The auxiliary base model class for other model classes. More...

#include <NPbase.h>

Inheritance diagram for NPbase:

Detailed Description

The auxiliary base model class for other model classes.

Author: HEPfit Collaboration

Copyright: GNU General Public License

This is an auxiliary Model class containing the basic structure to compute new physics (NP) contributions to the electroweak precision observables. The NP contributions are described by the following quantities:

$\Delta G$ (with DeltaGF()),
$S$, $T$ and $U$ (with obliqueS(), obliqueT() and obliqueU()),

Using these quantities, the mass and width of the $W$ boson and the NP contributions to the effective vector and axial-vector couplings of the $Z$-boson to leptons and quarks are computed:

$M_W$, $c_W^2$ and $s_W^2$ (with Mw(), cW2() and sW2()),
$\Gamma_W$ (with GammaW()),
$\delta g_V^f$ (with deltaGVl() and deltaGVq()),
$\delta g_A^f$ (with deltaGAl() and deltaGAq()).

In the model classes that are inherited from the current class (see the inheritance diagram above), some of these methods are reimplemented to account for the details of more specific scenarios.

Initialization

This class is intended to be used with an inherited model class.

Model parameters

There is no model parameter in the current class.

Model flags

There is no model flag in the current class.

Important member functions

The functions are explained above.

Definition at line 66 of file NPbase.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, $\mathcal{A}_f$. More...

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, $A^f_{FB}$. More...

virtual const double	alphaMz () const
	The electromagnetic coupling at the $Z$-mass scale, $\alpha(M_Z^2)=\alpha/(1-\Delta\alpha(M_Z^2))$. More...

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]). More...

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]). More...

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

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

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

virtual const double	BR_Zf (const Particle f) const
	The Branching ratio of the $Z$ boson into a given fermion pair, $BR_Z^{f}$. More...

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

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

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

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

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

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

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

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

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

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

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

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

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

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

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

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

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. More...

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. More...

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. More...

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

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

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

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

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

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. More...

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

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

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

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

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

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

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

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

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

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

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

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. More...

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. More...

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. More...

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

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

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

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. More...

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. More...

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. More...

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. More...

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. More...

virtual const double	cbminuscc () const

virtual const double	cbminusctau () const

virtual const double	ccminusctau () const

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

virtual const double	cgaga_HB (const double mu) const
	The Higgs-basis coupling $c_{\gamma\gamma}$. (See LHCHXSWG-INT-2015-001 document.) More...

virtual const double	cgaplusct () const

virtual const double	cgg_HB (const double mu) const
	The Higgs-basis coupling $c_{gg}$. (See LHCHXSWG-INT-2015-001 document.) More...

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.) More...

virtual const double	cgminuscga () const

virtual const double	cgplusct () const

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

virtual const double	cVpluscb () const

virtual const double	cVplusctau () const

virtual const double	cZBox_HB (const double mu) const
	The Higgs-basis coupling $c_{z\Box}$. (See LHCHXSWG-INT-2015-001 document.) More...

virtual const double	cZga_HB (const double mu) const
	The Higgs-basis coupling $c_{z\gamma}$. (See LHCHXSWG-INT-2015-001 document.) More...

virtual const double	cZZ_HB (const double mu) const
	The Higgs-basis coupling $c_{zz}$. (See LHCHXSWG-INT-2015-001 document.) More...

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

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. More...

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. More...

virtual const double	delta_mubbH_1 (const double sqrt_s) const

virtual const double	delta_mubbH_2 (const double sqrt_s) const

virtual const double	delta_muggH_1 (const double sqrt_s) const

virtual const double	delta_muggH_2 (const double sqrt_s) const

virtual const double	delta_mutH_1 (const double sqrt_s) const

virtual const double	delta_mutH_2 (const double sqrt_s) const

virtual const double	delta_muttH_1 (const double sqrt_s) const

virtual const double	delta_muttH_2 (const double sqrt_s) const

virtual const double	delta_muVBF_1 (const double sqrt_s) const

virtual const double	delta_muVBF_2 (const double sqrt_s) const

virtual const double	delta_muVH_1 (const double sqrt_s) const

virtual const double	delta_muVH_2 (const double sqrt_s) const

virtual const double	delta_muWH_1 (const double sqrt_s) const

virtual const double	delta_muWH_2 (const double sqrt_s) const

virtual const double	delta_muZH_1 (const double sqrt_s) const

virtual const double	delta_muZH_2 (const double sqrt_s) const

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, $\delta \mathcal{A}_f$. More...

