	The computation of the parity violating asymmetry in Moller scattering.

const double	Als (const double mu, const int Nf_in, const orders order=FULLNLO) const
	Computes the running strong coupling $\alpha_s(\mu)$ with $N_f$ active flavours in the $\overline{\mathrm{MS}}$ scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda().

const double	Als (const double mu, const orders order, const bool Nf_thr, const bool qed_flag) const
	The running QCD coupling $\alpha(\mu)$ in the $\overline{MS}$ scheme including QED corrections.

const double	Als (const double mu, const orders order=FULLNLO, const bool Nf_thr=true) const

const double	Alstilde5 (const double mu) const
	The value of $\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}$ at any scale $\mu$ with the number of flavours $n_f = 4$ and full EW corrections.

virtual const double	amuon () const
	The computation of the anomalous magnetic moment of the muon $a_\mu=(g_\mu-2)/2$.

const double	Beta_e (int nm, unsigned int nf) const
	QED beta function coefficients - eq. (36) hep-ph/0512066.

const double	Beta_s (int nm, unsigned int nf) const
	QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066.

virtual const double	BrHtobb () const
	The Br $(H\to b \bar{b})$ in the Standard Model.

virtual const double	BrHtocc () const
	The Br $(H\to c \bar{c})$ in the Standard Model.

virtual const double	BrHtogaga () const
	The Br $(H\to \gamma \gamma)$ in the Standard Model.

virtual const double	BrHtogg () const
	The Br $\(H\to gg)$ in the Standard Model.

virtual const double	BrHtomumu () const
	The Br $(H\to \mu^+ \mu^-)$ in the Standard Model.

virtual const double	BrHtoss () const
	The Br $(H\to s \bar{s})$ in the Standard Model.

virtual const double	BrHtotautau () const
	The Br $(H\to \tau^+ \tau^-)$ in the Standard Model.

virtual const double	BrHtoWWstar () const
	The Br $(H\to W W^*)$ in the Standard Model.

virtual const double	BrHtoZga () const
	The Br $(H\to Z \gamma)$ in the Standard Model.

virtual const double	BrHtoZZstar () const
	The Br $(H\to Z Z^*)$ in the Standard Model.

const double	c02 () const
	The square of the cosine of the weak mixing angle $c_0^2$ defined without weak radiative corrections.

virtual bool	CheckFlags () const
	A method to check the sanity of the set of model flags.

virtual bool	CheckParameters (const std::map< std::string, double > &DPars)
	A method to check if all the mandatory parameters for StandardModel have been provided in model initialization.

bool	checkSMparamsForEWPO ()
	A method to check whether the parameters relevant to the EWPO are updated.

const double	computeBrHto4f () const
	The Br $(H\to 4f)$ in the Standard Model.

const double	computeBrHto4l2 () const
	The Br $(H\to 4l)$ $l=e,\mu$ in the Standard Model.

const double	computeBrHto4l3 () const
	The Br $(H\to 4l)$ $l=e,\mu,\tau$ in the Standard Model.

const double	computeBrHto4q () const
	The Br $(H\to 4q)$ in the Standard Model.

const double	computeBrHto4v () const
	The Br $(H\to 4\nu)$ in the Standard Model.

const double	computeBrHtobb () const
	The Br $(H\to bb)$ in the Standard Model.

const double	computeBrHtocc () const
	The Br $(H\to cc)$ in the Standard Model.

const double	computeBrHtoevmuv () const
	The Br $(H\to e \nu \mu \nu)$ in the Standard Model.

const double	computeBrHtogaga () const
	The Br $(H\to\gamma\gamma)$ in the Standard Model.

const double	computeBrHtogg () const
	The Br $(H\to gg)$ in the Standard Model.

const double	computeBrHtollvv2 () const
	The Br $(H\to l^+ l^- \nu \nu)$ $l=e,\mu$ in the Standard Model.

const double	computeBrHtollvv3 () const
	The Br $(H\to l^+ l^- \nu \nu)$ $l=e,\mu,\tau$ in the Standard Model.

const double	computeBrHtomumu () const
	The Br $(H\to \mu\mu)$ in the Standard Model.

const double	computeBrHtoss () const
	The Br $(H\to ss)$ in the Standard Model.

const double	computeBrHtotautau () const
	The Br $(H\to \tau\tau)$ in the Standard Model.

const double	computeBrHtoWW () const
	The Br $(H\to WW)$ in the Standard Model.

const double	computeBrHtoZga () const
	The Br $(H\to Z\gamma)$ in the Standard Model.

const double	computeBrHtoZZ () const
	The Br $(H\to ZZ)$ in the Standard Model.

void	ComputeDeltaR_rem (const double Mw_i, double DeltaR_rem[orders_EW_size]) const
	A method to collect $\Delta r_{\mathrm{rem}}$ computed via subclasses.

void	ComputeDeltaRho (const double Mw_i, double DeltaRho[orders_EW_size]) const
	A method to collect $\Delta\rho$ computed via subclasses.

const double	computeGammaHgaga_tt () const
	The top loop contribution to $H\to\gamma\gamma$ in the Standard Model.

const double	computeGammaHgaga_tW () const
	The mixed $t-W$ loop contribution to $H\to\gamma\gamma$ in the Standard Model.

const double	computeGammaHgaga_WW () const
	The $W$ loop contribution to $H\to\gamma\gamma$ in the Standard Model.

const double	computeGammaHgg_bb () const
	The bottom loop contribution to $H\to gg$ in the Standard Model.

const double	computeGammaHgg_tb () const
	The top-bottom interference contribution to $H\to gg$ in the Standard Model.

const double	computeGammaHgg_tt () const
	The top loop contribution to $H\to gg$ in the Standard Model.

const double	computeGammaHTotal () const
	The Higgs total width in the Standard Model.

const double	computeGammaHZga_tt () const
	The top loop contribution to $H\to Z\gamma$ in the Standard Model.

const double	computeGammaHZga_tW () const
	The mixed $t-W$ loop contribution to $H\to Z\gamma$ in the Standard Model.

const double	computeGammaHZga_WW () const
	The $W$ loop contribution to $H\to Z\gamma$ in the Standard Model. Currently it returns the value of tab 41 in ref. [Heinemeyer:2013tqa].

const double	computeSigmabbH (const double sqrt_s) const
	The bbH production cross section in the Standard Model.

const double	computeSigmaggH (const double sqrt_s) const
	The ggH cross section in the Standard Model.

const double	computeSigmaggH_bb (const double sqrt_s) const
	The square of the bottom-quark contribution to the ggH cross section in the Standard Model.

const double	computeSigmaggH_tb (const double sqrt_s) const
	The top-bottom interference contribution to the ggH cross section in the Standard Model.

const double	computeSigmaggH_tt (const double sqrt_s) const
	The square of the top-quark contribution to the ggH cross section in the Standard Model.

const double	computeSigmatHq (const double sqrt_s) const
	The tHq production cross section in the Standard Model.

const double	computeSigmattH (const double sqrt_s) const
	The ttH production cross section in the Standard Model.

const double	computeSigmaVBF (const double sqrt_s) const
	The VBF cross section in the Standard Model.

const double	computeSigmaWF (const double sqrt_s) const
	The W fusion contribution $\sigma_{WF}$ to higgs-production cross section in the Standard Model.

const double	computeSigmaWH (const double sqrt_s) const
	The WH production cross section in the Standard Model.

const double	computeSigmaZF (const double sqrt_s) const
	The Z fusion contribution $\sigma_{ZF}$ to higgs-production cross section in the Standard Model.

const double	computeSigmaZH (const double sqrt_s) const
	The ZH production cross section in the Standard Model.

const double	computeSigmaZWF (const double sqrt_s) const
	The Z W interference fusion contribution $\sigma_{ZWF}$ to higgs-production cross section in the Standard Model.

virtual const double	cW2 () const

virtual const double	cW2 (const double Mw_i) const
	The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as $c_W^2$.

const double	DeltaAlpha () const
	The total corrections to the electromagnetic coupling $\alpha$ at the $Z$-mass scale, denoted as $\Delta\alpha(M_Z^2)$.

const double	DeltaAlphaL5q () const
	The sum of the leptonic and the five-flavour hadronic corrections to the electromagnetic coupling $\alpha$ at the $Z$-mass scale, denoted as $\Delta\alpha^{\ell+5q}(M_Z^2)$.

const double	DeltaAlphaLepton (const double s) const
	Leptonic contribution to the electromagnetic coupling $\alpha$, denoted as $\Delta\alpha_{\mathrm{lept}}(s)$.

const double	DeltaAlphaTop (const double s) const
	Top-quark contribution to the electromagnetic coupling $\alpha$, denoted as $\Delta\alpha_{\mathrm{top}}(s)$.

virtual const gslpp::complex	deltaKappaZ_f (const Particle f) const
	Flavour non-universal vertex corrections to $\kappa_Z^l$, denoted by $\Delta\kappa_Z^l$.

virtual const double	DeltaR () const
	The SM prediction for $\Delta r$ derived from that for the $W$ boson mass.

virtual const double	DeltaRbar () const
	The SM prediction for $\Delta \overline{r}$ derived from that for the $W$-boson mass.

virtual const gslpp::complex	deltaRhoZ_f (const Particle f) const
	Flavour non-universal vertex corrections to $\rho_Z^l$, denoted by $\Delta\rho_Z^l$.

virtual const double	eeffAFBbottom (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffAFBcharm (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffAFBe (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffAFBetsub (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffAFBmu (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffAFBstrange (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffAFBtau (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRbottom (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRcharm (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRelectron (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRelectrontsub (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRmuon (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRstrange (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRtau (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigma (const Particle f, const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const

virtual const double	eeffsigmaBottom (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaCharm (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaE (const double pol_e, const double pol_p, const double s) const

const double	eeffsigmaEbin (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const

virtual const double	eeffsigmaEtsub (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaHadron (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaMu (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaStrange (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaTau (const double pol_e, const double pol_p, const double s) const

virtual const double	epsilon1 () const
	The SM contribution to the epsilon parameter $\varepsilon_1$.

virtual const double	epsilon2 () const
	The SM contribution to the epsilon parameter $\varepsilon_2$.

virtual const double	epsilon3 () const
	The SM contribution to the epsilon parameter $\varepsilon_3$.

virtual const double	epsilonb () const
	The SM contribution to the epsilon parameter $\varepsilon_b$.

gslpp::complex	f_triangle (const double tau) const
	Loop function entering in the calculation of the effective $Hgg$ and $H\gamma\gamma$ couplings.

gslpp::complex	g_triangle (const double tau) const
	Loop function entering in the calculation of the effective $HZ\gamma$ coupling.

virtual const double	Gamma_inv () const
	The invisible partial decay width of the $Z$ boson, $\Gamma_{\mathrm{inv}}$.

virtual const double	Gamma_muon () const
	The computation of the muon decay.

virtual const double	Gamma_tau_l_nunu (const Particle l) const
	The computation of the leptonic tau decays.

virtual const double	GammaHtobb () const
	The $\Gamma(H\to b \bar{b})$ in the Standard Model.

virtual const double	GammaHtocc () const
	The $\Gamma(H\to c \bar{c})$ in the Standard Model.

virtual const double	GammaHtogaga () const
	The $\Gamma(H\to \gamma \gamma)$ in the Standard Model.

virtual const double	GammaHtogg () const
	The $\Gamma(H\to gg)$ in the Standard Model.

virtual const double	GammaHtomumu () const
	The $\Gamma(H\to \mu^+ \mu^-)$ in the Standard Model.

virtual const double	GammaHtoss () const
	The $\Gamma(H\to s \bar{s})$ in the Standard Model.

virtual const double	GammaHTot () const
	The total Higgs width $\Gamma(H)$ in the Standard Model.

virtual const double	GammaHtotautau () const
	The $\Gamma(H\to \tau^+ \tau^-)$ in the Standard Model.

virtual const double	GammaHtoWWstar () const
	The $\Gamma(H\to W W^*)$ in the Standard Model.

virtual const double	GammaHtoZga () const
	The $\Gamma(H\to Z \gamma)$ in the Standard Model.

virtual const double	GammaHtoZZstar () const
	The $\Gamma(H\to Z Z^*)$ in the Standard Model.

virtual const double	GammaZ (const Particle f) const
	The $Z\to \ell\bar{\ell}$ partial decay width, $\Gamma_\ell$.

virtual const double	gAnue () const
	The effective (muon) neutrino-electron axial-vector coupling: gAnue.

const double	getAle () const
	A get method to retrieve the fine-structure constant $\alpha$.

const double	getAlsMz () const
	A get method to access the value of $\alpha_s(M_Z)$.

virtual const double	getCBd () const
	The ratio of the absolute value of the $B_d$ mixing amplitude over the Standard Model value.

virtual const double	getCBs () const
	The ratio of the absolute value of the $B_s$ mixing amplitude over the Standard Model value.

virtual const double	getCCC1 () const
	A virtual implementation for the RealWeakEFTCC class.

virtual const double	getCCC2 () const
	A virtual implementation for the RealWeakEFTCC class.

virtual const double	getCCC3 () const
	A virtual implementation for the RealWeakEFTCC class.

virtual const double	getCCC4 () const
	A virtual implementation for the RealWeakEFTCC class.

virtual const double	getCCC5 () const
	A virtual implementation for the RealWeakEFTCC class.

virtual const double	getCDMK () const
	The ratio of the real part of the $K$ mixing amplitude over the Standard Model value.

virtual const double	getCepsK () const
	The ratio of the imaginary part of the $K$ mixing amplitude over the Standard Model value.

const CKM &	getCKM () const
	A get method to retrieve the member object of type CKM.

const double	getDAle5Mz () const
	A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, $\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)$.

const double	getDelGammaWlv () const
	A get method to retrieve the theoretical uncertainty in $\Gamma_W_{l\nu}$, denoted as $\delta\,\Gamma_W_{l\nu}$.

const double	getDelGammaWqq () const
	A get method to retrieve the theoretical uncertainty in $\Gamma_W_{qq}$, denoted as $\delta\,\Gamma_W_{qq}$.

const double	getDelGammaZ () const
	A get method to retrieve the theoretical uncertainty in $\Gamma_Z$, denoted as $\delta\,\Gamma_Z$.

const double	getDelMw () const
	A get method to retrieve the theoretical uncertainty in $M_W$, denoted as $\delta\,M_W$.

const double	getDelR0b () const
	A get method to retrieve the theoretical uncertainty in $R_b^0$, denoted as $\delta\,R_b^0$.

const double	getDelR0c () const
	A get method to retrieve the theoretical uncertainty in $R_c^0$, denoted as $\delta\,R_c^0$.

const double	getDelR0l () const
	A get method to retrieve the theoretical uncertainty in $R_l^0$, denoted as $\delta\,R_l^0$.

const double	getDelSigma0H () const
	A get method to retrieve the theoretical uncertainty in $\sigma_{Hadron}^0$, denoted as $\delta\,\sigma_{Hadron}^0$.

const double	getDelSin2th_b () const
	A get method to retrieve the theoretical uncertainty in $\sin^2\theta_{\rm eff}^{b}$, denoted as $\delta\sin^2\theta_{\rm eff}^{b}$.

const double	getDelSin2th_l () const
	A get method to retrieve the theoretical uncertainty in $\sin^2\theta_{\rm eff}^{\rm lept}$, denoted as $\delta\sin^2\theta_{\rm eff}^{\rm lept}$.

const double	getDelSin2th_q () const
	A get method to retrieve the theoretical uncertainty in $\sin^2\theta_{\rm eff}^{q\not = b,t}$, denoted as $\delta\sin^2\theta_{\rm eff}^{q\not = b,t}$.

const std::string	getFlagKappaZ () const
	A method to retrieve the model flag KappaZ.

const std::string	getFlagMw () const
	A method to retrieve the model flag Mw.

const std::string	getFlagRhoZ () const
	A method to retrieve the model flag RhoZ.

const Flavour &	getFlavour () const

const double	getGF () const
	A get method to retrieve the Fermi constant $G_\mu$.

const int	getIterationNo () const

const Particle &	getLeptons (const QCD::lepton p) const
	A get method to retrieve the member object of a lepton.

virtual const double	getMHl () const
	A get method to retrieve the Higgs mass $m_h$.

virtual const double	getmq (const QCD::quark q, const double mu) const
	The MSbar running quark mass computed at NLO.

const double	getMuw () const
	A get method to retrieve the matching scale $\mu_W$ around the weak scale.

const double	getMw () const
	A get method to access the input value of the mass of the $W$ boson $M_W$.

EWSMApproximateFormulae *	getMyApproximateFormulae () const
	A get method to retrieve the member pointer of type EWSMApproximateFormulae.

EWSMcache *	getMyEWSMcache () const
	A get method to retrieve the member pointer of type EWSMcache.

LeptonFlavour *	getMyLeptonFlavour () const

EWSMOneLoopEW *	getMyOneLoopEW () const
	A get method to retrieve the member pointer of type EWSMOneLoopEW,.

EWSMThreeLoopEW *	getMyThreeLoopEW () const

EWSMThreeLoopEW2QCD *	getMyThreeLoopEW2QCD () const

EWSMThreeLoopQCD *	getMyThreeLoopQCD () const

EWSMTwoFermionsLEP2 *	getMyTwoFermionsLEP2 () const
	A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2.

EWSMTwoLoopEW *	getMyTwoLoopEW () const

EWSMTwoLoopQCD *	getMyTwoLoopQCD () const

const double	getMz () const
	A get method to access the mass of the $Z$ boson $M_Z$.

virtual const double	getPhiBd () const
	Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one.

virtual const double	getPhiBs () const
	Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one.

const gslpp::matrix< gslpp::complex >	getUPMNS () const
	A get method to retrieve the object of the PMNS matrix.

const gslpp::matrix< gslpp::complex >	getVCKM () const
	A get method to retrieve the CKM matrix.

const gslpp::matrix< gslpp::complex > &	getYd () const
	A get method to retrieve the Yukawa matrix of the down-type quarks, $Y_d$.

const gslpp::matrix< gslpp::complex > &	getYe () const
	A get method to retrieve the Yukawa matrix of the charged leptons, $Y_e$.

const gslpp::matrix< gslpp::complex > &	getYn () const
	A get method to retrieve the Yukawa matrix of the neutrinos, $Y_\nu$.

const gslpp::matrix< gslpp::complex > &	getYu () const
	A get method to retrieve the Yukawa matrix of the up-type quarks, $Y_u$.

virtual const double	gLnuN2 () const
	The effective neutrino nucleon LH coupling: gLnuN2.

virtual const double	gRnuN2 () const
	The effective neutrino nucleon RH coupling: gRnuN2.

virtual const double	gVnue () const
	The effective (muon) neutrino-electron vector coupling: gVnue.

gslpp::complex	I_triangle_1 (const double tau, const double lambda) const
	Loop function entering in the calculation of the effective $HZ\gamma$ coupling.

gslpp::complex	I_triangle_2 (const double tau, const double lambda) const
	Loop function entering in the calculation of the effective $HZ\gamma$ coupling.

virtual bool	Init (const std::map< std::string, double > &DPars)
	A method to initialize the model parameters.

virtual bool	InitializeModel ()
	A method to initialize the model.

const double	intMLL2eeeeus2 (const double s, const double t0, const double t1) const

const double	intMLR2eeeets2 (const double s, const double t0, const double t1) const

const double	intMLRtilde2eeeest2 (const double s, const double t0, const double t1) const

const double	intMRR2eeeeus2 (const double s, const double t0, const double t1) const

const bool	IsFlagNoApproximateGammaZ () const
	A method to retrieve the model flag NoApproximateGammaZ.

const bool	IsFlagWithoutNonUniversalVC () const
	A method to retrieve the model flag WithoutNonUniversalVC.

const bool	isSMSuccess () const
	A get method to retrieve the success status of the Standard Model update and matching.

virtual const double	LEP2AFBbottom (const double s) const

virtual const double	LEP2AFBcharm (const double s) const

virtual const double	LEP2AFBe (const double s) const

virtual const double	LEP2AFBmu (const double s) const

virtual const double	LEP2AFBtau (const double s) const

virtual const double	LEP2dsigmadcosBinE (const double s, const double cos, const double cosmin, const double cosmax) const

virtual const double	LEP2dsigmadcosBinMu (const double s, const double cos, const double cosmin, const double cosmax) const

virtual const double	LEP2dsigmadcosBinTau (const double s, const double cos, const double cosmin, const double cosmax) const

virtual const double	LEP2dsigmadcosE (const double s, const double cos) const

virtual const double	LEP2dsigmadcosMu (const double s, const double cos) const

virtual const double	LEP2dsigmadcosTau (const double s, const double cos) const

virtual const double	LEP2Rbottom (const double s) const

virtual const double	LEP2Rcharm (const double s) const

virtual const double	LEP2sigmaBottom (const double s) const

virtual const double	LEP2sigmaCharm (const double s) const

virtual const double	LEP2sigmaE (const double s) const

virtual const double	LEP2sigmaHadron (const double s) const

virtual const double	LEP2sigmaMu (const double s) const

virtual const double	LEP2sigmaTau (const double s) const

const double	MLL2eeff (const Particle f, const double s, const double t) const

const double	MLR2eeff (const Particle f, const double s) const

const double	MRL2eeff (const Particle f, const double s) const

const double	MRR2eeff (const Particle f, const double s, const double t) const

const double	Mw_tree () const
	The tree-level mass of the $W$ boson, $M_W^{\mathrm{tree}}$.

const double	MwbarFromMw (const double Mw) const
	A method to convert the $W$-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme.

const double	MwFromMwbar (const double Mwbar) const
	A method to convert the $W$-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme.

double	Mzbar () const
	The $Z$-boson mass $\overline{M}_Z$ in the complex-pole/fixed-width scheme.

virtual const double	Qwemoller (const double q2, const double y) const
	The computation of the electron's weak charge.

virtual const double	Qwn () const
	The computation of the neutron weak charge: Qwn.

virtual const double	Qwp () const
	The computation of the proton weak charge: Qwp.

virtual const double	rho_GammaW (const Particle fi, const Particle fj) const
	EW radiative corrections to the width of $W \to f_i \bar{f}_j$, denoted as $\rho^W_{ij}$.

const double	s02 () const
	The square of the sine of the weak mixing angle $s_0^2$ defined without weak radiative corrections.

void	setCKM (const CKM &CKMMatrix)
	A set method to change the CKM matrix.

void	setFlagCacheInStandardModel (bool FlagCacheInStandardModel)
	A set method to change the model flag CacheInStandardModel of StandardModel.

void	setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ)

bool	setFlagSigmaForAFB (const bool flagSigmaForAFB_i)

bool	setFlagSigmaForR (const bool flagSigmaForR_i)

void	setRequireCKM (bool requireCKM)
	A set method to change the value of requireCKM.

void	setSMSuccess (bool success) const
	A set method to change the success status of the Standard Model update and matching.

void	setYd (const gslpp::matrix< gslpp::complex > &Yd)
	A set method to set the Yukawa matrix of the down-type quarks, $Y_d$.

void	setYe (const gslpp::matrix< gslpp::complex > &Ye)
	A set method to set the Yukawa matrix of the charged leptons, $Y_e$.

void	setYu (const gslpp::matrix< gslpp::complex > &Yu)
	A set method to set the Yukawa matrix of the up-type quarks, $Y_u$.

virtual const double	SigmaeeHee (const double sqrt_s, const double Pe, const double Pp) const
	The $\sigma(e^+ e^- \to e^+ e^- H)$ in the Standard Model.

virtual const double	SigmaeeHvv (const double sqrt_s, const double Pe, const double Pp) const
	The $\sigma(e^+ e^- \to \nu \bar{\nu} H)$ in the Standard Model.

virtual const double	SigmaeeZH (const double sqrt_s, const double Pe, const double Pp) const
	The $\sigma(e^+ e^- \to Z H)$ in the Standard Model.

	StandardModel ()
	The default constructor.

const double	sW2 () const

virtual const double	sW2 (const double Mw_i) const
	The square of the sine of the weak mixing angle in the on-shell scheme, denoted as $s_W^2$.

const double	sW2_MSbar_Approx () const
	The (approximated formula for the) square of the sine of the weak mixing angle in the MSbar scheme, denoted as $\hat{s}_{W}^2$. See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022)

const double	sW2_ND () const
	The square of the sine of the weak mixing angle in the MSbar-ND scheme (w/o decoupling $\alpha\ln(m_t/M_Z)$ terms), denoted as $\hat{s}_{ND}^2$. See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) (eq. 10.13a/10.13b)

virtual const double	TauLFU_gmuge () const
	The computation of the LFU ratio $g_\mu/ g_e $.

virtual const double	TauLFU_gtauge () const
	The computation of the LFU ratio $g_\tau/ g_e $.

virtual const double	TauLFU_gtaugmu () const
	The computation of the LFU ratio $g_\tau/ g_\mu $.

virtual const double	TauLFU_gtaugmuK () const
	The computation of the LFU ratio $\left(g_\tau/ g_\mu\right)_K $.

virtual const double	TauLFU_gtaugmuPi () const
	The computation of the LFU ratio $\left(g_\tau/ g_\mu\right)_\pi $.

virtual const double	ThetaLnuN () const
	The effective neutrino nucleon LH parameter: ThetaLnuN.

virtual const double	ThetaRnuN () const
	The effective neutrino nucleon RH parameter: ThetaRnuN.

const double	tovers2 (const double cosmin, const double cosmax) const

const double	uovers2 (const double cosmin, const double cosmax) const

const double	v () const
	The Higgs vacuum expectation value.

virtual	~StandardModel ()
	The default destructor.

Public Member Functions inherited from QCD
const double	AboveTh (const double mu) const
	The active flavour threshold above the scale $\mu$ as defined in QCD::Thresholds().

void	addParameters (std::vector< std::string > params_i)
	A method to add parameters that are specific to only one set of observables.

const double	Als (const double mu, const int Nf_in, const orders order=FULLNLO) const
	Computes the running strong coupling $\alpha_s(\mu)$ with $N_f$ active flavours in the $\overline{\mathrm{MS}}$ scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda().

const double	Als (const double mu, const orders order=FULLNLO, const bool Nf_thr=true) const

const double	Als4 (const double mu) const
	The value of $\alpha_s^{\mathrm{FULLNLO}}$ at any scale $\mu$ with the number of flavours $n_f = 4$.

const double	AlsByOrder (const double mu, const int Nf_in, const orders order=FULLNLO) const

const double	AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const

const double	AlsOLD (const double mu, const orders order=FULLNLO) const
	Computes the running strong coupling $\alpha_s(\mu)$ in the $\overline{\mathrm{MS}}$ scheme. In the cases of LO, NLO and FULLNNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda().

const double	AlsWithInit (const double mu, const double alsi, const double mu_i, const int nf, const orders order) const
	Computes the running strong coupling $\alpha_s(\mu)$ from $\alpha_s(\mu_i)$ in the $\overline{\mathrm{MS}}$ scheme, where it is forbidden to across a flavour threshold in the RG running from $\mu_i$ to $\mu$.

const double	AlsWithLambda (const double mu, const orders order) const
	Computes the running strong coupling $\alpha_s(\mu)$ in the $\overline{\mathrm{MS}}$ scheme with the use of $\Lambda_{\rm QCD}$.

const double	BelowTh (const double mu) const
	The active flavour threshold below the scale $\mu$ as defined in QCD::Thresholds().

const double	Beta0 (const double nf) const
	The $\beta_0(n_f)$ coefficient for a certain number of flavours $n_f$.

const double	Beta1 (const double nf) const
	The $\beta_1(n_f)$ coefficient for a certain number of flavours $n_f$.

const double	Beta2 (const double nf) const
	The $\beta_2(n_f)$ coefficient for a certain number of flavours $n_f$.

const double	Beta3 (const double nf) const
	The $\beta_3(n_f)$ coefficient for a certain number of flavours $n_f$.

void	CacheShift (double cache[][5], int n) const
	A member used to manage the caching for this class.

void	CacheShift (int cache[][5], int n) const

const orders	FullOrder (orders order) const
	Return the FULLORDER enum corresponding to order.

const double	Gamma0 (const double nf) const
	The $\gamma_0$ coefficient used to compute the running of a mass.

const double	Gamma1 (const double nf) const
	The $\gamma_1$ coefficient used to compute the running of a mass.

const double	Gamma2 (const double nf) const
	The $\gamma_2$ coefficient used to compute the running of a mass.

const double	getAlsM () const
	A get method to access the value of $\alpha_s(M_{\alpha_s})$.

const BParameter &	getBBd () const
	For getting the bag parameters corresponding to the operator basis $O_1 -O_5$ in $\Delta b = 2$ process in the $B_d$ meson system.

const BParameter &	getBBd_subleading () const
	For getting the subleading bag parameters $R_2 - R_3$ in $\Delta b = 2$ process in the $B_d$ meson system.

const BParameter &	getBBs () const
	For getting the bag parameters corresponding to the operator basis $O_1 -O_5$ in $\Delta b = 2$ process in the $B_s$ meson system.

const BParameter &	getBBs_subleading () const
	For getting the subleading bag parameters $R_2 - R_3$ in $\Delta b = 2$ process in the $B_s$ meson system.

const BParameter &	getBD () const
	For getting the bag parameters corresponding to the operator basis $O_1 -O_5$ in $\Delta c = 2$ process in the $D^0$ meson system.

const BParameter &	getBK () const
	For getting the bag parameters corresponding to the operator basis $O_1 -O_5$ in $\Delta s = 2$ process in the $K^0$ meson system.

const BParameter &	getBKd1 () const

const BParameter &	getBKd3 () const

const double	getCF () const
	A get method to access the Casimir factor of QCD.

const double	getMAls () const
	A get method to access the mass scale $M_{\alpha_s}$ at which the strong coupling constant measurement is provided.

const Meson &	getMesons (const QCD::meson m) const
	A get method to access a meson as an object of the type Meson.

const double	getMtpole () const
	A get method to access the pole mass of the top quark.

const double	getMub () const
	A get method to access the threshold between five- and four-flavour theory in GeV.

const double	getMuc () const
	A get method to access the threshold between four- and three-flavour theory in GeV.

const double	getMut () const
	A get method to access the threshold between six- and five-flavour theory in GeV.

const double	getNc () const
	A get method to access the number of colours $N_c$.

const double	getOptionalParameter (std::string name) const
	A method to get parameters that are specific to only one set of observables.

const Particle &	getQuarks (const QCD::quark q) const
	A get method to access a quark as an object of the type Particle.

std::vector< std::string >	getUnknownParameters ()
	A method to get the vector of the parameters that have been specified in the configuration file but not being used.

void	initializeBParameter (std::string name_i) const
	A method to initialize B Parameter and the corresponding meson.

void	initializeMeson (QCD::meson meson_i) const
	A method to initialize a meson.

bool	isQCDsuccess () const
	A getter for the QCDsuccess flag.

const double	logLambda (const double nf, orders order) const
	Computes $\ln\Lambda_\mathrm{QCD}$ with nf flavours in GeV.

const double	Mbar2Mp (const double mbar, const quark q, const orders order=FULLNNLO) const
	Converts the $\overline{\mathrm{MS}}$ mass $m(m)$ to the pole mass.

const double	Mofmu2Mbar (const double m, const double mu, const quark q) const
	Converts a quark running mass at an arbitrary scale to the corresponding $\overline{\mathrm{MS}}$ mass $m(m)$.

const double	Mp2Mbar (const double mp, const quark q, orders order=FULLNNLO) const
	Converts a quark pole mass to the corresponding $\overline{\mathrm{MS}}$ mass $m(m)$.

const double	Mrun (const double mu, const double m, const quark q, const orders order=FULLNNLO) const
	Computes a running quark mass $m(\mu)$ from $m(m)$.

const double	Mrun (const double mu_f, const double mu_i, const double m, const quark q, const orders order=FULLNNLO) const
	Runs a quark mass from $\mu_i$ to $\mu_f$.

const double	Mrun4 (const double mu_f, const double mu_i, const double m) const
	The running of a mass with the number of flavours $n_f = 4$.

const double	MS2DRqmass (const double MSbar) const
	Converts a quark mass from the $\overline{\mathrm{MS}}$ scheme to the $\overline{\mathrm{DR}}$ scheme.

const double	MS2DRqmass (const double MSscale, const double MSbar) const
	Converts a quark mass from the $\overline{\mathrm{MS}}$ scheme to the $\overline{\mathrm{DR}}$ scheme.

const double	Nf (const double mu) const
	The number of active flavour at scale $\mu$.

const double	NfThresholdCorrections (double mu, double M, double als, int nf, orders order) const
	Threshold corrections in matching $\alpha_s(n_f+1)$ with $\alpha_s(n_f)$ from eq. (34) of hep-ph/0512060.

const std::string	orderToString (const orders order) const
	Converts an object of the enum type "orders" to the corresponding string.

	QCD ()
	Constructor.

void	setComputemt (bool computemt)
	A set method to change the value of computemt.

void	setMtpole (double mtpole_in)
	A method to set the pole mass of the top quark.

void	setNc (double Nc)
	A set method to change the number of colours $N_c$.

void	setOptionalParameter (std::string name, double value)
	A method to set the parameter value for the parameters that are specific to only one set of observables.

void	setQuarkMass (const quark q, const double mass)
	A set method to change the mass of a quark.

const double	Thresholds (const int i) const
	For accessing the active flavour threshold scales.

Public Member Functions inherited from Model
void	addMissingModelParameter (const std::string &missingParameterName)

std::vector< std::string >	getmissingModelParameters ()

unsigned int	getMissingModelParametersCount ()

std::string	getModelName () const
	A method to fetch the name of the model.

const double &	getModelParam (std::string name) const

bool	isModelFWC_DF2 () const

bool	isModelGeneralTHDM () const

bool	isModelGeorgiMachacek () const

bool	IsModelInitialized () const
	A method to check if the model is initialized.

bool	isModelLinearized () const

bool	isModelNPquadratic () const

bool	isModelParam (std::string name) const

bool	isModelSUSY () const

bool	isModelTHDM () const

bool	isModelTHDMW () const

bool	IsUpdateError () const
	A method to check if there was any error in the model update process.

	Model ()
	The default constructor.

void	raiseMissingModelParameterCount ()

void	setModelFWC_DF2 ()

void	setModelGeneralTHDM ()

void	setModelGeorgiMachacek ()

void	setModelInitialized (bool ModelInitialized)
	A set method to fix the failure or success of the initialization of the model.

void	setModelLinearized (bool linearized=true)

void	setModelName (const std::string name)
	A method to set the name of the model.

void	setModelNPquadratic (bool NPquadratic=true)

void	setModelSUSY ()

void	setModelTHDM ()

void	setModelTHDMW ()

void	setSliced (bool Sliced)

void	setUpdateError (bool UpdateError)
	A set method to fix the update status as success or failure.

virtual	~Model ()
	The default destructor.

Static Public Attributes
static const int	NNPSMEFTd6GeneralVars = 2708-208 + 79
	The number of the model parameters in NPSMEFTd6General (including the 18 parameters needed for the SM and 79 auxiliary parameters).

static const std::string	NPSMEFTd6GeneralVars [NNPSMEFTd6GeneralVars]
	A string array containing the labels of the model parameters in NPSMEFTd6General.

Static Public Attributes inherited from StandardModel
static const double	GeVminus2_to_nb = 389379.338

static const double	Mw_error = 0.00001
	The target accuracy of the iterative calculation of the $W$-boson mass in units of GeV.

static const int	NSMvars = 28
	The number of the model parameters in StandardModel.

static const int	NumSMParamsForEWPO = 35
	The number of the SM parameters that are relevant to the EW precision observables.

static std::string	SMvars [NSMvars]
	A string array containing the labels of the model parameters in StandardModel.

Static Public Attributes inherited from QCD
static const int	NQCDvars = 11
	The number of model parameters in QCD.

static std::string	QCDvars [NQCDvars]
	An array containing the labels under which all QCD parameters are stored in a vector of ModelParameter via InputParser::ReadParameters().

Additional Inherited Members
Public Types inherited from StandardModel
enum	LEP2RCs { Weak = 0 , WeakBox , ISR , QEDFSR , QCDFSR , NUMofLEP2RCs }

enum	orders_EW { EW1 = 0 , EW1QCD1 , EW1QCD2 , EW2 , EW2QCD1 , EW3 , orders_EW_size }
	An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More...

Public Types inherited from QCD
enum	lepton { NEUTRINO_1 , ELECTRON , NEUTRINO_2 , MU , NEUTRINO_3 , TAU , NOLEPTON }
	An enum type for leptons. More...

enum	meson { P_0 , P_P , K_0 , K_P , D_0 , D_P , D_S , B_D , B_P , B_S , B_C , PHI , K_star , K_star_P , K_S , D_star_P , RHO , RHO_P , OMEGA , MESON_END }
	An enum type for mesons. More...

enum	quark { UP , DOWN , CHARM , STRANGE , TOP , BOTTOM }
	An enum type for quarks. More...

Protected Member Functions inherited from StandardModel
const double	AFB_NoISR_l (const QCD::lepton l_flavor, const double s) const

const double	AFB_NoISR_q (const QCD::quark q_flavor, const double s) const

bool	checkEWPOscheme (const std::string scheme) const
	A method to check if a given scheme name in string form is valid.

virtual void	computeCKM ()
	The method to compute the CKM matrix.

virtual void	computeYukawas ()
	The method to compute the Yukawas matrix.

double	Delta_EWQCD (const QCD::quark q) const
	The non-factorizable EW-QCD corrections to the partial widths for $Z\to q\bar{q}$, denoted as $\Delta_{\mathrm{EW/QCD}}$.

const double	getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm133 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm167 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm172 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm183 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm189 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm192 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm196 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm200 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm202 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm205 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm207 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu130 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu136 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu161 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu172 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu183 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu189 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu192 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu196 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu200 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu202 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu205 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu207 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau130 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau136 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau161 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau172 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau183 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau189 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau192 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau196 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau200 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau202 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau205 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau207 (double x) const

const double	getIntegrand_dsigmaBox_bottom130 (double x) const

const double	getIntegrand_dsigmaBox_bottom133 (double x) const

const double	getIntegrand_dsigmaBox_bottom136 (double x) const

const double	getIntegrand_dsigmaBox_bottom161 (double x) const

const double	getIntegrand_dsigmaBox_bottom167 (double x) const

const double	getIntegrand_dsigmaBox_bottom172 (double x) const

const double	getIntegrand_dsigmaBox_bottom183 (double x) const

const double	getIntegrand_dsigmaBox_bottom189 (double x) const

const double	getIntegrand_dsigmaBox_bottom192 (double x) const

const double	getIntegrand_dsigmaBox_bottom196 (double x) const

const double	getIntegrand_dsigmaBox_bottom200 (double x) const

const double	getIntegrand_dsigmaBox_bottom202 (double x) const

const double	getIntegrand_dsigmaBox_bottom205 (double x) const

const double	getIntegrand_dsigmaBox_bottom207 (double x) const

const double	getIntegrand_dsigmaBox_charm130 (double x) const

const double	getIntegrand_dsigmaBox_charm133 (double x) const

const double	getIntegrand_dsigmaBox_charm136 (double x) const

const double	getIntegrand_dsigmaBox_charm161 (double x) const

const double	getIntegrand_dsigmaBox_charm167 (double x) const

const double	getIntegrand_dsigmaBox_charm172 (double x) const

const double	getIntegrand_dsigmaBox_charm183 (double x) const

const double	getIntegrand_dsigmaBox_charm189 (double x) const

const double	getIntegrand_dsigmaBox_charm192 (double x) const

const double	getIntegrand_dsigmaBox_charm196 (double x) const

const double	getIntegrand_dsigmaBox_charm200 (double x) const

const double	getIntegrand_dsigmaBox_charm202 (double x) const

const double	getIntegrand_dsigmaBox_charm205 (double x) const

const double	getIntegrand_dsigmaBox_charm207 (double x) const

const double	getIntegrand_dsigmaBox_down130 (double x) const

const double	getIntegrand_dsigmaBox_down133 (double x) const

const double	getIntegrand_dsigmaBox_down136 (double x) const

const double	getIntegrand_dsigmaBox_down161 (double x) const

const double	getIntegrand_dsigmaBox_down167 (double x) const

const double	getIntegrand_dsigmaBox_down172 (double x) const

const double	getIntegrand_dsigmaBox_down183 (double x) const

const double	getIntegrand_dsigmaBox_down189 (double x) const

const double	getIntegrand_dsigmaBox_down192 (double x) const

const double	getIntegrand_dsigmaBox_down196 (double x) const

const double	getIntegrand_dsigmaBox_down200 (double x) const

const double	getIntegrand_dsigmaBox_down202 (double x) const

const double	getIntegrand_dsigmaBox_down205 (double x) const

const double	getIntegrand_dsigmaBox_down207 (double x) const

const double	getIntegrand_dsigmaBox_mu130 (double x) const

const double	getIntegrand_dsigmaBox_mu133 (double x) const

const double	getIntegrand_dsigmaBox_mu136 (double x) const

const double	getIntegrand_dsigmaBox_mu161 (double x) const

const double	getIntegrand_dsigmaBox_mu167 (double x) const

const double	getIntegrand_dsigmaBox_mu172 (double x) const

const double	getIntegrand_dsigmaBox_mu183 (double x) const

const double	getIntegrand_dsigmaBox_mu189 (double x) const

const double	getIntegrand_dsigmaBox_mu192 (double x) const

const double	getIntegrand_dsigmaBox_mu196 (double x) const

const double	getIntegrand_dsigmaBox_mu200 (double x) const

const double	getIntegrand_dsigmaBox_mu202 (double x) const

const double	getIntegrand_dsigmaBox_mu205 (double x) const

const double	getIntegrand_dsigmaBox_mu207 (double x) const

const double	getIntegrand_dsigmaBox_strange130 (double x) const

const double	getIntegrand_dsigmaBox_strange133 (double x) const

const double	getIntegrand_dsigmaBox_strange136 (double x) const

const double	getIntegrand_dsigmaBox_strange161 (double x) const

const double	getIntegrand_dsigmaBox_strange167 (double x) const

const double	getIntegrand_dsigmaBox_strange172 (double x) const

const double	getIntegrand_dsigmaBox_strange183 (double x) const

const double	getIntegrand_dsigmaBox_strange189 (double x) const

const double	getIntegrand_dsigmaBox_strange192 (double x) const

const double	getIntegrand_dsigmaBox_strange196 (double x) const

const double	getIntegrand_dsigmaBox_strange200 (double x) const

const double	getIntegrand_dsigmaBox_strange202 (double x) const

const double	getIntegrand_dsigmaBox_strange205 (double x) const

const double	getIntegrand_dsigmaBox_strange207 (double x) const

const double	getIntegrand_dsigmaBox_tau130 (double x) const

const double	getIntegrand_dsigmaBox_tau133 (double x) const

const double	getIntegrand_dsigmaBox_tau136 (double x) const

const double	getIntegrand_dsigmaBox_tau161 (double x) const

const double	getIntegrand_dsigmaBox_tau167 (double x) const

const double	getIntegrand_dsigmaBox_tau172 (double x) const

const double	getIntegrand_dsigmaBox_tau183 (double x) const

const double	getIntegrand_dsigmaBox_tau189 (double x) const

const double	getIntegrand_dsigmaBox_tau192 (double x) const

const double	getIntegrand_dsigmaBox_tau196 (double x) const

const double	getIntegrand_dsigmaBox_tau200 (double x) const

const double	getIntegrand_dsigmaBox_tau202 (double x) const

const double	getIntegrand_dsigmaBox_tau205 (double x) const

const double	getIntegrand_dsigmaBox_tau207 (double x) const

const double	getIntegrand_dsigmaBox_up130 (double x) const

const double	getIntegrand_dsigmaBox_up133 (double x) const

const double	getIntegrand_dsigmaBox_up136 (double x) const

const double	getIntegrand_dsigmaBox_up161 (double x) const

const double	getIntegrand_dsigmaBox_up167 (double x) const

const double	getIntegrand_dsigmaBox_up172 (double x) const

const double	getIntegrand_dsigmaBox_up183 (double x) const

const double	getIntegrand_dsigmaBox_up189 (double x) const

const double	getIntegrand_dsigmaBox_up192 (double x) const

const double	getIntegrand_dsigmaBox_up196 (double x) const

const double	getIntegrand_dsigmaBox_up200 (double x) const

const double	getIntegrand_dsigmaBox_up202 (double x) const

const double	getIntegrand_dsigmaBox_up205 (double x) const

const double	getIntegrand_dsigmaBox_up207 (double x) const

const double	getIntegrand_sigmaWithISR_bottom130 (double x) const

const double	getIntegrand_sigmaWithISR_bottom133 (double x) const

const double	getIntegrand_sigmaWithISR_bottom136 (double x) const

const double	getIntegrand_sigmaWithISR_bottom161 (double x) const

const double	getIntegrand_sigmaWithISR_bottom167 (double x) const

const double	getIntegrand_sigmaWithISR_bottom172 (double x) const

const double	getIntegrand_sigmaWithISR_bottom183 (double x) const

const double	getIntegrand_sigmaWithISR_bottom189 (double x) const

const double	getIntegrand_sigmaWithISR_bottom192 (double x) const

const double	getIntegrand_sigmaWithISR_bottom196 (double x) const

const double	getIntegrand_sigmaWithISR_bottom200 (double x) const

const double	getIntegrand_sigmaWithISR_bottom202 (double x) const

const double	getIntegrand_sigmaWithISR_bottom205 (double x) const

const double	getIntegrand_sigmaWithISR_bottom207 (double x) const

const double	getIntegrand_sigmaWithISR_charm130 (double x) const

const double	getIntegrand_sigmaWithISR_charm133 (double x) const

const double	getIntegrand_sigmaWithISR_charm136 (double x) const

const double	getIntegrand_sigmaWithISR_charm161 (double x) const

const double	getIntegrand_sigmaWithISR_charm167 (double x) const

const double	getIntegrand_sigmaWithISR_charm172 (double x) const

const double	getIntegrand_sigmaWithISR_charm183 (double x) const

const double	getIntegrand_sigmaWithISR_charm189 (double x) const

const double	getIntegrand_sigmaWithISR_charm192 (double x) const

const double	getIntegrand_sigmaWithISR_charm196 (double x) const

const double	getIntegrand_sigmaWithISR_charm200 (double x) const

const double	getIntegrand_sigmaWithISR_charm202 (double x) const

const double	getIntegrand_sigmaWithISR_charm205 (double x) const

const double	getIntegrand_sigmaWithISR_charm207 (double x) const

const double	getIntegrand_sigmaWithISR_down130 (double x) const

const double	getIntegrand_sigmaWithISR_down133 (double x) const

const double	getIntegrand_sigmaWithISR_down136 (double x) const

const double	getIntegrand_sigmaWithISR_down161 (double x) const

const double	getIntegrand_sigmaWithISR_down167 (double x) const

const double	getIntegrand_sigmaWithISR_down172 (double x) const

const double	getIntegrand_sigmaWithISR_down183 (double x) const

const double	getIntegrand_sigmaWithISR_down189 (double x) const

const double	getIntegrand_sigmaWithISR_down192 (double x) const

const double	getIntegrand_sigmaWithISR_down196 (double x) const

const double	getIntegrand_sigmaWithISR_down200 (double x) const

const double	getIntegrand_sigmaWithISR_down202 (double x) const

const double	getIntegrand_sigmaWithISR_down205 (double x) const

const double	getIntegrand_sigmaWithISR_down207 (double x) const

const double	getIntegrand_sigmaWithISR_mu130 (double x) const

const double	getIntegrand_sigmaWithISR_mu136 (double x) const

const double	getIntegrand_sigmaWithISR_mu161 (double x) const

const double	getIntegrand_sigmaWithISR_mu172 (double x) const

const double	getIntegrand_sigmaWithISR_mu183 (double x) const

const double	getIntegrand_sigmaWithISR_mu189 (double x) const

const double	getIntegrand_sigmaWithISR_mu192 (double x) const

const double	getIntegrand_sigmaWithISR_mu196 (double x) const

const double	getIntegrand_sigmaWithISR_mu200 (double x) const

const double	getIntegrand_sigmaWithISR_mu202 (double x) const

const double	getIntegrand_sigmaWithISR_mu205 (double x) const

const double	getIntegrand_sigmaWithISR_mu207 (double x) const

const double	getIntegrand_sigmaWithISR_strange130 (double x) const

const double	getIntegrand_sigmaWithISR_strange133 (double x) const

const double	getIntegrand_sigmaWithISR_strange136 (double x) const

const double	getIntegrand_sigmaWithISR_strange161 (double x) const

const double	getIntegrand_sigmaWithISR_strange167 (double x) const

const double	getIntegrand_sigmaWithISR_strange172 (double x) const

const double	getIntegrand_sigmaWithISR_strange183 (double x) const

const double	getIntegrand_sigmaWithISR_strange189 (double x) const

const double	getIntegrand_sigmaWithISR_strange192 (double x) const

const double	getIntegrand_sigmaWithISR_strange196 (double x) const

const double	getIntegrand_sigmaWithISR_strange200 (double x) const

const double	getIntegrand_sigmaWithISR_strange202 (double x) const

const double	getIntegrand_sigmaWithISR_strange205 (double x) const

const double	getIntegrand_sigmaWithISR_strange207 (double x) const

const double	getIntegrand_sigmaWithISR_tau130 (double x) const

const double	getIntegrand_sigmaWithISR_tau136 (double x) const

const double	getIntegrand_sigmaWithISR_tau161 (double x) const

const double	getIntegrand_sigmaWithISR_tau172 (double x) const

const double	getIntegrand_sigmaWithISR_tau183 (double x) const

const double	getIntegrand_sigmaWithISR_tau189 (double x) const

const double	getIntegrand_sigmaWithISR_tau192 (double x) const

const double	getIntegrand_sigmaWithISR_tau196 (double x) const

const double	getIntegrand_sigmaWithISR_tau200 (double x) const

const double	getIntegrand_sigmaWithISR_tau202 (double x) const

const double	getIntegrand_sigmaWithISR_tau205 (double x) const

const double	getIntegrand_sigmaWithISR_tau207 (double x) const

const double	getIntegrand_sigmaWithISR_up130 (double x) const

const double	getIntegrand_sigmaWithISR_up133 (double x) const

const double	getIntegrand_sigmaWithISR_up136 (double x) const

const double	getIntegrand_sigmaWithISR_up161 (double x) const

const double	getIntegrand_sigmaWithISR_up167 (double x) const

const double	getIntegrand_sigmaWithISR_up172 (double x) const

const double	getIntegrand_sigmaWithISR_up183 (double x) const

const double	getIntegrand_sigmaWithISR_up189 (double x) const

const double	getIntegrand_sigmaWithISR_up192 (double x) const

const double	getIntegrand_sigmaWithISR_up196 (double x) const

const double	getIntegrand_sigmaWithISR_up200 (double x) const

const double	getIntegrand_sigmaWithISR_up202 (double x) const

const double	getIntegrand_sigmaWithISR_up205 (double x) const

const double	getIntegrand_sigmaWithISR_up207 (double x) const

const double	Integrand_AFBnumeratorWithISR_l (double x, const QCD::lepton l_flavor, const double s) const

const double	Integrand_AFBnumeratorWithISR_q (double x, const QCD::quark q_flavor, const double s) const

const double	Integrand_dsigmaBox_l (double cosTheta, const QCD::lepton l_flavor, const double s) const

const double	Integrand_dsigmaBox_q (double cosTheta, const QCD::quark q_flavor, const double s) const

const double	Integrand_sigmaWithISR_l (double x, const QCD::lepton l_flavor, const double s) const

const double	Integrand_sigmaWithISR_q (double x, const QCD::quark q_flavor, const double s) const

double	m_q (const QCD::quark q, const double mu, const orders order=FULLNLO) const

double	RAq (const QCD::quark q) const
	The radiator factor associated with the final-state QED and QCD corrections to the the axial-vector-current interactions, $R_A^q(M_Z^2)$.

double	resumKappaZ (const double DeltaRho[orders_EW_size], const double deltaKappa_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
	A method to compute the real part of the effetvive coupling $\kappa_Z^f$ from $\Delta\rho$, $\delta\rho_{\rm rem}^{f}$ and $\Delta r_{\mathrm{rem}}$.

double	resumMw (const double Mw_i, const double DeltaRho[orders_EW_size], const double DeltaR_rem[orders_EW_size]) const
	A method to compute the $W$-boson mass from $\Delta\rho$ and $\Delta r_{\mathrm{rem}}$.

double	resumRhoZ (const double DeltaRho[orders_EW_size], const double deltaRho_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
	A method to compute the real part of the effective coupling $\rho_Z^f$ from $\Delta\rho$, $\delta\rho_{\rm rem}^{f}$ and $\Delta r_{\mathrm{rem}}$.

double	RVh () const
	The singlet vector corrections to the hadronic $Z$-boson width, denoted as $R_V^h$.

double	RVq (const QCD::quark q) const
	The radiator factor associated with the final-state QED and QCD corrections to the the vector-current interactions, $R_V^q(M_Z^2)$.

double	SchemeToDouble (const std::string scheme) const
	A method to convert a given scheme name in string form into a floating-point number with double precision.

virtual void	setParameter (const std::string name, const double &value)
	A method to set the value of a parameter of StandardModel.

const double	sigma_NoISR_l (const QCD::lepton l_flavor, const double s) const

const double	sigma_NoISR_q (const QCD::quark q_flavor, const double s) const

double	taub () const
	Top-mass corrections to the $Zb\bar{b}$ vertex, denoted by $\tau_b$.

Protected Member Functions inherited from QCD
const double	MassOfNf (int nf) const
	The Mbar mass of the heaviest quark in the theory with Nf active flavour.

Protected Attributes inherited from StandardModel
double	A
	The CKM parameter $A$ in the Wolfenstein parameterization.

double	ale
	The fine-structure constant $\alpha$.

double	alpha21

double	alpha31

double	AlsMz
	The strong coupling constant at the Z-boson mass, $\alpha_s(M_Z)$.

bool	bSigmaForAFB

bool	bSigmaForR

double	dAl5hMz
	The five-flavour hadronic contribution to the electromagnetic coupling, $\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)$. (Non-input parameter)

double	dAle5Mz
	The five-flavour hadronic contribution to the electromagnetic coupling, $\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)$, used as input for FlagMWinput = FALSE.

double	delGammaWlv
	The theoretical uncertainty in $\Gamma_W_{l\nu}$, denoted as $\delta\,\Gamma_W_{l\nu}$.

double	delGammaWqq
	The theoretical uncertainty in $\Gamma_W_{qq}$, denoted as $\delta\,\Gamma_W_{qq}$.

double	delGammaZ
	The theoretical uncertainty in $\Gamma_Z$, denoted as $\delta\,\Gamma_Z$, in GeV.

double	delMw
	The theoretical uncertainty in $M_W$, denoted as $\delta\,M_W$, in GeV.

double	delR0b
	The theoretical uncertainty in $R_b^0$, denoted as $\delta\,R_b^0$.

double	delR0c
	The theoretical uncertainty in $R_c^0$, denoted as $\delta\,R_c^0$.

double	delR0l
	The theoretical uncertainty in $R_l^0$, denoted as $\delta\,R_l^0$.

double	delsigma0H
	The theoretical uncertainty in $\sigma_{Hadron}^0$, denoted as $\delta\,\sigma_{Hadron}^0$ in nb.

double	delSin2th_b
	The theoretical uncertainty in $\sin^2\theta_{\rm eff}^{b}$, denoted as $\delta\sin^2\theta_{\rm eff}^{b}$.

double	delSin2th_l
	The theoretical uncertainty in $\sin^2\theta_{\rm eff}^{\rm lept}$, denoted as $\delta\sin^2\theta_{\rm eff}^{\rm lept}$.

double	delSin2th_q
	The theoretical uncertainty in $\sin^2\theta_{\rm eff}^{q\not = b,t}$, denoted as $\delta\sin^2\theta_{\rm eff}^{q\not = b,t}$.

double	delta

double	etab
	The CKM parameter $\bar{\eta}$ in the Wolfenstein parameterization.

bool	flag_order [orders_EW_size]
	An array of internal flags controlling the inclusions of higher-order corrections.

bool	FlagFixMuwMut
	A boolean for the model flag FixMuwMut.

bool	flagLEP2 [NUMofLEP2RCs]

double	gamma
	$\gamma $ used as an input for FlagWolfenstein = FALSE

double	GF
	The Fermi constant $G_\mu$ in ${\rm GeV}^{-2}$.

double	lambda
	The CKM parameter $\lambda$ in the Wolfenstein parameterization.

Particle	leptons [6]
	An array of Particle objects for the leptons.

double	mHl
	The Higgs mass $m_h$ in GeV.

double	muw
	A matching scale $\mu_W$ around the weak scale in GeV.

double	Mw_inp
	The mass of the $W$ boson in GeV used as input for FlagMWinput = TRUE.

CKM	myCKM
	An object of type CKM.

PMNS	myPMNS

double	Mz
	The mass of the $Z$ boson in GeV.

bool	requireCKM
	An internal flag to control whether the CKM matrix has to be recomputed.

bool	requireYe
	An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed.

bool	requireYn
	An internal flag to control whether the neutrino Yukawa matrix has to be recomputed.

double	rhob
	The CKM parameter $\bar{\rho}$ in the Wolfenstein parameterization.

double	s12

double	s13

double	s23

Flavour	SMFlavour
	An object of type Flavour.

Matching< StandardModelMatching, StandardModel >	SMM
	An object of type Matching.

double	Vcb
	$\vert V_{cb} \vert $ used as an input for FlagWolfenstein = FALSE

double	Vub
	$\vert V_{ub} \vert $ used as an input for FlagWolfenstein = FALSE

double	Vud
	$\vert V_{ud} \vert $ used as an input for FlagWolfenstein = FALSE and FlagUseVud = TRUE

double	Vus
	$\vert V_{us} \vert $ used as an input for FlagWolfenstein = FALSE

gslpp::matrix< gslpp::complex >	Yd
	The Yukawa matrix of the down-type quarks.

gslpp::matrix< gslpp::complex >	Ye
	The Yukawa matrix of the charged leptons.

gslpp::matrix< gslpp::complex >	Yn
	The Yukawa matrix of the neutrinos.

gslpp::matrix< gslpp::complex >	Yu
	The Yukawa matrix of the up-type quarks.

Protected Attributes inherited from QCD
double	AlsM
	The strong coupling constant at the mass scale MAls, $\alpha_s(M_{\alpha_s})$.

double	CA

double	CF

bool	computemt
	Switch for computing the $\overline{\mathrm{MS}}$ mass of the top quark.

double	dAdA_NA

double	dFdA_NA

double	dFdF_NA

bool	FlagMpole2MbarNumeric
	A flag to determine whether the pole mass to $\over \mathrm{MS}$ mass conversion is done numerically.

bool	FlagMtPole
	A flag to determine whether the pole mass of the top quark is used as input.

double	MAls
	The mass scale in GeV at which the strong coupling measurement is provided.

double	mtpole
	The pole mass of the top quark.

double	mub
	The threshold between five- and four-flavour theory in GeV.

double	muc
	The threshold between four- and three-flavour theory in GeV.

double	mut
	The threshold between six- and five-flavour theory in GeV.

double	NA

double	Nc
	The number of colours.

bool	QCDsuccess =true

Particle	quarks [6]
	The vector of all SM quarks.

bool	requireYd
	Switch for generating the Yukawa couplings to the down-type quarks.

bool	requireYu
	Switch for generating the Yukawa couplings to the up-type quarks.

double	TF

Protected Attributes inherited from Model
bool	isSliced = false
	A boolean set to true if the current istance is a slice of an extended object.

std::map< std::string, std::reference_wrapper< const double > >	ModelParamMap

bool	UpdateError = false
	A boolean set to false if update is successful.

Constructor & Destructor Documentation

◆ NPSMEFTd6General()

NPSMEFTd6General::NPSMEFTd6General ( )

Constructor.

Definition at line 330 of file NPSMEFTd6General.cpp.

:
NPbase(), NPSMEFTd6GM(*this),
        SMEFTEvolEW(), 
        SMEFTEvolMH(), SMEFTEvol240(), SMEFTEvol365(), SMEFTEvol550(), 
        SMEFTEvol1000(), SMEFTEvol1500(), SMEFTEvol3000(), SMEFTEvol5000(), 
        SMEFTEvolUV(),
        VuL(gslpp::matrix<complex>::Id(3)), VuLd(gslpp::matrix<complex>::Id(3)), 
        VuR(gslpp::matrix<complex>::Id(3)), VuRd(gslpp::matrix<complex>::Id(3)), 
        VdL(gslpp::matrix<complex>::Id(3)), VdLd(gslpp::matrix<complex>::Id(3)), 
        VdR(gslpp::matrix<complex>::Id(3)), VdRd(gslpp::matrix<complex>::Id(3)), 
        VeL(gslpp::matrix<complex>::Id(3)), VeLd(gslpp::matrix<complex>::Id(3)), 
        VeR(gslpp::matrix<complex>::Id(3)), VeRd(gslpp::matrix<complex>::Id(3)), 
        MUQ(3, 0.), MDQ(3, 0.) {
    
    setModelName("NPSMEFTd6General");
    
    FlagMWinput = false;
    FlagQuadraticTerms = false;
    FlagHiggsSM = false;
    FlagLoopHd6 = false;
    FlagLoopH3d6Quad = false;
    FlagRGEci = true;
    FlagCorrsInSMRunning = true;
    FlagmultiScaleRGE = false;
    FlagfiniteNLO = false;
    FlagmatchLEFT = true;
    FlagNewTerms = false;
    FlagMomProp = true;
    FlagMomVert = true;
    FlagHiggsExch = true;
    FlagQuadraticWC = false;
    SMEFTBasisFlag = "UP";
    flavBas = 1;
    setModelLinearized();
 
    w_WW = gsl_integration_cquad_workspace_alloc(100);
 
    SMM.setObj((StandardModelMatching&) NPSMEFTd6GM.getObj());
 
    if (getModelName().compare("NPSMEFTd6General") == 0) {
        // Map for the purely bosonic operators: CP even 
        ModelParamMap.insert(std::make_pair("CG_LNP", std::cref(CG_LNP)));
        ModelParamMap.insert(std::make_pair("CW_LNP", std::cref(CW_LNP)));
        ModelParamMap.insert(std::make_pair("CHG_LNP", std::cref(CHG_LNP)));
        ModelParamMap.insert(std::make_pair("CHW_LNP", std::cref(CHW_LNP)));
        ModelParamMap.insert(std::make_pair("CHB_LNP", std::cref(CHB_LNP)));
        ModelParamMap.insert(std::make_pair("CHWB_LNP", std::cref(CHWB_LNP)));
        ModelParamMap.insert(std::make_pair("CHD_LNP", std::cref(CHD_LNP)));
        ModelParamMap.insert(std::make_pair("CHbox_LNP", std::cref(CHbox_LNP)));
        ModelParamMap.insert(std::make_pair("CH_LNP", std::cref(CH_LNP)));
        // Map for the purely bosonic operators: CP odd 
        ModelParamMap.insert(std::make_pair("CGtilde_LNP", std::cref(CGtilde_LNP)));
        ModelParamMap.insert(std::make_pair("CWtilde_LNP", std::cref(CWtilde_LNP)));
        ModelParamMap.insert(std::make_pair("CHGtilde_LNP", std::cref(CHGtilde_LNP)));
        ModelParamMap.insert(std::make_pair("CHWtilde_LNP", std::cref(CHWtilde_LNP)));
        ModelParamMap.insert(std::make_pair("CHBtilde_LNP", std::cref(CHBtilde_LNP)));
        ModelParamMap.insert(std::make_pair("CHWtildeB_LNP", std::cref(CHWtildeB_LNP)));
        // Map for the Higgs-Lepton operators 
        ModelParamMap.insert(std::make_pair("CHl1_11r_LNP", std::cref(CHl1_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CHl1_12r_LNP", std::cref(CHl1_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CHl1_13r_LNP", std::cref(CHl1_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CHl1_22r_LNP", std::cref(CHl1_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CHl1_23r_LNP", std::cref(CHl1_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CHl1_33r_LNP", std::cref(CHl1_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CHl1_12i_LNP", std::cref(CHl1_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CHl1_13i_LNP", std::cref(CHl1_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CHl1_23i_LNP", std::cref(CHl1_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CHl3_11r_LNP", std::cref(CHl3_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CHl3_12r_LNP", std::cref(CHl3_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CHl3_13r_LNP", std::cref(CHl3_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CHl3_22r_LNP", std::cref(CHl3_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CHl3_23r_LNP", std::cref(CHl3_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CHl3_33r_LNP", std::cref(CHl3_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CHl3_12i_LNP", std::cref(CHl3_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CHl3_13i_LNP", std::cref(CHl3_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CHl3_23i_LNP", std::cref(CHl3_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CHe_11r_LNP", std::cref(CHe_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CHe_12r_LNP", std::cref(CHe_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CHe_13r_LNP", std::cref(CHe_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CHe_22r_LNP", std::cref(CHe_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CHe_23r_LNP", std::cref(CHe_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CHe_33r_LNP", std::cref(CHe_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CHe_12i_LNP", std::cref(CHe_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CHe_13i_LNP", std::cref(CHe_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CHe_23i_LNP", std::cref(CHe_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_11r_LNP", std::cref(CeH_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_12r_LNP", std::cref(CeH_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_13r_LNP", std::cref(CeH_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_21r_LNP", std::cref(CeH_21r_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_22r_LNP", std::cref(CeH_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_23r_LNP", std::cref(CeH_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_31r_LNP", std::cref(CeH_31r_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_32r_LNP", std::cref(CeH_32r_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_33r_LNP", std::cref(CeH_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_11i_LNP", std::cref(CeH_11i_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_12i_LNP", std::cref(CeH_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_13i_LNP", std::cref(CeH_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_21i_LNP", std::cref(CeH_21i_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_22i_LNP", std::cref(CeH_22i_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_23i_LNP", std::cref(CeH_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_31i_LNP", std::cref(CeH_31i_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_32i_LNP", std::cref(CeH_32i_LNP)));
        ModelParamMap.insert(std::make_pair("CeH_33i_LNP", std::cref(CeH_33i_LNP)));
        // Map for the Four-Lepton four-fermion operators 
        ModelParamMap.insert(std::make_pair("Cll_1111r_LNP", std::cref(Cll_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1112r_LNP", std::cref(Cll_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1113r_LNP", std::cref(Cll_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1122r_LNP", std::cref(Cll_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1123r_LNP", std::cref(Cll_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1133r_LNP", std::cref(Cll_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1212r_LNP", std::cref(Cll_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1213r_LNP", std::cref(Cll_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1221r_LNP", std::cref(Cll_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1222r_LNP", std::cref(Cll_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1223r_LNP", std::cref(Cll_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1231r_LNP", std::cref(Cll_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1232r_LNP", std::cref(Cll_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1233r_LNP", std::cref(Cll_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1313r_LNP", std::cref(Cll_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1322r_LNP", std::cref(Cll_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1323r_LNP", std::cref(Cll_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1331r_LNP", std::cref(Cll_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1332r_LNP", std::cref(Cll_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1333r_LNP", std::cref(Cll_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_2222r_LNP", std::cref(Cll_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_2223r_LNP", std::cref(Cll_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_2233r_LNP", std::cref(Cll_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_2323r_LNP", std::cref(Cll_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_2332r_LNP", std::cref(Cll_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_2333r_LNP", std::cref(Cll_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_3333r_LNP", std::cref(Cll_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1112i_LNP", std::cref(Cll_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1113i_LNP", std::cref(Cll_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1123i_LNP", std::cref(Cll_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1212i_LNP", std::cref(Cll_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1213i_LNP", std::cref(Cll_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1222i_LNP", std::cref(Cll_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1223i_LNP", std::cref(Cll_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1231i_LNP", std::cref(Cll_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1232i_LNP", std::cref(Cll_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1233i_LNP", std::cref(Cll_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1313i_LNP", std::cref(Cll_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1322i_LNP", std::cref(Cll_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1323i_LNP", std::cref(Cll_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1332i_LNP", std::cref(Cll_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_1333i_LNP", std::cref(Cll_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_2223i_LNP", std::cref(Cll_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_2323i_LNP", std::cref(Cll_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cll_2333i_LNP", std::cref(Cll_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1111r_LNP", std::cref(Cee_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1112r_LNP", std::cref(Cee_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1113r_LNP", std::cref(Cee_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1122r_LNP", std::cref(Cee_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1123r_LNP", std::cref(Cee_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1133r_LNP", std::cref(Cee_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1212r_LNP", std::cref(Cee_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1213r_LNP", std::cref(Cee_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1222r_LNP", std::cref(Cee_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1223r_LNP", std::cref(Cee_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1232r_LNP", std::cref(Cee_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1233r_LNP", std::cref(Cee_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1313r_LNP", std::cref(Cee_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1323r_LNP", std::cref(Cee_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1333r_LNP", std::cref(Cee_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_2222r_LNP", std::cref(Cee_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_2223r_LNP", std::cref(Cee_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_2233r_LNP", std::cref(Cee_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_2323r_LNP", std::cref(Cee_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_2333r_LNP", std::cref(Cee_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_3333r_LNP", std::cref(Cee_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1112i_LNP", std::cref(Cee_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1113i_LNP", std::cref(Cee_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1123i_LNP", std::cref(Cee_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1212i_LNP", std::cref(Cee_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1213i_LNP", std::cref(Cee_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1222i_LNP", std::cref(Cee_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1223i_LNP", std::cref(Cee_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1232i_LNP", std::cref(Cee_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1233i_LNP", std::cref(Cee_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1313i_LNP", std::cref(Cee_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1323i_LNP", std::cref(Cee_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_1333i_LNP", std::cref(Cee_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_2223i_LNP", std::cref(Cee_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_2323i_LNP", std::cref(Cee_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cee_2333i_LNP", std::cref(Cee_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1111r_LNP", std::cref(Cle_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1112r_LNP", std::cref(Cle_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1113r_LNP", std::cref(Cle_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1122r_LNP", std::cref(Cle_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1123r_LNP", std::cref(Cle_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1133r_LNP", std::cref(Cle_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1211r_LNP", std::cref(Cle_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1212r_LNP", std::cref(Cle_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1213r_LNP", std::cref(Cle_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1221r_LNP", std::cref(Cle_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1222r_LNP", std::cref(Cle_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1223r_LNP", std::cref(Cle_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1231r_LNP", std::cref(Cle_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1232r_LNP", std::cref(Cle_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1233r_LNP", std::cref(Cle_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1311r_LNP", std::cref(Cle_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1312r_LNP", std::cref(Cle_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1313r_LNP", std::cref(Cle_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1321r_LNP", std::cref(Cle_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1322r_LNP", std::cref(Cle_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1323r_LNP", std::cref(Cle_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1331r_LNP", std::cref(Cle_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1332r_LNP", std::cref(Cle_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1333r_LNP", std::cref(Cle_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2211r_LNP", std::cref(Cle_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2212r_LNP", std::cref(Cle_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2213r_LNP", std::cref(Cle_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2222r_LNP", std::cref(Cle_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2223r_LNP", std::cref(Cle_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2233r_LNP", std::cref(Cle_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2311r_LNP", std::cref(Cle_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2312r_LNP", std::cref(Cle_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2313r_LNP", std::cref(Cle_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2321r_LNP", std::cref(Cle_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2322r_LNP", std::cref(Cle_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2323r_LNP", std::cref(Cle_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2331r_LNP", std::cref(Cle_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2332r_LNP", std::cref(Cle_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2333r_LNP", std::cref(Cle_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_3311r_LNP", std::cref(Cle_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_3312r_LNP", std::cref(Cle_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_3313r_LNP", std::cref(Cle_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_3322r_LNP", std::cref(Cle_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_3323r_LNP", std::cref(Cle_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_3333r_LNP", std::cref(Cle_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1112i_LNP", std::cref(Cle_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1113i_LNP", std::cref(Cle_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1123i_LNP", std::cref(Cle_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1211i_LNP", std::cref(Cle_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1212i_LNP", std::cref(Cle_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1213i_LNP", std::cref(Cle_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1221i_LNP", std::cref(Cle_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1222i_LNP", std::cref(Cle_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1223i_LNP", std::cref(Cle_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1231i_LNP", std::cref(Cle_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1232i_LNP", std::cref(Cle_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1233i_LNP", std::cref(Cle_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1311i_LNP", std::cref(Cle_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1312i_LNP", std::cref(Cle_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1313i_LNP", std::cref(Cle_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1321i_LNP", std::cref(Cle_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1322i_LNP", std::cref(Cle_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1323i_LNP", std::cref(Cle_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1331i_LNP", std::cref(Cle_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1332i_LNP", std::cref(Cle_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_1333i_LNP", std::cref(Cle_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2212i_LNP", std::cref(Cle_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2213i_LNP", std::cref(Cle_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2223i_LNP", std::cref(Cle_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2312i_LNP", std::cref(Cle_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2313i_LNP", std::cref(Cle_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2321i_LNP", std::cref(Cle_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2322i_LNP", std::cref(Cle_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2323i_LNP", std::cref(Cle_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2331i_LNP", std::cref(Cle_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2332i_LNP", std::cref(Cle_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2333i_LNP", std::cref(Cle_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_2311i_LNP", std::cref(Cle_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_3312i_LNP", std::cref(Cle_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_3313i_LNP", std::cref(Cle_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cle_3323i_LNP", std::cref(Cle_3323i_LNP)));
        // Map for the Higgs-Quark operators 
        ModelParamMap.insert(std::make_pair("CHq1_11r_LNP", std::cref(CHq1_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CHq1_12r_LNP", std::cref(CHq1_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CHq1_13r_LNP", std::cref(CHq1_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CHq1_22r_LNP", std::cref(CHq1_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CHq1_23r_LNP", std::cref(CHq1_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CHq1_33r_LNP", std::cref(CHq1_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CHq1_12i_LNP", std::cref(CHq1_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CHq1_13i_LNP", std::cref(CHq1_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CHq1_23i_LNP", std::cref(CHq1_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CHq3_11r_LNP", std::cref(CHq3_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CHq3_12r_LNP", std::cref(CHq3_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CHq3_13r_LNP", std::cref(CHq3_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CHq3_22r_LNP", std::cref(CHq3_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CHq3_23r_LNP", std::cref(CHq3_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CHq3_33r_LNP", std::cref(CHq3_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CHq3_12i_LNP", std::cref(CHq3_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CHq3_13i_LNP", std::cref(CHq3_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CHq3_23i_LNP", std::cref(CHq3_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CHu_11r_LNP", std::cref(CHu_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CHu_12r_LNP", std::cref(CHu_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CHu_13r_LNP", std::cref(CHu_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CHu_22r_LNP", std::cref(CHu_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CHu_23r_LNP", std::cref(CHu_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CHu_33r_LNP", std::cref(CHu_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CHu_12i_LNP", std::cref(CHu_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CHu_13i_LNP", std::cref(CHu_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CHu_23i_LNP", std::cref(CHu_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CHd_11r_LNP", std::cref(CHd_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CHd_12r_LNP", std::cref(CHd_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CHd_13r_LNP", std::cref(CHd_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CHd_22r_LNP", std::cref(CHd_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CHd_23r_LNP", std::cref(CHd_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CHd_33r_LNP", std::cref(CHd_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CHd_12i_LNP", std::cref(CHd_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CHd_13i_LNP", std::cref(CHd_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CHd_23i_LNP", std::cref(CHd_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_11r_LNP", std::cref(CHud_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_12r_LNP", std::cref(CHud_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_13r_LNP", std::cref(CHud_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_21r_LNP", std::cref(CHud_21r_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_22r_LNP", std::cref(CHud_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_23r_LNP", std::cref(CHud_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_31r_LNP", std::cref(CHud_31r_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_32r_LNP", std::cref(CHud_32r_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_33r_LNP", std::cref(CHud_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_11i_LNP", std::cref(CHud_11i_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_12i_LNP", std::cref(CHud_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_13i_LNP", std::cref(CHud_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_21i_LNP", std::cref(CHud_21i_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_22i_LNP", std::cref(CHud_22i_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_23i_LNP", std::cref(CHud_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_31i_LNP", std::cref(CHud_31i_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_32i_LNP", std::cref(CHud_32i_LNP)));
        ModelParamMap.insert(std::make_pair("CHud_33i_LNP", std::cref(CHud_33i_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_11r_LNP", std::cref(CuH_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_12r_LNP", std::cref(CuH_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_13r_LNP", std::cref(CuH_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_21r_LNP", std::cref(CuH_21r_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_22r_LNP", std::cref(CuH_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_23r_LNP", std::cref(CuH_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_31r_LNP", std::cref(CuH_31r_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_32r_LNP", std::cref(CuH_32r_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_33r_LNP", std::cref(CuH_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_11i_LNP", std::cref(CuH_11i_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_12i_LNP", std::cref(CuH_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_13i_LNP", std::cref(CuH_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_21i_LNP", std::cref(CuH_21i_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_22i_LNP", std::cref(CuH_22i_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_23i_LNP", std::cref(CuH_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_31i_LNP", std::cref(CuH_31i_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_32i_LNP", std::cref(CuH_32i_LNP)));
        ModelParamMap.insert(std::make_pair("CuH_33i_LNP", std::cref(CuH_33i_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_11r_LNP", std::cref(CdH_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_12r_LNP", std::cref(CdH_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_13r_LNP", std::cref(CdH_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_21r_LNP", std::cref(CdH_21r_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_22r_LNP", std::cref(CdH_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_23r_LNP", std::cref(CdH_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_31r_LNP", std::cref(CdH_31r_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_32r_LNP", std::cref(CdH_32r_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_33r_LNP", std::cref(CdH_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_11i_LNP", std::cref(CdH_11i_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_12i_LNP", std::cref(CdH_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_13i_LNP", std::cref(CdH_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_21i_LNP", std::cref(CdH_21i_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_22i_LNP", std::cref(CdH_22i_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_23i_LNP", std::cref(CdH_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_31i_LNP", std::cref(CdH_31i_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_32i_LNP", std::cref(CdH_32i_LNP)));
        ModelParamMap.insert(std::make_pair("CdH_33i_LNP", std::cref(CdH_33i_LNP)));
        // Map for the dipole operators 
        ModelParamMap.insert(std::make_pair("CuG_11r_LNP", std::cref(CuG_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_12r_LNP", std::cref(CuG_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_13r_LNP", std::cref(CuG_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_21r_LNP", std::cref(CuG_21r_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_22r_LNP", std::cref(CuG_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_23r_LNP", std::cref(CuG_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_31r_LNP", std::cref(CuG_31r_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_32r_LNP", std::cref(CuG_32r_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_33r_LNP", std::cref(CuG_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_11i_LNP", std::cref(CuG_11i_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_12i_LNP", std::cref(CuG_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_13i_LNP", std::cref(CuG_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_21i_LNP", std::cref(CuG_21i_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_22i_LNP", std::cref(CuG_22i_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_23i_LNP", std::cref(CuG_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_31i_LNP", std::cref(CuG_31i_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_32i_LNP", std::cref(CuG_32i_LNP)));
        ModelParamMap.insert(std::make_pair("CuG_33i_LNP", std::cref(CuG_33i_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_11r_LNP", std::cref(CuW_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_12r_LNP", std::cref(CuW_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_13r_LNP", std::cref(CuW_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_21r_LNP", std::cref(CuW_21r_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_22r_LNP", std::cref(CuW_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_23r_LNP", std::cref(CuW_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_31r_LNP", std::cref(CuW_31r_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_32r_LNP", std::cref(CuW_32r_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_33r_LNP", std::cref(CuW_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_11i_LNP", std::cref(CuW_11i_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_12i_LNP", std::cref(CuW_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_13i_LNP", std::cref(CuW_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_21i_LNP", std::cref(CuW_21i_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_22i_LNP", std::cref(CuW_22i_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_23i_LNP", std::cref(CuW_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_31i_LNP", std::cref(CuW_31i_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_32i_LNP", std::cref(CuW_32i_LNP)));
        ModelParamMap.insert(std::make_pair("CuW_33i_LNP", std::cref(CuW_33i_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_11r_LNP", std::cref(CuB_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_12r_LNP", std::cref(CuB_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_13r_LNP", std::cref(CuB_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_21r_LNP", std::cref(CuB_21r_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_22r_LNP", std::cref(CuB_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_23r_LNP", std::cref(CuB_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_31r_LNP", std::cref(CuB_31r_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_32r_LNP", std::cref(CuB_32r_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_33r_LNP", std::cref(CuB_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_11i_LNP", std::cref(CuB_11i_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_12i_LNP", std::cref(CuB_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_13i_LNP", std::cref(CuB_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_21i_LNP", std::cref(CuB_21i_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_22i_LNP", std::cref(CuB_22i_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_23i_LNP", std::cref(CuB_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_31i_LNP", std::cref(CuB_31i_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_32i_LNP", std::cref(CuB_32i_LNP)));
        ModelParamMap.insert(std::make_pair("CuB_33i_LNP", std::cref(CuB_33i_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_11r_LNP", std::cref(CdG_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_12r_LNP", std::cref(CdG_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_13r_LNP", std::cref(CdG_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_21r_LNP", std::cref(CdG_21r_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_22r_LNP", std::cref(CdG_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_23r_LNP", std::cref(CdG_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_31r_LNP", std::cref(CdG_31r_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_32r_LNP", std::cref(CdG_32r_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_33r_LNP", std::cref(CdG_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_11i_LNP", std::cref(CdG_11i_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_12i_LNP", std::cref(CdG_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_13i_LNP", std::cref(CdG_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_21i_LNP", std::cref(CdG_21i_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_22i_LNP", std::cref(CdG_22i_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_23i_LNP", std::cref(CdG_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_31i_LNP", std::cref(CdG_31i_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_32i_LNP", std::cref(CdG_32i_LNP)));
        ModelParamMap.insert(std::make_pair("CdG_33i_LNP", std::cref(CdG_33i_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_11r_LNP", std::cref(CdW_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_12r_LNP", std::cref(CdW_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_13r_LNP", std::cref(CdW_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_21r_LNP", std::cref(CdW_21r_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_22r_LNP", std::cref(CdW_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_23r_LNP", std::cref(CdW_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_31r_LNP", std::cref(CdW_31r_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_32r_LNP", std::cref(CdW_32r_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_33r_LNP", std::cref(CdW_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_11i_LNP", std::cref(CdW_11i_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_12i_LNP", std::cref(CdW_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_13i_LNP", std::cref(CdW_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_21i_LNP", std::cref(CdW_21i_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_22i_LNP", std::cref(CdW_22i_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_23i_LNP", std::cref(CdW_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_31i_LNP", std::cref(CdW_31i_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_32i_LNP", std::cref(CdW_32i_LNP)));
        ModelParamMap.insert(std::make_pair("CdW_33i_LNP", std::cref(CdW_33i_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_11r_LNP", std::cref(CdB_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_12r_LNP", std::cref(CdB_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_13r_LNP", std::cref(CdB_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_21r_LNP", std::cref(CdB_21r_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_22r_LNP", std::cref(CdB_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_23r_LNP", std::cref(CdB_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_31r_LNP", std::cref(CdB_31r_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_32r_LNP", std::cref(CdB_32r_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_33r_LNP", std::cref(CdB_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_11i_LNP", std::cref(CdB_11i_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_12i_LNP", std::cref(CdB_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_13i_LNP", std::cref(CdB_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_21i_LNP", std::cref(CdB_21i_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_22i_LNP", std::cref(CdB_22i_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_23i_LNP", std::cref(CdB_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_31i_LNP", std::cref(CdB_31i_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_32i_LNP", std::cref(CdB_32i_LNP)));
        ModelParamMap.insert(std::make_pair("CdB_33i_LNP", std::cref(CdB_33i_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_11r_LNP", std::cref(CeW_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_12r_LNP", std::cref(CeW_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_13r_LNP", std::cref(CeW_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_21r_LNP", std::cref(CeW_21r_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_22r_LNP", std::cref(CeW_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_23r_LNP", std::cref(CeW_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_31r_LNP", std::cref(CeW_31r_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_32r_LNP", std::cref(CeW_32r_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_33r_LNP", std::cref(CeW_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_11i_LNP", std::cref(CeW_11i_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_12i_LNP", std::cref(CeW_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_13i_LNP", std::cref(CeW_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_21i_LNP", std::cref(CeW_21i_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_22i_LNP", std::cref(CeW_22i_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_23i_LNP", std::cref(CeW_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_31i_LNP", std::cref(CeW_31i_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_32i_LNP", std::cref(CeW_32i_LNP)));
        ModelParamMap.insert(std::make_pair("CeW_33i_LNP", std::cref(CeW_33i_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_11r_LNP", std::cref(CeB_11r_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_12r_LNP", std::cref(CeB_12r_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_13r_LNP", std::cref(CeB_13r_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_21r_LNP", std::cref(CeB_21r_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_22r_LNP", std::cref(CeB_22r_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_23r_LNP", std::cref(CeB_23r_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_31r_LNP", std::cref(CeB_31r_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_32r_LNP", std::cref(CeB_32r_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_33r_LNP", std::cref(CeB_33r_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_11i_LNP", std::cref(CeB_11i_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_12i_LNP", std::cref(CeB_12i_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_13i_LNP", std::cref(CeB_13i_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_21i_LNP", std::cref(CeB_21i_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_22i_LNP", std::cref(CeB_22i_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_23i_LNP", std::cref(CeB_23i_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_31i_LNP", std::cref(CeB_31i_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_32i_LNP", std::cref(CeB_32i_LNP)));
        ModelParamMap.insert(std::make_pair("CeB_33i_LNP", std::cref(CeB_33i_LNP)));
        // Map for the Four-Quark four-fermion operators: LL, RR, LLRR 
        ModelParamMap.insert(std::make_pair("Cqq1_1111r_LNP", std::cref(Cqq1_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1112r_LNP", std::cref(Cqq1_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1113r_LNP", std::cref(Cqq1_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1122r_LNP", std::cref(Cqq1_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1123r_LNP", std::cref(Cqq1_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1133r_LNP", std::cref(Cqq1_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1212r_LNP", std::cref(Cqq1_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1213r_LNP", std::cref(Cqq1_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1221r_LNP", std::cref(Cqq1_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1222r_LNP", std::cref(Cqq1_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1223r_LNP", std::cref(Cqq1_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1231r_LNP", std::cref(Cqq1_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1232r_LNP", std::cref(Cqq1_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1233r_LNP", std::cref(Cqq1_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1313r_LNP", std::cref(Cqq1_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1322r_LNP", std::cref(Cqq1_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1323r_LNP", std::cref(Cqq1_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1331r_LNP", std::cref(Cqq1_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1332r_LNP", std::cref(Cqq1_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1333r_LNP", std::cref(Cqq1_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_2222r_LNP", std::cref(Cqq1_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_2223r_LNP", std::cref(Cqq1_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_2233r_LNP", std::cref(Cqq1_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_2323r_LNP", std::cref(Cqq1_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_2332r_LNP", std::cref(Cqq1_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_2333r_LNP", std::cref(Cqq1_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_3333r_LNP", std::cref(Cqq1_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1112i_LNP", std::cref(Cqq1_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1113i_LNP", std::cref(Cqq1_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1123i_LNP", std::cref(Cqq1_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1212i_LNP", std::cref(Cqq1_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1213i_LNP", std::cref(Cqq1_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1222i_LNP", std::cref(Cqq1_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1223i_LNP", std::cref(Cqq1_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1231i_LNP", std::cref(Cqq1_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1232i_LNP", std::cref(Cqq1_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1233i_LNP", std::cref(Cqq1_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1313i_LNP", std::cref(Cqq1_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1322i_LNP", std::cref(Cqq1_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1323i_LNP", std::cref(Cqq1_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1332i_LNP", std::cref(Cqq1_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_1333i_LNP", std::cref(Cqq1_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_2223i_LNP", std::cref(Cqq1_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_2323i_LNP", std::cref(Cqq1_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq1_2333i_LNP", std::cref(Cqq1_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1111r_LNP", std::cref(Cqq3_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1112r_LNP", std::cref(Cqq3_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1113r_LNP", std::cref(Cqq3_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1122r_LNP", std::cref(Cqq3_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1123r_LNP", std::cref(Cqq3_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1133r_LNP", std::cref(Cqq3_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1212r_LNP", std::cref(Cqq3_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1213r_LNP", std::cref(Cqq3_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1221r_LNP", std::cref(Cqq3_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1222r_LNP", std::cref(Cqq3_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1223r_LNP", std::cref(Cqq3_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1231r_LNP", std::cref(Cqq3_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1232r_LNP", std::cref(Cqq3_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1233r_LNP", std::cref(Cqq3_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1313r_LNP", std::cref(Cqq3_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1322r_LNP", std::cref(Cqq3_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1323r_LNP", std::cref(Cqq3_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1331r_LNP", std::cref(Cqq3_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1332r_LNP", std::cref(Cqq3_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1333r_LNP", std::cref(Cqq3_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_2222r_LNP", std::cref(Cqq3_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_2223r_LNP", std::cref(Cqq3_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_2233r_LNP", std::cref(Cqq3_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_2323r_LNP", std::cref(Cqq3_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_2332r_LNP", std::cref(Cqq3_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_2333r_LNP", std::cref(Cqq3_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_3333r_LNP", std::cref(Cqq3_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1112i_LNP", std::cref(Cqq3_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1113i_LNP", std::cref(Cqq3_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1123i_LNP", std::cref(Cqq3_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1212i_LNP", std::cref(Cqq3_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1213i_LNP", std::cref(Cqq3_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1222i_LNP", std::cref(Cqq3_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1223i_LNP", std::cref(Cqq3_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1231i_LNP", std::cref(Cqq3_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1232i_LNP", std::cref(Cqq3_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1233i_LNP", std::cref(Cqq3_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1313i_LNP", std::cref(Cqq3_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1322i_LNP", std::cref(Cqq3_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1323i_LNP", std::cref(Cqq3_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1332i_LNP", std::cref(Cqq3_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_1333i_LNP", std::cref(Cqq3_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_2223i_LNP", std::cref(Cqq3_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_2323i_LNP", std::cref(Cqq3_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqq3_2333i_LNP", std::cref(Cqq3_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1111r_LNP", std::cref(Cuu_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1112r_LNP", std::cref(Cuu_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1113r_LNP", std::cref(Cuu_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1122r_LNP", std::cref(Cuu_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1123r_LNP", std::cref(Cuu_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1133r_LNP", std::cref(Cuu_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1212r_LNP", std::cref(Cuu_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1213r_LNP", std::cref(Cuu_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1221r_LNP", std::cref(Cuu_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1222r_LNP", std::cref(Cuu_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1223r_LNP", std::cref(Cuu_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1231r_LNP", std::cref(Cuu_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1232r_LNP", std::cref(Cuu_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1233r_LNP", std::cref(Cuu_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1313r_LNP", std::cref(Cuu_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1322r_LNP", std::cref(Cuu_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1323r_LNP", std::cref(Cuu_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1331r_LNP", std::cref(Cuu_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1332r_LNP", std::cref(Cuu_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1333r_LNP", std::cref(Cuu_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_2222r_LNP", std::cref(Cuu_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_2223r_LNP", std::cref(Cuu_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_2233r_LNP", std::cref(Cuu_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_2323r_LNP", std::cref(Cuu_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_2332r_LNP", std::cref(Cuu_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_2333r_LNP", std::cref(Cuu_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_3333r_LNP", std::cref(Cuu_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1112i_LNP", std::cref(Cuu_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1113i_LNP", std::cref(Cuu_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1123i_LNP", std::cref(Cuu_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1212i_LNP", std::cref(Cuu_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1213i_LNP", std::cref(Cuu_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1222i_LNP", std::cref(Cuu_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1223i_LNP", std::cref(Cuu_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1231i_LNP", std::cref(Cuu_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1232i_LNP", std::cref(Cuu_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1233i_LNP", std::cref(Cuu_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1313i_LNP", std::cref(Cuu_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1322i_LNP", std::cref(Cuu_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1323i_LNP", std::cref(Cuu_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1332i_LNP", std::cref(Cuu_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_1333i_LNP", std::cref(Cuu_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_2223i_LNP", std::cref(Cuu_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_2323i_LNP", std::cref(Cuu_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cuu_2333i_LNP", std::cref(Cuu_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1111r_LNP", std::cref(Cdd_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1112r_LNP", std::cref(Cdd_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1113r_LNP", std::cref(Cdd_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1122r_LNP", std::cref(Cdd_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1123r_LNP", std::cref(Cdd_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1133r_LNP", std::cref(Cdd_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1212r_LNP", std::cref(Cdd_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1213r_LNP", std::cref(Cdd_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1221r_LNP", std::cref(Cdd_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1222r_LNP", std::cref(Cdd_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1223r_LNP", std::cref(Cdd_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1231r_LNP", std::cref(Cdd_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1232r_LNP", std::cref(Cdd_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1233r_LNP", std::cref(Cdd_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1313r_LNP", std::cref(Cdd_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1322r_LNP", std::cref(Cdd_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1323r_LNP", std::cref(Cdd_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1331r_LNP", std::cref(Cdd_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1332r_LNP", std::cref(Cdd_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1333r_LNP", std::cref(Cdd_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_2222r_LNP", std::cref(Cdd_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_2223r_LNP", std::cref(Cdd_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_2233r_LNP", std::cref(Cdd_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_2323r_LNP", std::cref(Cdd_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_2332r_LNP", std::cref(Cdd_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_2333r_LNP", std::cref(Cdd_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_3333r_LNP", std::cref(Cdd_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1112i_LNP", std::cref(Cdd_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1113i_LNP", std::cref(Cdd_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1123i_LNP", std::cref(Cdd_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1212i_LNP", std::cref(Cdd_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1213i_LNP", std::cref(Cdd_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1222i_LNP", std::cref(Cdd_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1223i_LNP", std::cref(Cdd_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1231i_LNP", std::cref(Cdd_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1232i_LNP", std::cref(Cdd_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1233i_LNP", std::cref(Cdd_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1313i_LNP", std::cref(Cdd_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1322i_LNP", std::cref(Cdd_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1323i_LNP", std::cref(Cdd_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1332i_LNP", std::cref(Cdd_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_1333i_LNP", std::cref(Cdd_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_2223i_LNP", std::cref(Cdd_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_2323i_LNP", std::cref(Cdd_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cdd_2333i_LNP", std::cref(Cdd_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1111r_LNP", std::cref(Cud1_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1112r_LNP", std::cref(Cud1_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1113r_LNP", std::cref(Cud1_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1122r_LNP", std::cref(Cud1_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1123r_LNP", std::cref(Cud1_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1133r_LNP", std::cref(Cud1_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1211r_LNP", std::cref(Cud1_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1212r_LNP", std::cref(Cud1_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1213r_LNP", std::cref(Cud1_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1221r_LNP", std::cref(Cud1_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1222r_LNP", std::cref(Cud1_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1223r_LNP", std::cref(Cud1_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1231r_LNP", std::cref(Cud1_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1232r_LNP", std::cref(Cud1_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1233r_LNP", std::cref(Cud1_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1311r_LNP", std::cref(Cud1_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1312r_LNP", std::cref(Cud1_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1313r_LNP", std::cref(Cud1_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1321r_LNP", std::cref(Cud1_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1322r_LNP", std::cref(Cud1_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1323r_LNP", std::cref(Cud1_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1331r_LNP", std::cref(Cud1_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1332r_LNP", std::cref(Cud1_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1333r_LNP", std::cref(Cud1_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2211r_LNP", std::cref(Cud1_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2212r_LNP", std::cref(Cud1_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2213r_LNP", std::cref(Cud1_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2222r_LNP", std::cref(Cud1_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2223r_LNP", std::cref(Cud1_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2233r_LNP", std::cref(Cud1_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2311r_LNP", std::cref(Cud1_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2312r_LNP", std::cref(Cud1_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2313r_LNP", std::cref(Cud1_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2321r_LNP", std::cref(Cud1_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2322r_LNP", std::cref(Cud1_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2323r_LNP", std::cref(Cud1_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2331r_LNP", std::cref(Cud1_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2332r_LNP", std::cref(Cud1_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2333r_LNP", std::cref(Cud1_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_3311r_LNP", std::cref(Cud1_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_3312r_LNP", std::cref(Cud1_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_3313r_LNP", std::cref(Cud1_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_3322r_LNP", std::cref(Cud1_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_3323r_LNP", std::cref(Cud1_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_3333r_LNP", std::cref(Cud1_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1112i_LNP", std::cref(Cud1_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1113i_LNP", std::cref(Cud1_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1123i_LNP", std::cref(Cud1_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1211i_LNP", std::cref(Cud1_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1212i_LNP", std::cref(Cud1_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1213i_LNP", std::cref(Cud1_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1221i_LNP", std::cref(Cud1_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1222i_LNP", std::cref(Cud1_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1223i_LNP", std::cref(Cud1_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1231i_LNP", std::cref(Cud1_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1232i_LNP", std::cref(Cud1_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1233i_LNP", std::cref(Cud1_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1311i_LNP", std::cref(Cud1_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1312i_LNP", std::cref(Cud1_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1313i_LNP", std::cref(Cud1_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1321i_LNP", std::cref(Cud1_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1322i_LNP", std::cref(Cud1_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1323i_LNP", std::cref(Cud1_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1331i_LNP", std::cref(Cud1_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1332i_LNP", std::cref(Cud1_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_1333i_LNP", std::cref(Cud1_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2212i_LNP", std::cref(Cud1_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2213i_LNP", std::cref(Cud1_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2223i_LNP", std::cref(Cud1_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2312i_LNP", std::cref(Cud1_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2313i_LNP", std::cref(Cud1_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2321i_LNP", std::cref(Cud1_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2322i_LNP", std::cref(Cud1_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2323i_LNP", std::cref(Cud1_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2331i_LNP", std::cref(Cud1_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2332i_LNP", std::cref(Cud1_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2333i_LNP", std::cref(Cud1_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_2311i_LNP", std::cref(Cud1_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_3312i_LNP", std::cref(Cud1_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_3313i_LNP", std::cref(Cud1_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud1_3323i_LNP", std::cref(Cud1_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1111r_LNP", std::cref(Cud8_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1112r_LNP", std::cref(Cud8_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1113r_LNP", std::cref(Cud8_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1122r_LNP", std::cref(Cud8_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1123r_LNP", std::cref(Cud8_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1133r_LNP", std::cref(Cud8_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1211r_LNP", std::cref(Cud8_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1212r_LNP", std::cref(Cud8_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1213r_LNP", std::cref(Cud8_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1221r_LNP", std::cref(Cud8_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1222r_LNP", std::cref(Cud8_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1223r_LNP", std::cref(Cud8_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1231r_LNP", std::cref(Cud8_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1232r_LNP", std::cref(Cud8_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1233r_LNP", std::cref(Cud8_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1311r_LNP", std::cref(Cud8_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1312r_LNP", std::cref(Cud8_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1313r_LNP", std::cref(Cud8_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1321r_LNP", std::cref(Cud8_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1322r_LNP", std::cref(Cud8_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1323r_LNP", std::cref(Cud8_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1331r_LNP", std::cref(Cud8_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1332r_LNP", std::cref(Cud8_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1333r_LNP", std::cref(Cud8_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2211r_LNP", std::cref(Cud8_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2212r_LNP", std::cref(Cud8_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2213r_LNP", std::cref(Cud8_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2222r_LNP", std::cref(Cud8_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2223r_LNP", std::cref(Cud8_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2233r_LNP", std::cref(Cud8_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2311r_LNP", std::cref(Cud8_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2312r_LNP", std::cref(Cud8_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2313r_LNP", std::cref(Cud8_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2321r_LNP", std::cref(Cud8_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2322r_LNP", std::cref(Cud8_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2323r_LNP", std::cref(Cud8_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2331r_LNP", std::cref(Cud8_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2332r_LNP", std::cref(Cud8_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2333r_LNP", std::cref(Cud8_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_3311r_LNP", std::cref(Cud8_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_3312r_LNP", std::cref(Cud8_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_3313r_LNP", std::cref(Cud8_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_3322r_LNP", std::cref(Cud8_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_3323r_LNP", std::cref(Cud8_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_3333r_LNP", std::cref(Cud8_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1112i_LNP", std::cref(Cud8_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1113i_LNP", std::cref(Cud8_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1123i_LNP", std::cref(Cud8_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1211i_LNP", std::cref(Cud8_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1212i_LNP", std::cref(Cud8_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1213i_LNP", std::cref(Cud8_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1221i_LNP", std::cref(Cud8_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1222i_LNP", std::cref(Cud8_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1223i_LNP", std::cref(Cud8_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1231i_LNP", std::cref(Cud8_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1232i_LNP", std::cref(Cud8_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1233i_LNP", std::cref(Cud8_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1311i_LNP", std::cref(Cud8_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1312i_LNP", std::cref(Cud8_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1313i_LNP", std::cref(Cud8_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1321i_LNP", std::cref(Cud8_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1322i_LNP", std::cref(Cud8_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1323i_LNP", std::cref(Cud8_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1331i_LNP", std::cref(Cud8_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1332i_LNP", std::cref(Cud8_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_1333i_LNP", std::cref(Cud8_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2212i_LNP", std::cref(Cud8_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2213i_LNP", std::cref(Cud8_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2223i_LNP", std::cref(Cud8_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2312i_LNP", std::cref(Cud8_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2313i_LNP", std::cref(Cud8_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2321i_LNP", std::cref(Cud8_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2322i_LNP", std::cref(Cud8_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2323i_LNP", std::cref(Cud8_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2331i_LNP", std::cref(Cud8_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2332i_LNP", std::cref(Cud8_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2333i_LNP", std::cref(Cud8_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_2311i_LNP", std::cref(Cud8_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_3312i_LNP", std::cref(Cud8_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_3313i_LNP", std::cref(Cud8_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cud8_3323i_LNP", std::cref(Cud8_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1111r_LNP", std::cref(Cqu1_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1112r_LNP", std::cref(Cqu1_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1113r_LNP", std::cref(Cqu1_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1122r_LNP", std::cref(Cqu1_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1123r_LNP", std::cref(Cqu1_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1133r_LNP", std::cref(Cqu1_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1211r_LNP", std::cref(Cqu1_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1212r_LNP", std::cref(Cqu1_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1213r_LNP", std::cref(Cqu1_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1221r_LNP", std::cref(Cqu1_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1222r_LNP", std::cref(Cqu1_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1223r_LNP", std::cref(Cqu1_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1231r_LNP", std::cref(Cqu1_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1232r_LNP", std::cref(Cqu1_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1233r_LNP", std::cref(Cqu1_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1311r_LNP", std::cref(Cqu1_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1312r_LNP", std::cref(Cqu1_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1313r_LNP", std::cref(Cqu1_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1321r_LNP", std::cref(Cqu1_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1322r_LNP", std::cref(Cqu1_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1323r_LNP", std::cref(Cqu1_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1331r_LNP", std::cref(Cqu1_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1332r_LNP", std::cref(Cqu1_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1333r_LNP", std::cref(Cqu1_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2211r_LNP", std::cref(Cqu1_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2212r_LNP", std::cref(Cqu1_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2213r_LNP", std::cref(Cqu1_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2222r_LNP", std::cref(Cqu1_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2223r_LNP", std::cref(Cqu1_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2233r_LNP", std::cref(Cqu1_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2311r_LNP", std::cref(Cqu1_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2312r_LNP", std::cref(Cqu1_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2313r_LNP", std::cref(Cqu1_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2321r_LNP", std::cref(Cqu1_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2322r_LNP", std::cref(Cqu1_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2323r_LNP", std::cref(Cqu1_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2331r_LNP", std::cref(Cqu1_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2332r_LNP", std::cref(Cqu1_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2333r_LNP", std::cref(Cqu1_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_3311r_LNP", std::cref(Cqu1_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_3312r_LNP", std::cref(Cqu1_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_3313r_LNP", std::cref(Cqu1_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_3322r_LNP", std::cref(Cqu1_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_3323r_LNP", std::cref(Cqu1_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_3333r_LNP", std::cref(Cqu1_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1112i_LNP", std::cref(Cqu1_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1113i_LNP", std::cref(Cqu1_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1123i_LNP", std::cref(Cqu1_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1211i_LNP", std::cref(Cqu1_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1212i_LNP", std::cref(Cqu1_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1213i_LNP", std::cref(Cqu1_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1221i_LNP", std::cref(Cqu1_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1222i_LNP", std::cref(Cqu1_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1223i_LNP", std::cref(Cqu1_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1231i_LNP", std::cref(Cqu1_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1232i_LNP", std::cref(Cqu1_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1233i_LNP", std::cref(Cqu1_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1311i_LNP", std::cref(Cqu1_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1312i_LNP", std::cref(Cqu1_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1313i_LNP", std::cref(Cqu1_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1321i_LNP", std::cref(Cqu1_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1322i_LNP", std::cref(Cqu1_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1323i_LNP", std::cref(Cqu1_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1331i_LNP", std::cref(Cqu1_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1332i_LNP", std::cref(Cqu1_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_1333i_LNP", std::cref(Cqu1_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2212i_LNP", std::cref(Cqu1_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2213i_LNP", std::cref(Cqu1_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2223i_LNP", std::cref(Cqu1_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2312i_LNP", std::cref(Cqu1_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2313i_LNP", std::cref(Cqu1_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2321i_LNP", std::cref(Cqu1_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2322i_LNP", std::cref(Cqu1_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2323i_LNP", std::cref(Cqu1_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2331i_LNP", std::cref(Cqu1_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2332i_LNP", std::cref(Cqu1_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2333i_LNP", std::cref(Cqu1_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_2311i_LNP", std::cref(Cqu1_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_3312i_LNP", std::cref(Cqu1_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_3313i_LNP", std::cref(Cqu1_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu1_3323i_LNP", std::cref(Cqu1_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1111r_LNP", std::cref(Cqu8_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1112r_LNP", std::cref(Cqu8_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1113r_LNP", std::cref(Cqu8_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1122r_LNP", std::cref(Cqu8_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1123r_LNP", std::cref(Cqu8_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1133r_LNP", std::cref(Cqu8_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1211r_LNP", std::cref(Cqu8_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1212r_LNP", std::cref(Cqu8_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1213r_LNP", std::cref(Cqu8_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1221r_LNP", std::cref(Cqu8_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1222r_LNP", std::cref(Cqu8_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1223r_LNP", std::cref(Cqu8_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1231r_LNP", std::cref(Cqu8_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1232r_LNP", std::cref(Cqu8_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1233r_LNP", std::cref(Cqu8_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1311r_LNP", std::cref(Cqu8_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1312r_LNP", std::cref(Cqu8_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1313r_LNP", std::cref(Cqu8_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1321r_LNP", std::cref(Cqu8_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1322r_LNP", std::cref(Cqu8_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1323r_LNP", std::cref(Cqu8_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1331r_LNP", std::cref(Cqu8_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1332r_LNP", std::cref(Cqu8_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1333r_LNP", std::cref(Cqu8_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2211r_LNP", std::cref(Cqu8_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2212r_LNP", std::cref(Cqu8_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2213r_LNP", std::cref(Cqu8_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2222r_LNP", std::cref(Cqu8_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2223r_LNP", std::cref(Cqu8_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2233r_LNP", std::cref(Cqu8_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2311r_LNP", std::cref(Cqu8_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2312r_LNP", std::cref(Cqu8_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2313r_LNP", std::cref(Cqu8_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2321r_LNP", std::cref(Cqu8_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2322r_LNP", std::cref(Cqu8_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2323r_LNP", std::cref(Cqu8_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2331r_LNP", std::cref(Cqu8_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2332r_LNP", std::cref(Cqu8_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2333r_LNP", std::cref(Cqu8_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_3311r_LNP", std::cref(Cqu8_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_3312r_LNP", std::cref(Cqu8_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_3313r_LNP", std::cref(Cqu8_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_3322r_LNP", std::cref(Cqu8_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_3323r_LNP", std::cref(Cqu8_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_3333r_LNP", std::cref(Cqu8_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1112i_LNP", std::cref(Cqu8_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1113i_LNP", std::cref(Cqu8_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1123i_LNP", std::cref(Cqu8_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1211i_LNP", std::cref(Cqu8_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1212i_LNP", std::cref(Cqu8_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1213i_LNP", std::cref(Cqu8_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1221i_LNP", std::cref(Cqu8_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1222i_LNP", std::cref(Cqu8_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1223i_LNP", std::cref(Cqu8_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1231i_LNP", std::cref(Cqu8_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1232i_LNP", std::cref(Cqu8_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1233i_LNP", std::cref(Cqu8_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1311i_LNP", std::cref(Cqu8_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1312i_LNP", std::cref(Cqu8_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1313i_LNP", std::cref(Cqu8_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1321i_LNP", std::cref(Cqu8_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1322i_LNP", std::cref(Cqu8_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1323i_LNP", std::cref(Cqu8_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1331i_LNP", std::cref(Cqu8_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1332i_LNP", std::cref(Cqu8_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_1333i_LNP", std::cref(Cqu8_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2212i_LNP", std::cref(Cqu8_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2213i_LNP", std::cref(Cqu8_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2223i_LNP", std::cref(Cqu8_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2312i_LNP", std::cref(Cqu8_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2313i_LNP", std::cref(Cqu8_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2321i_LNP", std::cref(Cqu8_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2322i_LNP", std::cref(Cqu8_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2323i_LNP", std::cref(Cqu8_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2331i_LNP", std::cref(Cqu8_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2332i_LNP", std::cref(Cqu8_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2333i_LNP", std::cref(Cqu8_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_2311i_LNP", std::cref(Cqu8_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_3312i_LNP", std::cref(Cqu8_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_3313i_LNP", std::cref(Cqu8_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqu8_3323i_LNP", std::cref(Cqu8_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1111r_LNP", std::cref(Cqd1_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1112r_LNP", std::cref(Cqd1_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1113r_LNP", std::cref(Cqd1_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1122r_LNP", std::cref(Cqd1_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1123r_LNP", std::cref(Cqd1_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1133r_LNP", std::cref(Cqd1_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1211r_LNP", std::cref(Cqd1_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1212r_LNP", std::cref(Cqd1_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1213r_LNP", std::cref(Cqd1_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1221r_LNP", std::cref(Cqd1_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1222r_LNP", std::cref(Cqd1_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1223r_LNP", std::cref(Cqd1_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1231r_LNP", std::cref(Cqd1_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1232r_LNP", std::cref(Cqd1_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1233r_LNP", std::cref(Cqd1_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1311r_LNP", std::cref(Cqd1_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1312r_LNP", std::cref(Cqd1_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1313r_LNP", std::cref(Cqd1_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1321r_LNP", std::cref(Cqd1_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1322r_LNP", std::cref(Cqd1_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1323r_LNP", std::cref(Cqd1_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1331r_LNP", std::cref(Cqd1_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1332r_LNP", std::cref(Cqd1_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1333r_LNP", std::cref(Cqd1_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2211r_LNP", std::cref(Cqd1_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2212r_LNP", std::cref(Cqd1_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2213r_LNP", std::cref(Cqd1_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2222r_LNP", std::cref(Cqd1_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2223r_LNP", std::cref(Cqd1_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2233r_LNP", std::cref(Cqd1_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2311r_LNP", std::cref(Cqd1_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2312r_LNP", std::cref(Cqd1_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2313r_LNP", std::cref(Cqd1_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2321r_LNP", std::cref(Cqd1_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2322r_LNP", std::cref(Cqd1_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2323r_LNP", std::cref(Cqd1_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2331r_LNP", std::cref(Cqd1_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2332r_LNP", std::cref(Cqd1_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2333r_LNP", std::cref(Cqd1_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_3311r_LNP", std::cref(Cqd1_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_3312r_LNP", std::cref(Cqd1_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_3313r_LNP", std::cref(Cqd1_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_3322r_LNP", std::cref(Cqd1_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_3323r_LNP", std::cref(Cqd1_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_3333r_LNP", std::cref(Cqd1_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1112i_LNP", std::cref(Cqd1_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1113i_LNP", std::cref(Cqd1_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1123i_LNP", std::cref(Cqd1_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1211i_LNP", std::cref(Cqd1_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1212i_LNP", std::cref(Cqd1_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1213i_LNP", std::cref(Cqd1_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1221i_LNP", std::cref(Cqd1_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1222i_LNP", std::cref(Cqd1_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1223i_LNP", std::cref(Cqd1_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1231i_LNP", std::cref(Cqd1_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1232i_LNP", std::cref(Cqd1_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1233i_LNP", std::cref(Cqd1_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1311i_LNP", std::cref(Cqd1_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1312i_LNP", std::cref(Cqd1_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1313i_LNP", std::cref(Cqd1_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1321i_LNP", std::cref(Cqd1_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1322i_LNP", std::cref(Cqd1_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1323i_LNP", std::cref(Cqd1_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1331i_LNP", std::cref(Cqd1_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1332i_LNP", std::cref(Cqd1_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_1333i_LNP", std::cref(Cqd1_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2212i_LNP", std::cref(Cqd1_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2213i_LNP", std::cref(Cqd1_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2223i_LNP", std::cref(Cqd1_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2312i_LNP", std::cref(Cqd1_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2313i_LNP", std::cref(Cqd1_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2321i_LNP", std::cref(Cqd1_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2322i_LNP", std::cref(Cqd1_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2323i_LNP", std::cref(Cqd1_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2331i_LNP", std::cref(Cqd1_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2332i_LNP", std::cref(Cqd1_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2333i_LNP", std::cref(Cqd1_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_2311i_LNP", std::cref(Cqd1_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_3312i_LNP", std::cref(Cqd1_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_3313i_LNP", std::cref(Cqd1_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd1_3323i_LNP", std::cref(Cqd1_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1111r_LNP", std::cref(Cqd8_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1112r_LNP", std::cref(Cqd8_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1113r_LNP", std::cref(Cqd8_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1122r_LNP", std::cref(Cqd8_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1123r_LNP", std::cref(Cqd8_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1133r_LNP", std::cref(Cqd8_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1211r_LNP", std::cref(Cqd8_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1212r_LNP", std::cref(Cqd8_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1213r_LNP", std::cref(Cqd8_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1221r_LNP", std::cref(Cqd8_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1222r_LNP", std::cref(Cqd8_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1223r_LNP", std::cref(Cqd8_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1231r_LNP", std::cref(Cqd8_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1232r_LNP", std::cref(Cqd8_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1233r_LNP", std::cref(Cqd8_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1311r_LNP", std::cref(Cqd8_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1312r_LNP", std::cref(Cqd8_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1313r_LNP", std::cref(Cqd8_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1321r_LNP", std::cref(Cqd8_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1322r_LNP", std::cref(Cqd8_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1323r_LNP", std::cref(Cqd8_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1331r_LNP", std::cref(Cqd8_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1332r_LNP", std::cref(Cqd8_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1333r_LNP", std::cref(Cqd8_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2211r_LNP", std::cref(Cqd8_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2212r_LNP", std::cref(Cqd8_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2213r_LNP", std::cref(Cqd8_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2222r_LNP", std::cref(Cqd8_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2223r_LNP", std::cref(Cqd8_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2233r_LNP", std::cref(Cqd8_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2311r_LNP", std::cref(Cqd8_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2312r_LNP", std::cref(Cqd8_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2313r_LNP", std::cref(Cqd8_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2321r_LNP", std::cref(Cqd8_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2322r_LNP", std::cref(Cqd8_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2323r_LNP", std::cref(Cqd8_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2331r_LNP", std::cref(Cqd8_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2332r_LNP", std::cref(Cqd8_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2333r_LNP", std::cref(Cqd8_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_3311r_LNP", std::cref(Cqd8_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_3312r_LNP", std::cref(Cqd8_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_3313r_LNP", std::cref(Cqd8_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_3322r_LNP", std::cref(Cqd8_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_3323r_LNP", std::cref(Cqd8_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_3333r_LNP", std::cref(Cqd8_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1112i_LNP", std::cref(Cqd8_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1113i_LNP", std::cref(Cqd8_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1123i_LNP", std::cref(Cqd8_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1211i_LNP", std::cref(Cqd8_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1212i_LNP", std::cref(Cqd8_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1213i_LNP", std::cref(Cqd8_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1221i_LNP", std::cref(Cqd8_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1222i_LNP", std::cref(Cqd8_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1223i_LNP", std::cref(Cqd8_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1231i_LNP", std::cref(Cqd8_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1232i_LNP", std::cref(Cqd8_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1233i_LNP", std::cref(Cqd8_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1311i_LNP", std::cref(Cqd8_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1312i_LNP", std::cref(Cqd8_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1313i_LNP", std::cref(Cqd8_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1321i_LNP", std::cref(Cqd8_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1322i_LNP", std::cref(Cqd8_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1323i_LNP", std::cref(Cqd8_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1331i_LNP", std::cref(Cqd8_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1332i_LNP", std::cref(Cqd8_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_1333i_LNP", std::cref(Cqd8_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2212i_LNP", std::cref(Cqd8_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2213i_LNP", std::cref(Cqd8_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2223i_LNP", std::cref(Cqd8_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2312i_LNP", std::cref(Cqd8_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2313i_LNP", std::cref(Cqd8_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2321i_LNP", std::cref(Cqd8_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2322i_LNP", std::cref(Cqd8_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2323i_LNP", std::cref(Cqd8_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2331i_LNP", std::cref(Cqd8_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2332i_LNP", std::cref(Cqd8_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2333i_LNP", std::cref(Cqd8_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_2311i_LNP", std::cref(Cqd8_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_3312i_LNP", std::cref(Cqd8_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_3313i_LNP", std::cref(Cqd8_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqd8_3323i_LNP", std::cref(Cqd8_3323i_LNP)));
        // Map for the Lepton-Quark four-fermion operators: LL, RR, LLRR 
        ModelParamMap.insert(std::make_pair("Clq1_1111r_LNP", std::cref(Clq1_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1112r_LNP", std::cref(Clq1_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1113r_LNP", std::cref(Clq1_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1122r_LNP", std::cref(Clq1_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1123r_LNP", std::cref(Clq1_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1133r_LNP", std::cref(Clq1_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1211r_LNP", std::cref(Clq1_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1212r_LNP", std::cref(Clq1_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1213r_LNP", std::cref(Clq1_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1221r_LNP", std::cref(Clq1_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1222r_LNP", std::cref(Clq1_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1223r_LNP", std::cref(Clq1_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1231r_LNP", std::cref(Clq1_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1232r_LNP", std::cref(Clq1_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1233r_LNP", std::cref(Clq1_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1311r_LNP", std::cref(Clq1_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1312r_LNP", std::cref(Clq1_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1313r_LNP", std::cref(Clq1_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1321r_LNP", std::cref(Clq1_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1322r_LNP", std::cref(Clq1_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1323r_LNP", std::cref(Clq1_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1331r_LNP", std::cref(Clq1_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1332r_LNP", std::cref(Clq1_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1333r_LNP", std::cref(Clq1_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2211r_LNP", std::cref(Clq1_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2212r_LNP", std::cref(Clq1_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2213r_LNP", std::cref(Clq1_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2222r_LNP", std::cref(Clq1_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2223r_LNP", std::cref(Clq1_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2233r_LNP", std::cref(Clq1_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2311r_LNP", std::cref(Clq1_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2312r_LNP", std::cref(Clq1_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2313r_LNP", std::cref(Clq1_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2321r_LNP", std::cref(Clq1_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2322r_LNP", std::cref(Clq1_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2323r_LNP", std::cref(Clq1_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2331r_LNP", std::cref(Clq1_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2332r_LNP", std::cref(Clq1_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2333r_LNP", std::cref(Clq1_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_3311r_LNP", std::cref(Clq1_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_3312r_LNP", std::cref(Clq1_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_3313r_LNP", std::cref(Clq1_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_3322r_LNP", std::cref(Clq1_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_3323r_LNP", std::cref(Clq1_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_3333r_LNP", std::cref(Clq1_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1112i_LNP", std::cref(Clq1_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1113i_LNP", std::cref(Clq1_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1123i_LNP", std::cref(Clq1_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1211i_LNP", std::cref(Clq1_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1212i_LNP", std::cref(Clq1_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1213i_LNP", std::cref(Clq1_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1221i_LNP", std::cref(Clq1_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1222i_LNP", std::cref(Clq1_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1223i_LNP", std::cref(Clq1_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1231i_LNP", std::cref(Clq1_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1232i_LNP", std::cref(Clq1_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1233i_LNP", std::cref(Clq1_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1311i_LNP", std::cref(Clq1_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1312i_LNP", std::cref(Clq1_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1313i_LNP", std::cref(Clq1_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1321i_LNP", std::cref(Clq1_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1322i_LNP", std::cref(Clq1_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1323i_LNP", std::cref(Clq1_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1331i_LNP", std::cref(Clq1_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1332i_LNP", std::cref(Clq1_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_1333i_LNP", std::cref(Clq1_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2212i_LNP", std::cref(Clq1_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2213i_LNP", std::cref(Clq1_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2223i_LNP", std::cref(Clq1_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2312i_LNP", std::cref(Clq1_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2313i_LNP", std::cref(Clq1_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2321i_LNP", std::cref(Clq1_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2322i_LNP", std::cref(Clq1_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2323i_LNP", std::cref(Clq1_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2331i_LNP", std::cref(Clq1_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2332i_LNP", std::cref(Clq1_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2333i_LNP", std::cref(Clq1_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_2311i_LNP", std::cref(Clq1_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_3312i_LNP", std::cref(Clq1_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_3313i_LNP", std::cref(Clq1_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq1_3323i_LNP", std::cref(Clq1_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1111r_LNP", std::cref(Clq3_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1112r_LNP", std::cref(Clq3_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1113r_LNP", std::cref(Clq3_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1122r_LNP", std::cref(Clq3_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1123r_LNP", std::cref(Clq3_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1133r_LNP", std::cref(Clq3_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1211r_LNP", std::cref(Clq3_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1212r_LNP", std::cref(Clq3_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1213r_LNP", std::cref(Clq3_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1221r_LNP", std::cref(Clq3_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1222r_LNP", std::cref(Clq3_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1223r_LNP", std::cref(Clq3_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1231r_LNP", std::cref(Clq3_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1232r_LNP", std::cref(Clq3_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1233r_LNP", std::cref(Clq3_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1311r_LNP", std::cref(Clq3_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1312r_LNP", std::cref(Clq3_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1313r_LNP", std::cref(Clq3_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1321r_LNP", std::cref(Clq3_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1322r_LNP", std::cref(Clq3_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1323r_LNP", std::cref(Clq3_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1331r_LNP", std::cref(Clq3_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1332r_LNP", std::cref(Clq3_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1333r_LNP", std::cref(Clq3_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2211r_LNP", std::cref(Clq3_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2212r_LNP", std::cref(Clq3_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2213r_LNP", std::cref(Clq3_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2222r_LNP", std::cref(Clq3_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2223r_LNP", std::cref(Clq3_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2233r_LNP", std::cref(Clq3_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2311r_LNP", std::cref(Clq3_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2312r_LNP", std::cref(Clq3_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2313r_LNP", std::cref(Clq3_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2321r_LNP", std::cref(Clq3_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2322r_LNP", std::cref(Clq3_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2323r_LNP", std::cref(Clq3_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2331r_LNP", std::cref(Clq3_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2332r_LNP", std::cref(Clq3_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2333r_LNP", std::cref(Clq3_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_3311r_LNP", std::cref(Clq3_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_3312r_LNP", std::cref(Clq3_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_3313r_LNP", std::cref(Clq3_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_3322r_LNP", std::cref(Clq3_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_3323r_LNP", std::cref(Clq3_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_3333r_LNP", std::cref(Clq3_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1112i_LNP", std::cref(Clq3_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1113i_LNP", std::cref(Clq3_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1123i_LNP", std::cref(Clq3_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1211i_LNP", std::cref(Clq3_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1212i_LNP", std::cref(Clq3_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1213i_LNP", std::cref(Clq3_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1221i_LNP", std::cref(Clq3_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1222i_LNP", std::cref(Clq3_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1223i_LNP", std::cref(Clq3_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1231i_LNP", std::cref(Clq3_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1232i_LNP", std::cref(Clq3_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1233i_LNP", std::cref(Clq3_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1311i_LNP", std::cref(Clq3_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1312i_LNP", std::cref(Clq3_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1313i_LNP", std::cref(Clq3_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1321i_LNP", std::cref(Clq3_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1322i_LNP", std::cref(Clq3_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1323i_LNP", std::cref(Clq3_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1331i_LNP", std::cref(Clq3_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1332i_LNP", std::cref(Clq3_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_1333i_LNP", std::cref(Clq3_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2212i_LNP", std::cref(Clq3_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2213i_LNP", std::cref(Clq3_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2223i_LNP", std::cref(Clq3_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2312i_LNP", std::cref(Clq3_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2313i_LNP", std::cref(Clq3_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2321i_LNP", std::cref(Clq3_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2322i_LNP", std::cref(Clq3_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2323i_LNP", std::cref(Clq3_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2331i_LNP", std::cref(Clq3_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2332i_LNP", std::cref(Clq3_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2333i_LNP", std::cref(Clq3_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_2311i_LNP", std::cref(Clq3_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_3312i_LNP", std::cref(Clq3_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_3313i_LNP", std::cref(Clq3_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clq3_3323i_LNP", std::cref(Clq3_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1111r_LNP", std::cref(Ceu_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1112r_LNP", std::cref(Ceu_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1113r_LNP", std::cref(Ceu_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1122r_LNP", std::cref(Ceu_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1123r_LNP", std::cref(Ceu_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1133r_LNP", std::cref(Ceu_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1211r_LNP", std::cref(Ceu_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1212r_LNP", std::cref(Ceu_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1213r_LNP", std::cref(Ceu_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1221r_LNP", std::cref(Ceu_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1222r_LNP", std::cref(Ceu_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1223r_LNP", std::cref(Ceu_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1231r_LNP", std::cref(Ceu_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1232r_LNP", std::cref(Ceu_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1233r_LNP", std::cref(Ceu_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1311r_LNP", std::cref(Ceu_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1312r_LNP", std::cref(Ceu_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1313r_LNP", std::cref(Ceu_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1321r_LNP", std::cref(Ceu_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1322r_LNP", std::cref(Ceu_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1323r_LNP", std::cref(Ceu_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1331r_LNP", std::cref(Ceu_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1332r_LNP", std::cref(Ceu_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1333r_LNP", std::cref(Ceu_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2211r_LNP", std::cref(Ceu_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2212r_LNP", std::cref(Ceu_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2213r_LNP", std::cref(Ceu_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2222r_LNP", std::cref(Ceu_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2223r_LNP", std::cref(Ceu_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2233r_LNP", std::cref(Ceu_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2311r_LNP", std::cref(Ceu_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2312r_LNP", std::cref(Ceu_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2313r_LNP", std::cref(Ceu_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2321r_LNP", std::cref(Ceu_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2322r_LNP", std::cref(Ceu_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2323r_LNP", std::cref(Ceu_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2331r_LNP", std::cref(Ceu_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2332r_LNP", std::cref(Ceu_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2333r_LNP", std::cref(Ceu_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_3311r_LNP", std::cref(Ceu_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_3312r_LNP", std::cref(Ceu_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_3313r_LNP", std::cref(Ceu_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_3322r_LNP", std::cref(Ceu_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_3323r_LNP", std::cref(Ceu_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_3333r_LNP", std::cref(Ceu_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1112i_LNP", std::cref(Ceu_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1113i_LNP", std::cref(Ceu_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1123i_LNP", std::cref(Ceu_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1211i_LNP", std::cref(Ceu_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1212i_LNP", std::cref(Ceu_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1213i_LNP", std::cref(Ceu_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1221i_LNP", std::cref(Ceu_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1222i_LNP", std::cref(Ceu_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1223i_LNP", std::cref(Ceu_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1231i_LNP", std::cref(Ceu_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1232i_LNP", std::cref(Ceu_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1233i_LNP", std::cref(Ceu_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1311i_LNP", std::cref(Ceu_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1312i_LNP", std::cref(Ceu_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1313i_LNP", std::cref(Ceu_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1321i_LNP", std::cref(Ceu_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1322i_LNP", std::cref(Ceu_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1323i_LNP", std::cref(Ceu_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1331i_LNP", std::cref(Ceu_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1332i_LNP", std::cref(Ceu_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_1333i_LNP", std::cref(Ceu_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2212i_LNP", std::cref(Ceu_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2213i_LNP", std::cref(Ceu_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2223i_LNP", std::cref(Ceu_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2312i_LNP", std::cref(Ceu_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2313i_LNP", std::cref(Ceu_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2321i_LNP", std::cref(Ceu_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2322i_LNP", std::cref(Ceu_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2323i_LNP", std::cref(Ceu_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2331i_LNP", std::cref(Ceu_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2332i_LNP", std::cref(Ceu_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2333i_LNP", std::cref(Ceu_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_2311i_LNP", std::cref(Ceu_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_3312i_LNP", std::cref(Ceu_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_3313i_LNP", std::cref(Ceu_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Ceu_3323i_LNP", std::cref(Ceu_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1111r_LNP", std::cref(Ced_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1112r_LNP", std::cref(Ced_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1113r_LNP", std::cref(Ced_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1122r_LNP", std::cref(Ced_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1123r_LNP", std::cref(Ced_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1133r_LNP", std::cref(Ced_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1211r_LNP", std::cref(Ced_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1212r_LNP", std::cref(Ced_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1213r_LNP", std::cref(Ced_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1221r_LNP", std::cref(Ced_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1222r_LNP", std::cref(Ced_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1223r_LNP", std::cref(Ced_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1231r_LNP", std::cref(Ced_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1232r_LNP", std::cref(Ced_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1233r_LNP", std::cref(Ced_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1311r_LNP", std::cref(Ced_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1312r_LNP", std::cref(Ced_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1313r_LNP", std::cref(Ced_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1321r_LNP", std::cref(Ced_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1322r_LNP", std::cref(Ced_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1323r_LNP", std::cref(Ced_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1331r_LNP", std::cref(Ced_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1332r_LNP", std::cref(Ced_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1333r_LNP", std::cref(Ced_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2211r_LNP", std::cref(Ced_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2212r_LNP", std::cref(Ced_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2213r_LNP", std::cref(Ced_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2222r_LNP", std::cref(Ced_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2223r_LNP", std::cref(Ced_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2233r_LNP", std::cref(Ced_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2311r_LNP", std::cref(Ced_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2312r_LNP", std::cref(Ced_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2313r_LNP", std::cref(Ced_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2321r_LNP", std::cref(Ced_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2322r_LNP", std::cref(Ced_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2323r_LNP", std::cref(Ced_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2331r_LNP", std::cref(Ced_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2332r_LNP", std::cref(Ced_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2333r_LNP", std::cref(Ced_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_3311r_LNP", std::cref(Ced_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_3312r_LNP", std::cref(Ced_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_3313r_LNP", std::cref(Ced_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_3322r_LNP", std::cref(Ced_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_3323r_LNP", std::cref(Ced_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_3333r_LNP", std::cref(Ced_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1112i_LNP", std::cref(Ced_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1113i_LNP", std::cref(Ced_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1123i_LNP", std::cref(Ced_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1211i_LNP", std::cref(Ced_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1212i_LNP", std::cref(Ced_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1213i_LNP", std::cref(Ced_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1221i_LNP", std::cref(Ced_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1222i_LNP", std::cref(Ced_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1223i_LNP", std::cref(Ced_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1231i_LNP", std::cref(Ced_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1232i_LNP", std::cref(Ced_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1233i_LNP", std::cref(Ced_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1311i_LNP", std::cref(Ced_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1312i_LNP", std::cref(Ced_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1313i_LNP", std::cref(Ced_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1321i_LNP", std::cref(Ced_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1322i_LNP", std::cref(Ced_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1323i_LNP", std::cref(Ced_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1331i_LNP", std::cref(Ced_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1332i_LNP", std::cref(Ced_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_1333i_LNP", std::cref(Ced_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2212i_LNP", std::cref(Ced_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2213i_LNP", std::cref(Ced_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2223i_LNP", std::cref(Ced_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2312i_LNP", std::cref(Ced_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2313i_LNP", std::cref(Ced_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2321i_LNP", std::cref(Ced_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2322i_LNP", std::cref(Ced_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2323i_LNP", std::cref(Ced_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2331i_LNP", std::cref(Ced_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2332i_LNP", std::cref(Ced_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2333i_LNP", std::cref(Ced_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_2311i_LNP", std::cref(Ced_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_3312i_LNP", std::cref(Ced_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_3313i_LNP", std::cref(Ced_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Ced_3323i_LNP", std::cref(Ced_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1111r_LNP", std::cref(Clu_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1112r_LNP", std::cref(Clu_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1113r_LNP", std::cref(Clu_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1122r_LNP", std::cref(Clu_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1123r_LNP", std::cref(Clu_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1133r_LNP", std::cref(Clu_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1211r_LNP", std::cref(Clu_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1212r_LNP", std::cref(Clu_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1213r_LNP", std::cref(Clu_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1221r_LNP", std::cref(Clu_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1222r_LNP", std::cref(Clu_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1223r_LNP", std::cref(Clu_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1231r_LNP", std::cref(Clu_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1232r_LNP", std::cref(Clu_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1233r_LNP", std::cref(Clu_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1311r_LNP", std::cref(Clu_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1312r_LNP", std::cref(Clu_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1313r_LNP", std::cref(Clu_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1321r_LNP", std::cref(Clu_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1322r_LNP", std::cref(Clu_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1323r_LNP", std::cref(Clu_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1331r_LNP", std::cref(Clu_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1332r_LNP", std::cref(Clu_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1333r_LNP", std::cref(Clu_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2211r_LNP", std::cref(Clu_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2212r_LNP", std::cref(Clu_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2213r_LNP", std::cref(Clu_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2222r_LNP", std::cref(Clu_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2223r_LNP", std::cref(Clu_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2233r_LNP", std::cref(Clu_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2311r_LNP", std::cref(Clu_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2312r_LNP", std::cref(Clu_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2313r_LNP", std::cref(Clu_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2321r_LNP", std::cref(Clu_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2322r_LNP", std::cref(Clu_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2323r_LNP", std::cref(Clu_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2331r_LNP", std::cref(Clu_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2332r_LNP", std::cref(Clu_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2333r_LNP", std::cref(Clu_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_3311r_LNP", std::cref(Clu_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_3312r_LNP", std::cref(Clu_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_3313r_LNP", std::cref(Clu_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_3322r_LNP", std::cref(Clu_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_3323r_LNP", std::cref(Clu_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_3333r_LNP", std::cref(Clu_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1112i_LNP", std::cref(Clu_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1113i_LNP", std::cref(Clu_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1123i_LNP", std::cref(Clu_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1211i_LNP", std::cref(Clu_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1212i_LNP", std::cref(Clu_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1213i_LNP", std::cref(Clu_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1221i_LNP", std::cref(Clu_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1222i_LNP", std::cref(Clu_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1223i_LNP", std::cref(Clu_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1231i_LNP", std::cref(Clu_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1232i_LNP", std::cref(Clu_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1233i_LNP", std::cref(Clu_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1311i_LNP", std::cref(Clu_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1312i_LNP", std::cref(Clu_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1313i_LNP", std::cref(Clu_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1321i_LNP", std::cref(Clu_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1322i_LNP", std::cref(Clu_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1323i_LNP", std::cref(Clu_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1331i_LNP", std::cref(Clu_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1332i_LNP", std::cref(Clu_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_1333i_LNP", std::cref(Clu_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2212i_LNP", std::cref(Clu_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2213i_LNP", std::cref(Clu_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2223i_LNP", std::cref(Clu_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2312i_LNP", std::cref(Clu_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2313i_LNP", std::cref(Clu_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2321i_LNP", std::cref(Clu_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2322i_LNP", std::cref(Clu_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2323i_LNP", std::cref(Clu_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2331i_LNP", std::cref(Clu_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2332i_LNP", std::cref(Clu_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2333i_LNP", std::cref(Clu_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_2311i_LNP", std::cref(Clu_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_3312i_LNP", std::cref(Clu_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_3313i_LNP", std::cref(Clu_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clu_3323i_LNP", std::cref(Clu_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1111r_LNP", std::cref(Cld_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1112r_LNP", std::cref(Cld_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1113r_LNP", std::cref(Cld_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1122r_LNP", std::cref(Cld_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1123r_LNP", std::cref(Cld_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1133r_LNP", std::cref(Cld_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1211r_LNP", std::cref(Cld_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1212r_LNP", std::cref(Cld_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1213r_LNP", std::cref(Cld_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1221r_LNP", std::cref(Cld_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1222r_LNP", std::cref(Cld_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1223r_LNP", std::cref(Cld_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1231r_LNP", std::cref(Cld_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1232r_LNP", std::cref(Cld_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1233r_LNP", std::cref(Cld_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1311r_LNP", std::cref(Cld_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1312r_LNP", std::cref(Cld_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1313r_LNP", std::cref(Cld_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1321r_LNP", std::cref(Cld_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1322r_LNP", std::cref(Cld_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1323r_LNP", std::cref(Cld_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1331r_LNP", std::cref(Cld_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1332r_LNP", std::cref(Cld_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1333r_LNP", std::cref(Cld_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2211r_LNP", std::cref(Cld_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2212r_LNP", std::cref(Cld_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2213r_LNP", std::cref(Cld_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2222r_LNP", std::cref(Cld_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2223r_LNP", std::cref(Cld_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2233r_LNP", std::cref(Cld_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2311r_LNP", std::cref(Cld_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2312r_LNP", std::cref(Cld_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2313r_LNP", std::cref(Cld_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2321r_LNP", std::cref(Cld_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2322r_LNP", std::cref(Cld_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2323r_LNP", std::cref(Cld_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2331r_LNP", std::cref(Cld_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2332r_LNP", std::cref(Cld_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2333r_LNP", std::cref(Cld_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_3311r_LNP", std::cref(Cld_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_3312r_LNP", std::cref(Cld_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_3313r_LNP", std::cref(Cld_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_3322r_LNP", std::cref(Cld_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_3323r_LNP", std::cref(Cld_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_3333r_LNP", std::cref(Cld_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1112i_LNP", std::cref(Cld_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1113i_LNP", std::cref(Cld_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1123i_LNP", std::cref(Cld_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1211i_LNP", std::cref(Cld_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1212i_LNP", std::cref(Cld_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1213i_LNP", std::cref(Cld_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1221i_LNP", std::cref(Cld_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1222i_LNP", std::cref(Cld_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1223i_LNP", std::cref(Cld_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1231i_LNP", std::cref(Cld_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1232i_LNP", std::cref(Cld_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1233i_LNP", std::cref(Cld_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1311i_LNP", std::cref(Cld_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1312i_LNP", std::cref(Cld_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1313i_LNP", std::cref(Cld_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1321i_LNP", std::cref(Cld_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1322i_LNP", std::cref(Cld_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1323i_LNP", std::cref(Cld_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1331i_LNP", std::cref(Cld_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1332i_LNP", std::cref(Cld_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_1333i_LNP", std::cref(Cld_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2212i_LNP", std::cref(Cld_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2213i_LNP", std::cref(Cld_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2223i_LNP", std::cref(Cld_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2312i_LNP", std::cref(Cld_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2313i_LNP", std::cref(Cld_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2321i_LNP", std::cref(Cld_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2322i_LNP", std::cref(Cld_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2323i_LNP", std::cref(Cld_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2331i_LNP", std::cref(Cld_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2332i_LNP", std::cref(Cld_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2333i_LNP", std::cref(Cld_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_2311i_LNP", std::cref(Cld_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_3312i_LNP", std::cref(Cld_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_3313i_LNP", std::cref(Cld_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cld_3323i_LNP", std::cref(Cld_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1111r_LNP", std::cref(Cqe_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1112r_LNP", std::cref(Cqe_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1113r_LNP", std::cref(Cqe_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1122r_LNP", std::cref(Cqe_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1123r_LNP", std::cref(Cqe_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1133r_LNP", std::cref(Cqe_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1211r_LNP", std::cref(Cqe_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1212r_LNP", std::cref(Cqe_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1213r_LNP", std::cref(Cqe_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1221r_LNP", std::cref(Cqe_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1222r_LNP", std::cref(Cqe_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1223r_LNP", std::cref(Cqe_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1231r_LNP", std::cref(Cqe_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1232r_LNP", std::cref(Cqe_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1233r_LNP", std::cref(Cqe_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1311r_LNP", std::cref(Cqe_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1312r_LNP", std::cref(Cqe_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1313r_LNP", std::cref(Cqe_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1321r_LNP", std::cref(Cqe_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1322r_LNP", std::cref(Cqe_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1323r_LNP", std::cref(Cqe_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1331r_LNP", std::cref(Cqe_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1332r_LNP", std::cref(Cqe_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1333r_LNP", std::cref(Cqe_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2211r_LNP", std::cref(Cqe_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2212r_LNP", std::cref(Cqe_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2213r_LNP", std::cref(Cqe_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2222r_LNP", std::cref(Cqe_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2223r_LNP", std::cref(Cqe_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2233r_LNP", std::cref(Cqe_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2311r_LNP", std::cref(Cqe_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2312r_LNP", std::cref(Cqe_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2313r_LNP", std::cref(Cqe_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2321r_LNP", std::cref(Cqe_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2322r_LNP", std::cref(Cqe_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2323r_LNP", std::cref(Cqe_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2331r_LNP", std::cref(Cqe_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2332r_LNP", std::cref(Cqe_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2333r_LNP", std::cref(Cqe_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_3311r_LNP", std::cref(Cqe_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_3312r_LNP", std::cref(Cqe_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_3313r_LNP", std::cref(Cqe_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_3322r_LNP", std::cref(Cqe_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_3323r_LNP", std::cref(Cqe_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_3333r_LNP", std::cref(Cqe_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1112i_LNP", std::cref(Cqe_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1113i_LNP", std::cref(Cqe_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1123i_LNP", std::cref(Cqe_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1211i_LNP", std::cref(Cqe_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1212i_LNP", std::cref(Cqe_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1213i_LNP", std::cref(Cqe_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1221i_LNP", std::cref(Cqe_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1222i_LNP", std::cref(Cqe_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1223i_LNP", std::cref(Cqe_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1231i_LNP", std::cref(Cqe_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1232i_LNP", std::cref(Cqe_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1233i_LNP", std::cref(Cqe_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1311i_LNP", std::cref(Cqe_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1312i_LNP", std::cref(Cqe_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1313i_LNP", std::cref(Cqe_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1321i_LNP", std::cref(Cqe_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1322i_LNP", std::cref(Cqe_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1323i_LNP", std::cref(Cqe_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1331i_LNP", std::cref(Cqe_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1332i_LNP", std::cref(Cqe_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_1333i_LNP", std::cref(Cqe_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2212i_LNP", std::cref(Cqe_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2213i_LNP", std::cref(Cqe_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2223i_LNP", std::cref(Cqe_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2312i_LNP", std::cref(Cqe_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2313i_LNP", std::cref(Cqe_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2321i_LNP", std::cref(Cqe_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2322i_LNP", std::cref(Cqe_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2323i_LNP", std::cref(Cqe_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2331i_LNP", std::cref(Cqe_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2332i_LNP", std::cref(Cqe_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2333i_LNP", std::cref(Cqe_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_2311i_LNP", std::cref(Cqe_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_3312i_LNP", std::cref(Cqe_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_3313i_LNP", std::cref(Cqe_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cqe_3323i_LNP", std::cref(Cqe_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1111r_LNP", std::cref(Cledq_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1112r_LNP", std::cref(Cledq_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1113r_LNP", std::cref(Cledq_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1121r_LNP", std::cref(Cledq_1121r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1122r_LNP", std::cref(Cledq_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1123r_LNP", std::cref(Cledq_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1131r_LNP", std::cref(Cledq_1131r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1132r_LNP", std::cref(Cledq_1132r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1133r_LNP", std::cref(Cledq_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1211r_LNP", std::cref(Cledq_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1212r_LNP", std::cref(Cledq_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1213r_LNP", std::cref(Cledq_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1221r_LNP", std::cref(Cledq_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1222r_LNP", std::cref(Cledq_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1223r_LNP", std::cref(Cledq_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1231r_LNP", std::cref(Cledq_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1232r_LNP", std::cref(Cledq_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1233r_LNP", std::cref(Cledq_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1311r_LNP", std::cref(Cledq_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1312r_LNP", std::cref(Cledq_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1313r_LNP", std::cref(Cledq_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1321r_LNP", std::cref(Cledq_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1322r_LNP", std::cref(Cledq_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1323r_LNP", std::cref(Cledq_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1331r_LNP", std::cref(Cledq_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1332r_LNP", std::cref(Cledq_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1333r_LNP", std::cref(Cledq_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2111r_LNP", std::cref(Cledq_2111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2112r_LNP", std::cref(Cledq_2112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2113r_LNP", std::cref(Cledq_2113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2121r_LNP", std::cref(Cledq_2121r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2122r_LNP", std::cref(Cledq_2122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2123r_LNP", std::cref(Cledq_2123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2131r_LNP", std::cref(Cledq_2131r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2132r_LNP", std::cref(Cledq_2132r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2133r_LNP", std::cref(Cledq_2133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2211r_LNP", std::cref(Cledq_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2212r_LNP", std::cref(Cledq_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2213r_LNP", std::cref(Cledq_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2221r_LNP", std::cref(Cledq_2221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2222r_LNP", std::cref(Cledq_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2223r_LNP", std::cref(Cledq_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2231r_LNP", std::cref(Cledq_2231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2232r_LNP", std::cref(Cledq_2232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2233r_LNP", std::cref(Cledq_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2311r_LNP", std::cref(Cledq_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2312r_LNP", std::cref(Cledq_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2313r_LNP", std::cref(Cledq_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2321r_LNP", std::cref(Cledq_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2322r_LNP", std::cref(Cledq_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2323r_LNP", std::cref(Cledq_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2331r_LNP", std::cref(Cledq_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2332r_LNP", std::cref(Cledq_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2333r_LNP", std::cref(Cledq_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3111r_LNP", std::cref(Cledq_3111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3112r_LNP", std::cref(Cledq_3112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3113r_LNP", std::cref(Cledq_3113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3121r_LNP", std::cref(Cledq_3121r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3122r_LNP", std::cref(Cledq_3122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3123r_LNP", std::cref(Cledq_3123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3131r_LNP", std::cref(Cledq_3131r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3132r_LNP", std::cref(Cledq_3132r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3133r_LNP", std::cref(Cledq_3133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3211r_LNP", std::cref(Cledq_3211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3212r_LNP", std::cref(Cledq_3212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3213r_LNP", std::cref(Cledq_3213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3221r_LNP", std::cref(Cledq_3221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3222r_LNP", std::cref(Cledq_3222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3223r_LNP", std::cref(Cledq_3223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3231r_LNP", std::cref(Cledq_3231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3232r_LNP", std::cref(Cledq_3232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3233r_LNP", std::cref(Cledq_3233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3311r_LNP", std::cref(Cledq_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3312r_LNP", std::cref(Cledq_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3313r_LNP", std::cref(Cledq_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3321r_LNP", std::cref(Cledq_3321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3322r_LNP", std::cref(Cledq_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3323r_LNP", std::cref(Cledq_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3331r_LNP", std::cref(Cledq_3331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3332r_LNP", std::cref(Cledq_3332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3333r_LNP", std::cref(Cledq_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1111i_LNP", std::cref(Cledq_1111i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1112i_LNP", std::cref(Cledq_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1113i_LNP", std::cref(Cledq_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1121i_LNP", std::cref(Cledq_1121i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1122i_LNP", std::cref(Cledq_1122i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1123i_LNP", std::cref(Cledq_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1131i_LNP", std::cref(Cledq_1131i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1132i_LNP", std::cref(Cledq_1132i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1133i_LNP", std::cref(Cledq_1133i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1211i_LNP", std::cref(Cledq_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1212i_LNP", std::cref(Cledq_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1213i_LNP", std::cref(Cledq_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1221i_LNP", std::cref(Cledq_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1222i_LNP", std::cref(Cledq_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1223i_LNP", std::cref(Cledq_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1231i_LNP", std::cref(Cledq_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1232i_LNP", std::cref(Cledq_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1233i_LNP", std::cref(Cledq_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1311i_LNP", std::cref(Cledq_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1312i_LNP", std::cref(Cledq_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1313i_LNP", std::cref(Cledq_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1321i_LNP", std::cref(Cledq_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1322i_LNP", std::cref(Cledq_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1323i_LNP", std::cref(Cledq_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1331i_LNP", std::cref(Cledq_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1332i_LNP", std::cref(Cledq_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_1333i_LNP", std::cref(Cledq_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2111i_LNP", std::cref(Cledq_2111i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2112i_LNP", std::cref(Cledq_2112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2113i_LNP", std::cref(Cledq_2113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2121i_LNP", std::cref(Cledq_2121i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2122i_LNP", std::cref(Cledq_2122i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2123i_LNP", std::cref(Cledq_2123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2131i_LNP", std::cref(Cledq_2131i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2132i_LNP", std::cref(Cledq_2132i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2133i_LNP", std::cref(Cledq_2133i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2211i_LNP", std::cref(Cledq_2211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2212i_LNP", std::cref(Cledq_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2213i_LNP", std::cref(Cledq_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2221i_LNP", std::cref(Cledq_2221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2222i_LNP", std::cref(Cledq_2222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2223i_LNP", std::cref(Cledq_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2231i_LNP", std::cref(Cledq_2231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2232i_LNP", std::cref(Cledq_2232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2233i_LNP", std::cref(Cledq_2233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2311i_LNP", std::cref(Cledq_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2312i_LNP", std::cref(Cledq_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2313i_LNP", std::cref(Cledq_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2321i_LNP", std::cref(Cledq_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2322i_LNP", std::cref(Cledq_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2323i_LNP", std::cref(Cledq_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2331i_LNP", std::cref(Cledq_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2332i_LNP", std::cref(Cledq_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_2333i_LNP", std::cref(Cledq_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3111i_LNP", std::cref(Cledq_3111i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3112i_LNP", std::cref(Cledq_3112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3113i_LNP", std::cref(Cledq_3113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3121i_LNP", std::cref(Cledq_3121i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3122i_LNP", std::cref(Cledq_3122i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3123i_LNP", std::cref(Cledq_3123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3131i_LNP", std::cref(Cledq_3131i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3132i_LNP", std::cref(Cledq_3132i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3133i_LNP", std::cref(Cledq_3133i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3211i_LNP", std::cref(Cledq_3211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3212i_LNP", std::cref(Cledq_3212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3213i_LNP", std::cref(Cledq_3213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3221i_LNP", std::cref(Cledq_3221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3222i_LNP", std::cref(Cledq_3222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3223i_LNP", std::cref(Cledq_3223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3231i_LNP", std::cref(Cledq_3231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3232i_LNP", std::cref(Cledq_3232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3233i_LNP", std::cref(Cledq_3233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3311i_LNP", std::cref(Cledq_3311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3312i_LNP", std::cref(Cledq_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3313i_LNP", std::cref(Cledq_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3321i_LNP", std::cref(Cledq_3321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3322i_LNP", std::cref(Cledq_3322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3323i_LNP", std::cref(Cledq_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3331i_LNP", std::cref(Cledq_3331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3332i_LNP", std::cref(Cledq_3332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cledq_3333i_LNP", std::cref(Cledq_3333i_LNP)));
        // Map for the Four-Quark four-fermion operators: LRLR
        ModelParamMap.insert(std::make_pair("Cquqd1_1111r_LNP", std::cref(Cquqd1_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1112r_LNP", std::cref(Cquqd1_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1113r_LNP", std::cref(Cquqd1_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1121r_LNP", std::cref(Cquqd1_1121r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1122r_LNP", std::cref(Cquqd1_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1123r_LNP", std::cref(Cquqd1_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1131r_LNP", std::cref(Cquqd1_1131r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1132r_LNP", std::cref(Cquqd1_1132r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1133r_LNP", std::cref(Cquqd1_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1211r_LNP", std::cref(Cquqd1_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1212r_LNP", std::cref(Cquqd1_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1213r_LNP", std::cref(Cquqd1_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1221r_LNP", std::cref(Cquqd1_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1222r_LNP", std::cref(Cquqd1_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1223r_LNP", std::cref(Cquqd1_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1231r_LNP", std::cref(Cquqd1_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1232r_LNP", std::cref(Cquqd1_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1233r_LNP", std::cref(Cquqd1_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1311r_LNP", std::cref(Cquqd1_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1312r_LNP", std::cref(Cquqd1_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1313r_LNP", std::cref(Cquqd1_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1321r_LNP", std::cref(Cquqd1_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1322r_LNP", std::cref(Cquqd1_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1323r_LNP", std::cref(Cquqd1_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1331r_LNP", std::cref(Cquqd1_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1332r_LNP", std::cref(Cquqd1_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1333r_LNP", std::cref(Cquqd1_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2111r_LNP", std::cref(Cquqd1_2111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2112r_LNP", std::cref(Cquqd1_2112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2113r_LNP", std::cref(Cquqd1_2113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2121r_LNP", std::cref(Cquqd1_2121r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2122r_LNP", std::cref(Cquqd1_2122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2123r_LNP", std::cref(Cquqd1_2123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2131r_LNP", std::cref(Cquqd1_2131r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2132r_LNP", std::cref(Cquqd1_2132r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2133r_LNP", std::cref(Cquqd1_2133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2211r_LNP", std::cref(Cquqd1_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2212r_LNP", std::cref(Cquqd1_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2213r_LNP", std::cref(Cquqd1_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2221r_LNP", std::cref(Cquqd1_2221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2222r_LNP", std::cref(Cquqd1_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2223r_LNP", std::cref(Cquqd1_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2231r_LNP", std::cref(Cquqd1_2231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2232r_LNP", std::cref(Cquqd1_2232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2233r_LNP", std::cref(Cquqd1_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2311r_LNP", std::cref(Cquqd1_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2312r_LNP", std::cref(Cquqd1_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2313r_LNP", std::cref(Cquqd1_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2321r_LNP", std::cref(Cquqd1_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2322r_LNP", std::cref(Cquqd1_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2323r_LNP", std::cref(Cquqd1_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2331r_LNP", std::cref(Cquqd1_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2332r_LNP", std::cref(Cquqd1_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2333r_LNP", std::cref(Cquqd1_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3111r_LNP", std::cref(Cquqd1_3111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3112r_LNP", std::cref(Cquqd1_3112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3113r_LNP", std::cref(Cquqd1_3113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3121r_LNP", std::cref(Cquqd1_3121r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3122r_LNP", std::cref(Cquqd1_3122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3123r_LNP", std::cref(Cquqd1_3123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3131r_LNP", std::cref(Cquqd1_3131r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3132r_LNP", std::cref(Cquqd1_3132r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3133r_LNP", std::cref(Cquqd1_3133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3211r_LNP", std::cref(Cquqd1_3211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3212r_LNP", std::cref(Cquqd1_3212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3213r_LNP", std::cref(Cquqd1_3213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3221r_LNP", std::cref(Cquqd1_3221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3222r_LNP", std::cref(Cquqd1_3222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3223r_LNP", std::cref(Cquqd1_3223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3231r_LNP", std::cref(Cquqd1_3231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3232r_LNP", std::cref(Cquqd1_3232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3233r_LNP", std::cref(Cquqd1_3233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3311r_LNP", std::cref(Cquqd1_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3312r_LNP", std::cref(Cquqd1_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3313r_LNP", std::cref(Cquqd1_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3321r_LNP", std::cref(Cquqd1_3321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3322r_LNP", std::cref(Cquqd1_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3323r_LNP", std::cref(Cquqd1_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3331r_LNP", std::cref(Cquqd1_3331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3332r_LNP", std::cref(Cquqd1_3332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3333r_LNP", std::cref(Cquqd1_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1111i_LNP", std::cref(Cquqd1_1111i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1112i_LNP", std::cref(Cquqd1_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1113i_LNP", std::cref(Cquqd1_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1121i_LNP", std::cref(Cquqd1_1121i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1122i_LNP", std::cref(Cquqd1_1122i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1123i_LNP", std::cref(Cquqd1_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1131i_LNP", std::cref(Cquqd1_1131i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1132i_LNP", std::cref(Cquqd1_1132i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1133i_LNP", std::cref(Cquqd1_1133i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1211i_LNP", std::cref(Cquqd1_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1212i_LNP", std::cref(Cquqd1_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1213i_LNP", std::cref(Cquqd1_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1221i_LNP", std::cref(Cquqd1_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1222i_LNP", std::cref(Cquqd1_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1223i_LNP", std::cref(Cquqd1_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1231i_LNP", std::cref(Cquqd1_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1232i_LNP", std::cref(Cquqd1_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1233i_LNP", std::cref(Cquqd1_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1311i_LNP", std::cref(Cquqd1_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1312i_LNP", std::cref(Cquqd1_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1313i_LNP", std::cref(Cquqd1_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1321i_LNP", std::cref(Cquqd1_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1322i_LNP", std::cref(Cquqd1_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1323i_LNP", std::cref(Cquqd1_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1331i_LNP", std::cref(Cquqd1_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1332i_LNP", std::cref(Cquqd1_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_1333i_LNP", std::cref(Cquqd1_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2111i_LNP", std::cref(Cquqd1_2111i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2112i_LNP", std::cref(Cquqd1_2112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2113i_LNP", std::cref(Cquqd1_2113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2121i_LNP", std::cref(Cquqd1_2121i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2122i_LNP", std::cref(Cquqd1_2122i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2123i_LNP", std::cref(Cquqd1_2123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2131i_LNP", std::cref(Cquqd1_2131i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2132i_LNP", std::cref(Cquqd1_2132i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2133i_LNP", std::cref(Cquqd1_2133i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2211i_LNP", std::cref(Cquqd1_2211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2212i_LNP", std::cref(Cquqd1_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2213i_LNP", std::cref(Cquqd1_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2221i_LNP", std::cref(Cquqd1_2221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2222i_LNP", std::cref(Cquqd1_2222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2223i_LNP", std::cref(Cquqd1_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2231i_LNP", std::cref(Cquqd1_2231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2232i_LNP", std::cref(Cquqd1_2232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2233i_LNP", std::cref(Cquqd1_2233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2311i_LNP", std::cref(Cquqd1_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2312i_LNP", std::cref(Cquqd1_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2313i_LNP", std::cref(Cquqd1_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2321i_LNP", std::cref(Cquqd1_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2322i_LNP", std::cref(Cquqd1_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2323i_LNP", std::cref(Cquqd1_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2331i_LNP", std::cref(Cquqd1_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2332i_LNP", std::cref(Cquqd1_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_2333i_LNP", std::cref(Cquqd1_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3111i_LNP", std::cref(Cquqd1_3111i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3112i_LNP", std::cref(Cquqd1_3112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3113i_LNP", std::cref(Cquqd1_3113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3121i_LNP", std::cref(Cquqd1_3121i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3122i_LNP", std::cref(Cquqd1_3122i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3123i_LNP", std::cref(Cquqd1_3123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3131i_LNP", std::cref(Cquqd1_3131i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3132i_LNP", std::cref(Cquqd1_3132i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3133i_LNP", std::cref(Cquqd1_3133i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3211i_LNP", std::cref(Cquqd1_3211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3212i_LNP", std::cref(Cquqd1_3212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3213i_LNP", std::cref(Cquqd1_3213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3221i_LNP", std::cref(Cquqd1_3221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3222i_LNP", std::cref(Cquqd1_3222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3223i_LNP", std::cref(Cquqd1_3223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3231i_LNP", std::cref(Cquqd1_3231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3232i_LNP", std::cref(Cquqd1_3232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3233i_LNP", std::cref(Cquqd1_3233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3311i_LNP", std::cref(Cquqd1_3311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3312i_LNP", std::cref(Cquqd1_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3313i_LNP", std::cref(Cquqd1_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3321i_LNP", std::cref(Cquqd1_3321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3322i_LNP", std::cref(Cquqd1_3322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3323i_LNP", std::cref(Cquqd1_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3331i_LNP", std::cref(Cquqd1_3331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3332i_LNP", std::cref(Cquqd1_3332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd1_3333i_LNP", std::cref(Cquqd1_3333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1111r_LNP", std::cref(Cquqd8_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1112r_LNP", std::cref(Cquqd8_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1113r_LNP", std::cref(Cquqd8_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1121r_LNP", std::cref(Cquqd8_1121r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1122r_LNP", std::cref(Cquqd8_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1123r_LNP", std::cref(Cquqd8_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1131r_LNP", std::cref(Cquqd8_1131r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1132r_LNP", std::cref(Cquqd8_1132r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1133r_LNP", std::cref(Cquqd8_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1211r_LNP", std::cref(Cquqd8_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1212r_LNP", std::cref(Cquqd8_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1213r_LNP", std::cref(Cquqd8_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1221r_LNP", std::cref(Cquqd8_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1222r_LNP", std::cref(Cquqd8_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1223r_LNP", std::cref(Cquqd8_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1231r_LNP", std::cref(Cquqd8_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1232r_LNP", std::cref(Cquqd8_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1233r_LNP", std::cref(Cquqd8_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1311r_LNP", std::cref(Cquqd8_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1312r_LNP", std::cref(Cquqd8_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1313r_LNP", std::cref(Cquqd8_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1321r_LNP", std::cref(Cquqd8_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1322r_LNP", std::cref(Cquqd8_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1323r_LNP", std::cref(Cquqd8_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1331r_LNP", std::cref(Cquqd8_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1332r_LNP", std::cref(Cquqd8_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1333r_LNP", std::cref(Cquqd8_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2111r_LNP", std::cref(Cquqd8_2111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2112r_LNP", std::cref(Cquqd8_2112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2113r_LNP", std::cref(Cquqd8_2113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2121r_LNP", std::cref(Cquqd8_2121r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2122r_LNP", std::cref(Cquqd8_2122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2123r_LNP", std::cref(Cquqd8_2123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2131r_LNP", std::cref(Cquqd8_2131r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2132r_LNP", std::cref(Cquqd8_2132r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2133r_LNP", std::cref(Cquqd8_2133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2211r_LNP", std::cref(Cquqd8_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2212r_LNP", std::cref(Cquqd8_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2213r_LNP", std::cref(Cquqd8_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2221r_LNP", std::cref(Cquqd8_2221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2222r_LNP", std::cref(Cquqd8_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2223r_LNP", std::cref(Cquqd8_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2231r_LNP", std::cref(Cquqd8_2231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2232r_LNP", std::cref(Cquqd8_2232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2233r_LNP", std::cref(Cquqd8_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2311r_LNP", std::cref(Cquqd8_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2312r_LNP", std::cref(Cquqd8_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2313r_LNP", std::cref(Cquqd8_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2321r_LNP", std::cref(Cquqd8_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2322r_LNP", std::cref(Cquqd8_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2323r_LNP", std::cref(Cquqd8_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2331r_LNP", std::cref(Cquqd8_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2332r_LNP", std::cref(Cquqd8_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2333r_LNP", std::cref(Cquqd8_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3111r_LNP", std::cref(Cquqd8_3111r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3112r_LNP", std::cref(Cquqd8_3112r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3113r_LNP", std::cref(Cquqd8_3113r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3121r_LNP", std::cref(Cquqd8_3121r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3122r_LNP", std::cref(Cquqd8_3122r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3123r_LNP", std::cref(Cquqd8_3123r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3131r_LNP", std::cref(Cquqd8_3131r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3132r_LNP", std::cref(Cquqd8_3132r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3133r_LNP", std::cref(Cquqd8_3133r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3211r_LNP", std::cref(Cquqd8_3211r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3212r_LNP", std::cref(Cquqd8_3212r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3213r_LNP", std::cref(Cquqd8_3213r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3221r_LNP", std::cref(Cquqd8_3221r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3222r_LNP", std::cref(Cquqd8_3222r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3223r_LNP", std::cref(Cquqd8_3223r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3231r_LNP", std::cref(Cquqd8_3231r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3232r_LNP", std::cref(Cquqd8_3232r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3233r_LNP", std::cref(Cquqd8_3233r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3311r_LNP", std::cref(Cquqd8_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3312r_LNP", std::cref(Cquqd8_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3313r_LNP", std::cref(Cquqd8_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3321r_LNP", std::cref(Cquqd8_3321r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3322r_LNP", std::cref(Cquqd8_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3323r_LNP", std::cref(Cquqd8_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3331r_LNP", std::cref(Cquqd8_3331r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3332r_LNP", std::cref(Cquqd8_3332r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3333r_LNP", std::cref(Cquqd8_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1111i_LNP", std::cref(Cquqd8_1111i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1112i_LNP", std::cref(Cquqd8_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1113i_LNP", std::cref(Cquqd8_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1121i_LNP", std::cref(Cquqd8_1121i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1122i_LNP", std::cref(Cquqd8_1122i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1123i_LNP", std::cref(Cquqd8_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1131i_LNP", std::cref(Cquqd8_1131i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1132i_LNP", std::cref(Cquqd8_1132i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1133i_LNP", std::cref(Cquqd8_1133i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1211i_LNP", std::cref(Cquqd8_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1212i_LNP", std::cref(Cquqd8_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1213i_LNP", std::cref(Cquqd8_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1221i_LNP", std::cref(Cquqd8_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1222i_LNP", std::cref(Cquqd8_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1223i_LNP", std::cref(Cquqd8_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1231i_LNP", std::cref(Cquqd8_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1232i_LNP", std::cref(Cquqd8_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1233i_LNP", std::cref(Cquqd8_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1311i_LNP", std::cref(Cquqd8_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1312i_LNP", std::cref(Cquqd8_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1313i_LNP", std::cref(Cquqd8_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1321i_LNP", std::cref(Cquqd8_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1322i_LNP", std::cref(Cquqd8_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1323i_LNP", std::cref(Cquqd8_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1331i_LNP", std::cref(Cquqd8_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1332i_LNP", std::cref(Cquqd8_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_1333i_LNP", std::cref(Cquqd8_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2111i_LNP", std::cref(Cquqd8_2111i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2112i_LNP", std::cref(Cquqd8_2112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2113i_LNP", std::cref(Cquqd8_2113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2121i_LNP", std::cref(Cquqd8_2121i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2122i_LNP", std::cref(Cquqd8_2122i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2123i_LNP", std::cref(Cquqd8_2123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2131i_LNP", std::cref(Cquqd8_2131i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2132i_LNP", std::cref(Cquqd8_2132i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2133i_LNP", std::cref(Cquqd8_2133i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2211i_LNP", std::cref(Cquqd8_2211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2212i_LNP", std::cref(Cquqd8_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2213i_LNP", std::cref(Cquqd8_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2221i_LNP", std::cref(Cquqd8_2221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2222i_LNP", std::cref(Cquqd8_2222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2223i_LNP", std::cref(Cquqd8_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2231i_LNP", std::cref(Cquqd8_2231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2232i_LNP", std::cref(Cquqd8_2232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2233i_LNP", std::cref(Cquqd8_2233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2311i_LNP", std::cref(Cquqd8_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2312i_LNP", std::cref(Cquqd8_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2313i_LNP", std::cref(Cquqd8_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2321i_LNP", std::cref(Cquqd8_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2322i_LNP", std::cref(Cquqd8_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2323i_LNP", std::cref(Cquqd8_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2331i_LNP", std::cref(Cquqd8_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2332i_LNP", std::cref(Cquqd8_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_2333i_LNP", std::cref(Cquqd8_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3111i_LNP", std::cref(Cquqd8_3111i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3112i_LNP", std::cref(Cquqd8_3112i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3113i_LNP", std::cref(Cquqd8_3113i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3121i_LNP", std::cref(Cquqd8_3121i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3122i_LNP", std::cref(Cquqd8_3122i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3123i_LNP", std::cref(Cquqd8_3123i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3131i_LNP", std::cref(Cquqd8_3131i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3132i_LNP", std::cref(Cquqd8_3132i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3133i_LNP", std::cref(Cquqd8_3133i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3211i_LNP", std::cref(Cquqd8_3211i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3212i_LNP", std::cref(Cquqd8_3212i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3213i_LNP", std::cref(Cquqd8_3213i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3221i_LNP", std::cref(Cquqd8_3221i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3222i_LNP", std::cref(Cquqd8_3222i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3223i_LNP", std::cref(Cquqd8_3223i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3231i_LNP", std::cref(Cquqd8_3231i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3232i_LNP", std::cref(Cquqd8_3232i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3233i_LNP", std::cref(Cquqd8_3233i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3311i_LNP", std::cref(Cquqd8_3311i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3312i_LNP", std::cref(Cquqd8_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3313i_LNP", std::cref(Cquqd8_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3321i_LNP", std::cref(Cquqd8_3321i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3322i_LNP", std::cref(Cquqd8_3322i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3323i_LNP", std::cref(Cquqd8_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3331i_LNP", std::cref(Cquqd8_3331i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3332i_LNP", std::cref(Cquqd8_3332i_LNP)));
        ModelParamMap.insert(std::make_pair("Cquqd8_3333i_LNP", std::cref(Cquqd8_3333i_LNP)));
        // Map for the Lepton-Quark four-fermion operators: LRLR 
        ModelParamMap.insert(std::make_pair("Clequ1_1111r_LNP", std::cref(Clequ1_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1112r_LNP", std::cref(Clequ1_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1113r_LNP", std::cref(Clequ1_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1121r_LNP", std::cref(Clequ1_1121r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1122r_LNP", std::cref(Clequ1_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1123r_LNP", std::cref(Clequ1_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1131r_LNP", std::cref(Clequ1_1131r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1132r_LNP", std::cref(Clequ1_1132r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1133r_LNP", std::cref(Clequ1_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1211r_LNP", std::cref(Clequ1_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1212r_LNP", std::cref(Clequ1_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1213r_LNP", std::cref(Clequ1_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1221r_LNP", std::cref(Clequ1_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1222r_LNP", std::cref(Clequ1_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1223r_LNP", std::cref(Clequ1_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1231r_LNP", std::cref(Clequ1_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1232r_LNP", std::cref(Clequ1_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1233r_LNP", std::cref(Clequ1_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1311r_LNP", std::cref(Clequ1_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1312r_LNP", std::cref(Clequ1_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1313r_LNP", std::cref(Clequ1_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1321r_LNP", std::cref(Clequ1_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1322r_LNP", std::cref(Clequ1_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1323r_LNP", std::cref(Clequ1_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1331r_LNP", std::cref(Clequ1_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1332r_LNP", std::cref(Clequ1_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1333r_LNP", std::cref(Clequ1_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2111r_LNP", std::cref(Clequ1_2111r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2112r_LNP", std::cref(Clequ1_2112r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2113r_LNP", std::cref(Clequ1_2113r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2121r_LNP", std::cref(Clequ1_2121r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2122r_LNP", std::cref(Clequ1_2122r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2123r_LNP", std::cref(Clequ1_2123r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2131r_LNP", std::cref(Clequ1_2131r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2132r_LNP", std::cref(Clequ1_2132r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2133r_LNP", std::cref(Clequ1_2133r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2211r_LNP", std::cref(Clequ1_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2212r_LNP", std::cref(Clequ1_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2213r_LNP", std::cref(Clequ1_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2221r_LNP", std::cref(Clequ1_2221r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2222r_LNP", std::cref(Clequ1_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2223r_LNP", std::cref(Clequ1_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2231r_LNP", std::cref(Clequ1_2231r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2232r_LNP", std::cref(Clequ1_2232r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2233r_LNP", std::cref(Clequ1_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2311r_LNP", std::cref(Clequ1_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2312r_LNP", std::cref(Clequ1_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2313r_LNP", std::cref(Clequ1_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2321r_LNP", std::cref(Clequ1_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2322r_LNP", std::cref(Clequ1_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2323r_LNP", std::cref(Clequ1_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2331r_LNP", std::cref(Clequ1_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2332r_LNP", std::cref(Clequ1_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2333r_LNP", std::cref(Clequ1_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3111r_LNP", std::cref(Clequ1_3111r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3112r_LNP", std::cref(Clequ1_3112r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3113r_LNP", std::cref(Clequ1_3113r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3121r_LNP", std::cref(Clequ1_3121r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3122r_LNP", std::cref(Clequ1_3122r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3123r_LNP", std::cref(Clequ1_3123r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3131r_LNP", std::cref(Clequ1_3131r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3132r_LNP", std::cref(Clequ1_3132r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3133r_LNP", std::cref(Clequ1_3133r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3211r_LNP", std::cref(Clequ1_3211r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3212r_LNP", std::cref(Clequ1_3212r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3213r_LNP", std::cref(Clequ1_3213r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3221r_LNP", std::cref(Clequ1_3221r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3222r_LNP", std::cref(Clequ1_3222r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3223r_LNP", std::cref(Clequ1_3223r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3231r_LNP", std::cref(Clequ1_3231r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3232r_LNP", std::cref(Clequ1_3232r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3233r_LNP", std::cref(Clequ1_3233r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3311r_LNP", std::cref(Clequ1_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3312r_LNP", std::cref(Clequ1_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3313r_LNP", std::cref(Clequ1_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3321r_LNP", std::cref(Clequ1_3321r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3322r_LNP", std::cref(Clequ1_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3323r_LNP", std::cref(Clequ1_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3331r_LNP", std::cref(Clequ1_3331r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3332r_LNP", std::cref(Clequ1_3332r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3333r_LNP", std::cref(Clequ1_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1111i_LNP", std::cref(Clequ1_1111i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1112i_LNP", std::cref(Clequ1_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1113i_LNP", std::cref(Clequ1_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1121i_LNP", std::cref(Clequ1_1121i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1122i_LNP", std::cref(Clequ1_1122i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1123i_LNP", std::cref(Clequ1_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1131i_LNP", std::cref(Clequ1_1131i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1132i_LNP", std::cref(Clequ1_1132i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1133i_LNP", std::cref(Clequ1_1133i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1211i_LNP", std::cref(Clequ1_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1212i_LNP", std::cref(Clequ1_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1213i_LNP", std::cref(Clequ1_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1221i_LNP", std::cref(Clequ1_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1222i_LNP", std::cref(Clequ1_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1223i_LNP", std::cref(Clequ1_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1231i_LNP", std::cref(Clequ1_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1232i_LNP", std::cref(Clequ1_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1233i_LNP", std::cref(Clequ1_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1311i_LNP", std::cref(Clequ1_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1312i_LNP", std::cref(Clequ1_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1313i_LNP", std::cref(Clequ1_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1321i_LNP", std::cref(Clequ1_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1322i_LNP", std::cref(Clequ1_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1323i_LNP", std::cref(Clequ1_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1331i_LNP", std::cref(Clequ1_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1332i_LNP", std::cref(Clequ1_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_1333i_LNP", std::cref(Clequ1_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2111i_LNP", std::cref(Clequ1_2111i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2112i_LNP", std::cref(Clequ1_2112i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2113i_LNP", std::cref(Clequ1_2113i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2121i_LNP", std::cref(Clequ1_2121i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2122i_LNP", std::cref(Clequ1_2122i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2123i_LNP", std::cref(Clequ1_2123i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2131i_LNP", std::cref(Clequ1_2131i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2132i_LNP", std::cref(Clequ1_2132i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2133i_LNP", std::cref(Clequ1_2133i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2211i_LNP", std::cref(Clequ1_2211i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2212i_LNP", std::cref(Clequ1_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2213i_LNP", std::cref(Clequ1_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2221i_LNP", std::cref(Clequ1_2221i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2222i_LNP", std::cref(Clequ1_2222i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2223i_LNP", std::cref(Clequ1_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2231i_LNP", std::cref(Clequ1_2231i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2232i_LNP", std::cref(Clequ1_2232i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2233i_LNP", std::cref(Clequ1_2233i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2311i_LNP", std::cref(Clequ1_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2312i_LNP", std::cref(Clequ1_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2313i_LNP", std::cref(Clequ1_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2321i_LNP", std::cref(Clequ1_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2322i_LNP", std::cref(Clequ1_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2323i_LNP", std::cref(Clequ1_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2331i_LNP", std::cref(Clequ1_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2332i_LNP", std::cref(Clequ1_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_2333i_LNP", std::cref(Clequ1_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3111i_LNP", std::cref(Clequ1_3111i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3112i_LNP", std::cref(Clequ1_3112i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3113i_LNP", std::cref(Clequ1_3113i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3121i_LNP", std::cref(Clequ1_3121i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3122i_LNP", std::cref(Clequ1_3122i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3123i_LNP", std::cref(Clequ1_3123i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3131i_LNP", std::cref(Clequ1_3131i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3132i_LNP", std::cref(Clequ1_3132i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3133i_LNP", std::cref(Clequ1_3133i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3211i_LNP", std::cref(Clequ1_3211i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3212i_LNP", std::cref(Clequ1_3212i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3213i_LNP", std::cref(Clequ1_3213i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3221i_LNP", std::cref(Clequ1_3221i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3222i_LNP", std::cref(Clequ1_3222i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3223i_LNP", std::cref(Clequ1_3223i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3231i_LNP", std::cref(Clequ1_3231i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3232i_LNP", std::cref(Clequ1_3232i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3233i_LNP", std::cref(Clequ1_3233i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3311i_LNP", std::cref(Clequ1_3311i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3312i_LNP", std::cref(Clequ1_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3313i_LNP", std::cref(Clequ1_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3321i_LNP", std::cref(Clequ1_3321i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3322i_LNP", std::cref(Clequ1_3322i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3323i_LNP", std::cref(Clequ1_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3331i_LNP", std::cref(Clequ1_3331i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3332i_LNP", std::cref(Clequ1_3332i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ1_3333i_LNP", std::cref(Clequ1_3333i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1111r_LNP", std::cref(Clequ3_1111r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1112r_LNP", std::cref(Clequ3_1112r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1113r_LNP", std::cref(Clequ3_1113r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1121r_LNP", std::cref(Clequ3_1121r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1122r_LNP", std::cref(Clequ3_1122r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1123r_LNP", std::cref(Clequ3_1123r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1131r_LNP", std::cref(Clequ3_1131r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1132r_LNP", std::cref(Clequ3_1132r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1133r_LNP", std::cref(Clequ3_1133r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1211r_LNP", std::cref(Clequ3_1211r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1212r_LNP", std::cref(Clequ3_1212r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1213r_LNP", std::cref(Clequ3_1213r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1221r_LNP", std::cref(Clequ3_1221r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1222r_LNP", std::cref(Clequ3_1222r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1223r_LNP", std::cref(Clequ3_1223r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1231r_LNP", std::cref(Clequ3_1231r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1232r_LNP", std::cref(Clequ3_1232r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1233r_LNP", std::cref(Clequ3_1233r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1311r_LNP", std::cref(Clequ3_1311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1312r_LNP", std::cref(Clequ3_1312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1313r_LNP", std::cref(Clequ3_1313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1321r_LNP", std::cref(Clequ3_1321r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1322r_LNP", std::cref(Clequ3_1322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1323r_LNP", std::cref(Clequ3_1323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1331r_LNP", std::cref(Clequ3_1331r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1332r_LNP", std::cref(Clequ3_1332r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1333r_LNP", std::cref(Clequ3_1333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2111r_LNP", std::cref(Clequ3_2111r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2112r_LNP", std::cref(Clequ3_2112r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2113r_LNP", std::cref(Clequ3_2113r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2121r_LNP", std::cref(Clequ3_2121r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2122r_LNP", std::cref(Clequ3_2122r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2123r_LNP", std::cref(Clequ3_2123r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2131r_LNP", std::cref(Clequ3_2131r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2132r_LNP", std::cref(Clequ3_2132r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2133r_LNP", std::cref(Clequ3_2133r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2211r_LNP", std::cref(Clequ3_2211r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2212r_LNP", std::cref(Clequ3_2212r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2213r_LNP", std::cref(Clequ3_2213r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2221r_LNP", std::cref(Clequ3_2221r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2222r_LNP", std::cref(Clequ3_2222r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2223r_LNP", std::cref(Clequ3_2223r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2231r_LNP", std::cref(Clequ3_2231r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2232r_LNP", std::cref(Clequ3_2232r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2233r_LNP", std::cref(Clequ3_2233r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2311r_LNP", std::cref(Clequ3_2311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2312r_LNP", std::cref(Clequ3_2312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2313r_LNP", std::cref(Clequ3_2313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2321r_LNP", std::cref(Clequ3_2321r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2322r_LNP", std::cref(Clequ3_2322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2323r_LNP", std::cref(Clequ3_2323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2331r_LNP", std::cref(Clequ3_2331r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2332r_LNP", std::cref(Clequ3_2332r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2333r_LNP", std::cref(Clequ3_2333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3111r_LNP", std::cref(Clequ3_3111r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3112r_LNP", std::cref(Clequ3_3112r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3113r_LNP", std::cref(Clequ3_3113r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3121r_LNP", std::cref(Clequ3_3121r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3122r_LNP", std::cref(Clequ3_3122r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3123r_LNP", std::cref(Clequ3_3123r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3131r_LNP", std::cref(Clequ3_3131r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3132r_LNP", std::cref(Clequ3_3132r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3133r_LNP", std::cref(Clequ3_3133r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3211r_LNP", std::cref(Clequ3_3211r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3212r_LNP", std::cref(Clequ3_3212r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3213r_LNP", std::cref(Clequ3_3213r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3221r_LNP", std::cref(Clequ3_3221r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3222r_LNP", std::cref(Clequ3_3222r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3223r_LNP", std::cref(Clequ3_3223r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3231r_LNP", std::cref(Clequ3_3231r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3232r_LNP", std::cref(Clequ3_3232r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3233r_LNP", std::cref(Clequ3_3233r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3311r_LNP", std::cref(Clequ3_3311r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3312r_LNP", std::cref(Clequ3_3312r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3313r_LNP", std::cref(Clequ3_3313r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3321r_LNP", std::cref(Clequ3_3321r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3322r_LNP", std::cref(Clequ3_3322r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3323r_LNP", std::cref(Clequ3_3323r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3331r_LNP", std::cref(Clequ3_3331r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3332r_LNP", std::cref(Clequ3_3332r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3333r_LNP", std::cref(Clequ3_3333r_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1111i_LNP", std::cref(Clequ3_1111i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1112i_LNP", std::cref(Clequ3_1112i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1113i_LNP", std::cref(Clequ3_1113i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1121i_LNP", std::cref(Clequ3_1121i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1122i_LNP", std::cref(Clequ3_1122i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1123i_LNP", std::cref(Clequ3_1123i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1131i_LNP", std::cref(Clequ3_1131i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1132i_LNP", std::cref(Clequ3_1132i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1133i_LNP", std::cref(Clequ3_1133i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1211i_LNP", std::cref(Clequ3_1211i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1212i_LNP", std::cref(Clequ3_1212i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1213i_LNP", std::cref(Clequ3_1213i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1221i_LNP", std::cref(Clequ3_1221i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1222i_LNP", std::cref(Clequ3_1222i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1223i_LNP", std::cref(Clequ3_1223i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1231i_LNP", std::cref(Clequ3_1231i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1232i_LNP", std::cref(Clequ3_1232i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1233i_LNP", std::cref(Clequ3_1233i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1311i_LNP", std::cref(Clequ3_1311i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1312i_LNP", std::cref(Clequ3_1312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1313i_LNP", std::cref(Clequ3_1313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1321i_LNP", std::cref(Clequ3_1321i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1322i_LNP", std::cref(Clequ3_1322i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1323i_LNP", std::cref(Clequ3_1323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1331i_LNP", std::cref(Clequ3_1331i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1332i_LNP", std::cref(Clequ3_1332i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_1333i_LNP", std::cref(Clequ3_1333i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2111i_LNP", std::cref(Clequ3_2111i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2112i_LNP", std::cref(Clequ3_2112i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2113i_LNP", std::cref(Clequ3_2113i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2121i_LNP", std::cref(Clequ3_2121i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2122i_LNP", std::cref(Clequ3_2122i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2123i_LNP", std::cref(Clequ3_2123i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2131i_LNP", std::cref(Clequ3_2131i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2132i_LNP", std::cref(Clequ3_2132i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2133i_LNP", std::cref(Clequ3_2133i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2211i_LNP", std::cref(Clequ3_2211i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2212i_LNP", std::cref(Clequ3_2212i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2213i_LNP", std::cref(Clequ3_2213i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2221i_LNP", std::cref(Clequ3_2221i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2222i_LNP", std::cref(Clequ3_2222i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2223i_LNP", std::cref(Clequ3_2223i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2231i_LNP", std::cref(Clequ3_2231i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2232i_LNP", std::cref(Clequ3_2232i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2233i_LNP", std::cref(Clequ3_2233i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2311i_LNP", std::cref(Clequ3_2311i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2312i_LNP", std::cref(Clequ3_2312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2313i_LNP", std::cref(Clequ3_2313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2321i_LNP", std::cref(Clequ3_2321i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2322i_LNP", std::cref(Clequ3_2322i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2323i_LNP", std::cref(Clequ3_2323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2331i_LNP", std::cref(Clequ3_2331i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2332i_LNP", std::cref(Clequ3_2332i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_2333i_LNP", std::cref(Clequ3_2333i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3111i_LNP", std::cref(Clequ3_3111i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3112i_LNP", std::cref(Clequ3_3112i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3113i_LNP", std::cref(Clequ3_3113i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3121i_LNP", std::cref(Clequ3_3121i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3122i_LNP", std::cref(Clequ3_3122i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3123i_LNP", std::cref(Clequ3_3123i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3131i_LNP", std::cref(Clequ3_3131i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3132i_LNP", std::cref(Clequ3_3132i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3133i_LNP", std::cref(Clequ3_3133i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3211i_LNP", std::cref(Clequ3_3211i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3212i_LNP", std::cref(Clequ3_3212i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3213i_LNP", std::cref(Clequ3_3213i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3221i_LNP", std::cref(Clequ3_3221i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3222i_LNP", std::cref(Clequ3_3222i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3223i_LNP", std::cref(Clequ3_3223i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3231i_LNP", std::cref(Clequ3_3231i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3232i_LNP", std::cref(Clequ3_3232i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3233i_LNP", std::cref(Clequ3_3233i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3311i_LNP", std::cref(Clequ3_3311i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3312i_LNP", std::cref(Clequ3_3312i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3313i_LNP", std::cref(Clequ3_3313i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3321i_LNP", std::cref(Clequ3_3321i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3322i_LNP", std::cref(Clequ3_3322i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3323i_LNP", std::cref(Clequ3_3323i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3331i_LNP", std::cref(Clequ3_3331i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3332i_LNP", std::cref(Clequ3_3332i_LNP)));
        ModelParamMap.insert(std::make_pair("Clequ3_3333i_LNP", std::cref(Clequ3_3333i_LNP)));
 
    }
 
    ModelParamMap.insert(std::make_pair("Lambda_NP", std::cref(Lambda_NP)));
    ModelParamMap.insert(std::make_pair("BrHinv", std::cref(BrHinv)));
    ModelParamMap.insert(std::make_pair("BrHexo", std::cref(BrHexo)));
    ModelParamMap.insert(std::make_pair("eggFint", std::cref(eggFint)));
    ModelParamMap.insert(std::make_pair("eggFpar", std::cref(eggFpar)));
    ModelParamMap.insert(std::make_pair("ettHint", std::cref(ettHint)));
    ModelParamMap.insert(std::make_pair("ettHpar", std::cref(ettHpar)));
    ModelParamMap.insert(std::make_pair("eVBFint", std::cref(eVBFint)));
    ModelParamMap.insert(std::make_pair("eVBFpar", std::cref(eVBFpar)));
    ModelParamMap.insert(std::make_pair("eWHint", std::cref(eWHint)));
    ModelParamMap.insert(std::make_pair("eWHpar", std::cref(eWHpar)));
    ModelParamMap.insert(std::make_pair("eZHint", std::cref(eZHint)));
    ModelParamMap.insert(std::make_pair("eZHpar", std::cref(eZHpar)));
    ModelParamMap.insert(std::make_pair("eeeWBFint", std::cref(eeeWBFint)));
    ModelParamMap.insert(std::make_pair("eeeWBFpar", std::cref(eeeWBFpar)));
    ModelParamMap.insert(std::make_pair("eeeZHint", std::cref(eeeZHint)));
    ModelParamMap.insert(std::make_pair("eeeZHpar", std::cref(eeeZHpar)));
    ModelParamMap.insert(std::make_pair("eeettHint", std::cref(eeettHint)));
    ModelParamMap.insert(std::make_pair("eeettHpar", std::cref(eeettHpar)));
    ModelParamMap.insert(std::make_pair("eepWBFint", std::cref(eepWBFint)));
    ModelParamMap.insert(std::make_pair("eepWBFpar", std::cref(eepWBFpar)));
    ModelParamMap.insert(std::make_pair("eepZBFint", std::cref(eepZBFint)));
    ModelParamMap.insert(std::make_pair("eepZBFpar", std::cref(eepZBFpar)));
    ModelParamMap.insert(std::make_pair("eHggint", std::cref(eHggint)));
    ModelParamMap.insert(std::make_pair("eHggpar", std::cref(eHggpar)));
    ModelParamMap.insert(std::make_pair("eHWWint", std::cref(eHWWint)));
    ModelParamMap.insert(std::make_pair("eHWWpar", std::cref(eHWWpar)));
    ModelParamMap.insert(std::make_pair("eHZZint", std::cref(eHZZint)));
    ModelParamMap.insert(std::make_pair("eHZZpar", std::cref(eHZZpar)));
    ModelParamMap.insert(std::make_pair("eHZgaint", std::cref(eHZgaint)));
    ModelParamMap.insert(std::make_pair("eHZgapar", std::cref(eHZgapar)));
    ModelParamMap.insert(std::make_pair("eHgagaint", std::cref(eHgagaint)));
    ModelParamMap.insert(std::make_pair("eHgagapar", std::cref(eHgagapar)));
    ModelParamMap.insert(std::make_pair("eHmumuint", std::cref(eHmumuint)));
    ModelParamMap.insert(std::make_pair("eHmumupar", std::cref(eHmumupar)));
    ModelParamMap.insert(std::make_pair("eHtautauint", std::cref(eHtautauint)));
    ModelParamMap.insert(std::make_pair("eHtautaupar", std::cref(eHtautaupar)));
    ModelParamMap.insert(std::make_pair("eHccint", std::cref(eHccint)));
    ModelParamMap.insert(std::make_pair("eHccpar", std::cref(eHccpar)));
    ModelParamMap.insert(std::make_pair("eHbbint", std::cref(eHbbint)));
    ModelParamMap.insert(std::make_pair("eHbbpar", std::cref(eHbbpar)));
    ModelParamMap.insert(std::make_pair("eeeWWint", std::cref(eeeWWint)));
    ModelParamMap.insert(std::make_pair("edeeWWdcint", std::cref(edeeWWdcint)));
    ModelParamMap.insert(std::make_pair("eggFHgaga", std::cref(eggFHgaga)));
    ModelParamMap.insert(std::make_pair("eggFHZga", std::cref(eggFHZga)));
    ModelParamMap.insert(std::make_pair("eggFHZZ", std::cref(eggFHZZ)));
    ModelParamMap.insert(std::make_pair("eggFHWW", std::cref(eggFHWW)));
    ModelParamMap.insert(std::make_pair("eggFHtautau", std::cref(eggFHtautau)));
    ModelParamMap.insert(std::make_pair("eggFHbb", std::cref(eggFHbb)));
    ModelParamMap.insert(std::make_pair("eggFHmumu", std::cref(eggFHmumu)));
    ModelParamMap.insert(std::make_pair("eVBFHgaga", std::cref(eVBFHgaga)));
    ModelParamMap.insert(std::make_pair("eVBFHZga", std::cref(eVBFHZga)));
    ModelParamMap.insert(std::make_pair("eVBFHZZ", std::cref(eVBFHZZ)));
    ModelParamMap.insert(std::make_pair("eVBFHWW", std::cref(eVBFHWW)));
    ModelParamMap.insert(std::make_pair("eVBFHtautau", std::cref(eVBFHtautau)));
    ModelParamMap.insert(std::make_pair("eVBFHbb", std::cref(eVBFHbb)));
    ModelParamMap.insert(std::make_pair("eVBFHmumu", std::cref(eVBFHmumu)));
    ModelParamMap.insert(std::make_pair("eWHgaga", std::cref(eWHgaga)));
    ModelParamMap.insert(std::make_pair("eWHZga", std::cref(eWHZga)));
    ModelParamMap.insert(std::make_pair("eWHZZ", std::cref(eWHZZ)));
    ModelParamMap.insert(std::make_pair("eWHWW", std::cref(eWHWW)));
    ModelParamMap.insert(std::make_pair("eWHtautau", std::cref(eWHtautau)));
    ModelParamMap.insert(std::make_pair("eWHbb", std::cref(eWHbb)));
    ModelParamMap.insert(std::make_pair("eWHmumu", std::cref(eWHmumu)));
    ModelParamMap.insert(std::make_pair("eZHgaga", std::cref(eZHgaga)));
    ModelParamMap.insert(std::make_pair("eZHZga", std::cref(eZHZga)));
    ModelParamMap.insert(std::make_pair("eZHZZ", std::cref(eZHZZ)));
    ModelParamMap.insert(std::make_pair("eZHWW", std::cref(eZHWW)));
    ModelParamMap.insert(std::make_pair("eZHtautau", std::cref(eZHtautau)));
    ModelParamMap.insert(std::make_pair("eZHbb", std::cref(eZHbb)));
    ModelParamMap.insert(std::make_pair("eZHmumu", std::cref(eZHmumu)));
    ModelParamMap.insert(std::make_pair("ettHgaga", std::cref(ettHgaga)));
    ModelParamMap.insert(std::make_pair("ettHZga", std::cref(ettHZga)));
    ModelParamMap.insert(std::make_pair("ettHZZ", std::cref(ettHZZ)));
    ModelParamMap.insert(std::make_pair("ettHWW", std::cref(ettHWW)));
    ModelParamMap.insert(std::make_pair("ettHtautau", std::cref(ettHtautau)));
    ModelParamMap.insert(std::make_pair("ettHbb", std::cref(ettHbb)));
    ModelParamMap.insert(std::make_pair("ettHmumu", std::cref(ettHmumu)));
    ModelParamMap.insert(std::make_pair("eVBFHinv", std::cref(eVBFHinv)));
    ModelParamMap.insert(std::make_pair("eVHinv", std::cref(eVHinv)));
 
    if (FlagMWinput) {
        //  MW scheme
        cAsch = 0.;
        cWsch = 1.;
    } else {
        //  ALpha scheme
        cAsch = 1.;
        cWsch = 0.;
    }
 
    if (!FlagLoopHd6) {
        cLHd6 = 0.0;
    } else {
        cLHd6 = 1.0;
    }
    
    if (!FlagHiggsSM) {
        cHSM = 0.0;
    } else {
        cHSM = 1.0;
    }
    
    if (FlagLoopH3d6Quad || FlagQuadraticTerms) {
        cLH3d62 = 1.0;
    } else {
        cLH3d62 = 0.0;
    }
    
    if (!FlagfiniteNLO) {
        cNLOd6 = 0.0;
    } else {
        cNLOd6 = 1.0;
    }
 
}

Member Function Documentation

◆ A_f()

const double NPSMEFTd6General::A_f ( const Particle f ) const

virtual

The left-right asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $\mathcal{A}_f$.

\[ \mathcal{A}_f = \mathcal{A}_f^{SM} + \Delta \mathcal{A}_f^{(1)} + \Delta \mathcal{A}_f^{(2)} \]

Parameters

[in] f a lepton or quark

Returns: $\mathcal{A}_f$, including SM plus $\mathcal{O}(\Lambda^{-2})$ and $\mathcal{O}(\Lambda^{-4})$ NP contributions

Attention: This function is applicable only to the NP model classes that are inherited from NPbase.