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, $\Delta \mathcal{A}_f^{(2)}$. More...

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, $\delta A^f_{FB}$. More...

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, $\Delta A^f_{FB}$. More...

virtual const double	deltacZ_HB (const double mu) const
	The Higgs-basis coupling $\delta c_z$. (See LHCHXSWG-INT-2015-001 document.) More...

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]. More...

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

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

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

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

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

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. More...

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. More...

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

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

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

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

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]. More...

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

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

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

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

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

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

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

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

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

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

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

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

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. More...

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. More...

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

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

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

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

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. More...

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. More...

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

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. More...

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

virtual const double	deltaGA_f_2 (const Particle f) const

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

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, $\delta \Gamma_Z^{f}$. More...

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

virtual const double	deltaGamma_Z_2 () const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the total decay width of the $Z$ boson, $\Delta \Gamma_Z^{(2)}$. More...

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, $\delta \Gamma_Z^{f}$. More...

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, $\Delta \Gamma_{Z,f}^{(2)}$. More...

virtual const double	deltaGamma_Zhad () const
	The new physics contribution to the hadronic decay width of the $Z$ boson, $\delta \Gamma_{Z,had}$. More...

virtual const double	deltaGamma_Zhad_2 () const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the hadronic decay width of the $Z$ boson, $\Delta \Gamma_{Z,had}^{(2)}$. More...

virtual const double	deltaGammaHbbRatio1 () const

virtual const double	deltaGammaHbbRatio2 () const

virtual const double	deltaGammaHccRatio1 () const

virtual const double	deltaGammaHccRatio2 () const

virtual const double	deltaGammaHgagaRatio1 () const

virtual const double	deltaGammaHgagaRatio2 () const

virtual const double	deltaGammaHggRatio1 () const

virtual const double	deltaGammaHggRatio2 () const

virtual const double	deltaGammaHmumuRatio1 () const

virtual const double	deltaGammaHmumuRatio2 () const

virtual const double	deltaGammaHtautauRatio1 () const

virtual const double	deltaGammaHtautauRatio2 () const

virtual const double	deltaGammaHWWRatio1 () const

virtual const double	deltaGammaHWWRatio2 () const

virtual const double	deltaGammaHZgaRatio1 () const

virtual const double	deltaGammaHZgaRatio2 () const

virtual const double	deltaGammaHZZRatio1 () const

virtual const double	deltaGammaHZZRatio2 () const

virtual const double	deltaGammaTotalRatio1 () const

virtual const double	deltaGammaTotalRatio2 () const

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

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

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

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

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

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

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

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

virtual const double	deltaGV_f_2 (const Particle f) const

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

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]. More...

virtual const double	deltaN_nu () const
	The new physics contribution to the number of neutrinos dervied from the $Z$ pole measurements. More...

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. More...

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: More...

virtual const double	deltaR_inv () const
	The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the $Z$ boson, $\delta R_{inv}$. More...

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: More...

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: More...

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, $\delta \sigma_h^0$. More...

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, $\Delta \sigma_h^{0,(2)}$. More...

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. More...

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. More...

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. More...

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. More...

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]. More...

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. More...

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. More...

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. More...