Reimplemented from NPbase.

Definition at line 16494 of file NPSMEFTd6General.cpp.

{    
    return (trueSM.A_f(f) + deltaA_f(f));
}

◆ AFB()

const double NPSMEFTd6General::AFB ( const Particle f ) const

virtual

The forward-backward asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $A^f_{FB}$.

\[ A_{FB,f} = A_{FB,f}^{SM} + \Delta A_{FB,f}^{(1)} + \Delta A_{FB,f}^{(2)} \]

Parameters

[in] f a lepton or quark

Returns: $A^f_{FB}$, including SM plus $\mathcal{O}(\Lambda^{-2})$ and $\mathcal{O}(\Lambda^{-4})$ NP contributions

Reimplemented from NPbase.

Definition at line 16722 of file NPSMEFTd6General.cpp.

{
    return (trueSM.AFB(f) + deltaAFB(f));
}

◆ alphaMz()

const double NPSMEFTd6General::alphaMz ( ) const

virtual

The electromagnetic coupling at the $Z$-mass scale.

Returns: $\alpha(M_Z^2)$

Reimplemented from NPbase.

Definition at line 15557 of file NPSMEFTd6General.cpp.

                                             {
    
    double deltaNLO;
    
    // Finite NLO corrections in W mass scheme
    deltaNLO = cWsch * (-0.000072 * getSMEFTCoeffEW("CW")  -0.000016 * getSMEFTCoeffEW("CHbox")  -0.000478 * getSMEFTCoeffEW("CHD")  -0.000014 * getSMEFTCoeffEW("CHB")   
            -0.000017 * getSMEFTCoeffEW("CHW")  -0.00081 * getSMEFTCoeffEW("CHWB")  -0.000144 * getSMEFTCoeffEW("CuWR",2, 2) -0.000438 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.00003 * getSMEFTCoeffEW("CHl1R",0, 0) -0.00003 * getSMEFTCoeffEW("CHl1R",1, 1) -0.000023 * getSMEFTCoeffEW("CHl1R",2, 2) -0.000672 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.000672 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000014 * getSMEFTCoeffEW("CHl3R",2, 2) -0.000023 * getSMEFTCoeffEW("CHeR",0, 0) -0.000023 * getSMEFTCoeffEW("CHeR",1, 1)  
            -0.000023 * getSMEFTCoeffEW("CHeR",2, 2) +0.000023 * getSMEFTCoeffEW("CHq1R",0, 0) +0.000023 * getSMEFTCoeffEW("CHq1R",1, 1) -0.001004 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.000043 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000043 * getSMEFTCoeffEW("CHq3R",1, 1) +0.000584 * getSMEFTCoeffEW("CHq3R",2, 2) +0.000045 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.000045 * getSMEFTCoeffEW("CHuR",1, 1) +0.001179 * getSMEFTCoeffEW("CHuR",2, 2) -0.000023 * getSMEFTCoeffEW("CHdR",0, 0) -0.000023 * getSMEFTCoeffEW("CHdR",1, 1)  
            -0.000023 * getSMEFTCoeffEW("CHdR",2, 2) -0.000128 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.000495 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) +0.00011 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
            +0.00011 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) ) * v2; 
    
    return (trueSM.alphaMz() * (1.0 + 2.0 * delta_e + delta_A) + cNLOd6 * deltaNLO );
}

◆ aPskPol()

const double NPSMEFTd6General::aPskPol	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

the angular parameter $a$ from $\mu_{e^+e^- \to ZH}$ (arXiv:1708.09079 [hep-ph]).

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $a_{eeZH}$

Reimplemented from NPbase.

Definition at line 24878 of file NPSMEFTd6General.cpp.

                                                                                                          {
 
    // Expression missing Cll contributions!
 
    double aL, aR, aPol;
    double sM = sqrt_s * sqrt_s;
    double Mz2 = Mz*Mz;
    double MH2 = mHl*mHl;
    double dMz = 0.0;
    double dMH = 0.0;
    double dv, dg, dgp, dgL, dgR;
    double kCM, kCM2, EZ, EZ2, kZ, kH;
    double EtaZ;
    double CHpsk, CTpsk, CHl, CHlp, CHE;
    double CWB, CBB, CWW;
 
    // Convention for dim 6 operators
    CWB = g2_tree * g2_tree / (8.0 * g2_tree * g1_tree) * getSMEFTCoeffEW("CHWB") * v2;
    CBB = 0.25 * (g2_tree * g2_tree / g1_tree / g1_tree) * getSMEFTCoeffEW("CHB") * v2;
    CWW = 0.25 * getSMEFTCoeffEW("CHW") * v2;
 
    CHpsk = (-2.0 * getSMEFTCoeffEW("CHbox") + 0.25 * getSMEFTCoeffEW("CHD")) * v2;
    CTpsk = -0.5 * getSMEFTCoeffEW("CHD") * v2;
    CHl = getSMEFTCoeffEW("CHl1R", 0, 0) * v2;
    CHlp = getSMEFTCoeffEW("CHl3R", 0, 0) * v2;
    CHE = getSMEFTCoeffEW("CHeR", 0, 0) * v2;
 
    //  Other parameters (1): Missing Cll!!!
    dv = 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) * v2;
 
    // WFR
    EtaZ = -(1.0 / 2.0) * CHpsk + 2.0 * dMz - dv - CTpsk;
 
    // Kinematics
    kCM = sqrt((sM * sM + (MH2 - Mz2)*(MH2 - Mz2) - 2.0 * sM * (MH2 + Mz2)) / (4.0 * sM));
    kCM2 = kCM*kCM;
 
    EZ = sqrt(Mz2 + kCM2);
    EZ2 = EZ*EZ;
 
    kZ = 2.0 * Mz2 / (sM - Mz2) + (EZ * Mz2) / (2 * kCM2 * sqrt_s) - Mz2 / (2 * kCM2) - (EZ2 / Mz2) / (2.0 + EZ2 / Mz2)*(1.0 - Mz2 / (EZ * sqrt_s));
 
    kH = -((EZ * MH2) / (2 * kCM2 * sqrt_s)) - (EZ2 / Mz2) / (2 + EZ2 / Mz2) * MH2 / (EZ * sqrt_s);
 
    //  Other parameters (2): Missing Cll!!!
    dg = -(1.0 / (g1_tree * (cW2_tree * cW2_tree - sW2_tree * sW2_tree))) * (dv * cW2_tree * g1_tree
            - cW2_tree * dMz * g1_tree + 0.25 * getSMEFTCoeffEW("CHD") * cW2_tree * g1_tree * v2
            + getSMEFTCoeffEW("CHW") * cW2_tree * cW2_tree * g1_tree * v2 + getSMEFTCoeffEW("CHWB") * cW2_tree * g2_tree * sW2_tree * v2
            - getSMEFTCoeffEW("CHW") * g1_tree * sW2_tree * sW2_tree * v2 + getSMEFTCoeffEW("CHWB") * g2_tree * sW2_tree * sW2_tree * v2);
 
 
    dgp = -(1.0 / (cW2_tree * g1_tree * g1_tree * (-cW2_tree * cW2_tree + sW2_tree * sW2_tree))) * (dv * cW2_tree * g1_tree * g1_tree * sW2_tree
            - cW2_tree * dMz * g1_tree * g1_tree * sW2_tree + 0.25 * getSMEFTCoeffEW("CHD") * cW2_tree * g1_tree * g1_tree * sW2_tree * v2
            + getSMEFTCoeffEW("CHWB") * cW2_tree * cW2_tree * g1_tree * g2_tree * sW2_tree * v2
            - getSMEFTCoeffEW("CHB") * cW2_tree * cW2_tree * g2_tree * g2_tree * sW2_tree * v2
            + getSMEFTCoeffEW("CHWB") * cW2_tree * g1_tree * g2_tree * sW2_tree * sW2_tree * v2
            + getSMEFTCoeffEW("CHB") * g2_tree * g2_tree * sW2_tree * sW2_tree * sW2_tree * v2);
 
    dgL = (1.0 / (0.5 - sW2_tree))*(cW2_tree * (0.5 + sW2_tree) * dg
            - sW2_tree * (0.5 + cW2_tree) * dgp
            + 0.5 * (CHl + CHlp)
            + 0.25 * cW2_tree * (1.0 + 2.0 * sW2_tree)*8.0 * CWW
            - 0.5 * sW2_tree * (1.0 - 2.0 * sW2_tree)*8.0 * CWB
            - 0.25 * sW2_tree * sW2_tree / cW2_tree * (1.0 + 2.0 * cW2_tree)*8.0 * CBB);
 
    dgR = -cW2_tree * dg + (1.0 + cW2_tree) * dgp
            - 1.0 / (2.0 * sW2_tree) * CHE - 0.5 * cW2_tree * 8 * CWW
            + cW2_tree * 8.0 * CWB + 0.5 * sW2_tree / cW2_tree * (1.0 + cW2_tree)*8.0 * CBB;
 
 
    //  LH and RH pars            
 
    aL = dgL + 2 * dMz - dv + EtaZ + (sM - Mz2) / (2 * Mz2)*(CHl + CHlp) / (0.5 - sW2_tree) + kZ * dMz + kH*dMH;
    aR = dgR + 2 * dMz - dv + EtaZ - (sM - Mz2) / (2 * Mz2) * CHE / sW2_tree + kZ * dMz + kH*dMH;
 
    //  Polarized a parameter
    aPol = 0.25 * ((1.0 - Pol_em / 100.0)*(1.0 + Pol_ep / 100.0) * aL
            + (1.0 + Pol_em / 100.0)*(1.0 - Pol_ep / 100.0) * aR);
 
    return aPol;
}

◆ bPskPol()

const double NPSMEFTd6General::bPskPol	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

the angular parameter $b$ from $\mu_{e^+e^- \to ZH}$ (arXiv:1708.09079 [hep-ph]).

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $b_{eeZH}$

Reimplemented from NPbase.

Definition at line 24960 of file NPSMEFTd6General.cpp.

                                                                                                          {
    double bL, bR, bPol;
    double sM = sqrt_s * sqrt_s;
    double Mz2 = Mz*Mz;
 
    double ZetaZ, ZetaAZ;
    double CWB, CBB, CWW;
 
    // Convention for dim 6 operators
    CWB = g2_tree * g2_tree / (8.0 * g2_tree * g1_tree) * getSMEFTCoeffEW("CHWB") * v2;
    CBB = 0.25 * (g2_tree * g2_tree / g1_tree / g1_tree) * getSMEFTCoeffEW("CHB") * v2;
    CWW = 0.25 * getSMEFTCoeffEW("CHW") * v2;
 
    ZetaZ = cW2_tree * 8.0 * CWW + 2.0 * sW2_tree * 8 * CWB + (sW2_tree * sW2_tree / cW2_tree)*8.0 * CBB;
    ZetaAZ = sW_tree * cW_tree * (8.0 * CWW - (1.0 - sW2_tree / cW2_tree)*8 * CWB - (sW2_tree / cW2_tree)*8.0 * CBB);
 
    //  LH and RH pars 
    bL = ZetaZ + (sW_tree * cW_tree) / (0.5 - sW2_tree)*(sM - Mz2) / sM*ZetaAZ;
    bR = ZetaZ - (cW_tree / sW_tree)*(sM - Mz2) / sM*ZetaAZ;
 
    //  Polarized b parameter
    bPol = 0.25 * ((1.0 - Pol_em / 100.0)*(1.0 + Pol_ep / 100.0) * bL
            + (1.0 + Pol_em / 100.0)*(1.0 - Pol_ep / 100.0) * bR);
 
    return bPol;
}

◆ Br_H_exo()

const double NPSMEFTd6General::Br_H_exo ( ) const

virtual

The branching ratio of the of the Higgs into exotic particles.

Returns: Br $(H\to exotic)$

Reimplemented from NPbase.

Definition at line 35201 of file NPSMEFTd6General.cpp.

                                              {
    if (BrHexo < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return BrHexo;
}

◆ Br_H_inv()

const double NPSMEFTd6General::Br_H_inv ( ) const

virtual

The branching ratio of the of the Higgs into invisible particles.

Returns: Br $(H\to invisible)$

Reimplemented from NPbase.

Definition at line 35207 of file NPSMEFTd6General.cpp.

                                              {
    //  Contributions from both modifications in H->ZZ->4v and the extra invisible decays
    double BR4v;
 
    BR4v = BrHZZ4vRatio()*(trueSM.computeBrHto4v());
 
    //  BR4v positivity is already checked inside BrHZZ4vRatio()
    //  and will be nan if negative. Check here BrHinv, to make sure both are positive
    if (BrHinv < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return BR4v + BrHinv;
}

◆ Br_H_inv_NP()

const double NPSMEFTd6General::Br_H_inv_NP ( ) const

virtual

The branching ratio of the of the Higgs into invisible particles (only invisible new particles).

Returns: Br $(H\to invisible,NP)$

Reimplemented from NPbase.

Definition at line 35220 of file NPSMEFTd6General.cpp.

                                                 {
 
    //  BR4v positivity is already checked inside BrHZZ4vRatio()
    //  and will be nan if negative. Check here BrHinv, to make sure both are positive
    if (BrHinv < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return BrHinv;
}

◆ BrH2d2dRatio()

const double NPSMEFTd6General::BrH2d2dRatio ( ) const

virtual

The ratio of the Br $(H\to 2d2d)$ in the current model and in the Standard Model.

Returns: Br $(H\to 2d2d)$/Br $(H\to 2d2d)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 30415 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2d2dRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2d2dRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2e2muRatio()

const double NPSMEFTd6General::BrH2e2muRatio ( ) const

virtual

The ratio of the Br $(H\to 2e 2\mu)$ in the current model and in the Standard Model.

Returns: Br $(H\to 2L2L)$/Br $(H\to 2e 2\mu)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 29184 of file NPSMEFTd6General.cpp.

                                                   {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2e2muRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2e2muRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2e2vRatio()

const double NPSMEFTd6General::BrH2e2vRatio ( ) const

virtual

The ratio of the Br $(H\to 2e2v)$ in the current model and in the Standard Model.

Returns: Br $(H\to 2e2v)$/Br $(H\to 2e2v)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 29818 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2e2vRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2e2vRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2evRatio()

const double NPSMEFTd6General::BrH2evRatio ( ) const

virtual

The ratio of the Br $(H\to 2ev)$ in the current model and in the Standard Model.

Returns: Br $(H\to 2ev)$/Br $(H\to 2ev)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 34363 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2evRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2evRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2L2dRatio()

const double NPSMEFTd6General::BrH2L2dRatio ( ) const

virtual

The ratio of the Br $(H\to 2L2d)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: Br $(H\to 2L2d)$/Br $(H\to 2L2d)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 31365 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2L2dRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2L2dRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2L2LRatio()

const double NPSMEFTd6General::BrH2L2LRatio ( ) const

virtual

The ratio of the Br $(H\to 2L2L')$ ( $L,L'=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: Br $(H\to 2L2L')$/Br $(H\to 2L2L')_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 29091 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2L2LRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2L2LRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2L2uRatio()

const double NPSMEFTd6General::BrH2L2uRatio ( ) const

virtual

The ratio of the Br $(H\to 2L2u)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: Br $(H\to 2L2u)$/Br $(H\to 2L2u)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 31021 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2L2uRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2L2uRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2L2v2Ratio()

const double NPSMEFTd6General::BrH2L2v2Ratio ( ) const

virtual

The ratio of the Br $(H\to 2L2v)$ ( $L=e,\mu$) in the current model and in the Standard Model.

Returns: Br $(H\to 2L2v)$/Br $(H\to 2L2v)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 29725 of file NPSMEFTd6General.cpp.

                                                   {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2L2v2Ratio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2L2v2Ratio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2L2vRatio()

const double NPSMEFTd6General::BrH2L2vRatio ( ) const

virtual

The ratio of the Br $(H\to 2L2v)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: Br $(H\to 2L2v)$/Br $(H\to 2L2v)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 29630 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2L2vRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2L2vRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2l2vRatio()

const double NPSMEFTd6General::BrH2l2vRatio ( ) const

virtual

The ratio of the Br $(H\to 2l2v)$ ( $l=e,\mu$) in the current model and in the Standard Model.

Returns: Br $(H\to 2l2v)$/Br $(H\to 2l2v)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 34857 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2l2vRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2l2vRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2Lv2Ratio()

const double NPSMEFTd6General::BrH2Lv2Ratio ( ) const

virtual

The ratio of the Br $(H\to 2Lv)$ ( $L=e,\mu$) in the current model and in the Standard Model.

Returns: Br $(H\to 2Lv)$/Br $(H\to 2Lv)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 34268 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2Lv2Ratio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2Lv2Ratio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2LvRatio()

const double NPSMEFTd6General::BrH2LvRatio ( ) const

virtual

The ratio of the Br $(H\to 2Lv)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: Br $(H\to 2Lv)$/Br $(H\to 2Lv)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 34169 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2LvRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2LvRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2mu2vRatio()

const double NPSMEFTd6General::BrH2mu2vRatio ( ) const

virtual

The ratio of the Br $(H\to 2\mu 2v)$ in the current model and in the Standard Model.

Returns: Br $(H\to 2\mu 2v)$/Br $(H\to 2\mu 2v)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 29910 of file NPSMEFTd6General.cpp.

                                                   {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2mu2vRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2mu2vRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2muvRatio()

const double NPSMEFTd6General::BrH2muvRatio ( ) const

virtual

The ratio of the Br $(H\to 2ev)$ in the current model and in the Standard Model.

Returns: Br $(H\to 2\mu v)$/Br $(H\to 2\mu v)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 34458 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2muvRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2muvRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2u2dRatio()

const double NPSMEFTd6General::BrH2u2dRatio ( ) const

virtual

The ratio of the Br $(H\to 2u2d)$ in the current model and in the Standard Model.

Returns: Br $(H\to 2u2d)$/Br $(H\to 2u2d)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 30710 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2u2dRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2u2dRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2u2uRatio()

const double NPSMEFTd6General::BrH2u2uRatio ( ) const

virtual

The ratio of the Br $(H\to 2u2u)$ in the current model and in the Standard Model.

Returns: Br $(H\to 2u2u)$/Br $(H\to 2u2u)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 30145 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2u2uRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2u2uRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2udRatio()

const double NPSMEFTd6General::BrH2udRatio ( ) const

virtual

The ratio of the Br $(H\to 2ud)$ in the current model and in the Standard Model.

Returns: Br $(H\to 2ud)$/Br $(H\to 2ud)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 33967 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2udRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2udRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2v2dRatio()

const double NPSMEFTd6General::BrH2v2dRatio ( ) const

virtual

The ratio of the Br $(H\to 2v2d)$ in the current model and in the Standard Model.

Returns: Br $(H\to 2v2d)$/Br $(H\to 2v2d)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 31938 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2v2dRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2v2dRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2v2uRatio()

const double NPSMEFTd6General::BrH2v2uRatio ( ) const

virtual

The ratio of the Br $(H\to 2v2u)$ in the current model and in the Standard Model.

Returns: Br $(H\to 2v2u)$/Br $(H\to 2v2u)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 31632 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2v2uRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2v2uRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH2v2vRatio()

const double NPSMEFTd6General::BrH2v2vRatio ( ) const

virtual

The ratio of the Br $(H\to 2v2v)$ in the current model and in the Standard Model.

Returns: Br $(H\to 2v2v)$/Br $(H\to 2v2v)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 29388 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH2v2vRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH2v2vRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH4dRatio()

const double NPSMEFTd6General::BrH4dRatio ( ) const

virtual

The ratio of the Br $(H\to 4d)$ in the current model and in the Standard Model.

Returns: Br $(H\to 4d)$/Br $(H\to 4d)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 33181 of file NPSMEFTd6General.cpp.

                                                {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH4dRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH4dRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH4eRatio()

const double NPSMEFTd6General::BrH4eRatio ( ) const

virtual

The ratio of the Br $(H\to 4e)$ in the current model and in the Standard Model.

Returns: Br $(H\to 4e)$/Br $(H\to 4e)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 32362 of file NPSMEFTd6General.cpp.

                                                {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH4eRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH4eRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH4fCCRatio()

const double NPSMEFTd6General::BrH4fCCRatio ( ) const

virtual

The ratio of the Br $(H\to 4f, CC)$ in the current model and in the Standard Model.

Returns: Br $(H\to 4f, CC)$/Br $(H\to 4f, CC)_{\mathrm{SM}}$

Definition at line 34729 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH4fCCRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH4fCCRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH4fNCRatio()

const double NPSMEFTd6General::BrH4fNCRatio ( ) const

virtual

The ratio of the Br $(H\to 4f, NC)$ in the current model and in the Standard Model.

Returns: Br $(H\to 4f, NC)$/Br $(H\to 4f, NC)_{\mathrm{SM}}$

Definition at line 34654 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH4fNCRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH4fNCRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH4fRatio()

const double NPSMEFTd6General::BrH4fRatio ( ) const

virtual

The ratio of the Br $(H\to 4f)$ in the current model and in the Standard Model.

Returns: Br $(H\to 4f)$/Br $(H\to 4f)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 34565 of file NPSMEFTd6General.cpp.

                                                {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH4fRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH4fRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH4L2Ratio()

const double NPSMEFTd6General::BrH4L2Ratio ( ) const

virtual

The ratio of the Br $(H\to 4L)$ ( $L=e,\mu$) in the current model and in the Standard Model.

Returns: Br $(H\to 4L)$/Br $(H\to 4L)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 32272 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH4L2Ratio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH4L2Ratio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH4LRatio()

const double NPSMEFTd6General::BrH4LRatio ( ) const

virtual

The ratio of the Br $(H\to 4L)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: Br $(H\to 4L)$/Br $(H\to 4L)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 32179 of file NPSMEFTd6General.cpp.

                                                {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH4LRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH4LRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH4lRatio()

const double NPSMEFTd6General::BrH4lRatio ( ) const

virtual

The ratio of the Br $(H\to 4l)$ ( $l=e,\mu$) in the current model and in the Standard Model.

Returns: Br $(H\to 4l)$/Br $(H\to 4l)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 34793 of file NPSMEFTd6General.cpp.

                                                {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH4lRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH4lRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH4muRatio()

const double NPSMEFTd6General::BrH4muRatio ( ) const

virtual

The ratio of the Br $(H\to 4\mu)$ in the current model and in the Standard Model.

Returns: Br $(H\to 4\mu)$/Br $(H\to 4\mu)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 32452 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH4muRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH4muRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH4uRatio()

const double NPSMEFTd6General::BrH4uRatio ( ) const

virtual

The ratio of the Br $(H\to 4u)$ in the current model and in the Standard Model.

Returns: Br $(H\to 4u)$/Br $(H\to 4u)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 32902 of file NPSMEFTd6General.cpp.

                                                {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH4uRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH4uRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrH4vRatio()

const double NPSMEFTd6General::BrH4vRatio ( ) const

virtual

The ratio of the Br $(H\to 4v)$ in the current model and in the Standard Model.

Returns: Br $(H\to 4v)$/Br $(H\to 4v)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 32654 of file NPSMEFTd6General.cpp.

                                                {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaH4vRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaH4vRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHbbRatio()

const double NPSMEFTd6General::BrHbbRatio ( ) const

virtual

The ratio of the Br $(H\to b\bar{b})$ in the current model and in the Standard Model.

Returns: Br $(H\to b\bar{b})$/Br $(H\to b\bar{b})_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28838 of file NPSMEFTd6General.cpp.

                                                {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHbbRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHbbRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHccRatio()

const double NPSMEFTd6General::BrHccRatio ( ) const

virtual

The ratio of the Br $(H\to c\bar{c})$ in the current model and in the Standard Model.

Returns: Br $(H\to c\bar{c})$/Br $(H\to c\bar{c})_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28639 of file NPSMEFTd6General.cpp.

                                                {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHccRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHccRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHevmuvRatio()

const double NPSMEFTd6General::BrHevmuvRatio ( ) const

virtual

The ratio of the Br $(H\to e\nu \mu\nu)$ in the current model and in the Standard Model.

Returns: Br $(H\to e\nu \mu\nu)$/Br $(H\to e\nu \mu\nu)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 33416 of file NPSMEFTd6General.cpp.

                                                   {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHevmuvRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHevmuvRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHgagaRatio()

const double NPSMEFTd6General::BrHgagaRatio ( ) const

virtual

The ratio of the Br $(H\to \gamma\gamma)$ in the current model and in the Standard Model.

Returns: Br $(H\to \gamma\gamma)$/Br $(H\to \gamma\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28337 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHgagaRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHgagaRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHggRatio()

const double NPSMEFTd6General::BrHggRatio ( ) const

virtual

The ratio of the Br $(H\to gg)$ in the current model and in the Standard Model.

Returns: Br $(H\to gg)$/Br $(H\to gg)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 26068 of file NPSMEFTd6General.cpp.

                                                {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHggRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHggRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHll_vvorjjRatio()

const double NPSMEFTd6General::BrHll_vvorjjRatio ( ) const

virtual

The ratio of the Br $(H\to l l \nu\nu, l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model.

Returns: Br $(H\to l l \nu\nu, l l j j)$/Br $(H\to l l \nu\nu, l l j j)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 35174 of file NPSMEFTd6General.cpp.

                                                       {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHll_vvorjjRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHll_vvorjjRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHlv_lvorjjRatio()

const double NPSMEFTd6General::BrHlv_lvorjjRatio ( ) const

virtual

The ratio of the Br $(H\to l \nu l \nu, l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model.

Returns: Br $(H\to l \nu l \nu, l \nu j j)$/Br $(H\to l \nu l \nu, l \nu j j)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 35112 of file NPSMEFTd6General.cpp.

                                                       {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHlv_lvorjjRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHlv_lvorjjRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHlvjjRatio()

const double NPSMEFTd6General::BrHlvjjRatio ( ) const

virtual

The ratio of the Br $(H\to l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model.

Returns: Br $(H\to l \nu j j)$/Br $(H\to l \nu j j)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 35049 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHlvjjRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHlvjjRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHLvudRatio()

const double NPSMEFTd6General::BrHLvudRatio ( ) const

virtual

The ratio of the Br $(H\to Lvud)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: Br $(H\to Lvud)$/Br $(H\to Lvud)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 33738 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHLvudRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHLvudRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHLvvLRatio()

const double NPSMEFTd6General::BrHLvvLRatio ( ) const

virtual

The ratio of the Br $(H\to LvvL)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: Br $(H\to LvvL)$/Br $(H\to LvvL)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 33325 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHLvvLRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHLvvLRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHmumuRatio()

const double NPSMEFTd6General::BrHmumuRatio ( ) const

virtual

The ratio of the Br $(H\to \mu^+\mu^-)$ in the current model and in the Standard Model.

Returns: Br $(H\to \mu^+\mu^-)$/Br $(H\to \mu^+\mu^-)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28450 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHmumuRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHmumuRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHssRatio()

const double NPSMEFTd6General::BrHssRatio ( ) const

virtual

The ratio of the Br $(H\to s\bar{s})$ in the current model and in the Standard Model.

Returns: Br $(H\to s\bar{s})$/Br $(H\to s\bar{s})_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28738 of file NPSMEFTd6General.cpp.

                                                {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHssRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHssRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHtautauRatio()

const double NPSMEFTd6General::BrHtautauRatio ( ) const

virtual

The ratio of the Br $(H\to \tau^+\tau^-)$ in the current model and in the Standard Model.

Returns: Br $(H\to \tau^+\tau^-)$/Br $(H\to \tau^+\tau^-)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28537 of file NPSMEFTd6General.cpp.

                                                    {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHtautauRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHtautauRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHtoinvRatio()

const double NPSMEFTd6General::BrHtoinvRatio ( ) const

virtual

The ratio of the Br $(H\to invisible)$ in the current model and in the Standard Model.

Returns: Br $(H\to invisible)$/Br $(H\to ZZ \to invisible)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 35278 of file NPSMEFTd6General.cpp.

                                                   {
    // H->ZZ*->4v + H->inv (NP)
    return ( Br_H_inv() / (trueSM.computeBrHto4v()) );
}

◆ BrHudduRatio()

const double NPSMEFTd6General::BrHudduRatio ( ) const

virtual

The ratio of the Br $(H\to uddu)$ in the current model and in the Standard Model.

Returns: Br $(H\to uddu)$/Br $(H\to uddu)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 33571 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHudduRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHudduRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHvisRatio()

const double NPSMEFTd6General::BrHvisRatio ( ) const

virtual

The ratio of the Br $(H\to visible)$ in the current model and in the Standard Model.

Returns: Br $(H\to visible)$/Br $(H\to visible)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 35229 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dvis1 = 0.0, dvis2 = 0.0, delta2SM;
    double GHvisR = 1.0;
 
    //  Sum over decays of visible SM and exotic modes
    dvis1 = (trueSM.computeBrHtogg() * deltaGammaHggRatio1()
            //            + trueSM.computeBrHtoWW() * deltaGammaHWWRatio1()
            //            + trueSM.computeBrHtoZZ() * deltaGammaHZZRatio1()
            + trueSM.computeBrHto4f() * deltaGammaH4fRatio1()
            + trueSM.computeBrHtoZga() * deltaGammaHZgaRatio1()
            + trueSM.computeBrHtogaga() * deltaGammaHgagaRatio1()
            + trueSM.computeBrHtomumu() * deltaGammaHmumuRatio1()
            + trueSM.computeBrHtotautau() * deltaGammaHtautauRatio1()
            + trueSM.computeBrHtocc() * deltaGammaHccRatio1()
            + trueSM.computeBrHtoss() * deltaGammaHssRatio1()
            + trueSM.computeBrHtobb() * deltaGammaHbbRatio1()
            + BrHexo);
 
    Br += dvis1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        //  Sum over decays of visible SM and exotic modes
        delta2SM = trueSM.computeBrHtogg() * deltaGammaHggRatio2()
                + trueSM.computeBrHtoWW() * deltaGammaHWWRatio2()
                + trueSM.computeBrHtoZZ() * deltaGammaHZZRatio2()
                + trueSM.computeBrHtoZga() * deltaGammaHZgaRatio2()
                + trueSM.computeBrHtogaga() * deltaGammaHgagaRatio2()
                + trueSM.computeBrHtomumu() * deltaGammaHmumuRatio2()
                + trueSM.computeBrHtotautau() * deltaGammaHtautauRatio2()
                + trueSM.computeBrHtocc() * deltaGammaHccRatio2()
                + trueSM.computeBrHtoss() * deltaGammaHssRatio2()
                + trueSM.computeBrHtobb() * deltaGammaHbbRatio2();
 
        dvis2 = delta2SM + (BrHexo)*(BrHexo + delta2SM);
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dvis1 * dGammaHTotR1
                + dvis2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHvisR += dvis1 + dvis2;
    if ((Br < 0) || (GHvisR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHVVRatio()

const double NPSMEFTd6General::BrHVVRatio ( ) const

virtual

The ratio of the Br $(H\to VV)$ in the current model and in the Standard Model.

Returns: Br $(H\to VV)$/Br $(H\to VV)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 27917 of file NPSMEFTd6General.cpp.

                                                {
    double BrZZSM = trueSM.computeBrHtoZZ(), BrWWSM = trueSM.computeBrHtoWW();
 
    return (BrZZSM * BrHZZRatio() + BrWWSM * BrHWWRatio()) / (BrZZSM + BrWWSM);
}

◆ BrHWffRatio()

const double NPSMEFTd6General::BrHWffRatio ( ) const

virtual

The ratio of the Br $(H\to W f f)$, with $f$ any fermion, in the current model and in the Standard Model.

Returns: Br $(H\to W f f)$/Br $(H\to W f f)_{\mathrm{SM}}$

Definition at line 26515 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHWffRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHWffRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHWjjRatio()

const double NPSMEFTd6General::BrHWjjRatio ( ) const

virtual

The ratio of the Br $(H\to W j j)$ in the current model and in the Standard Model.

Returns: Br $(H\to W j j)$/Br $(H\to W j j)_{\mathrm{SM}}$

Definition at line 26356 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHWjjRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHWjjRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHWlvRatio()

const double NPSMEFTd6General::BrHWlvRatio ( ) const

virtual

The ratio of the Br $(H\to W l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model.

Returns: Br $(H\to Wl\nu)$/Br $(H\to Wl\nu)_{\mathrm{SM}}$

Definition at line 26197 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHWlvRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHWlvRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHWW2l2vRatio()

const double NPSMEFTd6General::BrHWW2l2vRatio ( ) const

virtual

The ratio of the Br $(H\to WW^*\to l\nu l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model.

Returns: Br $(H\to WW^*\to l\nu l\nu)$/Br $(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}$

Definition at line 26279 of file NPSMEFTd6General.cpp.

                                                    {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHWW2l2vRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHWW2l2vRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHWW4fRatio()

const double NPSMEFTd6General::BrHWW4fRatio ( ) const

virtual

The ratio of the Br $(H\to WW^*\to 4f)$, with $f$ any fermion, in the current model and in the Standard Model.

Returns: Br $(H\to WW^*\to 4f)$/Br $(H\to WW^*\to 4f)_{\mathrm{SM}}$

Definition at line 26658 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHWW4fRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHWW4fRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHWW4jRatio()

const double NPSMEFTd6General::BrHWW4jRatio ( ) const

virtual

The ratio of the Br $(H\to WW^*\to 4j)$ in the current model and in the Standard Model.

Returns: Br $(H\to WW^*\to 4j)$/Br $(H\to WW^*\to 4j)_{\mathrm{SM}}$

Definition at line 26437 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHWW4jRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHWW4jRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHWWRatio()

const double NPSMEFTd6General::BrHWWRatio ( ) const

virtual

The ratio of the Br $(H\to WW)$ in the current model and in the Standard Model.

Returns: Br $(H\to WW)$/Br $(H\to WW)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 26137 of file NPSMEFTd6General.cpp.

                                                {
 
//    return BrHWW4fRatio();
    return BrH4fCCRatio();
 
}

◆ BrHZddRatio()

const double NPSMEFTd6General::BrHZddRatio ( ) const

virtual

The ratio of the Br $(H\to Z d d)$ ( $d=d,s,b $) in the current model and in the Standard Model.

Returns: Br $(H\to Z d d)$/Br $(H\to Z d d)_{\mathrm{SM}}$

Definition at line 27572 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHZddRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHZddRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHZffRatio()

const double NPSMEFTd6General::BrHZffRatio ( ) const

virtual

The ratio of the Br $(H\to Zff)$, with $f$ any fermion, in the current model and in the Standard Model.

Returns: Br $(H\to Zff)$/Br $(H\to Zff)_{\mathrm{SM}}$

Definition at line 27672 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHZffRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHZffRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHZgaeeRatio()

const double NPSMEFTd6General::BrHZgaeeRatio ( ) const

virtual

The ratio of the Br $(H\to Z\gamma\to ee\gamma)$ in the current model and in the Standard Model.

Returns: Br $(H\to Z\gamma\to ee\gamma)$/Br $(H\to Z\gamma\to ee\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28100 of file NPSMEFTd6General.cpp.

                                                   {
    double deltaBRratio;
 
    deltaBRratio = deltaGamma_Zf(leptons[ELECTRON]) / (trueSM.GammaZ(leptons[ELECTRON]));
 
    deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
 
    return ( BrHZgaRatio() + deltaBRratio);
}

◆ BrHZgallRatio()

const double NPSMEFTd6General::BrHZgallRatio ( ) const

virtual

The ratio of the Br $(H\to Z\gamma\to ll\gamma)$ ( $l=e,\mu $) in the current model and in the Standard Model.

Returns: Br $(H\to Z\gamma\to ll\gamma)$/Br $(H\to Z\gamma\to ll\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28086 of file NPSMEFTd6General.cpp.

                                                   {
    double deltaBRratio;
 
    deltaBRratio = deltaGamma_Zf(leptons[ELECTRON])
            + deltaGamma_Zf(leptons[MU]);
 
    deltaBRratio = deltaBRratio /
            (trueSM.GammaZ(leptons[ELECTRON]) + trueSM.GammaZ(leptons[MU]));
 
    deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
 
    return ( BrHZgaRatio() + deltaBRratio);
}

◆ BrHZgamumuRatio()

const double NPSMEFTd6General::BrHZgamumuRatio ( ) const

virtual

The ratio of the Br $(H\to Z\gamma\to \mu\mu\gamma)$ in the current model and in the Standard Model.

Returns: Br $(H\to Z\gamma\to \mu\mu\gamma)$/Br $(H\to Z\gamma\to \mu\mu\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28110 of file NPSMEFTd6General.cpp.

                                                     {
    double deltaBRratio;
 
    deltaBRratio = deltaGamma_Zf(leptons[MU]) / (trueSM.GammaZ(leptons[MU]));
 
    deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
 
    return ( BrHZgaRatio() + deltaBRratio);
}

◆ BrHZgaRatio()

const double NPSMEFTd6General::BrHZgaRatio ( ) const

virtual

The ratio of the Br $(H\to Z\gamma)$ in the current model and in the Standard Model.

Returns: Br $(H\to Z\gamma)$/Br $(H\to Z\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28061 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHZgaRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHZgaRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
 
}

◆ BrHZllRatio()

const double NPSMEFTd6General::BrHZllRatio ( ) const

virtual

The ratio of the Br $(H\to Zll)$ ( $l=e,\mu $) in the current model and in the Standard Model.

Returns: Br $(H\to Zll)$/Br $(H\to Zll)_{\mathrm{SM}}$

Definition at line 26786 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHZllRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHZllRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHZuuRatio()

const double NPSMEFTd6General::BrHZuuRatio ( ) const

virtual

The ratio of the Br $(H\to Z u u)$ ( $u=u,c $) in the current model and in the Standard Model.

Returns: Br $(H\to Z u u)$/Br $(H\to Z u u)_{\mathrm{SM}}$

Definition at line 27479 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHZuuRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHZuuRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHZvvRatio()

const double NPSMEFTd6General::BrHZvvRatio ( ) const

virtual

The ratio of the Br $(H\to Z\nu\nu)$ in the current model and in the Standard Model.

Returns: Br $(H\to Z\nu\nu)$/Br $(H\to Z\nu\nu)_{\mathrm{SM}}$

Definition at line 27317 of file NPSMEFTd6General.cpp.

                                                 {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHZvvRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHZvvRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHZZ2e2muRatio()

const double NPSMEFTd6General::BrHZZ2e2muRatio ( ) const

virtual

The ratio of the Br $(H\to ZZ* \to 2e 2\mu)$ in the current model and in the Standard Model.

Returns: Br $(H\to ZZ* \to 2e 2\mu)$/Br $(H\to ZZ* \to 2e 2\mu)_{\mathrm{SM}}$

Definition at line 27156 of file NPSMEFTd6General.cpp.

                                                     {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHZZ2e2muRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHZZ2e2muRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHZZ4dRatio()

const double NPSMEFTd6General::BrHZZ4dRatio ( ) const

virtual

The ratio of the Br $(H\to ZZ* \to 4 d)$ ( $d=d,s,b $) in the current model and in the Standard Model.

Returns: Br $(H\to ZZ* \to 4 d)$/Br $(H\to ZZ* \to 4 d)_{\mathrm{SM}}$

Definition at line 27596 of file NPSMEFTd6General.cpp.

                                                  {
    double deltaBRratio;
 
    deltaBRratio = deltaGamma_Zf(quarks[DOWN])
            + deltaGamma_Zf(quarks[STRANGE])
            + deltaGamma_Zf(quarks[BOTTOM]);
 
    deltaBRratio = deltaBRratio /
            (trueSM.GammaZ(quarks[DOWN])
            + trueSM.GammaZ(quarks[STRANGE])
            + trueSM.GammaZ(quarks[BOTTOM]));
 
    deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
 
    return ( BrHZddRatio() + deltaBRratio);
}

◆ BrHZZ4eRatio()

const double NPSMEFTd6General::BrHZZ4eRatio ( ) const

virtual

The ratio of the Br $(H\to ZZ* \to 4e)$ in the current model and in the Standard Model.

Returns: Br $(H\to ZZ* \to 4e)$/Br $(H\to ZZ* \to 4e)_{\mathrm{SM}}$

Definition at line 27073 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHZZ4eRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHZZ4eRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHZZ4fRatio()

const double NPSMEFTd6General::BrHZZ4fRatio ( ) const

virtual

The ratio of the Br $(H\to ZZ* \to 4f)$, with $f$ any fermion, in the current model and in the Standard Model.

Returns: Br $(H\to ZZ* \to 4f)$/Br $(H\to ZZ* \to 4f)_{\mathrm{SM}}$

Definition at line 27893 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHZZ4fRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHZZ4fRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHZZ4lRatio()

const double NPSMEFTd6General::BrHZZ4lRatio ( ) const

virtual

The ratio of the Br $(H\to ZZ* \to 4l)$ ( $l=e,\mu $) in the current model and in the Standard Model.

Returns: Br $(H\to ZZ* \to 4l)$/Br $(H\to ZZ* \to 4l)_{\mathrm{SM}}$

Definition at line 26990 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHZZ4lRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHZZ4lRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHZZ4muRatio()

const double NPSMEFTd6General::BrHZZ4muRatio ( ) const

virtual

The ratio of the Br $(H\to ZZ* \to 4\mu)$ in the current model and in the Standard Model.

Returns: Br $(H\to ZZ* \to 4\mu)$/Br $(H\to ZZ* \to 4\mu)_{\mathrm{SM}}$

Definition at line 27239 of file NPSMEFTd6General.cpp.

                                                   {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHZZ4muRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHZZ4muRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHZZ4uRatio()

const double NPSMEFTd6General::BrHZZ4uRatio ( ) const

virtual

The ratio of the Br $(H\to ZZ* \to 4 u)$ ( $u=u,c $) in the current model and in the Standard Model.

Returns: Br $(H\to ZZ* \to 4 u)$/Br $(H\to ZZ* \to 4 u)_{\mathrm{SM}}$

Definition at line 27503 of file NPSMEFTd6General.cpp.

                                                  {
    double deltaBRratio;
 
    deltaBRratio = deltaGamma_Zf(quarks[UP])
            + deltaGamma_Zf(quarks[CHARM]);
 
    deltaBRratio = deltaBRratio /
            (trueSM.GammaZ(quarks[UP]) + trueSM.GammaZ(quarks[CHARM]));
 
    deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
 
    return ( BrHZuuRatio() + deltaBRratio);
}

◆ BrHZZ4vRatio()

const double NPSMEFTd6General::BrHZZ4vRatio ( ) const

virtual

The ratio of the Br $(H\to ZZ* \to 4\nu)$ in the current model and in the Standard Model.

Returns: Br $(H\to ZZ* \to 4\nu)$/Br $(H\to ZZ* \to 4\nu)_{\mathrm{SM}}$

Definition at line 27400 of file NPSMEFTd6General.cpp.

                                                  {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiR2 = 0.0, GHiR = 1.0;
 
    dGHiR1 = deltaGammaHZZ4vRatio1();
 
    Br += dGHiR1 - dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
 
        dGHiR2 = deltaGammaHZZ4vRatio2();
 
        //Add contributions that are quadratic in the effective coefficients
        Br += -dGHiR1 * dGammaHTotR1
                + dGHiR2 - dGammaHTotR2
                + pow(dGammaHTotR1, 2.0);
    }
 
    GHiR += dGHiR1 + dGHiR2;
    if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ BrHZZRatio()

const double NPSMEFTd6General::BrHZZRatio ( ) const

virtual

The ratio of the Br $(H\to ZZ)$ in the current model and in the Standard Model.

Returns: Br $(H\to ZZ)$/Br $(H\to ZZ)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 26726 of file NPSMEFTd6General.cpp.

                                                {
    //return BrHZZ4fRatio();    
    return BrH4fNCRatio();
}

◆ BrW()

const double NPSMEFTd6General::BrW	(	const Particle	fi,
		const Particle	fj
	)		const

virtual

The branching ratio of the $W$ boson decaying into a SM fermion pair, $Br(W\to f_i f_j)$.

Returns: $Br(W\to f_i f_j)$ in GeV

Reimplemented from NPbase.

Definition at line 16148 of file NPSMEFTd6General.cpp.

                                                                             {
    double GammW0 = trueSM.GammaW();
    double dGammW = deltaGamma_W();
    
    double GammWij0 = trueSM.GammaW(fi, fj);
    double dGammWij = deltaGamma_Wff(fi, fj);
 
    return GammWij0 / GammW0 + dGammWij / GammW0 - GammWij0 * dGammW / GammW0 / GammW0;
}

◆ cbW_TWG()

const double NPSMEFTd6General::cbW_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47530 of file NPSMEFTd6General.cpp.

                                                            {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // Minus sign because of difference in covariant derivative convention of Top WG    
    comb = - getSMEFTCoeff("CdWR", 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ CeeLL_bottom()

const double NPSMEFTd6General::CeeLL_bottom ( const double mu ) const

Definition at line 45871 of file NPSMEFTd6General.cpp.

                                                                 {
    return (getSMEFTCoeff("Clq1R", 0, 0, 2, 2, mu) + getSMEFTCoeff("Clq3R", 0, 0, 2, 2, mu));
}

◆ CeeLL_charm()

const double NPSMEFTd6General::CeeLL_charm ( const double mu ) const

Definition at line 45855 of file NPSMEFTd6General.cpp.

                                                                {
    return (getSMEFTCoeff("Clq1R", 0, 0, 1, 1, mu) - getSMEFTCoeff("Clq3R", 0, 0, 1, 1, mu));
}

◆ CeeLL_down()

const double NPSMEFTd6General::CeeLL_down ( const double mu ) const

Definition at line 45863 of file NPSMEFTd6General.cpp.

                                                               {
    return (getSMEFTCoeff("Clq1R", 0, 0, 0, 0, mu) + getSMEFTCoeff("Clq3R", 0, 0, 0, 0, mu));
}

◆ CeeLL_e()

const double NPSMEFTd6General::CeeLL_e ( const double mu ) const

Definition at line 45839 of file NPSMEFTd6General.cpp.

                                                            {
    return 2.0 * (getSMEFTCoeff("CllR", 0, 0, 0, 0, mu));
}

◆ CeeLL_mu()

const double NPSMEFTd6General::CeeLL_mu ( const double mu ) const

Definition at line 45843 of file NPSMEFTd6General.cpp.

                                                             {
    return 2.0 * (getSMEFTCoeff("CllR", 0, 0, 1, 1, mu) + getSMEFTCoeff("CllR", 0, 1, 1, 0, mu));
}

◆ CeeLL_strange()

const double NPSMEFTd6General::CeeLL_strange ( const double mu ) const

Definition at line 45867 of file NPSMEFTd6General.cpp.

                                                                  {
    return (getSMEFTCoeff("Clq1R", 0, 0, 1, 1, mu) + getSMEFTCoeff("Clq3R", 0, 0, 1, 1, mu));
}

◆ CeeLL_tau()

const double NPSMEFTd6General::CeeLL_tau ( const double mu ) const

Definition at line 45847 of file NPSMEFTd6General.cpp.

                                                              {
    return 2.0 * (getSMEFTCoeff("CllR", 0, 0, 2, 2, mu) + getSMEFTCoeff("CllR", 0, 2, 2, 0, mu));
}

◆ CeeLL_top()

const double NPSMEFTd6General::CeeLL_top ( const double mu ) const

Definition at line 45859 of file NPSMEFTd6General.cpp.

                                                              {
    return (getSMEFTCoeff("Clq1R", 0, 0, 2, 2, mu) - getSMEFTCoeff("Clq3R", 0, 0, 2, 2, mu));
}

◆ CeeLL_up()

const double NPSMEFTd6General::CeeLL_up ( const double mu ) const

Definition at line 45851 of file NPSMEFTd6General.cpp.

                                                             {
    return (getSMEFTCoeff("Clq1R", 0, 0, 0, 0, mu) - getSMEFTCoeff("Clq3R", 0, 0, 0, 0, mu));
}

◆ CeeLR_bottom()

const double NPSMEFTd6General::CeeLR_bottom ( const double mu ) const

Definition at line 45907 of file NPSMEFTd6General.cpp.

                                                                 {
    return (getSMEFTCoeff("CldR", 0, 0, 2, 2, mu));
}

◆ CeeLR_charm()

const double NPSMEFTd6General::CeeLR_charm ( const double mu ) const

Definition at line 45891 of file NPSMEFTd6General.cpp.

                                                                {
    return (getSMEFTCoeff("CluR", 0, 0, 1, 1, mu));
}

◆ CeeLR_down()

const double NPSMEFTd6General::CeeLR_down ( const double mu ) const

Definition at line 45899 of file NPSMEFTd6General.cpp.

                                                               {
    return (getSMEFTCoeff("CldR", 0, 0, 0, 0, mu));
}

◆ CeeLR_e()

const double NPSMEFTd6General::CeeLR_e ( const double mu ) const

Definition at line 45875 of file NPSMEFTd6General.cpp.

                                                            {
    return (getSMEFTCoeff("CleR", 0, 0, 0, 0, mu));
}

◆ CeeLR_mu()

const double NPSMEFTd6General::CeeLR_mu ( const double mu ) const

Definition at line 45879 of file NPSMEFTd6General.cpp.

                                                             {
    return (getSMEFTCoeff("CleR", 0, 0, 1, 1, mu));
}

◆ CeeLR_strange()

const double NPSMEFTd6General::CeeLR_strange ( const double mu ) const

Definition at line 45903 of file NPSMEFTd6General.cpp.

                                                                  {
    return (getSMEFTCoeff("CldR", 0, 0, 1, 1, mu));
}

◆ CeeLR_tau()

const double NPSMEFTd6General::CeeLR_tau ( const double mu ) const

Definition at line 45883 of file NPSMEFTd6General.cpp.

                                                              {
    return (getSMEFTCoeff("CleR", 0, 0, 2, 2, mu));
}

◆ CeeLR_top()

const double NPSMEFTd6General::CeeLR_top ( const double mu ) const

Definition at line 45895 of file NPSMEFTd6General.cpp.

                                                              {
    return (getSMEFTCoeff("CluR", 0, 0, 2, 2, mu));
}

◆ CeeLR_up()

const double NPSMEFTd6General::CeeLR_up ( const double mu ) const

Definition at line 45887 of file NPSMEFTd6General.cpp.

                                                             {
    return (getSMEFTCoeff("CluR", 0, 0, 0, 0, mu));
}

◆ CeeRL_bottom()

const double NPSMEFTd6General::CeeRL_bottom ( const double mu ) const

Definition at line 45944 of file NPSMEFTd6General.cpp.

                                                                 {
    return (getSMEFTCoeff("CqeR", 2, 2, 0, 0, mu));
}

◆ CeeRL_charm()

const double NPSMEFTd6General::CeeRL_charm ( const double mu ) const

Definition at line 45928 of file NPSMEFTd6General.cpp.

                                                                {
    return (getSMEFTCoeff("CqeR", 1, 1, 0, 0, mu));
}

◆ CeeRL_down()

const double NPSMEFTd6General::CeeRL_down ( const double mu ) const

Definition at line 45936 of file NPSMEFTd6General.cpp.

                                                               {
    return (getSMEFTCoeff("CqeR", 0, 0, 0, 0, mu));
}

◆ CeeRL_e()

const double NPSMEFTd6General::CeeRL_e ( const double mu ) const

Definition at line 45911 of file NPSMEFTd6General.cpp.

                                                            {
    // Same as LR by definition
    return CeeLR_e(mu);
}

◆ CeeRL_mu()

const double NPSMEFTd6General::CeeRL_mu ( const double mu ) const

Definition at line 45916 of file NPSMEFTd6General.cpp.

                                                             {
    return (getSMEFTCoeff("CleR", 1, 1, 0, 0, mu));
}

◆ CeeRL_strange()

const double NPSMEFTd6General::CeeRL_strange ( const double mu ) const

Definition at line 45940 of file NPSMEFTd6General.cpp.

                                                                  {
    return (getSMEFTCoeff("CqeR", 1, 1, 0, 0, mu));
}

◆ CeeRL_tau()

const double NPSMEFTd6General::CeeRL_tau ( const double mu ) const

Definition at line 45920 of file NPSMEFTd6General.cpp.

                                                              {
    return (getSMEFTCoeff("CleR", 2, 2, 0, 0, mu));
}

◆ CeeRL_top()

const double NPSMEFTd6General::CeeRL_top ( const double mu ) const

Definition at line 45932 of file NPSMEFTd6General.cpp.

                                                              {
    return (getSMEFTCoeff("CqeR", 2, 2, 0, 0, mu));
}

◆ CeeRL_up()

const double NPSMEFTd6General::CeeRL_up ( const double mu ) const

Definition at line 45924 of file NPSMEFTd6General.cpp.

                                                             {
    return (getSMEFTCoeff("CqeR", 0, 0, 0, 0, mu));
}

◆ CeeRR_bottom()

const double NPSMEFTd6General::CeeRR_bottom ( const double mu ) const

Definition at line 45980 of file NPSMEFTd6General.cpp.

                                                                 {
    return (getSMEFTCoeff("CedR", 0, 0, 2, 2, mu));
}

◆ CeeRR_charm()

const double NPSMEFTd6General::CeeRR_charm ( const double mu ) const

Definition at line 45964 of file NPSMEFTd6General.cpp.

                                                                {
    return (getSMEFTCoeff("CeuR", 0, 0, 1, 1, mu));
}

◆ CeeRR_down()

const double NPSMEFTd6General::CeeRR_down ( const double mu ) const

Definition at line 45972 of file NPSMEFTd6General.cpp.

                                                               {
    return (getSMEFTCoeff("CedR", 0, 0, 0, 0, mu));
}

◆ CeeRR_e()

const double NPSMEFTd6General::CeeRR_e ( const double mu ) const

Definition at line 45948 of file NPSMEFTd6General.cpp.

                                                            {
    return 2.0 * (getSMEFTCoeff("CeeR", 0, 0, 0, 0, mu));
}

◆ CeeRR_mu()

const double NPSMEFTd6General::CeeRR_mu ( const double mu ) const

Definition at line 45952 of file NPSMEFTd6General.cpp.

                                                             {
    return 4.0 * (getSMEFTCoeff("CeeR", 0, 0, 1, 1, mu));
}

◆ CeeRR_strange()

const double NPSMEFTd6General::CeeRR_strange ( const double mu ) const

Definition at line 45976 of file NPSMEFTd6General.cpp.

                                                                  {
    return (getSMEFTCoeff("CedR", 0, 0, 1, 1, mu));
}

◆ CeeRR_tau()

const double NPSMEFTd6General::CeeRR_tau ( const double mu ) const

Definition at line 45956 of file NPSMEFTd6General.cpp.

                                                              {
    return 4.0 * (getSMEFTCoeff("CeeR", 0, 0, 2, 2, mu));
}

◆ CeeRR_top()

const double NPSMEFTd6General::CeeRR_top ( const double mu ) const

Definition at line 45968 of file NPSMEFTd6General.cpp.

                                                              {
    return (getSMEFTCoeff("CeuR", 0, 0, 2, 2, mu));
}

◆ CeeRR_up()

const double NPSMEFTd6General::CeeRR_up ( const double mu ) const

Definition at line 45960 of file NPSMEFTd6General.cpp.

                                                             {
    return (getSMEFTCoeff("CeuR", 0, 0, 0, 0, mu));
}

◆ CEWHd11()

const double NPSMEFTd6General::CEWHd11 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hd})_{11}$.

Returns: $(\hat{C}_{Hd})_{11}$

Reimplemented from NPbase.

Definition at line 43324 of file NPSMEFTd6General.cpp.

                                                            {
    return getSMEFTCoeff("CHdR", 0, 0, mu) + (1.0 / 6.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHd22()

const double NPSMEFTd6General::CEWHd22 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hd})_{22}$.

Returns: $(\hat{C}_{Hd})_{22}$

Reimplemented from NPbase.

Definition at line 43328 of file NPSMEFTd6General.cpp.

                                                            {
    return getSMEFTCoeff("CHdR", 1, 1, mu) + (1.0 / 6.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHd33()

const double NPSMEFTd6General::CEWHd33 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hd})_{33}$.

Returns: $(\hat{C}_{Hd})_{33}$

Reimplemented from NPbase.

Definition at line 43332 of file NPSMEFTd6General.cpp.

                                                            {
    return getSMEFTCoeff("CHdR", 2, 2, mu) + (1.0 / 6.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHe11()

const double NPSMEFTd6General::CEWHe11 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{He})_{11}$.

Returns: $(\hat{C}_{He})_{11}$

Reimplemented from NPbase.

Definition at line 43300 of file NPSMEFTd6General.cpp.

                                                            {
    return getSMEFTCoeff("CHeR", 0, 0, mu) + (1.0 / 2.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHe22()

const double NPSMEFTd6General::CEWHe22 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{He})_{22}$.

Returns: $(\hat{C}_{He})_{22}$

Reimplemented from NPbase.

Definition at line 43304 of file NPSMEFTd6General.cpp.

                                                            {
    return getSMEFTCoeff("CHeR", 1, 1, mu) + (1.0 / 2.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHe33()

const double NPSMEFTd6General::CEWHe33 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{He})_{33}$.

Returns: $(\hat{C}_{He})_{33}$

Reimplemented from NPbase.

Definition at line 43308 of file NPSMEFTd6General.cpp.

                                                            {
    return getSMEFTCoeff("CHeR", 2, 2, mu) + (1.0 / 2.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHL111()

const double NPSMEFTd6General::CEWHL111 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(1)})_{11}$.

Returns: $(\hat{C}_{HL}^{(1)})_{11}$

Reimplemented from NPbase.

Definition at line 43244 of file NPSMEFTd6General.cpp.

                                                             {
    return getSMEFTCoeff("CHl1R", 0, 0, mu) + (1.0 / 4.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHL122()

const double NPSMEFTd6General::CEWHL122 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(1)})_{22}$.

Returns: $(\hat{C}_{HL}^{(1)})_{22}$

Reimplemented from NPbase.

Definition at line 43248 of file NPSMEFTd6General.cpp.

                                                             {
    return getSMEFTCoeff("CHl1R", 1, 1, mu) + (1.0 / 4.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHL133()

const double NPSMEFTd6General::CEWHL133 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(1)})_{33}$.

Returns: $(\hat{C}_{HL}^{(1)})_{33}$

Reimplemented from NPbase.

Definition at line 43252 of file NPSMEFTd6General.cpp.

                                                             {
    return getSMEFTCoeff("CHl1R", 2, 2, mu) + (1.0 / 4.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHL311()

const double NPSMEFTd6General::CEWHL311 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(3)})_{11}$.

Returns: $(\hat{C}_{HL}^{(3)})_{11}$

Reimplemented from NPbase.

Definition at line 43256 of file NPSMEFTd6General.cpp.

                                                             {
    return getSMEFTCoeff("CHl3R", 0, 0, mu) + (1.0 / 4.0) * (cW2_tree / sW2_tree) * getSMEFTCoeff("CHD", mu) + (cW_tree / sW_tree) * getSMEFTCoeff("CHWB", mu);
}

◆ CEWHL322()

const double NPSMEFTd6General::CEWHL322 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(3)})_{22}$.

Returns: $(\hat{C}_{HL}^{(3)})_{22}$

Reimplemented from NPbase.

Definition at line 43260 of file NPSMEFTd6General.cpp.

                                                             {
    return getSMEFTCoeff("CHl3R", 1, 1, mu) + (1.0 / 4.0) * (cW2_tree / sW2_tree) * getSMEFTCoeff("CHD", mu) + (cW_tree / sW_tree) * getSMEFTCoeff("CHWB", mu);
}

◆ CEWHL333()

const double NPSMEFTd6General::CEWHL333 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(3)})_{33}$.

Returns: $(\hat{C}_{HL}^{(3)})_{33}$

Reimplemented from NPbase.

Definition at line 43264 of file NPSMEFTd6General.cpp.

                                                             {
    return getSMEFTCoeff("CHl3R", 2, 2, mu) + (1.0 / 4.0) * (cW2_tree / sW2_tree) * getSMEFTCoeff("CHD", mu) + (cW_tree / sW_tree) * getSMEFTCoeff("CHWB", mu);
}

◆ CEWHQ111()

const double NPSMEFTd6General::CEWHQ111 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(1)})_{11}$.

Returns: $(\hat{C}_{HQ}^{(1)})_{11}$

Reimplemented from NPbase.

Definition at line 43268 of file NPSMEFTd6General.cpp.

                                                             {
    return getSMEFTCoeff("CHq1R", 0, 0, mu) - (1.0 / 12.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHQ122()

const double NPSMEFTd6General::CEWHQ122 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(1)})_{22}$.

Returns: $(\hat{C}_{HQ}^{(1)})_{22}$

Reimplemented from NPbase.

Definition at line 43272 of file NPSMEFTd6General.cpp.

                                                             {
    return getSMEFTCoeff("CHq1R", 1, 1, mu) - (1.0 / 12.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHQ133()

const double NPSMEFTd6General::CEWHQ133 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(1)})_{33}$.

Returns: $(\hat{C}_{HQ}^{(1)})_{33}$

Reimplemented from NPbase.

Definition at line 43276 of file NPSMEFTd6General.cpp.

                                                             {
    return getSMEFTCoeff("CHq1R", 2, 2, mu) - (1.0 / 12.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHQ311()

const double NPSMEFTd6General::CEWHQ311 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(3)})_{11}$.

Returns: $(\hat{C}_{HQ}^{(3)})_{11}$

Reimplemented from NPbase.

Definition at line 43280 of file NPSMEFTd6General.cpp.

                                                             {
    return getSMEFTCoeff("CHq3R", 0, 0, mu) + (1.0 / 4.0) * (cW2_tree / sW2_tree) * getSMEFTCoeff("CHD", mu) + (cW_tree / sW_tree) * getSMEFTCoeff("CHWB", mu);
}

◆ CEWHQ322()

const double NPSMEFTd6General::CEWHQ322 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(3)})_{22}$.

Returns: $(\hat{C}_{HQ}^{(3)})_{22}$

Reimplemented from NPbase.

Definition at line 43284 of file NPSMEFTd6General.cpp.

                                                             {
    return getSMEFTCoeff("CHq3R", 1, 1, mu) + (1.0 / 4.0) * (cW2_tree / sW2_tree) * getSMEFTCoeff("CHD", mu) + (cW_tree / sW_tree) * getSMEFTCoeff("CHWB", mu);
}

◆ CEWHQ333()

const double NPSMEFTd6General::CEWHQ333 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(3)})_{33}$.

Returns: $(\hat{C}_{HQ}^{(3)})_{33}$

Reimplemented from NPbase.

Definition at line 43288 of file NPSMEFTd6General.cpp.

                                                             {
    return getSMEFTCoeff("CHq3R", 2, 2, mu) + (1.0 / 4.0) * (cW2_tree / sW2_tree) * getSMEFTCoeff("CHD", mu) + (cW_tree / sW_tree) * getSMEFTCoeff("CHWB", mu);
}

◆ CEWHQd33()

const double NPSMEFTd6General::CEWHQd33 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(d)})_{33}$.

Returns: $(\hat{C}_{HQ}^{(d)})_{33}$

Reimplemented from NPbase.

Definition at line 43292 of file NPSMEFTd6General.cpp.

                                                             {
    return 0.5 * (CEWHQ133(mu) + CEWHQ333(mu));
}

◆ CEWHQu33()

const double NPSMEFTd6General::CEWHQu33 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis not constrained by EWPO (at LO) $(\hat{C}_{HQ}^{(u)})_{33}$.

Returns: $(\hat{C}_{HQ}^{(u)})_{33}$

Reimplemented from NPbase.

Definition at line 43296 of file NPSMEFTd6General.cpp.

                                                             {
    return 0.5 * (CEWHQ133(mu) - CEWHQ333(mu));
}

◆ CEWHu11()

const double NPSMEFTd6General::CEWHu11 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hu})_{11}$.

Returns: $(\hat{C}_{Hu})_{11}$

Reimplemented from NPbase.

Definition at line 43312 of file NPSMEFTd6General.cpp.

                                                            {
    return getSMEFTCoeff("CHuR", 0, 0, mu) - (1.0 / 3.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHu22()

const double NPSMEFTd6General::CEWHu22 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hu})_{22}$.

Returns: $(\hat{C}_{Hu})_{22}$

Reimplemented from NPbase.

Definition at line 43316 of file NPSMEFTd6General.cpp.

                                                            {
    return getSMEFTCoeff("CHuR", 1, 1, mu) - (1.0 / 3.0) * getSMEFTCoeff("CHD", mu);
}

◆ CEWHu33()

const double NPSMEFTd6General::CEWHu33 ( const double mu ) const

virtual

Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hu})_{33}$.

Returns: $(\hat{C}_{Hu})_{33}$

Reimplemented from NPbase.

Definition at line 43320 of file NPSMEFTd6General.cpp.

                                                            {
    return getSMEFTCoeff("CHuR", 2, 2, mu) - (1.0 / 3.0) * getSMEFTCoeff("CHD", mu);
}

◆ cgaga_HB()

const double NPSMEFTd6General::cgaga_HB ( const double mu ) const

virtual

The Higgs-basis coupling $c_{\gamma\gamma}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $c_{\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 43201 of file NPSMEFTd6General.cpp.

                                                             {
    double ciHB;
 
    ciHB = (4.0 / eeMz2)*(sW2_tree * getSMEFTCoeff("CHW", mu) + cW2_tree * getSMEFTCoeff("CHB", mu) - sW_tree * cW_tree * getSMEFTCoeff("CHWB", mu)) * v2;
 
    return ciHB;
}

◆ cgg_HB()

const double NPSMEFTd6General::cgg_HB ( const double mu ) const

virtual

The Higgs-basis coupling $c_{gg}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $c_{gg}$

Reimplemented from NPbase.

Definition at line 43209 of file NPSMEFTd6General.cpp.

                                                           {
    double ciHB;
 
    ciHB = (1.0 / (M_PI * AlsMz)) * getSMEFTCoeff("CHG", mu) * v2;
 
    return ciHB;
}

◆ cggEff_HB()

const double NPSMEFTd6General::cggEff_HB ( const double mu ) const

virtual

The effective Higgs-basis coupling $c_{gg}^{Eff}$. (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $c_{gg}^{Eff}$

Reimplemented from NPbase.

Definition at line 43217 of file NPSMEFTd6General.cpp.

                                                              {
    double ciHB;
 
    double m_t = mtpole;
    double m_b = quarks[BOTTOM].getMass();
    double m_c = quarks[CHARM].getMass();
 
    double At = deltayt_HB(mu) * AH_f(4.0 * m_t * m_t / mHl / mHl).real();
    double Ab = deltayb_HB(mu) * AH_f(4.0 * m_b * m_b / mHl / mHl).real();
    double Ac = deltayc_HB(mu) * AH_f(4.0 * m_c * m_c / mHl / mHl).real();
 
    ciHB = cgg_HB(mu) + (1.0 / 16.0 / M_PI / M_PI) * (At + Ab + Ac);
 
    return ciHB;
}

◆ cHb_TWG()

const double NPSMEFTd6General::cHb_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47455 of file NPSMEFTd6General.cpp.

                                                            {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    comb = getSMEFTCoeff("CHdR", 2, 2, mu);
 
    return (toTeVm2 * comb);
}

◆ cHQ3_TWG()

const double NPSMEFTd6General::cHQ3_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47435 of file NPSMEFTd6General.cpp.

                                                             {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    comb = getSMEFTCoeff("CHq3R", 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ cHQm_TWG()

const double NPSMEFTd6General::cHQm_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47415 of file NPSMEFTd6General.cpp.

                                                             {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    comb = getSMEFTCoeff("CHq1R", 2, 2, mu) - getSMEFTCoeff("CHq3R", 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ cHQp_TWG()

const double NPSMEFTd6General::cHQp_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47425 of file NPSMEFTd6General.cpp.

                                                             {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    comb = getSMEFTCoeff("CHq1R", 2, 2, mu) + getSMEFTCoeff("CHq3R", 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ cHt_TWG()

const double NPSMEFTd6General::cHt_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47445 of file NPSMEFTd6General.cpp.

                                                            {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    comb = getSMEFTCoeff("CHuR", 2, 2, mu);
 
    return (toTeVm2 * comb);
}

◆ cHtb_TWG()

const double NPSMEFTd6General::cHtb_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47465 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    comb = getSMEFTCoeff("CHudR", 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ computeGammaTotalRatio()

const double NPSMEFTd6General::computeGammaTotalRatio ( ) const

virtual

The ratio of the $\Gamma(H)$ in the current model and in the Standard Model.

Returns: $\Gamma(H)$/ $\Gamma(H)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 25875 of file NPSMEFTd6General.cpp.

                                                            {
    double width = 1.0;
 
    width += dGammaHTotR1;
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += dGammaHTotR2;
    }
 
    if (width < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return width;
 
}

◆ cQd1_TWG()

const double NPSMEFTd6General::cQd1_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47317 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = getSMEFTCoeff("Cqd1R", 2, 2, 0, 0, mu);
  
    return (toTeVm2 * comb);
}

◆ cQd8_TWG()

const double NPSMEFTd6General::cQd8_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47328 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = getSMEFTCoeff("Cqd8R", 2, 2, 0, 0, mu);
  
    return (toTeVm2 * comb);
}

◆ cQe_TWG()

const double NPSMEFTd6General::cQe_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47574 of file NPSMEFTd6General.cpp.

                                                            {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // Take first family for leptons
    comb = getSMEFTCoeff("CqeR", 2, 2, 0, 0, mu);
   
    return (toTeVm2 * comb);
}

◆ cQl3_TWG()

const double NPSMEFTd6General::cQl3_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47563 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // Take first family for leptons
    comb = getSMEFTCoeff("Clq3R", 0, 0, 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ cQlM_TWG()

const double NPSMEFTd6General::cQlM_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47541 of file NPSMEFTd6General.cpp.

                                                             {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    // Take first family for leptons
    comb = getSMEFTCoeff("Clq1R", 0, 0, 2, 2, mu) - getSMEFTCoeff("Clq3R", 0, 0, 2, 2, mu);
 
    return (toTeVm2 * comb);
}

◆ cQlP_TWG()

const double NPSMEFTd6General::cQlP_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47552 of file NPSMEFTd6General.cpp.

                                                             {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    // Take first family for leptons
    comb = getSMEFTCoeff("Clq1R", 0, 0, 2, 2, mu) + getSMEFTCoeff("Clq3R", 0, 0, 2, 2, mu);
 
    return (toTeVm2 * comb);
}

◆ cQq11_TWG()

const double NPSMEFTd6General::cQq11_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47273 of file NPSMEFTd6General.cpp.

                                                              {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = getSMEFTCoeff("Cqq1R", 0, 0, 2, 2, mu) + (1.0/6.0) * getSMEFTCoeff("Cqq1R", 0, 2, 2, 0, mu) + 0.5 * getSMEFTCoeff("Cqq3R", 0, 2, 2, 0, mu);
  
    return (toTeVm2 * comb);
}

◆ cQq18_TWG()

const double NPSMEFTd6General::cQq18_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47284 of file NPSMEFTd6General.cpp.

                                                              {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = getSMEFTCoeff("Cqq1R", 0, 2, 2, 0, mu) + 3.0 * getSMEFTCoeff("Cqq3R", 0, 2, 2, 0, mu);
  
    return (toTeVm2 * comb);
}

◆ cQQ1_TWG()

const double NPSMEFTd6General::cQQ1_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47201 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    comb = 2.0 * getSMEFTCoeff("Cqq1R", 2, 2, 2, 2, mu) - (2.0/3.0) * getSMEFTCoeff("Cqq3R", 2, 2, 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ cQq31_TWG()

const double NPSMEFTd6General::cQq31_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47251 of file NPSMEFTd6General.cpp.

                                                              {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = getSMEFTCoeff("Cqq3R", 0, 0, 2, 2, mu) + (1.0/6.0) * ( getSMEFTCoeff("Cqq1R", 0, 2, 2, 0, mu) - getSMEFTCoeff("Cqq3R", 0, 2, 2, 0, mu) );
  
    return (toTeVm2 * comb);
}

◆ cQq38_TWG()

const double NPSMEFTd6General::cQq38_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47262 of file NPSMEFTd6General.cpp.

                                                              {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = getSMEFTCoeff("Cqq1R", 0, 2, 2, 0, mu) - getSMEFTCoeff("Cqq3R", 0, 2, 2, 0, mu);
  
    return (toTeVm2 * comb);
}

◆ cQQ8_TWG()

const double NPSMEFTd6General::cQQ8_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47211 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    comb = 8.0 * getSMEFTCoeff("Cqq3R", 2, 2, 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ cQt1_TWG()

const double NPSMEFTd6General::cQt1_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47231 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    comb = getSMEFTCoeff("Cqu1R", 2, 2, 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ cQt8_TWG()

const double NPSMEFTd6General::cQt8_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47241 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    comb = getSMEFTCoeff("Cqu8R", 2, 2, 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ cQu1_TWG()

const double NPSMEFTd6General::cQu1_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47295 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = getSMEFTCoeff("Cqu1R", 2, 2, 0, 0, mu);
  
    return (toTeVm2 * comb);
}

◆ cQu8_TWG()

const double NPSMEFTd6General::cQu8_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47306 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = getSMEFTCoeff("Cqu8R", 2, 2, 0, 0, mu);
  
    return (toTeVm2 * comb);
}

◆ ctd1_TWG()

const double NPSMEFTd6General::ctd1_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47383 of file NPSMEFTd6General.cpp.

                                                             {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = getSMEFTCoeff("Cud1R", 2, 2, 0, 0, mu);
  
    return (toTeVm2 * comb);
}

◆ ctd8_TWG()

const double NPSMEFTd6General::ctd8_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47394 of file NPSMEFTd6General.cpp.

                                                             {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = getSMEFTCoeff("Cud8R", 2, 2, 0, 0, mu);
  
    return (toTeVm2 * comb);
}

◆ cte_TWG()

const double NPSMEFTd6General::cte_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47596 of file NPSMEFTd6General.cpp.

                                                            {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    // Take first family for leptons
    comb = getSMEFTCoeff("CeuR", 0, 0, 2, 2, mu);
    
    return (toTeVm2 * comb);
}

◆ ctG_TWG()

const double NPSMEFTd6General::ctG_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47519 of file NPSMEFTd6General.cpp.

                                                            {
 
    double comb;
    double toTeVm2 = 1000000.; 
 
    // Minus sign because of difference in covariant derivative convention of Top WG        
    comb = - getSMEFTCoeff("CuGR", 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ ctH_TWG()

const double NPSMEFTd6General::ctH_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47405 of file NPSMEFTd6General.cpp.

                                                            {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    comb = getSMEFTCoeff("CuHR", 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ ctl_TWG()

const double NPSMEFTd6General::ctl_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47585 of file NPSMEFTd6General.cpp.

                                                            {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // Take first family for leptons
    comb = getSMEFTCoeff("CluR", 0, 0, 2, 2, mu);
   
    return (toTeVm2 * comb);
}

◆ ctlS_TWG()

const double NPSMEFTd6General::ctlS_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47607 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // Take first family for leptons
    comb = getSMEFTCoeff("Clequ1R", 0, 0, 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ ctlT_TWG()

const double NPSMEFTd6General::ctlT_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47618 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // Take first family for leptons
    comb = getSMEFTCoeff("Clequ3R", 0, 0, 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ ctq1_TWG()

const double NPSMEFTd6General::ctq1_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47339 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = getSMEFTCoeff("Cqu1R", 0, 0, 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ ctq8_TWG()

const double NPSMEFTd6General::ctq8_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47350 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = getSMEFTCoeff("Cqu8R", 0, 0, 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ ctt1_TWG()

const double NPSMEFTd6General::ctt1_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47221 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    comb = getSMEFTCoeff("CuuR", 2, 2, 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ ctu1_TWG()

const double NPSMEFTd6General::ctu1_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47361 of file NPSMEFTd6General.cpp.

                                                             {
    
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = getSMEFTCoeff("CuuR", 0, 0, 2, 2, mu) + getSMEFTCoeff("CuuR", 0, 2, 2, 0, mu)/3.0;
  
    return (toTeVm2 * comb);
}

◆ ctu8_TWG()

const double NPSMEFTd6General::ctu8_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47372 of file NPSMEFTd6General.cpp.

                                                             {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    // LHC Top WG uses U(2)^3 for quarks. Here take i=0 (1st family)
    comb = 2.0 * getSMEFTCoeff("CuuR", 0, 2, 2, 0, mu);
  
    return (toTeVm2 * comb);
}

◆ ctW_TWG()

const double NPSMEFTd6General::ctW_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47475 of file NPSMEFTd6General.cpp.

                                                            {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    // Minus sign because of difference in covariant derivative convention of Top WG
    comb = - getSMEFTCoeff("CuWR", 2, 2, mu);
  
    return (toTeVm2 * comb);
}

◆ ctZ_TWG()

const double NPSMEFTd6General::ctZ_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47497 of file NPSMEFTd6General.cpp.

                                                            {
 
    double comb;
    double toTeVm2 = 1000000.; 
    
    // Minus sign because of difference in covariant derivative convention of Top WG
    comb = - ( - sW_tree * getSMEFTCoeff("CuBR", 2, 2, mu) + cW_tree * getSMEFTCoeff("CuWR", 2, 2, mu) );
  
    return (toTeVm2 * comb);
}

◆ cZBox_HB()

const double NPSMEFTd6General::cZBox_HB ( const double mu ) const

virtual

The Higgs-basis coupling $c_{z\Box}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $c_{z\Box}$

Reimplemented from NPbase.

Definition at line 43174 of file NPSMEFTd6General.cpp.

                                                             {
    double d_GF_mu;
    double ciHB;
    
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
 
    ciHB = (sW2_tree / eeMz2)*(d_GF_mu + 0.5 * getSMEFTCoeff("CHD", mu) * v2);
 
    return ciHB;
}

◆ cZga_HB()

const double NPSMEFTd6General::cZga_HB ( const double mu ) const

virtual

The Higgs-basis coupling $c_{z\gamma}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $c_{z\gamma}$

Reimplemented from NPbase.

Definition at line 43193 of file NPSMEFTd6General.cpp.

                                                            {
    double ciHB;
 
    ciHB = (sW2_tree * cW2_tree / eeMz2)*(4.0 * getSMEFTCoeff("CHW", mu) - 4.0 * getSMEFTCoeff("CHB", mu) - (2.0 * (cW2_tree - sW2_tree) / sW_tree / cW_tree) * getSMEFTCoeff("CHWB", mu)) * v2;
 
    return ciHB;
}

◆ cZZ_HB()

const double NPSMEFTd6General::cZZ_HB ( const double mu ) const

virtual

The Higgs-basis coupling $c_{zz}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $c_{zz}$

Reimplemented from NPbase.

Definition at line 43185 of file NPSMEFTd6General.cpp.

                                                           {
    double ciHB;
 
    ciHB = (4.0 * sW2_tree * cW2_tree / eeMz2)*(cW2_tree * getSMEFTCoeff("CHW", mu) + sW2_tree * getSMEFTCoeff("CHB", mu) + sW_tree * cW_tree * getSMEFTCoeff("CHWB", mu)) * v2;
 
    return ciHB;
}

◆ Dalpha5hMz()

const double NPSMEFTd6General::Dalpha5hMz ( ) const

virtual

The 5-quark contribution to the running of the em constant to the $Z$ pole. $\Delta\alpha_{had}^{(5)}(M_Z)$.

Returns: $\Delta\alpha_{had}^{(5)}(M_Z)$

Reimplemented from NPbase.

Definition at line 15575 of file NPSMEFTd6General.cpp.

                                                {
    
    double deltaNLO, alphaZ;
    
    alphaZ = trueSM.alphaMz();
    
    // Finite NLO corrections in W mass scheme
    deltaNLO = cWsch * (-0.000072 * getSMEFTCoeffEW("CW")  -0.000016 * getSMEFTCoeffEW("CHbox")  -0.000478 * getSMEFTCoeffEW("CHD")  -0.000014 * getSMEFTCoeffEW("CHB")   
            -0.000017 * getSMEFTCoeffEW("CHW")  -0.00081 * getSMEFTCoeffEW("CHWB")  -0.000144 * getSMEFTCoeffEW("CuWR",2, 2) -0.000438 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.00003 * getSMEFTCoeffEW("CHl1R",0, 0) -0.00003 * getSMEFTCoeffEW("CHl1R",1, 1) -0.000023 * getSMEFTCoeffEW("CHl1R",2, 2) -0.000672 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.000672 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000014 * getSMEFTCoeffEW("CHl3R",2, 2) -0.000023 * getSMEFTCoeffEW("CHeR",0, 0) -0.000023 * getSMEFTCoeffEW("CHeR",1, 1)  
            -0.000023 * getSMEFTCoeffEW("CHeR",2, 2) +0.000023 * getSMEFTCoeffEW("CHq1R",0, 0) +0.000023 * getSMEFTCoeffEW("CHq1R",1, 1) -0.001004 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.000043 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000043 * getSMEFTCoeffEW("CHq3R",1, 1) +0.000584 * getSMEFTCoeffEW("CHq3R",2, 2) +0.000045 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.000045 * getSMEFTCoeffEW("CHuR",1, 1) +0.001179 * getSMEFTCoeffEW("CHuR",2, 2) -0.000023 * getSMEFTCoeffEW("CHdR",0, 0) -0.000023 * getSMEFTCoeffEW("CHdR",1, 1)  
            -0.000023 * getSMEFTCoeffEW("CHdR",2, 2) -0.000128 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.000495 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) +0.00011 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
            +0.00011 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) ) * v2; 
    
    return (trueSM.Dalpha5hMz() + (ale/alphaZ) * ( 2.0 * delta_e + delta_A + cNLOd6 * deltaNLO / alphaZ ) );
}

◆ del_A_mu()

const double NPSMEFTd6General::del_A_mu ( const double mu ) const

virtual

Correction to photon WF.

Parameters

[in] mu the RG scale associated to the observable where the function is used

Returns: $\delta A(\mu)$

Definition at line 15334 of file NPSMEFTd6General.cpp.

                                                             {
    double d_A_mu;
    
    // Same expressions as in PostUpdate, with scale dependence (on NP only)
    d_A_mu = -2.0 * sW_tree * cW_tree * getSMEFTCoeff("CHWB", mu) * v2;
 
    return d_A_mu;    
}

◆ del_e_mu()

const double NPSMEFTd6General::del_e_mu ( const double mu ) const

virtual

Correction to electric charge.

Parameters

[in] mu the RG scale associated to the observable where the function is used

Returns: $\delta e(\mu)$

Definition at line 15362 of file NPSMEFTd6General.cpp.

                                                             {
    double d_MW_mu, d_MZ_mu, d_GF_mu, d_e_mu;
    
    // Same expressions as in PostUpdate, with scale dependence (on NP only)
    d_MW_mu = (3.0 / 8.0) * (getSMEFTCoeff("CH", mu) / lambdaH_tree) * v2;
    d_MZ_mu = (sW_tree * cW_tree * getSMEFTCoeff("CHWB", mu) + 0.25 * getSMEFTCoeff("CHD", mu) + (3.0 / 8.0) * getSMEFTCoeff("CH", mu) / lambdaH_tree) * v2;
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
    
    d_e_mu = cAsch * (-0.5 * del_A_mu(mu))
            + cWsch * ((cW2_tree / sW2_tree) * (d_MW_mu - d_MZ_mu) - 0.5 * d_GF_mu);
 
    return d_e_mu;
}

◆ del_sW2_mu()

const double NPSMEFTd6General::del_sW2_mu ( const double mu ) const

virtual

Correction to (sin squared of) weak mixing angle.

Parameters

[in] mu the RG scale associated to the observable where the function is used

Returns: $\delta s_W^2(\mu)$

Definition at line 15376 of file NPSMEFTd6General.cpp.

                                                               {
    double d_GF_mu, d_MW_mu, d_MZ_mu, d_sW2_mu;
    
    // Same expressions as in PostUpdate, with scale dependence (on NP only)
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
    d_MW_mu = (3.0 / 8.0) * (getSMEFTCoeff("CH", mu) / lambdaH_tree) * v2;
    d_MZ_mu = (sW_tree * cW_tree * getSMEFTCoeff("CHWB", mu) + 0.25 * getSMEFTCoeff("CHD", mu) + (3.0 / 8.0) * getSMEFTCoeff("CH", mu) / lambdaH_tree) * v2;
    
    d_sW2_mu = cAsch * (-cW2_tree * (d_GF_mu - 2.0 * (d_MW_mu - d_MZ_mu) - del_A_mu(mu)) / (sW2_tree - cW2_tree))
            + cWsch * (2.0 * cW2_tree * (d_MW_mu - d_MZ_mu) / sW2_tree);
    
    return d_sW2_mu;    
}

◆ del_Z_mu()

const double NPSMEFTd6General::del_Z_mu ( const double mu ) const

virtual

Correction to Z WF.

Parameters

[in] mu the RG scale associated to the observable where the function is used

Returns: $\delta Z(\mu)$

Definition at line 15343 of file NPSMEFTd6General.cpp.

                                                             {
    double d_Z_mu;
    
    // Same expressions as in PostUpdate, with scale dependence (on NP only)
    d_Z_mu = 2.0 * sW_tree * cW_tree * getSMEFTCoeff("CHWB", mu) * v2; 
    
    return d_Z_mu;
}

◆ del_ZA_mu()

const double NPSMEFTd6General::del_ZA_mu ( const double mu ) const

virtual

Correction to Z-A mixing.

Parameters

[in] mu the RG scale associated to the observable where the function is used

Returns: $\delta ZA(\mu)$

Definition at line 15352 of file NPSMEFTd6General.cpp.

                                                              {
    double d_ZA_mu;
    
    // Same expressions as in PostUpdate, with scale dependence (on NP only)
    d_ZA_mu = (cW2_tree - sW2_tree) * getSMEFTCoeff("CHWB", mu) * v2;
    
    return d_ZA_mu;
}

◆ delQ_gNC()

const double NPSMEFTd6General::delQ_gNC ( const double mu ) const

virtual

Separate, charge-proportional, indirect correction to EW neutral currents.

Parameters

[in] mu the RG scale associated to the observable where the function is used

Returns: $\delta g_{NC}^{Q}(\mu)$

Definition at line 15409 of file NPSMEFTd6General.cpp.

                                                             {
    
    double dg;
    
    // Same expressions as in PostUpdate, with scale dependence (on NP only)
    dg = -(sW_tree * cW_tree * del_ZA_mu(mu) + sW2_tree * del_sW2_mu(mu));
    
    return dg;
}

◆ delta2sBRH3()

const double NPSMEFTd6General::delta2sBRH3	(	const double	C1prod,
		const double	C1Hxx
	)		const

virtual

Quadratic contribution from the Higgs self-couplings modifications to the signal strength for $\sigma \times BR(H\to xx)$ in the current model.

Returns: $\delta^{(2)}_{h^3}$

Reimplemented from NPbase.

Definition at line 15310 of file NPSMEFTd6General.cpp.

{
    double delta2;
    
    delta2 = deltaH3L2(C1prod) + deltaH3L2(C1Hxx) - deltaH3L2(C1Htotal);
    
    // Extra contributions from the product and branching ratio. Only active depending on the flags
    delta2 += cLHd6 * cLH3d62 * (C1Htotal - C1Hxx) * (C1Htotal - C1prod) / (1.0 + C1Htotal) / (1.0 + C1Htotal) / (1.0 + C1Hxx) / (1.0 + C1prod);
    
    // Add the quadratic dependence
    delta2 = delta2 * deltaG_hhhRatio() * deltaG_hhhRatio();
 
    return delta2;
}

◆ delta2sH3()

const double NPSMEFTd6General::delta2sH3 ( const double C1 ) const

virtual

Quadratic contribution from the Higgs self-couplings modifications to the signal strength for an observable $\sigma$ in the current model.

Returns: $\delta^{(2)}_{h^3}$

Reimplemented from NPbase.

Definition at line 15298 of file NPSMEFTd6General.cpp.

{
    double delta2;
    
    delta2 = deltaH3L2(C1);
    
    // Add the quadratic dependence. Only active depending on the flags
    delta2 = cLHd6 * cLH3d62 * delta2 * deltaG_hhhRatio() * deltaG_hhhRatio();
 
    return delta2;
}

◆ delta_AFB_ee()

const double NPSMEFTd6General::delta_AFB_ee	(	const double	pol_e,
		const double	pol_p,
		const double	s
	)		const

virtual

Definition at line 46904 of file NPSMEFTd6General.cpp.

                                                                                                        {
 
    double coscut = 0.90; // As in LEP2  
    double xsSMF, xsSMB, xsSM;
    double dxsF, dxsB, dxs;
    double dAFB;
    
    // SM cross sections
    xsSM = trueSM.eeffsigmaEbin(pol_e, pol_p, s, -coscut, coscut);
    xsSMF = trueSM.eeffsigmaEbin(pol_e, pol_p, s, 0.0, coscut);
    xsSMB = trueSM.eeffsigmaEbin(pol_e, pol_p, s, -coscut, 0.0);
    
    // Corrections to each
    dxs = delta_sigma_ee(pol_e, pol_p, s, -coscut, coscut);
    dxsF = delta_sigma_ee(pol_e, pol_p, s, 0.0, coscut);
    dxsB = delta_sigma_ee(pol_e, pol_p, s, -coscut, 0.0);
 
    // Correction to asymmetry
    dAFB = (dxsF - dxsB)/xsSM - (xsSMF - xsSMB)*dxs/xsSM/xsSM;
    
    return dAFB;
}

◆ delta_AFB_f()

const double NPSMEFTd6General::delta_AFB_f	(	const Particle	f,
		const double	pol_e,
		const double	pol_p,
		const double	s
	)		const

virtual

Definition at line 46585 of file NPSMEFTd6General.cpp.

                                                                                                                         {
    //  Only valid for f=/=e (MLL2, MRR2 do not depend on t for f=/=e. Simply enter t=1 as argument)
    double tdumm = 1.;
 
    // Definitions      
    double Qf, geLSM, gfLSM, geRSM, gfRSM, is2c2, GZ, Mz2s;
 
    //double MXX2SM, MXY2SM, M2SM;
    
    double MLR2SM, MRL2SM, MLL2SM, MRR2SM, numdA, dendA;
 
    double dAFB;
    
    double pLH, pRH; //Polarization factors, minus the 1/4 average
    
    pLH = (1.0 - pol_e) * (1.0 + pol_p);
    pRH = (1.0 + pol_e) * (1.0 - pol_p);
 
    // -------------------------------------------
 
    geLSM = gZlL;
    geRSM = gZlR;
 
    is2c2 = 1. / sW2_tree / cW2_tree;
 
    GZ = trueSM.Gamma_Z();
 
    Mz2s = Mz * Mz - s;
 
    switch(f.getIndex()){
    //if (f.is("MU")) {
        case 3:
        Qf = leptons[ELECTRON].getCharge();
        gfLSM = gZlL;
        gfRSM = gZlR;
        break;
    //} else if (f.is("TAU")) {
        case 5:
        Qf = leptons[ELECTRON].getCharge();
        gfLSM = gZlL;
        gfRSM = gZlR;
        break;
    //} else if (f.is("UP")) {
        case 6:
        Qf = quarks[UP].getCharge();
        gfLSM = gZuL;
        gfRSM = gZuR;
        break;
    //} else if (f.is("CHARM")) {
        case 8:
        Qf = quarks[UP].getCharge();
        gfLSM = gZuL;
        gfRSM = gZuR;
        break;
    //} else if (f.is("DOWN")) {
        case 7:
        Qf = quarks[DOWN].getCharge();
        gfLSM = gZdL;
        gfRSM = gZdR;
        break;
    //} else if (f.is("STRANGE")) {
        case 9:
        Qf = quarks[DOWN].getCharge();
        gfLSM = gZdL;
        gfRSM = gZdR;
        break;
    //} else if (f.is("BOTTOM")) {
        case 11:
        Qf = quarks[DOWN].getCharge();
        gfLSM = gZdL;
        gfRSM = gZdR;
        break;
        default:            
        throw std::runtime_error("NPSMEFTd6General::delta_AFB_f(): wrong argument");
    }
 
    // Sum of LL and RR SM amplitudes
    //MXX2SM = 2.0 * Qf * Qf
    //        + (is2c2 * is2c2 * (geLSM * geLSM * gfLSM * gfLSM + geRSM * geRSM * gfRSM * gfRSM) * s * s
    //        + 2.0 * Qf * is2c2 * (geLSM * gfLSM + geRSM * gfRSM) * Mz2s * s) / (Mz2s * Mz2s + Mz * Mz * GZ * GZ);
 
 
    // Sum of LR and RL SM amplitudes
    //MXY2SM = 2.0 * Qf * Qf
    //        + (is2c2 * is2c2 * (geLSM * geLSM * gfRSM * gfRSM + geRSM * geRSM * gfLSM * gfLSM) * s * s
    //        + 2.0 * Qf * is2c2 * (geLSM * gfRSM + geRSM * gfLSM) * Mz2s * s) / (Mz2s * Mz2s + Mz * Mz * GZ * GZ);
 
    // Full SM amplitude
    //M2SM = MXX2SM + MXY2SM;
    
    // LR, RL, LL and RR SM squared amplitudes
    MLR2SM = Qf * Qf
            + (is2c2 * is2c2 * (geLSM * geLSM * gfRSM * gfRSM) * s * s
            + 2.0 * Qf * is2c2 * (geLSM * gfRSM) * Mz2s * s) / (Mz2s * Mz2s + Mz * Mz * GZ * GZ);
    
    MRL2SM = Qf * Qf
            + (is2c2 * is2c2 * (geRSM * geRSM * gfLSM * gfLSM) * s * s
            + 2.0 * Qf * is2c2 * (geRSM * gfLSM) * Mz2s * s) / (Mz2s * Mz2s + Mz * Mz * GZ * GZ); 
    
    MLL2SM = Qf * Qf
            + (is2c2 * is2c2 * (geLSM * geLSM * gfLSM * gfLSM) * s * s
            + 2.0 * Qf * is2c2 * (geLSM * gfLSM) * Mz2s * s) / (Mz2s * Mz2s + Mz * Mz * GZ * GZ); 
    
    MRR2SM = Qf * Qf
            + (is2c2 * is2c2 * (geRSM * geRSM * gfRSM * gfRSM) * s * s
            + 2.0 * Qf * is2c2 * (geRSM * gfRSM) * Mz2s * s) / (Mz2s * Mz2s + Mz * Mz * GZ * GZ); 
    
    numdA = 3.0 * ( -( MRR2SM * pRH + MLL2SM * pLH ) * ( pLH * deltaMLR2_f(f, s) + pRH * deltaMRL2_f(f, s) ) 
            + ( MRL2SM * pRH + MLR2SM * pLH ) * ( pLH * deltaMLL2_f(f, s, tdumm) + pRH * deltaMRR2_f(f, s, tdumm) ) );
            
    dendA = ((MRL2SM + MRR2SM) * pRH + (MLL2SM + MLR2SM) * pLH);
    
    dendA = 2.0 * dendA * dendA;
    
    // Asymmetry correction 
    //dAFB = -MXX2SM * (deltaMLR2_f(f, s) + deltaMRL2_f(f, s))
    //        + MXY2SM * (deltaMLL2_f(f, s, tdumm) + deltaMRR2_f(f, s, tdumm));
 
    //dAFB = 3.0 * dAFB / 2.0 / M2SM / M2SM;
    
    dAFB = numdA/dendA;
 
    return dAFB;
}

◆ delta_alrmoller()

const double NPSMEFTd6General::delta_alrmoller	(	const double	q2,
		const double	y
	)		const

virtual

The computation of the parity violating asymmetry in Moller scattering.

Parameters

[in]	q2	the $Q^2$ of the process
[in]	y

Returns: $A_{LR}$

Definition at line 46969 of file NPSMEFTd6General.cpp.

                                                                                    {
    return 0.;
}

◆ delta_amuon()

const double NPSMEFTd6General::delta_amuon ( ) const

virtual

The computation of the anomalous magnetic moment of the muon $a_\mu=(g_\mu-2)/2$.

Returns: $a_\mu=(g_\mu-2)/2$

Definition at line 46934 of file NPSMEFTd6General.cpp.

                                                 {
    return 0.;
}

◆ delta_Dsigma_f()

const double NPSMEFTd6General::delta_Dsigma_f	(	const Particle	f,
		const double	pol_e,
		const double	pol_p,
		const double	s,
		const double	cos
	)		const

virtual

Definition at line 46501 of file NPSMEFTd6General.cpp.

                                                                                                                                              {
    double sumM2, dsigma;
    double topb = 0.3894e+9;
 
    double t, u;
 
    double Nf;
    
    double pLH, pRH; //Polarization factors, minus the 1/4 average
    double pLLH, pRRH; 
    
    pLH = (1.0 - pol_e) * (1.0 + pol_p);
    pRH = (1.0 + pol_e) * (1.0 - pol_p);
    
    pLLH = (1.0 - pol_e) * (1.0 - pol_p);
    pRRH = (1.0 + pol_e) * (1.0 + pol_p);
 
    //if (f.is("LEPTON")) {
    if ( f.getIndex() < 6 ) {
        Nf = 1.0;
    } else {
        Nf = 3.0;
    }
 
    // Values of t and u, assuming massless final state fermions
    t = -0.5 * s * (1.0 - cos);
    u = -0.5 * s * (1.0 + cos);
 
    sumM2 = (pLH * deltaMLR2_f(f, s) + pRH * deltaMRL2_f(f, s)) * t * t / s / s
            + (pLH * deltaMLL2_f(f, s, t) + pRH * deltaMRR2_f(f, s, t)) * u * u / s / s;
 
    // Add t-channel contributions for f=e
    //if (f.is("ELECTRON")) {
    if ( f.getIndex() == 1 ) {
        sumM2 = sumM2 + (pLLH * deltaMLR2t_e(s,t) + pRRH * deltaMRL2t_e(s,t)) * s * s / t / t;
    }
 
    dsigma = Nf * 0.5 * M_PI * (trueSM.alphaMz())*(trueSM.alphaMz()) * sumM2 / s;
 
    return topb * dsigma;
}

◆ delta_gAnue()

const double NPSMEFTd6General::delta_gAnue ( ) const

virtual

The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gAnue.

Returns: $\Delta g_A^{\nu_\mu e}$

Definition at line 47083 of file NPSMEFTd6General.cpp.

                                                 {
    double dCnueVLL2211, dCnueVLR2211, delta;
 
    dCnueVLL2211 = (getMatching().getCnueVLL(1, 1, 0, 0)).real();
    dCnueVLR2211 = (getMatching().getCnueVLR(1, 1, 0, 0)).real();
 
    // Modification in terms of the LEFT basis (at low energies)        
    delta = (-1. / GF / 2. / sqrt(2.)) * (dCnueVLL2211 - dCnueVLR2211);
 
    return delta;
}

◆ delta_gLnuN2()

const double NPSMEFTd6General::delta_gLnuN2 ( ) const

virtual

The computation of the correction to the effective neutrino nucleon LH coupling: delta_gLnuN2.

Returns: $\Delta g_L^2(\nu N)$

Definition at line 47027 of file NPSMEFTd6General.cpp.

                                                  {
    double eLuSM, eLdSM, deLu, deLd;
    double dFCC, Vud;
    double delta;
 
    // SM vvqq couplings (up to -4GF/sqrt(2))
    eLuSM = 2.0 * gZvL*gZuL;
    eLdSM = 2.0 * gZvL*gZdL;
 
    // Scattering is with muon neutrinos -> only (22) interfere
    deLu = (-1. / GF / 2. / sqrt(2.)) * (getMatching().getCnuuVLL(1, 1, 0, 0)).real();
    deLd = (-1. / GF / 2. / sqrt(2.)) * (getMatching().getCnudVLL(1, 1, 0, 0)).real();
 
    Vud = 0.97373; // PDG 2023
 
    dFCC = 2.0 * (-sqrt(2.0) / 4 / GF) * ((getMatching().getCnueduVLL(1, 1, 0, 0)) / Vud).real();
 
    delta = 2.0 * (eLuSM * deLu + eLdSM * deLd) + (trueSM.gLnuN2())*(-dFCC);
 
    return delta;
}

◆ delta_gRnuN2()

const double NPSMEFTd6General::delta_gRnuN2 ( ) const

virtual

The computation of the correction to the effective neutrino nucleon RH coupling: delta_gRnuN2.

Returns: $\Delta g_R^2(\nu N)$

Definition at line 47049 of file NPSMEFTd6General.cpp.

                                                  {
    double eRuSM, eRdSM, deRu, deRd;
    double dFCC, Vud;
    double delta;
 
    // SM vvqq couplings (up to -4GF/sqrt(2))
    eRuSM = 2.0 * gZvL*gZuR;
    eRdSM = 2.0 * gZvL*gZdR;
 
    // Scattering is with muon neutrinos -> only (22) interfere
    deRu = (-1. / GF / 2. / sqrt(2.)) * (getMatching().getCnuuVLR(1, 1, 0, 0)).real();
    deRd = (-1. / GF / 2. / sqrt(2.)) * (getMatching().getCnudVLR(1, 1, 0, 0)).real();
 
    Vud = 0.97373; // PDG 2023
 
    dFCC = 2.0 * (-sqrt(2.0) / 4 / GF) * ((getMatching().getCnueduVLL(1, 1, 0, 0)) / Vud).real();
 
    delta = 2.0 * (eRuSM * deRu + eRdSM * deRd) + (trueSM.gRnuN2())*(-dFCC);
 
    return delta;
}

◆ delta_gVnue()

const double NPSMEFTd6General::delta_gVnue ( ) const

virtual

The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gVnue.

Returns: $\Delta g_V^{\nu_\mu e}$

Definition at line 47071 of file NPSMEFTd6General.cpp.

                                                 {
    double dCnueVLL2211, dCnueVLR2211, delta;
 
    dCnueVLL2211 = (getMatching().getCnueVLL(1, 1, 0, 0)).real();
    dCnueVLR2211 = (getMatching().getCnueVLR(1, 1, 0, 0)).real();
 
    // Modification in terms of the LEFT basis (at low energies)        
    delta = (-1. / GF / 2. / sqrt(2.)) * (dCnueVLL2211 + dCnueVLR2211);
 
    return delta;
}

◆ delta_mubbH_1()

virtual const double NPSMEFTd6General::delta_mubbH_1 ( const double sqrt_s ) const

inlinevirtual

The SMEFT linear correction to the ratio $\mu_{bbH}$ between the bbH production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 2247 of file NPSMEFTd6General.h.

◆ delta_mubbH_2()

virtual const double NPSMEFTd6General::delta_mubbH_2 ( const double sqrt_s ) const

inlinevirtual

The SMEFT quadratic correction to the ratio $\mu_{bbH}$ between the bbH production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 2251 of file NPSMEFTd6General.h.

◆ delta_muggH_1()

const double NPSMEFTd6General::delta_muggH_1 ( const double sqrt_s ) const

virtual

The SMEFT linear correction to the ratio $\mu_{ggH}$ between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 17904 of file NPSMEFTd6General.cpp.

                                                                      {
    double mu = 0.0;
    double C1 = 0.0066; //It seems to be independent of energy 
    
    double CHG = 0.0, CDH = 0.0, CHD = 0.0, CuHR33 = 0.0, CtGR = 0.0, CHl3R11 = 0.0, CHl3R22 = 0.0, Cll1221 = 0.0; 
    double muRG = 125.1;
    
//  Wilson coefficients definitions 
    CHG = getSMEFTCoeff("CHG",muRG); 
    CDH = getSMEFTCoeff("CHbox",muRG); 
    CHD = getSMEFTCoeff("CHD",muRG); 
    CuHR33 = getSMEFTCoeff("CuHR",2,2,muRG); 
    CtGR = (getSMEFTCoeff("CuGR",2,2,muRG) / g3_tree); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0,muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1,muRG); 
    Cll1221 = getSMEFTCoeff("CllR",0,1,1,0,muRG); 
 
    /*
    double m_t = mtpole;
    //double m_t = quarks[TOP].getMass();
    double m_b = quarks[BOTTOM].getMass();
    double m_c = quarks[CHARM].getMass();
 
    // L_eff_SM = (G_eff_t_SM + G_eff_b_SM)*hGG 
    gslpp::complex G_eff_t_SM = AlsMz / 16.0 / M_PI / v() * AH_f(4.0 * m_t * m_t / mHl / mHl);
    gslpp::complex G_eff_b_SM = AlsMz / 16.0 / M_PI / v() * AH_f(4.0 * m_b * m_b / mHl / mHl);
    gslpp::complex G_eff_c_SM = AlsMz / 16.0 / M_PI / v() * AH_f(4.0 * m_c * m_c / mHl / mHl);
    gslpp::complex G_eff_SM = G_eff_t_SM + G_eff_b_SM + G_eff_c_SM;
 
    //double sigma_tt_SM = trueSM.computeSigmaggH_tt(sqrt_s);
    //double sigma_bb_SM = trueSM.computeSigmaggH_bb(sqrt_s);
    //double sigma_tb_SM = trueSM.computeSigmaggH_tb(sqrt_s);
    //gslpp::complex tmp = (2.0 * dKappa_t * sigma_tt_SM
    //        + 2.0 * dKappa_b * sigma_bb_SM
    //        + (dKappa_t + dKappa_b) * sigma_tb_SM)
    //        / (sigma_tt_SM + sigma_bb_SM + sigma_tb_SM);
 
    gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
    gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
    gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
 
    gslpp::complex tmpHG = getSMEFTCoeffEW("CHG") / v() * v2 / G_eff_SM;
    gslpp::complex tmpt = G_eff_t_SM * dKappa_t / G_eff_SM;
    gslpp::complex tmpb = G_eff_b_SM * dKappa_b / G_eff_SM;
    gslpp::complex tmpc = G_eff_c_SM * dKappa_c / G_eff_SM;
 
    double mu = (1.0 + 2.0 * (tmpt.real() + tmpb.real() + tmpc.real() + tmpHG.real()));*/
 
    //AG:
    // Obtained with SMEFETatNLO. cuG_Warsaw = g3_tree*cuG_SMEFTatNLO    
    if (sqrt_s == 8.0) {
        //mu += cWsch * (   // Same for alpha & MW scheme at LO
        mu += (
                ((0.12124142781783014) * getSMEFTCoeffEW("CHbox")
                + (-0.030314752945313873) * getSMEFTCoeffEW("CHD")
                + (39.31144) * getSMEFTCoeffEW("CHG") //
                + (-0.1224898892210304) * getSMEFTCoeffEW("CuHR", 2, 2)
                - (1.1269562159310709) * getSMEFTCoeffEW("CuGR", 2, 2) * g3_tree
                + (-0.060629505890627745) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.060629505890627745) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.060629505890627745) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
    } else if (sqrt_s == 13.0) {
        //mu += cWsch * (   // Same for alpha & MW scheme at LO
        mu +=  (
                ((0.121) * getSMEFTCoeffEW("CHbox")
                + (-0.03031) * getSMEFTCoeffEW("CHD")
                + (39.31144) * getSMEFTCoeffEW("CHG")
                + (-0.12245) * getSMEFTCoeffEW("CuHR", 2, 2)
                - (1.127) * getSMEFTCoeffEW("CuGR", 2, 2) * g3_tree
                + (-0.06062) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.06062) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0606) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
    } else if (sqrt_s == 14.0) {
        //mu += cWsch * (   // Same for alpha & MW scheme at LO
        mu +=  (
                +34861157. * CHG 
                +121542. * CDH 
                -30260.6 * CHD 
                -121842. * CuHR33 
                -1577851. * CtGR 
                -60687.9 * (CHl3R11 + CHl3R22 - Cll1221)  
                );
    } else if (sqrt_s == 50.0) {
        //mu += cWsch * (   // Same for alpha & MW scheme at LO
        mu +=  (
                +34861330. * CHG 
                +121551. * CDH 
                -30261.2 * CHD 
                -121874. * CuHR33 
                -1577818. * CtGR 
                -60706.6 * (CHl3R11 + CHl3R22 - Cll1221)
                );
    } else if (sqrt_s == 84.0) {
        //mu += cWsch * (   // Same for alpha & MW scheme at LO
        mu +=  (
                +34860509. * CHG 
                +121540. * CDH 
                -30278.6 * CHD 
                -121876. * CuHR33 
                -1577893. * CtGR 
                -60714. * (CHl3R11 + CHl3R22 - Cll1221)
                );
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::delta_muggH_1()");
    //AG:end
 
    //  Linear contribution from Higgs self-coupling
    mu += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    return mu;
}

◆ delta_muggH_2()

const double NPSMEFTd6General::delta_muggH_2 ( const double sqrt_s ) const

virtual

The SMEFT quadratic correction to the ratio $\mu_{ggH}$ between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 18019 of file NPSMEFTd6General.cpp.

                                                                      {
    double mu = 0.0;
 
    if (FlagQuadraticTerms) {
        if (sqrt_s == 8.0) {
            mu += 0.0;
        } else if (sqrt_s == 13.0) {
            mu += 0.0;
        } else
            throw std::runtime_error("Bad argument in NPSMEFTd6General::delta_muggH_2()");
    }
 
    //  Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
    //  mu = mu + cLHd6 * cLH3d62 * deltaH3L2(C1) * deltaG_hhhRatio() * deltaG_hhhRatio();
 
    return mu;
}

◆ delta_mutH_1()

const double NPSMEFTd6General::delta_mutH_1 ( const double sqrt_s ) const

virtual

The SMEFT linear correction to the ratio $\mu_{tH}$ between the t-Higgs associated production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 20097 of file NPSMEFTd6General.cpp.

                                                                     {
    double mu = 0.0;
    double C1 = 0.0;
 
    // Obtained with MG5 in the 5Flavor-scheme (p p > h t j)
    if (sqrt_s == 8.0) {
        C1 = 0; // to be added
        mu += cWsch * (
                ((0.12122) * getSMEFTCoeffEW("CHbox")
                + (-0.03034483) * getSMEFTCoeffEW("CHD")
                + (0.2149) * getSMEFTCoeffEW("CHW")
                + (-0.07668) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.009001) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.03961) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.043175) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (-0.500813) * getSMEFTCoeffEW("CuWR", 2, 2)
                + (-0.97677) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + (0.1629) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + (-0.079828) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                + (0.013296) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                + (-0.1822825) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1822825) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18181) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
    } else if (sqrt_s == 13.0) {
        C1 = 0.0091;
        mu += cWsch * (
                ((0.12116) * getSMEFTCoeffEW("CHbox")
                + (-0.03031732) * getSMEFTCoeffEW("CHD")
                + (0.14294) * getSMEFTCoeffEW("CHW")
                + (-0.1183) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.014446) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.05131) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.020319) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (-0.337708) * getSMEFTCoeffEW("CuWR", 2, 2)
                + (-0.67007) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + (0.11138) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + (-0.068432) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                + (0.011428) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                + (-0.1818849) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1818849) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18178) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::delta_mutH_1()");
 
    //  Linear contribution from Higgs self-coupling
    mu += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio();
 
 
    return mu;
}

◆ delta_mutH_2()

const double NPSMEFTd6General::delta_mutH_2 ( const double sqrt_s ) const

virtual

The SMEFT quadratic correction to the ratio $\mu_{tH}$ between the t-Higgs associated production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 20151 of file NPSMEFTd6General.cpp.

                                                                     {
    double mu = 0.0;
 
    if (FlagQuadraticTerms) {
        if (sqrt_s == 8.0) {
            mu += 0.0;
        } else if (sqrt_s == 13.0) {
            mu += cWsch * (
                    +(0.014714) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                    + (0.0009197) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                    + (0.10664) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                    + (0.397) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                    + (0.04262) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                    + (0.18668) * pow(getSMEFTCoeffEW("CHq3R", 2, 2), 2.0)
                    + (0.011788) * pow(getSMEFTCoeffEW("CuHR", 2, 2), 2.0)
                    + (0.7536) * pow(getSMEFTCoeffEW("CuWR", 2, 2), 2.0)
                    + (14.225) * pow(getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2), 2.0)
                    + (3.555) * pow(getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0), 2.0)
                    + (0.652) * pow(getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2), 2.0)
                    + (0.16289) * pow(getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1), 2.0)
                    + (0.010994) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                    + (-0.001836136) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                    + (0.008656) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                    + (-0.000798) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.004219) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 2, 2)
                    + (-0.0012381) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CuHR", 2, 2)
                    + (-0.0293566) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CuWR", 2, 2)
                    + (-0.01836136) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.01836136) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.01839) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.0021629) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHW")
                    + (0.0002008) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (-0.0010582) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 2, 2)
                    + (0.0003102) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CuHR", 2, 2)
                    + (0.007338) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CuWR", 2, 2)
                    + (0.0045973) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.0045973) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.00459305) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.08103) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.009231) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (0.09655) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 2, 2)
                    + (-0.0179965) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CuHR", 2, 2)
                    + (-0.188379) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CuWR", 2, 2)
                    + (-0.021629) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.021629) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.021637) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.0018) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (0.157) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 2, 2)
                    + (-0.0585129) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CuHR", 2, 2)
                    + (-0.00854) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CuWR", 2, 2)
                    + (0.011151) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.011151) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.01114) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.0194) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 2, 2)
                    + (-0.0079104) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CuHR", 2, 2)
                    + (0.004977) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CuWR", 2, 2)
                    + (0.0013522) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.0013522) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.0013467) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.0633763) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CuHR", 2, 2)
                    + (-0.089472) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CuWR", 2, 2)
                    + (0.00245) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.00245) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.00249) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.040817) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("CuWR", 2, 2)
                    + (0.003102) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.003102) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.0030947) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.04541) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.04541) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.0453941) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-4.78) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                    + (-0.05) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                    + (-0.04) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                    + (-0.01) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                    + (-0.011) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                    + (-0.216) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                    + (-0.216) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.02754112) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.02754112) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    ) * pow(1000000.0, 2.0);
 
        } else
            throw std::runtime_error("Bad argument in NPSMEFTd6General::delta_mutH_2()");
    }
 
    //  Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
    //  mu = mu + cLHd6 * cLH3d62 * deltaH3L2(C1) * deltaG_hhhRatio() * deltaG_hhhRatio();
 
    return mu;
}

◆ delta_muttH_1()

const double NPSMEFTd6General::delta_muttH_1 ( const double sqrt_s ) const

virtual

The SMEFT linear correction to the ratio $\mu_{ttH}$ between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 19244 of file NPSMEFTd6General.cpp.

                                                                      {
    double mu = 0.0;
    double C1 = 0.0;
    
    double CG = 0.0, CuHR33 = 0.0, CHq1R11 = 0.0, CHq3R11 = 0.0, CHuR11 = 0.0;
    double CHdR11 = 0.0, CHq1R22 = 0.0, CHq3R22 = 0.0, CHuR22 = 0.0, CHdR22 = 0.0;
    double CHq1R33 = 0.0, CHq3R33 = 0.0, CHuR33 = 0.0, CuGR33 = 0.0, Cqq1R1133 = 0.0;
    double Cqq1R1331 = 0.0, Cqq1R2233 = 0.0, Cqq1R2332 = 0.0, Cqq3R1133 = 0.0, Cqq3R1331 = 0.0;
    double Cqq3R2233 = 0.0, Cqq3R2332 = 0.0, CuuR1133 = 0.0, CuuR2233 = 0.0, CuuR1331 = 0.0;
    double CuuR2332 = 0.0, Cud1R3311 = 0.0, Cud1R3322 = 0.0, Cud8R3311 = 0.0, Cud8R3322 = 0.0;
    double Cqu1R1133 = 0.0, Cqu1R2233 = 0.0, Cqu1R3311 = 0.0, Cqu1R3322 = 0.0, Cqu8R1133 = 0.0;
    double Cqu8R2233 = 0.0, Cqu8R3311 = 0.0, Cqu8R3322 = 0.0, Cqd1R3311 = 0.0, Cqd1R3322 = 0.0, Cqd8R3311 = 0.0, Cqd8R3322 = 0.0; 
    double muRG = 240.;
    
//  Wilson coefficients definitions 
    CG = getSMEFTCoeff("CG", muRG); 
    CuHR33 = getSMEFTCoeff("CuHR",2,2, muRG); 
    CHq1R11 = getSMEFTCoeff("CHq1R",0,0, muRG); 
    CHq3R11 = getSMEFTCoeff("CHq3R",0,0, muRG); 
    CHuR11 = getSMEFTCoeff("CHuR",0,0, muRG); 
    CHdR11 = getSMEFTCoeff("CHdR",0,0, muRG); 
    CHq1R22 = getSMEFTCoeff("CHq1R",1,1, muRG); 
    CHq3R22 = getSMEFTCoeff("CHq3R",1,1, muRG); 
    CHuR22 = getSMEFTCoeff("CHuR",1,1, muRG); 
    CHdR22 = getSMEFTCoeff("CHdR",1,1, muRG); 
    CHq1R33 = getSMEFTCoeff("CHq1R",2,2, muRG); 
    CHq3R33 = getSMEFTCoeff("CHq3R",2,2, muRG); 
    CHuR33 = getSMEFTCoeff("CHuR",2,2, muRG); 
    CuGR33 = getSMEFTCoeff("CuGR",2,2, muRG); 
    Cqq1R1133 = getSMEFTCoeff("Cqq1R",0,0,2,2, muRG); 
    Cqq1R1331 = getSMEFTCoeff("Cqq1R",0,2,2,0, muRG); 
    Cqq1R2233 = getSMEFTCoeff("Cqq1R",1,1,2,2, muRG); 
    Cqq1R2332 = getSMEFTCoeff("Cqq1R",1,2,2,1, muRG); 
    Cqq3R1133 = getSMEFTCoeff("Cqq3R",0,0,2,2, muRG); 
    Cqq3R1331 = getSMEFTCoeff("Cqq3R",0,2,2,0, muRG); 
    Cqq3R2233 = getSMEFTCoeff("Cqq3R",1,1,2,2, muRG); 
    Cqq3R2332 = getSMEFTCoeff("Cqq3R",1,2,2,1, muRG); 
    CuuR1133 = getSMEFTCoeff("CuuR",0,0,2,2, muRG); 
    CuuR2233 = getSMEFTCoeff("CuuR",1,1,2,2, muRG); 
    CuuR1331 = getSMEFTCoeff("CuuR",0,2,2,0, muRG); 
    CuuR2332 = getSMEFTCoeff("CuuR",1,2,2,1, muRG); 
    Cud1R3311 = getSMEFTCoeff("Cud1R",2,2,0,0, muRG); 
    Cud1R3322 = getSMEFTCoeff("Cud1R",2,2,1,1, muRG); 
    Cud8R3311 = getSMEFTCoeff("Cud8R",2,2,0,0, muRG); 
    Cud8R3322 = getSMEFTCoeff("Cud8R",2,2,1,1, muRG); 
    Cqu1R1133 = getSMEFTCoeff("Cqu1R",0,0,2,2, muRG); 
    Cqu1R2233 = getSMEFTCoeff("Cqu1R",1,1,2,2, muRG); 
    Cqu1R3311 = getSMEFTCoeff("Cqu1R",2,2,0,0, muRG); 
    Cqu1R3322 = getSMEFTCoeff("Cqu1R",2,2,1,1, muRG); 
    Cqu8R1133 = getSMEFTCoeff("Cqu8R",0,0,2,2, muRG); 
    Cqu8R2233 = getSMEFTCoeff("Cqu8R",1,1,2,2, muRG); 
    Cqu8R3311 = getSMEFTCoeff("Cqu8R",2,2,0,0, muRG); 
    Cqu8R3322 = getSMEFTCoeff("Cqu8R",2,2,1,1, muRG); 
    Cqd1R3311 = getSMEFTCoeff("Cqd1R",2,2,0,0, muRG); 
    Cqd1R3322 = getSMEFTCoeff("Cqd1R",2,2,1,1, muRG); 
    Cqd8R3311 = getSMEFTCoeff("Cqd8R",2,2,0,0, muRG); 
    Cqd8R3322 = getSMEFTCoeff("Cqd8R",2,2,1,1, muRG); 
 
    // 4F ccontributions computed using SMEFTsimA
    if (sqrt_s == 1.96) {
 
        C1 = 0.0; // N.A.
 
        mu +=
                +423765. * getSMEFTCoeffEW("CHG")
                - 4152.27 * getSMEFTCoeffEW("CG")
                + 568696. * getSMEFTCoeffEW("CuGR", 2, 2)
                - 2.844 * deltaG_hff(quarks[TOP]).real()
                + 57950.7 * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                + 572237. * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                + 68506.5 * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + 689368. * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + 34359.2 * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                + 562953. * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                - 1123.41 * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                + 15070.6 * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                + 22531.7 * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                + 13290.1 * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                + 152635. * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                + 137479. * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                - 890.245 * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                + 15388.5 * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                ;
    } else if (sqrt_s == 7.0) {
 
        C1 = 0.0387;
 
        mu +=
                +531046. * getSMEFTCoeffEW("CHG")
                - 85174.4 * getSMEFTCoeffEW("CG")
                + 810365. * getSMEFTCoeffEW("CuGR", 2, 2)
                - 2.846 * deltaG_hff(quarks[TOP]).real()
                + 19387.7 * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                + 309431. * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                + 53723.7 * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + 633768. * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + 19654.7 * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                + 303278. * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                - 3442.03 * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                + 41220. * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                + 6827.86 * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                + 7038.59 * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                + 116509. * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                + 74277.5 * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                - 2514.79 * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                + 41346.5 * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                ;
    } else if (sqrt_s == 8.0) {
 
        C1 = 0.0378;
 
        /*mu +=
                +535133. * getSMEFTCoeffEW("CHG")
                - 86316.6 * getSMEFTCoeffEW("CG")
                + 824047. * getSMEFTCoeffEW("CuGR", 2, 2)
                - 2.846 * deltaG_hff(quarks[TOP]).real()
                + 18617. * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                + 294168. * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                + 51386.8 * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + 603913. * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + 18807. * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                + 287709. * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                - 3419.45 * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                + 39513.7 * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                + 6838.91 * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                + 6363.98 * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                + 110752. * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                + 70573.7 * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                - 2659.57 * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                + 39608.7 * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                ;*/
 
        //AG:begin
        mu += cWsch * (
                ((0.1213) * getSMEFTCoeffEW("CHbox")
                + (-0.03042977) * getSMEFTCoeffEW("CHD")
                + (0.0013429) * getSMEFTCoeffEW("CHW")
                + (0.00034889) * getSMEFTCoeffEW("CHB")
                + (-0.001046257) * getSMEFTCoeffEW("CHWB")
                + (-0.0008895) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (6.729e-05) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0006294) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0041079) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.00015173) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.00062947) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.52771) * getSMEFTCoeffEW("CHG")
                + (-0.1223697) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (-0.839333) * getSMEFTCoeffEW("CuGR", 2, 2)
                + (0.08296) * getSMEFTCoeffEW("CG")
                + (-0.0097958) * getSMEFTCoeffEW("CuWR", 2, 2)
                + (-0.0033868) * getSMEFTCoeffEW("CuBR", 2, 2)
                + (0.019807) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                + (0.2932) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                + (-0.0007416) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                + (0.0055071) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                + (0.05702) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + (0.60888) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + (0.0021613) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                + (0.030738) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                + (0.019568) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                + (0.28692) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                + (0.00036217) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                + (0.0053893) * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                + (-0.00285764) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                + (-0.000223758) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                + (0.041058) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                + (0.0032835) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                + (0.007507) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                + (0.0064828) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                + (-0.00012226) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                + (0.00012461) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                + (0.11116) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                + (0.070065) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                + (0.0045917) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                + (0.0013165) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                + (-0.0019135) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                + (-0.0001571758) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                + (0.041092) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                + (0.0032845) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                + (-0.0609562) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0609562) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.06105) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
        //AG:end
    } else if (sqrt_s == 13.0) {
 
        C1 = 0.0351;    // 13 TeV
        
        /*mu +=
                +538046. * getSMEFTCoeffEW("CHG")
                - 85159.5 * getSMEFTCoeffEW("CG")
                + 861157. * getSMEFTCoeffEW("CuGR", 2, 2)
                - 2.846 * deltaG_hff(quarks[TOP]).real()
                + 13574.9 * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                + 227043. * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                + 41257.5 * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + 473396. * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + 14488.3 * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                + 221664. * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                - 3400.07 * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                + 31615.5 * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                + 4516.51 * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                + 4161.27 * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                + 85356.9 * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                + 53893.6 * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                - 2791.1 * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                + 30575.2 * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                ;*/
 
        //AG:begin
        // mu += cWsch * // QCD LO contribution should be alpha-MW scheme independent. Use as first approx for the moment 
        mu +=  (
                ((0.12121) * getSMEFTCoeffEW("CHbox")
                + (-0.03042744) * getSMEFTCoeffEW("CHD")
                + (0.001047) * getSMEFTCoeffEW("CHW")
                + (0.00026451) * getSMEFTCoeffEW("CHB")
                + (-0.00075726) * getSMEFTCoeffEW("CHWB")
                + (-0.0007866) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0004779) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0041559) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.00020603) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.00047808) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.53368) * getSMEFTCoeffEW("CHG")
                + (-0.122585689) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (-0.887533) * getSMEFTCoeffEW("CuGR", 2, 2)
                + (0.08762) * getSMEFTCoeffEW("CG")
                + (-0.00752105) * getSMEFTCoeffEW("CuWR", 2, 2)
                + (-0.0025626) * getSMEFTCoeffEW("CuBR", 2, 2)
                + (0.015813) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                + (0.23866) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                + (-0.0009533) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                + (0.0062474) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                + (0.048406) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + (0.5037) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + (0.002587) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                + (0.036061) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                + (0.016338) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                + (0.23349) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                + (0.00041585) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                + (0.0061126) * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                + (-0.00245583) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                + (-0.000269396) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                + (0.034461) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                + (0.003882) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                + (0.0058827) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                + (0.0050841) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                + (-0.00013204) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                + (0.00013861) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                + (0.09143) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                + (0.057019) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                + (0.0053692) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                + (0.0014935) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                + (-0.001545363) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                + (-0.000181173) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                + (0.034487) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                + (0.00388) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                + (-0.06091715) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.06091715) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.060881) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
        //AG:end 
 
    } else if (sqrt_s == 14.0) {
 
        //  Mw scheme. Only interference with QCD 
 
        C1 = 0.0347;
 
        mu +=  (
                +83480.4 * CG 
                -122879. * CuHR33 
                -4.73871 * CHq1R11 
                -231.66 * CHq3R11 
                -91.7543 * CHuR11 
                +87.4143 * CHdR11 
                -24.8507 * CHq1R22 
                +16.9517 * CHq3R22 
                -17.2674 * CHuR22 
                -15.1008 * CHdR22 
                -115.164 * CHq1R33 
                -217.306 * CHq3R33 
                -239.384 * CHuR33 
                -865559. * CuGR33 
                -115.367 * Cqq1R1133 
                +172262. * Cqq1R1331 
                -8.83359 * Cqq1R2233 
                +5264.44 * Cqq1R2332 
                -102.174 * Cqq3R1133 
                +376043. * Cqq3R1331 
                -10.6569 * Cqq3R2233 
                +31547.6 * Cqq3R2332 
                -46.0629 * CuuR1133 
                -48.4844 * CuuR2233 
                +173243. * CuuR1331 
                +5195.12 * CuuR2332 
                -77.2185 * Cud1R3311 
                -72.1335 * Cud1R3322 
                +26016.4 * Cud8R3311 
                +1960.64 * Cud8R3322 
                -130.929 * Cqu1R1133 
                -46.8336 * Cqu1R2233 
                -202.882 * Cqu1R3311 
                -30.1958 * Cqu1R3322 
                +68525.2 * Cqu8R1133 
                +4494.83 * Cqu8R2233 
                +42510. * Cqu8R3311 
                +1281.44 * Cqu8R3322 
                -152.4 * Cqd1R3311 
                -37.2748 * Cqd1R3322 
                +26242.2 * Cqd8R3311 
                +1993.33 * Cqd8R3322 
                );
 
    } else if (sqrt_s == 27.0) {
 
        //  Old (but ok) implementation + Missing 4F
 
        C1 = 0.0320; // From arXiv: 1902.00134
 
        mu +=
                +519682. * getSMEFTCoeffEW("CHG")
                - 68463.1 * getSMEFTCoeffEW("CG")
                + 884060. * getSMEFTCoeffEW("CuGR", 2, 2)
                - 2.849 * deltaG_hff(quarks[TOP]).real()
                ;
        
    } else if (sqrt_s == 50.0) {
 
        //  Mw scheme. Only interference with QCD
 
        C1 = 0.0; // N.A.
 
        mu +=  (
                +48030.8 * CG 
                -122979. * CuHR33 
                -205.704 * CHq1R11 
                -174.036 * CHq3R11 
                +35.0258 * CHuR11 
                +9.29779 * CHdR11 
                -106.234 * CHq1R22 
                -23.9319 * CHq3R22 
                -78.4184 * CHuR22 
                -10.0042 * CHdR22 
                -85.4844 * CHq1R33 
                -242.855 * CHq3R33 
                -258.711 * CHuR33 
                -886651. * CuGR33 
                -80.4492 * Cqq1R1133 
                +87600.9 * Cqq1R1331 
                -18.1512 * Cqq1R2233 
                +6155.28 * Cqq1R2332 
                +30.6261 * Cqq3R1133 
                +198713. * Cqq3R1331 
                -48.6117 * Cqq3R2233 
                +28525.5 * Cqq3R2332 
                -210.478 * CuuR1133 
                -20.4365 * CuuR2233 
                +88038.5 * CuuR1331 
                +6188.99 * CuuR2332 
                -110.028 * Cud1R3311 
                -80.9324 * Cud1R3322 
                +14322.3 * Cud8R3311 
                +2112.96 * Cud8R3322 
                -195.357 * Cqu1R1133 
                -32.7726 * Cqu1R2233 
                -6.33031 * Cqu1R3311 
                -49.1434 * Cqu1R3322 
                +35537.6 * Cqu8R1133 
                +4228.53 * Cqu8R2233 
                +21136.8 * Cqu8R3311 
                +1540.47 * Cqu8R3322 
                -152.389 * Cqd1R3311 
                -20.2313 * Cqd1R3322 
                +13562.3 * Cqd8R3311 
                +2031.46 * Cqd8R3322 
                );
        
    } else if (sqrt_s == 84.0) {
 
        //  Mw scheme. Only interference with QCD
 
        C1 = 0.0; // N.A.
 
        mu +=  (
                +29568.5 * CG 
                -122466. * CuHR33 
                -188.515 * CHq1R11 
                -161.156 * CHq3R11 
                -18.7298 * CHuR11 
                +84.0969 * CHdR11 
                -60.6269 * CHq1R22 
                +3.04679 * CHq3R22 
                -33.1077 * CHuR22 
                -10.836 * CHdR22 
                +33.4766 * CHq1R33 
                -249.387 * CHq3R33 
                -170.736 * CHuR33 
                -882584. * CuGR33 
                +165.169 * Cqq1R1133 
                +66847.5 * Cqq1R1331 
                -29.2351 * Cqq1R2233 
                +6258.47 * Cqq1R2332 
                +71.2558 * Cqq3R1133 
                +153407. * Cqq3R1331 
                -31.3139 * Cqq3R2233 
                +26872.2 * Cqq3R2332 
                -27.0795 * CuuR1133 
                -49.9167 * CuuR2233 
                +66805.3 * CuuR1331 
                +6238.71 * CuuR2332 
                -2.604 * Cud1R3311 
                -100.751 * Cud1R3322 
                +11049.3 * Cud8R3311 
                +2000. * Cud8R3322 
                +82.7029 * Cqu1R1133 
                -5.7992 * Cqu1R2233 
                -28.88 * Cqu1R3311 
                -56.5691 * Cqu1R3322 
                +27287.5 * Cqu8R1133 
                +4036.71 * Cqu8R2233 
                +15311. * Cqu8R3311 
                +1562.51 * Cqu8R3322 
                -40.5882 * Cqd1R3311 
                -14.8135 * Cqd1R3322 
                +10857.1 * Cqd8R3311 
                +1948.06 * Cqd8R3322
                );
 
    } else if (sqrt_s == 100.0) {
 
        //  Old (but ok) implementation + Missing 4F
 
        C1 = 0.0; // N.A.
 
        mu +=
                +467438. * getSMEFTCoeffEW("CHG")
                - 22519. * getSMEFTCoeffEW("CG")
                + 880378. * getSMEFTCoeffEW("CuGR", 2, 2)
                - 2.837 * deltaG_hff(quarks[TOP]).real()
                ;
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::delta_muttH_1()");
 
    //  Linear contribution from Higgs self-coupling
    mu += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    return mu;
}

◆ delta_muttH_2()

const double NPSMEFTd6General::delta_muttH_2 ( const double sqrt_s ) const

virtual

The SMEFT quadratic correction to the ratio $\mu_{ttH}$ between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 19694 of file NPSMEFTd6General.cpp.

                                                                      {
    double mu = 0.0;
 
    if (FlagQuadraticTerms) {
        if (sqrt_s == 8.0) {
            mu += 0.0;
        } else if (sqrt_s == 13.0) {
            mu += cWsch * (
                    +(0.014702) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                    + (0.0009337) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                    + (0.04044) * pow(getSMEFTCoeffEW("CHq1R", 0, 0), 2.0)
                    + (0.001357) * pow(getSMEFTCoeffEW("CHq1R", 1, 1), 2.0)
                    + (0.0404) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                    + (0.0013565) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                    + (0.7841) * pow(getSMEFTCoeffEW("CHG"), 2.0)
                    + (0.00375) * pow(getSMEFTCoeffEW("CuHR", 2, 2), 2.0)
                    + (1.087) * pow(getSMEFTCoeffEW("CuGR", 2, 2), 2.0)
                    + (2.3045) * pow(getSMEFTCoeffEW("CG"), 2.0)
                    + (0.014584) * pow(getSMEFTCoeffEW("CuWR", 2, 2), 2.0)
                    + (0.005576) * pow(getSMEFTCoeffEW("CuBR", 2, 2), 2.0)
                    + (0.6789) * pow(getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2), 2.0)
                    + (0.4348) * pow(getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0), 2.0)
                    + (0.02768) * pow(getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2), 2.0)
                    + (0.008345) * pow(getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1), 2.0)
                    + (0.68) * pow(getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2), 2.0)
                    + (1.4142) * pow(getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0), 2.0)
                    + (0.02769) * pow(getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2), 2.0)
                    + (0.08561) * pow(getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1), 2.0)
                    + (0.4348) * pow(getSMEFTCoeffEW("CuuR", 0, 0, 2, 2), 2.0)
                    + (0.4348) * pow(getSMEFTCoeffEW("CuuR", 0, 2, 2, 0), 2.0)
                    + (0.008345) * pow(getSMEFTCoeffEW("CuuR", 1, 1, 2, 2), 2.0)
                    + (0.008345) * pow(getSMEFTCoeffEW("CuuR", 1, 2, 2, 1), 2.0)
                    + (0.06132) * pow(getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0), 2.0)
                    + (0.004841) * pow(getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1), 2.0)
                    + (0.013625) * pow(getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0), 2.0)
                    + (0.0010732) * pow(getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1), 2.0)
                    + (0.16996) * pow(getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2), 2.0)
                    + (0.10881) * pow(getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0), 2.0)
                    + (0.006934) * pow(getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2), 2.0)
                    + (0.0020928) * pow(getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1), 2.0)
                    + (0.03774) * pow(getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2), 2.0)
                    + (0.024096) * pow(getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0), 2.0)
                    + (0.0015337) * pow(getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2), 2.0)
                    + (0.0004612) * pow(getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1), 2.0)
                    + (0.06119) * pow(getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0), 2.0)
                    + (0.004829) * pow(getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1), 2.0)
                    + (0.013597) * pow(getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0), 2.0)
                    + (0.0010673) * pow(getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1), 2.0)
                    + (-0.007357295) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                    + (0.00050321) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.028502) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHG")
                    + (-0.01484933) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CuHR", 2, 2)
                    + (-0.107575) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CuGR", 2, 2)
                    + (0.010564) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CG")
                    + (-0.000912358) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CuWR", 2, 2)
                    + (-0.000310819) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CuBR", 2, 2)
                    + (0.0019226) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                    + (0.028947) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                    + (-0.00011542) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                    + (0.00075765) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                    + (0.0058677) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                    + (0.061084) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                    + (0.00031326) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                    + (0.0043669) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                    + (0.0019799) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                    + (0.028312) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                    + (0.00074137) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                    + (-0.000298441) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                    + (0.0041771) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                    + (0.00047054) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                    + (0.00071321) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                    + (0.00061642) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                    + (0.0110873) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                    + (0.0069104) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                    + (0.00065058) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                    + (0.00018121) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                    + (-0.0001874256) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                    + (0.0041783) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.00047084) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.0071375) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CuGR", 2, 2)
                    + (0.0037252) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CG")
                    + (0.026911) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CuWR", 2, 2)
                    + (-0.0026404) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CuBR", 2, 2)
                    + (0.00021154) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                    + (0.00059) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                    + (-0.00101219) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                    + (-0.00731675) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                    + (-0.000191691) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                    + (-0.00143574) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                    + (-0.0155257) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                    + (-0.001117055) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                    + (-0.00273813) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                    + (-0.00782204) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                    + (-0.0002044194) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                    + (0.00041247) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                    + (-0.001044099) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                    + (-0.0001176787) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                    + (-0.000617426) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                    + (-0.000865933) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                    + (-0.00277261) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                    + (-0.001727692) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                    + (-0.0001626746) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (0.00026339) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("Cqd8R", 1, 1, 2, 2)
                    + (-0.001045699) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.0001177004) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq1R", 1, 1)
                    + (-0.0242) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CuHR", 2, 2)
                    + (0.000716) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                    + (-0.034646) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                    + (-0.007406) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                    + (-0.009617) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                    + (-0.015716) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                    + (0.010743) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                    + (0.0009319) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CuWR", 2, 2)
                    + (-0.0013849) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                    + (-0.00013945) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                    + (0.0005455) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                    + (-0.0007824) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                    + (0.000349) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (-0.00047073) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CuBR", 2, 2)
                    + (-0.000101878) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                    + (-0.001303) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                    + (-0.00157647) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                    + (0.00023622) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                    + (-0.0081488) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                    + (0.0007056) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                    + (-0.00045995) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                    + (0.00019478) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                    + (0.00082057) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                    + (0.00027355) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                    + (-0.000124622) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                    + (-0.00025589) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (0.0010011) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("Cqd1R", 1, 1, 2, 2)
                    + (-0.000298658) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (0.00045) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                    + (-0.002292) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                    + (0.0004973) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                    + (0.009579) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                    + (0.007383) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                    + (0.034689) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                    + (-0.000958) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                    + (-0.003224) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                    + (-0.00050371) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                    + (-0.00050371) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                    + (0.00050288) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                    + (-0.00012965) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                    + (-0.0005446) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                    + (0.00013994) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                    + (0.0013804) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                    + (-0.0005041) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                    + (0.0001237) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                    + (-0.001176913) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                    + (0.00021557) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                    + (0.0013101) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                    + (0.0015776) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                    + (-0.00023607) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                    + (0.008153) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                    + (-0.0007042) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                    + (0.00046004) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                    + (-0.000194607) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                    + (-0.0008201) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                    + (-0.000273441) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                    + (0.00012454) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                    + (0.0002565) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                    + (-0.00100107) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                    + (0.00029847) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                    + (-0.012472) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                    + (-0.90423) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                    + (0.0929) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                    + (0.087161) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                    + (0.0019958) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                    + (0.19048) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                    + (0.0121443) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                    + (0.087145) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("Cqd1R", 1, 1, 2, 2)
                    + (0.0019961) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                    + (0.012923) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                    + (0.00126871) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                    + (0.034738) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("CG")
                    + (0.021802) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("CuWR", 2, 2)
                    + (0.0017674) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("CuBR", 2, 2)
                    + (0.00049917) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                    + (0.012927) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                    + (0.00126852) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                    + (-0.0101842) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                    + (-0.0101842) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                    + (0.010186) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                    + (0.084054) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                    + (-0.010671) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                    + (0.00070203) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                    + (0.00024481) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                    + (-0.001927) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                    + (-0.0292148) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                    + (0.00011522) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                    + (-0.000764818) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                    + (-0.0058127) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                    + (-0.0616611) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                    + (-0.000311842) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (-0.004405432) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 1, 1, 2, 2)
                    + (-0.00198732) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                    + (-0.0285725) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                    + (-0.00074887) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqd8R", 1, 1, 2, 2)
                    + (0.00029942) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                    + (-0.00422357) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.000475661) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.00072331) * getSMEFTCoeffEW("CuHR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.0006366) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("CG")
                    + (-0.01119465) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                    + (-0.00698442) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                    + (-0.000656429) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                    + (-0.0001830691) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                    + (0.00019355) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                    + (-0.00422373) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                    + (-0.00047546) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                    + (0.0037431) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                    + (0.0037431) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                    + (-0.003741291) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                    + (1.2499) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                    + (-0.126853) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                    + (-0.002833057) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                    + (-0.275727) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 1, 1, 2, 2)
                    + (-0.0170037) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                    + (-0.126864) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cqd8R", 1, 1, 2, 2)
                    + (-0.002833131) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                    + (-0.01862109) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.00177154) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("CuWR", 2, 2)
                    + (-0.0503556) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                    + (-0.0317301) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                    + (-0.00247985) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                    + (-0.000708879) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                    + (-0.01864009) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                    + (-0.001772083) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                    + (-0.01862109) * getSMEFTCoeffEW("CuGR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.00177154) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("CuWR", 2, 2)
                    + (-0.0503556) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                    + (-0.0317301) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                    + (-0.00247985) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                    + (-0.000708879) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                    + (-0.01864009) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                    + (-0.001772083) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                    + (0.0269) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                    + (0.0269) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                    + (-0.0269037) * getSMEFTCoeffEW("CG") * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                    + (0.0007731) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                    + (-0.034008) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (-0.0276195) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 1, 1, 2, 2)
                    + (0.0028091) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                    + (-0.000619) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                    + (-0.13154) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (0.004949) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("Cqd8R", 1, 1, 2, 2)
                    + (-0.006521) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                    + (0.002492) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                    + (0.00044879) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.00014959) * getSMEFTCoeffEW("CuWR", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.017057) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                    + (0.00022461) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                    + (0.0014015) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                    + (0.00091266) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                    + (0.00091266) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (-0.000912218) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 1, 1, 2, 2)
                    + (-0.0230086) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                    + (-0.0046743) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                    + (-0.00117563) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (-0.000103453) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("Cqd8R", 1, 1, 2, 2)
                    + (-0.005022) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                    + (-0.0106677) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                    + (0.00055688) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.000680356) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.058583) * getSMEFTCoeffEW("CuBR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.0195304) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                    + (-0.0013111) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                    + (-0.00043707) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                    + (0.008605) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                    + (0.00082027) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                    + (-0.0115044) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                    + (-0.0293196) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                    + (-0.00058824) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                    + (0.0086014) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                    + (0.00081998) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                    + (0.00031031) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                    + (0.00031031) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                    + (-0.00031033) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (0.285) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqd8R", 1, 1, 2, 2)
                    + (-0.001) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                    + (-0.0008) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                    + (0.3785) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.61551) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.23842) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0) * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                    + (-0.001926) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0) * getSMEFTCoeffEW("Cqd8R", 1, 1, 2, 2)
                    + (-0.001926) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                    + (0.0019241) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                    + (-0.0015) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.0015) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.28911) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.86736) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                    + (0.05014) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                    + (0.066855) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                    + (-0.0151167) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.0151167) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.015126) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.00556) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                    + (-0.021927) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                    + (0.031335) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                    + (0.0113331) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                    + (0.00011539) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                    + (0.00011539) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                    + (-0.00011547) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                    + (0.0055636) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                    + (0.01669) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2) * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                    + (0.00108813) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                    + (0.0014524) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                    + (-0.000395291) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                    + (-0.000395291) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                    + (0.00039521) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0) * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                    + (-0.042) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                    + (-0.0019) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                    + (-0.002) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                    + (0.06253) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                    + (-0.0058702) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                    + (-0.0058702) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                    + (0.0058678) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                    + (-0.003) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                    + (-0.002) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                    + (0.10864) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                    + (0.14487) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                    + (-0.0305092) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                    + (-0.0305092) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                    + (0.030531) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                    + (-0.0202) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                    + (-0.0047994) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                    + (-0.000313303) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                    + (-0.000313303) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                    + (0.00031331) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                    + (0.0064625) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.0086274) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                    + (-0.00212214) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0) * getSMEFTCoeffEW("Cqd1R", 1, 1, 2, 2)
                    + (-0.00212214) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                    + (0.0021228) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                    + (0.285) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0) * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (-0.0015) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0) * getSMEFTCoeffEW("Cqd8R", 1, 1, 2, 2)
                    + (-0.0015) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                    + (-0.0015) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.0015) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.00556) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                    + (-0.0002) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0) * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (0.043884) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                    + (0.00029842) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                    + (0.00029842) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                    + (-0.000298606) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1) * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (0.0040322) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2) * getSMEFTCoeffEW("Cqd1R", 1, 1, 2, 2)
                    + (0.0097484) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.00209006) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                    + (-0.00209006) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                    + (0.0020882) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                    + (0.00089675) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1) * getSMEFTCoeffEW("Cqd1R", 1, 1, 2, 2)
                    + (-0.000235425) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                    + (-0.000235425) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                    + (0.00023517) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1) * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (-0.0012) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1) * getSMEFTCoeffEW("Cqd8R", 1, 1, 2, 2)
                    + (-0.0004) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                    + (-0.0004) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                    + (-0.00071357) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.00071357) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.00071314) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.0004) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                    + (-0.0005) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                    + (-0.0006162615) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                    + (-0.0006162615) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                    + (0.00061646) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2) * getSMEFTCoeffEW("Cqd1R", 0, 0, 2, 2)
                    + (-0.00554128) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.00554128) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.0055443) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.003456905) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.003456905) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.0034557) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    ) * pow(1000000.0, 2.0);
 
        } else
            throw std::runtime_error("Bad argument in NPSMEFTd6General::delta_muttH_2()");
    }
 
    //  Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
    //  mu = mu + cLHd6 * cLH3d62 * deltaH3L2(C1) * deltaG_hhhRatio() * deltaG_hhhRatio();
 
    return mu;
}

◆ delta_muVBF_1()

const double NPSMEFTd6General::delta_muVBF_1 ( const double sqrt_s ) const

virtual

The SMEFT linear correction to the ratio $\mu_{VBF}$ between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 18055 of file NPSMEFTd6General.cpp.

                                                                      {
    double mu = 0.0;
    double C1 = 0.0;
    
    double CHB = 0.0, CHW = 0.0, CHWB = 0.0, CHG = 0.0, CHD = 0.0, CHbox = 0.0; 
    double CHl3R11 = 0.0, CHl3R22 = 0.0, CllR1221 = 0.0, CHq1R11 = 0.0, CHq3R11 = 0.0;
    double CHq1R22 = 0.0, CHq3R22 = 0.0, CHuR11 = 0.0, CHuR22 = 0.0, CHdR11 = 0.0, CHdR22 = 0.0; 
    
    double muRG = muw;
    
//  Wilson coefficients definitions 
    CHB = getSMEFTCoeff("CHB", muRG); 
    CHW = getSMEFTCoeff("CHW", muRG); 
    CHWB = getSMEFTCoeff("CHWB", muRG); 
    CHG = getSMEFTCoeff("CHG", muRG); 
    CHD = getSMEFTCoeff("CHD", muRG); 
    CHbox = getSMEFTCoeff("CHbox", muRG); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG); 
    CHq1R11 = getSMEFTCoeff("CHq1R",0,0, muRG); 
    CHq3R11 = getSMEFTCoeff("CHq3R",0,0, muRG); 
    CHq1R22 = getSMEFTCoeff("CHq1R",1,1, muRG); 
    CHq3R22 = getSMEFTCoeff("CHq3R",1,1, muRG); 
    CHuR11 = getSMEFTCoeff("CHuR",0,0, muRG); 
    CHuR22 = getSMEFTCoeff("CHuR",1,1, muRG); 
    CHdR11 = getSMEFTCoeff("CHdR",0,0, muRG); 
    CHdR22 = getSMEFTCoeff("CHdR",1,1, muRG); 
 
    if (sqrt_s == 1.96) {
 
        C1 = 0.0; // N.A.
 
        mu +=
                +121321. * getSMEFTCoeffEW("CHbox")
                + 5770.95 * getSMEFTCoeffEW("CHB")
                - 51626.2 * getSMEFTCoeffEW("CHW")
                + 57783.8 * getSMEFTCoeffEW("CHG")
                - 15060.5 * getSMEFTCoeffEW("CHq1R", 0, 0)
                - 1122.91 * getSMEFTCoeffEW("CHq1R", 1, 1)
                - 9988.6 * getSMEFTCoeffEW("CHuR", 0, 0)
                - 629.4 * getSMEFTCoeffEW("CHuR", 1, 1)
                + 2994.79 * getSMEFTCoeffEW("CHdR", 0, 0)
                + 467.105 * getSMEFTCoeffEW("CHdR", 1, 1)
                - 205793. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 16751.6 * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-170868. * getSMEFTCoeffEW("CHD")
                - 322062. * getSMEFTCoeffEW("CHWB")
                - 4.567 * delta_GF
                - 3.498 * deltaMwd6())
                + cWsch * (-13112. * getSMEFTCoeffEW("CHD")
                + 21988.3 * getSMEFTCoeffEW("CHWB")
                - 3.003 * delta_GF)
                ;
 
    } else if (sqrt_s == 7.0) {
 
        C1 = 0.0065;
 
        mu +=
                +121090. * getSMEFTCoeffEW("CHbox")
                - 810.554 * getSMEFTCoeffEW("CHB")
                - 86724.3 * getSMEFTCoeffEW("CHW")
                - 155709. * getSMEFTCoeffEW("CHG")
                + 15633.8 * getSMEFTCoeffEW("CHq1R", 0, 0)
                - 2932.56 * getSMEFTCoeffEW("CHq1R", 1, 1)
                - 24997.3 * getSMEFTCoeffEW("CHuR", 0, 0)
                - 2380.75 * getSMEFTCoeffEW("CHuR", 1, 1)
                + 7157.18 * getSMEFTCoeffEW("CHdR", 0, 0)
                + 1508.92 * getSMEFTCoeffEW("CHdR", 1, 1)
                - 355189. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 52211.2 * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-166792. * getSMEFTCoeffEW("CHD")
                - 316769. * getSMEFTCoeffEW("CHWB")
                - 4.542 * delta_GF
                - 3.253 * deltaMwd6())
                + cWsch * (-11689.4 * getSMEFTCoeffEW("CHD")
                + 23083.4 * getSMEFTCoeffEW("CHWB")
                - 3.004 * delta_GF)
                ;
 
    } else if (sqrt_s == 8.0) {
 
        C1 = 0.0065;
 
        /*mu +=
                +121100. * getSMEFTCoeffEW("CHbox")
                - 684.545 * getSMEFTCoeffEW("CHB")
                - 85129.2 * getSMEFTCoeffEW("CHW")
                - 136876. * getSMEFTCoeffEW("CHG")
                + 15225.3 * getSMEFTCoeffEW("CHq1R", 0, 0)
                - 3114.83 * getSMEFTCoeffEW("CHq1R", 1, 1)
                - 25391.2 * getSMEFTCoeffEW("CHuR", 0, 0)
                - 2583.43 * getSMEFTCoeffEW("CHuR", 1, 1)
                + 7410.87 * getSMEFTCoeffEW("CHdR", 0, 0)
                + 1629.31 * getSMEFTCoeffEW("CHdR", 1, 1)
                - 363032. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 56263.7 * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-166792. * getSMEFTCoeffEW("CHD")
                - 317073. * getSMEFTCoeffEW("CHWB")
                - 4.541 * delta_GF
                - 3.347 * deltaMwd6())
                + cWsch * (-11741.3 * getSMEFTCoeffEW("CHD")
                + 22626.6 *  getSMEFTCoeffEW("CHWB")
                - 3.003 * delta_GF)
                ;*/
        //AG:begin
        mu += cWsch * (
                ((0.1212) * getSMEFTCoeffEW("CHbox")
                + (0.09705) * getSMEFTCoeffEW("CHW")
                + (0.005368) * getSMEFTCoeffEW("CHB")
                + (-0.009586) * getSMEFTCoeffEW("CHD")
                + (0.04278) * getSMEFTCoeffEW("CHWB")
                + (-0.00204) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.002219) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.17898) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.007077) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.01424) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (9.3e-05) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.005403) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.0004033) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.1818681) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1818681) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18188) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-0.146) * deltaGwd6()
                + (-0.0732) * deltaGzd6()
                );
        //AG:end
 
    } else if (sqrt_s == 13.0) {
 
        C1 = 0.0064;
 
        /*mu +=
                +121332. * getSMEFTCoeffEW("CHbox")
                - 283.27 * getSMEFTCoeffEW("CHB")
                - 80829.5 * getSMEFTCoeffEW("CHW")
                - 90637.9 * getSMEFTCoeffEW("CHG")
                + 13466.3 * getSMEFTCoeffEW("CHq1R", 0, 0)
                - 3912.24 * getSMEFTCoeffEW("CHq1R", 1, 1)
                - 26789.8 * getSMEFTCoeffEW("CHuR", 0, 0)
                - 3408.16 * getSMEFTCoeffEW("CHuR", 1, 1)
                + 8302.17 * getSMEFTCoeffEW("CHdR", 0, 0)
                + 2107.16 * getSMEFTCoeffEW("CHdR", 1, 1)
                - 389656. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 72334.1 * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-166707. * getSMEFTCoeffEW("CHD")
                - 317068. * getSMEFTCoeffEW("CHWB")
                - 4.532 * delta_GF
                - 3.247 * deltaMwd6())
                + cWsch * (-11844.9 * getSMEFTCoeffEW("CHD")
                + 21545. * getSMEFTCoeffEW("CHWB")
                - 2.999 * delta_GF)
                ;*/
        //AG:begin
        mu += cWsch * (
                ((0.1213) * getSMEFTCoeffEW("CHbox")
                + (-0.05852) * getSMEFTCoeffEW("CHW")
                + (-0.0034826) * getSMEFTCoeffEW("CHB")
                + (-0.012075) * getSMEFTCoeffEW("CHD")
                + (0.013098) * getSMEFTCoeffEW("CHWB")
                + (0.012076) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.006699) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.3236105) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0730228) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.02151748) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.002749016) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.006742) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0022914) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.1818213) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1818213) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18192) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-0.107) * deltaGwd6()
                + (-0.051) * deltaGzd6()
 
                );
        //AG:end
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else if (sqrt_s == 14.0) {
 
        // Mw scheme
 
        C1 = 0.0064;
 
        mu +=
                cWsch * (
                -149.911 * CHB 
                -82290.4 * CHW 
                +21589.7 * CHWB 
                -64109.4 * CHG 
                -11380.7 * CHD 
                +121758. * CHbox 
                -182196. * CHl3R11 
                -181307. * CHl3R22 
                +183438. * CllR1221 
                +15981.4 * CHq1R11 
                -385489. * CHq3R11 
                -5754.62 * CHq1R22 
                -81679.1 * CHq3R22 
                -25756.3 * CHuR11 
                -3379.74 * CHuR22 
                +8049.27 * CHdR11 
                +2139.42 * CHdR22
                );
 
    } else if (sqrt_s == 27.0) {
 
        // Only Alpha scheme
 
        C1 = 0.0062; // From arXiv: 1902.00134
 
        mu +=
                +120777. * getSMEFTCoeffEW("CHbox")
                + 6664.27 * getSMEFTCoeffEW("CHq1R", 0, 0)
                - 34230.7 * getSMEFTCoeffEW("CHuR", 0, 0)
                + 12917.3 * getSMEFTCoeffEW("CHdR", 0, 0)
                - 536216. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 163493. * getSMEFTCoeffEW("CHD")
                + 58.33 * getSMEFTCoeffEW("CHB")
                - 81360.5 * getSMEFTCoeffEW("CHW")
                - 313026. * getSMEFTCoeffEW("CHWB")
                - 16430. * getSMEFTCoeffEW("CHG")
                - 4.475 * delta_GF
                - 2.99 * deltaMwd6()
                ;
        
    } else if (sqrt_s == 50.0) {
 
        // Mw scheme
 
        C1 = 0.0; // N.A.
 
        mu +=
                cWsch * (
                +63.2251 * CHB 
                -84681.3 * CHW 
                +20726.1 * CHWB 
                -34760.9 * CHG 
                -10986.7 * CHD 
                +121258. * CHbox 
                -181170. * CHl3R11 
                -181540. * CHl3R22 
                +183281. * CllR1221 
                +11576.7 * CHq1R11 
                -461606. * CHq3R11 
                -8442.73 * CHq1R22 
                -134822. * CHq3R22 
                -29766.6 * CHuR11 
                -6031.76 * CHuR22 
                +10677.4 * CHdR11 
                +3637.44 * CHdR22 
                );
        
    } else if (sqrt_s == 84.0) {
 
        // Mw scheme
 
        C1 = 0.0; // N.A.
 
        mu +=
                cWsch * (
                +49.3432 * CHB 
                -88355. * CHW 
                +20554. * CHWB 
                -32006.7 * CHG 
                -11122. * CHD 
                +121764. * CHbox 
                -181033. * CHl3R11 
                -181604. * CHl3R22 
                +184047. * CllR1221 
                +9449.49 * CHq1R11 
                -490153. * CHq3R11 
                -9699.98 * CHq1R22 
                -160491. * CHq3R22 
                -31231.9 * CHuR11 
                -7518.66 * CHuR22 
                +11885.7 * CHdR11 
                +4545.8 * CHdR22 
                );
 
    } else if (sqrt_s == 100.0) {
 
        // Only Alpha scheme
 
        C1 = 0.0; // N.A.
 
        mu +=
                +121714. * getSMEFTCoeffEW("CHbox")
                - 2261.73 * getSMEFTCoeffEW("CHq1R", 0, 0)
                - 42045.4 * getSMEFTCoeffEW("CHuR", 0, 0)
                + 17539.2 * getSMEFTCoeffEW("CHdR", 0, 0)
                - 674206. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 163344. * getSMEFTCoeffEW("CHD")
                + 71.488 * getSMEFTCoeffEW("CHB")
                - 90808.2 * getSMEFTCoeffEW("CHW")
                - 312544. * getSMEFTCoeffEW("CHWB")
                - 8165.65 * getSMEFTCoeffEW("CHG")
                - 4.452 * delta_GF
                - 2.949 * deltaMwd6()
                ;
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::delta_muVBF_1()");
 
    //  Linear contribution from Higgs self-coupling
    mu += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    return mu;
}

◆ delta_muVBF_2()

const double NPSMEFTd6General::delta_muVBF_2 ( const double sqrt_s ) const

virtual

The SMEFT quadratic correction to the ratio $\mu_{VBF}$ between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 18371 of file NPSMEFTd6General.cpp.

                                                                      {
    double mu = 0.0;
 
    if (FlagQuadraticTerms) {
        if (sqrt_s == 8.0) {
            mu += 0.0;
        } else if (sqrt_s == 13.0) {
            mu += cWsch * (
                    +(0.014669) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                    + (0.03814) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                    + (0.0001606) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                    + (0.0012512) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                    + (0.002816) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                    + (0.04114) * pow(getSMEFTCoeffEW("CHq1R", 0, 0), 2.0)
                    + (0.005951) * pow(getSMEFTCoeffEW("CHq1R", 1, 1), 2.0)
                    + (0.12999) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                    + (0.021) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                    + (0.02614) * pow(getSMEFTCoeffEW("CHuR", 0, 0), 2.0)
                    + (0.002254) * pow(getSMEFTCoeffEW("CHuR", 1, 1), 2.0)
                    + (0.01424) * pow(getSMEFTCoeffEW("CHdR", 0, 0), 2.0)
                    + (0.003715) * pow(getSMEFTCoeffEW("CHdR", 1, 1), 2.0)
                    + (0.011029) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                    + (0.011029) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                    + (0.011025) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                    + (-0.0070851) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                    + (-0.00042041) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                    + (-0.0051343) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                    + (0.0015819) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                    + (0.0014674) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 0, 0)
                    + (-0.0008105) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 1, 1)
                    + (-0.03923489) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (-0.00884719) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (-0.002606668) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 0, 0)
                    + (-0.0003321783) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 1, 1)
                    + (0.0008181) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 0, 0)
                    + (0.00027756) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 1, 1)
                    + (-0.0147203) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.0147203) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.014696) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.0038751) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                    + (0.0009616) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                    + (0.0063486) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                    + (-0.0012817) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 0, 0)
                    + (0.0005912) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 1, 1)
                    + (0.036381) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.007742) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (0.0018475) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 0, 0)
                    + (0.0002321) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 1, 1)
                    + (-0.00057524) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHdR", 0, 0)
                    + (-0.00019275) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHdR", 1, 1)
                    + (0.00709) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.00709) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.0070951) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.00030585) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                    + (0.0026636) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                    + (-0.0004294) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                    + (0.00016956) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                    + (0.0023133) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.00047684) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (0.0005299) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHuR", 0, 0)
                    + (-0.0001649) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 0, 0)
                    + (0.00042179) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.00042179) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.00042005) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.0016858) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                    + (0.001146) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 0, 0)
                    + (0.00035237) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 1, 1)
                    + (0.007992) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.0019854) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (0.0032017) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 0, 0)
                    + (0.00041567) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 1, 1)
                    + (-0.001009181) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 0, 0)
                    + (-0.000346716) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 1, 1)
                    + (0.0014614) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.0014614) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.0014596) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.0014258) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                    + (0.0001052) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                    + (-0.0023342) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (-0.0004515) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (0.0025923) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 0, 0)
                    + (0.00032608) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 1, 1)
                    + (-0.00080841) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 0, 0)
                    + (-0.00027189) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 1, 1)
                    + (-0.0015826) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.0015826) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.0015764) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.024622) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (-0.0014685) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.0014685) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.0014626) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.0002688) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.0028941) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (0.0008132) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.0008132) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.00080835) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.0028) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (-0.0003598) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHuR", 0, 0)
                    + (-0.00012322) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHuR", 1, 1)
                    + (0.00017138) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHdR", 0, 0)
                    + (0.039187) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.039187) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.03918207) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.00019908) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHuR", 0, 0)
                    + (0.008845) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.008845) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.00885679) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.0026059) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.0026059) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.002607191) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.00033244) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.00033244) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.0003324333) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.000817569) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.000817569) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.0008182) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.00027752) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.00027752) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.00027744) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.01101) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.02202142) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.02202142) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    ) * pow(1000000.0, 2.0);
        } else
            throw std::runtime_error("Bad argument in NPSMEFTd6General::delta_muVBF_2()");
    }
 
    //  Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
    //  mu = mu + cLHd6 * cLH3d62 * deltaH3L2(C1) * deltaG_hhhRatio() * deltaG_hhhRatio();
 
    return mu;
}

◆ delta_muVH_1()

const double NPSMEFTd6General::delta_muVH_1 ( const double sqrt_s ) const

virtual

The SMEFT linear correction to the ratio $\mu_{VH}$ between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 20261 of file NPSMEFTd6General.cpp.

                                                                     {
    double mu = 0.0;
 
    double sigmaWH_SM = computeSigmaWH(sqrt_s);
    double sigmaZH_SM = computeSigmaZH(sqrt_s);
 
    double sigmaWH_1 = delta_muWH_1(sqrt_s) * sigmaWH_SM;
    double sigmaZH_1 = delta_muZH_1(sqrt_s) * sigmaZH_SM;
    mu += ((sigmaWH_1 + sigmaZH_1) / (sigmaWH_SM + sigmaZH_SM));
 
    return mu;
}

◆ delta_muVH_2()

const double NPSMEFTd6General::delta_muVH_2 ( const double sqrt_s ) const

virtual

The SMEFT quadratic correction to the ratio $\mu_{VH}$ between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 20274 of file NPSMEFTd6General.cpp.

                                                                     {
    double mu = 0.0;
 
    if (FlagQuadraticTerms) {
        double sigmaWH_SM = computeSigmaWH(sqrt_s);
        double sigmaZH_SM = computeSigmaZH(sqrt_s);
 
        double sigmaWH_2 = delta_muWH_2(sqrt_s) * sigmaWH_SM;
        double sigmaZH_2 = delta_muZH_2(sqrt_s) * sigmaZH_SM;
        mu += ((sigmaWH_2 + sigmaZH_2) / (sigmaWH_SM + sigmaZH_SM));
    }
 
    return mu;
}

◆ delta_muWH_1()

const double NPSMEFTd6General::delta_muWH_1 ( const double sqrt_s ) const

virtual

The SMEFT linear correction to the ratio $\mu_{WH}$ between the W-Higgs associated production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 18522 of file NPSMEFTd6General.cpp.

                                                                     {
    double mu = 0.0;
    double C1 = 0.0;
    
    double CHW = 0.0, CHWB = 0.0, CHD = 0.0, CHbox = 0.0, CHl3R11 = 0.0, CHl3R22 = 0.0, CllR1221 = 0.0, CHq3R11 = 0.0, CHq3R22 = 0.0;
    double muRG = muw;
    
//  Wilson coefficients definitions 
    CHW = getSMEFTCoeff("CHW", muRG); 
    CHWB = getSMEFTCoeff("CHWB", muRG); 
    CHD = getSMEFTCoeff("CHD", muRG); 
    CHbox = getSMEFTCoeff("CHbox", muRG); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG); 
    CHq3R11 = getSMEFTCoeff("CHq3R",0,0, muRG); 
    CHq3R22 = getSMEFTCoeff("CHq3R",1,1, muRG); 
 
    if (sqrt_s == 1.96) {
 
        C1 = 0.0; // N.A.
 
        mu +=
                +121231. * getSMEFTCoeffEW("CHbox")
                + 855498. * getSMEFTCoeffEW("CHW")
                + 1554889. * getSMEFTCoeffEW("CHq3R", 0, 0)
                + 10415.1 * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-160273. * getSMEFTCoeffEW("CHD")
                - 284953. * getSMEFTCoeffEW("CHWB")
                - 3.288 * delta_GF
                - 2.258 * deltaMwd6())
                + cWsch * (-30311.6 * getSMEFTCoeffEW("CHD")
                + 0. * getSMEFTCoeffEW("CHWB")
                - 2. * delta_GF)
                ;
    } else if (sqrt_s == 7.0) {
 
        C1 = 0.0106;
 
        mu +=
                +121215. * getSMEFTCoeffEW("CHbox")
                + 874536. * getSMEFTCoeffEW("CHW")
                + 1688781. * getSMEFTCoeffEW("CHq3R", 0, 0)
                + 101677. * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-160236. * getSMEFTCoeffEW("CHD")
                - 284911. * getSMEFTCoeffEW("CHWB")
                - 3.286 * delta_GF
                - 2.217 * deltaMwd6())
                + cWsch * (-30300.4 * getSMEFTCoeffEW("CHD")
                + 0. * getSMEFTCoeffEW("CHWB")
                - 1.999 * delta_GF)
                ;
    } else if (sqrt_s == 8.0) {
 
        C1 = 0.0105;
 
        /*mu +=
                +121222. * getSMEFTCoeffEW("CHbox")
                + 877503. * getSMEFTCoeffEW("CHW")
                + 1716018. * getSMEFTCoeffEW("CHq3R", 0, 0)
                + 113210. * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-160294. * getSMEFTCoeffEW("CHD")
                - 284954. * getSMEFTCoeffEW("CHWB")
                - 3.287 * delta_GF
                - 2.179 * deltaMwd6())
                + cWsch * (-30310.6 * getSMEFTCoeffEW("CHD")
                + 0. * getSMEFTCoeffEW("CHWB")
                - 1.999 * delta_GF)
                ;*/
 
        //AG:begin
        mu += cWsch * (
                ((0.121211) * getSMEFTCoeffEW("CHbox")
                + (-0.030304941) * getSMEFTCoeffEW("CHD")
                + (0.87535) * getSMEFTCoeffEW("CHW")
                + (1.6911) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.13786) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.12128307) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.12128307) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.121211) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
        //AG:end
    } else if (sqrt_s == 13.0) {
 
        C1 = 0.0103;
 
        /*mu +=
                +121126. * getSMEFTCoeffEW("CHbox")
                + 886205. * getSMEFTCoeffEW("CHW")
                + 1792005. * getSMEFTCoeffEW("CHq3R", 0, 0)
                + 161535. * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-160176. * getSMEFTCoeffEW("CHD")
                - 284823. * getSMEFTCoeffEW("CHWB")
                - 3.287 * delta_GF
                - 2.139 * deltaMwd6())
                + cWsch * (-30285.8 * getSMEFTCoeffEW("CHD")
                + 0. * getSMEFTCoeffEW("CHWB")
                - 1.999 * delta_GF)
                ;*/
        // AG:begin
        mu += cWsch * (
                ((0.121283) * getSMEFTCoeffEW("CHbox")
                + (-0.0303129) * getSMEFTCoeffEW("CHD")
                + (0.88562) * getSMEFTCoeffEW("CHW")
                + (1.7298) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.19535) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.121234) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.121234) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.121283) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
        mu += cWsch * ((0.0016) * deltaGwd6());
        //AG:end
    } else if (sqrt_s == 14.0) {
 
        // Mw scheme
 
        C1 = 0.0103;
 
        mu +=
                cWsch * (
                +884638. * CHW 
                -12.8388 * CHWB 
                -30014.6 * CHD 
                +121050. * CHbox 
                -121033. * (CHl3R11 + CHl3R22 -CllR1221)  
                +1763715. * CHq3R11 
                +189400. * CHq3R22 
                );
    } else if (sqrt_s == 27.0) {
 
        // Only Alpha scheme
 
        C1 = 0.0101; // From arXiv: 1902.00134
 
        mu +=
                +120696. * getSMEFTCoeffEW("CHbox")
                + 2105646. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 159695. * getSMEFTCoeffEW("CHD")
                + 900162. * getSMEFTCoeffEW("CHW")
                - 283257. * getSMEFTCoeffEW("CHWB")
                - 3.256 * delta_GF
                - 2.063 * deltaMwd6()
                ;
    } else if (sqrt_s == 50.0) {
 
        // Mw scheme
 
        C1 = 0.0; // N.A. 
 
        mu +=
                cWsch * (
                +894965. * CHW 
                -5.20074 * CHWB 
                -30691.6 * CHD 
                +120571. * CHbox 
                -121425. * (CHl3R11 + CHl3R22 -CllR1221) 
                +1831037. * CHq3R11 
                +352873. * CHq3R22 
                );
    } else if (sqrt_s == 84.0) {
 
        // Mw scheme
 
        C1 = 0.0; // N.A. 
 
        mu +=
                cWsch * (
                +897281. * CHW 
                -43.9532 * CHWB 
                -30887.3 * CHD 
                +120409. * CHbox 
                -121441. * (CHl3R11 + CHl3R22 -CllR1221) 
                +1828221. * CHq3R11 
                +424079. * CHq3R22 
                );
    } else if (sqrt_s == 100.0) {
 
        // Only Alpha scheme
 
        C1 = 0.0; // N.A. 
 
        mu +=
                +121319. * getSMEFTCoeffEW("CHbox")
                + 2294991. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 159242. * getSMEFTCoeffEW("CHD")
                + 908130. * getSMEFTCoeffEW("CHW")
                - 282574. * getSMEFTCoeffEW("CHWB")
                - 3.259 * delta_GF
                - 2.047 * deltaMwd6()
                ;
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::delta_muWH_1()");
 
    //  Linear contribution from Higgs self-coupling
    mu += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    return mu;
}

◆ delta_muWH_2()

const double NPSMEFTd6General::delta_muWH_2 ( const double sqrt_s ) const

virtual

The SMEFT quadratic correction to the ratio $\mu_{WH}$ between the W-Higgs associated production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 18722 of file NPSMEFTd6General.cpp.

                                                                     {
    double mu = 0.0;
 
    if (FlagQuadraticTerms) {
        if (sqrt_s == 8.0) {
            mu += 0.0;
        } else if (sqrt_s == 13.0) {
            mu += cWsch * (
                    (+(0.014703) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                    + (0.0009196) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                    + (0.46) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                    + (2.6808) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                    + (0.16559) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                    + (0.0036771) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                    + (0.0036771) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                    + (0.0036771) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                    + (-0.00735169) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                    + (0.107336) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                    + (0.20952) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.023682) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (-0.00735169) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.00735169) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.0073527) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.0268286) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHW")
                    + (-0.0523729) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (-0.00592073) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (0.00183843) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.00183843) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.00183825) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.94797) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.100674) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (-0.0536603) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.0536603) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.053669) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.002) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (-0.10475) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.10475) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.104756) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.0118402) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.0118402) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.0118411) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.00735169) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.00735169) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    ) * pow(1000000.0, 2.0)
                    );
            mu += cWsch * ((-0.0007) * pow(deltaGwd6(), 2.0));
 
            mu += cWsch * (
                    +(-0.00019) * deltaGwd6() * getSMEFTCoeffEW("CHbox")
                    + (-0.000155) * deltaGwd6() * getSMEFTCoeffEW("CHD")
                    + (-0.0007) * deltaGwd6() * getSMEFTCoeffEW("CHW")
                    + (-0.0019) * deltaGwd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (-0.0003) * deltaGwd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (-0.00063) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.00063) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.00019) * deltaGwd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    )*1000000;
        } else
            throw std::runtime_error("Bad argument in NPSMEFTd6General::delta_muWH_2()");
    }
 
    //  Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
    //  mu = mu + cLHd6 * cLH3d62 * deltaH3L2(C1) * deltaG_hhhRatio() * deltaG_hhhRatio();
 
    return mu;
}

◆ delta_muZH_1()

const double NPSMEFTd6General::delta_muZH_1 ( const double sqrt_s ) const

virtual

The SMEFT linear correction to the ratio $\mu_{ZH}$ between the Z-Higgs associated production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 18807 of file NPSMEFTd6General.cpp.

                                                                     {
    double mu = 0.0;
    double C1 = 0.0;
    
    double CHB = 0.0, CHW = 0.0, CHWB = 0.0, CHD = 0.0, CHbox = 0.0, CHl3R11 = 0.0;
    double CHl3R22 = 0.0, CllR1221 = 0.0, CHq1R11 = 0.0, CHq3R11 = 0.0, CHq1R22 = 0.0;
    double CHq3R22 = 0.0, CHuR11 = 0.0, CHuR22 = 0.0, CHdR11 = 0.0, CHdR22 = 0.0;
    double muRG = muw;
    
//  Wilson coefficients definitions 
    CHB = getSMEFTCoeff("CHB", muRG); 
    CHW = getSMEFTCoeff("CHW", muRG); 
    CHWB = getSMEFTCoeff("CHWB", muRG); 
    CHD = getSMEFTCoeff("CHD", muRG); 
    CHbox = getSMEFTCoeff("CHbox", muRG); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG); 
    CHq1R11 = getSMEFTCoeff("CHq1R",0,0, muRG); 
    CHq3R11 = getSMEFTCoeff("CHq3R",0,0, muRG); 
    CHq1R22 = getSMEFTCoeff("CHq1R",1,1, muRG); 
    CHq3R22 = getSMEFTCoeff("CHq3R",1,1, muRG); 
    CHuR11 = getSMEFTCoeff("CHuR",0,0, muRG); 
    CHuR22 = getSMEFTCoeff("CHuR",1,1, muRG); 
    CHdR11 = getSMEFTCoeff("CHdR",0,0, muRG); 
    CHdR22 = getSMEFTCoeff("CHdR",1,1, muRG); 
 
    if (sqrt_s == 1.96) {
 
        C1 = 0.0; // N.A.
 
        mu +=
                +121186. * getSMEFTCoeffEW("CHbox")
                + 79191.5 * getSMEFTCoeffEW("CHB")
                + 712325. * getSMEFTCoeffEW("CHW")
                - 813859. * getSMEFTCoeffEW("CHq1R", 0, 0)
                + 3350.92 * getSMEFTCoeffEW("CHq1R", 1, 1)
                + 527754. * getSMEFTCoeffEW("CHuR", 0, 0)
                + 1274.21 * getSMEFTCoeffEW("CHuR", 1, 1)
                - 67806.5 * getSMEFTCoeffEW("CHdR", 0, 0)
                - 1130.86 * getSMEFTCoeffEW("CHdR", 1, 1)
                + 1558454. * getSMEFTCoeffEW("CHq3R", 0, 0)
                + 9076.74 * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-16406.7 * getSMEFTCoeffEW("CHD")
                + 189539. * getSMEFTCoeffEW("CHWB")
                - 2.54 * delta_GF)
                + cWsch * (+38221.8 * getSMEFTCoeffEW("CHD")
                + 309296. * getSMEFTCoeffEW("CHWB")
                - 2. * delta_GF)
                ;
    } else if (sqrt_s == 7.0) {
 
        C1 = 0.0123;
 
        mu +=
                +121226. * getSMEFTCoeffEW("CHbox")
                + 87099.3 * getSMEFTCoeffEW("CHB")
                + 717825. * getSMEFTCoeffEW("CHW")
                - 213136. * getSMEFTCoeffEW("CHq1R", 0, 0)
                + 30259.1 * getSMEFTCoeffEW("CHq1R", 1, 1)
                + 405194. * getSMEFTCoeffEW("CHuR", 0, 0)
                + 16467.8 * getSMEFTCoeffEW("CHuR", 1, 1)
                - 127014. * getSMEFTCoeffEW("CHdR", 0, 0)
                - 12241.3 * getSMEFTCoeffEW("CHdR", 1, 1)
                + 1608269. * getSMEFTCoeffEW("CHq3R", 0, 0)
                + 104261. * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-15321.2 * getSMEFTCoeffEW("CHD")
                + 203123. * getSMEFTCoeffEW("CHWB")
                - 2.506 * delta_GF)
                + cWsch * (+35707.6 * getSMEFTCoeffEW("CHD")
                + 315273. * getSMEFTCoeffEW("CHWB")
                - 1.999 * delta_GF)
                ;
    } else if (sqrt_s == 8.0) {
 
        C1 = 0.0122;
 
        /*mu +=
                +121277. * getSMEFTCoeffEW("CHbox")
                + 87409.1 * getSMEFTCoeffEW("CHB")
                + 721014. * getSMEFTCoeffEW("CHW")
                - 211101. * getSMEFTCoeffEW("CHq1R", 0, 0)
                + 32881.7 * getSMEFTCoeffEW("CHq1R", 1, 1)
                + 409966. * getSMEFTCoeffEW("CHuR", 0, 0)
                + 18389.4 * getSMEFTCoeffEW("CHuR", 1, 1)
                - 129402. * getSMEFTCoeffEW("CHdR", 0, 0)
                - 13507. * getSMEFTCoeffEW("CHdR", 1, 1)
                + 1632382. * getSMEFTCoeffEW("CHq3R", 0, 0)
                + 115538. * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-15333.2 * getSMEFTCoeffEW("CHD")
                + 204451. * getSMEFTCoeffEW("CHWB")
                - 2.506 * delta_GF)
                + cWsch * (+35736.8 * getSMEFTCoeffEW("CHD")
                + 316485. * getSMEFTCoeffEW("CHWB")
                - 2. * delta_GF)
                ;*/
 
        // AG: begin
        mu += cWsch * (
                ((0.121219) * getSMEFTCoeffEW("CHbox")
                + (0.036781) * getSMEFTCoeffEW("CHD")
                + (0.72711) * getSMEFTCoeffEW("CHW")
                + (0.081545) * getSMEFTCoeffEW("CHB")
                + (0.31005) * getSMEFTCoeffEW("CHWB")
                + (-0.19211) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.082808) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (1.61236) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.158059) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.38108) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.0158969) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.1238226) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.02100008) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.12119837) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.12119837) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.121219) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
        //AG:end
    } else if (sqrt_s == 13.0) {
 
        C1 = 0.0119;
 
        /*mu +=
                +121234. * getSMEFTCoeffEW("CHbox")
                + 88512.4 * getSMEFTCoeffEW("CHB")
                + 728790. * getSMEFTCoeffEW("CHW")
                - 196945. * getSMEFTCoeffEW("CHq1R", 0, 0)
                + 43331.9 * getSMEFTCoeffEW("CHq1R", 1, 1)
                + 422018. * getSMEFTCoeffEW("CHuR", 0, 0)
                + 26503. * getSMEFTCoeffEW("CHuR", 1, 1)
                - 136921. * getSMEFTCoeffEW("CHdR", 0, 0)
                - 18730.5 * getSMEFTCoeffEW("CHdR", 1, 1)
                + 1700150. * getSMEFTCoeffEW("CHq3R", 0, 0)
                + 162456. * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-15274.7 * getSMEFTCoeffEW("CHD")
                + 207822. * getSMEFTCoeffEW("CHWB")
                - 2.502 * delta_GF)
                + cWsch * (+35605.2 * getSMEFTCoeffEW("CHD")
                + 319361. * getSMEFTCoeffEW("CHWB")
                - 1.999 * delta_GF)
                ;*/
        // AG: begin
        mu += cWsch * (
                ((0.121184) * getSMEFTCoeffEW("CHbox")
                + (0.036574) * getSMEFTCoeffEW("CHD")
                + (0.73619) * getSMEFTCoeffEW("CHW")
                + (0.082602) * getSMEFTCoeffEW("CHB")
                + (0.31339) * getSMEFTCoeffEW("CHWB")
                + (-0.1927) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.108112) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (1.6542) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.21874) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.39005) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.023369) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.1274518) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.02848691) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.121233) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.121233) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.121184) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
        //AG:end
    } else if (sqrt_s == 14.0) {
 
        // Mw scheme
 
        C1 = 0.0118;
 
        mu +=
                cWsch * (
                +82708.7 * CHB 
                +736201. * CHW 
                +313759. * CHWB 
                +36761.1 * CHD 
                +121603. * CHbox 
                -121162. * (CHl3R11 + CHl3R22 - CllR1221)  
                -232996. * CHq1R11 
                +1675060. * CHq3R11 
                +77454.8 * CHq1R22 
                +203131. * CHq3R22 
                +404665. * CHuR11 
                +26641. * CHuR22 
                -132321. * CHdR11 
                -18720.6 * CHdR22
                );
    } else if (sqrt_s == 27.0) {
 
        // Only Alpha scheme
 
        C1 = 0.0116; // From arXiv: 1902.00134
 
        mu +=
                +121206. * getSMEFTCoeffEW("CHbox")
                - 101865. * getSMEFTCoeffEW("CHq1R", 0, 0)
                + 468029. * getSMEFTCoeffEW("CHuR", 0, 0)
                - 173377. * getSMEFTCoeffEW("CHdR", 0, 0)
                + 2002478. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 15486.3 * getSMEFTCoeffEW("CHD")
                + 89958. * getSMEFTCoeffEW("CHB")
                + 735013. * getSMEFTCoeffEW("CHW")
                + 211026. * getSMEFTCoeffEW("CHWB")
                - 2.505 * delta_GF
                ;
    } else if (sqrt_s == 50.0) {
 
        // Mw scheme
 
        C1 = 0.0; // N.A.
 
        mu +=
                cWsch * (
                +84651.9 * CHB 
                +745844. * CHW 
                +317941. * CHWB 
                +36732.9 * CHD 
                +121413. * CHbox 
                -121096. * (CHl3R11 + CHl3R22 - CllR1221)
                -166824. * CHq1R11 
                +1735550. * CHq3R11 
                +105478. * CHq1R22 
                +357701. * CHq3R22 
                +404281. * CHuR11 
                +53551.6 * CHuR22 
                -142253. * CHdR11 
                -34995.9 * CHdR22
                );
    } else if (sqrt_s == 84.0) {
 
        // Mw scheme
 
        C1 = 0.0; // N.A.
 
        mu +=
                cWsch * (
                +85156.7 * CHB 
                +748204. * CHW 
                +318992. * CHWB 
                +36536.9 * CHD 
                +121415. * CHbox 
                -120911. * (CHl3R11 + CHl3R22 - CllR1221)
                -136107. * CHq1R11 
                +1730540. * CHq3R11 
                +115332. * CHq1R22 
                +424682. * CHq3R22 
                +396960. * CHuR11 
                +65688.9 * CHuR22 
                -144251. * CHdR11 
                -41973.4 * CHdR22 
                );
    } else if (sqrt_s == 100.0) {
 
        // Only Alpha scheme
 
        C1 = 0.0; // N.A.
 
        mu +=
                +121269. * getSMEFTCoeffEW("CHbox")
                + 90.68 * getSMEFTCoeffEW("CHq1R", 0, 0)
                + 484275. * getSMEFTCoeffEW("CHuR", 0, 0)
                - 197878. * getSMEFTCoeffEW("CHdR", 0, 0)
                + 2175601. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 14992.4 * getSMEFTCoeffEW("CHD")
                + 91707.3 * getSMEFTCoeffEW("CHB")
                + 741805. * getSMEFTCoeffEW("CHW")
                + 215319. * getSMEFTCoeffEW("CHWB")
                - 2.504 * delta_GF
                ;
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::delta_muZH_1()");
 
    //  Linear contribution from Higgs self-coupling
    mu += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    return mu;
}

◆ delta_muZH_2()

const double NPSMEFTd6General::delta_muZH_2 ( const double sqrt_s ) const

virtual

The SMEFT quadratic correction to the ratio $\mu_{ZH}$ between the Z-Higgs associated production cross-section in the current model and in the Standard Model.

Reimplemented from NPbase.

Definition at line 19082 of file NPSMEFTd6General.cpp.

                                                                     {
    double mu = 0.0;
 
    if (FlagQuadraticTerms) {
        if (sqrt_s == 8.0) {
            mu += 0.0;
        } else if (sqrt_s == 13.0) {
            mu += cWsch * (
                    (+(0.014709) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                    + (0.0001828) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                    + (0.33883) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                    + (0.03517) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                    + (0.06101) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                    + (2.4309) * pow(getSMEFTCoeffEW("CHq1R", 0, 0), 2.0)
                    + (0.17818) * pow(getSMEFTCoeffEW("CHq1R", 1, 1), 2.0)
                    + (2.4309) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                    + (0.17818) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                    + (1.512) * pow(getSMEFTCoeffEW("CHuR", 0, 0), 2.0)
                    + (0.051115) * pow(getSMEFTCoeffEW("CHuR", 1, 1), 2.0)
                    + (0.9114) * pow(getSMEFTCoeffEW("CHdR", 0, 0), 2.0)
                    + (0.12658) * pow(getSMEFTCoeffEW("CHdR", 1, 1), 2.0)
                    + (0.0036747) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                    + (0.0036747) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                    + (0.0036747) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                    + (0.0007706) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                    + (0.089253) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                    + (0.0100228) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                    + (0.038007) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                    + (-0.023331) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 0, 0)
                    + (0.013107) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 1, 1)
                    + (0.20054) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.02653) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (0.04728) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 0, 0)
                    + (0.0028337) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 1, 1)
                    + (-0.0154464) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 0, 0)
                    + (-0.00345757) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 1, 1)
                    + (-0.00735198) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.00735198) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.0073517) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.023824) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHW")
                    + (-0.0186024) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHB")
                    + (-0.0163142) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                    + (-0.0223393) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 0, 0)
                    + (-0.00245371) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 1, 1)
                    + (0.0083336) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (-0.00056189) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (-0.0522227) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 0, 0)
                    + (-0.003119027) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 1, 1)
                    + (0.017032) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 0, 0)
                    + (0.0038028) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 1, 1)
                    + (-0.00222376) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.00222376) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.0022196) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.003359) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                    + (0.21456) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                    + (-0.17418) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 0, 0)
                    + (0.042875) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 1, 1)
                    + (0.84884) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.099481) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (0.0184103) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 0, 0)
                    + (0.0012777) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 1, 1)
                    + (-0.00612324) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHdR", 0, 0)
                    + (-0.00153483) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHdR", 1, 1)
                    + (-0.0446364) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.0446364) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.044638) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.073521) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                    + (0.071113) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                    + (0.0100257) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                    + (0.006735) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.0069349) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (0.183946) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHuR", 0, 0)
                    + (0.0100203) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHuR", 1, 1)
                    + (-0.059448) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 0, 0)
                    + (-0.0123557) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 1, 1)
                    + (-0.0050083) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.0050083) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.0050114) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.009927) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                    + (0.021428) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                    + (0.29213) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.038981) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (0.132604) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 0, 0)
                    + (0.0070524) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 1, 1)
                    + (-0.0427501) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 0, 0)
                    + (-0.008726) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 1, 1)
                    + (-0.0190091) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.0190091) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.0190052) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-1.1966) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (0.011703) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.011703) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.01167) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.15048) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                    + (-0.0065592) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.0065592) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.0065532) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.100277) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.100277) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.100266) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.0132704) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.0132704) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.0132638) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.02364103) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.02364103) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.023635) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.001417969) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (-0.001417969) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (0.00141704) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.0077183) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.0077183) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.0077248) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (0.0017279) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.0017279) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                    + (-0.00172848) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.00735198) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    + (-0.00735198) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                    ) * pow(1000000.0, 2.0)
                    );
 
            mu += cWsch * ((0.008) * pow(deltaGzd6(), 2.0));
 
            mu += cWsch * (
                    +(0.00021) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                    + (-0.0015) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                    + (0.0007) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                    + (-0.0007) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                    + (-0.014) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 0, 0)
                    + (0.0024) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                    + (-0.0012) * deltaGzd6() * getSMEFTCoeffEW("CHuR", 0, 0)
                    + (0.00084) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 0, 0)
                    + (0.00045) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + (0.00016) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                    )*1000000;
        } else
            throw std::runtime_error("Bad argument in NPSMEFTd6General::delta_muZH_2()");
    }
 
    //  Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
    //  mu = mu + cLHd6 * cLH3d62 * deltaH3L2(C1) * deltaG_hhhRatio() * deltaG_hhhRatio();
 
    return mu;
}

◆ delta_Qwemoller()

const double NPSMEFTd6General::delta_Qwemoller	(	const double	q2,
		const double	y
	)		const

virtual

The computation of the electron's weak charge.

Parameters

[in]	q2	the $Q^2$ at which the weak charge is measured
[in]	y

Returns: $Q_{w}(e)$

Definition at line 46940 of file NPSMEFTd6General.cpp.

                                                                                    {
    double deltaQ;
    double deltaCe;
 
    double dCeeVRR1111, dCeeVLL1111; // NP corrections to LEFT operators at low energy 
 
    dCeeVRR1111 = (getMatching().getCeeVRR(0, 0, 0, 0)).real();
    dCeeVLL1111 = (getMatching().getCeeVLL(0, 0, 0, 0)).real(); //RGE effects very small
 
    // Modification in terms of the LEFT basis (at low energies)
    deltaCe = (1. / GF / sqrt(2.)) * (dCeeVRR1111 - dCeeVLL1111);
 
    //double dgLe, dgRe, gLe, gRe;
 
    //dgLe = deltaGL_f(leptons[ELECTRON]);
    //dgRe = deltaGR_f(leptons[ELECTRON]);
 
    //gLe = gZlL;
    //gRe = gZlR;
 
    //deltaQ = trueSM.Qwemoller(q2,y) * ((dgLe - dgRe)/(gLe - gRe) + (dgLe + dgRe)/(gLe + gRe));
 
    //deltaQ += (getSMEFTCoeffEW("CllR", 0, 0, 0, 0) - getSMEFTCoeffEW("CeeR", 0, 0, 0, 0)) * v2; 
 
    deltaQ = -2. * deltaCe;
 
    return deltaQ;
}

◆ delta_Qwn()

const double NPSMEFTd6General::delta_Qwn ( ) const

virtual

The computation of the neutron weak charge: Qwn.

Returns: $Q_{W}(n)$

Definition at line 47000 of file NPSMEFTd6General.cpp.

                                               {
    double deltaQ;
    double deltaC1u, deltaC1d;
 
    double dCeuVLL1111, dCeuVRR1111, dCeuVLR1111, dCueVLR1111; // NP corrections to LEFT operators at low energy
    double dCedVLL1111, dCedVRR1111, dCedVLR1111, dCdeVLR1111; // NP corrections to LEFT operators at low energy
 
    dCeuVLL1111 = (getMatching().getCeuVLL(0, 0, 0, 0)).real();
    dCeuVRR1111 = (getMatching().getCeuVRR(0, 0, 0, 0)).real();
    dCeuVLR1111 = (getMatching().getCeuVLR(0, 0, 0, 0)).real();
    dCueVLR1111 = (getMatching().getCueVLR(0, 0, 0, 0)).real(); //RGE effects very small
 
    dCedVLL1111 = (getMatching().getCedVLL(0, 0, 0, 0)).real();
    dCedVRR1111 = (getMatching().getCedVRR(0, 0, 0, 0)).real();
    dCedVLR1111 = (getMatching().getCedVLR(0, 0, 0, 0)).real();
    dCdeVLR1111 = (getMatching().getCdeVLR(0, 0, 0, 0)).real(); //RGE effects very small
 
    // Modification in terms of the LEFT basis (at low energies)
    deltaC1u = (1. / GF / 2. / sqrt(2.)) * (-dCeuVLL1111 + dCeuVRR1111 - dCeuVLR1111 + dCueVLR1111);
    deltaC1d = (1. / GF / 2. / sqrt(2.)) * (-dCedVLL1111 + dCedVRR1111 - dCedVLR1111 + dCdeVLR1111);
 
    // Neutron Z=0, N=1
    deltaQ = -2. * (deltaC1u + 2. * deltaC1d);
 
    return deltaQ;
}

◆ delta_Qwp()

const double NPSMEFTd6General::delta_Qwp ( ) const

virtual

The computation of the proton weak charge: Qwp.

Returns: $Q_{W}(p)$

Definition at line 46973 of file NPSMEFTd6General.cpp.

                                               {
    double deltaQ;
    double deltaC1u, deltaC1d;
 
    double dCeuVLL1111, dCeuVRR1111, dCeuVLR1111, dCueVLR1111; // NP corrections to LEFT operators at low energy
    double dCedVLL1111, dCedVRR1111, dCedVLR1111, dCdeVLR1111; // NP corrections to LEFT operators at low energy
 
    dCeuVLL1111 = (getMatching().getCeuVLL(0, 0, 0, 0)).real();
    dCeuVRR1111 = (getMatching().getCeuVRR(0, 0, 0, 0)).real();
    dCeuVLR1111 = (getMatching().getCeuVLR(0, 0, 0, 0)).real();
    dCueVLR1111 = (getMatching().getCueVLR(0, 0, 0, 0)).real(); //RGE effects very small
 
    dCedVLL1111 = (getMatching().getCedVLL(0, 0, 0, 0)).real();
    dCedVRR1111 = (getMatching().getCedVRR(0, 0, 0, 0)).real();
    dCedVLR1111 = (getMatching().getCedVLR(0, 0, 0, 0)).real();
    dCdeVLR1111 = (getMatching().getCdeVLR(0, 0, 0, 0)).real(); //RGE effects very small
 
    // Modification in terms of the LEFT basis (at low energies)
    deltaC1u = (1. / GF / 2. / sqrt(2.)) * (-dCeuVLL1111 + dCeuVRR1111 - dCeuVLR1111 + dCueVLR1111);
    deltaC1d = (1. / GF / 2. / sqrt(2.)) * (-dCedVLL1111 + dCedVRR1111 - dCedVLR1111 + dCdeVLR1111);
 
    // Proton Z=1, N=0
    deltaQ = -2. * (2. * deltaC1u + deltaC1d);
 
    return deltaQ;
}

◆ delta_sigma_ee()

const double NPSMEFTd6General::delta_sigma_ee	(	const double	pol_e,
		const double	pol_p,
		const double	s,
		const double	cosmin,
		const double	cosmax
	)		const

virtual

Definition at line 46864 of file NPSMEFTd6General.cpp.

                                                                                                                                                    {
 
    double sumM2, dsigma;
    double topb = 0.3894e+9; 
    double t0, t1, lambdaK;
    
    double pLH, pRH; //Polarization factors, minus the 1/4 average
    double pLLH, pRRH; 
    
    pLH = (1.0 - pol_e) * (1.0 + pol_p);
    pRH = (1.0 + pol_e) * (1.0 - pol_p);
    
    pLLH = (1.0 - pol_e) * (1.0 - pol_p);
    pRRH = (1.0 + pol_e) * (1.0 + pol_p);
    
    // t values for cosmin and cosmax
    t0 = 0.5 * s * ( -1.0 + cosmin );
    t1 = 0.5 * s * ( -1.0 + cosmax );
    
    // Kähllén function of (s,0,0)
    lambdaK = s*s;
    
    // Sum of the integrals of the amplitudes squared x (t/s)^2, (s/t)^2, (u/s)^2 
    sumM2 = pLH * intDMLL2eus2(s, t0, t1) + pRH * intDMRR2eus2(s, t0, t1) +
            pLH * intDMLR2ets2(s, t0, t1) + pRH * intDMRL2ets2(s, t0, t1) + 
            pLLH * intDMLR2etildest2(s, t0, t1) + pRRH * intDMRL2etildest2(s, t0, t1);   
    
    // Build the cross section
    dsigma = M_PI * (trueSM.alphaMz())*(trueSM.alphaMz()) * sumM2 / s / sqrt(lambdaK);
    
    return topb * dsigma;
}

◆ delta_sigma_f()

const double NPSMEFTd6General::delta_sigma_f	(	const Particle	f,
		const double	pol_e,
		const double	pol_p,
		const double	s,
		const double	cosmin,
		const double	cosmax
	)		const

virtual

Definition at line 46543 of file NPSMEFTd6General.cpp.

                                                                                                                                                                     {
    //  Only valid for f=/=e (MLL2, MRR2 do not depend on t for f=/=e. Simply enter t=1 as argument)
    double sumM2, dsigma;
    double tdumm = 1.;
    double topb = 0.3894e+9;
 
    double Nf;
    
    double pLH, pRH; //Polarization factors, minus the 1/4 average
    
    pLH = (1.0 - pol_e) * (1.0 + pol_p);
    pRH = (1.0 + pol_e) * (1.0 - pol_p);
 
    //if (f.is("LEPTON")) {
    if ( f.getIndex() < 6 ) {
        Nf = 1.0;
    } else {
        Nf = 3.0;
    }
 
    sumM2 = (pLH * deltaMLR2_f(f, s) + pRH * deltaMRL2_f(f, s)) * tovers2(cosmin, cosmax)
            + (pLH * deltaMLL2_f(f, s, tdumm) + pRH * deltaMRR2_f(f, s, tdumm)) * uovers2(cosmin, cosmax);
 
    dsigma = Nf * 0.5 * M_PI * (trueSM.alphaMz())*(trueSM.alphaMz()) * sumM2 / s;
 
    return topb * dsigma;
}

◆ delta_sigma_had()

const double NPSMEFTd6General::delta_sigma_had	(	const double	pol_e,
		const double	pol_p,
		const double	s,
		const double	cosmin,
		const double	cosmax
	)		const

virtual

Definition at line 46571 of file NPSMEFTd6General.cpp.

                                                                                                                                                     {
    double dsigma;
 
    dsigma = delta_sigma_f(quarks[UP], pol_e, pol_p, s, cosmin, cosmax) + delta_sigma_f(quarks[DOWN], pol_e, pol_p, s, cosmin, cosmax)
            + delta_sigma_f(quarks[CHARM], pol_e, pol_p, s, cosmin, cosmax) + delta_sigma_f(quarks[STRANGE], pol_e, pol_p, s, cosmin, cosmax)
            + delta_sigma_f(quarks[BOTTOM], pol_e, pol_p, s, cosmin, cosmax);
 
    return dsigma;
}

◆ delta_sigmaTot_ee()

const double NPSMEFTd6General::delta_sigmaTot_ee	(	const double	pol_e,
		const double	pol_p,
		const double	s
	)		const

virtual

Definition at line 46898 of file NPSMEFTd6General.cpp.

                                                                                                             {
    double coscut = 0.90; // As in LEP2
    return delta_sigma_ee(pol_e, pol_p, s, -coscut, coscut);
}

◆ delta_sigmaTot_f()

const double NPSMEFTd6General::delta_sigmaTot_f	(	const Particle	f,
		const double	pol_e,
		const double	pol_p,
		const double	s
	)		const

virtual

Definition at line 46581 of file NPSMEFTd6General.cpp.

                                                                                                                              {
    return delta_sigma_f(f, pol_e, pol_p, s, -1., 1.);
}

◆ delta_TauLFU_gmuge()

const double NPSMEFTd6General::delta_TauLFU_gmuge ( ) const

virtual

The computation of the correction to the LFU ratio $g_\mu/ g_e $.

Returns: $\delta g_\mu/ g_e $

Definition at line 47100 of file NPSMEFTd6General.cpp.

                                                        {
    double dCnueVLL3223, dCnueVLL3113, delta;
 
    dCnueVLL3223 = (getMatching().getCnueVLL(2, 1, 1, 2)).real();
    dCnueVLL3113 = (getMatching().getCnueVLR(2, 0, 0, 2)).real();
 
    // Modification in terms of the LEFT basis (at low energies)        
    delta = (-1. / GF / 2. / sqrt(2.)) * (dCnueVLL3223 - dCnueVLL3113);
 
    return (trueSM.TauLFU_gmuge())*delta;
}

◆ delta_TauLFU_gtauge()

const double NPSMEFTd6General::delta_TauLFU_gtauge ( ) const

virtual

The computation of the correction to the LFU ratio $g_\tau/ g_e $.

Returns: $\delta g_\tau/ g_e $

Definition at line 47124 of file NPSMEFTd6General.cpp.

                                                         {
    double dCnueVLL3223, dCnueVLL2112, delta;
 
    dCnueVLL3223 = (getMatching().getCnueVLL(2, 1, 1, 2)).real();
    dCnueVLL2112 = (getMatching().getCnueVLR(1, 0, 0, 1)).real();
 
    // Modification in terms of the LEFT basis (at low energies)        
    delta = (-1. / GF / 2. / sqrt(2.)) * (dCnueVLL3223 - dCnueVLL2112);
 
    return (trueSM.TauLFU_gtauge())*delta;
}

◆ delta_TauLFU_gtaugmu()

const double NPSMEFTd6General::delta_TauLFU_gtaugmu ( ) const

virtual

The computation of the correction to the LFU ratio $g_\tau/ g_\mu $.

Returns: $\delta g_\tau/ g_\mu $

Definition at line 47112 of file NPSMEFTd6General.cpp.

                                                          {
    double dCnueVLL3113, dCnueVLL2112, delta;
 
    dCnueVLL3113 = (getMatching().getCnueVLL(2, 0, 0, 2)).real();
    dCnueVLL2112 = (getMatching().getCnueVLR(1, 0, 0, 1)).real();
 
    // Modification in terms of the LEFT basis (at low energies)        
    delta = (-1. / GF / 2. / sqrt(2.)) * (dCnueVLL3113 - dCnueVLL2112);
 
    return (trueSM.TauLFU_gtaugmu())*delta;
}

◆ delta_TauLFU_gtaugmuK()

const double NPSMEFTd6General::delta_TauLFU_gtaugmuK ( ) const

virtual

The computation of the correction to the LFU ratio $\left(g_\tau/ g_\mu\right)_K $.

Returns: $\delta\left(g_\tau/ g_\mu\right)_K $

Definition at line 47165 of file NPSMEFTd6General.cpp.

                                                           {
    // Follow Eqs. A.1, A.2 in 2311.00020 
    double dCnueduVLL3321, dCnueduVLL2221;
    double dCnueduSRL3321, dCnueduSRL2221;
    double Vus, mK, chitauK, chimuK, etaS;
    double delta;
 
    Vus = 0.2243; // PDG 2023
    mK = 0.493677; // From PDG 2024 in GeV
 
    chitauK = mK * mK / (leptons[TAU].getMass()) / (quarks[STRANGE].getMass() + quarks[UP].getMass());
    chimuK = chitauK * (leptons[TAU].getMass()) / (leptons[MU].getMass());
 
    etaS = 1.57;
 
    // Vector operators
    dCnueduVLL3321 = ((getMatching().getCnueduVLL(2, 2, 1, 0)) / Vus).real();
    dCnueduVLL2221 = ((getMatching().getCnueduVLL(1, 1, 1, 0)) / Vus).real();
 
    // Scalar operators
    dCnueduSRL3321 = etaS * ((getMatching().getCnueduSRL(2, 2, 1, 0)) / Vus).real();
    dCnueduSRL2221 = etaS * ((getMatching().getCnueduSRL(1, 1, 1, 0)) / Vus).real();
 
    // Modification in terms of the LEFT basis (at low energies)        
    delta = (-1. / GF / 2. / sqrt(2.)) * (dCnueduVLL3321 - dCnueduVLL2221 + chitauK * dCnueduSRL3321 - chimuK * dCnueduSRL2221);
 
    return delta;
}

◆ delta_TauLFU_gtaugmuPi()

const double NPSMEFTd6General::delta_TauLFU_gtaugmuPi ( ) const

virtual

The computation of the correction to the LFU ratio $\left(g_\tau/ g_\mu\right)_\pi $.

Returns: $\delta \left(g_\tau/ g_\mu\right)_\pi $

Definition at line 47136 of file NPSMEFTd6General.cpp.

                                                            {
    // Follow Eqs. A.1, A.2 in 2311.00020 
    double dCnueduVLL3311, dCnueduVLL2211;
    double dCnueduSRL3311, dCnueduSRL2211;
    double Vud, mPi, chitauPi, chimuPi, etaS;
    double delta;
 
    Vud = 0.97373; // PDG 2023
    mPi = 0.13957039; // From PDG 2024 in GeV
 
    chitauPi = mPi * mPi / (leptons[TAU].getMass()) / (quarks[DOWN].getMass() + quarks[UP].getMass());
    chimuPi = chitauPi * (leptons[TAU].getMass()) / (leptons[MU].getMass());
 
    etaS = 1.57;
 
    // Vector operators
    dCnueduVLL3311 = ((getMatching().getCnueduVLL(2, 2, 0, 0)) / Vud).real();
    dCnueduVLL2211 = ((getMatching().getCnueduVLL(1, 1, 0, 0)) / Vud).real();
 
    // Scalar operators
    dCnueduSRL3311 = etaS * ((getMatching().getCnueduSRL(2, 2, 0, 0)) / Vud).real();
    dCnueduSRL2211 = etaS * ((getMatching().getCnueduSRL(1, 1, 0, 0)) / Vud).real();
 
    // Modification in terms of the LEFT basis (at low energies)        
    delta = (-1. / GF / 2. / sqrt(2.)) * (dCnueduVLL3311 - dCnueduVLL2211 + chitauPi * dCnueduSRL3311 - chimuPi * dCnueduSRL2211);
 
    return delta;
}

◆ deltaa0()

const double NPSMEFTd6General::deltaa0 ( ) const

virtual

The relative correction to the electromagnetic constant at zero momentum, $\delta \alpha(0)/\alpha(0)$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $\delta \alpha(0)/\alpha(0)$

Definition at line 15526 of file NPSMEFTd6General.cpp.

                                             {
    //  Ref. value used in MG simulations
    return ( (aleMz - 0.0072973525664) / 0.0072973525664);
}

◆ deltaa02()

const double NPSMEFTd6General::deltaa02 ( ) const

virtual

The relative correction to the electromagnetic constant at zero momentum, $(\delta \alpha(0)/\alpha(0))^2$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $(\delta \alpha(0)/\alpha(0))^2$

Definition at line 15531 of file NPSMEFTd6General.cpp.

                                              {
    return ( 0.0);
}

◆ deltaA_f()

const double NPSMEFTd6General::deltaA_f ( const Particle f ) const

virtual

The new physics contribution to the left-right asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $\delta \mathcal{A}_f$.

Parameters

[in] f a lepton or quark

Returns: $\delta \mathcal{A}_f$

Reimplemented from NPbase.

Definition at line 16347 of file NPSMEFTd6General.cpp.

{
    double dAf = 0.;
    double delGVf = deltaGV_f(f);
    double delGAf = deltaGA_f(f);
    
    double deltaNLO;  
    
    if (delGVf != 0.0 || delGAf != 0.0) {
        double gVf = trueSM.gV_f(f).real();
        double gAf = trueSM.gA_f(f).real();
        double Gf = gVf * gVf + gAf*gAf;
        double delGVfOverGAf = (gAf * delGVf - gVf * delGAf) / gAf / gAf;
 
        dAf = -2.0 * (gVf * gVf - gAf * gAf) * gAf * gAf / Gf / Gf*delGVfOverGAf;
    }
 
    // Finite NLO corrections: Not available for u and d    
    switch(f.getIndex()){
    //if (f.is("ELECTRON")) {
        case 1:
            deltaNLO = (+0.018161 * getSMEFTCoeffEW("CW")  +0.00453 * getSMEFTCoeffEW("CHbox")  +0.237511 * getSMEFTCoeffEW("CHD")  +0.001559 * getSMEFTCoeffEW("CHB")   
            +0.002674 * getSMEFTCoeffEW("CHW")  +0.283607 * getSMEFTCoeffEW("CHWB")  -0.034521 * getSMEFTCoeffEW("CuWR",2, 2) +0.048793 * getSMEFTCoeffEW("CuBR",2, 2)  
            +0.163367 * getSMEFTCoeffEW("CHl1R",0, 0) +0.002591 * getSMEFTCoeffEW("CHl1R",1, 1) +0.002591 * getSMEFTCoeffEW("CHl1R",2, 2) +0.223109 * getSMEFTCoeffEW("CHl3R",0, 0)  
            +0.072891 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000142 * getSMEFTCoeffEW("CHl3R",2, 2) +0.034734 * getSMEFTCoeffEW("CHeR",0, 0) +0.002591 * getSMEFTCoeffEW("CHeR",1, 1)  
            +0.002591 * getSMEFTCoeffEW("CHeR",2, 2) -0.002591 * getSMEFTCoeffEW("CHq1R",0, 0) -0.002591 * getSMEFTCoeffEW("CHq1R",1, 1) +0.222737 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.000425 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000425 * getSMEFTCoeffEW("CHq3R",1, 1) -0.139992 * getSMEFTCoeffEW("CHq3R",2, 2) -0.005181 * getSMEFTCoeffEW("CHuR",0, 0)  
            -0.005181 * getSMEFTCoeffEW("CHuR",1, 1) -0.272811 * getSMEFTCoeffEW("CHuR",2, 2) +0.002591 * getSMEFTCoeffEW("CHdR",0, 0) +0.002591 * getSMEFTCoeffEW("CHdR",1, 1)  
            +0.002591 * getSMEFTCoeffEW("CHdR",2, 2) +0.000753 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) +0.001491 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.001491 * getSMEFTCoeffEW("CllR",0, 0, 2, 2)  
            -0.073487 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000738 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) -0.000745 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) -0.000745 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1)  
            +0.032966 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) -0.007772 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.007772 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) -0.041483 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
            +0.002583 * getSMEFTCoeffEW("CeeR",0, 0, 0, 0) +0.002583 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1) +0.002583 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2) -0.001845 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0)  
            -0.001845 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1) -0.047901 * getSMEFTCoeffEW("CeuR",0, 0, 2, 2) +0.000923 * getSMEFTCoeffEW("CedR",0, 0, 0, 0) +0.000923 * getSMEFTCoeffEW("CedR",0, 0, 1, 1)  
            +0.000923 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) +0.001668 * getSMEFTCoeffEW("CleR",0, 0, 0, 0) +0.000745 * getSMEFTCoeffEW("CleR",0, 0, 1, 1) +0.000745 * getSMEFTCoeffEW("CleR",0, 0, 2, 2)  
            +0.000923 * getSMEFTCoeffEW("CleR",1, 1, 0, 0) +0.000923 * getSMEFTCoeffEW("CleR",2, 2, 0, 0) -0.001491 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) -0.001491 * getSMEFTCoeffEW("CluR",0, 0, 1, 1)  
            -0.038706 * getSMEFTCoeffEW("CluR",0, 0, 2, 2) +0.000745 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) +0.000745 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) +0.000745 * getSMEFTCoeffEW("CldR",0, 0, 2, 2)  
            -0.000923 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0) -0.000923 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0) +0.040798 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0) ) * v2; 
        break;
    //} else if (f.is("MUON")) {
        case 3:
            deltaNLO = (+0.018161 * getSMEFTCoeffEW("CW")  +0.00453 * getSMEFTCoeffEW("CHbox")  +0.237511 * getSMEFTCoeffEW("CHD")  +0.001559 * getSMEFTCoeffEW("CHB")   
            +0.002674 * getSMEFTCoeffEW("CHW")  +0.283607 * getSMEFTCoeffEW("CHWB")  -0.034521 * getSMEFTCoeffEW("CuWR",2, 2) +0.048793 * getSMEFTCoeffEW("CuBR",2, 2)  
            +0.002591 * getSMEFTCoeffEW("CHl1R",0, 0) +0.163367 * getSMEFTCoeffEW("CHl1R",1, 1) +0.002591 * getSMEFTCoeffEW("CHl1R",2, 2) +0.072891 * getSMEFTCoeffEW("CHl3R",0, 0)  
            +0.223109 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000142 * getSMEFTCoeffEW("CHl3R",2, 2) +0.002591 * getSMEFTCoeffEW("CHeR",0, 0) +0.034734 * getSMEFTCoeffEW("CHeR",1, 1)  
            +0.002591 * getSMEFTCoeffEW("CHeR",2, 2) -0.002591 * getSMEFTCoeffEW("CHq1R",0, 0) -0.002591 * getSMEFTCoeffEW("CHq1R",1, 1) +0.222737 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.000425 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000425 * getSMEFTCoeffEW("CHq3R",1, 1) -0.139992 * getSMEFTCoeffEW("CHq3R",2, 2) -0.005181 * getSMEFTCoeffEW("CHuR",0, 0)  
            -0.005181 * getSMEFTCoeffEW("CHuR",1, 1) -0.272811 * getSMEFTCoeffEW("CHuR",2, 2) +0.002591 * getSMEFTCoeffEW("CHdR",0, 0) +0.002591 * getSMEFTCoeffEW("CHdR",1, 1)  
            +0.002591 * getSMEFTCoeffEW("CHdR",2, 2) +0.001491 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) -0.073487 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) +0.000753 * getSMEFTCoeffEW("CllR",1, 1, 1, 1)  
            +0.001491 * getSMEFTCoeffEW("CllR",1, 1, 2, 2) -0.000738 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) -0.000745 * getSMEFTCoeffEW("Clq1R",1, 1, 0, 0) -0.000745 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1)  
            +0.032966 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2) -0.007772 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0) -0.007772 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) -0.041483 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2)  
            +0.002583 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1) +0.002583 * getSMEFTCoeffEW("CeeR",1, 1, 1, 1) +0.002583 * getSMEFTCoeffEW("CeeR",1, 1, 2, 2) -0.001845 * getSMEFTCoeffEW("CeuR",1, 1, 0, 0)  
            -0.001845 * getSMEFTCoeffEW("CeuR",1, 1, 1, 1) -0.047901 * getSMEFTCoeffEW("CeuR",1, 1, 2, 2) +0.000923 * getSMEFTCoeffEW("CedR",1, 1, 0, 0) +0.000923 * getSMEFTCoeffEW("CedR",1, 1, 1, 1)  
            +0.000923 * getSMEFTCoeffEW("CedR",1, 1, 2, 2) +0.000923 * getSMEFTCoeffEW("CleR",0, 0, 1, 1) +0.000745 * getSMEFTCoeffEW("CleR",1, 1, 0, 0) +0.001668 * getSMEFTCoeffEW("CleR",1, 1, 1, 1)  
            +0.000745 * getSMEFTCoeffEW("CleR",1, 1, 2, 2) +0.000923 * getSMEFTCoeffEW("CleR",2, 2, 1, 1) -0.001491 * getSMEFTCoeffEW("CluR",1, 1, 0, 0) -0.001491 * getSMEFTCoeffEW("CluR",1, 1, 1, 1)  
            -0.038706 * getSMEFTCoeffEW("CluR",1, 1, 2, 2) +0.000745 * getSMEFTCoeffEW("CldR",1, 1, 0, 0) +0.000745 * getSMEFTCoeffEW("CldR",1, 1, 1, 1) +0.000745 * getSMEFTCoeffEW("CldR",1, 1, 2, 2)  
            -0.000923 * getSMEFTCoeffEW("CqeR",0, 0, 1, 1) -0.000923 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1) +0.040798 * getSMEFTCoeffEW("CqeR",2, 2, 1, 1) ) * v2; 
        break;
    //} else if (f.is("TAU")) {
        case 5:
            deltaNLO = (+0.018161 * getSMEFTCoeffEW("CW")  +0.00453 * getSMEFTCoeffEW("CHbox")  +0.237511 * getSMEFTCoeffEW("CHD")  +0.001559 * getSMEFTCoeffEW("CHB")   
            +0.002674 * getSMEFTCoeffEW("CHW")  +0.283607 * getSMEFTCoeffEW("CHWB")  -0.034521 * getSMEFTCoeffEW("CuWR",2, 2) +0.048793 * getSMEFTCoeffEW("CuBR",2, 2)  
            +0.002591 * getSMEFTCoeffEW("CHl1R",0, 0) +0.002591 * getSMEFTCoeffEW("CHl1R",1, 1) +0.163367 * getSMEFTCoeffEW("CHl1R",2, 2) +0.072891 * getSMEFTCoeffEW("CHl3R",0, 0)  
            +0.072891 * getSMEFTCoeffEW("CHl3R",1, 1) +0.15036 * getSMEFTCoeffEW("CHl3R",2, 2) +0.002591 * getSMEFTCoeffEW("CHeR",0, 0) +0.002591 * getSMEFTCoeffEW("CHeR",1, 1)  
            +0.034734 * getSMEFTCoeffEW("CHeR",2, 2) -0.002591 * getSMEFTCoeffEW("CHq1R",0, 0) -0.002591 * getSMEFTCoeffEW("CHq1R",1, 1) +0.222737 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.000425 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000425 * getSMEFTCoeffEW("CHq3R",1, 1) -0.139992 * getSMEFTCoeffEW("CHq3R",2, 2) -0.005181 * getSMEFTCoeffEW("CHuR",0, 0)  
            -0.005181 * getSMEFTCoeffEW("CHuR",1, 1) -0.272811 * getSMEFTCoeffEW("CHuR",2, 2) +0.002591 * getSMEFTCoeffEW("CHdR",0, 0) +0.002591 * getSMEFTCoeffEW("CHdR",1, 1)  
            +0.002591 * getSMEFTCoeffEW("CHdR",2, 2) +0.001491 * getSMEFTCoeffEW("CllR",0, 0, 2, 2) -0.072749 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000738 * getSMEFTCoeffEW("CllR",0, 2, 2, 0)  
            +0.001491 * getSMEFTCoeffEW("CllR",1, 1, 2, 2) -0.000738 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) +0.000753 * getSMEFTCoeffEW("CllR",2, 2, 2, 2) -0.000745 * getSMEFTCoeffEW("Clq1R",2, 2, 0, 0)  
            -0.000745 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1) +0.032966 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2) -0.007772 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0) -0.007772 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1)  
            -0.041483 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) +0.002583 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2) +0.002583 * getSMEFTCoeffEW("CeeR",1, 1, 2, 2) +0.002583 * getSMEFTCoeffEW("CeeR",2, 2, 2, 2)  
            -0.001845 * getSMEFTCoeffEW("CeuR",2, 2, 0, 0) -0.001845 * getSMEFTCoeffEW("CeuR",2, 2, 1, 1) -0.047901 * getSMEFTCoeffEW("CeuR",2, 2, 2, 2) +0.000923 * getSMEFTCoeffEW("CedR",2, 2, 0, 0)  
            +0.000923 * getSMEFTCoeffEW("CedR",2, 2, 1, 1) +0.000923 * getSMEFTCoeffEW("CedR",2, 2, 2, 2) +0.000923 * getSMEFTCoeffEW("CleR",0, 0, 2, 2) +0.000923 * getSMEFTCoeffEW("CleR",1, 1, 2, 2)  
            +0.000745 * getSMEFTCoeffEW("CleR",2, 2, 0, 0) +0.000745 * getSMEFTCoeffEW("CleR",2, 2, 1, 1) +0.001668 * getSMEFTCoeffEW("CleR",2, 2, 2, 2) -0.001491 * getSMEFTCoeffEW("CluR",2, 2, 0, 0)  
            -0.001491 * getSMEFTCoeffEW("CluR",2, 2, 1, 1) -0.038706 * getSMEFTCoeffEW("CluR",2, 2, 2, 2) +0.000745 * getSMEFTCoeffEW("CldR",2, 2, 0, 0) +0.000745 * getSMEFTCoeffEW("CldR",2, 2, 1, 1)  
            +0.000745 * getSMEFTCoeffEW("CldR",2, 2, 2, 2) -0.000923 * getSMEFTCoeffEW("CqeR",0, 0, 2, 2) -0.000923 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) +0.040798 * getSMEFTCoeffEW("CqeR",2, 2, 2, 2) ) * v2; 
        break;
    //} else if (f.is("STRANGE")) {
        case 9:
            deltaNLO = (+0.001425 * getSMEFTCoeffEW("CW")  +0.000355 * getSMEFTCoeffEW("CHbox")  +0.026008 * getSMEFTCoeffEW("CHD")  +0.000122 * getSMEFTCoeffEW("CHB")   
            +0.00021 * getSMEFTCoeffEW("CHW")  +0.030199 * getSMEFTCoeffEW("CHWB")  -0.002708 * getSMEFTCoeffEW("CuWR",2, 2) +0.003828 * getSMEFTCoeffEW("CuBR",2, 2)  
            +0.000203 * getSMEFTCoeffEW("CHl1R",0, 0) +0.000203 * getSMEFTCoeffEW("CHl1R",1, 1) +0.000203 * getSMEFTCoeffEW("CHl1R",2, 2) +0.005585 * getSMEFTCoeffEW("CHl3R",0, 0)  
            +0.005585 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000203 * getSMEFTCoeffEW("CHeR",0, 0) +0.000203 * getSMEFTCoeffEW("CHeR",1, 1) +0.000203 * getSMEFTCoeffEW("CHeR",2, 2)  
            -0.000203 * getSMEFTCoeffEW("CHq1R",0, 0) +0.016811 * getSMEFTCoeffEW("CHq1R",1, 1) +0.017474 * getSMEFTCoeffEW("CHq1R",2, 2) +0.000033 * getSMEFTCoeffEW("CHq3R",0, 0)  
            +0.016348 * getSMEFTCoeffEW("CHq3R",1, 1) -0.010982 * getSMEFTCoeffEW("CHq3R",2, 2) -0.000406 * getSMEFTCoeffEW("CHuR",0, 0) -0.000406 * getSMEFTCoeffEW("CHuR",1, 1)  
            -0.021402 * getSMEFTCoeffEW("CHuR",2, 2) +0.000203 * getSMEFTCoeffEW("CHdR",0, 0) +0.057219 * getSMEFTCoeffEW("CHdR",1, 1) +0.000203 * getSMEFTCoeffEW("CHdR",2, 2)  
            -0.005574 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000117 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1) -0.000089 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) -0.000206 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1)  
            +0.005172 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2) -0.000089 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) -0.001219 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1) +0.000058 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0)  
            -0.001161 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1) -0.006509 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) +0.006967 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1) +0.000058 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1)  
            +0.000058 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1) +0.000058 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1) -0.000203 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) -0.000203 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1)  
            -0.000203 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1) +0.000668 * getSMEFTCoeffEW("CddR",0, 0, 1, 1) +0.000089 * getSMEFTCoeffEW("CddR",0, 1, 1, 0) +0.000757 * getSMEFTCoeffEW("CddR",1, 1, 1, 1)  
            +0.000668 * getSMEFTCoeffEW("CddR",1, 1, 2, 2) +0.000089 * getSMEFTCoeffEW("CddR",1, 2, 2, 1) +0.000334 * getSMEFTCoeffEW("CedR",0, 0, 1, 1) +0.000334 * getSMEFTCoeffEW("CedR",1, 1, 1, 1)  
            +0.000334 * getSMEFTCoeffEW("CedR",2, 2, 1, 1) -0.000668 * getSMEFTCoeffEW("Cud1R",0, 0, 1, 1) -0.000668 * getSMEFTCoeffEW("Cud1R",1, 1, 1, 1) -0.017347 * getSMEFTCoeffEW("Cud1R",2, 2, 1, 1)  
            +0.000334 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) +0.000334 * getSMEFTCoeffEW("CldR",1, 1, 1, 1) +0.000334 * getSMEFTCoeffEW("CldR",2, 2, 1, 1) +0.000058 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0)  
            +0.000058 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1) +0.000058 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) -0.000117 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0) -0.000117 * getSMEFTCoeffEW("Cqu1R",1, 1, 1, 1)  
            -0.003037 * getSMEFTCoeffEW("Cqu1R",1, 1, 2, 2) -0.000334 * getSMEFTCoeffEW("Cqd1R",0, 0, 1, 1) +0.000058 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0) -0.000276 * getSMEFTCoeffEW("Cqd1R",1, 1, 1, 1)  
            +0.000058 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) +0.014774 * getSMEFTCoeffEW("Cqd1R",2, 2, 1, 1) ) * v2; 
        break;
    //} else if (f.is("CHARM")) {
        case 8:
            deltaNLO = (+0.007742 * getSMEFTCoeffEW("CW")  +0.001931 * getSMEFTCoeffEW("CHbox")  +0.144562 * getSMEFTCoeffEW("CHD")  +0.000665 * getSMEFTCoeffEW("CHB")   
            +0.00114 * getSMEFTCoeffEW("CHW")  +0.167453 * getSMEFTCoeffEW("CHWB")  -0.014717 * getSMEFTCoeffEW("CuWR",2, 2) +0.020802 * getSMEFTCoeffEW("CuBR",2, 2)  
            +0.001104 * getSMEFTCoeffEW("CHl1R",0, 0) +0.001104 * getSMEFTCoeffEW("CHl1R",1, 1) +0.001104 * getSMEFTCoeffEW("CHl1R",2, 2) +0.030745 * getSMEFTCoeffEW("CHl3R",0, 0)  
            +0.030745 * getSMEFTCoeffEW("CHl3R",1, 1) +0.00006 * getSMEFTCoeffEW("CHl3R",2, 2) +0.001104 * getSMEFTCoeffEW("CHeR",0, 0) +0.001104 * getSMEFTCoeffEW("CHeR",1, 1)  
            +0.001104 * getSMEFTCoeffEW("CHeR",2, 2) -0.001104 * getSMEFTCoeffEW("CHq1R",0, 0) -0.094927 * getSMEFTCoeffEW("CHq1R",1, 1) +0.094959 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.000181 * getSMEFTCoeffEW("CHq3R",0, 0) +0.089851 * getSMEFTCoeffEW("CHq3R",1, 1) -0.059683 * getSMEFTCoeffEW("CHq3R",2, 2) -0.002209 * getSMEFTCoeffEW("CHuR",0, 0)  
            -0.115557 * getSMEFTCoeffEW("CHuR",1, 1) -0.116308 * getSMEFTCoeffEW("CHuR",2, 2) +0.001104 * getSMEFTCoeffEW("CHdR",0, 0) +0.001104 * getSMEFTCoeffEW("CHdR",1, 1)  
            +0.001104 * getSMEFTCoeffEW("CHdR",2, 2) -0.030685 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) +0.000636 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1) -0.000399 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0)  
            +0.000236 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1) -0.028109 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2) -0.019173 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) -0.006627 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1)  
            +0.000569 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0) -0.006058 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1) -0.035371 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) -0.018205 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1)  
            -0.000318 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) -0.000318 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1) -0.000318 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1) -0.001104 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1)  
            -0.001104 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) -0.001104 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1) +0.002995 * getSMEFTCoeffEW("CuuR",0, 0, 1, 1) +0.000399 * getSMEFTCoeffEW("CuuR",0, 1, 1, 0)  
            +0.003395 * getSMEFTCoeffEW("CuuR",1, 1, 1, 1) +0.077766 * getSMEFTCoeffEW("CuuR",1, 1, 2, 2) +0.046983 * getSMEFTCoeffEW("CuuR",1, 2, 2, 1) -0.000749 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1)  
            -0.000749 * getSMEFTCoeffEW("CeuR",1, 1, 1, 1) -0.000749 * getSMEFTCoeffEW("CeuR",2, 2, 1, 1) -0.000749 * getSMEFTCoeffEW("Cud1R",1, 1, 0, 0) -0.000749 * getSMEFTCoeffEW("Cud1R",1, 1, 1, 1)  
            -0.000749 * getSMEFTCoeffEW("Cud1R",1, 1, 2, 2) -0.000749 * getSMEFTCoeffEW("CluR",0, 0, 1, 1) -0.000749 * getSMEFTCoeffEW("CluR",1, 1, 1, 1) -0.000749 * getSMEFTCoeffEW("CluR",2, 2, 1, 1)  
            -0.000318 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0) -0.000318 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1) -0.000318 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) +0.000749 * getSMEFTCoeffEW("Cqu1R",0, 0, 1, 1)  
            +0.000636 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0) +0.001384 * getSMEFTCoeffEW("Cqu1R",1, 1, 1, 1) +0.016502 * getSMEFTCoeffEW("Cqu1R",1, 1, 2, 2) -0.033117 * getSMEFTCoeffEW("Cqu1R",2, 2, 1, 1)  
            -0.000318 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0) -0.000318 * getSMEFTCoeffEW("Cqd1R",1, 1, 1, 1) -0.000318 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) ) * v2; 
        break;
    //} else if (f.is("BOTTOM")) {
        case 11:
            deltaNLO = (+0.001072 * getSMEFTCoeffEW("CW")  +0.000355 * getSMEFTCoeffEW("CHbox")  +0.029789 * getSMEFTCoeffEW("CHD")  +0.000122 * getSMEFTCoeffEW("CHB")   
            +0.00021 * getSMEFTCoeffEW("CHW")  +0.03436 * getSMEFTCoeffEW("CHWB")  -0.004743 * getSMEFTCoeffEW("CuWR",2, 2) +0.003557 * getSMEFTCoeffEW("CuBR",2, 2)  
            +0.000203 * getSMEFTCoeffEW("CHl1R",0, 0) +0.000203 * getSMEFTCoeffEW("CHl1R",1, 1) +0.000203 * getSMEFTCoeffEW("CHl1R",2, 2) +0.006546 * getSMEFTCoeffEW("CHl3R",0, 0)  
            +0.006546 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000203 * getSMEFTCoeffEW("CHeR",0, 0) +0.000203 * getSMEFTCoeffEW("CHeR",1, 1) +0.000203 * getSMEFTCoeffEW("CHeR",2, 2)  
            -0.000203 * getSMEFTCoeffEW("CHq1R",0, 0) -0.000203 * getSMEFTCoeffEW("CHq1R",1, 1) +0.038131 * getSMEFTCoeffEW("CHq1R",2, 2) +0.000033 * getSMEFTCoeffEW("CHq3R",0, 0)  
            +0.000033 * getSMEFTCoeffEW("CHq3R",1, 1) +0.004738 * getSMEFTCoeffEW("CHq3R",2, 2) -0.000406 * getSMEFTCoeffEW("CHuR",0, 0) -0.000406 * getSMEFTCoeffEW("CHuR",1, 1)  
            -0.02192 * getSMEFTCoeffEW("CHuR",2, 2) +0.000203 * getSMEFTCoeffEW("CHdR",0, 0) +0.000203 * getSMEFTCoeffEW("CHdR",1, 1) +0.069347 * getSMEFTCoeffEW("CHdR",2, 2)  
            -0.006535 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000117 * getSMEFTCoeffEW("Cqq1R",0, 0, 2, 2) -0.000089 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0) -0.000117 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2)  
            -0.000089 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) +0.005083 * getSMEFTCoeffEW("Cqq1R",2, 2, 2, 2) -0.001219 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2) +0.000058 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0)  
            -0.001219 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) +0.000058 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1) +0.000458 * getSMEFTCoeffEW("Cqq3R",2, 2, 2, 2) +0.000058 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2)  
            +0.000058 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2) +0.000058 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2) -0.000203 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.000203 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2)  
            -0.000203 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) +0.000668 * getSMEFTCoeffEW("CddR",0, 0, 2, 2) +0.000089 * getSMEFTCoeffEW("CddR",0, 2, 2, 0) +0.000668 * getSMEFTCoeffEW("CddR",1, 1, 2, 2)  
            +0.000089 * getSMEFTCoeffEW("CddR",1, 2, 2, 1) +0.000757 * getSMEFTCoeffEW("CddR",2, 2, 2, 2) +0.000334 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) +0.000334 * getSMEFTCoeffEW("CedR",1, 1, 2, 2)  
            +0.000334 * getSMEFTCoeffEW("CedR",2, 2, 2, 2) -0.000668 * getSMEFTCoeffEW("Cud1R",0, 0, 2, 2) -0.000668 * getSMEFTCoeffEW("Cud1R",1, 1, 2, 2) -0.017347 * getSMEFTCoeffEW("Cud1R",2, 2, 2, 2)  
            +0.000334 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) +0.000334 * getSMEFTCoeffEW("CldR",1, 1, 2, 2) +0.000334 * getSMEFTCoeffEW("CldR",2, 2, 2, 2) +0.000058 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0)  
            +0.000058 * getSMEFTCoeffEW("CqeR",2, 2, 1, 1) +0.000058 * getSMEFTCoeffEW("CqeR",2, 2, 2, 2) -0.000117 * getSMEFTCoeffEW("Cqu1R",2, 2, 0, 0) -0.000117 * getSMEFTCoeffEW("Cqu1R",2, 2, 1, 1)  
            -0.003037 * getSMEFTCoeffEW("Cqu1R",2, 2, 2, 2) -0.000334 * getSMEFTCoeffEW("Cqd1R",0, 0, 2, 2) -0.000334 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) +0.000058 * getSMEFTCoeffEW("Cqd1R",2, 2, 0, 0)  
            +0.000058 * getSMEFTCoeffEW("Cqd1R",2, 2, 1, 1) +0.014833 * getSMEFTCoeffEW("Cqd1R",2, 2, 2, 2) ) * v2; 
        break;
    //} else {
        default:
            deltaNLO = 0.;
    }
 
    return dAf + cNLOd6 * deltaNLO;
}

◆ deltaAFB()

const double NPSMEFTd6General::deltaAFB ( const Particle f ) const

virtual

The new physics contribution to the forward-backward asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $\delta A^f_{FB}$.

Parameters

[in] f a lepton or quark

Returns: $\delta A^f_{FB}$

Reimplemented from NPbase.

Definition at line 16500 of file NPSMEFTd6General.cpp.

{
    double dAFB = 0.;
    //double delGVf = deltaGV_f(f);
    //double delGAf = deltaGA_f(f);
    
    //double deltaNLO;
    
    // The electron part is needed for any final state
    //double gVe = trueSM.gV_f(f).real();
    //double gAe = trueSM.gA_f(f).real();
    //double Ge = gVe * gVe + gAe * gAe;
        
    double AeSM = trueSM.A_f(leptons[ELECTRON]); //2.0 * gAe * gVe / Ge;
    double delAe = deltaA_f(leptons[ELECTRON]);
    
    //if (f.is("ELECTRON")) {
    if ( f.getIndex() == 1 ) {
        
        dAFB = (3.0/2.0) * AeSM * delAe;
        
        //if (delGVf != 0.0 || delGAf != 0.0) {
        //    double gVe = trueSM.gV_f(f).real();
        //    double gAe = trueSM.gA_f(f).real();
        //    double Ge = gVe * gVe + gAe*gAe;
        //    double delGVeOverGAe = (gAe * delGVf - gVe * delGAf) / gAe / gAe;
        //    dAFB = -6.0 * gVe * gAe * (gVe * gVe - gAe * gAe) * gAe * gAe / Ge / Ge / Ge*delGVeOverGAe;
        //}
    } else {
 
        //double gVf = trueSM.gV_f(f).real();
        //double gAf = trueSM.gA_f(f).real();
        //double Gf = gVf * gVf + gAf * gAf;
        
        double AfSM = trueSM.A_f(f); //2.0 * gAf * gVf / Gf;
        double delAf = deltaA_f(f);      
        
        dAFB = (3.0/4.0) * ( AfSM * delAe + AeSM * delAf );
                
        //double delGVe = deltaGV_f(leptons[ELECTRON]);
        //double delGAe = deltaGA_f(leptons[ELECTRON]);
        //if (delGVe != 0.0 || delGAe != 0.0 || delGVf != 0.0 || delGAf != 0.0) {
        //    double gVe = trueSM.gV_f(leptons[ELECTRON]).real();
        //    double gAe = trueSM.gA_f(leptons[ELECTRON]).real();
        //    double Ge = gVe * gVe + gAe*gAe;
        //    double delGVeOverGAe = (gAe * delGVe - gVe * delGAe) / gAe / gAe;
            //
        //    double gVf = trueSM.gV_f(f).real();
        //    double gAf = trueSM.gA_f(f).real();
        //    double Gf = gVf * gVf + gAf*gAf;
        //    double delGVfOverGAf = (gAf * delGVf - gVf * delGAf) / gAf / gAf;
 
        //    dAFB = -(3.0 * gVf * gAf * (gVe * gVe - gAe * gAe) * gAe * gAe / Gf / Ge / Ge * delGVeOverGAe
        //            + 3.0 * gVe * gAe * (gVf * gVf - gAf * gAf) * gAf * gAf / Ge / Gf / Gf * delGVfOverGAf);
        //}
    }
 
    // Finite NLO corrections: not available for u and d   
    //switch(f.getIndex()){
    //if (f.is("ELECTRON")) {
    //    case 1:
    //        deltaNLO = (+0.00572 * getSMEFTCoeffEW("CW")  +0.001427 * getSMEFTCoeffEW("CHbox")  -0.252903 * getSMEFTCoeffEW("CHD")  +0.000491 * getSMEFTCoeffEW("CHB")   
    //        +0.000842 * getSMEFTCoeffEW("CHW")  -0.262264 * getSMEFTCoeffEW("CHWB")  -0.010873 * getSMEFTCoeffEW("CuWR",2, 2) +0.015368 * getSMEFTCoeffEW("CuBR",2, 2)  
    //        -0.13715 * getSMEFTCoeffEW("CHl1R",0, 0) +0.000816 * getSMEFTCoeffEW("CHl1R",1, 1) +0.000816 * getSMEFTCoeffEW("CHl1R",2, 2) -0.118334 * getSMEFTCoeffEW("CHl3R",0, 0)  
    //        +0.022957 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000045 * getSMEFTCoeffEW("CHl3R",2, 2) -0.222466 * getSMEFTCoeffEW("CHeR",0, 0) +0.000816 * getSMEFTCoeffEW("CHeR",1, 1)  
    //        +0.000816 * getSMEFTCoeffEW("CHeR",2, 2) -0.000816 * getSMEFTCoeffEW("CHq1R",0, 0) -0.000816 * getSMEFTCoeffEW("CHq1R",1, 1) +0.070151 * getSMEFTCoeffEW("CHq1R",2, 2)  
    //        +0.000134 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000134 * getSMEFTCoeffEW("CHq3R",1, 1) -0.044091 * getSMEFTCoeffEW("CHq3R",2, 2) -0.001632 * getSMEFTCoeffEW("CHuR",0, 0)  
    //        -0.001632 * getSMEFTCoeffEW("CHuR",1, 1) -0.085923 * getSMEFTCoeffEW("CHuR",2, 2) +0.000816 * getSMEFTCoeffEW("CHdR",0, 0) +0.000816 * getSMEFTCoeffEW("CHdR",1, 1)  
    //        +0.000816 * getSMEFTCoeffEW("CHdR",2, 2) +0.000237 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) +0.00047 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.00047 * getSMEFTCoeffEW("CllR",0, 0, 2, 2)  
    //        -0.023145 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000232 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) -0.000235 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) -0.000235 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1)  
    //        +0.010383 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) -0.002448 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.002448 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) -0.013065 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
    //        +0.000814 * getSMEFTCoeffEW("CeeR",0, 0, 0, 0) +0.000814 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1) +0.000814 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2) -0.000581 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0)  
    //        -0.000581 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1) -0.015087 * getSMEFTCoeffEW("CeuR",0, 0, 2, 2) +0.000291 * getSMEFTCoeffEW("CedR",0, 0, 0, 0) +0.000291 * getSMEFTCoeffEW("CedR",0, 0, 1, 1)  
    //        +0.000291 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) +0.000525 * getSMEFTCoeffEW("CleR",0, 0, 0, 0) +0.000235 * getSMEFTCoeffEW("CleR",0, 0, 1, 1) +0.000235 * getSMEFTCoeffEW("CleR",0, 0, 2, 2)  
    //        +0.000291 * getSMEFTCoeffEW("CleR",1, 1, 0, 0) +0.000291 * getSMEFTCoeffEW("CleR",2, 2, 0, 0) -0.00047 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) -0.00047 * getSMEFTCoeffEW("CluR",0, 0, 1, 1)  
    //        -0.012191 * getSMEFTCoeffEW("CluR",0, 0, 2, 2) +0.000235 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) +0.000235 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) +0.000235 * getSMEFTCoeffEW("CldR",0, 0, 2, 2)  
    //        -0.000291 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0) -0.000291 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0) +0.012849 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0) ) * v2; 
    //    break;
    //} else if (f.is("MUON")) {
    //    case 3:
    //        deltaNLO = (+0.00572 * getSMEFTCoeffEW("CW")  +0.001427 * getSMEFTCoeffEW("CHbox")  -0.252903 * getSMEFTCoeffEW("CHD")  +0.000491 * getSMEFTCoeffEW("CHB")   
    //        +0.000842 * getSMEFTCoeffEW("CHW")  -0.262264 * getSMEFTCoeffEW("CHWB")  -0.010873 * getSMEFTCoeffEW("CuWR",2, 2) +0.015368 * getSMEFTCoeffEW("CuBR",2, 2)  
    //        -0.068167 * getSMEFTCoeffEW("CHl1R",0, 0) -0.068167 * getSMEFTCoeffEW("CHl1R",1, 1) +0.000816 * getSMEFTCoeffEW("CHl1R",2, 2) -0.047688 * getSMEFTCoeffEW("CHl3R",0, 0)  
    //        -0.047688 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000045 * getSMEFTCoeffEW("CHl3R",2, 2) -0.110825 * getSMEFTCoeffEW("CHeR",0, 0) -0.110825 * getSMEFTCoeffEW("CHeR",1, 1)  
    //        +0.000816 * getSMEFTCoeffEW("CHeR",2, 2) -0.000816 * getSMEFTCoeffEW("CHq1R",0, 0) -0.000816 * getSMEFTCoeffEW("CHq1R",1, 1) +0.070151 * getSMEFTCoeffEW("CHq1R",2, 2)  
    //        +0.000134 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000134 * getSMEFTCoeffEW("CHq3R",1, 1) -0.044091 * getSMEFTCoeffEW("CHq3R",2, 2) -0.001632 * getSMEFTCoeffEW("CHuR",0, 0)  
    //        -0.001632 * getSMEFTCoeffEW("CHuR",1, 1) -0.085923 * getSMEFTCoeffEW("CHuR",2, 2) +0.000816 * getSMEFTCoeffEW("CHdR",0, 0) +0.000816 * getSMEFTCoeffEW("CHdR",1, 1)  
    //        +0.000816 * getSMEFTCoeffEW("CHdR",2, 2) +0.000119 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) +0.00047 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.000235 * getSMEFTCoeffEW("CllR",0, 0, 2, 2)  
    //        -0.023145 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000116 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) +0.000119 * getSMEFTCoeffEW("CllR",1, 1, 1, 1) +0.000235 * getSMEFTCoeffEW("CllR",1, 1, 2, 2)  
    //        -0.000116 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) -0.000117 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) -0.000117 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) +0.005191 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2)  
    //        -0.000117 * getSMEFTCoeffEW("Clq1R",1, 1, 0, 0) -0.000117 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1) +0.005191 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2) -0.001224 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0)  
    //        -0.001224 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) -0.006533 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.001224 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0) -0.001224 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1)  
    //        -0.006533 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) +0.000407 * getSMEFTCoeffEW("CeeR",0, 0, 0, 0) +0.000814 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1) +0.000407 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2)  
    //        +0.000407 * getSMEFTCoeffEW("CeeR",1, 1, 1, 1) +0.000407 * getSMEFTCoeffEW("CeeR",1, 1, 2, 2) -0.000291 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0) -0.000291 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1)  
    //        -0.007543 * getSMEFTCoeffEW("CeuR",0, 0, 2, 2) -0.000291 * getSMEFTCoeffEW("CeuR",1, 1, 0, 0) -0.000291 * getSMEFTCoeffEW("CeuR",1, 1, 1, 1) -0.007543 * getSMEFTCoeffEW("CeuR",1, 1, 2, 2)  
    //        +0.000145 * getSMEFTCoeffEW("CedR",0, 0, 0, 0) +0.000145 * getSMEFTCoeffEW("CedR",0, 0, 1, 1) +0.000145 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) +0.000145 * getSMEFTCoeffEW("CedR",1, 1, 0, 0)  
    //        +0.000145 * getSMEFTCoeffEW("CedR",1, 1, 1, 1) +0.000145 * getSMEFTCoeffEW("CedR",1, 1, 2, 2) +0.000263 * getSMEFTCoeffEW("CleR",0, 0, 0, 0) +0.000263 * getSMEFTCoeffEW("CleR",0, 0, 1, 1)  
    //        +0.000117 * getSMEFTCoeffEW("CleR",0, 0, 2, 2) +0.000263 * getSMEFTCoeffEW("CleR",1, 1, 0, 0) +0.000263 * getSMEFTCoeffEW("CleR",1, 1, 1, 1) +0.000117 * getSMEFTCoeffEW("CleR",1, 1, 2, 2)  
    //        +0.000145 * getSMEFTCoeffEW("CleR",2, 2, 0, 0) +0.000145 * getSMEFTCoeffEW("CleR",2, 2, 1, 1) -0.000235 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) -0.000235 * getSMEFTCoeffEW("CluR",0, 0, 1, 1)  
    //        -0.006095 * getSMEFTCoeffEW("CluR",0, 0, 2, 2) -0.000235 * getSMEFTCoeffEW("CluR",1, 1, 0, 0) -0.000235 * getSMEFTCoeffEW("CluR",1, 1, 1, 1) -0.006095 * getSMEFTCoeffEW("CluR",1, 1, 2, 2)  
    //        +0.000117 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) +0.000117 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) +0.000117 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) +0.000117 * getSMEFTCoeffEW("CldR",1, 1, 0, 0)  
    //        +0.000117 * getSMEFTCoeffEW("CldR",1, 1, 1, 1) +0.000117 * getSMEFTCoeffEW("CldR",1, 1, 2, 2) -0.000145 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0) -0.000145 * getSMEFTCoeffEW("CqeR",0, 0, 1, 1)  
    //        -0.000145 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0) -0.000145 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1) +0.006425 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0) +0.006425 * getSMEFTCoeffEW("CqeR",2, 2, 1, 1) ) * v2; 
    //    break;
    //    case 5:
    //        deltaNLO = (+0.00572 * getSMEFTCoeffEW("CW")  +0.001427 * getSMEFTCoeffEW("CHbox")  -0.252903 * getSMEFTCoeffEW("CHD")  +0.000491 * getSMEFTCoeffEW("CHB")   
    //        +0.000842 * getSMEFTCoeffEW("CHW")  -0.262264 * getSMEFTCoeffEW("CHWB")  -0.010873 * getSMEFTCoeffEW("CuWR",2, 2) +0.015368 * getSMEFTCoeffEW("CuBR",2, 2)  
    //        -0.068167 * getSMEFTCoeffEW("CHl1R",0, 0) +0.000816 * getSMEFTCoeffEW("CHl1R",1, 1) -0.068167 * getSMEFTCoeffEW("CHl1R",2, 2) -0.047688 * getSMEFTCoeffEW("CHl3R",0, 0)  
    //        +0.022957 * getSMEFTCoeffEW("CHl3R",1, 1) -0.070601 * getSMEFTCoeffEW("CHl3R",2, 2) -0.110825 * getSMEFTCoeffEW("CHeR",0, 0) +0.000816 * getSMEFTCoeffEW("CHeR",1, 1)  
    //        -0.110825 * getSMEFTCoeffEW("CHeR",2, 2) -0.000816 * getSMEFTCoeffEW("CHq1R",0, 0) -0.000816 * getSMEFTCoeffEW("CHq1R",1, 1) +0.070151 * getSMEFTCoeffEW("CHq1R",2, 2)  
    //        +0.000134 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000134 * getSMEFTCoeffEW("CHq3R",1, 1) -0.044091 * getSMEFTCoeffEW("CHq3R",2, 2) -0.001632 * getSMEFTCoeffEW("CHuR",0, 0)  
    //        -0.001632 * getSMEFTCoeffEW("CHuR",1, 1) -0.085923 * getSMEFTCoeffEW("CHuR",2, 2) +0.000816 * getSMEFTCoeffEW("CHdR",0, 0) +0.000816 * getSMEFTCoeffEW("CHdR",1, 1)  
    //        +0.000816 * getSMEFTCoeffEW("CHdR",2, 2) +0.000119 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) +0.000235 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.00047 * getSMEFTCoeffEW("CllR",0, 0, 2, 2)  
    //        -0.023029 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000232 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) +0.000235 * getSMEFTCoeffEW("CllR",1, 1, 2, 2) -0.000116 * getSMEFTCoeffEW("CllR",1, 2, 2, 1)  
    //        +0.000119 * getSMEFTCoeffEW("CllR",2, 2, 2, 2) -0.000117 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) -0.000117 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) +0.005191 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2)  
    //        -0.000117 * getSMEFTCoeffEW("Clq1R",2, 2, 0, 0) -0.000117 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1) +0.005191 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2) -0.001224 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0)  
    //        -0.001224 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) -0.006533 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.001224 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0) -0.001224 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1)  
    //        -0.006533 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) +0.000407 * getSMEFTCoeffEW("CeeR",0, 0, 0, 0) +0.000407 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1) +0.000814 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2)  
    //        +0.000407 * getSMEFTCoeffEW("CeeR",1, 1, 2, 2) +0.000407 * getSMEFTCoeffEW("CeeR",2, 2, 2, 2) -0.000291 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0) -0.000291 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1)  
    //        -0.007543 * getSMEFTCoeffEW("CeuR",0, 0, 2, 2) -0.000291 * getSMEFTCoeffEW("CeuR",2, 2, 0, 0) -0.000291 * getSMEFTCoeffEW("CeuR",2, 2, 1, 1) -0.007543 * getSMEFTCoeffEW("CeuR",2, 2, 2, 2)  
    //        +0.000145 * getSMEFTCoeffEW("CedR",0, 0, 0, 0) +0.000145 * getSMEFTCoeffEW("CedR",0, 0, 1, 1) +0.000145 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) +0.000145 * getSMEFTCoeffEW("CedR",2, 2, 0, 0)  
    //        +0.000145 * getSMEFTCoeffEW("CedR",2, 2, 1, 1) +0.000145 * getSMEFTCoeffEW("CedR",2, 2, 2, 2) +0.000263 * getSMEFTCoeffEW("CleR",0, 0, 0, 0) +0.000117 * getSMEFTCoeffEW("CleR",0, 0, 1, 1)  
    //        +0.000263 * getSMEFTCoeffEW("CleR",0, 0, 2, 2) +0.000145 * getSMEFTCoeffEW("CleR",1, 1, 0, 0) +0.000145 * getSMEFTCoeffEW("CleR",1, 1, 2, 2) +0.000263 * getSMEFTCoeffEW("CleR",2, 2, 0, 0)  
    //        +0.000117 * getSMEFTCoeffEW("CleR",2, 2, 1, 1) +0.000263 * getSMEFTCoeffEW("CleR",2, 2, 2, 2) -0.000235 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) -0.000235 * getSMEFTCoeffEW("CluR",0, 0, 1, 1)  
    //        -0.006095 * getSMEFTCoeffEW("CluR",0, 0, 2, 2) -0.000235 * getSMEFTCoeffEW("CluR",2, 2, 0, 0) -0.000235 * getSMEFTCoeffEW("CluR",2, 2, 1, 1) -0.006095 * getSMEFTCoeffEW("CluR",2, 2, 2, 2)  
    //        +0.000117 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) +0.000117 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) +0.000117 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) +0.000117 * getSMEFTCoeffEW("CldR",2, 2, 0, 0)  
    //        +0.000117 * getSMEFTCoeffEW("CldR",2, 2, 1, 1) +0.000117 * getSMEFTCoeffEW("CldR",2, 2, 2, 2) -0.000145 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0) -0.000145 * getSMEFTCoeffEW("CqeR",0, 0, 2, 2)  
    //        -0.000145 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0) -0.000145 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) +0.006425 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0) +0.006425 * getSMEFTCoeffEW("CqeR",2, 2, 2, 2) ) * v2; 
    //    break;
    //} else if (f.is("STRANGE")) {
    //    case 9:
    //        deltaNLO = (+0.013035 * getSMEFTCoeffEW("CW")  +0.003252 * getSMEFTCoeffEW("CHbox")  +0.146227 * getSMEFTCoeffEW("CHD")  +0.001119 * getSMEFTCoeffEW("CHB")   
    //        +0.00192 * getSMEFTCoeffEW("CHW")  +0.177551 * getSMEFTCoeffEW("CHWB")  -0.024778 * getSMEFTCoeffEW("CuWR",2, 2) +0.035022 * getSMEFTCoeffEW("CuBR",2, 2)  
    //        +0.108046 * getSMEFTCoeffEW("CHl1R",0, 0) +0.001859 * getSMEFTCoeffEW("CHl1R",1, 1) +0.001859 * getSMEFTCoeffEW("CHl1R",2, 2) +0.151035 * getSMEFTCoeffEW("CHl3R",0, 0)  
    //        +0.052297 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000102 * getSMEFTCoeffEW("CHl3R",2, 2) +0.015591 * getSMEFTCoeffEW("CHeR",0, 0) +0.001859 * getSMEFTCoeffEW("CHeR",1, 1)  
    //        +0.001859 * getSMEFTCoeffEW("CHeR",2, 2) -0.001859 * getSMEFTCoeffEW("CHq1R",0, 0) -0.006578 * getSMEFTCoeffEW("CHq1R",1, 1) +0.159871 * getSMEFTCoeffEW("CHq1R",2, 2)  
    //        +0.000305 * getSMEFTCoeffEW("CHq3R",0, 0) -0.004524 * getSMEFTCoeffEW("CHq3R",1, 1) -0.10048 * getSMEFTCoeffEW("CHq3R",2, 2) -0.003719 * getSMEFTCoeffEW("CHuR",0, 0)  
    //        -0.003719 * getSMEFTCoeffEW("CHuR",1, 1) -0.195812 * getSMEFTCoeffEW("CHuR",2, 2) +0.001859 * getSMEFTCoeffEW("CHdR",0, 0) -0.031424 * getSMEFTCoeffEW("CHdR",1, 1)  
    //        +0.001859 * getSMEFTCoeffEW("CHdR",2, 2) +0.000531 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) +0.001052 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.001052 * getSMEFTCoeffEW("CllR",0, 0, 2, 2)  
    //        -0.052716 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000521 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) -0.000018 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1) -0.000014 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0)  
    //        -0.000032 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1) +0.000815 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2) -0.000014 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) -0.000192 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1)  
    //        +0.000009 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0) -0.000183 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1) -0.001025 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) +0.001097 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1)  
    //        -0.000526 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) -0.000517 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) +0.023254 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) +0.000009 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1)  
    //        +0.000009 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1) -0.005482 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.005514 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) -0.029262 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
    //        -0.000032 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) -0.000032 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1) +0.001822 * getSMEFTCoeffEW("CeeR",0, 0, 0, 0) +0.001822 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1)  
    //        +0.001822 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2) +0.000105 * getSMEFTCoeffEW("CddR",0, 0, 1, 1) +0.000014 * getSMEFTCoeffEW("CddR",0, 1, 1, 0) +0.000119 * getSMEFTCoeffEW("CddR",1, 1, 1, 1)  
    //        +0.000105 * getSMEFTCoeffEW("CddR",1, 1, 2, 2) +0.000014 * getSMEFTCoeffEW("CddR",1, 2, 2, 1) -0.001302 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0) -0.001302 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1)  
    //        -0.033789 * getSMEFTCoeffEW("CeuR",0, 0, 2, 2) +0.000651 * getSMEFTCoeffEW("CedR",0, 0, 0, 0) +0.000703 * getSMEFTCoeffEW("CedR",0, 0, 1, 1) +0.000651 * getSMEFTCoeffEW("CedR",0, 0, 2, 2)  
    //        +0.000053 * getSMEFTCoeffEW("CedR",1, 1, 1, 1) +0.000053 * getSMEFTCoeffEW("CedR",2, 2, 1, 1) -0.000105 * getSMEFTCoeffEW("Cud1R",0, 0, 1, 1) -0.000105 * getSMEFTCoeffEW("Cud1R",1, 1, 1, 1)  
    //        -0.002732 * getSMEFTCoeffEW("Cud1R",2, 2, 1, 1) +0.001177 * getSMEFTCoeffEW("CleR",0, 0, 0, 0) +0.000526 * getSMEFTCoeffEW("CleR",0, 0, 1, 1) +0.000526 * getSMEFTCoeffEW("CleR",0, 0, 2, 2)  
    //        +0.000651 * getSMEFTCoeffEW("CleR",1, 1, 0, 0) +0.000651 * getSMEFTCoeffEW("CleR",2, 2, 0, 0) -0.001052 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) -0.001052 * getSMEFTCoeffEW("CluR",0, 0, 1, 1)  
    //        -0.027303 * getSMEFTCoeffEW("CluR",0, 0, 2, 2) +0.000526 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) +0.000578 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) +0.000526 * getSMEFTCoeffEW("CldR",0, 0, 2, 2)  
    //        +0.000053 * getSMEFTCoeffEW("CldR",1, 1, 1, 1) +0.000053 * getSMEFTCoeffEW("CldR",2, 2, 1, 1) -0.000651 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0) -0.000642 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0)  
    //        +0.000009 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1) +0.000009 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) +0.028779 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0) -0.000018 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0)  
    //        -0.000018 * getSMEFTCoeffEW("Cqu1R",1, 1, 1, 1) -0.000478 * getSMEFTCoeffEW("Cqu1R",1, 1, 2, 2) -0.000053 * getSMEFTCoeffEW("Cqd1R",0, 0, 1, 1) +0.000009 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0)  
    //        -0.000043 * getSMEFTCoeffEW("Cqd1R",1, 1, 1, 1) +0.000009 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) +0.002327 * getSMEFTCoeffEW("Cqd1R",2, 2, 1, 1) ) * v2; 
    //    break;
    //    case 8:
    //        deltaNLO = (+0.010682 * getSMEFTCoeffEW("CW")  +0.002665 * getSMEFTCoeffEW("CHbox")  +0.007558 * getSMEFTCoeffEW("CHD")  +0.000917 * getSMEFTCoeffEW("CHB")   
    //        +0.001573 * getSMEFTCoeffEW("CHW")  +0.025056 * getSMEFTCoeffEW("CHWB")  -0.020306 * getSMEFTCoeffEW("CuWR",2, 2) +0.028701 * getSMEFTCoeffEW("CuBR",2, 2)  
    //        +0.045525 * getSMEFTCoeffEW("CHl1R",0, 0) +0.001524 * getSMEFTCoeffEW("CHl1R",1, 1) +0.001524 * getSMEFTCoeffEW("CHl1R",2, 2) +0.081322 * getSMEFTCoeffEW("CHl3R",0, 0)  
    //        +0.042823 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000083 * getSMEFTCoeffEW("CHl3R",2, 2) -0.030951 * getSMEFTCoeffEW("CHeR",0, 0) +0.001524 * getSMEFTCoeffEW("CHeR",1, 1)  
    //        +0.001524 * getSMEFTCoeffEW("CHeR",2, 2) -0.001524 * getSMEFTCoeffEW("CHq1R",0, 0) +0.023905 * getSMEFTCoeffEW("CHq1R",1, 1) +0.131016 * getSMEFTCoeffEW("CHq1R",2, 2)  
    //        +0.00025 * getSMEFTCoeffEW("CHq3R",0, 0) -0.025833 * getSMEFTCoeffEW("CHq3R",1, 1) -0.082345 * getSMEFTCoeffEW("CHq3R",2, 2) -0.003048 * getSMEFTCoeffEW("CHuR",0, 0)  
    //        +0.073836 * getSMEFTCoeffEW("CHuR",1, 1) -0.16047 * getSMEFTCoeffEW("CHuR",2, 2) +0.001524 * getSMEFTCoeffEW("CHdR",0, 0) +0.001524 * getSMEFTCoeffEW("CHdR",1, 1)  
    //        +0.001524 * getSMEFTCoeffEW("CHdR",2, 2) +0.000392 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) +0.000777 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.000777 * getSMEFTCoeffEW("CllR",0, 0, 2, 2)  
    //        -0.043124 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000385 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) +0.0001 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1) -0.000063 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0)  
    //        +0.000037 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1) -0.004426 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2) -0.003019 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) -0.001044 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1)  
    //        +0.00009 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0) -0.000954 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1) -0.00557 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) -0.002867 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1)  
    //        -0.000388 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) -0.000438 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) +0.017178 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) -0.00005 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1)  
    //        -0.00005 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1) -0.00405 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.004224 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) -0.021616 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
    //        -0.000174 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) -0.000174 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1) +0.001346 * getSMEFTCoeffEW("CeeR",0, 0, 0, 0) +0.001346 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1)  
    //        +0.001346 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2) +0.000472 * getSMEFTCoeffEW("CuuR",0, 0, 1, 1) +0.000063 * getSMEFTCoeffEW("CuuR",0, 1, 1, 0) +0.000535 * getSMEFTCoeffEW("CuuR",1, 1, 1, 1)  
    //        +0.012246 * getSMEFTCoeffEW("CuuR",1, 1, 2, 2) +0.007399 * getSMEFTCoeffEW("CuuR",1, 2, 2, 1) -0.000961 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0) -0.001079 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1)  
    //        -0.02496 * getSMEFTCoeffEW("CeuR",0, 0, 2, 2) -0.000118 * getSMEFTCoeffEW("CeuR",1, 1, 1, 1) -0.000118 * getSMEFTCoeffEW("CeuR",2, 2, 1, 1) +0.000481 * getSMEFTCoeffEW("CedR",0, 0, 0, 0)  
    //        +0.000481 * getSMEFTCoeffEW("CedR",0, 0, 1, 1) +0.000481 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) -0.000118 * getSMEFTCoeffEW("Cud1R",1, 1, 0, 0) -0.000118 * getSMEFTCoeffEW("Cud1R",1, 1, 1, 1)  
    //        -0.000118 * getSMEFTCoeffEW("Cud1R",1, 1, 2, 2) +0.000869 * getSMEFTCoeffEW("CleR",0, 0, 0, 0) +0.000388 * getSMEFTCoeffEW("CleR",0, 0, 1, 1) +0.000388 * getSMEFTCoeffEW("CleR",0, 0, 2, 2)  
    //        +0.000481 * getSMEFTCoeffEW("CleR",1, 1, 0, 0) +0.000481 * getSMEFTCoeffEW("CleR",2, 2, 0, 0) -0.000777 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) -0.000895 * getSMEFTCoeffEW("CluR",0, 0, 1, 1)  
    //        -0.020169 * getSMEFTCoeffEW("CluR",0, 0, 2, 2) -0.000118 * getSMEFTCoeffEW("CluR",1, 1, 1, 1) -0.000118 * getSMEFTCoeffEW("CluR",2, 2, 1, 1) +0.000388 * getSMEFTCoeffEW("CldR",0, 0, 0, 0)  
    //        +0.000388 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) +0.000388 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) -0.000481 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0) -0.000531 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0)  
    //        -0.00005 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1) -0.00005 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) +0.021258 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0) +0.000118 * getSMEFTCoeffEW("Cqu1R",0, 0, 1, 1)  
    //        +0.0001 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0) +0.000218 * getSMEFTCoeffEW("Cqu1R",1, 1, 1, 1) +0.002599 * getSMEFTCoeffEW("Cqu1R",1, 1, 2, 2) -0.005215 * getSMEFTCoeffEW("Cqu1R",2, 2, 1, 1)  
    //        -0.00005 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0) -0.00005 * getSMEFTCoeffEW("Cqd1R",1, 1, 1, 1) -0.00005 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) ) * v2; 
    //    break;
    //} else if (f.is("BOTTOM")) {
    //    case 11:
    //        deltaNLO = (+0.012979 * getSMEFTCoeffEW("CW")  +0.003252 * getSMEFTCoeffEW("CHbox")  +0.144659 * getSMEFTCoeffEW("CHD")  +0.001119 * getSMEFTCoeffEW("CHB")   
    //        +0.00192 * getSMEFTCoeffEW("CHW")  +0.175886 * getSMEFTCoeffEW("CHWB")  -0.025098 * getSMEFTCoeffEW("CuWR",2, 2) +0.034979 * getSMEFTCoeffEW("CuBR",2, 2)  
    //        +0.106801 * getSMEFTCoeffEW("CHl1R",0, 0) +0.001859 * getSMEFTCoeffEW("CHl1R",1, 1) +0.001859 * getSMEFTCoeffEW("CHl1R",2, 2) +0.149942 * getSMEFTCoeffEW("CHl3R",0, 0)  
    //        +0.052448 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000102 * getSMEFTCoeffEW("CHl3R",2, 2) +0.014051 * getSMEFTCoeffEW("CHeR",0, 0) +0.001859 * getSMEFTCoeffEW("CHeR",1, 1)  
    //        +0.001859 * getSMEFTCoeffEW("CHeR",2, 2) -0.001859 * getSMEFTCoeffEW("CHq1R",0, 0) -0.001859 * getSMEFTCoeffEW("CHq1R",1, 1) +0.155726 * getSMEFTCoeffEW("CHq1R",2, 2)  
    //        +0.000305 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000305 * getSMEFTCoeffEW("CHq3R",1, 1) -0.105403 * getSMEFTCoeffEW("CHq3R",2, 2) -0.003719 * getSMEFTCoeffEW("CHuR",0, 0)  
    //        -0.003719 * getSMEFTCoeffEW("CHuR",1, 1) -0.195894 * getSMEFTCoeffEW("CHuR",2, 2) +0.001859 * getSMEFTCoeffEW("CHdR",0, 0) +0.001859 * getSMEFTCoeffEW("CHdR",1, 1)  
    //        -0.029514 * getSMEFTCoeffEW("CHdR",2, 2) +0.000531 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) +0.001052 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.001052 * getSMEFTCoeffEW("CllR",0, 0, 2, 2)  
    //        -0.052867 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000521 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) -0.000018 * getSMEFTCoeffEW("Cqq1R",0, 0, 2, 2) -0.000014 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0)  
    //        -0.000018 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2) -0.000014 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) +0.000801 * getSMEFTCoeffEW("Cqq1R",2, 2, 2, 2) -0.000192 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2)  
    //        +0.000009 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0) -0.000192 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) +0.000009 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1) +0.000072 * getSMEFTCoeffEW("Cqq3R",2, 2, 2, 2)  
    //        -0.000526 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) -0.000526 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) +0.023264 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) +0.000009 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2)  
    //        +0.000009 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2) -0.005482 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.005482 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) -0.029294 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
    //        -0.000032 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.000032 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) +0.001822 * getSMEFTCoeffEW("CeeR",0, 0, 0, 0) +0.001822 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1)  
    //        +0.001822 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2) +0.000105 * getSMEFTCoeffEW("CddR",0, 0, 2, 2) +0.000014 * getSMEFTCoeffEW("CddR",0, 2, 2, 0) +0.000105 * getSMEFTCoeffEW("CddR",1, 1, 2, 2)  
    //        +0.000014 * getSMEFTCoeffEW("CddR",1, 2, 2, 1) +0.000119 * getSMEFTCoeffEW("CddR",2, 2, 2, 2) -0.001302 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0) -0.001302 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1)  
    //        -0.033789 * getSMEFTCoeffEW("CeuR",0, 0, 2, 2) +0.000651 * getSMEFTCoeffEW("CedR",0, 0, 0, 0) +0.000651 * getSMEFTCoeffEW("CedR",0, 0, 1, 1) +0.000703 * getSMEFTCoeffEW("CedR",0, 0, 2, 2)  
    //        +0.000053 * getSMEFTCoeffEW("CedR",1, 1, 2, 2) +0.000053 * getSMEFTCoeffEW("CedR",2, 2, 2, 2) -0.000105 * getSMEFTCoeffEW("Cud1R",0, 0, 2, 2) -0.000105 * getSMEFTCoeffEW("Cud1R",1, 1, 2, 2)  
    //        -0.002732 * getSMEFTCoeffEW("Cud1R",2, 2, 2, 2) +0.001177 * getSMEFTCoeffEW("CleR",0, 0, 0, 0) +0.000526 * getSMEFTCoeffEW("CleR",0, 0, 1, 1) +0.000526 * getSMEFTCoeffEW("CleR",0, 0, 2, 2)  
    //        +0.000651 * getSMEFTCoeffEW("CleR",1, 1, 0, 0) +0.000651 * getSMEFTCoeffEW("CleR",2, 2, 0, 0) -0.001052 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) -0.001052 * getSMEFTCoeffEW("CluR",0, 0, 1, 1)  
    //        -0.027303 * getSMEFTCoeffEW("CluR",0, 0, 2, 2) +0.000526 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) +0.000526 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) +0.000578 * getSMEFTCoeffEW("CldR",0, 0, 2, 2)  
    //        +0.000053 * getSMEFTCoeffEW("CldR",1, 1, 2, 2) +0.000053 * getSMEFTCoeffEW("CldR",2, 2, 2, 2) -0.000651 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0) -0.000651 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0)  
    //        +0.028788 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0) +0.000009 * getSMEFTCoeffEW("CqeR",2, 2, 1, 1) +0.000009 * getSMEFTCoeffEW("CqeR",2, 2, 2, 2) -0.000018 * getSMEFTCoeffEW("Cqu1R",2, 2, 0, 0)  
    //        -0.000018 * getSMEFTCoeffEW("Cqu1R",2, 2, 1, 1) -0.000478 * getSMEFTCoeffEW("Cqu1R",2, 2, 2, 2) -0.000053 * getSMEFTCoeffEW("Cqd1R",0, 0, 2, 2) -0.000053 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2)  
    //        +0.000009 * getSMEFTCoeffEW("Cqd1R",2, 2, 0, 0) +0.000009 * getSMEFTCoeffEW("Cqd1R",2, 2, 1, 1) +0.002336 * getSMEFTCoeffEW("Cqd1R",2, 2, 2, 2) ) * v2; 
    //    break;
    //    default:
    //        deltaNLO = 0.;
    //}
 
    return dAFB; // + cNLOd6 * deltaNLO;
}

◆ deltaaMZ()

const double NPSMEFTd6General::deltaaMZ ( ) const

virtual

The relative correction to the electromagnetic constant at the Z pole, $\delta \alpha(M_Z^2)/\alpha(M_Z^2)$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $\delta \alpha(M_Z^2)/\alpha(M_Z^2)$

Definition at line 15517 of file NPSMEFTd6General.cpp.

                                              {
    //  Ref. value used in MG simulations
    return ( (aleMz - 0.007754633699856456) / 0.007754633699856456);
}

◆ deltaaMZ2()

const double NPSMEFTd6General::deltaaMZ2 ( ) const

virtual

The relative correction to the electromagnetic constant at the Z pole, $(\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $(\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2$

Definition at line 15522 of file NPSMEFTd6General.cpp.

                                               {
    return ( 0.0);
}

◆ deltaaSMZ()

const double NPSMEFTd6General::deltaaSMZ ( ) const

virtual

The relative correction to the strong coupling constant at the Z pole, $\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)$

Definition at line 15535 of file NPSMEFTd6General.cpp.

                                               {
    //  Ref. value used in MG simulations
    return ( (AlsMz - 0.1180) / 0.1180);
}

◆ deltaaSMZ2()

const double NPSMEFTd6General::deltaaSMZ2 ( ) const

virtual

The relative correction to the strong coupling constant at the Z pole, $(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2$

Definition at line 15540 of file NPSMEFTd6General.cpp.

                                                {
    return ( 0.0);
}

◆ deltacZ_HB()

const double NPSMEFTd6General::deltacZ_HB ( const double mu ) const

virtual

The Higgs-basis coupling $\delta c_z$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta c_z$

Reimplemented from NPbase.

Definition at line 43162 of file NPSMEFTd6General.cpp.

                                                               {
    double d_h_mu, d_GF_mu;
    double ciHB;
    
    d_h_mu = (-getSMEFTCoeff("CHD", mu) / 4.0 + getSMEFTCoeff("CHbox", mu) ) * v2;
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
 
    ciHB = d_h_mu - (3.0 / 2.0) * d_GF_mu;
 
    return ciHB;
}

◆ deltadxsdcoseeWWlvjjLEP2()

const double NPSMEFTd6General::deltadxsdcoseeWWlvjjLEP2	(	const double	sqrt_s,
		const int	bin
	)		const

virtual

The new physics contribution to the differential cross section in pb for $e^+ e^- \to W^+ W^- \to lv jj $, with $ l= e,\mu $ for the 4 $ cos{\theta}$ bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph].

Returns: $\delta d\sigma/d\cos{\theta}$ [pb]

Reimplemented from NPbase.

Definition at line 37672 of file NPSMEFTd6General.cpp.

                                                                                                {
 
    //  Returns differential cross section in pb  
    //  bin = 1, 2, 3, 4
 
    double xspb = 0.0;
 
    double xspbSM = 0.0;
    // SM values from Table 8 in hep-ex/0409016
    // Sum bin contents into B1=[-1,-0.8], B2=[-0.4,-0.2], B3=[0.4,0.6], B4=[0.8,1]
    double xslvjjSM183[4] = {0.74, 1.20, 2.86, 5.47};
    double xslvjjSM206[4] = {0.52, 0.98, 2.92, 7.80};
 
    double dgWve, dgWpm1, dgWpm2, dmZ2, dmW2, dGW, dGF, dgZ, dsW2, dgVZee, dgAZee, dgZ1, dgga1, dkga, dkZ, dlga, dlZ, deem;
 
    double gVZeeSM, gAZeeSM;
 
    //  Values of the couplings: final-state independent couplings
    gVZeeSM = -0.25 + sW2_tree;
    gAZeeSM = -0.25;
 
    dGF = delta_GF / sqrt(2.0);
 
    dmZ2 = cAsch * (0.5 * getSMEFTCoeffEW("CHD") + 2.0 * cW_tree * sW_tree * getSMEFTCoeffEW("CHWB")) * v2
            + cWsch * (0.5 * getSMEFTCoeffEW("CHD") + 2.0 * (Mw_inp / Mz) * sqrt(1.0 - Mw_inp * Mw_inp / Mz / Mz) * getSMEFTCoeffEW("CHWB")) * v2;
 
    dmW2 = -2.0 * deltaMwd6(); //There is a minus sign between refs. definition of dmW2 and ours
 
    dGW = deltaGwd6();
 
    dsW2 = cAsch * (-0.5 * (cW2_tree / (1.0 - 2.0 * sW2_tree)) * ((getSMEFTCoeffEW("CHD")
            + 2.0 * getSMEFTCoeffEW("CHWB") / cW_tree / sW_tree) * v2
            + 2.0 * sqrt(2.0) * dGF))
            + cWsch * (1.0 / sW2_tree) * (0.5 * Mw_inp * Mw_inp * getSMEFTCoeffEW("CHD") / Mz / Mz + Mw_inp * sqrt(1.0 - Mw_inp * Mw_inp / Mz / Mz) * getSMEFTCoeffEW("CHWB") / Mz) * v2;
 
    dgZ = -dGF / sqrt(2.0) - 0.5 * dmZ2
            + cW_tree * sW_tree * getSMEFTCoeffEW("CHWB") * v2;
 
    dgVZee = dgZ * gVZeeSM
            - 0.25 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl3R", 0, 0)) * v2
            - sW2_tree * dsW2;
 
    dgAZee = dgZ * gAZeeSM
            + 0.25 * (getSMEFTCoeffEW("CHeR", 0, 0) - getSMEFTCoeffEW("CHl1R", 0, 0) - getSMEFTCoeffEW("CHl3R", 0, 0)) * v2;
 
    dgWve = 0.5 * getSMEFTCoeffEW("CHl3R", 0, 0) * v2
            + cAsch * (0.25 * (cW_tree * getSMEFTCoeffEW("CHWB") / sW_tree) * v2 + 0.25 * dsW2)
            + cWsch * (-dGF / 2.0 / sqrt(2.0));
 
    dgZ1 = deltag1ZNP(sqrt_s);
 
    dgga1 = deltag1gaNP(sqrt_s);
 
    dkga = deltaKgammaNP(sqrt_s);
 
    dkZ = dgZ1 - (sW2_tree / cW2_tree) * (dkga - dgga1);
 
    dlga = -lambdaZNP(sqrt_s);
 
    dlZ = -lambdaZNP(sqrt_s);
 
    deem = delta_e + 0.5 * delta_A;
 
    //  Values of the couplings for the W decays: I assume ME from arXiv: 1606.06693 [hep-ph] are, as in
    //  the LEP2 experimental analyses they use, for l=e, mu    
    dgWpm1 = 0.25 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) * v2
            + cAsch * (0.25 * (cW_tree * getSMEFTCoeffEW("CHWB") / sW_tree) * v2 + 0.25 * dsW2)
            + cWsch * (-dGF / 2.0 / sqrt(2.0));
 
    dgWpm2 = 0.25 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1)) * v2
            + cAsch * (0.25 * (cW_tree * getSMEFTCoeffEW("CHWB") / sW_tree) * v2 + 0.25 * dsW2)
            + cWsch * (-dGF / 2.0 / sqrt(2.0));
 
    if (sqrt_s == 0.1827) {
 
        switch (bin) {
            case 1:
                //  Bin 1        
                xspbSM = xslvjjSM183[0];
                xspb += cAsch * (-1.6 * dmW2
                        - 1.5 * dGW
                        + 12.0 * dgWve
                        + 2.9 * dgWpm1
                        + 2.9 * dgWpm2
                        + 4.1 * dgVZee
                        + 3.0 * dgAZee
                        - 0.44 * dgZ1
                        - 0.34 * dkga
                        - 0.47 * dkZ
                        - 0.32 * dlga
                        - 0.45 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -1.5 * dGW
                        + 12.0 * dgWve
                        + 2.9 * dgWpm1
                        + 2.9 * dgWpm2
                        + 4.3 * dgVZee
                        + 3.0 * dgAZee
                        - 0.42 * dgZ1
                        - 0.37 * dkga
                        - 0.45 * dkZ
                        - 0.35 * dlga
                        - 0.43 * dlZ
                        - 0.34 * dgga1
                        - 0.71 * deem
                        );
 
                break;
 
            case 2:
                //  Bin 2   
                xspbSM = xslvjjSM183[1];
                xspb += cAsch * (-1.5 * dmW2
                        - 2.8 * dGW
                        + 16.0 * dgWve
                        + 5.5 * dgWpm1
                        + 5.5 * dgWpm2
                        + 3.5 * dgVZee
                        + 2.2 * dgAZee
                        - 0.30 * dgZ1
                        - 0.32 * dkga
                        - 0.39 * dkZ
                        - 0.26 * dlga
                        - 0.34 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -2.8 * dGW
                        + 16.0 * dgWve
                        + 5.4 * dgWpm1
                        + 5.4 * dgWpm2
                        + 3.7 * dgVZee
                        + 2.3 * dgAZee
                        - 0.29 * dgZ1
                        - 0.35 * dkga
                        - 0.38 * dkZ
                        - 0.28 * dlga
                        - 0.32 * dlZ
                        - 0.27 * dgga1
                        - 0.62 * deem
                        );
 
                break;
 
            case 3:
                //  Bin 3      
                xspbSM = xslvjjSM183[2];
                xspb += cAsch * (0.16 * dmW2
                        - 5.3 * dGW
                        + 22.0 * dgWve
                        + 10.0 * dgWpm1
                        + 10.0 * dgWpm2
                        + 1.5 * dgVZee
                        + 0.2 * dgAZee
                        - 0.04 * dgZ1
                        - 0.14 * dkga
                        - 0.06 * dkZ
                        - 0.06 * dlga
                        + 0.026 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -5.2 * dGW
                        + 22.0 * dgWve
                        + 10.2 * dgWpm1
                        + 10.2 * dgWpm2
                        + 1.7 * dgVZee
                        + 0.2 * dgAZee
                        - 0.04 * dgZ1
                        - 0.16 * dkga
                        - 0.06 * dkZ
                        - 0.08 * dlga
                        + 0.03 * dlZ
                        - 0.12 * dgga1
                        - 0.29 * deem
                        );
 
                break;
 
            case 4:
                //  Bin 4        
                xspbSM = xslvjjSM183[3];
                xspb += cAsch * (18.0 * dmW2
                        - 14.0 * dGW
                        + 39.0 * dgWve
                        + 27.0 * dgWpm1
                        + 27.0 * dgWpm2
                        - 7.7 * dgVZee
                        - 8.8 * dgAZee
                        + 1.2 * dgZ1
                        + 0.62 * dkga
                        + 1.3 * dkZ
                        + 0.63 * dlga
                        + 1.3 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -14.1 * dGW
                        + 40.0 * dgWve
                        + 27.5 * dgWpm1
                        + 27.5 * dgWpm2
                        - 7.8 * dgVZee
                        - 9.0 * dgAZee
                        + 1.20 * dgZ1
                        + 0.67 * dkga
                        + 1.27 * dkZ
                        + 0.68 * dlga
                        + 1.27 * dlZ
                        + 0.64 * dgga1
                        + 1.30 * deem
                        );
 
                break;
 
        }
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
    } else if (sqrt_s == 0.2059) {
 
        switch (bin) {
            case 1:
                //  Bin 1        
                xspbSM = xslvjjSM206[0];
                xspb += cAsch * (-1.1 * dmW2
                        - 0.9 * dGW
                        + 11.0 * dgWve
                        + 1.8 * dgWpm1
                        + 1.8 * dgWpm2
                        + 4.9 * dgVZee
                        + 3.0 * dgAZee
                        - 0.44 * dgZ1
                        - 0.44 * dkga
                        - 0.50 * dkZ
                        - 0.40 * dlga
                        - 0.46 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -0.9 * dGW
                        + 10.0 * dgWve
                        + 1.8 * dgWpm1
                        + 1.8 * dgWpm2
                        + 4.9 * dgVZee
                        + 2.9 * dgAZee
                        - 0.40 * dgZ1
                        - 0.47 * dkga
                        - 0.46 * dkZ
                        - 0.43 * dlga
                        - 0.43 * dlZ
                        - 0.41 * dgga1
                        - 0.88 * deem
                        );
 
                break;
 
            case 2:
                //  Bin 2        
                xspbSM = xslvjjSM206[1];
                xspb += cAsch * (-1.7 * dmW2
                        - 2.1 * dGW
                        + 15.0 * dgWve
                        + 4.1 * dgWpm1
                        + 4.1 * dgWpm2
                        + 5.0 * dgVZee
                        + 2.8 * dgAZee
                        - 0.34 * dgZ1
                        - 0.53 * dkga
                        - 0.55 * dkZ
                        - 0.37 * dlga
                        - 0.41 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -2.0 * dGW
                        + 15.0 * dgWve
                        + 4.0 * dgWpm1
                        + 4.0 * dgWpm2
                        + 5.1 * dgVZee
                        + 2.8 * dgAZee
                        - 0.31 * dgZ1
                        - 0.57 * dkga
                        - 0.51 * dkZ
                        - 0.40 * dlga
                        - 0.38 * dlZ
                        - 0.35 * dgga1
                        - 0.92 * deem
                        );
 
                break;
 
            case 3:
                //  Bin 3        
                xspbSM = xslvjjSM206[2];
                xspb += cAsch * (-2.3 * dmW2
                        - 4.6 * dGW
                        + 22.0 * dgWve
                        + 9.0 * dgWpm1
                        + 9.0 * dgWpm2
                        + 3.5 * dgVZee
                        + 1.2 * dgAZee
                        - 0.19 * dgZ1
                        - 0.35 * dkga
                        - 0.25 * dkZ
                        - 0.19 * dlga
                        - 0.086 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -4.5 * dGW
                        + 22.0 * dgWve
                        + 8.8 * dgWpm1
                        + 8.8 * dgWpm2
                        + 3.7 * dgVZee
                        + 1.2 * dgAZee
                        - 0.17 * dgZ1
                        - 0.39 * dkga
                        - 0.22 * dkZ
                        - 0.21 * dlga
                        - 0.07 * dlZ
                        - 0.27 * dgga1
                        - 0.66 * deem
                        );
 
                break;
 
            case 4:
                //  Bin 4        
                xspbSM = xslvjjSM206[3];
                xspb += cAsch * (10.0 * dmW2
                        - 20.0 * dGW
                        + 59.0 * dgWve
                        + 39.0 * dgWpm1
                        + 39.0 * dgWpm2
                        - 9.6 * dgVZee
                        - 11.0 * dgAZee
                        + 1.5 * dgZ1
                        + 0.86 * dkga
                        + 1.7 * dkZ
                        + 0.9 * dlga
                        + 1.7 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -19.8 * dGW
                        + 59.0 * dgWve
                        + 39.0 * dgWpm1
                        + 39.0 * dgWpm2
                        - 9.5 * dgVZee
                        - 11.4 * dgAZee
                        + 1.48 * dgZ1
                        + 0.88 * dkga
                        + 1.63 * dkZ
                        + 0.93 * dlga
                        + 1.67 * dlZ
                        + 0.81 * dgga1
                        + 1.69 * deem
                        );
 
                break;
        }
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::deltadxsdcoseeWWlvjjLEP2()");
 
    //Add relative theory errors (free par). (Assume they are constant in energy.)
    xspb += edeeWWdcint * xspbSM;
 
    if ((xspbSM + xspb) < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return xspb;
}

◆ deltaeNP()

const double NPSMEFTd6General::deltaeNP ( const double mu ) const

virtual

The new physics relative contribution to the EW coupling constant $e$.

Returns: $\delta e$

Reimplemented from NPbase.

Definition at line 36474 of file NPSMEFTd6General.cpp.

                                                             {
    
    double NPindirect;
 
    NPindirect = del_e_mu(mu) + 0.5 * del_A_mu(mu);
 
    return NPindirect;
}

◆ deltaG1_hWW()

const double NPSMEFTd6General::deltaG1_hWW ( ) const

virtual

The new physics contribution to the coupling of the effective interaction $H W_{\mu\nu}^\dagger W^{\mu\nu}$.

Returns: $\delta g_{HWW}^{(1)}$

Reimplemented from NPbase.

Definition at line 17302 of file NPSMEFTd6General.cpp.

                                                 {
    return ((2.0 * getSMEFTCoeffEW("CHW")) * v2 / v());
}

◆ deltaG1_hWW_mu()

const double NPSMEFTd6General::deltaG1_hWW_mu ( const double mu ) const

virtual

The new physics contribution to the coupling of the effective interaction $H W_{\mu\nu}^\dagger W^{\mu\nu}$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HWW}^{(1)}(\mu)$

Reimplemented from NPbase.

Definition at line 17551 of file NPSMEFTd6General.cpp.

                                                                   {
    return ((2.0 * getSMEFTCoeff("CHW", mu)) * v2 / v());
}

◆ deltaG1_hZA()

const double NPSMEFTd6General::deltaG1_hZA ( ) const

virtual

The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} F^{\mu\nu}$.

Returns: $\delta g_{HZA}^{(1)}$

Reimplemented from NPbase.

Definition at line 17339 of file NPSMEFTd6General.cpp.

                                                 {
    return ( delta_AZ / v());
}

◆ deltaG1_hZA_mu()

const double NPSMEFTd6General::deltaG1_hZA_mu ( const double mu ) const

virtual

The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} F^{\mu\nu}$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HZA}^{(1)}(\mu)$

Reimplemented from NPbase.

Definition at line 17600 of file NPSMEFTd6General.cpp.

                                                                   {
    
    double d_AZ_mu; 
    
    // delta_AZ as function os scale
    d_AZ_mu = 2.0 * sW_tree * cW_tree * (getSMEFTCoeff("CHW", mu) - getSMEFTCoeff("CHB", mu)) * v2
            - (cW2_tree - sW2_tree) * getSMEFTCoeff("CHWB", mu) * v2;
    
    return ( d_AZ_mu / v());
}

◆ deltaG1_hZARatio()

const double NPSMEFTd6General::deltaG1_hZARatio ( ) const

virtual

The full new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} F^{A \mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value.

Returns: $\delta g_{HZA}^{(1)}/g_{HZA}^{(1),SM}$

Reimplemented from NPbase.

Definition at line 17343 of file NPSMEFTd6General.cpp.

                                                      {
    double m_t = mtpole;
    double m_b = quarks[BOTTOM].getMass();
    double m_c = quarks[CHARM].getMass();
    double m_s = quarks[STRANGE].getMass();
    double m_tau = leptons[TAU].getMass();
    double m_mu = leptons[MU].getMass();
 
    double M_w_2 = (trueSM.Mw())*(trueSM.Mw());
 
    double Qt = quarks[TOP].getCharge();
    double Qb = quarks[BOTTOM].getCharge();
    double Qc = quarks[CHARM].getCharge();
    double Qs = quarks[STRANGE].getCharge();
    double Qtau = leptons[TAU].getCharge();
    double Qmu = leptons[MU].getCharge();
 
    double tau_t = 4.0 * m_t * m_t / mHl / mHl;
    double tau_b = 4.0 * m_b * m_b / mHl / mHl;
    double tau_c = 4.0 * m_c * m_c / mHl / mHl;
    double tau_s = 4.0 * m_s * m_s / mHl / mHl;
    double tau_tau = 4.0 * m_tau * m_tau / mHl / mHl;
    double tau_mu = 4.0 * m_mu * m_mu / mHl / mHl;
    double tau_W = 4.0 * M_w_2 / mHl / mHl;
 
    double lambda_t = 4.0 * m_t * m_t / Mz / Mz;
    double lambda_b = 4.0 * m_b * m_b / Mz / Mz;
    double lambda_c = 4.0 * m_c * m_c / Mz / Mz;
    double lambda_s = 4.0 * m_s * m_s / Mz / Mz;
    double lambda_tau = 4.0 * m_tau * m_tau / Mz / Mz;
    double lambda_mu = 4.0 * m_mu * m_mu / Mz / Mz;
    double lambda_W = 4.0 * M_w_2 / Mz / Mz;
    double alpha2 = sqrt(2.0) * GF * M_w_2 / M_PI;
    double aPiv = sqrt(ale * alpha2) / 4.0 / M_PI / v();
 
    //  mod. of Higgs couplings
    gslpp::complex gSM, dg;
    gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
    gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
    gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
    gslpp::complex dKappa_s = cLHd6 * deltaG_hff(quarks[STRANGE]) / (-m_s / v());
    gslpp::complex dKappa_tau = cLHd6 * deltaG_hff(leptons[TAU]) / (-m_tau / v());
    gslpp::complex dKappa_mu = cLHd6 * deltaG_hff(leptons[MU]) / (-m_mu / v());
    double dKappa_W = cLHd6 * (0.5 * v() / M_w_2) * deltaG3_hWW();
 
    //  mod of EW vector couplings vf =2 gvf    
    double vSMt = 2.0 * (quarks[TOP].getIsospin()) - 4.0 * Qt * sW2_tree;
    double vSMb = 2.0 * (quarks[BOTTOM].getIsospin()) - 4.0 * Qb * sW2_tree;
    double vSMc = 2.0 * (quarks[CHARM].getIsospin()) - 4.0 * Qc * sW2_tree;
    double vSMs = 2.0 * (quarks[STRANGE].getIsospin()) - 4.0 * Qs * sW2_tree;
    double vSMtau = 2.0 * (leptons[TAU].getIsospin()) - 4.0 * Qtau * sW2_tree;
    double vSMmu = 2.0 * (leptons[MU].getIsospin()) - 4.0 * Qmu * sW2_tree;
 
    double dvSMt = cLHd6 * 2.0 * deltaGV_f(quarks[TOP]);
    double dvSMb = cLHd6 * 2.0 * deltaGV_f(quarks[BOTTOM]);
    double dvSMc = cLHd6 * 2.0 * deltaGV_f(quarks[CHARM]);
    double dvSMs = cLHd6 * 2.0 * deltaGV_f(quarks[STRANGE]);
    double dvSMtau = cLHd6 * 2.0 * deltaGV_f(leptons[TAU]);
    double dvSMmu = cLHd6 * 2.0 * deltaGV_f(leptons[MU]);
 
    double deltaloc = deltaG1_hZA();
 
    gSM = -aPiv * ((3.0 * vSMt * Qt * AHZga_f(tau_t, lambda_t) +
            3.0 * vSMb * Qb * AHZga_f(tau_b, lambda_b) +
            3.0 * vSMc * Qc * AHZga_f(tau_c, lambda_c) +
            3.0 * vSMs * Qs * AHZga_f(tau_s, lambda_s) +
            vSMtau * Qtau * AHZga_f(tau_tau, lambda_tau) +
            vSMmu * Qmu * AHZga_f(tau_mu, lambda_mu)) / cW_tree +
            AHZga_W(tau_W, lambda_W));
 
    dg = deltaloc / gSM - (aPiv / gSM) * (
            (3.0 * vSMt * dKappa_t * Qt * AHZga_f(tau_t, lambda_t) +
            3.0 * vSMb * dKappa_b * Qb * AHZga_f(tau_b, lambda_b) +
            3.0 * vSMc * dKappa_c * Qc * AHZga_f(tau_c, lambda_c) +
            3.0 * vSMs * dKappa_s * Qs * AHZga_f(tau_s, lambda_s) +
            dKappa_tau * vSMtau * Qtau * AHZga_f(tau_tau, lambda_tau) +
            dKappa_mu * vSMmu * Qmu * AHZga_f(tau_mu, lambda_mu)) / cW_tree +
            dKappa_W * AHZga_W(tau_W, lambda_W) +
            (3.0 * dvSMt * Qt * AHZga_f(tau_t, lambda_t) +
            3.0 * dvSMb * Qb * AHZga_f(tau_b, lambda_b) +
            3.0 * dvSMc * Qc * AHZga_f(tau_c, lambda_c) +
            3.0 * dvSMs * Qs * AHZga_f(tau_s, lambda_s) +
            dvSMtau * Qtau * AHZga_f(tau_tau, lambda_tau) +
            dvSMmu * Qmu * AHZga_f(tau_mu, lambda_mu)) / cW_tree
            );
 
    return dg.real();
}

◆ deltaG1_hZARatio_mu()

const double NPSMEFTd6General::deltaG1_hZARatio_mu ( const double mu ) const

virtual

The full new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} F^{A \mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HZA}^{(1)}(\mu)/g_{HZA}^{(1),SM}(\mu)$

Reimplemented from NPbase.

Definition at line 17611 of file NPSMEFTd6General.cpp.

                                                                        {
    double m_t = mtpole;
    double m_b = quarks[BOTTOM].getMass();
    double m_c = quarks[CHARM].getMass();
    double m_s = quarks[STRANGE].getMass();
    double m_tau = leptons[TAU].getMass();
    double m_mu = leptons[MU].getMass();
 
    double M_w_2 = (trueSM.Mw())*(trueSM.Mw());
 
    double Qt = quarks[TOP].getCharge();
    double Qb = quarks[BOTTOM].getCharge();
    double Qc = quarks[CHARM].getCharge();
    double Qs = quarks[STRANGE].getCharge();
    double Qtau = leptons[TAU].getCharge();
    double Qmu = leptons[MU].getCharge();
 
    double tau_t = 4.0 * m_t * m_t / mHl / mHl;
    double tau_b = 4.0 * m_b * m_b / mHl / mHl;
    double tau_c = 4.0 * m_c * m_c / mHl / mHl;
    double tau_s = 4.0 * m_s * m_s / mHl / mHl;
    double tau_tau = 4.0 * m_tau * m_tau / mHl / mHl;
    double tau_mu = 4.0 * m_mu * m_mu / mHl / mHl;
    double tau_W = 4.0 * M_w_2 / mHl / mHl;
 
    double lambda_t = 4.0 * m_t * m_t / Mz / Mz;
    double lambda_b = 4.0 * m_b * m_b / Mz / Mz;
    double lambda_c = 4.0 * m_c * m_c / Mz / Mz;
    double lambda_s = 4.0 * m_s * m_s / Mz / Mz;
    double lambda_tau = 4.0 * m_tau * m_tau / Mz / Mz;
    double lambda_mu = 4.0 * m_mu * m_mu / Mz / Mz;
    double lambda_W = 4.0 * M_w_2 / Mz / Mz;
    double alpha2 = sqrt(2.0) * GF * M_w_2 / M_PI;
    double aPiv = sqrt(ale * alpha2) / 4.0 / M_PI / v();
 
    //  mod. of Higgs couplings
    gslpp::complex gSM, dg;
    gslpp::complex dKappa_t = cLHd6 * deltaG_hff_mu(quarks[TOP], mu) / (-m_t / v());
    gslpp::complex dKappa_b = cLHd6 * deltaG_hff_mu(quarks[BOTTOM], mu) / (-m_b / v());
    gslpp::complex dKappa_c = cLHd6 * deltaG_hff_mu(quarks[CHARM], mu) / (-m_c / v());
    gslpp::complex dKappa_s = cLHd6 * deltaG_hff_mu(quarks[STRANGE], mu) / (-m_s / v());
    gslpp::complex dKappa_tau = cLHd6 * deltaG_hff_mu(leptons[TAU], mu) / (-m_tau / v());
    gslpp::complex dKappa_mu = cLHd6 * deltaG_hff_mu(leptons[MU], mu) / (-m_mu / v());
    double dKappa_W = cLHd6 * (0.5 * v() / M_w_2) * deltaG3_hWW_mu(mu);
 
    //  mod of EW vector couplings vf =2 gvf    
    double vSMt = 2.0 * (quarks[TOP].getIsospin()) - 4.0 * Qt * sW2_tree;
    double vSMb = 2.0 * (quarks[BOTTOM].getIsospin()) - 4.0 * Qb * sW2_tree;
    double vSMc = 2.0 * (quarks[CHARM].getIsospin()) - 4.0 * Qc * sW2_tree;
    double vSMs = 2.0 * (quarks[STRANGE].getIsospin()) - 4.0 * Qs * sW2_tree;
    double vSMtau = 2.0 * (leptons[TAU].getIsospin()) - 4.0 * Qtau * sW2_tree;
    double vSMmu = 2.0 * (leptons[MU].getIsospin()) - 4.0 * Qmu * sW2_tree;
 
    double dvSMt = cLHd6 * 2.0 * (deltaGL_f_mu(quarks[TOP], mu) + deltaGR_f_mu(quarks[TOP], mu)); //deltaGV_f(quarks[TOP]);
    double dvSMb = cLHd6 * 2.0 * (deltaGL_f_mu(quarks[BOTTOM], mu) + deltaGR_f_mu(quarks[BOTTOM], mu)); //deltaGV_f(quarks[BOTTOM]);
    double dvSMc = cLHd6 * 2.0 * (deltaGL_f_mu(quarks[CHARM], mu) + deltaGR_f_mu(quarks[CHARM], mu)); //deltaGV_f(quarks[CHARM]);
    double dvSMs = cLHd6 * 2.0 * (deltaGL_f_mu(quarks[STRANGE], mu) + deltaGR_f_mu(quarks[STRANGE], mu)); //deltaGV_f(quarks[STRANGE]);
    double dvSMtau = cLHd6 * 2.0 * (deltaGL_f_mu(leptons[TAU], mu) + deltaGR_f_mu(leptons[TAU], mu)); //deltaGV_f(leptons[TAU]);
    double dvSMmu = cLHd6 * 2.0 * (deltaGL_f_mu(leptons[MU], mu) + deltaGR_f_mu(leptons[MU], mu)); //deltaGV_f(leptons[MU]);
 
    double deltaloc = deltaG1_hZA_mu(mu);
 
    gSM = -aPiv * ((3.0 * vSMt * Qt * AHZga_f(tau_t, lambda_t) +
            3.0 * vSMb * Qb * AHZga_f(tau_b, lambda_b) +
            3.0 * vSMc * Qc * AHZga_f(tau_c, lambda_c) +
            3.0 * vSMs * Qs * AHZga_f(tau_s, lambda_s) +
            vSMtau * Qtau * AHZga_f(tau_tau, lambda_tau) +
            vSMmu * Qmu * AHZga_f(tau_mu, lambda_mu)) / cW_tree +
            AHZga_W(tau_W, lambda_W));
 
    dg = deltaloc / gSM - (aPiv / gSM) * (
            (3.0 * vSMt * dKappa_t * Qt * AHZga_f(tau_t, lambda_t) +
            3.0 * vSMb * dKappa_b * Qb * AHZga_f(tau_b, lambda_b) +
            3.0 * vSMc * dKappa_c * Qc * AHZga_f(tau_c, lambda_c) +
            3.0 * vSMs * dKappa_s * Qs * AHZga_f(tau_s, lambda_s) +
            dKappa_tau * vSMtau * Qtau * AHZga_f(tau_tau, lambda_tau) +
            dKappa_mu * vSMmu * Qmu * AHZga_f(tau_mu, lambda_mu)) / cW_tree +
            dKappa_W * AHZga_W(tau_W, lambda_W) +
            (3.0 * dvSMt * Qt * AHZga_f(tau_t, lambda_t) +
            3.0 * dvSMb * Qb * AHZga_f(tau_b, lambda_b) +
            3.0 * dvSMc * Qc * AHZga_f(tau_c, lambda_c) +
            3.0 * dvSMs * Qs * AHZga_f(tau_s, lambda_s) +
            dvSMtau * Qtau * AHZga_f(tau_tau, lambda_tau) +
            dvSMmu * Qmu * AHZga_f(tau_mu, lambda_mu)) / cW_tree
            );
 
    return dg.real();
}

◆ deltaG1_hZZ()

const double NPSMEFTd6General::deltaG1_hZZ ( ) const

virtual

The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} Z^{\mu\nu}$.

Returns: $\delta g_{HZZ}^{(1)}$

Reimplemented from NPbase.

Definition at line 17323 of file NPSMEFTd6General.cpp.

                                                 {
    return ( delta_ZZ / v());
}

◆ deltaG1_hZZ_mu()

const double NPSMEFTd6General::deltaG1_hZZ_mu ( const double mu ) const

virtual

The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} Z^{\mu\nu}$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HZZ}^{(1)}(\mu)$

Reimplemented from NPbase.

Definition at line 17573 of file NPSMEFTd6General.cpp.

                                                                   {
    
    double d_ZZ_mu;
    
    // delta_ZZ as function os scale
    d_ZZ_mu = (cW2_tree * getSMEFTCoeff("CHW", mu) + sW2_tree * getSMEFTCoeff("CHB", mu) + sW_tree * cW_tree * getSMEFTCoeff("CHWB", mu)) * v2;
 
    return ( d_ZZ_mu / v());
}

◆ deltag1gaNP()

const double NPSMEFTd6General::deltag1gaNP ( const double mu ) const

virtual

The new physics contribution to the anomalous triple gauge coupling $g_{1,\gamma}$.

Returns: $\delta g_{1,\gamma}$

Reimplemented from NPbase.

Definition at line 36507 of file NPSMEFTd6General.cpp.

                                                                {
    double NPindirect;
 
    NPindirect = del_e_mu(mu) + 0.5 * del_A_mu(mu);
 
    return NPindirect;
}

◆ deltag1ZNP()

const double NPSMEFTd6General::deltag1ZNP ( const double mu ) const

virtual

The new physics contribution to the anomalous triple gauge coupling $g_{1,Z}$.

Returns: $\delta g_{1,Z}$

Reimplemented from NPbase.

Definition at line 36485 of file NPSMEFTd6General.cpp.

                                                               {
    double NPdirect, NPindirect;
 
    NPdirect = 0.;
 
    //      NPindirect = - 1.0 / (cW2_tree-sW2_tree);
 
    //      NPindirect = NPindirect * (sW_tree * getSMEFTCoeffEW("CHWB") / cW_tree 
    //              + 0.25 * getSMEFTCoeffEW("CHD") ) * v2
    //              + 0.5 * NPindirect * delta_GF ;
 
    NPindirect = del_e_mu(mu) - 0.5 * del_sW2_mu(mu) / cW2_tree + 0.5 * del_Z_mu(mu) - sW_tree * del_ZA_mu(mu) / cW_tree;
 
    return NPdirect + NPindirect;
}

◆ deltag1ZNPEff()

const double NPSMEFTd6General::deltag1ZNPEff ( ) const

virtual

The new physics contribution to the effective anomalous triple gauge coupling $g_{1,Z}^{Eff}$ from arXiv: 1708.09079 [hep-ph].

Returns: $\delta g_{1,Z}$

Reimplemented from NPbase.

Definition at line 36537 of file NPSMEFTd6General.cpp.

                                                   {
    // From arXiv:1708.09079 [hep-ph]. In our case, delta_e=0 since it is taken as inputs and its effects propagated
    // everywhere else 
    double dgEff;
 
    dgEff = (1.0 / cW2_tree) * ((cW2_tree - sW2_tree) * deltaGL_f(leptons[ELECTRON]) / gZlL +
            sW2_tree * deltaGR_f(leptons[ELECTRON]) / gZlR -
            2.0 * deltaGL_Wff(leptons[NEUTRINO_1], leptons[ELECTRON]).real() / UevL);
 
    return dgEff + deltag1ZNP(muw);
}

◆ deltaG2_hWW()

const double NPSMEFTd6General::deltaG2_hWW ( ) const

virtual

The new physics contribution to the coupling of the effective interaction $H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}$.

Returns: $\delta g_{HWW}^{(2)}$

Reimplemented from NPbase.

Definition at line 17306 of file NPSMEFTd6General.cpp.

                                                 {
    return 0.0;
}

◆ deltaG2_hWW_mu()

const double NPSMEFTd6General::deltaG2_hWW_mu ( const double mu ) const

virtual

The new physics contribution to the coupling of the effective interaction $H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HWW}^{(2)}(\mu)$

Reimplemented from NPbase.

Definition at line 17555 of file NPSMEFTd6General.cpp.

                                                                   {
    return 0.0;
}

◆ deltaG2_hZA()

const double NPSMEFTd6General::deltaG2_hZA ( ) const

virtual

The new physics contribution to the coupling of the effective interaction $H Z_{\nu} \partial^\mu F^{\mu\nu}$.

Returns: $\delta g_{HZA}^{(2)}$

Reimplemented from NPbase.

Definition at line 17432 of file NPSMEFTd6General.cpp.

                                                 {
    return 0.0;
}

◆ deltaG2_hZA_mu()

const double NPSMEFTd6General::deltaG2_hZA_mu ( const double mu ) const

virtual

The new physics contribution to the coupling of the effective interaction $H Z_{\nu} \partial^\mu F^{\mu\nu}$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HZA}^{(2)}(\mu)$

Reimplemented from NPbase.

Definition at line 17700 of file NPSMEFTd6General.cpp.

                                                                   {
    return 0.0;
}

◆ deltaG2_hZZ()

const double NPSMEFTd6General::deltaG2_hZZ ( ) const

virtual

The new physics contribution to the coupling of the effective interaction $H Z_{\nu} \partial^\mu Z^{\mu\nu}$.

Returns: $\delta g_{HZZ}^{(2)}$

Reimplemented from NPbase.

Definition at line 17327 of file NPSMEFTd6General.cpp.

                                                 {
    return 0.0;
}

◆ deltaG2_hZZ_mu()

const double NPSMEFTd6General::deltaG2_hZZ_mu ( const double mu ) const

virtual

The new physics contribution to the coupling of the effective interaction $H Z_{\nu} \partial^\mu Z^{\mu\nu}$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HZZ}^{(2)}(\mu)$

Reimplemented from NPbase.

Definition at line 17583 of file NPSMEFTd6General.cpp.

                                                                   {
    return 0.0;
}

◆ deltaG3_hWW()

const double NPSMEFTd6General::deltaG3_hWW ( ) const

virtual

The new physics contribution to the coupling of the effective interaction $H W_{\mu}^\dagger W^{\mu}$.

Returns: $\delta g_{HWW}^{(3)}$

Reimplemented from NPbase.

Definition at line 17310 of file NPSMEFTd6General.cpp.

                                                 {
    double NPindirect;
 
    //    NPindirect = 2.0 * cW2_tree * Mz * Mz / v()
    //                * (delta_h - 1.0 / 2.0 / (cW2_tree - sW2_tree)
    //                * ((4.0 * sW_tree * cW_tree * getSMEFTCoeffEW("CHWB") + cW2_tree * getSMEFTCoeffEW("CHD")) * v2_over_LambdaNP2 + delta_GF));
 
    NPindirect = 2.0 * cW2_tree * Mz * Mz / v()
            * (delta_h + 0.5 * delta_GF + 2.0 * delta_e - delta_sW2);
 
    return NPindirect;
}

◆ deltaG3_hWW_mu()

const double NPSMEFTd6General::deltaG3_hWW_mu ( const double mu ) const

virtual

The new physics contribution to the coupling of the effective interaction $H W_{\mu}^\dagger W^{\mu}$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HWW}^{(3)}(\mu)$

Reimplemented from NPbase.

Definition at line 17559 of file NPSMEFTd6General.cpp.

                                                                   {
    double NPindirect;
 
    double d_h_mu, d_GF_mu;
    
    d_h_mu = (-getSMEFTCoeff("CHD", mu) / 4.0 + getSMEFTCoeff("CHbox", mu)) * v2;
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
 
    NPindirect = 2.0 * cW2_tree * Mz * Mz / v()
            * (d_h_mu + 0.5 * d_GF_mu + 2.0 * del_e_mu(mu) - del_sW2_mu(mu));
 
    return NPindirect;
}

◆ deltaG3_hZZ()

const double NPSMEFTd6General::deltaG3_hZZ ( ) const

virtual

The new physics contribution to the coupling of the effective interaction $H Z_{\mu} Z^{\mu}$.

Returns: $\delta g_{HZZ}^{(3)}$

Reimplemented from NPbase.

Definition at line 17331 of file NPSMEFTd6General.cpp.

                                                 {
    //    double NPindirect = Mz * Mz / v() * (-0.5 * getSMEFTCoeffEW("CHD") * v2_over_LambdaNP2 + delta_h - 0.5 * delta_GF);
    double NPindirect = Mz * Mz / v() * (delta_Z + delta_h + 0.5 * delta_GF + 2.0 * delta_e - (1.0 - sW2_tree / cW2_tree) * delta_sW2);
    double NPdirect = Mz * Mz / v() * getSMEFTCoeffEW("CHD") * v2;
 
    return (NPindirect + NPdirect);
}

◆ deltaG3_hZZ_mu()

const double NPSMEFTd6General::deltaG3_hZZ_mu ( const double mu ) const

virtual

The new physics contribution to the coupling of the effective interaction $H Z_{\mu} Z^{\mu}$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HZZ}^{(3)}(\mu)$

Reimplemented from NPbase.

Definition at line 17587 of file NPSMEFTd6General.cpp.

                                                                   {
    
    double d_h_mu, d_GF_mu;
    
    d_h_mu = (-getSMEFTCoeff("CHD", mu) / 4.0 + getSMEFTCoeff("CHbox", mu)) * v2;
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
 
    double NPindirect = Mz * Mz / v() * (del_Z_mu(mu) + d_h_mu + 0.5 * d_GF_mu + 2.0 * del_e_mu(mu) - (1.0 - sW2_tree / cW2_tree) * del_sW2_mu(mu));
    double NPdirect = Mz * Mz / v() * getSMEFTCoeff("CHD", mu) * v2;
 
    return (NPindirect + NPdirect);
}

◆ deltag3G()

const double NPSMEFTd6General::deltag3G ( ) const

The new physics contribution to the coupling of the effective interaction $f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C$.

Returns: $\delta g_{3G}$

Definition at line 17880 of file NPSMEFTd6General.cpp.

                                              {
    // Set to 0. for the moment 
 
    return 0.;
}

◆ deltaG_Aff()

gslpp::complex NPSMEFTd6General::deltaG_Aff ( const Particle p ) const

The new physics contribution to the coupling of the effective interaction $A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$.

Parameters

[in] p a lepton or quark

Returns: $\delta g_{Aff}$

Definition at line 17874 of file NPSMEFTd6General.cpp.

                                                                {
    // Set to 0. for the moment 
 
    return 0.;
}

◆ deltaG_Gff()

gslpp::complex NPSMEFTd6General::deltaG_Gff ( const Particle p ) const

The new physics contribution to the coupling of the effective interaction $G_{\mu\nu}^A \bar{f}\sigma^{\mu\nu} T_A f$.

Parameters

[in] p a lepton or quark

Returns: $\delta g_{Gff}$

Definition at line 17862 of file NPSMEFTd6General.cpp.

                                                                {
    // Set to 0. for the moment 
 
    return 0.;
}

◆ deltaG_hAA()

const double NPSMEFTd6General::deltaG_hAA ( ) const

virtual

The new physics contribution to the coupling of the effective interaction $H F_{\mu\nu} F^{\mu\nu}$.

Returns: $\delta g_{HAA}$

Reimplemented from NPbase.

Definition at line 17436 of file NPSMEFTd6General.cpp.

                                                {
    return (delta_AA / v());
}

◆ deltaG_hAA_mu()

const double NPSMEFTd6General::deltaG_hAA_mu ( const double mu ) const

virtual

The new physics contribution to the coupling of the effective interaction $H F_{\mu\nu} F^{\mu\nu}$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HAA}(\mu)$

Reimplemented from NPbase.

Definition at line 17704 of file NPSMEFTd6General.cpp.

                                                                  {
    
    double d_AA_mu;
    
    // delta_AA as function os scale
    d_AA_mu = (sW2_tree * getSMEFTCoeff("CHW", mu) + cW2_tree * getSMEFTCoeff("CHB", mu) - sW_tree * cW_tree * getSMEFTCoeff("CHWB", mu)) * v2;
 
    return (d_AA_mu / v());
}

◆ deltaG_hAARatio()

const double NPSMEFTd6General::deltaG_hAARatio ( ) const

virtual

The full new physics contribution to the coupling of the effective interaction $H F_{\mu\nu} F^{\mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value.

Returns: $\delta g_{HAA}/g_{HAA}^SM}$

Reimplemented from NPbase.

Definition at line 17440 of file NPSMEFTd6General.cpp.

                                                     {
    double m_t = mtpole;
    double m_b = quarks[BOTTOM].getMass();
    double m_c = quarks[CHARM].getMass();
    double m_s = quarks[STRANGE].getMass();
    double m_tau = leptons[TAU].getMass();
    double m_mu = leptons[MU].getMass();
 
    double M_w_2 = (trueSM.Mw())*(trueSM.Mw());
 
    double Qt = quarks[TOP].getCharge();
    double Qb = quarks[BOTTOM].getCharge();
    double Qc = quarks[CHARM].getCharge();
    double Qs = quarks[STRANGE].getCharge();
    double Qtau = leptons[TAU].getCharge();
    double Qmu = leptons[MU].getCharge();
 
    double tau_t = 4.0 * m_t * m_t / mHl / mHl;
    double tau_b = 4.0 * m_b * m_b / mHl / mHl;
    double tau_c = 4.0 * m_c * m_c / mHl / mHl;
    double tau_s = 4.0 * m_s * m_s / mHl / mHl;
    double tau_tau = 4.0 * m_tau * m_tau / mHl / mHl;
    double tau_mu = 4.0 * m_mu * m_mu / mHl / mHl;
    double tau_W = 4.0 * M_w_2 / mHl / mHl;
 
    double aPiv = ale / 8.0 / M_PI / v();
    gslpp::complex gSM, dg;
    gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
    gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
    gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
    gslpp::complex dKappa_s = cLHd6 * deltaG_hff(quarks[STRANGE]) / (-m_s / v());
    gslpp::complex dKappa_tau = cLHd6 * deltaG_hff(leptons[TAU]) / (-m_tau / v());
    gslpp::complex dKappa_mu = cLHd6 * deltaG_hff(leptons[MU]) / (-m_mu / v());
    double dKappa_W = cLHd6 * (0.5 * v() / M_w_2) * deltaG3_hWW();
 
    double deltaloc = deltaG_hAA();
 
    gSM = aPiv * (3.0 * Qt * Qt * AH_f(tau_t) +
            3.0 * Qb * Qb * AH_f(tau_b) +
            3.0 * Qc * Qc * AH_f(tau_c) +
            3.0 * Qs * Qs * AH_f(tau_s) +
            Qtau * Qtau * AH_f(tau_tau) +
            Qmu * Qmu * AH_f(tau_mu) +
            AH_W(tau_W));
 
    dg = deltaloc / gSM + (aPiv / gSM) * (
            3.0 * Qt * Qt * dKappa_t * AH_f(tau_t) +
            3.0 * Qb * Qb * dKappa_b * AH_f(tau_b) +
            3.0 * Qc * Qc * dKappa_c * AH_f(tau_c) +
            3.0 * Qs * Qs * dKappa_s * AH_f(tau_s) +
            dKappa_tau * Qtau * Qtau * AH_f(tau_tau) +
            dKappa_mu * Qmu * Qmu * AH_f(tau_mu) +
            dKappa_W * AH_W(tau_W)
            );
 
    return dg.real();
}

◆ deltaG_hAARatio_mu()

const double NPSMEFTd6General::deltaG_hAARatio_mu ( const double mu ) const

virtual

The full new physics contribution to the coupling of the effective interaction $H F_{\mu\nu} F^{\mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HAA}(\mu)/g_{HAA}^SM(\mu)}$

Reimplemented from NPbase.

Definition at line 17714 of file NPSMEFTd6General.cpp.

                                                                       {
    double m_t = mtpole;
    double m_b = quarks[BOTTOM].getMass();
    double m_c = quarks[CHARM].getMass();
    double m_s = quarks[STRANGE].getMass();
    double m_tau = leptons[TAU].getMass();
    double m_mu = leptons[MU].getMass();
 
    double M_w_2 = (trueSM.Mw())*(trueSM.Mw());
 
    double Qt = quarks[TOP].getCharge();
    double Qb = quarks[BOTTOM].getCharge();
    double Qc = quarks[CHARM].getCharge();
    double Qs = quarks[STRANGE].getCharge();
    double Qtau = leptons[TAU].getCharge();
    double Qmu = leptons[MU].getCharge();
 
    double tau_t = 4.0 * m_t * m_t / mHl / mHl;
    double tau_b = 4.0 * m_b * m_b / mHl / mHl;
    double tau_c = 4.0 * m_c * m_c / mHl / mHl;
    double tau_s = 4.0 * m_s * m_s / mHl / mHl;
    double tau_tau = 4.0 * m_tau * m_tau / mHl / mHl;
    double tau_mu = 4.0 * m_mu * m_mu / mHl / mHl;
    double tau_W = 4.0 * M_w_2 / mHl / mHl;
 
    double aPiv = ale / 8.0 / M_PI / v();
    gslpp::complex gSM, dg;
    gslpp::complex dKappa_t = cLHd6 * deltaG_hff_mu(quarks[TOP], mu) / (-m_t / v());
    gslpp::complex dKappa_b = cLHd6 * deltaG_hff_mu(quarks[BOTTOM], mu) / (-m_b / v());
    gslpp::complex dKappa_c = cLHd6 * deltaG_hff_mu(quarks[CHARM], mu) / (-m_c / v());
    gslpp::complex dKappa_s = cLHd6 * deltaG_hff_mu(quarks[STRANGE], mu) / (-m_s / v());
    gslpp::complex dKappa_tau = cLHd6 * deltaG_hff_mu(leptons[TAU], mu) / (-m_tau / v());
    gslpp::complex dKappa_mu = cLHd6 * deltaG_hff_mu(leptons[MU], mu) / (-m_mu / v());
    double dKappa_W = cLHd6 * (0.5 * v() / M_w_2) * deltaG3_hWW_mu(mu);
 
    double deltaloc = deltaG_hAA_mu(mu);
 
    gSM = aPiv * (3.0 * Qt * Qt * AH_f(tau_t) +
            3.0 * Qb * Qb * AH_f(tau_b) +
            3.0 * Qc * Qc * AH_f(tau_c) +
            3.0 * Qs * Qs * AH_f(tau_s) +
            Qtau * Qtau * AH_f(tau_tau) +
            Qmu * Qmu * AH_f(tau_mu) +
            AH_W(tau_W));
 
    dg = deltaloc / gSM + (aPiv / gSM) * (
            3.0 * Qt * Qt * dKappa_t * AH_f(tau_t) +
            3.0 * Qb * Qb * dKappa_b * AH_f(tau_b) +
            3.0 * Qc * Qc * dKappa_c * AH_f(tau_c) +
            3.0 * Qs * Qs * dKappa_s * AH_f(tau_s) +
            dKappa_tau * Qtau * Qtau * AH_f(tau_tau) +
            dKappa_mu * Qmu * Qmu * AH_f(tau_mu) +
            dKappa_W * AH_W(tau_W)
            );
 
    return dg.real();
}

◆ deltaG_hAff()

gslpp::complex NPSMEFTd6General::deltaG_hAff ( const Particle p ) const

The new physics contribution to the coupling of the effective interaction $H A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$.

Parameters

[in] p a lepton or quark

Returns: $\delta g_{hAff}$

Definition at line 17854 of file NPSMEFTd6General.cpp.

                                                                 {
    // Set to 0. for the moment 
 
    return 0.;
}

◆ deltaG_hff()

gslpp::complex NPSMEFTd6General::deltaG_hff ( const Particle p ) const

virtual

The new physics contribution to the coupling of the effective interaction $H f\bar{f}$.

Parameters

[in] p a lepton or quark

Returns: $\delta g_{Hff}$

Reimplemented from NPbase.

Definition at line 17498 of file NPSMEFTd6General.cpp.

                                                                {
    // The effects of the RG running are neglected. 
    double mf;
    if (p.is("TOP"))
        //mf = p.getMass(); // m_t(m_t)
        mf = mtpole; // pole mass
    else
        mf = p.getMass();
    gslpp::complex CfH = CfH_diag(p);
    return (-mf / v() * (delta_h - 0.5 * delta_GF)
            + CfH * v2 / sqrt(2.0));
}

◆ deltaG_hff_mu()

gslpp::complex NPSMEFTd6General::deltaG_hff_mu	(	const Particle	p,
		const double	mu
	)		const

virtual

The new physics contribution to the coupling of the effective interaction $H f\bar{f}$.

Parameters

[in]	p	a lepton or quark
[in]	mu	the RG scale to be used in the evaluation

Returns: $\delta g_{Hff}(\mu)$

Reimplemented from NPbase.

Definition at line 17772 of file NPSMEFTd6General.cpp.

                                                                                    {
    // The effects of the SM RG running are neglected. 
    double mf;
    
    double d_h_mu, d_GF_mu;
    
    d_h_mu = (-getSMEFTCoeff("CHD", mu) / 4.0 + getSMEFTCoeff("CHbox", mu)) * v2;
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
    
    if (p.is("TOP"))
        //mf = p.getMass(); // m_t(m_t)
        mf = mtpole; // pole mass
    else
        mf = p.getMass();
 
    gslpp::complex CfH = CfH_diag_mu(p, mu);
    
    return (-mf / v() * (d_h_mu - 0.5 * d_GF_mu)
            + CfH * v2 / sqrt(2.0));
}

◆ deltaG_hGff()

gslpp::complex NPSMEFTd6General::deltaG_hGff ( const Particle p ) const

The new physics contribution to the coupling of the effective interaction $H G_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$.

Parameters

[in] p a lepton or quark

Returns: $\delta g_{hGff}$

Definition at line 17842 of file NPSMEFTd6General.cpp.

                                                                 {
    // Set to 0. for the moment 
 
    return 0.;
}

◆ deltaG_hgg()

const double NPSMEFTd6General::deltaG_hgg ( ) const

virtual

The new physics contribution to the coupling of the effective interaction $H G_{\mu\nu}^AG^{A \mu\nu}$.

Returns: $\delta g_{HGG}$

Reimplemented from NPbase.

Definition at line 17273 of file NPSMEFTd6General.cpp.

                                                {
    return (getSMEFTCoeffEW("CHG") * v2 / v());
}

◆ deltaG_hgg_mu()

const double NPSMEFTd6General::deltaG_hgg_mu ( const double mu ) const

virtual

The new physics contribution to the coupling of the effective interaction $H G_{\mu\nu}^AG^{A \mu\nu}$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HGG}(\mu)$

Reimplemented from NPbase.

Definition at line 17522 of file NPSMEFTd6General.cpp.

                                                                  {
    return (getSMEFTCoeff("CHG", mu) * v2 / v());
}

◆ deltaG_hggRatio()

const double NPSMEFTd6General::deltaG_hggRatio ( ) const

virtual

The full new physics contribution to the coupling of the effective interaction $H G_{\mu\nu}^AG^{A \mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value.

Returns: $\delta g_{HGG}/g_{HGG}^SM}$

Reimplemented from NPbase.

Definition at line 17277 of file NPSMEFTd6General.cpp.

                                                     {
    double m_t = mtpole;
    double m_b = quarks[BOTTOM].getMass();
    double m_c = quarks[CHARM].getMass();
    double m_s = quarks[STRANGE].getMass();
    double tau_t = 4.0 * m_t * m_t / mHl / mHl;
    double tau_b = 4.0 * m_b * m_b / mHl / mHl;
    double tau_c = 4.0 * m_c * m_c / mHl / mHl;
    double tau_s = 4.0 * m_s * m_s / mHl / mHl;
    double aSPiv = AlsMz / 16.0 / M_PI / v();
    gslpp::complex gSM, dg;
    gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
    gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
    gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
    gslpp::complex dKappa_s = cLHd6 * deltaG_hff(quarks[STRANGE]) / (-m_s / v());
    
    double deltaloc = deltaG_hgg();
 
    gSM = aSPiv * (AH_f(tau_t) + AH_f(tau_b) + AH_f(tau_c));
 
    dg = deltaloc / gSM + (aSPiv / gSM) * (dKappa_t * AH_f(tau_t) + dKappa_b * AH_f(tau_b) + dKappa_c * AH_f(tau_c) + dKappa_s * AH_f(tau_s));
 
    return dg.real();
}

◆ deltaG_hggRatio_mu()

const double NPSMEFTd6General::deltaG_hggRatio_mu ( const double mu ) const

virtual

The full new physics contribution to the coupling of the effective interaction $H G_{\mu\nu}^AG^{A \mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HGG}(\mu)/g_{HGG}^SM}(\mu)$

Reimplemented from NPbase.

Definition at line 17526 of file NPSMEFTd6General.cpp.

                                                                       {
    double m_t = mtpole;
    double m_b = quarks[BOTTOM].getMass();
    double m_c = quarks[CHARM].getMass();
    double m_s = quarks[STRANGE].getMass();
    double tau_t = 4.0 * m_t * m_t / mHl / mHl;
    double tau_b = 4.0 * m_b * m_b / mHl / mHl;
    double tau_c = 4.0 * m_c * m_c / mHl / mHl;
    double tau_s = 4.0 * m_s * m_s / mHl / mHl;
    double aSPiv = AlsMz / 16.0 / M_PI / v();
    gslpp::complex gSM, dg;
    gslpp::complex dKappa_t = cLHd6 * deltaG_hff_mu(quarks[TOP], mu) / (-m_t / v());
    gslpp::complex dKappa_b = cLHd6 * deltaG_hff_mu(quarks[BOTTOM], mu) / (-m_b / v());
    gslpp::complex dKappa_c = cLHd6 * deltaG_hff_mu(quarks[CHARM], mu) / (-m_c / v());
    gslpp::complex dKappa_s = cLHd6 * deltaG_hff_mu(quarks[STRANGE], mu) / (-m_s / v());
    
    double deltaloc = deltaG_hgg_mu(mu);
 
    gSM = aSPiv * (AH_f(tau_t) + AH_f(tau_b) + AH_f(tau_c));
 
    dg = deltaloc / gSM + (aSPiv / gSM) * (dKappa_t * AH_f(tau_t) + dKappa_b * AH_f(tau_b) + dKappa_c * AH_f(tau_c) + dKappa_s * AH_f(tau_s));
 
    return dg.real();
}

◆ deltaG_hhhRatio()

const double NPSMEFTd6General::deltaG_hhhRatio ( ) const

virtual

The new physics contribution to the Higgs self-coupling $ H H H$. Normalized to the SM value.

Returns: $\delta g_{HHH}/g_{HHH}^SM}$

Reimplemented from NPbase.

Definition at line 17511 of file NPSMEFTd6General.cpp.

                                                     {
    double dg;
 
    dg = -0.5 * delta_GF + 3.0 * delta_h - 2.0 * getSMEFTCoeffEW("CH") * v2 * v2 / mHl / mHl;
 
    return dg;
}

◆ deltaG_hhhRatio_mu()

const double NPSMEFTd6General::deltaG_hhhRatio_mu ( const double mu ) const

virtual

The new physics contribution to the Higgs self-coupling $ H H H$. Normalized to the SM value.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta g_{HHH}/g_{HHH}^SM}(\mu)$

Reimplemented from NPbase.

Definition at line 17793 of file NPSMEFTd6General.cpp.

                                                                       {
    double dg;
    double d_h_mu, d_GF_mu;
    
    d_h_mu = (-getSMEFTCoeff("CHD", mu) / 4.0 + getSMEFTCoeff("CHbox", mu)) * v2;
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
 
    dg = -0.5 * d_GF_mu + 3.0 * d_h_mu - 2.0 * getSMEFTCoeff("CH", mu) * v2 * v2 / mHl / mHl;
 
    return dg;
}

◆ deltaG_hZff()

gslpp::complex NPSMEFTd6General::deltaG_hZff ( const Particle p ) const

The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$.

Parameters

[in] p a lepton or quark

Returns: $\delta g_{hZff}$

Definition at line 17848 of file NPSMEFTd6General.cpp.

                                                                 {
    // Set to 0. for the moment 
 
    return 0.;
}

◆ deltaG_Zff()

gslpp::complex NPSMEFTd6General::deltaG_Zff ( const Particle p ) const

The new physics contribution to the coupling of the effective interaction $Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$.

Parameters

[in] p a lepton or quark

Returns: $\delta g_{Zff}$

Definition at line 17868 of file NPSMEFTd6General.cpp.

                                                                {
    // Set to 0. for the moment 
 
    return 0.;
}

◆ deltaGA_f()

const double NPSMEFTd6General::deltaGA_f ( const Particle p ) const

virtual

New physics contribution to the neutral-current axial-vector coupling $g_A^f$.

Parameters

[in] f a lepton or quark

Returns: $\delta g_A^f$

Reimplemented from NPbase.

Definition at line 17019 of file NPSMEFTd6General.cpp.

                                                               {
    return (deltaGL_f(p) - deltaGR_f(p));
}

◆ deltaGamma_W()

const double NPSMEFTd6General::deltaGamma_W ( ) const

virtual

The new physics contribution to the total decay width of the $W$ boson, $\delta \Gamma_W$.

Returns: $\delta \Gamma_W$ in GeV

Reimplemented from NPbase.

Definition at line 15723 of file NPSMEFTd6General.cpp.

                                                  {
    double G0 = GF * pow(Mz*cW_tree, 3.0) / 6.0 / sqrt(2.0) / M_PI;
    double GammaW_tree = (3.0 + 2.0 * Nc) * G0;
 
    //    return (- 3.0 * GammaW_tree / 4.0 / (cW2_tree - sW2_tree)
    //            *(4.0 * sW_tree * cW_tree * getSMEFTCoeffEW("CHWB") * v2_over_LambdaNP2
    //            + cW2_tree * getSMEFTCoeffEW("CHD") * v2_over_LambdaNP2
    //            + 2.0 * (1.0 + cW2_tree) / 3.0 * delta_GF)
    //            + 2.0 * G0 * (getSMEFTCoeffEW("CHl3R",0,0) + getSMEFTCoeffEW("CHl3R",1,1) + getSMEFTCoeffEW("CHl3R",2,2) + Nc*(getSMEFTCoeffEW("CHq3R",0,0) + getSMEFTCoeffEW("CHq3R",1,1))) * v2_over_LambdaNP2);          
 
    double deltaNLO;
 
    // Finite NLO corrections    
    deltaNLO = (-0.001145 * getSMEFTCoeffEW("CW")  -0.000142 * getSMEFTCoeffEW("CHbox")  +0.020351 * getSMEFTCoeffEW("CHD")  -0.001153 * getSMEFTCoeffEW("CHW")   
            +0.045955 * getSMEFTCoeffEW("CHWB")  +0.004077 * getSMEFTCoeffEW("CuWR",2, 2) -0.002262 * getSMEFTCoeffEW("CHl1R",0, 0) -0.002262 * getSMEFTCoeffEW("CHl1R",1, 1)  
            -0.000171 * getSMEFTCoeffEW("CHl1R",2, 2) -0.076031 * getSMEFTCoeffEW("CHl3R",0, 0) -0.076031 * getSMEFTCoeffEW("CHl3R",1, 1) +0.010463 * getSMEFTCoeffEW("CHl3R",2, 2)  
            +0.000171 * getSMEFTCoeffEW("CHq1R",0, 0) +0.000171 * getSMEFTCoeffEW("CHq1R",1, 1) +0.082251 * getSMEFTCoeffEW("CHq3R",0, 0) +0.082251 * getSMEFTCoeffEW("CHq3R",1, 1)  
            -0.001014 * getSMEFTCoeffEW("CHq3R",2, 2) -0.000376 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) -0.034503 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.03437 * getSMEFTCoeffEW("CllR",0, 1, 1, 0)  
            -0.000751 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) -0.000376 * getSMEFTCoeffEW("CllR",1, 1, 1, 1) -0.000751 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) -0.000376 * getSMEFTCoeffEW("CllR",2, 2, 2, 2)  
            -0.001127 * getSMEFTCoeffEW("Cqq1R",0, 0, 0, 0) -0.002253 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) -0.012833 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0) -0.001127 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1)  
            -0.012833 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) -0.012983 * getSMEFTCoeffEW("Cqq3R",0, 0, 0, 0) -0.028219 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1) -0.033367 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2)  
            +0.002253 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0) +0.012833 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0) -0.012983 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1) -0.033367 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2)  
            +0.012833 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1) -0.004703 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.004703 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) +0.024198 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
            -0.004703 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0) -0.004703 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) +0.024198 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.004703 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0)  
            -0.004703 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1) -0.005561 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) ) * v2; 
    
    return ( GammaW_tree * (deltaMwd6() + 2.0 * delta_UgCC)
            + 2.0 * G0 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1) + getSMEFTCoeffEW("CHl3R", 2, 2) + Nc * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1))) * v2
            + cNLOd6 * deltaNLO );
}

◆ deltaGamma_Wff()

const double NPSMEFTd6General::deltaGamma_Wff	(	const Particle	fi,
		const Particle	fj
	)		const

virtual

The new physics contribution to the decay width of the $W$ boson into a given fermion pair, $\delta \Gamma_Z^{f}$.

Parameters

[in]	fi	a lepton or quark
[in]	fj	a lepton or quark

Returns: $\delta \Gamma_W^{ff}$ in GeV

Reimplemented from NPbase.

Definition at line 15625 of file NPSMEFTd6General.cpp.

                                                                                        {
    double G0 = GF * pow(Mz*cW_tree, 3.0) / 6.0 / sqrt(2.0) / M_PI;
    double deltaGamma_Wij;
    double GammaW_tree;
    double CHF3ij;
    
    double deltaNLO;
    
    if (fj.getIndex() - fi.getIndex() == 1)
        //CHF3ij = CHF3_diag(fi);
        CHF3ij = CHF3CC_diag(fi).real();
    else
        CHF3ij = 0.;
    
    //if (fi.is("QUARK")) {
    if ( fi.getIndex() > 5 ) {
        GammaW_tree = Nc * G0;
    } else {
        GammaW_tree = G0;
    }
 
    //    deltaGamma_Wij = - 3.0 * GammaW_tree / 4.0 / (cW2_tree - sW2_tree)
    //            *(4.0 * sW_tree * cW_tree * getSMEFTCoeffEW("CHWB") * v2_over_LambdaNP2
    //            + cW2_tree * getSMEFTCoeffEW("CHD") * v2_over_LambdaNP2
    //            + 2.0 * (1.0 + cW2_tree) / 3.0 * delta_GF);
 
    //    deltaGamma_Wij = deltaGamma_Wij + 2.0 * GammaW_tree * CHF3ij * v2_over_LambdaNP2;
 
    deltaGamma_Wij = deltaMwd6() + 2.0 * delta_UgCC;
 
    deltaGamma_Wij = GammaW_tree * (deltaGamma_Wij + 2.0 * CHF3ij * v2);
 
    // Finite NLO corrections    
    // NLO only for leptonic decays for lepton universality tests. 
    // This function is only used for the calculation of BR, RWc and universality tests. W width includes total NLO corrections separately.
    switch(fj.getIndex()){
    //if (fj.is("ELECTRON")) {
        case 1:
            deltaNLO = (-0.000127 * getSMEFTCoeffEW("CW")  -0.000016 * getSMEFTCoeffEW("CHbox")  +0.00211 * getSMEFTCoeffEW("CHD")  -0.000128 * getSMEFTCoeffEW("CHW")   
            +0.004837 * getSMEFTCoeffEW("CHWB")  +0.000453 * getSMEFTCoeffEW("CuWR",2, 2) -0.000403 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000232 * getSMEFTCoeffEW("CHl1R",1, 1)  
            +0.003165 * getSMEFTCoeffEW("CHl3R",0, 0) -0.003623 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000408 * getSMEFTCoeffEW("CHl3R",2, 2) +0.001225 * getSMEFTCoeffEW("CHq3R",0, 0)  
            +0.001225 * getSMEFTCoeffEW("CHq3R",1, 1) -0.000113 * getSMEFTCoeffEW("CHq3R",2, 2) -0.000376 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) -0.003834 * getSMEFTCoeffEW("CllR",0, 0, 1, 1)  
            -0.002052 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000376 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) -0.002352 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.002352 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1)  
            -0.002255 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) +0.003307 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) ) * v2;  
        break;
    //} else if (fj.is("MUON")) {
        case 3:
            deltaNLO = (-0.000127 * getSMEFTCoeffEW("CW")  -0.000016 * getSMEFTCoeffEW("CHbox")  +0.00211 * getSMEFTCoeffEW("CHD")  -0.000128 * getSMEFTCoeffEW("CHW")   
            +0.004837 * getSMEFTCoeffEW("CHWB")  +0.000453 * getSMEFTCoeffEW("CuWR",2, 2) -0.000232 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000403 * getSMEFTCoeffEW("CHl1R",1, 1)  
            -0.003623 * getSMEFTCoeffEW("CHl3R",0, 0) +0.003165 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000408 * getSMEFTCoeffEW("CHl3R",2, 2) +0.001225 * getSMEFTCoeffEW("CHq3R",0, 0)  
            +0.001225 * getSMEFTCoeffEW("CHq3R",1, 1) -0.000113 * getSMEFTCoeffEW("CHq3R",2, 2) -0.003834 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) -0.002052 * getSMEFTCoeffEW("CllR",0, 1, 1, 0)  
            -0.000376 * getSMEFTCoeffEW("CllR",1, 1, 1, 1) -0.000376 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) +0.003307 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.002352 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0)  
            -0.002352 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) -0.002255 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) ) * v2;  
        break;
    //} else if (fj.is("TAU")) {
        case 5:
            deltaNLO = (-0.000127 * getSMEFTCoeffEW("CW")  -0.000016 * getSMEFTCoeffEW("CHbox")  +0.00211 * getSMEFTCoeffEW("CHD")  -0.000128 * getSMEFTCoeffEW("CHW")   
            +0.004837 * getSMEFTCoeffEW("CHWB")  +0.000453 * getSMEFTCoeffEW("CuWR",2, 2) -0.000232 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000232 * getSMEFTCoeffEW("CHl1R",1, 1)  
            -0.000171 * getSMEFTCoeffEW("CHl1R",2, 2) -0.003623 * getSMEFTCoeffEW("CHl3R",0, 0) -0.003623 * getSMEFTCoeffEW("CHl3R",1, 1) +0.007196 * getSMEFTCoeffEW("CHl3R",2, 2)  
            +0.001225 * getSMEFTCoeffEW("CHq3R",0, 0) +0.001225 * getSMEFTCoeffEW("CHq3R",1, 1) -0.000113 * getSMEFTCoeffEW("CHq3R",2, 2) -0.003834 * getSMEFTCoeffEW("CllR",0, 0, 1, 1)  
            -0.001677 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000376 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) -0.000376 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) -0.000376 * getSMEFTCoeffEW("CllR",2, 2, 2, 2)  
            +0.003307 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) +0.003307 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.002352 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0) -0.002352 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1)  
            -0.005561 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) ) * v2; 
        break;
    //} else if (fi.is("UP")) {
        case 6:
            deltaNLO = (-0.000382 * getSMEFTCoeffEW("CW")  -0.000047 * getSMEFTCoeffEW("CHbox")  +0.00701 * getSMEFTCoeffEW("CHD")  -0.000384 * getSMEFTCoeffEW("CHW")   
            +0.015722 * getSMEFTCoeffEW("CHWB")  +0.001359 * getSMEFTCoeffEW("CuWR",2, 2) -0.000697 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000697 * getSMEFTCoeffEW("CHl1R",1, 1)  
            -0.035975 * getSMEFTCoeffEW("CHl3R",0, 0) -0.035975 * getSMEFTCoeffEW("CHl3R",1, 1) +0.001225 * getSMEFTCoeffEW("CHl3R",2, 2) +0.000171 * getSMEFTCoeffEW("CHq1R",0, 0)  
            +0.0749 * getSMEFTCoeffEW("CHq3R",0, 0) +0.003675 * getSMEFTCoeffEW("CHq3R",1, 1) -0.000338 * getSMEFTCoeffEW("CHq3R",2, 2) -0.011501 * getSMEFTCoeffEW("CllR",0, 0, 1, 1)  
            +0.020076 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.001127 * getSMEFTCoeffEW("Cqq1R",0, 0, 0, 0) -0.001127 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) -0.012833 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0)  
            -0.012983 * getSMEFTCoeffEW("Cqq3R",0, 0, 0, 0) -0.014109 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1) -0.033367 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2) +0.001127 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0)  
            +0.012833 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0) -0.002352 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) +0.00992 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.002352 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0)  
            +0.00992 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.002352 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0) ) * v2; 
        break;
    //} else if (fi.is("CHARM")) {
        case 8:
            deltaNLO = (-0.000382 * getSMEFTCoeffEW("CW")  -0.000047 * getSMEFTCoeffEW("CHbox")  +0.00701 * getSMEFTCoeffEW("CHD")  -0.000384 * getSMEFTCoeffEW("CHW")   
            +0.015722 * getSMEFTCoeffEW("CHWB")  +0.001359 * getSMEFTCoeffEW("CuWR",2, 2) -0.000697 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000697 * getSMEFTCoeffEW("CHl1R",1, 1)  
            -0.035975 * getSMEFTCoeffEW("CHl3R",0, 0) -0.035975 * getSMEFTCoeffEW("CHl3R",1, 1) +0.001225 * getSMEFTCoeffEW("CHl3R",2, 2) +0.000171 * getSMEFTCoeffEW("CHq1R",1, 1)  
            +0.003675 * getSMEFTCoeffEW("CHq3R",0, 0) +0.0749 * getSMEFTCoeffEW("CHq3R",1, 1) -0.000338 * getSMEFTCoeffEW("CHq3R",2, 2) -0.011501 * getSMEFTCoeffEW("CllR",0, 0, 1, 1)  
            +0.020076 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.001127 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) -0.001127 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1) -0.012833 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1)  
            -0.014109 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1) +0.001127 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0) -0.012983 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1) -0.033367 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2)  
            +0.012833 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1) -0.002352 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) +0.00992 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.002352 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1)  
            +0.00992 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.002352 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1) ) * v2; 
        break;   
    //} else {
        default:
            deltaNLO = 0.;
    }
    
    return deltaGamma_Wij + cNLOd6 * deltaNLO;
}

◆ deltaGamma_Z()

const double NPSMEFTd6General::deltaGamma_Z ( ) const

virtual

The new physics contribution to the total decay width of the $Z$ boson, $\delta \Gamma_Z$.

Returns: $\delta \Gamma_Z$ in GeV

Reimplemented from NPbase.

Definition at line 16042 of file NPSMEFTd6General.cpp.

{
    double deltaGamma_Z = 0.;
    bool nonZeroNP = false;
    
    double deltaNLO;
    
    double delGVl[6], delGAl[6], delGVq[6], delGAq[6];
    for (int p = 0; p < 6; ++p) {
        delGVl[p] = deltaGV_f(leptons[p]);
        delGAl[p] = deltaGA_f(leptons[p]);
        delGVq[p] = deltaGV_f(quarks[p]);
        delGAq[p] = deltaGA_f(quarks[p]);
        if (delGVl[p] != 0.0 || delGAl[p] != 0.0
                || delGVq[p] != 0.0 || delGAq[p] != 0.0)
            nonZeroNP = true;
    }
 
    if (nonZeroNP) {
        double gVf, gAf;
        double deltaGl[6], deltaGq[6];
        double delGammaZ = 0.0;
        for (int p = 0; p < 6; ++p) {
            gVf = trueSM.gV_f(leptons[p]).real();
            gAf = trueSM.gA_f(leptons[p]).real();
            deltaGl[p] = 2.0 * (gVf * delGVl[p] + gAf * delGAl[p]);
 
            gVf = trueSM.gV_f(quarks[p]).real();
            gAf = trueSM.gA_f(quarks[p]).real();
            deltaGq[p] = 2.0 * (gVf * delGVq[p] + gAf * delGAq[p]);
 
            delGammaZ += deltaGl[p] + 3.0 * deltaGq[p];
        }
 
        double alpha = trueSM.alphaMz();       
        double sW2_SM = trueSM.sW2();
        double cW2_SM = trueSM.cW2();
        deltaGamma_Z = alpha * Mz / 12.0 / sW2_SM / cW2_SM
                * delGammaZ;
    }
 
    // Finite NLO corrections    
    deltaNLO = (+0.002254 * getSMEFTCoeffEW("CW")  -0.001125 * getSMEFTCoeffEW("CHbox")  -0.05222 * getSMEFTCoeffEW("CHD")  +0.000053 * getSMEFTCoeffEW("CHB")   
            -0.000766 * getSMEFTCoeffEW("CHW")  +0.060315 * getSMEFTCoeffEW("CHWB")  -0.023483 * getSMEFTCoeffEW("CuWR",2, 2) +0.014583 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.014841 * getSMEFTCoeffEW("CHl1R",0, 0) -0.014841 * getSMEFTCoeffEW("CHl1R",1, 1) -0.012341 * getSMEFTCoeffEW("CHl1R",2, 2) -0.10303 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.10303 * getSMEFTCoeffEW("CHl3R",1, 1) +0.014177 * getSMEFTCoeffEW("CHl3R",2, 2) -0.011546 * getSMEFTCoeffEW("CHeR",0, 0) -0.011546 * getSMEFTCoeffEW("CHeR",1, 1)  
            -0.011546 * getSMEFTCoeffEW("CHeR",2, 2) +0.017864 * getSMEFTCoeffEW("CHq1R",0, 0) +0.017864 * getSMEFTCoeffEW("CHq1R",1, 1) +0.019278 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.099668 * getSMEFTCoeffEW("CHq3R",0, 0) +0.099668 * getSMEFTCoeffEW("CHq3R",1, 1) +0.024797 * getSMEFTCoeffEW("CHq3R",2, 2) +0.033884 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.033884 * getSMEFTCoeffEW("CHuR",1, 1) +0.01902 * getSMEFTCoeffEW("CHuR",2, 2) -0.016816 * getSMEFTCoeffEW("CHdR",0, 0) -0.016816 * getSMEFTCoeffEW("CHdR",1, 1)  
            -0.016816 * getSMEFTCoeffEW("CHdR",2, 2) -0.000462 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) -0.041502 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) -0.000256 * getSMEFTCoeffEW("CllR",0, 0, 2, 2)  
            +0.055124 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000669 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) -0.000462 * getSMEFTCoeffEW("CllR",1, 1, 1, 1) -0.000256 * getSMEFTCoeffEW("CllR",1, 1, 2, 2)  
            -0.000669 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) -0.000462 * getSMEFTCoeffEW("CllR",2, 2, 2, 2) -0.001063 * getSMEFTCoeffEW("Cqq1R",0, 0, 0, 0) -0.000256 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1)  
            +0.004926 * getSMEFTCoeffEW("Cqq1R",0, 0, 2, 2) -0.001871 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) -0.019296 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0) -0.001063 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1)  
            +0.004926 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2) -0.019296 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) +0.031756 * getSMEFTCoeffEW("Cqq1R",2, 2, 2, 2) -0.013001 * getSMEFTCoeffEW("Cqq3R",0, 0, 0, 0)  
            -0.027804 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1) -0.081823 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2) +0.001802 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0) +0.026622 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0)  
            -0.013001 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1) -0.081823 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) +0.026622 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1) +0.002863 * getSMEFTCoeffEW("Cqq3R",2, 2, 2, 2)  
            +0.000128 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) +0.000128 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) -0.002463 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) +0.000128 * getSMEFTCoeffEW("Clq1R",1, 1, 0, 0)  
            +0.000128 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1) -0.002463 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2) +0.000128 * getSMEFTCoeffEW("Clq1R",2, 2, 0, 0) +0.000128 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1)  
            -0.002463 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2) -0.004634 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.004634 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) +0.021939 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
            -0.004634 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0) -0.004634 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) +0.021939 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.004634 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0)  
            -0.004634 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1) -0.013637 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) -0.000179 * getSMEFTCoeffEW("CeeR",0, 0, 0, 0) -0.000358 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1)  
            -0.000358 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2) -0.000179 * getSMEFTCoeffEW("CeeR",1, 1, 1, 1) -0.000358 * getSMEFTCoeffEW("CeeR",1, 1, 2, 2) -0.000179 * getSMEFTCoeffEW("CeeR",2, 2, 2, 2)  
            -0.00058 * getSMEFTCoeffEW("CuuR",0, 0, 0, 0) -0.001023 * getSMEFTCoeffEW("CuuR",0, 0, 1, 1) -0.013282 * getSMEFTCoeffEW("CuuR",0, 0, 2, 2) -0.000136 * getSMEFTCoeffEW("CuuR",0, 1, 1, 0)  
            -0.008025 * getSMEFTCoeffEW("CuuR",0, 2, 2, 0) -0.00058 * getSMEFTCoeffEW("CuuR",1, 1, 1, 1) -0.013282 * getSMEFTCoeffEW("CuuR",1, 1, 2, 2) -0.008025 * getSMEFTCoeffEW("CuuR",1, 2, 2, 1)  
            -0.000145 * getSMEFTCoeffEW("CddR",0, 0, 0, 0) -0.000256 * getSMEFTCoeffEW("CddR",0, 0, 1, 1) -0.000256 * getSMEFTCoeffEW("CddR",0, 0, 2, 2) -0.000034 * getSMEFTCoeffEW("CddR",0, 1, 1, 0)  
            -0.000034 * getSMEFTCoeffEW("CddR",0, 2, 2, 0) -0.000145 * getSMEFTCoeffEW("CddR",1, 1, 1, 1) -0.000256 * getSMEFTCoeffEW("CddR",1, 1, 2, 2) -0.000034 * getSMEFTCoeffEW("CddR",1, 2, 2, 1)  
            -0.000145 * getSMEFTCoeffEW("CddR",2, 2, 2, 2) +0.000256 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0) +0.000256 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1) +0.003321 * getSMEFTCoeffEW("CeuR",0, 0, 2, 2)  
            +0.000256 * getSMEFTCoeffEW("CeuR",1, 1, 0, 0) +0.000256 * getSMEFTCoeffEW("CeuR",1, 1, 1, 1) +0.003321 * getSMEFTCoeffEW("CeuR",1, 1, 2, 2) +0.000256 * getSMEFTCoeffEW("CeuR",2, 2, 0, 0)  
            +0.000256 * getSMEFTCoeffEW("CeuR",2, 2, 1, 1) +0.003321 * getSMEFTCoeffEW("CeuR",2, 2, 2, 2) -0.000128 * getSMEFTCoeffEW("CedR",0, 0, 0, 0) -0.000128 * getSMEFTCoeffEW("CedR",0, 0, 1, 1)  
            -0.000128 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) -0.000128 * getSMEFTCoeffEW("CedR",1, 1, 0, 0) -0.000128 * getSMEFTCoeffEW("CedR",1, 1, 1, 1) -0.000128 * getSMEFTCoeffEW("CedR",1, 1, 2, 2)  
            -0.000128 * getSMEFTCoeffEW("CedR",2, 2, 0, 0) -0.000128 * getSMEFTCoeffEW("CedR",2, 2, 1, 1) -0.000128 * getSMEFTCoeffEW("CedR",2, 2, 2, 2) +0.000256 * getSMEFTCoeffEW("Cud1R",0, 0, 0, 0)  
            +0.000256 * getSMEFTCoeffEW("Cud1R",0, 0, 1, 1) +0.000256 * getSMEFTCoeffEW("Cud1R",0, 0, 2, 2) +0.000256 * getSMEFTCoeffEW("Cud1R",1, 1, 0, 0) +0.000256 * getSMEFTCoeffEW("Cud1R",1, 1, 1, 1)  
            +0.000256 * getSMEFTCoeffEW("Cud1R",1, 1, 2, 2) +0.003321 * getSMEFTCoeffEW("Cud1R",2, 2, 0, 0) +0.003321 * getSMEFTCoeffEW("Cud1R",2, 2, 1, 1) +0.003321 * getSMEFTCoeffEW("Cud1R",2, 2, 2, 2)  
            -0.000128 * getSMEFTCoeffEW("CleR",0, 0, 0, 0) -0.000128 * getSMEFTCoeffEW("CleR",0, 0, 1, 1) -0.000128 * getSMEFTCoeffEW("CleR",0, 0, 2, 2) -0.000128 * getSMEFTCoeffEW("CleR",1, 1, 0, 0)  
            -0.000128 * getSMEFTCoeffEW("CleR",1, 1, 1, 1) -0.000128 * getSMEFTCoeffEW("CleR",1, 1, 2, 2) -0.000128 * getSMEFTCoeffEW("CleR",2, 2, 0, 0) -0.000128 * getSMEFTCoeffEW("CleR",2, 2, 1, 1)  
            -0.000128 * getSMEFTCoeffEW("CleR",2, 2, 2, 2) +0.000256 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) +0.000256 * getSMEFTCoeffEW("CluR",0, 0, 1, 1) +0.003321 * getSMEFTCoeffEW("CluR",0, 0, 2, 2)  
            +0.000256 * getSMEFTCoeffEW("CluR",1, 1, 0, 0) +0.000256 * getSMEFTCoeffEW("CluR",1, 1, 1, 1) +0.003321 * getSMEFTCoeffEW("CluR",1, 1, 2, 2) +0.000256 * getSMEFTCoeffEW("CluR",2, 2, 0, 0)  
            +0.000256 * getSMEFTCoeffEW("CluR",2, 2, 1, 1) +0.003321 * getSMEFTCoeffEW("CluR",2, 2, 2, 2) -0.000128 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) -0.000128 * getSMEFTCoeffEW("CldR",0, 0, 1, 1)  
            -0.000128 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) -0.000128 * getSMEFTCoeffEW("CldR",1, 1, 0, 0) -0.000128 * getSMEFTCoeffEW("CldR",1, 1, 1, 1) -0.000128 * getSMEFTCoeffEW("CldR",1, 1, 2, 2)  
            -0.000128 * getSMEFTCoeffEW("CldR",2, 2, 0, 0) -0.000128 * getSMEFTCoeffEW("CldR",2, 2, 1, 1) -0.000128 * getSMEFTCoeffEW("CldR",2, 2, 2, 2) +0.000128 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0)  
            +0.000128 * getSMEFTCoeffEW("CqeR",0, 0, 1, 1) +0.000128 * getSMEFTCoeffEW("CqeR",0, 0, 2, 2) +0.000128 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0) +0.000128 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1)  
            +0.000128 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) -0.002463 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0) -0.002463 * getSMEFTCoeffEW("CqeR",2, 2, 1, 1) -0.002463 * getSMEFTCoeffEW("CqeR",2, 2, 2, 2)  
            -0.000256 * getSMEFTCoeffEW("Cqu1R",0, 0, 0, 0) -0.000256 * getSMEFTCoeffEW("Cqu1R",0, 0, 1, 1) -0.003321 * getSMEFTCoeffEW("Cqu1R",0, 0, 2, 2) -0.000256 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0)  
            -0.000256 * getSMEFTCoeffEW("Cqu1R",1, 1, 1, 1) -0.003321 * getSMEFTCoeffEW("Cqu1R",1, 1, 2, 2) +0.004926 * getSMEFTCoeffEW("Cqu1R",2, 2, 0, 0) +0.004926 * getSMEFTCoeffEW("Cqu1R",2, 2, 1, 1)  
            -0.01897 * getSMEFTCoeffEW("Cqu1R",2, 2, 2, 2) +0.000128 * getSMEFTCoeffEW("Cqd1R",0, 0, 0, 0) +0.000128 * getSMEFTCoeffEW("Cqd1R",0, 0, 1, 1) +0.000128 * getSMEFTCoeffEW("Cqd1R",0, 0, 2, 2)  
            +0.000128 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0) +0.000128 * getSMEFTCoeffEW("Cqd1R",1, 1, 1, 1) +0.000128 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) -0.002463 * getSMEFTCoeffEW("Cqd1R",2, 2, 0, 0)  
            -0.002463 * getSMEFTCoeffEW("Cqd1R",2, 2, 1, 1) -0.002463 * getSMEFTCoeffEW("Cqd1R",2, 2, 2, 2) ) * v2; 
 
    return deltaGamma_Z + cNLOd6 * deltaNLO;
}

◆ deltaGamma_Zf()

const double NPSMEFTd6General::deltaGamma_Zf ( const Particle f ) const

virtual

The new physics contribution to the decay width of the $Z$ boson into a given fermion pair, $\delta \Gamma_Z^{f}$.

Parameters

[in] f a lepton or quark

Returns: $\delta \Gamma_Z^{f}$ in GeV

Reimplemented from NPbase.

Definition at line 15768 of file NPSMEFTd6General.cpp.