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]. More...

virtual const double	deltayb_HB (const double mu) const
	The Higgs-basis coupling $\delta y_b$. (See LHCHXSWG-INT-2015-001 document.) More...

virtual const double	deltayc_HB (const double mu) const
	The Higgs-basis coupling $\delta y_c$. (See LHCHXSWG-INT-2015-001 document.) More...

virtual const double	deltaymu_HB (const double mu) const
	The Higgs-basis coupling $\delta y_\mu$. (See LHCHXSWG-INT-2015-001 document.) More...

virtual const double	deltays_HB (const double mu) const
	The Higgs-basis coupling $\delta y_s$. (See LHCHXSWG-INT-2015-001 document.) More...

virtual const double	deltayt_HB (const double mu) const
	The Higgs-basis coupling $\delta y_t$. (See LHCHXSWG-INT-2015-001 document.) More...

virtual const double	deltaytau_HB (const double mu) const
	The Higgs-basis coupling $\delta y_\tau$. (See LHCHXSWG-INT-2015-001 document.) More...

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]. Defined only for the NPSMEFTd6 class. More...

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. More...

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. More...

virtual const gslpp::complex	gA_f (const Particle f) const
	The total (SM+NP) contribution to the neutral-current axial-vector coupling $g_A^f$. More...

virtual const double	Gamma_had () const
	The hadronic decay width of the $Z$ boson, $\Gamma_{Z,had}$. More...

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

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

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

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

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

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

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

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

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

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

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

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

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

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. More...

virtual const StandardModel &	getTrueSM () const
	A method to return a StandardModel object from NPbase. More...

virtual const gslpp::complex	gV_f (const Particle f) const
	The total (SM+NP) contribution to the neutral-current vector coupling $g_V^f$. More...

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

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

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

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

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

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

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

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

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

virtual const gslpp::complex	kappaZ_f (const Particle f) const
	The effective neutral-current coupling $\kappa_Z^f$ including SM plus NP contributions. More...

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

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

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

virtual const double	lambz_HB (const double mu) const
	The Higgs-basis coupling $\lambda_{z}$. (See LHCHXSWG-INT-2015-001 document.) More...

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

virtual const double	muggHbb (const double sqrt_s) const

virtual const double	muggHgaga (const double sqrt_s) const

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. More...

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. More...

virtual const double	muggHmumu (const double sqrt_s) const

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	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. More...

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	muggHtautau (const double sqrt_s) const

virtual const double	muggHWW (const double sqrt_s) const

virtual const double	muggHWW2l2v (const double sqrt_s) const

virtual const double	muggHZga (const double sqrt_s) const

virtual const double	muggHZZ (const double sqrt_s) const

virtual const double	muggHZZ4l (const double sqrt_s) const

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

virtual const double	muppHmumu (const double sqrt_s) const

virtual const double	muppHZga (const double sqrt_s) const

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 NPSMEFTd6 class. More...

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. More...

virtual const double	mutHgaga (const double sqrt_s) const

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. More...