{
    double deltaGamma_Zf = 0.;
    bool nonZeroNP = false;
 
    double delGVf = deltaGV_f(f);
    double delGAf = deltaGA_f(f);
    
    double gVf = trueSM.gV_f(f).real();
    double gAf = trueSM.gA_f(f).real(); 
    
    double Nf;
    
    double deltaNLO;
    
    //if (f.is("LEPTON")) {
    //    Nf = 1.0;
    //} else {
    //    Nf = 3.0;
    //}
    
    if ( f.getIndex() < 6 ) {
        Nf = 1.0;
    } else {
        Nf = 3.0;
    }
    
    double alpha = trueSM.alphaMz();
    double sW2_SM = trueSM.sW2();
    double cW2_SM = trueSM.cW2();
    
    if (delGVf != 0.0 || delGAf != 0.0)
            nonZeroNP = true;
 
    if (nonZeroNP) {
        double delGammaZf = 0.0;
        delGammaZf = 2.0 * Nf * (gVf * delGVf + gAf * delGAf);
        
        deltaGamma_Zf = alpha * Mz / 12.0 / sW2_SM / cW2_SM * delGammaZf;
    }
 
    // Finite NLO corrections    
    // NLO only for leptonic decays for lepton universality tests . 
    // This function is only used for the calculation of corrections to BR and test of universality. Z width includes total NLO corrections separately.
    switch(f.getIndex()){
    //if (f.is("NEUTRINO_1")) {
        case 0:
            deltaNLO = (-0.000125 * getSMEFTCoeffEW("CW")  -0.000183 * getSMEFTCoeffEW("CHbox")  -0.005003 * getSMEFTCoeffEW("CHD")  -0.000033 * getSMEFTCoeffEW("CHB")   
            -0.000115 * getSMEFTCoeffEW("CHW")  +0.000882 * getSMEFTCoeffEW("CHWB")  +0.000081 * getSMEFTCoeffEW("CuWR",2, 2) -0.000044 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.012448 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000256 * getSMEFTCoeffEW("CHl1R",1, 1) -0.000086 * getSMEFTCoeffEW("CHl1R",2, 2) +0.002853 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.007785 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000298 * getSMEFTCoeffEW("CHl3R",2, 2) -0.000086 * getSMEFTCoeffEW("CHeR",0, 0) -0.000086 * getSMEFTCoeffEW("CHeR",1, 1)  
            -0.000086 * getSMEFTCoeffEW("CHeR",2, 2) +0.000086 * getSMEFTCoeffEW("CHq1R",0, 0) +0.000086 * getSMEFTCoeffEW("CHq1R",1, 1) -0.00743 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.000895 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000895 * getSMEFTCoeffEW("CHq3R",1, 1) +0.003579 * getSMEFTCoeffEW("CHq3R",2, 2) +0.000172 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.000172 * getSMEFTCoeffEW("CHuR",1, 1) +0.007935 * getSMEFTCoeffEW("CHuR",2, 2) -0.000086 * getSMEFTCoeffEW("CHdR",0, 0) -0.000086 * getSMEFTCoeffEW("CHdR",1, 1)  
            -0.000086 * getSMEFTCoeffEW("CHdR",2, 2) -0.000542 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) -0.003087 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) -0.000286 * getSMEFTCoeffEW("CllR",0, 0, 2, 2)  
            +0.003656 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000256 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) +0.000143 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) +0.000143 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1)  
            -0.006328 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) -0.001492 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.001492 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) -0.005547 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
            +0.002416 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.000143 * getSMEFTCoeffEW("CleR",0, 0, 0, 0) -0.000143 * getSMEFTCoeffEW("CleR",0, 0, 1, 1) -0.000143 * getSMEFTCoeffEW("CleR",0, 0, 2, 2)  
            +0.000286 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) +0.000286 * getSMEFTCoeffEW("CluR",0, 0, 1, 1) +0.00743 * getSMEFTCoeffEW("CluR",0, 0, 2, 2) -0.000143 * getSMEFTCoeffEW("CldR",0, 0, 0, 0)  
            -0.000143 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) -0.000143 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) ) * v2;              
        break;            
    //if (f.is("ELECTRON")) {
        case 1:
            deltaNLO = (+0.000102 * getSMEFTCoeffEW("CW")  -0.000051 * getSMEFTCoeffEW("CHbox")  -0.010075 * getSMEFTCoeffEW("CHD")  -0.000003 * getSMEFTCoeffEW("CHB")   
            -0.000034 * getSMEFTCoeffEW("CHW")  -0.008133 * getSMEFTCoeffEW("CHWB")  -0.000273 * getSMEFTCoeffEW("CuWR",2, 2) +0.000422 * getSMEFTCoeffEW("CuBR",2, 2)  
            +0.000112 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000106 * getSMEFTCoeffEW("CHl1R",1, 1) -0.00002 * getSMEFTCoeffEW("CHl1R",2, 2) -0.003345 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.002441 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000152 * getSMEFTCoeffEW("CHl3R",2, 2) -0.011199 * getSMEFTCoeffEW("CHeR",0, 0) -0.00002 * getSMEFTCoeffEW("CHeR",1, 1)  
            -0.00002 * getSMEFTCoeffEW("CHeR",2, 2) +0.00002 * getSMEFTCoeffEW("CHq1R",0, 0) +0.00002 * getSMEFTCoeffEW("CHq1R",1, 1) -0.001728 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.000456 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000456 * getSMEFTCoeffEW("CHq3R",1, 1) +0.000535 * getSMEFTCoeffEW("CHq3R",2, 2) +0.00004 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.00004 * getSMEFTCoeffEW("CHuR",1, 1) +0.001527 * getSMEFTCoeffEW("CHuR",2, 2) -0.00002 * getSMEFTCoeffEW("CHdR",0, 0) -0.00002 * getSMEFTCoeffEW("CHdR",1, 1)  
            -0.00002 * getSMEFTCoeffEW("CHdR",2, 2) +0.00008 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) -0.001258 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.000158 * getSMEFTCoeffEW("CllR",0, 0, 2, 2)  
            +0.000406 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000078 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) -0.000079 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) -0.000079 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1)  
            +0.0035 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) -0.000825 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.000825 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) -0.003183 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
            +0.001222 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.000179 * getSMEFTCoeffEW("CeeR",0, 0, 0, 0) -0.000179 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1) -0.000179 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2)  
            +0.000128 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0) +0.000128 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1) +0.003321 * getSMEFTCoeffEW("CeuR",0, 0, 2, 2) -0.000064 * getSMEFTCoeffEW("CedR",0, 0, 0, 0)  
            -0.000064 * getSMEFTCoeffEW("CedR",0, 0, 1, 1) -0.000064 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) +0.000015 * getSMEFTCoeffEW("CleR",0, 0, 0, 0) +0.000079 * getSMEFTCoeffEW("CleR",0, 0, 1, 1)  
            +0.000079 * getSMEFTCoeffEW("CleR",0, 0, 2, 2) -0.000064 * getSMEFTCoeffEW("CleR",1, 1, 0, 0) -0.000064 * getSMEFTCoeffEW("CleR",2, 2, 0, 0) -0.000158 * getSMEFTCoeffEW("CluR",0, 0, 0, 0)  
            -0.000158 * getSMEFTCoeffEW("CluR",0, 0, 1, 1) -0.004109 * getSMEFTCoeffEW("CluR",0, 0, 2, 2) +0.000079 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) +0.000079 * getSMEFTCoeffEW("CldR",0, 0, 1, 1)  
            +0.000079 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) +0.000064 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0) +0.000064 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0) -0.002828 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0) ) * v2; 
        break;
    //if (f.is("NEUTRINO_2")) {
        case 2:
            deltaNLO = (-0.000125 * getSMEFTCoeffEW("CW")  -0.000183 * getSMEFTCoeffEW("CHbox")  -0.005003 * getSMEFTCoeffEW("CHD")  -0.000033 * getSMEFTCoeffEW("CHB")   
            -0.000115 * getSMEFTCoeffEW("CHW")  +0.000882 * getSMEFTCoeffEW("CHWB")  +0.000081 * getSMEFTCoeffEW("CuWR",2, 2) -0.000044 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.000256 * getSMEFTCoeffEW("CHl1R",0, 0) -0.012448 * getSMEFTCoeffEW("CHl1R",1, 1) -0.000086 * getSMEFTCoeffEW("CHl1R",2, 2) -0.007785 * getSMEFTCoeffEW("CHl3R",0, 0)  
            +0.002853 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000298 * getSMEFTCoeffEW("CHl3R",2, 2) -0.000086 * getSMEFTCoeffEW("CHeR",0, 0) -0.000086 * getSMEFTCoeffEW("CHeR",1, 1)  
            -0.000086 * getSMEFTCoeffEW("CHeR",2, 2) +0.000086 * getSMEFTCoeffEW("CHq1R",0, 0) +0.000086 * getSMEFTCoeffEW("CHq1R",1, 1) -0.00743 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.000895 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000895 * getSMEFTCoeffEW("CHq3R",1, 1) +0.003579 * getSMEFTCoeffEW("CHq3R",2, 2) +0.000172 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.000172 * getSMEFTCoeffEW("CHuR",1, 1) +0.007935 * getSMEFTCoeffEW("CHuR",2, 2) -0.000086 * getSMEFTCoeffEW("CHdR",0, 0) -0.000086 * getSMEFTCoeffEW("CHdR",1, 1)  
            -0.000086 * getSMEFTCoeffEW("CHdR",2, 2) -0.003087 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.003656 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000542 * getSMEFTCoeffEW("CllR",1, 1, 1, 1)  
            -0.000286 * getSMEFTCoeffEW("CllR",1, 1, 2, 2) -0.000256 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) +0.000143 * getSMEFTCoeffEW("Clq1R",1, 1, 0, 0) +0.000143 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1)  
            -0.006328 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2) +0.002416 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.001492 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0) -0.001492 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1)  
            -0.005547 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.000143 * getSMEFTCoeffEW("CleR",1, 1, 0, 0) -0.000143 * getSMEFTCoeffEW("CleR",1, 1, 1, 1) -0.000143 * getSMEFTCoeffEW("CleR",1, 1, 2, 2)  
            +0.000286 * getSMEFTCoeffEW("CluR",1, 1, 0, 0) +0.000286 * getSMEFTCoeffEW("CluR",1, 1, 1, 1) +0.00743 * getSMEFTCoeffEW("CluR",1, 1, 2, 2) -0.000143 * getSMEFTCoeffEW("CldR",1, 1, 0, 0)  
            -0.000143 * getSMEFTCoeffEW("CldR",1, 1, 1, 1) -0.000143 * getSMEFTCoeffEW("CldR",1, 1, 2, 2) ) * v2; 
        break;        
    //} else if (f.is("MUON")) {
        case 3:
            deltaNLO = (+0.000102 * getSMEFTCoeffEW("CW")  -0.000051 * getSMEFTCoeffEW("CHbox")  -0.010075 * getSMEFTCoeffEW("CHD")  -0.000003 * getSMEFTCoeffEW("CHB")   
            -0.000034 * getSMEFTCoeffEW("CHW")  -0.008133 * getSMEFTCoeffEW("CHWB")  -0.000273 * getSMEFTCoeffEW("CuWR",2, 2) +0.000422 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.000106 * getSMEFTCoeffEW("CHl1R",0, 0) +0.000112 * getSMEFTCoeffEW("CHl1R",1, 1) -0.00002 * getSMEFTCoeffEW("CHl1R",2, 2) -0.002441 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.003345 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000152 * getSMEFTCoeffEW("CHl3R",2, 2) -0.00002 * getSMEFTCoeffEW("CHeR",0, 0) -0.011199 * getSMEFTCoeffEW("CHeR",1, 1)  
            -0.00002 * getSMEFTCoeffEW("CHeR",2, 2) +0.00002 * getSMEFTCoeffEW("CHq1R",0, 0) +0.00002 * getSMEFTCoeffEW("CHq1R",1, 1) -0.001728 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.000456 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000456 * getSMEFTCoeffEW("CHq3R",1, 1) +0.000535 * getSMEFTCoeffEW("CHq3R",2, 2) +0.00004 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.00004 * getSMEFTCoeffEW("CHuR",1, 1) +0.001527 * getSMEFTCoeffEW("CHuR",2, 2) -0.00002 * getSMEFTCoeffEW("CHdR",0, 0) -0.00002 * getSMEFTCoeffEW("CHdR",1, 1)  
            -0.00002 * getSMEFTCoeffEW("CHdR",2, 2) -0.001258 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.000406 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) +0.00008 * getSMEFTCoeffEW("CllR",1, 1, 1, 1)  
            +0.000158 * getSMEFTCoeffEW("CllR",1, 1, 2, 2) -0.000078 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) -0.000079 * getSMEFTCoeffEW("Clq1R",1, 1, 0, 0) -0.000079 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1)  
            +0.0035 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2) +0.001222 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.000825 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0) -0.000825 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1)  
            -0.003183 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.000179 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1) -0.000179 * getSMEFTCoeffEW("CeeR",1, 1, 1, 1) -0.000179 * getSMEFTCoeffEW("CeeR",1, 1, 2, 2)  
            +0.000128 * getSMEFTCoeffEW("CeuR",1, 1, 0, 0) +0.000128 * getSMEFTCoeffEW("CeuR",1, 1, 1, 1) +0.003321 * getSMEFTCoeffEW("CeuR",1, 1, 2, 2) -0.000064 * getSMEFTCoeffEW("CedR",1, 1, 0, 0)  
            -0.000064 * getSMEFTCoeffEW("CedR",1, 1, 1, 1) -0.000064 * getSMEFTCoeffEW("CedR",1, 1, 2, 2) -0.000064 * getSMEFTCoeffEW("CleR",0, 0, 1, 1) +0.000079 * getSMEFTCoeffEW("CleR",1, 1, 0, 0)  
            +0.000015 * getSMEFTCoeffEW("CleR",1, 1, 1, 1) +0.000079 * getSMEFTCoeffEW("CleR",1, 1, 2, 2) -0.000064 * getSMEFTCoeffEW("CleR",2, 2, 1, 1) -0.000158 * getSMEFTCoeffEW("CluR",1, 1, 0, 0)  
            -0.000158 * getSMEFTCoeffEW("CluR",1, 1, 1, 1) -0.004109 * getSMEFTCoeffEW("CluR",1, 1, 2, 2) +0.000079 * getSMEFTCoeffEW("CldR",1, 1, 0, 0) +0.000079 * getSMEFTCoeffEW("CldR",1, 1, 1, 1)  
            +0.000079 * getSMEFTCoeffEW("CldR",1, 1, 2, 2) +0.000064 * getSMEFTCoeffEW("CqeR",0, 0, 1, 1) +0.000064 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1) -0.002828 * getSMEFTCoeffEW("CqeR",2, 2, 1, 1) ) * v2;  
        break;
    //if (f.is("NEUTRINO_3")) {
        case 4:
            deltaNLO = (-0.000125 * getSMEFTCoeffEW("CW")  -0.000183 * getSMEFTCoeffEW("CHbox")  -0.005003 * getSMEFTCoeffEW("CHD")  -0.000033 * getSMEFTCoeffEW("CHB")   
            -0.000115 * getSMEFTCoeffEW("CHW")  +0.000882 * getSMEFTCoeffEW("CHWB")  +0.000081 * getSMEFTCoeffEW("CuWR",2, 2) -0.000044 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.000256 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000256 * getSMEFTCoeffEW("CHl1R",1, 1) -0.012278 * getSMEFTCoeffEW("CHl1R",2, 2) -0.007785 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.007785 * getSMEFTCoeffEW("CHl3R",1, 1) +0.010936 * getSMEFTCoeffEW("CHl3R",2, 2) -0.000086 * getSMEFTCoeffEW("CHeR",0, 0) -0.000086 * getSMEFTCoeffEW("CHeR",1, 1)  
            -0.000086 * getSMEFTCoeffEW("CHeR",2, 2) +0.000086 * getSMEFTCoeffEW("CHq1R",0, 0) +0.000086 * getSMEFTCoeffEW("CHq1R",1, 1) -0.00743 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.000895 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000895 * getSMEFTCoeffEW("CHq3R",1, 1) +0.003579 * getSMEFTCoeffEW("CHq3R",2, 2) +0.000172 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.000172 * getSMEFTCoeffEW("CHuR",1, 1) +0.007935 * getSMEFTCoeffEW("CHuR",2, 2) -0.000086 * getSMEFTCoeffEW("CHdR",0, 0) -0.000086 * getSMEFTCoeffEW("CHdR",1, 1)  
            -0.000086 * getSMEFTCoeffEW("CHdR",2, 2) -0.002801 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) -0.000286 * getSMEFTCoeffEW("CllR",0, 0, 2, 2) +0.003913 * getSMEFTCoeffEW("CllR",0, 1, 1, 0)  
            -0.000256 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) -0.000286 * getSMEFTCoeffEW("CllR",1, 1, 2, 2) -0.000256 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) -0.000542 * getSMEFTCoeffEW("CllR",2, 2, 2, 2)  
            +0.000143 * getSMEFTCoeffEW("Clq1R",2, 2, 0, 0) +0.000143 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1) -0.006328 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2) +0.002416 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
            +0.002416 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.001492 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0) -0.001492 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1) -0.007963 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2)  
            -0.000143 * getSMEFTCoeffEW("CleR",2, 2, 0, 0) -0.000143 * getSMEFTCoeffEW("CleR",2, 2, 1, 1) -0.000143 * getSMEFTCoeffEW("CleR",2, 2, 2, 2) +0.000286 * getSMEFTCoeffEW("CluR",2, 2, 0, 0)  
            +0.000286 * getSMEFTCoeffEW("CluR",2, 2, 1, 1) +0.00743 * getSMEFTCoeffEW("CluR",2, 2, 2, 2) -0.000143 * getSMEFTCoeffEW("CldR",2, 2, 0, 0) -0.000143 * getSMEFTCoeffEW("CldR",2, 2, 1, 1)  
            -0.000143 * getSMEFTCoeffEW("CldR",2, 2, 2, 2) ) * v2; 
        break;
    //} else if (f.is("TAU")) {
        case 5:
            deltaNLO = (+0.000102 * getSMEFTCoeffEW("CW")  -0.000051 * getSMEFTCoeffEW("CHbox")  -0.010075 * getSMEFTCoeffEW("CHD")  -0.000003 * getSMEFTCoeffEW("CHB")   
            -0.000034 * getSMEFTCoeffEW("CHW")  -0.008133 * getSMEFTCoeffEW("CHWB")  -0.000273 * getSMEFTCoeffEW("CuWR",2, 2) +0.000422 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.000106 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000106 * getSMEFTCoeffEW("CHl1R",1, 1) +0.000198 * getSMEFTCoeffEW("CHl1R",2, 2) -0.002441 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.002441 * getSMEFTCoeffEW("CHl3R",1, 1) -0.000751 * getSMEFTCoeffEW("CHl3R",2, 2) -0.00002 * getSMEFTCoeffEW("CHeR",0, 0) -0.00002 * getSMEFTCoeffEW("CHeR",1, 1)  
            -0.011199 * getSMEFTCoeffEW("CHeR",2, 2) +0.00002 * getSMEFTCoeffEW("CHq1R",0, 0) +0.00002 * getSMEFTCoeffEW("CHq1R",1, 1) -0.001728 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.000456 * getSMEFTCoeffEW("CHq3R",0, 0) +0.000456 * getSMEFTCoeffEW("CHq3R",1, 1) +0.000535 * getSMEFTCoeffEW("CHq3R",2, 2) +0.00004 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.00004 * getSMEFTCoeffEW("CHuR",1, 1) +0.001527 * getSMEFTCoeffEW("CHuR",2, 2) -0.00002 * getSMEFTCoeffEW("CHdR",0, 0) -0.00002 * getSMEFTCoeffEW("CHdR",1, 1)  
            -0.00002 * getSMEFTCoeffEW("CHdR",2, 2) -0.001416 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.000158 * getSMEFTCoeffEW("CllR",0, 0, 2, 2) +0.000484 * getSMEFTCoeffEW("CllR",0, 1, 1, 0)  
            -0.000078 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) +0.000158 * getSMEFTCoeffEW("CllR",1, 1, 2, 2) -0.000078 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) +0.00008 * getSMEFTCoeffEW("CllR",2, 2, 2, 2)  
            -0.000079 * getSMEFTCoeffEW("Clq1R",2, 2, 0, 0) -0.000079 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1) +0.0035 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2) +0.001222 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
            +0.001222 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.000825 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0) -0.000825 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1) -0.004404 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2)  
            -0.000179 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2) -0.000179 * getSMEFTCoeffEW("CeeR",1, 1, 2, 2) -0.000179 * getSMEFTCoeffEW("CeeR",2, 2, 2, 2) +0.000128 * getSMEFTCoeffEW("CeuR",2, 2, 0, 0)  
            +0.000128 * getSMEFTCoeffEW("CeuR",2, 2, 1, 1) +0.003321 * getSMEFTCoeffEW("CeuR",2, 2, 2, 2) -0.000064 * getSMEFTCoeffEW("CedR",2, 2, 0, 0) -0.000064 * getSMEFTCoeffEW("CedR",2, 2, 1, 1)  
            -0.000064 * getSMEFTCoeffEW("CedR",2, 2, 2, 2) -0.000064 * getSMEFTCoeffEW("CleR",0, 0, 2, 2) -0.000064 * getSMEFTCoeffEW("CleR",1, 1, 2, 2) +0.000079 * getSMEFTCoeffEW("CleR",2, 2, 0, 0)  
            +0.000079 * getSMEFTCoeffEW("CleR",2, 2, 1, 1) +0.000015 * getSMEFTCoeffEW("CleR",2, 2, 2, 2) -0.000158 * getSMEFTCoeffEW("CluR",2, 2, 0, 0) -0.000158 * getSMEFTCoeffEW("CluR",2, 2, 1, 1)  
            -0.004109 * getSMEFTCoeffEW("CluR",2, 2, 2, 2) +0.000079 * getSMEFTCoeffEW("CldR",2, 2, 0, 0) +0.000079 * getSMEFTCoeffEW("CldR",2, 2, 1, 1) +0.000079 * getSMEFTCoeffEW("CldR",2, 2, 2, 2)  
            +0.000064 * getSMEFTCoeffEW("CqeR",0, 0, 2, 2) +0.000064 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) -0.002828 * getSMEFTCoeffEW("CqeR",2, 2, 2, 2) ) * v2; 
        break;
    //if (f.is("UP")) {
        case 6:    
            deltaNLO = (+0.001041 * getSMEFTCoeffEW("CW")  -0.000005 * getSMEFTCoeffEW("CHbox")  -0.002874 * getSMEFTCoeffEW("CHD")  +0.00005 * getSMEFTCoeffEW("CHB")   
            -0.000015 * getSMEFTCoeffEW("CHW")  +0.012204 * getSMEFTCoeffEW("CHWB")  -0.002252 * getSMEFTCoeffEW("CuWR",2, 2) +0.003307 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.000266 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000266 * getSMEFTCoeffEW("CHl1R",1, 1) +0.00003 * getSMEFTCoeffEW("CHl1R",2, 2) -0.013774 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.013774 * getSMEFTCoeffEW("CHl3R",1, 1) +0.00053 * getSMEFTCoeffEW("CHl3R",2, 2) +0.00003 * getSMEFTCoeffEW("CHeR",0, 0) +0.00003 * getSMEFTCoeffEW("CHeR",1, 1)  
            +0.00003 * getSMEFTCoeffEW("CHeR",2, 2) -0.038605 * getSMEFTCoeffEW("CHq1R",0, 0) -0.00003 * getSMEFTCoeffEW("CHq1R",1, 1) +0.002478 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.03623 * getSMEFTCoeffEW("CHq3R",0, 0) +0.001591 * getSMEFTCoeffEW("CHq3R",1, 1) -0.003461 * getSMEFTCoeffEW("CHq3R",2, 2) +0.033092 * getSMEFTCoeffEW("CHuR",0, 0)  
            -0.00006 * getSMEFTCoeffEW("CHuR",1, 1) -0.00507 * getSMEFTCoeffEW("CHuR",2, 2) +0.00003 * getSMEFTCoeffEW("CHdR",0, 0) +0.00003 * getSMEFTCoeffEW("CHdR",1, 1)  
            +0.00003 * getSMEFTCoeffEW("CHdR",2, 2) -0.004888 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.007027 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) +0.000224 * getSMEFTCoeffEW("Cqq1R",0, 0, 0, 0)  
            +0.000603 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1) -0.026657 * getSMEFTCoeffEW("Cqq1R",0, 0, 2, 2) -0.000379 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) -0.018182 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0)  
            -0.005745 * getSMEFTCoeffEW("Cqq3R",0, 0, 0, 0) -0.006284 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1) -0.033544 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2) +0.00054 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0)  
            -0.017264 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0) -0.000301 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) -0.000301 * getSMEFTCoeffEW("Clq1R",1, 1, 0, 0) -0.000301 * getSMEFTCoeffEW("Clq1R",2, 2, 0, 0)  
            -0.001047 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) +0.004216 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.001047 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0) +0.004216 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2)  
            -0.001047 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0) -0.00058 * getSMEFTCoeffEW("CuuR",0, 0, 0, 0) -0.000512 * getSMEFTCoeffEW("CuuR",0, 0, 1, 1) -0.013282 * getSMEFTCoeffEW("CuuR",0, 0, 2, 2)  
            -0.000068 * getSMEFTCoeffEW("CuuR",0, 1, 1, 0) -0.008025 * getSMEFTCoeffEW("CuuR",0, 2, 2, 0) +0.000128 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0) +0.000128 * getSMEFTCoeffEW("CeuR",1, 1, 0, 0)  
            +0.000128 * getSMEFTCoeffEW("CeuR",2, 2, 0, 0) +0.000128 * getSMEFTCoeffEW("Cud1R",0, 0, 0, 0) +0.000128 * getSMEFTCoeffEW("Cud1R",0, 0, 1, 1) +0.000128 * getSMEFTCoeffEW("Cud1R",0, 0, 2, 2)  
            +0.000128 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) +0.000128 * getSMEFTCoeffEW("CluR",1, 1, 0, 0) +0.000128 * getSMEFTCoeffEW("CluR",2, 2, 0, 0) -0.000301 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0)  
            -0.000301 * getSMEFTCoeffEW("CqeR",0, 0, 1, 1) -0.000301 * getSMEFTCoeffEW("CqeR",0, 0, 2, 2) +0.000475 * getSMEFTCoeffEW("Cqu1R",0, 0, 0, 0) +0.000603 * getSMEFTCoeffEW("Cqu1R",0, 0, 1, 1)  
            +0.015649 * getSMEFTCoeffEW("Cqu1R",0, 0, 2, 2) -0.000128 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0) +0.005656 * getSMEFTCoeffEW("Cqu1R",2, 2, 0, 0) -0.000301 * getSMEFTCoeffEW("Cqd1R",0, 0, 0, 0)  
            -0.000301 * getSMEFTCoeffEW("Cqd1R",0, 0, 1, 1) -0.000301 * getSMEFTCoeffEW("Cqd1R",0, 0, 2, 2) ) * v2;  
        break;             
    //if (f.is("DOWN")) {
        case 7:
            deltaNLO = (+0.000814 * getSMEFTCoeffEW("CW")  -0.000137 * getSMEFTCoeffEW("CHbox")  -0.000388 * getSMEFTCoeffEW("CHD")  +0.00002 * getSMEFTCoeffEW("CHB")   
            -0.000096 * getSMEFTCoeffEW("CHW")  +0.020102 * getSMEFTCoeffEW("CHWB")  -0.001898 * getSMEFTCoeffEW("CuWR",2, 2) +0.002841 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.000416 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000416 * getSMEFTCoeffEW("CHl1R",1, 1) -0.000036 * getSMEFTCoeffEW("CHl1R",2, 2) -0.022179 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.022179 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000677 * getSMEFTCoeffEW("CHl3R",2, 2) -0.000036 * getSMEFTCoeffEW("CHeR",0, 0) -0.000036 * getSMEFTCoeffEW("CHeR",1, 1)  
            -0.000036 * getSMEFTCoeffEW("CHeR",2, 2) +0.056109 * getSMEFTCoeffEW("CHq1R",0, 0) +0.000036 * getSMEFTCoeffEW("CHq1R",1, 1) -0.003224 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.053732 * getSMEFTCoeffEW("CHq3R",0, 0) +0.00203 * getSMEFTCoeffEW("CHq3R",1, 1) -0.000416 * getSMEFTCoeffEW("CHq3R",2, 2) +0.000072 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.000072 * getSMEFTCoeffEW("CHuR",1, 1) +0.001337 * getSMEFTCoeffEW("CHuR",2, 2) -0.016486 * getSMEFTCoeffEW("CHdR",0, 0) -0.000036 * getSMEFTCoeffEW("CHdR",1, 1)  
            -0.000036 * getSMEFTCoeffEW("CHdR",2, 2) -0.006273 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.013516 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.001287 * getSMEFTCoeffEW("Cqq1R",0, 0, 0, 0)  
            -0.000731 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1) +0.032313 * getSMEFTCoeffEW("Cqq1R",0, 0, 2, 2) -0.000557 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) -0.000557 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0)  
            -0.007256 * getSMEFTCoeffEW("Cqq3R",0, 0, 0, 0) -0.007618 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1) -0.040661 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2) +0.000362 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0)  
            +0.043525 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0) +0.000365 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) +0.000365 * getSMEFTCoeffEW("Clq1R",1, 1, 0, 0) +0.000365 * getSMEFTCoeffEW("Clq1R",2, 2, 0, 0)  
            -0.00127 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) +0.00541 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.00127 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0) +0.00541 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2)  
            -0.00127 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0) -0.000145 * getSMEFTCoeffEW("CddR",0, 0, 0, 0) -0.000128 * getSMEFTCoeffEW("CddR",0, 0, 1, 1) -0.000128 * getSMEFTCoeffEW("CddR",0, 0, 2, 2)  
            -0.000017 * getSMEFTCoeffEW("CddR",0, 1, 1, 0) -0.000017 * getSMEFTCoeffEW("CddR",0, 2, 2, 0) -0.000064 * getSMEFTCoeffEW("CedR",0, 0, 0, 0) -0.000064 * getSMEFTCoeffEW("CedR",1, 1, 0, 0)  
            -0.000064 * getSMEFTCoeffEW("CedR",2, 2, 0, 0) +0.000128 * getSMEFTCoeffEW("Cud1R",0, 0, 0, 0) +0.000128 * getSMEFTCoeffEW("Cud1R",1, 1, 0, 0) +0.003321 * getSMEFTCoeffEW("Cud1R",2, 2, 0, 0)  
            -0.000064 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) -0.000064 * getSMEFTCoeffEW("CldR",1, 1, 0, 0) -0.000064 * getSMEFTCoeffEW("CldR",2, 2, 0, 0) +0.000365 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0)  
            +0.000365 * getSMEFTCoeffEW("CqeR",0, 0, 1, 1) +0.000365 * getSMEFTCoeffEW("CqeR",0, 0, 2, 2) -0.000731 * getSMEFTCoeffEW("Cqu1R",0, 0, 0, 0) -0.000731 * getSMEFTCoeffEW("Cqu1R",0, 0, 1, 1)  
            -0.01897 * getSMEFTCoeffEW("Cqu1R",0, 0, 2, 2) +0.000429 * getSMEFTCoeffEW("Cqd1R",0, 0, 0, 0) +0.000365 * getSMEFTCoeffEW("Cqd1R",0, 0, 1, 1) +0.000365 * getSMEFTCoeffEW("Cqd1R",0, 0, 2, 2)  
            +0.000064 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0) -0.002828 * getSMEFTCoeffEW("Cqd1R",2, 2, 0, 0) ) * v2; 
        break;          
    //} else if (f.is("CHARM")) {
        case 8:
            deltaNLO = (+0.001041 * getSMEFTCoeffEW("CW")  -0.000005 * getSMEFTCoeffEW("CHbox")  -0.002874 * getSMEFTCoeffEW("CHD")  +0.00005 * getSMEFTCoeffEW("CHB")   
            -0.000015 * getSMEFTCoeffEW("CHW")  +0.012204 * getSMEFTCoeffEW("CHWB")  -0.002252 * getSMEFTCoeffEW("CuWR",2, 2) +0.003307 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.000266 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000266 * getSMEFTCoeffEW("CHl1R",1, 1) +0.00003 * getSMEFTCoeffEW("CHl1R",2, 2) -0.013774 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.013774 * getSMEFTCoeffEW("CHl3R",1, 1) +0.00053 * getSMEFTCoeffEW("CHl3R",2, 2) +0.00003 * getSMEFTCoeffEW("CHeR",0, 0) +0.00003 * getSMEFTCoeffEW("CHeR",1, 1)  
            +0.00003 * getSMEFTCoeffEW("CHeR",2, 2) -0.00003 * getSMEFTCoeffEW("CHq1R",0, 0) -0.038605 * getSMEFTCoeffEW("CHq1R",1, 1) +0.002478 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.001591 * getSMEFTCoeffEW("CHq3R",0, 0) +0.03623 * getSMEFTCoeffEW("CHq3R",1, 1) -0.003461 * getSMEFTCoeffEW("CHq3R",2, 2) -0.00006 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.033092 * getSMEFTCoeffEW("CHuR",1, 1) -0.00507 * getSMEFTCoeffEW("CHuR",2, 2) +0.00003 * getSMEFTCoeffEW("CHdR",0, 0) +0.00003 * getSMEFTCoeffEW("CHdR",1, 1)  
            +0.00003 * getSMEFTCoeffEW("CHdR",2, 2) -0.004888 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.007027 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) +0.000603 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1)  
            -0.000379 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) +0.000224 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1) -0.026657 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2) -0.018182 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1)  
            -0.006284 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1) +0.00054 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0) -0.005745 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1) -0.033544 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2)  
            -0.017264 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1) -0.000301 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) -0.000301 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1) -0.000301 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1)  
            -0.001047 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) +0.004216 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.001047 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) +0.004216 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2)  
            -0.001047 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1) -0.000512 * getSMEFTCoeffEW("CuuR",0, 0, 1, 1) -0.000068 * getSMEFTCoeffEW("CuuR",0, 1, 1, 0) -0.00058 * getSMEFTCoeffEW("CuuR",1, 1, 1, 1)  
            -0.013282 * getSMEFTCoeffEW("CuuR",1, 1, 2, 2) -0.008025 * getSMEFTCoeffEW("CuuR",1, 2, 2, 1) +0.000128 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1) +0.000128 * getSMEFTCoeffEW("CeuR",1, 1, 1, 1)  
            +0.000128 * getSMEFTCoeffEW("CeuR",2, 2, 1, 1) +0.000128 * getSMEFTCoeffEW("Cud1R",1, 1, 0, 0) +0.000128 * getSMEFTCoeffEW("Cud1R",1, 1, 1, 1) +0.000128 * getSMEFTCoeffEW("Cud1R",1, 1, 2, 2)  
            +0.000128 * getSMEFTCoeffEW("CluR",0, 0, 1, 1) +0.000128 * getSMEFTCoeffEW("CluR",1, 1, 1, 1) +0.000128 * getSMEFTCoeffEW("CluR",2, 2, 1, 1) -0.000301 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0)  
            -0.000301 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1) -0.000301 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) -0.000128 * getSMEFTCoeffEW("Cqu1R",0, 0, 1, 1) +0.000603 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0)  
            +0.000475 * getSMEFTCoeffEW("Cqu1R",1, 1, 1, 1) +0.015649 * getSMEFTCoeffEW("Cqu1R",1, 1, 2, 2) +0.005656 * getSMEFTCoeffEW("Cqu1R",2, 2, 1, 1) -0.000301 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0)  
            -0.000301 * getSMEFTCoeffEW("Cqd1R",1, 1, 1, 1) -0.000301 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) ) * v2;             
        break;          
    //if (f.is("STRANGE")) {
        case 9:
            deltaNLO = (+0.000814 * getSMEFTCoeffEW("CW")  -0.000137 * getSMEFTCoeffEW("CHbox")  -0.000388 * getSMEFTCoeffEW("CHD")  +0.00002 * getSMEFTCoeffEW("CHB")   
            -0.000096 * getSMEFTCoeffEW("CHW")  +0.020102 * getSMEFTCoeffEW("CHWB")  -0.001898 * getSMEFTCoeffEW("CuWR",2, 2) +0.002841 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.000416 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000416 * getSMEFTCoeffEW("CHl1R",1, 1) -0.000036 * getSMEFTCoeffEW("CHl1R",2, 2) -0.022179 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.022179 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000677 * getSMEFTCoeffEW("CHl3R",2, 2) -0.000036 * getSMEFTCoeffEW("CHeR",0, 0) -0.000036 * getSMEFTCoeffEW("CHeR",1, 1)  
            -0.000036 * getSMEFTCoeffEW("CHeR",2, 2) +0.000036 * getSMEFTCoeffEW("CHq1R",0, 0) +0.056109 * getSMEFTCoeffEW("CHq1R",1, 1) -0.003224 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.00203 * getSMEFTCoeffEW("CHq3R",0, 0) +0.053732 * getSMEFTCoeffEW("CHq3R",1, 1) -0.000416 * getSMEFTCoeffEW("CHq3R",2, 2) +0.000072 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.000072 * getSMEFTCoeffEW("CHuR",1, 1) +0.001337 * getSMEFTCoeffEW("CHuR",2, 2) -0.000036 * getSMEFTCoeffEW("CHdR",0, 0) -0.016486 * getSMEFTCoeffEW("CHdR",1, 1)  
            -0.000036 * getSMEFTCoeffEW("CHdR",2, 2) -0.006273 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.013516 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000731 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1)  
            -0.000557 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) -0.001287 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1) +0.032313 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2) -0.000557 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1)  
            -0.007618 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1) +0.000362 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0) -0.007256 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1) -0.040661 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2)  
            +0.043525 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1) +0.000365 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) +0.000365 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1) +0.000365 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1)  
            -0.00127 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) +0.00541 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.00127 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) +0.00541 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2)  
            -0.00127 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1) -0.000128 * getSMEFTCoeffEW("CddR",0, 0, 1, 1) -0.000017 * getSMEFTCoeffEW("CddR",0, 1, 1, 0) -0.000145 * getSMEFTCoeffEW("CddR",1, 1, 1, 1)  
            -0.000128 * getSMEFTCoeffEW("CddR",1, 1, 2, 2) -0.000017 * getSMEFTCoeffEW("CddR",1, 2, 2, 1) -0.000064 * getSMEFTCoeffEW("CedR",0, 0, 1, 1) -0.000064 * getSMEFTCoeffEW("CedR",1, 1, 1, 1)  
            -0.000064 * getSMEFTCoeffEW("CedR",2, 2, 1, 1) +0.000128 * getSMEFTCoeffEW("Cud1R",0, 0, 1, 1) +0.000128 * getSMEFTCoeffEW("Cud1R",1, 1, 1, 1) +0.003321 * getSMEFTCoeffEW("Cud1R",2, 2, 1, 1)  
            -0.000064 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) -0.000064 * getSMEFTCoeffEW("CldR",1, 1, 1, 1) -0.000064 * getSMEFTCoeffEW("CldR",2, 2, 1, 1) +0.000365 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0)  
            +0.000365 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1) +0.000365 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) -0.000731 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0) -0.000731 * getSMEFTCoeffEW("Cqu1R",1, 1, 1, 1)  
            -0.01897 * getSMEFTCoeffEW("Cqu1R",1, 1, 2, 2) +0.000064 * getSMEFTCoeffEW("Cqd1R",0, 0, 1, 1) +0.000365 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0) +0.000429 * getSMEFTCoeffEW("Cqd1R",1, 1, 1, 1)  
            +0.000365 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) -0.002828 * getSMEFTCoeffEW("Cqd1R",2, 2, 1, 1) ) * v2; 
        break;        
    //} else if (f.is("BOTTOM")) {
        case 11:
            deltaNLO = (-0.001389 * getSMEFTCoeffEW("CW")  -0.000137 * getSMEFTCoeffEW("CHbox")  -0.000463 * getSMEFTCoeffEW("CHD")  +0.00002 * getSMEFTCoeffEW("CHB")   
            -0.000096 * getSMEFTCoeffEW("CHW")  +0.017458 * getSMEFTCoeffEW("CHWB")  -0.014607 * getSMEFTCoeffEW("CuWR",2, 2) +0.001149 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.000416 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000416 * getSMEFTCoeffEW("CHl1R",1, 1) -0.000036 * getSMEFTCoeffEW("CHl1R",2, 2) -0.010179 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.010179 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000677 * getSMEFTCoeffEW("CHl3R",2, 2) -0.000036 * getSMEFTCoeffEW("CHeR",0, 0) -0.000036 * getSMEFTCoeffEW("CHeR",1, 1)  
            -0.000036 * getSMEFTCoeffEW("CHeR",2, 2) +0.000036 * getSMEFTCoeffEW("CHq1R",0, 0) +0.000036 * getSMEFTCoeffEW("CHq1R",1, 1) +0.048246 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +0.00203 * getSMEFTCoeffEW("CHq3R",0, 0) +0.00203 * getSMEFTCoeffEW("CHq3R",1, 1) +0.020209 * getSMEFTCoeffEW("CHq3R",2, 2) +0.000072 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.000072 * getSMEFTCoeffEW("CHuR",1, 1) -0.0019 * getSMEFTCoeffEW("CHuR",2, 2) -0.000036 * getSMEFTCoeffEW("CHdR",0, 0) -0.000036 * getSMEFTCoeffEW("CHdR",1, 1)  
            -0.016486 * getSMEFTCoeffEW("CHdR",2, 2) -0.006273 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.001516 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.000731 * getSMEFTCoeffEW("Cqq1R",0, 0, 2, 2)  
            -0.000557 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0) -0.000731 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2) -0.000557 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) +0.031756 * getSMEFTCoeffEW("Cqq1R",2, 2, 2, 2)  
            -0.007618 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2) +0.000362 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0) -0.007618 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) +0.000362 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1)  
            +0.002863 * getSMEFTCoeffEW("Cqq3R",2, 2, 2, 2) +0.000365 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) +0.000365 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2) +0.000365 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2)  
            +0.004141 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) +0.004141 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.00127 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) -0.000128 * getSMEFTCoeffEW("CddR",0, 0, 2, 2)  
            -0.000017 * getSMEFTCoeffEW("CddR",0, 2, 2, 0) -0.000128 * getSMEFTCoeffEW("CddR",1, 1, 2, 2) -0.000017 * getSMEFTCoeffEW("CddR",1, 2, 2, 1) -0.000145 * getSMEFTCoeffEW("CddR",2, 2, 2, 2)  
            -0.000064 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) -0.000064 * getSMEFTCoeffEW("CedR",1, 1, 2, 2) -0.000064 * getSMEFTCoeffEW("CedR",2, 2, 2, 2) +0.000128 * getSMEFTCoeffEW("Cud1R",0, 0, 2, 2)  
            +0.000128 * getSMEFTCoeffEW("Cud1R",1, 1, 2, 2) +0.003321 * getSMEFTCoeffEW("Cud1R",2, 2, 2, 2) -0.000064 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) -0.000064 * getSMEFTCoeffEW("CldR",1, 1, 2, 2)  
            -0.000064 * getSMEFTCoeffEW("CldR",2, 2, 2, 2) +0.000365 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0) +0.000365 * getSMEFTCoeffEW("CqeR",2, 2, 1, 1) +0.000365 * getSMEFTCoeffEW("CqeR",2, 2, 2, 2)  
            -0.000731 * getSMEFTCoeffEW("Cqu1R",2, 2, 0, 0) -0.000731 * getSMEFTCoeffEW("Cqu1R",2, 2, 1, 1) -0.01897 * getSMEFTCoeffEW("Cqu1R",2, 2, 2, 2) +0.000064 * getSMEFTCoeffEW("Cqd1R",0, 0, 2, 2)  
            +0.000064 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) +0.000365 * getSMEFTCoeffEW("Cqd1R",2, 2, 0, 0) +0.000365 * getSMEFTCoeffEW("Cqd1R",2, 2, 1, 1) -0.002463 * getSMEFTCoeffEW("Cqd1R",2, 2, 2, 2) ) * v2; 
        break;
        default:
            deltaNLO = 0.;
    }
 
    return deltaGamma_Zf + cNLOd6 * deltaNLO;
}

◆ deltaGammaH2d2dRatio1()

const double NPSMEFTd6General::deltaGammaH2d2dRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2d2d)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2d2d)$/ $\Gamma(H\to 2d2d)_{\mathrm{SM}}$

Definition at line 30184 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121209. * getSMEFTCoeff("CHbox",muRG)
            - 109493. * getSMEFTCoeff("CHB",muRG)
            + 40559.6 * getSMEFTCoeff("CHW",muRG)
            + 43704.5 * (getSMEFTCoeff("CHq1R", 0, 0,muRG) + getSMEFTCoeff("CHq3R", 0, 0,muRG))
            + 43686.8 * (getSMEFTCoeff("CHq1R", 1, 1,muRG) + getSMEFTCoeff("CHq3R", 1, 1,muRG))
            + 48405. * (getSMEFTCoeff("CHq1R", 2, 2,muRG) + getSMEFTCoeff("CHq3R", 2, 2,muRG))
            - 7957.66 * getSMEFTCoeff("CHdR", 0, 0,muRG)
            - 7942.9 * getSMEFTCoeff("CHdR", 1, 1,muRG)
            - 8231.05 * getSMEFTCoeff("CHdR", 2, 2,muRG)
            - 55688.4 * getSMEFTCoeff("CHD",muRG)
            - 202420. * getSMEFTCoeff("CHWB",muRG)
            - 3.837 * delta_GF
            - 0.829 * deltaGzd6()
            );
            /*+ cWsch * (+28762.7 * getSMEFTCoeff("CHD")
            - 17533.6 * getSMEFTCoeff("CHWB")
            - 3. * delta_GF
            - 0.829 * deltaGzd6()
            ));*/
 
    //------ Old alpha scheme expression: End
    
    // AG: 
    dwidth += cWsch * (
            ((0.12095) * getSMEFTCoeff("CHbox",muRG)
            + (0.037885) * getSMEFTCoeff("CHW",muRG)
            + (-0.106698) * getSMEFTCoeff("CHB",muRG)
            + (0.029535) * getSMEFTCoeff("CHD",muRG)
            + (-0.0189127) * getSMEFTCoeff("CHWB",muRG)
            + (0.0435) * getSMEFTCoeff("CHq1R", 0, 0,muRG)
            + (0.043466) * getSMEFTCoeff("CHq1R", 1, 1,muRG)
            + (0.048137) * getSMEFTCoeff("CHq1R", 2, 2,muRG)
            + (0.0435) * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + (0.043466) * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + (0.048137) * getSMEFTCoeff("CHq3R", 2, 2,muRG)
            + (-0.007595) * getSMEFTCoeff("CHdR", 0, 0,muRG)
            + (-0.0075958) * getSMEFTCoeff("CHdR", 1, 1,muRG)
            + (-0.0078264) * getSMEFTCoeff("CHdR", 2, 2,muRG)
            + (-0.181359) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.181359) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.18142) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.826) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-9.78 * deltaMz()
            + 16.533 * deltaMh()
            - 0.55 * deltaaMZ()
            + 2.769 * deltaGmu()))
            + cWsch * (cHSM * (-13.39 * deltaMz()
            + 16.533 * deltaMh()
            + 2.228 * deltaGmu()
            + 2.601 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2d2dRatio2()

const double NPSMEFTd6General::deltaGammaH2d2dRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2d2d)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2d2d)$/ $\Gamma(H\to 2d2d)_{\mathrm{SM}}$

Definition at line 30255 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014652) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.013992) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.002345) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (-0.00049844) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.0024799) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.0013233) * pow(getSMEFTCoeffEW("CHq1R", 0, 0), 2.0)
                + (0.001324) * pow(getSMEFTCoeffEW("CHq1R", 1, 1), 2.0)
                + (0.0014861) * pow(getSMEFTCoeffEW("CHq1R", 2, 2), 2.0)
                + (0.0013233) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                + (0.001324) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                + (0.0014861) * pow(getSMEFTCoeffEW("CHq3R", 2, 2), 2.0)
                + (0.0013225) * pow(getSMEFTCoeffEW("CHdR", 0, 0), 2.0)
                + (0.0013239) * pow(getSMEFTCoeffEW("CHdR", 1, 1), 2.0)
                + (0.001485) * pow(getSMEFTCoeffEW("CHdR", 2, 2), 2.0)
                + (0.010987) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.010987) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.010987) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (0.0046) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.0129346) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (-0.0022905) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (0.0052759) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0052737) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0058395) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0052759) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0052737) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0058395) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.000921702) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.000921711) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.000948092) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.0146752) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0146752) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.014678) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0200055) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (-0.0067433) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.0310973) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (0.0006793) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0006842) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0007669) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0006793) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0006842) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0007669) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.0045821) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0045815) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0046) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.007028) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (0.017325) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (-0.00504565) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.00504237) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.00550773) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.00504565) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00504237) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00550773) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.0005692) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0005693) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.0005646) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.012951) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.012951) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0129346) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0023514) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (0.0022438) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0022464) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0022931) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0022438) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0022464) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0022931) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.000551) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.00055081) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.00072654) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.0035825) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0035825) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0035844) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00212189) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.00212373) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.00232565) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.00212189) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00212373) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00232565) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.0012709) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0012722) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.0013618) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.0022976) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0022976) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0022905) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00016) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.000192) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0026472) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.00015973) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.00019157) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.0052765) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0052765) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0052759) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000191) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.00015973) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0026472) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.00019165) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.00527248) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00527248) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0052737) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00019157) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.00019165) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0029704) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.00584244) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00584244) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0058395) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00016) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.000192) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.0052765) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0052765) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0052759) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000191) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.00527248) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00527248) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0052737) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00584244) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00584244) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0058395) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00092155) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00092155) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.000827894) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00092121) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00092121) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.000921711) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000949) * getSMEFTCoeffEW("CHdR", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.000949) * getSMEFTCoeffEW("CHdR", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.000948092) * getSMEFTCoeffEW("CHdR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.01105) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.02200835) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.02200835) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.74) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.0955) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (-0.0433) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.09154) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (-0.02254) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.02369) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (-0.0382) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0376) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0424) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0382) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0376) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0424) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.006704) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.006547) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.007081) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.1461) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.1461) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.1433) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaH2e2muRatio1()

const double NPSMEFTd6General::deltaGammaH2e2muRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2e 2\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2e 2\mu)$/ $\Gamma(H\to 2e 2\mu)_{\mathrm{SM}}$

Definition at line 29130 of file NPSMEFTd6General.cpp.

                                                            {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+121249. * getSMEFTCoeff("CHbox",muRG)
            - 59336.7 * getSMEFTCoeff("CHB",muRG)
            - 7152.53 * getSMEFTCoeff("CHW",muRG)
            + 63753.6 * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 0, 0,muRG))
            + 63771.3 * (getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG))
            - 54745.8 * getSMEFTCoeff("CHeR", 0, 0,muRG)
            - 54706. * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + cAsch * (-42424.4 * getSMEFTCoeff("CHD",muRG)
            - 111863. * getSMEFTCoeff("CHWB",muRG)
            - 3.401 * delta_GF
            - 0.837 * deltaGzd6()
            )
            + cWsch * (-2206.38 * getSMEFTCoeff("CHD",muRG)
            - 23677.2 * getSMEFTCoeff("CHWB",muRG)
            - 3.001 * delta_GF
            - 0.837 * deltaGzd6()
            ));
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-10.452 * deltaMz()
            + 16.193 * deltaMh()
            - 0.096 * deltaaMZ()
            + 2.281 * deltaGmu()))
            + cWsch * (cHSM * (-11.25 * deltaMz()
            + 16.193 * deltaMh()
            + 2.17 * deltaGmu()
            + 0.522 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2e2muRatio2()

const double NPSMEFTd6General::deltaGammaH2e2muRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2e 2\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2e 2\mu)$/ $\Gamma(H\to 2e 2\mu)_{\mathrm{SM}}$

Definition at line 29174 of file NPSMEFTd6General.cpp.

                                                            {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaH2e2vRatio1()

const double NPSMEFTd6General::deltaGammaH2e2vRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2e2v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2e2v)$/ $\Gamma(H\to 2e2v)_{\mathrm{SM}}$

Definition at line 29764 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+121287. * getSMEFTCoeff("CHbox",muRG)
            - 35405.9 * getSMEFTCoeff("CHB",muRG)
            - 27195.5 * getSMEFTCoeff("CHW",muRG)
            + 65790.6 * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 0, 0,muRG))
            - 28690.7 * (getSMEFTCoeff("CHl1R", 1, 1,muRG) - getSMEFTCoeff("CHl3R", 1, 1,muRG))
            - 28703.9 * (getSMEFTCoeff("CHl1R", 2, 2,muRG) - getSMEFTCoeff("CHl3R", 2, 2,muRG))
            - 56575.7 * getSMEFTCoeff("CHeR", 0, 0,muRG)
            + cAsch * (-36350.8 * getSMEFTCoeff("CHD",muRG)
            - 68896.2 * getSMEFTCoeff("CHWB",muRG)
            - 3.199 * delta_GF
            - 0.846 * deltaGzd6())
            + cWsch * (-16304.9 * getSMEFTCoeff("CHD",muRG)
            - 24376.4 * getSMEFTCoeff("CHWB",muRG)
            - 3. * delta_GF
            - 0.846 * deltaGzd6())
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (cAsch * (-10.705 * deltaMz()
            + 15.922 * deltaMh()
            + 0.079 * deltaaMZ()
            + 2.103 * deltaGmu())
            + cWsch * (
            -10.099 * deltaMz()
            + 15.922 * deltaMh()
            + 2.191 * deltaGmu()
            - 0.445 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2e2vRatio2()

const double NPSMEFTd6General::deltaGammaH2e2vRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2e2v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2e2v)$/ $\Gamma(H\to 2e2v)_{\mathrm{SM}}$

Definition at line 29808 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaH2evRatio1()

const double NPSMEFTd6General::deltaGammaH2evRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2ev)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2ev)$/ $\Gamma(H\to 2ev)_{\mathrm{SM}}$

Definition at line 34307 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    dwidth += (+121306. * getSMEFTCoeff("CHbox",muRG)
            + 1054.18 * getSMEFTCoeff("CHB",muRG)
            - 91797.7 * getSMEFTCoeff("CHW",muRG)
            - 411.183 * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            - 2684.07 * getSMEFTCoeff("CHeR", 0, 0,muRG)
            + 136899. * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + cAsch * (-198266. * getSMEFTCoeff("CHD",muRG)
            - 364381. * getSMEFTCoeff("CHWB",muRG)
            - 4.629 * delta_GF
            - 0.037 * deltaGzd6()
            - 13.549 * deltaMwd6()
            - 0.965 * deltaGwd6())
            + cWsch * (-33589.4 * getSMEFTCoeff("CHD",muRG)
            - 3458.14 * getSMEFTCoeff("CHWB",muRG)
            - 2.999 * delta_GF
            - 0.037 * deltaGzd6()
            - 0.965 * deltaGwd6())
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (cAsch * (-12.638 * deltaMz()
            + 14.08 * deltaMh()
            + 1.901 * deltaaMZ()
            + 0.103 * deltaGmu())
            + cWsch * (-0.103 * deltaMz()
            - 8.875 * deltaMw()
            + 14.08 * deltaMh()
            + 2.015 * deltaGmu()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)  
    // Dominated by CC => Use HWW uncertainty
    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
}

◆ deltaGammaH2evRatio2()

const double NPSMEFTd6General::deltaGammaH2evRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2ev)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2ev)$/ $\Gamma(H\to 2ev)_{\mathrm{SM}}$

Definition at line 34353 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaH2L2dRatio1()

const double NPSMEFTd6General::deltaGammaH2L2dRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2L2d)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2L2d)$/ $\Gamma(H\to 2L2d)_{\mathrm{SM}}$

Definition at line 31060 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg    
    dwidth += cAsch * (+121289. * getSMEFTCoeff("CHbox",muRG)
            - 84134.2 * getSMEFTCoeff("CHB",muRG)
            + 17402.7 * getSMEFTCoeff("CHW",muRG)
            + 21075. * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 0, 0,muRG))
            + 21073.9 * (getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG))
            + 20966.2 * (getSMEFTCoeff("CHl1R", 2, 2,muRG) + getSMEFTCoeff("CHl3R", 2, 2,muRG))
            + 23026.5 * (getSMEFTCoeff("CHq1R", 0, 0,muRG) + getSMEFTCoeff("CHq3R", 0, 0,muRG))
            + 23023.9 * (getSMEFTCoeff("CHq1R", 1, 1,muRG) + getSMEFTCoeff("CHq3R", 1, 1,muRG))
            + 22666. * (getSMEFTCoeff("CHq1R", 2, 2,muRG) + getSMEFTCoeff("CHq3R", 2, 2,muRG))
            - 18090.2 * getSMEFTCoeff("CHeR", 0, 0,muRG)
            - 18067. * getSMEFTCoeff("CHeR", 1, 1,muRG)
            - 17980.6 * getSMEFTCoeff("CHeR", 2, 2,muRG)
            - 4190.57 * getSMEFTCoeff("CHdR", 0, 0,muRG)
            - 4189.38 * getSMEFTCoeff("CHdR", 1, 1,muRG)
            - 3850.11 * getSMEFTCoeff("CHdR", 2, 2,muRG)
            - 48948.9 * getSMEFTCoeff("CHD",muRG)
            - 158101. * getSMEFTCoeff("CHWB",muRG)
            - 3.617 * delta_GF
            - 0.837 * deltaGzd6()
            );
            /*+ cWsch * (+13172. * getSMEFTCoeff("CHD")
            - 21275. * getSMEFTCoeff("CHWB")
            - 3. * delta_GF
            - 0.837 * deltaGzd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.12067) * getSMEFTCoeff("CHbox",muRG)
            + (0.02221) * getSMEFTCoeff("CHW",muRG)
            + (-0.08987) * getSMEFTCoeff("CHB",muRG)
            + (0.0195) * getSMEFTCoeff("CHD",muRG)
            + (-0.02029) * getSMEFTCoeff("CHWB",muRG)
            + (0.021341) * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            + (0.021391) * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            + (0.021248) * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            + (-0.1582728) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.158513) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.021248) * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + (-0.01721521) * getSMEFTCoeff("CHeR", 0, 0,muRG)
            + (-0.0172416) * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + (-0.0171251) * getSMEFTCoeff("CHeR", 2, 2,muRG)
            + (0.022094) * getSMEFTCoeff("CHq1R", 0, 0,muRG)
            + (0.02214) * getSMEFTCoeff("CHq1R", 1, 1,muRG)
            + (0.023737) * getSMEFTCoeff("CHq1R", 2, 2,muRG)
            + (0.022094) * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + (0.02214) * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + (0.023737) * getSMEFTCoeff("CHq3R", 2, 2,muRG)
            + (-0.003856346) * getSMEFTCoeff("CHdR", 0, 0,muRG)
            + (-0.00384488) * getSMEFTCoeff("CHdR", 1, 1,muRG)
            + (-0.003870856) * getSMEFTCoeff("CHdR", 2, 2,muRG)
            + (0.18095) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.831) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-10.043 * deltaMz()
            + 16.281 * deltaMh()
            - 0.342 * deltaaMZ()
            + 2.516 * deltaGmu()))
            + cWsch * (cHSM * (-12.322 * deltaMz()
            + 16.281 * deltaMh()
            + 2.201 * deltaGmu()
            + 1.57 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2L2dRatio2()

const double NPSMEFTd6General::deltaGammaH2L2dRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2L2d)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2L2d)$/ $\Gamma(H\to 2L2d)_{\mathrm{SM}}$

Definition at line 31144 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014825) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.08465) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.10657) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (0.007578) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.032649) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.001005) * pow(getSMEFTCoeffEW("CHl1R", 0, 0), 2.0)
                + (0.0010092) * pow(getSMEFTCoeffEW("CHl1R", 1, 1), 2.0)
                + (0.0010064) * pow(getSMEFTCoeffEW("CHl1R", 2, 2), 2.0)
                + (0.009463) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.009375) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.0010064) * pow(getSMEFTCoeffEW("CHl3R", 2, 2), 2.0)
                + (0.0010054) * pow(getSMEFTCoeffEW("CHeR", 0, 0), 2.0)
                + (0.0010055) * pow(getSMEFTCoeffEW("CHeR", 1, 1), 2.0)
                + (0.0010051) * pow(getSMEFTCoeffEW("CHeR", 2, 2), 2.0)
                + (0.0006784) * pow(getSMEFTCoeffEW("CHq1R", 0, 0), 2.0)
                + (0.000655) * pow(getSMEFTCoeffEW("CHq1R", 1, 1), 2.0)
                + (0.0007329) * pow(getSMEFTCoeffEW("CHq1R", 2, 2), 2.0)
                + (0.0006784) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                + (0.000655) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                + (0.0007329) * pow(getSMEFTCoeffEW("CHq3R", 2, 2), 2.0)
                + (0.0006792) * pow(getSMEFTCoeffEW("CHdR", 0, 0), 2.0)
                + (0.0006779) * pow(getSMEFTCoeffEW("CHdR", 1, 1), 2.0)
                + (0.0007332) * pow(getSMEFTCoeffEW("CHdR", 2, 2), 2.0)
                + (0.011121) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (0.002721) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.010906) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (-0.0012719) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.0024549) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (0.0026064) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0026073) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.002596) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.01207611) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.01209367) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.002596) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.0020974) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.00209905) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.00208636) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.0026944) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0026923) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0028925) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0026944) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0026923) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0028925) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.00047059) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.0004699201) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.014684) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.1563694) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (0.018562) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.1022427) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (0.0006588) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0006557) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0006715) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.002116) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.002118) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0006715) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0001906) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0001915) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.000173) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.0002293) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0002229) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0002215) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0002293) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0002229) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0002215) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.0001371) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.000138) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.0001006) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.002694) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0207025) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (0.059846) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (-0.00294565) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.00294453) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.00293256) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.007992) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.007978) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00293256) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0013157) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0013112) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.001313) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.0018767) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0018778) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0020349) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0018767) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0018778) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0020349) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.0001977) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0001982) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.0001883) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.010907) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000988) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (0.0025211) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0025204) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.002511) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0001134) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0001259) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.002511) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.001268) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0012691) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0012823) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.0008924) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.000892) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0009143) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0008924) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.000892) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0009143) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.0003253) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.00032566) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.00039497) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.0024039) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0003186) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0003249) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0003404) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.002784) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.002786) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0003404) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.002898) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0028961) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0028869) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.0008712) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0008626) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0009395) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0008712) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0008626) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0009395) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.00061055) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.00060968) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.00063252) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.0024548) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.000590513) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0026049) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0026064) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00260457) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.000590967) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0026073) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00259549) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00259549) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0020129) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.002596) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00581) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.002642) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0020996) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.002098) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0020855) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.002638086) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0026360054) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.002830181) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.002638086) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0026360054) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.002830181) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.0004606) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.00046071) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.00046383) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.01942) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.002561) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0020996) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0020983) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0020855) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.002636675) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.002640509) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.002831097) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.002636675) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.002640509) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.002831097) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.00046075) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.00046077) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.00046367) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.01943808) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.002596) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0020974) * getSMEFTCoeffEW("CHeR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00209905) * getSMEFTCoeffEW("CHeR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00208636) * getSMEFTCoeffEW("CHeR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0013588) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0026944) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00135887) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0026923) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00147085) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.0028925) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0026944) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0026923) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0028925) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00047059) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0004699201) * getSMEFTCoeffEW("CHdR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.77) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.095) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (-0.0213) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.0747) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (-0.0162) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.023) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (-0.0187) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.01838) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.01821) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.108636) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.114941) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.01821) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0142) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.015339) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.014586) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.01942) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.01967) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.02085) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.01942) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.01967) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.02085) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.003423) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0032534) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.0032839) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.142) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaH2L2LRatio1()

const double NPSMEFTd6General::deltaGammaH2L2LRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2L2L')$ ( $L,L'=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2L2L')$/ $\Gamma(H\to 2L2L')_{\mathrm{SM}}$

Definition at line 28877 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    
    dwidth += cAsch * (+121302. * getSMEFTCoeff("CHbox",muRG)
            - 59592.5 * getSMEFTCoeff("CHB",muRG)
            - 6187.97 * getSMEFTCoeff("CHW",muRG)
            + 42404.3 * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 0, 0,muRG))
            + 42440.7 * (getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG))
            + 42633.3 * (getSMEFTCoeff("CHl1R", 2, 2,muRG) + getSMEFTCoeff("CHl3R", 2, 2,muRG))
            - 36384.4 * getSMEFTCoeff("CHeR", 0, 0,muRG)
            - 36395.3 * getSMEFTCoeff("CHeR", 1, 1,muRG)
            - 36589.1 * getSMEFTCoeff("CHeR", 2, 2,muRG)
            - 42519.3 * getSMEFTCoeff("CHD",muRG)
            - 112124. * getSMEFTCoeff("CHWB",muRG)
            - 3.401 * delta_GF
            - 0.836 * deltaGzd6()
            );
            /*+ cWsch * (-1940.8 * getSMEFTCoeff("CHD")
            - 23529. * getSMEFTCoeff("CHWB")
            - 3.002 * delta_GF
            - 0.836 * deltaGzd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.12111) * getSMEFTCoeff("CHbox",muRG)
            + (0.00953) * getSMEFTCoeff("CHW",muRG)
            + (-0.0764) * getSMEFTCoeff("CHB",muRG)
            + (0.01008) * getSMEFTCoeff("CHD",muRG)
            + (-0.02236) * getSMEFTCoeff("CHWB",muRG)
            + (0.043324) * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            + (0.043349) * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            + (0.043607) * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            + (-0.1385393) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.1385419) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.043607) * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + (-0.03486366) * getSMEFTCoeff("CHeR", 0, 0,muRG)
            + (-0.03493756) * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + (-0.03507062) * getSMEFTCoeff("CHeR", 2, 2,muRG)
            + (0.18171) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.815) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-10.484 * deltaMz()
            + 16.233 * deltaMh()
            - 0.114 * deltaaMZ()
            + 2.278 * deltaGmu()))
            + cWsch * (cHSM * (-11.298 * deltaMz()
            + 16.233 * deltaMh()
            + 2.163 * deltaGmu()
            + 0.552 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2L2LRatio2()

const double NPSMEFTd6General::deltaGammaH2L2LRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2L2L')$ ( $L,L'=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2L2L')$/ $\Gamma(H\to 2L2L')_{\mathrm{SM}}$

Definition at line 28947 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
 
        dwidth += cWsch * (
                +(0.014691) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.18009) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.48021) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (0.0159) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.1418) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.0020415) * pow(getSMEFTCoeffEW("CHl1R", 0, 0), 2.0)
                + (0.0020419) * pow(getSMEFTCoeffEW("CHl1R", 1, 1), 2.0)
                + (0.0020604) * pow(getSMEFTCoeffEW("CHl1R", 2, 2), 2.0)
                + (0.007781) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.007808) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.0020604) * pow(getSMEFTCoeffEW("CHl3R", 2, 2), 2.0)
                + (0.0020398) * pow(getSMEFTCoeffEW("CHeR", 0, 0), 2.0)
                + (0.0020412) * pow(getSMEFTCoeffEW("CHeR", 1, 1), 2.0)
                + (0.0020619) * pow(getSMEFTCoeffEW("CHeR", 2, 2), 2.0)
                + (0.011019) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (0.001152) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.00926) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (-0.0024578) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.002726) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (0.0052648) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0052647) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0052995) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.0094343) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0094397) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0052995) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.004236321) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.004237771) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.0042564489) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.014702) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.132391) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (0.044171) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.2607976) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (-0.00107) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.001071) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0013914) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0013727) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0013766) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.001152) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.046792) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (-0.190576) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (-0.0046147) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.0046248) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.0046253) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.004583) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.004645) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0046253) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0017605) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0017583) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0017491) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.00926) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.003693) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (0.0046375) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0046306) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0046353) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.003425) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.003419) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0046353) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0029378) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0029368) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0030038) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.001227) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0009464) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0009426) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0009911) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.003648) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.003656) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0009911) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0055397) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0055456) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0055823) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.002726) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000181) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.000179) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.001181687) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.005088263) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.00017612) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00014542) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.000140787) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.0052648) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000183) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.005085178) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0011831968) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.00017606) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.000145462) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.000140905) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.0052647) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.005124758) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.005119363) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0041247) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.000141677) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.000141659) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0052995) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000695) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.005099) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.004239) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0040937) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.004119) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.016786442) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.005125) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0040916) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0042405) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0041174) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.01678974) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.000141677) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.000141659) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0052995) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000121) * getSMEFTCoeffEW("CHeR", 0, 0) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.000121) * getSMEFTCoeffEW("CHeR", 0, 0) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.004236321) * getSMEFTCoeffEW("CHeR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000118) * getSMEFTCoeffEW("CHeR", 1, 1) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.004237771) * getSMEFTCoeffEW("CHeR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0042564489) * getSMEFTCoeffEW("CHeR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.72) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.0982) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (-0.0146) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.0726) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (-0.0063) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.0262) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (-0.0381) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.0373) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.0384) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.1078) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.10943) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0384) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.03042) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.03003) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.03121) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.148) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
 
    }
 
    return dwidth;
}

◆ deltaGammaH2L2uRatio1()

const double NPSMEFTd6General::deltaGammaH2L2uRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2L2u)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2L2u)$/ $\Gamma(H\to 2L2u)_{\mathrm{SM}}$

Definition at line 30749 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121251. * getSMEFTCoeff("CHbox",muRG)
            - 103956. * getSMEFTCoeff("CHB",muRG)
            + 35760.1 * getSMEFTCoeff("CHW",muRG)
            + 21276.1 * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 0, 0,muRG))
            + 21284.8 * (getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG))
            + 21179.4 * (getSMEFTCoeff("CHl1R", 2, 2,muRG) + getSMEFTCoeff("CHl3R", 2, 2,muRG))
            - 35906.7 * (getSMEFTCoeff("CHq1R", 0, 0,muRG) - getSMEFTCoeff("CHq3R", 0, 0,muRG))
            - 35849.3 * (getSMEFTCoeff("CHq1R", 1, 1,muRG) - getSMEFTCoeff("CHq3R", 1, 1,muRG))
            - 18274.6 * getSMEFTCoeff("CHeR", 0, 0,muRG)
            - 18258.1 * getSMEFTCoeff("CHeR", 1, 1,muRG)
            - 18170.5 * getSMEFTCoeff("CHeR", 2, 2,muRG)
            + 15975.7 * getSMEFTCoeff("CHuR", 0, 0,muRG)
            + 15912.4 * getSMEFTCoeff("CHuR", 1, 1,muRG)
            - 54348.3 * getSMEFTCoeff("CHD",muRG)
            - 194795. * getSMEFTCoeff("CHWB",muRG)
            - 3.791 * delta_GF
            - 0.836 * deltaGzd6()
            );
            /*+ cWsch * (+25556.3 * getSMEFTCoeff("CHD")
            - 19191.5 * getSMEFTCoeff("CHWB")
            - 3. * delta_GF
            - 0.836 * deltaGzd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.12136) * getSMEFTCoeff("CHbox",muRG)
            + (0.04252) * getSMEFTCoeff("CHW",muRG)
            + (-0.11176) * getSMEFTCoeff("CHB",muRG)
            + (0.0333) * getSMEFTCoeff("CHD",muRG)
            + (-0.01805) * getSMEFTCoeff("CHWB",muRG)
            + (0.021514) * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            + (0.021631) * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            + (0.021538) * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            + (-0.16016) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.1598348) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.021538) * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + (-0.01711641) * getSMEFTCoeff("CHeR", 0, 0,muRG)
            + (-0.01727087) * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + (-0.01726594) * getSMEFTCoeff("CHeR", 2, 2,muRG)
            + (-0.03561039) * getSMEFTCoeff("CHq1R", 0, 0,muRG)
            + (-0.03558411) * getSMEFTCoeff("CHq1R", 1, 1,muRG)
            + (0.035628) * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + (0.035464) * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + (0.015096) * getSMEFTCoeff("CHuR", 0, 0,muRG)
            + (0.014986) * getSMEFTCoeff("CHuR", 1, 1,muRG)
            + (0.18207) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.816) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-9.689 * deltaMz()
            + 16.184 * deltaMh()
            - 0.517 * deltaaMZ()
            + 2.692 * deltaGmu()))
            + cWsch * (cHSM * (-13.135 * deltaMz()
            + 16.184 * deltaMh()
            + 2.157 * deltaGmu()
            + 2.403 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2L2uRatio2()

const double NPSMEFTd6General::deltaGammaH2L2uRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2L2u)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2L2u)$/ $\Gamma(H\to 2L2u)_{\mathrm{SM}}$

Definition at line 30828 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014712) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.11704) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.23808) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (0.010204) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.06973) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.0010203) * pow(getSMEFTCoeffEW("CHl1R", 0, 0), 2.0)
                + (0.0010184) * pow(getSMEFTCoeffEW("CHl1R", 1, 1), 2.0)
                + (0.0010188) * pow(getSMEFTCoeffEW("CHl1R", 2, 2), 2.0)
                + (0.0094) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.0094) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.0010188) * pow(getSMEFTCoeffEW("CHl3R", 2, 2), 2.0)
                + (0.0010192) * pow(getSMEFTCoeffEW("CHeR", 0, 0), 2.0)
                + (0.0010184) * pow(getSMEFTCoeffEW("CHeR", 1, 1), 2.0)
                + (0.0010172) * pow(getSMEFTCoeffEW("CHeR", 2, 2), 2.0)
                + (0.0013261) * pow(getSMEFTCoeffEW("CHq1R", 0, 0), 2.0)
                + (0.0013229) * pow(getSMEFTCoeffEW("CHq1R", 1, 1), 2.0)
                + (0.0013261) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                + (0.0013229) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                + (0.0013245) * pow(getSMEFTCoeffEW("CHuR", 0, 0), 2.0)
                + (0.0013226) * pow(getSMEFTCoeffEW("CHuR", 1, 1), 2.0)
                + (0.011033) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (0.005234) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.013568) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (0.0004184) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.002182) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (0.0026337) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.002631) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0026204) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.01206044) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.01206456) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0026204) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.002118503) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.0021174) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.002109743) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.00433568) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.004327143) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0043399) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0043328) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0018366) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.0018281) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.014692) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.143958) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (0.023022) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.1570976) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (0.0015154) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0015196) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0015219) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.003728) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.003781) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0015219) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.0005571) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.0006072) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.0006202) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.0001747) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0001548) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0001772) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0001611) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0005458) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.000531) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.005234) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.028141) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (-0.031371) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (-0.0038795) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.0038758) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.0038654) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.009644) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.009688) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0038654) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0019463) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0019533) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0019535) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.003307) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.003269) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0032933) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0032703) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0007667) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.0007652) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.013568) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00144) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (0.0028307) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.002828) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0028158) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.001232) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0012439) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0028158) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0010537) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0010534) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0010662) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.0023745) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0023721) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0023765) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0023712) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00127183) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00127912) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.00406) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0001408) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0001334) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0001475) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.002294) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.002296) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0001475) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0031757) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0031774) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.003167) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.0005142) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0005087) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0005083) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0004994) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0023805) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00237786) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.002182) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0005904659) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00263259) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0026337) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0026362) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.000590148) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.002631) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00261892) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00261892) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0020389) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0026204) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00576) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00261) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0021198) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0021178) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0021066) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.0042491) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0042424) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.00424852) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.004239582) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.001799671) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.001792115) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.01938906) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.002607) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0021198) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0021178) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0021066) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.0042503) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0042428) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.004249441) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.004243656) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.001798463) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.001791597) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.01938972) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0026204) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.002118503) * getSMEFTCoeffEW("CHeR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0021174) * getSMEFTCoeffEW("CHeR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.002109743) * getSMEFTCoeffEW("CHeR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00265285) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00433568) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00265126) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.004327143) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0043399) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0043328) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0018366) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0018281) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.75) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.0968) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (-0.0449) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.1028) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (-0.028) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.0219) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (-0.01853) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.01905) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.01862) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.12306) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.12259) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.01862) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.01454) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.015637) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.014707) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.031184) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.027789) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0327) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0315) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.01361) * deltaGzd6() * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.01343) * deltaGzd6() * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.145) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
 
    }
 
    return dwidth;
}

◆ deltaGammaH2L2v2Ratio1()

const double NPSMEFTd6General::deltaGammaH2L2v2Ratio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2L2v)$/ $\Gamma(H\to 2L2v)_{\mathrm{SM}}$

Definition at line 29669 of file NPSMEFTd6General.cpp.

                                                            {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+121298. * getSMEFTCoeff("CHbox",muRG)
            - 35499.1 * getSMEFTCoeff("CHB",muRG)
            - 27241.9 * getSMEFTCoeff("CHW",muRG)
            + 18600.1 * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            + 18562.6 * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            - 28682. * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            - 28294.2 * getSMEFTCoeff("CHeR", 0, 0,muRG)
            - 28285.3 * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + 47342.8 * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + 47360.7 * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + 28708.8 * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + cAsch * (-36443.1 * getSMEFTCoeff("CHD",muRG)
            - 68837.8 * getSMEFTCoeff("CHWB",muRG)
            - 3.201 * delta_GF
            - 0.839 * deltaGzd6()
            )
            + cWsch * (-16226. * getSMEFTCoeff("CHD",muRG)
            - 24353. * getSMEFTCoeff("CHWB",muRG)
            - 3.002 * delta_GF
            - 0.839 * deltaGzd6()
            ));
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-10.697 * deltaMz()
            + 16.002 * deltaMh()
            + 0.083 * deltaaMZ()
            + 2.115 * deltaGmu()))
            + cWsch * (cHSM * (-10.137 * deltaMz()
            + 16.002 * deltaMh()
            + 2.179 * deltaGmu()
            - 0.466 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2L2v2Ratio2()

const double NPSMEFTd6General::deltaGammaH2L2v2Ratio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2L2v)$/ $\Gamma(H\to 2L2v)_{\mathrm{SM}}$

Definition at line 29717 of file NPSMEFTd6General.cpp.

                                                            {
    double dwidth = 0.0;
 
    //Contributions that are quadratic in the effective coefficients
    return ( dwidth);
 
}

◆ deltaGammaH2L2vRatio1()

const double NPSMEFTd6General::deltaGammaH2L2vRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2L2v)$/ $\Gamma(H\to 2L2v)_{\mathrm{SM}}$

Definition at line 29427 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
    
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121291. * getSMEFTCoeff("CHbox",muRG)
            - 35349.6 * getSMEFTCoeff("CHB",muRG)
            - 27095.7 * getSMEFTCoeff("CHW",muRG)
            + 3026.29 * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            + 3021.87 * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            + 2746.62 * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            - 18924.3 * getSMEFTCoeff("CHeR", 0, 0,muRG)
            - 18918.4 * getSMEFTCoeff("CHeR", 1, 1,muRG)
            - 18820.4 * getSMEFTCoeff("CHeR", 2, 2,muRG)
            + 41085.2 * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + 41121.1 * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + 41134.2 * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            - 36393. * getSMEFTCoeff("CHD",muRG)
            - 69325.9 * getSMEFTCoeff("CHWB",muRG)
            - 3.201 * delta_GF
            - 0.846 * deltaGzd6()
            );
            /*+ cWsch * (-16170.3 * getSMEFTCoeff("CHD")
            - 24273.2 * getSMEFTCoeff("CHWB")
            - 3. * delta_GF
            - 0.846 * deltaGzd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.1213) * getSMEFTCoeff("CHbox",muRG)
            + (-0.01494) * getSMEFTCoeff("CHW",muRG)
            + (-0.040852) * getSMEFTCoeff("CHB",muRG)
            + (-0.009936) * getSMEFTCoeff("CHD",muRG)
            + (-0.023597) * getSMEFTCoeff("CHWB",muRG)
            + (0.003651) * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            + (0.003794) * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            + (0.003449) * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            + (-0.139236) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.138049) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.041527) * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + (-0.0181637) * getSMEFTCoeff("CHeR", 0, 0,muRG)
            + (-0.0181476) * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + (-0.0180375) * getSMEFTCoeff("CHeR", 2, 2,muRG)
            + (0.1819) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.831) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-10.683 * deltaMz()
            + 15.939 * deltaMh()
            + 0.095 * deltaaMZ()
            + 2.099 * deltaGmu()))
            + cWsch * (cHSM * (-10.108 * deltaMz()
            + 15.939 * deltaMh()
            + 2.178 * deltaGmu()
            - 0.402 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2l2vRatio1()

const double NPSMEFTd6General::deltaGammaH2l2vRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2l2v)$ ( $l=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2l2v)$/ $\Gamma(H\to 2l2v)_{\mathrm{SM}}$

Definition at line 34832 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    // SM decay widths (from MG simmulations)
    double wH2L2v2SM = 0.18213e-05, wHevmuvSM = 0.19421e-04, wH2Lv2SM = 0.18353e-04;
 
    // Sum
    double wH2l2vSM = wH2L2v2SM + wHevmuvSM + wH2Lv2SM;
 
    dwidth += (wH2L2v2SM * deltaGammaH2L2v2Ratio1() + wHevmuvSM * deltaGammaHevmuvRatio1()
            + wH2Lv2SM * deltaGammaH2Lv2Ratio1()) / wH2l2vSM;
 
    return dwidth;
}

◆ deltaGammaH2L2vRatio2()

const double NPSMEFTd6General::deltaGammaH2L2vRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2L2v)$/ $\Gamma(H\to 2L2v)_{\mathrm{SM}}$

Definition at line 29499 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += cWsch * (
                +(0.0147) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.073334) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.070511) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (0.00727) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.02474) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.0015651) * pow(getSMEFTCoeffEW("CHl1R", 0, 0), 2.0)
                + (0.0015665) * pow(getSMEFTCoeffEW("CHl1R", 1, 1), 2.0)
                + (0.0015709) * pow(getSMEFTCoeffEW("CHl1R", 2, 2), 2.0)
                + (0.00756) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.00754) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.0015709) * pow(getSMEFTCoeffEW("CHl3R", 2, 2), 2.0)
                + (0.0010729) * pow(getSMEFTCoeffEW("CHeR", 0, 0), 2.0)
                + (0.0010725) * pow(getSMEFTCoeffEW("CHeR", 1, 1), 2.0)
                + (0.0010717) * pow(getSMEFTCoeffEW("CHeR", 2, 2), 2.0)
                + (0.01103) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (-0.0018682) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.0049606) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (-0.0048972) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.0028616) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (0.0004288) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0004278) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0003926) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.00965737) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00965793) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0050567) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00220467) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.00220376) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.00219322) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.014703) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.1491845) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (0.021695) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.0828173) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (-0.0010147) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.0009678) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.0009749) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0006629) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0006513) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0013712) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.00174) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0017382) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.001721) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.0018682) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0194976) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (0.075507) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (0.0006084) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.000613) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0006208) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0026763) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0026821) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0023806) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.0049606) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00292) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (0.0014409) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0014413) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.001437) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0035829) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0035822) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0023398) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.00193758) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.00193767) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0019465) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.0012277) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0019702) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0019726) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0019855) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.002644) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.002641) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00015) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.002477) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0024764) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0024663) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.0028616) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0001474) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.0001471) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.00072424) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0004297) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0004288) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0001487) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.0004276) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00072447) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0004278) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.000397) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0003963) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.00113809) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0003926) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00109) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00492) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0022043) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0021427) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.00213396) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.01701421) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0049) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.00214211) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.00220462) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.00213375) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.017004442) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0050567) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00220467) * getSMEFTCoeffEW("CHeR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00220376) * getSMEFTCoeffEW("CHeR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00219322) * getSMEFTCoeffEW("CHeR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.74) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.102) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (0.00348) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.0282) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (0.00716) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.0178) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (-0.00316) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.00347) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.00309) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.107) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.11147) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.03691) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.01632) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0158) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.01655) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.154) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaH2l2vRatio2()

const double NPSMEFTd6General::deltaGammaH2l2vRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2l2v)$ ( $l=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2l2v)$/ $\Gamma(H\to 2l2v)_{\mathrm{SM}}$

Definition at line 34847 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaH2Lv2Ratio1()

const double NPSMEFTd6General::deltaGammaH2Lv2Ratio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2Lv)$/ $\Gamma(H\to 2Lv)_{\mathrm{SM}}$

Definition at line 34208 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    dwidth += (+121215. * getSMEFTCoeff("CHbox",muRG)
            + 1054.39 * getSMEFTCoeff("CHB",muRG)
            - 91849.7 * getSMEFTCoeff("CHW",muRG)
            - 205.44 * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            - 205.933 * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            - 1345.15 * getSMEFTCoeff("CHeR", 0, 0,muRG)
            - 1299.22 * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + 68383.7 * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + 68347.6 * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + cAsch * (-198193. * getSMEFTCoeff("CHD",muRG)
            - 364163. * getSMEFTCoeff("CHWB",muRG)
            - 4.627 * delta_GF
            - 13.439 * deltaMwd6()
            - 0.961 * deltaGwd6()
            - 0.042 * deltaGzd6()
            )
            + cWsch * (-33577.8 * getSMEFTCoeff("CHD",muRG)
            - 3457.89 * getSMEFTCoeff("CHWB",muRG)
            - 2.999 * delta_GF
            - 0.042 * deltaGzd6()
            - 0.961 * deltaGwd6()
            ));
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-12.755 * deltaMz()
            + 14.08 * deltaMh()
            + 1.884 * deltaaMZ()
            + 0.121 * deltaGmu()))
            + cWsch * (cHSM * (-0.118 * deltaMz()
            - 8.746 * deltaMw()
            + 14.08 * deltaMh()
            + 2.002 * deltaGmu()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)  
    // Dominated by CC => Use HWW uncertainty
    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
}

◆ deltaGammaH2Lv2Ratio2()

const double NPSMEFTd6General::deltaGammaH2Lv2Ratio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2Lv)$/ $\Gamma(H\to 2Lv)_{\mathrm{SM}}$

Definition at line 34258 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaH2LvRatio1()

const double NPSMEFTd6General::deltaGammaH2LvRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2Lv)$/ $\Gamma(H\to 2Lv)_{\mathrm{SM}}$

Definition at line 34006 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121133. * getSMEFTCoeff("CHbox",muRG)
            + 1057.61 * getSMEFTCoeff("CHB",muRG)
            - 91969.3 * getSMEFTCoeff("CHW",muRG)
            - 137.279 * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            - 137.825 * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            - 123.03 * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            - 897.801 * getSMEFTCoeff("CHeR", 0, 0,muRG)
            - 865.641 * getSMEFTCoeff("CHeR", 1, 1,muRG)
            - 862.721 * getSMEFTCoeff("CHeR", 2, 2,muRG)
            + 45408.9 * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + 45540.1 * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + 45765.4 * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            - 198032. * getSMEFTCoeff("CHD",muRG)
            - 364301. * getSMEFTCoeff("CHWB",muRG)
            - 4.631 * delta_GF
            - 13.529 * deltaMwd6()
            - 0.956 * deltaGwd6()
            - 0.037 * deltaGzd6()
            );
            /*+ cWsch * (-33553.1 * getSMEFTCoeff("CHD")
            - 3437.65 * getSMEFTCoeff("CHWB")
            - 3.001 * delta_GF
            - 0.036 * deltaGzd6()
            - 0.956 * deltaGwd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.12114) * getSMEFTCoeff("CHbox",muRG)
            + (-0.0916348) * getSMEFTCoeff("CHW",muRG)
            + (0.000592) * getSMEFTCoeff("CHB",muRG)
            + (-0.0333329) * getSMEFTCoeff("CHD",muRG)
            + (-0.003342) * getSMEFTCoeff("CHWB",muRG)
            + (-0.00014956) * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            + (-0.0001496) * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            + (-0.0001277) * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            + (-0.1360386) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.1361577) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.045354) * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + (-0.000816964) * getSMEFTCoeff("CHeR", 0, 0,muRG)
            + (-0.000817925) * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + (-0.000817821) * getSMEFTCoeff("CHeR", 2, 2,muRG)
            + (0.1817) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.938) * deltaGwd6()
            + (-0.041) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-12.684 * deltaMz()
            + 13.95 * deltaMh()
            + 1.899 * deltaaMZ()
            + 0.151 * deltaGmu()))
            + cWsch * (cHSM * (-0.128 * deltaMz()
            - 8.864 * deltaMw()
            + 13.95 * deltaMh()
            + 2.045 * deltaGmu()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)  
    // Dominated by CC => Use HWW uncertainty
    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
}

◆ deltaGammaH2LvRatio2()

const double NPSMEFTd6General::deltaGammaH2LvRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2Lv)$/ $\Gamma(H\to 2Lv)_{\mathrm{SM}}$

Definition at line 34083 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014703) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.010735) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.018974) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (0.0013761) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.007877) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.007426) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.007427) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.0019336) * pow(getSMEFTCoeffEW("CHl3R", 2, 2), 2.0)
                + (0.011029) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (-0.01111144) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.007719474) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.00040589) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (-0.00915104) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00914935) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0055012) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.014685) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.037699) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (0.0042941) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.0236584) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (0.005298) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0052989) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00576922) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.01111144) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00133872) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (0.023535) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (0.00032712) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (0.00268) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0026807) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00134623) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00403804) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00038329) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00038372) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.000111398) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.00011135) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.00011094) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.00040588) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.005492) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.016504846) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00549) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.016487234) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0055012) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.78) * pow(deltaGwd6(), 2.0) + (0.03) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.113) * deltaGwd6() * getSMEFTCoeffEW("CHbox")
                + (0.08401) * deltaGwd6() * getSMEFTCoeffEW("CHW")
                + (0.00021) * deltaGwd6() * getSMEFTCoeffEW("CHB")
                + (0.02799) * deltaGwd6() * getSMEFTCoeffEW("CHD")
                + (0.000269) * deltaGwd6() * getSMEFTCoeffEW("CHWB")
                + (1.29e-05) * deltaGwd6() * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (5.8e-06) * deltaGwd6() * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (1.13e-05) * deltaGwd6() * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.12714) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.12563) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0429) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (3.154e-05) * deltaGwd6() * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-2.23e-06) * deltaGwd6() * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-2.448e-05) * deltaGwd6() * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.1695) * deltaGwd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0052) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (0.000409) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.001324) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (0.000337) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.00102) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (-8.5e-05) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-5.01e-05) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.000104) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.006545) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.004527) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0015) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0007588) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0007016) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.00072326) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.0078) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaH2mu2vRatio1()

const double NPSMEFTd6General::deltaGammaH2mu2vRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2\mu 2v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2\mu 2v)$/ $\Gamma(H\to 2\mu 2v)_{\mathrm{SM}}$

Definition at line 29857 of file NPSMEFTd6General.cpp.

                                                            {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+121291. * getSMEFTCoeff("CHbox",muRG)
            - 35658.4 * getSMEFTCoeff("CHB",muRG)
            - 26866.3 * getSMEFTCoeff("CHW",muRG)
            - 28684.4 * (getSMEFTCoeff("CHl1R", 0, 0,muRG) - getSMEFTCoeff("CHl3R", 0, 0,muRG))
            + 65832. * (getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG))
            - 28703.3 * (getSMEFTCoeff("CHl1R", 2, 2,muRG) - getSMEFTCoeff("CHl3R", 2, 2,muRG))
            - 56559.6 * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + cAsch * (-36391.6 * getSMEFTCoeff("CHD",muRG)
            - 69347.6 * getSMEFTCoeff("CHWB",muRG)
            - 3.198 * delta_GF
            - 0.842 * deltaGzd6())
            + cWsch * (-16131.8 * getSMEFTCoeff("CHD",muRG)
            - 24298.9 * getSMEFTCoeff("CHWB",muRG)
            - 3. * delta_GF
            - 0.842 * deltaGzd6())
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (cAsch * (-10.716 * deltaMz()
            + 15.962 * deltaMh()
            + 0.082 * deltaaMZ()
            + 2.075 * deltaGmu())
            + cWsch * (-10.13 * deltaMz()
            + 15.962 * deltaMh()
            + 2.177 * deltaGmu()
            - 0.489 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2mu2vRatio2()

const double NPSMEFTd6General::deltaGammaH2mu2vRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2\mu 2v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2\mu 2v)$/ $\Gamma(H\to 2\mu 2v)_{\mathrm{SM}}$

Definition at line 29900 of file NPSMEFTd6General.cpp.

                                                            {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaH2muvRatio1()

const double NPSMEFTd6General::deltaGammaH2muvRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2\mu v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2\mu v)$/ $\Gamma(H\to 2\mu v)_{\mathrm{SM}}$

Definition at line 34402 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    dwidth += (+121244. * getSMEFTCoeff("CHbox",muRG)
            + 1045.26 * getSMEFTCoeff("CHB",muRG)
            - 91781. * getSMEFTCoeff("CHW",muRG)
            - 410.738 * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            - 2593.82 * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + 136695. * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + cAsch * (-198022. * getSMEFTCoeff("CHD",muRG)
            - 364213. * getSMEFTCoeff("CHWB",muRG)
            - 4.625 * delta_GF
            - 0.031 * deltaGzd6())
            + cWsch * (-33559. * getSMEFTCoeff("CHD",muRG)
            - 3447.11 * getSMEFTCoeff("CHWB",muRG)
            - 2.998 * delta_GF
            - 0.031 * deltaGzd6())
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (cAsch * (-12.671 * deltaMz()
            - 13.492 * deltaMwd6()
            - 0.957 * deltaGwd6()
            + 14.005 * deltaMh()
            + 1.868 * deltaaMZ()
            + 0.103 * deltaGmu())
            + cWsch * (-0.177 * deltaMz()
            - 8.833 * deltaMw()
            - 0.957 * deltaGwd6()
            + 14.005 * deltaMh()
            + 1.959 * deltaGmu()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)  
    // Dominated by CC => Use HWW uncertainty
    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
}

◆ deltaGammaH2muvRatio2()

const double NPSMEFTd6General::deltaGammaH2muvRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2\mu v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2\mu v)$/ $\Gamma(H\to 2\mu v)_{\mathrm{SM}}$

Definition at line 34448 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaH2u2dRatio1()

const double NPSMEFTd6General::deltaGammaH2u2dRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2u2d)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2u2d)$/ $\Gamma(H\to 2u2d)_{\mathrm{SM}}$

Definition at line 30454 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121245. * getSMEFTCoeff("CHbox",muRG)
            - 129896. * getSMEFTCoeff("CHB",muRG)
            + 58951.9 * getSMEFTCoeff("CHW",muRG)
            - 18953.2 * getSMEFTCoeff("CHq1R", 0, 0,muRG)
            - 18954.1 * getSMEFTCoeff("CHq1R", 1, 1,muRG)
            + 36775. * getSMEFTCoeff("CHq1R", 2, 2,muRG)
            + 15639.1 * getSMEFTCoeff("CHuR", 0, 0,muRG)
            + 15598.5 * getSMEFTCoeff("CHuR", 1, 1,muRG)
            - 2951.74 * getSMEFTCoeff("CHdR", 0, 0,muRG)
            - 2940.03 * getSMEFTCoeff("CHdR", 1, 1,muRG)
            - 6238.49 * getSMEFTCoeff("CHdR", 2, 2,muRG)
            + 51319. * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + 51289.2 * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + 36755.6 * getSMEFTCoeff("CHq3R", 2, 2,muRG)
            - 60973.2 * getSMEFTCoeff("CHD",muRG)
            - 238821. * getSMEFTCoeff("CHWB",muRG)
            - 4.013 * delta_GF
            - 0.832 * deltaGzd6()
            );
            /*+ cWsch * (+41194.1 * getSMEFTCoeff("CHD")
            - 14774.7 * getSMEFTCoeff("CHWB")
            - 3.001 * delta_GF
            - 0.832 * deltaGzd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.1212) * getSMEFTCoeff("CHbox",muRG)
            + (0.057954) * getSMEFTCoeff("CHW",muRG)
            + (-0.12929) * getSMEFTCoeff("CHB",muRG)
            + (0.043672) * getSMEFTCoeff("CHD",muRG)
            + (-0.016284) * getSMEFTCoeff("CHWB",muRG)
            + (-0.019017) * getSMEFTCoeff("CHq1R", 0, 0,muRG)
            + (-0.019103) * getSMEFTCoeff("CHq1R", 1, 1,muRG)
            + (0.036608) * getSMEFTCoeff("CHq1R", 2, 2,muRG)
            + (0.051357) * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + (0.051276) * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + (0.036608) * getSMEFTCoeff("CHq3R", 2, 2,muRG)
            + (0.014886) * getSMEFTCoeff("CHuR", 0, 0,muRG)
            + (0.014851) * getSMEFTCoeff("CHuR", 1, 1,muRG)
            + (-0.002823638) * getSMEFTCoeff("CHdR", 0, 0,muRG)
            + (-0.002812766) * getSMEFTCoeff("CHdR", 1, 1,muRG)
            + (-0.00594515) * getSMEFTCoeff("CHdR", 2, 2,muRG)
            + (-0.181783) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.181783) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.18182) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.802) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-9.34 * deltaMz()
            + 16.613 * deltaMh()
            - 0.716 * deltaaMZ()
            + 2.838 * deltaGmu()))
            + cWsch * (cHSM * (-14.238 * deltaMz()
            + 16.613 * deltaMh()
            + 2.133 * deltaGmu()
            + 3.346 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2u2dRatio2()

const double NPSMEFTd6General::deltaGammaH2u2dRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2u2d)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2u2d)$/ $\Gamma(H\to 2u2d)_{\mathrm{SM}}$

Definition at line 30532 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014695) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.039324) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.033113) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (0.0022317) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.011348) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.00179) * pow(getSMEFTCoeffEW("CHq1R", 0, 0), 2.0)
                + (0.0017897) * pow(getSMEFTCoeffEW("CHq1R", 1, 1), 2.0)
                + (0.00113) * pow(getSMEFTCoeffEW("CHq1R", 2, 2), 2.0)
                + (0.00179) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                + (0.0017897) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                + (0.00113) * pow(getSMEFTCoeffEW("CHq3R", 2, 2), 2.0)
                + (0.001296) * pow(getSMEFTCoeffEW("CHuR", 0, 0), 2.0)
                + (0.0012961) * pow(getSMEFTCoeffEW("CHuR", 1, 1), 2.0)
                + (0.00049373) * pow(getSMEFTCoeffEW("CHdR", 0, 0), 2.0)
                + (0.00049057) * pow(getSMEFTCoeffEW("CHdR", 1, 1), 2.0)
                + (0.0011314) * pow(getSMEFTCoeffEW("CHdR", 2, 2), 2.0)
                + (0.011019) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.011019) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.011019) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (0.006886) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.015571) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (0.0016252) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.0019574) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (-0.002309) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0023147) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0044402) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0062245) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0062191) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0044402) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.0018054) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.0018013) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.0003419172) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.000340856) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.000721154) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.0147031) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0147031) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.014698) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0642138) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (-0.000834) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.0573053) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (0.0001529) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0001488) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0021791) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0016906) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0016234) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0021791) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.0001656) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.0001627) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.0002752) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.0068912) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0068912) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.006886) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.000459) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (0.033411) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (0.0019038) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0019508) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0057366) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0068118) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0067877) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0057366) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.00111553) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00111376) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.00031123) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.00030304) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.0006683) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.015629) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.015629) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.015571) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0027622) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (-0.0017088) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0017166) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0022723) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.003769) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0037624) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0022723) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.00107784) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00108799) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.00016963) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0001701) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.00046646) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.0052936) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0052936) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0052919) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0021911) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0017537) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0017338) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0021911) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.00248676) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00248368) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.00050869) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.00050349) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.0011318) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.0019662) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0019662) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0019574) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.000259) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.000154) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0016047) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00015498) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.0023037) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0023037) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.002309) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.000154) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0016123) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00015353) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.0023125) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0023125) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0023147) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00015503) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.00015329) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0022593) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.004436654) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.004436654) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0044402) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000259) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.000156) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.00622384) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00622384) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0062245) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000154) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.00621958) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00621958) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0062191) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.004436654) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.004436654) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0044402) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00180408) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00180408) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0018054) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00180249) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00180249) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0018013) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00034209) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00034209) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0003419172) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00034101) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00034101) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.000340856) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0007216) * getSMEFTCoeffEW("CHdR", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0007216) * getSMEFTCoeffEW("CHdR", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.000721154) * getSMEFTCoeffEW("CHdR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.01104) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0220565) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0220565) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.66) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.0999) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (-0.0604) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.1133) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (-0.0362) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.0245) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (0.01605) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.01555) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0326) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0458) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0465) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0326) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.01307) * deltaGzd6() * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.01299) * deltaGzd6() * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.0025172) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0023751) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.005281) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.14682) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.14682) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.1499) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaH2u2uRatio1()

const double NPSMEFTd6General::deltaGammaH2u2uRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2u2u)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2u2u)$/ $\Gamma(H\to 2u2u)_{\mathrm{SM}}$

Definition at line 29949 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121242. * getSMEFTCoeff("CHbox",muRG)
            - 147406. * getSMEFTCoeff("CHB",muRG)
            + 73926.6 * getSMEFTCoeff("CHW",muRG)
            - 71435.3 * (getSMEFTCoeff("CHq1R", 0, 0,muRG) - getSMEFTCoeff("CHq3R", 0, 0,muRG))
            - 71331.9 * (getSMEFTCoeff("CHq1R", 1, 1,muRG) - getSMEFTCoeff("CHq3R", 1, 1,muRG))
            + 31760.4 * getSMEFTCoeff("CHuR", 0, 0,muRG)
            + 31666.6 * getSMEFTCoeff("CHuR", 1, 1,muRG)
            - 66129.8 * getSMEFTCoeff("CHD",muRG)
            - 270623. * getSMEFTCoeff("CHWB",muRG)
            - 4.182 * delta_GF
            - 0.827 * deltaGzd6()
            );
            /*+ cWsch * (+53075.8 * getSMEFTCoeff("CHD")
            - 9701.32 * getSMEFTCoeff("CHWB")
            - 3.002 * delta_GF
            - 0.827 * deltaGzd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.121221) * getSMEFTCoeff("CHbox",muRG)
            + (0.0747) * getSMEFTCoeff("CHW",muRG)
            + (-0.148967) * getSMEFTCoeff("CHB",muRG)
            + (0.057368) * getSMEFTCoeff("CHD",muRG)
            + (-0.011196) * getSMEFTCoeff("CHWB",muRG)
            + (-0.071576) * getSMEFTCoeff("CHq1R", 0, 0,muRG)
            + (-0.071476) * getSMEFTCoeff("CHq1R", 1, 1,muRG)
            + (0.071574) * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + (0.071473) * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + (0.030282) * getSMEFTCoeff("CHuR", 0, 0,muRG)
            + (0.030178) * getSMEFTCoeff("CHuR", 1, 1,muRG)
            + (-0.181763) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.181763) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.18186) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.801) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-9.043 * deltaMz()
            + 16.707 * deltaMh()
            - 0.908 * deltaaMZ()
            + 3.065 * deltaGmu()))
            + cWsch * (cHSM * (-15.04 * deltaMz()
            + 16.707 * deltaMh()
            + 2.177 * deltaGmu()
            + 4.215 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2u2uRatio2()

const double NPSMEFTd6General::deltaGammaH2u2uRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2u2u)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2u2u)$/ $\Gamma(H\to 2u2u)_{\mathrm{SM}}$

Definition at line 30015 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014716) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.06274) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.09129) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (0.00513) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.026875) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.002647) * pow(getSMEFTCoeffEW("CHq1R", 0, 0), 2.0)
                + (0.0026461) * pow(getSMEFTCoeffEW("CHq1R", 1, 1), 2.0)
                + (0.002647) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                + (0.0026461) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                + (0.002648) * pow(getSMEFTCoeffEW("CHuR", 0, 0), 2.0)
                + (0.0026461) * pow(getSMEFTCoeffEW("CHuR", 1, 1), 2.0)
                + (0.011037) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.011037) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.011034) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (0.009076) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.018068) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (0.0032896) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.001344) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (-0.00868253) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.00867303) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0086747) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.00867) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0036743) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.0036607) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.0147042) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0147042) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.014712) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0860094) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (0.004936) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.0862249) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (-0.0043116) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0041397) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0043074) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.00415) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0009706) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.0009075) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.009046) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.009046) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.009076) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0086983) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (0.013604) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (0.011699) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.01154) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0117092) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.011543) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0032871) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.0032289) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.01807) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.01807) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.018068) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0023272) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (-0.00645833) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.00643743) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0064561) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0064367) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00182137) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00184267) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.0069681) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0069681) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0069646) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0023122) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0022494) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0023093) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0022472) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00547273) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00542879) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.001348) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.001348) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.001344) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000569) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.005300265) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00057357) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00023902) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.008675) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.008675) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00868253) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00057357) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00529391) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00024275) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.0086683) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0086683) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00867303) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000569) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.00023907) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.0086817) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0086817) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0086747) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00024302) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.0086672) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0086672) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.00867) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000101) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.00367303) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00367303) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0036743) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00365915) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00365915) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0036607) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.01099) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0220568) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0220568) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.7) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.0987) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (-0.0818) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.1374) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (-0.0456) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.024) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (0.06193) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.06291) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0627) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0646) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0272) * deltaGzd6() * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.02668) * deltaGzd6() * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.14658) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.14658) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.1481) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaH2udRatio1()

const double NPSMEFTd6General::deltaGammaH2udRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2ud)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2ud)$/ $\Gamma(H\to 2ud)_{\mathrm{SM}}$

Definition at line 33777 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121425. * getSMEFTCoeff("CHbox",muRG)
            - 3244.8 * getSMEFTCoeff("CHB",muRG)
            - 88391.2 * getSMEFTCoeff("CHW",muRG)
            - 55282. * getSMEFTCoeff("CHG",muRG)
            - 23.442 * getSMEFTCoeff("CHq1R", 0, 0,muRG)
            - 22.98 * getSMEFTCoeff("CHq1R", 1, 1,muRG)
            + 559.485 * getSMEFTCoeff("CHuR", 0, 0,muRG)
            + 560.558 * getSMEFTCoeff("CHuR", 1, 1,muRG)
            - 217.102 * getSMEFTCoeff("CHdR", 0, 0,muRG)
            - 218.04 * getSMEFTCoeff("CHdR", 1, 1,muRG)
            + 68556.8 * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + 68783.1 * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            - 199535. * getSMEFTCoeff("CHD",muRG)
            - 375669. * getSMEFTCoeff("CHWB",muRG)
            - 4.696 * delta_GF
            - 0.026 * deltaGzd6()
            - 13.64 * deltaMwd6()
            - 0.944 * deltaGwd6()
            );
            /*+ cWsch * (-28852.8 * getSMEFTCoeff("CHD")
            - 1306.57 * getSMEFTCoeff("CHWB")
            - 3.002 * delta_GF
            - 0.026 * deltaGzd6()
            - 0.944 * deltaGwd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.12135) * getSMEFTCoeff("CHbox",muRG)
            + (-0.0851047) * getSMEFTCoeff("CHW",muRG)
            + (-0.0045438) * getSMEFTCoeff("CHB",muRG)
            + (-0.02822615) * getSMEFTCoeff("CHD",muRG)
            + (-0.0017067) * getSMEFTCoeff("CHWB",muRG)
            + (-0.05868) * getSMEFTCoeff("CHG",muRG)
            + (0.070123) * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + (0.069746) * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + (0.0006591) * getSMEFTCoeff("CHuR", 0, 0,muRG)
            + (0.00065708) * getSMEFTCoeff("CHuR", 1, 1,muRG)
            + (-0.000256626) * getSMEFTCoeff("CHdR", 0, 0,muRG)
            + (-0.000252814) * getSMEFTCoeff("CHdR", 1, 1,muRG)
            + (-0.181971) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.181971) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.182) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.895) * deltaGwd6()
            + (-0.0262) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-12.708 * deltaMz()
            + 14.393 * deltaMh()
            + 1.82 * deltaaMZ()
            + 0.188 * deltaGmu()))
            + cWsch * (cHSM * (-0.441 * deltaMz()
            - 8.601 * deltaMw()
            + 14.393 * deltaMh()
            + 2.022 * deltaGmu()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)  
    // Dominated by CC => Use HWW uncertainty
    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
}

◆ deltaGammaH2udRatio2()

const double NPSMEFTd6General::deltaGammaH2udRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2ud)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2ud)$/ $\Gamma(H\to 2ud)_{\mathrm{SM}}$

Definition at line 33854 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014695) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.000994) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.015278) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (0.0010088) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.005252) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (11.456) * pow(getSMEFTCoeffEW("CHG"), 2.0)
                + (0.0029759) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                + (0.0029646) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                + (0.011018) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.011018) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.011018) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (-0.01033512) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.00055115) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (-0.007099838) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.00020639) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (-0.007042) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHG")
                + (0.0085086) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0084775) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.01470364) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.01470364) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.014725) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0126698) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (0.0027047) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.01297797) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (-0.0006016) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHG")
                + (-0.00851159) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00850078) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.010333) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.010333) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.01033512) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00015239) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (0.0031685) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (-0.00038338) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00038161) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0005526) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0005526) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0005511) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0017583) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHG")
                + (-0.00188801) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00188114) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0034285) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0034285) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00342549) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00013828) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00013656) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.000111953) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.0001115399) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.00020662) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00020667) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00020631) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0009234) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0009279) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.003528) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.003528) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0035169) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00851568) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00851568) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0085086) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.008478119) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.008478119) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0084775) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0111) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.02206664) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.02206664) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.74) * pow(deltaGwd6(), 2.0) + (0.0087) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.1123) * deltaGwd6() * getSMEFTCoeffEW("CHbox")
                + (0.08154) * deltaGwd6() * getSMEFTCoeffEW("CHW")
                + (9.3e-05) * deltaGwd6() * getSMEFTCoeffEW("CHB")
                + (0.028249) * deltaGwd6() * getSMEFTCoeffEW("CHD")
                + (3.7e-05) * deltaGwd6() * getSMEFTCoeffEW("CHWB")
                + (-0.0106) * deltaGwd6() * getSMEFTCoeffEW("CHG")
                + (-9e-06) * deltaGwd6() * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (3e-06) * deltaGwd6() * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0653) * deltaGwd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0654) * deltaGwd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (3e-06) * deltaGwd6() * getSMEFTCoeffEW("CHuR", 0, 0)
                + (8.3e-06) * deltaGwd6() * getSMEFTCoeffEW("CHuR", 1, 1)
                + (2.25e-06) * deltaGwd6() * getSMEFTCoeffEW("CHdR", 0, 0)
                + (1.38e-06) * deltaGwd6() * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.16645) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.16645) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.1685) * deltaGwd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0039) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (-0.002882) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.005316) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (-0.0013023) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.001036) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (-0.005) * deltaGzd6() * getSMEFTCoeffEW("CHG")
                + (5.1e-05) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (9.65e-05) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.00263) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00228) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0006) * deltaGzd6() * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.000582) * deltaGzd6() * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.0002321) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0002269) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.00641) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00641) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0059) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaH2v2dRatio1()

const double NPSMEFTd6General::deltaGammaH2v2dRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2v2d)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2v2d)$/ $\Gamma(H\to 2v2d)_{\mathrm{SM}}$

Definition at line 31671 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121140. * getSMEFTCoeff("CHbox",muRG)
            - 57872.8 * getSMEFTCoeff("CHB",muRG)
            - 4371.77 * getSMEFTCoeff("CHW",muRG)
            - 18746.1 * (getSMEFTCoeff("CHl1R", 0, 0,muRG) - getSMEFTCoeff("CHl3R", 0, 0,muRG))
            - 18746.1 * (getSMEFTCoeff("CHl1R", 1, 1,muRG) - getSMEFTCoeff("CHl3R", 1, 1,muRG))
            - 18868.3 * (getSMEFTCoeff("CHl1R", 2, 2,muRG) - getSMEFTCoeff("CHl3R", 2, 2,muRG))
            + 23856.6 * (getSMEFTCoeff("CHq1R", 0, 0,muRG) + getSMEFTCoeff("CHq3R", 0, 0,muRG))
            + 23828.1 * (getSMEFTCoeff("CHq1R", 1, 1,muRG) + getSMEFTCoeff("CHq3R", 1, 1,muRG))
            + 23481.4 * (getSMEFTCoeff("CHq1R", 2, 2,muRG) + getSMEFTCoeff("CHq3R", 2, 2,muRG))
            - 4335.75 * getSMEFTCoeff("CHdR", 0, 0,muRG)
            - 4341.01 * getSMEFTCoeff("CHdR", 1, 1,muRG)
            - 4000. * getSMEFTCoeff("CHdR", 2, 2,muRG)
            - 42945.7 * getSMEFTCoeff("CHD",muRG)
            - 113953. * getSMEFTCoeff("CHWB",muRG)
            - 3.412 * delta_GF
            - 0.842 * deltaGzd6()
            );
            /*+ cWsch * (-837.5 * getSMEFTCoeff("CHD")
            - 21725.9 * getSMEFTCoeff("CHWB")
            - 2.996 * delta_GF
            - 0.842 * deltaGzd6()
            ));*/
            
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.12129) * getSMEFTCoeff("CHbox",muRG)
            + (-0.005765) * getSMEFTCoeff("CHW",muRG)
            + (-0.0553328) * getSMEFTCoeff("CHB",muRG)
            + (-0.0003856) * getSMEFTCoeff("CHD",muRG)
            + (-0.0226353) * getSMEFTCoeff("CHWB",muRG)
            + (-0.01872246) * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            + (-0.01856267) * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            + (-0.01867078) * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            + (-0.161664) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.1624422) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.01871) * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + (0.023787) * getSMEFTCoeff("CHq1R", 0, 0,muRG)
            + (0.023795) * getSMEFTCoeff("CHq1R", 1, 1,muRG)
            + (0.023434) * getSMEFTCoeff("CHq1R", 2, 2,muRG)
            + (0.023787) * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + (0.023795) * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + (0.023434) * getSMEFTCoeff("CHq3R", 2, 2,muRG)
            + (-0.00413664) * getSMEFTCoeff("CHdR", 0, 0,muRG)
            + (-0.00413066) * getSMEFTCoeff("CHdR", 1, 1,muRG)
            + (-0.00380964) * getSMEFTCoeff("CHdR", 2, 2,muRG)
            + (0.1819) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.826) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-10.269 * deltaMz()
            + 15.979 * deltaMh()
            - 0.143 * deltaaMZ()
            + 2.286 * deltaGmu()))
            + cWsch * (cHSM * (-11.132 * deltaMz()
            + 15.979 * deltaMh()
            + 2.144 * deltaGmu()
            + 0.598 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2v2dRatio2()

const double NPSMEFTd6General::deltaGammaH2v2dRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2v2d)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2v2d)$/ $\Gamma(H\to 2v2d)_{\mathrm{SM}}$

Definition at line 31749 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.01475) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.004384) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (-0.0006489) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (-0.00113902) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.0015868) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.00048923) * pow(getSMEFTCoeffEW("CHl1R", 0, 0), 2.0)
                + (0.0004894) * pow(getSMEFTCoeffEW("CHl1R", 1, 1), 2.0)
                + (0.00048977) * pow(getSMEFTCoeffEW("CHl1R", 2, 2), 2.0)
                + (0.00924) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.009278) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.00048977) * pow(getSMEFTCoeffEW("CHl3R", 2, 2), 2.0)
                + (0.0007335) * pow(getSMEFTCoeffEW("CHq1R", 0, 0), 2.0)
                + (0.0007336) * pow(getSMEFTCoeffEW("CHq1R", 1, 1), 2.0)
                + (0.0007284) * pow(getSMEFTCoeffEW("CHq1R", 2, 2), 2.0)
                + (0.0007335) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                + (0.0007336) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                + (0.0007284) * pow(getSMEFTCoeffEW("CHq3R", 2, 2), 2.0)
                + (0.0007359) * pow(getSMEFTCoeffEW("CHdR", 0, 0), 2.0)
                + (0.0007354) * pow(getSMEFTCoeffEW("CHdR", 1, 1), 2.0)
                + (0.00073) * pow(getSMEFTCoeffEW("CHdR", 2, 2), 2.0)
                + (0.01106) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (-0.0006919) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.00671583) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (-0.00372275) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.00273962) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (-0.0022930912) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.002295757) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.002294138) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.01240966) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.012412956) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0022956) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0028811) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0028831) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0028413) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0028811) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0028831) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0028413) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.00050295) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.0005030348) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.000462466) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.014712) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00987) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (-0.003878) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.01842346) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (-0.00021) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.000208) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.000208) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0008856) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0009176) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.00021571) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00160087) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.00160191) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.00154323) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.00160087) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00160191) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00154323) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.00039676) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0003971) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.00033274) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.0006919) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0056261) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (0.0096878) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (0.0020444) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0020531) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0020521) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0046779) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0046784) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.002059516) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.0005872) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.000586691) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.00056713) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0005872) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.000586691) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00056713) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.00671583) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0001361) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (-0.00065058) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.000649782) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.00065018) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.00069657) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00069682) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.00065069) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.00041577) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.00041586) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.00037775) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.00041577) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.00041586) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.00037775) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.00044187) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.00044214) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.00047114) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.0012559) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.00124975) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0012523) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0014392) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0014379) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00125923) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.000512984) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.000513525) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.000476106) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.000512984) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.000513525) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.000476106) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.00056571) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.00056548) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.0005314) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.00273962) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00131131) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0022936) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0022930912) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0022951) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00131083) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.002295757) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0022956) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0022956) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0009841401) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.002294138) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00636) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.002308) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.0028265) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.00282878) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.002788849) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0028265) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00282878) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.002788849) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.00049339) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.00049359) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.00045796) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.01974979) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.002339) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.002827586) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.002830241) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.00279057) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.002827586) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.002830241) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00279057) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.00049346) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0004937) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.00045793) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.01975021) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0022956) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0014696) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0028811) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0014696) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0028831) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0014591) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.0028413) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0028811) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0028831) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0028413) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00050295) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0005030348) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.000462466) * getSMEFTCoeffEW("CHdR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.75) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.101) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (-0.00041) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.048287) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (0.00036) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.02179) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (0.0149079) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0172908) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.017088) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.13395) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.1303) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.01742) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.02056) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0189) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.02124) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.02056) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0189) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.02124) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.003758) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.003796) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.003317) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.152) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaH2v2uRatio1()

const double NPSMEFTd6General::deltaGammaH2v2uRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2v2u)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2v2u)$/ $\Gamma(H\to 2v2u)_{\mathrm{SM}}$

Definition at line 31404 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121248. * getSMEFTCoeff("CHbox",muRG)
            - 76316.6 * getSMEFTCoeff("CHB",muRG)
            + 13981.5 * getSMEFTCoeff("CHW",muRG)
            - 19052.2 * (getSMEFTCoeff("CHl1R", 0, 0,muRG) - getSMEFTCoeff("CHl3R", 0, 0,muRG))
            - 19081.3 * (getSMEFTCoeff("CHl1R", 1, 1,muRG) - getSMEFTCoeff("CHl3R", 1, 1,muRG))
            - 19088.9 * (getSMEFTCoeff("CHl1R", 2, 2,muRG) - getSMEFTCoeff("CHl3R", 2, 2,muRG))
            - 37234.1 * (getSMEFTCoeff("CHq1R", 0, 0,muRG) - getSMEFTCoeff("CHq3R", 0, 0,muRG))
            - 37155.9 * (getSMEFTCoeff("CHq1R", 1, 1,muRG) - getSMEFTCoeff("CHq3R", 1, 1,muRG))
            + 16564.7 * getSMEFTCoeff("CHuR", 0, 0,muRG)
            + 16487.2 * getSMEFTCoeff("CHuR", 1, 1,muRG)
            - 48203. * getSMEFTCoeff("CHD",muRG)
            - 150929. * getSMEFTCoeff("CHWB",muRG)
            - 3.589 * delta_GF
            - 0.849 * deltaGzd6()
            );
            /*+ cWsch * (+11461.3 * getSMEFTCoeff("CHD")
            - 20220.2 * getSMEFTCoeff("CHWB")
            - 2.998 * delta_GF
            - 0.849 * deltaGzd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.12122) * getSMEFTCoeff("CHbox",muRG)
            + (0.01598) * getSMEFTCoeff("CHW",muRG)
            + (-0.074959) * getSMEFTCoeff("CHB",muRG)
            + (0.013404) * getSMEFTCoeff("CHD",muRG)
            + (-0.021103) * getSMEFTCoeff("CHWB",muRG)
            + (-0.01884082) * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            + (-0.01874224) * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            + (-0.01879955) * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            + (-0.161822) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.1613675) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.018957) * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + (-0.037156) * getSMEFTCoeff("CHq1R", 0, 0,muRG)
            + (-0.0371722) * getSMEFTCoeff("CHq1R", 1, 1,muRG)
            + (0.037258) * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + (0.037209) * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + (0.015779) * getSMEFTCoeff("CHuR", 0, 0,muRG)
            + (0.015702) * getSMEFTCoeff("CHuR", 1, 1,muRG)
            + (0.1818) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.832) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-9.867 * deltaMz()
            + 15.889 * deltaMh()
            - 0.28 * deltaaMZ()
            + 2.519 * deltaGmu()))
            + cWsch * (cHSM * (-11.908 * deltaMz()
            + 15.889 * deltaMh()
            + 2.169 * deltaGmu()
            + 1.303 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2v2uRatio2()

const double NPSMEFTd6General::deltaGammaH2v2uRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2v2u)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2v2u)$/ $\Gamma(H\to 2v2u)_{\mathrm{SM}}$

Definition at line 31477 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014683) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.029977) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.020534) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (0.0011316) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.009588) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.00049619) * pow(getSMEFTCoeffEW("CHl1R", 0, 0), 2.0)
                + (0.00049702) * pow(getSMEFTCoeffEW("CHl1R", 1, 1), 2.0)
                + (0.00049647) * pow(getSMEFTCoeffEW("CHl1R", 2, 2), 2.0)
                + (0.00922) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.00919) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.00049647) * pow(getSMEFTCoeffEW("CHl3R", 2, 2), 2.0)
                + (0.0013928) * pow(getSMEFTCoeffEW("CHq1R", 0, 0), 2.0)
                + (0.0013902) * pow(getSMEFTCoeffEW("CHq1R", 1, 1), 2.0)
                + (0.0013928) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                + (0.0013902) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                + (0.0013945) * pow(getSMEFTCoeffEW("CHuR", 0, 0), 2.0)
                + (0.0013955) * pow(getSMEFTCoeffEW("CHuR", 1, 1), 2.0)
                + (0.01101) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (0.001982) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.0090937) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (-0.0020315) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.0025573) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (-0.002318106) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.002317968) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.01237941) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.01238009) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0023188) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00451966) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.00451184) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0045183) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0045101) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0019117) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.0019033) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.0147057) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0561529) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (0.0005954) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.0455873) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (-0.0010602) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.001113) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.001132) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.001144) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.001023) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0010671) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0023205) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0023067) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.00230254) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00228524) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00149435) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00149032) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.001982) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0003054) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (0.034986) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (0.0028311) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0028277) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0028398) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.006269) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0062789) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00283266) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0011441) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.00114) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.001135831) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00113128) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0090937) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.000408) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (-0.0009051) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.00090638) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.00090555) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.0007383) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0007345) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.00090609) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00162977) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.001624214) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0016305) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0016236) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00167945) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00168335) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.0016461) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0014831) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0014813) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0014901) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.001034) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0010168) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00148265) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.000102) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0021338) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00214234) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.0025573) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00132225) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0023183) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.002318106) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.002319) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0013223) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0023188) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0023188) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.000997117) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.002317968) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00638) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00233) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0044333) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0044255) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.00443452) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0044265) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.001876252) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.0018688) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.0197481) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0023) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0044334) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0044253) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.00443484) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00442866) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.001875899) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00186879) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.01972415) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0023188) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00279155) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00451966) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00278867) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00451184) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0045183) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0045101) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0019117) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0019033) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.757) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.099) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (-0.01511) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.07347) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (-0.01184) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.02039) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (0.01399) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.015557) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.01326) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.13487) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.13114) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.01462) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.03421) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.03301) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0335) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.034) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0134) * deltaGzd6() * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.01395) * deltaGzd6() * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.148) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaH2v2vRatio1()

const double NPSMEFTd6General::deltaGammaH2v2vRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2v2v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2v2v)$/ $\Gamma(H\to 2v2v)_{\mathrm{SM}}$

Definition at line 29223 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121344. * getSMEFTCoeff("CHbox",muRG)
            - 14021.1 * getSMEFTCoeff("CHB",muRG)
            - 46733.1 * getSMEFTCoeff("CHW",muRG)
            - 39647.5 * (getSMEFTCoeff("CHl1R", 0, 0,muRG) - getSMEFTCoeff("CHl3R", 0, 0,muRG))
            - 39690.9 * (getSMEFTCoeff("CHl1R", 1, 1,muRG) - getSMEFTCoeff("CHl3R", 1, 1,muRG))
            - 39622.3 * (getSMEFTCoeff("CHl1R", 2, 2,muRG) - getSMEFTCoeff("CHl3R", 2, 2,muRG))
            - 30324.8 * getSMEFTCoeff("CHD",muRG)
            - 25575.1 * getSMEFTCoeff("CHWB",muRG)
            - 3.003 * delta_GF
            - 0.847 * deltaGzd6()
            );
            /*+ cWsch * (-30324.8 * getSMEFTCoeff("CHD")
            - 25575.1 * getSMEFTCoeff("CHWB")
            - 3.003 * delta_GF
            - 0.847 * deltaGzd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.121319) * getSMEFTCoeff("CHbox",muRG)
            + (-0.0473339) * getSMEFTCoeff("CHW",muRG)
            + (-0.01358688) * getSMEFTCoeff("CHB",muRG)
            + (-0.0303464) * getSMEFTCoeff("CHD",muRG)
            + (-0.0253525) * getSMEFTCoeff("CHWB",muRG)
            + (-0.039647621) * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            + (-0.03965331) * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            + (-0.03967702) * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            + (-0.14240624) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.14220981) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.03968) * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + (0.18201) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.825) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-10.87 * deltaMz()
            + 15.738 * deltaMh()
            + 0.292 * deltaaMZ()
            + 1.853 * deltaGmu()))
            + cWsch * (cHSM * (-8.952 * deltaMz()
            + 15.738 * deltaMh()
            + 2.164 * deltaGmu()
            - 1.149 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH2v2vRatio2()

const double NPSMEFTd6General::deltaGammaH2v2vRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 2v2v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 2v2v)$/ $\Gamma(H\to 2v2v)_{\mathrm{SM}}$

Definition at line 29286 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += cWsch * (
                +(0.014715) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (-0.00492776) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (-0.00157955) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (-0.00091971) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (-0.00059168) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.0010428) * pow(getSMEFTCoeffEW("CHl1R", 0, 0), 2.0)
                + (0.0010396) * pow(getSMEFTCoeffEW("CHl1R", 1, 1), 2.0)
                + (0.0010413) * pow(getSMEFTCoeffEW("CHl1R", 2, 2), 2.0)
                + (0.007271) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.007277) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.0010413) * pow(getSMEFTCoeffEW("CHl3R", 2, 2), 2.0)
                + (0.011034) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (-0.00573523) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.001647119) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (-0.00735786) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.00307385) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (-0.004812955) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.004812852) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.004808936) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.009915377) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00990658) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.004811) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0147117) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00046464) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (0.00143336) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.00374267) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (0.0028723) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0028722) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.002873) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0028623) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0028624) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00287322) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00573523) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0022564) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (-0.001287724) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (0.00082433) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.00082434) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.00082455) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.00082142) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00082156) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.000824707) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.001647119) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0024896) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (0.0037252) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0037252) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.003677513) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00153868) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.00153874) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.00153902) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0015333) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00153356) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00153952) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00307385) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0001357) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0001341) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.002721) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0046768) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.000131172) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.004812955) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0001394) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0046772) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0027206) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.000131214) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.004812852) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.004674) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0046785) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0020839) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.004808936) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.001553) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.004677) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.017264274) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.004686) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.017274024) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.004811) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.7) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.1008) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (0.03623) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.01039) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (0.02495) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.01941) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (0.0363) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.03548) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.03566) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.11278) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.11353) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0354) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.1512) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaH4dRatio1()

const double NPSMEFTd6General::deltaGammaH4dRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4d)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4d)$/ $\Gamma(H\to 4d)_{\mathrm{SM}}$

Definition at line 32941 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121248. * getSMEFTCoeff("CHbox",muRG)
            - 106312. * getSMEFTCoeff("CHB",muRG)
            + 37722.3 * getSMEFTCoeff("CHW",muRG)
            - 368494. * getSMEFTCoeff("CHG",muRG)
            + 43669.1 * (getSMEFTCoeff("CHq1R", 0, 0,muRG) + getSMEFTCoeff("CHq3R", 0, 0,muRG))
            + 43649.7 * (getSMEFTCoeff("CHq1R", 1, 1,muRG) + getSMEFTCoeff("CHq3R", 1, 1,muRG))
            + 45003.6 * (getSMEFTCoeff("CHq1R", 2, 2,muRG) + getSMEFTCoeff("CHq3R", 2, 2,muRG))
            - 7637.9 * getSMEFTCoeff("CHdR", 0, 0,muRG)
            - 7633.36 * getSMEFTCoeff("CHdR", 1, 1,muRG)
            - 7294.61 * getSMEFTCoeff("CHdR", 2, 2,muRG)
            - 56026.9 * getSMEFTCoeff("CHD",muRG)
            - 199805. * getSMEFTCoeff("CHWB",muRG)
            - 3.841 * delta_GF
            - 0.778 * deltaGzd6()
            );
            /*+ cWsch * (+29594.4 * getSMEFTCoeff("CHD")
            - 12377.7 * getSMEFTCoeff("CHWB")
            - 2.995 * delta_GF
            - 0.778 * deltaGzd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.12101) * getSMEFTCoeff("CHbox",muRG)
            + (0.035301) * getSMEFTCoeff("CHW",muRG)
            + (-0.1036126) * getSMEFTCoeff("CHB",muRG)
            + (0.030428) * getSMEFTCoeff("CHD",muRG)
            + (-0.013792) * getSMEFTCoeff("CHWB",muRG)
            + (-0.36157) * getSMEFTCoeff("CHG",muRG)
            + (0.043464) * getSMEFTCoeff("CHq1R", 0, 0,muRG)
            + (0.043459) * getSMEFTCoeff("CHq1R", 1, 1,muRG)
            + (0.044816) * getSMEFTCoeff("CHq1R", 2, 2,muRG)
            + (0.043464) * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + (0.043459) * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + (0.044816) * getSMEFTCoeff("CHq3R", 2, 2,muRG)
            + (-0.0072915) * getSMEFTCoeff("CHdR", 0, 0,muRG)
            + (-0.0072923) * getSMEFTCoeff("CHdR", 1, 1,muRG)
            + (-0.00694917) * getSMEFTCoeff("CHdR", 2, 2,muRG)
            + (-0.181499) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.181499) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.18154) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.786) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-9.19 * deltaMz()
            + 16.387 * deltaMh()
            - 0.596 * deltaaMZ()
            + 2.807 * deltaGmu()))
            + cWsch * (cHSM * (-13.077 * deltaMz()
            + 16.387 * deltaMh()
            + 2.268 * deltaGmu()
            + 2.743 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH4dRatio2()

const double NPSMEFTd6General::deltaGammaH4dRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4d)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4d)$/ $\Gamma(H\to 4d)_{\mathrm{SM}}$

Definition at line 33014 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014663) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.012757) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.001286) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (-0.00052975) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.0018933) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (10.635) * pow(getSMEFTCoeffEW("CHG"), 2.0)
                + (0.0013812) * pow(getSMEFTCoeffEW("CHq1R", 0, 0), 2.0)
                + (0.0013804) * pow(getSMEFTCoeffEW("CHq1R", 1, 1), 2.0)
                + (0.0014343) * pow(getSMEFTCoeffEW("CHq1R", 2, 2), 2.0)
                + (0.0013812) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                + (0.0013804) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                + (0.0014343) * pow(getSMEFTCoeffEW("CHq3R", 2, 2), 2.0)
                + (0.0012767) * pow(getSMEFTCoeffEW("CHdR", 0, 0), 2.0)
                + (0.0012783) * pow(getSMEFTCoeffEW("CHdR", 1, 1), 2.0)
                + (0.0013171) * pow(getSMEFTCoeffEW("CHdR", 2, 2), 2.0)
                + (0.011) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.011) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.011) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (0.0042683) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.0125738) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (-0.0016726) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (-0.043734) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHG")
                + (0.0052642) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0052762) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0054406) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0052642) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0052762) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0054406) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.000884882) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.000883694) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.000843951) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.01468531) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.01468531) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.01468) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.01805505) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (-0.0064336) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.02863887) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (-0.003268) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHG")
                + (0.0004845) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.000485) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0008983) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0004845) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.000485) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0008983) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.00010197) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.00010131) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.0042711) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0042713) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0042682) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.006856) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (0.016282) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (0.013229) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHG")
                + (-0.0047668) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.00476478) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.00533894) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0047668) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00476478) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00533894) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.00051711) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.00051703) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.00050983) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.012561) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.012561) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0125738) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0023965) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (0.0022286) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0022325) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0024145) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0022286) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0022325) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0024145) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.00054611) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.00054673) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.00062679) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (-0.0036907) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0036907) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0036904) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0148432) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHG")
                + (-0.00193883) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.00193998) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.00216367) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.00193883) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00193998) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00216367) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.001208) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0012071) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.001218) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.0016683) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0016679) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.001673) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0036955) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0036986) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0039625) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0036955) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0036986) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0039625) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.0006428) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0006448) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.021874) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.021874) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0218734) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0027621) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.005281107) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.005281107) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0052642) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0027657) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.005268493) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.005268493) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0052762) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0028667) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (-0.005440848) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.005440848) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0054406) * getSMEFTCoeffEW("CHq1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.005281107) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.005281107) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0052642) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.005268493) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.005268493) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0052762) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.005440848) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.005440848) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0054406) * getSMEFTCoeffEW("CHq3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00088499) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00088499) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.000884882) * getSMEFTCoeffEW("CHdR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00088467) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00088467) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.000883694) * getSMEFTCoeffEW("CHdR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00084416) * getSMEFTCoeffEW("CHdR", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.00084416) * getSMEFTCoeffEW("CHdR", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.000843951) * getSMEFTCoeffEW("CHdR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.01103) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.02201481) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.02201481) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.75) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.0906) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (-0.0398) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.0836) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (-0.0216) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.02187) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (-0.0128) * deltaGzd6() * getSMEFTCoeffEW("CHG")
                + (-0.0362) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0371) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0369) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (-0.0362) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0371) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0369) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.006371) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.006501) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 1, 1)
                + (0.006169) * deltaGzd6() * getSMEFTCoeffEW("CHdR", 2, 2)
                + (0.1413) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.1413) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.1361) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaH4eRatio1()

const double NPSMEFTd6General::deltaGammaH4eRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4e)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4e)$/ $\Gamma(H\to 4e)_{\mathrm{SM}}$

Definition at line 32311 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+121313. * getSMEFTCoeff("CHbox",muRG)
            - 101223. * getSMEFTCoeff("CHB",muRG)
            - 25774.5 * getSMEFTCoeff("CHW",muRG)
            + 122287. * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 0, 0,muRG))
            - 104859. * getSMEFTCoeff("CHeR", 0, 0,muRG)
            + cAsch * (-43133.2 * getSMEFTCoeff("CHD",muRG)
            - 82523.3 * getSMEFTCoeff("CHWB",muRG)
            - 3.424 * delta_GF
            - 0.754 * deltaGzd6())
            + cWsch * (-321.416 * getSMEFTCoeff("CHD",muRG)
            + 10203.3 * getSMEFTCoeff("CHWB",muRG)
            - 3. * delta_GF
            - 0.754 * deltaGzd6())
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (cAsch * (-9.739 * deltaMz()
            + 15.858 * deltaMh()
            - 0.16 * deltaaMZ()
            + 2.408 * deltaGmu())
            + cWsch * (-10.859 * deltaMz()
            + 15.858 * deltaMh()
            + 2.236 * deltaGmu()
            + 0.749 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH4eRatio2()

const double NPSMEFTd6General::deltaGammaH4eRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4e)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4e)$/ $\Gamma(H\to 4e)_{\mathrm{SM}}$

Definition at line 32352 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaH4fCCRatio1()

const double NPSMEFTd6General::deltaGammaH4fCCRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4f, CC)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4f, CC)$/ $\Gamma(H\to 4f, CC)_{\mathrm{SM}}$

Definition at line 34694 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    
    // SM decay widths (from MG simulations) 
    double wHLvvLSM = 6.318e-05, wHudduSM = 0.0001716, wHLvudSM = 0.0003606;
    double wH2udSM = 0.0001758, wH2LvSM = 3.164e-05;
 
    // Sum
    double wH4fSM = wHLvvLSM + wHudduSM + wHLvudSM + wH2udSM + wH2LvSM;
 
    dwidth += (wHLvvLSM * deltaGammaHLvvLRatio1() + wHudduSM * deltaGammaHudduRatio1() + wHLvudSM * deltaGammaHLvudRatio1() +
            wH2udSM * deltaGammaH2udRatio1() + wH2LvSM * deltaGammaH2LvRatio1()) / wH4fSM;
    
    return dwidth;
}

◆ deltaGammaH4fCCRatio2()

const double NPSMEFTd6General::deltaGammaH4fCCRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4f, CC)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4f, CC)$/ $\Gamma(H\to 4f, CC)_{\mathrm{SM}}$

Definition at line 34710 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        // SM decay widths (from MG simulations)
        double wHLvvLSM = 6.318e-05, wHudduSM = 0.0001716, wHLvudSM = 0.0003606;
        double wH2udSM = 0.0001758, wH2LvSM = 3.164e-05;
 
        // Sum
        double wH4fSM = wHLvvLSM + wHudduSM + wHLvudSM + wH2udSM + wH2LvSM;
 
        //Contributions that are quadratic in the effective coefficients
        dwidth += (wHLvvLSM * deltaGammaHLvvLRatio2() + wHudduSM * deltaGammaHudduRatio2() + wHLvudSM * deltaGammaHLvudRatio2() +
                wH2udSM * deltaGammaH2udRatio2() + wH2LvSM * deltaGammaH2LvRatio2()) / wH4fSM;
    }
 
    return dwidth;
}

◆ deltaGammaH4fNCRatio1()

const double NPSMEFTd6General::deltaGammaH4fNCRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4f, NC)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4f, NC)$/ $\Gamma(H\to 4f, NC)_{\mathrm{SM}}$

Definition at line 34605 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    
    // SM decay widths (from MG simulations) 
    double wH2L2LSM = 6.905e-07, wH2v2vSM = 2.922e-06, wH2L2vSM = 2.844e-06;
    double wH2u2uSM = 2.406e-06, wH2d2dSM = 1.265e-05, wH2u2dSM = 1.291e-05;
    double wH2L2uSM = 4.402e-06, wH2L2dSM = 8.593e-06, wH2v2uSM = 9.831e-06, wH2v2dSM = 1.867e-05;
    double wH4LSM = 3.565e-07, wH4vSM = 1.747e-06;
    double wH4uSM = 2.533e-06, wH4dSM = 6.394e-06;
 
    // Sum
    double wH4fSM = wH2L2LSM + wH2v2vSM + wH2L2vSM + wH2u2uSM + wH2d2dSM + wH2u2dSM +
            wH2L2uSM + wH2L2dSM + wH2v2uSM + wH2v2dSM + wH4LSM + wH4vSM + wH4uSM + wH4dSM;
 
    dwidth += (wH2L2LSM * deltaGammaH2L2LRatio1() + wH2v2vSM * deltaGammaH2v2vRatio1() + wH2L2vSM * deltaGammaH2L2vRatio1() +
            wH2u2uSM * deltaGammaH2u2uRatio1() + wH2d2dSM * deltaGammaH2d2dRatio1() + wH2u2dSM * deltaGammaH2u2dRatio1() +
            wH2L2uSM * deltaGammaH2L2uRatio1() + wH2L2dSM * deltaGammaH2L2dRatio1() + wH2v2uSM * deltaGammaH2v2uRatio1() +
            wH2v2dSM * deltaGammaH2v2dRatio1() + wH4LSM * deltaGammaH4LRatio1() + wH4vSM * deltaGammaH4vRatio1() +
            wH4uSM * deltaGammaH4uRatio1() + wH4dSM * deltaGammaH4dRatio1()) / wH4fSM;
    
    return dwidth;
}

◆ deltaGammaH4fNCRatio2()

const double NPSMEFTd6General::deltaGammaH4fNCRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4f, NC)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4f, NC)$/ $\Gamma(H\to 4f, NC)_{\mathrm{SM}}$

Definition at line 34628 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        // SM decay widths (from MG simulations)
        double wH2L2LSM = 6.905e-07, wH2v2vSM = 2.922e-06, wH2L2vSM = 2.844e-06;
        double wH2u2uSM = 2.406e-06, wH2d2dSM = 1.265e-05, wH2u2dSM = 1.291e-05;
        double wH2L2uSM = 4.402e-06, wH2L2dSM = 8.593e-06, wH2v2uSM = 9.831e-06, wH2v2dSM = 1.867e-05;
        double wH4LSM = 3.565e-07, wH4vSM = 1.747e-06;
        double wH4uSM = 2.533e-06, wH4dSM = 6.394e-06;
 
        // Sum
        double wH4fSM = wH2L2LSM + wH2v2vSM + wH2L2vSM + wH2u2uSM + wH2d2dSM + wH2u2dSM +
                wH2L2uSM + wH2L2dSM + wH2v2uSM + wH2v2dSM + wH4LSM + wH4vSM + wH4uSM + wH4dSM;
 
        //Contributions that are quadratic in the effective coefficients
        dwidth += (wH2L2LSM * deltaGammaH2L2LRatio2() + wH2v2vSM * deltaGammaH2v2vRatio2() + wH2L2vSM * deltaGammaH2L2vRatio2() +
                wH2u2uSM * deltaGammaH2u2uRatio2() + wH2d2dSM * deltaGammaH2d2dRatio2() + wH2u2dSM * deltaGammaH2u2dRatio2() +
                wH2L2uSM * deltaGammaH2L2uRatio2() + wH2L2dSM * deltaGammaH2L2dRatio2() + wH2v2uSM * deltaGammaH2v2uRatio2() +
                wH2v2dSM * deltaGammaH2v2dRatio2() + wH4LSM * deltaGammaH4LRatio2() + wH4vSM * deltaGammaH4vRatio2() +
                wH4uSM * deltaGammaH4uRatio2() + wH4dSM * deltaGammaH4dRatio2()) / wH4fSM;
    }
 
    return dwidth;
}

◆ deltaGammaH4fRatio1()

const double NPSMEFTd6General::deltaGammaH4fRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4f)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4f)$/ $\Gamma(H\to 4f)_{\mathrm{SM}}$

Definition at line 34497 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
    
    // SM decay widths (from MG simulations)
    /*double wH2L2LSM = 0.65682e-06, wH2v2vSM = 0.28126e-05, wH2L2vSM = 0.27224e-05;
    double wH2u2uSM = 0.22500e-05, wH2d2dSM = 0.11906e-04, wH2u2dSM = 0.12361e-04;
    double wH2L2uSM = 0.45029e-05, wH2L2dSM = 0.85830e-05, wH2v2uSM = 0.93233e-05;
    double wH2v2dSM = 0.17794e-04, wH4LSM = 0.33973e-06, wH4vSM = 0.16884e-05;
    double wH4uSM = 0.23669e-05, wH4dSM = 0.60254e-05;
    double wHLvvLSM = 0.58098e-04, wHudduSM = 0.13384e-03, wHLvudSM = 0.34149e-03;
    double wH2udSM = 0.13711e-03, wH2LvSM = 0.27557e-04;*/
 
    // AG: 
    double wH2L2LSM = 6.905e-07, wH2v2vSM = 2.922e-06, wH2L2vSM = 2.844e-06;
    double wH2u2uSM = 2.406e-06, wH2d2dSM = 1.265e-05, wH2u2dSM = 1.291e-05;
    double wH2L2uSM = 4.402e-06, wH2L2dSM = 8.593e-06, wH2v2uSM = 9.831e-06, wH2v2dSM = 1.867e-05;
    double wH4LSM = 3.565e-07, wH4vSM = 1.747e-06;
    double wH4uSM = 2.533e-06, wH4dSM = 6.394e-06;
    double wHLvvLSM = 6.318e-05, wHudduSM = 0.0001716, wHLvudSM = 0.0003606;
    double wH2udSM = 0.0001758, wH2LvSM = 3.164e-05;
 
    // Sum
    double wH4fSM = wH2L2LSM + wH2v2vSM + wH2L2vSM + wH2u2uSM + wH2d2dSM + wH2u2dSM +
            wH2L2uSM + wH2L2dSM + wH2v2uSM + wH2v2dSM + wH4LSM + wH4vSM + wH4uSM + wH4dSM + wHLvvLSM + wHudduSM +
            wHLvudSM + wH2udSM + wH2LvSM;
 
    dwidth += (wH2L2LSM * deltaGammaH2L2LRatio1() + wH2v2vSM * deltaGammaH2v2vRatio1() + wH2L2vSM * deltaGammaH2L2vRatio1() +
            wH2u2uSM * deltaGammaH2u2uRatio1() + wH2d2dSM * deltaGammaH2d2dRatio1() + wH2u2dSM * deltaGammaH2u2dRatio1() +
            wH2L2uSM * deltaGammaH2L2uRatio1() + wH2L2dSM * deltaGammaH2L2dRatio1() + wH2v2uSM * deltaGammaH2v2uRatio1() +
            wH2v2dSM * deltaGammaH2v2dRatio1() + wH4LSM * deltaGammaH4LRatio1() + wH4vSM * deltaGammaH4vRatio1() +
            wH4uSM * deltaGammaH4uRatio1() + wH4dSM * deltaGammaH4dRatio1() +
            wHLvvLSM * deltaGammaHLvvLRatio1() + wHudduSM * deltaGammaHudduRatio1() + wHLvudSM * deltaGammaHLvudRatio1() +
            wH2udSM * deltaGammaH2udRatio1() + wH2LvSM * deltaGammaH2LvRatio1()) / wH4fSM;
    
    return dwidth;
}

◆ deltaGammaH4fRatio2()

const double NPSMEFTd6General::deltaGammaH4fRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4f)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4f)$/ $\Gamma(H\to 4f)_{\mathrm{SM}}$

Definition at line 34534 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        // SM decay widths (from MG simulations)
        double wH2L2LSM = 6.905e-07, wH2v2vSM = 2.922e-06, wH2L2vSM = 2.844e-06;
        double wH2u2uSM = 2.406e-06, wH2d2dSM = 1.265e-05, wH2u2dSM = 1.291e-05;
        double wH2L2uSM = 4.402e-06, wH2L2dSM = 8.593e-06, wH2v2uSM = 9.831e-06, wH2v2dSM = 1.867e-05;
        double wH4LSM = 3.565e-07, wH4vSM = 1.747e-06;
        double wH4uSM = 2.533e-06, wH4dSM = 6.394e-06;
        double wHLvvLSM = 6.318e-05, wHudduSM = 0.0001716, wHLvudSM = 0.0003606;
        double wH2udSM = 0.0001758, wH2LvSM = 3.164e-05;
 
        // Sum
        double wH4fSM = wH2L2LSM + wH2v2vSM + wH2L2vSM + wH2u2uSM + wH2d2dSM + wH2u2dSM +
                wH2L2uSM + wH2L2dSM + wH2v2uSM + wH2v2dSM + wH4LSM + wH4vSM + wH4uSM + wH4dSM + wHLvvLSM + wHudduSM +
                wHLvudSM + wH2udSM + wH2LvSM;
 
        //Contributions that are quadratic in the effective coefficients
        dwidth += (wH2L2LSM * deltaGammaH2L2LRatio2() + wH2v2vSM * deltaGammaH2v2vRatio2() + wH2L2vSM * deltaGammaH2L2vRatio2() +
                wH2u2uSM * deltaGammaH2u2uRatio2() + wH2d2dSM * deltaGammaH2d2dRatio2() + wH2u2dSM * deltaGammaH2u2dRatio2() +
                wH2L2uSM * deltaGammaH2L2uRatio2() + wH2L2dSM * deltaGammaH2L2dRatio2() + wH2v2uSM * deltaGammaH2v2uRatio2() +
                wH2v2dSM * deltaGammaH2v2dRatio2() + wH4LSM * deltaGammaH4LRatio2() + wH4vSM * deltaGammaH4vRatio2() +
                wH4uSM * deltaGammaH4uRatio2() + wH4dSM * deltaGammaH4dRatio2() +
                wHLvvLSM * deltaGammaHLvvLRatio2() + wHudduSM * deltaGammaHudduRatio2() + wHLvudSM * deltaGammaHLvudRatio2() +
                wH2udSM * deltaGammaH2udRatio2() + wH2LvSM * deltaGammaH2LvRatio2()) / wH4fSM;
    }
 
    return dwidth;
}

◆ deltaGammaH4L2Ratio1()

const double NPSMEFTd6General::deltaGammaH4L2Ratio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4L)$/ $\Gamma(H\to 4L)_{\mathrm{SM}}$

Definition at line 32218 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+121305. * getSMEFTCoeff("CHbox",muRG)
            - 101068. * getSMEFTCoeff("CHB",muRG)
            - 26272.7 * getSMEFTCoeff("CHW",muRG)
            + 61265. * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 0, 0,muRG))
            + 61239.2 * (getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG))
            - 52542.2 * getSMEFTCoeff("CHeR", 0, 0,muRG)
            - 52658.5 * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + cAsch * (-43256.5 * getSMEFTCoeff("CHD",muRG)
            - 82588.8 * getSMEFTCoeff("CHWB",muRG)
            - 3.426 * delta_GF
            - 0.761 * deltaGzd6()
            )
            + cWsch * (-451.131 * getSMEFTCoeff("CHD",muRG)
            + 10429. * getSMEFTCoeff("CHWB",muRG)
            - 3.003 * delta_GF
            - 0.761 * deltaGzd6()
            ));
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-9.718 * deltaMz()
            + 15.845 * deltaMh()
            - 0.163 * deltaaMZ()
            + 2.408 * deltaGmu()))
            + cWsch * (cHSM * (-10.905 * deltaMz()
            + 15.845 * deltaMh()
            + 2.236 * deltaGmu()
            + 0.81 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH4L2Ratio2()

const double NPSMEFTd6General::deltaGammaH4L2Ratio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4L)$/ $\Gamma(H\to 4L)_{\mathrm{SM}}$

Definition at line 32262 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaH4LRatio1()

const double NPSMEFTd6General::deltaGammaH4LRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4L)$/ $\Gamma(H\to 4L)_{\mathrm{SM}}$

Definition at line 31977 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth +=  cAsch * (+121291. * getSMEFTCoeff("CHbox",muRG)
            - 103587. * getSMEFTCoeff("CHB",muRG)
            - 25126.1 * getSMEFTCoeff("CHW",muRG)
            + 40801.2 * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 0, 0,muRG))
            + 40841.5 * (getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG))
            + 40593.4 * (getSMEFTCoeff("CHl1R", 2, 2,muRG) + getSMEFTCoeff("CHl3R", 2, 2,muRG))
            - 35062.5 * getSMEFTCoeff("CHeR", 0, 0,muRG)
            - 35200.6 * getSMEFTCoeff("CHeR", 1, 1,muRG)
            - 34739.1 * getSMEFTCoeff("CHeR", 2, 2,muRG)
            - 43327.2 * getSMEFTCoeff("CHD",muRG)
            - 83516.6 * getSMEFTCoeff("CHWB",muRG)
            - 3.426 * delta_GF
            - 0.759 * deltaGzd6()
            );
            /*+ cWsch * (-79.855 * getSMEFTCoeff("CHD")
            + 10882.3 * getSMEFTCoeff("CHWB")
            - 3. * delta_GF
            - 0.759 * deltaGzd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.12134) * getSMEFTCoeff("CHbox",muRG)
            + (-0.0103) * getSMEFTCoeff("CHW",muRG)
            + (-0.11604) * getSMEFTCoeff("CHB",muRG)
            + (0.01268) * getSMEFTCoeff("CHD",muRG)
            + (0.01261) * getSMEFTCoeff("CHWB",muRG)
            + (0.041857) * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            + (0.041873) * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            + (0.041607) * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            + (-0.1401455) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.1401933) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.041607) * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + (-0.03372101) * getSMEFTCoeff("CHeR", 0, 0,muRG)
            + (-0.0338238) * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + (-0.03341988) * getSMEFTCoeff("CHeR", 2, 2,muRG)
            + (0.18199) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.741) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-9.741 * deltaMz()
            + 15.903 * deltaMh()
            - 0.172 * deltaaMZ()
            + 2.401 * deltaGmu()))
            + cWsch * (cHSM * (-10.943 * deltaMz()
            + 15.903 * deltaMh()
            + 2.234 * deltaGmu()
            + 0.855 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH4lRatio1()

const double NPSMEFTd6General::deltaGammaH4lRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4l)$ ( $l=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4l)$/ $\Gamma(H\to 4l)_{\mathrm{SM}}$

Definition at line 34769 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
 
    // SM decay widths (from MG simmulations)
    double wH2e2muSM = 0.22065e-06, wH4L2SM = 0.22716e-06;
 
    // Sum
    double wH4lSM = wH2e2muSM + wH4L2SM;
 
    dwidth += (wH2e2muSM * deltaGammaH2e2muRatio1() + wH4L2SM * deltaGammaH4L2Ratio1()) / wH4lSM;
 
    return dwidth;
}

◆ deltaGammaH4LRatio2()

const double NPSMEFTd6General::deltaGammaH4LRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4L)$/ $\Gamma(H\to 4L)_{\mathrm{SM}}$

Definition at line 32046 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014714) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.15495) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.41542) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (0.016983) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.12035) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.0018392) * pow(getSMEFTCoeffEW("CHl1R", 0, 0), 2.0)
                + (0.0018429) * pow(getSMEFTCoeffEW("CHl1R", 1, 1), 2.0)
                + (0.0018273) * pow(getSMEFTCoeffEW("CHl1R", 2, 2), 2.0)
                + (0.007796) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.007789) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.0018273) * pow(getSMEFTCoeffEW("CHl3R", 2, 2), 2.0)
                + (0.0018903) * pow(getSMEFTCoeffEW("CHeR", 0, 0), 2.0)
                + (0.0018939) * pow(getSMEFTCoeffEW("CHeR", 1, 1), 2.0)
                + (0.0018728) * pow(getSMEFTCoeffEW("CHeR", 2, 2), 2.0)
                + (0.011032) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (-0.001236) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.014072) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (-0.002148) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (0.001548) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (0.0050712) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.005074) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0050473) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.0096309) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0096384) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0050473) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.004107204) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.0041018682) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.004054257) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.014714) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.11378) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (0.041377) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.220374) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (-0.001359) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.001361) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.000772) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.00015) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.000772) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0005633) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0005763) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0009145) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.001236) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.036515) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (-0.158913) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (-0.00351) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.003531) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.004109) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.010605) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.010582) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.004109) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.002904) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0029155) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0025168) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.014072) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.006449) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (0.0044927) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0045029) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0046153) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.002944) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.002976) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0046153) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0027333) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0027367) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0027896) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.001536) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0019896) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0019886) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0017711) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.000446) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.000441) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0017711) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0056796) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0056827) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0054722) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.001548) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.001397086) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.005076786) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00028075) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0050712) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.005076755) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.001395393) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00028124) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.005074) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.005049493) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.005049493) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0036579) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00026148) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.0050473) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.000891) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.005056) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0038179) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0041009) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0040482) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.016984847) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.005046) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0041001) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0038194) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0040482) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.01697742) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00026148) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.0050473) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.004107204) * getSMEFTCoeffEW("CHeR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0041018682) * getSMEFTCoeffEW("CHeR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.004054257) * getSMEFTCoeffEW("CHeR", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.67) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.0901) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (-0.0072) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.0523) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (-0.0031) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.0204) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (-0.0344) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.0343) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.0352) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.10209) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.1005) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0352) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.028177) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.028204) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.028786) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 2, 2)
                + (-0.1348) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaH4lRatio2()

const double NPSMEFTd6General::deltaGammaH4lRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4l)$ ( $l=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4l)$/ $\Gamma(H\to 4l)_{\mathrm{SM}}$

Definition at line 34783 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaH4muRatio1()

const double NPSMEFTd6General::deltaGammaH4muRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4\mu)$/ $\Gamma(H\to 4\mu)_{\mathrm{SM}}$

Definition at line 32401 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+121280. * getSMEFTCoeff("CHbox",muRG)
            - 101266. * getSMEFTCoeff("CHB",muRG)
            - 25189.1 * getSMEFTCoeff("CHW",muRG)
            + 122245. * (getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG))
            - 105313. * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + cAsch * (-43187.7 * getSMEFTCoeff("CHD",muRG)
            - 82284. * getSMEFTCoeff("CHWB",muRG)
            - 3.424 * delta_GF
            - 0.756 * deltaGzd6())
            + cWsch * (-448.867 * getSMEFTCoeff("CHD",muRG)
            + 10693.5 * getSMEFTCoeff("CHWB",muRG)
            - 2.999 * delta_GF
            - 0.756 * deltaGzd6())
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (cAsch * (-9.697 * deltaMz()
            + 15.843 * deltaMh()
            - 0.171 * deltaaMZ()
            + 2.408 * deltaGmu())
            + cWsch * (-10.868 * deltaMz()
            + 15.843 * deltaMh()
            + 2.244 * deltaGmu()
            + 0.672 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH4muRatio2()

const double NPSMEFTd6General::deltaGammaH4muRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4\mu)$/ $\Gamma(H\to 4\mu)_{\mathrm{SM}}$

Definition at line 32442 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaH4uRatio1()

const double NPSMEFTd6General::deltaGammaH4uRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4u)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4u)$/ $\Gamma(H\to 4u)_{\mathrm{SM}}$

Definition at line 32693 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121283. * getSMEFTCoeff("CHbox",muRG)
            - 153814. * getSMEFTCoeff("CHB",muRG)
            + 70762.7 * getSMEFTCoeff("CHW",muRG)
            - 476614. * getSMEFTCoeff("CHG",muRG)
            - 70157.4 * (getSMEFTCoeff("CHq1R", 0, 0,muRG) - getSMEFTCoeff("CHq3R", 0, 0,muRG))
            - 70569. * (getSMEFTCoeff("CHq1R", 1, 1,muRG) - getSMEFTCoeff("CHq3R", 1, 1,muRG))
            + 30328.1 * getSMEFTCoeff("CHuR", 0, 0,muRG)
            + 30455.3 * getSMEFTCoeff("CHuR", 1, 1,muRG)
            - 67742.3 * getSMEFTCoeff("CHD",muRG)
            - 272758. * getSMEFTCoeff("CHWB",muRG)
            - 4.233 * delta_GF
            - 0.781 * deltaGzd6()
            );
            /*+ cWsch * (+56825.9 * getSMEFTCoeff("CHD")
            + 5.842 * getSMEFTCoeff("CHWB")
            - 3.002 * delta_GF
            - 0.781 * deltaGzd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.12118) * getSMEFTCoeff("CHbox",muRG)
            + (0.07154) * getSMEFTCoeff("CHW",muRG)
            + (-0.154493) * getSMEFTCoeff("CHB",muRG)
            + (0.06099) * getSMEFTCoeff("CHD",muRG)
            + (-0.001621) * getSMEFTCoeff("CHWB",muRG)
            + (-0.46458) * getSMEFTCoeff("CHG",muRG)
            + (-0.070151) * getSMEFTCoeff("CHq1R", 0, 0,muRG)
            + (-0.070597) * getSMEFTCoeff("CHq1R", 1, 1,muRG)
            + (0.070159) * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + (0.070584) * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + (0.028845) * getSMEFTCoeff("CHuR", 0, 0,muRG)
            + (0.028945) * getSMEFTCoeff("CHuR", 1, 1,muRG)
            + (-0.181705) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.181705) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.18178) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.773) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-8.52 * deltaMz()
            + 16.373 * deltaMh()
            - 0.942 * deltaaMZ()
            + 3.167 * deltaGmu()))
            + cWsch * (cHSM * (-14.978 * deltaMz()
            + 16.373 * deltaMh()
            + 2.198 * deltaGmu()
            + 4.578 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH4uRatio2()

const double NPSMEFTd6General::deltaGammaH4uRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4u)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4u)$/ $\Gamma(H\to 4u)_{\mathrm{SM}}$

Definition at line 32761 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014723) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.05967) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.08583) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (0.005284) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.024458) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (17.441) * pow(getSMEFTCoeffEW("CHG"), 2.0)
                + (0.002695) * pow(getSMEFTCoeffEW("CHq1R", 0, 0), 2.0)
                + (0.0027093) * pow(getSMEFTCoeffEW("CHq1R", 1, 1), 2.0)
                + (0.0026965) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                + (0.0027074) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                + (0.0025407) * pow(getSMEFTCoeffEW("CHuR", 0, 0), 2.0)
                + (0.002553) * pow(getSMEFTCoeffEW("CHuR", 1, 1), 2.0)
                + (0.01104) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.01104) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.01104) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (0.008706) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.018754) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (0.003716) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.0001986) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (-0.056564) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHG")
                + (-0.00851468) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0085655) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.0085081) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0085634) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0034974) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.0035094) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.014696081) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.014696081) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.014695) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0816219) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (0.00511) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.0808873) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (0.008774) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHG")
                + (-0.003999) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0042009) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.003996) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.004189) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0007209) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.000785) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.008701) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.008701) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.008706) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.007909) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (0.013811) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (0.07569) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHG")
                + (0.011419) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.011655) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0114147) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0116652) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0030623) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.0031141) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.01874) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.01874) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.018754) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0024203) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (-0.006369) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHG")
                + (-0.0065229) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.006595) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.006513) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0065908) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00178349) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00179882) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.0073925) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0073925) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.007378) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.053831) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHG")
                + (0.0019895) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0020763) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0019874) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0020812) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00515343) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00521536) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.0001955) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0001955) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0001986) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.007733) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.007768) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.007704) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.007748) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0032671) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.0031513) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.028219) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.028219) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.028292) * getSMEFTCoeffEW("CHG") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00538675) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00022976) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.0085081) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0085081) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00851468) * getSMEFTCoeffEW("CHq1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00542127) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.00022419) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.0085634) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0085634) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0085655) * getSMEFTCoeffEW("CHq1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00022949) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00851468) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00851468) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0085081) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00022382) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.0085655) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0085655) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0085634) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00349993) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00349993) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0034974) * getSMEFTCoeffEW("CHuR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00350917) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00350917) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0035094) * getSMEFTCoeffEW("CHuR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.01099) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.02204873) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.02204873) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.68) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.0933) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (-0.0736) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.1281) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (-0.0475) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.02) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (0.0122) * deltaGzd6() * getSMEFTCoeffEW("CHG")
                + (0.05898) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.06058) * deltaGzd6() * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0604) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0578) * deltaGzd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0254) * deltaGzd6() * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.0252) * deltaGzd6() * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.1397) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.1397) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.1399) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaH4vRatio1()

const double NPSMEFTd6General::deltaGammaH4vRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4v)$/ $\Gamma(H\to 4v)_{\mathrm{SM}}$

Definition at line 32491 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121311. * getSMEFTCoeff("CHbox",muRG)
            - 13320.2 * getSMEFTCoeff("CHB",muRG)
            - 44355.6 * getSMEFTCoeff("CHW",muRG)
            - 37027.3 * (getSMEFTCoeff("CHl1R", 0, 0,muRG) - getSMEFTCoeff("CHl3R", 0, 0,muRG))
            - 36969.3 * (getSMEFTCoeff("CHl1R", 1, 1,muRG) - getSMEFTCoeff("CHl3R", 1, 1,muRG))
            - 37032.5 * (getSMEFTCoeff("CHl1R", 2, 2,muRG) - getSMEFTCoeff("CHl3R", 2, 2,muRG))
            - 30309.7 * getSMEFTCoeff("CHD",muRG)
            - 24266.2 * getSMEFTCoeff("CHWB",muRG)
            - 2.998 * delta_GF
            - 0.715 * deltaGzd6()
            );
            /*+ cWsch * (-30309.7 * getSMEFTCoeff("CHD")
            - 24266.2 * getSMEFTCoeff("CHWB")
            - 2.998 * delta_GF
            - 0.715 * deltaGzd6()
            ));*/
 
    //------ Old alpha scheme expression: End
    
    // AG: 
    dwidth += cWsch * (
            ((0.12132) * getSMEFTCoeff("CHbox",muRG)
            + (-0.0448947) * getSMEFTCoeff("CHW",muRG)
            + (-0.01288824) * getSMEFTCoeff("CHB",muRG)
            + (-0.0303007) * getSMEFTCoeff("CHD",muRG)
            + (-0.02405184) * getSMEFTCoeff("CHWB",muRG)
            + (-0.03687556) * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            + (-0.03708882) * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            + (-0.03709052) * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            + (-0.1447394) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.144877) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.037099) * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + (0.18201) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.705) * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-9.608 * deltaMz()
            + 14.774 * deltaMh()
            + 0.233 * deltaaMZ()
            + 2.016 * deltaGmu()))
            + cWsch * (cHSM * (-7.952 * deltaMz()
            + 14.777 * deltaMh()
            + 2.262 * deltaGmu()
            - 1.206 * deltaMw()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
}

◆ deltaGammaH4vRatio2()

const double NPSMEFTd6General::deltaGammaH4vRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to 4v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to 4v)$/ $\Gamma(H\to 4v)_{\mathrm{SM}}$

Definition at line 32554 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014726) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (-0.00480382) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (-0.00151116) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (-0.00092039) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (-0.000594135) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.0008871) * pow(getSMEFTCoeffEW("CHl1R", 0, 0), 2.0)
                + (0.0008922) * pow(getSMEFTCoeffEW("CHl1R", 1, 1), 2.0)
                + (0.000888) * pow(getSMEFTCoeffEW("CHl1R", 2, 2), 2.0)
                + (0.007436) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.007428) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.000888) * pow(getSMEFTCoeffEW("CHl3R", 2, 2), 2.0)
                + (0.011046) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (-0.00544326) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.001563085) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (-0.0073519) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.002917112) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (-0.004492723) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.004495401) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.004497299) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.0102118) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.01020412) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0044983) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.014709) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00037571) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (0.0013626) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.003676079) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (0.0026637) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.002664) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0026642) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0027871) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0027884) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00266319) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00544326) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0021446) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (-0.00125948) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (0.00076461) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0007646) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.00076468) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0007999) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0008002) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.000764423) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.001563085) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0023664) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (-0.000202074) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.000202026) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.000202041) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0038785) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0038773) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.00020215) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.003674358) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0014271) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0014271) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0014274) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.0014932) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0014938) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.001426273) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.002917112) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0027238) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0044994) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.004492723) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0044991) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0027251) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.004495401) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0044983) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0044983) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.001768826) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.004497299) * getSMEFTCoeffEW("CHl1R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00197) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.004519) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.01754772) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00451) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.01756145) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0044983) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.66) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.0835) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (0.031722) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.009061) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (0.02045) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.01684) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (0.029482) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.028462) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.030133) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (0.09418) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.09646) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0301) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.1251) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaHbbRatio1()

const double NPSMEFTd6General::deltaGammaHbbRatio1 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to bb)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to bb)$/ $\Gamma(H\to bb)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28778 of file NPSMEFTd6General.cpp.

{
    double dwidth = 0.0;
 
    double C1 = 0.0;
    double muRG = 125.1;
    
    //if (FlagLoopHd6) {
 
    //    dwidth += (+121248. * getSMEFTCoeff("CHbox",muRG)
    //            - 558.186 * getSMEFTCoeff("CuHR", 2, 2,muRG)
    //            - 5027051. * getSMEFTCoeff("CdHR", 2, 2,muRG)
    //            - 30312.1 * getSMEFTCoeff("CHD",muRG)
    //            - 60624.1 * delta_GF / v() / v());
 
    //} else {
 
        /*dwidth += (+121248. * getSMEFTCoeff("CHbox")
                - 5050180. * getSMEFTCoeff("CdHR", 2, 2)
                - 30312.1 * getSMEFTCoeff("CHD")
                - 60624.1 * delta_GF / v() / v());*/
 
        //AG:begin
        double mf = quarks[BOTTOM].getMass();
        double CifH = getSMEFTCoeff("CdHR", 2, 2,muRG);
        dwidth = deltaGammaHffRatio1(mf, CifH);
        //AG:end
    //}
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (+1. * deltaGmu()
            - 0.23 * deltaaSMZ()
            + 1.007 * deltaMh()
            + 0.001 * deltamt()
            + 1.992 * deltamb());
        
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHbbint + eHbbpar;
 
    return dwidth;
}

◆ deltaGammaHbbRatio2()

const double NPSMEFTd6General::deltaGammaHbbRatio2 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to bb)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to bb)$/ $\Gamma(H\to bb)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28824 of file NPSMEFTd6General.cpp.

{
    double dwidth = 0.0;
 
    if (FlagQuadraticTerms) {
        //AG:begin
        double mf = leptons[BOTTOM].getMass();
        double CifH = getSMEFTCoeffEW("CdHR", 2, 2);
        dwidth += deltaGammaHffRatio2(mf, CifH);
        //AG:end
    }
    return ( dwidth);
}

◆ deltaGammaHccRatio1()

const double NPSMEFTd6General::deltaGammaHccRatio1 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to cc)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to cc)$/ $\Gamma(H\to cc)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28577 of file NPSMEFTd6General.cpp.

{
    double dwidth = 0.0;
 
    double C1 = 0.0;
    double muRG = 125.1;
    
    //if (FlagLoopHd6) {
 
    //    dwidth += (+121248. * getSMEFTCoeff("CHbox",muRG)
    //            - 16421890. * getSMEFTCoeff("CuHR", 1, 1,muRG)
    //            - 992.159 * getSMEFTCoeff("CuHR", 2, 2,muRG)
    //            - 30312.1 * getSMEFTCoeff("CHD",muRG)
    //            - 60624.1 * delta_GF / v() / v());
 
    //} else {
 
        /*dwidth += (+121248. * getSMEFTCoeff("CHbox")
                - 16556668. * getSMEFTCoeff("CuHR", 1, 1)
                - 30312.1 * getSMEFTCoeff("CHD")
                - 60624.1 * delta_GF / v() / v());*/
 
        //AG:begin
        double mf = quarks[CHARM].getMass();
        double CifH = getSMEFTCoeff("CuHR", 1, 1,muRG);
        dwidth = deltaGammaHffRatio1(mf, CifH);
        //AG:end
 
    //}
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (+1. * deltaGmu()
            - 0.789 * deltaaSMZ()
            + 1.004 * deltaMh()
            + 0.001 * deltamt()
            + 1.995 * deltamc());
    
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHccint + eHccpar;
 
    return dwidth;
}

◆ deltaGammaHccRatio2()

const double NPSMEFTd6General::deltaGammaHccRatio2 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to cc)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to cc)$/ $\Gamma(H\to cc)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28624 of file NPSMEFTd6General.cpp.

{
    double dwidth = 0.0;
 
    if (FlagQuadraticTerms) {
        //AG:begin
        double mf = quarks[CHARM].getMass();
        double CifH = getSMEFTCoeffEW("CuHR", 1, 1);
        dwidth += deltaGammaHffRatio2(mf, CifH);
        //AG:end
    }
    //Contributions that are quadratic in the effective coefficients
    return ( dwidth);
}

◆ deltaGammaHevmuvRatio1()

const double NPSMEFTd6General::deltaGammaHevmuvRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to e\nu \mu\nu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to e\nu \mu\nu)$/ $\Gamma(H\to e\nu \mu\nu)_{\mathrm{SM}}$

Definition at line 33364 of file NPSMEFTd6General.cpp.

                                                            {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    dwidth += (+121407. * getSMEFTCoeff("CHbox",muRG)
            - 91741.5 * getSMEFTCoeff("CHW",muRG)
            + 68126.1 * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + 68223.8 * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + cAsch * (-203550. * getSMEFTCoeff("CHD",muRG)
            - 380035. * getSMEFTCoeff("CHWB",muRG)
            - 4.711 * delta_GF
            - 13.53 * deltaMwd6()
            - 0.964 * deltaGwd6()
            )
            + cWsch * (-30299.6 * getSMEFTCoeff("CHD",muRG)
            + 0. * getSMEFTCoeff("CHWB",muRG)
            - 3. * delta_GF
            - 0.964 * deltaGwd6()
            ));
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-12.178 * deltaMz()
            + 13.623 * deltaMh()
            + 1.825 * deltaaMZ()
            + 0.233 * deltaGmu()))
            + cWsch * (cHSM * (-0.016 * deltaMz()
            - 8.445 * deltaMw()
            + 13.623 * deltaMh()
            + 2.089 * deltaGmu()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
}

◆ deltaGammaHevmuvRatio2()

const double NPSMEFTd6General::deltaGammaHevmuvRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to e\nu \mu\nu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to e\nu \mu\nu)$/ $\Gamma(H\to e\nu \mu\nu)_{\mathrm{SM}}$

Definition at line 33406 of file NPSMEFTd6General.cpp.

                                                            {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHffRatio1()

const double NPSMEFTd6General::deltaGammaHffRatio1	(	const double	mf,
		const double	CifH
	)		const

The ratio of the $\Gamma(H\to ff)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to ff)$/ $\Gamma(H\to ff)_{\mathrm{SM}}$

Definition at line 28362 of file NPSMEFTd6General.cpp.

{
    double muRG = 125.1;
    
    double CiHbox = getSMEFTCoeff("CHbox",muRG);
    double CiHD = getSMEFTCoeff("CHD",muRG);
 
    return (-delta_GF + 2.0 * CiHbox * v2 - CiHD * v2 / 2.0 - pow(2.0, 0.5) * CifH * pow(v(), 3.0) / mf);
}

◆ deltaGammaHffRatio2()

const double NPSMEFTd6General::deltaGammaHffRatio2	(	const double	mf,
		const double	CifH
	)		const

The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the ratio of the $\Gamma(H\to ff)$ in the current model and in the Standard Model at order Lambd.

Returns: $\Gamma(H\to ff)$/ $\Gamma(H\to ff)_{\mathrm{SM}}$

Definition at line 28372 of file NPSMEFTd6General.cpp.

{
    double dwidth = 0.0;
 
    if (FlagQuadraticTerms) {
        double CiHbox = getSMEFTCoeffEW("CHbox");
        double CiHD = getSMEFTCoeffEW("CHD");
 
        dwidth += (pow(delta_GF, 2.0) - delta_GF_2 - CifH * delta_GF * pow(v(), 3.0) / pow(2.0, 0.5) / mf
                + 4.0 * pow(CiHbox, 2.0) * pow(v(), 4.0) - 2.0 * CiHbox * CiHD * pow(v(), 4.0) + pow(CiHD, 2.0) * pow(v(), 4.0) / 4.0
                - 2.0 * pow(2.0, 0.5) * CifH * CiHbox * pow(v(), 5.0) / mf + CifH * CiHD * pow(v(), 5.0) / pow(2.0, 0.5) / mf
                + pow(CifH, 2.0) * pow(v(), 6.0) / 2.0 / pow(mf, 2.0));
    }
    return dwidth;
}

◆ deltaGammaHgagaRatio1()

const double NPSMEFTd6General::deltaGammaHgagaRatio1 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to \gamma\gamma)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to \gamma\gamma)$/ $\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28135 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0049;
    double muRG = 125.1;
 
    //  It does not include modifications of MW
    //  Write the tree-level contributions directly as a function 
    //  of delta_AA (or deltaG_hAA) to account for variations of sw2 and cw2
    /*dwidth += (-255156.97 * deltaG_hAA()
            //            -48314158. *getSMEFTCoeff("CHB",muRG) 
            //            -14510502. * getSMEFTCoeff("CHW",muRG) 
            //            +26477588. * getSMEFTCoeff("CHWB",muRG)  
            + cLHd6 * (
            +119766. * getSMEFTCoeff("CHbox",muRG)
            - 42565.7 * getSMEFTCoeff("CeHR", 2, 2,muRG)
            - 48868.1 * getSMEFTCoeff("CuHR", 1, 1,muRG)
            + 32078.2 * getSMEFTCoeff("CuHR", 2, 2,muRG)
            - 18428.3 * getSMEFTCoeff("CdHR", 2, 2,muRG)
            - 137452. * getSMEFTCoeff("CHD",muRG)
            - 235677. * getSMEFTCoeff("CHWB",muRG)
            - 124462. * delta_GF / v() / v()
            - 1.257 * deltaMwd6())
            );*/
 
    //AG:begin
    /*
     * Numeric parametrizations based on arXiV:1805.00302.
     * The analytical expressions were entered into a Mathematica notebook, and a numeric
     parametrization was obtained upon using the updated input values in the MW-scheme.
     * The contribution from eq.411 was rederived in the MW-scheme which now depends on cHD.
     * CKM=1. Pending to add the CKM into the cdH, coming from defining the SU2-doublet as (u,Vd).
     * Future improvement: change to analytic parametrization. 
     */
    double cHbox = getSMEFTCoeffEW("CHbox");
    double cHD = getSMEFTCoeffEW("CHD");
    double cHW = getSMEFTCoeffEW("CHW");
    double cHB = getSMEFTCoeffEW("CHB");
    double cHWB = getSMEFTCoeffEW("CHWB");
    double cW = getSMEFTCoeffEW("CW");
    double dgf = delta_GF;
    double ceH11 = getSMEFTCoeffEW("CeHR", 0, 0);
    double ceH22 = getSMEFTCoeffEW("CeHR", 1, 1);
    double ceH33 = getSMEFTCoeffEW("CeHR", 2, 2);
    double cuH11 = getSMEFTCoeffEW("CuHR", 0, 0);
    double cuH22 = getSMEFTCoeffEW("CuHR", 1, 1);
    double cuH33 = getSMEFTCoeffEW("CuHR", 2, 2);
    double cdH11 = getSMEFTCoeffEW("CdHR", 0, 0);
    double cdH22 = getSMEFTCoeffEW("CdHR", 1, 1);
    double cdH33 = getSMEFTCoeffEW("CdHR", 2, 2);
    double ceB11 = getSMEFTCoeffEW("CeBR", 0, 0);
    double ceB22 = getSMEFTCoeffEW("CeBR", 1, 1);
    double ceB33 = getSMEFTCoeffEW("CeBR", 2, 2);
    double ceW11 = getSMEFTCoeffEW("CeWR", 0, 0);
    double ceW22 = getSMEFTCoeffEW("CeWR", 1, 1);
    double ceW33 = getSMEFTCoeffEW("CeWR", 2, 2);
    double cuB11 = getSMEFTCoeffEW("CuBR", 0, 0);
    double cuB22 = getSMEFTCoeffEW("CuBR", 1, 1);
    double cuB33 = getSMEFTCoeffEW("CuBR", 2, 2);
    double cuW11 = getSMEFTCoeffEW("CuWR", 0, 0);
    double cuW22 = getSMEFTCoeffEW("CuWR", 1, 1);
    double cuW33 = getSMEFTCoeffEW("CuWR", 2, 2);
    double cdB11 = getSMEFTCoeffEW("CdBR", 0, 0);
    double cdB22 = getSMEFTCoeffEW("CdBR", 1, 1);
    double cdB33 = getSMEFTCoeffEW("CdBR", 2, 2);
    double cdW11 = getSMEFTCoeffEW("CdWR", 0, 0);
    double cdW22 = getSMEFTCoeffEW("CdWR", 1, 1);
    double cdW33 = getSMEFTCoeffEW("CdWR", 2, 2);
 
    /*double cHbox = 0.;
    double cHD = 0.;
    double cHW = 0.;
    double cHB = 0.;
    double cHWB = 0.;
    double cW = 0.;
    double dgf = 0.;
    double ceH11 = 0.;
    double ceH22 = 0.;
    double ceH33 = 0.;
    double cuH11 = 0.;
    double cuH22 = 0.;
    double cuH33 = 0.;
    double cdH11 = 0.;
    double cdH22 = 0.;
    double cdH33 = 0.;
    double ceB11=0.;
    double ceB22=0.;
    double ceB33=0.;
    double ceW11=1.;
    double ceW22=0.;
    double ceW33=0.;
    double cuB11=0.;
    double cuB22=0.;
    double cuB33=0.;
    double cuW11=0.;
    double cuW22=0.;
    double cuW33=0.;
    double cdB11=0.;
    double cdB22=0.;
    double cdB33=0.;
    double cdW11=0.;
    double cdW22=0.;
    double cdW33=0.;*/
 
    double MuS = mHl;
    double MuS2 = MuS*MuS;
    double MZ = Mz;
    double MZ2 = MZ*MZ;
 
    double deltaGammaHgaga_Prefactor, dGammaHgagaRatio_HiggsField;
    double dGammaHgagaRatio_Yukawa, dGammaHgagaRatio_dipoleOp;
    double dGammaHgagaRatio_cW;
    double dGammaHgaga_cHB, dGammaHgaga_cHW, dGammaHgaga_cHWB, dGammaHgagaRatio_tree;
 
    //-- Indirect effects from the theory-scheme prefactors:
    deltaGammaHgaga_Prefactor = (-0.211587 * cHD - 0.352136 * cHWB) * pow(1000, 2) - 0.181872 * dgf;
 
    //-- Indirect effect from Higgs-shift:
    dGammaHgagaRatio_HiggsField = sqrt(2)*(cHbox - cHD / 4.) / GF;
 
    //-- Insertions in fermion-loop:
    dGammaHgagaRatio_Yukawa =
            (-0.000257658 * cdH11 - 0.00248474 * cdH22 - 0.0186489 * cdH33
            - 0.000126593 * ceH11 - 0.00812649 * ceH22 - 0.0430632 * ceH33
            - 0.000562257 * cuH11 - 0.0493429 * cuH22 + 0.0342643 * cuH33) * pow(1000, 2);
 
    dGammaHgagaRatio_dipoleOp = (
            cuB33 * (1.863305361 - 0.828073331 * log(MuS2 / MZ2)) +
            cuW33 * (0.966911579 - 0.429706107 * log(MuS2 / MZ2)) +
            cuB22 * (-0.027127066 - 0.006102554 * log(MuS2 / MZ2)) +
            cdW33 * (-0.017084248 - 0.005211430 * log(MuS2 / MZ2)) +
            cuW22 * (-0.014076852 - 0.003166754 * log(MuS2 / MZ2)) +
            ceW33 * (-0.009110967 - 0.002215306 * log(MuS2 / MZ2)) +
            ceW22 * (-0.000912481 - 0.000131729 * log(MuS2 / MZ2)) +
            cdW22 * (-0.000820980 - 0.000116446 * log(MuS2 / MZ2)) +
            cuB11 * (-0.000147805 - 0.000010570 * log(MuS2 / MZ2)) +
            cdW11 * (-0.000065914 - 5.822339464e-6 * log(MuS2 / MZ2)) +
            cuW11 * (-0.000076699 - 5.485466633e-6 * log(MuS2 / MZ2)) +
            ceW11 * (-0.000011198 - 6.370897972e-7 * log(MuS2 / MZ2)) +
            ceB11 * (0.000021579 + 1.227716019e-6 * log(MuS2 / MZ2)) +
            cdB11 * (0.000127022 + 0.000011220 * log(MuS2 / MZ2)) +
            cdB22 * (0.001582086 + 0.000224401 * log(MuS2 / MZ2)) +
            ceB22 * (0.001758414 + 0.000253852 * log(MuS2 / MZ2)) +
            ceB33 * (0.01755746253200913 + 0.004269048861525898 * log(MuS2 / MZ2)) +
            cdB33 * (0.03292252565024579 + 0.010042785723792674 * log(MuS2 / MZ2))) * pow(1000, 2);
 
    //-- Insertions in boson-loop: 
    dGammaHgagaRatio_cW = (-0.0338638 * cW) * pow(1000, 2);
 
    //-- Tree-Level contributions:
    dGammaHgaga_cHB = (-45.2606 + 0.975724 * log(MuS2 / MZ2)) * pow(1000, 2);
    dGammaHgaga_cHW = (-13.0377 + 0.196935 * log(MuS2 / MZ2)) * pow(1000, 2);
    dGammaHgaga_cHWB = (24.4444 - 0.500946 * log(MuS2 / MZ2)) * pow(1000, 2);
 
    dGammaHgagaRatio_tree = dGammaHgaga_cHB * cHB + dGammaHgaga_cHW * cHW + dGammaHgaga_cHWB*cHWB;
 
    //--- TOTAL:
    dwidth += deltaGammaHgaga_Prefactor + dGammaHgagaRatio_HiggsField
            + dGammaHgagaRatio_Yukawa + dGammaHgagaRatio_dipoleOp
            + dGammaHgagaRatio_cW
            + dGammaHgagaRatio_tree;
 
    //std::cout<<"deltaGammaHgaga_Prefactor = "<<deltaGammaHgaga_Prefactor<<std::endl;
    //std::cout<<"dGammaZgagaRatio_HiggsField = "<<dGammaHgagaRatio_HiggsField<<std::endl;
    //std::cout<<"dGammaZgagaRatio_Yukawa = "<<dGammaHgagaRatio_Yukawa<<std::endl;
    //std::cout<<"dGammaHgagaRatio_dipoleOp = "<<dGammaHgagaRatio_dipoleOp<<std::endl;
    //std::cout<<"dGammaZgagaRatio_cW = "<<dGammaHgagaRatio_cW<<std::endl;
    //std::cout<<"dGammaHZgagaRatio_tree = "<<dGammaHgagaRatio_tree<<std::endl;
    //AG:end
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (+2. * deltaa0()
            + 0.27 * deltaaMZ()
            + 0.736 * deltaGmu()
            - 1.797 * deltaMz()
            + 0.02 * deltaaSMZ()
            + 4.195 * deltaMh()
            + 0.047 * deltamt()
            + 0.008 * deltamb()
            + 0.009 * deltamc()
            + 0.01 * deltamtau());
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHgagaint + eHgagapar;
 
    return dwidth;
}

◆ deltaGammaHgagaRatio2()

const double NPSMEFTd6General::deltaGammaHgagaRatio2 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to \gamma\gamma)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to \gamma\gamma)$/ $\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28327 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHggRatio1()

const double NPSMEFTd6General::deltaGammaHggRatio1 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to gg)$ in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.

Returns: $\delta \Gamma(H\to gg)$/ $\Gamma(H\to gg)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 25986 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
    
    double CHG = 0.0, CDH = 0.0, CHD = 0.0, CuHR33 = 0.0, CtGR = 0.0, CHl3R11 = 0.0, CHl3R22 = 0.0, Cll1221 = 0.0;
 
    double C1 = 0.0066;    
    double muRG = 125.1;
    
//  Wilson coefficients definitions 
    CHG = getSMEFTCoeff("CHG",muRG); 
    CDH = getSMEFTCoeff("CHbox",muRG); 
    CHD = getSMEFTCoeff("CHD",muRG); 
    CuHR33 = getSMEFTCoeff("CuHR",2,2,muRG); 
    CtGR = (getSMEFTCoeff("CuGR",2,2,muRG) / g3_tree); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0,muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1,muRG); 
    Cll1221 = getSMEFTCoeff("CllR",0,1,1,0,muRG); 
 
    /*dwidth += (+37526258. * getSMEFTCoeffEW("CHG")
            + cLHd6 * (
            +121248. * getSMEFTCoeffEW("CHbox")
            + 173353. * getSMEFTCoeffEW("CuHR", 1, 1)
            - 129155. * getSMEFTCoeffEW("CuHR", 2, 2)
            + 248530. * getSMEFTCoeffEW("CdHR", 2, 2)
            - 30312.1 * getSMEFTCoeffEW("CHD")
            - 60624.1 * delta_GF / v() / v())
            );*/
 
    // AG:begin
    // Obtained with SMEFTatNLO. 
    // cuG_Warsaw = g3_tree*cuG_SMEFTatNLO
    // Used reweigthing procedure for cHG
    //  This should be at LO independent of alpha-MW scheme
    //dwidth += cWsch * ((
    /*dwidth += ((
            (39.3001) * getSMEFTCoeff("CHG",muRG)
            + (0.12124) * getSMEFTCoeff("CHbox",muRG)
            + (-0.12251) * getSMEFTCoeff("CuHR", 2, 2,muRG)
            - (1.12694) * getSMEFTCoeff("CuGR", 2, 2,muRG) * g3_tree
            + (-0.03032) * getSMEFTCoeff("CHD",muRG)
            + (-0.06064) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.06064) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.06064) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            );*/
    //AG:end
      
    dwidth +=   38059528. * CHG 
                +121279. * CDH 
                -30319.9 * CHD 
                -122154. * CuHR33 
                -1577777. * CtGR 
                -60606.1 * (CHl3R11 + CHl3R22 - Cll1221) 
                ;    
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (+1.003 * deltaGmu()
            + 2.31 * deltaaSMZ()
            + 3.276 * deltaMh()
            - 0.134 * deltamt()
            - 0.106 * deltamb()
            - 0.03 * deltamc());
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHggint + eHggpar;
 
    return dwidth;
}

◆ deltaGammaHggRatio2()

const double NPSMEFTd6General::deltaGammaHggRatio2 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to gg)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to gg)$/ $\Gamma(H\to gg)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 26058 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHll_vvorjjRatio1()

const double NPSMEFTd6General::deltaGammaHll_vvorjjRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to l l \nu\nu, l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to l l \nu\nu, l l j j)$/ $\Gamma(H\to l l \nu\nu, l l j j)_{\mathrm{SM}}$

Definition at line 35151 of file NPSMEFTd6General.cpp.

                                                                {
    double dwidth = 0.0;
 
    // SM decay widths (from MG simmulations)
    double wH2L2v2SM = 0.18213e-05, wHlljjSM = 0.69061E-05;
 
    // Sum
    double wHll_vvorjjSM = wH2L2v2SM + wHlljjSM;
 
    dwidth += (wH2L2v2SM * deltaGammaH2L2v2Ratio1()
            + wHlljjSM * deltaGammaHlljjRatio1()) / wHll_vvorjjSM;
 
    return dwidth;
}

◆ deltaGammaHll_vvorjjRatio2()

const double NPSMEFTd6General::deltaGammaHll_vvorjjRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to l l \nu\nu, l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to l l \nu\nu, l l j j)$/ $\Gamma(H\to l l \nu\nu, l l j j)_{\mathrm{SM}}$

Definition at line 35166 of file NPSMEFTd6General.cpp.

                                                                {
    double dwidth = 0.0;
 
    //Contributions that are quadratic in the effective coefficients
    return ( dwidth);
 
}

◆ deltaGammaHlv_lvorjjRatio1()

const double NPSMEFTd6General::deltaGammaHlv_lvorjjRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to l \nu l \nu, l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to l \nu l \nu, l \nu j j)$/ $\Gamma(H\to l \nu l \nu, l \nu j j)_{\mathrm{SM}}$

Definition at line 35088 of file NPSMEFTd6General.cpp.

                                                                {
    double dwidth = 0.0;
 
    // SM decay widths (from MG simulations)
    double wH2Lv2SM = 0.18353e-04, wHevmuvSM = 0.19421e-04, wHlvjjSM = 0.228e-03;
 
    // Sum
    double wHlv_lvorjjSM = wH2Lv2SM + wHevmuvSM + wHlvjjSM;
 
    dwidth += (wH2Lv2SM * deltaGammaH2Lv2Ratio1()
            + wHevmuvSM * deltaGammaHevmuvRatio1()
            + wHlvjjSM * deltaGammaHlvjjRatio1()) / wHlv_lvorjjSM;
 
    return dwidth;
}

◆ deltaGammaHlv_lvorjjRatio2()

const double NPSMEFTd6General::deltaGammaHlv_lvorjjRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to l \nu l \nu, l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to l \nu l \nu, l \nu j j)$/ $\Gamma(H\to l \nu l \nu, l \nu j j)_{\mathrm{SM}}$

Definition at line 35104 of file NPSMEFTd6General.cpp.

                                                                {
    double dwidth = 0.0;
 
    //Contributions that are quadratic in the effective coefficients
    return ( dwidth);
 
}

◆ deltaGammaHlvjjRatio1()

const double NPSMEFTd6General::deltaGammaHlvjjRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to l \nu j j)$/ $\Gamma(H\to l \nu j j)_{\mathrm{SM}}$

Definition at line 34997 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    dwidth += (+121253. * getSMEFTCoeff("CHbox",muRG)
            - 93392.5 * getSMEFTCoeff("CHW",muRG)
            + 33596.1 * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + 33564.4 * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + 34752.8 * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + 34719.9 * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + cAsch * (-203815. * getSMEFTCoeff("CHD",muRG)
            - 380827. * getSMEFTCoeff("CHWB",muRG)
            - 4.723 * delta_GF
            - 13.742 * deltaMwd6()
            - 0.962 * deltaGwd6()
            )
            + cWsch * (-30332.8 * getSMEFTCoeff("CHD",muRG)
            + 0. * getSMEFTCoeff("CHWB",muRG)
            - 3.004 * delta_GF
            - 0.962 * deltaGwd6()
            ));
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-12.383 * deltaMz()
            + 13.843 * deltaMh()
            + 1.845 * deltaaMZ()
            + 0.244 * deltaGmu()))
            + cWsch * (cHSM * (-0.034 * deltaMz()
            - 8.477 * deltaMw()
            + 13.843 * deltaMh()
            + 2.008 * deltaGmu()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
}

◆ deltaGammaHlvjjRatio2()

const double NPSMEFTd6General::deltaGammaHlvjjRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to l \nu j j)$/ $\Gamma(H\to l \nu j j)_{\mathrm{SM}}$

Definition at line 35041 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    //Contributions that are quadratic in the effective coefficients
    return ( dwidth);
 
}

◆ deltaGammaHLvudRatio1()

const double NPSMEFTd6General::deltaGammaHLvudRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Lvud)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Lvud)$/ $\Gamma(H\to Lvud)_{\mathrm{SM}}$

Definition at line 33610 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121281. * getSMEFTCoeff("CHbox",muRG)
            - 93409.7 * getSMEFTCoeff("CHW",muRG)
            + 22531.9 * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + 22479. * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + 22364.3 * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + 34744.7 * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + 34720.9 * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            - 203784. * getSMEFTCoeff("CHD",muRG)
            - 380028. * getSMEFTCoeff("CHWB",muRG)
            - 4.721 * delta_GF
            - 13.591 * deltaMwd6()
            - 0.969 * deltaGwd6()
            );
            /*+ cWsch * (-30359.9 * getSMEFTCoeff("CHD")
            + 0. * getSMEFTCoeff("CHWB")
            - 3.004 * delta_GF
            - 0.969 * deltaGwd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.12133) * getSMEFTCoeff("CHbox",muRG)
            + (-0.0905501) * getSMEFTCoeff("CHW",muRG)
            + (-0.03027917) * getSMEFTCoeff("CHD",muRG)
            + (-0.1591054) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.15932529) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.022578) * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + (0.034785) * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + (0.034757) * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + (0.18198) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.964) * deltaGwd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-12.333 * deltaMz()
            + 13.766 * deltaMh()
            + 1.852 * deltaaMZ()
            + 0.169 * deltaGmu()))
            + cWsch * (cHSM * (-0.015 * deltaMz()
            - 8.492 * deltaMw()
            + 13.769 * deltaMh()
            + 2.065 * deltaGmu()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
}

◆ deltaGammaHLvudRatio2()

const double NPSMEFTd6General::deltaGammaHLvudRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Lvud)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Lvud)$/ $\Gamma(H\to Lvud)_{\mathrm{SM}}$

Definition at line 33672 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014754) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (-0.0080971) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.0009223) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.008885) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.008893) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.0005886) * pow(getSMEFTCoeffEW("CHl3R", 2, 2), 2.0)
                + (0.00093) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                + (0.0009298) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                + (0.011069) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (-0.01098128) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.007344733) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.01194738) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.01195405) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.002738) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.0042166) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0042142) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.014703) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.002745) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (0.0080855) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0080922) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00288826) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00445065) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.00444505) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.01098128) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0029893) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0029899) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00068459) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00105334) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0010533816) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.003670687) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.003869) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.003866211) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.01929275) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.003867978) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0038718043) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.01930829) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0003448) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.00034402) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.002738) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0042166) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0042142) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.94) * pow(deltaGwd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.117) * deltaGwd6() * getSMEFTCoeffEW("CHbox")
                + (0.08693) * deltaGwd6() * getSMEFTCoeffEW("CHW")
                + (0.02861) * deltaGwd6() * getSMEFTCoeffEW("CHD")
                + (0.14745) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.14791) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.02192) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.0338) * deltaGwd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0329) * deltaGwd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.1754) * deltaGwd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
 
    }
 
    return dwidth;
}

◆ deltaGammaHLvvLRatio1()

const double NPSMEFTd6General::deltaGammaHLvvLRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to LvvL)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to LvvL)$/ $\Gamma(H\to LvvL)_{\mathrm{SM}}$

Definition at line 33220 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121150. * getSMEFTCoeff("CHbox",muRG)
            - 91767.5 * getSMEFTCoeff("CHW",muRG)
            + 45140.3 * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + 45192.1 * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + 45407.7 * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            - 203598. * getSMEFTCoeff("CHD",muRG)
            - 379536. * getSMEFTCoeff("CHWB",muRG)
            - 4.713 * delta_GF
            - 13.743 * deltaMwd6()
            - 0.962 * deltaGwd6()
            );
            /*+ cWsch * (-30310.3 * getSMEFTCoeff("CHD")
            + 0. * getSMEFTCoeff("CHWB")
            - 2.996 * delta_GF
            - 0.962 * deltaGwd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.12141) * getSMEFTCoeff("CHbox",muRG)
            + (-0.0905945) * getSMEFTCoeff("CHW",muRG)
            + (-0.03032886) * getSMEFTCoeff("CHD",muRG)
            + (-0.1367504) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.1366861) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.045303) * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            + (0.18211) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.919) * deltaGwd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-12.232 * deltaMz()
            + 13.669 * deltaMh()
            + 1.829 * deltaaMZ()
            + 0.189 * deltaGmu()))
            + cWsch * (cHSM * (-0.016 * deltaMz()
            - 8.548 * deltaMw()
            + 13.67 * deltaMh()
            + 2.003 * deltaGmu()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
}

◆ deltaGammaHLvvLRatio2()

const double NPSMEFTd6General::deltaGammaHLvvLRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to LvvL)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to LvvL)$/ $\Gamma(H\to LvvL)_{\mathrm{SM}}$

Definition at line 33278 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014737) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (-0.0080873) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.0009211) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.006746) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.00673) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.001181) * pow(getSMEFTCoeffEW("CHl3R", 2, 2), 2.0)
                + (0.011052) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (-0.01099103) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.007355586) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.009228766) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.009234217) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0054912) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (0.014714) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0027512) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (0.0052117) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0052036) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00578441) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.01099103) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0023085) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0023079) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0013725648) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.003676614) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.01658196) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.01658238) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0054912) * getSMEFTCoeffEW("CHl3R", 2, 2) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.688) * pow(deltaGwd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.1095) * deltaGwd6() * getSMEFTCoeffEW("CHbox")
                + (0.08596) * deltaGwd6() * getSMEFTCoeffEW("CHW")
                + (0.028419) * deltaGwd6() * getSMEFTCoeffEW("CHD")
                + (0.12977) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.125384) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0435) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.1641) * deltaGwd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
    }
 
    return dwidth;
}

◆ deltaGammaHmumuRatio1()

const double NPSMEFTd6General::deltaGammaHmumuRatio1 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to \mu\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to \mu\mu)$/ $\Gamma(H\to \mu\mu)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28403 of file NPSMEFTd6General.cpp.

{
    double dwidth = 0.0;
 
    double C1 = 0.0;
    double muRG = 125.1;
    
    /*dwidth += (+121248. * getSMEFTCoeff("CHbox")
            - 199792511. * getSMEFTCoeff("CeHR", 1, 1)
            - 30312.1 * getSMEFTCoeff("CHD")
            - 60624.1 * delta_GF / v() / v());*/
 
    //AG:begin
    double mf = leptons[MU].getMass();
    double CifH = getSMEFTCoeff("CeHR", 1, 1,muRG);
    dwidth = deltaGammaHffRatio1(mf, CifH);
    //AG:end
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (+1. * deltaGmu()
            + 1. * deltaMh());
    
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHmumuint + eHmumupar;
 
    return dwidth;
}

◆ deltaGammaHmumuRatio2()

const double NPSMEFTd6General::deltaGammaHmumuRatio2 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to \mu\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to \mu\mu)$/ $\Gamma(H\to \mu\mu)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28435 of file NPSMEFTd6General.cpp.

{
    double dwidth = 0.0;
 
    if (FlagQuadraticTerms) {
        //AG:begin  
        double mf = leptons[MU].getMass();
        double CifH = getSMEFTCoeffEW("CeHR", 1, 1);
        dwidth += deltaGammaHffRatio2(mf, CifH);
        //AG:end 
    }
    //Contributions that are quadratic in the effective coefficients
    return ( dwidth);
}

◆ deltaGammaHssRatio1()

const double NPSMEFTd6General::deltaGammaHssRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ss)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ss)$/ $\Gamma(H\to ss)_{\mathrm{SM}}$

Definition at line 28680 of file NPSMEFTd6General.cpp.

{
    double dwidth = 0.0;
 
    double C1 = 0.0;
    double muRG = 125.1;
    
    //if (FlagLoopHd6) {
 
    //    dwidth += (+121248. * getSMEFTCoeff("CHbox",muRG)
    //            - 16421890. * getSMEFTCoeff("CuHR", 1, 1,muRG)
    //            - 992.159 * getSMEFTCoeff("CuHR", 2, 2,muRG)
    //            - 30312.1 * getSMEFTCoeff("CHD",muRG)
    //            - 60624.1 * delta_GF / v() / v());
 
    //} else {
 
        /*dwidth += (+121248. * getSMEFTCoeff("CHbox",muRG)
                - 16556668. * getSMEFTCoeff("CuHR", 1, 1,muRG)
                - 30312.1 * getSMEFTCoeff("CHD",muRG)
                - 60624.1 * delta_GF / v() / v());*/
 
    //    double mf = quarks[STRANGE].getMass();
    //    double CifH = getSMEFTCoeff("CdHR", 1, 1,muRG);
    //    dwidth = deltaGammaHffRatio1(mf, CifH);
 
    //}
    
        double mf = quarks[STRANGE].getMass();
        double CifH = getSMEFTCoeff("CdHR", 1, 1,muRG);
        dwidth = deltaGammaHffRatio1(mf, CifH);
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters. Not here    
    dwidth += cHSM * (0.);
        
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHssint + eHsspar; // Defined but still not included as part of the model free parameters!
 
    return dwidth;
}

◆ deltaGammaHssRatio2()

const double NPSMEFTd6General::deltaGammaHssRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ss)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ss)$/ $\Gamma(H\to ss)_{\mathrm{SM}}$

Definition at line 28725 of file NPSMEFTd6General.cpp.

{
    double dwidth = 0.0;
 
    if (FlagQuadraticTerms) {
        double mf = quarks[STRANGE].getMass();
        double CifH = getSMEFTCoeffEW("CdHR", 1, 1);
        dwidth += deltaGammaHffRatio2(mf, CifH);
    }
    //Contributions that are quadratic in the effective coefficients
    return ( dwidth);
}

◆ deltaGammaHtautauRatio1()

const double NPSMEFTd6General::deltaGammaHtautauRatio1 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to \tau\tau)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to \tau\tau)$/ $\Gamma(H\to \tau\tau)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28490 of file NPSMEFTd6General.cpp.

{
    double dwidth = 0.0;
 
    double C1 = 0.0;
    double muRG = 125.1;
    
    /*dwidth += (+121248. * getSMEFTCoeff("CHbox")
            - 11880369. * getSMEFTCoeff("CeHR", 2, 2)
            - 30312.1 * getSMEFTCoeff("CHD")
            - 60624.1 * delta_GF / v() / v());*/
    //AG:begin
    double mf = leptons[TAU].getMass();
    double CifH = getSMEFTCoeff("CeHR", 2, 2,muRG);
    dwidth = deltaGammaHffRatio1(mf, CifH);
    //AG:end
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (+1. * deltaGmu()
            + 1.002 * deltaMh()
            + 1.998 * deltamtau());
    
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHtautauint + eHtautaupar;
 
    return dwidth;
}

◆ deltaGammaHtautauRatio2()

const double NPSMEFTd6General::deltaGammaHtautauRatio2 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to \tau\tau)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to \tau\tau)$/ $\Gamma(H\to \tau\tau)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28522 of file NPSMEFTd6General.cpp.

{
    double dwidth = 0.0;
 
    if (FlagQuadraticTerms) {
        //AG:begin
        double mf = leptons[TAU].getMass();
        double CifH = getSMEFTCoeffEW("CeHR", 2, 2);
        dwidth += deltaGammaHffRatio2(mf, CifH);
        //AG:end   
    }
 
    return dwidth;
}

◆ deltaGammaHudduRatio1()

const double NPSMEFTd6General::deltaGammaHudduRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to uddu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to uddu)$/ $\Gamma(H\to uddu)_{\mathrm{SM}}$

Definition at line 33455 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    dwidth += cAsch * (+121333. * getSMEFTCoeff("CHbox",muRG)
            - 92283.9 * getSMEFTCoeff("CHW",muRG)
            + 68273.4 * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + 68176.3 * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            - 203776. * getSMEFTCoeff("CHD",muRG)
            - 380178. * getSMEFTCoeff("CHWB",muRG)
            - 4.719 * delta_GF
            - 14.006 * deltaMwd6()
            - 0.956 * deltaGwd6()
            );
            /*+ cWsch * (-30312.7 * getSMEFTCoeff("CHD")
            + 0. * getSMEFTCoeff("CHWB")
            - 3.003 * delta_GF
            - 0.956 * deltaGwd6()
            ));*/
    
    //------ Old alpha scheme expression: End
 
    // AG: 
    dwidth += cWsch * (
            ((0.12079) * getSMEFTCoeff("CHbox",muRG)
            + (-0.0903745) * getSMEFTCoeff("CHW",muRG)
            + (-0.03023476) * getSMEFTCoeff("CHD",muRG)
            + (0.06934) * getSMEFTCoeff("CHq3R", 0, 0,muRG)
            + (0.069517) * getSMEFTCoeff("CHq3R", 1, 1,muRG)
            + (-0.1813696) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.1813696) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.18117) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            + (-0.955) * deltaGwd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cAsch * (cHSM * (-12.618 * deltaMz()
            + 14.254 * deltaMh()
            + 1.912 * deltaaMZ()
            + 0.149 * deltaGmu()))
            + cWsch * (cHSM * (-0.018 * deltaMz()
            - 8.857 * deltaMw()
            + 14.251 * deltaMh()
            + 2.073 * deltaGmu()));
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
}

◆ deltaGammaHudduRatio2()

const double NPSMEFTd6General::deltaGammaHudduRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to uddu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to uddu)$/ $\Gamma(H\to uddu)_{\mathrm{SM}}$

Definition at line 33513 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        dwidth += cWsch * (
                +(0.014687) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (-0.008077632) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.0009178) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.0018572) * pow(getSMEFTCoeffEW("CHq3R", 0, 0), 2.0)
                + (0.0018574) * pow(getSMEFTCoeffEW("CHq3R", 1, 1), 2.0)
                + (0.011013) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.011013) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.011013) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (-0.010959679) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.007334116) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (0.0084087) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0084295) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.01466739) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.01466739) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.014653) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.002741) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.008875263) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.008882525) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.010964) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.010964) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.010959679) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.002100955) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.002107679) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0036638) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0036638) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.003668205) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0084038) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0084038) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0084087) * getSMEFTCoeffEW("CHq3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00843117) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.00843117) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0084295) * getSMEFTCoeffEW("CHq3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.02200743) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.02200743) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.85) * pow(deltaGwd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.1163) * deltaGwd6() * getSMEFTCoeffEW("CHbox")
                + (0.086111) * deltaGwd6() * getSMEFTCoeffEW("CHW")
                + (0.029355) * deltaGwd6() * getSMEFTCoeffEW("CHD")
                + (-0.0689) * deltaGwd6() * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0682) * deltaGwd6() * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.17534) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.17534) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.1744) * deltaGwd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
 
    }
 
    return dwidth;
}

◆ deltaGammaHWffRatio1()

const double NPSMEFTd6General::deltaGammaHWffRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to W f f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to W f f)$/ $\Gamma(H\to W f f)_{\mathrm{SM}}$

Definition at line 26476 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    dwidth += (+121288. * getSMEFTCoeff("CHbox",muRG)
            + 5395.21 * (1.0 / 3.0) * (getSMEFTCoeff("CHl3R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 2, 2,muRG))
            + 11680.9 * (1.0 / 2.0) * (getSMEFTCoeff("CHq3R", 0, 0,muRG) + getSMEFTCoeff("CHq3R", 1, 1,muRG))
            - 159787. * getSMEFTCoeff("CHD",muRG)
            - 91509.1 * getSMEFTCoeff("CHW",muRG)
            - 283092. * getSMEFTCoeff("CHWB",muRG)
            - 3.259 * delta_GF
            - 15.196 * deltaMwd6());
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    //dwidth += cHSM * ( 0.0 ); 
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    //dwidth += eHWWint + eHWWpar;
 
    return dwidth;
 
}

◆ deltaGammaHWffRatio2()

const double NPSMEFTd6General::deltaGammaHWffRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to W f f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to W f f)$/ $\Gamma(H\to W f f)_{\mathrm{SM}}$

Definition at line 26505 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHWjjRatio1()

const double NPSMEFTd6General::deltaGammaHWjjRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to W j j)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to W j j)$/ $\Gamma(H\to W j j)_{\mathrm{SM}}$

Definition at line 26318 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    dwidth += (+121611. * getSMEFTCoeff("CHbox",muRG)
            + 17701.4 * (1.0 / 2.0) * (getSMEFTCoeff("CHq3R", 0, 0,muRG) + getSMEFTCoeff("CHq3R", 1, 1,muRG))
            - 159273. * getSMEFTCoeff("CHD",muRG)
            - 91021.6 * getSMEFTCoeff("CHW",muRG)
            - 282574. * getSMEFTCoeff("CHWB",muRG)
            - 3.259 * delta_GF
            - 15.198 * deltaMwd6());
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    //dwidth += cHSM * ( 0.0 ); 
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    //dwidth += eHWWint + eHWWpar;
 
    return dwidth;
 
}

◆ deltaGammaHWjjRatio2()

const double NPSMEFTd6General::deltaGammaHWjjRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to W j j)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to W j j)$/ $\Gamma(H\to W j j)_{\mathrm{SM}}$

Definition at line 26346 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHWlvRatio1()

const double NPSMEFTd6General::deltaGammaHWlvRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Wl\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Wl\nu)$/ $\Gamma(H\to Wl\nu)_{\mathrm{SM}}$

Definition at line 26159 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    dwidth += (+121875. * getSMEFTCoeff("CHbox",muRG)
            + 18351.9 * (1.0 / 2.0) * (getSMEFTCoeff("CHl3R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG))
            - 159873. * getSMEFTCoeff("CHD",muRG)
            - 91288.7 * getSMEFTCoeff("CHW",muRG)
            - 284689. * getSMEFTCoeff("CHWB",muRG)
            - 3.292 * delta_GF
            - 15.14 * deltaMwd6());
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    //dwidth += cHSM * ( 0.0 );
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    //dwidth += eHWWint + eHWWpar;
 
    return dwidth;
 
}

◆ deltaGammaHWlvRatio2()

const double NPSMEFTd6General::deltaGammaHWlvRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Wl\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Wl\nu)$/ $\Gamma(H\to Wl\nu)_{\mathrm{SM}}$

Definition at line 26187 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHWW2l2vRatio1()

const double NPSMEFTd6General::deltaGammaHWW2l2vRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to l\nu l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to WW^*\to l\nu l\nu)$/ $\Gamma(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}$

Definition at line 26236 of file NPSMEFTd6General.cpp.