virtual const double	muTHUggHbb (const double sqrt_s) const

virtual const double	muTHUggHgaga (const double sqrt_s) const

virtual const double	muTHUggHmumu (const double sqrt_s) const

virtual const double	muTHUggHtautau (const double sqrt_s) const

virtual const double	muTHUggHWW (const double sqrt_s) const

virtual const double	muTHUggHWW2l2v (const double sqrt_s) const

virtual const double	muTHUggHZga (const double sqrt_s) const

virtual const double	muTHUggHZgamumu (const double sqrt_s) const

virtual const double	muTHUggHZZ (const double sqrt_s) const

virtual const double	muTHUggHZZ4l (const double sqrt_s) const

virtual const double	muTHUggHZZ4mu (const double sqrt_s) const

virtual const double	muTHUttHbb (const double sqrt_s) const

virtual const double	muTHUttHgaga (const double sqrt_s) const

virtual const double	muTHUttHmumu (const double sqrt_s) const

virtual const double	muTHUttHtautau (const double sqrt_s) const

virtual const double	muTHUttHWW (const double sqrt_s) const

virtual const double	muTHUttHWW2l2v (const double sqrt_s) const

virtual const double	muTHUttHZga (const double sqrt_s) const

virtual const double	muTHUttHZZ (const double sqrt_s) const

virtual const double	muTHUttHZZ4l (const double sqrt_s) const

virtual const double	muTHUVBFBRinv (const double sqrt_s) const

virtual const double	muTHUVBFHbb (const double sqrt_s) const

virtual const double	muTHUVBFHgaga (const double sqrt_s) const

virtual const double	muTHUVBFHinv (const double sqrt_s) const

virtual const double	muTHUVBFHmumu (const double sqrt_s) const

virtual const double	muTHUVBFHtautau (const double sqrt_s) const

virtual const double	muTHUVBFHWW (const double sqrt_s) const

virtual const double	muTHUVBFHWW2l2v (const double sqrt_s) const

virtual const double	muTHUVBFHZga (const double sqrt_s) const

virtual const double	muTHUVBFHZZ (const double sqrt_s) const

virtual const double	muTHUVBFHZZ4l (const double sqrt_s) const

virtual const double	muTHUVHbb (const double sqrt_s) const

virtual const double	muTHUVHBRinv (const double sqrt_s) const

virtual const double	muTHUVHgaga (const double sqrt_s) const

virtual const double	muTHUVHinv (const double sqrt_s) const

virtual const double	muTHUVHmumu (const double sqrt_s) const

virtual const double	muTHUVHtautau (const double sqrt_s) const

virtual const double	muTHUVHWW (const double sqrt_s) const

virtual const double	muTHUVHWW2l2v (const double sqrt_s) const

virtual const double	muTHUVHZga (const double sqrt_s) const

virtual const double	muTHUVHZZ (const double sqrt_s) const

virtual const double	muTHUVHZZ4l (const double sqrt_s) const

virtual const double	muTHUWHbb (const double sqrt_s) const

virtual const double	muTHUWHgaga (const double sqrt_s) const

virtual const double	muTHUWHmumu (const double sqrt_s) const

virtual const double	muTHUWHtautau (const double sqrt_s) const

virtual const double	muTHUWHWW (const double sqrt_s) const

virtual const double	muTHUWHWW2l2v (const double sqrt_s) const

virtual const double	muTHUWHZga (const double sqrt_s) const

virtual const double	muTHUWHZZ (const double sqrt_s) const

virtual const double	muTHUWHZZ4l (const double sqrt_s) const

virtual const double	muTHUZHbb (const double sqrt_s) const

virtual const double	muTHUZHgaga (const double sqrt_s) const

virtual const double	muTHUZHmumu (const double sqrt_s) const

virtual const double	muTHUZHtautau (const double sqrt_s) const

virtual const double	muTHUZHWW (const double sqrt_s) const

virtual const double	muTHUZHWW2l2v (const double sqrt_s) const

virtual const double	muTHUZHZga (const double sqrt_s) const

virtual const double	muTHUZHZZ (const double sqrt_s) const

virtual const double	muTHUZHZZ4l (const double sqrt_s) const

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. More...

virtual const double	muttHbb (const double sqrt_s) const

virtual const double	muttHgaga (const double sqrt_s) const

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. More...

virtual const double	muttHmumu (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	muttHtautau (const double sqrt_s) const

virtual const double	muttHWW (const double sqrt_s) const

virtual const double	muttHWW2l2v (const double sqrt_s) const

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. More...

virtual const double	muttHZga (const double sqrt_s) const

virtual const double	muttHZZ (const double sqrt_s) const

virtual const double	muttHZZ4l (const double sqrt_s) const

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. More...

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. More...

virtual const double	muVBFHbb (const double sqrt_s) const

virtual const double	muVBFHgaga (const double sqrt_s) const

virtual const double	muVBFHmumu (const double sqrt_s) const

virtual const double	muVBFHtautau (const double sqrt_s) const

virtual const double	muVBFHWW (const double sqrt_s) const

virtual const double	muVBFHWW2l2v (const double sqrt_s) const

virtual const double	muVBFHZga (const double sqrt_s) const

virtual const double	muVBFHZZ (const double sqrt_s) const

virtual const double	muVBFHZZ4l (const double sqrt_s) const

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. More...

virtual const double	muVBFpVH_Hmumu (const double sqrt_s) const

virtual const double	muVBFpVH_HZga (const double sqrt_s) const

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. More...

virtual const double	muVHbb (const double sqrt_s) const

virtual const double	muVHcc (const double sqrt_s) const

virtual const double	muVHgaga (const double sqrt_s) const

virtual const double	muVHmumu (const double sqrt_s) const

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. More...

virtual const double	muVHtautau (const double sqrt_s) const

virtual const double	muVHWW (const double sqrt_s) const

virtual const double	muVHWW2l2v (const double sqrt_s) const

virtual const double	muVHZga (const double sqrt_s) const

virtual const double	muVHZZ (const double sqrt_s) const

virtual const double	muVHZZ4l (const double sqrt_s) const

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. More...

virtual const double	muWHbb (const double sqrt_s) const

virtual const double	muWHgaga (const double sqrt_s) const

virtual const double	muWHmumu (const double sqrt_s) const

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. More...

virtual const double	muWHtautau (const double sqrt_s) const

virtual const double	muWHWW (const double sqrt_s) const

virtual const double	muWHWW2l2v (const double sqrt_s) const

virtual const double	muWHZga (const double sqrt_s) const

virtual const double	muWHZZ (const double sqrt_s) const

virtual const double	muWHZZ4l (const double sqrt_s) const

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. More...

virtual const double	muZHbb (const double sqrt_s) const

virtual const double	muZHgaga (const double sqrt_s) const

virtual const double	muZHmumu (const double sqrt_s) const

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. More...

virtual const double	muZHtautau (const double sqrt_s) const

virtual const double	muZHWW (const double sqrt_s) const

virtual const double	muZHWW2l2v (const double sqrt_s) const

virtual const double	muZHZga (const double sqrt_s) const

virtual const double	muZHZZ (const double sqrt_s) const

virtual const double	muZHZZ4l (const double sqrt_s) const

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

virtual const double	N_nu () const
	The number of neutrinos dervied from the $Z$ pole measurements, $N_{\nu}$. More...

	NPbase ()
	The default constructor. More...

virtual const double	obliqueS () const
	The oblique parameter $S$. More...

virtual const double	obliqueT () const
	The oblique parameter $T$. More...

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

virtual const double	obliqueW () const
	The oblique parameter $W$. More...

virtual const double	obliqueY () const
	The oblique parameter $Y$. More...

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 NPSMEFTd6 class. More...

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. More...

virtual const double	R_inv () const
	The ratio of the invisible and leptonic (electron) decay widths of the $Z$ boson, $R_{inv}$. More...

virtual const gslpp::complex	rhoZ_f (const Particle f) const
	The effective neutral-current coupling $\rho_Z^f$ including SM plus NP contributions. More...

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. More...

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

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

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

virtual bool	setFlag (const std::string name, const bool value)
	A method to set a flag of NPbase. More...

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

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. More...

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

virtual const double	STXS12_ggH_pTH10_200_Nj0 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j = 0, 10<~p_{TH} [GeV]<200$. More...

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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. More...

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

virtual const double	STXS_ttHtH (const double sqrt_s) const
	The STXS bin $ ttH + tH $. More...

virtual const double	STXS_WHqqHqq_pTj1_200 (const double sqrt_s) const
	The STXS bin $ qq \to WH \to H qq $. More...

virtual const double	STXS_WHqqHqq_Rest (const double sqrt_s) const
	The STXS bin $ qq \to WH \to H qq $. More...

virtual const double	STXS_WHqqHqq_VBFtopo_j3 (const double sqrt_s) const
	The STXS bin $ qq \to WH \to H qq $. More...