                                                             {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    dwidth += (+120742. * getSMEFTCoeff("CHbox",muRG)
            + 131582. * (1.0 / 2.0) * (getSMEFTCoeff("CHl3R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG))
            - 204043. * getSMEFTCoeff("CHD",muRG)
            - 91463.9 * getSMEFTCoeff("CHW",muRG)
            - 379529. * getSMEFTCoeff("CHWB",muRG)
            - 4.705 * delta_GF
            - 13.735 * deltaMwd6()
            - 0.965 * deltaGwd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (-12.123 * deltaMz()
            + 13.615 * deltaMh()
            + 1.756 * deltaaMZ()
            + 0.216 * deltaGmu());
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
 
}

◆ deltaGammaHWW2l2vRatio2()

const double NPSMEFTd6General::deltaGammaHWW2l2vRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to l\nu l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to WW^*\to l\nu l\nu)$/ $\Gamma(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}$

Definition at line 26269 of file NPSMEFTd6General.cpp.

                                                             {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHWW4fRatio1()

const double NPSMEFTd6General::deltaGammaHWW4fRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to WW^*\to 4f)$/ $\Gamma(H\to WW^*\to 4f)_{\mathrm{SM}}$

Definition at line 26554 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    double CWff, sf;
 
    CWff = (getSMEFTCoeff("CHl3R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 2, 2,muRG)) * v2 +
            Nc * (getSMEFTCoeff("CHq3R", 0, 0,muRG) + getSMEFTCoeff("CHq3R", 1, 1,muRG)) * v2;
 
    CWff = CWff / (3.0 + 2.0 * Nc);
 
    sf = 90362.5 * (1.0 / 2.0) * (3.0 + 2.0 * Nc) / (Nc * v2); // Coefficient of the CWff term. From the getSMEFTCoeff("CHq3R",0,0) term in the ME.
 
    dwidth += cAsch * (+121886. * getSMEFTCoeff("CHbox",muRG)
            + sf * CWff
            - 204009. * getSMEFTCoeff("CHD",muRG)
            - 91455.7 * getSMEFTCoeff("CHW",muRG)
            - 382903. * getSMEFTCoeff("CHWB",muRG)
            - 4.757 * delta_GF
            - 13.716 * deltaMwd6()
            - 0.963 * deltaGwd6()
            );
    
    //------ Old alpha scheme expression: End
 
    //AG:begin
    dwidth += cWsch * (
            ((0.12133) * getSMEFTCoeff("CHbox",muRG)
            + (-0.0905777) * getSMEFTCoeff("CHW",muRG)
            + (-0.03034378) * getSMEFTCoeff("CHD",muRG)
            + (-0.11424153) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.1141935) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (0.18202) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            );
 
    dwidth += cWsch * (+(-0.94) * deltaGwd6());
 
 
    //AG:end
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (-12.271 * deltaMz()
            + 13.665 * deltaMh()
            + 1.85 * deltaaMZ()
            + 0.224 * deltaGmu());
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
 
}

◆ deltaGammaHWW4fRatio2()

const double NPSMEFTd6General::deltaGammaHWW4fRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to WW^*\to 4f)$/ $\Gamma(H\to WW^*\to 4f)_{\mathrm{SM}}$

Definition at line 26614 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += cWsch * (
                +(0.01471) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (-0.0081083) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (0.0009192) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.005083) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.00508) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.011034) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (-0.01097899) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.0073562947) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.00649564) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0064908) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.014711) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0027439) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (0.0023097) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0023154) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.01097899) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0016225) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0016221) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.0036781165) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.00439) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.013843218) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.01384871) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.85) * pow(deltaGwd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.1119) * deltaGwd6() * getSMEFTCoeffEW("CHbox")
                + (0.0842) * deltaGwd6() * getSMEFTCoeffEW("CHW")
                + (0.029323) * deltaGwd6() * getSMEFTCoeffEW("CHD")
                + (0.10437) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.10931) * deltaGwd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.1679) * deltaGwd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
 
    }
 
    return dwidth;
}

◆ deltaGammaHWW4jRatio1()

const double NPSMEFTd6General::deltaGammaHWW4jRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to 4j)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to WW^*\to 4j)$/ $\Gamma(H\to WW^*\to 4j)_{\mathrm{SM}}$

Definition at line 26395 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0073;
    double muRG = 125.1;
 
    dwidth += (+121936. * getSMEFTCoeff("CHbox",muRG)
            + 138860. * (1.0 / 2.0) * (getSMEFTCoeff("CHq3R", 0, 0,muRG) + getSMEFTCoeff("CHq3R", 1, 1,muRG))
            - 205023. * getSMEFTCoeff("CHD",muRG)
            - 89938.5 * getSMEFTCoeff("CHW",muRG)
            - 383944. * getSMEFTCoeff("CHWB",muRG)
            - 4.816 * delta_GF
            - 13.647 * deltaMwd6()
            - 0.959 * deltaGwd6());
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (-12.168 * deltaMz()
            + 13.66 * deltaMh()
            + 1.899 * deltaaMZ()
            + 0.189 * deltaGmu());
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
 
}

◆ deltaGammaHWW4jRatio2()

const double NPSMEFTd6General::deltaGammaHWW4jRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to 4j)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to WW^*\to 4j)$/ $\Gamma(H\to WW^*\to 4j)_{\mathrm{SM}}$

Definition at line 26427 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHWWRatio1()

const double NPSMEFTd6General::deltaGammaHWWRatio1 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to WW)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to WW)$/ $\Gamma(H\to WW)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 26108 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
 
    //    double C1 = 0.0073;
 
    dwidth = deltaGammaHWW4fRatio1();
 
    //  Linear contribution from Higgs self-coupling
    //    dwidth += cLHd6*(C1 + 2.0*dZH1)*deltaG_hhhRatio(); 
    //  Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
    //    dwidth += cLHd6*cLH3d62*dZH2*deltaG_hhhRatio()*deltaG_hhhRatio();
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    //    dwidth += eHWWint + eHWWpar;
 
    return dwidth;
 
}

◆ deltaGammaHWWRatio2()

const double NPSMEFTd6General::deltaGammaHWWRatio2 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to WW)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to WW)$/ $\Gamma(H\to WW)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 26127 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
 
    if (FlagQuadraticTerms) {
        dwidth = deltaGammaHWW4fRatio2();
    }
 
    return dwidth;
}

◆ deltaGammaHZddRatio1()

const double NPSMEFTd6General::deltaGammaHZddRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Z d d)$ ( $d=d,s,b $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Z d d)$/ $\Gamma(H\to Z d d)_{\mathrm{SM}}$

Definition at line 27532 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+121756. * getSMEFTCoeff("CHbox",muRG)
            + 9252.73 * (1.0 / 3.0) * (getSMEFTCoeff("CHq1R", 0, 0,muRG) + getSMEFTCoeff("CHq1R", 1, 1,muRG) + getSMEFTCoeff("CHq1R", 2, 2,muRG))
            - 1471.03 * (1.0 / 3.0) * (getSMEFTCoeff("CHdR", 0, 0,muRG) + getSMEFTCoeff("CHdR", 1, 1,muRG) + getSMEFTCoeff("CHdR", 2, 2,muRG))
            + 9252.73 * (1.0 / 3.0) * (getSMEFTCoeff("CHq3R", 0, 0,muRG) + getSMEFTCoeff("CHq3R", 1, 1,muRG) + getSMEFTCoeff("CHq3R", 2, 2,muRG))
            - 12714.3 * getSMEFTCoeff("CHD",muRG)
            - 13589.3 * getSMEFTCoeff("CHB",muRG)
            - 45689.4 * getSMEFTCoeff("CHW",muRG)
            - 85582.3 * getSMEFTCoeff("CHWB",muRG)
            - 2.427 * delta_GF);
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    //dwidth += cHSM * ( 0.0 ); 
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    //dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZddRatio2()

const double NPSMEFTd6General::deltaGammaHZddRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Z d d)$ ( $d=d,s,b $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Z d d)$/ $\Gamma(H\to Z d d)_{\mathrm{SM}}$

Definition at line 27562 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHZeeRatio1()

const double NPSMEFTd6General::deltaGammaHZeeRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Zee)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Zee)$/ $\Gamma(H\to Zee)_{\mathrm{SM}}$

Definition at line 26825 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //  Derived from the HZll expression for l=e only
 
    dwidth += (+121715. * getSMEFTCoeff("CHbox",muRG)
            + 8726.9 * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            - 7315.2 * getSMEFTCoeff("CHeR", 0, 0,muRG)
            + 8726.9 * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            - 5544.15 * getSMEFTCoeff("CHD",muRG)
            - 13560.9 * getSMEFTCoeff("CHB",muRG)
            - 45585.2 * getSMEFTCoeff("CHW",muRG)
            - 53507.9 * getSMEFTCoeff("CHWB",muRG)
            - 2.204 * delta_GF);
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    //dwidth += cHSM * ( 0.0 ); 
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    //dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZeeRatio2()

const double NPSMEFTd6General::deltaGammaHZeeRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Zee)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Zee)$/ $\Gamma(H\to Zee)_{\mathrm{SM}}$

Definition at line 26857 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHZffRatio1()

const double NPSMEFTd6General::deltaGammaHZffRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Z ff)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Z f f)$/ $\Gamma(H\to Z f f)_{\mathrm{SM}}$

Definition at line 27628 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+121551. * getSMEFTCoeff("CHbox",muRG)
            - 824.482 * (1.0 / 3.0) * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl1R", 2, 2,muRG))
            + 1840.54 * (1.0 / 12.0) * (5.0 * getSMEFTCoeff("CHq1R", 0, 0,muRG) + 5.0 * getSMEFTCoeff("CHq1R", 1, 1,muRG) + 2.0 * getSMEFTCoeff("CHq1R", 2, 2,muRG) - getSMEFTCoeff("CHq3R", 0, 0,muRG) - getSMEFTCoeff("CHq3R", 1, 1,muRG) + 2.0 * getSMEFTCoeff("CHq3R", 2, 2,muRG))
            - 795.383 * (1.0 / 3.0) * (getSMEFTCoeff("CHeR", 0, 0,muRG) + getSMEFTCoeff("CHeR", 1, 1,muRG) + getSMEFTCoeff("CHeR", 2, 2,muRG))
            + 1069.4 * (1.0 / 2.0) * (getSMEFTCoeff("CHuR", 0, 0,muRG) + getSMEFTCoeff("CHuR", 1, 1,muRG))
            - 579.563 * (1.0 / 3.0) * (getSMEFTCoeff("CHdR", 0, 0,muRG) + getSMEFTCoeff("CHdR", 1, 1,muRG) + getSMEFTCoeff("CHdR", 2, 2,muRG))
            + 3164.56 * (1.0 / 3.0) * (getSMEFTCoeff("CHl3R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 2, 2,muRG))
            + 6413.99 * (-1.0 / 12.0) * (getSMEFTCoeff("CHq1R", 0, 0,muRG) + getSMEFTCoeff("CHq1R", 1, 1,muRG) - 2.0 * getSMEFTCoeff("CHq1R", 2, 2,muRG) - 5.0 * getSMEFTCoeff("CHq3R", 0, 0,muRG) - 5.0 * getSMEFTCoeff("CHq3R", 1, 1,muRG) - 2.0 * getSMEFTCoeff("CHq3R", 2, 2,muRG))
            - 10839.5 * getSMEFTCoeff("CHD",muRG)
            - 14222.3 * getSMEFTCoeff("CHB",muRG)
            - 45455.6 * getSMEFTCoeff("CHW",muRG)
            - 75343.1 * getSMEFTCoeff("CHWB",muRG)
            - 2.356 * delta_GF);
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    //dwidth += cHSM * ( 0.0 ); 
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    //dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZffRatio2()

const double NPSMEFTd6General::deltaGammaHZffRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Z ff)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Z f f)$/ $\Gamma(H\to Z f f)_{\mathrm{SM}}$

Definition at line 27662 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHZgaRatio1()

const double NPSMEFTd6General::deltaGammaHZgaRatio1 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to Z\gamma)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Z\gamma)$/ $\Gamma(H\to Z\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 27938 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0;
    double muRG = 125.1;
 
    //  It includes modifications of Zff vertices and MW, but not on the pure VVV and VVVV vertices
    //  Write the tree-level contributions directly as a function 
    //  of delta_ZA (or deltaG1_hZA()) to account for variations of sw2 and cw
    /*dwidth += (-71769.02 * deltaG1_hZA()
            //            +14894914. *getSMEFTCoeff("CHB",muRG) 
            //            -14894913. * getSMEFTCoeff("CHW",muRG) 
            //            +9508089. * getSMEFTCoeff("CHWB",muRG) 
            + cLHd6 * (
            +120002. * getSMEFTCoeff("CHbox",muRG)
            + 50.12 * getSMEFTCoeff("CHl1R", 2, 2,muRG)
            + 17401. * getSMEFTCoeff("CHq1R", 2, 2,muRG)
            + 50.12 * getSMEFTCoeff("CHeR", 2, 2,muRG)
            + 17188.7 * getSMEFTCoeff("CHuR", 2, 2,muRG)
            + 212.376 * getSMEFTCoeff("CHdR", 2, 2,muRG)
            + 50.12 * getSMEFTCoeff("CHl3R", 2, 2,muRG)
            - 16976.3 * getSMEFTCoeff("CHq3R", 2, 2,muRG)
            - 373.856 * getSMEFTCoeff("CeHR", 2, 2,muRG)
            - 2953.05 * getSMEFTCoeff("CuHR", 1, 1,muRG)
            + 6636.34 * getSMEFTCoeff("CuHR", 2, 2,muRG)
            - 6121.66 * getSMEFTCoeff("CdHR", 2, 2,muRG)
            - 111254. * getSMEFTCoeff("CHD",muRG)
            - 162538. * getSMEFTCoeff("CHWB",muRG)
            - 96076.1 * delta_GF / v() / v()
            - 0.123 * deltaMwd6())
            );*/
 
    //AG:begin
    // Ref: https://arxiv.org/pdf/1903.12046.pdf
    double cHbox = getSMEFTCoeffEW("CHbox");
    double cHD = getSMEFTCoeffEW("CHD");
    double cHW = getSMEFTCoeffEW("CHW");
    double cHB = getSMEFTCoeffEW("CHB");
    double cHWB = getSMEFTCoeffEW("CHWB");
    double cW = getSMEFTCoeffEW("CW");
    double cHu33 = getSMEFTCoeffEW("CHuR", 2, 2);
    double cuH33 = getSMEFTCoeffEW("CuHR", 2, 2);
    double cdH33 = getSMEFTCoeffEW("CdHR", 2, 2);
    double cuB33 = getSMEFTCoeffEW("CuBR", 2, 2);
    double cuW22 = getSMEFTCoeffEW("CuWR", 1, 1);
    double cuW33 = getSMEFTCoeffEW("CuWR", 2, 2);
    double cdW33 = getSMEFTCoeffEW("CdWR", 2, 2);
    double cHq133 = getSMEFTCoeffEW("CHq1R", 2, 2);
    double cHq333 = getSMEFTCoeffEW("CHq3R", 2, 2);
    double cHl311 = getSMEFTCoeffEW("CHl3R", 0, 0);
    double cHl322 = getSMEFTCoeffEW("CHl3R", 1, 1);
    double cLL = getSMEFTCoeffEW("CllR", 0, 1, 1, 0);
 
    //dwidth += cWsch * (   // Allow it in both schemes until alpha is ready
    dwidth += (
            (-0.01 * cdH33
            - 0.01 * cdW33
            + 14.6799 * cHB
            + 0.12 * cHbox
            - 0.12 * cHD
            - 0.18 * cHl311
            - 0.18 * cHl322
            + 0.02 * cHq133
            - 0.02 * cHq333
            + 0.02 * cHu33
            - 14.7471 * cHW
            + 9.20962 * cHWB
            + 0.18 * cLL
            - 0.0745564 * cuB33
            + 0.01 * cuH33
            - 0.01 * cuW22
            + 0.461895 * cuW33
            - 0.0772181 * cW)*1000000
            );
 
    //std::cout<<"deltaG1_hZA()="<<deltaG1_hZA()<<std::endl;
    //std::cout<<"delta_GF="<<delta_GF<<std::endl;
    //std::cout<<"delta_AZ="<<delta_AZ<<std::endl;
    //std::cout<<"eeMz="<<eeMz<<std::endl;
    //std::cout<<"sW_tree="<<sW_tree<<std::endl;
    //std::cout<<"cW_tree="<<cW_tree<<std::endl;
    //std::cout<<"v2="<<v2<<std::endl;
    //std::cout<<"cAsch="<<cAsch<<std::endl;
    //std::cout<<"cWsch="<<cWsch<<std::endl;
    //std::cout<<"Mw_inp="<<Mw_inp<<std::endl;
    //std::cout<<"Mz="<<Mz<<std::endl;
    //std::cout<<"GF="<<GF<<std::endl;
    //std::cout<<"aleMz="<<aleMz<<std::endl;
 
    //AG:end
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (+1. * deltaa0()
            - 0.629 * deltaaMZ()
            + 2.629 * deltaGmu()
            - 4.926 * deltaMz()
            + 0.004 * deltaaSMZ()
            + 11.167 * deltaMh()
            + 0.013 * deltamt()
            + 0.004 * deltamb()
            + 0.001 * deltamc()
            + 0. * deltamtau());
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZgaint + eHZgapar;
 
    return dwidth;
}

◆ deltaGammaHZgaRatio2()

const double NPSMEFTd6General::deltaGammaHZgaRatio2 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to Z\gamma)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Z\gamma)$/ $\Gamma(H\to Z\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28051 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHZllRatio1()

const double NPSMEFTd6General::deltaGammaHZllRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Zll)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Zll)$/ $\Gamma(H\to Zll)_{\mathrm{SM}}$

Definition at line 26746 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+121715. * getSMEFTCoeff("CHbox",muRG)
            + 8726.9 * (1.0 / 2.0) * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl1R", 1, 1,muRG))
            - 7315.2 * (1.0 / 2.0) * (getSMEFTCoeff("CHeR", 0, 0,muRG) + getSMEFTCoeff("CHeR", 1, 1,muRG))
            + 8726.9 * (1.0 / 2.0) * (getSMEFTCoeff("CHl3R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG))
            - 5544.15 * getSMEFTCoeff("CHD",muRG)
            - 13560.9 * getSMEFTCoeff("CHB",muRG)
            - 45585.2 * getSMEFTCoeff("CHW",muRG)
            - 53507.9 * getSMEFTCoeff("CHWB",muRG)
            - 2.204 * delta_GF);
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    //dwidth += cHSM * ( 0.0 ); 
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    //dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZllRatio2()

const double NPSMEFTd6General::deltaGammaHZllRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Zll)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Zll)$/ $\Gamma(H\to Zll)_{\mathrm{SM}}$

Definition at line 26776 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHZmumuRatio1()

const double NPSMEFTd6General::deltaGammaHZmumuRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Z\mu\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Z\mu\mu)$/ $\Gamma(H\to Z\mu\mu)_{\mathrm{SM}}$

Definition at line 26882 of file NPSMEFTd6General.cpp.

                                                            {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //  Derived from the HZll expression for l=mu only
 
    dwidth += (+121715. * getSMEFTCoeff("CHbox",muRG)
            + 8726.9 * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            - 7315.2 * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + 8726.9 * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            - 5544.15 * getSMEFTCoeff("CHD",muRG)
            - 13560.9 * getSMEFTCoeff("CHB",muRG)
            - 45585.2 * getSMEFTCoeff("CHW",muRG)
            - 53507.9 * getSMEFTCoeff("CHWB",muRG)
            - 2.204 * delta_GF);
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    //dwidth += cHSM * ( 0.0 ); 
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    //dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZmumuRatio2()

const double NPSMEFTd6General::deltaGammaHZmumuRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Z\mu\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Z\mu\mu)$/ $\Gamma(H\to Z\mu\mu)_{\mathrm{SM}}$

Definition at line 26914 of file NPSMEFTd6General.cpp.

                                                            {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHZuuRatio1()

const double NPSMEFTd6General::deltaGammaHZuuRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Z u u)$ ( $u=u,c $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Z u u)$/ $\Gamma(H\to Z u u)_{\mathrm{SM}}$

Definition at line 27439 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+121512. * getSMEFTCoeff("CHbox",muRG)
            - 9648.28 * (1.0 / 2.0) * (getSMEFTCoeff("CHq1R", 0, 0,muRG) + getSMEFTCoeff("CHq1R", 1, 1,muRG))
            + 4218.6 * (1.0 / 2.0) * (getSMEFTCoeff("CHuR", 0, 0,muRG) + getSMEFTCoeff("CHuR", 1, 1,muRG))
            + 9648.28 * (1.0 / 2.0) * (getSMEFTCoeff("CHq3R", 0, 0,muRG) + getSMEFTCoeff("CHq3R", 1, 1,muRG))
            - 17762.5 * getSMEFTCoeff("CHD",muRG)
            - 13473.3 * getSMEFTCoeff("CHB",muRG)
            - 45667.9 * getSMEFTCoeff("CHW",muRG)
            - 110057. * getSMEFTCoeff("CHWB",muRG)
            - 2.6 * delta_GF);
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    //dwidth += cHSM * ( 0.0 ); 
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    //dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZuuRatio2()

const double NPSMEFTd6General::deltaGammaHZuuRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Z u u)$ ( $u=u,c $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Z u u)$/ $\Gamma(H\to Z u u)_{\mathrm{SM}}$

Definition at line 27469 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHZvvRatio1()

const double NPSMEFTd6General::deltaGammaHZvvRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Z\nu\nu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Z\nu\nu)$/ $\Gamma(H\to Z\nu\nu)_{\mathrm{SM}}$

Definition at line 27278 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+121530. * getSMEFTCoeff("CHbox",muRG)
            - 7943.34 * (1.0 / 3.0) * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl1R", 2, 2,muRG))
            + 7943.34 * (1.0 / 3.0) * (getSMEFTCoeff("CHl3R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 2, 2,muRG))
            - 229.41 * getSMEFTCoeff("CHD",muRG)
            - 13535.2 * getSMEFTCoeff("CHB",muRG)
            - 45480.6 * getSMEFTCoeff("CHW",muRG)
            - 24891. * getSMEFTCoeff("CHWB",muRG)
            - 2. * delta_GF);
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    //dwidth += cHSM * ( 0.0 ); 
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    //dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZvvRatio2()

const double NPSMEFTd6General::deltaGammaHZvvRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to Z\nu\nu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to Z\nu\nu)$/ $\Gamma(H\to Z\nu\nu)_{\mathrm{SM}}$

Definition at line 27307 of file NPSMEFTd6General.cpp.

                                                          {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHZZ2e2muRatio1()

const double NPSMEFTd6General::deltaGammaHZZ2e2muRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 2e2\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 2e2\mu)$/ $\Gamma(H\to ZZ* \to 2e2\mu)_{\mathrm{SM}}$

Definition at line 27112 of file NPSMEFTd6General.cpp.

                                                              {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+120836. * getSMEFTCoeff("CHbox",muRG)
            + 126374. * (1.0 / 2.0) * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl1R", 1, 1,muRG))
            - 109064. * (1.0 / 2.0) * (getSMEFTCoeff("CHeR", 0, 0,muRG) + getSMEFTCoeff("CHeR", 1, 1,muRG))
            + 126374. * (1.0 / 2.0) * (getSMEFTCoeff("CHl3R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG))
            - 42370.4 * getSMEFTCoeff("CHD",muRG)
            - 14299. * getSMEFTCoeff("CHB",muRG)
            - 47298.2 * getSMEFTCoeff("CHW",muRG)
            - 83098.2 * getSMEFTCoeff("CHWB",muRG)
            - 3.378 * delta_GF
            - 0.85 * deltaGzd6());
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (-10.07 * deltaMz()
            + 15.626 * deltaMh()
            - 0.128 * deltaaMZ()
            + 2.258 * deltaGmu());
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZZ2e2muRatio2()

const double NPSMEFTd6General::deltaGammaHZZ2e2muRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 2e2\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 2e2\mu)$/ $\Gamma(H\to ZZ* \to 2e2\mu)_{\mathrm{SM}}$

Definition at line 27146 of file NPSMEFTd6General.cpp.

                                                              {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHZZ4dRatio1()

const double NPSMEFTd6General::deltaGammaHZZ4dRatio1 ( ) const

inline

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4 d)$ ( $d=d,s,b $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4 d)$/ $\Gamma(H\to ZZ* \to 4 d)_{\mathrm{SM}}$

Definition at line 2865 of file NPSMEFTd6General.h.

                                               {
        return 0.0;
    };

◆ deltaGammaHZZ4dRatio2()

const double NPSMEFTd6General::deltaGammaHZZ4dRatio2 ( ) const

inline

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4 d)$ ( $d=d,s,b $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4 d)$/ $\Gamma(H\to ZZ* \to 4 d)_{\mathrm{SM}}$

Definition at line 2875 of file NPSMEFTd6General.h.

                                               {
        return 0.0;
    };

◆ deltaGammaHZZ4eRatio1()

const double NPSMEFTd6General::deltaGammaHZZ4eRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4e)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4e)$/ $\Gamma(H\to ZZ* \to 4e)_{\mathrm{SM}}$

Definition at line 27029 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+121386. * getSMEFTCoeff("CHbox",muRG)
            + 123413. * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            - 103717. * getSMEFTCoeff("CHeR", 0, 0,muRG)
            + 123413. * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            - 44056.9 * getSMEFTCoeff("CHD",muRG)
            - 13385.3 * getSMEFTCoeff("CHB",muRG)
            - 45127.7 * getSMEFTCoeff("CHW",muRG)
            - 91708.7 * getSMEFTCoeff("CHWB",muRG)
            - 3.462 * delta_GF
            - 0.769 * deltaGzd6());
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (-9.228 * deltaMz()
            + 15.148 * deltaMh()
            - 0.229 * deltaaMZ()
            + 2.493 * deltaGmu());
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZZ4eRatio2()

const double NPSMEFTd6General::deltaGammaHZZ4eRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4e)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4e)$/ $\Gamma(H\to ZZ* \to 4e)_{\mathrm{SM}}$

Definition at line 27063 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHZZ4fRatio1()

const double NPSMEFTd6General::deltaGammaHZZ4fRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4f)$/ $\Gamma(H\to ZZ* \to 4f)_{\mathrm{SM}}$

Definition at line 27711 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    //------ Old alpha scheme expression: Beg
    double CZff, sf;
 
    CZff = gZvL * (-0.5 * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl1R", 2, 2,muRG) - getSMEFTCoeff("CHl3R", 0, 0,muRG) - getSMEFTCoeff("CHl3R", 1, 1,muRG) - getSMEFTCoeff("CHl3R", 2, 2,muRG)) * v2) +
            gZlL * (-0.5 * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl1R", 2, 2,muRG) + getSMEFTCoeff("CHl3R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 2, 2,muRG)) * v2) +
            gZlR * (-0.5 * (getSMEFTCoeff("CHeR", 0, 0,muRG) + getSMEFTCoeff("CHeR", 1, 1,muRG) + getSMEFTCoeff("CHeR", 2, 2,muRG)) * v2) +
            Nc * (
            gZdL * (-0.5 * (getSMEFTCoeff("CHq1R", 0, 0,muRG) + getSMEFTCoeff("CHq1R", 1, 1,muRG) + getSMEFTCoeff("CHq1R", 2, 2,muRG) + getSMEFTCoeff("CHq3R", 0, 0,muRG) + getSMEFTCoeff("CHq3R", 1, 1,muRG) + getSMEFTCoeff("CHq3R", 2, 2,muRG)) * v2) +
            gZdR * (-0.5 * (getSMEFTCoeff("CHdR", 0, 0,muRG) + getSMEFTCoeff("CHdR", 1, 1,muRG) + getSMEFTCoeff("CHdR", 2, 2,muRG)) * v2) +
            gZuL * (-0.5 * (getSMEFTCoeff("CHq1R", 0, 0,muRG) + getSMEFTCoeff("CHq1R", 1, 1,muRG) - getSMEFTCoeff("CHq3R", 0, 0,muRG) - getSMEFTCoeff("CHq3R", 1, 1,muRG)) * v2) +
            gZuR * (-0.5 * (getSMEFTCoeff("CHuR", 0, 0,muRG) + getSMEFTCoeff("CHuR", 1, 1,muRG)) * v2)
            );
 
    CZff = CZff / (
            3.0 * (gZvL * gZvL + gZlL * gZlL + gZlR * gZlR) +
            Nc * (3.0 * (gZdL * gZdL + gZdR * gZdR) + 2.0 * (gZuL * gZuL + gZuR * gZuR))
            );
 
    sf = -11267.6 * (1.0 / 3.0) * (
            3.0 * (gZvL * gZvL + gZlL * gZlL + gZlR * gZlR) +
            Nc * (3.0 * (gZdL * gZdL + gZdR * gZdR) + 2.0 * (gZuL * gZuL + gZuR * gZuR))
            );
 
    sf = sf / (-0.5 * (gZlL + gZvL) * v2); // Coefficient of the CZff term. From the getSMEFTCoeff("CHl1R",0,0) term in the ME.
 
    dwidth += cAsch * (+121373. * getSMEFTCoeff("CHbox",muRG)
            + sf * CZff
            - 50927.1 * getSMEFTCoeff("CHD",muRG)
            - 14137.9 * getSMEFTCoeff("CHB",muRG)
            - 46350.1 * getSMEFTCoeff("CHW",muRG)
            - 126336. * getSMEFTCoeff("CHWB",muRG)
            - 3.715 * delta_GF
            - 0.834 * deltaGzd6()
            );
    
    //------ Old alpha scheme expression: End
 
    //AG:begin
    dwidth += cWsch * (
            ((0.12104) * getSMEFTCoeff("CHbox",muRG)
            + (-0.02372) * getSMEFTCoeff("CHW",muRG)
            + (-0.03647) * getSMEFTCoeff("CHB",muRG)
            + (-0.016569) * getSMEFTCoeff("CHD",muRG)
            + (-0.021999) * getSMEFTCoeff("CHWB",muRG)
            + (-0.017927) * getSMEFTCoeff("CHl1R", 0, 0,muRG)
            + (-0.017925) * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            + (-0.1213776) * getSMEFTCoeff("CHl3R", 0, 0,muRG)
            + (-0.1215437) * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            + (-0.01686521) * getSMEFTCoeff("CHeR", 0, 0,muRG)
            + (-0.01688863) * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + (0.18165) * getSMEFTCoeff("CllR", 0, 1, 1, 0,muRG)) * 1000000
            );
 
    dwidth += cWsch * (+(-0.797) * deltaGzd6());
 
    //AG:end
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (-9.548 * deltaMz()
            + 15.799 * deltaMh()
            - 0.412 * deltaaMZ()
            + 2.569 * deltaGmu());
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZZ4fRatio2()

const double NPSMEFTd6General::deltaGammaHZZ4fRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4f)$/ $\Gamma(H\to ZZ* \to 4f)_{\mathrm{SM}}$

Definition at line 27791 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += cWsch * (
                +(0.01438) * pow(getSMEFTCoeffEW("CHbox"), 2.0)
                + (0.4094) * pow(getSMEFTCoeffEW("CHW"), 2.0)
                + (1.1627) * pow(getSMEFTCoeffEW("CHB"), 2.0)
                + (0.00456) * pow(getSMEFTCoeffEW("CHD"), 2.0)
                + (0.378) * pow(getSMEFTCoeffEW("CHWB"), 2.0)
                + (0.001943) * pow(getSMEFTCoeffEW("CHl1R", 0, 0), 2.0)
                + (0.001583) * pow(getSMEFTCoeffEW("CHl1R", 1, 1), 2.0)
                + (0.005694) * pow(getSMEFTCoeffEW("CHl3R", 0, 0), 2.0)
                + (0.00575) * pow(getSMEFTCoeffEW("CHl3R", 1, 1), 2.0)
                + (0.000979) * pow(getSMEFTCoeffEW("CHeR", 0, 0), 2.0)
                + (0.0009751) * pow(getSMEFTCoeffEW("CHeR", 1, 1), 2.0)
                + (0.01079) * pow(getSMEFTCoeffEW("CllR", 0, 1, 1, 0), 2.0)
                + (-0.002848) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHW")
                + (-0.004447) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHB")
                + (-0.005693) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHD")
                + (-0.0026556) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHWB")
                + (-0.00229) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.002115) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.00740797) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.007346) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.001997847) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.002008333) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0.0146) * getSMEFTCoeffEW("CHbox") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.23185) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHB")
                + (0.016075) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHD")
                + (-0.696823) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHWB")
                + (0.0014623) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.001441) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.000525) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.000586) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.001284) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.001275) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.002852) * getSMEFTCoeffEW("CHW") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.013314) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHD")
                + (-0.42542) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHWB")
                + (0.000223) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.000233) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.001511) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.001507) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0002824) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0002599) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.004446) * getSMEFTCoeffEW("CHB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00184) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHWB")
                + (0.0016472) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0016545) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0043953) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0043919) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0016695) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0016726) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.002015) * getSMEFTCoeffEW("CHD") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.002499) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.002498) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0016531) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0016563) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0024083) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.0024057) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.0026557) * getSMEFTCoeffEW("CHWB") * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.00041) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0021669) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.002104) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.00229) * getSMEFTCoeffEW("CHl1R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.002018) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.0021733) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (-0.002115) * getSMEFTCoeffEW("CHl1R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.0034) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.0019783) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.001986) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.0147319) * getSMEFTCoeffEW("CHl3R", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (0.0019818) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.00198) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.01463445) * getSMEFTCoeffEW("CHl3R", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.001997847) * getSMEFTCoeffEW("CHeR", 0, 0) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                + (-0.002008333) * getSMEFTCoeffEW("CHeR", 1, 1) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                ) * pow(1000000.0, 2.0);
 
        dwidth += cWsch * ((0.71) * pow(deltaGzd6(), 2.0));
 
        dwidth += cWsch * (
                +(-0.095) * deltaGzd6() * getSMEFTCoeffEW("CHbox")
                + (0.0101) * deltaGzd6() * getSMEFTCoeffEW("CHW")
                + (0.0301) * deltaGzd6() * getSMEFTCoeffEW("CHB")
                + (0.01178) * deltaGzd6() * getSMEFTCoeffEW("CHD")
                + (0.023) * deltaGzd6() * getSMEFTCoeffEW("CHWB")
                + (0.016) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (0.0179) * deltaGzd6() * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (0.0971) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (0.078) * deltaGzd6() * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.01439) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 0, 0)
                + (0.01349) * deltaGzd6() * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.143) * deltaGzd6() * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                )*1000000;
 
    }
 
    return dwidth;
}

◆ deltaGammaHZZ4lRatio1()

const double NPSMEFTd6General::deltaGammaHZZ4lRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4l)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4l)$/ $\Gamma(H\to ZZ* \to 4l)_{\mathrm{SM}}$

Definition at line 26939 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    double CZll, sf;
 
    CZll = gZlL * (-0.5 * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG)) * v2) +
            gZlR * (-0.5 * (getSMEFTCoeff("CHeR", 0, 0,muRG) + getSMEFTCoeff("CHeR", 1, 1,muRG)) * v2);
 
    CZll = CZll / (2.0 * (gZlL * gZlL + gZlR * gZlR));
 
    sf = 124479. * (1.0 / 2.0) * (2.0 * (gZlL * gZlL + gZlR * gZlR)) / (-0.5 * gZlL * v2); // Coefficient of the CZll term. From the getSMEFTCoeff("CHl1R",0,0) term in the ME.
 
    dwidth += (+122273. * getSMEFTCoeff("CHbox",muRG)
            + sf * CZll
            - 44025.7 * getSMEFTCoeff("CHD",muRG)
            - 13602.6 * getSMEFTCoeff("CHB",muRG)
            - 45248.6 * getSMEFTCoeff("CHW",muRG)
            - 88372.1 * getSMEFTCoeff("CHWB",muRG)
            - 3.462 * delta_GF
            - 0.808 * deltaGzd6());
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (-9.734 * deltaMz()
            + 15.37 * deltaMh()
            - 0.154 * deltaaMZ()
            + 2.339 * deltaGmu());
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZZ4lRatio2()

const double NPSMEFTd6General::deltaGammaHZZ4lRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4l)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4l)$/ $\Gamma(H\to ZZ* \to 4l)_{\mathrm{SM}}$

Definition at line 26980 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHZZ4muRatio1()

const double NPSMEFTd6General::deltaGammaHZZ4muRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4\mu)$/ $\Gamma(H\to ZZ* \to 4\mu)_{\mathrm{SM}}$

Definition at line 27195 of file NPSMEFTd6General.cpp.

                                                            {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+120688. * getSMEFTCoeff("CHbox",muRG)
            + 123059. * getSMEFTCoeff("CHl1R", 1, 1,muRG)
            - 103862. * getSMEFTCoeff("CHeR", 1, 1,muRG)
            + 123059. * getSMEFTCoeff("CHl3R", 1, 1,muRG)
            - 43977.1 * getSMEFTCoeff("CHD",muRG)
            - 13575.5 * getSMEFTCoeff("CHB",muRG)
            - 45200.8 * getSMEFTCoeff("CHW",muRG)
            - 91625.2 * getSMEFTCoeff("CHWB",muRG)
            - 3.471 * delta_GF
            - 0.774 * deltaGzd6());
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (-9.254 * deltaMz()
            + 15.109 * deltaMh()
            - 0.207 * deltaaMZ()
            + 2.405 * deltaGmu());
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZZ4muRatio2()

const double NPSMEFTd6General::deltaGammaHZZ4muRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4\mu)$/ $\Gamma(H\to ZZ* \to 4\mu)_{\mathrm{SM}}$

Definition at line 27229 of file NPSMEFTd6General.cpp.

                                                            {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHZZ4uRatio1()

const double NPSMEFTd6General::deltaGammaHZZ4uRatio1 ( ) const

inline

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4 u)$ ( $u=u,c $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4 u)$/ $\Gamma(H\to ZZ* \to 4 u)_{\mathrm{SM}}$

Definition at line 2803 of file NPSMEFTd6General.h.

                                               {
        return 0.0;
    };

◆ deltaGammaHZZ4uRatio2()

const double NPSMEFTd6General::deltaGammaHZZ4uRatio2 ( ) const

inline

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4 u)$ ( $u=u,c $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4 u)$/ $\Gamma(H\to ZZ* \to 4 u)_{\mathrm{SM}}$

Definition at line 2813 of file NPSMEFTd6General.h.

                                               {
        return 0.0;
    };

◆ deltaGammaHZZ4vRatio1()

const double NPSMEFTd6General::deltaGammaHZZ4vRatio1 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4\nu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4\nu)$/ $\Gamma(H\to ZZ* \to 4\nu)_{\mathrm{SM}}$

Definition at line 27356 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
 
    double C1 = 0.0083;
    double muRG = 125.1;
 
    dwidth += (+120596. * getSMEFTCoeff("CHbox",muRG)
            - 115532. * (1.0 / 3.0) * (getSMEFTCoeff("CHl1R", 0, 0,muRG) + getSMEFTCoeff("CHl1R", 1, 1,muRG) + getSMEFTCoeff("CHl1R", 2, 2,muRG))
            + 115532. * (1.0 / 3.0) * (getSMEFTCoeff("CHl3R", 0, 0,muRG) + getSMEFTCoeff("CHl3R", 1, 1,muRG) + getSMEFTCoeff("CHl3R", 2, 2,muRG))
            - 28744.1 * getSMEFTCoeff("CHD",muRG)
            - 13816.7 * getSMEFTCoeff("CHB",muRG)
            - 44782.1 * getSMEFTCoeff("CHW",muRG)
            - 25256.6 * getSMEFTCoeff("CHWB",muRG)
            - 3.013 * delta_GF
            - 0.787 * deltaGzd6()
            );
 
    //  Linear contribution from Higgs self-coupling
    dwidth += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    // Add modifications due to small variations of the SM parameters    
    dwidth += cHSM * (-10.49 * deltaMz()
            + 15.294 * deltaMh()
            + 0.255 * deltaaMZ()
            + 1.979 * deltaGmu());
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZZ4vRatio2()

const double NPSMEFTd6General::deltaGammaHZZ4vRatio2 ( ) const

The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4\nu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ* \to 4\nu)$/ $\Gamma(H\to ZZ* \to 4\nu)_{\mathrm{SM}}$

Definition at line 27390 of file NPSMEFTd6General.cpp.

                                                           {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaHZZRatio1()

const double NPSMEFTd6General::deltaGammaHZZRatio1 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to ZZ)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ)$/ $\Gamma(H\to ZZ)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 26697 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
 
    //    double C1 = 0.0083;
 
    dwidth = deltaGammaHZZ4fRatio1();
 
    //  Linear contribution from Higgs self-coupling
    //    dwidth += cLHd6*(C1 + 2.0*dZH1)*deltaG_hhhRatio();
    //  Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
    //    dwidth += cLHd6*cLH3d62*dZH2*deltaG_hhhRatio()*deltaG_hhhRatio();
 
    // SM (1) + intrinsic + parametric theory relative errors (free pars)    
    //    dwidth += eHZZint + eHZZpar;
 
    return dwidth;
 
}

◆ deltaGammaHZZRatio2()

const double NPSMEFTd6General::deltaGammaHZZRatio2 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H\to ZZ)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns: $\delta \Gamma(H\to ZZ)$/ $\Gamma(H\to ZZ)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 26716 of file NPSMEFTd6General.cpp.

                                                         {
    double dwidth = 0.0;
    if (FlagQuadraticTerms) {
        //Contributions that are quadratic in the effective coefficients
        dwidth += 0.0;
    }
 
    return dwidth;
}

◆ deltaGammaTotalRatio1()

const double NPSMEFTd6General::deltaGammaTotalRatio1 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H)$ in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.

Returns: $\delta \Gamma(H)$/ $\Gamma(H)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 25891 of file NPSMEFTd6General.cpp.

                                                           {
    double deltaGammaRatio;
 
    //  The change in the ratio assuming only SM decays
    deltaGammaRatio = (trueSM.computeBrHtogg() * deltaGammaHggRatio1()
            //            + trueSM.computeBrHtoWW() * deltaGammaHWWRatio1()
            //            + trueSM.computeBrHtoZZ() * deltaGammaHZZRatio1()
            + trueSM.computeBrHto4f() * deltaGammaH4fRatio1()
            + trueSM.computeBrHtoZga() * deltaGammaHZgaRatio1()
            + trueSM.computeBrHtogaga() * deltaGammaHgagaRatio1()
            + trueSM.computeBrHtomumu() * deltaGammaHmumuRatio1()
            + trueSM.computeBrHtotautau() * deltaGammaHtautauRatio1()
            + trueSM.computeBrHtocc() * deltaGammaHccRatio1()
            + trueSM.computeBrHtoss() * deltaGammaHssRatio1()
            + trueSM.computeBrHtobb() * deltaGammaHbbRatio1());
 
    //  Add the effect of the invisible and exotic BR. Include also here the
    //  pure contribution from BrHinv and BrHexo even in case of no dim 6 contributions    
    deltaGammaRatio = -1.0 + (1.0 + deltaGammaRatio) / (1.0 - BrHinv - BrHexo);
 
    //std::cout<<"deltaGammaHggRatio1()="<<deltaGammaHggRatio1()<<std::endl;
    //std::cout<<"deltaGammaH4fRatio1()="<<deltaGammaH4fRatio1()<<std::endl;
    //std::cout<<"deltaGammaHZgaRatio1()="<<deltaGammaHZgaRatio1()<<std::endl;
    //std::cout<<"deltaGammaHgagaRatio1()="<<deltaGammaHgagaRatio1()<<std::endl;
    //std::cout<<"deltaGammaHmumuRatio1()="<<deltaGammaHmumuRatio1()<<std::endl;
    //std::cout<<"deltaGammaHtautauRatio1()="<<deltaGammaHtautauRatio1()<<std::endl;
    //std::cout<<"deltaGammaHccRatio1()="<<deltaGammaHccRatio1()<<std::endl;
    //std::cout<<"deltaGammaHbbRatio1()="<<deltaGammaHbbRatio1()<<std::endl;
 
    return deltaGammaRatio;
}

◆ deltaGammaTotalRatio1noError()

const double NPSMEFTd6General::deltaGammaTotalRatio1noError ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H)$ in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors.

Returns: $\delta \Gamma(H)$/ $\Gamma(H)_{\mathrm{SM}}$

Definition at line 25923 of file NPSMEFTd6General.cpp.

                                                                  {
    double deltaGammaRatio;
 
    //  The change in the ratio assuming only SM decays
    deltaGammaRatio = (trueSM.computeBrHtogg() * (deltaGammaHggRatio1() - eHggint - eHggpar)
            //            + trueSM.computeBrHtoWW() * (deltaGammaHWWRatio1() - eHWWint - eHWWpar )
            //            + trueSM.computeBrHtoZZ() * (deltaGammaHZZRatio1() - eHZZint - eHZZpar )          
            + trueSM.computeBrHto4f() * deltaGammaH4fRatio1()
            - trueSM.computeBrHtoWW() * (eHWWint + eHWWpar)
            - trueSM.computeBrHtoZZ() * (eHZZint + eHZZpar)
            + trueSM.computeBrHtoZga() * (deltaGammaHZgaRatio1() - eHZgaint - eHZgapar)
            + trueSM.computeBrHtogaga() * (deltaGammaHgagaRatio1() - eHgagaint - eHgagapar)
            + trueSM.computeBrHtomumu() * (deltaGammaHmumuRatio1() - eHmumuint - eHmumupar)
            + trueSM.computeBrHtotautau() * (deltaGammaHtautauRatio1() - eHtautauint - eHtautaupar)
            + trueSM.computeBrHtocc() * (deltaGammaHccRatio1() - eHccint - eHccpar)
            + trueSM.computeBrHtoss() * (deltaGammaHssRatio1() - eHssint - eHsspar)
            + trueSM.computeBrHtobb() * (deltaGammaHbbRatio1() - eHbbint - eHbbpar));
 
    //  Add the effect of the invisible and exotic BR. Include also here the
    //  pure contribution from BrHinv and BrHexo even in case of no dim 6 contributions    
    deltaGammaRatio = -1.0 + (1.0 + deltaGammaRatio) / (1.0 - BrHinv - BrHexo);
 
    return deltaGammaRatio;
}

◆ deltaGammaTotalRatio2()

const double NPSMEFTd6General::deltaGammaTotalRatio2 ( ) const

virtual

The new physics contribution to the ratio of the $\Gamma(H)$ in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients.

Returns: $\delta \Gamma(H)$/ $\Gamma(H)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 25948 of file NPSMEFTd6General.cpp.

                                                           {
    double deltaGammaRatio = 0.0;
 
    if (FlagQuadraticTerms) {
        //  The change in the ratio assuming only SM decays
        deltaGammaRatio = trueSM.computeBrHtogg() * deltaGammaHggRatio2()
                //            + trueSM.computeBrHtoWW() * deltaGammaHWWRatio2()
                //            + trueSM.computeBrHtoZZ() * deltaGammaHZZRatio2()
                + trueSM.computeBrHto4f() * deltaGammaH4fRatio2()
                + trueSM.computeBrHtoZga() * deltaGammaHZgaRatio2()
                + trueSM.computeBrHtogaga() * deltaGammaHgagaRatio2()
                + trueSM.computeBrHtomumu() * deltaGammaHmumuRatio2()
                + trueSM.computeBrHtotautau() * deltaGammaHtautauRatio2()
                + trueSM.computeBrHtocc() * deltaGammaHccRatio2()
                + trueSM.computeBrHtoss() * deltaGammaHssRatio2()
                + trueSM.computeBrHtobb() * deltaGammaHbbRatio2();
 
        //  Add the effect of the invisible and exotic BR and return     
        deltaGammaRatio = (deltaGammaRatio / (1.0 - BrHinv - BrHexo));
    }
    return deltaGammaRatio;
}

◆ DeltaGF()

const double NPSMEFTd6General::DeltaGF ( ) const

virtual

New physics contribution to the Fermi constant.

The new physics contribution $\Delta G$ is defined as

\[ G_\mu = G_{\mu,\mathrm{SM}}(1+\Delta G)\,, \]

where $G_\mu$ is the experimental value measured through muon decays, and $G_{\mu,\mathrm{SM}}$ is the Fermi constant in the SM.

Returns: $\Delta G$

Reimplemented from NPbase.

Definition at line 15327 of file NPSMEFTd6General.cpp.

                                             {
    return ((getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1) - 0.5 * (getSMEFTCoeffEW("CllR", 0, 1, 1, 0) + getSMEFTCoeffEW("CllR", 1, 0, 0, 1))) * v2);
}

◆ deltaGL_f()

const double NPSMEFTd6General::deltaGL_f ( const Particle p ) const

New physics contribution to the neutral-current left-handed coupling $g_L^f$.

Parameters

[in] f a lepton or quark

Returns: $\delta g_L^f$

Definition at line 17023 of file NPSMEFTd6General.cpp.

                                                               {
    double I3p = p.getIsospin(), Qp = p.getCharge();
    double CHF1 = CHF1_diag(p);
    double CHF3 = CHF3_diag(p);
    double NPindirect;
 
    //    NPindirect = -I3p / 4.0 * (getSMEFTCoeffEW("CHD") * v2_over_LambdaNP2 + 2.0 * delta_GF)
    //                - Qp * sW2_tree / 4.0 / (cW2_tree - sW2_tree)
    //                *((4.0 * cW_tree / sW_tree * getSMEFTCoeffEW("CHWB") + getSMEFTCoeffEW("CHD")) * v2_over_LambdaNP2 + 2.0 * delta_GF);
 
    NPindirect = (I3p - Qp * sW2_tree) * delta_UgNC + Qp * delta_QgNC;
 
    double NPdirect = -0.5 * (CHF1 - 2.0 * I3p * CHF3) * v2;
    return (NPindirect + NPdirect);
}

◆ deltaGL_f_mu()

const double NPSMEFTd6General::deltaGL_f_mu	(	const Particle	p,
		const double	mu
	)		const

New physics contribution to the neutral-current left-handed coupling $g_L^f$.

Parameters

[in]	f	a lepton or quark
[in]	mu	the RG scale to be used in the evaluation

Returns: $\delta g_L^f(\mu)$

Definition at line 17054 of file NPSMEFTd6General.cpp.

                                                                                   {
    double I3p = p.getIsospin(), Qp = p.getCharge();
    double CHF;
    double NPindirect;
    
    // Parameters from the indirect corrections depending on the RG scale
    double d_UgNC_mu, d_QgNC_mu;
    
    //  NP indirect corrections to EW fermion couplings
    d_UgNC_mu = delU_gNC(mu);
    d_QgNC_mu = delQ_gNC(mu);    
    
    NPindirect = (I3p - Qp * sW2_tree) * d_UgNC_mu + Qp * d_QgNC_mu;
    
    // Direct contribution  
    switch(p.getIndex()){
    //if (p.is("NEUTRINO_1"))
        case 0:
            CHF = getSMEFTCoeff("CHl1R", 0, 0, mu) - getSMEFTCoeff("CHl3R", 0, 0, mu);
            break;
    //else if (p.is("ELECTRON"))
        case 1:
            CHF = getSMEFTCoeff("CHl1R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 0, 0, mu);
            break;
    //else if (p.is("NEUTRINO_2"))
        case 2:
            CHF = getSMEFTCoeff("CHl1R", 1, 1, mu) - getSMEFTCoeff("CHl3R", 1, 1, mu);
            break;
    //else if (p.is("MU"))
        case 3:
            CHF = getSMEFTCoeff("CHl1R", 1, 1, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu);
            break;
    //else if (p.is("NEUTRINO_3"))
        case 4:
            CHF = getSMEFTCoeff("CHl1R", 2, 2, mu) - getSMEFTCoeff("CHl3R", 2, 2, mu);
            break;
    //else if (p.is("TAU"))
        case 5:
            CHF = getSMEFTCoeff("CHl1R", 2, 2, mu) + getSMEFTCoeff("CHl3R", 2, 2, mu);
            break;
    //else if (p.is("UP"))
        case 6:
            CHF = getSMEFTCoeff("CHq1R", 0, 0, mu) - getSMEFTCoeff("CHq3R", 0, 0, mu);
            break;
        case 7:
            CHF = getSMEFTCoeff("CHq1R", 0, 0, mu) + getSMEFTCoeff("CHq3R", 0, 0, mu);
            break;
        case 8:
            CHF = getSMEFTCoeff("CHq1R", 1, 1, mu) - getSMEFTCoeff("CHq3R", 1, 1, mu);
            break;
    //else if (p.is("STRANGE"))
        case 9:
            CHF = getSMEFTCoeff("CHq1R", 1, 1, mu) + getSMEFTCoeff("CHq3R", 1, 1, mu);
            break;
    //else if (p.is("TOP"))
        case 10:
            CHF = getSMEFTCoeff("CHq1R", 2, 2, mu) - getSMEFTCoeff("CHq3R", 2, 2, mu);
            break;
    //else if (p.is("BOTTOM"))
        case 11:
            CHF = getSMEFTCoeff("CHq1R", 2, 2, mu) + getSMEFTCoeff("CHq3R", 2, 2, mu);
            break;
    //else
        default:
            throw std::runtime_error("NPSMEFTd6General::deltaGL_f_mu(): wrong argument");
    }
 
    double NPdirect = -0.5 * CHF * v2;
    return (NPindirect + NPdirect);
}

◆ deltaGL_Wff()

gslpp::complex NPSMEFTd6General::deltaGL_Wff	(	const Particle	pbar,
		const Particle	p
	)		const

virtual

New physics contribution to the charged current coupling $W_\mu \bar{f_L}\gamma^mu f_L$.

Parameters

[in]	pbar	a lepton or quark
[in]	p	a lepton or quark

Returns: $\delta g_{Wff}^{L}$

Reimplemented from NPbase.

Definition at line 17194 of file NPSMEFTd6General.cpp.

                                                                                      {
    if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
        throw std::runtime_error("NPSMEFTd6General::deltaGL_Wff(): Not implemented");
 
    //double CHF3 = CHF3_diag(pbar);
    gslpp::complex CHF3 = CHF3CC_diag(pbar);
    
    gslpp::complex NPindirect;
 
    //    NPindirect = -cW2_tree / 4.0 / (cW2_tree - sW2_tree)
    //                * ((4.0 * sW_tree / cW_tree * getSMEFTCoeffEW("CHWB") + getSMEFTCoeffEW("CHD")) * v2_over_LambdaNP2 + 2.0 * delta_GF);
 
    NPindirect = gslpp::complex(delta_UgCC, 0.0, false);
    
    return (NPindirect + CHF3 * v2 );
}

◆ deltaGL_Wff_mu()

gslpp::complex NPSMEFTd6General::deltaGL_Wff_mu	(	const Particle	pbar,
		const Particle	p,
		const double	mu
	)		const

virtual

New physics contribution to the charged current coupling $W_\mu \bar{f_L}\gamma^mu f_L$.

Parameters

[in]	pbar	a lepton or quark
[in]	p	a lepton or quark
[in]	mu	the RG scale to be used in the evaluation (for those models where it is available)

Returns: $\delta g_{Wff}^{L}$

Reimplemented from NPbase.

Definition at line 17220 of file NPSMEFTd6General.cpp.

                                                                                                          {
    if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
        throw std::runtime_error("NPSMEFTd6General::deltaGL_Wff(): Not implemented");
 
    double CHF3;
    double NPindirect;
 
    //  NP indirect corrections to EW fermion couplings
    NPindirect = delU_gCC(mu);
    
    // Direct contribution
    if (pbar.is("NEUTRINO_1") || pbar.is("ELECTRON"))
        CHF3 = getSMEFTCoeff("CHl3R", 0, 0, mu);
    else if (pbar.is("NEUTRINO_2") || pbar.is("MU"))
        CHF3 = getSMEFTCoeff("CHl3R", 1, 1, mu);
    else if (pbar.is("NEUTRINO_3") || pbar.is("TAU"))
        CHF3 = getSMEFTCoeff("CHl3R", 2, 2, mu);
    else if (pbar.is("UP") || pbar.is("DOWN"))
        CHF3 = getSMEFTCoeff("CHq3R", 0, 0, mu);
    else if (pbar.is("CHARM") || pbar.is("STRANGE"))
        CHF3 = getSMEFTCoeff("CHq3R", 1, 1, mu);
    else if (pbar.is("TOP") || pbar.is("BOTTOM"))
        CHF3 = getSMEFTCoeff("CHq3R", 2, 2, mu);
    else
        throw std::runtime_error("NPSMEFTd6General::deltaGL_Wff_mu(): wrong argument");
 
    double NPdirect = CHF3 * v2;
    return (NPindirect + NPdirect);
}

◆ deltaGL_Wffh()

gslpp::complex NPSMEFTd6General::deltaGL_Wffh	(	const Particle	pbar,
		const Particle	p
	)		const

The new physics contribution to the coupling of the effective interaction $H W_\mu \bar{f_L}\gamma^mu f_L$.

Parameters

[in]	pbar	a lepton or quark
[in]	p	a lepton or quark

Returns: $\delta g_{WffH}^{L}$

Definition at line 17810 of file NPSMEFTd6General.cpp.

                                                                                       {
    if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
        throw std::runtime_error("NPSMEFTd6General::deltaGL_Wffh(): Not implemented");
 
    //double CHF3 = CHF3_diag(pbar);
    gslpp::complex CHF3 = CHF3CC_diag(pbar);
    
    return (2.0 * sqrt(2.0) * Mz * cW_tree / v() / v() * CHF3 * v2);
}

◆ deltaGL_Zffh()

const double NPSMEFTd6General::deltaGL_Zffh ( const Particle p ) const

The new physics contribution to the coupling of the effective interaction $H Z_\mu \bar{f_L}\gamma^mu f_L$.

Parameters

[in] p a lepton or quark

Returns: $\delta g_{ZffH}^{L}$

Definition at line 17828 of file NPSMEFTd6General.cpp.

                                                                  {
    double I3p = p.getIsospin();
    double CHF1 = CHF1_diag(p);
    double CHF3 = CHF3_diag(p);
    return (-2.0 * Mz / v() / v() * (CHF1 - 2.0 * I3p * CHF3) * v2);
}

◆ deltaGmu()

const double NPSMEFTd6General::deltaGmu ( ) const

virtual

The relative correction to the muon decay constant, $\delta G_\mu/G_\mu$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $\delta G_\mu/G_\mu$

Definition at line 15508 of file NPSMEFTd6General.cpp.

                                              {
    //  Ref. value used in MG simulations
    return ( (GF - 1.16637 / 100000.0) / (1.16637 / 100000.0));
}

◆ deltaGmu2()

const double NPSMEFTd6General::deltaGmu2 ( ) const

virtual

The relative correction to the muon decay constant, $(\delta G_\mu/G_\mu)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $(\delta G_\mu/G_\mu)^2$

Definition at line 15513 of file NPSMEFTd6General.cpp.

                                               {
    return ( 0.0);
}

◆ deltaGR_f()

const double NPSMEFTd6General::deltaGR_f ( const Particle p ) const

New physics contribution to the neutral-current right-handed coupling $g_R^f$.

Parameters

[in] f a lepton or quark

Returns: $\delta g_R^f$

Definition at line 17039 of file NPSMEFTd6General.cpp.

                                                               {
    double Qp = p.getCharge();
    double CHf = CHf_diag(p);
    double NPindirect;
 
    //    NPindirect = -Qp * sW2_tree / 4.0 / (cW2_tree - sW2_tree)
    //                *((4.0 * cW_tree / sW_tree * getSMEFTCoeffEW("CHWB") + getSMEFTCoeffEW("CHD")) * v2_over_LambdaNP2 + 2.0 * delta_GF);
 
    NPindirect = (-Qp * sW2_tree) * delta_UgNC + Qp * delta_QgNC;
 
    double NPdirect = -0.5 * CHf * v2;
    return (NPindirect + NPdirect);
}

◆ deltaGR_f_mu()

const double NPSMEFTd6General::deltaGR_f_mu	(	const Particle	p,
		const double	mu
	)		const

New physics contribution to the neutral-current right-handed coupling $g_R^f$.

Parameters

[in]	f	a lepton or quark
[in]	mu	the RG scale to be used in the evaluation

Returns: $\delta g_R^f(\mu)$

Definition at line 17125 of file NPSMEFTd6General.cpp.

                                                                                   {
    double Qp = p.getCharge();
    double CHf;
    double NPindirect;
    
    // Parameters from the indirect corrections depending on the RG scale
    double d_UgNC_mu, d_QgNC_mu;
    
    //  NP indirect corrections to EW fermion couplings
    d_UgNC_mu = delU_gNC(mu);
    d_QgNC_mu = delQ_gNC(mu);   
    
    NPindirect = (-Qp * sW2_tree) * d_UgNC_mu + Qp * d_QgNC_mu;
    
    // Direct contribution  
    switch(p.getIndex()){
    //if (p.is("NEUTRINO_1") || p.is("NEUTRINO_2") || p.is("NEUTRINO_3"))
        case 0:
            CHf = 0.0;
            break;
    //else if (p.is("ELECTRON"))
        case 1:
            CHf = getSMEFTCoeff("CHeR", 0, 0, mu);
            break;
        case 2:
            CHf = 0.;
            break;
    //else if (p.is("MU"))
        case 3:
            CHf = getSMEFTCoeff("CHeR", 1, 1, mu);
            break;
        case 4:
            CHf = 0.;
            break;
    //else if (p.is("TAU"))
        case 5:
            CHf = getSMEFTCoeff("CHeR", 2, 2, mu);
            break;
    //else if (p.is("UP"))
        case 6:
            CHf = getSMEFTCoeff("CHuR", 0, 0, mu);
            break;
    //else if (p.is("DOWN"))
        case 7:
            CHf = getSMEFTCoeff("CHdR", 0, 0, mu);
            break;
        case 8:
            CHf = getSMEFTCoeff("CHuR", 1, 1, mu);
            break;
        case 9:
            CHf = getSMEFTCoeff("CHdR", 1, 1, mu);
            break;
        case 10:
            CHf = getSMEFTCoeff("CHuR", 2, 2, mu);
            break;
    //else if (p.is("BOTTOM"))
        case 11:
            CHf = getSMEFTCoeff("CHdR", 2, 2, mu);
            break;
    //else
        default:
            throw std::runtime_error("NPSMEFTd6General::deltaGR_f_mu(): wrong argument");
    }
 
    double NPdirect = -0.5 * CHf * v2;
    return (NPindirect + NPdirect);
}

◆ deltaGR_Wff()

gslpp::complex NPSMEFTd6General::deltaGR_Wff	(	const Particle	pbar,
		const Particle	p
	)		const

virtual

New physics contribution to the charged current coupling $W_\mu \bar{f_R}\gamma^mu f_R$.

Parameters

[in]	pbar	a lepton or quark
[in]	p	a lepton or quark

Returns: $\delta g_{Wff}^{R}$

Reimplemented from NPbase.

Definition at line 17211 of file NPSMEFTd6General.cpp.

                                                                                      {
    if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
        throw std::runtime_error("NPSMEFTd6General::deltaGR_Wff(): Not implemented");
 
    gslpp::complex CHud = CHud_diag(pbar);
    return (0.5 * CHud * v2);
}

◆ deltaGR_Wff_mu()

gslpp::complex NPSMEFTd6General::deltaGR_Wff_mu	(	const Particle	pbar,
		const Particle	p,
		const double	mu
	)		const

virtual

New physics contribution to the charged current coupling $W_\mu \bar{f_R}\gamma^mu f_R$.

Parameters

[in]	pbar	a lepton or quark
[in]	p	a lepton or quark
[in]	mu	the RG scale to be used in the evaluation (for those models where it is available)

Returns: $\delta g_{Wff}^{R}$

Reimplemented from NPbase.

Definition at line 17250 of file NPSMEFTd6General.cpp.

                                                                                                          {
    if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
        throw std::runtime_error("NPSMEFTd6General::deltaGR_Wff_mu(): Not implemented");
 
    gslpp::complex CHud;
    
    if (!pbar.is("QUARK") || pbar.getIndex() % 2 != 0)
        throw std::runtime_error("NPSMEFTd6General::deltaGR_Wff_mu(): wrong argument");
 
    if (pbar.is("UP"))
        CHud = gslpp::complex(getSMEFTCoeff("CHudR", 0, 0, mu), getSMEFTCoeff("CHudI", 0, 0, mu), false);
    else if (pbar.is("CHARM"))
        CHud = gslpp::complex(getSMEFTCoeff("CHudR", 1, 1, mu), getSMEFTCoeff("CHudI", 1, 1, mu), false);
    else if (pbar.is("TOP"))
        CHud = gslpp::complex(getSMEFTCoeff("CHudR", 2, 2, mu), getSMEFTCoeff("CHudI", 2, 2, mu), false);
    else
        throw std::runtime_error("NPSMEFTd6General::deltaGR_Wff_mu(): wrong argument");    
    
    return (0.5 * CHud * v2);
}

◆ deltaGR_Wffh()

gslpp::complex NPSMEFTd6General::deltaGR_Wffh	(	const Particle	pbar,
		const Particle	p
	)		const

The new physics contribution to the coupling of the effective interaction $H W_\mu \bar{f_R}\gamma^mu f_R$.

Parameters

[in]	pbar	a lepton or quark
[in]	p	a lepton or quark

Returns: $\delta g_{WffH}^{R}$

Definition at line 17820 of file NPSMEFTd6General.cpp.

                                                                                       {
    if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
        throw std::runtime_error("NPSMEFTd6General::deltaGR_Wffh(): Not implemented");
 
    gslpp::complex CHud = CHud_diag(pbar);
    return (sqrt(2.0) * Mz * cW_tree / v() / v() * CHud * v2);
}

◆ deltaGR_Zffh()

const double NPSMEFTd6General::deltaGR_Zffh ( const Particle p ) const

The new physics contribution to the coupling of the effective interaction $H Z_\mu \bar{f_R}\gamma^mu f_R$.

Parameters

[in] p a lepton or quark

Returns: $\delta g_{ZffH}^{R}$

Definition at line 17835 of file NPSMEFTd6General.cpp.

                                                                  {
    double CHf = CHf_diag(p);
    return (-2.0 * Mz / v() / v() * CHf * v2);
}

◆ deltaGV_f()

const double NPSMEFTd6General::deltaGV_f ( const Particle p ) const

virtual

New physics contribution to the neutral-current vector coupling $g_V^f$.

Parameters

[in] f a lepton or quark

Returns: $\delta g_V^f$

Reimplemented from NPbase.

Definition at line 17015 of file NPSMEFTd6General.cpp.

                                                               {
    return (deltaGL_f(p) + deltaGR_f(p));
}

◆ deltaGwd6()

const double NPSMEFTd6General::deltaGwd6 ( ) const

virtual

The relative NP corrections to the width of the $W$ boson, $\delta \Gamma_W/\Gamma_W$.

Returns: $\delta \Gamma_W/\Gamma_W$

Definition at line 15758 of file NPSMEFTd6General.cpp.

                                               {
    return ( deltaGamma_W() / trueSM.GammaW());
}

◆ deltaGwd62()

const double NPSMEFTd6General::deltaGwd62 ( ) const

virtual

The relative NP corrections to the width of the $W$ boson squared, $(\delta \Gamma_W/\Gamma_W)^2$.

Returns: $(\delta \Gamma_W/\Gamma_W)^2$

Definition at line 15762 of file NPSMEFTd6General.cpp.

                                                {
    double dWW = 0.0;
 
    return (dWW * dWW);
}

◆ deltaGzd6()

const double NPSMEFTd6General::deltaGzd6 ( ) const

virtual

The relative NP corrections to the width of the $Z$ boson, $\delta \Gamma_Z/\Gamma_Z$.

Returns: $\delta \Gamma_Z/\Gamma_Z$

Definition at line 16138 of file NPSMEFTd6General.cpp.

                                               {
    return ( deltaGamma_Z() / trueSM.Gamma_Z());
}

◆ deltaGzd62()

const double NPSMEFTd6General::deltaGzd62 ( ) const

virtual

The relative NP corrections to the width of the $Z$ boson squared, $(\delta \Gamma_Z/\Gamma_Z)^2$.

Returns: $(\delta \Gamma_Z/\Gamma_Z)^2$

Definition at line 16142 of file NPSMEFTd6General.cpp.

                                                {
    double dWZ = 0.0;
 
    return (dWZ * dWZ);
}

◆ deltaH3L1()

const double NPSMEFTd6General::deltaH3L1 ( double C1 ) const

virtual

The coefficient of the 1-loop linear term in the Higgs selfcoupling.

Definition at line 15275 of file NPSMEFTd6General.cpp.

{
    double lin;
    
    lin = ( -C1 - 2.0 * dZH - C1 * dZH );
    
    lin = lin / (1.0 + C1)/(-1.0 + dZH);
    
    return lin;
}

◆ deltaH3L2()

const double NPSMEFTd6General::deltaH3L2 ( double C1 ) const

virtual

The coefficient of the 1-loop quadratic term in the Higgs selfcoupling.

Definition at line 15287 of file NPSMEFTd6General.cpp.

{
    double quad;
    
    quad = dZH * ( 1.0 + 3.0 * dZH + C1 * (3.0 + dZH) );
    
    quad = quad / (1.0 + C1)/(-1.0 + dZH)/(-1.0 + dZH);
    
    return quad;
}

◆ deltaKgammaNP()

const double NPSMEFTd6General::deltaKgammaNP ( const double mu ) const

virtual

The new physics contribution to the anomalous triple gauge coupling $\kappa_{\gamma}$.

Returns: $\delta \kappa_{\gamma}$

Reimplemented from NPbase.

Definition at line 36515 of file NPSMEFTd6General.cpp.

                                                                  {
    double NPdirect, NPindirect;
 
    NPdirect = eeMz / 4.0 / sW2_tree;
 
    NPdirect = NPdirect * ((4.0 * sW_tree * cW_tree / eeMz) * getSMEFTCoeff("CHWB",mu)) * v2;
 
    NPindirect = del_e_mu(mu) + 0.5 * del_A_mu(mu);
 
    return NPdirect + NPindirect;
}

◆ deltaKgammaNPEff()

const double NPSMEFTd6General::deltaKgammaNPEff ( ) const

virtual

The new physics contribution to the effective anomalous triple gauge coupling $\kappa_{\gamma}^{Eff}$ from arXiv: 1708.09079 [hep-ph].

Returns: $\delta \kappa_{\gamma}$

Reimplemented from NPbase.

Definition at line 36549 of file NPSMEFTd6General.cpp.

                                                      {
    // From arXiv:1708.09079 [hep-ph]. In our case, delta_e=0 since it is taken as inputs and its effects propagated
    // everywhere else 
    double dgEff;
 
    dgEff = (cW2_tree - sW2_tree)*(deltaGL_f(leptons[ELECTRON]) / gZlL - deltaGR_f(leptons[ELECTRON]) / gZlR)
            - 2.0 * deltaGL_Wff(leptons[NEUTRINO_1], leptons[ELECTRON]).real() / UevL;
 
    return dgEff + deltaKgammaNP(muw);
}

◆ deltaKZNP()

const double NPSMEFTd6General::deltaKZNP ( const double mu ) const

virtual

The new physics contribution to the anomalous triple gauge coupling $\kappa_{Z}$.

Returns: $\delta \kappa_{Z}$

Definition at line 36501 of file NPSMEFTd6General.cpp.

                                                              {
    // Obtain from the other aTGC  
 
    return ( deltag1ZNP(mu) - (sW2_tree / cW2_tree) * (deltaKgammaNP(mu) - deltag1gaNP(mu)));
}

◆ deltamb()

const double NPSMEFTd6General::deltamb ( ) const

virtual

The relative correction to the mass of the $b$ quark, $\delta m_b/m_b$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $\delta m_b/m_b$

Definition at line 15481 of file NPSMEFTd6General.cpp.

                                             {
    //  Ref. value used in MG simulations
    return ( ((quarks[BOTTOM].getMass()) - 4.18) / 4.18);
}

◆ deltamb2()

const double NPSMEFTd6General::deltamb2 ( ) const

virtual

The relative correction to the mass of the $b$ quark squared, $(\delta m_b/m_b)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $(\delta m_b/m_b)^2$

Definition at line 15486 of file NPSMEFTd6General.cpp.

                                              {
    return ( 0.0);
}

◆ deltamc()

const double NPSMEFTd6General::deltamc ( ) const

virtual

The relative correction to the mass of the $c$ quark, $\delta m_c/m_c$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $\delta m_c/m_c$

Definition at line 15490 of file NPSMEFTd6General.cpp.

                                             {
    //  Ref. value used in MG simulations
    return ( ((quarks[CHARM].getMass()) - 1.275) / 1.275);
}

◆ deltamc2()

const double NPSMEFTd6General::deltamc2 ( ) const

virtual

The relative correction to the mass of the $c$ quark squared, $(\delta m_c/m_c)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $(\delta m_c/m_c)^2$

Definition at line 15495 of file NPSMEFTd6General.cpp.

                                              {
    return ( 0.0);
}

◆ deltaMh()

const double NPSMEFTd6General::deltaMh ( ) const

virtual

The relative correction to the mass of the $H$ boson, $\delta M_H/M_H$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $\delta M_H/M_H$

Definition at line 15463 of file NPSMEFTd6General.cpp.

                                             {
    //  Ref. value used in MG simulations
    return ( (mHl - 125.1) / 125.1);
}

◆ deltaMh2()

const double NPSMEFTd6General::deltaMh2 ( ) const

virtual

The relative correction to the mass of the $H$ boson squared, $(\delta M_H/M_H)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $(\delta M_H/M_H)^2$

Definition at line 15468 of file NPSMEFTd6General.cpp.

                                              {
    return ( 0.0);
}

◆ deltaMLL2_f()

const double NPSMEFTd6General::deltaMLL2_f	(	const Particle	f,
		const double	s,
		const double	t
	)		const

Definition at line 46254 of file NPSMEFTd6General.cpp.

                                                                                                 {
    // Definitions      
    double Qf, geSM, gfSM, deltage, deltagf, deltaGammaZ, is2c2;
    
    // RG scale of the process
    double muRG;
 
    // Four-fermion contribution
    double Aeeff;
 
    // Propagator
    gslpp::complex propZ, propZc;
    double propZt;
 
    // Correction to amplitude
    gslpp::complex deltaM2a, deltaM2b, deltaM2;
 
    // -------------------------------------------
    
    muRG = sqrt(s);
 
    geSM = gZlL;
    deltage = deltaGL_f_mu(leptons[ELECTRON], muRG);
 
    is2c2 = 1. / sW2_tree / cW2_tree;
 
    switch(f.getIndex()){
    //if (f.is("ELECTRON")) {
        case 1:
        Aeeff = 2.0 * CeeLL_e(muRG);
        Qf = leptons[ELECTRON].getCharge();
        gfSM = gZlL;
        deltagf = deltaGL_f_mu(leptons[ELECTRON], muRG);
        break;
    //} else if (f.is("MU")) {
        case 3:
        Aeeff = CeeLL_mu(muRG);
        Qf = leptons[ELECTRON].getCharge();
        gfSM = gZlL;
        deltagf = deltaGL_f_mu(leptons[MU], muRG);
        break;
    //} else if (f.is("TAU")) {
        case 5:
        Aeeff = CeeLL_tau(muRG);
        Qf = leptons[ELECTRON].getCharge();
        gfSM = gZlL;
        deltagf = deltaGL_f_mu(leptons[TAU], muRG);
        break;
    //} else if (f.is("UP")) {
        case 6:
        Aeeff = CeeLL_up(muRG);
        Qf = quarks[UP].getCharge();
        gfSM = gZuL;
        deltagf = deltaGL_f_mu(quarks[UP], muRG);
        break;
    //} else if (f.is("CHARM")) {
        case 8:
        Aeeff = CeeLL_charm(muRG);
        Qf = quarks[UP].getCharge();
        gfSM = gZuL;
        deltagf = deltaGL_f_mu(quarks[CHARM], muRG);
        break;
    //} else if (f.is("DOWN")) {
        case 7:
        Aeeff = CeeLL_down(muRG);
        Qf = quarks[DOWN].getCharge();
        gfSM = gZdL;
        deltagf = deltaGL_f_mu(quarks[DOWN], muRG);
        break;
    //} else if (f.is("STRANGE")) {
        case 9:
        Aeeff = CeeLL_strange(muRG);
        Qf = quarks[DOWN].getCharge();
        gfSM = gZdL;
        deltagf = deltaGL_f_mu(quarks[STRANGE], muRG);
        break;
    //} else if (f.is("BOTTOM")) {
        case 11:
        Aeeff = CeeLL_bottom(muRG);
        Qf = quarks[DOWN].getCharge();
        gfSM = gZdL;
        deltagf = deltaGL_f_mu(quarks[BOTTOM], muRG);
        break;
        default:
        throw std::runtime_error("NPSMEFTd6General::deltaMLL2_f(): wrong argument");
    }
 
    // Add the remaining factors that enter with the four-fermion operator
    Aeeff = Aeeff * s / (4. * M_PI * trueSM.alphaMz());
 
    deltaGammaZ = deltaGamma_Z();
 
    // -------------------------------------------
 
    propZ = s / (s - Mz * Mz - Mz * trueSM.Gamma_Z() * (gslpp::complex::i()));
 
    propZc = propZ.conjugate();
 
    propZt = s / (t - Mz * Mz);
 
    deltaM2a = (-Qf + is2c2 * geSM * gfSM * propZ);
 
    deltaM2b = -Qf * delta_em + Aeeff
            + is2c2 * (geSM * deltagf + gfSM * deltage) * propZc
            - (gslpp::complex::i()) * is2c2 * geSM * gfSM * Mz * deltaGammaZ * propZc * propZc / s;
 
    // Add t-channel contributions for f=e
    if (f.is("ELECTRON")) {
        deltaM2a = deltaM2a + is2c2 * geSM * gfSM * propZt + s / t;
        deltaM2b = deltaM2b + is2c2 * (geSM * deltagf + gfSM * deltage) * propZt;
    }
 
    deltaM2 = deltaM2a * deltaM2b;
 
    return 2.0 * deltaM2.real();
 
}

◆ deltaMLR2_f()

const double NPSMEFTd6General::deltaMLR2_f	(	const Particle	f,
		const double	s
	)		const

Definition at line 45984 of file NPSMEFTd6General.cpp.

                                                                                 {
    // Definitions      
    double Qf, geSM, gfSM, deltage, deltagf, deltaGammaZ, is2c2;
 
    double muRG;
    
    // Four-fermion contribution
    double Aeeff;
 
    // Propagator
    gslpp::complex propZ, propZc;
 
    // Correction to amplitude
    gslpp::complex deltaM2a, deltaM2b, deltaM2;
 
    // -------------------------------------------
    
    muRG = sqrt(s);
 
    geSM = gZlL;
    deltage = deltaGL_f_mu(leptons[ELECTRON], muRG);
 
    is2c2 = 1. / sW2_tree / cW2_tree;
 
    switch(f.getIndex()){
    //if (f.is("ELECTRON")) {
        case 1:
        Aeeff = CeeLR_e(muRG);
        Qf = leptons[ELECTRON].getCharge();
        gfSM = gZlR;
        deltagf = deltaGR_f_mu(leptons[ELECTRON], muRG);
        break;
    //} else if (f.is("MU")) {
        case 3:
        Aeeff = CeeLR_mu(muRG);
        Qf = leptons[ELECTRON].getCharge();
        gfSM = gZlR;
        deltagf = deltaGR_f_mu(leptons[MU], muRG);
        break;
    //} else if (f.is("TAU")) {
        case 5:
        Aeeff = CeeLR_tau(muRG);
        Qf = leptons[ELECTRON].getCharge();
        gfSM = gZlR;
        deltagf = deltaGR_f_mu(leptons[TAU], muRG);
        break;
    //} else if (f.is("UP")) {
        case 6:
        Aeeff = CeeLR_up(muRG);
        Qf = quarks[UP].getCharge();
        gfSM = gZuR;
        deltagf = deltaGR_f_mu(quarks[UP], muRG);
        break;
    //} else if (f.is("CHARM")) {
        case 8:
        Aeeff = CeeLR_charm(muRG);
        Qf = quarks[UP].getCharge();
        gfSM = gZuR;
        deltagf = deltaGR_f_mu(quarks[CHARM], muRG);
        break;
    //} else if (f.is("DOWN")) {
        case 7:
        Aeeff = CeeLR_down(muRG);
        Qf = quarks[DOWN].getCharge();
        gfSM = gZdR;
        deltagf = deltaGR_f_mu(quarks[DOWN], muRG);
        break;
    //} else if (f.is("STRANGE")) {
        case 9:
        Aeeff = CeeLR_strange(muRG);
        Qf = quarks[DOWN].getCharge();
        gfSM = gZdR;
        deltagf = deltaGR_f_mu(quarks[STRANGE], muRG);
        break;
    //} else if (f.is("BOTTOM")) {
        case 11:
        Aeeff = CeeLR_bottom(muRG);
        Qf = quarks[DOWN].getCharge();
        gfSM = gZdR;
        deltagf = deltaGR_f_mu(quarks[BOTTOM], muRG);
        break;
    //} else
        default:
        throw std::runtime_error("NPSMEFTd6General::deltaMLR2_f(): wrong argument");
    }
 
    // Add the remaining factors that enter with the four-fermion operator
    Aeeff = Aeeff * s / (4. * M_PI * trueSM.alphaMz());
 
    deltaGammaZ = deltaGamma_Z();
 
    // -------------------------------------------
 
    propZ = s / (s - Mz * Mz - Mz * trueSM.Gamma_Z() * (gslpp::complex::i()));
 
    propZc = propZ.conjugate();
 
    deltaM2a = (-Qf + is2c2 * geSM * gfSM * propZ);
 
    deltaM2b = -Qf * delta_em + Aeeff
            + is2c2 * (geSM * deltagf + gfSM * deltage) * propZc
            - (gslpp::complex::i()) * is2c2 * geSM * gfSM * Mz * deltaGammaZ * propZc * propZc / s;
 
    deltaM2 = deltaM2a * deltaM2b;
 
    return 2.0 * deltaM2.real();
 
}

◆ deltaMLR2t_e()

const double NPSMEFTd6General::deltaMLR2t_e	(	const double	s,
		const double	t
	)		const

Definition at line 46202 of file NPSMEFTd6General.cpp.

                                                                                {
    // Definitions      
    double Qf, geSM, gfSM, deltage, deltagf, is2c2;
    
    // RG scale of the process
    double muRG;
 
    // Four-fermion contribution
    double Aeeff;
 
    // t-channel propagator
    double propZ;
 
    // Correction to amplitude
    double deltaM2a, deltaM2b, deltaM2;
 
    // -------------------------------------------
    
    muRG = sqrt(s);
 
    geSM = gZlL;
    deltage = deltaGL_f_mu(leptons[ELECTRON], muRG);
 
    is2c2 = 1. / sW2_tree / cW2_tree;
 
    Aeeff = CeeLR_e(muRG);
    Qf = leptons[ELECTRON].getCharge();
    gfSM = gZlR;
    deltagf = deltaGR_f_mu(leptons[ELECTRON], muRG);
 
    // Add the remaining factors that enter with the four-fermion operator
    Aeeff = Aeeff * t / (4. * M_PI * trueSM.alphaMz());
 
    // -------------------------------------------
 
    propZ = t / (t - Mz * Mz);
 
    deltaM2a = (-Qf + is2c2 * geSM * gfSM * propZ);
 
    deltaM2b = -Qf * delta_em + Aeeff
            + is2c2 * (geSM * deltagf + gfSM * deltage) * propZ;
 
    deltaM2 = deltaM2a * deltaM2b;
 
    return 2.0 * deltaM2;
 
}

◆ deltaMRL2_f()

const double NPSMEFTd6General::deltaMRL2_f	(	const Particle	f,
		const double	s
	)		const

Definition at line 46093 of file NPSMEFTd6General.cpp.

                                                                                 {
    // Definitions      
    double Qf, geSM, gfSM, deltage, deltagf, deltaGammaZ, is2c2;
    
    double muRG;
 
    // Four-fermion contribution
    double Aeeff;
 
    // Propagator
    gslpp::complex propZ, propZc;
 
    // Correction to amplitude
    gslpp::complex deltaM2a, deltaM2b, deltaM2;
 
    // -------------------------------------------
    
    muRG = sqrt(s);
 
    geSM = gZlR;
    deltage = deltaGR_f_mu(leptons[ELECTRON], muRG);
 
    is2c2 = 1. / sW2_tree / cW2_tree;
 
    switch(f.getIndex()){
    //if (f.is("ELECTRON")) {
        case 1:
        Aeeff = CeeRL_e(muRG);
        Qf = leptons[ELECTRON].getCharge();
        gfSM = gZlL;
        deltagf = deltaGL_f_mu(leptons[ELECTRON], muRG);
        break;
    //} else if (f.is("MU")) {
        case 3:
        Aeeff = CeeRL_mu(muRG);
        Qf = leptons[ELECTRON].getCharge();
        gfSM = gZlL;
        deltagf = deltaGL_f_mu(leptons[MU], muRG);
        break;
    //} else if (f.is("TAU")) {
        case 5:
        Aeeff = CeeRL_tau(muRG);
        Qf = leptons[ELECTRON].getCharge();
        gfSM = gZlL;
        deltagf = deltaGL_f_mu(leptons[TAU], muRG);
        break;
    //} else if (f.is("UP")) {
        case 6:
        Aeeff = CeeRL_up(muRG);
        Qf = quarks[UP].getCharge();
        gfSM = gZuL;
        deltagf = deltaGL_f_mu(quarks[UP], muRG);
        break;
    //} else if (f.is("CHARM")) {
        case 8:
        Aeeff = CeeRL_charm(muRG);
        Qf = quarks[UP].getCharge();
        gfSM = gZuL;
        deltagf = deltaGL_f_mu(quarks[CHARM], muRG);
        break;
    //} else if (f.is("DOWN")) {
        case 7:
        Aeeff = CeeRL_down(muRG);
        Qf = quarks[DOWN].getCharge();
        gfSM = gZdL;
        deltagf = deltaGL_f_mu(quarks[DOWN], muRG);
        break;
    //} else if (f.is("STRANGE")) {
        case 9:
        Aeeff = CeeRL_strange(muRG);
        Qf = quarks[DOWN].getCharge();
        gfSM = gZdL;
        deltagf = deltaGL_f_mu(quarks[STRANGE], muRG);
        break;
    //} else if (f.is("BOTTOM")) {
        case 11:
        Aeeff = CeeRL_bottom(muRG);
        Qf = quarks[DOWN].getCharge();
        gfSM = gZdL;
        deltagf = deltaGL_f_mu(quarks[BOTTOM], muRG);
        break;
    //} else
        default:
        throw std::runtime_error("NPSMEFTd6General::deltaMRL2_f(): wrong argument");
    }
 
    // Add the remaining factors that enter with the four-fermion operator
    Aeeff = Aeeff * s / (4. * M_PI * trueSM.alphaMz());
 
    deltaGammaZ = deltaGamma_Z();
 
    // -------------------------------------------
 
    propZ = s / (s - Mz * Mz - Mz * trueSM.Gamma_Z() * (gslpp::complex::i()));
 
    propZc = propZ.conjugate();
 
    deltaM2a = (-Qf + is2c2 * geSM * gfSM * propZ);
 
    deltaM2b = -Qf * delta_em + Aeeff
            + is2c2 * (geSM * deltagf + gfSM * deltage) * propZc
            - (gslpp::complex::i()) * is2c2 * geSM * gfSM * Mz * deltaGammaZ * propZc * propZc / s;
 
    deltaM2 = deltaM2a * deltaM2b;
 
    return 2.0 * deltaM2.real();
 
}

◆ deltaMRL2t_e()

const double NPSMEFTd6General::deltaMRL2t_e	(	const double	s,
		const double	t
	)		const

Definition at line 46250 of file NPSMEFTd6General.cpp.

                                                                                {
    return deltaMLR2t_e(s, t);
}

◆ deltaMRR2_f()

const double NPSMEFTd6General::deltaMRR2_f	(	const Particle	f,
		const double	s,
		const double	t
	)		const

Definition at line 46372 of file NPSMEFTd6General.cpp.

                                                                                                 {
    // Definitions      
    double Qf, geSM, gfSM, deltage, deltagf, deltaGammaZ, is2c2;
    
    // RG scale of the process
    double muRG;
 
    // Four-fermion contribution
    double Aeeff;
 
    // Propagator
    gslpp::complex propZ, propZc;
    double propZt;
 
    // Correction to amplitude
    gslpp::complex deltaM2a, deltaM2b, deltaM2;
 
    // -------------------------------------------
    
    muRG = sqrt(s);
 
    geSM = gZlR;
    deltage = deltaGR_f_mu(leptons[ELECTRON], muRG);
 
    is2c2 = 1. / sW2_tree / cW2_tree;
 
    switch(f.getIndex()){
    //if (f.is("ELECTRON")) {
        case 1:
        Aeeff = 2.0 * CeeRR_e(muRG);
        Qf = leptons[ELECTRON].getCharge();
        gfSM = gZlR;
        deltagf = deltaGR_f_mu(leptons[ELECTRON], muRG);
        break;
    //} else if (f.is("MU")) {
        case 3:
        Aeeff = CeeRR_mu(muRG);
        Qf = leptons[ELECTRON].getCharge();
        gfSM = gZlR;
        deltagf = deltaGR_f_mu(leptons[MU], muRG);
        break;
    //} else if (f.is("TAU")) {
        case 5:
        Aeeff = CeeRR_tau(muRG);
        Qf = leptons[ELECTRON].getCharge();
        gfSM = gZlR;
        deltagf = deltaGR_f_mu(leptons[TAU], muRG);
        break;
    //} else if (f.is("UP")) {
        case 6:
        Aeeff = CeeRR_up(muRG);
        Qf = quarks[UP].getCharge();
        gfSM = gZuR;
        deltagf = deltaGR_f_mu(quarks[UP], muRG);
        break;
    //} else if (f.is("CHARM")) {
        case 8:
        Aeeff = CeeRR_charm(muRG);
        Qf = quarks[UP].getCharge();
        gfSM = gZuR;
        deltagf = deltaGR_f_mu(quarks[CHARM], muRG);
        break;
    //} else if (f.is("DOWN")) {
        case 7:
        Aeeff = CeeRR_down(muRG);
        Qf = quarks[DOWN].getCharge();
        gfSM = gZdR;
        deltagf = deltaGR_f_mu(quarks[DOWN], muRG);
        break;
    //} else if (f.is("STRANGE")) {
        case 9:
        Aeeff = CeeRR_strange(muRG);
        Qf = quarks[DOWN].getCharge();
        gfSM = gZdR;
        deltagf = deltaGR_f_mu(quarks[STRANGE], muRG);
        break;
    //} else if (f.is("BOTTOM")) {
        case 11:
        Aeeff = CeeRR_bottom(muRG);
        Qf = quarks[DOWN].getCharge();
        gfSM = gZdR;
        deltagf = deltaGR_f_mu(quarks[BOTTOM], muRG);
        break;
        default:
        throw std::runtime_error("NPSMEFTd6General::deltaMRR2_f(): wrong argument");
    }
 
    // Add the remaining factors that enter with the four-fermion operator
    Aeeff = Aeeff * s / (4. * M_PI * trueSM.alphaMz());
 
    deltaGammaZ = deltaGamma_Z();
 
    // -------------------------------------------
 
    propZ = s / (s - Mz * Mz - Mz * trueSM.Gamma_Z() * (gslpp::complex::i()));
 
    propZc = propZ.conjugate();
 
    propZt = s / (t - Mz * Mz);
 
    deltaM2a = (-Qf + is2c2 * geSM * gfSM * propZ);
 
    deltaM2b = -Qf * delta_em + Aeeff
            + is2c2 * (geSM * deltagf + gfSM * deltage) * propZc
            - (gslpp::complex::i()) * is2c2 * geSM * gfSM * Mz * deltaGammaZ * propZc * propZc / s;
 
    // Add t-channel contributions for f=e
    //if (f.is("ELECTRON")) {
    if ( f.getIndex() == 1 ) {
        deltaM2a = deltaM2a + is2c2 * geSM * gfSM * propZt + s / t;
        deltaM2b = deltaM2b + is2c2 * (geSM * deltagf + gfSM * deltage) * propZt;
    }
 
    deltaM2 = deltaM2a * deltaM2b;
 
    return 2.0 * deltaM2.real();
 
}

◆ deltamt()

const double NPSMEFTd6General::deltamt ( ) const

virtual

The relative correction to the mass of the $t$ quark, $\delta m_t/m_t$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $\delta m_t/m_t$

Definition at line 15472 of file NPSMEFTd6General.cpp.

                                             {
    //  Ref. value used in MG simulations
    return ( (mtpole - 173.0) / 173.0);
}

◆ deltamt2()

const double NPSMEFTd6General::deltamt2 ( ) const

virtual

The relative correction to the mass of the $t$ quark squared, $(\delta m_t/m_t)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $(\delta m_t/m_t)^2$

Definition at line 15477 of file NPSMEFTd6General.cpp.

                                              {
    return ( 0.0);
}

◆ deltamtau()

const double NPSMEFTd6General::deltamtau ( ) const

virtual

The relative correction to the mass of the $\tau$ lepton, $\delta m_\tau/m_\tau$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $\delta m_\tau/m_\tau$

Definition at line 15499 of file NPSMEFTd6General.cpp.

                                               {
    //  Ref. value used in MG simulations
    return ( ((leptons[TAU].getMass()) - 1.77682) / 1.77682);
}

◆ deltamtau2()

const double NPSMEFTd6General::deltamtau2 ( ) const

virtual

The relative correction to the mass of the $\tau$ lepton squared, $(\delta m_\tau/m_\tau)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $(\delta m_\tau/m_\tau)^2$

Definition at line 15504 of file NPSMEFTd6General.cpp.

                                                {
    return ( 0.0);
}

◆ deltaMw()

const double NPSMEFTd6General::deltaMw ( ) const

virtual

The relative correction to the mass of the $W$ boson, $\delta M_W/M_W$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $\delta M_W/M_W$

Definition at line 15544 of file NPSMEFTd6General.cpp.

                                             {
    //  Ref. value used in MG simulations
    //  (Value chosen to produce the same tree level SM pars as in the Alpha scheme with the input pars above)
    return ( (Mw_inp - 79.96717329554225) / 79.96717329554225);
}

◆ deltaMw2()

const double NPSMEFTd6General::deltaMw2 ( ) const

virtual

The relative correction to the mass of the $W$ boson squared, $(\delta M_W/M_W)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $(\delta M_W/M_W)^2$

Definition at line 15550 of file NPSMEFTd6General.cpp.

                                              {
    return ( 0.0);
}

◆ deltaMwd6()

const double NPSMEFTd6General::deltaMwd6 ( ) const

virtual

The relative NP corrections to the mass of the $W$ boson, $\delta M_W/M_W$.

Returns: $\delta M_W/M_W$

Definition at line 15605 of file NPSMEFTd6General.cpp.

                                               {
    //    return (- 1.0 / 4.0 / (cW2_tree - sW2_tree)
    //            *(4.0 * sW_tree * cW_tree * getSMEFTCoeffEW("CHWB") * v2_over_LambdaNP2
    //            + cW2_tree * getSMEFTCoeffEW("CHD") * v2_over_LambdaNP2
    //            + 2.0 * sW2_tree * delta_GF));
    
    double deltaNLO;
 
    // Finite NLO corrections in alpha scheme (set to zero for the moment)
    deltaNLO = 0.; 
 
    return (delta_e - 0.5 * delta_sW2 + delta_v + cNLOd6 * deltaNLO);
}

◆ deltaMwd62()

const double NPSMEFTd6General::deltaMwd62 ( ) const

virtual

The relative NP corrections to the mass of the $W$ boson squared, $(\delta M_W/M_W)^2$.

Returns: $(\delta M_W/M_W)^2$

Definition at line 15619 of file NPSMEFTd6General.cpp.

                                                {
    double dMW = 0.0;
 
    return (dMW * dMW);
}

◆ deltaMz()

const double NPSMEFTd6General::deltaMz ( ) const

virtual

The relative correction to the mass of the $Z$ boson, $\delta M_Z/M_Z$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $\delta M_Z/M_Z$

Definition at line 15454 of file NPSMEFTd6General.cpp.

                                             {
    //  Ref. value used in MG simulations
    return ( (Mz - 91.1879) / 91.1879);
}

◆ deltaMz2()

const double NPSMEFTd6General::deltaMz2 ( ) const

virtual

The relative correction to the mass of the $Z$ boson squared, $(\delta M_Z/M_Z)^2$, with respect to ref. point used in the SM calculation of Higgs observables.

Returns: $(\delta M_Z/M_Z)^2$

Definition at line 15459 of file NPSMEFTd6General.cpp.

                                              {
    return ( 0.0);
}

◆ DeltaOalphtoW()

const double NPSMEFTd6General::DeltaOalphtoW	(	const double	dOSMdalpha,
		const double	mu
	)		const

virtual

Difference in prediction in $\alpha$ scheme and W mass scheme, computed from observable in $\alpha$ scheme. Difference at tree level.

The difference $\Delta O$ is defined as

\[ \Delta O = O_{\alpha} - O_{W} \,, \]

where $O$ is a given observable in the SMEFT.

Parameters

[in]	dOSMdalpha	the derivative with respect to $\alpha$ of the SM tree-level prediction of $O$ (in the $\alpha$ scheme)
[in]	mu	the RG scale associated to the observable

Returns: The tree level difference between schemes $\Delta O$

Definition at line 15230 of file NPSMEFTd6General.cpp.

                                                                                           {
    
    double alphatoW;
    double d_GF_mu;
    double deltaOLO;
    
    // delta_GF, including RG scale dependence
    d_GF_mu = (getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2;
    
    // Combinations of parameters to control the change of SM EW input scheme
    // Combination multiplying d OSM/d alpha
    alphatoW = ( GF/sqrt(2.0)/Mz/Mz/M_PI ) * ( pow(Mw_inp,4) * ( getSMEFTCoeff("CHD", mu) * v2 - 2.0 * d_GF_mu ) 
            + 2.0 * pow(Mz*Mw_inp,2) * (d_GF_mu + 2.0 * sW_tree * cW_tree * getSMEFTCoeff("CHWB", mu) * v2 ) );
    
    deltaOLO = dOSMdalpha * alphatoW;
            
    return deltaOLO;
}

◆ DeltaOWtoalph()

const double NPSMEFTd6General::DeltaOWtoalph	(	const double	dOSMdMW,
		const double	mu
	)		const

virtual

Difference in prediction in $\alpha$ scheme and W mass scheme, computed from observable in W mass scheme. Difference at tree level.

The difference $\Delta O$ is defined as

\[ \Delta O = O_{\alpha} - O_{W} \,, \]

where $O$ is a given observable in the SMEFT.

Parameters

[in]	dOSMdMW	the derivative with respect to $M_W$ of the SM tree-level prediction of $O$ (in the $M_W$ scheme)
[in]	mu	the RG scale associated to the observable

Returns: The tree level difference between schemes $\Delta O$

Definition at line 15249 of file NPSMEFTd6General.cpp.

                                                                                        {
    
    double Wtoalpha;
    double d_GF_mu;
    double deltaOLO;
    
    // delta_GF, including RG scale dependence
    d_GF_mu = (getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2;
 
    // Combinations of parameters to control the change of SM EW input scheme    
    // Combination multiplying d OSM/d MW    
    Wtoalpha = ( sqrt(M_PI * aleMz / sW2_tree)/( 8.0 * GF * sqrt( sqrt(2.0) * GF ) * Mz*Mz * sW2_tree*sW2_tree * (sW2_tree - cW2_tree) ) )
            * ( sqrt(2.0) * M_PI * sW2_tree * aleMz * getSMEFTCoeff("CHD", mu) * v2
            + ( 4.0 * GF * Mz*Mz * sW2_tree - 2.0 * sqrt(2.0) * aleMz * M_PI * (1.0 + sW2_tree) ) * d_GF_mu 
            + ( 8.0 * GF * Mz*Mz * sW2_tree - 4.0 * sqrt(2.0) * aleMz * M_PI ) * sW_tree * cW_tree * getSMEFTCoeff("CHWB", mu) * v2 );
    
    deltaOLO = dOSMdMW * Wtoalpha;
            
    return deltaOLO;
}

◆ deltaR0_f()

const double NPSMEFTd6General::deltaR0_f ( const Particle f ) const

virtual

The new physics contribution to the ratio $R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell$, $R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}$ and $R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}$, for charged leptons, quarks and neutrinos, respectively.

Parameters

f	a lepton or quark

Returns: $\delta R_f^0$

Reimplemented from NPbase.

Definition at line 16728 of file NPSMEFTd6General.cpp.

{
    double dR0_f = 0., delGVl = 0., delGAl = 0., deltaGl = 0., Gl = 0.;
    bool nonZeroNP = false;
    
    int findex = f.getIndex();
    
    double deltaNLO;
    
    //if (f.is("LEPTON")) {
    if ( findex < 6 ) {
        delGVl = deltaGV_f(f);
        delGAl = deltaGA_f(f);
        if (delGVl != 0.0 || delGAl != 0.0) nonZeroNP = true;
    }
 
    double delGVq[6], delGAq[6];
    for (int q = 0; q < 6; ++q) {
        delGVq[q] = deltaGV_f(quarks[q]);
        delGAq[q] = deltaGA_f(quarks[q]);
        if (delGVq[q] != 0.0 || delGAq[q] != 0.0) nonZeroNP = true;
    }
 
    if (nonZeroNP) {
        double CF = 1.;
        //if (f.is("LEPTON")) {
        if ( findex < 6 ) {
            double gVl = trueSM.gV_f(f).real();
            double gAl = trueSM.gA_f(f).real();
            Gl = gVl * gVl + gAl*gAl;
            deltaGl = 2.0 * (gVl * delGVl + gAl * delGAl);
            CF = 3.;
        }
        double Gq[6], deltaGq[6];
        double gVq, gAq;
        double Gq_sum = 0.0, delGq_sum = 0.0;
        for (int q = 0; q < 6; ++q) {
            gVq = trueSM.gV_f(quarks[q]).real();
            gAq = trueSM.gA_f(quarks[q]).real();
            Gq[q] = gVq * gVq + gAq*gAq;
            deltaGq[q] = 2.0 * (gVq * delGVq[q] + gAq * delGAq[q]);
 
            Gq_sum += CF * Gq[q];
            delGq_sum += CF * deltaGq[q];
        }
        //if (f.is("LEPTON"))
        if ( findex < 6 )        
            if ( (findex == 0) || (findex == 2) || (findex == 4)  ) {
            //if ( f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3")  ) {
                dR0_f = deltaGl / Gq_sum - Gl * delGq_sum / Gq_sum / Gq_sum;                
            } else {
                dR0_f = delGq_sum / Gl - Gq_sum * deltaGl / Gl / Gl;
            }
        else
            dR0_f = deltaGq[f.getIndex() - 6] / Gq_sum
                - Gq[f.getIndex() - 6] * delGq_sum / Gq_sum / Gq_sum;
    }
 
    // Finite NLO corrections: not available for u, d and s   
    switch(findex){
    //if (f.is("ELECTRON")) {
        case 1:
            deltaNLO = (+0.003062 * getSMEFTCoeffEW("CW")  +0.007318 * getSMEFTCoeffEW("CHbox")  +2.44086 * getSMEFTCoeffEW("CHD")  +0.002518 * getSMEFTCoeffEW("CHB")   
            +0.00432 * getSMEFTCoeffEW("CHW")  +2.73273 * getSMEFTCoeffEW("CHWB")  -0.20729 * getSMEFTCoeffEW("CuWR",2, 2) +0.058637 * getSMEFTCoeffEW("CuBR",2, 2)  
            -1.30043 * getSMEFTCoeffEW("CHl1R",0, 0) +0.004185 * getSMEFTCoeffEW("CHl1R",1, 1) +0.004185 * getSMEFTCoeffEW("CHl1R",2, 2) -0.848528 * getSMEFTCoeffEW("CHl3R",0, 0)  
            +0.18628 * getSMEFTCoeffEW("CHl3R",1, 1) +3.70685 * getSMEFTCoeffEW("CHeR",0, 0) +0.004185 * getSMEFTCoeffEW("CHeR",1, 1) +0.004185 * getSMEFTCoeffEW("CHeR",2, 2)  
            +0.203989 * getSMEFTCoeffEW("CHq1R",0, 0) +0.203989 * getSMEFTCoeffEW("CHq1R",1, 1) +0.970933 * getSMEFTCoeffEW("CHq1R",2, 2) +1.02553 * getSMEFTCoeffEW("CHq3R",0, 0)  
            +1.02553 * getSMEFTCoeffEW("CHq3R",1, 1) +0.017291 * getSMEFTCoeffEW("CHq3R",2, 2) +0.386004 * getSMEFTCoeffEW("CHuR",0, 0) +0.386004 * getSMEFTCoeffEW("CHuR",1, 1)  
            -0.479269 * getSMEFTCoeffEW("CHuR",2, 2) -0.191495 * getSMEFTCoeffEW("CHdR",0, 0) -0.191495 * getSMEFTCoeffEW("CHdR",1, 1) -0.191495 * getSMEFTCoeffEW("CHdR",2, 2)  
            -0.019239 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) -0.038099 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) -0.038099 * getSMEFTCoeffEW("CllR",0, 0, 2, 2) -0.167192 * getSMEFTCoeffEW("CllR",0, 1, 1, 0)  
            +0.01886 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) -0.012676 * getSMEFTCoeffEW("Cqq1R",0, 0, 0, 0) -0.00305 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1) +0.058724 * getSMEFTCoeffEW("Cqq1R",0, 0, 2, 2)  
            -0.022302 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) -0.230042 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0) -0.012676 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1) +0.058724 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2)  
            -0.230042 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) +0.378602 * getSMEFTCoeffEW("Cqq1R",2, 2, 2, 2) -0.154995 * getSMEFTCoeffEW("Cqq3R",0, 0, 0, 0) -0.331478 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1)  
            -0.975495 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2) +0.021489 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0) +0.317392 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0) -0.154995 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1)  
            -0.975495 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) +0.317392 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1) +0.034136 * getSMEFTCoeffEW("Cqq3R",2, 2, 2, 2) +0.019812 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0)  
            +0.019812 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) -0.838052 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) +0.000762 * getSMEFTCoeffEW("Clq1R",1, 1, 0, 0) +0.000762 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1)  
            +0.004356 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2) +0.000762 * getSMEFTCoeffEW("Clq1R",2, 2, 0, 0) +0.000762 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1) +0.004356 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2)  
            +0.170972 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) +0.170972 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) +1.04492 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.027623 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0)  
            -0.027623 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) -0.015136 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.027623 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0) -0.027623 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1)  
            -0.015136 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) +0.043099 * getSMEFTCoeffEW("CeeR",0, 0, 0, 0) +0.043099 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1) +0.043099 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2)  
            -0.006913 * getSMEFTCoeffEW("CuuR",0, 0, 0, 0) -0.012199 * getSMEFTCoeffEW("CuuR",0, 0, 1, 1) -0.158354 * getSMEFTCoeffEW("CuuR",0, 0, 2, 2) -0.001627 * getSMEFTCoeffEW("CuuR",0, 1, 1, 0)  
            -0.09567 * getSMEFTCoeffEW("CuuR",0, 2, 2, 0) -0.006913 * getSMEFTCoeffEW("CuuR",1, 1, 1, 1) -0.158354 * getSMEFTCoeffEW("CuuR",1, 1, 2, 2) -0.09567 * getSMEFTCoeffEW("CuuR",1, 2, 2, 1)  
            -0.001728 * getSMEFTCoeffEW("CddR",0, 0, 0, 0) -0.00305 * getSMEFTCoeffEW("CddR",0, 0, 1, 1) -0.00305 * getSMEFTCoeffEW("CddR",0, 0, 2, 2) -0.000407 * getSMEFTCoeffEW("CddR",0, 1, 1, 0)  
            -0.000407 * getSMEFTCoeffEW("CddR",0, 2, 2, 0) -0.001728 * getSMEFTCoeffEW("CddR",1, 1, 1, 1) -0.00305 * getSMEFTCoeffEW("CddR",1, 1, 2, 2) -0.000407 * getSMEFTCoeffEW("CddR",1, 2, 2, 1)  
            -0.001728 * getSMEFTCoeffEW("CddR",2, 2, 2, 2) -0.02926 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0) -0.02926 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1) -0.799223 * getSMEFTCoeffEW("CeuR",0, 0, 2, 2)  
            +0.001525 * getSMEFTCoeffEW("CeuR",1, 1, 0, 0) +0.001525 * getSMEFTCoeffEW("CeuR",1, 1, 1, 1) +0.001525 * getSMEFTCoeffEW("CeuR",2, 2, 0, 0) +0.001525 * getSMEFTCoeffEW("CeuR",2, 2, 1, 1)  
            +0.01463 * getSMEFTCoeffEW("CedR",0, 0, 0, 0) +0.01463 * getSMEFTCoeffEW("CedR",0, 0, 1, 1) +0.01463 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) -0.000762 * getSMEFTCoeffEW("CedR",1, 1, 0, 0)  
            -0.000762 * getSMEFTCoeffEW("CedR",1, 1, 1, 1) -0.000762 * getSMEFTCoeffEW("CedR",1, 1, 2, 2) -0.000762 * getSMEFTCoeffEW("CedR",2, 2, 0, 0) -0.000762 * getSMEFTCoeffEW("CedR",2, 2, 1, 1)  
            -0.000762 * getSMEFTCoeffEW("CedR",2, 2, 2, 2) +0.00305 * getSMEFTCoeffEW("Cud1R",0, 0, 0, 0) +0.00305 * getSMEFTCoeffEW("Cud1R",0, 0, 1, 1) +0.00305 * getSMEFTCoeffEW("Cud1R",0, 0, 2, 2)  
            +0.00305 * getSMEFTCoeffEW("Cud1R",1, 1, 0, 0) +0.00305 * getSMEFTCoeffEW("Cud1R",1, 1, 1, 1) +0.00305 * getSMEFTCoeffEW("Cud1R",1, 1, 2, 2) +0.039589 * getSMEFTCoeffEW("Cud1R",2, 2, 0, 0)  
            +0.039589 * getSMEFTCoeffEW("Cud1R",2, 2, 1, 1) +0.039589 * getSMEFTCoeffEW("Cud1R",2, 2, 2, 2) -0.003657 * getSMEFTCoeffEW("CleR",0, 0, 0, 0) -0.019049 * getSMEFTCoeffEW("CleR",0, 0, 1, 1)  
            -0.019049 * getSMEFTCoeffEW("CleR",0, 0, 2, 2) +0.015393 * getSMEFTCoeffEW("CleR",1, 1, 0, 0) +0.015393 * getSMEFTCoeffEW("CleR",2, 2, 0, 0) +0.039623 * getSMEFTCoeffEW("CluR",0, 0, 0, 0)  
            +0.039623 * getSMEFTCoeffEW("CluR",0, 0, 1, 1) +0.989083 * getSMEFTCoeffEW("CluR",0, 0, 2, 2) +0.001525 * getSMEFTCoeffEW("CluR",1, 1, 0, 0) +0.001525 * getSMEFTCoeffEW("CluR",1, 1, 1, 1)  
            +0.001525 * getSMEFTCoeffEW("CluR",2, 2, 0, 0) +0.001525 * getSMEFTCoeffEW("CluR",2, 2, 1, 1) -0.019812 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) -0.019812 * getSMEFTCoeffEW("CldR",0, 0, 1, 1)  
            -0.019812 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) -0.000762 * getSMEFTCoeffEW("CldR",1, 1, 0, 0) -0.000762 * getSMEFTCoeffEW("CldR",1, 1, 1, 1) -0.000762 * getSMEFTCoeffEW("CldR",1, 1, 2, 2)  
            -0.000762 * getSMEFTCoeffEW("CldR",2, 2, 0, 0) -0.000762 * getSMEFTCoeffEW("CldR",2, 2, 1, 1) -0.000762 * getSMEFTCoeffEW("CldR",2, 2, 2, 2) -0.01463 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0)  
            +0.000762 * getSMEFTCoeffEW("CqeR",0, 0, 1, 1) +0.000762 * getSMEFTCoeffEW("CqeR",0, 0, 2, 2) -0.01463 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0) +0.000762 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1)  
            +0.000762 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) +0.685059 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0) +0.004356 * getSMEFTCoeffEW("CqeR",2, 2, 1, 1) +0.004356 * getSMEFTCoeffEW("CqeR",2, 2, 2, 2)  
            -0.00305 * getSMEFTCoeffEW("Cqu1R",0, 0, 0, 0) -0.00305 * getSMEFTCoeffEW("Cqu1R",0, 0, 1, 1) -0.039589 * getSMEFTCoeffEW("Cqu1R",0, 0, 2, 2) -0.00305 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0)  
            -0.00305 * getSMEFTCoeffEW("Cqu1R",1, 1, 1, 1) -0.039589 * getSMEFTCoeffEW("Cqu1R",1, 1, 2, 2) +0.058724 * getSMEFTCoeffEW("Cqu1R",2, 2, 0, 0) +0.058724 * getSMEFTCoeffEW("Cqu1R",2, 2, 1, 1)  
            -0.226156 * getSMEFTCoeffEW("Cqu1R",2, 2, 2, 2) +0.001525 * getSMEFTCoeffEW("Cqd1R",0, 0, 0, 0) +0.001525 * getSMEFTCoeffEW("Cqd1R",0, 0, 1, 1) +0.001525 * getSMEFTCoeffEW("Cqd1R",0, 0, 2, 2)  
            +0.001525 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0) +0.001525 * getSMEFTCoeffEW("Cqd1R",1, 1, 1, 1) +0.001525 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) -0.029362 * getSMEFTCoeffEW("Cqd1R",2, 2, 0, 0)  
            -0.029362 * getSMEFTCoeffEW("Cqd1R",2, 2, 1, 1) -0.029362 * getSMEFTCoeffEW("Cqd1R",2, 2, 2, 2) ) * v2; 
        break;
    //} else if (f.is("MUON")) {
        case 3:
            deltaNLO = (+0.003062 * getSMEFTCoeffEW("CW")  +0.007318 * getSMEFTCoeffEW("CHbox")  +2.44086 * getSMEFTCoeffEW("CHD")  +0.002518 * getSMEFTCoeffEW("CHB")   
            +0.00432 * getSMEFTCoeffEW("CHW")  +2.73273 * getSMEFTCoeffEW("CHWB")  -0.20729 * getSMEFTCoeffEW("CuWR",2, 2) +0.058637 * getSMEFTCoeffEW("CuBR",2, 2)  
            +0.004185 * getSMEFTCoeffEW("CHl1R",0, 0) -1.30043 * getSMEFTCoeffEW("CHl1R",1, 1) +0.004185 * getSMEFTCoeffEW("CHl1R",2, 2) +0.18628 * getSMEFTCoeffEW("CHl3R",0, 0)  
            -0.848528 * getSMEFTCoeffEW("CHl3R",1, 1) +0.004185 * getSMEFTCoeffEW("CHeR",0, 0) +3.70685 * getSMEFTCoeffEW("CHeR",1, 1) +0.004185 * getSMEFTCoeffEW("CHeR",2, 2)  
            +0.203989 * getSMEFTCoeffEW("CHq1R",0, 0) +0.203989 * getSMEFTCoeffEW("CHq1R",1, 1) +0.970933 * getSMEFTCoeffEW("CHq1R",2, 2) +1.02553 * getSMEFTCoeffEW("CHq3R",0, 0)  
            +1.02553 * getSMEFTCoeffEW("CHq3R",1, 1) +0.017291 * getSMEFTCoeffEW("CHq3R",2, 2) +0.386004 * getSMEFTCoeffEW("CHuR",0, 0) +0.386004 * getSMEFTCoeffEW("CHuR",1, 1)  
            -0.479269 * getSMEFTCoeffEW("CHuR",2, 2) -0.191495 * getSMEFTCoeffEW("CHdR",0, 0) -0.191495 * getSMEFTCoeffEW("CHdR",1, 1) -0.191495 * getSMEFTCoeffEW("CHdR",2, 2)  
            -0.038099 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) -0.167192 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.019239 * getSMEFTCoeffEW("CllR",1, 1, 1, 1) -0.038099 * getSMEFTCoeffEW("CllR",1, 1, 2, 2)  
            +0.01886 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) -0.012676 * getSMEFTCoeffEW("Cqq1R",0, 0, 0, 0) -0.00305 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1) +0.058724 * getSMEFTCoeffEW("Cqq1R",0, 0, 2, 2)  
            -0.022302 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) -0.230042 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0) -0.012676 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1) +0.058724 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2)  
            -0.230042 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) +0.378602 * getSMEFTCoeffEW("Cqq1R",2, 2, 2, 2) -0.154995 * getSMEFTCoeffEW("Cqq3R",0, 0, 0, 0) -0.331478 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1)  
            -0.975495 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2) +0.021489 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0) +0.317392 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0) -0.154995 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1)  
            -0.975495 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) +0.317392 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1) +0.034136 * getSMEFTCoeffEW("Cqq3R",2, 2, 2, 2) +0.000762 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0)  
            +0.000762 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) +0.004356 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) +0.019812 * getSMEFTCoeffEW("Clq1R",1, 1, 0, 0) +0.019812 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1)  
            -0.838052 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2) +0.000762 * getSMEFTCoeffEW("Clq1R",2, 2, 0, 0) +0.000762 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1) +0.004356 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2)  
            -0.027623 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.027623 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) -0.015136 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) +0.170972 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0)  
            +0.170972 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) +1.04492 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) -0.027623 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0) -0.027623 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1)  
            -0.015136 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) +0.043099 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1) +0.043099 * getSMEFTCoeffEW("CeeR",1, 1, 1, 1) +0.043099 * getSMEFTCoeffEW("CeeR",1, 1, 2, 2)  
            -0.006913 * getSMEFTCoeffEW("CuuR",0, 0, 0, 0) -0.012199 * getSMEFTCoeffEW("CuuR",0, 0, 1, 1) -0.158354 * getSMEFTCoeffEW("CuuR",0, 0, 2, 2) -0.001627 * getSMEFTCoeffEW("CuuR",0, 1, 1, 0)  
            -0.09567 * getSMEFTCoeffEW("CuuR",0, 2, 2, 0) -0.006913 * getSMEFTCoeffEW("CuuR",1, 1, 1, 1) -0.158354 * getSMEFTCoeffEW("CuuR",1, 1, 2, 2) -0.09567 * getSMEFTCoeffEW("CuuR",1, 2, 2, 1)  
            -0.001728 * getSMEFTCoeffEW("CddR",0, 0, 0, 0) -0.00305 * getSMEFTCoeffEW("CddR",0, 0, 1, 1) -0.00305 * getSMEFTCoeffEW("CddR",0, 0, 2, 2) -0.000407 * getSMEFTCoeffEW("CddR",0, 1, 1, 0)  
            -0.000407 * getSMEFTCoeffEW("CddR",0, 2, 2, 0) -0.001728 * getSMEFTCoeffEW("CddR",1, 1, 1, 1) -0.00305 * getSMEFTCoeffEW("CddR",1, 1, 2, 2) -0.000407 * getSMEFTCoeffEW("CddR",1, 2, 2, 1)  
            -0.001728 * getSMEFTCoeffEW("CddR",2, 2, 2, 2) +0.001525 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0) +0.001525 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1) -0.02926 * getSMEFTCoeffEW("CeuR",1, 1, 0, 0)  
            -0.02926 * getSMEFTCoeffEW("CeuR",1, 1, 1, 1) -0.799223 * getSMEFTCoeffEW("CeuR",1, 1, 2, 2) +0.001525 * getSMEFTCoeffEW("CeuR",2, 2, 0, 0) +0.001525 * getSMEFTCoeffEW("CeuR",2, 2, 1, 1)  
            -0.000762 * getSMEFTCoeffEW("CedR",0, 0, 0, 0) -0.000762 * getSMEFTCoeffEW("CedR",0, 0, 1, 1) -0.000762 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) +0.01463 * getSMEFTCoeffEW("CedR",1, 1, 0, 0)  
            +0.01463 * getSMEFTCoeffEW("CedR",1, 1, 1, 1) +0.01463 * getSMEFTCoeffEW("CedR",1, 1, 2, 2) -0.000762 * getSMEFTCoeffEW("CedR",2, 2, 0, 0) -0.000762 * getSMEFTCoeffEW("CedR",2, 2, 1, 1)  
            -0.000762 * getSMEFTCoeffEW("CedR",2, 2, 2, 2) +0.00305 * getSMEFTCoeffEW("Cud1R",0, 0, 0, 0) +0.00305 * getSMEFTCoeffEW("Cud1R",0, 0, 1, 1) +0.00305 * getSMEFTCoeffEW("Cud1R",0, 0, 2, 2)  
            +0.00305 * getSMEFTCoeffEW("Cud1R",1, 1, 0, 0) +0.00305 * getSMEFTCoeffEW("Cud1R",1, 1, 1, 1) +0.00305 * getSMEFTCoeffEW("Cud1R",1, 1, 2, 2) +0.039589 * getSMEFTCoeffEW("Cud1R",2, 2, 0, 0)  
            +0.039589 * getSMEFTCoeffEW("Cud1R",2, 2, 1, 1) +0.039589 * getSMEFTCoeffEW("Cud1R",2, 2, 2, 2) +0.015393 * getSMEFTCoeffEW("CleR",0, 0, 1, 1) -0.019049 * getSMEFTCoeffEW("CleR",1, 1, 0, 0)  
            -0.003657 * getSMEFTCoeffEW("CleR",1, 1, 1, 1) -0.019049 * getSMEFTCoeffEW("CleR",1, 1, 2, 2) +0.015393 * getSMEFTCoeffEW("CleR",2, 2, 1, 1) +0.001525 * getSMEFTCoeffEW("CluR",0, 0, 0, 0)  
            +0.001525 * getSMEFTCoeffEW("CluR",0, 0, 1, 1) +0.039623 * getSMEFTCoeffEW("CluR",1, 1, 0, 0) +0.039623 * getSMEFTCoeffEW("CluR",1, 1, 1, 1) +0.989083 * getSMEFTCoeffEW("CluR",1, 1, 2, 2)  
            +0.001525 * getSMEFTCoeffEW("CluR",2, 2, 0, 0) +0.001525 * getSMEFTCoeffEW("CluR",2, 2, 1, 1) -0.000762 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) -0.000762 * getSMEFTCoeffEW("CldR",0, 0, 1, 1)  
            -0.000762 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) -0.019812 * getSMEFTCoeffEW("CldR",1, 1, 0, 0) -0.019812 * getSMEFTCoeffEW("CldR",1, 1, 1, 1) -0.019812 * getSMEFTCoeffEW("CldR",1, 1, 2, 2)  
            -0.000762 * getSMEFTCoeffEW("CldR",2, 2, 0, 0) -0.000762 * getSMEFTCoeffEW("CldR",2, 2, 1, 1) -0.000762 * getSMEFTCoeffEW("CldR",2, 2, 2, 2) +0.000762 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0)  
            -0.01463 * getSMEFTCoeffEW("CqeR",0, 0, 1, 1) +0.000762 * getSMEFTCoeffEW("CqeR",0, 0, 2, 2) +0.000762 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0) -0.01463 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1)  
            +0.000762 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) +0.004356 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0) +0.685059 * getSMEFTCoeffEW("CqeR",2, 2, 1, 1) +0.004356 * getSMEFTCoeffEW("CqeR",2, 2, 2, 2)  
            -0.00305 * getSMEFTCoeffEW("Cqu1R",0, 0, 0, 0) -0.00305 * getSMEFTCoeffEW("Cqu1R",0, 0, 1, 1) -0.039589 * getSMEFTCoeffEW("Cqu1R",0, 0, 2, 2) -0.00305 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0)  
            -0.00305 * getSMEFTCoeffEW("Cqu1R",1, 1, 1, 1) -0.039589 * getSMEFTCoeffEW("Cqu1R",1, 1, 2, 2) +0.058724 * getSMEFTCoeffEW("Cqu1R",2, 2, 0, 0) +0.058724 * getSMEFTCoeffEW("Cqu1R",2, 2, 1, 1)  
            -0.226156 * getSMEFTCoeffEW("Cqu1R",2, 2, 2, 2) +0.001525 * getSMEFTCoeffEW("Cqd1R",0, 0, 0, 0) +0.001525 * getSMEFTCoeffEW("Cqd1R",0, 0, 1, 1) +0.001525 * getSMEFTCoeffEW("Cqd1R",0, 0, 2, 2)  
            +0.001525 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0) +0.001525 * getSMEFTCoeffEW("Cqd1R",1, 1, 1, 1) +0.001525 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) -0.029362 * getSMEFTCoeffEW("Cqd1R",2, 2, 0, 0)  
            -0.029362 * getSMEFTCoeffEW("Cqd1R",2, 2, 1, 1) -0.029362 * getSMEFTCoeffEW("Cqd1R",2, 2, 2, 2) ) * v2; 
        break;
    //} else if (f.is("TAU")) {
        case 5:
            deltaNLO = (+0.003062 * getSMEFTCoeffEW("CW")  +0.007318 * getSMEFTCoeffEW("CHbox")  +2.44086 * getSMEFTCoeffEW("CHD")  +0.002518 * getSMEFTCoeffEW("CHB")   
            +0.00432 * getSMEFTCoeffEW("CHW")  +2.73273 * getSMEFTCoeffEW("CHWB")  -0.20729 * getSMEFTCoeffEW("CuWR",2, 2) +0.058637 * getSMEFTCoeffEW("CuBR",2, 2)  
            +0.004185 * getSMEFTCoeffEW("CHl1R",0, 0) +0.004185 * getSMEFTCoeffEW("CHl1R",1, 1) -1.30043 * getSMEFTCoeffEW("CHl1R",2, 2) +0.18628 * getSMEFTCoeffEW("CHl3R",0, 0)  
            +0.18628 * getSMEFTCoeffEW("CHl3R",1, 1) -1.03458 * getSMEFTCoeffEW("CHl3R",2, 2) +0.004185 * getSMEFTCoeffEW("CHeR",0, 0) +0.004185 * getSMEFTCoeffEW("CHeR",1, 1)  
            +3.70685 * getSMEFTCoeffEW("CHeR",2, 2) +0.203989 * getSMEFTCoeffEW("CHq1R",0, 0) +0.203989 * getSMEFTCoeffEW("CHq1R",1, 1) +0.970933 * getSMEFTCoeffEW("CHq1R",2, 2)  
            +1.02553 * getSMEFTCoeffEW("CHq3R",0, 0) +1.02553 * getSMEFTCoeffEW("CHq3R",1, 1) +0.017291 * getSMEFTCoeffEW("CHq3R",2, 2) +0.386004 * getSMEFTCoeffEW("CHuR",0, 0)  
            +0.386004 * getSMEFTCoeffEW("CHuR",1, 1) -0.479269 * getSMEFTCoeffEW("CHuR",2, 2) -0.191495 * getSMEFTCoeffEW("CHdR",0, 0) -0.191495 * getSMEFTCoeffEW("CHdR",1, 1)  
            -0.191495 * getSMEFTCoeffEW("CHdR",2, 2) -0.038099 * getSMEFTCoeffEW("CllR",0, 0, 2, 2) -0.186051 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) +0.01886 * getSMEFTCoeffEW("CllR",0, 2, 2, 0)  
            -0.038099 * getSMEFTCoeffEW("CllR",1, 1, 2, 2) +0.01886 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) -0.019239 * getSMEFTCoeffEW("CllR",2, 2, 2, 2) -0.012676 * getSMEFTCoeffEW("Cqq1R",0, 0, 0, 0)  
            -0.00305 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1) +0.058724 * getSMEFTCoeffEW("Cqq1R",0, 0, 2, 2) -0.022302 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) -0.230042 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0)  
            -0.012676 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1) +0.058724 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2) -0.230042 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) +0.378602 * getSMEFTCoeffEW("Cqq1R",2, 2, 2, 2)  
            -0.154995 * getSMEFTCoeffEW("Cqq3R",0, 0, 0, 0) -0.331478 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1) -0.975495 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2) +0.021489 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0)  
            +0.317392 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0) -0.154995 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1) -0.975495 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) +0.317392 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1)  
            +0.034136 * getSMEFTCoeffEW("Cqq3R",2, 2, 2, 2) +0.000762 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) +0.000762 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) +0.004356 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2)  
            +0.000762 * getSMEFTCoeffEW("Clq1R",1, 1, 0, 0) +0.000762 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1) +0.004356 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2) +0.019812 * getSMEFTCoeffEW("Clq1R",2, 2, 0, 0)  
            +0.019812 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1) -0.838052 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2) -0.027623 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.027623 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1)  
            -0.015136 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) -0.027623 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0) -0.027623 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) -0.015136 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2)  
            +0.170972 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0) +0.170972 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1) +1.04492 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) +0.043099 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2)  
            +0.043099 * getSMEFTCoeffEW("CeeR",1, 1, 2, 2) +0.043099 * getSMEFTCoeffEW("CeeR",2, 2, 2, 2) -0.006913 * getSMEFTCoeffEW("CuuR",0, 0, 0, 0) -0.012199 * getSMEFTCoeffEW("CuuR",0, 0, 1, 1)  
            -0.158354 * getSMEFTCoeffEW("CuuR",0, 0, 2, 2) -0.001627 * getSMEFTCoeffEW("CuuR",0, 1, 1, 0) -0.09567 * getSMEFTCoeffEW("CuuR",0, 2, 2, 0) -0.006913 * getSMEFTCoeffEW("CuuR",1, 1, 1, 1)  
            -0.158354 * getSMEFTCoeffEW("CuuR",1, 1, 2, 2) -0.09567 * getSMEFTCoeffEW("CuuR",1, 2, 2, 1) -0.001728 * getSMEFTCoeffEW("CddR",0, 0, 0, 0) -0.00305 * getSMEFTCoeffEW("CddR",0, 0, 1, 1)  
            -0.00305 * getSMEFTCoeffEW("CddR",0, 0, 2, 2) -0.000407 * getSMEFTCoeffEW("CddR",0, 1, 1, 0) -0.000407 * getSMEFTCoeffEW("CddR",0, 2, 2, 0) -0.001728 * getSMEFTCoeffEW("CddR",1, 1, 1, 1)  
            -0.00305 * getSMEFTCoeffEW("CddR",1, 1, 2, 2) -0.000407 * getSMEFTCoeffEW("CddR",1, 2, 2, 1) -0.001728 * getSMEFTCoeffEW("CddR",2, 2, 2, 2) +0.001525 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0)  
            +0.001525 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1) +0.001525 * getSMEFTCoeffEW("CeuR",1, 1, 0, 0) +0.001525 * getSMEFTCoeffEW("CeuR",1, 1, 1, 1) -0.02926 * getSMEFTCoeffEW("CeuR",2, 2, 0, 0)  
            -0.02926 * getSMEFTCoeffEW("CeuR",2, 2, 1, 1) -0.799223 * getSMEFTCoeffEW("CeuR",2, 2, 2, 2) -0.000762 * getSMEFTCoeffEW("CedR",0, 0, 0, 0) -0.000762 * getSMEFTCoeffEW("CedR",0, 0, 1, 1)  
            -0.000762 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) -0.000762 * getSMEFTCoeffEW("CedR",1, 1, 0, 0) -0.000762 * getSMEFTCoeffEW("CedR",1, 1, 1, 1) -0.000762 * getSMEFTCoeffEW("CedR",1, 1, 2, 2)  
            +0.01463 * getSMEFTCoeffEW("CedR",2, 2, 0, 0) +0.01463 * getSMEFTCoeffEW("CedR",2, 2, 1, 1) +0.01463 * getSMEFTCoeffEW("CedR",2, 2, 2, 2) +0.00305 * getSMEFTCoeffEW("Cud1R",0, 0, 0, 0)  
            +0.00305 * getSMEFTCoeffEW("Cud1R",0, 0, 1, 1) +0.00305 * getSMEFTCoeffEW("Cud1R",0, 0, 2, 2) +0.00305 * getSMEFTCoeffEW("Cud1R",1, 1, 0, 0) +0.00305 * getSMEFTCoeffEW("Cud1R",1, 1, 1, 1)  
            +0.00305 * getSMEFTCoeffEW("Cud1R",1, 1, 2, 2) +0.039589 * getSMEFTCoeffEW("Cud1R",2, 2, 0, 0) +0.039589 * getSMEFTCoeffEW("Cud1R",2, 2, 1, 1) +0.039589 * getSMEFTCoeffEW("Cud1R",2, 2, 2, 2)  
            +0.015393 * getSMEFTCoeffEW("CleR",0, 0, 2, 2) +0.015393 * getSMEFTCoeffEW("CleR",1, 1, 2, 2) -0.019049 * getSMEFTCoeffEW("CleR",2, 2, 0, 0) -0.019049 * getSMEFTCoeffEW("CleR",2, 2, 1, 1)  
            -0.003657 * getSMEFTCoeffEW("CleR",2, 2, 2, 2) +0.001525 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) +0.001525 * getSMEFTCoeffEW("CluR",0, 0, 1, 1) +0.001525 * getSMEFTCoeffEW("CluR",1, 1, 0, 0)  
            +0.001525 * getSMEFTCoeffEW("CluR",1, 1, 1, 1) +0.039623 * getSMEFTCoeffEW("CluR",2, 2, 0, 0) +0.039623 * getSMEFTCoeffEW("CluR",2, 2, 1, 1) +0.989083 * getSMEFTCoeffEW("CluR",2, 2, 2, 2)  
            -0.000762 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) -0.000762 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) -0.000762 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) -0.000762 * getSMEFTCoeffEW("CldR",1, 1, 0, 0)  
            -0.000762 * getSMEFTCoeffEW("CldR",1, 1, 1, 1) -0.000762 * getSMEFTCoeffEW("CldR",1, 1, 2, 2) -0.019812 * getSMEFTCoeffEW("CldR",2, 2, 0, 0) -0.019812 * getSMEFTCoeffEW("CldR",2, 2, 1, 1)  
            -0.019812 * getSMEFTCoeffEW("CldR",2, 2, 2, 2) +0.000762 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0) +0.000762 * getSMEFTCoeffEW("CqeR",0, 0, 1, 1) -0.01463 * getSMEFTCoeffEW("CqeR",0, 0, 2, 2)  
            +0.000762 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0) +0.000762 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1) -0.01463 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) +0.004356 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0)  
            +0.004356 * getSMEFTCoeffEW("CqeR",2, 2, 1, 1) +0.685059 * getSMEFTCoeffEW("CqeR",2, 2, 2, 2) -0.00305 * getSMEFTCoeffEW("Cqu1R",0, 0, 0, 0) -0.00305 * getSMEFTCoeffEW("Cqu1R",0, 0, 1, 1)  
            -0.039589 * getSMEFTCoeffEW("Cqu1R",0, 0, 2, 2) -0.00305 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0) -0.00305 * getSMEFTCoeffEW("Cqu1R",1, 1, 1, 1) -0.039589 * getSMEFTCoeffEW("Cqu1R",1, 1, 2, 2)  
            +0.058724 * getSMEFTCoeffEW("Cqu1R",2, 2, 0, 0) +0.058724 * getSMEFTCoeffEW("Cqu1R",2, 2, 1, 1) -0.226156 * getSMEFTCoeffEW("Cqu1R",2, 2, 2, 2) +0.001525 * getSMEFTCoeffEW("Cqd1R",0, 0, 0, 0)  
            +0.001525 * getSMEFTCoeffEW("Cqd1R",0, 0, 1, 1) +0.001525 * getSMEFTCoeffEW("Cqd1R",0, 0, 2, 2) +0.001525 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0) +0.001525 * getSMEFTCoeffEW("Cqd1R",1, 1, 1, 1)  
            +0.001525 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) -0.029362 * getSMEFTCoeffEW("Cqd1R",2, 2, 0, 0) -0.029362 * getSMEFTCoeffEW("Cqd1R",2, 2, 1, 1) -0.029362 * getSMEFTCoeffEW("Cqd1R",2, 2, 2, 2) ) * v2; 
        break;
    //} else if (f.is("CHARM")) {
        case 8:
            deltaNLO = (+0.000381 * getSMEFTCoeffEW("CW")  +0.000039 * getSMEFTCoeffEW("CHbox")  -0.001741 * getSMEFTCoeffEW("CHD")  +0.000014 * getSMEFTCoeffEW("CHB")   
            +0.000023 * getSMEFTCoeffEW("CHW")  -0.001841 * getSMEFTCoeffEW("CHWB")  +0.000982 * getSMEFTCoeffEW("CuWR",2, 2) +0.000596 * getSMEFTCoeffEW("CuBR",2, 2)  
            +0.000023 * getSMEFTCoeffEW("CHl1R",0, 0) +0.000023 * getSMEFTCoeffEW("CHl1R",1, 1) +0.000023 * getSMEFTCoeffEW("CHl1R",2, 2) +0.000077 * getSMEFTCoeffEW("CHl3R",0, 0)  
            +0.000077 * getSMEFTCoeffEW("CHl3R",1, 1) +0.000023 * getSMEFTCoeffEW("CHeR",0, 0) +0.000023 * getSMEFTCoeffEW("CHeR",1, 1) +0.000023 * getSMEFTCoeffEW("CHeR",2, 2)  
            -0.001351 * getSMEFTCoeffEW("CHq1R",0, 0) -0.012228 * getSMEFTCoeffEW("CHq1R",1, 1) -0.000752 * getSMEFTCoeffEW("CHq1R",2, 2) -0.004142 * getSMEFTCoeffEW("CHq3R",0, 0)  
            +0.00441 * getSMEFTCoeffEW("CHq3R",1, 1) -0.000797 * getSMEFTCoeffEW("CHq3R",2, 2) -0.002515 * getSMEFTCoeffEW("CHuR",0, 0) +0.012011 * getSMEFTCoeffEW("CHuR",1, 1)  
            -0.002049 * getSMEFTCoeffEW("CHuR",2, 2) +0.001245 * getSMEFTCoeffEW("CHdR",0, 0) +0.001245 * getSMEFTCoeffEW("CHdR",1, 1) +0.001245 * getSMEFTCoeffEW("CHdR",2, 2)  
            -0.000075 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) +0.000107 * getSMEFTCoeffEW("Cqq1R",0, 0, 0, 0) +0.000382 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1) -0.000497 * getSMEFTCoeffEW("Cqq1R",0, 0, 2, 2)  
            -0.000035 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) +0.001948 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0) +0.00024 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1) -0.016239 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2)  
            -0.00879 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) -0.003206 * getSMEFTCoeffEW("Cqq1R",2, 2, 2, 2) +0.001312 * getSMEFTCoeffEW("Cqq3R",0, 0, 0, 0) -0.000904 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1)  
            +0.00826 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2) +0.000137 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0) -0.002687 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0) -0.00208 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1)  
            -0.011549 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) -0.012883 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1) -0.000289 * getSMEFTCoeffEW("Cqq3R",2, 2, 2, 2) -0.000006 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0)  
            -0.000184 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) -0.000037 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) -0.000006 * getSMEFTCoeffEW("Clq1R",1, 1, 0, 0) -0.000184 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1)  
            -0.000037 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2) -0.000006 * getSMEFTCoeffEW("Clq1R",2, 2, 0, 0) -0.000184 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1) -0.000037 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2)  
            +0.000234 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.000385 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) +0.000128 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) +0.000234 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0)  
            -0.000385 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) +0.000128 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) +0.000234 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0) -0.000385 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1)  
            +0.000128 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) +0.000059 * getSMEFTCoeffEW("CuuR",0, 0, 0, 0) -0.000199 * getSMEFTCoeffEW("CuuR",0, 0, 1, 1) +0.001341 * getSMEFTCoeffEW("CuuR",0, 0, 2, 2)  
            -0.000027 * getSMEFTCoeffEW("CuuR",0, 1, 1, 0) +0.00081 * getSMEFTCoeffEW("CuuR",0, 2, 2, 0) -0.000284 * getSMEFTCoeffEW("CuuR",1, 1, 1, 1) -0.006503 * getSMEFTCoeffEW("CuuR",1, 1, 2, 2)  
            -0.003929 * getSMEFTCoeffEW("CuuR",1, 2, 2, 1) +0.000015 * getSMEFTCoeffEW("CddR",0, 0, 0, 0) +0.000026 * getSMEFTCoeffEW("CddR",0, 0, 1, 1) +0.000026 * getSMEFTCoeffEW("CddR",0, 0, 2, 2)  
            +0.000003 * getSMEFTCoeffEW("CddR",0, 1, 1, 0) +0.000003 * getSMEFTCoeffEW("CddR",0, 2, 2, 0) +0.000015 * getSMEFTCoeffEW("CddR",1, 1, 1, 1) +0.000026 * getSMEFTCoeffEW("CddR",1, 1, 2, 2)  
            +0.000003 * getSMEFTCoeffEW("CddR",1, 2, 2, 1) +0.000015 * getSMEFTCoeffEW("CddR",2, 2, 2, 2) -0.000013 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0) +0.000063 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1)  
            -0.000013 * getSMEFTCoeffEW("CeuR",1, 1, 0, 0) +0.000063 * getSMEFTCoeffEW("CeuR",1, 1, 1, 1) -0.000013 * getSMEFTCoeffEW("CeuR",2, 2, 0, 0) +0.000063 * getSMEFTCoeffEW("CeuR",2, 2, 1, 1)  
            +0.000006 * getSMEFTCoeffEW("CedR",0, 0, 0, 0) +0.000006 * getSMEFTCoeffEW("CedR",0, 0, 1, 1) +0.000006 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) +0.000006 * getSMEFTCoeffEW("CedR",1, 1, 0, 0)  
            +0.000006 * getSMEFTCoeffEW("CedR",1, 1, 1, 1) +0.000006 * getSMEFTCoeffEW("CedR",1, 1, 2, 2) +0.000006 * getSMEFTCoeffEW("CedR",2, 2, 0, 0) +0.000006 * getSMEFTCoeffEW("CedR",2, 2, 1, 1)  
            +0.000006 * getSMEFTCoeffEW("CedR",2, 2, 2, 2) -0.000026 * getSMEFTCoeffEW("Cud1R",0, 0, 0, 0) -0.000026 * getSMEFTCoeffEW("Cud1R",0, 0, 1, 1) -0.000026 * getSMEFTCoeffEW("Cud1R",0, 0, 2, 2)  
            +0.00005 * getSMEFTCoeffEW("Cud1R",1, 1, 0, 0) +0.00005 * getSMEFTCoeffEW("Cud1R",1, 1, 1, 1) +0.00005 * getSMEFTCoeffEW("Cud1R",1, 1, 2, 2) -0.000335 * getSMEFTCoeffEW("Cud1R",2, 2, 0, 0)  
            -0.000335 * getSMEFTCoeffEW("Cud1R",2, 2, 1, 1) -0.000335 * getSMEFTCoeffEW("Cud1R",2, 2, 2, 2) -0.000013 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) +0.000063 * getSMEFTCoeffEW("CluR",0, 0, 1, 1)  
            -0.000013 * getSMEFTCoeffEW("CluR",1, 1, 0, 0) +0.000063 * getSMEFTCoeffEW("CluR",1, 1, 1, 1) -0.000013 * getSMEFTCoeffEW("CluR",2, 2, 0, 0) +0.000063 * getSMEFTCoeffEW("CluR",2, 2, 1, 1)  
            +0.000006 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) +0.000006 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) +0.000006 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) +0.000006 * getSMEFTCoeffEW("CldR",1, 1, 0, 0)  
            +0.000006 * getSMEFTCoeffEW("CldR",1, 1, 1, 1) +0.000006 * getSMEFTCoeffEW("CldR",1, 1, 2, 2) +0.000006 * getSMEFTCoeffEW("CldR",2, 2, 0, 0) +0.000006 * getSMEFTCoeffEW("CldR",2, 2, 1, 1)  
            +0.000006 * getSMEFTCoeffEW("CldR",2, 2, 2, 2) -0.000006 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0) -0.000006 * getSMEFTCoeffEW("CqeR",0, 0, 1, 1) -0.000006 * getSMEFTCoeffEW("CqeR",0, 0, 2, 2)  
            -0.000184 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0) -0.000184 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1) -0.000184 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) -0.000037 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0)  
            -0.000037 * getSMEFTCoeffEW("CqeR",2, 2, 1, 1) -0.000037 * getSMEFTCoeffEW("CqeR",2, 2, 2, 2) +0.000026 * getSMEFTCoeffEW("Cqu1R",0, 0, 0, 0) -0.00005 * getSMEFTCoeffEW("Cqu1R",0, 0, 1, 1)  
            +0.000335 * getSMEFTCoeffEW("Cqu1R",0, 0, 2, 2) +0.000382 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0) +0.000306 * getSMEFTCoeffEW("Cqu1R",1, 1, 1, 1) +0.009577 * getSMEFTCoeffEW("Cqu1R",1, 1, 2, 2)  
            -0.000497 * getSMEFTCoeffEW("Cqu1R",2, 2, 0, 0) +0.002843 * getSMEFTCoeffEW("Cqu1R",2, 2, 1, 1) +0.001915 * getSMEFTCoeffEW("Cqu1R",2, 2, 2, 2) -0.000013 * getSMEFTCoeffEW("Cqd1R",0, 0, 0, 0)  
            -0.000013 * getSMEFTCoeffEW("Cqd1R",0, 0, 1, 1) -0.000013 * getSMEFTCoeffEW("Cqd1R",0, 0, 2, 2) -0.000191 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0) -0.000191 * getSMEFTCoeffEW("Cqd1R",1, 1, 1, 1)  
            -0.000191 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) +0.000249 * getSMEFTCoeffEW("Cqd1R",2, 2, 0, 0) +0.000249 * getSMEFTCoeffEW("Cqd1R",2, 2, 1, 1) +0.000249 * getSMEFTCoeffEW("Cqd1R",2, 2, 2, 2) ) * v2; 
        break;
    //} else if (f.is("BOTTOM")) {
        case 11:
            deltaNLO = (-0.001121 * getSMEFTCoeffEW("CW")  -0.000026 * getSMEFTCoeffEW("CHbox")  +0.001288 * getSMEFTCoeffEW("CHD")  -0.000009 * getSMEFTCoeffEW("CHB")   
            -0.000016 * getSMEFTCoeffEW("CHW")  +0.001622 * getSMEFTCoeffEW("CHWB")  -0.005659 * getSMEFTCoeffEW("CuWR",2, 2) -0.001063 * getSMEFTCoeffEW("CuBR",2, 2)  
            -0.000015 * getSMEFTCoeffEW("CHl1R",0, 0) -0.000015 * getSMEFTCoeffEW("CHl1R",1, 1) -0.000015 * getSMEFTCoeffEW("CHl1R",2, 2) +0.002311 * getSMEFTCoeffEW("CHl3R",0, 0)  
            +0.002311 * getSMEFTCoeffEW("CHl3R",1, 1) -0.000015 * getSMEFTCoeffEW("CHeR",0, 0) -0.000015 * getSMEFTCoeffEW("CHeR",1, 1) -0.000015 * getSMEFTCoeffEW("CHeR",2, 2)  
            -0.001495 * getSMEFTCoeffEW("CHq1R",0, 0) -0.001495 * getSMEFTCoeffEW("CHq1R",1, 1) +0.012327 * getSMEFTCoeffEW("CHq1R",2, 2) -0.003301 * getSMEFTCoeffEW("CHq3R",0, 0)  
            -0.003301 * getSMEFTCoeffEW("CHq3R",1, 1) +0.000214 * getSMEFTCoeffEW("CHq3R",2, 2) -0.002752 * getSMEFTCoeffEW("CHuR",0, 0) -0.002752 * getSMEFTCoeffEW("CHuR",1, 1)  
            +0.000091 * getSMEFTCoeffEW("CHuR",2, 2) +0.001359 * getSMEFTCoeffEW("CHdR",0, 0) +0.001359 * getSMEFTCoeffEW("CHdR",1, 1) -0.005829 * getSMEFTCoeffEW("CHdR",2, 2)  
            -0.002312 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) +0.000138 * getSMEFTCoeffEW("Cqq1R",0, 0, 0, 0) +0.000033 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1) -0.00107 * getSMEFTCoeffEW("Cqq1R",0, 0, 2, 2)  
            +0.000242 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) +0.002171 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0) +0.000138 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1) -0.00107 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2)  
            +0.002171 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) +0.01464 * getSMEFTCoeffEW("Cqq1R",2, 2, 2, 2) +0.001684 * getSMEFTCoeffEW("Cqq3R",0, 0, 0, 0) +0.003602 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1)  
            +0.006101 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2) -0.000234 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0) -0.003235 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0) +0.001684 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1)  
            +0.006101 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) -0.003235 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1) +0.00132 * getSMEFTCoeffEW("Cqq3R",2, 2, 2, 2) -0.000008 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0)  
            -0.000008 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) +0.000168 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) -0.000008 * getSMEFTCoeffEW("Clq1R",1, 1, 0, 0) -0.000008 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1)  
            +0.000168 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2) -0.000008 * getSMEFTCoeffEW("Clq1R",2, 2, 0, 0) -0.000008 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1) +0.000168 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2)  
            +0.0003 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) +0.0003 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) -0.000585 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2) +0.0003 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0)  
            +0.0003 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) -0.000585 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) +0.0003 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0) +0.0003 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1)  
            -0.000585 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) +0.000075 * getSMEFTCoeffEW("CuuR",0, 0, 0, 0) +0.000133 * getSMEFTCoeffEW("CuuR",0, 0, 1, 1) +0.001721 * getSMEFTCoeffEW("CuuR",0, 0, 2, 2)  
            +0.000018 * getSMEFTCoeffEW("CuuR",0, 1, 1, 0) +0.00104 * getSMEFTCoeffEW("CuuR",0, 2, 2, 0) +0.000075 * getSMEFTCoeffEW("CuuR",1, 1, 1, 1) +0.001721 * getSMEFTCoeffEW("CuuR",1, 1, 2, 2)  
            +0.00104 * getSMEFTCoeffEW("CuuR",1, 2, 2, 1) +0.000019 * getSMEFTCoeffEW("CddR",0, 0, 0, 0) +0.000033 * getSMEFTCoeffEW("CddR",0, 0, 1, 1) -0.000042 * getSMEFTCoeffEW("CddR",0, 0, 2, 2)  
            +0.000004 * getSMEFTCoeffEW("CddR",0, 1, 1, 0) -0.000006 * getSMEFTCoeffEW("CddR",0, 2, 2, 0) +0.000019 * getSMEFTCoeffEW("CddR",1, 1, 1, 1) -0.000042 * getSMEFTCoeffEW("CddR",1, 1, 2, 2)  
            -0.000006 * getSMEFTCoeffEW("CddR",1, 2, 2, 1) -0.000067 * getSMEFTCoeffEW("CddR",2, 2, 2, 2) -0.000017 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0) -0.000017 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1)  
            -0.000017 * getSMEFTCoeffEW("CeuR",1, 1, 0, 0) -0.000017 * getSMEFTCoeffEW("CeuR",1, 1, 1, 1) -0.000017 * getSMEFTCoeffEW("CeuR",2, 2, 0, 0) -0.000017 * getSMEFTCoeffEW("CeuR",2, 2, 1, 1)  
            +0.000008 * getSMEFTCoeffEW("CedR",0, 0, 0, 0) +0.000008 * getSMEFTCoeffEW("CedR",0, 0, 1, 1) -0.000029 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) +0.000008 * getSMEFTCoeffEW("CedR",1, 1, 0, 0)  
            +0.000008 * getSMEFTCoeffEW("CedR",1, 1, 1, 1) -0.000029 * getSMEFTCoeffEW("CedR",1, 1, 2, 2) +0.000008 * getSMEFTCoeffEW("CedR",2, 2, 0, 0) +0.000008 * getSMEFTCoeffEW("CedR",2, 2, 1, 1)  
            -0.000029 * getSMEFTCoeffEW("CedR",2, 2, 2, 2) -0.000033 * getSMEFTCoeffEW("Cud1R",0, 0, 0, 0) -0.000033 * getSMEFTCoeffEW("Cud1R",0, 0, 1, 1) +0.000042 * getSMEFTCoeffEW("Cud1R",0, 0, 2, 2)  
            -0.000033 * getSMEFTCoeffEW("Cud1R",1, 1, 0, 0) -0.000033 * getSMEFTCoeffEW("Cud1R",1, 1, 1, 1) +0.000042 * getSMEFTCoeffEW("Cud1R",1, 1, 2, 2) -0.00043 * getSMEFTCoeffEW("Cud1R",2, 2, 0, 0)  
            -0.00043 * getSMEFTCoeffEW("Cud1R",2, 2, 1, 1) +0.001531 * getSMEFTCoeffEW("Cud1R",2, 2, 2, 2) -0.000017 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) -0.000017 * getSMEFTCoeffEW("CluR",0, 0, 1, 1)  
            -0.000017 * getSMEFTCoeffEW("CluR",1, 1, 0, 0) -0.000017 * getSMEFTCoeffEW("CluR",1, 1, 1, 1) -0.000017 * getSMEFTCoeffEW("CluR",2, 2, 0, 0) -0.000017 * getSMEFTCoeffEW("CluR",2, 2, 1, 1)  
            +0.000008 * getSMEFTCoeffEW("CldR",0, 0, 0, 0) +0.000008 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) -0.000029 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) +0.000008 * getSMEFTCoeffEW("CldR",1, 1, 0, 0)  
            +0.000008 * getSMEFTCoeffEW("CldR",1, 1, 1, 1) -0.000029 * getSMEFTCoeffEW("CldR",1, 1, 2, 2) +0.000008 * getSMEFTCoeffEW("CldR",2, 2, 0, 0) +0.000008 * getSMEFTCoeffEW("CldR",2, 2, 1, 1)  
            -0.000029 * getSMEFTCoeffEW("CldR",2, 2, 2, 2) -0.000008 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0) -0.000008 * getSMEFTCoeffEW("CqeR",0, 0, 1, 1) -0.000008 * getSMEFTCoeffEW("CqeR",0, 0, 2, 2)  
            -0.000008 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0) -0.000008 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1) -0.000008 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) +0.000168 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0)  
            +0.000168 * getSMEFTCoeffEW("CqeR",2, 2, 1, 1) +0.000168 * getSMEFTCoeffEW("CqeR",2, 2, 2, 2) +0.000033 * getSMEFTCoeffEW("Cqu1R",0, 0, 0, 0) +0.000033 * getSMEFTCoeffEW("Cqu1R",0, 0, 1, 1)  
            +0.00043 * getSMEFTCoeffEW("Cqu1R",0, 0, 2, 2) +0.000033 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0) +0.000033 * getSMEFTCoeffEW("Cqu1R",1, 1, 1, 1) +0.00043 * getSMEFTCoeffEW("Cqu1R",1, 1, 2, 2)  
            -0.00107 * getSMEFTCoeffEW("Cqu1R",2, 2, 0, 0) -0.00107 * getSMEFTCoeffEW("Cqu1R",2, 2, 1, 1) -0.008745 * getSMEFTCoeffEW("Cqu1R",2, 2, 2, 2) -0.000017 * getSMEFTCoeffEW("Cqd1R",0, 0, 0, 0)  
            -0.000017 * getSMEFTCoeffEW("Cqd1R",0, 0, 1, 1) +0.000021 * getSMEFTCoeffEW("Cqd1R",0, 0, 2, 2) -0.000017 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0) -0.000017 * getSMEFTCoeffEW("Cqd1R",1, 1, 1, 1)  
            +0.000021 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2) +0.000535 * getSMEFTCoeffEW("Cqd1R",2, 2, 0, 0) +0.000535 * getSMEFTCoeffEW("Cqd1R",2, 2, 1, 1) -0.001135 * getSMEFTCoeffEW("Cqd1R",2, 2, 2, 2) ) * v2; 
        break;
    //} else {
        default:
            deltaNLO = 0.;
    }
       
    return dR0_f + cNLOd6 * deltaNLO;
}

◆ deltaSigmaHadron()

const double NPSMEFTd6General::deltaSigmaHadron ( ) const

virtual

The new physics contribution to the cross section for the process $e^+ e^-\to Z\to \mathrm{hadrons}$ at the $Z$ pole, $\delta \sigma_h^0$.

Returns: $\delta \sigma_h^0$ in GeV $^{-2}$

Reimplemented from NPbase.

Definition at line 16242 of file NPSMEFTd6General.cpp.

{
    double sigma_had = 0.;
    bool nonZeroNP = false;
    
    double deltaNLO;
    
    double delGVl[6], delGAl[6], delGVq[6], delGAq[6];
    for (int p = 0; p < 6; ++p) {
        delGVl[p] = deltaGV_f(leptons[p]);
        delGAl[p] = deltaGA_f(leptons[p]);
        delGVq[p] = deltaGV_f(quarks[p]);
        delGAq[p] = deltaGA_f(quarks[p]);
        if (delGVl[p] != 0.0 || delGAl[p] != 0.0
                || delGVq[p] != 0.0 || delGAq[p] != 0.0)
            nonZeroNP = true;
    }
 
    if (nonZeroNP) {
        double gVf, gAf;
        double Gl[6], deltaGl[6], Gq[6], deltaGq[6];
        double Gq_sum = 0.0, delGq_sum = 0.0;
        double Gf_sum = 0.0, delGf_sum = 0.0;
        for (int p = 0; p < 6; ++p) {
            gVf = trueSM.gV_f(leptons[p]).real();
            gAf = trueSM.gA_f(leptons[p]).real();
            Gl[p] = gVf * gVf + gAf*gAf;
            deltaGl[p] = 2.0 * (gVf * delGVl[p] + gAf * delGAl[p]);
 
            gVf = trueSM.gV_f(quarks[p]).real();
            gAf = trueSM.gA_f(quarks[p]).real();
            Gq[p] = gVf * gVf + gAf*gAf;
            deltaGq[p] = 2.0 * (gVf * delGVq[p] + gAf * delGAq[p]);
 
            Gq_sum += 3.0 * Gq[p];
            Gf_sum += Gl[p] + 3.0 * Gq[p];
            delGq_sum += 3.0 * deltaGq[p];
            delGf_sum += deltaGl[p] + 3.0 * deltaGq[p];
        }
 
        sigma_had = 12.0 * M_PI / Mz / Mz
                * Gl[ELECTRON] * Gq_sum / Gf_sum / Gf_sum
                * (deltaGl[ELECTRON] / Gl[ELECTRON]
                + delGq_sum / Gq_sum - 2.0 * delGf_sum / Gf_sum);
    }
 
    // Finite NLO corrections [in nb] => Need to be translated to GeV^-2    
    deltaNLO = (+0.031306 * getSMEFTCoeffEW("CW")  +0.002537 * getSMEFTCoeffEW("CHbox")  -3.66342 * getSMEFTCoeffEW("CHD")  +0.000873 * getSMEFTCoeffEW("CHB")   
            +0.001497 * getSMEFTCoeffEW("CHW")  -4.03907 * getSMEFTCoeffEW("CHWB")  +0.10258 * getSMEFTCoeffEW("CuWR",2, 2) +0.043554 * getSMEFTCoeffEW("CuBR",2, 2)  
            -1.03648 * getSMEFTCoeffEW("CHl1R",0, 0) +0.226921 * getSMEFTCoeffEW("CHl1R",1, 1) +0.226921 * getSMEFTCoeffEW("CHl1R",2, 2) -1.50874 * getSMEFTCoeffEW("CHl3R",0, 0)  
            +0.316297 * getSMEFTCoeffEW("CHl3R",1, 1) +0.313483 * getSMEFTCoeffEW("CHl3R",2, 2) -4.29271 * getSMEFTCoeffEW("CHeR",0, 0) +0.199561 * getSMEFTCoeffEW("CHeR",1, 1)  
            +0.199561 * getSMEFTCoeffEW("CHeR",2, 2) -0.14288 * getSMEFTCoeffEW("CHq1R",0, 0) -0.14288 * getSMEFTCoeffEW("CHq1R",1, 1) -0.218148 * getSMEFTCoeffEW("CHq1R",2, 2)  
            -0.552673 * getSMEFTCoeffEW("CHq3R",0, 0) -0.552673 * getSMEFTCoeffEW("CHq3R",1, 1) -0.125393 * getSMEFTCoeffEW("CHq3R",2, 2) -0.268081 * getSMEFTCoeffEW("CHuR",0, 0)  
            -0.268081 * getSMEFTCoeffEW("CHuR",1, 1) -0.121694 * getSMEFTCoeffEW("CHuR",2, 2) +0.132828 * getSMEFTCoeffEW("CHdR",0, 0) +0.132828 * getSMEFTCoeffEW("CHdR",1, 1)  
            +0.132828 * getSMEFTCoeffEW("CHdR",2, 2) +0.05596 * getSMEFTCoeffEW("CllR",0, 0, 0, 0) +0.088109 * getSMEFTCoeffEW("CllR",0, 0, 1, 1) +0.088109 * getSMEFTCoeffEW("CllR",0, 0, 2, 2)  
            -0.019051 * getSMEFTCoeffEW("CllR",0, 1, 1, 0) -0.016238 * getSMEFTCoeffEW("CllR",0, 2, 2, 0) +0.015911 * getSMEFTCoeffEW("CllR",1, 1, 1, 1) +0.008802 * getSMEFTCoeffEW("CllR",1, 1, 2, 2)  
            +0.02302 * getSMEFTCoeffEW("CllR",1, 2, 2, 1) +0.015911 * getSMEFTCoeffEW("CllR",2, 2, 2, 2) +0.010198 * getSMEFTCoeffEW("Cqq1R",0, 0, 0, 0) +0.002454 * getSMEFTCoeffEW("Cqq1R",0, 0, 1, 1)  
            -0.047245 * getSMEFTCoeffEW("Cqq1R",0, 0, 2, 2) +0.017942 * getSMEFTCoeffEW("Cqq1R",0, 1, 1, 0) +0.185075 * getSMEFTCoeffEW("Cqq1R",0, 2, 2, 0) +0.010198 * getSMEFTCoeffEW("Cqq1R",1, 1, 1, 1)  
            -0.047245 * getSMEFTCoeffEW("Cqq1R",1, 1, 2, 2) +0.185075 * getSMEFTCoeffEW("Cqq1R",1, 2, 2, 1) -0.304596 * getSMEFTCoeffEW("Cqq1R",2, 2, 2, 2) +0.124698 * getSMEFTCoeffEW("Cqq3R",0, 0, 0, 0)  
            +0.266683 * getSMEFTCoeffEW("Cqq3R",0, 0, 1, 1) +0.784812 * getSMEFTCoeffEW("Cqq3R",0, 0, 2, 2) -0.017288 * getSMEFTCoeffEW("Cqq3R",0, 1, 1, 0) -0.25535 * getSMEFTCoeffEW("Cqq3R",0, 2, 2, 0)  
            +0.124698 * getSMEFTCoeffEW("Cqq3R",1, 1, 1, 1) +0.784812 * getSMEFTCoeffEW("Cqq3R",1, 1, 2, 2) -0.25535 * getSMEFTCoeffEW("Cqq3R",1, 2, 2, 1) -0.027464 * getSMEFTCoeffEW("Cqq3R",2, 2, 2, 2)  
            -0.042467 * getSMEFTCoeffEW("Clq1R",0, 0, 0, 0) -0.042467 * getSMEFTCoeffEW("Clq1R",0, 0, 1, 1) +1.84739 * getSMEFTCoeffEW("Clq1R",0, 0, 2, 2) -0.002814 * getSMEFTCoeffEW("Clq1R",1, 1, 0, 0)  
            -0.002814 * getSMEFTCoeffEW("Clq1R",1, 1, 1, 1) +0.093811 * getSMEFTCoeffEW("Clq1R",1, 1, 2, 2) -0.002814 * getSMEFTCoeffEW("Clq1R",2, 2, 0, 0) -0.002814 * getSMEFTCoeffEW("Clq1R",2, 2, 1, 1)  
            +0.093811 * getSMEFTCoeffEW("Clq1R",2, 2, 2, 2) -0.311452 * getSMEFTCoeffEW("Clq3R",0, 0, 0, 0) -0.311452 * getSMEFTCoeffEW("Clq3R",0, 0, 1, 1) -1.7689 * getSMEFTCoeffEW("Clq3R",0, 0, 2, 2)  
            +0.101948 * getSMEFTCoeffEW("Clq3R",1, 1, 0, 0) +0.101948 * getSMEFTCoeffEW("Clq3R",1, 1, 1, 1) +0.437729 * getSMEFTCoeffEW("Clq3R",1, 1, 2, 2) +0.101948 * getSMEFTCoeffEW("Clq3R",2, 2, 0, 0)  
            +0.101948 * getSMEFTCoeffEW("Clq3R",2, 2, 1, 1) +0.437729 * getSMEFTCoeffEW("Clq3R",2, 2, 2, 2) -0.083555 * getSMEFTCoeffEW("CeeR",0, 0, 0, 0) -0.077394 * getSMEFTCoeffEW("CeeR",0, 0, 1, 1)  
            -0.077394 * getSMEFTCoeffEW("CeeR",0, 0, 2, 2) +0.006162 * getSMEFTCoeffEW("CeeR",1, 1, 1, 1) +0.012323 * getSMEFTCoeffEW("CeeR",1, 1, 2, 2) +0.006162 * getSMEFTCoeffEW("CeeR",2, 2, 2, 2)  
            +0.005562 * getSMEFTCoeffEW("CuuR",0, 0, 0, 0) +0.009815 * getSMEFTCoeffEW("CuuR",0, 0, 1, 1) +0.1274 * getSMEFTCoeffEW("CuuR",0, 0, 2, 2) +0.001309 * getSMEFTCoeffEW("CuuR",0, 1, 1, 0)  
            +0.076969 * getSMEFTCoeffEW("CuuR",0, 2, 2, 0) +0.005562 * getSMEFTCoeffEW("CuuR",1, 1, 1, 1) +0.1274 * getSMEFTCoeffEW("CuuR",1, 1, 2, 2) +0.076969 * getSMEFTCoeffEW("CuuR",1, 2, 2, 1)  
            +0.00139 * getSMEFTCoeffEW("CddR",0, 0, 0, 0) +0.002454 * getSMEFTCoeffEW("CddR",0, 0, 1, 1) +0.002454 * getSMEFTCoeffEW("CddR",0, 0, 2, 2) +0.00139 * getSMEFTCoeffEW("CddR",1, 1, 1, 1)  
            +0.002454 * getSMEFTCoeffEW("CddR",1, 1, 2, 2) +0.00139 * getSMEFTCoeffEW("CddR",2, 2, 2, 2) +0.058456 * getSMEFTCoeffEW("CeuR",0, 0, 0, 0) +0.058456 * getSMEFTCoeffEW("CeuR",0, 0, 1, 1)  
            +1.54943 * getSMEFTCoeffEW("CeuR",0, 0, 2, 2) -0.005628 * getSMEFTCoeffEW("CeuR",1, 1, 0, 0) -0.005628 * getSMEFTCoeffEW("CeuR",1, 1, 1, 1) -0.114259 * getSMEFTCoeffEW("CeuR",1, 1, 2, 2)  
            -0.005628 * getSMEFTCoeffEW("CeuR",2, 2, 0, 0) -0.005628 * getSMEFTCoeffEW("CeuR",2, 2, 1, 1) -0.114259 * getSMEFTCoeffEW("CeuR",2, 2, 2, 2) -0.029228 * getSMEFTCoeffEW("CedR",0, 0, 0, 0)  
            -0.029228 * getSMEFTCoeffEW("CedR",0, 0, 1, 1) -0.029228 * getSMEFTCoeffEW("CedR",0, 0, 2, 2) +0.002814 * getSMEFTCoeffEW("CedR",1, 1, 0, 0) +0.002814 * getSMEFTCoeffEW("CedR",1, 1, 1, 1)  
            +0.002814 * getSMEFTCoeffEW("CedR",1, 1, 2, 2) +0.002814 * getSMEFTCoeffEW("CedR",2, 2, 0, 0) +0.002814 * getSMEFTCoeffEW("CedR",2, 2, 1, 1) +0.002814 * getSMEFTCoeffEW("CedR",2, 2, 2, 2)  
            -0.002454 * getSMEFTCoeffEW("Cud1R",0, 0, 0, 0) -0.002454 * getSMEFTCoeffEW("Cud1R",0, 0, 1, 1) -0.002454 * getSMEFTCoeffEW("Cud1R",0, 0, 2, 2) -0.002454 * getSMEFTCoeffEW("Cud1R",1, 1, 0, 0)  
            -0.002454 * getSMEFTCoeffEW("Cud1R",1, 1, 1, 1) -0.002454 * getSMEFTCoeffEW("Cud1R",1, 1, 2, 2) -0.03185 * getSMEFTCoeffEW("Cud1R",2, 2, 0, 0) -0.03185 * getSMEFTCoeffEW("Cud1R",2, 2, 1, 1)  
            -0.03185 * getSMEFTCoeffEW("Cud1R",2, 2, 2, 2) +0.012013 * getSMEFTCoeffEW("CleR",0, 0, 0, 0) +0.044055 * getSMEFTCoeffEW("CleR",0, 0, 1, 1) +0.044055 * getSMEFTCoeffEW("CleR",0, 0, 2, 2)  
            -0.027641 * getSMEFTCoeffEW("CleR",1, 1, 0, 0) +0.004401 * getSMEFTCoeffEW("CleR",1, 1, 1, 1) +0.004401 * getSMEFTCoeffEW("CleR",1, 1, 2, 2) -0.027641 * getSMEFTCoeffEW("CleR",2, 2, 0, 0)  
            +0.004401 * getSMEFTCoeffEW("CleR",2, 2, 1, 1) +0.004401 * getSMEFTCoeffEW("CleR",2, 2, 2, 2) -0.084935 * getSMEFTCoeffEW("CluR",0, 0, 0, 0) -0.084935 * getSMEFTCoeffEW("CluR",0, 0, 1, 1)  
            -2.17316 * getSMEFTCoeffEW("CluR",0, 0, 2, 2) -0.005628 * getSMEFTCoeffEW("CluR",1, 1, 0, 0) -0.005628 * getSMEFTCoeffEW("CluR",1, 1, 1, 1) -0.114259 * getSMEFTCoeffEW("CluR",1, 1, 2, 2)  
            -0.005628 * getSMEFTCoeffEW("CluR",2, 2, 0, 0) -0.005628 * getSMEFTCoeffEW("CluR",2, 2, 1, 1) -0.114259 * getSMEFTCoeffEW("CluR",2, 2, 2, 2) +0.042467 * getSMEFTCoeffEW("CldR",0, 0, 0, 0)  
            +0.042467 * getSMEFTCoeffEW("CldR",0, 0, 1, 1) +0.042467 * getSMEFTCoeffEW("CldR",0, 0, 2, 2) +0.002814 * getSMEFTCoeffEW("CldR",1, 1, 0, 0) +0.002814 * getSMEFTCoeffEW("CldR",1, 1, 1, 1)  
            +0.002814 * getSMEFTCoeffEW("CldR",1, 1, 2, 2) +0.002814 * getSMEFTCoeffEW("CldR",2, 2, 0, 0) +0.002814 * getSMEFTCoeffEW("CldR",2, 2, 1, 1) +0.002814 * getSMEFTCoeffEW("CldR",2, 2, 2, 2)  
            +0.029228 * getSMEFTCoeffEW("CqeR",0, 0, 0, 0) -0.002814 * getSMEFTCoeffEW("CqeR",0, 0, 1, 1) -0.002814 * getSMEFTCoeffEW("CqeR",0, 0, 2, 2) +0.029228 * getSMEFTCoeffEW("CqeR",1, 1, 0, 0)  
            -0.002814 * getSMEFTCoeffEW("CqeR",1, 1, 1, 1) -0.002814 * getSMEFTCoeffEW("CqeR",1, 1, 2, 2) -1.32316 * getSMEFTCoeffEW("CqeR",2, 2, 0, 0) +0.093811 * getSMEFTCoeffEW("CqeR",2, 2, 1, 1)  
            +0.093811 * getSMEFTCoeffEW("CqeR",2, 2, 2, 2) +0.002454 * getSMEFTCoeffEW("Cqu1R",0, 0, 0, 0) +0.002454 * getSMEFTCoeffEW("Cqu1R",0, 0, 1, 1) +0.03185 * getSMEFTCoeffEW("Cqu1R",0, 0, 2, 2)  
            +0.002454 * getSMEFTCoeffEW("Cqu1R",1, 1, 0, 0) +0.002454 * getSMEFTCoeffEW("Cqu1R",1, 1, 1, 1) +0.03185 * getSMEFTCoeffEW("Cqu1R",1, 1, 2, 2) -0.047245 * getSMEFTCoeffEW("Cqu1R",2, 2, 0, 0)  
            -0.047245 * getSMEFTCoeffEW("Cqu1R",2, 2, 1, 1) +0.181949 * getSMEFTCoeffEW("Cqu1R",2, 2, 2, 2) -0.001227 * getSMEFTCoeffEW("Cqd1R",0, 0, 0, 0) -0.001227 * getSMEFTCoeffEW("Cqd1R",0, 0, 1, 1)  
            -0.001227 * getSMEFTCoeffEW("Cqd1R",0, 0, 2, 2) -0.001227 * getSMEFTCoeffEW("Cqd1R",1, 1, 0, 0) -0.001227 * getSMEFTCoeffEW("Cqd1R",1, 1, 1, 1) -0.001227 * getSMEFTCoeffEW("Cqd1R",1, 1, 2, 2)  
            +0.023623 * getSMEFTCoeffEW("Cqd1R",2, 2, 0, 0) +0.023623 * getSMEFTCoeffEW("Cqd1R",2, 2, 1, 1) +0.023623 * getSMEFTCoeffEW("Cqd1R",2, 2, 2, 2) ) * v2; 
    
    // Translated to GeV^-2 
    deltaNLO = deltaNLO / trueSM.GeVminus2_to_nb;
    
    return sigma_had + cNLOd6 * deltaNLO;
}

◆ deltaxseeWW4fLEP2()

const double NPSMEFTd6General::deltaxseeWW4fLEP2	(	const double	sqrt_s,
		const int	fstate
	)		const

virtual

The new physics contribution to the cross section in pb for $e^+ e^- \to W^+ W^- \to 4f $, with $ 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) $ the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].

Returns: $\delta sigma$ [pb]

Reimplemented from NPbase.

Definition at line 36562 of file NPSMEFTd6General.cpp.

                                                                                            {
 
    //  Returns cross section in pb
 
    //  fstate = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj),
    //       4 (e v e v), 5 (mu v mu v), 6 (tau v tau v),
    //       7 (e v mu v), 8 (e v tau v), 9 (mu v tau v)
    //      10 (l v jj), 11 (l v l v)
 
    double xspb = 0.0;
 
    double xspbSM0;
    double xspbSM[8] = {0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0};
    // SM values from hep-ex/0409016    
    double xsjjjjSM[8] = {7.42, 7.56, 7.68, 7.76, 7.79, 7.81, 7.82, 7.82};
    double xslvjjSM[8] = {7.14, 7.26, 7.38, 7.44, 7.47, 7.50, 7.50, 7.50}; // All leptons. Divide by 3 for each
    double xslvlvSM[8] = {1.72, 1.76, 1.79, 1.80, 1.81, 1.82, 1.82, 1.82}; // All leptons. Divide by 6 for each
 
    double dgWve, dgWpm1, dgWpm2, dmZ2, dmW2, dGW, dGZ, dGF, dgZ, dsW2, dgVZee, dgAZee, dgZ1, dgga1, dkga, dkZ, dlga, dlZ, deem;
 
    double gVZeeSM, gAZeeSM;
 
    double norm4f = 1.0;
 
    //  Values of the couplings: final-state independent couplings
    gVZeeSM = -0.25 + sW2_tree;
    gAZeeSM = -0.25;
 
    dGF = delta_GF / sqrt(2.0);
 
    dmZ2 = cAsch * (0.5 * getSMEFTCoeffEW("CHD") + 2.0 * cW_tree * sW_tree * getSMEFTCoeffEW("CHWB")) * v2
            + cWsch * (0.5 * getSMEFTCoeffEW("CHD") + 2.0 * (Mw_inp / Mz) * sqrt(1.0 - Mw_inp * Mw_inp / Mz / Mz) * getSMEFTCoeffEW("CHWB")) * v2;
 
    dmW2 = -2.0 * deltaMwd6(); //There is a minus sign between refs. definition of dmW2 and ours
 
    dGW = deltaGwd6();
 
    dGZ = deltaGzd6();
 
    dsW2 = cAsch * (-0.5 * (cW2_tree / (1.0 - 2.0 * sW2_tree)) * ((getSMEFTCoeffEW("CHD")
            + 2.0 * getSMEFTCoeffEW("CHWB") / cW_tree / sW_tree) * v2
            + 2.0 * sqrt(2.0) * dGF))
            + cWsch * (1.0 / sW2_tree) * (0.5 * Mw_inp * Mw_inp * getSMEFTCoeffEW("CHD") / Mz / Mz + Mw_inp * sqrt(1.0 - Mw_inp * Mw_inp / Mz / Mz) * getSMEFTCoeffEW("CHWB") / Mz) * v2;
 
    dgZ = -dGF / sqrt(2.0) - 0.5 * dmZ2
            + cW_tree * sW_tree * getSMEFTCoeffEW("CHWB") * v2;
 
    dgVZee = dgZ * gVZeeSM
            - 0.25 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl3R", 0, 0)) * v2
            - sW2_tree * dsW2;
 
    dgAZee = dgZ * gAZeeSM
            + 0.25 * (getSMEFTCoeffEW("CHeR", 0, 0) - getSMEFTCoeffEW("CHl1R", 0, 0) - getSMEFTCoeffEW("CHl3R", 0, 0)) * v2;
 
    dgWve = 0.5 * getSMEFTCoeffEW("CHl3R", 0, 0) * v2
            + cAsch * (0.25 * (cW_tree * getSMEFTCoeffEW("CHWB") / sW_tree) * v2 + 0.25 * dsW2)
            + cWsch * (-dGF / 2.0 / sqrt(2.0));
 
    dgZ1 = deltag1ZNP(sqrt_s);
 
    dgga1 = deltag1gaNP(sqrt_s);
 
    dkga = deltaKgammaNP(sqrt_s);
 
    dkZ = dgZ1 - (sW2_tree / cW2_tree) * (dkga - dgga1);
 
    dlga = -lambdaZNP(sqrt_s);
 
    dlZ = -lambdaZNP(sqrt_s);
 
    deem = delta_e + 0.5 * delta_A;
 
    //  Values of the couplings: final-state dependent couplings
    dgWpm1 = 0.0;
    dgWpm2 = 0.0;
 
    switch (fstate) {
 
        case 0:
            //  fstate = 0 (jjjj)       
            dgWpm1 = 0.5 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1));
            dgWpm2 = 0.5 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1));
            norm4f = 1.01;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xsjjjjSM[i];
            }
            break;
        case 1:
            //  fstate = 1 (e v jj)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 0, 0);
            dgWpm2 = 0.5 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1));
            norm4f = 1.0;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvjjSM[i] / 3.0;
            }
            break;
        case 2:
            //  fstate = 2 (mu v jj)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 1, 1);
            dgWpm2 = 0.5 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1));
            norm4f = 1.0;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvjjSM[i] / 3.0;
            }
            break;
        case 3:
            //  fstate = 3 (tau v jj)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 2, 2);
            dgWpm2 = 0.5 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1));
            norm4f = 1.0;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvjjSM[i] / 3.0;
            }
            break;
        case 4:
            //  fstate = 4 (e v e v)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 0, 0);
            dgWpm2 = getSMEFTCoeffEW("CHl3R", 0, 0);
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i] / 6.0;
            }
            break;
        case 5:
            //  fstate = 5 (mu v mu v)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 1, 1);
            dgWpm2 = getSMEFTCoeffEW("CHl3R", 1, 1);
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i] / 6.0;
            }
            break;
        case 6:
            //  fstate = 6 (tau v tau v)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 2, 2);
            dgWpm2 = getSMEFTCoeffEW("CHl3R", 2, 2);
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i] / 6.0;
            }
            break;
        case 7:
            //  fstate = 7 (e v mu v)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 0, 0);
            dgWpm2 = getSMEFTCoeffEW("CHl3R", 1, 1);
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i] / 6.0;
            }
            break;
        case 8:
            //  fstate = 8 (e v tau v)           
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 0, 0);
            dgWpm2 = getSMEFTCoeffEW("CHl3R", 2, 2);
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i] / 6.0;
            }
            break;
        case 9:
            //  fstate = 9 (mu v tau v)           
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 1, 1);
            dgWpm2 = getSMEFTCoeffEW("CHl3R", 2, 2);
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i] / 6.0;
            }
            break;
        case 10:
            //  fstate = 10 (l v jj)           
            dgWpm1 = (1.0 / 3.0) * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1) + getSMEFTCoeffEW("CHl3R", 2, 2));
            dgWpm2 = 0.5 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1));
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvjjSM[i];
            }
            break;
        case 11:
            //  fstate = 11 (l v l v)           
            dgWpm1 = (1.0 / 3.0) * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1) + getSMEFTCoeffEW("CHl3R", 2, 2));
            dgWpm2 = (1.0 / 3.0) * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1) + getSMEFTCoeffEW("CHl3R", 2, 2));
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i];
            }
            break;
    }
 
    dgWpm1 = 0.5 * dgWpm1
            + cAsch * (0.25 * (cW_tree * getSMEFTCoeffEW("CHWB") / sW_tree) * v2 + 0.25 * dsW2)
            + cWsch * (-dGF / 2.0 / sqrt(2.0));
 
    dgWpm2 = 0.5 * dgWpm2
            + cAsch * (0.25 * (cW_tree * getSMEFTCoeffEW("CHWB") / sW_tree) * v2 + 0.25 * dsW2)
            + cWsch * (-dGF / 2.0 / sqrt(2.0));
 
    if (sqrt_s == 0.1886) {
 
        xspb += norm4f * cAsch * (
                +2.6 * dmW2
                - 17.0 * dGW
                + 72.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 5.3 * dgVZee
                + 0.3 * dgAZee
                - 0.08 * dgZ1
                - 0.50 * dkga
                - 0.19 * dkZ
                - 0.29 * dlga
                + 0.026 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 72.0 * dgWve
                + 33.4 * dgWpm1
                + 33.4 * dgWpm2
                + 5.72 * dgVZee
                + 0.21 * dgAZee
                - 0.05 * dgZ1
                - 0.57 * dkga
                - 0.16 * dkZ
                - 0.34 * dlga
                + 0.051 * dlZ
                + 0.0005 * dGZ
                - 0.41 * dgga1
                - 0.98 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
        // Save the SM value, to check the total cross section, SM+NP is not negative
        xspbSM0 = xspbSM[0];
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[0];
 
    } else if (sqrt_s == 0.1916) {
 
        xspb += norm4f * cAsch * (
                +1.6 * dmW2
                - 17.0 * dGW
                + 73.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 5.8 * dgVZee
                + 0.4 * dgAZee
                - 0.10 * dgZ1
                - 0.56 * dkga
                - 0.22 * dkZ
                - 0.32 * dlga
                + 0.018 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 72.0 * dgWve
                + 33.6 * dgWpm1
                + 33.6 * dgWpm2
                + 6.26 * dgVZee
                + 0.33 * dgAZee
                - 0.07 * dgZ1
                - 0.64 * dkga
                - 0.19 * dkZ
                - 0.37 * dlga
                + 0.045 * dlZ
                + 0.0005 * dGZ
                - 0.41 * dgga1
                - 1.08 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        // Save the SM value, to check the total cross section, SM+NP is not negative
        xspbSM0 = xspbSM[1];
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[1];
 
    } else if (sqrt_s == 0.1955) {
 
        xspb += norm4f * cAsch * (
                +0.26 * dmW2
                - 17.0 * dGW
                + 74.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 6.5 * dgVZee
                + 0.6 * dgAZee
                - 0.12 * dgZ1
                - 0.64 * dkga
                - 0.27 * dkZ
                - 0.36 * dlga
                + 0.005 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 73.0 * dgWve
                + 33.8 * dgWpm1
                + 33.8 * dgWpm2
                + 6.91 * dgVZee
                + 0.50 * dgAZee
                - 0.09 * dgZ1
                - 0.72 * dkga
                - 0.22 * dkZ
                - 0.41 * dlga
                + 0.035 * dlZ
                + 0.0005 * dGZ
                - 0.49 * dgga1
                - 1.20 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        // Save the SM value, to check the total cross section, SM+NP is not negative
        xspbSM0 = xspbSM[2];
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[2];
 
    } else if (sqrt_s == 0.1995) {
 
        xspb += norm4f * cAsch * (
                -0.54 * dmW2
                - 17.0 * dGW
                + 75.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 7.1 * dgVZee
                + 0.8 * dgAZee
                - 0.15 * dgZ1
                - 0.71 * dkga
                - 0.31 * dkZ
                - 0.40 * dlga
                - 0.009 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 74.0 * dgWve
                + 33.7 * dgWpm1
                + 33.7 * dgWpm2
                + 7.52 * dgVZee
                + 0.68 * dgAZee
                - 0.11 * dgZ1
                - 0.79 * dkga
                - 0.26 * dkZ
                - 0.45 * dlga
                + 0.022 * dlZ
                + 0.0005 * dGZ
                - 0.53 * dgga1
                - 1.33 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        // Save the SM value, to check the total cross section, SM+NP is not negative
        xspbSM0 = xspbSM[3];
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[3];
 
    } else if (sqrt_s == 0.2016) {
 
        xspb += norm4f * cAsch * (
                -0.97 * dmW2
                - 17.0 * dGW
                + 75.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 7.4 * dgVZee
                + 0.9 * dgAZee
                - 0.16 * dgZ1
                - 0.75 * dkga
                - 0.33 * dkZ
                - 0.42 * dlga
                - 0.017 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 74.0 * dgWve
                + 33.7 * dgWpm1
                + 33.7 * dgWpm2
                + 7.82 * dgVZee
                + 0.78 * dgAZee
                - 0.12 * dgZ1
                - 0.83 * dkga
                - 0.28 * dkZ
                - 0.47 * dlga
                + 0.016 * dlZ
                + 0.0005 * dGZ
                - 0.55 * dgga1
                - 1.39 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        // Save the SM value, to check the total cross section, SM+NP is not negative
        xspbSM0 = xspbSM[4];
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[4];
 
    } else if (sqrt_s == 0.2049) {
 
        xspb += norm4f * cAsch * (
                -1.4 * dmW2
                - 17.0 * dGW
                + 75.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 7.8 * dgVZee
                + 1.0 * dgAZee
                - 0.18 * dgZ1
                - 0.80 * dkga
                - 0.37 * dkZ
                - 0.44 * dlga
                - 0.029 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 74.0 * dgWve
                + 33.5 * dgWpm1
                + 33.5 * dgWpm2
                + 8.24 * dgVZee
                + 0.93 * dgAZee
                - 0.14 * dgZ1
                - 0.89 * dkga
                - 0.32 * dkZ
                - 0.47 * dlga
                + 0.005 * dlZ
                + 0.0005 * dGZ
                - 0.58 * dgga1
                - 1.47 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        // Save the SM value, to check the total cross section, SM+NP is not negative
        xspbSM0 = xspbSM[5];
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[5];
 
    } else if (sqrt_s == 0.2066) {
 
        xspb += norm4f * cAsch * (
                -1.8 * dmW2
                - 17.0 * dGW
                + 76.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 8.0 * dgVZee
                + 1.1 * dgAZee
                - 0.19 * dgZ1
                - 0.83 * dkga
                - 0.39 * dkZ
                - 0.46 * dlga
                - 0.036 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 75.0 * dgWve
                + 33.4 * dgWpm1
                + 33.4 * dgWpm2
                + 8.45 * dgVZee
                + 1.01 * dgAZee
                - 0.15 * dgZ1
                - 0.92 * dkga
                - 0.33 * dkZ
                - 0.51 * dlga
                - 0.001 * dlZ
                + 0.0005 * dGZ
                - 0.60 * dgga1
                - 1.52 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        // Save the SM value, to check the total cross section, SM+NP is not negative
        xspbSM0 = xspbSM[6];
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[6];
 
    } else if (sqrt_s == 0.208) {
 
        xspb += norm4f * cAsch * (
                -2.0 * dmW2
                - 17.0 * dGW
                + 76.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 8.2 * dgVZee
                + 1.2 * dgAZee
                - 0.20 * dgZ1
                - 0.85 * dkga
                - 0.40 * dkZ
                - 0.47 * dlga
                - 0.042 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 75.0 * dgWve
                + 33.3 * dgWpm1
                + 33.3 * dgWpm2
                + 8.62 * dgVZee
                + 1.08 * dgAZee
                - 0.16 * dgZ1
                - 0.94 * dkga
                - 0.35 * dkZ
                - 0.52 * dlga
                - 0.007 * dlZ
                + 0.0005 * dGZ
                - 0.61 * dgga1
                - 1.55 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        // Save the SM value, to check the total cross section, SM+NP is not negative
        xspbSM0 = xspbSM[7];
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[7];
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::deltaxseeWW4fLEP2()");
 
    if ((xspbSM0 + xspb) < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return xspb;
}

◆ deltaxseeWWtotLEP2()

const double NPSMEFTd6General::deltaxseeWWtotLEP2 ( const double sqrt_s ) const

virtual

The new physics contribution to the total cross section in pb for $e^+ e^- \to W^+ W^-$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].

Returns: $\delta sigma$ [pb]

Reimplemented from NPbase.

Definition at line 37664 of file NPSMEFTd6General.cpp.

                                                                           {
    return ( deltaxseeWW4fLEP2(sqrt_s, 0) + deltaxseeWW4fLEP2(sqrt_s, 10) + deltaxseeWW4fLEP2(sqrt_s, 11));
}

◆ deltayb_HB()

const double NPSMEFTd6General::deltayb_HB ( const double mu ) const

virtual

The Higgs-basis coupling $\delta y_b$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta y_b$

Reimplemented from NPbase.

Definition at line 43097 of file NPSMEFTd6General.cpp.

                                                               {
    double mf = (quarks[BOTTOM].getMass());
    double d_h_mu, d_GF_mu;
    double ciHB;
    
    d_h_mu = (-getSMEFTCoeff("CHD", mu) / 4.0 + getSMEFTCoeff("CHbox", mu) ) * v2;
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
 
    ciHB = -(v() / mf / sqrt(2.0)) * getSMEFTCoeff("CdHR", 2, 2, mu) * v2 + d_h_mu - 0.5 * d_GF_mu;
 
    return ciHB;
}

◆ deltayc_HB()

const double NPSMEFTd6General::deltayc_HB ( const double mu ) const

virtual

The Higgs-basis coupling $\delta y_c$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta y_c$

Reimplemented from NPbase.

Definition at line 43123 of file NPSMEFTd6General.cpp.

                                                               {
    double mf = (quarks[CHARM].getMass());
    double d_h_mu, d_GF_mu;
    double ciHB;
    
    d_h_mu = (-getSMEFTCoeff("CHD", mu) / 4.0 + getSMEFTCoeff("CHbox", mu) ) * v2;
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
 
    ciHB = -(v() / mf / sqrt(2.0)) * getSMEFTCoeff("CuHR", 1, 1, mu) * v2 + d_h_mu - 0.5 * d_GF_mu;
 
    return ciHB;
}

◆ deltaymu_HB()

const double NPSMEFTd6General::deltaymu_HB ( const double mu ) const

virtual

The Higgs-basis coupling $\delta y_\mu$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta y_\mu$

Reimplemented from NPbase.

Definition at line 43149 of file NPSMEFTd6General.cpp.

                                                                {
    double mf = (leptons[MU].getMass());
    double d_h_mu, d_GF_mu;
    double ciHB;
 
    d_h_mu = (-getSMEFTCoeff("CHD", mu) / 4.0 + getSMEFTCoeff("CHbox", mu) ) * v2;
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
 
    ciHB = -(v() / mf / sqrt(2.0)) * getSMEFTCoeff("CeHR", 1, 1, mu) * v2 + d_h_mu - 0.5 * d_GF_mu;
 
    return ciHB;
}

◆ deltays_HB()

const double NPSMEFTd6General::deltays_HB ( const double mu ) const

virtual

The Higgs-basis coupling $\delta y_s$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta y_s$

Reimplemented from NPbase.