virtual const double	STXS_WHqqHqq_VBFtopo_j3v (const double sqrt_s) const
	The STXS bin $ qq \to WH \to H qq $. More...

virtual const double	STXS_WHqqHqq_VH2j (const double sqrt_s) const
	The STXS bin $ qq \to WH \to H qq $. More...

virtual const double	STXS_ZHqqHqq_pTj1_200 (const double sqrt_s) const
	The STXS bin $ qq \to ZH \to H qq $. More...

virtual const double	STXS_ZHqqHqq_Rest (const double sqrt_s) const
	The STXS bin $ qq \to ZH \to H qq $. More...

virtual const double	STXS_ZHqqHqq_VBFtopo_j3 (const double sqrt_s) const
	The STXS bin $ qq \to ZH \to H qq $. More...

virtual const double	STXS_ZHqqHqq_VBFtopo_j3v (const double sqrt_s) const
	The STXS bin $ qq \to ZH \to H qq $. More...

virtual const double	STXS_ZHqqHqq_VH2j (const double sqrt_s) const
	The STXS bin $ qq \to ZH \to H qq $. More...

virtual bool	Update (const std::map< std::string, double > &DPars)
	The update method for NPbase. More...

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	xseeWW (const double sqrt_s) const
	Total $e^+ e^- \to W^+ W^- \to jj \ell \nu$ cross section in pb, with $\ell= e, \mu$. More...

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]. Defined only for the NPSMEFTd6 class. More...

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. More...

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. More...

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. More...

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]. Defined only for the NPSMEFTd6 class. More...

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. More...

gslpp::complex	AH_W (const double tau) const
	W loop function entering in the calculation of the effective $H\gamma\gamma$ coupling. More...

gslpp::complex	AHZga_f (const double tau, const double lambda) const
	Fermionic loop function entering in the calculation of the effective $HZ\gamma$ coupling. More...

gslpp::complex	AHZga_W (const double tau, const double lambda) const
	W loop function entering in the calculation of the effective $HZ\gamma$ coupling. More...

const double	Ale (double mu, orders order, bool Nf_thr=true) const
	The running electromagnetic coupling $\alpha_e(\mu)$ in the $\overline{MS}$ scheme. More...

const double	ale_OS (const double mu, orders order=FULLNLO) const
	The running electromagnetic coupling $\alpha(\mu)$ in the on-shell scheme. More...

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

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(). More...

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. More...

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. More...

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

const double	Beta_e (int nm, unsigned int nf) const
	QED beta function coefficients - eq. (36) hep-ph/0512066. More...

const double	Beta_s (int nm, unsigned int nf) const
	QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066. More...

virtual const double	BrHtobb () const
	The Br $(H\to b \bar{b})$ in the Standard Model. More...

virtual const double	BrHtocc () const
	The Br $(H\to c \bar{c})$ in the Standard Model. More...

virtual const double	BrHtogaga () const
	The Br $(H\to \gamma \gamma)$ in the Standard Model. More...

virtual const double	BrHtogg () const
	The Br $\(H\to gg)$ in the Standard Model. More...

virtual const double	BrHtomumu () const
	The Br $(H\to \mu^+ \mu^-)$ in the Standard Model. More...

virtual const double	BrHtoss () const
	The Br $(H\to s \bar{s})$ in the Standard Model. More...

virtual const double	BrHtotautau () const
	The Br $(H\to \tau^+ \tau^-)$ in the Standard Model. More...

virtual const double	BrHtoWWstar () const
	The Br $(H\to W W^*)$ in the Standard Model. More...

virtual const double	BrHtoZga () const
	The Br $(H\to Z \gamma)$ in the Standard Model. More...

virtual const double	BrHtoZZstar () const
	The Br $(H\to Z Z^*)$ in the Standard Model. More...

const double	c02 () const
	The square of the cosine of the weak mixing angle $c_0^2$ defined without weak radiative corrections. More...

virtual bool	CheckFlags () const
	A method to check the sanity of the set of model flags. More...