Definition at line 43136 of file NPSMEFTd6General.cpp.

                                                               {
    double mf = (quarks[STRANGE].getMass());
    double d_h_mu, d_GF_mu;
    double ciHB;
    
    d_h_mu = (-getSMEFTCoeff("CHD", mu) / 4.0 + getSMEFTCoeff("CHbox", mu) ) * v2;
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
 
    ciHB = -(v() / mf / sqrt(2.0)) * getSMEFTCoeff("CdHR", 1, 1, mu) * v2 + d_h_mu - 0.5 * d_GF_mu;
 
    return ciHB;
}

◆ deltayt_HB()

const double NPSMEFTd6General::deltayt_HB ( const double mu ) const

virtual

The Higgs-basis coupling $\delta y_t$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta y_t$

Reimplemented from NPbase.

Definition at line 43084 of file NPSMEFTd6General.cpp.

                                                               {
    double mf = mtpole;
    double d_h_mu, d_GF_mu;
    double ciHB;
    
    d_h_mu = (-getSMEFTCoeff("CHD", mu) / 4.0 + getSMEFTCoeff("CHbox", mu) ) * v2;
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
 
    ciHB = -(v() / mf / sqrt(2.0)) * getSMEFTCoeff("CuHR", 2, 2, mu) * v2 + d_h_mu - 0.5 * d_GF_mu;
 
    return ciHB;
}

◆ deltaytau_HB()

const double NPSMEFTd6General::deltaytau_HB ( const double mu ) const

virtual

The Higgs-basis coupling $\delta y_\tau$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta y_\tau$

Reimplemented from NPbase.

Definition at line 43110 of file NPSMEFTd6General.cpp.

                                                                 {
    double mf = (leptons[TAU].getMass());
    double d_h_mu, d_GF_mu;
    double ciHB;
    
    d_h_mu = (-getSMEFTCoeff("CHD", mu) / 4.0 + getSMEFTCoeff("CHbox", mu) ) * v2;
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
 
    ciHB = -(v() / mf / sqrt(2.0)) * getSMEFTCoeff("CeHR", 2, 2, mu) * v2 + d_h_mu - 0.5 * d_GF_mu;
 
    return ciHB;
}

◆ delU_gCC()

const double NPSMEFTd6General::delU_gCC ( const double mu ) const

virtual

Universal indirect correction to EW charged currents.

Parameters

[in] mu the RG scale associated to the observable where the function is used

Returns: $\delta g_{CC}^{U}(\mu)$

Definition at line 15420 of file NPSMEFTd6General.cpp.

                                                             {
    
    double dg;
    
    // Same expressions as in PostUpdate, with scale dependence (on NP only)    
    dg = (del_e_mu(mu) - 0.5 * del_sW2_mu(mu));
    
    return dg;
}

◆ delU_gNC()

const double NPSMEFTd6General::delU_gNC ( const double mu ) const

virtual

Universal indirect correction to EW neutral currents.

Parameters

[in] mu the RG scale associated to the observable where the function is used

Returns: $\delta g_{NC}^{U}(\mu)$

Definition at line 15391 of file NPSMEFTd6General.cpp.

                                                             {
    
    double dg;
 
    double d_GF_mu, d_MW_mu, d_MZ_mu;
    
    // Same expressions as in PostUpdate, with scale dependence (on NP only)   
    d_GF_mu = ((getSMEFTCoeff("CHl3R", 0, 0, mu) + getSMEFTCoeff("CHl3R", 1, 1, mu) - 0.5 * (getSMEFTCoeff("CllR", 0, 1, 1, 0, mu) + getSMEFTCoeff("CllR", 1, 0, 0, 1, mu))) * v2);
    d_MW_mu = (3.0 / 8.0) * (getSMEFTCoeff("CH", mu) / lambdaH_tree) * v2;
    d_MZ_mu = (sW_tree * cW_tree * getSMEFTCoeff("CHWB", mu) + 0.25 * getSMEFTCoeff("CHD", mu) + (3.0 / 8.0) * getSMEFTCoeff("CH", mu) / lambdaH_tree) * v2;
    
    
    dg = (0.5 * del_Z_mu(mu) - 0.5 * d_GF_mu + d_MW_mu - d_MZ_mu);
    
    return dg;
}

◆ dxsdcoseeWWlvjjLEP2()

const double NPSMEFTd6General::dxsdcoseeWWlvjjLEP2	(	const double	sqrt_s,
		const int	bin
	)		const

virtual

The differential cross section in pb for $e^+ e^- \to W^+ W^- \to lv jj $, with $ l= e,\mu $ for the 4 $ cos{\theta}$ bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph].

Returns: $d\sigma/d\cos{\theta}$ [pb]

Reimplemented from NPbase.

Definition at line 38055 of file NPSMEFTd6General.cpp.

                                                                                           {
 
    //  Returns differential cross section in pb  
    //  bin = 1, 2, 3, 4
 
    double xspb = 0.0;
 
    double xspbSM = 0.0;
    // SM values from Table 8 in hep-ex/0409016
    // Sum bin contents into B1=[-1,-0.8], B2=[-0.4,-0.2], B3=[0.4,0.6], B4=[0.8,1]
    double xslvjjSM183[4] = {0.74, 1.20, 2.86, 5.47};
    double xslvjjSM206[4] = {0.52, 0.98, 2.92, 7.80};
 
    double dgWve, dgWpm1, dgWpm2, dmZ2, dmW2, dGW, dGF, dgZ, dsW2, dgVZee, dgAZee, dgZ1, dgga1, dkga, dkZ, dlga, dlZ, deem;
 
    double gVZeeSM, gAZeeSM;
 
    //  Values of the couplings: final-state independent couplings
    gVZeeSM = -0.25 + sW2_tree;
    gAZeeSM = -0.25;
 
    dGF = delta_GF / sqrt(2.0);
 
    dmZ2 = cAsch * (0.5 * getSMEFTCoeffEW("CHD") + 2.0 * cW_tree * sW_tree * getSMEFTCoeffEW("CHWB")) * v2
            + cWsch * (0.5 * getSMEFTCoeffEW("CHD") + 2.0 * (Mw_inp / Mz) * sqrt(1.0 - Mw_inp * Mw_inp / Mz / Mz) * getSMEFTCoeffEW("CHWB")) * v2;
 
    dmW2 = -2.0 * deltaMwd6(); //There is a minus sign between refs. definition of dmW2 and ours
 
    dGW = deltaGwd6();
 
    dsW2 = cAsch * (-0.5 * (cW2_tree / (1.0 - 2.0 * sW2_tree)) * ((getSMEFTCoeffEW("CHD")
            + 2.0 * getSMEFTCoeffEW("CHWB") / cW_tree / sW_tree) * v2
            + 2.0 * sqrt(2.0) * dGF))
            + cWsch * (1.0 / sW2_tree) * (0.5 * Mw_inp * Mw_inp * getSMEFTCoeffEW("CHD") / Mz / Mz + Mw_inp * sqrt(1.0 - Mw_inp * Mw_inp / Mz / Mz) * getSMEFTCoeffEW("CHWB") / Mz) * v2;
 
    dgZ = -dGF / sqrt(2.0) - 0.5 * dmZ2
            + cW_tree * sW_tree * getSMEFTCoeffEW("CHWB") * v2;
 
    dgVZee = dgZ * gVZeeSM
            - 0.25 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl3R", 0, 0)) * v2
            - sW2_tree * dsW2;
 
    dgAZee = dgZ * gAZeeSM
            + 0.25 * (getSMEFTCoeffEW("CHeR", 0, 0) - getSMEFTCoeffEW("CHl1R", 0, 0) - getSMEFTCoeffEW("CHl3R", 0, 0)) * v2;
 
    dgWve = 0.5 * getSMEFTCoeffEW("CHl3R", 0, 0) * v2
            + cAsch * (0.25 * (cW_tree * getSMEFTCoeffEW("CHWB") / sW_tree) * v2 + 0.25 * dsW2)
            + cWsch * (-dGF / 2.0 / sqrt(2.0));
 
    dgZ1 = deltag1ZNP(sqrt_s);
 
    dgga1 = deltag1gaNP(sqrt_s);
 
    dkga = deltaKgammaNP(sqrt_s);
 
    dkZ = dgZ1 - (sW2_tree / cW2_tree) * (dkga - dgga1);
 
    dlga = -lambdaZNP(sqrt_s);
 
    dlZ = -lambdaZNP(sqrt_s);
 
    deem = delta_e + 0.5 * delta_A;
 
    //  Values of the couplings for the W decays: I assume ME from arXiv: 1606.06693 [hep-ph] are, as in
    //  the LEP2 experimental analyses they use, for l=e, mu
    dgWpm1 = 0.25 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) * v2
            + cAsch * (0.25 * (cW_tree * getSMEFTCoeffEW("CHWB") / sW_tree) * v2 + 0.25 * dsW2)
            + cWsch * (-dGF / 2.0 / sqrt(2.0));
 
    dgWpm2 = 0.25 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1)) * v2
            + cAsch * (0.25 * (cW_tree * getSMEFTCoeffEW("CHWB") / sW_tree) * v2 + 0.25 * dsW2)
            + cWsch * (-dGF / 2.0 / sqrt(2.0));
 
    if (sqrt_s == 0.1827) {
 
        switch (bin) {
            case 1:
                //  Bin 1        
                xspbSM = xslvjjSM183[0];
                xspb += xspbSM
                        + cAsch * (-1.6 * dmW2
                        - 1.5 * dGW
                        + 12.0 * dgWve
                        + 2.9 * dgWpm1
                        + 2.9 * dgWpm2
                        + 4.1 * dgVZee
                        + 3.0 * dgAZee
                        - 0.44 * dgZ1
                        - 0.34 * dkga
                        - 0.47 * dkZ
                        - 0.32 * dlga
                        - 0.45 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -1.5 * dGW
                        + 12.0 * dgWve
                        + 2.9 * dgWpm1
                        + 2.9 * dgWpm2
                        + 4.3 * dgVZee
                        + 3.0 * dgAZee
                        - 0.42 * dgZ1
                        - 0.37 * dkga
                        - 0.45 * dkZ
                        - 0.35 * dlga
                        - 0.43 * dlZ
                        - 0.34 * dgga1
                        - 0.71 * deem
                        );
 
                break;
 
            case 2:
                //  Bin 2   
                xspbSM = xslvjjSM183[1];
                xspb += xspbSM
                        + cAsch * (-1.5 * dmW2
                        - 2.8 * dGW
                        + 16.0 * dgWve
                        + 5.5 * dgWpm1
                        + 5.5 * dgWpm2
                        + 3.5 * dgVZee
                        + 2.2 * dgAZee
                        - 0.30 * dgZ1
                        - 0.32 * dkga
                        - 0.39 * dkZ
                        - 0.26 * dlga
                        - 0.34 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -2.8 * dGW
                        + 16.0 * dgWve
                        + 5.4 * dgWpm1
                        + 5.4 * dgWpm2
                        + 3.7 * dgVZee
                        + 2.3 * dgAZee
                        - 0.29 * dgZ1
                        - 0.35 * dkga
                        - 0.38 * dkZ
                        - 0.28 * dlga
                        - 0.32 * dlZ
                        - 0.27 * dgga1
                        - 0.62 * deem
                        );
 
                break;
 
            case 3:
                //  Bin 3      
                xspbSM = xslvjjSM183[2];
                xspb += xspbSM
                        + cAsch * (+0.16 * dmW2
                        - 5.3 * dGW
                        + 22.0 * dgWve
                        + 10.0 * dgWpm1
                        + 10.0 * dgWpm2
                        + 1.5 * dgVZee
                        + 0.2 * dgAZee
                        - 0.04 * dgZ1
                        - 0.14 * dkga
                        - 0.06 * dkZ
                        - 0.06 * dlga
                        + 0.026 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -5.2 * dGW
                        + 22.0 * dgWve
                        + 10.2 * dgWpm1
                        + 10.2 * dgWpm2
                        + 1.7 * dgVZee
                        + 0.2 * dgAZee
                        - 0.04 * dgZ1
                        - 0.16 * dkga
                        - 0.06 * dkZ
                        - 0.08 * dlga
                        + 0.03 * dlZ
                        - 0.12 * dgga1
                        - 0.29 * deem
                        );
 
                break;
 
            case 4:
                //  Bin 4        
                xspbSM = xslvjjSM183[3];
                xspb += xspbSM
                        + cAsch * (+18.0 * dmW2
                        - 14.0 * dGW
                        + 39.0 * dgWve
                        + 27.0 * dgWpm1
                        + 27.0 * dgWpm2
                        - 7.7 * dgVZee
                        - 8.8 * dgAZee
                        + 1.2 * dgZ1
                        + 0.62 * dkga
                        + 1.3 * dkZ
                        + 0.63 * dlga
                        + 1.3 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -14.1 * dGW
                        + 40.0 * dgWve
                        + 27.5 * dgWpm1
                        + 27.5 * dgWpm2
                        - 7.8 * dgVZee
                        - 9.0 * dgAZee
                        + 1.20 * dgZ1
                        + 0.67 * dkga
                        + 1.27 * dkZ
                        + 0.68 * dlga
                        + 1.27 * dlZ
                        + 0.64 * dgga1
                        + 1.30 * deem
                        );
 
                break;
 
        }
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
    } else if (sqrt_s == 0.2059) {
 
        switch (bin) {
            case 1:
                //  Bin 1        
                xspbSM = xslvjjSM206[0];
                xspb += xspbSM
                        + cAsch * (-1.1 * dmW2
                        - 0.9 * dGW
                        + 11.0 * dgWve
                        + 1.8 * dgWpm1
                        + 1.8 * dgWpm2
                        + 4.9 * dgVZee
                        + 3.0 * dgAZee
                        - 0.44 * dgZ1
                        - 0.44 * dkga
                        - 0.50 * dkZ
                        - 0.40 * dlga
                        - 0.46 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -0.9 * dGW
                        + 10.0 * dgWve
                        + 1.8 * dgWpm1
                        + 1.8 * dgWpm2
                        + 4.9 * dgVZee
                        + 2.9 * dgAZee
                        - 0.40 * dgZ1
                        - 0.47 * dkga
                        - 0.46 * dkZ
                        - 0.43 * dlga
                        - 0.43 * dlZ
                        - 0.41 * dgga1
                        - 0.88 * deem
                        );
 
                break;
 
            case 2:
                //  Bin 2        
                xspbSM = xslvjjSM206[1];
                xspb += xspbSM
                        + cAsch * (-1.7 * dmW2
                        - 2.1 * dGW
                        + 15.0 * dgWve
                        + 4.1 * dgWpm1
                        + 4.1 * dgWpm2
                        + 5.0 * dgVZee
                        + 2.8 * dgAZee
                        - 0.34 * dgZ1
                        - 0.53 * dkga
                        - 0.55 * dkZ
                        - 0.37 * dlga
                        - 0.41 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -2.0 * dGW
                        + 15.0 * dgWve
                        + 4.0 * dgWpm1
                        + 4.0 * dgWpm2
                        + 5.1 * dgVZee
                        + 2.8 * dgAZee
                        - 0.31 * dgZ1
                        - 0.57 * dkga
                        - 0.51 * dkZ
                        - 0.40 * dlga
                        - 0.38 * dlZ
                        - 0.35 * dgga1
                        - 0.92 * deem
                        );
 
                break;
 
            case 3:
                //  Bin 3        
                xspbSM = xslvjjSM206[2];
                xspb += xspbSM
                        + cAsch * (-2.3 * dmW2
                        - 4.6 * dGW
                        + 22.0 * dgWve
                        + 9.0 * dgWpm1
                        + 9.0 * dgWpm2
                        + 3.5 * dgVZee
                        + 1.2 * dgAZee
                        - 0.19 * dgZ1
                        - 0.35 * dkga
                        - 0.25 * dkZ
                        - 0.19 * dlga
                        - 0.086 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -4.5 * dGW
                        + 22.0 * dgWve
                        + 8.8 * dgWpm1
                        + 8.8 * dgWpm2
                        + 3.7 * dgVZee
                        + 1.2 * dgAZee
                        - 0.17 * dgZ1
                        - 0.39 * dkga
                        - 0.22 * dkZ
                        - 0.21 * dlga
                        - 0.07 * dlZ
                        - 0.27 * dgga1
                        - 0.66 * deem
                        );
 
                break;
 
            case 4:
                //  Bin 4        
                xspbSM = xslvjjSM206[3];
                xspb += xspbSM
                        + cAsch * (+10.0 * dmW2
                        - 20.0 * dGW
                        + 59.0 * dgWve
                        + 39.0 * dgWpm1
                        + 39.0 * dgWpm2
                        - 9.6 * dgVZee
                        - 11.0 * dgAZee
                        + 1.5 * dgZ1
                        + 0.86 * dkga
                        + 1.7 * dkZ
                        + 0.9 * dlga
                        + 1.7 * dlZ)
                        ;
 
                xspb += cWsch * (
                        -19.8 * dGW
                        + 59.0 * dgWve
                        + 39.0 * dgWpm1
                        + 39.0 * dgWpm2
                        - 9.5 * dgVZee
                        - 11.4 * dgAZee
                        + 1.48 * dgZ1
                        + 0.88 * dkga
                        + 1.63 * dkZ
                        + 0.93 * dlga
                        + 1.67 * dlZ
                        + 0.81 * dgga1
                        + 1.69 * deem
                        );
 
                break;
        }
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::dxsdcoseeWWlvjjLEP2()");
 
    //Add relative theory errors (free par). (Assume they are constant in energy.)
    xspb += edeeWWdcint * xspbSM;
 
    if (xspb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return xspb;
}

◆ dxseeWWdcos()

const double NPSMEFTd6General::dxseeWWdcos	(	const double	sqrt_s,
		const double	cos
	)		const

virtual

The differential distribution for $e^+ e^- \to W^+ W^- \to jj \ell \nu$, with $\ell= e, \mu$, as a function of the $W$ polar angle.

Returns: $d\sigma/d\cos{\theta}$

Reimplemented from NPbase.

Definition at line 38448 of file NPSMEFTd6General.cpp.

                                                                                      {
    double sqrt_sGeV = 1000. * sqrt_s;
    double s = sqrt_sGeV * sqrt_sGeV;
    double cos2 = cos * cos;
    double sin2 = 1.0 - cos2;
    double sin = sqrt(sin2);
 
    double topb = 0.3894 * 1000000000.0;
 
    //  NC and CC couplings
    double gLe, gRe;
    gslpp::complex Uenu;
 
    gLe = -0.5 + sW2_tree + deltaGL_f(leptons[ELECTRON]);
    gRe = sW2_tree + deltaGR_f(leptons[ELECTRON]);
 
    Uenu = deltaGL_Wff(leptons[NEUTRINO_1], leptons[ELECTRON]);
    Uenu = 1.0 + Uenu;
 
    //  W mass
    double mw;
 
    mw = Mw();
 
    //  Wigner functions
    double d1pp[2], d1mm[2], d1p0[2], d1m0[2], d10p[2], d10m[2], d100[2];
 
    d1pp[0] = sqrt((1.0 - cos2) / 2.0);
    d1pp[1] = -sqrt((1.0 - cos2) / 2.0);
 
    d1mm[0] = d1pp[0];
    d1mm[1] = d1pp[1];
 
    d1p0[0] = (1.0 - cos) / 2.0;
    d1p0[1] = (1.0 + cos) / 2.0;
 
    d1m0[0] = d1p0[1];
    d1m0[1] = d1p0[0];
 
    d10p[0] = d1p0[1];
    d10p[1] = d1p0[0];
 
    d10m[0] = d1p0[0];
    d10m[1] = d1p0[1];
 
    d100[0] = d1pp[0];
    d100[1] = d1pp[1];
 
    gslpp::matrix<double> d1LH(3, 3, 0.0);
 
    gslpp::matrix<double> d1RH(3, 3, 0.0);
 
    d1LH.assign(0, 0, d1pp[0]);
    d1LH.assign(0, 1, d1p0[0]);
    d1LH.assign(0, 2, 0.0);
 
    d1LH.assign(1, 0, d10p[0]);
    d1LH.assign(1, 1, d100[0]);
    d1LH.assign(1, 2, d10m[0]);
 
    d1LH.assign(2, 0, 0.0);
    d1LH.assign(2, 1, d1m0[0]);
    d1LH.assign(2, 2, d1mm[0]);
 
    d1RH.assign(0, 0, d1pp[1]);
    d1RH.assign(0, 1, d1p0[1]);
    d1RH.assign(0, 2, 0.0);
 
    d1RH.assign(1, 0, d10p[1]);
    d1RH.assign(1, 1, d100[1]);
    d1RH.assign(1, 2, d10m[1]);
 
    d1RH.assign(2, 0, 0.0);
    d1RH.assign(2, 1, d1m0[1]);
    d1RH.assign(2, 2, d1mm[1]);
 
    //  TGC parameterization
    double g1Z, g1ga, kZ, kga, lambdaZ, lambdaga, g4Z, g4ga, g5Z, g5ga, ktZ, ktga, lambdatZ, lambdatga;
 
    //  TGC present in the SM     
    g1Z = 1.0 + deltag1ZNP(sqrt_s);
    g1ga = 1.0;
    kZ = 1.0 + deltag1ZNP(sqrt_s) - (sW2_tree / cW2_tree) * deltaKgammaNP(sqrt_s);
    kga = 1.0 + deltaKgammaNP(sqrt_s);
    //  TGC not present in the SM
    lambdaZ = lambdaZNP(sqrt_s); //Check normalization
    lambdaga = lambdaZ;
    g4Z = 0.0;
    g4ga = 0.0;
    g5Z = 0.0;
    g5ga = 0.0;
    ktZ = 0.0;
    ktga = 0.0;
    lambdatZ = 0.0;
    lambdatga = 0.0;
 
    double f3Z, f3ga;
 
    f3Z = g1Z + kZ + lambdaZ;
    f3ga = g1ga + kga + lambdaga;
 
    // Kinematic factors
    double beta, gamma, gamma2;
 
    beta = sqrt(1.0 - 4.0 * mw * mw / s);
    gamma = sqrt_sGeV / (2.0 * mw);
    gamma2 = gamma*gamma;
 
    //  J=1 Subamplitudes: Z
    gslpp::complex AZpp, AZmm, AZp0, AZm0, AZ0p, AZ0m, AZ00;
 
    AZpp = gslpp::complex(g1Z + 2.0 * gamma2* lambdaZ, (ktZ + lambdatZ - 2.0 * lambdatZ) / beta, false);
    AZmm = gslpp::complex(g1Z + 2.0 * gamma2* lambdaZ, -(ktZ + lambdatZ - 2.0 * lambdatZ) / beta, false);
    AZp0 = gslpp::complex(f3Z + beta * g5Z, -g4Z + (ktZ - lambdatZ) / beta, false);
    AZp0 = gamma * AZp0;
    AZm0 = gslpp::complex(f3Z - beta * g5Z, -g4Z - (ktZ - lambdatZ) / beta, false);
    AZm0 = gamma * AZm0;
    AZ0p = gslpp::complex(f3Z - beta * g5Z, g4Z + (ktZ - lambdatZ) / beta, false);
    AZ0p = gamma * AZ0p;
    AZ0m = gslpp::complex(f3Z + beta * g5Z, g4Z - (ktZ - lambdatZ) / beta, false);
    AZ0m = gamma * AZ0m;
    AZ00 = gslpp::complex(g1Z + 2.0 * gamma2*kZ, 0.0, false);
 
    //  Collect in matrices and separate LH and RH
    gslpp::matrix<gslpp::complex> AmpZLH(3, 3, 0.0);
    gslpp::matrix<gslpp::complex> AmpZRH(3, 3, 0.0);
 
    AmpZLH.assign(0, 0, AZpp * d1LH(0, 0));
    AmpZLH.assign(0, 1, AZp0 * d1LH(0, 1));
    AmpZLH.assign(0, 2, 0.0);
 
    AmpZLH.assign(1, 0, AZ0p * d1LH(1, 0));
    AmpZLH.assign(1, 1, AZ00 * d1LH(1, 1));
    AmpZLH.assign(1, 2, AZ0m * d1LH(1, 2));
 
    AmpZLH.assign(2, 0, 0.0);
    AmpZLH.assign(2, 1, AZm0 * d1LH(2, 1));
    AmpZLH.assign(2, 2, AZmm * d1LH(2, 2));
 
    AmpZLH = AmpZLH * beta * s / (s - Mz * Mz);
 
    //  Add the correct Zff coupling
    AmpZLH = AmpZLH * gLe / sW2_tree;
 
    AmpZRH.assign(0, 0, AZpp * d1RH(0, 0));
    AmpZRH.assign(0, 1, AZp0 * d1RH(0, 1));
    AmpZRH.assign(0, 2, 0.0);
 
    AmpZRH.assign(1, 0, AZ0p * d1RH(1, 0));
    AmpZRH.assign(1, 1, AZ00 * d1RH(1, 1));
    AmpZRH.assign(1, 2, AZ0m * d1RH(1, 2));
 
    AmpZRH.assign(2, 0, 0.0);
    AmpZRH.assign(2, 1, AZm0 * d1RH(2, 1));
    AmpZRH.assign(2, 2, AZmm * d1RH(2, 2));
 
    AmpZRH = AmpZRH * beta * s / (s - Mz * Mz);
 
    //  Add the correct Zff coupling    
    AmpZRH = AmpZRH * gRe / sW2_tree;
 
    //  J=1 Subamplitudes: gamma
    gslpp::complex Agapp, Agamm, Agap0, Agam0, Aga0p, Aga0m, Aga00;
 
    Agapp = gslpp::complex(g1ga + 2.0 * gamma2* lambdaga, (ktga + lambdatga - 2.0 * lambdatga) / beta, false);
    Agamm = gslpp::complex(g1ga + 2.0 * gamma2* lambdaga, -(ktga + lambdatga - 2.0 * lambdatga) / beta, false);
    Agap0 = gslpp::complex(f3ga + beta * g5ga, -g4ga + (ktga - lambdatga) / beta, false);
    Agap0 = gamma * Agap0;
    Agam0 = gslpp::complex(f3ga - beta * g5ga, -g4ga - (ktga - lambdatga) / beta, false);
    Agam0 = gamma * Agam0;
    Aga0p = gslpp::complex(f3ga - beta * g5ga, g4ga + (ktga - lambdatga) / beta, false);
    Aga0p = gamma * Aga0p;
    Aga0m = gslpp::complex(f3ga + beta * g5ga, g4ga - (ktga - lambdatga) / beta, false);
    Aga0m = gamma * Aga0m;
    Aga00 = gslpp::complex(g1ga + 2.0 * gamma2*kga, 0.0, false);
 
    //  Collect in matrices. Here LH = RH, except for the Wigner functions  
    gslpp::matrix<gslpp::complex> AmpgaLH(3, 3, 0.0);
    gslpp::matrix<gslpp::complex> AmpgaRH(3, 3, 0.0);
 
    AmpgaLH.assign(0, 0, Agapp * d1LH(0, 0));
    AmpgaLH.assign(0, 1, Agap0 * d1LH(0, 1));
    AmpgaLH.assign(0, 2, 0.0);
 
    AmpgaLH.assign(1, 0, Aga0p * d1LH(1, 0));
    AmpgaLH.assign(1, 1, Aga00 * d1LH(1, 1));
    AmpgaLH.assign(1, 2, Aga0m * d1LH(1, 2));
 
    AmpgaLH.assign(2, 0, 0.0);
    AmpgaLH.assign(2, 1, Agam0 * d1LH(2, 1));
    AmpgaLH.assign(2, 2, Agamm * d1LH(2, 2));
 
    AmpgaRH.assign(0, 0, Agapp * d1RH(0, 0));
    AmpgaRH.assign(0, 1, Agap0 * d1RH(0, 1));
    AmpgaRH.assign(0, 2, 0.0);
 
    AmpgaRH.assign(1, 0, Aga0p * d1RH(1, 0));
    AmpgaRH.assign(1, 1, Aga00 * d1RH(1, 1));
    AmpgaRH.assign(1, 2, Aga0m * d1RH(1, 2));
 
    AmpgaRH.assign(2, 0, 0.0);
    AmpgaRH.assign(2, 1, Agam0 * d1RH(2, 1));
    AmpgaRH.assign(2, 2, Agamm * d1RH(2, 2));
 
    AmpgaLH = -beta * AmpgaLH;
    AmpgaRH = -beta * AmpgaRH;
 
    //  J=1 Subamplitudes: neutrino
    gslpp::complex Bpp, Bmm, Bp0, Bm0, B0p, B0m, B00;
    gslpp::complex Cpp, Cmm, Cp0, Cm0, C0p, C0m, C00;
 
    Bpp = gslpp::complex(1.0, 0.0, false);
    Bmm = Bpp;
    Bp0 = gslpp::complex(2.0 * gamma, 0.0, false);
    Bm0 = Bp0;
    B0p = Bp0;
    B0m = Bp0;
    B00 = gslpp::complex(2.0 * gamma2, 0.0, false);
 
    Cpp = gslpp::complex(1.0 / gamma2, 0.0, false);
    Cmm = Cpp;
    Cp0 = gslpp::complex(2.0 * (1.0 + beta) / gamma, 0.0, false);
    Cm0 = gslpp::complex(2.0 * (1.0 - beta) / gamma, 0.0, false);
    C0p = Cm0;
    C0m = Cp0;
    C00 = gslpp::complex(2.0 / gamma2, 0.0, false);
 
    //  Collect in matrices. Here LH = RH    
    gslpp::matrix<gslpp::complex> Bnu(3, 3, 0.0);
    gslpp::matrix<gslpp::complex> Cnu(3, 3, 0.0);
 
    Bnu.assign(0, 0, Bpp * d1LH(0, 0));
    Bnu.assign(0, 1, Bp0 * d1LH(0, 1));
    Bnu.assign(0, 2, 0.0);
 
    Bnu.assign(1, 0, B0p * d1LH(1, 0));
    Bnu.assign(1, 1, B00 * d1LH(1, 1));
    Bnu.assign(1, 2, B0m * d1LH(1, 2));
 
    Bnu.assign(2, 0, 0.0);
    Bnu.assign(2, 1, Bm0 * d1LH(2, 1));
    Bnu.assign(2, 2, Bmm * d1LH(2, 2));
 
    Cnu.assign(0, 0, Cpp * d1LH(0, 0));
    Cnu.assign(0, 1, Cp0 * d1LH(0, 1));
    Cnu.assign(0, 2, 0.0);
 
    Cnu.assign(1, 0, C0p * d1LH(1, 0));
    Cnu.assign(1, 1, C00 * d1LH(1, 1));
    Cnu.assign(1, 2, C0m * d1LH(1, 2));
 
    Cnu.assign(2, 0, 0.0);
    Cnu.assign(2, 1, Cm0 * d1LH(2, 1));
    Cnu.assign(2, 2, Cmm * d1LH(2, 2));
 
    //  The matrix with the total J=1 neutrino amplitude (only LH neutrinos)  
    gslpp::matrix<gslpp::complex> Ampnu1(3, 3, 0.0);
 
    Ampnu1 = Bnu - Cnu / (1.0 + beta * beta - 2.0 * beta * cos);
 
    Ampnu1 = Uenu * Uenu.conjugate() * Ampnu1 / (2.0 * beta * sW2_tree);
 
    gslpp::matrix<gslpp::complex> Ampnu2(3, 3, 0.0);
 
    Ampnu2.assign(0, 2, (1.0 - cos) / 2.0);
    Ampnu2.assign(1, 1, 0.0);
    Ampnu2.assign(2, 0, -(1.0 + cos) / 2.0);
 
    Ampnu2 = (2.0 * eeMz2 / sW2_tree) * Uenu * Uenu.conjugate() * Ampnu2 * sin / (1.0 + beta * beta - 2.0 * beta * cos);
 
    //  Total amplitudes 
    gslpp::matrix<gslpp::complex> MRH(3, 3, 0.0);
    gslpp::matrix<gslpp::complex> MLH(3, 3, 0.0);
 
    MRH = sqrt(2.0) * eeMz2 * (AmpZRH + AmpgaRH);
    MLH = -sqrt(2.0) * eeMz2 * (AmpZLH + AmpgaLH + Ampnu1) + Ampnu2;
 
    //  Total amplitude squared and differential cross section (in pb)
    gslpp::matrix<double> M2(3, 3, 0.0);
    double dxsdcos;
 
    dxsdcos = 0.0;
 
    for (int i = 0; i < 3; i++) {
        for (int j = 0; j < 3; j++) {
            M2.assign(i, j, (MRH(i, j)* (MRH(i, j).conjugate())
                    + MLH(i, j)* (MLH(i, j).conjugate())).real());
 
            dxsdcos = dxsdcos + M2(i, j);
        }
    }
 
    //  Differential cross section in pb
    dxsdcos = (topb * beta / 32.0 / M_PI / s) * dxsdcos;
 
    return dxsdcos;
}

◆ dxseeWWdcosBin()

const double NPSMEFTd6General::dxseeWWdcosBin	(	const double	sqrt_s,
		const double	cos1,
		const double	cos2
	)		const

virtual

The integral of differential distribution for $e^+ e^- \to W^+ W^- \to jj \ell \nu$, with $\ell= e, \mu$ in a given bin of the $W$ polar angle.

Returns: $\int_{\cos{\theta_1}}^{\cos{\theta_2}} d\sigma/d\cos{\theta}$

Reimplemented from NPbase.

Definition at line 38746 of file NPSMEFTd6General.cpp.

                                                                                                             {
    double xsWWbin; // *< Gsl integral variable 
    double errWW; // *< Gsl integral variable 
 
    gsl_function FR; // *< Gsl integral variable 
 
    FR = convertToGslFunction(bind(&NPSMEFTd6General::dxseeWWdcos, &(*this), sqrt_s, _1));
 
    gsl_integration_cquad(&FR, cos1, cos2, 1.e-5, 1.e-4, w_WW, &xsWWbin, &errWW, NULL);
 
    //  Simple integration for testing
    //    double cosx;
 
    //    xsWWbin = 0.0;
 
    //    for (int i=1; i<100; i++){
    //        cosx = cos1 +  i*(cos2-cos1)/100;
    //        xsWWbin = xsWWbin + dxseeWWdcos(sqrt_s, cosx);
    //    }
 
    //    xsWWbin = xsWWbin + 0.5 * (dxseeWWdcos(sqrt_s, cos1) + dxseeWWdcos(sqrt_s, cos2));
 
    //    xsWWbin = xsWWbin * (cos2-cos1)/100;
 
    //  Compute the BR into e nu, mu nu for one W and into jets for the other
    double BRlv, BRjj;
 
    BRlv = GammaW(leptons[NEUTRINO_1], leptons[ELECTRON]) +
            GammaW(leptons[NEUTRINO_2], leptons[MU]) +
            GammaW(leptons[NEUTRINO_3], leptons[TAU]);
 
    BRjj = GammaW() - BRlv;
 
    BRlv = BRlv - GammaW(leptons[NEUTRINO_3], leptons[TAU]);
 
    BRlv = BRlv / GammaW();
 
    BRjj = BRjj / GammaW();
 
 
 
    return xsWWbin * BRlv * BRjj;
}

◆ Gamma_Z()

const double NPSMEFTd6General::Gamma_Z ( ) const

virtual

The total decay width of the $Z$ boson, $\Gamma_Z$.

\[ \Gamma_Z = \Gamma_Z^{SM} + \Delta \Gamma_Z^{(1)} + \Delta \Gamma_Z^{(2)} \]

Returns: $\Gamma_Z$ in GeV, including SM plus $\mathcal{O}(\Lambda^{-2})$ and $\mathcal{O}(\Lambda^{-4})$ NP contributions

Attention: This function is applicable only to the NP model classes that are inherited from NPbase.

Reimplemented from NPbase.

Definition at line 16133 of file NPSMEFTd6General.cpp.

{
    return (trueSM.Gamma_Z() + deltaGamma_Z());
}

◆ Gamma_Zf()

const double NPSMEFTd6General::Gamma_Zf ( const Particle f ) const

virtual

The decay width of the $Z$ boson into a given fermion pair, $\Gamma_Z^{f}$.

\[ \Gamma_Z^{f} = \Gamma_{Z,f}^{SM} + \Delta \Gamma_{Z,f}^{(1)} + \Delta \Gamma_{Z,f}^{(2)} \]

Parameters

[in] f a lepton or quark

Returns: $\Gamma_Z^{f}$ in GeV, including SM plus $\mathcal{O}(\Lambda^{-2})$ and $\mathcal{O}(\Lambda^{-4})$ NP contributions

Attention: This function is applicable only to the NP model classes that are inherited from NPbase.

Reimplemented from NPbase.

Definition at line 16036 of file NPSMEFTd6General.cpp.

{
    return (trueSM.GammaZ(f) + deltaGamma_Zf(f));
}

◆ GammaH2d2dRatio()

const double NPSMEFTd6General::GammaH2d2dRatio ( ) const

The ratio of the $\Gamma(H\to 2d2d)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2d2d)$/ $\Gamma(H\to 2d2d)_{\mathrm{SM}}$

Definition at line 30170 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2d2dRatio1
    double width = 1.0;
 
    width += deltaGammaH2d2dRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2d2dRatio2();
    }
 
    return width;
}

◆ GammaH2e2muRatio()

const double NPSMEFTd6General::GammaH2e2muRatio ( ) const

The ratio of the $\Gamma(H\to 2e 2\mu)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2e 2\mu)$/ $\Gamma(H\to 2e 2\mu)_{\mathrm{SM}}$

Definition at line 29116 of file NPSMEFTd6General.cpp.

                                                      {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2e2muRatio1
    double width = 1.0;
 
    width += deltaGammaH2e2muRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2e2muRatio2();
    }
 
    return width;
}

◆ GammaH2e2vRatio()

const double NPSMEFTd6General::GammaH2e2vRatio ( ) const

The ratio of the $\Gamma(H\to 2e2v)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2e2v)$/ $\Gamma(H\to 2e2v)_{\mathrm{SM}}$

Definition at line 29750 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2e2vRatio1
    double width = 1.0;
 
    width += deltaGammaH2e2vRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2e2vRatio2();
    }
 
    return width;
}

◆ GammaH2evRatio()

const double NPSMEFTd6General::GammaH2evRatio ( ) const

The ratio of the $\Gamma(H\to 2ev)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2ev)$/ $\Gamma(H\to 2ev)_{\mathrm{SM}}$

Definition at line 34293 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2evRatio1
    double width = 1.0;
 
    width += deltaGammaH2evRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2evRatio2();
    }
 
    return width;
}

◆ GammaH2L2dRatio()

const double NPSMEFTd6General::GammaH2L2dRatio ( ) const

The ratio of the $\Gamma(H\to 2L2d)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2L2d)$/ $\Gamma(H\to 2L2d)_{\mathrm{SM}}$

Definition at line 31046 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2L2dRatio1
    double width = 1.0;
 
    width += deltaGammaH2L2dRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2L2dRatio2();
    }
 
    return width;
}

◆ GammaH2L2LRatio()

const double NPSMEFTd6General::GammaH2L2LRatio ( ) const

The ratio of the $\Gamma(H\to 2L2L')$ ( $L,L'=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2L2L')$/ $\Gamma(H\to 2L2L')_{\mathrm{SM}}$

Definition at line 28863 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2L2LRatio1
    double width = 1.0;
 
    width += deltaGammaH2L2LRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2L2LRatio2();
    }
 
    return width;
}

◆ GammaH2L2uRatio()

const double NPSMEFTd6General::GammaH2L2uRatio ( ) const

The ratio of the $\Gamma(H\to 2L2u)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2L2u)$/ $\Gamma(H\to 2L2u)_{\mathrm{SM}}$

Definition at line 30735 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2L2uRatio1
    double width = 1.0;
 
    width += deltaGammaH2L2uRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2L2uRatio2();
    }
 
    return width;
}

◆ GammaH2L2v2Ratio()

const double NPSMEFTd6General::GammaH2L2v2Ratio ( ) const

The ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2L2v)$/ $\Gamma(H\to 2L2v)_{\mathrm{SM}}$

Definition at line 29655 of file NPSMEFTd6General.cpp.

                                                      {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2L2v2Ratio1
    double width = 1.0;
 
    width += deltaGammaH2L2v2Ratio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2L2v2Ratio2();
    }
 
    return width;
}

◆ GammaH2L2vRatio()

const double NPSMEFTd6General::GammaH2L2vRatio ( ) const

The ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2L2v)$/ $\Gamma(H\to 2L2v)_{\mathrm{SM}}$

Definition at line 29413 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2L2vRatio1
    double width = 1.0;
 
    width += deltaGammaH2L2vRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2L2vRatio2();
    }
 
    return width;
}

◆ GammaH2l2vRatio()

const double NPSMEFTd6General::GammaH2l2vRatio ( ) const

The ratio of the $\Gamma(H\to 2l2v)$ ( $l=e,\mu$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2l2v)$/ $\Gamma(H\to 2l2v)_{\mathrm{SM}}$

Definition at line 34818 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2l2vRatio1
    double width = 1.0;
 
    width += deltaGammaH2l2vRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2l2vRatio2();
    }
 
    return width;
}

◆ GammaH2Lv2Ratio()

const double NPSMEFTd6General::GammaH2Lv2Ratio ( ) const

The ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2Lv)$/ $\Gamma(H\to 2Lv)_{\mathrm{SM}}$

Definition at line 34194 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2Lv2Ratio1
    double width = 1.0;
 
    width += deltaGammaH2Lv2Ratio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2Lv2Ratio2();
    }
 
    return width;
}

◆ GammaH2LvRatio()

const double NPSMEFTd6General::GammaH2LvRatio ( ) const

The ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2Lv)$/ $\Gamma(H\to 2Lv)_{\mathrm{SM}}$

Definition at line 33992 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2LvRatio1
    double width = 1.0;
 
    width += deltaGammaH2LvRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2LvRatio2();
    }
 
    return width;
}

◆ GammaH2mu2vRatio()

const double NPSMEFTd6General::GammaH2mu2vRatio ( ) const

The ratio of the $\Gamma(H\to 2\mu 2v)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2\mu 2v)$/ $\Gamma(H\to 2\mu 2v)_{\mathrm{SM}}$

Definition at line 29843 of file NPSMEFTd6General.cpp.

                                                      {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2mu2vRatio1
    double width = 1.0;
 
    width += deltaGammaH2mu2vRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2mu2vRatio2();
    }
 
    return width;
}

◆ GammaH2muvRatio()

const double NPSMEFTd6General::GammaH2muvRatio ( ) const

The ratio of the $\Gamma(H\to 2\mu v)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2\mu v)$/ $\Gamma(H\to 2\mu v)_{\mathrm{SM}}$

Definition at line 34388 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2muvRatio1
    double width = 1.0;
 
    width += deltaGammaH2muvRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2muvRatio2();
    }
 
    return width;
}

◆ GammaH2u2dRatio()

const double NPSMEFTd6General::GammaH2u2dRatio ( ) const

The ratio of the $\Gamma(H\to 2u2d)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2u2d)$/ $\Gamma(H\to 2u2d)_{\mathrm{SM}}$

Definition at line 30440 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2u2dRatio1
    double width = 1.0;
 
    width += deltaGammaH2u2dRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2u2dRatio2();
    }
 
    return width;
}

◆ GammaH2u2uRatio()

const double NPSMEFTd6General::GammaH2u2uRatio ( ) const

The ratio of the $\Gamma(H\to 2u2u)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2u2u)$/ $\Gamma(H\to 2u2u)_{\mathrm{SM}}$

Definition at line 29935 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2u2uRatio1
    double width = 1.0;
 
    width += deltaGammaH2u2uRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2u2uRatio2();
    }
 
    return width;
}

◆ GammaH2udRatio()

const double NPSMEFTd6General::GammaH2udRatio ( ) const

The ratio of the $\Gamma(H\to 2ud)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2ud)$/ $\Gamma(H\to 2ud)_{\mathrm{SM}}$

Definition at line 33763 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2udRatio1
    double width = 1.0;
 
    width += deltaGammaH2udRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2udRatio2();
    }
 
    return width;
}

◆ GammaH2v2dRatio()

const double NPSMEFTd6General::GammaH2v2dRatio ( ) const

The ratio of the $\Gamma(H\to 2v2d)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2v2d)$/ $\Gamma(H\to 2v2d)_{\mathrm{SM}}$

Definition at line 31657 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2v2dRatio1
    double width = 1.0;
 
    width += deltaGammaH2v2dRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2v2dRatio2();
    }
 
    return width;
}

◆ GammaH2v2uRatio()

const double NPSMEFTd6General::GammaH2v2uRatio ( ) const

The ratio of the $\Gamma(H\to 2v2u)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2v2u)$/ $\Gamma(H\to 2v2u)_{\mathrm{SM}}$

Definition at line 31390 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2v2uRatio1
    double width = 1.0;
 
    width += deltaGammaH2v2uRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2v2uRatio2();
    }
 
    return width;
}

◆ GammaH2v2vRatio()

const double NPSMEFTd6General::GammaH2v2vRatio ( ) const

The ratio of the $\Gamma(H\to 2v2v)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 2v2v)$/ $\Gamma(H\to 2v2v)_{\mathrm{SM}}$

Definition at line 29209 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH2v2vRatio1
    double width = 1.0;
 
    width += deltaGammaH2v2vRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH2v2vRatio2();
    }
 
    return width;
}

◆ GammaH4dRatio()

const double NPSMEFTd6General::GammaH4dRatio ( ) const

The ratio of the $\Gamma(H\to 4d)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 4d)$/ $\Gamma(H\to 4d)_{\mathrm{SM}}$

Definition at line 32927 of file NPSMEFTd6General.cpp.

                                                   {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH4dRatio1
    double width = 1.0;
 
    width += deltaGammaH4dRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH4dRatio2();
    }
 
    return width;
}

◆ GammaH4eRatio()

const double NPSMEFTd6General::GammaH4eRatio ( ) const

The ratio of the $\Gamma(H\to 4e)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 4e)$/ $\Gamma(H\to 4e)_{\mathrm{SM}}$

Definition at line 32297 of file NPSMEFTd6General.cpp.

                                                   {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH4eRatio1
    double width = 1.0;
 
    width += deltaGammaH4eRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH4eRatio2();
    }
 
    return width;
}

◆ GammaH4fCCRatio()

const double NPSMEFTd6General::GammaH4fCCRatio ( ) const

The ratio of the $\Gamma(H\to 4f)$ via CC in the current model and in the Standard Model.

Returns: $\Gamma(H\to 4f, CC)$/ $\Gamma(H\to 4f, CC)_{\mathrm{SM}}$

Definition at line 34680 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH4fCCRatio1
    double width = 1.0;
 
    width += deltaGammaH4fCCRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH4fCCRatio2();
    }
 
    return width;
}

◆ GammaH4fNCRatio()

const double NPSMEFTd6General::GammaH4fNCRatio ( ) const

The ratio of the $\Gamma(H\to 4f)$ via NC in the current model and in the Standard Model.

Returns: $\Gamma(H\to 4f, NC)$/ $\Gamma(H\to 4f, NC)_{\mathrm{SM}}$

Definition at line 34591 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH4fNCRatio1
    double width = 1.0;
 
    width += deltaGammaH4fNCRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH4fNCRatio2();
    }
 
    return width;
}

◆ GammaH4fRatio()

const double NPSMEFTd6General::GammaH4fRatio ( ) const

The ratio of the $\Gamma(H\to 4f)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 4f)$/ $\Gamma(H\to 4f)_{\mathrm{SM}}$

Definition at line 34483 of file NPSMEFTd6General.cpp.

                                                   {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH4fRatio1
    double width = 1.0;
 
    width += deltaGammaH4fRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH4fRatio2();
    }
 
    return width;
}

◆ GammaH4L2Ratio()

const double NPSMEFTd6General::GammaH4L2Ratio ( ) const

The ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to 4L)$/ $\Gamma(H\to 4L)_{\mathrm{SM}}$

Definition at line 32204 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH4L2Ratio1
    double width = 1.0;
 
    width += deltaGammaH4L2Ratio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH4L2Ratio2();
    }
 
    return width;
}

◆ GammaH4LRatio()

const double NPSMEFTd6General::GammaH4LRatio ( ) const

The ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to 4L)$/ $\Gamma(H\to 4L)_{\mathrm{SM}}$

Definition at line 31963 of file NPSMEFTd6General.cpp.

                                                   {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH4LRatio1
    double width = 1.0;
 
    width += deltaGammaH4LRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH4LRatio2();
    }
 
    return width;
}

◆ GammaH4lRatio()

const double NPSMEFTd6General::GammaH4lRatio ( ) const

The ratio of the $\Gamma(H\to 4l)$ ( $l=e,\mu$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to 4l)$/ $\Gamma(H\to 4l)_{\mathrm{SM}}$

Definition at line 34755 of file NPSMEFTd6General.cpp.

                                                   {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH4lRatio1
    double width = 1.0;
 
    width += deltaGammaH4lRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH4lRatio2();
    }
 
    return width;
}

◆ GammaH4muRatio()

const double NPSMEFTd6General::GammaH4muRatio ( ) const

The ratio of the $\Gamma(H\to 4\mu)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 4\mu)$/ $\Gamma(H\to 4\mu)_{\mathrm{SM}}$

Definition at line 32387 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH4muRatio1
    double width = 1.0;
 
    width += deltaGammaH4muRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH4muRatio2();
    }
 
    return width;
}

◆ GammaH4uRatio()

const double NPSMEFTd6General::GammaH4uRatio ( ) const

The ratio of the $\Gamma(H\to 4u)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 4u)$/ $\Gamma(H\to 4u)_{\mathrm{SM}}$

Definition at line 32679 of file NPSMEFTd6General.cpp.

                                                   {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH4uRatio1
    double width = 1.0;
 
    width += deltaGammaH4uRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH4uRatio2();
    }
 
    return width;
}

◆ GammaH4vRatio()

const double NPSMEFTd6General::GammaH4vRatio ( ) const

The ratio of the $\Gamma(H\to 4v)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to 4v)$/ $\Gamma(H\to 4v)_{\mathrm{SM}}$

Definition at line 32477 of file NPSMEFTd6General.cpp.

                                                   {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaH4vRatio1
    double width = 1.0;
 
    width += deltaGammaH4vRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaH4vRatio2();
    }
 
    return width;
}

◆ GammaHbbRatio()

const double NPSMEFTd6General::GammaHbbRatio ( ) const

virtual

The ratio of the $\Gamma(H\to bb)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to bb)$/ $\Gamma(H\to bb)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28764 of file NPSMEFTd6General.cpp.

                                                   {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHbbRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHbbRatio2();
    }
 
    return width;
}

◆ GammaHccRatio()

const double NPSMEFTd6General::GammaHccRatio ( ) const

virtual

The ratio of the $\Gamma(H\to cc)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to cc)$/ $\Gamma(H\to cc)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28562 of file NPSMEFTd6General.cpp.

                                                   {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHccRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHccRatio2();
    }
 
    return width;
 
}

◆ GammaHevmuvRatio()

const double NPSMEFTd6General::GammaHevmuvRatio ( ) const

The ratio of the $\Gamma(H\to e\nu \mu\nu)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to e\nu \mu\nu)$/ $\Gamma(H\to e\nu \mu\nu)_{\mathrm{SM}}$

Definition at line 33350 of file NPSMEFTd6General.cpp.

                                                      {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHevmuvRatio1
    double width = 1.0;
 
    width += deltaGammaHevmuvRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHevmuvRatio2();
    }
 
    return width;
}

◆ GammaHgagaRatio()

const double NPSMEFTd6General::GammaHgagaRatio ( ) const

virtual

The ratio of the $\Gamma(H\to \gamma\gamma)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to \gamma\gamma)$/ $\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28120 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHgagaRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHgagaRatio2();
    }
 
    return width;
 
}

◆ GammaHggRatio()

const double NPSMEFTd6General::GammaHggRatio ( ) const

virtual

The ratio of the $\Gamma(H\to gg)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to gg)$/ $\Gamma(H\to gg)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 25971 of file NPSMEFTd6General.cpp.

                                                   {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHggRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHggRatio2();
    }
 
    return width;
 
}

◆ GammaHll_vvorjjRatio()

const double NPSMEFTd6General::GammaHll_vvorjjRatio ( ) const

The ratio of the $\Gamma(H\to l l \nu\nu, l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to l l \nu\nu, l l j j)$/ $\Gamma(H\to l l \nu\nu, l l j j)_{\mathrm{SM}}$

Definition at line 35137 of file NPSMEFTd6General.cpp.

                                                          {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHll_vvorjjRatio1
    double width = 1.0;
 
    width += deltaGammaHll_vvorjjRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHll_vvorjjRatio2();
    }
 
    return width;
}

◆ GammaHlv_lvorjjRatio()

const double NPSMEFTd6General::GammaHlv_lvorjjRatio ( ) const

The ratio of the $\Gamma(H\to l \nu l \nu, l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to l \nu l \nu, l \nu j j)$/ $\Gamma(H\to l \nu l \nu, l \nu j j)_{\mathrm{SM}}$

Definition at line 35074 of file NPSMEFTd6General.cpp.

                                                          {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHlv_lvorjjRatio1
    double width = 1.0;
 
    width += deltaGammaHlv_lvorjjRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHlv_lvorjjRatio2();
    }
 
    return width;
}

◆ GammaHlvjjRatio()

const double NPSMEFTd6General::GammaHlvjjRatio ( ) const

The ratio of the $\Gamma(H\to l l j j)$ ( $l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. @return $\Gamma(H\to l l j j) $/$\Gamma(H\to l l j j)_{\mathrm{SM}} $ */ const double GammaHlljjRatio() const; /** @brief The new physics contribution to the ratio of the $\Gamma(H\to l l j j) $ ($l=e,\mu,~~j\not=b $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) @return $\delta \Gamma(H\to l l j j) $/$\Gamma(H\to l l j j)_{\mathrm{SM}} $ */ const double deltaGammaHlljjRatio1() const; /** @brief The new physics contribution to the ratio of the $\Gamma(H\to l l j j) $ ($l=e,\mu,~~j\not=b $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) @return $\delta \Gamma(H\to l l j j) $/$\Gamma(H\to l l j j)_{\mathrm{SM}} $ */ const double deltaGammaHlljjRatio2() const; /** @brief The ratio of the Br$(H\to l l j j) $ ($l=e,\mu,~~j\not=b $) in the current model and in the Standard Model. @return Br$(H\to l l j j) $/Br$(H\to l l j j)_{\mathrm{SM}} $ */ virtual const double BrHlljjRatio() const; /** @brief The ratio of the $\Gamma(H\to l \nu j j) $ ($l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to l \nu j j)$/ $\Gamma(H\to l \nu j j)_{\mathrm{SM}}$

Definition at line 34983 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHlvjjRatio1
    double width = 1.0;
 
    width += deltaGammaHlvjjRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHlvjjRatio2();
    }
 
    return width;
}

◆ GammaHLvudRatio()

const double NPSMEFTd6General::GammaHLvudRatio ( ) const

The ratio of the $\Gamma(H\to Lvud)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to Lvud)$/ $\Gamma(H\to Lvud)_{\mathrm{SM}}$

Definition at line 33596 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHLvudRatio1
    double width = 1.0;
 
    width += deltaGammaHLvudRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHLvudRatio2();
    }
 
    return width;
}

◆ GammaHLvvLRatio()

const double NPSMEFTd6General::GammaHLvvLRatio ( ) const

The ratio of the $\Gamma(H\to LvvL)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model.

Returns: $\Gamma(H\to LvvL)$/ $\Gamma(H\to LvvL)_{\mathrm{SM}}$

Definition at line 33206 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHLvvLRatio1
    double width = 1.0;
 
    width += deltaGammaHLvvLRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHLvvLRatio2();
    }
 
    return width;
}

◆ GammaHmumuRatio()

const double NPSMEFTd6General::GammaHmumuRatio ( ) const

virtual

The ratio of the $\Gamma(H\to \mu\mu)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to \mu\mu)$/ $\Gamma(H\to \mu\mu)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28388 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHmumuRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHmumuRatio2();
    }
 
    return width;
 
}

◆ GammaHssRatio()

const double NPSMEFTd6General::GammaHssRatio ( ) const

virtual

The ratio of the $\Gamma(H\to ss)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to ss)$/ $\Gamma(H\to ss)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28665 of file NPSMEFTd6General.cpp.

                                                   {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHssRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHssRatio2();
    }
 
    return width;
 
}

◆ GammaHtautauRatio()

const double NPSMEFTd6General::GammaHtautauRatio ( ) const

virtual

The ratio of the $\Gamma(H\to \tau\tau)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to \tau\tau)$/ $\Gamma(H\to \tau\tau)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 28475 of file NPSMEFTd6General.cpp.

                                                       {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHtautauRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHtautauRatio2();
    }
 
    return width;
 
}

◆ GammaHudduRatio()

const double NPSMEFTd6General::GammaHudduRatio ( ) const

The ratio of the $\Gamma(H\to uddu)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to uddu)$/ $\Gamma(H\to uddu)_{\mathrm{SM}}$

Definition at line 33441 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHudduRatio1
    double width = 1.0;
 
    width += deltaGammaHudduRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHudduRatio2();
    }
 
    return width;
}

◆ GammaHWffRatio()

const double NPSMEFTd6General::GammaHWffRatio ( ) const

The ratio of the $\Gamma(H\to W f f)$, with $f$ any fermion, in the current model and in the Standard Model.

Returns: $\Gamma(H\to W f f)$/ $\Gamma(H\to W f f)_{\mathrm{SM}}$

Definition at line 26461 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHWffRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHWffRatio2();
    }
 
    return width;
 
}

◆ GammaHWjjRatio()

const double NPSMEFTd6General::GammaHWjjRatio ( ) const

The ratio of the $\Gamma(H\to W j j)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to W j j)$/ $\Gamma(H\to W j j)_{\mathrm{SM}}$

Definition at line 26303 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHWjjRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHWjjRatio2();
    }
 
    return width;
 
}

◆ GammaHWlvRatio()

const double NPSMEFTd6General::GammaHWlvRatio ( ) const

The ratio of the $\Gamma(H\to W l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model.

Returns: $\Gamma(H\to Wl\nu)$/ $\Gamma(H\to Wl\nu)_{\mathrm{SM}}$

Definition at line 26144 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHWlvRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHWlvRatio2();
    }
 
    return width;
 
}

◆ GammaHWW2l2vRatio()

const double NPSMEFTd6General::GammaHWW2l2vRatio ( ) const

The ratio of the $\Gamma(H\to WW^*\to l\nu l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model.

Returns: $\Gamma(H\to WW^*\to l\nu l\nu)$/ $\Gamma(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}$

Definition at line 26221 of file NPSMEFTd6General.cpp.

                                                       {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHWW2l2vRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHWW2l2vRatio2();
    }
 
    return width;
 
}

◆ GammaHWW4fRatio()

const double NPSMEFTd6General::GammaHWW4fRatio ( ) const

The ratio of the $\Gamma(H\to WW^*\to 4f)$, with $f$ any fermion, in the current model and in the Standard Model.

Returns: $\Gamma(H\to WW^*\to 4f)$/ $\Gamma(H\to WW^*\to 4f)_{\mathrm{SM}}$

Definition at line 26539 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHWW4fRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHWW4fRatio2();
    }
 
    return width;
 
}

◆ GammaHWW4jRatio()

const double NPSMEFTd6General::GammaHWW4jRatio ( ) const

The ratio of the $\Gamma(H\to WW^*\to 4j)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to WW^*\to 4j)$/ $\Gamma(H\to WW^*\to 4j)_{\mathrm{SM}}$

Definition at line 26380 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHWW4jRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHWW4jRatio2();
    }
 
    return width;
 
}

◆ GammaHWWRatio()

const double NPSMEFTd6General::GammaHWWRatio ( ) const

virtual

The ratio of the $\Gamma(H\to WW)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to WW)$/ $\Gamma(H\to WW)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 26093 of file NPSMEFTd6General.cpp.

                                                   {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHWWRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHWWRatio2();
    }
 
    return width;
 
}

◆ GammaHZddRatio()

const double NPSMEFTd6General::GammaHZddRatio ( ) const

The ratio of the $\Gamma(H\to Zd d)$ ( $d=d,s,b $) in the current model and in the Standard Model.

Returns: $\Gamma(H\to Zd d)$/ $\Gamma(H\to Zd d)_{\mathrm{SM}}$

Definition at line 27517 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZddRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZddRatio2();
    }
 
    return width;
 
}

◆ GammaHZeeRatio()

const double NPSMEFTd6General::GammaHZeeRatio ( ) const

The ratio of the $\Gamma(H\to Zee)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to Zee)$/ $\Gamma(H\to Zee)_{\mathrm{SM}}$

Definition at line 26810 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZeeRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZeeRatio2();
    }
 
    return width;
 
}

◆ GammaHZffRatio()

const double NPSMEFTd6General::GammaHZffRatio ( ) const

The ratio of the $\Gamma(H\to Zff)$, with $f$ any fermion, in the current model and in the Standard Model.

Returns: $\Gamma(H\to Zff)$/ $\Gamma(H\to Zff)_{\mathrm{SM}}$

Definition at line 27613 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZffRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZffRatio2();
    }
 
    return width;
 
}

◆ GammaHZgaRatio()

const double NPSMEFTd6General::GammaHZgaRatio ( ) const

virtual

The ratio of the $\Gamma(H\to Z\gamma)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to Z\gamma)$/ $\Gamma(H\to Z\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 27923 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZgaRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZgaRatio2();
    }
 
    return width;
 
}

◆ GammaHZllRatio()

const double NPSMEFTd6General::GammaHZllRatio ( ) const

The ratio of the $\Gamma(H\to Zll)$ ( $l=e,\mu $) in the current model and in the Standard Model.

Returns: $\Gamma(H\to Zll)$/ $\Gamma(H\to Zll)_{\mathrm{SM}}$

Definition at line 26731 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZllRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZllRatio2();
    }
 
    return width;
 
}

◆ GammaHZmumuRatio()

const double NPSMEFTd6General::GammaHZmumuRatio ( ) const

The ratio of the $\Gamma(H\to Z\mu\mu)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to Z\mu\mu)$/ $\Gamma(H\to Z\mu\mu)_{\mathrm{SM}}$

Definition at line 26867 of file NPSMEFTd6General.cpp.

                                                      {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZmumuRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZmumuRatio2();
    }
 
    return width;
 
}

◆ GammaHZuuRatio()

const double NPSMEFTd6General::GammaHZuuRatio ( ) const

The ratio of the $\Gamma(H\to Zu u)$ ( $u=u,c $) in the current model and in the Standard Model.

Returns: $\Gamma(H\to Zu u)$/ $\Gamma(H\to Zu u)_{\mathrm{SM}}$

Definition at line 27424 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZuuRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZuuRatio2();
    }
 
    return width;
 
}

◆ GammaHZvvRatio()

const double NPSMEFTd6General::GammaHZvvRatio ( ) const

The ratio of the $\Gamma(H\to Z\nu\nu)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to Z\nu\nu)$/ $\Gamma(H\to Z\nu\nu)_{\mathrm{SM}}$

Definition at line 27263 of file NPSMEFTd6General.cpp.

                                                    {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZvvRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZvvRatio2();
    }
 
    return width;
 
}

◆ GammaHZZ2e2muRatio()

const double NPSMEFTd6General::GammaHZZ2e2muRatio ( ) const

The ratio of the $\Gamma(H\to ZZ* \to 2e2\mu)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to ZZ* \to 2e2\mu)$/ $\Gamma(H\to ZZ* \to 2e2\mu)_{\mathrm{SM}}$

Definition at line 27097 of file NPSMEFTd6General.cpp.

                                                        {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZZ2e2muRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZZ2e2muRatio2();
    }
 
    return width;
 
}

◆ GammaHZZ4dRatio()

const double NPSMEFTd6General::GammaHZZ4dRatio ( ) const

inline

The ratio of the $\Gamma(H\to ZZ* \to 4 d)$ ( $d=d,s,b $) in the current model and in the Standard Model.

Returns: $\Gamma(H\to ZZ* \to 4 d)$/ $\Gamma(H\to ZZ* \to 4 d)_{\mathrm{SM}}$

Definition at line 2855 of file NPSMEFTd6General.h.

                                          {
        return 1.0;
    };

◆ GammaHZZ4eRatio()

const double NPSMEFTd6General::GammaHZZ4eRatio ( ) const

The ratio of the $\Gamma(H\to ZZ* \to 4e)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to ZZ* \to 4e)$/ $\Gamma(H\to ZZ* \to 4e)_{\mathrm{SM}}$

Definition at line 27014 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZZ4eRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZZ4eRatio2();
    }
 
    return width;
 
}

◆ GammaHZZ4fRatio()

const double NPSMEFTd6General::GammaHZZ4fRatio ( ) const

The ratio of the $\Gamma(H\to ZZ* \to 4f)$, with $f$ any fermion, in the current model and in the Standard Model.

Returns: $\Gamma(H\to ZZ* \to 4f)$/ $\Gamma(H\to ZZ* \to 4f)_{\mathrm{SM}}$

Definition at line 27696 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZZ4fRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZZ4fRatio2();
    }
 
    return width;
 
}

◆ GammaHZZ4lRatio()

const double NPSMEFTd6General::GammaHZZ4lRatio ( ) const

The ratio of the $\Gamma(H\to ZZ* \to 4l)$ ( $l=e,\mu $) in the current model and in the Standard Model.

Returns: $\Gamma(H\to ZZ* \to 4l)$/ $\Gamma(H\to ZZ* \to 4l)_{\mathrm{SM}}$

Definition at line 26924 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZZ4lRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZZ4lRatio2();
    }
 
    return width;
 
}

◆ GammaHZZ4muRatio()

const double NPSMEFTd6General::GammaHZZ4muRatio ( ) const

The ratio of the $\Gamma(H\to ZZ* \to 4\mu)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to ZZ* \to 4\mu)$/ $\Gamma(H\to ZZ* \to 4\mu)_{\mathrm{SM}}$

Definition at line 27180 of file NPSMEFTd6General.cpp.

                                                      {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZZ4muRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZZ4muRatio2();
    }
 
    return width;
 
}

◆ GammaHZZ4uRatio()

const double NPSMEFTd6General::GammaHZZ4uRatio ( ) const

inline

The ratio of the $\Gamma(H\to ZZ* \to 4 u)$ ( $u=u,c $) in the current model and in the Standard Model.

Returns: $\Gamma(H\to ZZ* \to 4u)$/ $\Gamma(H\to ZZ* \to 4u)_{\mathrm{SM}}$

Definition at line 2793 of file NPSMEFTd6General.h.

                                          {
        return 1.0;
    };

◆ GammaHZZ4vRatio()

const double NPSMEFTd6General::GammaHZZ4vRatio ( ) const

The ratio of the $\Gamma(H\to ZZ* \to 4\nu)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to ZZ* \to 4\nu)$/ $\Gamma(H\to ZZ* \to 4\nu)_{\mathrm{SM}}$

Definition at line 27341 of file NPSMEFTd6General.cpp.

                                                     {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZZ4vRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZZ4vRatio2();
    }
 
    return width;
 
}

◆ GammaHZZRatio()

const double NPSMEFTd6General::GammaHZZRatio ( ) const

virtual

The ratio of the $\Gamma(H\to ZZ)$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to ZZ)$/ $\Gamma(H\to ZZ)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 26682 of file NPSMEFTd6General.cpp.

                                                   {
    // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
    double width = 1.0;
 
    width += deltaGammaHZZRatio1();
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        width += deltaGammaHZZRatio2();
    }
 
    return width;
 
}

◆ GammaW() [1/2]

const double NPSMEFTd6General::GammaW ( ) const

virtual

The total width of the $W$ boson, $\Gamma_W$.

Returns: $\Gamma_W$ in GeV

Reimplemented from NPbase.

Definition at line 15754 of file NPSMEFTd6General.cpp.

                                            {
    return ( trueSM.GammaW() + deltaGamma_W());
}

◆ GammaW() [2/2]

const double NPSMEFTd6General::GammaW	(	const Particle	fi,
		const Particle	fj
	)		const

virtual

A partial decay width of the $W$ boson decay into a SM fermion pair.

Parameters

[in]	fi	a lepton or quark
[in]	fj	a lepton or quark

Returns: $\Gamma^W_{ij}$

Reimplemented from NPbase.

Definition at line 15719 of file NPSMEFTd6General.cpp.

                                                                                {
    return ( trueSM.GammaW(fi, fj) + deltaGamma_Wff(fi, fj));
}

◆ GenerateSMInitialConditions()

void NPSMEFTd6General::GenerateSMInitialConditions ( )

Generates the initial condition for the Standard Model parameters.

This method sets all the Standard Model parameters to their values and RG evolves them up to the New Physics scale.

Definition at line 8347 of file NPSMEFTd6General.cpp.

                                                    {
    //    std::cout<<"\033[1;31m Mw_inp = \033[0m "<< Mw_inp << std::endl;
 
    Lambda_NP = ModelParamMap.at("Lambda_NP");
    LambdaNP2 = Lambda_NP * Lambda_NP;
    LambdaNPm2 = 1. / LambdaNP2;
    
    //  1) Post-update operations involving SM parameters only 
 
    v2 = v() * v();
    v2_over_LambdaNP2 = v2 / LambdaNP2;
 
    // SM parameters using tree-level relations, depending on the input scheme
    aleMz = trueSM.alphaMz();
    eeMz = cAsch * sqrt(4.0 * M_PI * aleMz)
            + cWsch * sqrt(4.0 * sqrt(2.0) * GF * Mw_inp * Mw_inp * (1.0 - Mw_inp * Mw_inp / Mz / Mz));
    eeMz2 = eeMz*eeMz;
 
    sW2_tree = cAsch * (0.5 * (1.0 - sqrt(1.0 - eeMz2 / (sqrt(2.0) * GF * Mz * Mz))))
            + cWsch * (1.0 - Mw_inp * Mw_inp / Mz / Mz);
    cW2_tree = 1.0 - sW2_tree;
 
    sW_tree = sqrt(sW2_tree);
    cW_tree = sqrt(cW2_tree);
 
    g1_tree = eeMz / cW_tree;
    g2_tree = eeMz / sW_tree;
    g3_tree = sqrt(4.0 * M_PI * AlsMz);
 
    Mw_tree = cAsch * (Mz * cW_tree)
            + cWsch * Mw_inp;
 
    lambdaH_tree = mHl * mHl / 2.0 / v2;
 
    gZvL = (leptons[NEUTRINO_1].getIsospin());
    gZlL = (leptons[ELECTRON].getIsospin()) - (leptons[ELECTRON].getCharge()) * sW2_tree;
    gZlR = -(leptons[ELECTRON].getCharge()) * sW2_tree;
    gZuL = (quarks[UP].getIsospin()) - (quarks[UP].getCharge()) * sW2_tree;
    gZuR = -(quarks[UP].getCharge()) * sW2_tree;
    gZdL = (quarks[DOWN].getIsospin()) - (quarks[DOWN].getCharge()) * sW2_tree;
    gZdR = -(quarks[DOWN].getCharge()) * sW2_tree;
 
    dZH = -(9.0 / 16.0)*(GF * mHl * mHl / sqrt(2.0) / M_PI / M_PI)*(2.0 * M_PI / 3.0 / sqrt(3.0) - 1.0);
 
    dZH1 = dZH / (1.0 - dZH);
 
    dZH2 = dZH * (1 + 3.0 * dZH) / (1.0 - dZH) / (1.0 - dZH);
 
    //2) Post-update operations involving dimension-6 operators
 
    ChangeToEvolutorsBasisPureSM();
    //ChangeToEvolutorsBasisSMEFTtoSM();
    Mu_LEW[0] = mu_LEW;
    Mu_LEW[1] = mc_LEW;
    Mu_LEW[2] = mt_LEW;
 
    Md_LEW[0] = md_LEW;
    Md_LEW[1] = ms_LEW;
    Md_LEW[2] = mb_LEW;
 
    Me_LEW[0] = me_LEW;
    Me_LEW[1] = mmu_LEW;
    Me_LEW[2] = mtau_LEW;
    
    
    // Renormalization Group Evolution (RGE)
    
    // Logs of the scales used in the evolutors, from top to bottom
    tmu2 = log(500.0/Lambda_NP); 
    tmu3 = log(365.0/Lambda_NP); 
    tmu4 = log(240.0/Lambda_NP);
    tmu5 = log(mHl/Lambda_NP);
    tmuw = log(muw/Lambda_NP);
    
    // SMEFTEvol* setup
    
    if (FlagRGEci) {
 
        // SM initial conditions for RGEsolver SMEFTEvolEW
        SMEFTEvolEW.GenerateSMInitialConditions(muw, Lambda_NP, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
 
        }
    else {
 
        // SM initial conditions for RGEsolver SMEFTEvolEW        
        // Skip RGE by setting the two scales at Lambda_NP for the EFT and to muw for the SM pars
        SMEFTEvolEW.GenerateSMInitialConditions(muw, muw, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
    }
 
    isSMInitialConditionComputed = true;
}

◆ getCG_LNP()

double NPSMEFTd6General::getCG_LNP ( ) const

inline

Return CG_LNP.

Returns: $ CG_LNP $

Definition at line 687 of file NPSMEFTd6General.h.

                             {
        return CG_LNP;
    }

◆ getLambda_NP()

double NPSMEFTd6General::getLambda_NP ( ) const

inline

Return Lambda_NP.

Returns: $ Lambda_NP $

Definition at line 678 of file NPSMEFTd6General.h.

                                {
        return Lambda_NP;
    }

◆ getMatching()

virtual NPSMEFTd6GeneralMatching & NPSMEFTd6General::getMatching ( ) const

inlinevirtual

A method to get the Matching object for this model.

Returns: The matching object for this model

Reimplemented from StandardModel.

Definition at line 668 of file NPSMEFTd6General.h.

                                                          {
        return NPSMEFTd6GM.getObj();
    }

◆ IctW_TWG()

const double NPSMEFTd6General::IctW_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47486 of file NPSMEFTd6General.cpp.

                                                             {
 
    double comb;
    double toTeVm2 = 1000000.; 
 
    // Minus sign because of difference in covariant derivative convention of Top WG    
    comb = - getSMEFTCoeff("CuWI", 2, 2, mu);;
  
    return (toTeVm2 * comb);
}

◆ IctZ_TWG()

const double NPSMEFTd6General::IctZ_TWG ( const double mu ) const

virtual

< To change C/Lambda^2 from GeV to TeV

Definition at line 47508 of file NPSMEFTd6General.cpp.

                                                             {
 
    double comb;
    double toTeVm2 = 1000000.; 
 
    // Minus sign because of difference in covariant derivative convention of Top WG    
    comb = - ( - sW_tree * getSMEFTCoeff("CuBI", 2, 2, mu) + cW_tree * getSMEFTCoeff("CuWI", 2, 2, mu) );
  
    return (toTeVm2 * comb);
}

◆ intDMLL2eus2()

const double NPSMEFTd6General::intDMLL2eus2	(	const double	s,
		const double	t0,
		const double	t1
	)		const

virtual

Definition at line 46713 of file NPSMEFTd6General.cpp.

                                                                                                  {
    
    double intM2;
    double aEM, sw2cw2;
    double gLeSM;
    double deltagLe;
    double Aeeee;
    double GammaZSM, deltaGammaZ;
    double Mz2, Mz4, s2;
    // RG scale of the process
    double muRG;
    
    muRG = sqrt(s);
    
    aEM = trueSM.alphaMz();
    sw2cw2 = sW2_tree * cW2_tree;
    Aeeee = CeeLL_e(muRG);
    gLeSM = gZlL;
    deltagLe = deltaGL_f_mu(leptons[ELECTRON], muRG);
    GammaZSM = trueSM.Gamma_Z();
    deltaGammaZ = deltaGamma_Z();
    Mz2 = Mz * Mz;
    Mz4 = Mz2 * Mz2;
    s2 = s * s;
 
    intM2 = (1.0/(3.0*s2))*((2.0*gLeSM*gLeSM*gLeSM*Mz2*s2*GammaZSM*(gLeSM*(Mz4 + s2 - Mz2*(2.0*s + GammaZSM*GammaZSM))*deltaGammaZ + 2.0*GammaZSM*(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM))*deltagLe))/(sw2cw2*sw2cw2 * pow(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM),3.0)) + 
            2.0*(1.0 - (gLeSM*gLeSM*(Mz2 - s)*s)/(sw2cw2*((Mz2 - s)*(Mz2 - s) + Mz2*GammaZSM*GammaZSM)))*(delta_em + (s*Aeeee)/(2.0*M_PI*aEM) + (2.0*gLeSM*(Mz2 - s)*s*(gLeSM*Mz2*GammaZSM*deltaGammaZ - (Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM))*deltagLe))/(sw2cw2*pow(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM),2.0))))*(pow(s + t1 ,3.0) - pow(s + t0,3.0)) +
            ((2.0*delta_em + (4.0*gLeSM*gLeSM*Mz2*(Mz2 - s)*s*GammaZSM*deltaGammaZ)/(sw2cw2*pow(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM),2.0)) + (s*Aeeee)/(M_PI*aEM) - (4.0*gLeSM*(Mz2 - s)*s*deltagLe)/(sw2cw2*(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM))))/s)*(2*s*( t1 - t0) + (t1*t1 - t0*t0)/2.0 + s2*log(t1/t0)) +           
            (gLeSM *(gLeSM*(2.0*sw2cw2*delta_em + (4.0*gLeSM*gLeSM*Mz2*(Mz2 - s)*s*GammaZSM*deltaGammaZ)/pow(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM),2.0) + (s*sw2cw2*Aeeee)/(M_PI*aEM)) + 4.0*(sw2cw2 + (2.0*gLeSM*gLeSM*s*(-Mz2 + s))/(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM)))*deltagLe))/(s*sw2cw2*sw2cw2)*((1.0/2.0)*( t1*(2.0*Mz2 + 4.0*s + t1) - t0*(2.0*Mz2 + 4.0*s + t0)) + pow(Mz2 + s,2.0)*log((-Mz2 + t1)/(-Mz2 + t0))) +
            (4.0*gLeSM*deltagLe)/(Mz2*sw2cw2) * (Mz2*(t1 - t0) - s2*log(t1/t0) + pow(Mz2 + s,2.0)*log((-Mz2 + t1)/(-Mz2 + t0))) +
            (4.0*gLeSM*gLeSM*gLeSM*deltagLe)/(sw2cw2*sw2cw2)*(((Mz2 + s)*(Mz2 + s)/(Mz2 - t1) - (Mz2 + s)*(Mz2 + s)/(Mz2 - t0) + t1 - t0 + 2.0*(Mz2 + s)*log((-Mz2 + t1)/(-Mz2 + t0))));
 
    return intM2;
}

◆ intDMLR2etildest2()

const double NPSMEFTd6General::intDMLR2etildest2	(	const double	s,
		const double	t0,
		const double	t1
	)		const

virtual

Definition at line 46801 of file NPSMEFTd6General.cpp.

                                                                                                       {
 
    double intM2;
    double aEM, sw2cw2;
    double gLeSM, gReSM;
    double deltagLe, deltagRe;
    double Aeeee;
    double s2;
    // RG scale of the process
    double muRG;
    
    muRG = sqrt(s);
    
    aEM = trueSM.alphaMz();
    sw2cw2 = sW2_tree * cW2_tree;
    Aeeee = CeeLR_e(muRG);
    gLeSM = gZlL;
    gReSM = gZlR;
    deltagLe = deltaGL_f_mu(leptons[ELECTRON], muRG);
    deltagRe = deltaGR_f_mu(leptons[ELECTRON], muRG);
    s2 = s*s;
    
    intM2 = -2.0 * s2*delta_em *(1/t1 - 1/t0) -
            (2.0 * s2*(gReSM * deltagLe + gLeSM*(gReSM*delta_em + deltagRe)))/(Mz * Mz * sw2cw2)*(log(t1/t0) - log( (-Mz * Mz + t1)/(-Mz * Mz + t0) ) ) +
            (s2*Aeeee)/(2.0 * M_PI * aEM )* log(t1/t0) +
            (gLeSM*gReSM*(s2)*Aeeee )/(2.0 * M_PI * sw2cw2 * aEM) * log( (Mz * Mz - t1)/(Mz * Mz - t0) ) +
            ((2.0 *gLeSM*gReSM*s2*(gReSM*deltagLe +  gLeSM*deltagRe))/ sw2cw2/ sw2cw2) *(1.0/ (Mz * Mz - t1) - 1.0/ (Mz * Mz - t0));
 
    return intM2;
}

◆ intDMLR2ets2()

const double NPSMEFTd6General::intDMLR2ets2	(	const double	s,
		const double	t0,
		const double	t1
	)		const

virtual

Definition at line 46783 of file NPSMEFTd6General.cpp.

                                                                                                  {
    
    double intM2;
    
    intM2 = deltaMLR2_f(leptons[ELECTRON], s) * (t1*t1*t1 - t0*t0*t0)/3.0/s/s;
    
    return intM2;
}

◆ intDMRL2etildest2()

const double NPSMEFTd6General::intDMRL2etildest2	(	const double	s,
		const double	t0,
		const double	t1
	)		const

virtual

Definition at line 46832 of file NPSMEFTd6General.cpp.

                                                                                                       {
    
    double intM2;
    double aEM, sw2cw2;
    double gLeSM, gReSM;
    double deltagLe, deltagRe;
    double Aeeee;
    double s2;
    // RG scale of the process
    double muRG;
    
    muRG = sqrt(s);
    
    aEM = trueSM.alphaMz();
    sw2cw2 = sW2_tree * cW2_tree;
    Aeeee = CeeRL_e(muRG);
    gLeSM = gZlL;
    gReSM = gZlR;
    deltagLe = deltaGL_f_mu(leptons[ELECTRON], muRG);
    deltagRe = deltaGR_f_mu(leptons[ELECTRON], muRG);
    s2 = s*s;
    
    intM2 = -2.0 * s2*delta_em *(1/t1 - 1/t0) -
            (2.0 * s2*(gReSM * deltagLe + gLeSM*(gReSM*delta_em + deltagRe)))/(Mz * Mz * sw2cw2)*(log(t1/t0) - log( (-Mz * Mz + t1)/(-Mz * Mz + t0) ) ) +
            (s2*Aeeee)/(2.0 * M_PI * aEM )* log(t1/t0) +
            (gLeSM*gReSM*(s2)*Aeeee )/(2.0 * M_PI * sw2cw2 * aEM) * log( (Mz * Mz - t1)/(Mz * Mz - t0) ) +
            ((2.0 *gLeSM*gReSM*s2*(gReSM*deltagLe +  gLeSM*deltagRe))/ sw2cw2/ sw2cw2) *(1.0/ (Mz * Mz - t1) - 1.0/ (Mz * Mz - t0));
 
    return intM2;
}

◆ intDMRL2ets2()

const double NPSMEFTd6General::intDMRL2ets2	(	const double	s,
		const double	t0,
		const double	t1
	)		const

virtual

Definition at line 46792 of file NPSMEFTd6General.cpp.

                                                                                                  {
 
    double intM2;
    
    intM2 = deltaMRL2_f(leptons[ELECTRON], s) * (t1*t1*t1 - t0*t0*t0)/3.0/s/s;
    
    return intM2;
}

◆ intDMRR2eus2()

const double NPSMEFTd6General::intDMRR2eus2	(	const double	s,
		const double	t0,
		const double	t1
	)		const

virtual

Definition at line 46748 of file NPSMEFTd6General.cpp.

                                                                                                  {
    
    double intM2;
    double aEM, sw2cw2;
    double gReSM;
    double deltagRe;
    double Aeeee;
    double GammaZSM, deltaGammaZ;
    double Mz2, Mz4, s2;
    // RG scale of the process
    double muRG;
    
    muRG = sqrt(s);
    
    aEM = trueSM.alphaMz();
    sw2cw2 = sW2_tree * cW2_tree;
    Aeeee = CeeRR_e(muRG);
    gReSM = gZlR;
    deltagRe = deltaGR_f_mu(leptons[ELECTRON], muRG);
    GammaZSM = trueSM.Gamma_Z();
    deltaGammaZ = deltaGamma_Z();
    Mz2 = Mz * Mz;
    Mz4 = Mz2 * Mz2;
    s2 = s * s;
 
    intM2 = (1.0/(3.0*s2))*((2.0*gReSM*gReSM*gReSM*Mz2*s2*GammaZSM*(gReSM*(Mz4 + s2 - Mz2*(2.0*s + GammaZSM*GammaZSM))*deltaGammaZ + 2.0*GammaZSM*(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM))*deltagRe))/(sw2cw2*sw2cw2 * pow(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM),3.0)) + 
            2.0*(1.0 - (gReSM*gReSM*(Mz2 - s)*s)/(sw2cw2*((Mz2 - s)*(Mz2 - s) + Mz2*GammaZSM*GammaZSM)))*(delta_em + (s*Aeeee)/(2.0*M_PI*aEM) + (2.0*gReSM*(Mz2 - s)*s*(gReSM*Mz2*GammaZSM*deltaGammaZ - (Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM))*deltagRe))/(sw2cw2*pow(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM),2.0))))*(pow(s + t1 ,3.0) - pow(s + t0,3.0)) +
            ((2.0*delta_em + (4.0*gReSM*gReSM*Mz2*(Mz2 - s)*s*GammaZSM*deltaGammaZ)/(sw2cw2*pow(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM),2.0)) + (s*Aeeee)/(M_PI*aEM) - (4.0*gReSM*(Mz2 - s)*s*deltagRe)/(sw2cw2*(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM))))/s)*(2*s*( t1 - t0) + (t1*t1 - t0*t0)/2.0 + s2*log(t1/t0)) +           
            (gReSM *(gReSM*(2.0*sw2cw2*delta_em + (4.0*gReSM*gReSM*Mz2*(Mz2 - s)*s*GammaZSM*deltaGammaZ)/pow(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM),2.0) + (s*sw2cw2*Aeeee)/(M_PI*aEM)) + 4.0*(sw2cw2 + (2.0*gReSM*gReSM*s*(-Mz2 + s))/(Mz4 + s2 + Mz2*(-2.0*s + GammaZSM*GammaZSM)))*deltagRe))/(s*sw2cw2*sw2cw2)*((1.0/2.0)*( t1*(2.0*Mz2 + 4.0*s + t1) - t0*(2.0*Mz2 + 4.0*s + t0)) + pow(Mz2 + s,2.0)*log((-Mz2 + t1)/(-Mz2 + t0))) +
            (4.0*gReSM*deltagRe)/(Mz2*sw2cw2) * (Mz2*(t1 - t0) - s2*log(t1/t0) + pow(Mz2 + s,2.0)*log((-Mz2 + t1)/(-Mz2 + t0))) +
            (4.0*gReSM*gReSM*gReSM*deltagRe)/(sw2cw2*sw2cw2)*(((Mz2 + s)*(Mz2 + s)/(Mz2 - t1) - (Mz2 + s)*(Mz2 + s)/(Mz2 - t0) + t1 - t0 + 2.0*(Mz2 + s)*log((-Mz2 + t1)/(-Mz2 + t0))));
 
    return intM2;
}

◆ kappaAeff()

const double NPSMEFTd6General::kappaAeff ( ) const

virtual

The effective coupling $\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}$.

Returns: $\kappa_{A,eff}$

Reimplemented from NPbase.

Definition at line 43073 of file NPSMEFTd6General.cpp.

                                               {
    return sqrt(GammaHgagaRatio());
}

◆ kappabeff()

const double NPSMEFTd6General::kappabeff ( ) const

virtual

The effective coupling $\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}$.

Returns: $\kappa_{b,eff}$

Reimplemented from NPbase.

Definition at line 43049 of file NPSMEFTd6General.cpp.

                                               {
    return sqrt(GammaHbbRatio());
}

◆ kappaceff()

const double NPSMEFTd6General::kappaceff ( ) const

virtual

The effective coupling $\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}$.

Returns: $\kappa_{c,eff}$

Reimplemented from NPbase.

Definition at line 43041 of file NPSMEFTd6General.cpp.

                                               {
    return sqrt(GammaHccRatio());
}

◆ kappaGeff()

const double NPSMEFTd6General::kappaGeff ( ) const

virtual

The effective coupling $\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}$.

Returns: $\kappa_{G,eff}$

Reimplemented from NPbase.

Definition at line 43053 of file NPSMEFTd6General.cpp.

                                               {
    return sqrt(GammaHggRatio());
}

◆ kappamueff()

const double NPSMEFTd6General::kappamueff ( ) const

virtual

The effective coupling $\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}$.

Returns: $\kappa_{\mu,eff}$

Reimplemented from NPbase.

Definition at line 43033 of file NPSMEFTd6General.cpp.

                                                {
    return sqrt(GammaHmumuRatio());
}

◆ kappaseff()

const double NPSMEFTd6General::kappaseff ( ) const

virtual

The effective coupling $\kappa_{s,eff}=\sqrt{\Gamma_{Hss}/\Gamma_{Hss}^{SM}}$.

Returns: $\kappa_{s,eff}$

Definition at line 43045 of file NPSMEFTd6General.cpp.

                                               {
    return sqrt(GammaHssRatio());
}

◆ kappataueff()

const double NPSMEFTd6General::kappataueff ( ) const

virtual

The effective coupling $\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}$.

Returns: $\kappa_{\tau,eff}$

Reimplemented from NPbase.

Definition at line 43037 of file NPSMEFTd6General.cpp.

                                                 {
    return sqrt(GammaHtautauRatio());
}

◆ kappaW4feff()

const double NPSMEFTd6General::kappaW4feff ( ) const

virtual

The effective coupling $\kappa_{W4f,eff}=\sqrt{\Gamma_{H4f, CC}/\Gamma_{H4f, CC}^{SM}}$.

Returns: $\kappa_{W4f,eff}$

Reimplemented from NPbase.

Definition at line 43069 of file NPSMEFTd6General.cpp.

                                                 {
    return sqrt(GammaH4fCCRatio());
}

◆ kappaWeff()

const double NPSMEFTd6General::kappaWeff ( ) const

virtual

The effective coupling $\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}$.

Returns: $\kappa_{W,eff}$

Reimplemented from NPbase.

Definition at line 43061 of file NPSMEFTd6General.cpp.

                                               {
    return sqrt(GammaHWWRatio());
}

◆ kappaZ4feff()

const double NPSMEFTd6General::kappaZ4feff ( ) const

virtual

The effective coupling $\kappa_{Z4f,eff}=\sqrt{\Gamma_{H4f, NC}/\Gamma_{H4f, NC}^{SM}}$.

Returns: $\kappa_{Z4f,eff}$

Reimplemented from NPbase.

Definition at line 43065 of file NPSMEFTd6General.cpp.

                                                 {
    return sqrt(GammaH4fNCRatio());
}

◆ kappaZAeff()

const double NPSMEFTd6General::kappaZAeff ( ) const

virtual

The effective coupling $\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}$.

Returns: $\kappa_{ZA,eff}$

Reimplemented from NPbase.

Definition at line 43077 of file NPSMEFTd6General.cpp.

                                                {
    return sqrt(GammaHZgaRatio());
}

◆ kappaZeff()

const double NPSMEFTd6General::kappaZeff ( ) const

virtual

The effective coupling $\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}$.

Returns: $\kappa_{Z,eff}$

Reimplemented from NPbase.

Definition at line 43057 of file NPSMEFTd6General.cpp.

                                               {
    return sqrt(GammaHZZRatio());
}

◆ lambdaZNP()

const double NPSMEFTd6General::lambdaZNP ( const double mu ) const

virtual

The new physics contribution to the anomalous triple gauge coupling $\lambda_{Z}$.

Returns: $\lambda_{Z}$

Reimplemented from NPbase.

Definition at line 36527 of file NPSMEFTd6General.cpp.

                                                              {
    double NPdirect;
 
    NPdirect = (3.0 / 2.0) * (eeMz / sW_tree) * getSMEFTCoeff("CW", mu) * v2;
 
    return NPdirect;
}

◆ lambz_HB()

const double NPSMEFTd6General::lambz_HB ( const double mu ) const

virtual

The Higgs-basis coupling $\lambda_{z}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$.

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\lambda_{z}$

Reimplemented from NPbase.

Definition at line 43233 of file NPSMEFTd6General.cpp.

                                                             {
    double ciHB;
 
    ciHB = -(3.0 / 2.0)*(eeMz / sW_tree) * getSMEFTCoeff("CW", mu) * v2;
 
    return ciHB;
}

◆ mubbH()

virtual const double NPSMEFTd6General::mubbH ( const double sqrt_s ) const

inlinevirtual

The ratio $\mu_{bbH}$ between the bbH production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{bbH}$

Reimplemented from NPbase.

Definition at line 2152 of file NPSMEFTd6General.h.

    {
        return 1.0;
    };                             //AG:added

◆ mueeHee()

const double NPSMEFTd6General::mueeHee	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{e^+e^- \to He^+e^-}$ between the $ e^+e^- \to H e^+e^- $ associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{e^+e^- \to H e^+e^-}$

Reimplemented from NPbase.

Definition at line 22043 of file NPSMEFTd6General.cpp.

                                                                                                          {
 
    //  Mw scheme
 
    double mu = 1.0;
 
    double C1 = 0.0;
 
    // Wilson coefficients and scale    
    double CHB = 0.0, CHW = 0.0, CHWB = 0.0, CHD = 0.0, CHbox = 0.0, CHl1R11 = 0.0;
    double CHl3R11 = 0.0, CHl3R22 = 0.0, CHeR11 = 0.0, CllR1221 = 0.0; 
    double muRG = 0;
    
    // Polarization factors
    double Pe = Pol_em, Pp = Pol_ep;
    double fLR, fRL, fLL, fRR;
    
    // LR, RL, LL, and RR cross sections    
    double sigmaSMeLRa0 = 0.0, sigmaeLRa0 = 0.0, sigmaSMeLRa1 = 0.0, sigmaeLRa1 = 0.0; 
    double sigmaSMeRLa0 = 0.0, sigmaeRLa0 = 0.0, sigmaSMeRLa1 = 0.0, sigmaeRLa1 = 0.0;
    
    double sigmaSMeLLa0 = 0.0, sigmaeLLa0 = 0.0, sigmaSMeLLa1 = 0.0, sigmaeLLa1 = 0.0; 
    double sigmaSMeRRa0 = 0.0, sigmaeRRa0 = 0.0, sigmaSMeRRa1 = 0.0, sigmaeRRa1 = 0.0;
    
    double scalTH = 1.0;
    
    // -------------------------------------------------------------------------
    
    if ( sqrt_s > 0.5 ) {
        // Theory uncert. scaling like log^2(E/MW)
        
        scalTH = log(sqrt_s/0.080365)/log(0.5/0.080365);
        scalTH = scalTH * scalTH;
    }
    
    fLR = 0.25 * (1.0 - Pe) * (1.0 + Pp);
    fRL = 0.25 * (1.0 + Pe) * (1.0 - Pp);
    fLL = 0.25 * (1.0 - Pe) * (1.0 - Pp);
    fRR = 0.25 * (1.0 + Pe) * (1.0 + Pp);
    
    // RG scale in GeV
    muRG = 1000. * sqrt_s;
    
//  Wilson coefficients definitions 
    CHB = getSMEFTCoeff("CHB", muRG); 
    CHW = getSMEFTCoeff("CHW", muRG); 
    CHWB = getSMEFTCoeff("CHWB", muRG); 
    CHD = getSMEFTCoeff("CHD", muRG); 
    CHbox = getSMEFTCoeff("CHbox", muRG); 
    CHl1R11 = getSMEFTCoeff("CHl1R",0,0, muRG); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CHeR11 = getSMEFTCoeff("CHeR",0,0, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG);
    
    // Computed as the difference between e+ e- > H e+ e- and e+ e- > H Z, Z > e+ e-
    
    if (sqrt_s == 0.500) {
 
        C1 = 0.0067;
        
        // e+ e- > H e+ e- - e+ e- > H Z, Z > e+ e-
        // LR -------------------------------
        sigmaSMeLRa0 = 0.015502; 
 
        sigmaeLRa0 = cWsch * (sigmaSMeLRa0
                -4098.92 * CHB 
                +7192.41 * CHW 
                +6438.5 * CHWB 
                +4108.48 * CHD 
                +1877.39 * CHbox 
                +28079.5 * CHl1R11 
                +25267.8 * CHl3R11 
                -2824.24 * CHl3R22 
                -526.241 * CHeR11 
                +2810.1 * CllR1221 
                );
        
        sigmaSMeLRa1 = 0.003925; 
 
        sigmaeLRa1 = cWsch * (sigmaSMeLRa1
                -1760.76 * CHB 
                +6343.83 * CHW 
                +862.93 * CHWB 
                +624.83 * CHD 
                +475.03 * CHbox 
                +26386.7 * CHl1R11 
                +25667.3 * CHl3R11 
                -714.93 * CHl3R22 
                -421.83 * CHeR11 
                +711.83 * CllR1221               
                );
        
        // RL -------------------------------
        sigmaSMeRLa0 = 0.007657; 
 
        sigmaeRLa0 = cWsch * (sigmaSMeRLa0
                +1971.91 * CHB 
                -91.342 * CHW 
                +1373.22 * CHWB 
                -2764.85 * CHD 
                +924.564 * CHbox 
                +414.096 * CHl1R11 
                -976.972 * CHl3R11 
                -1394.52 * CHl3R22 
                -23347.4 * CHeR11 
                +1388.44 * CllR1221              
                );
        
        sigmaSMeRLa1 = 0.002563; 
 
        sigmaeRLa1 = cWsch * (sigmaSMeRLa1
                +2917.26 * CHB 
                +76.18 * CHW 
                +2218.96 * CHWB 
                -566.82 * CHD 
                +310.61 * CHbox 
                +340.09 * CHl1R11 
                -126.53 * CHl3R11 
                -466.71 * CHl3R22 
                -21174.2 * CHeR11 
                +464.69 * CllR1221               
                );   
        
        // LL -------------------------------
        sigmaSMeLLa0 = 0.006966; 
 
        sigmaeLLa0 = cWsch * (sigmaSMeLLa0
                +4733.36 * CHB 
                +1093.5 * CHW 
                -3452.57 * CHWB 
                -494.684 * CHD 
                +844.033 * CHbox 
                -1787.74 * CHl1R11 
                -3056.39 * CHl3R11 
                -1268.13 * CHl3R22 
                +2206.99 * CHeR11 
                +1266.16 * CllR1221
                );
        
        sigmaSMeLLa1 = 0.0; 
 
        sigmaeLLa1 = sigmaSMeLLa1;
        
        // RR -------------------------------
        sigmaSMeRRa0 = 0.006966; 
 
        sigmaeRRa0 = cWsch * (sigmaSMeRRa0
                +4735.97 * CHB 
                +1092.78 * CHW 
                -3453.81 * CHWB 
                -494.684 * CHD 
                +844.033 * CHbox 
                -1788.99 * CHl1R11 
                -3056.38 * CHl3R11 
                -1268.13 * CHl3R22 
                +2206.53 * CHeR11 
                +1266.16 * CllR1221             
                );
        
        sigmaSMeRRa1 = 0.0; 
 
        sigmaeRRa1 = sigmaSMeRRa1; 
 
    } else if (sqrt_s == 0.550) {
 
        C1 = 0.0067;
        
        // e+ e- > H e+ e- - e+ e- > H Z, Z > e+ e-
        // LR -------------------------------
        sigmaSMeLRa0 = 0.016705; 
 
        sigmaeLRa0 = cWsch * (sigmaSMeLRa0
                -4112.54 * CHB 
                +5601.16 * CHW 
                +7336.04 * CHWB 
                +4634.02 * CHD 
                +2029.88 * CHbox 
                +25858.5 * CHl1R11 
                +22849.8 * CHl3R11 
                -3039.76 * CHl3R22 
                -434.5 * CHeR11 
                +3041.28 * CllR1221
                );
        
        sigmaSMeLRa1 = 0.003172; 
 
        sigmaeLRa1 = cWsch * (sigmaSMeLRa1
                -1488.24 * CHB 
                +5327.07 * CHW 
                +689.75 * CHWB 
                +506.48 * CHD 
                +383.93 * CHbox 
                +25710.4 * CHl1R11 
                +25128.9 * CHl3R11 
                -576.71 * CHl3R22 
                -340.94 * CHeR11 
                +576.93 * CllR1221               
                );
        
        // RL -------------------------------
        sigmaSMeRLa0 = 0.007966; 
 
        sigmaeRLa0 = cWsch * (sigmaSMeRLa0
                +984.448 * CHB 
                -142.658 * CHW 
                +677.26 * CHWB 
                -3034.71 * CHD 
                +965.07 * CHbox 
                +340.095 * CHl1R11 
                -1101.65 * CHl3R11 
                -1452.34 * CHl3R22 
                -21978.4 * CHeR11 
                +1451.97 * CllR1221             
                );
        
        sigmaSMeRLa1 = 0.00207; 
 
        sigmaeRLa1 = cWsch * (sigmaSMeRLa1
                +2454.5 * CHB 
                +53.84 * CHW 
                +1880.89 * CHWB 
                -457.54 * CHD 
                +251.23 * CHbox 
                +275.71 * CHl1R11 
                -101.57 * CHl3R11 
                -376.05 * CHl3R22 
                -20653.6 * CHeR11 
                +376.16 * CllR1221                
                );   
        
        // LL -------------------------------
        sigmaSMeLLa0 = 0.008388; 
 
        sigmaeLLa0 = cWsch * (sigmaSMeLLa0
                +5210.05 * CHB 
                +1184.39 * CHW 
                -3856.1 * CHWB 
                -596.339 * CHD 
                +1015.68 * CHbox 
                -2279.34 * CHl1R11 
                -3807.33 * CHl3R11 
                -1526.87 * CHl3R22 
                +2813.4 * CHeR11 
                +1523.44 * CllR1221
                );
        
        sigmaSMeLLa1 = 0.0; 
 
        sigmaeLLa1 = sigmaSMeLLa1;
        
        // RR -------------------------------
        sigmaSMeRRa0 = 0.008388; 
 
        sigmaeRRa0 = cWsch * (sigmaSMeRRa0
                +5210.49 * CHB 
                +1183.86 * CHW 
                -3856.65 * CHWB 
                -594.298 * CHD 
                +1014.02 * CHbox 
                -2283.41 * CHl1R11 
                -3805.47 * CHl3R11 
                -1526.24 * CHl3R22 
                +2814.1 * CHeR11 
                +1522.51 * CllR1221             
                );
        
        sigmaSMeRRa1 = 0.0; 
 
        sigmaeRRa1 = sigmaSMeRRa1; 
 
    } else if (sqrt_s == 1.0) {
 
        C1 = 0.0065;
 
        // e+ e- > H e+ e- - e+ e- > H Z, Z > e+ e-
        // LR -------------------------------
        sigmaSMeLRa0 = 0.031515; 
 
        sigmaeLRa0 = cWsch * (sigmaSMeLRa0
                -5273.48 * CHB 
                -2563.62 * CHW 
                +16070.3 * CHWB 
                +9598.71 * CHD 
                +3803.15 * CHbox 
                +6786.78 * CHl1R11 
                +1156.86 * CHl3R11 
                -5735.46 * CHl3R22 
                -132.37 * CHeR11 
                +5728.09 * CllR1221
                );
        
        sigmaSMeLRa1 = 0.00088; 
 
        sigmaeLRa1 = cWsch * (sigmaSMeLRa1
                -482.328 * CHB 
                +1692.36 * CHW 
                +183.29 * CHWB 
                +140.1 * CHD 
                +106.2 * CHbox 
                +23325.2 * CHl1R11 
                +23162.1 * CHl3R11 
                -160.16 * CHl3R22 
                -94.45 * CHeR11 
                +159.86 * CllR1221               
                );
        
        // RL -------------------------------
        sigmaSMeRLa0 = 0.013671; 
 
        sigmaeRLa0 = cWsch * (sigmaSMeRLa0
                -4714.26 * CHB 
                -308.604 * CHW 
                -3682.04 * CHWB 
                -6021.83 * CHD 
                +1648.1 * CHbox 
                +93.8183 * CHl1R11 
                -2395.03 * CHl3R11 
                -2489.25 * CHl3R22 
                -11195.5 * CHeR11 
                +2484.75 * CllR1221             
                );
        
        sigmaSMeRLa1 = 0.000575; 
 
        sigmaeRLa1 = cWsch * (sigmaSMeRLa1
                +783.67 * CHB 
                +4.93 * CHW 
                +615.38 * CHWB 
                -127.27 * CHD 
                +69.67 * CHbox 
                +76.16 * CHl1R11 
                -28.32 * CHl3R11 
                -104.57 * CHl3R22 
                -18814. * CHeR11 
                +104.73 * CllR1221                
                );   
        
        // LL -------------------------------
        sigmaSMeLLa0 = 0.019938; 
 
        sigmaeLLa0 = cWsch * (sigmaSMeLLa0
                +7757.24 * CHB 
                +1628.67 * CHW 
                -6241.45 * CHWB 
                -1420.11 * CHD 
                +2407.24 * CHbox 
                -7405.21 * CHl1R11 
                -11030.9 * CHl3R11 
                -3630.32 * CHl3R22 
                +9152.39 * CHeR11 
                +3619.27 * CllR1221
                );
        
        sigmaSMeLLa1 = 0.0; 
 
        sigmaeLLa1 = sigmaSMeLLa1;
        
        // RR -------------------------------
        sigmaSMeRRa0 = 0.019938; 
 
        sigmaeRRa0 = cWsch * (sigmaSMeRRa0
                +7760.88 * CHB 
                +1629.58 * CHW 
                -6241.85 * CHWB 
                -1420.11 * CHD 
                +2407.24 * CHbox 
                -7416.83 * CHl1R11 
                -11036.3 * CHl3R11 
                -3630.32 * CHl3R22 
                +9151.14 * CHeR11 
                +3619.27 * CllR1221             
                );
        
        sigmaSMeRRa1 = 0.0; 
 
        sigmaeRRa1 = sigmaSMeRRa1; 
 
    } else if (sqrt_s == 1.4) {
 
        C1 = 0.0065;
 
        // e+ e- > H e+ e- - e+ e- > H Z, Z > e+ e-
        // LR -------------------------------
        sigmaSMeLRa0 = 0.043295; 
 
        sigmaeLRa0 = cWsch * (sigmaSMeLRa0
                -6192.44 * CHB 
                -5876.33 * CHW 
                +22064.3 * CHWB 
                +13310.3 * CHD 
                +5226.12 * CHbox 
                -8410.11 * CHl1R11 
                -16330.9 * CHl3R11 
                -7885.24 * CHl3R22 
                -80.8144 * CHeR11 
                +7861.2 * CllR1221
                );
        
        sigmaSMeLRa1 = 0.00044; 
 
        sigmaeLRa1 = cWsch * (sigmaSMeLRa1
                -249.516 * CHB 
                +871.46 * CHW 
                +91. * CHWB 
                +70.15 * CHD 
                +53.31 * CHbox 
                +22795.3 * CHl1R11 
                +22705.4 * CHl3R11 
                -80.019 * CHl3R22 
                -47.409 * CHeR11 
                +79.81 * CllR1221               
                );
        
        // RL -------------------------------
        sigmaSMeRLa0 = 0.018575; 
 
        sigmaeRLa0 = cWsch * (sigmaSMeRLa0
                -7253.38 * CHB 
                -354.216 * CHW 
                -6168.17 * CHWB 
                -8318.73 * CHD 
                +2239.38 * CHbox 
                +44.6 * CHl1R11 
                -3340.37 * CHl3R11 
                -3383.27 * CHl3R22 
                -3085.96 * CHeR11 
                +3370.78 * CllR1221             
                );
        
        sigmaSMeRLa1 = 0.000287; 
 
        sigmaeRLa1 = cWsch * (sigmaSMeRLa1
                +404.369 * CHB 
                +1.262 * CHW 
                +318.379 * CHWB 
                -63.65 * CHD 
                +34.837 * CHbox 
                +38.139 * CHl1R11 
                -14.289 * CHl3R11 
                -52.272 * CHl3R22 
                -18393.9 * CHeR11 
                +52.215 * CllR1221                
                );   
        
        // LL -------------------------------
        sigmaSMeLLa0 = 0.027967; 
 
        sigmaeLLa0 = cWsch * (sigmaSMeLLa0
                +8797.53 * CHB 
                +1783.21 * CHW 
                -7389.69 * CHWB 
                -1996.03 * CHD 
                +3374.01 * CHbox 
                -12077. * CHl1R11 
                -17157.9 * CHl3R11 
                -5092.09 * CHl3R22 
                +14929.2 * CHeR11 
                +5076.1 * CllR1221
                );
        
        sigmaSMeLLa1 = 0.0; 
 
        sigmaeLLa1 = sigmaSMeLLa1;
        
        // RR -------------------------------
        sigmaSMeRRa0 = 0.027967; 
 
        sigmaeRRa0 = cWsch * (sigmaSMeRRa0
                +8799.81 * CHB 
                +1789.18 * CHW 
                -7386.69 * CHWB 
                -1996.03 * CHD 
                +3374.07 * CHbox 
                -12093.2 * CHl1R11 
                -17168.1 * CHl3R11 
                -5092.1 * CHl3R22 
                +14921.5 * CHeR11 
                +5076.11 * CllR1221             
                );
        
        sigmaSMeRRa1 = 0.0; 
 
        sigmaeRRa1 = sigmaSMeRRa1;  
 
    } else if (sqrt_s == 1.5) {
 
        C1 = 0.0065; // Use the same as 1400 GeV
 
        // e+ e- > H e+ e- - e+ e- > H Z, Z > e+ e-
        // LR -------------------------------
        sigmaSMeLRa0 = 0.045902; 
 
        sigmaeLRa0 = cWsch * (sigmaSMeLRa0
                -6375.19 * CHB 
                -6460.92 * CHW 
                +23318.4 * CHWB 
                +14123. * CHD 
                +5539.23 * CHbox 
                -12062.5 * CHl1R11 
                -20377.7 * CHl3R11 
                -8361.26 * CHl3R22 
                -70.2473 * CHeR11 
                +8323.76 * CllR1221 
                );
        
        sigmaSMeLRa1 = 0.000382; 
 
        sigmaeLRa1 = cWsch * (sigmaSMeLRa1
                -217.463 * CHB 
                +760.524 * CHW 
                +78.744 * CHWB 
                +60.914 * CHD 
                +46.284 * CHbox 
                +22714.2 * CHl1R11 
                +22643.9 * CHl3R11 
                -69.698 * CHl3R22 
                -41.158 * CHeR11 
                +69.444 * CllR1221                
                );
        
        // RL -------------------------------
        sigmaSMeRLa0 = 0.019672; 
 
        sigmaeRLa0 = cWsch * (sigmaSMeRLa0
                -7723.03 * CHB 
                -363.499 * CHW 
                -6714.28 * CHWB 
                -8822.04 * CHD 
                +2368.63 * CHbox 
                +26.1277 * CHl1R11 
                -3541.43 * CHl3R11 
                -3586.63 * CHl3R22 
                -1139.61 * CHeR11 
                +3562.85 * CllR1221              
                );
        
        sigmaSMeRLa1 = 0.00025; 
 
        sigmaeRLa1 = cWsch * (sigmaSMeRLa1
                +353.423 * CHB 
                +0.877 * CHW 
                +278.093 * CHWB 
                -55.24 * CHD 
                +30.338 * CHbox 
                +33.078 * CHl1R11 
                -12.356 * CHl3R11 
                -45.362 * CHl3R22 
                -18343.1 * CHeR11 
                +45.449 * CllR1221                
                );   
        
        // LL -------------------------------
        sigmaSMeLLa0 = 0.029711; 
 
        sigmaeLLa0 = cWsch * (sigmaSMeLLa0
                +8980.14 * CHB 
                +1806.17 * CHW 
                -7606.24 * CHWB 
                -2122.01 * CHD 
                +3584.01 * CHbox 
                -13210.4 * CHl1R11 
                -18604.3 * CHl3R11 
                -5410.06 * CHl3R22 
                +16326.5 * CHeR11 
                +5389.08 * CllR1221 
                );
        
        sigmaSMeLLa1 = 0.0; 
 
        sigmaeLLa1 = sigmaSMeLLa1;
        
        // RR -------------------------------
        sigmaSMeRRa0 = 0.029711; 
 
        sigmaeRRa0 = cWsch * (sigmaSMeRRa0
                +8985.08 * CHB 
                +1815.25 * CHW 
                -7606.1 * CHWB 
                -2122.01 * CHD 
                +3584.06 * CHbox 
                -13225.4 * CHl1R11 
                -18615.2 * CHl3R11 
                -5410.07 * CHl3R22 
                +16320. * CHeR11 
                +5389.08 * CllR1221              
                );
        
        sigmaSMeRRa1 = 0.0; 
 
        sigmaeRRa1 = sigmaSMeRRa1;  
 
    } else if (sqrt_s == 3.0) {
 
        C1 = 0.0063;
 
        // e+ e- > H e+ e- - e+ e- > H Z, Z > e+ e-
        // LR -------------------------------
        sigmaSMeLRa0 = 0.074258; 
 
        sigmaeLRa0 = cWsch * (sigmaSMeLRa0
                -7890.8 * CHB 
                -10712. * CHW 
                +36102.9 * CHWB 
                +22954.4 * CHD 
                +8950.34 * CHbox 
                -58386.8 * CHl1R11 
                -71823.6 * CHl3R11 
                -13529.9 * CHl3R22 
                -84.4482 * CHeR11 
                +13440.9 * CllR1221 
                );
        
        sigmaSMeLRa1 = 0.000094; 
 
        sigmaeLRa1 = cWsch * (sigmaSMeLRa1
                -54.8938 * CHB 
                +191.442 * CHW 
                +19.136 * CHWB 
                +14.986 * CHD 
                +11.398 * CHbox 
                +22370.4 * CHl1R11 
                +22337.9 * CHl3R11 
                -17.152 * CHl3R22 
                -10.134 * CHeR11 
                +17.064 * CllR1221                
                );
        
        // RL -------------------------------
        sigmaSMeRLa0 = 0.031683; 
 
        sigmaeRLa0 = cWsch * (sigmaSMeRLa0
                -11227.5 * CHB 
                -410.83 * CHW 
                -12206.1 * CHWB 
                -14304.6 * CHD 
                +3817.17 * CHbox 
                -0.93975 * CHl1R11 
                -5766.16 * CHl3R11 
                -5772.65 * CHl3R22 
                +23381.2 * CHeR11 
                +5741.22 * CllR1221              
                );
        
        sigmaSMeRLa1 = 0.000061; 
 
        sigmaeRLa1 = cWsch * (sigmaSMeRLa1
                +89.174 * CHB 
                -0.004 * CHW 
                +70.224 * CHWB 
                -13.617 * CHD 
                +7.452 * CHbox 
                +8.178 * CHl1R11 
                -3.058 * CHl3R11 
                -11.199 * CHl3R22 
                -18063.7 * CHeR11 
                +11.123 * CllR1221                
                );   
        
        // LL -------------------------------
        sigmaSMeLLa0 = 0.048427; 
 
        sigmaeLLa0 = cWsch * (sigmaSMeLLa0
                +10268.1 * CHB 
                +1941.01 * CHW 
                -9431.02 * CHWB 
                -3454. * CHD 
                +5837. * CHbox 
                -27962.8 * CHl1R11 
                -36729.7 * CHl3R11 
                -8820.01 * CHl3R22 
                +34561.2 * CHeR11 
                +8778.01 * CllR1221 
                );
        
        sigmaSMeLLa1 = 0.0; 
 
        sigmaeLLa1 = sigmaSMeLLa1;
        
        // RR -------------------------------
        sigmaSMeRRa0 = 0.048427; 
 
        sigmaeRRa0 = cWsch * (sigmaSMeRRa0
                +10279.1 * CHB 
                +1965.01 * CHW 
                -9436.92 * CHWB 
                -3454. * CHD 
                +5837. * CHbox 
                -27968.7 * CHl1R11 
                -36755.7 * CHl3R11 
                -8820.01 * CHl3R22 
                +34557.2 * CHeR11 
                +8779.01 * CllR1221              
                );
        
        sigmaSMeRRa1 = 0.0; 
 
        sigmaeRRa1 = sigmaSMeRRa1;  
 
        sigmaeRRa1 = cWsch * (sigmaSMeRRa1
               
                ); 
        
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeHee()");
    
    // Construct the signal strength
    // Total cross section
    mu = fLR * (sigmaeLRa0 - sigmaeLRa1) + fRL * (sigmaeRLa0 - sigmaeRLa1) + fLL * (sigmaeLLa0 - sigmaeLLa1) + fRR * (sigmaeRRa0 - sigmaeRRa1);
    // Normalize to SM
    mu = mu / (fLR * (sigmaSMeLRa0 - sigmaSMeLRa1) + fRL * (sigmaSMeRLa0 - sigmaSMeRLa1) + fLL * (sigmaSMeLLa0 - sigmaSMeLLa1) + fRR * (sigmaSMeRRa0 - sigmaSMeRRa1));
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    //(Assume similar to WBF.)
    mu += scalTH * eeeWBFint + eeeWBFpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mueeHvv()

const double NPSMEFTd6General::mueeHvv	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{e^+e^- \to H\nu\bar{\nu}}$ between the $ e^+e^- \to H\nu\bar{\nu} $ associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{e^+e^- \to H\nu\bar{\nu}}$

Reimplemented from NPbase.

Definition at line 20658 of file NPSMEFTd6General.cpp.

                                                                                                          {
 
    //  Mw scheme
 
    double mu = 1.0;
 
    double C1 = 0.0;
    
    // Wilson coefficients and scale
    double CHB = 0.0, CHW = 0.0, CHWB = 0.0, CHD = 0.0, CHbox = 0.0, CHl1R11 = 0.0;
    double CHl3R11 = 0.0, CHl3R22 = 0.0, CHeR11 = 0.0, CllR1221 = 0.0; 
    double muRG = 0;    
 
    // Polarization factors
    double Pe = Pol_em, Pp = Pol_ep;
    double fLR, fRL;
 
    // LH and RH cross sections    
    double sigmaSMeLHa0 = 0.0, sigmaeLHa0 = 0.0, sigmaSMeLHa1 = 0.0, sigmaeLHa1 = 0.0; 
    double sigmaSMeRHa0 = 0.0, sigmaeRHa0 = 0.0, sigmaSMeRHa1 = 0.0, sigmaeRHa1 = 0.0;
 
    double scalTH = 1.0;
    
    // -------------------------------------------------------------------------
    
    if ( sqrt_s > 0.5 ) {
        // Theory uncert. scaling like log^2(E/MW)
        
        scalTH = log(sqrt_s/0.080365)/log(0.5/0.080365);
        scalTH = scalTH * scalTH;
    }
        
    fLR = 0.25 * (1.0 - Pe) * (1.0 + Pp);
    fRL = 0.25 * (1.0 + Pe) * (1.0 - Pp);
    
    // RG scale in GeV
    muRG = 1000. * sqrt_s;
    
    //  Wilson coefficients definitions 
    CHB = getSMEFTCoeff("CHB", muRG); 
    CHW = getSMEFTCoeff("CHW", muRG); 
    CHWB = getSMEFTCoeff("CHWB", muRG); 
    CHD = getSMEFTCoeff("CHD", muRG); 
    CHbox = getSMEFTCoeff("CHbox", muRG); 
    CHl1R11 = getSMEFTCoeff("CHl1R",0,0, muRG); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CHeR11 = getSMEFTCoeff("CHeR",0,0, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG);
    
    //  For the Higgs trilinear dependence assume the WBF mechanism dominates
    
    // Computed as the difference between e+ e- > H ve ve and e+ e- > H Z, Z > ve ve
 
    if (sqrt_s == 0.230) {
 
        C1 = 0.00639683;
 
        // e+ e- > H ve ve - e+ e- > H Z, Z > ve ve
        // LH -------------------------------
        sigmaSMeLHa0 = 0.059149; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -6703.9 * CHB 
                +28405.8 * CHW 
                +8204.2 * CHWB 
                +4505.86 * CHD 
                +7247.85 * CHbox 
                +46957.8 * CHl1R11 
                +41337.8 * CHl3R11 
                -10716.8 * CHl3R22 
                +50.057 * CHeR11 
                +10816.5 * CllR1221
                );
        
        sigmaSMeLHa1 = 0.029738; 
 
        sigmaeLHa1 = cWsch * (sigmaSMeLHa1
                -5698. * CHB 
                +24313. * CHW 
                +6634. * CHWB 
                +4154. * CHD 
                +3596. * CHbox 
                +37856. * CHl1R11 
                +39659. * CHl3R11 
                -5412. * CHl3R22 
                -2. * CHeR11 
                +5405. * CllR1221              
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.021932; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +11963.9 * CHB 
                +1660.64 * CHW 
                +6640.6 * CHWB 
                -5265.33 * CHD 
                +2635.77 * CHbox 
                -2626.19 * CHl1R11 
                -1364.38 * CHl3R11 
                -3977.51 * CHl3R22 
                -37857.4 * CHeR11 
                +3998.57 * CllR1221              
                );
        
        sigmaSMeRHa1 = 0.019411; 
 
        sigmaeRHa1 = cWsch * (sigmaSMeRHa1
                +10684.6 * CHB 
                +1491.6 * CHW 
                +5968.6 * CHWB 
                -4673.2 * CHD 
                +2359.6 * CHbox 
                -2347.2 * CHl1R11 
                -1176.4 * CHl3R11 
                -3522.7 * CHl3R22 
                -33504.4 * CHeR11 
                +3535.6 * CllR1221              
                );
        
    } else if (sqrt_s == 0.240) {
 
        C1 = 0.00639683;
        
        // e+ e- > H ve ve - e+ e- > H Z, Z > ve ve
        // LH -------------------------------
        sigmaSMeLHa0 = 0.064179; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -7582.01 * CHB 
                +31652.3 * CHW 
                +8473.6 * CHWB 
                +4551.21 * CHD 
                +7782.99 * CHbox 
                +53595.2 * CHl1R11 
                +46797.1 * CHl3R11 
                -11665.3 * CHl3R22 
                -34.399 * CHeR11 
                +11729.1 * CllR1221 
                );
        
        sigmaSMeLHa1 = 0.032478; 
 
        sigmaeLHa1 = cWsch * (sigmaSMeLHa1
                -6747. * CHB 
                +28236. * CHW 
                +7213. * CHWB 
                +4534. * CHD 
                +3930. * CHbox 
                +45348. * CHl1R11 
                +47337. * CHl3R11 
                -5915. * CHl3R22 
                -5. * CHeR11 
                +5905. * CllR1221              
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.024227; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +14216.9 * CHB 
                +1819.5 * CHW 
                +8263.49 * CHWB 
                -5810.48 * CHD 
                +2944.56 * CHbox 
                -2904.14 * CHl1R11 
                -1479.61 * CHl3R11 
                -4379.55 * CHl3R22 
                -45568.2 * CHeR11 
                +4424.17 * CllR1221              
                );
        
        sigmaSMeRHa1 = 0.021198; 
 
        sigmaeRHa1 = cWsch * (sigmaSMeRHa1
                +12477. * CHB 
                +1581. * CHW 
                +7265. * CHWB 
                -5103. * CHD 
                +2581. * CHbox 
                -2563.9 * CHl1R11 
                -1282.9 * CHl3R11 
                -3841.8 * CHl3R22 
                -39845. * CHeR11 
                +3860. * CllR1221              
                );
 
    } else if (sqrt_s == 0.250) {
 
        C1 = 0.0064;
 
        // e+ e- > H ve ve - e+ e- > H Z, Z > ve ve
        // LH -------------------------------
        sigmaSMeLHa0 = 0.067697; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -7842.55 * CHB 
                +32195.3 * CHW 
                +7995.72 * CHWB 
                +4345.9 * CHD 
                +8239.09 * CHbox 
                +56576.4 * CHl1R11 
                +47681.9 * CHl3R11 
                -12330.7 * CHl3R22 
                +4.62 * CHeR11 
                +12293.3 * CllR1221 
                );
        
        sigmaSMeLHa1 = 0.032502; 
 
        sigmaeLHa1 = cWsch * (sigmaSMeLHa1
                -7262. * CHB 
                +29887. * CHW 
                +7183. * CHWB 
                +4539. * CHD 
                +3925. * CHbox 
                +49603. * CHl1R11 
                +51583. * CHl3R11 
                -5918. * CHl3R22 
                -9. * CHeR11 
                +5897. * CllR1221              
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.024424; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +15200.9 * CHB 
                +1794.68 * CHW 
                +9134.34 * CHWB 
                -5883.35 * CHD 
                +2944.13 * CHbox 
                -2967.46 * CHl1R11 
                -1479.3 * CHl3R11 
                -4437.99 * CHl3R22 
                -49809.1 * CHeR11 
                +4461.27 * CllR1221              
                );
        
        sigmaSMeRHa1 = 0.021221; 
 
        sigmaeRHa1 = cWsch * (sigmaSMeRHa1
                +13253. * CHB 
                +1527. * CHW 
                +7972. * CHWB 
                -5113.4 * CHD 
                +2577. * CHbox 
                -2574.3 * CHl1R11 
                -1286. * CHl3R11 
                -3855.1 * CHl3R22 
                -43275. * CHeR11 
                +3856. * CllR1221               
                );
 
    } else if (sqrt_s == 0.350) {
 
        C1 = 0.0062;
 
        // e+ e- > H ve ve - e+ e- > H Z, Z > ve ve
        // LH -------------------------------
        sigmaSMeLHa0 = 0.134698; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -4610.61 * CHB 
                +13131.4 * CHW 
                +3271.33 * CHWB 
                -1426.48 * CHD 
                +16256.3 * CHbox 
                +52474.1 * CHl1R11 
                +5236.32 * CHl3R11 
                -24479. * CHl3R22 
                -79.73 * CHeR11 
                +24584.9 * CllR1221 
                );
        
        sigmaSMeLHa1 = 0.017502; 
 
        sigmaeLHa1 = cWsch * (sigmaSMeLHa1
                -6067.4 * CHB 
                +22837.2 * CHW 
                +3670.2 * CHWB 
                +2444.5 * CHD 
                +2120.8 * CHbox 
                +54404.2 * CHl1R11 
                +55470.2 * CHl3R11 
                -3184. * CHl3R22 
                -2.7 * CHeR11 
                +3180.2 * CllR1221              
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.013416; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +12262.3 * CHB 
                +674.27 * CHW 
                +8562.69 * CHWB 
                -3239.42 * CHD 
                +1628.99 * CHbox 
                -1664.92 * CHl1R11 
                -772.27 * CHl3R11 
                -2434.07 * CHl3R22 
                -53588.2 * CHeR11 
                +2433.13 * CllR1221               
                );
        
        sigmaSMeRHa1 = 0.011428; 
 
        sigmaeRHa1 = cWsch * (sigmaSMeRHa1
                +10380.3 * CHB 
                +578.1 * CHW 
                +7249.4 * CHWB 
                -2754.8 * CHD 
                +1382.8 * CHbox 
                -1386.5 * CHl1R11 
                -695.2 * CHl3R11 
                -2079.1 * CHl3R22 
                -45682.7 * CHeR11 
                +2080.1 * CllR1221              
                );
 
    } else if (sqrt_s == 0.365) {
 
        C1 = 0.00618352;
 
        // e+ e- > H ve ve - e+ e- > H Z, Z > ve ve
        // LH -------------------------------
        sigmaSMeLHa0 = 0.149505; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -4089.28 * CHB 
                +10219.8 * CHW 
                +2978.04 * CHWB 
                -2089.33 * CHD 
                +18094.8 * CHbox 
                +51560.3 * CHl1R11 
                -3886.54 * CHl3R11 
                -27167.1 * CHl3R22 
                +40.4 * CHeR11 
                +27244.9 * CllR1221 
                );
        
        sigmaSMeLHa1 = 0.015907; 
 
        sigmaeLHa1 = cWsch * (sigmaSMeLHa1
                -5736.2 * CHB 
                +21442.2 * CHW 
                +3310.6 * CHWB 
                +2221. * CHD 
                +1927.1 * CHbox 
                +53940.2 * CHl1R11 
                +54912.2 * CHl3R11 
                -2892.8 * CHl3R22 
                -1.6 * CHeR11 
                +2891.4 * CllR1221              
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.012207; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +11547.6 * CHB 
                +589.54 * CHW 
                +8177.48 * CHWB 
                -2948.28 * CHD 
                +1481.42 * CHbox 
                -1521.36 * CHl1R11 
                -701.48 * CHl3R11 
                -2218.87 * CHl3R22 
                -53022.9 * CHeR11 
                +2214.52 * CllR1221               
                );
        
        sigmaSMeRHa1 = 0.010386; 
 
        sigmaeRHa1 = cWsch * (sigmaSMeRHa1
                +9767.4 * CHB 
                +498.7 * CHW 
                +6888.4 * CHWB 
                -2501.9 * CHD 
                +1260.2 * CHbox 
                -1260.4 * CHl1R11 
                -632. * CHl3R11 
                -1889.5 * CHl3R22 
                -45151.6 * CHeR11 
                +1891.8 * CllR1221               
                );
 
    } else if (sqrt_s == 0.380) {
 
        C1 = 0.0062;
 
        // e+ e- > H ve ve - e+ e- > H Z, Z > ve ve
        // LH -------------------------------
        sigmaSMeLHa0 = 0.165164; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -3620.09 * CHB 
                +7262.01 * CHW 
                +2533.79 * CHWB 
                -2795.85 * CHD 
                +19930.1 * CHbox 
                +50455.6 * CHl1R11 
                -13297.1 * CHl3R11 
                -30129. * CHl3R22 
                -75.41 * CHeR11 
                +29935.6 * CllR1221
                );
        
        sigmaSMeLHa1 = 0.014504; 
 
        sigmaeLHa1 = cWsch * (sigmaSMeLHa1
                -5414.8 * CHB 
                +20137. * CHW 
                +3002.5 * CHWB 
                +2029.9 * CHD 
                +1760.6 * CHbox 
                +53470. * CHl1R11 
                +54342. * CHl3R11 
                -2636.3 * CHl3R22 
                +2.7 * CHeR11 
                +2640.2 * CllR1221              
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.011137; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +10870.8 * CHB 
                +511.27 * CHW 
                +7767.56 * CHWB 
                -2692.87 * CHD 
                +1349.76 * CHbox 
                -1394.99 * CHl1R11 
                -634.74 * CHl3R11 
                -2023.82 * CHl3R22 
                -52450.2 * CHeR11 
                +2030.93 * CllR1221              
                );
        
        sigmaSMeRHa1 = 0.009472; 
 
        sigmaeRHa1 = cWsch * (sigmaSMeRHa1
                +9181.6 * CHB 
                +430.1 * CHW 
                +6529.6 * CHWB 
                -2282.2 * CHD 
                +1147.4 * CHbox 
                -1151. * CHl1R11 
                -575.8 * CHl3R11 
                -1722.9 * CHl3R22 
                -44623.5 * CHeR11 
                +1726.7 * CllR1221              
                );
 
    } else if (sqrt_s == 0.500) {
 
        C1 = 0.0061;
 
        // e+ e- > H ve ve - e+ e- > H Z, Z > ve ve
        // LH -------------------------------
        sigmaSMeLHa0 = 0.302866; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -401.42 * CHB 
                -11755. * CHW 
                +877.96 * CHWB 
                -8221.05 * CHD 
                +36140. * CHbox 
                +45149.8 * CHl1R11 
                -95968.7 * CHl3R11 
                -55410.3 * CHl3R22 
                -243.04 * CHeR11 
                +54805.9 * CllR1221 
                );
        
        sigmaSMeLHa1 = 0.00776; 
 
        sigmaeLHa1 = cWsch * (sigmaSMeLHa1
                -3477.5 * CHB 
                +12550.9 * CHW 
                +1542.9 * CHWB 
                +1083.3 * CHD 
                +941.7 * CHbox 
                +50229.9 * CHl1R11 
                +50669.9 * CHl3R11 
                -1411.6 * CHl3R22 
                -0.7 * CHeR11 
                +1411. * CllR1221               
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.005968; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +6902.97 * CHB 
                +180.91 * CHW 
                +5139.82 * CHWB 
                -1436.97 * CHD 
                +722.43 * CHbox 
                -752.583 * CHl1R11 
                -332.172 * CHl3R11 
                -1083.6 * CHl3R22 
                -48701.4 * CHeR11 
                +1087.27 * CllR1221               
                );
        
        sigmaSMeRHa1 = 0.005067; 
 
        sigmaeRHa1 = cWsch * (sigmaSMeRHa1
                +5773.6 * CHB 
                +153.1 * CHW 
                +4277.7 * CHWB 
                -1220.2 * CHD 
                +614.4 * CHbox 
                -614.8 * CHl1R11 
                -307.7 * CHl3R11 
                -921.5 * CHl3R22 
                -41341.8 * CHeR11 
                +923.7 * CllR1221               
                );
 
    } else if (sqrt_s == 0.550) {
 
        C1 = 0.0061;
 
        // e+ e- > H ve ve - e+ e- > H Z, Z > ve ve
        // LH -------------------------------
        sigmaSMeLHa0 = 0.362269; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                +373.85 * CHB 
                -17839.8 * CHW 
                +734.48 * CHWB 
                -9923.28 * CHD 
                +43743. * CHbox 
                +44063.1 * CHl1R11 
                -132983. * CHl3R11 
                -65946.9 * CHl3R22 
                +152.15 * CHeR11 
                +66262.6 * CllR1221 
                );
        
        sigmaSMeLHa1 = 0.006271; 
 
        sigmaeLHa1 = cWsch * (sigmaSMeLHa1
                -2939. * CHB 
                +10537.5 * CHW 
                +1232.7 * CHWB 
                +876. * CHD 
                +761.8 * CHbox 
                +49277.3 * CHl1R11 
                +49629.3 * CHl3R11 
                -1139.8 * CHl3R22 
                -0.2 * CHeR11 
                +1140.9 * CllR1221              
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.004825; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +5824.16 * CHB 
                +125.188 * CHW 
                +4375.17 * CHWB 
                -1164.22 * CHD 
                +579.62 * CHbox 
                -613.231 * CHl1R11 
                -265.447 * CHl3R11 
                -877.103 * CHl3R22 
                -47624.2 * CHeR11 
                +876.017 * CllR1221              
                );
        
        sigmaSMeRHa1 = 0.004095; 
 
        sigmaeRHa1 = cWsch * (sigmaSMeRHa1
                +4857.9 * CHB 
                +105.3 * CHW 
                +3628.7 * CHWB 
                -986.7 * CHD 
                +497.2 * CHbox 
                -496.9 * CHl1R11 
                -248.5 * CHl3R11 
                -744.8 * CHl3R22 
                -40427.9 * CHeR11 
                +745.8 * CllR1221              
                );
 
    } else if (sqrt_s == 1.0) {
 
        C1 = 0.0059;
 
        // e+ e- > H ve ve - e+ e- > H Z, Z > ve ve
        // LH -------------------------------
        sigmaSMeLHa0 = 0.840445; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                +1799.69 * CHB 
                -46969.5 * CHW 
                +104.525 * CHWB 
                -25193.7 * CHD 
                +101623. * CHbox 
                +42181.4 * CHl1R11 
                -477637. * CHl3R11 
                -153174. * CHl3R22 
                -72.821 * CHeR11 
                +152853. * CllR1221
                );
        
        sigmaSMeLHa1 = 0.001741; 
 
        sigmaeLHa1 = cWsch * (sigmaSMeLHa1
                -952.62 * CHB 
                +3344.46 * CHW 
                +325.76 * CHWB 
                +243.3 * CHD 
                +211.6 * CHbox 
                +45697. * CHl1R11 
                +45787. * CHl3R11 
                -317.11 * CHl3R22 
                +0.04 * CHeR11 
                +317.06 * CllR1221              
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.001338; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +1883.78 * CHB 
                +12.31 * CHW 
                +1460.68 * CHWB 
                -322.405 * CHD 
                +162.126 * CHbox 
                -173.677 * CHl1R11 
                -69.869 * CHl3R11 
                -243.069 * CHl3R22 
                -43656.7 * CHeR11 
                +243.762 * CllR1221              
                );
        
        sigmaSMeRHa1 = 0.001137; 
 
        sigmaeRHa1 = cWsch * (sigmaSMeRHa1
                +1552.24 * CHB 
                +9.77 * CHW 
                +1192.24 * CHWB 
                -274. * CHD 
                +137.9 * CHbox 
                -138.09 * CHl1R11 
                -69.34 * CHl3R11 
                -207.12 * CHl3R22 
                -37101. * CHeR11 
                +207.27 * CllR1221              
                );
 
    } else if (sqrt_s == 1.4) {
 
        C1 = 0.0058;
 
        // e+ e- > H ve ve - e+ e- > H Z, Z > ve ve
        // LH -------------------------------
        sigmaSMeLHa0 = 1.16664; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                +1515.52 * CHB 
                -60139.2 * CHW 
                -313.042 * CHWB 
                -35595.8 * CHD 
                +140688. * CHbox 
                +44830.7 * CHl1R11 
                -760542. * CHl3R11 
                -212799. * CHl3R22 
                -216.739 * CHeR11 
                +212046. * CllR1221
                );
        
        sigmaSMeLHa1 = 0.00087; 
 
        sigmaeLHa1 = cWsch * (sigmaSMeLHa1
                -493.41 * CHB 
                +1722.63 * CHW 
                +160.89 * CHWB 
                +121.5 * CHD 
                +105.7 * CHbox 
                +44873.7 * CHl1R11 
                +44905.7 * CHl3R11 
                -158.44 * CHl3R22 
                +0.06 * CHeR11 
                +158.6 * CllR1221              
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.000668; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +978.328 * CHB 
                +2.9797 * CHW 
                +762.181 * CHWB 
                -161.445 * CHD 
                +80.9252 * CHbox 
                -87.7595 * CHl1R11 
                -34.4707 * CHl3R11 
                -121.863 * CHl3R22 
                -42733.6 * CHeR11 
                +121.358 * CllR1221              
                );
        
        sigmaSMeRHa1 = 0.000568; 
 
        sigmaeRHa1 = cWsch * (sigmaSMeRHa1
                +800.12 * CHB 
                +2.56 * CHW 
                +617.74 * CHWB 
                -137. * CHD 
                +69.04 * CHbox 
                -68.9 * CHl1R11 
                -34.69 * CHl3R11 
                -103.56 * CHl3R22 
                -36345.3 * CHeR11 
                +103.63 * CllR1221              
                );
 
    } else if (sqrt_s == 1.5) {
 
        C1 = 0.0058;
 
        // e+ e- > H ve ve - e+ e- > H Z, Z > ve ve
        // LH -------------------------------
        sigmaSMeLHa0 = 1.23716; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                +1360.69 * CHB 
                -62523.7 * CHW 
                -725.756 * CHWB 
                -37981.9 * CHD 
                +148772. * CHbox 
                +45105.6 * CHl1R11 
                -827326. * CHl3R11 
                -225838. * CHl3R22 
                -486.794 * CHeR11 
                +224000. * CllR1221 
                );
        
        sigmaSMeLHa1 = 0.000756; 
 
        sigmaeLHa1 = cWsch * (sigmaSMeLHa1
                -430.8 * CHB 
                +1501.77 * CHW 
                +139.53 * CHWB 
                +105.54 * CHD 
                +91.77 * CHbox 
                +44758. * CHl1R11 
                +44786. * CHl3R11 
                -137.66 * CHl3R22 
                +0.03 * CHeR11 
                +137.58 * CllR1221              
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.000581; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +854.12 * CHB 
                +2.2845 * CHW 
                +666.124 * CHWB 
                -140.103 * CHD 
                +70.3909 * CHbox 
                -76.2121 * CHl1R11 
                -29.8378 * CHl3R11 
                -105.842 * CHl3R22 
                -42598.1 * CHeR11 
                +105.12 * CllR1221              
                );
        
        sigmaSMeRHa1 = 0.000494; 
 
        sigmaeRHa1 = cWsch * (sigmaSMeRHa1
                +698.25 * CHB 
                +1.85 * CHW 
                +539.85 * CHWB 
                -119.02 * CHD 
                +59.95 * CHbox 
                -59.89 * CHl1R11 
                -30.15 * CHl3R11 
                -89.98 * CHl3R22 
                -36240.7 * CHeR11 
                +89.99 * CllR1221              
                );
 
    } else if (sqrt_s == 3.0) {
 
        C1 = 0.0057;
 
        // e+ e- > H ve ve - e+ e- > H Z, Z > ve ve
        // LH -------------------------------
        sigmaSMeLHa0 = 1.98635; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                +167.781 * CHB 
                -80364. * CHW 
                -1108.24 * CHWB 
                -61687.4 * CHD 
                +238369. * CHbox 
                +47553.5 * CHl1R11 
                -1654456. * CHl3R11 
                -363189. * CHl3R22 
                -1681.06 * CHeR11 
                +359731. * CllR1221
                );
        
        sigmaSMeLHa1 = 0.000186; 
 
        sigmaeLHa1 = cWsch * (sigmaSMeLHa1
                -108.342 * CHB 
                +378.008 * CHW 
                +34.078 * CHWB 
                +26.048 * CHD 
                +22.648 * CHbox 
                +44190.7 * CHl1R11 
                +44174.7 * CHl3R11 
                -33.916 * CHl3R22 
                +0.021 * CHeR11 
                +33.948 * CllR1221               
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.000143; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +217.438 * CHB 
                +0.099697 * CHW 
                +171.124 * CHWB 
                -34.49 * CHD 
                +17.3203 * CHbox 
                -18.9965 * CHl1R11 
                -7.08342 * CHl3R11 
                -26.059 * CHl3R22 
                -41954. * CHeR11 
                +25.932 * CllR1221              
                );
        
        sigmaSMeRHa1 = 0.000122; 
 
        sigmaeRHa1 = cWsch * (sigmaSMeRHa1
                +175.68 * CHB 
                +0.114 * CHW 
                +136.74 * CHWB 
                -29.295 * CHD 
                +14.797 * CHbox 
                -14.707 * CHl1R11 
                -7.394 * CHl3R11 
                -22.139 * CHl3R22 
                -35717.6 * CHeR11 
                +22.19 * CllR1221               
                );
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeHvv()");
    
    // Construct the signal strength
    // Total cross section
    mu = fLR * (sigmaeLHa0 - sigmaeLHa1) + fRL * (sigmaeRHa0 - sigmaeRHa1);
    // Normalize to SM
    mu = mu / (fLR * (sigmaSMeLHa0 - sigmaSMeLHa1) + fRL * (sigmaSMeRHa0 - sigmaSMeRHa1));
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += scalTH * eeeWBFint + eeeWBFpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mueettH()

const double NPSMEFTd6General::mueettH	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{eettH}$ between the $ e^{+}e^{-}\to t\bar{t} H $ production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eettH}$

Reimplemented from NPbase.

Definition at line 25119 of file NPSMEFTd6General.cpp.

                                                                                                          {
 
    //  Mw scheme
 
    double mu = 1.0;
 
    double C1 = 0.0;
 
    // Wilson coefficients and scale    
    double CuHR33 = 0.0, CuWR33 = 0.0, CuBR33 = 0.0, CHq1R33 = 0.0, CHq3R33 = 0.0, CHuR33 = 0.0;
    double CHB = 0.0, CHW = 0.0, CHWB = 0.0, CHD = 0.0, CHbox = 0.0, CHl1R11 = 0.0;
    double CHl3R11 = 0.0, CHl3R22 = 0.0, CHeR11 = 0.0, CllR1221 = 0.0, Clq1R1133 = 0.0;
    double Clq3R1133 = 0.0, CeuR1133 = 0.0, CluR1133 = 0.0, CqeR3311 = 0.0; 
    double muRG = 0;
    
    // Polarization factors
    double Pe = Pol_em, Pp = Pol_ep;
    double fLR, fRL;
 
    // LH and RH cross sections    
    double sigmaSMeLHa0 = 0.0, sigmaeLHa0 = 0.0; 
    double sigmaSMeRHa0 = 0.0, sigmaeRHa0 = 0.0;
    
    // -------------------------------------------------------------------------
 
    fLR = 0.25 * (1.0 - Pe) * (1.0 + Pp);
    fRL = 0.25 * (1.0 + Pe) * (1.0 - Pp);
    
    // RG scale in GeV
    muRG = 1000. * sqrt_s;
    
//  Wilson coefficients definitions 
    CuHR33 = getSMEFTCoeff("CuHR",2,2, muRG); 
    CuWR33 = getSMEFTCoeff("CuWR",2,2, muRG); 
    CuBR33 = getSMEFTCoeff("CuBR",2,2, muRG); 
    CHq1R33 = getSMEFTCoeff("CHq1R",2,2, muRG); 
    CHq3R33 = getSMEFTCoeff("CHq3R",2,2, muRG); 
    CHuR33 = getSMEFTCoeff("CHuR",2,2, muRG); 
    CHB = getSMEFTCoeff("CHB", muRG); 
    CHW = getSMEFTCoeff("CHW", muRG); 
    CHWB = getSMEFTCoeff("CHWB", muRG); 
    CHD = getSMEFTCoeff("CHD", muRG); 
    CHbox = getSMEFTCoeff("CHbox", muRG); 
    CHl1R11 = getSMEFTCoeff("CHl1R",0,0, muRG); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CHeR11 = getSMEFTCoeff("CHeR",0,0, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG); 
    Clq1R1133 = getSMEFTCoeff("Clq1R",0,0,2,2, muRG); 
    Clq3R1133 = getSMEFTCoeff("Clq3R",0,0,2,2, muRG); 
    CeuR1133 = getSMEFTCoeff("CeuR",0,0,2,2, muRG); 
    CluR1133 = getSMEFTCoeff("CluR",0,0,2,2, muRG); 
    CqeR3311 = getSMEFTCoeff("CqeR",2,2,0,0, muRG); 
    
    if (sqrt_s == 0.500) {
 
        C1 = 0.086;
 
        // LH -------------------------------
        sigmaSMeLHa0 = 0.000784; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0 
                -94.6115 * CuHR33 
                -1581.75 * CuWR33 
                -790.825 * CuBR33 
                -87.3955 * ( CHq1R33 - CHq3R33 )
                -84.292 * CHuR33 
                +63.829 * CHB 
                +150.202 * CHW 
                -293.781 * CHWB 
                -83.906 * CHD 
                +95.054 * CHbox 
                +99.373 * CHl1R11 
                -43.164 * CHl3R11 
                -142.68 * CHl3R22 
                +142.748 * CllR1221 
                -2460.16 * ( Clq1R1133 - Clq3R1133 ) 
                -2382.75 * CluR1133 
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.000306;
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0 
                -37.8182 * CuHR33 
                +27.0195 * CuWR33 
                -1035.38 * CuBR33 
                +42.106 * ( CHq1R33 - CHq3R33 )
                +44.175 * CHuR33 
                +84.692 * CHB 
                -1.403 * CHW 
                -229.508 * CHWB 
                -94.7248 * CHD 
                +37.112 * CHbox 
                -55.6873 * ( CHl3R11 + CHl3R22) 
                +47.609 * CHeR11 
                +55.67 * CllR1221 
                -1539.26 * CeuR1133 
                -1477.11 * CqeR3311              
                );
 
    } else if (sqrt_s == 0.550) {
 
        C1 = 0.086;
 
        // LH -------------------------------
        sigmaSMeLHa0 = 0.00312;
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0 
                -375.082 * CuHR33 
                -6978.68 * CuWR33 
                -3521.69 * CuBR33 
                -375.113 * ( CHq1R33 - CHq3R33 )
                -340.953 * CHuR33 
                +296.59 * CHB 
                +724.94 * CHW 
                -1223.44 * CHWB 
                -325.65 * CHD 
                +378.62 * CHbox 
                +534.61 * CHl1R11 
                -33.44 * CHl3R11 
                -567.338 * CHl3R22 
                +568.13 * CllR1221 
                -11968.1 * ( Clq1R1133 - Clq3R1133 ) 
                -11012.9 * CluR1133 
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.001237; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0 
                -151.896 * CuHR33 
                +104.147 * CuWR33 
                -4593.11 * CuBR33 
                +169.25 * ( CHq1R33 - CHq3R33 )
                +191.77 * CHuR33 
                +409.723 * CHB 
                -4.921 * CHW 
                -935.687 * CHWB 
                -381.661 * CHD 
                +150.086 * CHbox 
                -225.071 * ( CHl3R11 + CHl3R22) 
                +135.045 * CHeR11 
                +224.993 * CllR1221 
                -7563.24 * CeuR1133 
                -6791.07 * CqeR3311              
                );
 
    } else if (sqrt_s == 1.0) {
 
        C1 = 0.017;
 
        // LH -------------------------------
        sigmaSMeLHa0 = 0.005628; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0 
                -652.48 * CuHR33 
                -22912.9 * CuWR33 
                -12009.3 * CuBR33 
                -1002.82 * ( CHq1R33 - CHq3R33 )
                -650.53 * CHuR33 
                +1020.05 * CHB 
                +3026.6 * CHW 
                -2900.7 * CHWB 
                -487.19 * CHD 
                +681.99 * CHbox 
                +7556. * CHl1R11 
                +6526. * CHl3R11 
                -1024.23 * CHl3R22 
                +1024.69 * CllR1221 
                -74003.6 * ( Clq1R1133 - Clq3R1133 ) 
                -49960.2 * CluR1133 
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.002438; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0 
                -280.708 * CuHR33 
                +133.165 * CuWR33 
                -15458.3 * CuBR33 
                +306.64 * ( CHq1R33 - CHq3R33 )
                +537.89 * CHuR33 
                +1726.87 * CHB 
                -4.75 * CHW 
                -1901.18 * CHWB 
                -734.793 * CHD 
                +294.43 * CHbox 
                -443.534 * ( CHl3R11 + CHl3R22) 
                -4293.44 * CHeR11 
                +444. * CllR1221 
                -49006.1 * CeuR1133 
                -29616.4 * CqeR3311             
                );
 
    } else if (sqrt_s == 1.4) {
 
        C1 = 0.0094;
 
        // LH -------------------------------
        sigmaSMeLHa0 = 0.003663; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0 
                -413. * CuHR33 
                -20698.3 * CuWR33 
                -10960.3 * CuBR33 
                -765.64 * ( CHq1R33 - CHq3R33 ) 
                -431.605 * CHuR33 
                +846.79 * CHB 
                +2683.29 * CHW 
                -2175.52 * CHWB 
                -279.16 * CHD 
                +444.75 * CHbox 
                +14191.2 * CHl1R11 
                +13535.2 * CHl3R11 
                -664.85 * CHl3R22 
                +667.9 * CllR1221 
                -94432.1 * ( Clq1R1133 - Clq3R1133 ) 
                -55175.6 * CluR1133 
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.001649; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0 
                -181.837 * CuHR33 
                +67.2705 * CuWR33 
                -14087.6 * CuBR33 
                +197.955 * ( CHq1R33 - CHq3R33 ) 
                +416.786 * CHuR33 
                +1532.01 * CHB 
                -1.81 * CHW 
                -1307.84 * CHWB 
                -491.203 * CHD 
                +199.446 * CHbox 
                -299.647 * ( CHl3R11 + CHl3R22) 
                -9958.86 * CHeR11 
                +300.578 * CllR1221 
                -63614.1 * CeuR1133 
                -31936.4 * CqeR3311           
                );
 
    } else if (sqrt_s == 1.5) {
 
        C1 = 0.0094; // Use the same as 1400 GeV
 
        // LH -------------------------------
        sigmaSMeLHa0 = 0.003313; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0 
                -371.685 * CuHR33 
                -20045. * CuWR33 
                -10630.9 * CuBR33 
                -711.73 * ( CHq1R33 - CHq3R33 )
                -392.08 * CHuR33 
                +798.31 * CHB 
                +2557.11 * CHW 
                -2021.37 * CHWB 
                -246.88 * CHD 
                +401.08 * CHbox 
                +15729.7 * CHl1R11 
                +15133.9 * CHl3R11 
                -601.68 * CHl3R22 
                +603.39 * CllR1221 
                -97906.7 * ( Clq1R1133 - Clq3R1133 ) 
                -55732.7 * CluR1133 
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.001501; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0 
                -163.958 * CuHR33 
                +57.7855 * CuWR33 
                -13659.5 * CuBR33 
                +178.697 * ( CHq1R33 - CHq3R33 ) 
                +388.327 * CHuR33 
                +1461.23 * CHB 
                -1.005 * CHW 
                -1194.73 * CHWB 
                -445.862 * CHD 
                +181.946 * CHbox 
                -272.889 * ( CHl3R11 + CHl3R22) 
                -11285.9 * CHeR11 
                +273.7 * CllR1221 
                -66137.7 * CeuR1133 
                -32099.6 * CqeR3311             
                );
 
    } else if (sqrt_s == 3.0) {
 
        C1 = 0.0037;
 
        // LH -------------------------------
        sigmaSMeLHa0 = 0.001106; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0 
                -117.72 * CuHR33 
                -14308.7 * CuWR33 
                -7652.82 * CuBR33 
                -289.029 * ( CHq1R33 - CHq3R33 ) 
                -134.343 * CHuR33 
                +367.915 * CHB 
                +1265.49 * CHW 
                -847.142 * CHWB 
                -64.809 * CHD 
                +133.468 * CHbox 
                +33390.9 * CHl1R11 
                +33205.9 * CHl3R11 
                -201.282 * CHl3R22 
                +201.678 * CllR1221 
                -127854. * ( Clq1R1133 - Clq3R1133 ) 
                -59903. * CluR1133 
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.000527; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0 
                -53.268 * CuHR33 
                +11.318 * CuWR33 
                -9862.85 * CuBR33 
                +58.6365 * ( CHq1R33 - CHq3R33 ) 
                +159.909 * CHuR33 
                +723.378 * CHB 
                -0.326 * CHW 
                -436.909 * CHWB 
                -153.732 * CHD 
                +63.687 * CHbox 
                -95.841 * ( CHl3R11 + CHl3R22) 
                -26314.6 * CHeR11 
                +96.186 * CllR1221 
                -87964.5 * CeuR1133 
                -33133.1 * CqeR3311 
                );
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mueettH()");
    
    // Construct the signal strength
    // Total cross section
    mu = fLR * (sigmaeLHa0) + fRL * (sigmaeRHa0);
    // Normalize to SM
    mu = mu / (fLR * (sigmaSMeLHa0) + fRL * (sigmaSMeRHa0));
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eeettHint + eeettHpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mueeWBF()

const double NPSMEFTd6General::mueeWBF	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{eeWBF}$ between the $ e^{+}e^{-}\to \nu\bar{\nu} H $ production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eeWBF}$

Reimplemented from NPbase.

Definition at line 20432 of file NPSMEFTd6General.cpp.

                                                                                                          {
 
    //  Mw scheme
 
    double mu = 1.0;
 
    double C1 = 0.0;
    
    double CHW = 0.0, CHWB = 0.0, CHD = 0.0, CHbox = 0.0, CHl3R11 = 0.0, CHl3R22 = 0.0, CllR1221 = 0.0;
    double muRG = 0;
    
    double scalTH = 1.0;
    
    if ( sqrt_s > 0.5 ) {
        // Theory uncert. scaling like log^2(E/MW)
        
        scalTH = log(sqrt_s/0.080365)/log(0.5/0.080365);
        scalTH = scalTH * scalTH;
    }
    
    // RG scale in GeV
    muRG = 1000. * sqrt_s;
    
    //  Wilson coefficients definitions 
    CHW = getSMEFTCoeff("CHW", muRG); 
    CHWB = getSMEFTCoeff("CHWB", muRG); 
    CHD = getSMEFTCoeff("CHD", muRG); 
    CHbox = getSMEFTCoeff("CHbox", muRG); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG);
        
    //  Pure WBF, hence only initiated by LH fermions. No difference between polarizations at the linear level.
    //  Expand like other functions when quadratic terms are included
    
 
    if (sqrt_s == 0.230) {
 
        C1 = 0.00639683;
 
        mu += cWsch * (
                -22678.4 * CHW 
                -403.784 * CHWB 
                -30227.6 * CHD 
                +120870. * CHbox 
                -307776. * CHl3R11 
                -182383. * CHl3R22 
                +181458. * CllR1221 
                );
 
 
    } else if (sqrt_s == 0.240) {
 
        C1 = 0.00639683;
 
        mu += cWsch * (
                -24480.4 * CHW 
                -420.775 * CHWB 
                -30228.3 * CHD 
                +120890. * CHbox 
                -316741. * CHl3R11 
                -182335. * CHl3R22 
                +181564. * CllR1221 
                );
 
 
    } else if (sqrt_s == 0.250) {
 
        C1 = 0.0064;
 
        mu += cWsch * (
                -26656.2 * CHW 
                -536.424 * CHWB 
                -30398.4 * CHD 
                +120546. * CHbox 
                -325556. * CHl3R11 
                -182521. * CHl3R22 
                +181327. * CllR1221 
                );
 
 
    } else if (sqrt_s == 0.350) {
 
        C1 = 0.0062;
 
        mu += cWsch * (
                -39530.3 * CHW 
                -646.027 * CHWB 
                -30240.6 * CHD 
                +120881. * CHbox 
                -396701. * CHl3R11 
                -182400. * CHl3R22 
                +181394. * CllR1221 
                );
 
 
    } else if (sqrt_s == 0.365) {
 
        C1 = 0.00618352;
 
        mu += cWsch * (
                -40796.6 * CHW 
                -626.864 * CHWB 
                -30507.4 * CHD 
                +120603. * CHbox 
                -405380. * CHl3R11 
                -182353. * CHl3R22 
                +181575. * CllR1221
                );
 
 
    } else if (sqrt_s == 0.380) {
 
        C1 = 0.0062; // Use the same as 350 GeV
 
        mu += cWsch * (
                -41677.4 * CHW 
                -456.017 * CHWB 
                -30347.6 * CHD 
                +120703. * CHbox 
                -413858. * CHl3R11 
                -182188. * CHl3R22 
                +181341. * CllR1221 
                );
 
    } else if (sqrt_s == 0.500) {
 
        C1 = 0.0061;
 
        mu += cWsch * (
                -47053.9 * CHW 
                -244.306 * CHWB 
                -30283.9 * CHD 
                +121058. * CHbox 
                -471403. * CHl3R11 
                -181871. * CHl3R22 
                +181700. * CllR1221
                );
 
 
    } else if (sqrt_s == 0.550) {
 
        C1 = 0.0061;
 
        mu += cWsch * (
                -48186.2 * CHW 
                -331.282 * CHWB 
                -30408.3 * CHD 
                +121124. * CHbox 
                -491380. * CHl3R11 
                -181977. * CHl3R22 
                +181701. * CllR1221 
                );
 
 
    } else if (sqrt_s == 1.0) {
 
        C1 = 0.0059;
 
        mu += cWsch * (
                -49488.8 * CHW 
                -166.83 * CHWB 
                -30446.4 * CHD 
                +121190. * CHbox 
                -617416. * CHl3R11 
                -182202. * CHl3R22 
                +181511. * CllR1221 
                );
 
 
    } else if (sqrt_s == 1.4) {
 
        C1 = 0.0058;
 
        mu += cWsch * (
                -46762. * CHW 
                -145.836 * CHWB 
                -30411.2 * CHD 
                +121259. * CHbox 
                -689513. * CHl3R11 
                -182210. * CHl3R22 
                +181661. * CllR1221 
                );
 
 
    } else if (sqrt_s == 1.5) {
 
        mu += cWsch * (
                -46321.6 * CHW 
                -315.498 * CHWB 
                -30490.1 * CHD 
                +121143. * CHbox 
                -704469. * CHl3R11 
                -182156. * CHl3R22 
                +181112. * CllR1221 
                );
 
    } else if (sqrt_s == 3.0) {
 
        C1 = 0.0057;
 
        mu += cWsch * (
                -38546. * CHW 
                -674.92 * CHWB 
                -30159.9 * CHD 
                +121148. * CHbox 
                -857367. * CHl3R11 
                -182782. * CHl3R22 
                +180763. * CllR1221 
                );
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeWBF()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += scalTH * eeeWBFint + eeeWBFpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mueeWW()

const double NPSMEFTd6General::mueeWW	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{eeWW}$ between the $ e^{+}e^{-}\to W^{+}W^{-} $ production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eeWW}$

Reimplemented from NPbase.

Definition at line 38794 of file NPSMEFTd6General.cpp.

                                                                                                         {
 
    //  Mw scheme
    
    double mu = 1.0;
 
    // Wilson coefficients and scale    
    double CW = 0.0, CHWB = 0.0, CHD = 0.0, CHl1R11 = 0.0, CHl3R11 = 0.0;
    double CHl3R22 = 0.0, CHeR11 = 0.0, CllR1221 = 0.0; 
    double muRG = 0;
    
    // Polarization factors
    double Pe = Pol_em, Pp = Pol_ep;
    double fLR, fRL;
 
    // LH and RH cross sections    
    double sigmaSMeLHa0 = 0.0, sigmaeLHa0 = 0.0; 
    double sigmaSMeRHa0 = 0.0, sigmaeRHa0 = 0.0;
    
    // -------------------------------------------------------------------------
    
    fLR = 0.25 * (1.0 - Pe) * (1.0 + Pp);
    fRL = 0.25 * (1.0 + Pe) * (1.0 - Pp);
    
    // RG scale in GeV
    muRG = 1000. * sqrt_s;
    
//  Wilson coefficients definitions 
    CW = getSMEFTCoeff("CW", muRG); 
    CHWB = getSMEFTCoeff("CHWB", muRG); 
    CHD = getSMEFTCoeff("CHD", muRG); 
    CHl1R11 = getSMEFTCoeff("CHl1R",0,0, muRG); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CHeR11 = getSMEFTCoeff("CHeR",0,0, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG);
 
    if (sqrt_s == 0.161) {
 
        // LH -------------------------------
        sigmaSMeLHa0 = 12.9284; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -70. * CW 
                +38. * CHWB 
                -80. * CHD 
                -1416. * CHl1R11 
                +1568661. * CHl3R11 
                -1567486. * CHl3R22 
                -1073. * CHeR11 
                +1567418. * CllR1221
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.00232; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +122.385 * CW 
                +235.258 * CHWB 
                -488.691 * CHD 
                -0.0333 * CHl1R11 
                -281.296 * CHl3R11 
                -281.292 * CHl3R22 
                -1960.29 * CHeR11 
                +281.274 * CllR1221             
                );
 
    } else if (sqrt_s == 0.230) {
 
        // LH -------------------------------
        sigmaSMeLHa0 = 70.5564; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -402730. * CW 
                +23840. * CHWB 
                -226360. * CHD 
                -1745010. * CHl1R11 
                +10098670. * CHl3R11 
                -8510260. * CHl3R22 
                +10640. * CHeR11 
                +8598300. * CllR1221 
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.684821; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +32771. * CW 
                +275222. * CHWB 
                -144266. * CHD 
                -22. * CHl1R11 
                -82975. * CHl3R11 
                -82897. * CHl3R22 
                -1181168. * CHeR11 
                +83185. * CllR1221             
                );
 
 
    } else if (sqrt_s == 0.240) {
 
        // LH -------------------------------
        sigmaSMeLHa0 = 67.9294; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -439450. * CW 
                +40210. * CHWB 
                -228100. * CHD 
                -1866240. * CHl1R11 
                +9886460. * CHl3R11 
                -8196200. * CHl3R22 
                +3050. * CHeR11 
                +8272340. * CllR1221
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.639986; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +29994. * CW 
                +284436. * CHWB 
                -134835. * CHD 
                +4. * CHl1R11 
                -77575. * CHl3R11 
                -77505. * CHl3R22 
                -1201943. * CHeR11 
                +77766. * CllR1221             
                );
 
 
    } else if (sqrt_s == 0.250) {
 
        // LH -------------------------------
        sigmaSMeLHa0 = 65.3108; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -449120. * CW 
                +71270. * CHWB 
                -205800. * CHD 
                -1957840. * CHl1R11 
                +9671820. * CHl3R11 
                -7877690. * CHl3R22 
                +6620. * CHeR11 
                +7962190. * CllR1221
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.593472; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +27185. * CW 
                +288498. * CHWB 
                -125062. * CHD 
                -81. * CHl1R11 
                -71945. * CHl3R11 
                -71972. * CHl3R22 
                -1209216. * CHeR11 
                +72007. * CllR1221             
                );
 
 
    } else if (sqrt_s == 0.350) {
 
        // LH -------------------------------
        sigmaSMeLHa0 = 44.8939; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -439960. * CW 
                +155590. * CHWB 
                -118280. * CHD 
                -2143580. * CHl1R11 
                +7481240. * CHl3R11 
                -5415950. * CHl3R22 
                +10980. * CHeR11 
                +5473930. * CllR1221 
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.267037; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +9564. * CW 
                +230676. * CHWB 
                -56256. * CHD 
                -18. * CHl1R11 
                -32398. * CHl3R11 
                -32368. * CHl3R22 
                -1066430. * CHeR11 
                +32444. * CllR1221             
                );
 
 
    } else if (sqrt_s == 0.365) {
 
        // LH -------------------------------
        sigmaSMeLHa0 = 42.6742; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -426720. * CW 
                +156580. * CHWB 
                -109180. * CHD 
                -2125940. * CHl1R11 
                +7206190. * CHl3R11 
                -5148260. * CHl3R22 
                +10850. * CHeR11 
                +5202890. * CllR1221
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.239761; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +8244. * CW 
                +218802. * CHWB 
                -50510. * CHD 
                -25. * CHl1R11 
                -29102. * CHl3R11 
                -29066. * CHl3R22 
                -1041291. * CHeR11 
                +29116. * CllR1221              
                );
 
 
    } else if (sqrt_s == 0.380) {
 
        // LH -------------------------------
        sigmaSMeLHa0 = 40.6204; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -409440. * CW 
                +156620. * CHWB 
                -100050. * CHD 
                -2107634. * CHl1R11 
                +6949930. * CHl3R11 
                -4899610. * CHl3R22 
                +10740. * CHeR11 
                +4954360. * CllR1221
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.216166; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +7126. * CW 
                +207337. * CHWB 
                -45542. * CHD 
                -22. * CHl1R11 
                -26233. * CHl3R11 
                -26217. * CHl3R22 
                -1017531. * CHeR11 
                +26219. * CllR1221             
                );
 
 
    } else if (sqrt_s == 0.500) {
 
        // LH -------------------------------
        sigmaSMeLHa0 = 28.5996; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -294100. * CW 
                +129650. * CHWB 
                -55880. * CHD 
                -1935741. * CHl1R11 
                +5364950. * CHl3R11 
                -3446370. * CHl3R22 
                +9900. * CHeR11 
                +3485060. * CllR1221 
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.107613; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +2564.6 * CW 
                +135799. * CHWB 
                -22683.7 * CHD 
                -4.9 * CHl1R11 
                -13070.6 * CHl3R11 
                -13060.2 * CHl3R22 
                -876943. * CHeR11 
                +13043.6 * CllR1221              
                );
 
 
    } else if (sqrt_s == 0.550) {
 
        // LH -------------------------------
        sigmaSMeLHa0 = 25.1749; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -256296. * CW 
                +118140. * CHWB 
                -44500. * CHD 
                -1867097. * CHl1R11 
                +4896910. * CHl3R11 
                -3031578. * CHl3R22 
                +10830. * CHeR11 
                +3069940. * CllR1221
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.08506; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +1776.7 * CW 
                +115390. * CHWB 
                -17929.8 * CHD 
                +1.1 * CHl1R11 
                -10331. * CHl3R11 
                -10328. * CHl3R22 
                -838703. * CHeR11 
                +10323.6 * CllR1221             
                );
 
 
    } else if (sqrt_s == 1.0) {
 
        // LH -------------------------------
        sigmaSMeLHa0 = 10.6999; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -92382. * CW 
                +49273. * CHWB 
                -10274. * CHD 
                -1580824. * CHl1R11 
                +2884383. * CHl3R11 
                -1285157. * CHl3R22 
                +7857. * CHeR11 
                +1307083. * CllR1221 
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.021453; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +165.5 * CW 
                +38090.4 * CHWB 
                -4524.6 * CHD 
                +0.5 * CHl1R11 
                -2607.1 * CHl3R11 
                -2604.3 * CHl3R22 
                -699201. * CHeR11 
                +2603. * CllR1221             
                );
 
 
    } else if (sqrt_s == 1.4) {
 
        // LH -------------------------------
        sigmaSMeLHa0 = 6.38565; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -48428. * CW 
                +26846. * CHWB 
                -5517. * CHD 
                -1503300. * CHl1R11 
                +2282510. * CHl3R11 
                -766437. * CHl3R22 
                +4723. * CHeR11 
                +779623. * CllR1221
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.010445; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +41.49 * CW 
                +19779.7 * CHWB 
                -2202.72 * CHD 
                +0.64 * CHl1R11 
                -1268.91 * CHl3R11 
                -1267.89 * CHl3R22 
                -667234. * CHeR11 
                +1268.68 * CllR1221             
                );
 
 
    } else if (sqrt_s == 1.5) {
 
        // LH -------------------------------
        sigmaSMeLHa0 = 5.73018; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -42573. * CW 
                +23444. * CHWB 
                -5270. * CHD 
                -1493406. * CHl1R11 
                +2191484. * CHl3R11 
                -688035. * CHl3R22 
                +4044. * CHeR11 
                +699633. * CllR1221
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.009039; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +31.06 * CW 
                +17271.3 * CHWB 
                -1905.96 * CHD 
                +0.61 * CHl1R11 
                -1097.86 * CHl3R11 
                -1097.06 * CHl3R22 
                -662888. * CHeR11 
                +1097.77 * CllR1221              
                );
 
 
    } else if (sqrt_s == 3.0) {
 
        // LH -------------------------------
        sigmaSMeLHa0 = 1.85913; 
 
        sigmaeLHa0 = cWsch * (sigmaSMeLHa0
                -11055.6 * CW 
                +6174.7 * CHWB 
                -1334.5 * CHD 
                -1437804. * CHl1R11 
                +1662016. * CHl3R11 
                -225638. * CHl3R22 
                -109.3 * CHeR11 
                +225706. * CllR1221
                );
        
        // RH -------------------------------
        sigmaSMeRHa0 = 0.002184; 
 
        sigmaeRHa0 = cWsch * (sigmaSMeRHa0
                +1.26 * CW 
                +4369.21 * CHWB 
                -460.56 * CHD 
                +0.24 * CHl1R11 
                -265.13 * CHl3R11 
                -265.06 * CHl3R22 
                -640592. * CHeR11 
                +265.16 * CllR1221             
                );
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeWW()");
    
    // Construct the signal strength
    // Total cross section
    mu = fLR * (sigmaeLHa0) + fRL * (sigmaeRHa0);
    // Normalize to SM
    mu = mu / (fLR * (sigmaSMeLHa0) + fRL * (sigmaSMeRHa0));
    
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eeeWWint;
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mueeZBF()

const double NPSMEFTd6General::mueeZBF	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{eeZBF}$ between the $ e^{+}e^{-}\to e^{+}e^{-} H $ production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eeZBF}$

Reimplemented from NPbase.

Definition at line 21537 of file NPSMEFTd6General.cpp.

                                                                                                          {
 
    //  Mw scheme
 
    double mu = 1.0;
 
    double C1 = 0.0;
 
    // Wilson coefficients and scale    
    double CHB = 0.0, CHW = 0.0, CHWB = 0.0, CHD = 0.0, CHbox = 0.0, CHl1R11 = 0.0;
    double CHl3R11 = 0.0, CHl3R22 = 0.0, CHeR11 = 0.0, CllR1221 = 0.0; 
    double muRG = 0;
 
    // Polarization factors
    double Pe = Pol_em, Pp = Pol_ep;
    double fLR, fRL, fLL, fRR;
    
    // LR, RL, LL, and RR cross sections    
    double sigmaSMeLRa0 = 0.0, sigmaeLRa0 = 0.0; 
    double sigmaSMeRLa0 = 0.0, sigmaeRLa0 = 0.0;
    
    double sigmaSMeLLa0 = 0.0, sigmaeLLa0 = 0.0; 
    double sigmaSMeRRa0 = 0.0, sigmaeRRa0 = 0.0;
    
    double scalTH = 1.0;
    
    // -------------------------------------------------------------------------
    
    if ( sqrt_s > 0.5 ) {
        // Theory uncert. scaling like log^2(E/MW)
        
        scalTH = log(sqrt_s/0.080365)/log(0.5/0.080365);
        scalTH = scalTH * scalTH;
    }
        
    fLR = 0.25 * (1.0 - Pe) * (1.0 + Pp);
    fRL = 0.25 * (1.0 + Pe) * (1.0 - Pp);
    fLL = 0.25 * (1.0 - Pe) * (1.0 - Pp);
    fRR = 0.25 * (1.0 + Pe) * (1.0 + Pp);
    
    // RG scale in GeV
    muRG = 1000. * sqrt_s;
    
//  Wilson coefficients definitions 
    CHB = getSMEFTCoeff("CHB", muRG); 
    CHW = getSMEFTCoeff("CHW", muRG); 
    CHWB = getSMEFTCoeff("CHWB", muRG); 
    CHD = getSMEFTCoeff("CHD", muRG); 
    CHbox = getSMEFTCoeff("CHbox", muRG); 
    CHl1R11 = getSMEFTCoeff("CHl1R",0,0, muRG); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CHeR11 = getSMEFTCoeff("CHeR",0,0, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG);
    
    // Computed as the pure between e+ e- > H e+ e- via ZBF, without any s-channel contribution
    
    if (sqrt_s == 0.500) {
 
        C1 = 0.0067;
        
        // e+ e- > H e+ e- 
        // LR -------------------------------
        sigmaSMeLRa0 = 0.010339; 
 
        sigmaeLRa0 = cWsch * (sigmaSMeLRa0
                -2455.7 * CHB 
                -2622.7 * CHW 
                +6297. * CHWB 
                +3208. * CHD 
                +1254. * CHbox 
                -4875.8 * CHl1R11 
                -6752.7 * CHl3R11 
                -1881.1 * CHl3R22 
                +4. * CHeR11 
                +1882. * CllR1221
                );
        
        
        // RL -------------------------------
        sigmaSMeRLa0 = 0.004408; 
 
        sigmaeRLa0 = cWsch * (sigmaSMeRLa0
                -3017.2 * CHB 
                -185. * CHW 
                -1260.4 * CHWB 
                -1990.9 * CHD 
                +534.2 * CHbox 
                +0.9 * CHl1R11 
                -800.6 * CHl3R11 
                -802.2 * CHl3R22 
                +2575.2 * CHeR11 
                +802.3 * CllR1221              
                );
                
        // LL -------------------------------
        sigmaSMeLLa0 = 0.006964; 
 
        sigmaeLLa0 = cWsch * (sigmaSMeLLa0
                +4723.4 * CHB 
                +1092.9 * CHW 
                -3439.1 * CHWB 
                -491.9 * CHD 
                +844.7 * CHbox 
                -1785.4 * CHl1R11 
                -3050.5 * CHl3R11 
                -1267. * CHl3R22 
                +2215.4 * CHeR11 
                +1267.4 * CllR1221
                );
        
 
        // RR -------------------------------
        sigmaSMeRRa0 = 0.006964; 
 
        sigmaeRRa0 = cWsch * (sigmaSMeRRa0
                +4723.4 * CHB 
                +1096.3 * CHW 
                -3435.1 * CHWB 
                -490.4 * CHD 
                +842.2 * CHbox 
                -1784.7 * CHl1R11 
                -3050.7 * CHl3R11 
                -1264.2 * CHl3R22 
                +2213.9 * CHeR11 
                +1267.4 * CllR1221             
                );
 
    } else if (sqrt_s == 0.550) {
 
        C1 = 0.0067;
 
        // e+ e- > H e+ e- 
        // LR -------------------------------
        sigmaSMeLRa0 = 0.012531; 
 
        sigmaeLRa0 = cWsch * (sigmaSMeLRa0
                -2846.7 * CHB 
                -3153.5 * CHW 
                +7554. * CHWB 
                +3888. * CHD 
                +1521. * CHbox 
                -6342.7 * CHl1R11 
                -8619.3 * CHl3R11 
                -2278. * CHl3R22 
                +5. * CHeR11 
                +2283. * CllR1221
                );
        
        
        // RL -------------------------------
        sigmaSMeRLa0 = 0.005342; 
 
        sigmaeRLa0 = cWsch * (sigmaSMeRLa0
                -3571.2 * CHB 
                -205.3 * CHW 
                -1576.1 * CHWB 
                -2412.8 * CHD 
                +648.3 * CHbox 
                +1.3 * CHl1R11 
                -969.9 * CHl3R11 
                -971.6 * CHl3R22 
                +3351.3 * CHeR11 
                +973.1 * CllR1221             
                );
                
        // LL -------------------------------
        sigmaSMeLLa0 = 0.008384; 
 
        sigmaeLLa0 = cWsch * (sigmaSMeLLa0
                +5195.9 * CHB 
                +1184.5 * CHW 
                -3839.5 * CHWB 
                -592.5 * CHD 
                +1017.3 * CHbox 
                -2276.4 * CHl1R11 
                -3799.1 * CHl3R11 
                -1525. * CHl3R22 
                +2823.9 * CHeR11 
                +1526.4 * CllR1221
                );
        
 
        // RR -------------------------------
        sigmaSMeRRa0 = 0.008384; 
 
        sigmaeRRa0 = cWsch * (sigmaSMeRRa0
                +5197.9 * CHB 
                +1188.1 * CHW 
                -3835.5 * CHWB 
                -592.5 * CHD 
                +1017.3 * CHbox 
                -2277.5 * CHl1R11 
                -3800.4 * CHl3R11 
                -1525. * CHl3R22 
                +2823.9 * CHeR11 
                +1526.4 * CllR1221             
                );
 
    } else if (sqrt_s == 1.0) {
 
        C1 = 0.0065;
 
        // e+ e- > H e+ e- 
        // LR -------------------------------
        sigmaSMeLRa0 = 0.030357; 
 
        sigmaeLRa0 = cWsch * (sigmaSMeLRa0
                -5227. * CHB 
                -6830. * CHW 
                +17024. * CHWB 
                +9420. * CHD 
                +3687. * CHbox 
                -22051.9 * CHl1R11 
                -27585.4 * CHl3R11 
                -5520. * CHl3R22 
                +13. * CHeR11 
                +5532. * CllR1221
                );
        
        
        // RL -------------------------------
        sigmaSMeRLa0 = 0.012942; 
 
        sigmaeRLa0 = cWsch * (sigmaSMeRLa0
                -7216. * CHB 
                -304. * CHW 
                -4417.7 * CHWB 
                -5844.6 * CHD 
                +1572. * CHbox 
                +5. * CHl1R11 
                -2348. * CHl3R11 
                -2353. * CHl3R22 
                +11654. * CHeR11 
                +2358. * CllR1221              
                );
                
        // LL -------------------------------
        sigmaSMeLLa0 = 0.019928; 
 
        sigmaeLLa0 = cWsch * (sigmaSMeLLa0
                +7750. * CHB 
                +1636. * CHW 
                -6201. * CHWB 
                -1408. * CHD 
                +2420. * CHbox 
                -7400. * CHl1R11 
                -11020.6 * CHl3R11 
                -3625. * CHl3R22 
                +9176. * CHeR11 
                +3630. * CllR1221
                );
        
 
        // RR -------------------------------
        sigmaSMeRRa0 = 0.019928; 
 
        sigmaeRRa0 = cWsch * (sigmaSMeRRa0
                +7753. * CHB 
                +1648. * CHW 
                -6189. * CHWB 
                -1408. * CHD 
                +2420. * CHbox 
                -7396. * CHl1R11 
                -11020.1 * CHl3R11 
                -3625. * CHl3R22 
                +9174. * CHeR11 
                +3630. * CllR1221             
                );
 
    } else if (sqrt_s == 1.4) {
 
        C1 = 0.0065;
 
        // e+ e- > H e+ e- 
        // LR -------------------------------
        sigmaSMeLRa0 = 0.042715; 
 
        sigmaeLRa0 = cWsch * (sigmaSMeLRa0
                -6315. * CHB 
                -8759. * CHW 
                +22966. * CHWB 
                +13250. * CHD 
                +5175. * CHbox 
                -36465.5 * CHl1R11 
                -44246.7 * CHl3R11 
                -7755. * CHl3R22 
                +1. * CHeR11 
                +7782. * CllR1221 
                );
        
        
        // RL -------------------------------
        sigmaSMeRLa0 = 0.01821; 
 
        sigmaeRLa0 = cWsch * (sigmaSMeRLa0
                 -9021.3 * CHB 
                -343. * CHW 
                -6557. * CHWB 
                -8224.3 * CHD 
                +2207. * CHbox 
                +5. * CHl1R11 
                -3305. * CHl3R11 
                -3312. * CHl3R22 
                +19259. * CHeR11 
                +3318. * CllR1221             
                );
                
        // LL -------------------------------
        sigmaSMeLLa0 = 0.027954; 
 
        sigmaeLLa0 = cWsch * (sigmaSMeLLa0
                +8794. * CHB 
                +1796. * CHW 
                -7333. * CHWB 
                -1976. * CHD 
                +3388. * CHbox 
                -12072. * CHl1R11 
                -17149. * CHl3R11 
                -5084. * CHl3R22 
                +14954. * CHeR11 
                +5093. * CllR1221
                );
        
 
        // RR -------------------------------
        sigmaSMeRRa0 = 0.027954; 
 
        sigmaeRRa0 = cWsch * (sigmaSMeRRa0
                +8802. * CHB 
                +1812. * CHW 
                -7315. * CHWB 
                -1976. * CHD 
                +3388. * CHbox 
                -12060. * CHl1R11 
                -17151. * CHl3R11 
                -5084. * CHl3R22 
                +14953. * CHeR11 
                +5093. * CllR1221              
                );
 
    } else if (sqrt_s == 1.5) {
 
        C1 = 0.0065; // Use the same as 1400 GeV
 
        // e+ e- > H e+ e- 
        // LR -------------------------------
        sigmaSMeLRa0 = 0.045391; 
 
        sigmaeLRa0 = cWsch * (sigmaSMeLRa0
                -6499. * CHB 
                -9111. * CHW 
                +24208. * CHWB 
                +14078. * CHD 
                +5504. * CHbox 
                -39948.6 * CHl1R11 
                -48214.3 * CHl3R11 
                -8238. * CHl3R22 
                +2. * CHeR11 
                +8271. * CllR1221 
                );
        
        
        // RL -------------------------------
        sigmaSMeRLa0 = 0.019352; 
 
        sigmaeRLa0 = cWsch * (sigmaSMeRLa0
                -9353.7 * CHB 
                -348. * CHW 
                -7033. * CHWB 
                -8741. * CHD 
                +2346. * CHbox 
                +5. * CHl1R11 
                -3513. * CHl3R11 
                -3520. * CHl3R22 
                +21099. * CHeR11 
                +3526. * CllR1221              
                );
                
        // LL -------------------------------
        sigmaSMeLLa0 = 0.029695; 
 
        sigmaeLLa0 = cWsch * (sigmaSMeLLa0
                +8978. * CHB 
                +1827. * CHW 
                -7544. * CHWB 
                -2101. * CHD 
                +3601. * CHbox 
                -13199. * CHl1R11 
                -18594. * CHl3R11 
                -5400. * CHl3R22 
                +16352. * CHeR11 
                +5411. * CllR1221
                );
        
 
        // RR -------------------------------
        sigmaSMeRRa0 = 0.029695; 
 
        sigmaeRRa0 = cWsch * (sigmaSMeRRa0
                +8983. * CHB 
                +1841. * CHW 
                -7521. * CHWB 
                -2101. * CHD 
                +3601. * CHbox 
                -13187. * CHl1R11 
                -18597. * CHl3R11 
                -5400. * CHl3R22 
                +16353. * CHeR11 
                +5411. * CllR1221              
                );
 
    } else if (sqrt_s == 3.0) {
 
        C1 = 0.0063;
 
        // e+ e- > H e+ e- 
        // LR -------------------------------
        sigmaSMeLRa0 = 0.074102; 
 
        sigmaeLRa0 = cWsch * (sigmaSMeLRa0
                -7921. * CHB 
                -11849. * CHW 
                +36688. * CHWB 
                +23012. * CHD 
                +8976. * CHbox 
                -85300. * CHl1R11 
                -98820. * CHl3R11 
                -13463. * CHl3R22 
                -3. * CHeR11 
                +13507. * CllR1221 
                );
        
        
        // RL -------------------------------
        sigmaSMeRLa0 = 0.031592; 
 
        sigmaeRLa0 = cWsch * (sigmaSMeRLa0
                -11864. * CHB 
                -380. * CHW 
                -12283. * CHWB 
                -14264. * CHD 
                +3826. * CHbox 
                +8. * CHl1R11 
                -5737. * CHl3R11 
                -5744. * CHl3R22 
                +45048. * CHeR11 
                +5759. * CllR1221             
                );
                
        // LL -------------------------------
        sigmaSMeLLa0 = 0.048401; 
 
        sigmaeLLa0 = cWsch * (sigmaSMeLLa0
                +10290. * CHB 
                +1982. * CHW 
                -9308. * CHWB 
                -3411. * CHD 
                +5863. * CHbox 
                -27936. * CHl1R11 
                -36729. * CHl3R11 
                -8799. * CHl3R22 
                +34596. * CHeR11 
                +8824. * CllR1221
                );
        
 
        // RR -------------------------------
        sigmaSMeRRa0 = 0.048401; 
 
        sigmaeRRa0 = cWsch * (sigmaSMeRRa0
                +10301. * CHB 
                +2016. * CHW 
                -9292. * CHWB 
                -3411. * CHD 
                +5863. * CHbox 
                -27914. * CHl1R11 
                -36742. * CHl3R11 
                -8799. * CHl3R22 
                +34591. * CHeR11 
                +8824. * CllR1221             
                );
        
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZBF()");
    
    // Construct the signal strength
    // Total cross section
    mu = fLR * (sigmaeLRa0) + fRL * (sigmaeRLa0) + fLL * (sigmaeLLa0) + fRR * (sigmaeRRa0);
    // Normalize to SM
    mu = mu / (fLR * (sigmaSMeLRa0) + fRL * (sigmaSMeRLa0) + fLL * (sigmaSMeLLa0) + fRR * (sigmaSMeRRa0));
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    //(Assume similar to WBF.)
    mu += scalTH * eeeWBFint + eeeWBFpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mueeZH()

const double NPSMEFTd6General::mueeZH	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{eeZH}$ between the $e^{+}e^{-}\to ZH$ associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eeZH}$

Reimplemented from NPbase.

Definition at line 23156 of file NPSMEFTd6General.cpp.

                                                                                                         {
 
    double mu = 1.0;
    
    double dmuLO = 0.0;
    double dmuNLO = 0.0;
    
    double xsSMLO, xsSMNLOW, xsSMNLO;   
    
//     SM NLO absolute cross sections: Weak and Weak+QED [fb] 
  
    double xsSMweakLH[7] = {507.646, 247.943, 118.768, 95.0014, 23.7511, 9.27339, 1.76382}; 
    double xsSMweakRH[7] = {420.667, 204.977, 100.773, 81.189, 21.5294, 8.92131, 1.98509}; 
    double xsSMNLOLH[7] = {416.118, 267.004, 138.711, 113.282, 32.1297, 13.8278, 3.28209}; 
    double xsSMNLORH[7] = {361.39, 217.322, 113.689, 93.0279, 26.9557, 11.8709, 2.96837};  
    
//     SM NLO absolute corrections: Weak and QED [fb] 
  
    double dSMWLH[7] = {-72.6944, -35.9317, -19.7524, -16.947, -7.33368, -4.2239, -1.56196}; 
    double dSMWRH[7] = {44.8204, 21.1311, 11.0627, 8.68772, 1.39796, 0.18004, -0.16879}; // SM weak corrections (LH and RH) 
    double dSMQEDLH[7] = {-91.5282, 19.0611, 19.943, 18.2803, 8.37861, 4.55443, 1.51827}; 
    double dSMQEDRH[7] = {-59.2764, 12.3445, 12.9157, 11.8389, 5.42624, 2.94959, 0.98328}; // SM QED corrections (LH and RH) 
    
    double tofb = 3.894e+11;  // Conversion of the cross section to fb
    
    double s,s2, MH2, MW2, MZ2, MH4, MW4, MZ4, MW6, MZ6, MW8, MZ8;
    
    // For LO corrections
    double CHDden, CHWden, CHWBden; // Independent denominators
    double Cllnum, CHl111num, CHe11num, CHl322num, CHBnum, CHWnum, CHWBnum, CHDnum, CHboxnum; // Independent Numerators
    double derSMMW;
    
    // For NLO corrections
    //double C1 = 0.0;
    
    // RG scale of the process
    double muRG;
    
    double Ch2f1 = 0.0, Ch2f2 = 0.0;
    double Ch4f1 = 0.0, Ch4f2 = 0.0, Ch4f3 = 0.0, Ch4f4 = 0.0, Ch4f5 = 0.0, Ch4f6 = 0.0;
 
    // Energy dependent corrections for each operator: LH and RH initial electrons
    // (To normalize with SM NLO weak cross section)
  
    double d6LHCHD[7] = {-0.04299, -0.00717, 0.0003, 0.00163, 0.00606, 0.01022, 0.05332}; 
    double d6RHCHD[7] = {0.02165, -0.01445, -0.02584, -0.02757, -0.03435, -0.04432, -0.11827}; 
    double d6LHCHbox[7] = {-0.03952, -0.01798, -0.01631, -0.01713, -0.03571, -0.06942, -0.25989}; 
    double d6RHCHbox[7] = {-0.00321, 0.01412, 0.01872, 0.01903, 0.01298, -0.00227, -0.09124}; 
    double d6LHCHW[7] = {-0.24126, -0.1175, -0.06842, -0.058, -0.03242, -0.04867, -0.14268}; 
    double d6RHCHW[7] = {-0.00247, 0.01106, 0.01143, 0.01143, 0.01258, 0.0146, 0.01977};
    double d6LHCHB[7] = {0.04791, 0.02058, 0.00773, 0.00519, 0.00422, 0.01953, 0.09224}; 
    double d6RHCHB[7] = {-0.0325, 0.08517, 0.15935, 0.17883, 0.28562, 0.35672, 0.50909}; 
    double d6LHCHWB[7] = {-0.05099, 0.00165, 0.01518, 0.01774, 0.02588, 0.02493, 0.00208}; 
    double d6RHCHWB[7] = {-0.03449, 0.02039, 0.0588, 0.06846, 0.1088, 0.12043, 0.11923}; 
    double d6LHCHeR00[7] = {-0.00009, -0.00092, -0.00237, -0.00306, -0.01351, -0.03546, -0.18968}; 
    double d6RHCHeR00[7] = {0.17601, -0.07965, -0.21354, -0.22168, 0.97615, 6.14511, 61.1339}; 
    double d6LHCHl1R00[7] = {-0.39382, -0.41129, -0.8309, -1.09036, -6.88023, -23.8012, -192.589}; 
    double d6RHCHl1R00[7] = {0.00058, 0.00231, 0.00509, 0.00638, 0.02476, 0.06022, 0.27243}; 
    double d6LHCHl3R00[7] = {-0.14027, -0.19375, -0.62064, -0.87823, -6.52212, -22.8349, -184.162}; 
    double d6RHCHl3R00[7] = {0.18109, 0.16306, 0.15559, 0.15557, 0.16567, 0.17859, 0.20946}; 
    double d6LHCHl3R11[7] = {0.28034, 0.25281, 0.24915, 0.24974, 0.25337, 0.22484, -0.17093}; 
    double d6RHCHl3R11[7] = {0.18109, 0.16306, 0.15559, 0.15557, 0.16567, 0.17859, 0.20946};
    double d6LHCh4f2[7] = {-0.14156, -0.12918, -0.13022, -0.13195, -0.15634, -0.19052, -0.33624}; 
    double d6RHCh4f2[7] = {-0.09048, -0.08082, -0.07661, -0.07645, -0.08047, -0.08612, -0.09991};
    double d6LHCHq1R22[7] = {-0.01375, -0.02132, -0.02865, -0.03052, -0.03723, -0.03024, 0.08402}; 
    double d6RHCHq1R22[7] = {0.01363, 0.0161, 0.02163, 0.02358, 0.02967, 0.01375, -0.1589}; 
    double d6LHCHq3R22[7] = {-0.00938, -0.01891, -0.03284, -0.04004, -0.15147, -0.3839, -2.00432}; 
    double d6RHCHq3R22[7] = {0.01243, 0.02378, 0.02671, 0.02714, 0.02844, 0.02928, 0.03188}; 
    double d6LHCHuR22[7] = {0.00905, 0.03414, 0.04831, 0.05243, 0.09079, 0.15022, 0.50155}; 
    double d6RHCHuR22[7] = {-0.01212, -0.02946, -0.04383, -0.04964, -0.11046, -0.20081, -0.66506};
    double d6LHCuWR22[7] = {-0.00743, 0.0175, 0.03761, 0.04127, 0.05212, 0.05502, 0.06255}; 
    double d6RHCuWR22[7] = {0.00626, -0.00756, -0.01194, -0.01231, -0.00949, -0.00524, 0.00327};
    double d6LHCuBR22[7] = {-0.00247, -0.01796, -0.01902, -0.01898, -0.01769, -0.01696, -0.01713}; 
    double d6RHCuBR22[7] = {0.00291, 0.01241, 0.00533, 0.00365, -0.004, -0.00766, -0.01347}; 
    double d6LHCuHR22[7] = {0.00013, -0.0019, -0.00168, -0.00139, 0.00188, 0.00511, 0.01316}; 
    double d6RHCuHR22[7] = {0.00055, -0.0001, -0.00099, -0.0009, 0.00123, 0.00333, 0.00751}; 
    double d6LHCh2f1[7] = {-0.00009, -0.00092, -0.00237, -0.00306, -0.01351, -0.03546, -0.18968}; 
    double d6RHCh2f1[7] = {0.00069, 0.00242, 0.0052, 0.00649, 0.02488, 0.06034, 0.27257}; 
    double d6LHCh2f2[7] = {-0.00218, -0.00553, -0.01095, -0.01348, -0.05085, -0.12824, -0.66818}; 
    double d6RHCh2f2[7] = {0.00002, 0.00007, 0.00012, 0.00013, 0.00025, 0.00034, 0.00054};
    double d6LHCHl1R11[7] = {-0.00023, -0.00107, -0.00252, -0.00321, -0.01367, -0.03564, -0.18992}; 
    double d6RHCHl1R11[7] = {0.00058, 0.00231, 0.00509, 0.00638, 0.02476, 0.06022, 0.27243};
    double d6LHCH[7] = {-0.00801, -0.00111, 0.00111, 0.00152, 0.00266, 0.00285, 0.00322}; 
    double d6RHCH[7] = {-0.00626, -0.00087, 0.00085, 0.00115, 0.0019, 0.00192, 0.00185};
    double d6LHCW[7] = {0.02991, 0.05402, 0.07139, 0.07651, 0.11131, 0.14851, 0.33599}; 
    double d6RHCW[7] = {-0.00007, -0.00127, -0.00186, -0.00199, -0.00239, -0.00241, -0.00226};
    double d6LHCeuR0022[7] = {0., 0., 0., 0., 0., 0., 0.}; 
    double d6RHCeuR0022[7] = {0.00003, -0.08231, -0.27679, -0.35687, -1.32756, -3.00171, -12.4065};
    double d6LHCluR0022[7] = {-0.00003, 0.08455, 0.29183, 0.37898, 1.49534, 3.58836, 17.3504}; 
    double d6RHCluR0022[7] = {0., 0., 0., 0., 0., 0., 0.}; 
    double d6LHCqeR2200[7] = {0., 0., 0., 0., 0., 0., 0.}; 
    double d6RHCqeR2200[7] = {0.00651, 0.10815, 0.2918, 0.37025, 1.34648, 3.05393, 12.7244};
    double d6LHClq1R0022[7] = {-0.00671, -0.1111, -0.30765, -0.39318, -1.51665, -3.65078, -17.795}; 
    double d6RHClq1R0022[7] = {0., 0., 0., 0., 0., 0., 0.}; 
    double d6LHClq3R0022[7] = {-0.00484, 0.08613, 0.26288, 0.33941, 1.33495, 3.21002, 15.567}; 
    double d6RHClq3R0022[7] = {-0.00235, -0.00406, -0.0053, -0.0057, -0.00851, -0.01072, -0.01528}; 
    double d6LHClq3R1122[7] = {-0.003, -0.00518, -0.00694, -0.00753, -0.01191, -0.01592, -0.02655}; 
    double d6RHClq3R1122[7] = {-0.00235, -0.00406, -0.0053, -0.0057, -0.00851, -0.01072, -0.01528};
    double d6LHCh4f1[7] = {0.00075, 0.00173, 0.0033, 0.00404, 0.01482, 0.03709, 0.19217}; 
    double d6RHCh4f1[7] = {0., 0., 0., 0., 0., 0., 0.}; 
    double d6LHCh4f3[7] = {-0.00151, -0.001, 0.00016, 0.00075, 0.01041, 0.0316, 0.18378}; 
    double d6RHCh4f3[7] = {-0.00176, -0.00214, -0.0024, -0.00249, -0.00315, -0.0037, -0.00483}; 
    double d6LHCh4f4[7] = {-0.00037, -0.00086, -0.00164, -0.00201, -0.00737, -0.01843, -0.09552}; 
    double d6RHCh4f4[7] = {0., 0., 0., 0., 0., 0., 0.}; 
    double d6LHCh4f5[7] = {0., 0., 0., 0., 0., 0., 0.}; 
    double d6RHCh4f5[7] = {-0.00072, -0.00168, -0.00313, -0.0038, -0.01316, -0.03102, -0.13741}; 
    double d6LHCh4f6[7] = {0., 0., 0., 0., 0., 0., 0.}; 
    double d6RHCh4f6[7] = {-0.00029, -0.00067, -0.00125, -0.00152, -0.00526, -0.01241, -0.05497}; 
    double d6LHCleR0000[7] = {0.00075, 0.00173, 0.0033, 0.00404, 0.01482, 0.03709, 0.19217}; 
    double d6RHCleR0000[7] = {-0.00072, -0.00168, -0.00313, -0.0038, -0.01316, -0.03102, -0.13741}; 
    double d6LHCllR0000[7] = {0.00075, 0.00174, 0.00332, 0.00406, 0.01491, 0.0373, 0.19331}; 
    double d6RHCllR0000[7] = {0., 0., 0., 0., 0., 0., 0.};
    double d6LHCeeR0000[7] = {0., 0., 0., 0., 0., 0., 0.}; 
    double d6RHCeeR0000[7] = {-0.00203, -0.00471, -0.00877, -0.01064, -0.03684, -0.08686, -0.38476};
//    double d6LHCHBt[3] = {0.00278, 0.00803, 0.0103};
//    double d6RHCHBt[3] = {0.00551, 0.014, 0.0259};
//    double d6LHCHWt[3] = {0.0226, 0.0788, 0.112};
//    double d6RHCHWt[3] = {0.0009, 0.00081, 0.00038};
//    double d6LHCHWBt[3] = {0.00473, 0.0125, 0.0192};
//    double d6RHCHWBt[3] = {0.00478, 0.018, 0.0349};
//    double d6LHCWt[3] = {0.00608, 0.0215, 0.0334};
//    double d6RHCWt[3] = {0.00013, 0.00058, 0.00124};
    
    double d6NLOLH = 0., d6NLORH = 0.; // SMEFT absolute NLO corrections (LH and RH)
    
    // Current input of observables is in TeV -> Translate sqrt_s to GeV before operating
    double sqrt_sGeV;
    
    // Polarization factors
    double Pe = Pol_em, Pp = Pol_ep;
    double fLR, fRL;
    
    fLR = 0.25 * (1.0 - Pe) * (1.0 + Pp);
    fRL = 0.25 * (1.0 + Pe) * (1.0 - Pp);
    
    sqrt_sGeV = 1000. * sqrt_s;
    
    muRG = sqrt_sGeV;
    
    // Base implementation in W mass scheme
    s = sqrt_sGeV * sqrt_sGeV;
    s2 = s * s;
    MH2 = mHl * mHl;
    MW2 = Mw_tree * Mw_tree;
    MZ2 = Mz * Mz;
    MH4 = MH2 * MH2;
    MW4 = MW2 * MW2;
    MZ4 = MZ2 * MZ2;
    MW6 = MW4 * MW2;
    MZ6 = MZ4 * MZ2;
    MW8 = MW4 * MW4;
    MZ8 = MZ4 * MZ4;
    
    // SM cross section at LO
    xsSMLO = - GF*GF * (8.0 * MW4 * (-1.0 + Pe * Pp) - 4.0 * MW2 * MZ2 * (-3.0 + Pp + Pe * (-1.0 + 3.0 * Pp)) 
            + MZ4 * (-5.0 + 3.0 * Pp + Pe * (-3.0 + 5.0 * Pp))) * sqrt( MH4 + (MZ2 - s) * (MZ2 - s) - 2.0 * MH2 * (MZ2 + s) ) * (MH4 + MZ4 + 10.0 * MZ2 * s + s2 - 2.0 * MH2 * (MZ2 + s));
    
    xsSMLO = xsSMLO/( 48.0 * M_PI * (MZ2 - s) * (MZ2 - s) * s2 );
    
    // Independent denominators of the LO dimension-6 contrib.
    CHDden = GF * (8.0 * MW8 * MZ4 * (-1.0 + Pe * Pp) - 4.0 * MW6 * MZ6 * (-3.0 + Pp + Pe * (-1.0 + 3.0 * Pp)) + MW4 * MZ8 * (-5.0 + 3.0 * Pp + Pe * (-3.0 + 5.0 * Pp)));
        
    CHWden = CHDden * (MH4 * MZ2 + MZ6 + 10.0 * MZ4 * s + MZ2 * s2 + MH2 * (-2.0 * MZ4 - 2.0 * MZ2 * s));
 
    CHWBden = CHWden * MZ2 * MW2 * (MZ4 - MZ2 * s) * (MZ4 - MZ2 * s);
    
    // Independent numerators of the LO dimension-6 contrib.
    Cllnum = sqrt(2.0); 
    CHl111num = sqrt(2.0) * MW2 * MZ2 * (2.0 * MW4 * MZ2 - MW2 * MZ4) * (-1.0 + Pe) * (1.0 + Pp) * s; 
    CHe11num = 2.0 * sqrt(2.0) * MW2 * MZ2 * (MW4 * MZ2 - MW2 * MZ4) * (1.0 + Pe) * (-1.0 + Pp) * s; 
    CHl322num = -Cllnum;
    
    CHBnum = -12.0 * sqrt(2.0) * (MW4 * MZ2 - MW2 * MZ4) * (-MH2 * MZ2 + MZ4 + MZ2 * s) * (8.0 * MW8 * MZ2 * (-1.0 + Pe * Pp) 
            + MW4 * MZ4 * (-5.0 - 3.0 * Pe + 3.0 * Pp + 5.0 * Pe * Pp) * s 
            - 2.0 * MW6 * (-3.0 + Pp + Pe * (-1.0 + 3.0 * Pp)) * (MZ4 + MZ2 * s));
    
    CHWnum = 12.0 * sqrt(2.0) * MW2 * (-MH2 * MZ2 + MZ4 + MZ2 * s) * (8.0 * MW8 * MZ4 * (-1.0 + Pe * Pp) 
            - 2.0 * MW6 * MZ2 * (MZ4 * (-7.0 + Pp + Pe * (-1.0 + 7.0 * Pp)) -  MZ2 * (-1.0 + Pe) * (1.0 + Pp) * s) 
            + MW4 * (2.0 * MZ8 * (-3.0 + Pp + Pe * (-1.0 + 3.0 * Pp)) - MZ6 * (-1.0 + Pe) * (1.0 + Pp) * s)); 
    
    CHWBnum = 2.0 * sqrt(2.0) * sqrt( -((MW4 * MZ2)/( MW4 * MZ2 - MW2 * MZ4)) ) * (-MZ4 + MZ2 * s) * (-MZ4 + MZ2 * s)
            * (-((2.0 * MW8 * MZ4 - 3.0 * MW6 * MZ6 + MW4 * MZ8) * (-1.0 + Pe) * (1.0 + Pp) * (MH4 * MW2 * MZ4 + 12.0 * MW4 * MZ2 * (MZ4 + MZ2 * s) 
            + MW2 * (-5.0 * MZ8 + 4.0 * MZ6 * s + MZ4 * s2) + MH2 * MZ2 * (-12.0 * MW4 * MZ2 + MW2 * (4.0 * MZ4 - 2.0 * MZ2 * s)))) 
            - 2.0 * (-MW4 * MZ2 + MW2 * MZ4) * (-MW4 * MZ2 + MW2 * MZ4) * (1.0 + Pe) * (-1.0 + Pp) * (MH4 * MW2 * MZ4 + 12.0 * MW4 * MZ2 * (MZ4 + MZ2 * s) 
            - MW2 * (5.0 * MZ8 + 2.0 * MZ6 * s + 5.0 * MZ4 * s2) + MH2 * MZ2 * (-12.0 * MW4 * MZ2 + MW2 * (4.0 * MZ4 + 4.0 * MZ2 * s)))); 
    
    CHDnum = sqrt(2.0) * MW4 * MZ2 * (MW2 * MZ4 * (3.0 + Pe - Pp - 3.0 * Pe * Pp) + 4.0 * MW4 * MZ2 * (-1.0 + Pe * Pp)); 
    
    CHboxnum = sqrt(2.0);
    
    // Derivative of cross section wrt MW, normalized to SM
    derSMMW = 8.0 * Mw_tree * (MZ2 * (3.0 + Pe - Pp - 3.0 * Pe * Pp) + 4.0 * MW2 * (-1.0 + Pe * Pp));
    
    derSMMW = derSMMW / (8.0 * MW4 * (-1.0 + Pe * Pp) - 4.0 * MW2 * MZ2 * (-3.0 + Pp + Pe * (-1.0 + 3.0 * Pp)) + MZ4 * (-5.0 + 3.0 * Pp + Pe * (-3.0 + 5.0 * Pp)));
    
    // LO corrections to signal strength in W scheme
    dmuLO += 
                + ( CHboxnum/GF ) * getSMEFTCoeff("CHbox", muRG)
                + ( CHl111num/CHDden ) * getSMEFTCoeff("CHl1R", 0, 0, muRG)
                + ( CHe11num/CHDden ) * getSMEFTCoeff("CHeR", 0, 0, muRG)
                + ( CHl111num/CHDden + CHl322num/GF ) * getSMEFTCoeff("CHl3R", 0, 0, muRG)
                + ( CHl322num/GF ) * getSMEFTCoeff("CHl3R", 1, 1, muRG)
                + ( CHDnum/CHDden ) * getSMEFTCoeff("CHD", muRG)
                + ( CHBnum/CHWden/MW2 ) * getSMEFTCoeff("CHB", muRG)
                + ( CHWnum/CHWden ) * getSMEFTCoeff("CHW", muRG)
                + ( CHWBnum/CHWBden ) * getSMEFTCoeff("CHWB", muRG)
                + ( Cllnum/GF ) * getSMEFTCoeff("CllR", 0, 1, 1, 0, muRG);
    
    // Correction to alpha scheme: only added if the scheme is chosen
    dmuLO += cAsch * DeltaOWtoalph(derSMMW, muRG);
    
    if (FlagfiniteNLO && (sqrt_s < 3.100) ) {
        
        // Choose the right index in the different lists according to the selected energy
        int iECM;
        
        // Ordered according to the energies more commonly used
        if ( (sqrt_s > 0.220) && (sqrt_s < 0.260) ) {
            iECM = 0;
        } else if ( (sqrt_s > 0.340) && (sqrt_s < 0.390) ) {
            iECM = 1;  
        } else if ( (sqrt_s > 0.510) && (sqrt_s < 0.600) ) {
            iECM = 3;
        } else if ( (sqrt_s > 0.900) && (sqrt_s < 1.200) ) {
            iECM = 4;
        } else if ( (sqrt_s > 1.200) && (sqrt_s < 1.600) ) {
            iECM = 5;
        } else if ( (sqrt_s > 2.500) && (sqrt_s < 3.100) ) {
            iECM = 6;
        } else if ( (sqrt_s > 0.450) && (sqrt_s < 0.510) ) {
            iECM = 2;
        } else 
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZH(): NLO corrections not available for this energy");            
        
        
        // Include NLO corrections
        
        // SM Cross section including only EW corrections [fb]
        xsSMNLOW = tofb * xsSMLO 
                + fLR * dSMWLH[iECM] 
                + fRL * dSMWRH[iECM];
        xsSMNLO = xsSMNLOW
                + fLR * dSMQEDLH[iECM] 
                + fRL * dSMQEDRH[iECM];
        
        // Combination of dimension-6 coefficients
        Ch2f1 = getSMEFTCoeff("CHeR",1, 1, muRG) + getSMEFTCoeff("CHeR",2, 2, muRG) 
                + getSMEFTCoeff("CHdR",0, 0, muRG) + getSMEFTCoeff("CHdR",1, 1, muRG) + getSMEFTCoeff("CHdR",2, 2, muRG) 
                - 2.0 * getSMEFTCoeff("CHuR",0, 0, muRG) - 2.0 * getSMEFTCoeff("CHuR",1, 1, muRG) 
                - getSMEFTCoeff("CHq1R",0, 0, muRG) - getSMEFTCoeff("CHq1R",1, 1, muRG) + getSMEFTCoeff("CHl1R",2, 2, muRG);
        
        Ch2f2 = getSMEFTCoeff("CHl3R",2, 2, muRG) 
                + 3.0 * getSMEFTCoeff("CHq3R",0, 0, muRG) + 3.0 * getSMEFTCoeff("CHq3R",1, 1, muRG);
        
        Ch4f1 = getSMEFTCoeff("CldR",0, 0, 0, 0, muRG) + getSMEFTCoeff("CldR",0, 0, 1, 1, muRG) + getSMEFTCoeff("CldR",0, 0, 2, 2, muRG) 
                - 2.0*(getSMEFTCoeff("CluR",0, 0, 0, 0, muRG) + getSMEFTCoeff("CluR",0, 0, 1, 1, muRG)) 
                - getSMEFTCoeff("Clq1R",0, 0, 0, 0, muRG) - getSMEFTCoeff("Clq1R",0, 0, 1, 1, muRG) 
                + getSMEFTCoeff("CllR",0, 0, 2, 2, muRG) + getSMEFTCoeff("CllR",2, 2, 0, 0, muRG) 
                + getSMEFTCoeff("CleR",0, 0, 1, 1, muRG) + getSMEFTCoeff("CleR",0, 0, 2, 2, muRG) 
                - (3.0 * MW2)/(MZ2 - MW2)*(getSMEFTCoeff("Clq3R",0, 0, 0, 0, muRG) + getSMEFTCoeff("Clq3R",0, 0, 1, 1, muRG));
        
        Ch4f2 = getSMEFTCoeff("CllR",0, 1, 1, 0, muRG) + getSMEFTCoeff("CllR",1, 0, 0, 1, muRG);
        Ch4f3 = getSMEFTCoeff("CllR",0, 0, 1, 1, muRG) + getSMEFTCoeff("CllR",1, 1, 0, 0, muRG);
        Ch4f4 = getSMEFTCoeff("CllR",0, 2, 2, 0, muRG) + getSMEFTCoeff("CllR",2, 0, 0, 2, muRG);
        Ch4f5 = getSMEFTCoeff("CeeR",0, 0, 1, 1, muRG) + getSMEFTCoeff("CeeR",0, 0, 2, 2, muRG) + getSMEFTCoeff("CeeR",1, 1, 0, 0, muRG) + getSMEFTCoeff("CeeR",2, 2, 0, 0, muRG) 
                - getSMEFTCoeff("CqeR",0, 0, 0, 0, muRG) - getSMEFTCoeff("CqeR",1, 1, 0, 0, muRG) 
                - 2.0 * (getSMEFTCoeff("CeuR",0, 0, 0, 0, muRG) + getSMEFTCoeff("CeuR",0, 0, 1, 1, muRG) ) 
                + getSMEFTCoeff("CedR",0, 0, 0, 0, muRG) + getSMEFTCoeff("CedR",0, 0, 1, 1, muRG) + getSMEFTCoeff("CedR",0, 0, 2, 2, muRG) 
                + getSMEFTCoeff("CleR",1, 1, 0, 0, muRG) + getSMEFTCoeff("CleR",2, 2, 0, 0, muRG);
        Ch4f6 = getSMEFTCoeff("CeeR",0, 1, 1, 0, muRG) + getSMEFTCoeff("CeeR",1, 0, 0, 1, muRG) + getSMEFTCoeff("CeeR",0, 2, 2, 0, muRG) + getSMEFTCoeff("CeeR",2, 0, 0, 2, muRG);
 
        // Corrections for LH initial electrons
        d6NLOLH = d6LHCHD[iECM] * getSMEFTCoeff("CHD", muRG)
                + d6LHCHbox[iECM] * getSMEFTCoeff("CHbox", muRG)
                + d6LHCHW[iECM] * getSMEFTCoeff("CHW", muRG)
                + d6LHCHB[iECM] * getSMEFTCoeff("CHB", muRG)
                + d6LHCHWB[iECM] * getSMEFTCoeff("CHWB", muRG)
                + d6LHCHeR00[iECM] * getSMEFTCoeff("CHeR", 0, 0, muRG)
                + d6LHCHl1R00[iECM] * getSMEFTCoeff("CHl1R", 0, 0, muRG)
                + d6LHCHl3R00[iECM] * getSMEFTCoeff("CHl3R", 0, 0, muRG)
                + d6LHCHl3R11[iECM] * getSMEFTCoeff("CHl3R", 1, 1, muRG)
                + d6LHCh4f2[iECM] * Ch4f2                                
                + d6LHCHq1R22[iECM] * getSMEFTCoeff("CHq1R", 2, 2, muRG)
                + d6LHCHq3R22[iECM] * getSMEFTCoeff("CHq3R", 2, 2, muRG)
                + d6LHCHuR22[iECM] * getSMEFTCoeff("CHuR", 2, 2, muRG)
                + d6LHCuWR22[iECM] * getSMEFTCoeff("CuWR", 2, 2, muRG)
                + d6LHCuBR22[iECM] * getSMEFTCoeff("CuBR", 2, 2, muRG)
                + d6LHCuHR22[iECM] * getSMEFTCoeff("CuHR", 2, 2, muRG)
                + d6LHCh2f1[iECM] * Ch2f1
                + d6LHCh2f2[iECM] * Ch2f2                
                + d6LHCHl1R11[iECM] * getSMEFTCoeff("CHl1R", 1, 1, muRG)
                + d6LHCH[iECM] * getSMEFTCoeff("CH", muRG)
                + d6LHCW[iECM] * getSMEFTCoeff("CW", muRG)                
                + d6LHCeuR0022[iECM] * getSMEFTCoeff("CeuR",0, 0, 2, 2, muRG)
                + d6LHCluR0022[iECM] * getSMEFTCoeff("CluR",0, 0, 2, 2, muRG)
                + d6LHCqeR2200[iECM] * getSMEFTCoeff("CqeR",2, 2, 0, 0, muRG)
                + d6LHClq1R0022[iECM] * getSMEFTCoeff("Clq1R",0, 0, 2, 2, muRG)
                + d6LHClq3R0022[iECM] * getSMEFTCoeff("Clq3R",0, 0, 2, 2, muRG)
                + d6LHClq3R1122[iECM] * getSMEFTCoeff("Clq3R",1, 1, 2, 2, muRG)
                + d6LHCh4f1[iECM] * Ch4f1
                + d6LHCh4f3[iECM] * Ch4f3
                + d6LHCh4f4[iECM] * Ch4f4
                + d6LHCh4f5[iECM] * Ch4f5
                + d6LHCh4f6[iECM] * Ch4f6            
                + d6LHCleR0000[iECM] * getSMEFTCoeff("CleR",0, 0, 0, 0, muRG)
                + d6LHCllR0000[iECM] * getSMEFTCoeff("CllR",0, 0, 0, 0, muRG)
                + d6LHCeeR0000[iECM] * getSMEFTCoeff("CeeR",0, 0, 0, 0, muRG)                
                //+ d6LHCHBt[iECM] * getSMEFTCoeff("CHBtilde", muRG)
                //+ d6LHCHWt[iECM] * getSMEFTCoeff("CHWtilde", muRG)
                //+ d6LHCHWBt[iECM] * getSMEFTCoeff("CHWtildeB", muRG)
                //+ d6LHCWt[iECM] * getSMEFTCoeff("CWtilde", muRG)
                ;
                  
        // Corrections for RH initial electrons
        d6NLORH = d6RHCHD[iECM] * getSMEFTCoeff("CHD", muRG)
                + d6RHCHbox[iECM] * getSMEFTCoeff("CHbox", muRG)
                + d6RHCHW[iECM] * getSMEFTCoeff("CHW", muRG)
                + d6RHCHB[iECM] * getSMEFTCoeff("CHB", muRG)
                + d6RHCHWB[iECM] * getSMEFTCoeff("CHWB", muRG)
                + d6RHCHeR00[iECM] * getSMEFTCoeff("CHeR", 0, 0, muRG)
                + d6RHCHl1R00[iECM] * getSMEFTCoeff("CHl1R", 0, 0, muRG)
                + d6RHCHl3R00[iECM] * getSMEFTCoeff("CHl3R", 0, 0, muRG)
                + d6RHCHl3R11[iECM] * getSMEFTCoeff("CHl3R", 1, 1, muRG)
                + d6RHCh4f2[iECM] * Ch4f2                                
                + d6RHCHq1R22[iECM] * getSMEFTCoeff("CHq1R", 2, 2, muRG)
                + d6RHCHq3R22[iECM] * getSMEFTCoeff("CHq3R", 2, 2, muRG)
                + d6RHCHuR22[iECM] * getSMEFTCoeff("CHuR", 2, 2, muRG)
                + d6RHCuWR22[iECM] * getSMEFTCoeff("CuWR", 2, 2, muRG)
                + d6RHCuBR22[iECM] * getSMEFTCoeff("CuBR", 2, 2, muRG)
                + d6RHCuHR22[iECM] * getSMEFTCoeff("CuHR", 2, 2, muRG)
                + d6RHCh2f1[iECM] * Ch2f1
                + d6RHCh2f2[iECM] * Ch2f2                
                + d6RHCHl1R11[iECM] * getSMEFTCoeff("CHl1R", 1, 1, muRG)
                + d6RHCH[iECM] * getSMEFTCoeff("CH", muRG)
                + d6RHCW[iECM] * getSMEFTCoeff("CW", muRG)                
                + d6RHCeuR0022[iECM] * getSMEFTCoeff("CeuR",0, 0, 2, 2, muRG)
                + d6RHCluR0022[iECM] * getSMEFTCoeff("CluR",0, 0, 2, 2, muRG)
                + d6RHCqeR2200[iECM] * getSMEFTCoeff("CqeR",2, 2, 0, 0, muRG)
                + d6RHClq1R0022[iECM] * getSMEFTCoeff("Clq1R",0, 0, 2, 2, muRG)
                + d6RHClq3R0022[iECM] * getSMEFTCoeff("Clq3R",0, 0, 2, 2, muRG)
                + d6RHClq3R1122[iECM] * getSMEFTCoeff("Clq3R",1, 1, 2, 2, muRG)
                + d6RHCh4f1[iECM] * Ch4f1
                + d6RHCh4f3[iECM] * Ch4f3
                + d6RHCh4f4[iECM] * Ch4f4
                + d6RHCh4f5[iECM] * Ch4f5
                + d6RHCh4f6[iECM] * Ch4f6            
                + d6RHCleR0000[iECM] * getSMEFTCoeff("CleR",0, 0, 0, 0, muRG)
                + d6RHCllR0000[iECM] * getSMEFTCoeff("CllR",0, 0, 0, 0, muRG)
                + d6RHCeeR0000[iECM] * getSMEFTCoeff("CeeR",0, 0, 0, 0, muRG)                
                //+ d6RHCHBt[iECM] * getSMEFTCoeff("CHBtilde", muRG)
                //+ d6RHCHWt[iECM] * getSMEFTCoeff("CHWtilde", muRG)
                //+ d6RHCHWBt[iECM] * getSMEFTCoeff("CHWtildeB", muRG)
                //+ d6RHCWt[iECM] * getSMEFTCoeff("CWtilde", muRG)
                ;       
        
        // Correction to polarized cross section: Need to multiply by (Lambda=1000 GeV)^2
        dmuNLO += ( fLR * xsSMweakLH[iECM] * d6NLOLH  
                + fRL * xsSMweakRH[iECM] * d6NLORH ) * 1000000;
        // Normalize to SM full NLO cross section
        dmuNLO = dmuNLO /(fLR * xsSMNLOLH[iECM] + fRL * xsSMNLORH[iECM]);
        
        // Rescale the LO contribution and normalizer the NLO to the SM cross section
        dmuLO = dmuLO * (tofb * xsSMLO/xsSMNLO);
        
    }
    
    // Coefficient for Higgs self-coupling corrections (disabled for the moment as these are already included in NLO above)
    //if (sqrt_s == 240.) {
 
    //    C1 = 0.0173302;
        
    //} else if (sqrt_s == 250.) {
 
    //    C1 = 0.015;
 
    //} else if (sqrt_s == 350.) {
 
    //    C1 = 0.0057;
 
    //} else if (sqrt_s == 365.) {
 
    //    C1 = 0.00493549; 
 
    //} else if (sqrt_s == 380.) {
 
    //    C1 = 0.0057; // Use same as 350 GeV
 
    //} else if (sqrt_s == 500.) {
 
    //    C1 = 0.00099;
 
    //} else if (sqrt_s == 1000.) {
 
    //    C1 = -0.0012;
 
    //} else if (sqrt_s == 1400.) {
 
    //    C1 = -0.0011;
 
    //} else if (sqrt_s == 1500.) {
 
    //    C1 = -0.0011; // Use the same as 1400 GeV
 
    //} else if (sqrt_s == 3000.) {
 
    //    C1 = -0.00054;
 
    //} else
    //    throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZH()");
 
    // Add the LO and NLO corrections
    mu += dmuLO + dmuNLO;
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eeeZHint + eeeZHpar;
 
    //  Linear contribution from Higgs self-coupling
    // mu += cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio(); // Linear corrections already included
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mueeZHGen()

const double NPSMEFTd6General::mueeZHGen	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{eeZH}$ between the $ e^{+}e^{-}\to ZH $ associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eeZH}$

Reimplemented from NPbase.

Definition at line 23582 of file NPSMEFTd6General.cpp.

                                                                                                            {
 
    // Only Alpha scheme
 
    double mu = 1.0;
 
    double C1 = 0.0;
    
    double muRG = 0;
    
    // RG scale in GeV
    muRG = 1000. * sqrt_s;
    
    if ( (Pol_em != 0.) || (Pol_ep != 0) ) return mueeZHPol(sqrt_s, Pol_em, Pol_ep);
 
    if (sqrt_s == 0.240) {
 
        C1 = 0.0173302;
 
        mu +=
                +121263. * getSMEFTCoeffEW("CHbox")
                + 898682. * getSMEFTCoeffEW("CHl1R", 0, 0)
                - 767820. * getSMEFTCoeffEW("CHeR", 0, 0)
                + 898682. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 6046.36 * getSMEFTCoeffEW("CHD")
                + 122439. * getSMEFTCoeffEW("CHB")
                + 540057. * getSMEFTCoeffEW("CHW")
                + 231063. * getSMEFTCoeffEW("CHWB")
                - 2.2 * delta_GF
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (-0.2 * deltaaMZ()
                + 2.2 * deltaGmu()
                + 4.775 * deltaMz()
                - 3.071 * deltaMh());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else if (sqrt_s == 0.250) {
 
        C1 = 0.015;
 
        mu +=
                +121263. * getSMEFTCoeffEW("CHbox")
                + 975101. * getSMEFTCoeffEW("CHl1R", 0, 0)
                - 833750. * getSMEFTCoeffEW("CHeR", 0, 0)
                + 975101. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 6046.36 * getSMEFTCoeffEW("CHD")
                + 128443. * getSMEFTCoeffEW("CHB")
                + 568273. * getSMEFTCoeffEW("CHW")
                + 244206. * getSMEFTCoeffEW("CHWB")
                - 2.2 * delta_GF
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (-0.2 * deltaaMZ()
                + 2.2 * deltaGmu()
                + 5.219 * deltaMz()
                - 2.27 * deltaMh());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else if (sqrt_s == 0.350) {
 
        C1 = 0.0057;
 
        mu +=
                +121283. * getSMEFTCoeffEW("CHbox")
                + 1911340. * getSMEFTCoeffEW("CHl1R", 0, 0)
                - 1640958. * getSMEFTCoeffEW("CHeR", 0, 0)
                + 1911340. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 6009.52 * getSMEFTCoeffEW("CHD")
                + 173183. * getSMEFTCoeffEW("CHB")
                + 785843. * getSMEFTCoeffEW("CHW")
                + 344494. * getSMEFTCoeffEW("CHWB")
                - 2.201 * delta_GF
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (-0.2 * deltaaMZ()
                + 2.2 * deltaGmu()
                + 5.396 * deltaMz()
                - 0.729 * deltaMh());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else if (sqrt_s == 0.365) {
 
        C1 = 0.00493549;
 
        mu +=
                +121243. * getSMEFTCoeffEW("CHbox")
                + 2078482. * getSMEFTCoeffEW("CHl1R", 0, 0)
                - 1785085. * getSMEFTCoeffEW("CHeR", 0, 0)
                + 2078482. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 6010.65 * getSMEFTCoeffEW("CHD")
                + 178173. * getSMEFTCoeffEW("CHB")
                + 809806. * getSMEFTCoeffEW("CHW")
                + 355487. * getSMEFTCoeffEW("CHWB")
                - 2.201 * delta_GF
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (-0.2 * deltaaMZ()
                + 2.2 * deltaGmu()
                + 5.348 * deltaMz()
                - 0.664 * deltaMh());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else if (sqrt_s == 0.380) {
 
        C1 = 0.0057; // Use same as 350 GeV
 
        mu +=
                +121281. * getSMEFTCoeffEW("CHbox")
                + 2253013. * getSMEFTCoeffEW("CHl1R", 0, 0)
                - 1934557. * getSMEFTCoeffEW("CHeR", 0, 0)
                + 2253013. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 6026.37 * getSMEFTCoeffEW("CHD")
                + 182674. * getSMEFTCoeffEW("CHB")
                + 832109. * getSMEFTCoeffEW("CHW")
                + 365819. * getSMEFTCoeffEW("CHWB")
                - 2.202 * delta_GF
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (-0.2 * deltaaMZ()
                + 2.2 * deltaGmu()
                + 5.301 * deltaMz()
                - 0.609 * deltaMh());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else if (sqrt_s == 0.500) {
 
        C1 = 0.00099;
 
        mu +=
                +121264. * getSMEFTCoeffEW("CHbox")
                + 3900384. * getSMEFTCoeffEW("CHl1R", 0, 0)
                - 3350136. * getSMEFTCoeffEW("CHeR", 0, 0)
                + 3900384. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 6019.22 * getSMEFTCoeffEW("CHD")
                + 209229. * getSMEFTCoeffEW("CHB")
                + 959942. * getSMEFTCoeffEW("CHW")
                + 425112. * getSMEFTCoeffEW("CHWB")
                - 2.202 * delta_GF
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (-0.2 * deltaaMZ()
                + 2.2 * deltaGmu()
                + 5. * deltaMz()
                - 0.351 * deltaMh());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else if (sqrt_s == 1.0) {
 
        C1 = -0.0012;
 
        mu +=
                +121274. * getSMEFTCoeffEW("CHbox")
                + 15601820. * getSMEFTCoeffEW("CHl1R", 0, 0)
                - 13395670. * getSMEFTCoeffEW("CHeR", 0, 0)
                + 15601820. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 6040.16 * getSMEFTCoeffEW("CHD")
                + 243960. * getSMEFTCoeffEW("CHB")
                + 1128805. * getSMEFTCoeffEW("CHW")
                + 503138. * getSMEFTCoeffEW("CHWB")
                - 2.202 * delta_GF
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (-0.2 * deltaaMZ()
                + 2.2 * deltaGmu()
                + 4.574 * deltaMz()
                - 0.092 * deltaMh());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else if (sqrt_s == 1.4) {
 
        C1 = -0.0011;
 
        mu +=
                +121283. * getSMEFTCoeffEW("CHbox")
                + 30579278. * getSMEFTCoeffEW("CHl1R", 0, 0)
                - 26253064. * getSMEFTCoeffEW("CHeR", 0, 0)
                + 30579278. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 6010.77 * getSMEFTCoeffEW("CHD")
                + 250804. * getSMEFTCoeffEW("CHB")
                + 1161208. * getSMEFTCoeffEW("CHW")
                + 518040. * getSMEFTCoeffEW("CHWB")
                - 2.203 * delta_GF
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (-0.2 * deltaaMZ()
                + 2.2 * deltaGmu()
                + 4.491 * deltaMz()
                - 0.047 * deltaMh());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else if (sqrt_s == 1.5) {
 
        C1 = -0.0011; // Use the same as 1400 GeV
 
        mu +=
                +121262. * getSMEFTCoeffEW("CHbox")
                + 35102329. * getSMEFTCoeffEW("CHl1R", 0, 0)
                - 30135878. * getSMEFTCoeffEW("CHeR", 0, 0)
                + 35102329. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 6034.22 * getSMEFTCoeffEW("CHD")
                + 251576. * getSMEFTCoeffEW("CHB")
                + 1165634. * getSMEFTCoeffEW("CHW")
                + 519954. * getSMEFTCoeffEW("CHWB")
                - 2.203 * delta_GF
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (-0.2 * deltaaMZ()
                + 2.2 * deltaGmu()
                + 4.479 * deltaMz()
                - 0.041 * deltaMh());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else if (sqrt_s == 3.0) {
 
        C1 = -0.00054;
 
        mu +=
                +121279. * getSMEFTCoeffEW("CHbox")
                + 140413697. * getSMEFTCoeffEW("CHl1R", 0, 0)
                - 120540988. * getSMEFTCoeffEW("CHeR", 0, 0)
                + 140413697. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 6012.61 * getSMEFTCoeffEW("CHD")
                + 257222. * getSMEFTCoeffEW("CHB")
                + 1188444. * getSMEFTCoeffEW("CHW")
                + 530503. * getSMEFTCoeffEW("CHWB")
                - 2.202 * delta_GF
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (-0.2 * deltaaMZ()
                + 2.2 * deltaGmu()
                + 4.42 * deltaMz()
                - 0.01 * deltaMh());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZH()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eeeZHint + eeeZHpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mueeZHPol()

const double NPSMEFTd6General::mueeZHPol	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{eeZH}$ between the $ e^{+}e^{-}\to ZH $ associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eeZH}$

Definition at line 23929 of file NPSMEFTd6General.cpp.

                                                                                                            {
 
    // Only Alpha scheme
 
    double mu = 1.0;
 
    double C1 = 0.0;
    
    double muRG = 0;
    
    // RG scale in GeV
    muRG = 1000. * sqrt_s;
 
    if (sqrt_s == 0.240) {
 
        C1 = 0.0173302;
 
        if (Pol_em == 80. && Pol_ep == -30.) {
            mu +=
                    +121260. * getSMEFTCoeffEW("CHbox")
                    + 117191. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 1681596. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 117191. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 74555.1 * getSMEFTCoeffEW("CHD")
                    + 528105. * getSMEFTCoeffEW("CHB")
                    + 134403. * getSMEFTCoeffEW("CHW")
                    + 872560. * getSMEFTCoeffEW("CHWB")
                    + 0.459 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.46 * deltaaMZ()
                    - 0.46 * deltaGmu()
                    - 0.544 * deltaMz()
                    - 3.071 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 30.) {
            mu +=
                    +121254. * getSMEFTCoeffEW("CHbox")
                    + 1495015. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 76567.2 * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 1495015. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 67582.1 * getSMEFTCoeffEW("CHD")
                    - 187104. * getSMEFTCoeffEW("CHB")
                    + 849552. * getSMEFTCoeffEW("CHW")
                    - 258537. * getSMEFTCoeffEW("CHWB")
                    - 4.23 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.23 * deltaaMZ()
                    + 4.23 * deltaGmu()
                    + 8.834 * deltaMz()
                    - 3.071 * deltaMh());
 
        } else if (Pol_em == 80. && Pol_ep == 0.) {
            mu +=
                    +121256. * getSMEFTCoeffEW("CHbox")
                    + 204529. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 1578998. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 204529. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 65548.7 * getSMEFTCoeffEW("CHD")
                    + 482729. * getSMEFTCoeffEW("CHB")
                    + 179733. * getSMEFTCoeffEW("CHW")
                    + 800870. * getSMEFTCoeffEW("CHWB")
                    + 0.162 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.163 * deltaaMZ()
                    - 0.163 * deltaGmu()
                    + 0.05 * deltaMz()
                    - 3.071 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 0.) {
            mu +=
                    +121264. * getSMEFTCoeffEW("CHbox")
                    + 1442776. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 137405. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 1442776. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 62167.6 * getSMEFTCoeffEW("CHD")
                    - 159988. * getSMEFTCoeffEW("CHB")
                    + 822448. * getSMEFTCoeffEW("CHW")
                    - 215639. * getSMEFTCoeffEW("CHWB")
                    - 4.052 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.052 * deltaaMZ()
                    + 4.052 * deltaGmu()
                    + 8.479 * deltaMz()
                    - 3.071 * deltaMh());
 
        } else {
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZHPol()");
        }
 
    } else if (sqrt_s == 0.250) {
 
        C1 = 0.015;
 
        if (Pol_em == 80. && Pol_ep == -30.) {
            mu +=
                    +121264. * getSMEFTCoeffEW("CHbox")
                    + 127210. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 1824910. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 127210. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 74597.1 * getSMEFTCoeffEW("CHD")
                    + 560319. * getSMEFTCoeffEW("CHB")
                    + 136129. * getSMEFTCoeffEW("CHW")
                    + 902676. * getSMEFTCoeffEW("CHWB")
                    + 0.459 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.46 * deltaaMZ()
                    - 0.46 * deltaGmu()
                    - 0.1 * deltaMz()
                    - 2.27 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 30.) {
            mu +=
                    +121257. * getSMEFTCoeffEW("CHbox")
                    + 1622228. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 83107. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 1622228. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 67554.3 * getSMEFTCoeffEW("CHD")
                    - 201409. * getSMEFTCoeffEW("CHB")
                    + 898116. * getSMEFTCoeffEW("CHW")
                    - 258306. * getSMEFTCoeffEW("CHWB")
                    - 4.23 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.23 * deltaaMZ()
                    + 4.23 * deltaGmu()
                    + 9.279 * deltaMz()
                    - 2.27 * deltaMh());
 
        } else if (Pol_em == 80. && Pol_ep == 0.) {
            mu +=
                    +121309. * getSMEFTCoeffEW("CHbox")
                    + 221930. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 1714047. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 221930. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 65599.6 * getSMEFTCoeffEW("CHD")
                    + 512136. * getSMEFTCoeffEW("CHB")
                    + 184424. * getSMEFTCoeffEW("CHW")
                    + 829145. * getSMEFTCoeffEW("CHWB")
                    + 0.162 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.163 * deltaaMZ()
                    - 0.163 * deltaGmu()
                    + 0.494 * deltaMz()
                    - 2.27 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 0.) {
            mu +=
                    +121269. * getSMEFTCoeffEW("CHbox")
                    + 1565559. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 148908. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 1565559. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 62170. * getSMEFTCoeffEW("CHD")
                    - 172540. * getSMEFTCoeffEW("CHB")
                    + 869218. * getSMEFTCoeffEW("CHW")
                    - 214299. * getSMEFTCoeffEW("CHWB")
                    - 4.053 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.052 * deltaaMZ()
                    + 4.052 * deltaGmu()
                    + 8.923 * deltaMz()
                    - 2.27 * deltaMh());
 
        } else {
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZHPol()");
        }
 
    } else if (sqrt_s == 0.350) {
 
        C1 = 0.0057;
 
        if (Pol_em == 80. && Pol_ep == -30.) {
            mu +=
                    +121274. * getSMEFTCoeffEW("CHbox")
                    + 249309. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 3576996. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 249309. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 74596.5 * getSMEFTCoeffEW("CHD")
                    + 812491. * getSMEFTCoeffEW("CHB")
                    + 146212. * getSMEFTCoeffEW("CHW")
                    + 1135161. * getSMEFTCoeffEW("CHWB")
                    + 0.458 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.46 * deltaaMZ()
                    - 0.46 * deltaGmu()
                    + 0.077 * deltaMz()
                    - 0.729 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 30.) {
            mu +=
                    +121289. * getSMEFTCoeffEW("CHbox")
                    + 3179548. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 163347. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 3179548. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 67524.8 * getSMEFTCoeffEW("CHD")
                    - 314653. * getSMEFTCoeffEW("CHB")
                    + 1273817. * getSMEFTCoeffEW("CHW")
                    - 258947. * getSMEFTCoeffEW("CHWB")
                    - 4.231 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.23 * deltaaMZ()
                    + 4.23 * deltaGmu()
                    + 9.456 * deltaMz()
                    - 0.729 * deltaMh());
 
        } else if (Pol_em == 80. && Pol_ep == 0.) {
            mu +=
                    +121304. * getSMEFTCoeffEW("CHbox")
                    + 434952. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 3360980. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 434952. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 65624.7 * getSMEFTCoeffEW("CHD")
                    + 741142. * getSMEFTCoeffEW("CHB")
                    + 217654. * getSMEFTCoeffEW("CHW")
                    + 1046799. * getSMEFTCoeffEW("CHWB")
                    + 0.161 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.163 * deltaaMZ()
                    - 0.163 * deltaGmu()
                    + 0.671 * deltaMz()
                    - 0.729 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 0.) {
            mu +=
                    +121259. * getSMEFTCoeffEW("CHbox")
                    + 3068356. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 292427. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 3068356. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 62160.7 * getSMEFTCoeffEW("CHD")
                    - 271962. * getSMEFTCoeffEW("CHB")
                    + 1231171. * getSMEFTCoeffEW("CHW")
                    - 206112. * getSMEFTCoeffEW("CHWB")
                    - 4.053 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.052 * deltaaMZ()
                    + 4.052 * deltaGmu()
                    + 9.1 * deltaMz()
                    - 0.729 * deltaMh());
 
        } else {
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZHPol()");
        }
 
    } else if (sqrt_s == 0.365) {
 
        C1 = 0.00493549;
 
        if (Pol_em == 80. && Pol_ep == -30.) {
            mu +=
                    +121270. * getSMEFTCoeffEW("CHbox")
                    + 271098. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 3890169. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 271098. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 74554. * getSMEFTCoeffEW("CHD")
                    + 840573. * getSMEFTCoeffEW("CHB")
                    + 147108. * getSMEFTCoeffEW("CHW")
                    + 1160947. * getSMEFTCoeffEW("CHWB")
                    + 0.459 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.46 * deltaaMZ()
                    - 0.46 * deltaGmu()
                    + 0.029 * deltaMz()
                    - 0.664 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 30.) {
            mu +=
                    +121238. * getSMEFTCoeffEW("CHbox")
                    + 3457848. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 177584. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 3457848. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 67578.3 * getSMEFTCoeffEW("CHD")
                    - 327391. * getSMEFTCoeffEW("CHB")
                    + 1315671. * getSMEFTCoeffEW("CHW")
                    - 259142. * getSMEFTCoeffEW("CHWB")
                    - 4.231 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.23 * deltaaMZ()
                    + 4.23 * deltaGmu()
                    + 9.408 * deltaMz()
                    - 0.664 * deltaMh());
 
        } else if (Pol_em == 80. && Pol_ep == 0.) {
            mu +=
                    +121251. * getSMEFTCoeffEW("CHbox")
                    + 472985. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 3655203. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 472985. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 65559.4 * getSMEFTCoeffEW("CHD")
                    + 766585. * getSMEFTCoeffEW("CHB")
                    + 221202. * getSMEFTCoeffEW("CHW")
                    + 1070933. * getSMEFTCoeffEW("CHWB")
                    + 0.161 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.163 * deltaaMZ()
                    - 0.163 * deltaGmu()
                    + 0.623 * deltaMz()
                    - 0.664 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 0.) {
            mu +=
                    +121238. * getSMEFTCoeffEW("CHbox")
                    + 3336984. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 317944. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 3336984. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 62188.9 * getSMEFTCoeffEW("CHD")
                    - 283174. * getSMEFTCoeffEW("CHB")
                    + 1271272. * getSMEFTCoeffEW("CHW")
                    - 205330. * getSMEFTCoeffEW("CHWB")
                    - 4.053 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.052 * deltaaMZ()
                    + 4.052 * deltaGmu()
                    + 9.052 * deltaMz()
                    - 0.664 * deltaMh());
 
        } else {
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZHPol()");
        }
 
    } else if (sqrt_s == 0.380) {
 
        C1 = 0.0057; // Use same as 350 GeV
 
        if (Pol_em == 80. && Pol_ep == -30.) {
            mu +=
                    +121228. * getSMEFTCoeffEW("CHbox")
                    + 293860. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 4216491. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 293860. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 74561.4 * getSMEFTCoeffEW("CHD")
                    + 866754. * getSMEFTCoeffEW("CHB")
                    + 147982. * getSMEFTCoeffEW("CHW")
                    + 1184912. * getSMEFTCoeffEW("CHWB")
                    + 0.459 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.46 * deltaaMZ()
                    - 0.46 * deltaGmu()
                    - 0.018 * deltaMz()
                    - 0.609 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 30.) {
            mu +=
                    +121226. * getSMEFTCoeffEW("CHbox")
                    + 3747707. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 192650. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 3747707. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 67608.3 * getSMEFTCoeffEW("CHD")
                    - 339193. * getSMEFTCoeffEW("CHB")
                    + 1354040. * getSMEFTCoeffEW("CHW")
                    - 259321. * getSMEFTCoeffEW("CHWB")
                    - 4.23 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.23 * deltaaMZ()
                    + 4.23 * deltaGmu()
                    + 9.361 * deltaMz()
                    - 0.609 * deltaMh());
 
        } else if (Pol_em == 80. && Pol_ep == 0.) {
            mu +=
                    +121325. * getSMEFTCoeffEW("CHbox")
                    + 512707. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 3961665. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 512707. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 65601.7 * getSMEFTCoeffEW("CHD")
                    + 790306. * getSMEFTCoeffEW("CHB")
                    + 224394. * getSMEFTCoeffEW("CHW")
                    + 1093297. * getSMEFTCoeffEW("CHWB")
                    + 0.161 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.163 * deltaaMZ()
                    - 0.163 * deltaGmu()
                    + 0.576 * deltaMz()
                    - 0.609 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 0.) {
            mu +=
                    +121273. * getSMEFTCoeffEW("CHbox")
                    + 3617032. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 344629. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 3617032. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 62148.3 * getSMEFTCoeffEW("CHD")
                    - 293491. * getSMEFTCoeffEW("CHB")
                    + 1308558. * getSMEFTCoeffEW("CHW")
                    - 204594. * getSMEFTCoeffEW("CHWB")
                    - 4.053 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.052 * deltaaMZ()
                    + 4.052 * deltaGmu()
                    + 9.005 * deltaMz()
                    - 0.609 * deltaMh());
 
        } else {
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZHPol()");
        }
 
    } else if (sqrt_s == 0.500) {
 
        C1 = 0.00099;
 
        if (Pol_em == 80. && Pol_ep == -30.) {
            mu +=
                    +121268. * getSMEFTCoeffEW("CHbox")
                    + 508715. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 7299333. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 508715. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 74603.6 * getSMEFTCoeffEW("CHD")
                    + 1018069. * getSMEFTCoeffEW("CHB")
                    + 151257. * getSMEFTCoeffEW("CHW")
                    + 1323862. * getSMEFTCoeffEW("CHWB")
                    + 0.458 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.46 * deltaaMZ()
                    - 0.46 * deltaGmu()
                    - 0.319 * deltaMz()
                    - 0.351 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 30.) {
            mu +=
                    +121273. * getSMEFTCoeffEW("CHbox")
                    + 6488707. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 332950. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 6488707. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 67530.9 * getSMEFTCoeffEW("CHD")
                    - 408101. * getSMEFTCoeffEW("CHB")
                    + 1576859. * getSMEFTCoeffEW("CHW")
                    - 260777. * getSMEFTCoeffEW("CHWB")
                    - 4.231 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.23 * deltaaMZ()
                    + 4.23 * deltaGmu()
                    + 9.06 * deltaMz()
                    - 0.351 * deltaMh());
 
        } else if (Pol_em == 80. && Pol_ep == 0.) {
            mu +=
                    +121280. * getSMEFTCoeffEW("CHbox")
                    + 887632. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 6858533. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 887632. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 65606.6 * getSMEFTCoeffEW("CHD")
                    + 927745. * getSMEFTCoeffEW("CHB")
                    + 241619. * getSMEFTCoeffEW("CHW")
                    + 1223535. * getSMEFTCoeffEW("CHWB")
                    + 0.161 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.163 * deltaaMZ()
                    - 0.163 * deltaGmu()
                    + 0.275 * deltaMz()
                    - 0.351 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 0.) {
            mu +=
                    +121268. * getSMEFTCoeffEW("CHbox")
                    + 6262095. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 597046. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 6262095. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 62148.8 * getSMEFTCoeffEW("CHD")
                    - 353914. * getSMEFTCoeffEW("CHB")
                    + 1522841. * getSMEFTCoeffEW("CHW")
                    - 200684. * getSMEFTCoeffEW("CHWB")
                    - 4.054 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.052 * deltaaMZ()
                    + 4.052 * deltaGmu()
                    + 8.704 * deltaMz()
                    - 0.351 * deltaMh());
 
        } else {
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZHPol()");
        }
 
    } else if (sqrt_s == 1.0) {
 
        C1 = -0.0012;
 
        if (Pol_em == 80. && Pol_ep == -30.) {
            mu +=
                    +121236. * getSMEFTCoeffEW("CHbox")
                    + 2034785. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 29195703. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 2034785. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 74612.7 * getSMEFTCoeffEW("CHD")
                    + 1218284. * getSMEFTCoeffEW("CHB")
                    + 154779. * getSMEFTCoeffEW("CHW")
                    + 1507673. * getSMEFTCoeffEW("CHWB")
                    + 0.458 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.46 * deltaaMZ()
                    - 0.46 * deltaGmu()
                    - 0.745 * deltaMz()
                    - 0.092 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 30.) {
            mu +=
                    +121298. * getSMEFTCoeffEW("CHbox")
                    + 25954994. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 1333713. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 25954994. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 67536.7 * getSMEFTCoeffEW("CHD")
                    - 499699. * getSMEFTCoeffEW("CHB")
                    + 1872177. * getSMEFTCoeffEW("CHW")
                    - 263454. * getSMEFTCoeffEW("CHWB")
                    - 4.233 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.23 * deltaaMZ()
                    + 4.23 * deltaGmu()
                    + 8.633 * deltaMz()
                    - 0.092 * deltaMh());
 
        } else if (Pol_em == 80. && Pol_ep == -20.) {
            mu +=
                    +121257. * getSMEFTCoeffEW("CHbox")
                    + 2475072. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 28682974. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 2475072. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 72023. * getSMEFTCoeffEW("CHD")
                    + 1186280. * getSMEFTCoeffEW("CHB")
                    + 186435. * getSMEFTCoeffEW("CHW")
                    + 1475072. * getSMEFTCoeffEW("CHWB")
                    + 0.371 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-0.572 * deltaMz()
                    - 0.091 * deltaMh()
                    + 2.375 * deltaaMZ()
                    - 0.377 * deltaGmu());
 
        } else if (Pol_em == -80. && Pol_ep == 20.) {
            mu +=
                    +121306. * getSMEFTCoeffEW("CHbox")
                    + 25696973. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 1634825. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 25696973. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 65976.8 * getSMEFTCoeffEW("CHD")
                    - 480973. * getSMEFTCoeffEW("CHB")
                    + 1853631. * getSMEFTCoeffEW("CHW")
                    - 244288. * getSMEFTCoeffEW("CHWB")
                    - 4.182 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+8.536 * deltaMz()
                    - 0.09 * deltaMh()
                    - 2.178 * deltaaMZ()
                    + 4.178 * deltaGmu());
 
        } else if (Pol_em == 80. && Pol_ep == 0.) {
            mu +=
                    +121307. * getSMEFTCoeffEW("CHbox")
                    + 3550656. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 27432206. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 3550656. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 65607.4 * getSMEFTCoeffEW("CHD")
                    + 1109435. * getSMEFTCoeffEW("CHB")
                    + 263679. * getSMEFTCoeffEW("CHW")
                    + 1395519. * getSMEFTCoeffEW("CHWB")
                    + 0.159 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.163 * deltaaMZ()
                    - 0.163 * deltaGmu()
                    - 0.151 * deltaMz()
                    - 0.092 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 0.) {
            mu +=
                    +121327. * getSMEFTCoeffEW("CHbox")
                    + 25048839. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 2390358. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 25048839. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 62132.7 * getSMEFTCoeffEW("CHD")
                    - 434824. * getSMEFTCoeffEW("CHB")
                    + 1807095. * getSMEFTCoeffEW("CHW")
                    - 196264. * getSMEFTCoeffEW("CHWB")
                    - 4.056 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.052 * deltaaMZ()
                    + 4.052 * deltaGmu()
                    + 8.278 * deltaMz()
                    - 0.092 * deltaMh());
 
        } else {
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZHPol()");
        }
 
    } else if (sqrt_s == 1.4) {
 
        C1 = -0.0011;
 
        if (Pol_em == 80. && Pol_ep == -30.) {
            mu +=
                    +121277. * getSMEFTCoeffEW("CHbox")
                    + 3988231. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 57226150. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 3988231. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 74608.5 * getSMEFTCoeffEW("CHD")
                    + 1256970. * getSMEFTCoeffEW("CHB")
                    + 155358. * getSMEFTCoeffEW("CHW")
                    + 1542655. * getSMEFTCoeffEW("CHWB")
                    + 0.457 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.46 * deltaaMZ()
                    - 0.46 * deltaGmu()
                    - 0.828 * deltaMz()
                    - 0.047 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 30.) {
            mu +=
                    +121314. * getSMEFTCoeffEW("CHbox")
                    + 50871646. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 2614134. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 50871646. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 67535.5 * getSMEFTCoeffEW("CHD")
                    - 516385. * getSMEFTCoeffEW("CHB")
                    + 1928805. * getSMEFTCoeffEW("CHW")
                    - 264072. * getSMEFTCoeffEW("CHWB")
                    - 4.233 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.23 * deltaaMZ()
                    + 4.23 * deltaGmu()
                    + 8.55 * deltaMz()
                    - 0.047 * deltaMh());
 
        } else if (Pol_em == 80. && Pol_ep == 0.) {
            mu +=
                    +121250. * getSMEFTCoeffEW("CHbox")
                    + 6958750. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 53762500. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 6958750. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 65589.3 * getSMEFTCoeffEW("CHD")
                    + 1144464. * getSMEFTCoeffEW("CHB")
                    + 267732. * getSMEFTCoeffEW("CHW")
                    + 1428214. * getSMEFTCoeffEW("CHWB")
                    + 0.16 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.163 * deltaaMZ()
                    - 0.163 * deltaGmu()
                    - 0.234 * deltaMz()
                    - 0.047 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 0.) {
            mu +=
                    +121278. * getSMEFTCoeffEW("CHbox")
                    + 49094486. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 4685522. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 49094486. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 62150.9 * getSMEFTCoeffEW("CHD")
                    - 450090. * getSMEFTCoeffEW("CHB")
                    + 1861602. * getSMEFTCoeffEW("CHW")
                    - 195621. * getSMEFTCoeffEW("CHWB")
                    - 4.055 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.052 * deltaaMZ()
                    + 4.052 * deltaGmu()
                    + 8.195 * deltaMz()
                    - 0.047 * deltaMh());
 
        } else {
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZHPol()");
        }
 
    } else if (sqrt_s == 1.5) {
 
        C1 = -0.0011; // Use the same as 1400 GeV
 
        if (Pol_em == 80. && Pol_ep == -30.) {
            mu +=
                    +121268. * getSMEFTCoeffEW("CHbox")
                    + 4578315. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 65691823. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 4578315. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 74595.2 * getSMEFTCoeffEW("CHD")
                    + 1262261. * getSMEFTCoeffEW("CHB")
                    + 155435. * getSMEFTCoeffEW("CHW")
                    + 1547379. * getSMEFTCoeffEW("CHWB")
                    + 0.457 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.46 * deltaaMZ()
                    - 0.46 * deltaGmu()
                    - 0.84 * deltaMz()
                    - 0.041 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 30.) {
            mu +=
                    +121277. * getSMEFTCoeffEW("CHbox")
                    + 58398883. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 3000385. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 58398883. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 67535.8 * getSMEFTCoeffEW("CHD")
                    - 518798. * getSMEFTCoeffEW("CHB")
                    + 1936613. * getSMEFTCoeffEW("CHW")
                    - 264171. * getSMEFTCoeffEW("CHWB")
                    - 4.233 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.23 * deltaaMZ()
                    + 4.23 * deltaGmu()
                    + 8.539 * deltaMz()
                    - 0.041 * deltaMh());
 
        } else if (Pol_em == 80. && Pol_ep == 0.) {
            mu +=
                    +121289. * getSMEFTCoeffEW("CHbox")
                    + 7988570. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 61718691. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 7988570. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 65599. * getSMEFTCoeffEW("CHD")
                    + 1149083. * getSMEFTCoeffEW("CHB")
                    + 268317. * getSMEFTCoeffEW("CHW")
                    + 1432777. * getSMEFTCoeffEW("CHWB")
                    + 0.16 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.163 * deltaaMZ()
                    - 0.163 * deltaGmu()
                    - 0.246 * deltaMz()
                    - 0.041 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 0.) {
            mu +=
                    +121259. * getSMEFTCoeffEW("CHbox")
                    + 56356946. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 5378233. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 56356946. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 62168.7 * getSMEFTCoeffEW("CHD")
                    - 452149. * getSMEFTCoeffEW("CHB")
                    + 1869136. * getSMEFTCoeffEW("CHW")
                    - 195562. * getSMEFTCoeffEW("CHWB")
                    - 4.055 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.052 * deltaaMZ()
                    + 4.052 * deltaGmu()
                    + 8.183 * deltaMz()
                    - 0.041 * deltaMh());
 
        } else {
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZHPol()");
        }
 
    } else if (sqrt_s == 3.0) {
 
        C1 = -0.00054;
 
        if (Pol_em == 80. && Pol_ep == -30.) {
            mu +=
                    +121320. * getSMEFTCoeffEW("CHbox")
                    + 18314161. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 262773345. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 18314161. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 74663.6 * getSMEFTCoeffEW("CHD")
                    + 1289569. * getSMEFTCoeffEW("CHB")
                    + 155612. * getSMEFTCoeffEW("CHW")
                    + 1572580. * getSMEFTCoeffEW("CHWB")
                    + 0.456 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.46 * deltaaMZ()
                    - 0.46 * deltaGmu()
                    - 0.899 * deltaMz()
                    - 0.01 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 30.) {
            mu +=
                    +121305. * getSMEFTCoeffEW("CHbox")
                    + 233598342. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 12002450. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 233598342. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 67507.7 * getSMEFTCoeffEW("CHD")
                    - 531387. * getSMEFTCoeffEW("CHB")
                    + 1976750. * getSMEFTCoeffEW("CHW")
                    - 264661. * getSMEFTCoeffEW("CHWB")
                    - 4.233 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.23 * deltaaMZ()
                    + 4.23 * deltaGmu()
                    + 8.48 * deltaMz()
                    - 0.01 * deltaMh());
 
        } else if (Pol_em == 80. && Pol_ep == 0.) {
            mu +=
                    +121225. * getSMEFTCoeffEW("CHbox")
                    + 31953446. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 246870182. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 31953446. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    + 65576.5 * getSMEFTCoeffEW("CHD")
                    + 1173703. * getSMEFTCoeffEW("CHB")
                    + 270983. * getSMEFTCoeffEW("CHW")
                    + 1456032. * getSMEFTCoeffEW("CHWB")
                    + 0.16 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (+2.163 * deltaaMZ()
                    - 0.163 * deltaGmu()
                    - 0.305 * deltaMz()
                    - 0.01 * deltaMh());
 
        } else if (Pol_em == -80. && Pol_ep == 0.) {
            mu +=
                    +121248. * getSMEFTCoeffEW("CHbox")
                    + 225427310. * getSMEFTCoeffEW("CHl1R", 0, 0)
                    - 21505526. * getSMEFTCoeffEW("CHeR", 0, 0)
                    + 225427310. * getSMEFTCoeffEW("CHl3R", 0, 0)
                    - 62193.4 * getSMEFTCoeffEW("CHD")
                    - 463403. * getSMEFTCoeffEW("CHB")
                    + 1907593. * getSMEFTCoeffEW("CHW")
                    - 195017. * getSMEFTCoeffEW("CHWB")
                    - 4.054 * delta_GF
                    ;
 
            // Add modifications due to small variations of the SM parameters    
            mu += cHSM * (-2.052 * deltaaMZ()
                    + 4.052 * deltaGmu()
                    + 8.124 * deltaMz()
                    - 0.01 * deltaMh());
 
        } else {
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZHPol()");
        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mueeZHPol()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eeeZHint + eeeZHpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mueeZllH()

const double NPSMEFTd6General::mueeZllH	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}$ between the $ e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- $ associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}$

Reimplemented from NPbase.

Definition at line 23882 of file NPSMEFTd6General.cpp.

                                                                                                           {
    
    if ( (Pol_em != 0.) || (Pol_ep != 0) ) return mueeZllHPol(sqrt_s, Pol_em, Pol_ep);
 
    //  The signal strength eeZH
    double mu = mueeZH(sqrt_s, 0., 0.);
 
    //  The (relative) linear correction to the Z>ll BR
    double deltaBRratio;
 
    deltaBRratio = deltaGamma_Zf(leptons[ELECTRON])
            + deltaGamma_Zf(leptons[MU]);
 
    deltaBRratio = deltaBRratio /
            (trueSM.GammaZ(leptons[ELECTRON]) + trueSM.GammaZ(leptons[MU]));
 
    deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
 
    return mu + deltaBRratio;
}

◆ mueeZllHPol()

const double NPSMEFTd6General::mueeZllHPol	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}$ between the $ e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- $ associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}$

Definition at line 24835 of file NPSMEFTd6General.cpp.

                                                                                                              {
 
    //  The signal strength eeZH
    double mu = mueeZHPol(sqrt_s, Pol_em, Pol_ep);
 
    //  The (relative) linear correction to the Z>ll BR
    double deltaBRratio;
 
    deltaBRratio = deltaGamma_Zf(leptons[ELECTRON])
            + deltaGamma_Zf(leptons[MU]);
 
    deltaBRratio = deltaBRratio /
            (trueSM.GammaZ(leptons[ELECTRON]) + trueSM.GammaZ(leptons[MU]));
 
    deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
 
    return mu + deltaBRratio;
}

◆ mueeZqqH()

const double NPSMEFTd6General::mueeZqqH	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{eeZH, Z \to q \bar{q}}$ between the $ e^{+}e^{-}\to ZH, Z \to q \bar{q} $ associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eeZH, Z \to q \bar{q}}$

Reimplemented from NPbase.

Definition at line 23903 of file NPSMEFTd6General.cpp.

                                                                                                           {
    
    if ( (Pol_em != 0.) || (Pol_ep != 0) ) return mueeZqqHPol(sqrt_s, Pol_em, Pol_ep);
 
    //  The signal strength eeZH
    double mu = mueeZH(sqrt_s, 0., 0.);
 
    //  The (relative) linear correction to the Z>qq BR
    double deltaBRratio;
 
    deltaBRratio = deltaGamma_Zf(quarks[UP])
            + deltaGamma_Zf(quarks[DOWN])
            + deltaGamma_Zf(quarks[CHARM])
            + deltaGamma_Zf(quarks[STRANGE])
            + deltaGamma_Zf(quarks[BOTTOM]);
 
    deltaBRratio = deltaBRratio /
            (trueSM.GammaZ(quarks[UP]) + trueSM.GammaZ(quarks[DOWN])
            + trueSM.GammaZ(quarks[CHARM]) + trueSM.GammaZ(quarks[STRANGE])
            + trueSM.GammaZ(quarks[BOTTOM]));
 
    deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
 
    return mu + deltaBRratio;
}

◆ mueeZqqHPol()

const double NPSMEFTd6General::mueeZqqHPol	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{eeZH, Z \to q \bar{q}}$ between the $ e^{+}e^{-}\to ZH, Z \to q \bar{q} $ associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eeZH, Z \to q \bar{q}}$

Definition at line 24854 of file NPSMEFTd6General.cpp.

                                                                                                              {
 
    //  The signal strength eeZH
    double mu = mueeZHPol(sqrt_s, Pol_em, Pol_ep);
 
    //  The (relative) linear correction to the Z>qq BR
    double deltaBRratio;
 
    deltaBRratio = deltaGamma_Zf(quarks[UP])
            + deltaGamma_Zf(quarks[DOWN])
            + deltaGamma_Zf(quarks[CHARM])
            + deltaGamma_Zf(quarks[STRANGE])
            + deltaGamma_Zf(quarks[BOTTOM]);
 
    deltaBRratio = deltaBRratio /
            (trueSM.GammaZ(quarks[UP]) + trueSM.GammaZ(quarks[DOWN])
            + trueSM.GammaZ(quarks[CHARM]) + trueSM.GammaZ(quarks[STRANGE])
            + trueSM.GammaZ(quarks[BOTTOM]));
 
    deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
 
    return mu + deltaBRratio;
}

◆ muepWBF()

const double NPSMEFTd6General::muepWBF ( const double sqrt_s ) const

virtual

The ratio $\mu_{epWBF}$ between the $ e^{-} p\to \nu j H $ production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{epWBF}$

Reimplemented from NPbase.

Definition at line 22770 of file NPSMEFTd6General.cpp.

                                                                {
 
    //  2025 versions are for electron polarization -80% (1.2 and 1.3 TeV)
        
    double mu = 1.0;
    //double C1 = 0.0;
    
    double CHW = 0.0, CHWB = 0.0, CHD = 0.0, CHbox = 0.0, CHl3R11 = 0.0;
    double CHl3R22 = 0.0, CHq3R11 = 0.0, CHq3R22 = 0.0, CllR1221 = 0.0;
    double muRG = muw;
    
//  Wilson coefficients definitions 
    CHW = getSMEFTCoeff("CHW", muRG); 
    CHWB = getSMEFTCoeff("CHWB", muRG); 
    CHD = getSMEFTCoeff("CHD", muRG); 
    CHbox = getSMEFTCoeff("CHbox", muRG); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CHq3R11 = getSMEFTCoeff("CHq3R",0,0, muRG); 
    CHq3R22 = getSMEFTCoeff("CHq3R",1,1, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG); 
 
    if (sqrt_s == 1.2) {
 
        //C1 = 0.0;
        
        mu += cWsch * (
                -89863.9 * CHW 
                +1384.83 * CHWB 
                -29993.1 * CHD 
                +121095. * CHbox 
                -331289. * CHl3R11 
                -181498. * CHl3R22 
                -139640. * CHq3R11 
                -9061.74 * CHq3R22 
                +181670. * CllR1221 
                );
 
    } else if (sqrt_s == 1.3) {
        
        //C1 = 0.0;
        
        mu += cWsch * (
                -84713.5 * CHW 
                +2452.67 * CHWB 
                -29561.7 * CHD 
                +121718. * CHbox 
                -335293. * CHl3R11 
                -181119. * CHl3R22 
                -143207. * CHq3R11 
                -10057.4 * CHq3R22 
                +181876. * CllR1221 
                );
 
    } else if (sqrt_s == 1.8) {
        
    //  Only Alpha scheme
 
        mu +=
                +121867. * getSMEFTCoeffEW("CHbox")
                - 182643. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 181961. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 202400. * getSMEFTCoeffEW("CHD")
                - 78295.8 * getSMEFTCoeffEW("CHW")
                - 377193. * getSMEFTCoeffEW("CHWB")
                - 4.672 * delta_GF
                - 4.637 * deltaMwd6()
                ;
 
        //        if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
 
        //        }
 
    } else if (sqrt_s == 3.5) {
        
    //  Only Alpha scheme
 
        mu +=
                +121250. * getSMEFTCoeffEW("CHbox")
                - 216885. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 218544. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 202390. * getSMEFTCoeffEW("CHD")
                - 64783.2 * getSMEFTCoeffEW("CHW")
                - 377727. * getSMEFTCoeffEW("CHWB")
                - 4.688 * delta_GF
                - 4.573 * deltaMwd6()
                ;
 
        //        if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
 
        //        }
 
    } else if (sqrt_s == 5.0) {
 
        mu +=
                +119662. * getSMEFTCoeffEW("CHbox")
                - 237868. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 236470. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 203294. * getSMEFTCoeffEW("CHD")
                - 60911. * getSMEFTCoeffEW("CHW")
                - 378045. * getSMEFTCoeffEW("CHWB")
                - 4.667 * delta_GF
                - 4.437 * deltaMwd6()
                ;
 
        //        if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
 
        //        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::muepWBF()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eepWBFint + eepWBFpar;
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muepZBF()

const double NPSMEFTd6General::muepZBF ( const double sqrt_s ) const

virtual

The ratio $\mu_{epZBF}$ between the $ e^{-} p\to e^{-} j H $ production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{epZBF}$

Reimplemented from NPbase.

Definition at line 22893 of file NPSMEFTd6General.cpp.

                                                                {
 
    //  2025 versions are for electron polarization -80% (1.2 and 1.3 TeV)
    
    double mu = 1.0;
    //double C1 = 0.0;
    
    double CHB = 0.0, CHW = 0.0, CHWB = 0.0, CHD = 0.0, CHbox = 0.0, CHl1R11 = 0.0;
    double CHl3R11 = 0.0, CHl3R22 = 0.0, CHeR11 = 0.0, CHq1R11 = 0.0, CHq3R11 = 0.0;
    double CHq1R22 = 0.0, CHq3R22 = 0.0, CHuR11 = 0.0, CHuR22 = 0.0, CHdR11 = 0.0, CHdR22 = 0.0, CllR1221 = 0.0; 
    double muRG = muw;
    
//  Wilson coefficients definitions 
    CHB = getSMEFTCoeff("CHB", muRG); 
    CHW = getSMEFTCoeff("CHW", muRG); 
    CHWB = getSMEFTCoeff("CHWB", muRG); 
    CHD = getSMEFTCoeff("CHD", muRG); 
    CHbox = getSMEFTCoeff("CHbox", muRG); 
    CHl1R11 = getSMEFTCoeff("CHl1R",0,0, muRG); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CHeR11 = getSMEFTCoeff("CHeR",0,0, muRG); 
    CHq1R11 = getSMEFTCoeff("CHq1R",0,0, muRG); 
    CHq3R11 = getSMEFTCoeff("CHq3R",0,0, muRG); 
    CHq1R22 = getSMEFTCoeff("CHq1R",1,1, muRG); 
    CHq3R22 = getSMEFTCoeff("CHq3R",1,1, muRG); 
    CHuR11 = getSMEFTCoeff("CHuR",0,0, muRG); 
    CHuR22 = getSMEFTCoeff("CHuR",1,1, muRG); 
    CHdR11 = getSMEFTCoeff("CHdR",0,0, muRG); 
    CHdR22 = getSMEFTCoeff("CHdR",1,1, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG);
 
    if (sqrt_s == 1.2) {
 
        //C1 = 0.0;
        
        mu += cWsch * (
                -45626.8 * CHB 
                -233105. * CHW 
                +322530. * CHWB 
                +153678. * CHD 
                +122298. * CHbox 
                -223465. * CHl1R11 
                -405483. * CHl3R11 
                -180952. * CHl3R22 
                +19607.3 * CHeR11 
                +38972.5 * CHq1R11 
                -141632. * CHq3R11 
                -5274.11 * CHq1R22 
                -14946.6 * CHq3R22 
                -34549.1 * CHuR11 
                -1967. * CHuR22 
                +10146.9 * CHdR11 
                +1521.41 * CHdR22 
                +183749. * CllR1221 
                );
 
    } else if (sqrt_s == 1.3) {
        
        //C1 = 0.0;
        
        mu += cWsch * (
                -40452.1 * CHB 
                -222889. * CHW 
                +314229. * CHWB 
                +153151. * CHD 
                +120937. * CHbox 
                -232181. * CHl1R11 
                -414451. * CHl3R11 
                -182056. * CHl3R22 
                +19001.5 * CHeR11 
                +36594.9 * CHq1R11 
                -146957. * CHq3R11 
                -5715.25 * CHq1R22 
                -16408.9 * CHq3R22 
                -35934.4 * CHuR11 
                -2333.7 * CHuR22 
                +10800.1 * CHdR11 
                +1501.27 * CHdR22 
                +182692. * CllR1221
                );
 
    } else if (sqrt_s == 1.8) {
        
        //  Only Alpha scheme
 
        mu +=
                +120218. * getSMEFTCoeffEW("CHbox")
                - 173566. * getSMEFTCoeffEW("CHl1R", 0, 0)
                + 26307.1 * getSMEFTCoeffEW("CHq1R", 0, 0)
                + 142600. * getSMEFTCoeffEW("CHeR", 0, 0)
                - 47449. * getSMEFTCoeffEW("CHuR", 0, 0)
                + 14356.2 * getSMEFTCoeffEW("CHdR", 0, 0)
                - 173566. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 188606. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 174301. * getSMEFTCoeffEW("CHD")
                - 19800. * getSMEFTCoeffEW("CHB")
                - 103254. * getSMEFTCoeffEW("CHW")
                - 89049.2 * getSMEFTCoeffEW("CHWB")
                - 3.714 * delta_GF
                ;
 
        //        if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
 
        //        }
 
    } else if (sqrt_s == 3.5) {
        
        //  Only Alpha scheme
 
        mu +=
                +123119. * getSMEFTCoeffEW("CHbox")
                - 206981. * getSMEFTCoeffEW("CHl1R", 0, 0)
                + 18620.9 * getSMEFTCoeffEW("CHq1R", 0, 0)
                + 177706. * getSMEFTCoeffEW("CHeR", 0, 0)
                - 53822. * getSMEFTCoeffEW("CHuR", 0, 0)
                + 20491.5 * getSMEFTCoeffEW("CHdR", 0, 0)
                - 206981. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 227549. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 172298. * getSMEFTCoeffEW("CHD")
                - 6887.17 * getSMEFTCoeffEW("CHB")
                - 79245. * getSMEFTCoeffEW("CHW")
                - 103223. * getSMEFTCoeffEW("CHWB")
                - 3.721 * delta_GF
                ;
 
        //        if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
 
        //        }
 
    } else if (sqrt_s == 5.0) {
        
        //  Only Alpha scheme
 
        mu +=
                +121709. * getSMEFTCoeffEW("CHbox")
                - 225267. * getSMEFTCoeffEW("CHl1R", 0, 0)
                + 13471.8 * getSMEFTCoeffEW("CHq1R", 0, 0)
                + 193542. * getSMEFTCoeffEW("CHeR", 0, 0)
                - 57640.9 * getSMEFTCoeffEW("CHuR", 0, 0)
                + 22573. * getSMEFTCoeffEW("CHdR", 0, 0)
                - 225267. * getSMEFTCoeffEW("CHl3R", 0, 0)
                - 247738. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 172768. * getSMEFTCoeffEW("CHD")
                - 4524.89 * getSMEFTCoeffEW("CHB")
                - 71935.4 * getSMEFTCoeffEW("CHW")
                - 104998. * getSMEFTCoeffEW("CHWB")
                - 3.71 * delta_GF
                ;
 
        //        if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
 
        //        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::muepZBF()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eepZBFint + eepZBFpar;
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muggH()

const double NPSMEFTd6General::muggH ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH}$ between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH}$

Reimplemented from NPbase.

Definition at line 18037 of file NPSMEFTd6General.cpp.

{
    double mu = 1.0;
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eggFint + eggFpar;
 
    // Linear contribution (including the Higgs self-coupling)
    mu += delta_muggH_1(sqrt_s);
 
    // Quadratic contribution (including the Higgs self-coupling)
    mu += delta_muggH_2(sqrt_s);
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muggHbb()

const double NPSMEFTd6General::muggHbb ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,bb}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,bb}$

Reimplemented from NPbase.

Definition at line 35867 of file NPSMEFTd6General.cpp.

                                                                {
    return muggH(sqrt_s) * BrHbbRatio();
 
}

◆ muggHgaga()

const double NPSMEFTd6General::muggHgaga ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,\gamma\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 35627 of file NPSMEFTd6General.cpp.

                                                                  {
    return muggH(sqrt_s) * BrHgagaRatio();
 
}

◆ muggHH()

const double NPSMEFTd6General::muggHH ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggHH}$ between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].)

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggHH}$

Reimplemented from NPbase.

Definition at line 20309 of file NPSMEFTd6General.cpp.

                                                               {
    double mu = 1.0;
    double A1HH = 0.0, A2HH = 0.0, A3HH = 0.0, A4HH = 0.0, A5HH = 0.0;
    double A6HH = 0.0, A7HH = 0.0, A8HH = 0.0, A9HH = 0.0, A10HH = 0.0;
    double A11HH = 0.0, A12HH = 0.0, A13HH = 0.0, A14HH = 0.0, A15HH = 0.0;
    double ct, c2t, c3, cg, c2g;
 
    if (sqrt_s == 14.0) {
 
        // From the cut-based analysis. Table IV
 
        A1HH = 1.70;
        A2HH = 10.7;
        A3HH = 0.117;
        A4HH = 6.11;
        A5HH = 217.0;
        A6HH = -7.56;
        A7HH = -0.819;
        A8HH = 1.95;
        A9HH = 10.90;
        A10HH = 51.6;
        A11HH = -3.86;
        A12HH = -12.5;
        A13HH = 1.46;
        A14HH = 5.49;
        A15HH = 58.4;
 
    } else if (sqrt_s == 100.0) {
 
        // From the cut-based analysis. Table IV
 
        A1HH = 1.59;
        A2HH = 12.8;
        A3HH = 0.090;
        A4HH = 5.2;
        A5HH = 358.0;
        A6HH = -7.66;
        A7HH = -0.681;
        A8HH = 1.83;
        A9HH = 9.25;
        A10HH = 51.2;
        A11HH = -2.61;
        A12HH = -7.35;
        A13HH = 1.03;
        A14HH = 4.65;
        A15HH = 65.5;
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::muggHH()");
 
    ct = 1.0 - 0.5 * delta_GF + delta_h - v() * getSMEFTCoeffEW("CuHR", 2, 2) * v2 / sqrt(2.0) / mtpole;
    c2t = delta_h - 3.0 * v() * getSMEFTCoeffEW("CuHR", 2, 2) * v2 / 2.0 / sqrt(2.0) / mtpole;
    c3 = 1.0 + deltaG_hhhRatio();
    cg = M_PI * getSMEFTCoeffEW("CHG") * v2 / AlsMz;
    c2g = cg;
 
    // In the SM the Eq. returns 0.999. Fix that small offset by adding 0.0010    
    mu = 0.0010 + A1HH * ct * ct * ct * ct +
            A2HH * c2t * c2t +
            A3HH * ct * ct * c3 * c3 +
            A4HH * cg * cg * c3 * c3 +
            A5HH * c2g * c2g +
            A6HH * c2t * ct * ct +
            A7HH * ct * ct * ct * c3 +
            A8HH * c2t * ct * c3 +
            A9HH * c2t * cg * c3 +
            A10HH * c2t * c2g +
            A11HH * ct * ct * cg * c3 +
            A12HH * ct * ct * c2g +
            A13HH * ct * c3 * c3 * cg +
            A14HH * ct * c3 * c2g +
            A15HH * cg * c3*c2g;
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muggHmumu()

const double NPSMEFTd6General::muggHmumu ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,\mu\mu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 35807 of file NPSMEFTd6General.cpp.

                                                                  {
    return muggH(sqrt_s) * BrHmumuRatio();
 
}

◆ muggHpttH()

const double NPSMEFTd6General::muggHpttH ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH+ttH}$ between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH+ttH}$

Reimplemented from NPbase.

Definition at line 25106 of file NPSMEFTd6General.cpp.

                                                                  {
    double sigmaggH_SM = computeSigmaggH(sqrt_s);
    double sigmattH_SM = computeSigmattH(sqrt_s);
    double sigmaggH = muggH(sqrt_s) * sigmaggH_SM;
    double sigmattH = muttH(sqrt_s) * sigmattH_SM;
 
    double mu = ((sigmaggH + sigmattH) / (sigmaggH_SM + sigmattH_SM));
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muggHtautau()

const double NPSMEFTd6General::muggHtautau ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,\tau\tau}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 35837 of file NPSMEFTd6General.cpp.

                                                                    {
    return muggH(sqrt_s) * BrHtautauRatio();
 
}

◆ muggHWW()

const double NPSMEFTd6General::muggHWW ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,WW}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,WW}$

Reimplemented from NPbase.

Definition at line 35747 of file NPSMEFTd6General.cpp.

                                                                {
    return muggH(sqrt_s) * BrHWWRatio();
 
}

◆ muggHWW2l2v()

const double NPSMEFTd6General::muggHWW2l2v ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,WW\to 2l2\nu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 35777 of file NPSMEFTd6General.cpp.

                                                                    {
    return muggH(sqrt_s) * BrHWW2l2vRatio();
 
}

◆ muggHZga()

const double NPSMEFTd6General::muggHZga ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,Z\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 35657 of file NPSMEFTd6General.cpp.

                                                                 {
    return muggH(sqrt_s) * BrHZgaRatio();
 
}

◆ muggHZZ()

const double NPSMEFTd6General::muggHZZ ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,ZZ}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,ZZ}$

Reimplemented from NPbase.

Definition at line 35687 of file NPSMEFTd6General.cpp.

                                                                {
    return muggH(sqrt_s) * BrHZZRatio();
 
}

◆ muggHZZ4l()

const double NPSMEFTd6General::muggHZZ4l ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,ZZ\to 4l}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 35717 of file NPSMEFTd6General.cpp.

                                                                  {
    return muggH(sqrt_s) * BrHZZ4lRatio();
 
}

◆ mummH()

const double NPSMEFTd6General::mummH ( const double sqrt_s ) const

virtual

The ratio $\mu_{\mu\mu H}$ between the $\sigma(\mu \mu \to H)}$ production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{\mu\mu H}$

Reimplemented from NPbase.

Definition at line 25477 of file NPSMEFTd6General.cpp.

                                                              {
    double mu = 1.0;
 
    if (sqrt_s == 0.125) {
 
        //  Peak production cross section mu mu -> H -> X = 4 pi/mH^2 * BR(H->mu mu) * BR(H-> X)
        //  Use mu mu -> H = 4 pi/mH^2 * BR(H->mu mu), so the xs BR formulae still applies
        mu = BrHmumuRatio();
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mummH()");
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mummHmm()

const double NPSMEFTd6General::mummHmm ( const double sqrt_s ) const

virtual

The ratio $\mu_{\mu\mu H\mu\mu}$ between the $\sigma(\mu \mu \to H \mu \mu)}$ production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{\mu\mu H\mu\mu}$

Reimplemented from NPbase.

Definition at line 25687 of file NPSMEFTd6General.cpp.

                                                                {
 
    //  Mw scheme
 
    double mu = 1.0;
 
    double C1 = 0.0;
 
    // Wilson coefficients and scale    
    double CHB = 0.0, CHW = 0.0, CHWB = 0.0, CHD = 0.0, CHbox = 0.0, CHl1R22 = 0.0;
    double CHl3R11 = 0.0, CHl3R22 = 0.0, CHeR22 = 0.0, CllR1221 = 0.0;
    double muRG = 0;
    
    double scalTH = 1.0;
    
    if ( sqrt_s > 0.5 ) {
        // Theory uncert. scaling like log^2(E/MW)
        
        scalTH = log(sqrt_s/0.080365)/log(0.5/0.080365);
        scalTH = scalTH * scalTH;
    }
    
    // RG scale in GeV
    muRG = 1000. * sqrt_s;
    
//  Wilson coefficients definitions 
    CHB = getSMEFTCoeff("CHB", muRG); 
    CHW = getSMEFTCoeff("CHW", muRG); 
    CHWB = getSMEFTCoeff("CHWB", muRG); 
    CHD = getSMEFTCoeff("CHD", muRG); 
    CHbox = getSMEFTCoeff("CHbox", muRG); 
    CHl1R22 = getSMEFTCoeff("CHl1R",1,1, muRG); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CHeR22 = getSMEFTCoeff("CHeR",1,1, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG); 
    
    // Defined as (unpolarized) mu+ mu- > H mu+ mu-. At these energies it is mostly ZBF
 
    if (sqrt_s == 3.0) {
 
        C1 = 0.0063; // Use the same as CLIC
 
        mu += cWsch * (
                +8523.28 * CHB 
                -36317.7 * CHW 
                +24490.5 * CHWB 
                +8511.15 * CHD 
                +120628. * CHbox 
                -564246. * CHl1R22 
                -182191. * CHl3R11 
                -745892. * CHl3R22 
                +456271. * CHeR22 
                +181186. * CllR1221 
                );
 
    } else if (sqrt_s == 10.0) {
 
        C1 = 0.0; //NA
 
        mu += cWsch * (
                -562.405 * CHB 
                -27961.5 * CHW 
                +35431.1 * CHWB 
                +8154.94 * CHD 
                +119971. * CHbox 
                -920487. * CHl1R22 
                -182505. * CHl3R11 
                -1101897. * CHl3R22 
                +742050. * CHeR22 
                +181016. * CllR1221 
                );
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mummHmm()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    //(Assume similar to WBF.)
    mu += scalTH * eeeWBFint + eeeWBFpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mummHNWA()

const double NPSMEFTd6General::mummHNWA ( const double sqrt_s ) const

virtual

The ratio $\mu_{\mu\mu H}$ between the $\sigma(\mu \mu \to H)}$ production cross-section in the current model and in the Standard Model, in the narrow width approximation.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{\mu\mu H}$

Reimplemented from NPbase.

Definition at line 25494 of file NPSMEFTd6General.cpp.

                                                                 {
    double mu = 1.0;
 
    double dymu = deltaG_hff(leptons[MU]).real();
    double ymuSM = -(leptons[MU].getMass()) / v();
 
    //  The ratio is given by a scaling of the muon Yukawa.
    mu = 1.0 + 2.0 * dymu / ymuSM;
 
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        mu += dymu * dymu / ymuSM / ymuSM;
    }
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mummHvv()

const double NPSMEFTd6General::mummHvv ( const double sqrt_s ) const

virtual

The ratio $\mu_{\mu\mu H\nu\nu}$ between the $\sigma(\mu \mu \to H \nu \nu)}$ production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{\mu\mu H\nu\nu}$

Reimplemented from NPbase.

Definition at line 25597 of file NPSMEFTd6General.cpp.

                                                                {
 
    //  Mw scheme
 
    double mu = 1.0;
 
    double C1 = 0.0;
    
    // Wilson coefficients and scale 
    double CHB = 0.0, CHW = 0.0, CHWB = 0.0, CHD = 0.0, CHbox = 0.0, CHl1R22 = 0.0;
    double CHl3R11 = 0.0, CHl3R22 = 0.0, CHeR22 = 0.0, CllR1221 = 0.0;
    double muRG = 0;
    
    double scalTH = 1.0;
    
    if ( sqrt_s > 0.5 ) {
        // Theory uncert. scaling like log^2(E/MW)
        
        scalTH = log(sqrt_s/0.080365)/log(0.5/0.080365);
        scalTH = scalTH * scalTH;
    }
    
    // RG scale in GeV
    muRG = 1000. * sqrt_s;
    
//  Wilson coefficients definitions 
    CHB = getSMEFTCoeff("CHB", muRG); 
    CHW = getSMEFTCoeff("CHW", muRG); 
    CHWB = getSMEFTCoeff("CHWB", muRG); 
    CHD = getSMEFTCoeff("CHD", muRG); 
    CHbox = getSMEFTCoeff("CHbox", muRG); 
    CHl1R22 = getSMEFTCoeff("CHl1R",1,1, muRG); 
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CHeR22 = getSMEFTCoeff("CHeR",1,1, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG); 
 
    //  For the Higgs trilinear dependence assume the WBF mechanism dominates
    
    // Defined as (unpolarized) mu+ mu- > H vm vm~. At these energies it is mostly WBF
 
    if (sqrt_s == 3.0) {
 
        C1 = 0.0057; // Use the same as CLIC
 
        mu += cWsch * (
                -189.453 * CHB 
                -40354.5 * CHW 
                -498.257 * CHWB 
                -30770. * CHD 
                +120184. * CHbox 
                +23876.8 * CHl1R22 
                -182919. * CHl3R11 
                -833760. * CHl3R22 
                -21601.8 * CHeR22 
                +181050. * CllR1221 
                );
 
    } else if (sqrt_s == 10.0) {
 
        C1 = 0.0; // NA
 
        mu += cWsch * (
                -578.66 * CHB 
                -27152.7 * CHW 
                -101.506 * CHWB 
                -30749.2 * CHD 
                +120814. * CHbox 
                +14588.5 * CHl1R22 
                -182384. * CHl3R11 
                -1117285. * CHl3R22 
                -13721. * CHeR22 
                +181019. * CllR1221 
                );
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mummHvv()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += scalTH * eeeWBFint + eeeWBFpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mummttH()

const double NPSMEFTd6General::mummttH ( const double sqrt_s ) const

virtual

The ratio $\mu_{\mu\mu ttH}$ between the $\sigma(\mu \mu \to t\bar{t} H )}$ production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{\mu\mu ttH}$

Reimplemented from NPbase.

Definition at line 25776 of file NPSMEFTd6General.cpp.

                                                                {
 
    // Only Alpha scheme
 
    double mu = 1.0;
 
    double C1 = 0.0;
    
    double muRG = 0;
    
    // RG scale in GeV
    muRG = 1000. * sqrt_s;
 
    if (sqrt_s == 3.0) {
 
        C1 = 0.0037; // Use the same as CLIC
 
        mu +=
                +121703. * getSMEFTCoeffEW("CHbox")
                - 105827. * getSMEFTCoeffEW("CuHR", 2, 2)
                - 60143.2 * getSMEFTCoeffEW("CHD")
                + 696642. * getSMEFTCoeffEW("CHB")
                + 749580. * getSMEFTCoeffEW("CHW")
                - 625570. * getSMEFTCoeffEW("CHWB")
                + 8600327. * getSMEFTCoeffEW("CuWR", 2, 2)
                + 10933756. * getSMEFTCoeffEW("CuBR", 2, 2)
                + 19536100. * getSMEFTCoeffEW("CHl1R", 1, 1)
                - 16360523. * getSMEFTCoeffEW("CHeR", 1, 1)
                + 22577.7 * getSMEFTCoeffEW("CHuR", 2, 2)
                - 120.094 * getSMEFTCoeffEW("CHl3R", 0, 0)
                + 19529711. * getSMEFTCoeffEW("CHl3R", 1, 1)
                - 2.244 * delta_GF
                + 4.309 * -0.5 * (getSMEFTCoeffEW("CHq1R", 2, 2) - getSMEFTCoeffEW("CHq3R", 2, 2)) * v2
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (+2.486 * deltaMz()
                - 0.594 * deltaMh()
                + 0.777 * deltaaMZ()
                + 2.227 * deltaGmu()
                + 2.183 * deltamt());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else if (sqrt_s == 10.0) {
 
        C1 = 0.0037; //NA
 
        mu +=
                +121697. * getSMEFTCoeffEW("CHbox")
                - 99433. * getSMEFTCoeffEW("CuHR", 2, 2)
                - 59412.6 * getSMEFTCoeffEW("CHD")
                + 977027. * getSMEFTCoeffEW("CHB")
                + 1069899. * getSMEFTCoeffEW("CHW")
                - 816019. * getSMEFTCoeffEW("CHWB")
                + 48598343. * getSMEFTCoeffEW("CuWR", 2, 2)
                + 62025699. * getSMEFTCoeffEW("CuBR", 2, 2)
                + 300770201. * getSMEFTCoeffEW("CHl1R", 1, 1)
                - 257079386. * getSMEFTCoeffEW("CHeR", 1, 1)
                + 37385. * getSMEFTCoeffEW("CHuR", 2, 2)
                - 36.349 * getSMEFTCoeffEW("CHl3R", 0, 0)
                + 299984515. * getSMEFTCoeffEW("CHl3R", 1, 1)
                - 2.329 * delta_GF
                + 5.129 * -0.5 * (getSMEFTCoeffEW("CHq1R", 2, 2) - getSMEFTCoeffEW("CHq3R", 2, 2)) * v2
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (+2.661 * deltaMz()
                - 0.39 * deltaMh()
                + 0.693 * deltaaMZ()
                + 2.295 * deltaGmu()
                + 2.081 * deltamt());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mummttH()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eeettHint + eeettHpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mummZH()

const double NPSMEFTd6General::mummZH ( const double sqrt_s ) const

virtual

The ratio $\mu_{\mu\mu ZH}$ between the $\sigma(\mu \mu \to Z H)}$ production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{\mu\mu ZH}$

Reimplemented from NPbase.

Definition at line 25513 of file NPSMEFTd6General.cpp.

                                                               {
 
    // Only Alpha scheme
 
    double mu = 1.0;
 
    double C1 = 0.0;
    
    double muRG = 0;
    
    // RG scale in GeV
    muRG = 1000. * sqrt_s;
 
    if (sqrt_s == 3.0) {
 
        C1 = -0.00054; // Use the same as CLIC
 
        mu +=
                +120311. * getSMEFTCoeffEW("CHbox")
                - 5772.03 * getSMEFTCoeffEW("CHD")
                + 253308. * getSMEFTCoeffEW("CHB")
                + 1178831. * getSMEFTCoeffEW("CHW")
                + 526388. * getSMEFTCoeffEW("CHWB")
                + 139222448. * getSMEFTCoeffEW("CHl1R", 1, 1)
                - 119515557. * getSMEFTCoeffEW("CHeR", 1, 1)
                + 0. * getSMEFTCoeffEW("CHl3R", 0, 0)
                + 139217069. * getSMEFTCoeffEW("CHl3R", 1, 1)
                - 2.19 * delta_GF
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (+4.384 * deltaMz()
                - 0.009 * deltaMh()
                - 0.198 * deltaaMZ()
                + 2.199 * deltaGmu());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else if (sqrt_s == 10.0) {
 
        C1 = 0.0; // NA
 
        mu +=
                +110705. * getSMEFTCoeffEW("CHbox")
                - 2881.46 * getSMEFTCoeffEW("CHD")
                + 234510. * getSMEFTCoeffEW("CHB")
                + 1090997. * getSMEFTCoeffEW("CHW")
                + 487384. * getSMEFTCoeffEW("CHWB")
                + 1423231114. * getSMEFTCoeffEW("CHl1R", 1, 1)
                - 1221737534. * getSMEFTCoeffEW("CHeR", 1, 1)
                + 74.649 * getSMEFTCoeffEW("CHl3R", 0, 0)
                + 1423208868. * getSMEFTCoeffEW("CHl3R", 1, 1)
                - 2.096 * delta_GF
                ;
 
        // Add modifications due to small variations of the SM parameters    
        mu += cHSM * (+4.016 * deltaMz()
                + 0. * deltaMh()
                - 0.182 * deltaaMZ()
                + 2.183 * deltaGmu());
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mummZH()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eeeZHint + eeeZHpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio_mu(muRG);
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mupTVppWZ()

const double NPSMEFTd6General::mupTVppWZ	(	const double	sqrt_s,
		const double	pTV1,
		const double	pTV2
	)		const

virtual

The number of events in $ p p \to WZ$ in a given $p_{TV}$ bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6General class.

Returns: $N_{ev}^{p_{TV}}/N_{ev,SM}^{p_{TV}}$

Reimplemented from NPbase.

Definition at line 39289 of file NPSMEFTd6General.cpp.

                                                                                                        {
    double mu = 1.0;
 
    double cHWp = 0.0;
 
    // In the Warsaw basis the contact interactions are generated only by CiHQ3 but
    // in the modified basis ODHW also contribute
    // Master Equations below are for cHWp = Ci/Lambda^2 in units of TeV^{-2}, 
    // but LambdaNP is in GeV. Add conversion factor.
 
    cHWp = 4.0 * (sW2_tree / eeMz2) * (getSMEFTCoeffEW("CHq3R", 0, 0) ) * 1000000.0;
 
    //  Bin dependences assuming cutoff of the EFT at 5 TeV
    //  Normalize to the total number of events to remove the dependence on Lumi
    //  (Numbers correspond to 3/ab)
    if (sqrt_s == 14.0) {
 
        if (pTV1 == 100.) {
            mu += (558.0 * cHWp + 56.8 * cHWp * cHWp) / 3450.0;
 
        } else if (pTV1 == 150.) {
            mu += (410.0 * cHWp + 17.64 * cHWp * cHWp) / 2690.0;
 
        } else if (pTV1 == 220.) {
            
            cHWp = 4.0 * (sW2_tree / eeMz2) * (getSMEFTCoeff("CHq3R", 0, 0, 240.) ) * 1000000.0;
            
            mu += (266.0 * cHWp + 45.6 * cHWp * cHWp) / 925.0;
 
        } else if (pTV1 == 300.) {
            
            cHWp = 4.0 * (sW2_tree / eeMz2) * (getSMEFTCoeff("CHq3R", 0, 0, 350.) ) * 1000000.0;
            
            mu += (304.0 * cHWp + 108.0 * cHWp * cHWp) / 563.0;
 
        } else if (pTV1 == 500.) {
            
            cHWp = 4.0 * (sW2_tree / eeMz2) * (getSMEFTCoeff("CHq3R", 0, 0, 550.) ) * 1000000.0;
            
            mu += (114.40 * cHWp + 96.8 * cHWp * cHWp) / 85.1;
 
        } else if (pTV1 == 750.) {
            
            cHWp = 4.0 * (sW2_tree / eeMz2) * (getSMEFTCoeff("CHq3R", 0, 0, 1000.) ) * 1000000.0;
            
            mu += (46.20 * cHWp + 86.8 * cHWp * cHWp) / 14.9;
 
        } else {
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mupTVppWZ()");
        }
 
    } else if (sqrt_s == 27.0) {
 
        if (pTV1 == 150.) {
            mu += (824.0 * cHWp + 71.6 * cHWp * cHWp) / 5370.0;
 
        } else if (pTV1 == 220.) {
            mu += (510.0 * cHWp + 75.2 * cHWp * cHWp) / 2210.0;
 
        } else if (pTV1 == 300.) {
            mu += (808.0 * cHWp + 268.4 * cHWp * cHWp) / 1610.0;
 
        } else if (pTV1 == 500.) {
            mu += (374.0 * cHWp + 308.0 * cHWp * cHWp) / 331.0;
 
        } else if (pTV1 == 750.) {
            mu += (216.0 * cHWp + 420.0 * cHWp * cHWp) / 85.9;
 
        } else if (pTV1 == 1200.) {
            mu += (78.2 * cHWp + 325.2 * cHWp * cHWp) / 10.0;
 
        } else {
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mupTVppWZ()");
        }
 
    } else if (sqrt_s == 100.0) {
 
        if (pTV1 == 220.) {
            mu += (2000.0 * cHWp + 368.4 * cHWp * cHWp) / 8030.0;
 
        } else if (pTV1 == 300.) {
            mu += (2780.0 * cHWp + 1000.0 * cHWp * cHWp) / 7270.0;
 
        } else if (pTV1 == 500.) {
            mu += (1544.0 * cHWp + 1428.0 * cHWp * cHWp) / 2000.0;
 
        } else if (pTV1 == 750.) {
            mu += (1256.0 * cHWp + 2668.0 * cHWp * cHWp) / 717.0;
 
        } else if (pTV1 == 1200.) {
            mu += (678.0 * cHWp + 3400.0 * cHWp * cHWp) / 142.0;
 
        } else if (pTV1 == 1800.) {
            mu += (234.0 * cHWp + 2540.0 * cHWp * cHWp) / 27.5;
 
        } else {
            throw std::runtime_error("Bad argument in NPSMEFTd6General::mupTVppWZ()");
        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mupTVppWZ()");
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
 
}

◆ mutH()

const double NPSMEFTd6General::mutH ( const double sqrt_s ) const

virtual

The ratio $\mu_{tH}$ between the t-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{tH}$

Reimplemented from NPbase.

Definition at line 20243 of file NPSMEFTd6General.cpp.

{
    double mu = 1.0;
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    //mu += etHint + etHpar;
 
    // Linear contribution (including the Higgs self-coupling)
    mu += delta_mutH_1(sqrt_s);
 
    // Quadratic contribution (including the Higgs self-coupling)
    mu += delta_mutH_2(sqrt_s);
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ mutHq()

const double NPSMEFTd6General::mutHq ( const double sqrt_s ) const

virtual

The ratio $\mu_{tHq}$ between the t-q-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{tHq}$

Reimplemented from NPbase.

Definition at line 25014 of file NPSMEFTd6General.cpp.

                                                              {
    double mu = 1.0;
 
    double C1 = 0.0;
 
    if (sqrt_s == 7.0) {
 
        C1 = 0.0;
 
        mu += 0.0;
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
 
        }
 
    } else if (sqrt_s == 8.0) {
 
        C1 = 0.0;
 
        mu += 0.0;
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
 
        }
 
    } else if (sqrt_s == 13.0) {
 
        C1 = 0.0;
 
        mu += 0.0;
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
 
        }
 
    } else if (sqrt_s == 14.0) {
 
        C1 = 0.0;
 
        mu += 0.0;
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
 
        }
 
    } else if (sqrt_s == 27.0) {
 
        C1 = 0.0;
 
        mu += 0.0;
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
 
        }
 
    } else if (sqrt_s == 100.0) {
 
        C1 = 0.0;
 
        mu += 0.0;
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
 
        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::mutHq()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    //mu += etHqint + etHqpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio();
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muTHUggHbb()

const double NPSMEFTd6General::muTHUggHbb ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,bb}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,bb}$

Reimplemented from NPbase.

Definition at line 36359 of file NPSMEFTd6General.cpp.

                                                                   {
    if (FlagQuadraticTerms) {
        return ( muggH(sqrt_s) * BrHbbRatio() * (1.0 + eggFHbb) * (1.0 + eHwidth) / (1.0 + eggFint + eggFpar) / (1.0 + eHbbint + eHbbpar));
    } else {
        return ( muggH(sqrt_s) + BrHbbRatio() - 1.0 + eggFHbb - eggFint - eggFpar - eHbbint - eHbbpar + eHwidth);
    }
}

◆ muTHUggHgaga()

const double NPSMEFTd6General::muTHUggHgaga ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,\gamma\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 35903 of file NPSMEFTd6General.cpp.

                                                                     {
    if (FlagQuadraticTerms) {
        return ( muggH(sqrt_s) * BrHgagaRatio() * (1.0 + eggFHgaga) * (1.0 + eHwidth) / (1.0 + eggFint + eggFpar) / (1.0 + eHgagaint + eHgagapar));
    } else {
        return ( muggH(sqrt_s) + BrHgagaRatio() - 1.0 + eggFHgaga - eggFint - eggFpar - eHgagaint - eHgagapar + eHwidth);
    }
}

◆ muTHUggHmumu()

const double NPSMEFTd6General::muTHUggHmumu ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,\mu\mu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 36245 of file NPSMEFTd6General.cpp.

                                                                     {
    if (FlagQuadraticTerms) {
        return ( muggH(sqrt_s) * BrHmumuRatio() * (1.0 + eggFHmumu) * (1.0 + eHwidth) / (1.0 + eggFint + eggFpar) / (1.0 + eHmumuint + eHmumupar));
    } else {
        return ( muggH(sqrt_s) + BrHmumuRatio() - 1.0 + eggFHmumu - eggFint - eggFpar - eHmumuint - eHmumupar + eHwidth);
    }
}

◆ muTHUggHtautau()

const double NPSMEFTd6General::muTHUggHtautau ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,\tau\tau}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 36302 of file NPSMEFTd6General.cpp.

                                                                       {
    if (FlagQuadraticTerms) {
        return ( muggH(sqrt_s) * BrHtautauRatio() * (1.0 + eggFHtautau) * (1.0 + eHwidth) / (1.0 + eggFint + eggFpar) / (1.0 + eHtautauint + eHtautaupar));
    } else {
        return ( muggH(sqrt_s) + BrHtautauRatio() - 1.0 + eggFHtautau - eggFint - eggFpar - eHtautauint - eHtautaupar + eHwidth);
    }
}

◆ muTHUggHWW()

const double NPSMEFTd6General::muTHUggHWW ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,WW}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,WW}$

Reimplemented from NPbase.

Definition at line 36131 of file NPSMEFTd6General.cpp.

                                                                   {
    if (FlagQuadraticTerms) {
        return ( muggH(sqrt_s) * BrHWWRatio() * (1.0 + eggFHWW) * (1.0 + eHwidth) / (1.0 + eggFint + eggFpar) / (1.0 + eHWWint + eHWWpar));
    } else {
        return ( muggH(sqrt_s) + BrHWWRatio() - 1.0 + eggFHWW - eggFint - eggFpar - eHWWint - eHWWpar + eHwidth);
    }
}

◆ muTHUggHWW2l2v()

const double NPSMEFTd6General::muTHUggHWW2l2v ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,WW\to 2l2\nu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 36188 of file NPSMEFTd6General.cpp.

                                                                       {
    if (FlagQuadraticTerms) {
        return ( muggH(sqrt_s) * BrHWW2l2vRatio() * (1.0 + eggFHWW) * (1.0 + eHwidth) / (1.0 + eggFint + eggFpar) / (1.0 + eHWWint + eHWWpar));
    } else {
        return ( muggH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eggFHWW - eggFint - eggFpar - eHWWint - eHWWpar + eHwidth);
    }
}

◆ muTHUggHZga()

const double NPSMEFTd6General::muTHUggHZga ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,Z\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 35960 of file NPSMEFTd6General.cpp.

                                                                    {
    if (FlagQuadraticTerms) {
        return ( muggH(sqrt_s) * BrHZgaRatio() * (1.0 + eggFHZga) * (1.0 + eHwidth) / (1.0 + eggFint + eggFpar) / (1.0 + eHZgaint + eHZgapar));
    } else {
        return ( muggH(sqrt_s) + BrHZgaRatio() - 1.0 + eggFHZga - eggFint - eggFpar - eHZgaint - eHZgapar + eHwidth);
    }
}

◆ muTHUggHZgamumu()

const double NPSMEFTd6General::muTHUggHZgamumu ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,Z\gamma\to \gamma 2\mu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z \gamma\to \gamma 2\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,Z\gamma\to \gamma 2\mu}$

Reimplemented from NPbase.

Definition at line 36462 of file NPSMEFTd6General.cpp.

                                                                        {
    if (FlagQuadraticTerms) {
        return ( muggH(sqrt_s) * BrHZgamumuRatio() * (1.0 + eggFHZga) * (1.0 + eHwidth) / (1.0 + eggFint + eggFpar) / (1.0 + eHZgaint + eHZgapar));
    } else {
        return ( muggH(sqrt_s) + BrHZgamumuRatio() - 1.0 + eggFHZga - eggFint - eggFpar - eHZgaint - eHZgapar + eHwidth);
    }
}

◆ muTHUggHZZ()

const double NPSMEFTd6General::muTHUggHZZ ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,ZZ}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,ZZ}$

Reimplemented from NPbase.

Definition at line 36017 of file NPSMEFTd6General.cpp.

                                                                   {
    if (FlagQuadraticTerms) {
        return ( muggH(sqrt_s) * BrHZZRatio() * (1.0 + eggFHZZ) * (1.0 + eHwidth) / (1.0 + eggFint + eggFpar) / (1.0 + eHZZint + eHZZpar));
    } else {
        return ( muggH(sqrt_s) + BrHZZRatio() - 1.0 + eggFHZZ - eggFint - eggFpar - eHZZint - eHZZpar + eHwidth);
    }
}

◆ muTHUggHZZ4l()

const double NPSMEFTd6General::muTHUggHZZ4l ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,ZZ\to 4l}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 36074 of file NPSMEFTd6General.cpp.

                                                                     {
    if (FlagQuadraticTerms) {
        return ( muggH(sqrt_s) * BrHZZ4lRatio() * (1.0 + eggFHZZ) * (1.0 + eHwidth) / (1.0 + eggFint + eggFpar) / (1.0 + eHZZint + eHZZpar));
    } else {
        return ( muggH(sqrt_s) + BrHZZ4lRatio() - 1.0 + eggFHZZ - eggFint - eggFpar - eHZZint - eHZZpar + eHwidth);
    }
}

◆ muTHUggHZZ4mu()

const double NPSMEFTd6General::muTHUggHZZ4mu ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH,ZZ\to 4\mu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*\to 4\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,ZZ\to 4\mu}$

Reimplemented from NPbase.

Definition at line 36454 of file NPSMEFTd6General.cpp.

                                                                      {
    if (FlagQuadraticTerms) {
        return ( muggH(sqrt_s) * BrHZZ4muRatio() * (1.0 + eggFHZZ) * (1.0 + eHwidth) / (1.0 + eggFint + eggFpar) / (1.0 + eHZZint + eHZZpar));
    } else {
        return ( muggH(sqrt_s) + BrHZZ4muRatio() - 1.0 + eggFHZZ - eggFint - eggFpar - eHZZint - eHZZpar + eHwidth);
    }
}

◆ muTHUttHbb()

const double NPSMEFTd6General::muTHUttHbb ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,bb}$ between the ttH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,bb}$

Reimplemented from NPbase.

Definition at line 36408 of file NPSMEFTd6General.cpp.

                                                                   {
    if (FlagQuadraticTerms) {
        return ( muttH(sqrt_s) * BrHbbRatio() * (1.0 + ettHbb) * (1.0 + eHwidth) / (1.0 + eeettHint + eeettHpar) / (1.0 + eHbbint + eHbbpar));
    } else {
        return ( muttH(sqrt_s) + BrHbbRatio() - 1.0 + ettHbb - eeettHint - eeettHpar - eHbbint - eHbbpar + eHwidth);
    }
}

◆ muTHUttHgaga()

const double NPSMEFTd6General::muTHUttHgaga ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,\gamma\gamma}$ between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 35952 of file NPSMEFTd6General.cpp.

                                                                     {
    if (FlagQuadraticTerms) {
        return ( muttH(sqrt_s) * BrHgagaRatio() * (1.0 + ettHgaga) * (1.0 + eHwidth) / (1.0 + eeettHint + eeettHpar) / (1.0 + eHgagaint + eHgagapar));
    } else {
        return ( muttH(sqrt_s) + BrHgagaRatio() - 1.0 + ettHgaga - eeettHint - eeettHpar - eHgagaint - eHgagapar + eHwidth);
    }
}

◆ muTHUttHmumu()

const double NPSMEFTd6General::muTHUttHmumu ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,\mu\mu}$ between the ttH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 36294 of file NPSMEFTd6General.cpp.

                                                                     {
    if (FlagQuadraticTerms) {
        return ( muttH(sqrt_s) * BrHmumuRatio() * (1.0 + ettHmumu) * (1.0 + eHwidth) / (1.0 + eeettHint + eeettHpar) / (1.0 + eHmumuint + eHmumupar));
    } else {
        return ( muttH(sqrt_s) + BrHmumuRatio() - 1.0 + ettHmumu - eeettHint - eeettHpar - eHmumuint - eHmumupar + eHwidth);
    }
}

◆ muTHUttHtautau()

const double NPSMEFTd6General::muTHUttHtautau ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,\tau\tau}$ between the ttH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 36351 of file NPSMEFTd6General.cpp.

                                                                       {
    if (FlagQuadraticTerms) {
        return ( muttH(sqrt_s) * BrHtautauRatio() * (1.0 + ettHtautau) * (1.0 + eHwidth) / (1.0 + eeettHint + eeettHpar) / (1.0 + eHtautauint + eHtautaupar));
    } else {
        return ( muttH(sqrt_s) + BrHtautauRatio() - 1.0 + ettHtautau - eeettHint - eeettHpar - eHtautauint - eHtautaupar + eHwidth);
    }
}

◆ muTHUttHWW()

const double NPSMEFTd6General::muTHUttHWW ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,WW}$ between the ttH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,WW}$

Reimplemented from NPbase.

Definition at line 36180 of file NPSMEFTd6General.cpp.

                                                                   {
    if (FlagQuadraticTerms) {
        return ( muttH(sqrt_s) * BrHWWRatio() * (1.0 + ettHWW) * (1.0 + eHwidth) / (1.0 + eeettHint + eeettHpar) / (1.0 + eHWWint + eHWWpar));
    } else {
        return ( muttH(sqrt_s) + BrHWWRatio() - 1.0 + ettHWW - eeettHint - eeettHpar - eHWWint - eHWWpar + eHwidth);
    }
}

◆ muTHUttHWW2l2v()

const double NPSMEFTd6General::muTHUttHWW2l2v ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,WW\to 2l2\nu}$ between the ttH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 36237 of file NPSMEFTd6General.cpp.

                                                                       {
    if (FlagQuadraticTerms) {
        return ( muttH(sqrt_s) * BrHWW2l2vRatio() * (1.0 + ettHWW) * (1.0 + eHwidth) / (1.0 + eeettHint + eeettHpar) / (1.0 + eHWWint + eHWWpar));
    } else {
        return ( muttH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + ettHWW - eeettHint - eeettHpar - eHWWint - eHWWpar + eHwidth);
    }
}

◆ muTHUttHZga()

const double NPSMEFTd6General::muTHUttHZga ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,Z\gamma}$ between the ttH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 36009 of file NPSMEFTd6General.cpp.

                                                                    {
    if (FlagQuadraticTerms) {
        return ( muttH(sqrt_s) * BrHZgaRatio() * (1.0 + ettHZga) * (1.0 + eHwidth) / (1.0 + eeettHint + eeettHpar) / (1.0 + eHZgaint + eHZgapar));
    } else {
        return ( muttH(sqrt_s) + BrHZgaRatio() - 1.0 + ettHZga - eeettHint - eeettHpar - eHZgaint - eHZgapar + eHwidth);
    }
}

◆ muTHUttHZZ()

const double NPSMEFTd6General::muTHUttHZZ ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,ZZ}$ between the ttH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,ZZ}$

Reimplemented from NPbase.

Definition at line 36066 of file NPSMEFTd6General.cpp.

                                                                   {
    if (FlagQuadraticTerms) {
        return ( muttH(sqrt_s) * BrHZZRatio() * (1.0 + ettHZZ) * (1.0 + eHwidth) / (1.0 + eeettHint + eeettHpar) / (1.0 + eHZZint + eHZZpar));
    } else {
        return ( muttH(sqrt_s) + BrHZZRatio() - 1.0 + ettHZZ - eeettHint - eeettHpar - eHZZint - eHZZpar + eHwidth);
    }
}

◆ muTHUttHZZ4l()

const double NPSMEFTd6General::muTHUttHZZ4l ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,ZZ\to 4l}$ between the ttH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 36123 of file NPSMEFTd6General.cpp.

                                                                     {
    if (FlagQuadraticTerms) {
        return ( muttH(sqrt_s) * BrHZZ4lRatio() * (1.0 + ettHZZ) * (1.0 + eHwidth) / (1.0 + eeettHint + eeettHpar) / (1.0 + eHZZint + eHZZpar));
    } else {
        return ( muttH(sqrt_s) + BrHZZ4lRatio() - 1.0 + ettHZZ - eeettHint - eeettHpar - eHZZint - eHZZpar + eHwidth);
    }
}

◆ muTHUVBFBRinv()

const double NPSMEFTd6General::muTHUVBFBRinv ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF}$ between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF}BR_{inv}$

Reimplemented from NPbase.

Definition at line 36416 of file NPSMEFTd6General.cpp.

                                                                      {
    return ( muVBF(sqrt_s) * Br_H_inv() * (1.0 + eVBFHinv) / (1.0 + eVBFint + eVBFpar));
}

◆ muTHUVBFHbb()

const double NPSMEFTd6General::muTHUVBFHbb ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,bb}$ between the VBF Higgs production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,bb}$

Reimplemented from NPbase.

Definition at line 36367 of file NPSMEFTd6General.cpp.

                                                                    {
    if (FlagQuadraticTerms) {
        return ( muVBF(sqrt_s) * BrHbbRatio() * (1.0 + eVBFHbb) * (1.0 + eHwidth) / (1.0 + eVBFint + eVBFpar) / (1.0 + eHbbint + eHbbpar));
    } else {
        return ( muVBF(sqrt_s) + BrHbbRatio() - 1.0 + eVBFHbb - eVBFint - eVBFpar - eHbbint - eHbbpar + eHwidth);
    }
}

◆ muTHUVBFHgaga()

const double NPSMEFTd6General::muTHUVBFHgaga ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,\gamma\gamma}$ between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 35911 of file NPSMEFTd6General.cpp.

                                                                      {
    if (FlagQuadraticTerms) {
        return ( muVBF(sqrt_s) * BrHgagaRatio() * (1.0 + eVBFHgaga) * (1.0 + eHwidth) / (1.0 + eVBFint + eVBFpar) / (1.0 + eHgagaint + eHgagapar));
    } else {
        return ( muVBF(sqrt_s) + BrHgagaRatio() - 1.0 + eVBFHgaga - eVBFint - eVBFpar - eHgagaint - eHgagapar + eHwidth);
    }
}

◆ muTHUVBFHinv()

const double NPSMEFTd6General::muTHUVBFHinv ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,inv}$ between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,inv}$

Reimplemented from NPbase.

Definition at line 36420 of file NPSMEFTd6General.cpp.

                                                                     {
    if (FlagQuadraticTerms) {
        return ( muVBF(sqrt_s) * BrHtoinvRatio() * (1.0 + eVBFHinv) / (1.0 + eVBFint + eVBFpar));
    } else {
        return ( muVBF(sqrt_s) + BrHtoinvRatio() - 1.0 + eVBFHinv - eVBFint - eVBFpar);
    }
}

◆ muTHUVBFHmumu()

const double NPSMEFTd6General::muTHUVBFHmumu ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,\mu\mu}$ between the VBF Higgs production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,\mu\mu}$

Reimplemented from NPbase.

Definition at line 36253 of file NPSMEFTd6General.cpp.

                                                                      {
    if (FlagQuadraticTerms) {
        return ( muVBF(sqrt_s) * BrHmumuRatio() * (1.0 + eVBFHmumu) * (1.0 + eHwidth) / (1.0 + eVBFint + eVBFpar) / (1.0 + eHmumuint + eHmumupar));
    } else {
        return ( muVBF(sqrt_s) + BrHmumuRatio() - 1.0 + eVBFHmumu - eVBFint - eVBFpar - eHmumuint - eHmumupar + eHwidth);
    }
}

◆ muTHUVBFHtautau()

const double NPSMEFTd6General::muTHUVBFHtautau ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,\tau\tau}$ between the VBF Higgs production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,\tau\tau}$

Reimplemented from NPbase.

Definition at line 36310 of file NPSMEFTd6General.cpp.

                                                                        {
    if (FlagQuadraticTerms) {
        return ( muVBF(sqrt_s) * BrHtautauRatio() * (1.0 + eVBFHtautau) * (1.0 + eHwidth) / (1.0 + eVBFint + eVBFpar) / (1.0 + eHtautauint + eHtautaupar));
    } else {
        return ( muVBF(sqrt_s) + BrHtautauRatio() - 1.0 + eVBFHtautau - eVBFint - eVBFpar - eHtautauint - eHtautaupar + eHwidth);
    }
}

◆ muTHUVBFHWW()

const double NPSMEFTd6General::muTHUVBFHWW ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,WW}$ between the VBF Higgs production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,WW}$

Reimplemented from NPbase.

Definition at line 36139 of file NPSMEFTd6General.cpp.

                                                                    {
    if (FlagQuadraticTerms) {
        return ( muVBF(sqrt_s) * BrHWWRatio() * (1.0 + eVBFHWW) * (1.0 + eHwidth) / (1.0 + eVBFint + eVBFpar) / (1.0 + eHWWint + eHWWpar));
    } else {
        return ( muVBF(sqrt_s) + BrHWWRatio() - 1.0 + eVBFHWW - eVBFint - eVBFpar - eHWWint - eHWWpar + eHwidth);
    }
}

◆ muTHUVBFHWW2l2v()

const double NPSMEFTd6General::muTHUVBFHWW2l2v ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,WW\to 2l2\nu}$ between the VBF Higgs production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 36196 of file NPSMEFTd6General.cpp.

                                                                        {
    if (FlagQuadraticTerms) {
        return ( muVBF(sqrt_s) * BrHWW2l2vRatio() * (1.0 + eVBFHWW) * (1.0 + eHwidth) / (1.0 + eVBFint + eVBFpar) / (1.0 + eHWWint + eHWWpar));
    } else {
        return ( muVBF(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eVBFHWW - eVBFint - eVBFpar - eHWWint - eHWWpar + eHwidth);
    }
}

◆ muTHUVBFHZga()

const double NPSMEFTd6General::muTHUVBFHZga ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,Z\gamma}$ between the VBF Higgs production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,Z\gamma}$

Reimplemented from NPbase.

Definition at line 35968 of file NPSMEFTd6General.cpp.

                                                                     {
    if (FlagQuadraticTerms) {
        return ( muVBF(sqrt_s) * BrHZgaRatio() * (1.0 + eVBFHZga) * (1.0 + eHwidth) / (1.0 + eVBFint + eVBFpar) / (1.0 + eHZgaint + eHZgapar));
    } else {
        return ( muVBF(sqrt_s) + BrHZgaRatio() - 1.0 + eVBFHZga - eVBFint - eVBFpar - eHZgaint - eHZgapar + eHwidth);
    }
}

◆ muTHUVBFHZZ()

const double NPSMEFTd6General::muTHUVBFHZZ ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,ZZ}$ between the VBF Higgs production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,ZZ}$

Reimplemented from NPbase.

Definition at line 36025 of file NPSMEFTd6General.cpp.

                                                                    {
    if (FlagQuadraticTerms) {
        return ( muVBF(sqrt_s) * BrHZZRatio() * (1.0 + eVBFHZZ) * (1.0 + eHwidth) / (1.0 + eVBFint + eVBFpar) / (1.0 + eHZZint + eHZZpar));
    } else {
        return ( muVBF(sqrt_s) + BrHZZRatio() - 1.0 + eVBFHZZ - eVBFint - eVBFpar - eHZZint - eHZZpar + eHwidth);
    }
}

◆ muTHUVBFHZZ4l()

const double NPSMEFTd6General::muTHUVBFHZZ4l ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,ZZ\to 4l}$ between the VBF Higgs production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 36082 of file NPSMEFTd6General.cpp.

                                                                      {
    if (FlagQuadraticTerms) {
        return ( muVBF(sqrt_s) * BrHZZ4lRatio() * (1.0 + eVBFHZZ) * (1.0 + eHwidth) / (1.0 + eVBFint + eVBFpar) / (1.0 + eHZZint + eHZZpar));
    } else {
        return ( muVBF(sqrt_s) + BrHZZ4lRatio() - 1.0 + eVBFHZZ - eVBFint - eVBFpar - eHZZint - eHZZpar + eHwidth);
    }
}

◆ muTHUVHbb()

const double NPSMEFTd6General::muTHUVHbb ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,bb}$ between the VH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,bb}$

Reimplemented from NPbase.

Definition at line 36391 of file NPSMEFTd6General.cpp.

                                                                  {
    //  Theory uncertainty in VH production, from the WH and ZH ones
    double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
    double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
    double eVHtot, eVHbb;
 
    eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    eVHbb = (eWHbb * sigmaWH_SM + eZHbb * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    if (FlagQuadraticTerms) {
        return ( muVH(sqrt_s) * BrHbbRatio() * (1.0 + eVHbb) * (1.0 + eHwidth) / (1.0 + eVHtot) / (1.0 + eHbbint + eHbbpar));
    } else {
        return ( muVH(sqrt_s) + BrHbbRatio() - 1.0 + eVHbb - eVHtot - eHbbint - eHbbpar + eHwidth);
    }
}

◆ muTHUVHBRinv()

const double NPSMEFTd6General::muTHUVHBRinv ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH}$ between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH}BR_{inv}$

Reimplemented from NPbase.

Definition at line 36428 of file NPSMEFTd6General.cpp.

                                                                     {
    //  Theory uncertainty in VH production, from the WH and ZH ones
    double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
    double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
    double eVHtot;
 
    eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    return ( muVH(sqrt_s) * Br_H_inv() * (1.0 + eVHinv) / (1.0 + eVHtot));
}

◆ muTHUVHgaga()

const double NPSMEFTd6General::muTHUVHgaga ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,\gamma\gamma}$ between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 35935 of file NPSMEFTd6General.cpp.

                                                                    {
    //  Theory uncertainty in VH production, from the WH and ZH ones
    double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
    double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
    double eVHtot, eVHgaga;
 
    eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    eVHgaga = (eWHgaga * sigmaWH_SM + eZHgaga * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    if (FlagQuadraticTerms) {
        return ( muVH(sqrt_s) * BrHgagaRatio() * (1.0 + eVHgaga) * (1.0 + eHwidth) / (1.0 + eVHtot) / (1.0 + eHgagaint + eHgagapar));
    } else {
        return ( muVH(sqrt_s) + BrHgagaRatio() - 1.0 + eVHgaga - eVHtot - eHgagaint - eHgagapar + eHwidth);
    }
}

◆ muTHUVHinv()

const double NPSMEFTd6General::muTHUVHinv ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,inv}$ between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,inv}$

Reimplemented from NPbase.

Definition at line 36439 of file NPSMEFTd6General.cpp.

                                                                   {
    //  Theory uncertainty in VH production, from the WH and ZH ones
    double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
    double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
    double eVHtot;
 
    eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    if (FlagQuadraticTerms) {
        return ( muVH(sqrt_s) * BrHtoinvRatio() * (1.0 + eVHinv) / (1.0 + eVHtot));
    } else {
        return ( muVH(sqrt_s) + BrHtoinvRatio() - 1.0 + eVHinv - eVHtot);
    }
}

◆ muTHUVHmumu()

const double NPSMEFTd6General::muTHUVHmumu ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,\mu\mu}$ between the VH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 36277 of file NPSMEFTd6General.cpp.

                                                                    {
    //  Theory uncertainty in VH production, from the WH and ZH ones
    double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
    double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
    double eVHtot, eVHmumu;
 
    eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    eVHmumu = (eWHmumu * sigmaWH_SM + eZHmumu * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    if (FlagQuadraticTerms) {
        return ( muVH(sqrt_s) * BrHmumuRatio() * (1.0 + eVHmumu) * (1.0 + eHwidth) / (1.0 + eVHtot) / (1.0 + eHmumuint + eHmumupar));
    } else {
        return ( muVH(sqrt_s) + BrHmumuRatio() - 1.0 + eVHmumu - eVHtot - eHmumuint - eHmumupar + eHwidth);
    }
}

◆ muTHUVHtautau()

const double NPSMEFTd6General::muTHUVHtautau ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,\tau\tau}$ between the VH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 36334 of file NPSMEFTd6General.cpp.

                                                                      {
    //  Theory uncertainty in VH production, from the WH and ZH ones
    double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
    double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
    double eVHtot, eVHtautau;
 
    eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    eVHtautau = (eWHtautau * sigmaWH_SM + eZHtautau * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    if (FlagQuadraticTerms) {
        return ( muVH(sqrt_s) * BrHtautauRatio() * (1.0 + eVHtautau) * (1.0 + eHwidth) / (1.0 + eVHtot) / (1.0 + eHtautauint + eHtautaupar));
    } else {
        return ( muVH(sqrt_s) + BrHtautauRatio() - 1.0 + eVHtautau - eVHtot - eHtautauint - eHtautaupar + eHwidth);
    }
}

◆ muTHUVHWW()

const double NPSMEFTd6General::muTHUVHWW ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,WW}$ between the VH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,WW}$

Reimplemented from NPbase.

Definition at line 36163 of file NPSMEFTd6General.cpp.

                                                                  {
    //  Theory uncertainty in VH production, from the WH and ZH ones
    double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
    double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
    double eVHtot, eVHWW;
 
    eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    eVHWW = (eWHWW * sigmaWH_SM + eZHWW * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    if (FlagQuadraticTerms) {
        return ( muVH(sqrt_s) * BrHWWRatio() * (1.0 + eVHWW) * (1.0 + eHwidth) / (1.0 + eVHtot) / (1.0 + eHWWint + eHWWpar));
    } else {
        return ( muVH(sqrt_s) + BrHWWRatio() - 1.0 + eVHWW - eVHtot - eHWWint - eHWWpar + eHwidth);
    }
}

◆ muTHUVHWW2l2v()

const double NPSMEFTd6General::muTHUVHWW2l2v ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,WW\to 2l2\nu}$ between the VH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 36220 of file NPSMEFTd6General.cpp.

                                                                      {
    //  Theory uncertainty in VH production, from the WH and ZH ones
    double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
    double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
    double eVHtot, eVHWW;
 
    eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    eVHWW = (eWHWW * sigmaWH_SM + eZHWW * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    if (FlagQuadraticTerms) {
        return ( muVH(sqrt_s) * BrHWW2l2vRatio() * (1.0 + eVHWW) * (1.0 + eHwidth) / (1.0 + eVHtot) / (1.0 + eHWWint + eHWWpar));
    } else {
        return ( muVH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eVHWW - eVHtot - eHWWint - eHWWpar + eHwidth);
    }
}

◆ muTHUVHZga()

const double NPSMEFTd6General::muTHUVHZga ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,Z\gamma}$ between the VH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 35992 of file NPSMEFTd6General.cpp.

                                                                   {
    //  Theory uncertainty in VH production, from the WH and ZH ones
    double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
    double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
    double eVHtot, eVHZga;
 
    eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    eVHZga = (eWHZga * sigmaWH_SM + eZHZga * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    if (FlagQuadraticTerms) {
        return ( muVH(sqrt_s) * BrHZgaRatio() * (1.0 + eVHZga) * (1.0 + eHwidth) / (1.0 + eVHtot) / (1.0 + eHZgaint + eHZgapar));
    } else {
        return ( muVH(sqrt_s) + BrHZgaRatio() - 1.0 + eVHZga - eVHtot - eHZgaint - eHZgapar + eHwidth);
    }
}

◆ muTHUVHZZ()

const double NPSMEFTd6General::muTHUVHZZ ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,ZZ}$ between the VH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,ZZ}$

Reimplemented from NPbase.

Definition at line 36049 of file NPSMEFTd6General.cpp.

                                                                  {
    //  Theory uncertainty in VH production, from the WH and ZH ones
    double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
    double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
    double eVHtot, eVHZZ;
 
    eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    eVHZZ = (eWHZZ * sigmaWH_SM + eZHZZ * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    if (FlagQuadraticTerms) {
        return ( muVH(sqrt_s) * BrHZZRatio() * (1.0 + eVHZZ) * (1.0 + eHwidth) / (1.0 + eVHtot) / (1.0 + eHZZint + eHZZpar));
    } else {
        return ( muVH(sqrt_s) + BrHZZRatio() - 1.0 + eVHZZ - eVHtot - eHZZint - eHZZpar + eHwidth);
    }
}

◆ muTHUVHZZ4l()

const double NPSMEFTd6General::muTHUVHZZ4l ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,ZZ\to 4l}$ between the VH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 36106 of file NPSMEFTd6General.cpp.

                                                                    {
    //  Theory uncertainty in VH production, from the WH and ZH ones
    double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
    double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
    double eVHtot, eVHZZ;
 
    eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    eVHZZ = (eWHZZ * sigmaWH_SM + eZHZZ * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
 
    if (FlagQuadraticTerms) {
        return ( muVH(sqrt_s) * BrHZZ4lRatio() * (1.0 + eVHZZ) * (1.0 + eHwidth) / (1.0 + eVHtot) / (1.0 + eHZZint + eHZZpar));
    } else {
        return ( muVH(sqrt_s) + BrHZZ4lRatio() - 1.0 + eVHZZ - eVHtot - eHZZint - eHZZpar + eHwidth);
    }
}

◆ muTHUWHbb()

const double NPSMEFTd6General::muTHUWHbb ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,bb}$ between the WH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,bb}$

Reimplemented from NPbase.

Definition at line 36383 of file NPSMEFTd6General.cpp.

                                                                  {
    if (FlagQuadraticTerms) {
        return ( muWH(sqrt_s) * BrHbbRatio() * (1.0 + eWHbb) * (1.0 + eHwidth) / (1.0 + eWHint + eWHpar) / (1.0 + eHbbint + eHbbpar));
    } else {
        return ( muWH(sqrt_s) + BrHbbRatio() - 1.0 + eWHbb - eWHint - eWHpar - eHbbint - eHbbpar + eHwidth);
    }
}

◆ muTHUWHgaga()

const double NPSMEFTd6General::muTHUWHgaga ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,\gamma\gamma}$ between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 35927 of file NPSMEFTd6General.cpp.

                                                                    {
    if (FlagQuadraticTerms) {
        return ( muWH(sqrt_s) * BrHgagaRatio() * (1.0 + eWHgaga) * (1.0 + eHwidth) / (1.0 + eWHint + eWHpar) / (1.0 + eHgagaint + eHgagapar));
    } else {
        return ( muWH(sqrt_s) + BrHgagaRatio() - 1.0 + eWHgaga - eWHint - eWHpar - eHgagaint - eHgagapar + eHwidth);
    }
}

◆ muTHUWHmumu()

const double NPSMEFTd6General::muTHUWHmumu ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,\mu\mu}$ between the WH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 36269 of file NPSMEFTd6General.cpp.

                                                                    {
    if (FlagQuadraticTerms) {
        return ( muWH(sqrt_s) * BrHmumuRatio() * (1.0 + eWHmumu) * (1.0 + eHwidth) / (1.0 + eWHint + eWHpar) / (1.0 + eHmumuint + eHmumupar));
    } else {
        return ( muWH(sqrt_s) + BrHmumuRatio() - 1.0 + eWHmumu - eWHint - eWHpar - eHmumuint - eHmumupar + eHwidth);
    }
}

◆ muTHUWHtautau()

const double NPSMEFTd6General::muTHUWHtautau ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,\tau\tau}$ between the WH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 36326 of file NPSMEFTd6General.cpp.

                                                                      {
    if (FlagQuadraticTerms) {
        return ( muWH(sqrt_s) * BrHtautauRatio() * (1.0 + eWHtautau) * (1.0 + eHwidth) / (1.0 + eWHint + eWHpar) / (1.0 + eHtautauint + eHtautaupar));
    } else {
        return ( muWH(sqrt_s) + BrHtautauRatio() - 1.0 + eWHtautau - eWHint - eWHpar - eHtautauint - eHtautaupar + eHwidth);
    }
}

◆ muTHUWHWW()

const double NPSMEFTd6General::muTHUWHWW ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,WW}$ between the WH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,WW}$

Reimplemented from NPbase.

Definition at line 36155 of file NPSMEFTd6General.cpp.

                                                                  {
    if (FlagQuadraticTerms) {
        return ( muWH(sqrt_s) * BrHWWRatio() * (1.0 + eWHWW) * (1.0 + eHwidth) / (1.0 + eWHint + eWHpar) / (1.0 + eHWWint + eHWWpar));
    } else {
        return ( muWH(sqrt_s) + BrHWWRatio() - 1.0 + eWHWW - eWHint - eWHpar - eHWWint - eHWWpar + eHwidth);
    }
}

◆ muTHUWHWW2l2v()

const double NPSMEFTd6General::muTHUWHWW2l2v ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,WW\to 2l2\nu}$ between the WH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 36212 of file NPSMEFTd6General.cpp.

                                                                      {
    if (FlagQuadraticTerms) {
        return ( muWH(sqrt_s) * BrHWW2l2vRatio() * (1.0 + eWHWW) * (1.0 + eHwidth) / (1.0 + eWHint + eWHpar) / (1.0 + eHWWint + eHWWpar));
    } else {
        return ( muWH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eWHWW - eWHint - eWHpar - eHWWint - eHWWpar + eHwidth);
    }
}

◆ muTHUWHZga()

const double NPSMEFTd6General::muTHUWHZga ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,Z\gamma}$ between the WH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 35984 of file NPSMEFTd6General.cpp.

                                                                   {
    if (FlagQuadraticTerms) {
        return ( muWH(sqrt_s) * BrHZgaRatio() * (1.0 + eWHZga) * (1.0 + eHwidth) / (1.0 + eWHint + eWHpar) / (1.0 + eHZgaint + eHZgapar));
    } else {
        return ( muWH(sqrt_s) + BrHZgaRatio() - 1.0 + eWHZga - eWHint - eWHpar - eHZgaint - eHZgapar + eHwidth);
    }
}

◆ muTHUWHZZ()

const double NPSMEFTd6General::muTHUWHZZ ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,ZZ}$ between the WH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,ZZ}$

Reimplemented from NPbase.

Definition at line 36041 of file NPSMEFTd6General.cpp.

                                                                  {
    if (FlagQuadraticTerms) {
        return ( muWH(sqrt_s) * BrHZZRatio() * (1.0 + eWHZZ) * (1.0 + eHwidth) / (1.0 + eWHint + eWHpar) / (1.0 + eHZZint + eHZZpar));
    } else {
        return ( muWH(sqrt_s) + BrHZZRatio() - 1.0 + eWHZZ - eWHint - eWHpar - eHZZint - eHZZpar + eHwidth);
    }
}

◆ muTHUWHZZ4l()

const double NPSMEFTd6General::muTHUWHZZ4l ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,ZZ\to 4l}$ between the WH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 36098 of file NPSMEFTd6General.cpp.

                                                                    {
    if (FlagQuadraticTerms) {
        return ( muWH(sqrt_s) * BrHZZ4lRatio() * (1.0 + eWHZZ) * (1.0 + eHwidth) / (1.0 + eWHint + eWHpar) / (1.0 + eHZZint + eHZZpar));
    } else {
        return ( muWH(sqrt_s) + BrHZZ4lRatio() - 1.0 + eWHZZ - eWHint - eWHpar - eHZZint - eHZZpar + eHwidth);
    }
}

◆ muTHUZHbb()

const double NPSMEFTd6General::muTHUZHbb ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,bb}$ between the ZH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,bb}$

Reimplemented from NPbase.

Definition at line 36375 of file NPSMEFTd6General.cpp.

                                                                  {
    if (FlagQuadraticTerms) {
        return ( muZH(sqrt_s) * BrHbbRatio() * (1.0 + eZHbb) * (1.0 + eHwidth) / (1.0 + eZHint + eZHpar) / (1.0 + eHbbint + eHbbpar));
    } else {
        return ( muZH(sqrt_s) + BrHbbRatio() - 1.0 + eZHbb - eZHint - eZHpar - eHbbint - eHbbpar + eHwidth);
    }
}

◆ muTHUZHgaga()

const double NPSMEFTd6General::muTHUZHgaga ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,\gamma\gamma}$ between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 35919 of file NPSMEFTd6General.cpp.

                                                                    {
    if (FlagQuadraticTerms) {
        return ( muZH(sqrt_s) * BrHgagaRatio() * (1.0 + eZHgaga) * (1.0 + eHwidth) / (1.0 + eZHint + eZHpar) / (1.0 + eHgagaint + eHgagapar));
    } else {
        return ( muZH(sqrt_s) + BrHgagaRatio() - 1.0 + eZHgaga - eZHint - eZHpar - eHgagaint - eHgagapar + eHwidth);
    }
}

◆ muTHUZHmumu()

const double NPSMEFTd6General::muTHUZHmumu ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,\mu\mu}$ between the ZH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 36261 of file NPSMEFTd6General.cpp.

                                                                    {
    if (FlagQuadraticTerms) {
        return ( muZH(sqrt_s) * BrHmumuRatio() * (1.0 + eZHmumu) * (1.0 + eHwidth) / (1.0 + eZHint + eZHpar) / (1.0 + eHmumuint + eHmumupar));
    } else {
        return ( muZH(sqrt_s) + BrHmumuRatio() - 1.0 + eZHmumu - eZHint - eZHpar - eHmumuint - eHmumupar + eHwidth);
    }
}

◆ muTHUZHtautau()

const double NPSMEFTd6General::muTHUZHtautau ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,\tau\tau}$ between the ZH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 36318 of file NPSMEFTd6General.cpp.

                                                                      {
    if (FlagQuadraticTerms) {
        return ( muZH(sqrt_s) * BrHtautauRatio() * (1.0 + eZHtautau) * (1.0 + eHwidth) / (1.0 + eZHint + eZHpar) / (1.0 + eHtautauint + eHtautaupar));
    } else {
        return ( muZH(sqrt_s) + BrHtautauRatio() - 1.0 + eZHtautau - eZHint - eZHpar - eHtautauint - eHtautaupar + eHwidth);
    }
}

◆ muTHUZHWW()

const double NPSMEFTd6General::muTHUZHWW ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,WW}$ between the ZH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,WW}$

Reimplemented from NPbase.

Definition at line 36147 of file NPSMEFTd6General.cpp.

                                                                  {
    if (FlagQuadraticTerms) {
        return ( muZH(sqrt_s) * BrHWWRatio() * (1.0 + eZHWW) * (1.0 + eHwidth) / (1.0 + eZHint + eZHpar) / (1.0 + eHWWint + eHWWpar));
    } else {
        return ( muZH(sqrt_s) + BrHWWRatio() - 1.0 + eZHWW - eZHint - eZHpar - eHWWint - eHWWpar + eHwidth);
    }
}

◆ muTHUZHWW2l2v()

const double NPSMEFTd6General::muTHUZHWW2l2v ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,WW\to 2l2\nu}$ between the ZH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 36204 of file NPSMEFTd6General.cpp.

                                                                      {
    if (FlagQuadraticTerms) {
        return ( muZH(sqrt_s) * BrHWW2l2vRatio() * (1.0 + eZHWW) * (1.0 + eHwidth) / (1.0 + eZHint + eZHpar) / (1.0 + eHWWint + eHWWpar));
    } else {
        return ( muZH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eZHWW - eZHint - eZHpar - eHWWint - eHWWpar + eHwidth);
    }
}

◆ muTHUZHZga()

const double NPSMEFTd6General::muTHUZHZga ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,Z\gamma}$ between the ZH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 35976 of file NPSMEFTd6General.cpp.

                                                                   {
    if (FlagQuadraticTerms) {
        return ( muZH(sqrt_s) * BrHZgaRatio() * (1.0 + eZHZga) * (1.0 + eHwidth) / (1.0 + eZHint + eZHpar) / (1.0 + eHZgaint + eHZgapar));
    } else {
        return ( muZH(sqrt_s) + BrHZgaRatio() - 1.0 + eZHZga - eZHint - eZHpar - eHZgaint - eHZgapar + eHwidth);
    }
}

◆ muTHUZHZZ()

const double NPSMEFTd6General::muTHUZHZZ ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,ZZ}$ between the ZH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,ZZ}$

Reimplemented from NPbase.

Definition at line 36033 of file NPSMEFTd6General.cpp.

                                                                  {
    if (FlagQuadraticTerms) {
        return ( muZH(sqrt_s) * BrHZZRatio() * (1.0 + eZHZZ) * (1.0 + eHwidth) / (1.0 + eZHint + eZHpar) / (1.0 + eHZZint + eHZZpar));
    } else {
        return ( muZH(sqrt_s) + BrHZZRatio() - 1.0 + eZHZZ - eZHint - eZHpar - eHZZint - eHZZpar + eHwidth);
    }
}

◆ muTHUZHZZ4l()

const double NPSMEFTd6General::muTHUZHZZ4l ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,ZZ\to 4l}$ between the ZH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 36090 of file NPSMEFTd6General.cpp.

                                                                    {
    if (FlagQuadraticTerms) {
        return ( muZH(sqrt_s) * BrHZZ4lRatio() * (1.0 + eZHZZ) * (1.0 + eHwidth) / (1.0 + eZHint + eZHpar) / (1.0 + eHZZint + eHZZpar));
    } else {
        return ( muZH(sqrt_s) + BrHZZ4lRatio() - 1.0 + eZHZZ - eZHint - eZHpar - eHZZint - eHZZpar + eHwidth);
    }
}

◆ muttH()

const double NPSMEFTd6General::muttH ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH}$ between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH}$

Reimplemented from NPbase.

Definition at line 20079 of file NPSMEFTd6General.cpp.

{
    double mu = 1.0;
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += ettHint + ettHpar;
 
    // Linear contribution (including the Higgs self-coupling)
    mu += delta_muttH_1(sqrt_s);
 
    // Quadratic contribution (including the Higgs self-coupling)
    mu += delta_muttH_2(sqrt_s);
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muttHbb()

const double NPSMEFTd6General::muttHbb ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,bb}$ between the ttH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,bb}$

Reimplemented from NPbase.

Definition at line 35892 of file NPSMEFTd6General.cpp.

                                                                {
    return muttH(sqrt_s) * BrHbbRatio();
 
}

◆ muttHgaga()

const double NPSMEFTd6General::muttHgaga ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,\gamma\gamma}$ between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 35652 of file NPSMEFTd6General.cpp.

                                                                  {
    return muttH(sqrt_s) * BrHgagaRatio();
 
}

◆ muttHgagaZeeboost()

const double NPSMEFTd6General::muttHgagaZeeboost ( const double sqrt_s ) const

virtual

The ratio $\sigma(ttH)/\sigma(ttZ)$ in the $H\to b\bar{b}$, $Z\to e^+e^-$ channel channel in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\sigma(ttH)/\sigma(ttZ)$ normalized to the SM

Reimplemented from NPbase.

Definition at line 35455 of file NPSMEFTd6General.cpp.

                                                                          {
    // Ratios of BR with the SM
    double delBRHgagaRatio, delBRZeeRatio;
    
    // Wilson Coefficients
    double CG = 0.0, CuHR33 = 0.0, CHq1R11 = 0.0, CHq3R11 = 0.0, CHuR11 = 0.0;
    double CHdR11 = 0.0, CHq1R22 = 0.0, CHq3R22 = 0.0, CHuR22 = 0.0, CHdR22 = 0.0;
    double CHq1R33 = 0.0, CHq3R33 = 0.0, CHuR33 = 0.0, CuGR33 = 0.0, Cqq1R1133 = 0.0;
    double Cqq1R1331 = 0.0, Cqq1R2233 = 0.0, Cqq1R2332 = 0.0, Cqq3R1133 = 0.0, Cqq3R1331 = 0.0;
    double Cqq3R2233 = 0.0, Cqq3R2332 = 0.0, CuuR1133 = 0.0, CuuR2233 = 0.0, CuuR1331 = 0.0;
    double CuuR2332 = 0.0, Cud1R3311 = 0.0, Cud1R3322 = 0.0, Cud8R3311 = 0.0, Cud8R3322 = 0.0;
    double Cqu1R1133 = 0.0, Cqu1R2233 = 0.0, Cqu1R3311 = 0.0, Cqu1R3322 = 0.0, Cqu8R1133 = 0.0;
    double Cqu8R2233 = 0.0, Cqu8R3311 = 0.0, Cqu8R3322 = 0.0, Cqd1R3311 = 0.0, Cqd1R3322 = 0.0;
    double Cqd8R3311 = 0.0, Cqd8R3322 = 0.0; 
    double CHl3R11 = 0.0, CHl3R22 = 0.0, CllR1221 = 0.0; 
    double muRG = 230.; // ttH done for 236 GeV, ttZ for 220 GeV
    
    double dsigmarat;
    
//  Corrections to ratios of BR for final states
    delBRHgagaRatio = deltaGammaHgagaRatio1() - dGammaHTotR1;
    
    delBRZeeRatio = deltaGamma_Zf(leptons[ELECTRON])/(trueSM.GammaZ(leptons[ELECTRON])) 
            - deltaGamma_Z()/ trueSM.Gamma_Z();
    
//  Wilson coefficients definitions 
    CG = getSMEFTCoeff("CG", muRG); 
    CuHR33 = getSMEFTCoeff("CuHR",2,2, muRG); 
    CHq1R11 = getSMEFTCoeff("CHq1R",0,0, muRG); 
    CHq3R11 = getSMEFTCoeff("CHq3R",0,0, muRG); 
    CHuR11 = getSMEFTCoeff("CHuR",0,0, muRG); 
    CHdR11 = getSMEFTCoeff("CHdR",0,0, muRG); 
    CHq1R22 = getSMEFTCoeff("CHq1R",1,1, muRG); 
    CHq3R22 = getSMEFTCoeff("CHq3R",1,1, muRG); 
    CHuR22 = getSMEFTCoeff("CHuR",1,1, muRG); 
    CHdR22 = getSMEFTCoeff("CHdR",1,1, muRG); 
    CHq1R33 = getSMEFTCoeff("CHq1R",2,2, muRG); 
    CHq3R33 = getSMEFTCoeff("CHq3R",2,2, muRG); 
    CHuR33 = getSMEFTCoeff("CHuR",2,2, muRG); 
    CuGR33 = getSMEFTCoeff("CuGR",2,2, muRG); 
    Cqq1R1133 = getSMEFTCoeff("Cqq1R",0,0,2,2, muRG); 
    Cqq1R1331 = getSMEFTCoeff("Cqq1R",0,2,2,0, muRG); 
    Cqq1R2233 = getSMEFTCoeff("Cqq1R",1,1,2,2, muRG); 
    Cqq1R2332 = getSMEFTCoeff("Cqq1R",1,2,2,1, muRG); 
    Cqq3R1133 = getSMEFTCoeff("Cqq3R",0,0,2,2, muRG); 
    Cqq3R1331 = getSMEFTCoeff("Cqq3R",0,2,2,0, muRG); 
    Cqq3R2233 = getSMEFTCoeff("Cqq3R",1,1,2,2, muRG); 
    Cqq3R2332 = getSMEFTCoeff("Cqq3R",1,2,2,1, muRG); 
    CuuR1133 = getSMEFTCoeff("CuuR",0,0,2,2, muRG); 
    CuuR2233 = getSMEFTCoeff("CuuR",1,1,2,2, muRG); 
    CuuR1331 = getSMEFTCoeff("CuuR",0,2,2,0, muRG); 
    CuuR2332 = getSMEFTCoeff("CuuR",1,2,2,1, muRG); 
    Cud1R3311 = getSMEFTCoeff("Cud1R",2,2,0,0, muRG); 
    Cud1R3322 = getSMEFTCoeff("Cud1R",2,2,1,1, muRG); 
    Cud8R3311 = getSMEFTCoeff("Cud8R",2,2,0,0, muRG); 
    Cud8R3322 = getSMEFTCoeff("Cud8R",2,2,1,1, muRG); 
    Cqu1R1133 = getSMEFTCoeff("Cqu1R",0,0,2,2, muRG); 
    Cqu1R2233 = getSMEFTCoeff("Cqu1R",1,1,2,2, muRG); 
    Cqu1R3311 = getSMEFTCoeff("Cqu1R",2,2,0,0, muRG); 
    Cqu1R3322 = getSMEFTCoeff("Cqu1R",2,2,1,1, muRG); 
    Cqu8R1133 = getSMEFTCoeff("Cqu8R",0,0,2,2, muRG); 
    Cqu8R2233 = getSMEFTCoeff("Cqu8R",1,1,2,2, muRG); 
    Cqu8R3311 = getSMEFTCoeff("Cqu8R",2,2,0,0, muRG); 
    Cqu8R3322 = getSMEFTCoeff("Cqu8R",2,2,1,1, muRG); 
    Cqd1R3311 = getSMEFTCoeff("Cqd1R",2,2,0,0, muRG); 
    Cqd1R3322 = getSMEFTCoeff("Cqd1R",2,2,1,1, muRG); 
    Cqd8R3311 = getSMEFTCoeff("Cqd8R",2,2,0,0, muRG); 
    Cqd8R3322 = getSMEFTCoeff("Cqd8R",2,2,1,1, muRG);     
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG); 
        
    // Madgraph simulations for 84 TeV
 
    dsigmarat = 1.0;
    //  ttH 84 TeV
    dsigmarat += (
                -814615. * CG 
                -122358. * CuHR33 
                +43.4869 * CHq1R11 
                +29.6743 * CHq3R11 
                +1.47314 * CHuR11 
                +71.5756 * CHdR11 
                +4.91872 * CHq1R22 
                -87.4079 * CHq3R22 
                -76.7362 * CHuR22 
                +11.5842 * CHdR22 
                -443.578 * CHq1R33 
                -293.356 * CHq3R33 
                -329.955 * CHuR33 
                -1237480. * CuGR33 
                +16.9383 * Cqq1R1133 
                +334309. * Cqq1R1331 
                -5.91142 * Cqq1R2233 
                +18575.1 * Cqq1R2332 
                -243.453 * Cqq3R1133 
                +743417. * Cqq3R1331 
                +58.8933 * Cqq3R2233 
                +90015.6 * Cqq3R2332 
                -23.0103 * CuuR1133 
                -44.938 * CuuR2233 
                +333804. * CuuR1331 
                +18524.5 * CuuR2332 
                -21.3446 * Cud1R3311 
                -41.7531 * Cud1R3322 
                +52881.4 * Cud8R3311 
                +6555.05 * Cud8R3322 
                +353.475 * Cqu1R1133 
                -74.8719 * Cqu1R2233 
                -192.922 * Cqu1R3311 
                -47.5578 * Cqu1R3322 
                +133978. * Cqu8R1133 
                +13659.6 * Cqu8R2233 
                +82844. * Cqu8R3311 
                +4587.38 * Cqu8R3322 
                -191.882 * Cqd1R3311 
                -76.3599 * Cqd1R3322 
                +53420.8 * Cqd8R3311 
                +6537.54 * Cqd8R3322 
                -61170.9 * (CHl3R11 + CHl3R22 - CllR1221 ) )
                ;            
            
    //  Divided (linearized) by ttZ 84 TeV
    dsigmarat = dsigmarat - (
                -1253959. * CG 
                -195.273 * CHq1R11 
                +5722.23 * CHq3R11 
                +939.285 * CHuR11 
                -840.086 * CHdR11 
                +316.078 * CHq1R22 
                +819.585 * CHq3R22 
                +97.2898 * CHuR22 
                -134.566 * CHdR22 
                -125938. * CHq1R33 
                +125889. * CHq3R33 
                +91464.4 * CHuR33 
                -564449. * CuGR33 
                -159.949 * Cqq1R1133 
                +371709. * Cqq1R1331 
                -68.0447 * Cqq1R2233 
                +17904.8 * Cqq1R2332 
                -91.1919 * Cqq3R1133 
                +1193228. * Cqq3R1331 
                +47.7377 * Cqq3R2233 
                +152055. * Cqq3R2332 
                -133.953 * CuuR1133 
                -17.3028 * CuuR2233 
                +181860. * CuuR1331 
                +9119.11 * CuuR2332 
                -195.733 * Cud1R3311 
                -39.4786 * Cud1R3322 
                +30947.2 * Cud8R3311 
                +3492.61 * Cud8R3322 
                -45.2385 * Cqu1R1133 
                -14.2913 * Cqu1R2233 
                -98.8336 * Cqu1R3311 
                -24.4606 * Cqu1R3322 
                +138699. * Cqu8R1133 
                +14699.9 * Cqu8R2233 
                +78699.3 * Cqu8R3311 
                +3755.34 * Cqu8R3322 
                -14.8631 * Cqd1R3311 
                -20.1378 * Cqd1R3322 
                +55799.6 * Cqd8R3311 
                +6291.33 * Cqd8R3322 
                -61231.8 * (CHl3R11 + CHl3R22 - CllR1221 ) );
 
    return (dsigmarat + delBRHgagaRatio - delBRZeeRatio);
 
}

◆ muttHmumu()

const double NPSMEFTd6General::muttHmumu ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,\mu\mu}$ between the ttH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 35832 of file NPSMEFTd6General.cpp.

                                                                  {
    return muttH(sqrt_s) * BrHmumuRatio();
 
}

◆ muttHtautau()

const double NPSMEFTd6General::muttHtautau ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,\tau\tau}$ between the ttH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 35862 of file NPSMEFTd6General.cpp.

                                                                    {
    return muttH(sqrt_s) * BrHtautauRatio();
 
}

◆ muttHWW()

const double NPSMEFTd6General::muttHWW ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,WW}$ between the ttH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,WW}$

Reimplemented from NPbase.

Definition at line 35772 of file NPSMEFTd6General.cpp.

                                                                {
    return muttH(sqrt_s) * BrHWWRatio();
 
}

◆ muttHWW2l2v()

const double NPSMEFTd6General::muttHWW2l2v ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,WW\to 2l2\nu}$ between the ttH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 35802 of file NPSMEFTd6General.cpp.

                                                                    {
    return muttH(sqrt_s) * BrHWW2l2vRatio();
 
}

◆ muttHZbbboost()

const double NPSMEFTd6General::muttHZbbboost ( const double sqrt_s ) const

virtual

The ratio $\sigma(ttH)/\sigma(ttZ)$ in the $H,Z\to b\bar{b}$ channel in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\sigma(ttH)/\sigma(ttZ)$ normalized to the SM

Reimplemented from NPbase.

Definition at line 35286 of file NPSMEFTd6General.cpp.

                                                                      {
    // Ratios of BR with the SM
    double delBRHbbRatio, delBRZbbRatio;
 
    double CG = 0.0, CuHR33 = 0.0, CHq1R11 = 0.0, CHq3R11 = 0.0, CHuR11 = 0.0;
    double CHdR11 = 0.0, CHq1R22 = 0.0, CHq3R22 = 0.0, CHuR22 = 0.0, CHdR22 = 0.0;
    double CHq1R33 = 0.0, CHq3R33 = 0.0, CHuR33 = 0.0, CuGR33 = 0.0, Cqq1R1133 = 0.0;
    double Cqq1R1331 = 0.0, Cqq1R2233 = 0.0, Cqq1R2332 = 0.0, Cqq3R1133 = 0.0, Cqq3R1331 = 0.0;
    double Cqq3R2233 = 0.0, Cqq3R2332 = 0.0, CuuR1133 = 0.0, CuuR2233 = 0.0, CuuR1331 = 0.0;
    double CuuR2332 = 0.0, Cud1R3311 = 0.0, Cud1R3322 = 0.0, Cud8R3311 = 0.0, Cud8R3322 = 0.0;
    double Cqu1R1133 = 0.0, Cqu1R2233 = 0.0, Cqu1R3311 = 0.0, Cqu1R3322 = 0.0, Cqu8R1133 = 0.0;
    double Cqu8R2233 = 0.0, Cqu8R3311 = 0.0, Cqu8R3322 = 0.0, Cqd1R3311 = 0.0, Cqd1R3322 = 0.0;
    double Cqd8R3311 = 0.0, Cqd8R3322 = 0.0; 
    double CHl3R11 = 0.0, CHl3R22 = 0.0, CllR1221 = 0.0; 
    double muRG = 230.; // ttH done for 236 GeV, ttZ for 220 GeV
    
    double dsigmarat;
    
//  Corrections to ratios of BR for final states
    delBRHbbRatio = deltaGammaHbbRatio1() - dGammaHTotR1;
    
    delBRZbbRatio = deltaGamma_Zf(quarks[BOTTOM])/(trueSM.GammaZ(quarks[BOTTOM])) 
            - deltaGamma_Z()/ trueSM.Gamma_Z();
    
//  Wilson coefficients definitions 
    CG = getSMEFTCoeff("CG", muRG); 
    CuHR33 = getSMEFTCoeff("CuHR",2,2, muRG); 
    CHq1R11 = getSMEFTCoeff("CHq1R",0,0, muRG); 
    CHq3R11 = getSMEFTCoeff("CHq3R",0,0, muRG); 
    CHuR11 = getSMEFTCoeff("CHuR",0,0, muRG); 
    CHdR11 = getSMEFTCoeff("CHdR",0,0, muRG); 
    CHq1R22 = getSMEFTCoeff("CHq1R",1,1, muRG); 
    CHq3R22 = getSMEFTCoeff("CHq3R",1,1, muRG); 
    CHuR22 = getSMEFTCoeff("CHuR",1,1, muRG); 
    CHdR22 = getSMEFTCoeff("CHdR",1,1, muRG); 
    CHq1R33 = getSMEFTCoeff("CHq1R",2,2, muRG); 
    CHq3R33 = getSMEFTCoeff("CHq3R",2,2, muRG); 
    CHuR33 = getSMEFTCoeff("CHuR",2,2, muRG); 
    CuGR33 = getSMEFTCoeff("CuGR",2,2, muRG); 
    Cqq1R1133 = getSMEFTCoeff("Cqq1R",0,0,2,2, muRG); 
    Cqq1R1331 = getSMEFTCoeff("Cqq1R",0,2,2,0, muRG); 
    Cqq1R2233 = getSMEFTCoeff("Cqq1R",1,1,2,2, muRG); 
    Cqq1R2332 = getSMEFTCoeff("Cqq1R",1,2,2,1, muRG); 
    Cqq3R1133 = getSMEFTCoeff("Cqq3R",0,0,2,2, muRG); 
    Cqq3R1331 = getSMEFTCoeff("Cqq3R",0,2,2,0, muRG); 
    Cqq3R2233 = getSMEFTCoeff("Cqq3R",1,1,2,2, muRG); 
    Cqq3R2332 = getSMEFTCoeff("Cqq3R",1,2,2,1, muRG); 
    CuuR1133 = getSMEFTCoeff("CuuR",0,0,2,2, muRG); 
    CuuR2233 = getSMEFTCoeff("CuuR",1,1,2,2, muRG); 
    CuuR1331 = getSMEFTCoeff("CuuR",0,2,2,0, muRG); 
    CuuR2332 = getSMEFTCoeff("CuuR",1,2,2,1, muRG); 
    Cud1R3311 = getSMEFTCoeff("Cud1R",2,2,0,0, muRG); 
    Cud1R3322 = getSMEFTCoeff("Cud1R",2,2,1,1, muRG); 
    Cud8R3311 = getSMEFTCoeff("Cud8R",2,2,0,0, muRG); 
    Cud8R3322 = getSMEFTCoeff("Cud8R",2,2,1,1, muRG); 
    Cqu1R1133 = getSMEFTCoeff("Cqu1R",0,0,2,2, muRG); 
    Cqu1R2233 = getSMEFTCoeff("Cqu1R",1,1,2,2, muRG); 
    Cqu1R3311 = getSMEFTCoeff("Cqu1R",2,2,0,0, muRG); 
    Cqu1R3322 = getSMEFTCoeff("Cqu1R",2,2,1,1, muRG); 
    Cqu8R1133 = getSMEFTCoeff("Cqu8R",0,0,2,2, muRG); 
    Cqu8R2233 = getSMEFTCoeff("Cqu8R",1,1,2,2, muRG); 
    Cqu8R3311 = getSMEFTCoeff("Cqu8R",2,2,0,0, muRG); 
    Cqu8R3322 = getSMEFTCoeff("Cqu8R",2,2,1,1, muRG); 
    Cqd1R3311 = getSMEFTCoeff("Cqd1R",2,2,0,0, muRG); 
    Cqd1R3322 = getSMEFTCoeff("Cqd1R",2,2,1,1, muRG); 
    Cqd8R3311 = getSMEFTCoeff("Cqd8R",2,2,0,0, muRG); 
    Cqd8R3322 = getSMEFTCoeff("Cqd8R",2,2,1,1, muRG);     
    CHl3R11 = getSMEFTCoeff("CHl3R",0,0, muRG); 
    CHl3R22 = getSMEFTCoeff("CHl3R",1,1, muRG); 
    CllR1221 = getSMEFTCoeff("CllR",0,1,1,0, muRG); 
        
    // Madgraph simulations for 84 TeV
 
    dsigmarat = 1.0;
    //  ttH 84 TeV
    dsigmarat += (
                -814615. * CG 
                -122358. * CuHR33 
                +43.4869 * CHq1R11 
                +29.6743 * CHq3R11 
                +1.47314 * CHuR11 
                +71.5756 * CHdR11 
                +4.91872 * CHq1R22 
                -87.4079 * CHq3R22 
                -76.7362 * CHuR22 
                +11.5842 * CHdR22 
                -443.578 * CHq1R33 
                -293.356 * CHq3R33 
                -329.955 * CHuR33 
                -1237480. * CuGR33 
                +16.9383 * Cqq1R1133 
                +334309. * Cqq1R1331 
                -5.91142 * Cqq1R2233 
                +18575.1 * Cqq1R2332 
                -243.453 * Cqq3R1133 
                +743417. * Cqq3R1331 
                +58.8933 * Cqq3R2233 
                +90015.6 * Cqq3R2332 
                -23.0103 * CuuR1133 
                -44.938 * CuuR2233 
                +333804. * CuuR1331 
                +18524.5 * CuuR2332 
                -21.3446 * Cud1R3311 
                -41.7531 * Cud1R3322 
                +52881.4 * Cud8R3311 
                +6555.05 * Cud8R3322 
                +353.475 * Cqu1R1133 
                -74.8719 * Cqu1R2233 
                -192.922 * Cqu1R3311 
                -47.5578 * Cqu1R3322 
                +133978. * Cqu8R1133 
                +13659.6 * Cqu8R2233 
                +82844. * Cqu8R3311 
                +4587.38 * Cqu8R3322 
                -191.882 * Cqd1R3311 
                -76.3599 * Cqd1R3322 
                +53420.8 * Cqd8R3311 
                +6537.54 * Cqd8R3322 
                -61170.9 * (CHl3R11 + CHl3R22 - CllR1221 ) )
                ;            
            
    //  Divided (linearized) by ttZ 84 TeV
    dsigmarat = dsigmarat - (
                -1253959. * CG 
                -195.273 * CHq1R11 
                +5722.23 * CHq3R11 
                +939.285 * CHuR11 
                -840.086 * CHdR11 
                +316.078 * CHq1R22 
                +819.585 * CHq3R22 
                +97.2898 * CHuR22 
                -134.566 * CHdR22 
                -125938. * CHq1R33 
                +125889. * CHq3R33 
                +91464.4 * CHuR33 
                -564449. * CuGR33 
                -159.949 * Cqq1R1133 
                +371709. * Cqq1R1331 
                -68.0447 * Cqq1R2233 
                +17904.8 * Cqq1R2332 
                -91.1919 * Cqq3R1133 
                +1193228. * Cqq3R1331 
                +47.7377 * Cqq3R2233 
                +152055. * Cqq3R2332 
                -133.953 * CuuR1133 
                -17.3028 * CuuR2233 
                +181860. * CuuR1331 
                +9119.11 * CuuR2332 
                -195.733 * Cud1R3311 
                -39.4786 * Cud1R3322 
                +30947.2 * Cud8R3311 
                +3492.61 * Cud8R3322 
                -45.2385 * Cqu1R1133 
                -14.2913 * Cqu1R2233 
                -98.8336 * Cqu1R3311 
                -24.4606 * Cqu1R3322 
                +138699. * Cqu8R1133 
                +14699.9 * Cqu8R2233 
                +78699.3 * Cqu8R3311 
                +3755.34 * Cqu8R3322 
                -14.8631 * Cqd1R3311 
                -20.1378 * Cqd1R3322 
                +55799.6 * Cqd8R3311 
                +6291.33 * Cqd8R3322 
                -61231.8 * (CHl3R11 + CHl3R22 - CllR1221 ) );
 
    return (dsigmarat + delBRHbbRatio - delBRZbbRatio);
}

◆ muttHZga()

const double NPSMEFTd6General::muttHZga ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,Z\gamma}$ between the ttH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 35682 of file NPSMEFTd6General.cpp.

                                                                 {
    return muttH(sqrt_s) * BrHZgaRatio();
 
}

◆ muttHZZ()

const double NPSMEFTd6General::muttHZZ ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,ZZ}$ between the ttH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,ZZ}$

Reimplemented from NPbase.

Definition at line 35712 of file NPSMEFTd6General.cpp.

                                                                {
    return muttH(sqrt_s) * BrHZZRatio();
 
}

◆ muttHZZ4l()

const double NPSMEFTd6General::muttHZZ4l ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH,ZZ\to 4l}$ between the ttH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 35742 of file NPSMEFTd6General.cpp.

                                                                  {
    return muttH(sqrt_s) * BrHZZ4lRatio();
 
}

◆ muVBF()

const double NPSMEFTd6General::muVBF ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF}$ between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF}$

Reimplemented from NPbase.

Definition at line 18504 of file NPSMEFTd6General.cpp.

{
    double mu = 1.0;
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eVBFint + eVBFpar;
 
    // Linear contribution (including the Higgs self-coupling)
    mu += delta_muVBF_1(sqrt_s);
 
    // Quadratic contribution (including the Higgs self-coupling)
    mu += delta_muVBF_2(sqrt_s);
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muVBFgamma()

const double NPSMEFTd6General::muVBFgamma ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF+\gamma}$ between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF+\gamma}$

Reimplemented from NPbase.

Definition at line 20387 of file NPSMEFTd6General.cpp.

                                                                   {
    double mu = 1.0;
 
    double C1 = 0.0; //Use same values as VBF
 
    if (sqrt_s == 13.0) {
 
        C1 = 0.0064;
 
        mu +=
                +121253. * getSMEFTCoeffEW("CHbox")
                + 11791.5 * getSMEFTCoeffEW("CHB")
                - 130714. * getSMEFTCoeffEW("CHW")
                + 23472.1 * getSMEFTCoeffEW("CW")
                - 461704. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 35103.4 * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-203622. * getSMEFTCoeffEW("CHD")
                - 270077. * getSMEFTCoeffEW("CHWB")
                - 4.714 * delta_GF
                - 5.764 * deltaMwd6())
                + cWsch * (-131254. * getSMEFTCoeffEW("CHD")
                - 111576. * getSMEFTCoeffEW("CHWB")
                - 3.998 * delta_GF)
                ;
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::muVBFgamma()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy. Use same as VBF.)
    mu += eVBFint + eVBFpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio();
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muVBFHbb()

const double NPSMEFTd6General::muVBFHbb ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,bb}$ between the VBF Higgs production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,bb}$

Reimplemented from NPbase.

Definition at line 35872 of file NPSMEFTd6General.cpp.

                                                                 {
    return muVBF(sqrt_s) * BrHbbRatio();
 
}

◆ muVBFHgaga()

const double NPSMEFTd6General::muVBFHgaga ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,\gamma\gamma}$ between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 35632 of file NPSMEFTd6General.cpp.

                                                                   {
    return muVBF(sqrt_s) * BrHgagaRatio();
 
}

◆ muVBFHmumu()

const double NPSMEFTd6General::muVBFHmumu ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,\mu\mu}$ between the VBF Higgs production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,\mu\mu}$

Reimplemented from NPbase.

Definition at line 35812 of file NPSMEFTd6General.cpp.

                                                                   {
    return muVBF(sqrt_s) * BrHmumuRatio();
 
}

◆ muVBFHtautau()

const double NPSMEFTd6General::muVBFHtautau ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,\tau\tau}$ between the VBF Higgs production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,\tau\tau}$

Reimplemented from NPbase.

Definition at line 35842 of file NPSMEFTd6General.cpp.

                                                                     {
    return muVBF(sqrt_s) * BrHtautauRatio();
 
}

◆ muVBFHWW()

const double NPSMEFTd6General::muVBFHWW ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,WW}$ between the VBF Higgs production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,WW}$

Reimplemented from NPbase.

Definition at line 35752 of file NPSMEFTd6General.cpp.

                                                                 {
    return muVBF(sqrt_s) * BrHWWRatio();
 
}

◆ muVBFHWW2l2v()

const double NPSMEFTd6General::muVBFHWW2l2v ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,WW\to 2l2\nu}$ between the VBF Higgs production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 35782 of file NPSMEFTd6General.cpp.

                                                                     {
    return muVBF(sqrt_s) * BrHWW2l2vRatio();
 
}

◆ muVBFHZga()

const double NPSMEFTd6General::muVBFHZga ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,Z\gamma}$ between the VBF Higgs production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,Z\gamma}$

Reimplemented from NPbase.

Definition at line 35662 of file NPSMEFTd6General.cpp.

                                                                  {
    return muVBF(sqrt_s) * BrHZgaRatio();
 
}

◆ muVBFHZZ()

const double NPSMEFTd6General::muVBFHZZ ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,ZZ}$ between the VBF Higgs production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,ZZ}$

Reimplemented from NPbase.

Definition at line 35692 of file NPSMEFTd6General.cpp.

                                                                 {
    return muVBF(sqrt_s) * BrHZZRatio();
 
}

◆ muVBFHZZ4l()

const double NPSMEFTd6General::muVBFHZZ4l ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF,ZZ\to 4l}$ between the VBF Higgs production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 35722 of file NPSMEFTd6General.cpp.

                                                                   {
    return muVBF(sqrt_s) * BrHZZ4lRatio();
 
}

◆ muVBFpVH()

const double NPSMEFTd6General::muVBFpVH ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF+VH}$ between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF+VH}$

Reimplemented from NPbase.

Definition at line 25000 of file NPSMEFTd6General.cpp.

                                                                 {
    double sigmaWH_SM = computeSigmaWH(sqrt_s);
    double sigmaZH_SM = computeSigmaZH(sqrt_s);
    double sigmaVBF_SM = computeSigmaVBF(sqrt_s);
    double sigmaWH = muWH(sqrt_s) * sigmaWH_SM;
    double sigmaZH = muZH(sqrt_s) * sigmaZH_SM;
    double sigmaVBF = muVBF(sqrt_s) * sigmaVBF_SM;
    double mu = ((sigmaWH + sigmaZH + sigmaVBF) / (sigmaWH_SM + sigmaZH_SM + sigmaVBF_SM));
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muVH()

const double NPSMEFTd6General::muVH ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH}$ between the WH+ZH associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH}$

Reimplemented from NPbase.

Definition at line 20289 of file NPSMEFTd6General.cpp.

                                                             {
    double mu = 1.0;
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    //mu += ;
 
    // Linear contribution 
    mu += delta_muVH_1(sqrt_s);
 
    // Quadratic contribution 
    mu += delta_muVH_2(sqrt_s);
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muVHbb()

const double NPSMEFTd6General::muVHbb ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,bb}$ between the VH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,bb}$

Reimplemented from NPbase.

Definition at line 35887 of file NPSMEFTd6General.cpp.

                                                               {
    return muVH(sqrt_s) * BrHbbRatio();
 
}

◆ muVHgaga()

const double NPSMEFTd6General::muVHgaga ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,\gamma\gamma}$ between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 35647 of file NPSMEFTd6General.cpp.

                                                                 {
    return muVH(sqrt_s) * BrHgagaRatio();
 
}

◆ muVHmumu()

const double NPSMEFTd6General::muVHmumu ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,\mu\mu}$ between the VH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 35827 of file NPSMEFTd6General.cpp.

                                                                 {
    return muVH(sqrt_s) * BrHmumuRatio();
 
}

◆ muVHpT250()

const double NPSMEFTd6General::muVHpT250 ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH}$ between the WH+ZH associated production cross-section in the current model and in the Standard Model, with $p_{T,H}>250$ GeV.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH}$

Reimplemented from NPbase.

Definition at line 24987 of file NPSMEFTd6General.cpp.

                                                                  {
    //Use MG SM values
    double sigmaWH_SM = 0.26944e-01;
    double sigmaZH_SM = 0.14600e-01;
    double sigmaWH = muWHpT250(sqrt_s) * sigmaWH_SM;
    double sigmaZH = muZHpT250(sqrt_s) * sigmaZH_SM;
    double mu = ((sigmaWH + sigmaZH) / (sigmaWH_SM + sigmaZH_SM));
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muVHtautau()

const double NPSMEFTd6General::muVHtautau ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,\tau\tau}$ between the VH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 35857 of file NPSMEFTd6General.cpp.

                                                                   {
    return muVH(sqrt_s) * BrHtautauRatio();
 
}

◆ muVHWW()

const double NPSMEFTd6General::muVHWW ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,WW}$ between the VH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,WW}$

Reimplemented from NPbase.

Definition at line 35767 of file NPSMEFTd6General.cpp.

                                                               {
    return muVH(sqrt_s) * BrHWWRatio();
 
}

◆ muVHWW2l2v()

const double NPSMEFTd6General::muVHWW2l2v ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,WW\to 2l2\nu}$ between the VH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 35797 of file NPSMEFTd6General.cpp.

                                                                   {
    return muVH(sqrt_s) * BrHWW2l2vRatio();
 
}

◆ muVHZga()

const double NPSMEFTd6General::muVHZga ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,Z\gamma}$ between the VH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 35677 of file NPSMEFTd6General.cpp.

                                                                {
    return muVH(sqrt_s) * BrHZgaRatio();
 
}

◆ muVHZZ()

const double NPSMEFTd6General::muVHZZ ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,ZZ}$ between the VH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,ZZ}$

Reimplemented from NPbase.

Definition at line 35707 of file NPSMEFTd6General.cpp.

                                                               {
    return muVH(sqrt_s) * BrHZZRatio();
 
}

◆ muVHZZ4l()

const double NPSMEFTd6General::muVHZZ4l ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH,ZZ\to 4l}$ between the VH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 35737 of file NPSMEFTd6General.cpp.

                                                                 {
    return muVH(sqrt_s) * BrHZZ4lRatio();
 
}

◆ muWH()

const double NPSMEFTd6General::muWH ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH}$ between the W-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH}$

Reimplemented from NPbase.

Definition at line 18789 of file NPSMEFTd6General.cpp.

{
    double mu = 1.0;
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eWHint + eWHpar;
 
    // Linear contribution (including the Higgs self-coupling)
    mu += delta_muWH_1(sqrt_s);
 
    // Quadratic contribution (including the Higgs self-coupling)
    mu += delta_muWH_2(sqrt_s);
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muWHbb()

const double NPSMEFTd6General::muWHbb ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,bb}$ between the WH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,bb}$

Reimplemented from NPbase.

Definition at line 35882 of file NPSMEFTd6General.cpp.

                                                               {
    return muWH(sqrt_s) * BrHbbRatio();
 
}

◆ muWHgaga()

const double NPSMEFTd6General::muWHgaga ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,\gamma\gamma}$ between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 35642 of file NPSMEFTd6General.cpp.

                                                                 {
    return muWH(sqrt_s) * BrHgagaRatio();
 
}

◆ muWHmumu()

const double NPSMEFTd6General::muWHmumu ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,\mu\mu}$ between the WH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 35822 of file NPSMEFTd6General.cpp.

                                                                 {
    return muWH(sqrt_s) * BrHmumuRatio();
 
}

◆ muWHpT250()

const double NPSMEFTd6General::muWHpT250 ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH}$ between the W-Higgs associated production cross-section in the current model and in the Standard Model, with $p_{T,H}>250$ GeV.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH}$

Reimplemented from NPbase.

Definition at line 23061 of file NPSMEFTd6General.cpp.

                                                                  {
    double mu = 1.0;
 
    double C1 = 0.0;
 
    if (sqrt_s == 13.0) {
 
        C1 = 0.0119;
 
        mu +=
                +121150. * getSMEFTCoeffEW("CHbox")
                + 1095782. * getSMEFTCoeffEW("CHW")
                + 11951748. * getSMEFTCoeffEW("CHq3R", 0, 0)
                + 540010. * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-160282. * getSMEFTCoeffEW("CHD")
                - 285105. * getSMEFTCoeffEW("CHWB")
                - 3.287 * delta_GF
                - 1.986 * deltaMwd6())
                + cWsch * (-30279.5 * getSMEFTCoeffEW("CHD")
                + 0. * getSMEFTCoeffEW("CHWB")
                - 2. * delta_GF)
                ;
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
 
        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::muWHpT250()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eWHint + eWHpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio();
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muWHtautau()

const double NPSMEFTd6General::muWHtautau ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,\tau\tau}$ between the WH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 35852 of file NPSMEFTd6General.cpp.

                                                                   {
    return muWH(sqrt_s) * BrHtautauRatio();
 
}

◆ muWHWW()

const double NPSMEFTd6General::muWHWW ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,WW}$ between the WH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,WW}$

Reimplemented from NPbase.

Definition at line 35762 of file NPSMEFTd6General.cpp.

                                                               {
    return muWH(sqrt_s) * BrHWWRatio();
 
}

◆ muWHWW2l2v()

const double NPSMEFTd6General::muWHWW2l2v ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,WW\to 2l2\nu}$ between the WH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 35792 of file NPSMEFTd6General.cpp.

                                                                   {
    return muWH(sqrt_s) * BrHWW2l2vRatio();
 
}

◆ muWHZga()

const double NPSMEFTd6General::muWHZga ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,Z\gamma}$ between the WH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 35672 of file NPSMEFTd6General.cpp.

                                                                {
    return muWH(sqrt_s) * BrHZgaRatio();
 
}

◆ muWHZZ()

const double NPSMEFTd6General::muWHZZ ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,ZZ}$ between the WH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,ZZ}$

Reimplemented from NPbase.

Definition at line 35702 of file NPSMEFTd6General.cpp.

                                                               {
    return muWH(sqrt_s) * BrHZZRatio();
 
}

◆ muWHZZ4l()

const double NPSMEFTd6General::muWHZZ4l ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH,ZZ\to 4l}$ between the WH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 35732 of file NPSMEFTd6General.cpp.

                                                                 {
    return muWH(sqrt_s) * BrHZZ4lRatio();
 
}

◆ muZH()

const double NPSMEFTd6General::muZH ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH}$ between the Z-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH}$

Reimplemented from NPbase.

Definition at line 19226 of file NPSMEFTd6General.cpp.

{
    double mu = 1.0;
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eZHint + eZHpar;
 
    // Linear contribution (including the Higgs self-coupling)
    mu += delta_muZH_1(sqrt_s);
 
    // Quadratic contribution (including the Higgs self-coupling)
    mu += delta_muZH_2(sqrt_s);
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muZHbb()

const double NPSMEFTd6General::muZHbb ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,bb}$ between the ZH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,bb}$

Reimplemented from NPbase.

Definition at line 35877 of file NPSMEFTd6General.cpp.

                                                               {
    return muZH(sqrt_s) * BrHbbRatio();
 
}

◆ muZHgaga()

const double NPSMEFTd6General::muZHgaga ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,\gamma\gamma}$ between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 35637 of file NPSMEFTd6General.cpp.

                                                                 {
    return muZH(sqrt_s) * BrHgagaRatio();
 
}

◆ muZHmumu()

const double NPSMEFTd6General::muZHmumu ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,\mu\mu}$ between the ZH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 35817 of file NPSMEFTd6General.cpp.

                                                                 {
    return muZH(sqrt_s) * BrHmumuRatio();
 
}

◆ muZHpT250()

const double NPSMEFTd6General::muZHpT250 ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH}$ between the Z-Higgs associated production cross-section in the current model and in the Standard Model, with $p_{T,H}>250$ GeV.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH}$

Reimplemented from NPbase.

Definition at line 23105 of file NPSMEFTd6General.cpp.

                                                                  {
    double mu = 1.0;
 
    double C1 = 0.0;
 
    if (sqrt_s == 13.0) {
 
        C1 = 0.0119;
 
        mu +=
                +121102. * getSMEFTCoeffEW("CHbox")
                + 103334. * getSMEFTCoeffEW("CHB")
                + 968778. * getSMEFTCoeffEW("CHW")
                - 1507566. * getSMEFTCoeffEW("CHq1R", 0, 0)
                + 165375. * getSMEFTCoeffEW("CHq1R", 1, 1)
                + 2712770. * getSMEFTCoeffEW("CHuR", 0, 0)
                + 83533. * getSMEFTCoeffEW("CHuR", 1, 1)
                - 836015. * getSMEFTCoeffEW("CHdR", 0, 0)
                - 64306.7 * getSMEFTCoeffEW("CHdR", 1, 1)
                + 10690175. * getSMEFTCoeffEW("CHq3R", 0, 0)
                + 540904. * getSMEFTCoeffEW("CHq3R", 1, 1)
                + cAsch * (-15339.3 * getSMEFTCoeffEW("CHD")
                + 286518. * getSMEFTCoeffEW("CHWB")
                - 2.508 * delta_GF)
                + cWsch * (+35828.1 * getSMEFTCoeffEW("CHD")
                + 398987. * getSMEFTCoeffEW("CHWB")
                - 2. * delta_GF)
                ;
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            mu += 0.0;
 
        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::muZHpT250()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    mu += eZHint + eZHpar;
 
    //  Linear contribution from Higgs self-coupling
    mu = mu + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio();
 
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return mu;
}

◆ muZHtautau()

const double NPSMEFTd6General::muZHtautau ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,\tau\tau}$ between the ZH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 35847 of file NPSMEFTd6General.cpp.

                                                                   {
    return muZH(sqrt_s) * BrHtautauRatio();
 
}

◆ muZHWW()

const double NPSMEFTd6General::muZHWW ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,WW}$ between the ZH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,WW}$

Reimplemented from NPbase.

Definition at line 35757 of file NPSMEFTd6General.cpp.

                                                               {
    return muZH(sqrt_s) * BrHWWRatio();
 
}

◆ muZHWW2l2v()

const double NPSMEFTd6General::muZHWW2l2v ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,WW\to 2l2\nu}$ between the ZH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 35787 of file NPSMEFTd6General.cpp.

                                                                   {
    return muZH(sqrt_s) * BrHWW2l2vRatio();
 
}

◆ muZHZga()

const double NPSMEFTd6General::muZHZga ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,Z\gamma}$ between the ZH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 35667 of file NPSMEFTd6General.cpp.

                                                                {
    return muZH(sqrt_s) * BrHZgaRatio();
 
}

◆ muZHZZ()

const double NPSMEFTd6General::muZHZZ ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,ZZ}$ between the ZH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,ZZ}$

Reimplemented from NPbase.

Definition at line 35697 of file NPSMEFTd6General.cpp.

                                                               {
    return muZH(sqrt_s) * BrHZZRatio();
 
}

◆ muZHZZ4l()

const double NPSMEFTd6General::muZHZZ4l ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH,ZZ\to 4l}$ between the ZH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 35727 of file NPSMEFTd6General.cpp.

                                                                 {
    return muZH(sqrt_s) * BrHZZ4lRatio();
 
}

◆ Mw()

const double NPSMEFTd6General::Mw ( ) const

virtual

The mass of the $W$ boson, $M_W$.

Returns: $M_W$ in GeV

Reimplemented from NPbase.

Definition at line 15596 of file NPSMEFTd6General.cpp.

                                        {
    //    return (trueSM.Mw() - Mw_tree / 4.0 / (cW2_tree - sW2_tree)
    //            *(4.0 * sW_tree * cW_tree * getSMEFTCoeffEW("CHWB") * v2_over_LambdaNP2
    //            + cW2_tree * getSMEFTCoeffEW("CHD") * v2_over_LambdaNP2
    //            + 2.0 * sW2_tree * delta_GF));
 
    return (trueSM.Mw() + Mw_tree * deltaMwd6());
}

◆ obliqueS()

const double NPSMEFTd6General::obliqueS ( ) const

virtual

The oblique parameter $S$. (Simplified implementation. Contribution only from $O_{HWB}$.)