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. More...

bool	checkSMparamsForEWPO ()
	A method to check whether the parameters relevant to the EWPO are updated. More...

const double	computeBrHto4f () const
	The Br $(H\to 4f)$ in the Standard Model. More...

const double	computeBrHto4l2 () const
	The Br $(H\to 4l)$ $l=e,\mu$ in the Standard Model. More...

const double	computeBrHto4l3 () const
	The Br $(H\to 4l)$ $l=e,\mu,\tau$ in the Standard Model. More...

const double	computeBrHto4q () const
	The Br $(H\to 4q)$ in the Standard Model. More...

const double	computeBrHto4v () const
	The Br $(H\to 4\nu)$ in the Standard Model. More...

const double	computeBrHtobb () const
	The Br $(H\to bb)$ in the Standard Model. More...

const double	computeBrHtocc () const
	The Br $(H\to cc)$ in the Standard Model. More...

const double	computeBrHtoevmuv () const
	The Br $(H\to e \nu \mu \nu)$ in the Standard Model. More...

const double	computeBrHtogaga () const
	The Br $(H\to\gamma\gamma)$ in the Standard Model. More...

const double	computeBrHtogg () const
	The Br $(H\to gg)$ in the Standard Model. More...

const double	computeBrHtollvv2 () const
	The Br $(H\to l^+ l^- \nu \nu)$ $l=e,\mu$ in the Standard Model. More...

const double	computeBrHtollvv3 () const
	The Br $(H\to l^+ l^- \nu \nu)$ $l=e,\mu,\tau$ in the Standard Model. More...

const double	computeBrHtomumu () const
	The Br $(H\to \mu\mu)$ in the Standard Model. More...

const double	computeBrHtoss () const
	The Br $(H\to ss)$ in the Standard Model. More...

const double	computeBrHtotautau () const
	The Br $(H\to \tau\tau)$ in the Standard Model. More...

const double	computeBrHtoWW () const
	The Br $(H\to WW)$ in the Standard Model. More...

const double	computeBrHtoZga () const
	The Br $(H\to Z\gamma)$ in the Standard Model. More...

const double	computeBrHtoZZ () const
	The Br $(H\to ZZ)$ in the Standard Model. More...

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. More...

void	ComputeDeltaRho (const double Mw_i, double DeltaRho[orders_EW_size]) const
	A method to collect $\Delta\rho$ computed via subclasses. More...

const double	computeGammaHgaga_tt () const
	The top loop contribution to $H\to\gamma\gamma$ in the Standard Model. More...

const double	computeGammaHgaga_tW () const
	The mixed $t-W$ loop contribution to $H\to\gamma\gamma$ in the Standard Model. More...

const double	computeGammaHgaga_WW () const
	The $W$ loop contribution to $H\to\gamma\gamma$ in the Standard Model. More...

const double	computeGammaHgg_bb () const
	The bottom loop contribution to $H\to gg$ in the Standard Model. More...

const double	computeGammaHgg_tb () const
	The top-bottom interference contribution to $H\to gg$ in the Standard Model. More...

const double	computeGammaHgg_tt () const
	The top loop contribution to $H\to gg$ in the Standard Model. More...

const double	computeGammaHTotal () const
	The Higgs total width in the Standard Model. More...

const double	computeGammaHZga_tt () const
	The top loop contribution to $H\to Z\gamma$ in the Standard Model. More...

const double	computeGammaHZga_tW () const
	The mixed $t-W$ loop contribution to $H\to Z\gamma$ in the Standard Model. More...

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]. More...

const double	computeSigmabbH (const double sqrt_s) const
	The bbH production cross section in the Standard Model. More...

const double	computeSigmaggH (const double sqrt_s) const
	The ggH cross section in the Standard Model. More...

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. More...

const double	computeSigmaggH_tb (const double sqrt_s) const
	The top-bottom interference contribution to the ggH cross section in the Standard Model. More...