Returns: the value of $S$

Reimplemented from NPbase.

Reimplemented in NPd6SILH.

Definition at line 15432 of file NPSMEFTd6General.cpp.

                                              {
    return (4.0 * sW_tree * cW_tree * getSMEFTCoeffEW("CHWB") / aleMz * v2);
}

◆ obliqueT()

const double NPSMEFTd6General::obliqueT ( ) const

virtual

The oblique parameter $T$. (Simplified implementation. Contribution only from $O_{HD}$.)

Returns: the value of $T$

Reimplemented from NPbase.

Reimplemented in NPd6SILH.

Definition at line 15436 of file NPSMEFTd6General.cpp.

                                              {
    return (-getSMEFTCoeffEW("CHD") / 2.0 / aleMz * v2);
}

◆ obliqueU()

const double NPSMEFTd6General::obliqueU ( ) const

virtual

The oblique parameter $U$.

Returns: the value of $U$

Reimplemented from NPbase.

Definition at line 15440 of file NPSMEFTd6General.cpp.

                                              {
    return 0.0;
}

◆ obliqueW()

const double NPSMEFTd6General::obliqueW ( ) const

virtual

The oblique parameter $W$. (Simplified implementation. Contribution only from $O_{2W}$.)

Returns: the value of $W$

Reimplemented from NPbase.

Reimplemented in NPd6SILH.

Definition at line 15444 of file NPSMEFTd6General.cpp.

                                              {
    return 0.;
}

◆ obliqueY()

const double NPSMEFTd6General::obliqueY ( ) const

virtual

The oblique parameter $Y$. (Simplified implementation. Contribution only from $O_{2B}$.)

Returns: the value of $Y$

Reimplemented from NPbase.

Reimplemented in NPd6SILH.

Definition at line 15448 of file NPSMEFTd6General.cpp.

                                              {
    return 0.;
}

◆ PostUpdate()

bool NPSMEFTd6General::PostUpdate ( )

virtual

The post-update method for NPSMEFTd6General.

This method runs all the procedures that are need to be executed after the model is successfully updated.

Returns: a boolean that is true if the execution is successful

Reimplemented from StandardModel.

Reimplemented in NPd6SILH, NPSMEFTd6ATHDM, NPSMEFTd6CHRU, NPSMEFTd6MFP, NPSMEFTd6MFV, NPSMEFTd6U2, NPSMEFTd6U2qU1le, and NPSMEFTd6U3.

Definition at line 8443 of file NPSMEFTd6General.cpp.

                                  {
    
    if (!isSMInitialConditionComputed) GenerateSMInitialConditions();
 
    if (FlagRGEci) {
 
        // SMEFT initial conditions for RGEsolver SMEFTEvolEW
        setSMEFTEvolWC(SMEFTEvolEW);
        
        //printNonVanishingSMEFTCoeffEW();
        //std::cout << Lambda_NP << " " << muw << " " << SMEFTBasisFlag << std::endl;
        // Do the evolution of the SMEFT Coefficients at linear order first; THIS DOES NOT EVOLVE THE SM PARAMETERS, only computes the corrections to them due to the SMEFT coefficients
        SMEFTEvolEW.EvolveSMEFTOnly(Lambda_NP, muw);
        // Evolve the SM parameters with the SM RGEs
        SMEFTEvolEW.EvolveSMOnly("Numeric", Lambda_NP, muw);
        //Now everything has been evolved
        //printNonVanishingSMEFTCoeffEW();
        
        // Work with the extra instances of RGEsolver: would be better to have a deep copy of SMEFTEvolEW
 
        // SM initial conditions for RGEsolver        
        SMEFTEvolMH.GenerateSMInitialConditions(muw, Lambda_NP, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol240.GenerateSMInitialConditions(muw, Lambda_NP, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol365.GenerateSMInitialConditions(muw, Lambda_NP, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol550.GenerateSMInitialConditions(muw, Lambda_NP, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol1000.GenerateSMInitialConditions(muw, Lambda_NP, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol1500.GenerateSMInitialConditions(muw, Lambda_NP, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol3000.GenerateSMInitialConditions(muw, Lambda_NP, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol5000.GenerateSMInitialConditions(muw, Lambda_NP, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvolUV.GenerateSMInitialConditions(muw, Lambda_NP, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
 
        // SMEFT initial conditions for RGEsolver
        setSMEFTEvolWC(SMEFTEvolMH);
        setSMEFTEvolWC(SMEFTEvol240);
        setSMEFTEvolWC(SMEFTEvol365);
        setSMEFTEvolWC(SMEFTEvol550);
        setSMEFTEvolWC(SMEFTEvol1000);
        setSMEFTEvolWC(SMEFTEvol1500);
        setSMEFTEvolWC(SMEFTEvol3000);
        setSMEFTEvolWC(SMEFTEvol5000);
        setSMEFTEvolWC(SMEFTEvolUV); // Not evolved. Only for reference to retrieve C(Lambda)
        
        if (FlagmultiScaleRGE) {
        // Perform the evolution for the other RGE instances
            SMEFTEvolMH.EvolveSMEFTOnly(Lambda_NP, 125.1);
            SMEFTEvol240.EvolveSMEFTOnly(Lambda_NP, 240.);
            SMEFTEvol365.EvolveSMEFTOnly(Lambda_NP, 365.);
            SMEFTEvol550.EvolveSMEFTOnly(Lambda_NP, 550.);
            SMEFTEvol1000.EvolveSMEFTOnly(Lambda_NP, fmin(1000.,Lambda_NP) );
            SMEFTEvol1500.EvolveSMEFTOnly(Lambda_NP, fmin(1500.,Lambda_NP) );
            SMEFTEvol3000.EvolveSMEFTOnly(Lambda_NP, fmin(3000.,Lambda_NP) );
            SMEFTEvol5000.EvolveSMEFTOnly(Lambda_NP, fmin(5000.,Lambda_NP) );
        } else {
            SMEFTEvolMH.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
            SMEFTEvol240.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
            SMEFTEvol365.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
            SMEFTEvol550.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
            SMEFTEvol1000.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
            SMEFTEvol1500.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
            SMEFTEvol3000.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
            SMEFTEvol5000.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
        }
        
    } else {
 
        // SMEFT initial conditions for RGEsolver SMEFTEvolEW
        setSMEFTEvolWC(SMEFTEvolEW);
        
        SMEFTEvolEW.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
        SMEFTEvolEW.EvolveSMOnly("Numeric", muw, muw);
        
        // Work with the extra instances of RGEsolver: would be better to have a deep copy of SMEFTEvolEW
 
        // SM initial conditions for RGEsolver        
        SMEFTEvolMH.GenerateSMInitialConditions(muw, muw, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol240.GenerateSMInitialConditions(muw, muw, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol365.GenerateSMInitialConditions(muw, muw, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol550.GenerateSMInitialConditions(muw, muw, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol1000.GenerateSMInitialConditions(muw, muw, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol1500.GenerateSMInitialConditions(muw, muw, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol3000.GenerateSMInitialConditions(muw, muw, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvol5000.GenerateSMInitialConditions(muw, muw, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
        
        SMEFTEvolUV.GenerateSMInitialConditions(muw, muw, SMEFTBasisFlag, "Numeric",
            g1_LEW, g2_LEW, g3_LEW, lambdaH_LEW, mH2_LEW,
            Mu_LEW, Md_LEW, Me_LEW, s12CKM_LEW, s13CKM_LEW, s23CKM_LEW, dCKM_LEW);
 
        // SMEFT initial conditions for RGEsolver        
        setSMEFTEvolWC(SMEFTEvolMH);
        setSMEFTEvolWC(SMEFTEvol240);
        setSMEFTEvolWC(SMEFTEvol365);
        setSMEFTEvolWC(SMEFTEvol550);
        setSMEFTEvolWC(SMEFTEvol1000);
        setSMEFTEvolWC(SMEFTEvol1500);
        setSMEFTEvolWC(SMEFTEvol3000);
        setSMEFTEvolWC(SMEFTEvol5000);
        setSMEFTEvolWC(SMEFTEvolUV); // Not evolved. Only for reference to retrieve C(Lambda)
        
        // Skip RGE by setting the two scales at Lambda_NP for the EFT
        SMEFTEvolMH.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
        SMEFTEvol240.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
        SMEFTEvol365.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
        SMEFTEvol550.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
        SMEFTEvol1000.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
        SMEFTEvol1500.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
        SMEFTEvol3000.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
        SMEFTEvol5000.EvolveSMEFTOnly(Lambda_NP, Lambda_NP);
    }
    
    // Renormalization of gauge fields parameters
    delta_ZZ = (cW2_tree * getSMEFTCoeffEW("CHW") + sW2_tree * getSMEFTCoeffEW("CHB") + sW_tree * cW_tree * getSMEFTCoeffEW("CHWB")) * v2;
    delta_AA = (sW2_tree * getSMEFTCoeffEW("CHW") + cW2_tree * getSMEFTCoeffEW("CHB") - sW_tree * cW_tree * getSMEFTCoeffEW("CHWB")) * v2;
    delta_AZ = 2.0 * sW_tree * cW_tree * (getSMEFTCoeffEW("CHW") - getSMEFTCoeffEW("CHB")) * v2
            - (cW2_tree - sW2_tree) * getSMEFTCoeffEW("CHWB") * v2;
 
    // Similar definitions for the EWPO
    delta_Z = 2.0 * sW_tree * cW_tree * getSMEFTCoeffEW("CHWB") * v2;
    delta_A = -2.0 * sW_tree * cW_tree * getSMEFTCoeffEW("CHWB") * v2;
    delta_ZA = (cW2_tree - sW2_tree) * getSMEFTCoeffEW("CHWB") * v2;
 
    // Renormalization of Higgs field parameter
    delta_h = (-getSMEFTCoeffEW("CHD") / 4.0 + getSMEFTCoeffEW("CHbox")) * v2;
 
    //  Calculation of some quantities repeatedly used in the code
 
    //  NP corrections to Z and W mass Lagrangian parameters
    delta_MZ = (sW_tree * cW_tree * getSMEFTCoeffEW("CHWB") + 0.25 * getSMEFTCoeffEW("CHD") + (3.0 / 8.0) * getSMEFTCoeffEW("CH") / lambdaH_tree) * v2;
    delta_MW = (3.0 / 8.0) * (getSMEFTCoeffEW("CH") / lambdaH_tree) * v2;
 
    //  NP correction to Fermi constant, as extracted from muon decay
    delta_GF = DeltaGF();
 
    //  NP correction to the vev, as extracted from GF
    delta_v = 0.5 * delta_GF;
 
    //  NP corrections to electric constant parameter and weak mixing angle, depending on the input scheme
    delta_e = cAsch * (-0.5 * delta_A)
            + cWsch * ((cW2_tree / sW2_tree) * (delta_MW - delta_MZ) - 0.5 * delta_GF);
    
    delta_em = delta_e + 0.5 * delta_A; // Relative dimension 6 correction to the QED interaction vertex
 
    delta_sW2 = cAsch * (-cW2_tree * (delta_GF - 2.0 * (delta_MW - delta_MZ) - delta_A) / (sW2_tree - cW2_tree))
            + cWsch * (2.0 * cW2_tree * (delta_MW - delta_MZ) / sW2_tree);
 
    //  NP indirect corrections to EW fermion couplings
    delta_UgNC = (0.5 * delta_Z - 0.5 * delta_GF + delta_MW - delta_MZ);
 
    delta_QgNC = -(sW_tree * cW_tree * delta_ZA + sW2_tree * delta_sW2);
 
    delta_UgCC = (delta_e - 0.5 * delta_sW2);
    
    //AG:begin
    delta_ale = -2.0 * sW_tree * cW_tree * getSMEFTCoeffEW("CHWB") * v2;
 
    delta_Mz2 = (getSMEFTCoeffEW("CHD") / 2.0 + 2.0 * sW_tree * cW_tree * getSMEFTCoeffEW("CHWB")) * v2;
 
    delta_g1 = cAsch * (g1_tree * (cW2_tree * delta_ale - sW2_tree * (delta_Mz2 + delta_GF)) / 2.0 / (-1 + 2.0 * sW2_tree))
            + cWsch * (g1_tree * (-delta_Mz2 / 2.0 / sW2_tree - delta_GF / 2.0));
 
    delta_g2 = cAsch * (g2_tree * (sW2_tree * delta_ale - cW2_tree * (delta_Mz2 + delta_GF)) / 2.0 / (cW2_tree - sW2_tree))
            + cWsch * (g2_tree * (-delta_GF / 2.0));
 
    xWZ_tree = +g2_tree / pow((g1_tree * g1_tree + g2_tree * g2_tree), 0.5); // cbar of Manohar
    delta_xWZ = g1_tree * (g1_tree * delta_g2 - g2_tree * delta_g1 + g1_tree * g1_tree * getSMEFTCoeffEW("CHWB") * v2) / pow((g1_tree * g1_tree + g2_tree * g2_tree), 1.5);
 
    xBZ_tree = -g1_tree / pow((g1_tree * g1_tree + g2_tree * g2_tree), 0.5); // -sbar of Manohar
    delta_xBZ = g2_tree * (g1_tree * delta_g2 - g2_tree * delta_g1 - g2_tree * g2_tree * getSMEFTCoeffEW("CHWB") * v2) / pow((g1_tree * g1_tree + g2_tree * g2_tree), 1.5);
    //AG:end
 
    //Go to mass eigenstate basis first; this is done here since we need to reassign quark masses and the CKM matrix
 
    double vT = v();
    double delta_vT = getDelta_v();
    double vTosq2 = vT / sqrt(2.);
 
    // Let us first define the full mass matrices, including the effect of dimension six operators
 
    for (int i = 0; i < 3; i++)
        for (int j = 0; j < 3; j++) {
            MUQ.assignre(i, j, vTosq2 * (getSMEFTCoeffEW("YuR", i, j) * (1. + delta_vT) + FlagCorrsInSMRunning * getSMEFTCoeffEW("dYuR", i, j) - getSMEFTCoeffEW("CuHR", j, i) * v2 / 2.));
            MUQ.assignim(i, j, vTosq2 * (getSMEFTCoeffEW("YuI", i, j) * (1. + delta_vT) + FlagCorrsInSMRunning * getSMEFTCoeffEW("dYuI", i, j) + getSMEFTCoeffEW("CuHI", j, i) * v2 / 2.));
            MDQ.assignre(i, j, vTosq2 * (getSMEFTCoeffEW("YdR", i, j) * (1. + delta_vT) + FlagCorrsInSMRunning * getSMEFTCoeffEW("dYdR", i, j) - getSMEFTCoeffEW("CdHR", j, i) * v2 / 2.));
            MDQ.assignim(i, j, vTosq2 * (getSMEFTCoeffEW("YdI", i, j) * (1. + delta_vT) + FlagCorrsInSMRunning * getSMEFTCoeffEW("dYdI", i, j) + getSMEFTCoeffEW("CdHI", j, i) * v2 / 2.));
        }
 
    gslpp::vector<double> mmu(3), mmd(3);
    
    //std::cout<<"    |"<<MUQ(0,0)<<","<<MUQ(0,1)<<","<<MUQ(0,2)<<"|"<<std::endl;
    //std::cout<<"MUQ=|"<<MUQ(1,0)<<","<<MUQ(1,1)<<","<<MUQ(1,2)<<"|"<<std::endl;
    //std::cout<<"    |"<<MUQ(2,0)<<","<<MUQ(2,1)<<","<<MUQ(2,2)<<"|"<<std::endl;
    //std::cout<<"  "<<std::endl;
    //std::cout<<"    |"<<MDQ(0,0)<<","<<MDQ(0,1)<<","<<MDQ(0,2)<<"|"<<std::endl;
    //std::cout<<"MDQ=|"<<MDQ(1,0)<<","<<MDQ(1,1)<<","<<MDQ(1,2)<<"|"<<std::endl;
    //std::cout<<"    |"<<MDQ(2,0)<<","<<MDQ(2,1)<<","<<MDQ(2,2)<<"|"<<std::endl;
    //std::cout<<"  "<<std::endl;
 
    MUQ.singularvalue(VuR, VuL, mmu);
    if(mmu(2) < 50.0) {
        std::cout << "Warning: top quark mass is too low, m(2) = " << mmu(2) << std::endl;
        return false;
    }
 
    MDQ.singularvalue(VdR, VdL, mmd);
    if(mmd(2) < 2.5) {
        std::cout << "Warning: bottom quark mass is too low, m(2) = " << mmd(2) << std::endl;
        return false;
    }
 
    //do heavy quarks first to get the thresholds right
    quarks[TOP].setMass(Mofmu2Mbar(mmu(2), getMuw(), QCD::TOP));
    trueSM.setQuarkMass(TOP,Mofmu2Mbar(mmu(2), getMuw(), QCD::TOP));
    setMtpole(Mbar2Mp(quarks[TOP].getMass(), QCD::TOP));
    trueSM.setMtpole(Mbar2Mp(quarks[TOP].getMass(), QCD::TOP));
    quarks[BOTTOM].setMass(Mofmu2Mbar(mmd(2), getMuw(), QCD::BOTTOM));
    trueSM.setQuarkMass(BOTTOM,Mofmu2Mbar(mmd(2), getMuw(), QCD::BOTTOM));
    quarks[CHARM].setMass(Mofmu2Mbar(mmu(1), getMuw(), QCD::CHARM));
    trueSM.setQuarkMass(CHARM,Mofmu2Mbar(mmu(1), getMuw(), QCD::CHARM));
    quarks[STRANGE].setMass(Mrun(quarks[STRANGE].getMass_scale(), getMuw(), mmd(1), QCD::STRANGE));
    trueSM.setQuarkMass(STRANGE,Mrun(quarks[STRANGE].getMass_scale(), getMuw(), mmd(1), QCD::STRANGE));
    quarks[DOWN].setMass(Mrun(quarks[DOWN].getMass_scale(), getMuw(), mmd(0), QCD::DOWN));
    trueSM.setQuarkMass(DOWN,Mrun(quarks[DOWN].getMass_scale(), getMuw(), mmd(0), QCD::DOWN));
    quarks[UP].setMass(Mrun(quarks[UP].getMass_scale(), getMuw(), mmu(0), QCD::UP));
    trueSM.setQuarkMass(UP,Mrun(quarks[UP].getMass_scale(), getMuw(), mmu(0), QCD::UP));
 
    VuLd = VuL.hconjugate();
 
    // Computing the CKM
    gslpp::matrix<complex> CKMUnphys = VuLd * VdL;
 
    // std::cout << "CKM unphys = " << CKMUnphys << std::endl;
 
    myCKM.computeCKM(CKMUnphys(0, 1).abs(), CKMUnphys(1, 2).abs(), CKMUnphys(0, 2).abs(),
            (-CKMUnphys(0, 0) * CKMUnphys(0, 2).conjugate() / (CKMUnphys(1, 0) * CKMUnphys(1, 2).conjugate())).arg());
    trueSM.setCKM(myCKM);
 
    // std::cout << "computed CKM = " << getCKM().getCKM() << std::endl;
 
    double a11 = remainder(CKMUnphys(0, 0).arg() - getCKM().getV_ud().arg(), 2. * M_PI);
    double a12 = remainder(CKMUnphys(0, 1).arg() - getCKM().getV_us().arg(), 2. * M_PI);
    double a13 = remainder(CKMUnphys(0, 2).arg() - getCKM().getV_ub().arg(), 2. * M_PI);
 
    //    double a23 = (gslpp::complex(CKMUnphys(1, 0) / CKM(1, 0))).arg() - a11 + a13;
    //    double a33 = (gslpp::complex(CKMUnphys(2, 0) / CKM(2, 0))).arg() - a11 + a13;
    double a23 = remainder(CKMUnphys(1, 0).arg() - getCKM().getV_cd().arg(), 2. * M_PI) - a11 + a13;
    double a33 = remainder(CKMUnphys(2, 0).arg() - getCKM().getV_td().arg(), 2. * M_PI) - a11 + a13;
 
    gslpp::matrix<gslpp::complex> phi1(3, 3, 0.);
    phi1.assign(0, 0, 1.);
    phi1.assign(1, 1, gslpp::complex(1., a23 - a13, true));
    phi1.assign(2, 2, gslpp::complex(1., a33 - a13, true));
 
    gslpp::matrix<gslpp::complex> phi2dag(3, 3, 0.);
    phi2dag.assign(0, 0, gslpp::complex(1., -a11, true));
    phi2dag.assign(1, 1, gslpp::complex(1., -a12, true));
    phi2dag.assign(2, 2, gslpp::complex(1., -a13, true));
 
    VuL = VuL * phi1;
    VuR = VuR * phi1;
    VdL = VdL * phi2dag;
    VdR = VdR * phi2dag;
 
    // Hermitian conjugates
    VuLd = VuL.hconjugate();
    VuRd = VuR.hconjugate();
    VdLd = VdL.hconjugate();
    VdRd = VdR.hconjugate();
 
 
    // do the NPbase PostUpdate without recomputing the top mass and the CKM matrix
    computemt=false;
    trueSM.setComputemt(false);
    requireCKM=false;
    trueSM.setRequireCKM(false);
 
    if (!NPbase::PostUpdate()) return (false);
    if (!trueSM.PostUpdate()) return (false);
    
    // Also need to recompute some of the parameters that may depend of the top quark mass. 
    // In the W scheme, that is the case of alphaMz(), which is computed from Mw
    // In the alpha scheme this is an input so this does nothing. All derived quantities in
    // GenerateSMInitialConditions() stay at the same value
    aleMz = trueSM.alphaMz();   
 
    //  NP corrections to Total Higgs width
    dGammaHTotR1 = deltaGammaTotalRatio1();
 
    if (FlagQuadraticTerms) {
        dGammaHTotR2 = deltaGammaTotalRatio2();
    } else {
        dGammaHTotR2 = 0.0;
    }
 
    //  Total: to be used in BR functions to check positivity
    GammaHTotR = 1.0 + dGammaHTotR1 + dGammaHTotR2;
 
    // The total theory error in the H width: set to 0.0 for the moment
    eHwidth = deltaGammaTotalRatio1() - deltaGammaTotalRatio1noError();
    
    // C1 value for the total Higgs width
    C1Htotal = C1Htot();
 
    //The call to this method should be dropped once we have correctly implemented the matching
    //getWCFromEvolutor();
 
 
    UevL = 1.0; // Neglect PMNS effects in high-pT observables 
    VudL = 1.0; // Neglect CKM effects in high-pT observables 
 
    //    Yuke = sqrt(2.) * (leptons[ELECTRON].getMass()) / v();
    //    Yukmu = sqrt(2.) * (leptons[MU].getMass()) / v();
    //    Yuktau = sqrt(2.) * (leptons[TAU].getMass()) / v();
    //    Yuku = sqrt(2.) * (quarks[UP].getMass()) / v();
    //    Yukc = sqrt(2.) * (quarks[CHARM].getMass()) / v();
    //    Yukt = sqrt(2.) * mtpole / v();
    //    Yukd = sqrt(2.) * (quarks[DOWN].getMass()) / v();
    //    Yuks = sqrt(2.) * (quarks[STRANGE].getMass()) / v();
    //    Yukb = sqrt(2.) * (quarks[BOTTOM].getMass()) / v();
 
 
    //  Dimension-6 coefficients used in the STXS parameterization: to be discussed with AJL
    //    aiG = 16.0 * M_PI * M_PI * getSMEFTCoeffEW("CHG") * Mw_tree * Mw_tree / g3_tree / g3_tree / LambdaNP2;
    //    ai3G = getSMEFTCoeffEW("CG") * Mw_tree * Mw_tree / g3_tree / g3_tree / g3_tree / LambdaNP2;
    //    ai2G = 0.0; // Add
    //    aiT = 2.0 * getSMEFTCoeffEW("CHD") * v2;
    //    aiH = -2.0 * getSMEFTCoeffEW("CHbox") * v2;
    //    aiWW = 0.0; // Add
    //    aiB = 0.0; // Add
    //    aiHW = 0.0;
    //    aiHB = 0.0;
    //    aiA =getSMEFTCoeffEW("CHB") * Mw_tree * Mw_tree / g1_tree / g1_tree / LambdaNP2;
    //    aiHQ = getSMEFTCoeffEW("CHq1R",0,0) * v2; // Valid only for flavour universal NP
    //    aipHQ = getSMEFTCoeffEW("CHq3R",0,0) * v2; // Valid only for flavour universal NP
    //    aiHL = getSMEFTCoeffEW("CHl1R",0,0) * v2; // Valid only for flavour universal NP
    //    aipHL = getSMEFTCoeffEW("CHl3R",0,0) * v2; // Valid only for flavour universal NP. From HEL Lagrangian. Not in original note
    //    aiHu = getSMEFTCoeffEW("CHuR",0,0) * v2; // Valid only for flavour universal NP
    //    aiHd = getSMEFTCoeffEW("CHdR",0,0) * v2; // Valid only for flavour universal NP
    //    aiHe = getSMEFTCoeffEW("CHeR",0,0) * v2; // Valid only for flavour universal NP
    //    aiu = -getSMEFTCoeffEW("CuHR",2,2) * v2 / Yukt;
    //    aiuG = getSMEFTCoeffEW("CuGR",2,2) * Mw_tree * Mw_tree / g3_tree / LambdaNP2 / getSMEFTCoeffEW("YuR",2,2) / 4.0; // From HEL.fr Lagrangian. Not in original note. Valid only for flavour universal NP
 
    //  Dim 6 SMEFT-LEFT matching
 
    // update LEFT Wilson coefficients (time consuming, do only if FlagmatchLEFT=true
    if (FlagmatchLEFT) getMatching().updateLEFTGeneralParameters();
    
    
    //  3) Store some of the operators at the EW scale in the physical basis
    
    // Diagonal-elements of neutral-current (NC) combinations are always real
    
    // NC up-quark sector
    CHq1EWuu = getSMEFTCoeffEWMB("CHq1", 0, 0, VuLd, VuL).real();
    CHq1EWcc = getSMEFTCoeffEWMB("CHq1", 1, 1, VuLd, VuL).real();
    CHq1EWtt = getSMEFTCoeffEWMB("CHq1", 2, 2, VuLd, VuL).real();
    
    CHq3EWuu = getSMEFTCoeffEWMB("CHq3", 0, 0, VuLd, VuL).real();
    CHq3EWcc = getSMEFTCoeffEWMB("CHq3", 1, 1, VuLd, VuL).real();
    CHq3EWtt = getSMEFTCoeffEWMB("CHq3", 2, 2, VuLd, VuL).real();
    
    CHuEWuu = getSMEFTCoeffEWMB("CHu", 0, 0, VuRd, VuR).real();
    CHuEWcc = getSMEFTCoeffEWMB("CHu", 1, 1, VuRd, VuR).real();
    CHuEWtt = getSMEFTCoeffEWMB("CHu", 2, 2, VuRd, VuR).real();
    
    // NC down-quark sector
    CHq1EWdd = getSMEFTCoeffEWMB("CHq1", 0, 0, VdLd, VdL).real();
    CHq1EWss = getSMEFTCoeffEWMB("CHq1", 1, 1, VdLd, VdL).real();
    CHq1EWbb = getSMEFTCoeffEWMB("CHq1", 2, 2, VdLd, VdL).real();
    
    CHq3EWdd = getSMEFTCoeffEWMB("CHq3", 0, 0, VdLd, VdL).real();
    CHq3EWss = getSMEFTCoeffEWMB("CHq3", 1, 1, VdLd, VdL).real();
    CHq3EWbb = getSMEFTCoeffEWMB("CHq3", 2, 2, VdLd, VdL).real();
    
    CHdEWdd = getSMEFTCoeffEWMB("CHd", 0, 0, VdRd, VdR).real();
    CHdEWss = getSMEFTCoeffEWMB("CHd", 1, 1, VdRd, VdR).real();
    CHdEWbb = getSMEFTCoeffEWMB("CHd", 2, 2, VdRd, VdR).real();
    
    // Charged-Current up-down-quark sector (complex)   
    CHq3EWud = getSMEFTCoeffEWMB("CHq3", 0, 0, VuLd, VdL);
    CHq3EWcs = getSMEFTCoeffEWMB("CHq3", 1, 1, VuLd, VdL);
    CHq3EWtb = getSMEFTCoeffEWMB("CHq3", 2, 2, VuLd, VdL);
    
    
    return (true);
}

◆ ppZHprobe()

const double NPSMEFTd6General::ppZHprobe ( const double sqrt_s ) const

virtual

The direction constrained by $ p p \to Z H$ in the boosted regime, $g_p^Z$. From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6General class.

Returns: $g_p^Z$

Reimplemented from NPbase.

Definition at line 39254 of file NPSMEFTd6General.cpp.

                                                                  {
 
    double gpZ = 0.0;
 
    double ghZuL, ghZdL, ghZuR, ghZdR;
 
    // In the Warsaw basis the contact interactions are generated only by CHF ops but
    // in the modified basis ODHB, ODHW also contribute
 
    ghZuL = -(eeMz / sW_tree / cW_tree)*(getSMEFTCoeffEW("CHq1R", 0, 0) - getSMEFTCoeffEW("CHq3R", 0, 0) ) * v2;
    ghZdL = -(eeMz / sW_tree / cW_tree)*(getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq3R", 0, 0) ) * v2;
    ghZuR = -(eeMz / sW_tree / cW_tree)*(getSMEFTCoeffEW("CHuR", 0, 0) ) * v2;
    ghZdR = -(eeMz / sW_tree / cW_tree)*(getSMEFTCoeffEW("CHdR", 0, 0) ) * v2;
 
    if (sqrt_s == 14.0) {
 
        gpZ = ghZuL - 0.76 * ghZdL - 0.45 * ghZuR + 0.14 * ghZdR;
 
    } else if (sqrt_s == 27.0) {
        // Use the same as for 14 TeV for the moment 
 
        gpZ = ghZuL - 0.76 * ghZdL - 0.45 * ghZuR + 0.14 * ghZdR;
 
    } else if (sqrt_s == 100.0) {
 
        gpZ = ghZuL - 0.90 * ghZdL - 0.45 * ghZuR + 0.17 * ghZdR;
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::ppZHprobe()");
 
    return gpZ;
 
}

◆ PreUpdate()

bool NPSMEFTd6General::PreUpdate ( )

virtual

The pre-update method for NPSMEFTd6General.

This method runs all the procedures that are need to be executed before the model is successfully updated.

Returns: a boolean that is true if the execution is successful

Reimplemented from StandardModel.

Definition at line 3000 of file NPSMEFTd6General.cpp.

                                 {
    SMEFTEvolEW.Reset();    
    SMEFTEvolMH.Reset();
    SMEFTEvol240.Reset();
    SMEFTEvol365.Reset();
    SMEFTEvol550.Reset();
    SMEFTEvol1000.Reset();
    SMEFTEvol1500.Reset();
    SMEFTEvol3000.Reset();
    SMEFTEvol5000.Reset();
    SMEFTEvolUV.Reset();
 
    isSMInitialConditionComputed = false;
 
    if (!NPbase::PreUpdate()) return (false);
 
    return (true);
}

◆ R0_f()

const double NPSMEFTd6General::R0_f ( const Particle f ) const

virtual

The ratio $R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell$, $R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}$ and $R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}$, for charged leptons, quarks and neutrinos, respectively.

\[ R^0_f = R_f^{SM} + \Delta R_f^{(1)} + \Delta R_f^{(2)} \]

Parameters

[in] f a lepton or quark

Returns: $R_f^0$, including SM plus $\mathcal{O}(\Lambda^{-2})$ and $\mathcal{O}(\Lambda^{-4})$ NP contributions

Reimplemented from NPbase.

Definition at line 17008 of file NPSMEFTd6General.cpp.

{
    return (trueSM.R0_f(f) + deltaR0_f(f));
}

◆ RWc()

const double NPSMEFTd6General::RWc ( ) const

virtual

The ratio $R_{W,c)=\Gamma(W\to c + X)/\Gamma(W\to had)$.

Returns: $R_{W,c)$ in GeV

Reimplemented from NPbase.

Definition at line 16191 of file NPSMEFTd6General.cpp.

                                         {
    double GammWcX0, GammWhad0;
    double dGammWcX, dGammWhad;
 
    //  For the SM contributions to the of W widths, proceed as in the SM implementation, 
    //  using W->cX = W->cs and W->had = W->ud + W->cs. (See comments in StandardModel.cpp>RWc.)
 
    //  Add all the  W-> cX decays
    //  In SM GammaW fermion masses are ignored and CKM=1 but uses that SM CKM is unitary => I only need W->cs
    GammWcX0 = trueSM.GammaW(quarks[CHARM], quarks[STRANGE]);
 
    //  SMEFT NP effects, however, can break CKM unitarity and I need to add all fermion decays explicitly
    dGammWcX = deltaGamma_Wff(quarks[CHARM], quarks[STRANGE])
            + deltaGamma_Wff(quarks[CHARM], quarks[DOWN])
            + deltaGamma_Wff(quarks[CHARM], quarks[BOTTOM]);
 
    //  For the same reasons, I only need to add the W-> ud decays into the SM hadronic W width
    GammWhad0 = GammWcX0
            + trueSM.GammaW(quarks[UP], quarks[DOWN]);
 
    //  and, similarly, for the NP corrections to hadronic width I need all fermion decays explicitly
    dGammWhad = dGammWcX
            + deltaGamma_Wff(quarks[UP], quarks[STRANGE])
            + deltaGamma_Wff(quarks[UP], quarks[DOWN])
            + deltaGamma_Wff(quarks[UP], quarks[BOTTOM]);
 
    return GammWcX0 / GammWhad0 + dGammWcX / GammWhad0 - GammWcX0 * dGammWhad / GammWhad0 / GammWhad0;
}

◆ RWlilj()

const double NPSMEFTd6General::RWlilj	(	const Particle	li,
		const Particle	lj
	)		const

virtual

The lepton universality ratio $R_{W,l_i/l_j)=\Gamma(W\to l_i \nu_i)/\Gamma(W\to l_j \nu_j)$.

Returns: $R_{W,l_i/l_j)$ in GeV

Reimplemented from NPbase.

Definition at line 16158 of file NPSMEFTd6General.cpp.

                                                                                {
    double GammWli0, GammWlj0;
    double dGammWli, dGammWlj;
 
    if (li.is("ELECTRON")) {
        GammWli0 = trueSM.GammaW(leptons[NEUTRINO_1], li);
        dGammWli = deltaGamma_Wff(leptons[NEUTRINO_1], li);
    } else if (li.is("MU")) {
        GammWli0 = trueSM.GammaW(leptons[NEUTRINO_2], li);
        dGammWli = deltaGamma_Wff(leptons[NEUTRINO_2], li);
    } else if (li.is("TAU")) {
        GammWli0 = trueSM.GammaW(leptons[NEUTRINO_3], li);
        dGammWli = deltaGamma_Wff(leptons[NEUTRINO_3], li);
    } else {
        throw std::runtime_error("Error in NPSMEFTd6General::RWlilj. li must be a charged lepton");
    }
 
    if (lj.is("ELECTRON")) {
        GammWlj0 = trueSM.GammaW(leptons[NEUTRINO_1], lj);
        dGammWlj = deltaGamma_Wff(leptons[NEUTRINO_1], lj);
    } else if (lj.is("MU")) {
        GammWlj0 = trueSM.GammaW(leptons[NEUTRINO_2], lj);
        dGammWlj = deltaGamma_Wff(leptons[NEUTRINO_2], lj);
    } else if (lj.is("TAU")) {
        GammWlj0 = trueSM.GammaW(leptons[NEUTRINO_3], lj);
        dGammWlj = deltaGamma_Wff(leptons[NEUTRINO_3], lj);
    } else {
        throw std::runtime_error("Error in NPSMEFTd6General::RWlilj. lj must be a charged lepton");
    }
 
    return GammWli0 / GammWlj0 + dGammWli / GammWlj0 - GammWli0 * dGammWlj / GammWlj0 / GammWlj0;
}

◆ RZlilj()

const double NPSMEFTd6General::RZlilj	(	const Particle	li,
		const Particle	lj
	)		const

virtual

The lepton universality ratio $R_{Z,l_i/l_j)=\Gamma(Z\to l_i^+ l_i^-)/\Gamma(Z\to l_j^+ l_j^-)$.

Returns: $R_{Z,l_i/l_j)$ in GeV

Reimplemented from NPbase.

Definition at line 16220 of file NPSMEFTd6General.cpp.

                                                                                {
    double GammZli0, GammZlj0;
    double dGammZli, dGammZlj;
 
    if (li.is("ELECTRON") || li.is("MU") || li.is("TAU")) {
        GammZli0 = trueSM.GammaZ(li);
        dGammZli = deltaGamma_Zf(li);
    } else {
        throw std::runtime_error("Error in NPSMEFTd6General::RZlilj. li must be a charged lepton");
    }
 
    if (lj.is("ELECTRON") || lj.is("MU") || lj.is("TAU")) {
        GammZlj0 = trueSM.GammaZ(lj);
        dGammZlj = deltaGamma_Zf(lj);
    } else {
        throw std::runtime_error("Error in NPSMEFTd6General::RZlilj. lj must be a charged lepton");
    }
 
    return GammZli0 / GammZlj0 + dGammZli / GammZlj0 - GammZli0 * dGammZlj / GammZlj0 / GammZlj0;
}

◆ setFlag()

bool NPSMEFTd6General::setFlag	(	const std::string	name,
		const bool	value
	)

virtual

A method to check if all the mandatory parameters for NPSMEFTd6General have been provided in model initialization.

Parameters

[in] DPars a map of the parameters that are being updated in the Monte Carlo run (including parameters that are varied and those that are held constant)

Returns: a boolean that is true if the execution is successful

A method to set a flag of NPSMEFTd6General.

Parameters

[in]	name	name of a model flag
[in]	value	the boolean to be assigned to the flag specified by name

Returns: a boolean that is true if the execution is successful

Reimplemented from NPbase.

Reimplemented in NPd6SILH, and NPSMEFTd6CHRU.

Definition at line 14075 of file NPSMEFTd6General.cpp.

                                                                     {
    bool res = false;
    if (name.compare("MWinput") == 0) {
        FlagMWinput = value;
        //We need to fix FlagMWinput also in the StandardModel
        res = NPbase::setFlag(name, value);
        res = trueSM.setFlag(name, value);
        //    res = true;    
    } else if (name.compare("QuadraticTerms") == 0) {
        FlagQuadraticTerms = value;
        if (value) setModelLinearized(false);
        if (value) setModelNPquadratic(true); //AG:added
        res = true;
    } else if (name.compare("HiggsSM") == 0) {
        FlagHiggsSM = value;
        res = true;
    } else if (name.compare("LoopHd6") == 0) {
        FlagLoopHd6 = value;
        res = true;
    } else if (name.compare("LoopH3d6Quad") == 0) {
        FlagLoopH3d6Quad = value;
        res = true; 
    } else if (name.compare("RGEci") == 0) {
        FlagRGEci = value;
        res = true;
    } else if (name.compare("CorrsInSMRunning") == 0) {
        FlagCorrsInSMRunning = value;
        res = true;
    } else if (name.compare("multiScaleRGE") == 0) {
        FlagmultiScaleRGE = value;
        res = true;
    } else if (name.compare("finiteNLO") == 0) {
        FlagfiniteNLO = value;
        res = true;
    } else if (name.compare("matchLEFT") == 0) {
        FlagmatchLEFT = value;
        res = true;
    } else if (name.compare("NewTerms") == 0) {
        FlagNewTerms = value;
        res = true;
    } else if (name.compare("MomProp") == 0) {
        FlagMomProp = value;
        res = true;
    } else if (name.compare("MomVert") == 0) {
        FlagMomVert = value;
        res = true;
    } else if (name.compare("HiggsExch") == 0) {
        FlagHiggsExch= value;
        res = true;
    } else if (name.compare("QuadraticWC") == 0) {
        FlagQuadraticWC = value;
        res = true;
    } else
        res = NPbase::setFlag(name, value);
    
    if (FlagMWinput) {
        //  MW scheme
        cAsch = 0.;
        cWsch = 1.;
    } else {
        //  ALpha scheme
        cAsch = 1.;
        cWsch = 0.;
    }
    
    if (!FlagLoopHd6) {
        cLHd6 = 0.0;
    } else {
        cLHd6 = 1.0;
    }
    
    if (!FlagHiggsSM) {
        cHSM = 0.0;
    } else {
        cHSM = 1.0;
    }
    
    if (FlagLoopH3d6Quad || FlagQuadraticTerms) {
        cLH3d62 = 1.0;
    } else {
        cLH3d62 = 0.0;
    }
    
    if (!FlagfiniteNLO) {
        cNLOd6 = 0.0;
    } else {
        cNLOd6 = 1.0;
    }
 
    return (res);
}

◆ setFlagStr()

bool NPSMEFTd6General::setFlagStr	(	const std::string	name,
		const std::string	value
	)

virtual

A method to set a flag of NPSMEFTd6General.

Parameters

[in]	name	name of a model flag
[in]	value	the value to be assigned to the flag specified by name

Returns: a boolean that is true if the execution is successful

Reimplemented from StandardModel.

Definition at line 14167 of file NPSMEFTd6General.cpp.

{
    if (name.compare("SMEFTBasisFlag") == 0) {
        SMEFTBasisFlag = value;
        
        if (SMEFTBasisFlag == "UP") {
            flavBas = 1;
        } else if (SMEFTBasisFlag == "DOWN") {
            flavBas = 2;
        } else
            throw std::runtime_error("Bad argument in SMEFTBasisFlag. (Only UP or DOWN are currently allowed)");
        
        return true;
    } else
        return NPbase::setFlagStr(name, value);
    return false;
}

◆ sigma0_had()

const double NPSMEFTd6General::sigma0_had ( ) const

virtual

The cross section for the process $e^+ e^-\to Z\to \mathrm{hadrons}$ at the $Z$ pole, $\sigma_h^0$.

\[ \sigma_h = \sigma_h^{SM} + \Delta \sigma_h^{(1)} + \Delta \sigma_h^{(2)} \]

Returns: $\sigma_h^0$ in GeV $^{-2}$, including SM plus $\mathcal{O}(\Lambda^{-2})$ and $\mathcal{O}(\Lambda^{-4})$ NP contributions

Reimplemented from NPbase.

Definition at line 16341 of file NPSMEFTd6General.cpp.

{    
    return (trueSM.sigma0_had() + deltaSigmaHadron());
}

◆ STXS0_qqH()

const double NPSMEFTd6General::STXS0_qqH ( const double sqrt_s ) const

virtual

The STXS0 bin $pp \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39406 of file NPSMEFTd6General.cpp.

                                                                  {
 
    double STXSb = 1.0;
 
    double C1 = 0.0;
 
    if (sqrt_s == 13.0) {
 
        C1 = 0.0064; // Use the same as VBF 
 
        STXSb +=
                +121687. * getSMEFTCoeffEW("CHbox")
                - 162383. * getSMEFTCoeffEW("CHD")
                + 6933.53 * getSMEFTCoeffEW("CHB")
                + 133459. * getSMEFTCoeffEW("CHW")
                - 286707. * getSMEFTCoeffEW("CHWB")
                - 1929.85 * getSMEFTCoeffEW("CHq1R", 0, 0)
                + 1378.01 * getSMEFTCoeffEW("CHq1R", 1, 1)
                + 2505.13 * getSMEFTCoeffEW("CHq1R", 2, 2)
                + 17471.4 * getSMEFTCoeffEW("CHuR", 0, 0)
                + 532.133 * getSMEFTCoeffEW("CHuR", 1, 1)
                - 6552.85 * getSMEFTCoeffEW("CHdR", 0, 0)
                - 454.364 * getSMEFTCoeffEW("CHdR", 1, 1)
                - 437.319 * getSMEFTCoeffEW("CHdR", 2, 2)
                + 152289. * getSMEFTCoeffEW("CHq3R", 0, 0)
                - 2645.75 * getSMEFTCoeffEW("CHq3R", 1, 1)
                + 2515.78 * getSMEFTCoeffEW("CHq3R", 2, 2)
                - 4.496 * delta_GF
                - 0.084 * deltaGzd6()
                - 2.759 * deltaMwd6()
                - 0.142 * deltaGwd6()
                ;
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            STXSb += 0.0;
 
        }
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS0_qqH()");
 
    //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
    // Use the same as VBF
    STXSb += eVBFint + eVBFpar;
 
    //  Linear contribution from Higgs self-coupling
    STXSb = STXSb + cLHd6 * deltaH3L1(C1) * deltaG_hhhRatio();
    //  Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
    STXSb = STXSb + cLHd6 * cLH3d62 * deltaH3L2(C1) * deltaG_hhhRatio() * deltaG_hhhRatio();
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_BrH4lRatio()

const double NPSMEFTd6General::STXS12_BrH4lRatio ( ) const

virtual

The STXS BR $ H \to 4l $, $l=e,\mu$.

Reimplemented from NPbase.

Definition at line 40025 of file NPSMEFTd6General.cpp.

                                                       {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiTotR1 = 0.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    // 4l
    dGHiR1 = (0.12 * getSMEFTCoeffEW("CHbox") + 0.005 * getSMEFTCoeffEW("CHD") - 0.296 * getSMEFTCoeffEW("CHW") - 0.197 * getSMEFTCoeffEW("CHB") + 0.296 * getSMEFTCoeffEW("CHWB")
            + 0.126 * (getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl1R", 1, 1)) / 2.0 - 0.234 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) / 2.0
            - 0.101 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHeR", 1, 1)) / 2.0 + 0.181 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    // Tot
    dGHiTotR1 = (-0.001 * getSMEFTCoeffEW("CW") + 0.12 * getSMEFTCoeffEW("CHbox") - 0.030 * getSMEFTCoeffEW("CHD") + 1.362 * getSMEFTCoeffEW("CHG") - 0.048 * getSMEFTCoeffEW("CHW")
            - 0.049 * getSMEFTCoeffEW("CHB") + 0.046 * getSMEFTCoeffEW("CHWB") - 0.005 * getSMEFTCoeffEW("CeHR", 2, 2) - 0.012 * getSMEFTCoeffEW("CuHR", 2, 2) - 0.085 * getSMEFTCoeffEW("CdHR", 2, 2)
            + 0.051 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.002 * getSMEFTCoeffEW("CuWR", 2, 2) - 0.003 * getSMEFTCoeffEW("CuBR", 2, 2)
            - 0.150 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1) + getSMEFTCoeffEW("CHl3R", 2, 2)) / 3.0 + 0.013 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0
            + 0.079 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    Br += dGHiR1 - dGHiTotR1;
 
    if ((Br < 0) || (dGHiR1 < -1.0) || (dGHiTotR1 < -1.0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ STXS12_BrHbbRatio()

const double NPSMEFTd6General::STXS12_BrHbbRatio ( ) const

virtual

The STXS BR $ H \to bb $.

Reimplemented from NPbase.

Definition at line 40097 of file NPSMEFTd6General.cpp.

                                                       {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiTotR1 = 0.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
 
    // bb
    dGHiR1 = (0.12 * getSMEFTCoeffEW("CHbox") - 0.030 * getSMEFTCoeffEW("CHD") - 0.121 * getSMEFTCoeffEW("CdHR", 2, 2) - 0.121 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) / 2.0
            + 0.061 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    // Tot
    dGHiTotR1 = (-0.001 * getSMEFTCoeffEW("CW") + 0.12 * getSMEFTCoeffEW("CHbox") - 0.030 * getSMEFTCoeffEW("CHD") + 1.362 * getSMEFTCoeffEW("CHG") - 0.048 * getSMEFTCoeffEW("CHW")
            - 0.049 * getSMEFTCoeffEW("CHB") + 0.046 * getSMEFTCoeffEW("CHWB") - 0.005 * getSMEFTCoeffEW("CeHR", 2, 2) - 0.012 * getSMEFTCoeffEW("CuHR", 2, 2) - 0.085 * getSMEFTCoeffEW("CdHR", 2, 2)
            + 0.051 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.002 * getSMEFTCoeffEW("CuWR", 2, 2) - 0.003 * getSMEFTCoeffEW("CuBR", 2, 2)
            - 0.150 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1) + getSMEFTCoeffEW("CHl3R", 2, 2)) / 3.0 + 0.013 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0
            + 0.079 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    Br += dGHiR1 - dGHiTotR1;
 
    if ((Br < 0) || (dGHiR1 < -1.0) || (dGHiTotR1 < -1.0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ STXS12_BrHevmuvRatio()

const double NPSMEFTd6General::STXS12_BrHevmuvRatio ( ) const

virtual

The STXS BR $ H \to e\nu \mu\nu $.

Reimplemented from NPbase.

Definition at line 40049 of file NPSMEFTd6General.cpp.

                                                          {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiTotR1 = 0.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
 
    // e v mu v
    dGHiR1 = deltaGammaHevmuvRatio1();
 
    // Tot
    dGHiTotR1 = (-0.001 * getSMEFTCoeffEW("CW") + 0.12 * getSMEFTCoeffEW("CHbox") - 0.030 * getSMEFTCoeffEW("CHD") + 1.362 * getSMEFTCoeffEW("CHG") - 0.048 * getSMEFTCoeffEW("CHW")
            - 0.049 * getSMEFTCoeffEW("CHB") + 0.046 * getSMEFTCoeffEW("CHWB") - 0.005 * getSMEFTCoeffEW("CeHR", 2, 2) - 0.012 * getSMEFTCoeffEW("CuHR", 2, 2) - 0.085 * getSMEFTCoeffEW("CdHR", 2, 2)
            + 0.051 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.002 * getSMEFTCoeffEW("CuWR", 2, 2) - 0.003 * getSMEFTCoeffEW("CuBR", 2, 2)
            - 0.150 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1) + getSMEFTCoeffEW("CHl3R", 2, 2)) / 3.0 + 0.013 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0
            + 0.079 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    Br += dGHiR1 - dGHiTotR1;
 
    if ((Br < 0) || (dGHiR1 < -1.0) || (dGHiTotR1 < -1.0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ STXS12_BrHgagaRatio()

const double NPSMEFTd6General::STXS12_BrHgagaRatio ( ) const

virtual

The STXS BR $ H \to \gamma \gamma $.

Reimplemented from NPbase.

Definition at line 40072 of file NPSMEFTd6General.cpp.

                                                         {
    double Br = 1.0;
    double dGHiR1 = 0.0, dGHiTotR1 = 0.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    // gaga
    dGHiR1 = (-40.15 * getSMEFTCoeffEW("CHB") - 13.08 * getSMEFTCoeffEW("CHW") + 22.4 * getSMEFTCoeffEW("CHWB") - 0.9463 * getSMEFTCoeffEW("CW") + 0.12 * getSMEFTCoeffEW("CHbox")
            - 0.2417 * getSMEFTCoeffEW("CHD") + 0.03447 * getSMEFTCoeffEW("CuHR", 2, 2) - 1.151 * getSMEFTCoeffEW("CuWR", 2, 2) - 2.150 * getSMEFTCoeffEW("CuBR", 2, 2)
            - 0.3637 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) / 2.0 + 0.1819 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
    ;
 
    // Tot
    dGHiTotR1 = (-0.001 * getSMEFTCoeffEW("CW") + 0.12 * getSMEFTCoeffEW("CHbox") - 0.030 * getSMEFTCoeffEW("CHD") + 1.362 * getSMEFTCoeffEW("CHG") - 0.048 * getSMEFTCoeffEW("CHW")
            - 0.049 * getSMEFTCoeffEW("CHB") + 0.046 * getSMEFTCoeffEW("CHWB") - 0.005 * getSMEFTCoeffEW("CeHR", 2, 2) - 0.012 * getSMEFTCoeffEW("CuHR", 2, 2) - 0.085 * getSMEFTCoeffEW("CdHR", 2, 2)
            + 0.051 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.002 * getSMEFTCoeffEW("CuWR", 2, 2) - 0.003 * getSMEFTCoeffEW("CuBR", 2, 2)
            - 0.150 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1) + getSMEFTCoeffEW("CHl3R", 2, 2)) / 3.0 + 0.013 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0
            + 0.079 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    Br += dGHiR1 - dGHiTotR1;
 
    if ((Br < 0) || (dGHiR1 < -1.0) || (dGHiTotR1 < -1.0)) return std::numeric_limits<double>::quiet_NaN();
 
    return Br;
}

◆ STXS12_ggH_mjj0_350_pTH0_60_Nj1()

const double NPSMEFTd6General::STXS12_ggH_mjj0_350_pTH0_60_Nj1 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j \geq 1,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40497 of file NPSMEFTd6General.cpp.

{
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    double STXSb = 1.0;
    
    if (sqrt_s == 13.0) {
 
        
        
        STXSb += cWsch * (
                (0.) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH200_300()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_mjj0_350_pTH0_60_Nj2()

const double NPSMEFTd6General::STXS12_ggH_mjj0_350_pTH0_60_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j \geq 2,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40646 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        // To be fixed together with the UFO file when going beyond U(2)
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.033 * getSMEFTCoeffEW("CHD") + 46 * getSMEFTCoeffEW("CHG") - 0.128 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 1.63 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.132 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.065 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
        //AG:
        // Obtained with SMEFETatNLO. cuG_Warsaw = g3_tree*cuG_SMEFTatNLO
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.12117552334943638) * getSMEFTCoeffEW("CHbox")
                + (-0.03036231884057971) * getSMEFTCoeffEW("CHD")
                + (39.3) * getSMEFTCoeffEW("CHG") //To be updated
                + (-0.12262479871175523) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (1.0990338164251208) * getSMEFTCoeffEW("CuGR", 2, 2) * (-g3_tree)
                + (-0.060708534621578096) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.060708534621578096) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.06058776167471819) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_mjj0_350_pTH0_60_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_mjj0_350_pTH120_200_Nj2()

const double NPSMEFTd6General::STXS12_ggH_mjj0_350_pTH120_200_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j \geq 2,~m_{jj}[GeV]<350,~120<p_{TH} [GeV]<200$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40723 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        // To be fixed together with the UFO file when going beyond U(2)
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.032 * getSMEFTCoeffEW("CHD") + 46 * getSMEFTCoeffEW("CHG") - 0.132 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 1.48 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.130 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.066 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
        // AG: 
        // Obtained with SMEFETatNLO. cuG_Warsaw = g3_tree*cuG_SMEFTatNLO
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.121) * getSMEFTCoeffEW("CHbox")
                + (-0.0303) * getSMEFTCoeffEW("CHD")
                + (39.3) * getSMEFTCoeffEW("CHG") //To be updated
                + (-0.123) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (1.077) * getSMEFTCoeffEW("CuGR", 2, 2) * (-g3_tree)
                + (-0.061) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.061) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.061) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_mjj0_350_pTH120_200_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_mjj0_350_pTH60_120_Nj2()

const double NPSMEFTd6General::STXS12_ggH_mjj0_350_pTH60_120_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j \geq 2,~m_{jj}[GeV]<350,~60<p_{TH} [GeV]<120$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40684 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        // To be fixed together with the UFO file when going beyond U(2)
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.033 * getSMEFTCoeffEW("CHD") + 47 * getSMEFTCoeffEW("CHG") - 0.133 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 1.59 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.130 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.065 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
 
        //AG:
        // Obtained with SMEFETatNLO. cuG_Warsaw = g3_tree*cuG_SMEFTatNLO
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.121) * getSMEFTCoeffEW("CHbox")
                + (-0.0303) * getSMEFTCoeffEW("CHD")
                + (39.3) * getSMEFTCoeffEW("CHG") //To be updated
                + (-0.1224) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (1.093) * getSMEFTCoeffEW("CuGR", 2, 2) * (-g3_tree)
                + (-0.0606) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0606) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.061) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_mjj0_350_pTH60_120_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_mjj350_700_pTH0_200_Nj2()

const double NPSMEFTd6General::STXS12_ggH_mjj350_700_pTH0_200_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~<p_{TH} [GeV]<200$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40878 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        // Obtained with SMEFETatNLO. cuG_Warsaw = g3_tree*cuG_SMEFTatNLO
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.12121771217712178) * getSMEFTCoeffEW("CHbox")
                + (-0.030401291512915127) * getSMEFTCoeffEW("CHD")
                + (39.3) * getSMEFTCoeffEW("CHG") //To be updated
                + (-0.12283210332103321) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (0.992158671586716) * getSMEFTCoeffEW("CuGR", 2, 2) * (-g3_tree)
                + (-0.06079335793357934) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.06079335793357934) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.06060885608856089) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_mjj350_700_pTH0_200_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2()

const double NPSMEFTd6General::STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40761 of file NPSMEFTd6General.cpp.

                                                                                                     {
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.038 * getSMEFTCoeffEW("CHD") + 48 * getSMEFTCoeffEW("CHG") - 0.16 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 1.60 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.147 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.075 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2()

const double NPSMEFTd6General::STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40789 of file NPSMEFTd6General.cpp.

                                                                                                       {
    
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.033 * getSMEFTCoeffEW("CHD") + 42 * getSMEFTCoeffEW("CHG") - 0.131 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 1.43 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.124 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.064 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_mjj700_Inf_pTH0_200_Nj2()

const double NPSMEFTd6General::STXS12_ggH_mjj700_Inf_pTH0_200_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40911 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        // Obtained with SMEFETatNLO. cuG_Warsaw = g3_tree*cuG_SMEFTatNLO
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.12123629112662014) * getSMEFTCoeffEW("CHbox")
                + (-0.030348953140578262) * getSMEFTCoeffEW("CHD")
                + (39.3) * getSMEFTCoeffEW("CHG") //To be updated
                + (-0.12263210368893321) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (0.9950149551345963) * getSMEFTCoeffEW("CuGR", 2, 2) * (-g3_tree)
                + (-0.060697906281156525) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.060697906281156525) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.006083) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_mjj700_Inf_pTH0_200_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2()

const double NPSMEFTd6General::STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40819 of file NPSMEFTd6General.cpp.

                                                                                                     {
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.033 * getSMEFTCoeffEW("CHD") + 50 * getSMEFTCoeffEW("CHG") - 0.14 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 1.60 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.13 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.068 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2()

const double NPSMEFTd6General::STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40850 of file NPSMEFTd6General.cpp.

                                                                                                       {
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.030 * getSMEFTCoeffEW("CHD") + 44 * getSMEFTCoeffEW("CHG") - 0.13 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 1.4 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.13 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.061 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH0_10_Nj0()

const double NPSMEFTd6General::STXS12_ggH_pTH0_10_Nj0 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j=0,~p_{TH} [GeV]<10$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40222 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        // To be fixed together with the UFO file when going beyond U(2)
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0294 * getSMEFTCoeffEW("CHD") + 42.0 * getSMEFTCoeffEW("CHG") - 0.117 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 1.59 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.117 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.0587 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
        //AG: Obtained with SMEFETatNLO.
        // cuG_Warsaw = g3_tree*cuG_SMEFTatNLO
        STXSb += cWsch * (
                ((0.12127490039840637) * getSMEFTCoeffEW("CHbox")
                + (-0.030326693227091632) * getSMEFTCoeffEW("CHD")
                + (39.28731544) * getSMEFTCoeffEW("CHG")
                + (-0.12254980079681274) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (1.1274900398406373) * getSMEFTCoeffEW("CuGR", 2, 2) * (-g3_tree)
                + (-0.060669322709163344) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.060669322709163344) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.06064541832669322) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH0_10_Nj0()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH0_60_Nj1()

const double NPSMEFTd6General::STXS12_ggH_pTH0_60_Nj1 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j = 1,~p_{TH} [GeV]<60$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40531 of file NPSMEFTd6General.cpp.

{
 
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        // To be fixed together with the UFO file when going beyond U(2)
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0330 * getSMEFTCoeffEW("CHD") + 44.0 * getSMEFTCoeffEW("CHG") - 0.132 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 1.60 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.132 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.065 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
 
        //AG: 
        // Obtained with SMEFETatNLO. cuG_Warsaw = g3_tree*cuG_SMEFTatNLO
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.12123683316343867) * getSMEFTCoeffEW("CHbox")
                + (-0.030312606184165817) * getSMEFTCoeffEW("CHD")
                + (39.36687385) * getSMEFTCoeffEW("CHG")
                + (-0.12249405368671423) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (1.126741420319402) * getSMEFTCoeffEW("CuGR", 2, 2) * (-g3_tree)
                + (-0.060618416581719334) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.060618416581719334) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.060618416581719334) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH0_60_Nj1()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH10_200_Nj0()

const double NPSMEFTd6General::STXS12_ggH_pTH10_200_Nj0 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j=0,~p_{TH} [GeV]<10$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40262 of file NPSMEFTd6General.cpp.

{
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    double STXSb = 1.0;
    
    if (sqrt_s == 13.0) {
 
        
        
        STXSb += cWsch * (
                (0.) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH10_200_Nj0()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH10_Inf_Nj0()

const double NPSMEFTd6General::STXS12_ggH_pTH10_Inf_Nj0 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j=0,~10<p_{TH} [GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40469 of file NPSMEFTd6General.cpp.

                                                                                 {
 
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0295 * getSMEFTCoeffEW("CHD") + 42.2 * getSMEFTCoeffEW("CHG") - 0.1186 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 1.62 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.1182 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.0590 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH10_Inf_Nj0()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH120_200_Nj1()

const double NPSMEFTd6General::STXS12_ggH_pTH120_200_Nj1 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j = 1,~120<p_{TH} [GeV]<200$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40608 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        // To be fixed together with the UFO file when going beyond U(2)
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.028 * getSMEFTCoeffEW("CHD") + 44 * getSMEFTCoeffEW("CHG") - 0.118 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 1.60 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.112 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.058 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
        // AG: 
        // Obtained with SMEFETatNLO. cuG_Warsaw = g3_tree*cuG_SMEFTatNLO
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.12123076923076923) * getSMEFTCoeffEW("CHbox")
                + (-0.030307692307692306) * getSMEFTCoeffEW("CHD")
                + (40.11053009) * getSMEFTCoeffEW("CHG")
                + (-0.12248076923076923) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (1.115576923076923) * getSMEFTCoeffEW("CuGR", 2, 2) * (-g3_tree)
                + (-0.06061538461538461) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.06061538461538461) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.06061538461538461) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH120_200_Nj1()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH200_300()

const double NPSMEFTd6General::STXS12_ggH_pTH200_300 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $,200<~p_{TH} [GeV]<300$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40298 of file NPSMEFTd6General.cpp.

{
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    double STXSb = 1.0;
    
    if (sqrt_s == 13.0) {
 
        
        
        STXSb += cWsch * (
                (0.) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH200_300()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH200_300_Nj01()

const double NPSMEFTd6General::STXS12_ggH_pTH200_300_Nj01 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j\leq 1,~200<p_{TH} [GeV]<300$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40121 of file NPSMEFTd6General.cpp.

                                                                                   {
    // To be fixed together with the UFO file when going beyond U(2)
 
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.030 * getSMEFTCoeffEW("CHD") + 47 * getSMEFTCoeffEW("CHG") - 0.122 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 1.69 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.120 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.058 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH200_300_Nj01()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH300_450()

const double NPSMEFTd6General::STXS12_ggH_pTH300_450 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $,300<~p_{TH} [GeV]<450$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40332 of file NPSMEFTd6General.cpp.

{
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    double STXSb = 1.0;
    
    if (sqrt_s == 13.0) {
 
        
        
        STXSb += cWsch * (
                (0.) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH300_450()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH300_450_Nj01()

const double NPSMEFTd6General::STXS12_ggH_pTH300_450_Nj01 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j\leq 1,~300<p_{TH} [GeV]<450$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40146 of file NPSMEFTd6General.cpp.

                                                                                   {
 
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.029 * getSMEFTCoeffEW("CHD") + 60 * getSMEFTCoeffEW("CHG") - 0.12 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 2.1 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.11 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.055 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH300_450_Nj01()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH450_650()

const double NPSMEFTd6General::STXS12_ggH_pTH450_650 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $450<~p_{TH} [GeV]<650$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40400 of file NPSMEFTd6General.cpp.

{
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    double STXSb = 1.0;
    
    if (sqrt_s == 13.0) {
 
        
        
        STXSb += cWsch * (
                (0.) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH450_650()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH450_650_Nj01()

const double NPSMEFTd6General::STXS12_ggH_pTH450_650_Nj01 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j\leq 1,~450<p_{TH} [GeV]<650$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40171 of file NPSMEFTd6General.cpp.

                                                                                   {
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.030 * getSMEFTCoeffEW("CHD") + 70 * getSMEFTCoeffEW("CHG") - 0.14 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 2. * getSMEFTCoeffEW("CuGR", 2, 2) - 0.13 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.07 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH450_650_Nj01()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH450_Inf()

const double NPSMEFTd6General::STXS12_ggH_pTH450_Inf ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $,450<~p_{TH} [GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40366 of file NPSMEFTd6General.cpp.

{
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    double STXSb = 1.0;
    
    if (sqrt_s == 13.0) {
 
        
        
        STXSb += cWsch * (
                (0.) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH450_Inf()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH60_120_Nj1()

const double NPSMEFTd6General::STXS12_ggH_pTH60_120_Nj1 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j = 1,~60<p_{TH} [GeV]<120$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40570 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        // To be fixed together with the UFO file when going beyond U(2)
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0314 * getSMEFTCoeffEW("CHD") + 43.5 * getSMEFTCoeffEW("CHG") - 0.125 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 1.58 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.125 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.063 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
        //AG:
        // Obtained with SMEFETatNLO. cuG_Warsaw = g3_tree*cuG_SMEFTatNLO
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.12123503465658475) * getSMEFTCoeffEW("CHbox")
                + (-0.030315059861373662) * getSMEFTCoeffEW("CHD")
                + (39.68515459) * getSMEFTCoeffEW("CHG")
                + (-0.12249527410207939) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (1.119722747321991) * getSMEFTCoeffEW("CuGR", 2, 2) * (-g3_tree)
                + (-0.060636420919974794) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.060636420919974794) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.060636420919974794) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH60_120_Nj1()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH650_Inf()

const double NPSMEFTd6General::STXS12_ggH_pTH650_Inf ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $~p_{TH} [GeV]>650$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40434 of file NPSMEFTd6General.cpp.

{
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    double STXSb = 1.0;
    
    if (sqrt_s == 13.0) {
 
        
        
        STXSb += cWsch * (
                (0.) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH650_Inf()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggH_pTH650_Inf_Nj01()

const double NPSMEFTd6General::STXS12_ggH_pTH650_Inf_Nj01 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$, $N_j\leq 1,650<p_{TH} [GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40195 of file NPSMEFTd6General.cpp.

                                                                                   {
 
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.02 * getSMEFTCoeffEW("CHD") + 200 * getSMEFTCoeffEW("CHG") - 0.05 * getSMEFTCoeffEW("CuHR", 2, 2)
                - 10 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.07 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.06 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggH_pTH650_Inf_Nj01()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggHll_pTV0_75()

const double NPSMEFTd6General::STXS12_ggHll_pTV0_75 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H\ell\ell$, $p_{TV}[GeV]<75$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40944 of file NPSMEFTd6General.cpp.

                                                                             {
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0057 * getSMEFTCoeffEW("CHD") + 0.0090 * getSMEFTCoeffEW("CHWB")
                + 0.0454 * getSMEFTCoeffEW("CuHR", 2, 2) - 0.309 * getSMEFTCoeffEW("CuGR", 2, 2)
                - 0.0102 * 0.5 * (getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl1R", 1, 1) - getSMEFTCoeffEW("CHl3R", 0, 0) - getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.2932 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.0231 * 0.5 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHeR", 1, 1)) - 0.827 * CiHQ1
                - 0.289 * CiHQ3
                + 0.246 * CiHu + 0.296 * CiHd
                + 0.218 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggHll_pTV0_75()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggHll_pTV150_250_Nj0()

const double NPSMEFTd6General::STXS12_ggHll_pTV150_250_Nj0 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H\ell\ell$, $N_j = 0,~150<p_{TV}[GeV]<250$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41014 of file NPSMEFTd6General.cpp.

                                                                                    {
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") + 0.020 * getSMEFTCoeffEW("CHD") + 0.008 * getSMEFTCoeffEW("CHWB")
                + 0.100 * getSMEFTCoeffEW("CuHR", 2, 2) - 0.539 * getSMEFTCoeffEW("CuGR", 2, 2)
                - 0.0104 * 0.5 * (getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl1R", 1, 1) - getSMEFTCoeffEW("CHl3R", 0, 0) - getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.2974 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.0236 * 0.5 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHeR", 1, 1)) - 0.499 * CiHQ1
                - 0.199 * CiHQ3 + 0.105 * CiHu + 0.205 * CiHd
                + 0.223 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggHll_pTV150_250_Nj0()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggHll_pTV150_250_Nj1()

const double NPSMEFTd6General::STXS12_ggHll_pTV150_250_Nj1 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H\ell\ell$, $N_j = 1,~150<p_{TV}[GeV]<250$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41048 of file NPSMEFTd6General.cpp.

                                                                                    {
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") + 0.0142 * getSMEFTCoeffEW("CHD") + 0.0084 * getSMEFTCoeffEW("CHWB")
                + 0.0851 * getSMEFTCoeffEW("CuHR", 2, 2) - 0.491 * getSMEFTCoeffEW("CuGR", 2, 2)
                - 0.0103 * 0.5 * (getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl1R", 1, 1) - getSMEFTCoeffEW("CHl3R", 0, 0) - getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.2943 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.0233 * 0.5 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHeR", 1, 1)) - 0.552 * CiHQ1
                - 0.212 * CiHQ3 + 0.131 * CiHu + 0.219 * CiHd
                + 0.219 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggHll_pTV150_250_Nj1()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggHll_pTV250_Inf()

const double NPSMEFTd6General::STXS12_ggHll_pTV250_Inf ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H\ell\ell$, $250 < p_{TV}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41082 of file NPSMEFTd6General.cpp.

                                                                                {
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") + 0.050 * getSMEFTCoeffEW("CHD") + 0.0091 * getSMEFTCoeffEW("CHWB")
                + 0.163 * getSMEFTCoeffEW("CuHR", 2, 2) - 0.680 * getSMEFTCoeffEW("CuGR", 2, 2)
                - 0.0108 * 0.5 * (getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl1R", 1, 1) - getSMEFTCoeffEW("CHl3R", 0, 0) - getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.2968 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) - 0.0240 * 0.5 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHeR", 1, 1))
                - 0.352 * CiHQ1 - 0.171 * CiHQ3 + 0.020 * CiHu
                + 0.177 * CiHd + 0.221 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggHll_pTV250_Inf()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ggHll_pTV75_150()

const double NPSMEFTd6General::STXS12_ggHll_pTV75_150 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H\ell\ell$, $75<p_{TV}[GeV]<150$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40979 of file NPSMEFTd6General.cpp.

                                                                               {
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0015 * getSMEFTCoeffEW("CHD") + 0.0088 * getSMEFTCoeffEW("CHWB")
                + 0.0542 * getSMEFTCoeffEW("CuHR", 2, 2) - 0.387 * getSMEFTCoeffEW("CuGR", 2, 2)
                - 0.0103 * 0.5 * (getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl1R", 1, 1) - getSMEFTCoeffEW("CHl3R", 0, 0) - getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.2943 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.0235 * 0.5 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHeR", 1, 1)) - 0.698 * CiHQ1
                - 0.250 * CiHQ3
                + 0.199 * CiHu + 0.257 * CiHd
                + 0.220 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ggHll_pTV75_150()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHll_pTV0_150()

const double NPSMEFTd6General::STXS12_qqHll_pTV0_150 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\ell$, $0<p_{TV}<150[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42341 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += cWsch * (
                ((0.12123) * getSMEFTCoeffEW("CHbox")
                + (0.012881) * getSMEFTCoeffEW("CHD")
                + (0.70945) * getSMEFTCoeffEW("CHW")
                + (0.08197) * getSMEFTCoeffEW("CHB")
                + (0.31278) * getSMEFTCoeffEW("CHWB")
                + (-0.07723) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.10149) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (1.1939) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.20331) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.26871) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.021453) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.0973464) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.02656685) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.011957) * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.011952) * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.011971) * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.13992658) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.13999665) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.041673) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.01157) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.01147) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.011664) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.18184) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-1.158) * deltaGzd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            STXSb += 0.0;
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHll_pTV0_150()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHll_pTV0_75()

const double NPSMEFTd6General::STXS12_qqHll_pTV0_75 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\ell$, $p_{TV}[GeV]<75$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42051 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    /*double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") + 0.0129 * getSMEFTCoeffEW("CHD") + 0.665 * getSMEFTCoeffEW("CHW") + 0.0835 * getSMEFTCoeffEW("CHB")
                + 0.303 * getSMEFTCoeffEW("CHWB") - 0.0362 * 0.5 * (getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl1R", 1, 1) - getSMEFTCoeffEW("CHl3R", 0, 0) - getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.2772 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) - 0.0359 * 0.5 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHeR", 1, 1))
                + 0.029 * CiHQ1 + 1.27 * CiHQ3 + 0.245 * CiHu - 0.1064 * CiHd
                + 0.183 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
        // AG: 
        STXSb += cWsch * (
                ((0.12122) * getSMEFTCoeffEW("CHbox")
                + (0.01275) * getSMEFTCoeffEW("CHD")
                + (0.66498) * getSMEFTCoeffEW("CHW")
                + (0.07923) * getSMEFTCoeffEW("CHB")
                + (0.29801) * getSMEFTCoeffEW("CHWB")
                + (-0.05107) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.08713) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (0.9403) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.17685) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.20932) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.018933) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.0776056) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.0230333) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.011958) * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.011973) * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.011982) * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.1402374) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1403242) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.041685) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.0117029) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.0115373) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.0116341) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.18182) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-1.164) * deltaGzd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHll_pTV0_75()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHll_pTV150_250_Nj0()

const double NPSMEFTd6General::STXS12_qqHll_pTV150_250_Nj0 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\ell$, $N_j = 0,~150<p_{TV}[GeV]<250$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42170 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    /*double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") + 0.013 * getSMEFTCoeffEW("CHD") + 0.86 * getSMEFTCoeffEW("CHW") + 0.103 * getSMEFTCoeffEW("CHB")
                + 0.366 * getSMEFTCoeffEW("CHWB") - 0.035 * 0.5 * (getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl1R", 1, 1) - getSMEFTCoeffEW("CHl3R", 0, 0) - getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.267 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) - 0.0358 * 0.5 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHeR", 1, 1))
                - 0.12 * CiHQ1 + 3.63 * CiHQ3 + 0.87 * CiHu - 0.323 * CiHd
                + 0.177 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
        // AG: 
        STXSb += cWsch * (
                ((0.12131) * getSMEFTCoeffEW("CHbox")
                + (0.01327) * getSMEFTCoeffEW("CHD")
                + (0.9015) * getSMEFTCoeffEW("CHW")
                + (0.0923) * getSMEFTCoeffEW("CHB")
                + (0.37402) * getSMEFTCoeffEW("CHWB")
                + (-0.3625) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.20275) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (3.4124) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.38616) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.79679) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.038688) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.266298) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.05133963) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.011931) * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.011941) * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.011982) * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.14015811) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1400332) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.04169) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00795995) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.007957808) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.00793949) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.18198) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-1.17) * deltaGzd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHll_pTV150_250_Nj0()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHll_pTV150_250_Nj1()

const double NPSMEFTd6General::STXS12_qqHll_pTV150_250_Nj1 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\ell$, $N_j \geq 1,~150<p_{TV}[GeV]<250$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42230 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    /*double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") + 0.013 * getSMEFTCoeffEW("CHD") + 0.85 * getSMEFTCoeffEW("CHW") + 0.102 * getSMEFTCoeffEW("CHB")
                + 0.373 * getSMEFTCoeffEW("CHWB") - 0.036 * 0.5 * (getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl1R", 1, 1) - getSMEFTCoeffEW("CHl3R", 0, 0) - getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.266 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) - 0.0367 * 0.5 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHeR", 1, 1))
                - 0.10 * CiHQ1 + 3.19 * CiHQ3 + 0.77 * CiHu - 0.282 * CiHd
                + 0.177 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
        //AG: pTj=>30GeV
        STXSb += cWsch * (
                ((0.12186) * getSMEFTCoeffEW("CHbox")
                + (0.0117) * getSMEFTCoeffEW("CHD")
                + (0.8996) * getSMEFTCoeffEW("CHW")
                + (0.09276) * getSMEFTCoeffEW("CHB")
                + (0.37312) * getSMEFTCoeffEW("CHWB")
                + (-0.3902) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.16551) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (3.0189) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.38783) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.72034) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.047152) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.230024) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.048349) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.019699) * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.019614) * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.141473) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1415195) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.041872) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.008903) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.0089573) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.0089657) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.18278) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-1.113) * deltaGzd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHll_pTV150_250_Nj1()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHll_pTV250_400()

const double NPSMEFTd6General::STXS12_qqHll_pTV250_400 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\ell$, $250<p_{TV}<400[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42386 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += cWsch * (
                ((0.12128) * getSMEFTCoeffEW("CHbox")
                + (0.013624) * getSMEFTCoeffEW("CHD")
                + (0.9689) * getSMEFTCoeffEW("CHW")
                + (0.09471) * getSMEFTCoeffEW("CHB")
                + (0.395) * getSMEFTCoeffEW("CHWB")
                + (-1.023) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.32931) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (7.7452) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.61719) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (1.8529) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.060759) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.586475) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.0825726) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.011971) * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.011947) * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.01199) * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.1402367) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1402747) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.041712) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00793968) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.00794877) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.00792663) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.18192) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-1.173) * deltaGzd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            STXSb += 0.0;
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHll_pTV250_400()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHll_pTV250_Inf()

const double NPSMEFTd6General::STXS12_qqHll_pTV250_Inf ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\ell$, $250<p_{TV}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42289 of file NPSMEFTd6General.cpp.

                                                                                {
    
    double STXSb = (0.003784*STXS12_qqHll_pTV250_400(sqrt_s)+0.0007538*STXS12_qqHll_pTV400_Inf(sqrt_s))/(0.003784+0.0007538);
 
    /*
    // To be fixed together with the UFO file when going beyond U(2)
    double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") + 0.010 * getSMEFTCoeffEW("CHD") + 0.88 * getSMEFTCoeffEW("CHW") + 0.135 * getSMEFTCoeffEW("CHB")
                + 0.41 * getSMEFTCoeffEW("CHWB") - 0.037 * 0.5 * (getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl1R", 1, 1) - getSMEFTCoeffEW("CHl3R", 0, 0) - getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.271 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) - 0.036 * 0.5 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHeR", 1, 1))
                - 1.12 * CiHQ1 + 9.9 * CiHQ3 + 2.51 * CiHu - 0.81 * CiHd
                + 0.181 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHll_pTV250_Inf()");
 
    */
    
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
     
}

◆ STXS12_qqHll_pTV400_Inf()

const double NPSMEFTd6General::STXS12_qqHll_pTV400_Inf ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\ell$, $400<p_{TV}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42431 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += cWsch * (
                ((0.12137) * getSMEFTCoeffEW("CHbox")
                + (0.011638) * getSMEFTCoeffEW("CHD")
                + (1.0294) * getSMEFTCoeffEW("CHW")
                + (0.09718) * getSMEFTCoeffEW("CHB")
                + (0.41079) * getSMEFTCoeffEW("CHWB")
                + (-3.4338) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.54859) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (21.293) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (1.0603) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (5.2254) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.108) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-1.557636) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.1402551) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.021029) * getSMEFTCoeffEW("CHl1R", 0, 0)
                + (-0.021045) * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.021123) * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.14045) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1405169) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.041324) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.00540608) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.00540827) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (-0.0053773) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.18206) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-1.144) * deltaGzd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHll_pTV400_Inf()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHll_pTV75_150()

const double NPSMEFTd6General::STXS12_qqHll_pTV75_150 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\ell$, $75<p_{TV}[GeV]<150$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42111 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    /*double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") + 0.0128 * getSMEFTCoeffEW("CHD") + 0.771 * getSMEFTCoeffEW("CHW") + 0.092 * getSMEFTCoeffEW("CHB")
                + 0.341 * getSMEFTCoeffEW("CHWB") - 0.0360 * 0.5 * (getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl1R", 1, 1) - getSMEFTCoeffEW("CHl3R", 0, 0) - getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.274 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) - 0.0362 * 0.5 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHeR", 1, 1))
                + 0.01 * CiHQ1 + 1.80 * CiHQ3 + 0.403 * CiHu - 0.166 * CiHd
                + 0.182 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
        // AG: 
        STXSb += cWsch * (
                ((0.1071) * getSMEFTCoeffEW("CHbox")
                + (0.01084) * getSMEFTCoeffEW("CHD")
                + (0.7) * getSMEFTCoeffEW("CHW")
                + (0.07851) * getSMEFTCoeffEW("CHB")
                + (0.3063) * getSMEFTCoeffEW("CHWB")
                + (-0.093) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.113) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (1.53) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.2248) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.3302) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (0.02362) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (-0.1143) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (-0.0288097) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.011924) * getSMEFTCoeffEW("CHl1R", 1, 1)
                + (-0.011969) * getSMEFTCoeffEW("CHl1R", 2, 2)
                + (-0.1403624) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.14009461) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.041736) * getSMEFTCoeffEW("CHl3R", 2, 2)
                + (-0.0066) * getSMEFTCoeffEW("CHeR", 0, 0)
                + (-0.00815) * getSMEFTCoeffEW("CHeR", 1, 1)
                + (0) * getSMEFTCoeffEW("CHeR", 2, 2)
                + (0.18191) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-1.166) * deltaGzd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHll_pTV75_150()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHlv_pTV0_150()

const double NPSMEFTd6General::STXS12_qqHlv_pTV0_150 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\nu$, $0<p_{TV}<150[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41958 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += cWsch * (
                ((0.12122) * getSMEFTCoeffEW("CHbox")
                + (-0.03033245) * getSMEFTCoeffEW("CHD")
                + (0.86411) * getSMEFTCoeffEW("CHW")
                + (1.2279) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.18313) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.1411777) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1411553) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18183) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-1.002) * deltaGwd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHlv_pTV0_150)");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHlv_pTV0_75()

const double NPSMEFTd6General::STXS12_qqHlv_pTV0_75 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\nu$, $p_{TV}[GeV]<75$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41775 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    /*double CiHQ3; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0304 * getSMEFTCoeffEW("CHD") + 0.813 * getSMEFTCoeffEW("CHW")
                - 0.241 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 1.142 * CiHQ3 + 0.183 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0); */
        // AG:
        STXSb += cWsch * (
                ((0.12114) * getSMEFTCoeffEW("CHbox")
                + (-0.03031269) * getSMEFTCoeffEW("CHD")
                + (0.8155) * getSMEFTCoeffEW("CHW")
                + (0.9523) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.15907) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.1412857) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.14124287) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18176) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-1.012) * deltaGwd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHlv_pTV0_75()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHlv_pTV150_250_Nj0()

const double NPSMEFTd6General::STXS12_qqHlv_pTV150_250_Nj0 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\nu$, $N_j = 0,~150<p_{TV}[GeV]<250$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41855 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    /*double CiHQ3; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0312 * getSMEFTCoeffEW("CHD") + 1.06 * getSMEFTCoeffEW("CHW")
                - 0.247 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 4.07 * CiHQ3 + 0.187 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
        // AG: 
        STXSb += cWsch * (
                ((0.12103) * getSMEFTCoeffEW("CHbox")
                + (-0.03027479) * getSMEFTCoeffEW("CHD")
                + (1.0506) * getSMEFTCoeffEW("CHW")
                + (3.6846) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.34645) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.1403732) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1405017) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18154) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-1.017) * deltaGwd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHlv_pTV150_250_Nj0()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHlv_pTV150_250_Nj1()

const double NPSMEFTd6General::STXS12_qqHlv_pTV150_250_Nj1 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\nu$, $N_j \geq 1,~150<p_{TV}[GeV]<250$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41895 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    /*double CiHQ3; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0307 * getSMEFTCoeffEW("CHD") + 1.08 * getSMEFTCoeffEW("CHW")
                - 0.239 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 3.58 * CiHQ3 + 0.180 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
        // AG: pTj=>30GeV
        STXSb += cWsch * (
                ((0.12125) * getSMEFTCoeffEW("CHbox")
                + (-0.03035345) * getSMEFTCoeffEW("CHD")
                + (1.0561) * getSMEFTCoeffEW("CHW")
                + (3.2437) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.36816) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.1200448) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1201971) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18189) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-1.009) * deltaGwd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHlv_pTV150_250_Nj1()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHlv_pTV250_400()

const double NPSMEFTd6General::STXS12_qqHlv_pTV250_400 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\nu$, $250<p_{TV}<400[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41990 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += cWsch * (
                ((0.12126) * getSMEFTCoeffEW("CHbox")
                + (-0.03028419) * getSMEFTCoeffEW("CHD")
                + (1.1087) * getSMEFTCoeffEW("CHW")
                + (8.462) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.54273) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.1402818) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1402079) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18188) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-0.99) * deltaGwd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            STXSb += 0.0;
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHlv_pTV250_400()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHlv_pTV250_Inf()

const double NPSMEFTd6General::STXS12_qqHlv_pTV250_Inf ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\nu$, $250<p_{TV}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41935 of file NPSMEFTd6General.cpp.

                                                                                {
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
 
    if (sqrt_s == 13.0) {
 
        STXSb = (0.01127*STXS12_qqHlv_pTV250_400(sqrt_s) + 0.00339*STXS12_qqHlv_pTV400_Inf(sqrt_s))/(0.01127+0.00339);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHlv_pTV250_Inf()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHlv_pTV400_Inf()

const double NPSMEFTd6General::STXS12_qqHlv_pTV400_Inf ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\nu$, $400<p_{TV}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42020 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += cWsch * (
                ((0.1213) * getSMEFTCoeffEW("CHbox")
                + (-0.03031894) * getSMEFTCoeffEW("CHD")
                + (1.1361) * getSMEFTCoeffEW("CHW")
                + (25.302) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.9521) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.14003358) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.14005959) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18197) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-1.005) * deltaGwd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHlv_pTV400_Inf()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHlv_pTV75_150()

const double NPSMEFTd6General::STXS12_qqHlv_pTV75_150 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H\ell\nu$, $75<p_{TV}[GeV]<150$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41815 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    /*double CiHQ3; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0304 * getSMEFTCoeffEW("CHD") + 0.946 * getSMEFTCoeffEW("CHW")
                - 0.244 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 1.90 * CiHQ3 + 0.183 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
        // AG:
        STXSb += cWsch * (
                ((0.12127) * getSMEFTCoeffEW("CHbox")
                + (-0.03032518) * getSMEFTCoeffEW("CHD")
                + (0.9462) * getSMEFTCoeffEW("CHW")
                + (1.7004) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.22393) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.1410885) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1408925) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.1819) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                + (-0.996) * deltaGwd6()
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHlv_pTV75_150()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj0_60_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj0_60_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~m_{jj}[GeV]<60$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41212 of file NPSMEFTd6General.cpp.

                                                                                 {
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    
    
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    //double CiHQ1;    
    double CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    //CiHQ1 = (getSMEFTCoeffEW("CHq1R",0,0) + getSMEFTCoeffEW("CHq1R",1,1) + getSMEFTCoeffEW("CHq1R",2,2))/3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.011 * getSMEFTCoeffEW("CHD") + 0.38 * getSMEFTCoeffEW("CHW") + 0.012 * getSMEFTCoeffEW("CHB")
                + 0.060 * getSMEFTCoeffEW("CHWB") - 0.36 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.94 * CiHQ3 + 0.055 * CiHu - 0.022 * CiHd
                + 0.178 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj0_60_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~1000<m_{jj}[GeV]<1500,~p_{TH}[GeV]<200$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41615 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.12096) * getSMEFTCoeffEW("CHbox")
                + (-0.010795) * getSMEFTCoeffEW("CHD")
                + (-0.126544) * getSMEFTCoeffEW("CHW")
                + (-0.000155) * getSMEFTCoeffEW("CHB")
                + (0.020471) * getSMEFTCoeffEW("CHWB")
                + (0.013753) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0056663) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.334119) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0563833) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0222351) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00200624) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.0068001) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0018158) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.181549) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.181549) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18153) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~1000<m_{jj}[GeV],~p_{TH}[GeV]>200$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41735 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.12115277435803268) * getSMEFTCoeffEW("CHbox")
                + (-0.006700175570443445) * getSMEFTCoeffEW("CHD")
                + (0.14503609950278334) * getSMEFTCoeffEW("CHW")
                + (-0.001181392562850623) * getSMEFTCoeffEW("CHB")
                + (0.023797404695001557) * getSMEFTCoeffEW("CHWB")
                + (0.1267974703204301) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.020350888277334663) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-1.7030969805490792) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.2091291453108325) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.13908329182938856) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.008563055128991819) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.035275554702358033) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.007091459551226658) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.18157625796816287) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.18157625796816287) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18172255774352347) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj120_350_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj120_350_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~120<m_{jj}[GeV]<350$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41292 of file NPSMEFTd6General.cpp.

                                                                                    {
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0099 * getSMEFTCoeffEW("CHD") - 0.021 * getSMEFTCoeffEW("CHW") + 0.0017 * getSMEFTCoeffEW("CHB")
                + 0.0368 * getSMEFTCoeffEW("CHWB") - 0.363 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.003 * CiHQ1 - 0.155 * CiHQ3 - 0.0038 * CiHu
                + 0.0022 * CiHd + 0.181 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj120_350_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~1500<m_{jj}[GeV],~p_{TH}[GeV]<200$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41655 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.12137) * getSMEFTCoeffEW("CHbox")
                + (-0.010058) * getSMEFTCoeffEW("CHD")
                + (-0.126696) * getSMEFTCoeffEW("CHW")
                + (-4.9e-05) * getSMEFTCoeffEW("CHB")
                + (0.021522) * getSMEFTCoeffEW("CHWB")
                + (0.023913) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0034782) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.346713) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0398273) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.02563591) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.001467832) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.0064338) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0012111) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.181736) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.181736) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18193) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV]<1000,~p_{TH}[GeV]>200$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41695 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.12119388244615271) * getSMEFTCoeffEW("CHbox")
                + (-0.007520073014376603) * getSMEFTCoeffEW("CHD")
                + (0.20031065061792538) * getSMEFTCoeffEW("CHW")
                + (-0.0017028701729685037) * getSMEFTCoeffEW("CHB")
                + (0.025477338005929776) * getSMEFTCoeffEW("CHWB")
                + (0.05762202703511021) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.034704492909866734) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-1.5262530035586555) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.31670221602330967) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.11035352246217908) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.012911611060134444) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.03570087989045835) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.01138089675090921) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.1816546926779029) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1816546926779029) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18178862464555604) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj350_700_pTH0_200_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj350_700_pTH0_200_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41535 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.12116) * getSMEFTCoeffEW("CHbox")
                + (-0.011205) * getSMEFTCoeffEW("CHD")
                + (-0.133485) * getSMEFTCoeffEW("CHW")
                + (-0.000416) * getSMEFTCoeffEW("CHB")
                + (0.02047) * getSMEFTCoeffEW("CHWB")
                + (0.006534) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0081187) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.312986) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0850237) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.019281554) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.00320807) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.0068702) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0027355) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.1818408) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1818408) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18165) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj350_700_pTH0_200_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41386 of file NPSMEFTd6General.cpp.

                                                                                                       {
    
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    //double CiHQ1;
    double CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    //CiHQ1 = (getSMEFTCoeffEW("CHq1R",0,0) + getSMEFTCoeffEW("CHq1R",1,1) + getSMEFTCoeffEW("CHq1R",2,2))/3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0110 * getSMEFTCoeffEW("CHD") - 0.134 * getSMEFTCoeffEW("CHW") - 0.0014 * getSMEFTCoeffEW("CHB")
                + 0.0234 * getSMEFTCoeffEW("CHWB") - 0.368 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                - 0.371 * CiHQ3 - 0.0203 * CiHu
                + 0.0084 * CiHd + 0.184 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41424 of file NPSMEFTd6General.cpp.

                                                                                                         {
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    
    
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0101 * getSMEFTCoeffEW("CHD") - 0.143 * getSMEFTCoeffEW("CHW") + 0.027 * getSMEFTCoeffEW("CHWB")
                - 0.358 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) + 0.002 * CiHQ1
                - 0.38 * CiHQ3 - 0.0204 * CiHu + 0.0081 * CiHd
                + 0.183 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV],~200<p_{TH}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41327 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    /*double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0072 * getSMEFTCoeffEW("CHD") + 0.188 * getSMEFTCoeffEW("CHW") - 0.0012 * getSMEFTCoeffEW("CHB")
                + 0.038 * getSMEFTCoeffEW("CHWB") - 0.362 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.047 * CiHQ1 - 1.33 * CiHQ3 - 0.095 * CiHu
                + 0.0314 * CiHd + 0.181 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);*/
 
        //AG: pTj>30GeV
        STXSb += cWsch * (
                ((0.12125) * getSMEFTCoeffEW("CHbox")
                + (-0.007062) * getSMEFTCoeffEW("CHD")
                + (0.16946) * getSMEFTCoeffEW("CHW")
                + (-0.001466) * getSMEFTCoeffEW("CHB")
                + (0.024549) * getSMEFTCoeffEW("CHWB")
                + (0.09586) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.026874) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-1.622623) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.257163) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.1258851) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.01050939) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.035465) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0090063) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.181911) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.181911) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18186) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj60_120_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj60_120_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~60<m_{jj}[GeV]<120$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41250 of file NPSMEFTd6General.cpp.

                                                                                   {
    
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        
        STXSb += cWsch * ( 
    ( (0.12112) * getSMEFTCoeffEW("CHbox")
    + (-0.006618) * getSMEFTCoeffEW("CHD")
    + (0.7255) * getSMEFTCoeffEW("CHW")
    + (0.024324) * getSMEFTCoeffEW("CHB")
    + (0.10661) * getSMEFTCoeffEW("CHWB")
    + (-0.05202) * getSMEFTCoeffEW("CHq1R", 0,0)
    + (0.043564) * getSMEFTCoeffEW("CHq1R", 1,1)
    + (2.002) * getSMEFTCoeffEW("CHq3R", 0,0)
    + (0.26431) * getSMEFTCoeffEW("CHq3R", 1,1)
    + (0.14451) * getSMEFTCoeffEW("CHuR", 0,0)
    + (0.011187) * getSMEFTCoeffEW("CHuR", 1,1)
    + (-0.05057308) * getSMEFTCoeffEW("CHdR", 0,0)
    + (-0.01223433) * getSMEFTCoeffEW("CHdR", 1,1)
    + (-0.1806909) * getSMEFTCoeffEW("CHl3R", 0,0)
    + (-0.1806909) * getSMEFTCoeffEW("CHl3R", 1,1)
    + (0.1807) * getSMEFTCoeffEW("CllR", 0,1,1,0) ) * 1000000 
    + (-0.627) * deltaGwd6()
    + (-0.319) * deltaGzd6()
    );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj60_120_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~700<m_{jj}[GeV]<1000,~p_{TH}[GeV]<200$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41575 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        //pTj>30GeV
        STXSb += cWsch * (
                ((0.12117) * getSMEFTCoeffEW("CHbox")
                + (-0.011057) * getSMEFTCoeffEW("CHD")
                + (-0.128786) * getSMEFTCoeffEW("CHW")
                + (-0.00024) * getSMEFTCoeffEW("CHB")
                + (0.020319) * getSMEFTCoeffEW("CHWB")
                + (0.009981) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (-0.0068709) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.325754) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (-0.0692495) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (-0.0208126) * getSMEFTCoeffEW("CHuR", 0, 0)
                + (-0.002523013) * getSMEFTCoeffEW("CHuR", 1, 1)
                + (0.0068893) * getSMEFTCoeffEW("CHdR", 0, 0)
                + (0.0022378) * getSMEFTCoeffEW("CHdR", 1, 1)
                + (-0.1817542) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.1817542) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.18181) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41461 of file NPSMEFTd6General.cpp.

                                                                                                       {
    
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0101 * getSMEFTCoeffEW("CHD") - 0.117 * getSMEFTCoeffEW("CHW") - 0.0016 * getSMEFTCoeffEW("CHB")
                + 0.0231 * getSMEFTCoeffEW("CHWB") - 0.365 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.010 * CiHQ1 - 0.364 * CiHQ3 - 0.0216 * CiHu
                + 0.0074 * CiHd + 0.182 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2()

const double NPSMEFTd6General::STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41498 of file NPSMEFTd6General.cpp.

                                                                                                         {
    
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0096 * getSMEFTCoeffEW("CHD") - 0.168 * getSMEFTCoeffEW("CHW") + 0.023 * getSMEFTCoeffEW("CHWB")
                - 0.361 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) + 0.015 * CiHQ1
                - 0.442 * CiHQ3 - 0.0282 * CiHu + 0.0091 * CiHd
                + 0.180 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_Nj0()

const double NPSMEFTd6General::STXS12_qqHqq_Nj0 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j = 0$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41149 of file NPSMEFTd6General.cpp.

                                                                         {
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    //double CiHQ1;    
    double CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    //CiHQ1 = (getSMEFTCoeffEW("CHq1R",0,0) + getSMEFTCoeffEW("CHq1R",1,1) + getSMEFTCoeffEW("CHq1R",2,2))/3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.011 * getSMEFTCoeffEW("CHD") + 0.32 * getSMEFTCoeffEW("CHW") + 0.008 * getSMEFTCoeffEW("CHB")
                + 0.048 * getSMEFTCoeffEW("CHWB") - 0.36 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.46 * CiHQ3 + 0.027 * CiHu - 0.0125 * CiHd
                + 0.18 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_Nj0()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_Nj1()

const double NPSMEFTd6General::STXS12_qqHqq_Nj1 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j = 1$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41181 of file NPSMEFTd6General.cpp.

                                                                         {
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0111 * getSMEFTCoeffEW("CHD") + 0.187 * getSMEFTCoeffEW("CHW") + 0.0063 * getSMEFTCoeffEW("CHB")
                + 0.047 * getSMEFTCoeffEW("CHWB") - 0.368 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.003 * CiHQ1 + 0.39 * CiHQ3 + 0.0278 * CiHu
                - 0.0113 * CiHd + 0.183 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_Nj1()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_qqHqq_VH_veto_Nj01()

const double NPSMEFTd6General::STXS12_qqHqq_VH_veto_Nj01 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to Hqq$, $N_j = 0,1$ VH-veto Ref. 2402.05742.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 41117 of file NPSMEFTd6General.cpp.

{
    
    //NOT PROPERLY IMPLEMENTED, RETURNING A NaN
    return std::numeric_limits<double>::quiet_NaN();
    
    double STXSb = 1.0;
    
    if (sqrt_s == 13.0) {
 
        
        
        STXSb += cWsch * (
                (0.) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_qqHqq_VH_veto_Nj01()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_tH()

const double NPSMEFTd6General::STXS12_tH ( const double sqrt_s ) const

virtual

The STXS bin $pp \to tH$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 43002 of file NPSMEFTd6General.cpp.

{
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    /*double CiHQ3; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (0.12 * getSMEFTCoeffEW("CHbox") - 0.0272 * getSMEFTCoeffEW("CHD") + 0.254 * getSMEFTCoeffEW("CHG") + 0.1808 * getSMEFTCoeffEW("CHW")
                - 0.0764 * getSMEFTCoeffEW("CuHR", 2, 2) + 0.119 * getSMEFTCoeffEW("CuGR", 2, 2) + 0.170 * getSMEFTCoeffEW("CuWR", 2, 2)
                - 0.2679 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) + 0.319 * CiHQ3
                + 0.1341 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                //+ 0.418 * Ciqq3
                ) * (1000000.0);*/
 
        //AG:begin
        return mutH(13.0);
        //AG:end
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_tH()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ttH_pTH0_60()

const double NPSMEFTd6General::STXS12_ttH_pTH0_60 ( const double sqrt_s ) const

virtual

The STXS bin $pp \to ttH$, $p_{TH}[GeV]<60$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42477 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    /*double CiHQ3; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (-0.021 * getSMEFTCoeffEW("CG") + 0.12 * getSMEFTCoeffEW("CHbox") - 0.0301 * getSMEFTCoeffEW("CHD") + 0.411 * getSMEFTCoeffEW("CHG")
                - 0.121 * getSMEFTCoeffEW("CuHR", 2, 2) + 0.764 * getSMEFTCoeffEW("CuGR", 2, 2) + 0.004 * getSMEFTCoeffEW("CuWR", 2, 2)
                + 0.0015 * getSMEFTCoeffEW("CuBR", 2, 2) - 0.121 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.0031 * CiHQ3
                + 0.0612 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                //+ 0.0154 * Ciqq1 + 0.121 * Ciqq11 
                //+ 0.0142 * Ciqq3 + 0.299 * Ciqq31 
                //+ 0.0088 * Ciuu + 0.128 * Ciuu1 
                //- 0.0015 * Ciud1 + 0.0213 * Ciud8 
                //+ 0.0056 * Ciqu1 + 0.082 * Ciqu8 
                //- 0.001 * Ciqd1 + 0.0215 * Ciqd8
                ) * (1000000.0);*/
        // AG: 
        STXSb += cWsch * (
                ((0.12138) * getSMEFTCoeffEW("CHbox")
                + (-0.03041037) * getSMEFTCoeffEW("CHD")
                + (0.00057116) * getSMEFTCoeffEW("CHW")
                + (0.00014153) * getSMEFTCoeffEW("CHB")
                + (-0.000531127) * getSMEFTCoeffEW("CHWB")
                + (-9.889e-05) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (1.2627e-05) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.000339881) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.00038671) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (2.9689e-05) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.00033949) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.41274) * getSMEFTCoeffEW("CHG")
                + (-0.1225944) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (-0.776767) * getSMEFTCoeffEW("CuGR", 2, 2)
                + (0.00435) * getSMEFTCoeffEW("CG")
                + (-0.0047023) * getSMEFTCoeffEW("CuWR", 2, 2)
                + (-0.00153602) * getSMEFTCoeffEW("CuBR", 2, 2)
                + (0.007596) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                + (0.12404) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                + (-0.00063485) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                + (0.0041376) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                + (0.024355) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + (0.27065) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + (0.0016752) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                + (0.024707) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                + (0.008176) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                + (0.12146) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                + (0.00026666) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                + (0.0040529) * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                + (-0.001302936) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                + (-0.000180091) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                + (0.018975) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                + (0.0026805) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                + (0.0030841) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                + (0.0028183) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                + (-0.00011935) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                + (9.671e-05) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                + (0.048705) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                + (0.029737) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                + (0.0036627) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                + (0.0009909) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                + (-0.000901344) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                + (-0.000130598) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                + (0.018966) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                + (0.0026786) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                + (-0.0608986) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0608986) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.060896) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ttH_pTH0_60()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ttH_pTH120_200()

const double NPSMEFTd6General::STXS12_ttH_pTH120_200 ( const double sqrt_s ) const

virtual

The STXS bin $pp \to ttH$, $120<p_{TH}[GeV]<200$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42651 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    /*double CiHQ3; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (-0.152 * getSMEFTCoeffEW("CG") + 0.12 * getSMEFTCoeffEW("CHbox") - 0.0282 * getSMEFTCoeffEW("CHD") + 0.553 * getSMEFTCoeffEW("CHG")
                + 0.0013 * getSMEFTCoeffEW("CHW") - 0.113 * getSMEFTCoeffEW("CuHR", 2, 2) + 0.890 * getSMEFTCoeffEW("CuGR", 2, 2)
                + 0.007 * getSMEFTCoeffEW("CuWR", 2, 2) + 0.002 * getSMEFTCoeffEW("CuBR", 2, 2)
                - 0.114 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.0045 * CiHQ3 + 0.0569 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                //+ 0.0282 * Ciqq1 + 0.202 * Ciqq11 
                //+ 0.0275 * Ciqq3 + 0.493 * Ciqq31 
                //+ 0.0156 * Ciuu + 0.217 * Ciuu1 
                //- 0.0025 * Ciud1 + 0.0347 * Ciud8 
                //+ 0.0097 * Ciqu1 + 0.138 * Ciqu8 
                //- 0.0016 * Ciqd1 + 0.0345 * Ciqd8
                ) * (1000000.0);*/
        // AG: 
        STXSb += cWsch * (
                ((0.12143) * getSMEFTCoeffEW("CHbox")
                + (-0.030489) * getSMEFTCoeffEW("CHD")
                + (0.0011161) * getSMEFTCoeffEW("CHW")
                + (0.00027979) * getSMEFTCoeffEW("CHB")
                + (-0.00080248) * getSMEFTCoeffEW("CHWB")
                + (-0.0003474) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (6.353e-05) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.000517856) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0018597) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.00012826) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.00051778) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.59632) * getSMEFTCoeffEW("CHG")
                + (-0.1226997) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (-0.952237) * getSMEFTCoeffEW("CuGR", 2, 2)
                + (0.11918) * getSMEFTCoeffEW("CG")
                + (-0.00794352) * getSMEFTCoeffEW("CuWR", 2, 2)
                + (-0.00267574) * getSMEFTCoeffEW("CuBR", 2, 2)
                + (0.015284) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                + (0.2389) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                + (-0.0010437) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                + (0.0064995) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                + (0.048067) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + (0.51215) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + (0.0027253) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                + (0.038576) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                + (0.016124) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                + (0.23377) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                + (0.00042951) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                + (0.0063635) * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                + (-0.002501944) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                + (-0.00028836) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                + (0.035499) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                + (0.0041847) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                + (0.005906) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                + (0.0052058) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                + (-0.00015687) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                + (0.00014599) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                + (0.09268) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                + (0.057085) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                + (0.0057247) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                + (0.0015548) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                + (-0.00162258) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                + (-0.000196522) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                + (0.035455) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                + (0.0041763) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                + (-0.0610094) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0610094) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.060995) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ttH_pTH120_200()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ttH_pTH200_300()

const double NPSMEFTd6General::STXS12_ttH_pTH200_300 ( const double sqrt_s ) const

virtual

The STXS bin $pp \to ttH$, $200<p_{TH}[GeV]<300$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42739 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    /*double CiHQ1, CiHQ3; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (-0.311 * getSMEFTCoeffEW("CG") + 0.12 * getSMEFTCoeffEW("CHbox") - 0.0277 * getSMEFTCoeffEW("CHD") + 0.68 * getSMEFTCoeffEW("CHG")
                + 0.002 * getSMEFTCoeffEW("CHW") - 0.001 * getSMEFTCoeffEW("CHWB") - 0.112 * getSMEFTCoeffEW("CuHR", 2, 2)
                + 0.97 * getSMEFTCoeffEW("CuGR", 2, 2) + 0.0105 * getSMEFTCoeffEW("CuWR", 2, 2) + 0.003 * getSMEFTCoeffEW("CuBR", 2, 2)
                - 0.114 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) - 0.0015 * CiHQ1
                + 0.0091 * CiHQ3 + 0.0569 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                //+ 0.0493 * Ciqq1 + 0.336 * Ciqq11 
                //+ 0.0484 * Ciqq3 + 0.82 * Ciqq31 
                //+ 0.0268 * Ciuu + 0.358 * Ciuu1 
                //- 0.0042 * Ciud1 + 0.0545 * Ciud8 
                //+ 0.0159 * Ciqu1 + 0.228 * Ciqu8 
                //- 0.0025 * Ciqd1 + 0.0541 * Ciqd8
                ) * (1000000.0);*/
        // AG: 
        STXSb += cWsch * (
                ((0.1215) * getSMEFTCoeffEW("CHbox")
                + (-0.03053419) * getSMEFTCoeffEW("CHD")
                + (0.0017669) * getSMEFTCoeffEW("CHW")
                + (0.00044617) * getSMEFTCoeffEW("CHB")
                + (-0.001069327) * getSMEFTCoeffEW("CHWB")
                + (-0.0010712) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.00019776) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.000682555) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0063625) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.00038586) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0006827) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.699) * getSMEFTCoeffEW("CHG")
                + (-0.122786) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (-1.018646) * getSMEFTCoeffEW("CuGR", 2, 2)
                + (0.23561) * getSMEFTCoeffEW("CG")
                + (-0.01157907) * getSMEFTCoeffEW("CuWR", 2, 2)
                + (-0.00400075) * getSMEFTCoeffEW("CuBR", 2, 2)
                + (0.026362) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                + (0.39604) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                + (-0.0014893) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                + (0.009094) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                + (0.08184) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + (0.8361) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + (0.0039269) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                + (0.053073) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                + (0.027433) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                + (0.38713) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                + (0.00061782) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                + (0.008897) * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                + (-0.00415657) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                + (-0.000406717) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                + (0.057429) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                + (0.0057328) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                + (0.009662) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                + (0.008247) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                + (-0.00016591) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                + (0.00019516) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                + (0.15174) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                + (0.09449) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                + (0.007903) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                + (0.0021725) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                + (-0.002515173) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                + (-0.000258378) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                + (0.057392) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                + (0.0057293) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                + (-0.0611484) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0611484) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.061133) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ttH_pTH200_300()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ttH_pTH300_450()

const double NPSMEFTd6General::STXS12_ttH_pTH300_450 ( const double sqrt_s ) const

virtual

The STXS bin $pp \to ttH$, $300<p_{TH}[GeV]<450$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42869 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += cWsch * (
                ((0.12144) * getSMEFTCoeffEW("CHbox")
                + (-0.0304974) * getSMEFTCoeffEW("CHD")
                + (0.0026863) * getSMEFTCoeffEW("CHW")
                + (0.0006807) * getSMEFTCoeffEW("CHB")
                + (-0.001390866) * getSMEFTCoeffEW("CHWB")
                + (-0.003736) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (0.0005801) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.0008496083) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.022385) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (0.0011312) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.0008529) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.732) * getSMEFTCoeffEW("CHG")
                + (-0.1225144) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (-1.0107) * getSMEFTCoeffEW("CuGR", 2, 2)
                + (0.32789) * getSMEFTCoeffEW("CG")
                + (-0.01679391) * getSMEFTCoeffEW("CuWR", 2, 2)
                + (-0.00592538) * getSMEFTCoeffEW("CuBR", 2, 2)
                + (0.04717) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                + (0.67332) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                + (-0.002097) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                + (0.01284) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                + (0.14412) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + (1.3958) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + (0.005691) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                + (0.072025) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                + (0.048185) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                + (0.65757) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                + (0.0009062) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                + (0.012541) * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                + (-0.0071052) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                + (-0.000570256) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                + (0.09471) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                + (0.007746) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                + (0.015989) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                + (0.013192) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                + (-0.00012464) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                + (0.00025769) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                + (0.25508) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                + (0.16044) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                + (0.010784) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                + (0.003061) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                + (-0.003910363) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                + (-0.0003286955) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                + (0.09472) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                + (0.007745) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                + (-0.0612235) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0612235) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.061249) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ttH_pTH300_450()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ttH_pTH300_Inf()

const double NPSMEFTd6General::STXS12_ttH_pTH300_Inf ( const double sqrt_s ) const

virtual

The STXS bin $pp \to ttH$, $300<p_{TH}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42828 of file NPSMEFTd6General.cpp.

                                                                              {
    // VM: This is an old version of the function. IT'S NOT USED ANYMORE!!!
    // To be fixed together with the UFO file when going beyond U(2)
    double STXSb = 1.0;
 
    double CiHQ1, CiHQ3, CiHu, CiHd; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ1 = (getSMEFTCoeffEW("CHq1R", 0, 0) + getSMEFTCoeffEW("CHq1R", 1, 1) + getSMEFTCoeffEW("CHq1R", 2, 2)) / 3.0;
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;
    CiHu = (getSMEFTCoeffEW("CHuR", 0, 0) + getSMEFTCoeffEW("CHuR", 1, 1) + getSMEFTCoeffEW("CHuR", 2, 2)) / 3.0;
    CiHd = (getSMEFTCoeffEW("CHdR", 0, 0) + getSMEFTCoeffEW("CHdR", 1, 1) + getSMEFTCoeffEW("CHdR", 2, 2)) / 3.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += (-0.58 * getSMEFTCoeffEW("CG") + 0.12 * getSMEFTCoeffEW("CHbox") - 0.0276 * getSMEFTCoeffEW("CHD") + 0.84 * getSMEFTCoeffEW("CHG")
                + 0.003 * getSMEFTCoeffEW("CHW") - 0.001 * getSMEFTCoeffEW("CHWB") - 0.110 * getSMEFTCoeffEW("CuHR", 2, 2)
                + 1.04 * getSMEFTCoeffEW("CuGR", 2, 2) + 0.0186 * getSMEFTCoeffEW("CuWR", 2, 2) + 0.0068 * getSMEFTCoeffEW("CuBR", 2, 2)
                - 0.112 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1)) - 0.0105 * CiHQ1
                + 0.0503 * CiHQ3 + 0.0110 * CiHu - 0.0032 * CiHd
                + 0.056 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                //+ 0.120 * Ciqq1 + 0.75 * Ciqq11 
                //+ 0.122 * Ciqq3 + 1.70 * Ciqq31 
                //+ 0.064 * Ciuu + 0.78 * Ciuu1 
                //- 0.0091 * Ciud1 + 0.110 * Ciud8 
                //+ 0.0344 * Ciqu1 + 0.497 * Ciqu8 
                //- 0.0045 * Ciqd1 + 0.111 * Ciqd8
                ) * (1000000.0);
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ttH_pTH300_Inf()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ttH_pTH450_Inf()

const double NPSMEFTd6General::STXS12_ttH_pTH450_Inf ( const double sqrt_s ) const

virtual

The STXS bin $pp \to ttH$, $450<p_{TH}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42939 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    if (sqrt_s == 13.0) {
 
        STXSb += cWsch * (
                ((0.12111) * getSMEFTCoeffEW("CHbox")
                + (-0.030308) * getSMEFTCoeffEW("CHD")
                + (0.0044801) * getSMEFTCoeffEW("CHW")
                + (0.0011466) * getSMEFTCoeffEW("CHB")
                + (-0.00194247) * getSMEFTCoeffEW("CHWB")
                + (-0.1218236) * getSMEFTCoeffEW("CuHR", 2, 2)
                + (-1.07104) * getSMEFTCoeffEW("CuGR", 2, 2)
                + (0.33119) * getSMEFTCoeffEW("CG")
                + (-0.0285223) * getSMEFTCoeffEW("CuWR", 2, 2)
                + (-0.0104832) * getSMEFTCoeffEW("CuBR", 2, 2)
                + (0.11537) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                + (1.4881) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                + (-0.0030909) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                + (0.023079) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                + (0.33421) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + (2.9818) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + (0.010023) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                + (0.11364) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                + (0.11257) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                + (1.4506) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                + (0.0017341) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                + (0.022496) * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                + (-0.015613057) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                + (-0.000929212) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                + (0.19582) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                + (0.01189) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                + (0.033516) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                + (0.026074) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                + (0.000103) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                + (0.00040951) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                + (0.54906) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                + (0.3534) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                + (0.017338) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                + (0.0054804) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                + (-0.00728397) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                + (-0.000451772) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                + (0.19585) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                + (0.011884) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                + (-0.0613195) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0613195) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.06135) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ttH_pTH450_Inf()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS12_ttH_pTH60_120()

const double NPSMEFTd6General::STXS12_ttH_pTH60_120 ( const double sqrt_s ) const

virtual

The STXS bin $pp \to ttH$, $60<p_{TH}[GeV]<120$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 42565 of file NPSMEFTd6General.cpp.

{
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    /*double CiHQ3; // Cannot resolve fam. dependence -> assume universality for quarks. 
    CiHQ3 = (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1) + getSMEFTCoeffEW("CHq3R", 2, 2)) / 3.0;*/
 
    if (sqrt_s == 13.0) {
 
        /*STXSb += (-0.061 * getSMEFTCoeffEW("CG") + 0.12 * getSMEFTCoeffEW("CHbox") - 0.0286 * getSMEFTCoeffEW("CHD") + 0.450 * getSMEFTCoeffEW("CHG")
                - 0.1149 * getSMEFTCoeffEW("CuHR", 2, 2) + 0.790 * getSMEFTCoeffEW("CuGR", 2, 2) + 0.005 * getSMEFTCoeffEW("CuWR", 2, 2)
                + 0.0017 * getSMEFTCoeffEW("CuBR", 2, 2) - 0.1151 * 0.5 * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1))
                + 0.0032 * CiHQ3
                + 0.0574 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)
                //+ 0.0183 * Ciqq1 + 0.138 * Ciqq11 
                //+ 0.0175 * Ciqq3 + 0.340 * Ciqq31 
                //+ 0.0104 * Ciuu + 0.147 * Ciuu1 
                //- 0.0017 * Ciud1 + 0.0244 * Ciud8 
                //+ 0.0066 * Ciqu1 + 0.0968 * Ciqu8 
                //- 0.001 * Ciqd1 + 0.0243 * Ciqd8
                ) * (1000000.0);*/
        // AG: 
        STXSb += cWsch * (
                ((0.12137) * getSMEFTCoeffEW("CHbox")
                + (-0.03041016) * getSMEFTCoeffEW("CHD")
                + (0.00073702) * getSMEFTCoeffEW("CHW")
                + (0.00018385) * getSMEFTCoeffEW("CHB")
                + (-0.000620406) * getSMEFTCoeffEW("CHWB")
                + (-0.00015089) * getSMEFTCoeffEW("CHq1R", 0, 0)
                + (2.3128e-05) * getSMEFTCoeffEW("CHq1R", 1, 1)
                + (-0.000399286) * getSMEFTCoeffEW("CHq1R", 2, 2)
                + (0.0006773) * getSMEFTCoeffEW("CHq3R", 0, 0)
                + (5.0356e-05) * getSMEFTCoeffEW("CHq3R", 1, 1)
                + (0.00039923) * getSMEFTCoeffEW("CHq3R", 2, 2)
                + (0.48136) * getSMEFTCoeffEW("CHG")
                + (0.03963) * getSMEFTCoeffEW("CG")
                + (-0.00571315) * getSMEFTCoeffEW("CuWR", 2, 2)
                + (-0.00189) * getSMEFTCoeffEW("CuBR", 2, 2)
                + (0.009791) * getSMEFTCoeffEW("Cqq1R", 0, 0, 2, 2)
                + (0.15791) * getSMEFTCoeffEW("Cqq1R", 0, 2, 2, 0)
                + (-0.00076589) * getSMEFTCoeffEW("Cqq1R", 1, 1, 2, 2)
                + (0.0048919) * getSMEFTCoeffEW("Cqq1R", 1, 2, 2, 1)
                + (0.031236) * getSMEFTCoeffEW("Cqq3R", 0, 0, 2, 2)
                + (0.34185) * getSMEFTCoeffEW("Cqq3R", 0, 2, 2, 0)
                + (0.0020056) * getSMEFTCoeffEW("Cqq3R", 1, 1, 2, 2)
                + (0.029204) * getSMEFTCoeffEW("Cqq3R", 1, 2, 2, 1)
                + (0.010484) * getSMEFTCoeffEW("CuuR", 0, 0, 2, 2)
                + (0.15461) * getSMEFTCoeffEW("CuuR", 0, 2, 2, 0)
                + (0.00031756) * getSMEFTCoeffEW("CuuR", 1, 1, 2, 2)
                + (0.0047899) * getSMEFTCoeffEW("CuuR", 1, 2, 2, 1)
                + (-0.001652491) * getSMEFTCoeffEW("Cud1R", 2, 2, 0, 0)
                + (-0.0002149805) * getSMEFTCoeffEW("Cud1R", 2, 2, 1, 1)
                + (0.023897) * getSMEFTCoeffEW("Cud8R", 2, 2, 0, 0)
                + (0.0031647) * getSMEFTCoeffEW("Cud8R", 2, 2, 1, 1)
                + (0.0039242) * getSMEFTCoeffEW("Cqu1R", 0, 0, 2, 2)
                + (0.0035367) * getSMEFTCoeffEW("Cqu1R", 2, 2, 0, 0)
                + (-0.0001347) * getSMEFTCoeffEW("Cqu1R", 1, 1, 2, 2)
                + (0.00011278) * getSMEFTCoeffEW("Cqu1R", 2, 2, 1, 1)
                + (0.061685) * getSMEFTCoeffEW("Cqu8R", 0, 0, 2, 2)
                + (0.037794) * getSMEFTCoeffEW("Cqu8R", 2, 2, 0, 0)
                + (0.0043275) * getSMEFTCoeffEW("Cqu8R", 1, 1, 2, 2)
                + (0.0011707) * getSMEFTCoeffEW("Cqu8R", 2, 2, 1, 1)
                + (-0.00112222) * getSMEFTCoeffEW("Cqd1R", 2, 2, 0, 0)
                + (-0.000152545) * getSMEFTCoeffEW("Cqd1R", 2, 2, 1, 1)
                + (0.023878) * getSMEFTCoeffEW("Cqd8R", 2, 2, 0, 0)
                + (0.0031642) * getSMEFTCoeffEW("Cqd8R", 2, 2, 1, 1)
                + (-0.0608954) * getSMEFTCoeffEW("CHl3R", 0, 0)
                + (-0.0608954) * getSMEFTCoeffEW("CHl3R", 1, 1)
                + (0.060897) * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * 1000000
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
 
            STXSb += 0.0;
 
        }
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::STXS12_ttH_pTH60_120()");
 
    if (STXSb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return STXSb;
}

◆ STXS_ggH0j()

const double NPSMEFTd6General::STXS_ggH0j ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39489 of file NPSMEFTd6General.cpp.

                                                                   {
 
    // Warsaw parameterization
    // (HEL parameterization commented out)
 
    double STXSb = 1.0;
 
    //    STXSb = 1.0 + 55.2*aiG + 0.362*ai3G + 0.276*ai2G;
 
    STXSb += (35.0 * getSMEFTCoeffEW("CHG")) * (1000000.0);
 
    return STXSb;
}

◆ STXS_ggH1j_pTH_0_60()

const double NPSMEFTd6General::STXS_ggH1j_pTH_0_60 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39503 of file NPSMEFTd6General.cpp.

                                                                            {
 
    // Warsaw parameterization
    // (HEL parameterization commented out)
 
    double STXSb = 1.0;
 
    //    STXSb = 1.0 + 56.0*aiG + 1.52*ai3G + 1.19*ai2G;
 
    STXSb += (28.3 * getSMEFTCoeffEW("CHG")) * (1000000.0);
 
    return STXSb;
}

◆ STXS_ggH1j_pTH_120_200()

const double NPSMEFTd6General::STXS_ggH1j_pTH_120_200 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39531 of file NPSMEFTd6General.cpp.

                                                                               {
 
    // Warsaw parameterization
    // (HEL parameterization commented out)
 
    double STXSb = 1.0;
 
    //    STXSb = 1.0 + 56.5*aiG + 17.8*ai3G + 11.2*ai2G;
 
    STXSb += (23.1 * getSMEFTCoeffEW("CHG")) * (1000000.0);
 
    return STXSb;
}

◆ STXS_ggH1j_pTH_200()

const double NPSMEFTd6General::STXS_ggH1j_pTH_200 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39545 of file NPSMEFTd6General.cpp.

                                                                           {
 
    // Warsaw parameterization
    // (HEL parameterization commented out)
 
    double STXSb = 1.0;
 
    //    STXSb = 1.0 + 55.0*aiG + 52.0*ai3G + 34.0*ai2G;
 
    STXSb += (15.6 * getSMEFTCoeffEW("CHG")) * (1000000.0);
 
    return STXSb;
}

◆ STXS_ggH1j_pTH_60_120()

const double NPSMEFTd6General::STXS_ggH1j_pTH_60_120 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39517 of file NPSMEFTd6General.cpp.

                                                                              {
 
    // Warsaw parameterization
    // (HEL parameterization commented out)
 
    double STXSb = 1.0;
 
    //    STXSb = 1.0 + 55.5*aiG + 4.12*ai3G + 2.76*ai2G;
 
    STXSb += (26.1 * getSMEFTCoeffEW("CHG")) * (1000000.0);
 
    return STXSb;
}

◆ STXS_ggH2j_pTH_0_200()

const double NPSMEFTd6General::STXS_ggH2j_pTH_0_200 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39559 of file NPSMEFTd6General.cpp.

                                                                             {
 
    // Warsaw parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 + 16.0 * getSMEFTCoeffEW("CHG");
 
    return STXSb;
}

◆ STXS_ggH2j_pTH_0_60()

const double NPSMEFTd6General::STXS_ggH2j_pTH_0_60 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39570 of file NPSMEFTd6General.cpp.

                                                                            {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 + 55.6 * aiG + 3.66 * ai3G + 4.23 * ai2G;
 
    return STXSb;
}

◆ STXS_ggH2j_pTH_120_200()

const double NPSMEFTd6General::STXS_ggH2j_pTH_120_200 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39592 of file NPSMEFTd6General.cpp.

                                                                               {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 + 55.8 * aiG + 23.0 * ai3G + 17.5 * ai2G;
 
    return STXSb;
}

◆ STXS_ggH2j_pTH_200()

const double NPSMEFTd6General::STXS_ggH2j_pTH_200 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39603 of file NPSMEFTd6General.cpp.

                                                                           {
 
    // Warsaw parameterization
    // (HEL parameterization commented out)
 
    double STXSb = 1.0;
 
    //    STXSb = 1.0 + 56.0*aiG + 89.8*ai3G + 68.1*ai2G;
 
    STXSb += (15.6 * getSMEFTCoeffEW("CHG")) * (1000000.0);
 
    return STXSb;
}

◆ STXS_ggH2j_pTH_60_120()

const double NPSMEFTd6General::STXS_ggH2j_pTH_60_120 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39581 of file NPSMEFTd6General.cpp.

                                                                              {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 + 56.1 * aiG + 7.73 * ai3G + 6.81 * ai2G;
 
    return STXSb;
}

◆ STXS_ggH_VBFtopo_j3()

const double NPSMEFTd6General::STXS_ggH_VBFtopo_j3 ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39478 of file NPSMEFTd6General.cpp.

                                                                            {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 + 55.9 * aiG + 9.04 * ai3G + 8.1 * ai2G;
 
    return STXSb;
}

◆ STXS_ggH_VBFtopo_j3v()

const double NPSMEFTd6General::STXS_ggH_VBFtopo_j3v ( const double sqrt_s ) const

virtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39467 of file NPSMEFTd6General.cpp.

                                                                             {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 + 56.6 * aiG + 5.5 * ai3G + 4.36 * ai2G;
 
    return STXSb;
}

◆ STXS_qqHll_pTV_0_150()

const double NPSMEFTd6General::STXS_qqHll_pTV_0_150 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H \ell \ell$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39783 of file NPSMEFTd6General.cpp.

                                                                             {
 
    // Warsaw parameterization
    // (HEL parameterization commented out)
 
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    double CiHL1 = getSMEFTCoeffEW("CHl1R", 0, 0), CiHL3 = getSMEFTCoeffEW("CHl3R", 0, 0), CiHe = getSMEFTCoeffEW("CHeR", 0, 0);
    double CiHQ1 = getSMEFTCoeffEW("CHq1R", 0, 0), CiHQ3 = getSMEFTCoeffEW("CHq3R", 0, 0), CiHu = getSMEFTCoeffEW("CHuR", 0, 0), CiHd = getSMEFTCoeffEW("CHdR", 0, 0);
 
    //    STXSb = 1.0 - 1.0*aiH - 4.001*aiT + 29.82*aiWW + 8.43*aiB + 8.5*aiHW 
    //            + 2.545*aiHB + 0.0315*aiA - 1.89*aiHQ + 22.84*aipHQ + 5.247*aiHu 
    //            - 2.0*aiHd - 0.963*aiHL + 2.042*aipHL - 0.2307*aiHe;
 
    STXSb += (0.1218 * getSMEFTCoeffEW("CHbox") + 0.0259 * getSMEFTCoeffEW("CHD") + 0.696 * getSMEFTCoeffEW("CHW") + 0.0846 * getSMEFTCoeffEW("CHB")
            + 0.328 * getSMEFTCoeffEW("CHWB") + 0.1332 * CiHL1 - 0.231 * CiHL3 - 0.1076 * CiHe
            + 0.016 * CiHQ1 + 1.409 * CiHQ3 + 0.315 * CiHu - 0.1294 * CiHd
            + 0.182 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    return STXSb;
}

◆ STXS_qqHll_pTV_150_250()

const double NPSMEFTd6General::STXS_qqHll_pTV_150_250 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H \ell \ell$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39806 of file NPSMEFTd6General.cpp.

                                                                               {
 
    // Warsaw parameterization
 
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    double CiHL1 = getSMEFTCoeffEW("CHl1R", 0, 0), CiHL3 = getSMEFTCoeffEW("CHl3R", 0, 0), CiHe = getSMEFTCoeffEW("CHeR", 0, 0);
    double CiHQ1 = getSMEFTCoeffEW("CHq1R", 0, 0), CiHQ3 = getSMEFTCoeffEW("CHq3R", 0, 0), CiHu = getSMEFTCoeffEW("CHuR", 0, 0), CiHd = getSMEFTCoeffEW("CHdR", 0, 0);
 
 
    STXSb += (0.124 * getSMEFTCoeffEW("CHbox") + 0.026 * getSMEFTCoeffEW("CHD") + 0.85 * getSMEFTCoeffEW("CHW") + 0.102 * getSMEFTCoeffEW("CHB")
            + 0.389 * getSMEFTCoeffEW("CHWB") + 0.134 * CiHL1 - 0.232 * CiHL3 - 0.109 * CiHe
            - 0.16 * CiHQ1 + 3.56 * CiHQ3 + 0.85 * CiHu - 0.315 * CiHd
            + 0.184 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    return STXSb;
}

◆ STXS_qqHll_pTV_150_250_0j()

const double NPSMEFTd6General::STXS_qqHll_pTV_150_250_0j ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H \ell \ell$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39825 of file NPSMEFTd6General.cpp.

                                                                                  {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 0.993 * aiH - 4.0 * aiT + 62.4 * aiWW + 18.08 * aiB + 37.6 * aiHW
            + 11.22 * aiHB - 5.03 * aiHQ + 61.0 * aipHQ + 14.39 * aiHu - 5.17 * aiHd
            - 0.977 * aiHL + 2.08 * aipHL - 0.234 * aiHe;
 
    return STXSb;
}

◆ STXS_qqHll_pTV_150_250_1j()

const double NPSMEFTd6General::STXS_qqHll_pTV_150_250_1j ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H \ell \ell$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39838 of file NPSMEFTd6General.cpp.

                                                                                  {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 1.002 * aiH - 4.01 * aiT + 57.9 * aiWW + 16.78 * aiB + 32.8 * aiHW
            + 9.86 * aiHB - 4.58 * aiHQ + 55.6 * aipHQ + 13.54 * aiHu - 4.56 * aiHd
            - 0.989 * aiHL + 2.09 * aipHL - 0.235 * aiHe;
 
    return STXSb;
}

◆ STXS_qqHll_pTV_250()

const double NPSMEFTd6General::STXS_qqHll_pTV_250 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H \ell \ell$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39851 of file NPSMEFTd6General.cpp.

                                                                           {
 
    // Warsaw parameterization
    // (HEL parameterization commented out)
 
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    double CiHL1 = getSMEFTCoeffEW("CHl1R", 0, 0), CiHL3 = getSMEFTCoeffEW("CHl3R", 0, 0), CiHe = getSMEFTCoeffEW("CHeR", 0, 0);
    double CiHQ1 = getSMEFTCoeffEW("CHq1R", 0, 0), CiHQ3 = getSMEFTCoeffEW("CHq3R", 0, 0), CiHu = getSMEFTCoeffEW("CHuR", 0, 0), CiHd = getSMEFTCoeffEW("CHdR", 0, 0);
 
    //    STXSb = 1.0 - 0.998*aiH - 4.0*aiT + 153.1*aiWW + 45.6*aiB + 126.4*aiHW 
    //            + 37.9*aiHB - 13.85*aiHQ + 168.6*aipHQ + 41.7*aiHu - 13.48*aiHd 
    //            - 0.977*aiHL + 2.09*aipHL - 0.238*aiHe;
 
    STXSb += (0.122 * getSMEFTCoeffEW("CHbox") + 0.028 * getSMEFTCoeffEW("CHD") + 0.88 * getSMEFTCoeffEW("CHW") + 0.121 * getSMEFTCoeffEW("CHB")
            + 0.43 * getSMEFTCoeffEW("CHWB") + 0.137 * CiHL1 - 0.234 * CiHL3 - 0.113 * CiHe
            - 0.82 * CiHQ1 + 8.5 * CiHQ3 + 2.14 * CiHu - 0.71 * CiHd
            + 0.182 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    return STXSb;
}

◆ STXS_qqHlv_pTV_0_150()

const double NPSMEFTd6General::STXS_qqHlv_pTV_0_150 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H \ell \nu$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39731 of file NPSMEFTd6General.cpp.

                                                                             {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 1.001 * aiH + 33.63 * aiWW + 11.49 * aiHW + 23.62 * aipHQ + 2.013 * aipHL;
 
    return STXSb;
}

◆ STXS_qqHlv_pTV_0_250()

const double NPSMEFTd6General::STXS_qqHlv_pTV_0_250 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H \ell \nu$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39715 of file NPSMEFTd6General.cpp.

                                                                             {
 
    // Warsaw parameterization
 
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    double CiHL3 = getSMEFTCoeffEW("CHl3R", 0, 0);
    double CiHQ3 = getSMEFTCoeffEW("CHq3R", 0, 0);
 
    STXSb += (0.1212 * getSMEFTCoeffEW("CHbox") - 0.0304 * getSMEFTCoeffEW("CHD") + 0.874 * getSMEFTCoeffEW("CHW")
            - 0.242 * CiHL3 + 1.710 * CiHQ3 + 0.182 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    return STXSb;
}

◆ STXS_qqHlv_pTV_150_250_0j()

const double NPSMEFTd6General::STXS_qqHlv_pTV_150_250_0j ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H \ell \nu$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39742 of file NPSMEFTd6General.cpp.

                                                                                  {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 0.998 * aiH + 76.3 * aiWW + 50.7 * aiHW + 66.5 * aipHQ + 2.03 * aipHL;
 
    return STXSb;
}

◆ STXS_qqHlv_pTV_150_250_1j()

const double NPSMEFTd6General::STXS_qqHlv_pTV_150_250_1j ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H \ell \nu$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39753 of file NPSMEFTd6General.cpp.

                                                                                  {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 1.006 * aiH + 70.9 * aiWW + 45.5 * aiHW + 60.8 * aipHQ + 2.04 * aipHL;
 
    return STXSb;
}

◆ STXS_qqHlv_pTV_250()

const double NPSMEFTd6General::STXS_qqHlv_pTV_250 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H \ell \nu$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39764 of file NPSMEFTd6General.cpp.

                                                                           {
 
    // Warsaw parameterization
    // (HEL parameterization commented out)
 
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    double CiHL3 = getSMEFTCoeffEW("CHl3R", 0, 0);
    double CiHQ3 = getSMEFTCoeffEW("CHq3R", 0, 0);
 
    //    STXSb = 1.0 - 1.001*aiH + 196.5*aiWW + 169.4*aiHW + 186.3*aipHQ + 2.03*aipHL;
 
    STXSb += (0.121 * getSMEFTCoeffEW("CHbox") - 0.0299 * getSMEFTCoeffEW("CHD") + 1.06 * getSMEFTCoeffEW("CHW") - 0.237 * CiHL3
            + 10.9 * CiHQ3 + 0.184 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    return STXSb;
}

◆ STXS_qqHqq_nonVHtopo()

const double NPSMEFTd6General::STXS_qqHqq_nonVHtopo ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39644 of file NPSMEFTd6General.cpp.

                                                                             {
 
    // Warsaw parameterization
    // (HEL parameterization commented out)
 
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    double CiHL3 = getSMEFTCoeffEW("CHl3R", 0, 0);
    double CiHQ1 = getSMEFTCoeffEW("CHq1R", 0, 0), CiHQ3 = getSMEFTCoeffEW("CHq3R", 0, 0), CiHu = getSMEFTCoeffEW("CHuR", 0, 0), CiHd = getSMEFTCoeffEW("CHdR", 0, 0);
 
    //    STXSb = 1.0 + 1.389*aiWW - 0.0284*aiB - 6.23*aiHW - 0.417*aiHB;
 
    STXSb += (0.1213 * getSMEFTCoeffEW("CHbox") - 0.0107 * getSMEFTCoeffEW("CHD") - 0.008 * getSMEFTCoeffEW("CHW") + 0.0313 * getSMEFTCoeffEW("CHWB")
            - 0.364 * CiHL3 + 0.0043 * CiHQ1 - 0.212 * CiHQ3 - 0.0108 * CiHu
            + 0.0038 * CiHd + 0.182 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    return STXSb;
}

◆ STXS_qqHqq_pTj_200()

const double NPSMEFTd6General::STXS_qqHqq_pTj_200 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39695 of file NPSMEFTd6General.cpp.

                                                                           {
 
    // Warsaw parameterization
    // (HEL parameterization commented out)
 
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    double CiHL3 = getSMEFTCoeffEW("CHl3R", 0, 0);
    double CiHQ1 = getSMEFTCoeffEW("CHq1R", 0, 0), CiHQ3 = getSMEFTCoeffEW("CHq3R", 0, 0), CiHu = getSMEFTCoeffEW("CHuR", 0, 0), CiHd = getSMEFTCoeffEW("CHdR", 0, 0);
 
    //    STXSb = 1.0 + 7.82*aiWW - 0.1868*aiB - 30.65*aiHW - 2.371*aiHB;
 
    STXSb += (0.122 * getSMEFTCoeffEW("CHbox") - 0.0073 * getSMEFTCoeffEW("CHD") - 0.25 * getSMEFTCoeffEW("CHW") + 0.0024 * getSMEFTCoeffEW("CHB")
            + 0.045 * getSMEFTCoeffEW("CHWB") - 0.367 * CiHL3 + 0.030 * CiHQ1 - 0.47 * CiHQ3
            - 0.030 * CiHu + 0.0087 * CiHd + 0.180 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    return STXSb;
}

◆ STXS_qqHqq_Rest()

const double NPSMEFTd6General::STXS_qqHqq_Rest ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39684 of file NPSMEFTd6General.cpp.

                                                                        {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 + 1.546 * aiWW - 0.02509 * aiB - 3.631 * aiHW - 0.2361 * aiHB;
 
    return STXSb;
}

◆ STXS_qqHqq_VBFtopo_j3()

const double NPSMEFTd6General::STXS_qqHqq_VBFtopo_j3 ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39633 of file NPSMEFTd6General.cpp.

                                                                              {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 + 1.204 * aiWW - 0.02692 * aiB - 5.76 * aiHW - 0.4058 * aiHB;
 
    return STXSb;
}

◆ STXS_qqHqq_VBFtopo_j3v()

const double NPSMEFTd6General::STXS_qqHqq_VBFtopo_j3v ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39622 of file NPSMEFTd6General.cpp.

                                                                               {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 + 1.256 * aiWW - 0.02319 * aiB - 4.31 * aiHW - 0.2907 * aiHB;
 
    return STXSb;
}

◆ STXS_qqHqq_VBFtopo_Rest()

const double NPSMEFTd6General::STXS_qqHqq_VBFtopo_Rest ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39617 of file NPSMEFTd6General.cpp.

                                                                                {
 
    return STXS_qqHqq_Rest(sqrt_s);
}

◆ STXS_qqHqq_VHtopo()

const double NPSMEFTd6General::STXS_qqHqq_VHtopo ( const double sqrt_s ) const

virtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39664 of file NPSMEFTd6General.cpp.

                                                                          {
 
    // Warsaw parameterization
    // (HEL parameterization commented out)
 
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    double CiHL3 = getSMEFTCoeffEW("CHl3R", 0, 0);
    double CiHQ1 = getSMEFTCoeffEW("CHq1R", 0, 0), CiHQ3 = getSMEFTCoeffEW("CHq3R", 0, 0), CiHu = getSMEFTCoeffEW("CHuR", 0, 0), CiHd = getSMEFTCoeffEW("CHdR", 0, 0);
 
    //    STXSb = 1.0 + 1.389*aiWW - 0.0284*aiB - 6.23*aiHW - 0.417*aiHB;
 
    STXSb += (0.120 * getSMEFTCoeffEW("CHbox") - 0.0071 * getSMEFTCoeffEW("CHD") + 0.623 * getSMEFTCoeffEW("CHW") + 0.0215 * getSMEFTCoeffEW("CHB")
            + 0.098 * getSMEFTCoeffEW("CHWB") - 0.360 * CiHL3 - 0.026 * CiHQ1 + 1.86 * CiHQ3
            + 0.135 * CiHu - 0.0506 * CiHd + 0.181 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0)) * (1000000.0);
 
    return STXSb;
}

◆ STXS_ttHtH()

const double NPSMEFTd6General::STXS_ttHtH ( const double sqrt_s ) const

virtual

The STXS bin $ ttH + tH $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39874 of file NPSMEFTd6General.cpp.

                                                                   {
 
    // Warsaw parameterization
    // (HEL parameterization commented out)
 
    double STXSb = 1.0;
 
    // To be fixed together with the UFO file when going beyond U(2)
    double CiHL3 = getSMEFTCoeffEW("CHl3R", 0, 0);
    double CiHQ3 = getSMEFTCoeffEW("CHq3R", 0, 0);
 
    //  Set 4 quark operators to zero for the moment.
    double Cqq1 = 0.0, Cqq11 = 0.0, Cqq3 = 0.0, Cqq31 = 0.0;
    double Cuu = 0.0, Cuu1 = 0.0, Cud1 = 0.0, Cud8 = 0.0;
    double Cqu1 = 0.0, Cqu8 = 0.0, Cqd1 = 0.0, Cqd8 = 0.0;
 
    //    STXSb = 1.0 - 0.983*aiH + 2.949*aiu + 0.928*aiG + 313.6*aiuG 
    //            + 27.48*ai3G - 13.09*ai2G;
 
    STXSb += (0.133 * getSMEFTCoeffEW("CG") + 0.1182 * getSMEFTCoeffEW("CHbox") - 0.0296 * getSMEFTCoeffEW("CHD") + 0.532 * getSMEFTCoeffEW("CHG")
            + 0.0120 * getSMEFTCoeffEW("CHW") - 0.1152 * getSMEFTCoeffEW("CuHR", 2, 2) - 0.790 * getSMEFTCoeffEW("CuGR", 2, 2) - 0.0111 * getSMEFTCoeffEW("CuWR", 2, 2)
            - 0.0017 * getSMEFTCoeffEW("CuBR", 2, 2) - 0.1320 * CiHL3 + 0.0146 * CiHQ3
            + 0.0660 * getSMEFTCoeffEW("CllR", 0, 1, 1, 0) + 0.0218 * Cqq1 + 0.1601 * Cqq11 + 0.0263 * Cqq3
            + 0.388 * Cqq31 + 0.0114 * Cuu + 0.1681 * Cuu1 - 0.0018 * Cud1
            + 0.0265 * Cud8 + 0.007 * Cqu1 + 0.1087 * Cqu8
            - 0.0011 * Cqd1 + 0.0266 * Cqd8) * (1000000.0);
 
    return STXSb;
}

◆ STXS_WHqqHqq_pTj1_200()

const double NPSMEFTd6General::STXS_WHqqHqq_pTj1_200 ( const double sqrt_s ) const

virtual

The STXS bin $ qq \to WH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39948 of file NPSMEFTd6General.cpp.

                                                                              {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 1.003 * aiH + 181.2 * aiWW + 152.3 * aiHW + 173.7 * aipHQ;
 
    return STXSb;
}

◆ STXS_WHqqHqq_Rest()

const double NPSMEFTd6General::STXS_WHqqHqq_Rest ( const double sqrt_s ) const

virtual

The STXS bin $ qq \to WH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39937 of file NPSMEFTd6General.cpp.

                                                                          {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 1.002 * aiH + 34.29 * aiWW + 11.56 * aiHW + 26.27 * aipHQ;
 
    return STXSb;
}

◆ STXS_WHqqHqq_VBFtopo_j3()

const double NPSMEFTd6General::STXS_WHqqHqq_VBFtopo_j3 ( const double sqrt_s ) const

virtual

The STXS bin $ qq \to WH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39915 of file NPSMEFTd6General.cpp.

                                                                                {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 1.04 * aiH + 44.9 * aiWW + 20.3 * aiHW + 36.8 * aipHQ;
 
    return STXSb;
}

◆ STXS_WHqqHqq_VBFtopo_j3v()

const double NPSMEFTd6General::STXS_WHqqHqq_VBFtopo_j3v ( const double sqrt_s ) const

virtual

The STXS bin $ qq \to WH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39904 of file NPSMEFTd6General.cpp.

                                                                                 {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 0.94 * aiH + 39.5 * aiWW + 13.8 * aiHW + 32.1 * aipHQ;
 
    return STXSb;
}

◆ STXS_WHqqHqq_VH2j()

const double NPSMEFTd6General::STXS_WHqqHqq_VH2j ( const double sqrt_s ) const

virtual

The STXS bin $ qq \to WH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39926 of file NPSMEFTd6General.cpp.

                                                                          {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 0.996 * aiH + 45.57 * aiWW + 23.66 * aiHW + 37.55 * aipHQ;
 
    return STXSb;
}

◆ STXS_ZHqqHqq_pTj1_200()

const double NPSMEFTd6General::STXS_ZHqqHqq_pTj1_200 ( const double sqrt_s ) const

virtual

The STXS bin $ qq \to ZH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 40007 of file NPSMEFTd6General.cpp.

                                                                              {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 1.003 * aiH - 4.03 * aiT + 141.5 * aiWW + 41.6 * aiB + 112.5 * aiHW
            + 33.6 * aiHB - 11.52 * aiHQ + 156.2 * aipHQ + 38.9 * aiHu - 12.53 * aiHd;
 
    return STXSb;
}

◆ STXS_ZHqqHqq_Rest()

const double NPSMEFTd6General::STXS_ZHqqHqq_Rest ( const double sqrt_s ) const

virtual

The STXS bin $ qq \to ZH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39995 of file NPSMEFTd6General.cpp.

                                                                          {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 1.001 * aiH - 3.998 * aiT + 30.89 * aiWW + 8.35 * aiB + 8.71 * aiHW
            + 2.616 * aiHB - 1.782 * aiHQ + 26.1 * aipHQ + 5.942 * aiHu - 2.305 * aiHd;
 
    return STXSb;
}

◆ STXS_ZHqqHqq_VBFtopo_j3()

const double NPSMEFTd6General::STXS_ZHqqHqq_VBFtopo_j3 ( const double sqrt_s ) const

virtual

The STXS bin $ qq \to ZH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39971 of file NPSMEFTd6General.cpp.

                                                                                {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 0.97 * aiH - 3.98 * aiT + 38.1 * aiWW + 10.5 * aiB + 14.2 * aiHW
            + 4.15 * aiHB - 2.36 * aiHQ + 34.5 * aipHQ + 8.4 * aiHu - 2.79 * aiHd;
 
    return STXSb;
}

◆ STXS_ZHqqHqq_VBFtopo_j3v()

const double NPSMEFTd6General::STXS_ZHqqHqq_VBFtopo_j3v ( const double sqrt_s ) const

virtual

The STXS bin $ qq \to ZH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39959 of file NPSMEFTd6General.cpp.

                                                                                 {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 0.94 * aiH - 4.0 * aiT + 34.8 * aiWW + 10.0 * aiB + 9.9 * aiHW
            + 3.04 * aiHB - 2.14 * aiHQ + 31.1 * aipHQ + 7.6 * aiHu - 2.59 * aiHd;
 
    return STXSb;
}

◆ STXS_ZHqqHqq_VH2j()

const double NPSMEFTd6General::STXS_ZHqqHqq_VH2j ( const double sqrt_s ) const

virtual

The STXS bin $ qq \to ZH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 39983 of file NPSMEFTd6General.cpp.

                                                                          {
 
    // HEL parameterization
 
    double STXSb = 1.0;
 
    STXSb = 1.0 - 0.998 * aiH - 4.002 * aiT + 37.99 * aiWW + 10.47 * aiB + 16.45 * aiHW
            + 4.927 * aiHB - 2.401 * aiHQ + 34.45 * aipHQ + 7.94 * aiHu - 2.993 * aiHd;
 
    return STXSb;
}

◆ tovers2()

const double NPSMEFTd6General::tovers2	(	const double	cosmin,
		const double	cosmax
	)		const

Definition at line 46493 of file NPSMEFTd6General.cpp.

                                                                                     {
    return 0.25 * (cosmax * (1.0 - cosmax * (1.0 - cosmax / 3.0)) - cosmin * (1.0 - cosmin * (1.0 - cosmin / 3.0)));
}

◆ uovers2()

const double NPSMEFTd6General::uovers2	(	const double	cosmin,
		const double	cosmax
	)		const

Definition at line 46497 of file NPSMEFTd6General.cpp.

                                                                                     {
    return 0.25 * (cosmax * (1.0 + cosmax * (1.0 + cosmax / 3.0)) - cosmin * (1.0 + cosmin * (1.0 + cosmin / 3.0)));
}

◆ xseeWW()

const double NPSMEFTd6General::xseeWW ( const double sqrt_s ) const

virtual

Total $e^+ e^- \to W^+ W^- \to jj \ell \nu$ cross section in pb, with $\ell= e, \mu$.

Returns: $\sigma(e^+ e^- \to W^+ W^- \to jj \ell \nu) $

Reimplemented from NPbase.

Definition at line 38790 of file NPSMEFTd6General.cpp.

                                                               {
    return dxseeWWdcosBin(sqrt_s, -1.0, 1.0);
}

◆ xseeWW4fLEP2()

const double NPSMEFTd6General::xseeWW4fLEP2	(	const double	sqrt_s,
		const int	fstate
	)		const

virtual

The cross section in pb for $e^+ e^- \to W^+ W^- \to 4f $, with $ 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) $ the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].

Returns: $sigma$ [pb]

Reimplemented from NPbase.

Definition at line 37125 of file NPSMEFTd6General.cpp.

                                                                                       {
 
    //  Returns cross section in pb
 
    //  fstate = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj),
    //       4 (e v e v), 5 (mu v mu v), 6 (tau v tau v),
    //       7 (e v mu v), 8 (e v tau v), 9 (mu v tau v)
    //      10 (l v jj), 11 (l v l v)
 
    double xspb = 0.0;
 
    double xspbSM[8] = {0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0, 0.0};
    // SM values from hep-ex/0409016    
    double xsjjjjSM[8] = {7.42, 7.56, 7.68, 7.76, 7.79, 7.81, 7.82, 7.82};
    double xslvjjSM[8] = {7.14, 7.26, 7.38, 7.44, 7.47, 7.50, 7.50, 7.50}; // All leptons. Divide by 3 for each
    double xslvlvSM[8] = {1.72, 1.76, 1.79, 1.80, 1.81, 1.82, 1.82, 1.82}; // All leptons. Divide by 6 for each
 
    double dgWve, dgWpm1, dgWpm2, dmZ2, dmW2, dGW, dGZ, dGF, dgZ, dsW2, dgVZee, dgAZee, dgZ1, dgga1, dkga, dkZ, dlga, dlZ, deem;
 
    double gVZeeSM, gAZeeSM;
 
    double norm4f = 1.0;
 
    //  Values of the couplings: final-state independent couplings
    gVZeeSM = -0.25 + sW2_tree;
    gAZeeSM = -0.25;
 
    dGF = delta_GF / sqrt(2.0);
 
    dmZ2 = cAsch * (0.5 * getSMEFTCoeffEW("CHD") + 2.0 * cW_tree * sW_tree * getSMEFTCoeffEW("CHWB")) * v2
            + cWsch * (0.5 * getSMEFTCoeffEW("CHD") + 2.0 * (Mw_inp / Mz) * sqrt(1.0 - Mw_inp * Mw_inp / Mz / Mz) * getSMEFTCoeffEW("CHWB")) * v2;
 
    dmW2 = -2.0 * deltaMwd6(); //There is a minus sign between refs. definition of dmW2 and ours
 
    dGW = deltaGwd6();
 
    dGZ = deltaGzd6();
 
    dsW2 = cAsch * (-0.5 * (cW2_tree / (1.0 - 2.0 * sW2_tree)) * ((getSMEFTCoeffEW("CHD")
            + 2.0 * getSMEFTCoeffEW("CHWB") / cW_tree / sW_tree) * v2
            + 2.0 * sqrt(2.0) * dGF))
            + cWsch * (1.0 / sW2_tree) * (0.5 * Mw_inp * Mw_inp * getSMEFTCoeffEW("CHD") / Mz / Mz + Mw_inp * sqrt(1.0 - Mw_inp * Mw_inp / Mz / Mz) * getSMEFTCoeffEW("CHWB") / Mz) * v2;
 
    dgZ = -dGF / sqrt(2.0) - 0.5 * dmZ2
            + cW_tree * sW_tree * getSMEFTCoeffEW("CHWB") * v2;
 
    dgVZee = dgZ * gVZeeSM
            - 0.25 * (getSMEFTCoeffEW("CHeR", 0, 0) + getSMEFTCoeffEW("CHl1R", 0, 0) + getSMEFTCoeffEW("CHl3R", 0, 0)) * v2
            - sW2_tree * dsW2;
 
    dgAZee = dgZ * gAZeeSM
            + 0.25 * (getSMEFTCoeffEW("CHeR", 0, 0) - getSMEFTCoeffEW("CHl1R", 0, 0) - getSMEFTCoeffEW("CHl3R", 0, 0)) * v2;
 
    dgWve = 0.5 * getSMEFTCoeffEW("CHl3R", 0, 0) * v2
            + cAsch * (0.25 * (cW_tree * getSMEFTCoeffEW("CHWB") / sW_tree) * v2 + 0.25 * dsW2)
            + cWsch * (-dGF / 2.0 / sqrt(2.0));
 
    dgZ1 = deltag1ZNP(sqrt_s);
 
    dgga1 = deltag1gaNP(sqrt_s);
 
    dkga = deltaKgammaNP(sqrt_s);
 
    dkZ = dgZ1 - (sW2_tree / cW2_tree) * (dkga - dgga1);
 
    dlga = -lambdaZNP(sqrt_s);
 
    dlZ = -lambdaZNP(sqrt_s);
 
    deem = delta_e + 0.5 * delta_A;
 
    //  Values of the couplings: final-state dependent couplings
    dgWpm1 = 0.0;
    dgWpm2 = 0.0;
 
    switch (fstate) {
 
        case 0:
            //  fstate = 0 (jjjj)       
            dgWpm1 = 0.5 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1));
            dgWpm2 = 0.5 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1));
            norm4f = 1.01;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xsjjjjSM[i];
            }
            break;
        case 1:
            //  fstate = 1 (e v jj)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 0, 0);
            dgWpm2 = 0.5 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1));
            norm4f = 1.0;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvjjSM[i] / 3.0;
            }
            break;
        case 2:
            //  fstate = 2 (mu v jj)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 1, 1);
            dgWpm2 = 0.5 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1));
            norm4f = 1.0;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvjjSM[i] / 3.0;
            }
            break;
        case 3:
            //  fstate = 3 (tau v jj)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 2, 2);
            dgWpm2 = 0.5 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1));
            norm4f = 1.0;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvjjSM[i] / 3.0;
            }
            break;
        case 4:
            //  fstate = 4 (e v e v)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 0, 0);
            dgWpm2 = getSMEFTCoeffEW("CHl3R", 0, 0);
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i] / 6.0;
            }
            break;
        case 5:
            //  fstate = 5 (mu v mu v)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 1, 1);
            dgWpm2 = getSMEFTCoeffEW("CHl3R", 1, 1);
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i] / 6.0;
            }
            break;
        case 6:
            //  fstate = 6 (tau v tau v)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 2, 2);
            dgWpm2 = getSMEFTCoeffEW("CHl3R", 2, 2);
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i] / 6.0;
            }
            break;
        case 7:
            //  fstate = 7 (e v mu v)            
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 0, 0);
            dgWpm2 = getSMEFTCoeffEW("CHl3R", 1, 1);
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i] / 6.0;
            }
            break;
        case 8:
            //  fstate = 8 (e v tau v)           
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 0, 0);
            dgWpm2 = getSMEFTCoeffEW("CHl3R", 2, 2);
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i] / 6.0;
            }
            break;
        case 9:
            //  fstate = 9 (mu v tau v)           
            dgWpm1 = getSMEFTCoeffEW("CHl3R", 1, 1);
            dgWpm2 = getSMEFTCoeffEW("CHl3R", 2, 2);
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i] / 6.0;
            }
            break;
        case 10:
            //  fstate = 10 (l v jj)           
            dgWpm1 = (1.0 / 3.0) * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1) + getSMEFTCoeffEW("CHl3R", 2, 2));
            dgWpm2 = 0.5 * (getSMEFTCoeffEW("CHq3R", 0, 0) + getSMEFTCoeffEW("CHq3R", 1, 1));
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvjjSM[i];
            }
            break;
        case 11:
            //  fstate = 11 (l v l v)           
            dgWpm1 = (1.0 / 3.0) * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1) + getSMEFTCoeffEW("CHl3R", 2, 2));
            dgWpm2 = (1.0 / 3.0) * (getSMEFTCoeffEW("CHl3R", 0, 0) + getSMEFTCoeffEW("CHl3R", 1, 1) + getSMEFTCoeffEW("CHl3R", 2, 2));
            norm4f = 1.0 / 4.04;
            for (int i = 0; i < 8; ++i) {
                xspbSM[i] = xslvlvSM[i];
            }
            break;
    }
 
    dgWpm1 = 0.5 * dgWpm1
            + cAsch * (0.25 * (cW_tree * getSMEFTCoeffEW("CHWB") / sW_tree) * v2 + 0.25 * dsW2)
            + cWsch * (-dGF / 2.0 / sqrt(2.0));
 
    dgWpm2 = 0.5 * dgWpm2
            + cAsch * (0.25 * (cW_tree * getSMEFTCoeffEW("CHWB") / sW_tree) * v2 + 0.25 * dsW2)
            + cWsch * (-dGF / 2.0 / sqrt(2.0));
 
    if (sqrt_s == 0.1886) {
 
        xspb += xspbSM[0] + norm4f * cAsch * (
                +2.6 * dmW2
                - 17.0 * dGW
                + 72.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 5.3 * dgVZee
                + 0.3 * dgAZee
                - 0.08 * dgZ1
                - 0.50 * dkga
                - 0.19 * dkZ
                - 0.29 * dlga
                + 0.026 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 72.0 * dgWve
                + 33.4 * dgWpm1
                + 33.4 * dgWpm2
                + 5.72 * dgVZee
                + 0.21 * dgAZee
                - 0.05 * dgZ1
                - 0.57 * dkga
                - 0.16 * dkZ
                - 0.34 * dlga
                + 0.051 * dlZ
                + 0.0005 * dGZ
                - 0.41 * dgga1
                - 0.98 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[0];
 
    } else if (sqrt_s == 0.1916) {
 
        xspb += xspbSM[1] + norm4f * cAsch * (
                +1.6 * dmW2
                - 17.0 * dGW
                + 73.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 5.8 * dgVZee
                + 0.4 * dgAZee
                - 0.10 * dgZ1
                - 0.56 * dkga
                - 0.22 * dkZ
                - 0.32 * dlga
                + 0.018 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 72.0 * dgWve
                + 33.6 * dgWpm1
                + 33.6 * dgWpm2
                + 6.26 * dgVZee
                + 0.33 * dgAZee
                - 0.07 * dgZ1
                - 0.64 * dkga
                - 0.19 * dkZ
                - 0.37 * dlga
                + 0.045 * dlZ
                + 0.0005 * dGZ
                - 0.41 * dgga1
                - 1.08 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[1];
 
    } else if (sqrt_s == 0.1955) {
 
        xspb += xspbSM[2] + norm4f * cAsch * (
                +0.26 * dmW2
                - 17.0 * dGW
                + 74.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 6.5 * dgVZee
                + 0.6 * dgAZee
                - 0.12 * dgZ1
                - 0.64 * dkga
                - 0.27 * dkZ
                - 0.36 * dlga
                + 0.005 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 73.0 * dgWve
                + 33.8 * dgWpm1
                + 33.8 * dgWpm2
                + 6.91 * dgVZee
                + 0.50 * dgAZee
                - 0.09 * dgZ1
                - 0.72 * dkga
                - 0.22 * dkZ
                - 0.41 * dlga
                + 0.035 * dlZ
                + 0.0005 * dGZ
                - 0.49 * dgga1
                - 1.20 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[2];
 
    } else if (sqrt_s == 0.1995) {
 
        xspb += xspbSM[3] + norm4f * cAsch * (
                -0.54 * dmW2
                - 17.0 * dGW
                + 75.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 7.1 * dgVZee
                + 0.8 * dgAZee
                - 0.15 * dgZ1
                - 0.71 * dkga
                - 0.31 * dkZ
                - 0.40 * dlga
                - 0.009 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 74.0 * dgWve
                + 33.7 * dgWpm1
                + 33.7 * dgWpm2
                + 7.52 * dgVZee
                + 0.68 * dgAZee
                - 0.11 * dgZ1
                - 0.79 * dkga
                - 0.26 * dkZ
                - 0.45 * dlga
                + 0.022 * dlZ
                + 0.0005 * dGZ
                - 0.53 * dgga1
                - 1.33 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[3];
 
    } else if (sqrt_s == 0.2016) {
 
        xspb += xspbSM[4] + norm4f * cAsch * (
                -0.97 * dmW2
                - 17.0 * dGW
                + 75.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 7.4 * dgVZee
                + 0.9 * dgAZee
                - 0.16 * dgZ1
                - 0.75 * dkga
                - 0.33 * dkZ
                - 0.42 * dlga
                - 0.017 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 74.0 * dgWve
                + 33.7 * dgWpm1
                + 33.7 * dgWpm2
                + 7.82 * dgVZee
                + 0.78 * dgAZee
                - 0.12 * dgZ1
                - 0.83 * dkga
                - 0.28 * dkZ
                - 0.47 * dlga
                + 0.016 * dlZ
                + 0.0005 * dGZ
                - 0.55 * dgga1
                - 1.39 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[4];
 
    } else if (sqrt_s == 0.2049) {
 
        xspb += xspbSM[5] + norm4f * cAsch * (
                -1.4 * dmW2
                - 17.0 * dGW
                + 75.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 7.8 * dgVZee
                + 1.0 * dgAZee
                - 0.18 * dgZ1
                - 0.80 * dkga
                - 0.37 * dkZ
                - 0.44 * dlga
                - 0.029 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 74.0 * dgWve
                + 33.5 * dgWpm1
                + 33.5 * dgWpm2
                + 8.24 * dgVZee
                + 0.93 * dgAZee
                - 0.14 * dgZ1
                - 0.89 * dkga
                - 0.32 * dkZ
                - 0.47 * dlga
                + 0.005 * dlZ
                + 0.0005 * dGZ
                - 0.58 * dgga1
                - 1.47 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[5];
 
    } else if (sqrt_s == 0.2066) {
 
        xspb += xspbSM[6] + norm4f * cAsch * (
                -1.8 * dmW2
                - 17.0 * dGW
                + 76.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 8.0 * dgVZee
                + 1.1 * dgAZee
                - 0.19 * dgZ1
                - 0.83 * dkga
                - 0.39 * dkZ
                - 0.46 * dlga
                - 0.036 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 75.0 * dgWve
                + 33.4 * dgWpm1
                + 33.4 * dgWpm2
                + 8.45 * dgVZee
                + 1.01 * dgAZee
                - 0.15 * dgZ1
                - 0.92 * dkga
                - 0.33 * dkZ
                - 0.51 * dlga
                - 0.001 * dlZ
                + 0.0005 * dGZ
                - 0.60 * dgga1
                - 1.52 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[6];
 
    } else if (sqrt_s == 0.208) {
 
        xspb += xspbSM[7] + norm4f * cAsch * (
                -2.0 * dmW2
                - 17.0 * dGW
                + 76.0 * dgWve
                + 34.0 * dgWpm1
                + 34.0 * dgWpm2
                + 8.2 * dgVZee
                + 1.2 * dgAZee
                - 0.20 * dgZ1
                - 0.85 * dkga
                - 0.40 * dkZ
                - 0.47 * dlga
                - 0.042 * dlZ
                );
 
        xspb += norm4f * cWsch * (
                -17.0 * dGW
                + 75.0 * dgWve
                + 33.3 * dgWpm1
                + 33.3 * dgWpm2
                + 8.62 * dgVZee
                + 1.08 * dgAZee
                - 0.16 * dgZ1
                - 0.94 * dkga
                - 0.35 * dkZ
                - 0.52 * dlga
                - 0.007 * dlZ
                + 0.0005 * dGZ
                - 0.61 * dgga1
                - 1.55 * deem
                );
 
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            xspb += 0.0;
        }
 
        //Add relative theory errors (free par). (Assume they are constant in energy.)
        xspb += eeeWWint * xspbSM[7];
 
    } else
        throw std::runtime_error("Bad argument in NPSMEFTd6General::xseeWW4fLEP2()");
 
    if (xspb < 0) return std::numeric_limits<double>::quiet_NaN();
 
    return xspb;
}

◆ xseeWWtotLEP2()

const double NPSMEFTd6General::xseeWWtotLEP2 ( const double sqrt_s ) const

virtual

The total cross section in pb for $e^+ e^- \to W^+ W^-$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].

Returns: $sigma$ [pb]

Reimplemented from NPbase.

Definition at line 37668 of file NPSMEFTd6General.cpp.

                                                                      {
    return ( xseeWW4fLEP2(sqrt_s, 0) + xseeWW4fLEP2(sqrt_s, 10) + xseeWW4fLEP2(sqrt_s, 11));
}

Member Data Documentation

◆ NNPSMEFTd6GeneralVars

const int NPSMEFTd6General::NNPSMEFTd6GeneralVars = 2708-208 + 79

static

The number of the model parameters in NPSMEFTd6General (including the 18 parameters needed for the SM and 79 auxiliary parameters).

Definition at line 600 of file NPSMEFTd6General.h.

◆ NPSMEFTd6GeneralVars

const std::string NPSMEFTd6General::NPSMEFTd6GeneralVars

static

A string array containing the labels of the model parameters in NPSMEFTd6General.

Definition at line 20 of file NPSMEFTd6General.h.

           {L}_\mathrm{eff}
 * = \mathcal{L}_\mathrm{SM}
 *   + \sum_i \frac{C_i}{\Lambda^2} \mathcal{O}_i.
 * @f]
 * The implementation is written in the basis of \cite Grzadkowski:2010es.
 * For convenience, the parameterization also includes operators appearing in
 * other common bases. In particular, the complete set of parameters contains 4
 * redundancies, given by the coefficients \f$C_{2B,2W,DHB,DHW,DB,DW} \f$,
 * which correspond to operators not included in the basis of \cite Grzadkowski:2010es.
 * For meaningful physical results one must make sure to include only
 * a complete set of interactions in a given analysis.
 *
 * @anchor NPSMEFTd6GeneralInitialization
 * <h3>Initialization</h3>
 *
 * After creating an instance of the current class with the constructor
 * NPSMEFTd6General(), it is required to call the initialization method
 * InitializeModel().
 * In the Monte Carlo run, the constructor as well as the initialization
 * method are called in InputParser::ReadParameters().
 *
 *
 * @anchor NPSMEFTd6GeneralParameters
 * <h3>%Model parameters</h3>
 *
 * The model parameters of %NPSMEFTd6General are summarized below:
 * <table class="model">
 * <tr>
 *   <th>Label</th>
 *   <th>LaTeX symbol</th>
 *   <th>Description</th>
 * </tr>
 * <tr>
 *   <td class="mod_name">%g1_LNP </td>
 *   <td class="mod_symb">\f$g_1(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The hypercharge coupling constant at the New Physics scale. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%g2_LNP </td>
 *   <td class="mod_symb">\f$g_2(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The SU(2)@f$_L@f$ coupling constant at the New Physics scale. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%g1_LNP </td>
 *   <td class="mod_symb">\f$g_3(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The QCD coupling constant at the New Physics scale. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%lambdaH_LNP </td>
 *   <td class="mod_symb">\f$\lambda_H(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The coefficient of the @f$(H^\dagger H)^2@f$ term at the New Physics scale. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%muH_LNP </td>
 *   <td class="mod_symb">\f$\mu_H(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The square root of the coefficient of the @f$(H^\dagger H)@f$ term at the New Physics scale. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%Ye_LNP </td>
 *   <td class="mod_symb">\f$Y_e(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The electron Yukawa coupling at the New Physics scale. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%Ymu_LNP </td>
 *   <td class="mod_symb">\f$Y_\mu(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The muon Yukawa coupling at the New Physics scale. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%Ytau_LNP </td>
 *   <td class="mod_symb">\f$Y_\tau(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The tau Yukawa coupling at the New Physics scale. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%Yu_LNP </td>
 *   <td class="mod_symb">\f$Y_u(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The up quark Yukawa coupling at the New Physics scale in the up basis. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%Yc_LNP </td>
 *   <td class="mod_symb">\f$Y_c(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The charm quark Yukawa coupling at the New Physics scale in the up basis. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%Yt_LNP </td>
 *   <td class="mod_symb">\f$Y_t(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The top quark Yukawa coupling at the New Physics scale in the up basis. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%Yd_LNP </td>
 *   <td class="mod_symb">\f$Y_d(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The down quark Yukawa coupling at the New Physics scale in the down basis. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%Ys_LNP </td>
 *   <td class="mod_symb">\f$Y_s(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The strange quark Yukawa coupling at the New Physics scale in the down basis. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%Yb_LNP </td>
 *   <td class="mod_symb">\f$Y_b(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The bottom quark Yukawa coupling at the New Physics scale in the down basis. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%s12CKM_LNP </td>
 *   <td class="mod_symb">\f$s_{12}(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The sine of the @f$\theta_{12}@f$ angle parameterizing the relative orientation of up and down Yukawa couplings at the New Physics scale. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%s13CKM_LNP </td>
 *   <td class="mod_symb">\f$s_{13}(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The sine of the @f$\theta_{13}@f$ angle parameterizing the relative orientation of up and down Yukawa couplings at the New Physics scale. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%s23CKM_LNP </td>
 *   <td class="mod_symb">\f$s_{23}(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The sine of the @f$\theta_{23}@f$ angle parameterizing the relative orientation of up and down Yukawa couplings at the New Physics scale. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%dCKM_LNP </td>
 *   <td class="mod_symb">\f$\delta(\Lambda_\mathrm{NP})\f$</td>
 *   <td class="mod_desc">The CP-violating phase of the matrix describing the relative orientation of up and down Yukawa couplings at the New Physics scale. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CG </td>
 *   <td class="mod_symb">\f$C_{G} \f$</td>
 *   <td class="mod_desc">The coefficient of the operator
 *   \f${\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CW </td>
 *   <td class="mod_symb">\f$C_{W} \f$</td>
 *   <td class="mod_desc">The coefficient of the operator
 *   \f${\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHG </td>
 *   <td class="mod_symb">\f$C_{HG} \f$</td>
 *   <td class="mod_desc">The coefficient of the operator
 *   \f${\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHW </td>
 *   <td class="mod_symb">\f$C_{HW} \f$</td>
 *   <td class="mod_desc">The coefficient of the operator
 *   \f${\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHB </td>
 *   <td class="mod_symb">\f$C_{HB} \f$</td>
 *   <td class="mod_desc">The coefficient of the operator
 *   \f${\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHWB </td>
 *   <td class="mod_symb">\f$C_{HWB} \f$</td>
 *   <td class="mod_desc">The coefficient of the operator
 *   \f${\cal O}_{HWB}=\big(H^\dagger\sigma^a H\big)W_{\mu\nu}^a B^{\mu\nu}\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHD </td>
 *   <td class="mod_symb">\f$C_{HD}\f$</td>
 *   <td class="mod_desc">The coefficient of the operator
 *   \f${\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHbox </td>
 *   <td class="mod_symb">\f$C_{H\Box}\f$</td>
 *   <td class="mod_desc">The coefficient of the operator
 *   \f${\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CH </td>
 *   <td class="mod_symb">\f$C_{H}\f$</td>
 *   <td class="mod_desc">The coefficient of the operator
 *   \f${\cal O}_{H}=\big(H^\dagger H\big)^3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHl1_kk, CHl1_klr, CHl1_kli </td>
 *   <td class="mod_symb">\f$ (C_{HL}^{(1)})_{kk}, \mbox{Re}\big[(C_{HL}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(1)})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{HL}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big)
 *   \big(\overline{L^i}\,\gamma^\mu L^j\big)\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHl3_kk, CHl3_klr, CHl3_kli </td>
 *   <td class="mod_symb">\f$ (C_{HL}^{(3)})_{kk}, \mbox{Re}\big[(C_{HL}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(3)})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{HL}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big)
 *   \big(\overline{L^i}\,\gamma^\mu \sigma^a L^j\big)\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHe_kk, CHe_klr, CHe_kli </td>
 *   <td class="mod_symb">\f$ (C_{He})_{kk}, \mbox{Re}\big[(C_{He})_{kl}\big], \mbox{Im}\big[(C_{He})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big)
 *   \big(\overline{E^i}\,\gamma^\mu E^j\big)\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHq1_kk, CHq1_klr, CHq1_kli </td>
 *   <td class="mod_symb">\f$ (C_{HQ}^{(1)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(1)})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{HQ}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big)
 *   \big(\overline{Q^i}\,\gamma^\mu Q^j\big)\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHq3_kk, CHq3_klr, CHq3_kli </td>
 *   <td class="mod_symb">\f$ (C_{HQ}^{(3)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(3)})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{HQ}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big)
 *   \big(\overline{Q^i}\,\gamma^\mu \sigma^a Q^j\big)\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHu_kk, CHu_klr, CHu_kli </td>
 *   <td class="mod_symb">\f$ (C_{Hu})_{kk}, \mbox{Re}\big[(C_{Hu})_{kl}\big], \mbox{Im}\big[(C_{Hu})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{Hu})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big)
 *   \big(\overline{U^i}\,\gamma^\mu U^j\big)\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHd_kk, CHd_klr, CHd_kli </td>
 *   <td class="mod_symb">\f$ (C_{Hd})_{kk}, \mbox{Re}\big[(C_{Hd})_{kl}\big], \mbox{Im}\big[(C_{Hd})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{Hd})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big)
 *   \big(\overline{D^i}\,\gamma^\mu D^j\big)\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CHud_klr, CHud_kli </td>
 *   <td class="mod_symb">\f$\mbox{Re}\big[(C_{Hud})_{kl}\big], \mbox{Im}\big[(C_{Hud})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{Hud})_{ij} =i\big(\widetilde{H}^\dagger D_\mu H\big)
 *   \big(\overline{U^i}\,\gamma^\mu D^j\big)\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CeH_klr, CeH_kli </td>
 *   <td class="mod_symb">\f$\mbox{Re}\big[(C_{eH})_{kl}\big], \mbox{Im}\big[(C_{eH})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{eH})_{ij} =\big(H^\dagger H\big)
 *   \big(\overline{L^i}\,H E^j\big)\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CuH_klr, CuH_kli </td>
 *   <td class="mod_symb">\f$\mbox{Re}\big[(C_{uH})_{kl}\big], \mbox{Im}\big[(C_{uH})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{uH})_{ij} =\big(H^\dagger H\big)
 *   \big(\overline{Q^i}\,\widetilde{H} U^j\big)\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CdH_klr, CdH_kli </td>
 *   <td class="mod_symb">\f$\mbox{Re}\big[(C_{dH})_{kl}\big], \mbox{Im}\big[(C_{dH})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{dH})_{ij} =\big(H^\dagger H\big)
 *   \big(\overline{Q^i}\,H D^j\big)\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CuG_klr, CuG_kli </td>
 *   <td class="mod_symb">\f$\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CuW_klr, CuW_kli </td>
 *   <td class="mod_symb">\f$\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a U^j\big)\widetilde{H} W_{\mu\nu}^a\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CuB_klr, CuB_kli </td>
 *   <td class="mod_symb">\f$\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CdG_klr, CdG_kli </td>
 *   <td class="mod_symb">\f$\mbox{Re}\big[(C_{dG})_{kl}\big], \mbox{Im}\big[(C_{dG})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{dG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A D^j\big)H G_{\mu\nu}^A\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CdW_klr, CdW_kli </td>
 *   <td class="mod_symb">\f$\mbox{Re}\big[(C_{dW})_{kl}\big], \mbox{Im}\big[(C_{dW})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{dW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a D^j\big)H W_{\mu\nu}^a\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CdB_klr, CdB_kli </td>
 *   <td class="mod_symb">\f$\mbox{Re}\big[(C_{dB})_{kl}\big], \mbox{Im}\big[(C_{dB})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{dB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} D^j\big)H B_{\mu\nu}\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>
 *   <td class="mod_name">%CeW_klr, CeW_kli </td>
 *   <td class="mod_symb">\f$\mbox{Re}\big[(C_{eW})_{kl}\big], \mbox{Im}\big[(C_{eW})_{kl}\big] \f$</td>
 *   <td class="mod_desc">The real and imaginary parts of the coefficient of the operator
 *   \f$({\cal O}_{eW})_{ij} =\big(\overline{L^i}\sigma^{\mu\nu} \sigma_a E^j\big)H W_{\mu\nu}^a\f$, for \f$i,j=1,2,3\f$. </td>
 * </tr>
 * <tr>

The documentation for this class was generated from the following files:

Label	LaTeX symbol	Description
g1_LNP	\(g_1(\Lambda_\mathrm{NP})\)	The hypercharge coupling constant at the New Physics scale.
g2_LNP	\(g_2(\Lambda_\mathrm{NP})\)	The SU(2) \(_L\) coupling constant at the New Physics scale.
g1_LNP	\(g_3(\Lambda_\mathrm{NP})\)	The QCD coupling constant at the New Physics scale.
lambdaH_LNP	\(\lambda_H(\Lambda_\mathrm{NP})\)	The coefficient of the \((H^\dagger H)^2\) term at the New Physics scale.
muH_LNP	\(\mu_H(\Lambda_\mathrm{NP})\)	The square root of the coefficient of the \((H^\dagger H)\) term at the New Physics scale.
Ye_LNP	\(Y_e(\Lambda_\mathrm{NP})\)	The electron Yukawa coupling at the New Physics scale.
Ymu_LNP	\(Y_\mu(\Lambda_\mathrm{NP})\)	The muon Yukawa coupling at the New Physics scale.
Ytau_LNP	\(Y_\tau(\Lambda_\mathrm{NP})\)	The tau Yukawa coupling at the New Physics scale.
Yu_LNP	\(Y_u(\Lambda_\mathrm{NP})\)	The up quark Yukawa coupling at the New Physics scale in the up basis.
Yc_LNP	\(Y_c(\Lambda_\mathrm{NP})\)	The charm quark Yukawa coupling at the New Physics scale in the up basis.
Yt_LNP	\(Y_t(\Lambda_\mathrm{NP})\)	The top quark Yukawa coupling at the New Physics scale in the up basis.
Yd_LNP	\(Y_d(\Lambda_\mathrm{NP})\)	The down quark Yukawa coupling at the New Physics scale in the down basis.
Ys_LNP	\(Y_s(\Lambda_\mathrm{NP})\)	The strange quark Yukawa coupling at the New Physics scale in the down basis.
Yb_LNP	\(Y_b(\Lambda_\mathrm{NP})\)	The bottom quark Yukawa coupling at the New Physics scale in the down basis.
s12CKM_LNP	\(s_{12}(\Lambda_\mathrm{NP})\)	The sine of the \(\theta_{12}\) angle parameterizing the relative orientation of up and down Yukawa couplings at the New Physics scale.
s13CKM_LNP	\(s_{13}(\Lambda_\mathrm{NP})\)	The sine of the \(\theta_{13}\) angle parameterizing the relative orientation of up and down Yukawa couplings at the New Physics scale.
s23CKM_LNP	\(s_{23}(\Lambda_\mathrm{NP})\)	The sine of the \(\theta_{23}\) angle parameterizing the relative orientation of up and down Yukawa couplings at the New Physics scale.
dCKM_LNP	\(\delta(\Lambda_\mathrm{NP})\)	The CP-violating phase of the matrix describing the relative orientation of up and down Yukawa couplings at the New Physics scale.
CG	\(C_{G} \)	The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\).
CW	\(C_{W} \)	The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\).
CHG	\(C_{HG} \)	The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\).
CHW	\(C_{HW} \)	The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\).
CHB	\(C_{HB} \)	The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\).
CHWB	\(C_{HWB} \)	The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\sigma^a H\big)W_{\mu\nu}^a B^{\mu\nu}\).
CHD	\(C_{HD}\)	The coefficient of the operator \({\cal O}_{HD}=\big\|H^\dagger D_\mu H\big\|^2\).
CHbox	\(C_{H\Box}\)	The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\).
CH	\(C_{H}\)	The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\).
CHl1_kk, CHl1_klr, CHl1_kli	\( (C_{HL}^{(1)})_{kk}, \mbox{Re}\big[(C_{HL}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(1)})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^j\big)\), for \(i,j=1,2,3\).
CHl3_kk, CHl3_klr, CHl3_kli	\( (C_{HL}^{(3)})_{kk}, \mbox{Re}\big[(C_{HL}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(3)})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \sigma^a L^j\big)\), for \(i,j=1,2,3\).
CHe_kk, CHe_klr, CHe_kli	\( (C_{He})_{kk}, \mbox{Re}\big[(C_{He})_{kl}\big], \mbox{Im}\big[(C_{He})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^j\big)\), for \(i,j=1,2,3\).
CHq1_kk, CHq1_klr, CHq1_kli	\( (C_{HQ}^{(1)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(1)})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^j\big)\), for \(i,j=1,2,3\).
CHq3_kk, CHq3_klr, CHq3_kli	\( (C_{HQ}^{(3)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(3)})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \sigma^a Q^j\big)\), for \(i,j=1,2,3\).
CHu_kk, CHu_klr, CHu_kli	\( (C_{Hu})_{kk}, \mbox{Re}\big[(C_{Hu})_{kl}\big], \mbox{Im}\big[(C_{Hu})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hu})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^j\big)\), for \(i,j=1,2,3\).
CHd_kk, CHd_klr, CHd_kli	\( (C_{Hd})_{kk}, \mbox{Re}\big[(C_{Hd})_{kl}\big], \mbox{Im}\big[(C_{Hd})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hd})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\).
CHud_klr, CHud_kli	\(\mbox{Re}\big[(C_{Hud})_{kl}\big], \mbox{Im}\big[(C_{Hud})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ij} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\).
CeH_klr, CeH_kli	\(\mbox{Re}\big[(C_{eH})_{kl}\big], \mbox{Im}\big[(C_{eH})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{ij} =\big(H^\dagger H\big) \big(\overline{L^i}\,H E^j\big)\), for \(i,j=1,2,3\).
CuH_klr, CuH_kli	\(\mbox{Re}\big[(C_{uH})_{kl}\big], \mbox{Im}\big[(C_{uH})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,\widetilde{H} U^j\big)\), for \(i,j=1,2,3\).
CdH_klr, CdH_kli	\(\mbox{Re}\big[(C_{dH})_{kl}\big], \mbox{Im}\big[(C_{dH})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,H D^j\big)\), for \(i,j=1,2,3\).
CuG_klr, CuG_kli	\(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\).
CuW_klr, CuW_kli	\(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\).
CuB_klr, CuB_kli	\(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\).
CdG_klr, CdG_kli	\(\mbox{Re}\big[(C_{dG})_{kl}\big], \mbox{Im}\big[(C_{dG})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A D^j\big)H G_{\mu\nu}^A\), for \(i,j=1,2,3\).
CdW_klr, CdW_kli	\(\mbox{Re}\big[(C_{dW})_{kl}\big], \mbox{Im}\big[(C_{dW})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a D^j\big)H W_{\mu\nu}^a\), for \(i,j=1,2,3\).
CdB_klr, CdB_kli	\(\mbox{Re}\big[(C_{dB})_{kl}\big], \mbox{Im}\big[(C_{dB})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} D^j\big)H B_{\mu\nu}\), for \(i,j=1,2,3\).
CeW_klr, CeW_kli	\(\mbox{Re}\big[(C_{eW})_{kl}\big], \mbox{Im}\big[(C_{eW})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eW})_{ij} =\big(\overline{L^i}\sigma^{\mu\nu} \sigma_a E^j\big)H W_{\mu\nu}^a\), for \(i,j=1,2,3\).
CeB_klr, CeB_kli	\(\mbox{Re}\big[(C_{eB})_{kl}\big], \mbox{Im}\big[(C_{eB})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eB})_{ij} =\big(\overline{L^i}\sigma^{\mu\nu} E^j\big)H B_{\mu\nu}\), for \(i,j=1,2,3\).
Cll_1221, Cll_2112	\((C_{LL})_{1221,2112}\)	The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\).
Clq1	\(C_{LQ}^{(1)}\)	The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\).
Clq3	\(C_{LQ}^{(3)}\)	The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \sigma_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\).
Cee	\(C_{EE}\)	The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Ceu	\(C_{EU}\)	The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
Ced	\(C_{ED}\)	The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
Cle	\(C_{LE}\)	The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Clu	\(C_{LU}\)	The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
Cld	\(C_{LD}\)	The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
Cqe	\(C_{QE}\)	The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Cqq1_1133, Cqq1_1331, Cqq1_3333	\(C_{QQ}^{(1)}\)	The coefficient of the operator \(({\cal O}_{QQ}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\).
Cqq3_1133, Cqq3_1331, Cqq3_3333	\(C_{QQ}^{(3)}\)	The coefficient of the operator \(({\cal O}_{QQ}^{(3)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu \sigma_a Q^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\).
Cuu_1133, Cuu_1331, Cuu_3333	\(C_{uu}\)	The coefficient of the operator \(({\cal O}_{uu})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu u^j\big) \big(\overline{u^k}\,\gamma_\mu u^l\big)\).
Cud1_3311, Cud1_3333	\(C_{ud}^{(1)}\)	The coefficient of the operator \(({\cal O}_{ud}^{(1)})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu u^j\big) \big(\overline{d^k}\,\gamma_\mu d^l\big)\).
Cud8_3311, Cud8_3333	\(C_{ud}^{(8)}\)	The coefficient of the operator \(({\cal O}_{ud}^{(8)})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu T^A u^j\big) \big(\overline{d^k}\,\gamma_\mu T^A d^l\big)\).
Cqu1_1133, Cqu1_3311, Cqu1_3333	\(C_{Qu}^{(1)}\)	The coefficient of the operator \(({\cal O}_{Qu}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{u^k}\,\gamma_\mu u^l\big)\).
Cqu8_1133, Cqu8_3311, Cqu8_3333	\(C_{Qu}^{(8)}\)	The coefficient of the operator \(({\cal O}_{Qu}^{(8)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu T^A Q^j\big) \big(\overline{u^k}\,\gamma_\mu T^A u^l\big)\).
Cqd1_3311, Cqd1_3333	\(C_{Qd}^{(1)}\)	The coefficient of the operator \(({\cal O}_{Qd}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{d^k}\,\gamma_\mu d^l\big)\).
Cqd8_3311, Cqd8_3333	\(C_{Qd}^{(8)}\)	The coefficient of the operator \(({\cal O}_{Qd}^{(8)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu T^A Q^j\big) \big(\overline{d^k}\,\gamma_\mu T^A d^l\big)\).
Cquqd1_3333	\(C_{QuQd}^{(1)}\)	The coefficient of the operator \(({\cal O}_{QuQd}^{(1)})_{ijkl}=\big(\overline{Q^i}\, u^j\big) i\sigma_2 \big(\overline{Q^k}^T\, d^l\big)\).
Cquqd8_3333	\(C_{QuQd}^{(8)}\)	The coefficient of the operator \(({\cal O}_{QuQd}^{(8)})_{ijkl}=\big(\overline{Q^i}\, T^A u^j\big) i\sigma_2 \big(\overline{Q^k}^T\, T^A d^l\big)\).
Lambda_NP	\(\Lambda \)	The new physics scale.
BrHinv	Br \((H\to invisible)\)	The branching ratio of invisible Higgs decays. Only the absolute value of this parameter is considered.(Not part of the EFT. Only for tests.)
BrHexo	Br \((H\to exotic)\)	The branching ratio of exotic Higgs decays. Only the absolute value of this parameter is considered. (Not part of the EFT. Only for tests.)
dg1Z	\(\delta g_{1Z}\)	Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)
dKappaga	\(\delta \kappa_{\gamma}\)	Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)
lambZ	\(\lambda_{Z}\)	Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)

[in]	dOSMdalpha	the derivative with respect to \(\alpha\) of the SM tree-level prediction of \(O\) (in the \(\alpha\) scheme)
[in]	mu	the RG scale associated to the observable

[in]	dOSMdMW	the derivative with respect to \(M_W\) of the SM tree-level prediction of \(O\) (in the \(M_W\) scheme)
[in]	mu	the RG scale associated to the observable

Detailed Description

Initialization

Model parameters

Model flags

Important member functions

Public Member Functions

Static Public Attributes

Additional Inherited Members

Constructor & Destructor Documentation

◆ NPSMEFTd6General()

Member Function Documentation

◆ A_f()

◆ AFB()

◆ alphaMz()

◆ aPskPol()

◆ bPskPol()

◆ Br_H_exo()

◆ Br_H_inv()

◆ Br_H_inv_NP()

◆ BrH2d2dRatio()

◆ BrH2e2muRatio()

◆ BrH2e2vRatio()

◆ BrH2evRatio()

◆ BrH2L2dRatio()

◆ BrH2L2LRatio()

◆ BrH2L2uRatio()

◆ BrH2L2v2Ratio()

◆ BrH2L2vRatio()

◆ BrH2l2vRatio()

◆ BrH2Lv2Ratio()

◆ BrH2LvRatio()

◆ BrH2mu2vRatio()

◆ BrH2muvRatio()

◆ BrH2u2dRatio()

◆ BrH2u2uRatio()

◆ BrH2udRatio()

◆ BrH2v2dRatio()

◆ BrH2v2uRatio()

◆ BrH2v2vRatio()

◆ BrH4dRatio()

◆ BrH4eRatio()

◆ BrH4fCCRatio()

◆ BrH4fNCRatio()

◆ BrH4fRatio()

◆ BrH4L2Ratio()

◆ BrH4LRatio()

◆ BrH4lRatio()

◆ BrH4muRatio()

◆ BrH4uRatio()

◆ BrH4vRatio()

◆ BrHbbRatio()

◆ BrHccRatio()

◆ BrHevmuvRatio()

◆ BrHgagaRatio()

◆ BrHggRatio()

◆ BrHll_vvorjjRatio()

◆ BrHlv_lvorjjRatio()

◆ BrHlvjjRatio()

◆ BrHLvudRatio()

◆ BrHLvvLRatio()

◆ BrHmumuRatio()

◆ BrHssRatio()

◆ BrHtautauRatio()

◆ BrHtoinvRatio()

◆ BrHudduRatio()

◆ BrHvisRatio()

◆ BrHVVRatio()

◆ BrHWffRatio()

◆ BrHWjjRatio()

◆ BrHWlvRatio()

◆ BrHWW2l2vRatio()

◆ BrHWW4fRatio()

◆ BrHWW4jRatio()

◆ BrHWWRatio()

◆ BrHZddRatio()

◆ BrHZffRatio()

◆ BrHZgaeeRatio()

◆ BrHZgallRatio()

◆ BrHZgamumuRatio()

◆ BrHZgaRatio()