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. More...

const double	computeSigmatHq (const double sqrt_s) const
	The tHq production cross section in the Standard Model. More...

const double	computeSigmattH (const double sqrt_s) const
	The ttH production cross section in the Standard Model. More...

const double	computeSigmaVBF (const double sqrt_s) const
	The VBF cross section in the Standard Model. More...

const double	computeSigmaWF (const double sqrt_s) const
	The W fusion contribution $\sigma_{WF}$ to higgs-production cross section in the Standard Model. More...

const double	computeSigmaWH (const double sqrt_s) const
	The WH production cross section in the Standard Model. More...

const double	computeSigmaZF (const double sqrt_s) const
	The Z fusion contribution $\sigma_{ZF}$ to higgs-production cross section in the Standard Model. More...

const double	computeSigmaZH (const double sqrt_s) const
	The ZH production cross section in the Standard Model. More...

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. More...

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 $c_W^2$. More...

const double	DeltaAlpha () const
	The total corrections to the electromagnetic coupling $\alpha$ at the $Z$-mass scale, denoted as $\Delta\alpha(M_Z^2)$. More...

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 $\Delta\alpha^{\ell+5q}(M_Z^2)$. More...

const double	DeltaAlphaLepton (const double s) const
	Leptonic contribution to the electromagnetic coupling $\alpha$, denoted as $\Delta\alpha_{\mathrm{lept}}(s)$. More...

const double	DeltaAlphaTop (const double s) const
	Top-quark contribution to the electromagnetic coupling $\alpha$, denoted as $\Delta\alpha_{\mathrm{top}}(s)$. More...

virtual const gslpp::complex	deltaKappaZ_f (const Particle f) const
	Flavour non-universal vertex corrections to $\kappa_Z^l$, denoted by $\Delta\kappa_Z^l$. More...

virtual const double	DeltaR () const
	The SM prediction for $\Delta r$ derived from that for the $W$ boson mass. More...

virtual const double	DeltaRbar () const
	The SM prediction for $\Delta \overline{r}$ derived from that for the $W$-boson mass. More...

virtual const gslpp::complex	deltaRhoZ_f (const Particle f) const
	Flavour non-universal vertex corrections to $\rho_Z^l$, denoted by $\Delta\rho_Z^l$. More...

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 $\varepsilon_1$. More...

virtual const double	epsilon2 () const
	The SM contribution to the epsilon parameter $\varepsilon_2$. More...

virtual const double	epsilon3 () const
	The SM contribution to the epsilon parameter $\varepsilon_3$. More...

virtual const double	epsilonb () const
	The SM contribution to the epsilon parameter $\varepsilon_b$. More...

gslpp::complex	f_triangle (const double tau) const
	Loop function entering in the calculation of the effective $Hgg$ and $H\gamma\gamma$ couplings. More...

gslpp::complex	g_triangle (const double tau) const
	Loop function entering in the calculation of the effective $HZ\gamma$ coupling. More...

virtual const double	Gamma_inv () const
	The invisible partial decay width of the $Z$ boson, $\Gamma_{\mathrm{inv}}$. More...

virtual const double	Gamma_muon () const
	The computation of the muon decay. More...

virtual const double	Gamma_tau_l_nunu (const Particle l) const
	The computation of the leptonic tau decays. More...

virtual const double	GammaHtobb () const
	The $\Gamma(H\to b \bar{b})$ in the Standard Model. More...

virtual const double	GammaHtocc () const
	The $\Gamma(H\to c \bar{c})$ in the Standard Model. More...

virtual const double	GammaHtogaga () const
	The $\Gamma(H\to \gamma \gamma)$ in the Standard Model. More...

virtual const double	GammaHtogg () const
	The $\Gamma(H\to gg)$ in the Standard Model. More...

virtual const double	GammaHtomumu () const
	The $\Gamma(H\to \mu^+ \mu^-)$ in the Standard Model. More...

virtual const double	GammaHtoss () const
	The $\Gamma(H\to s \bar{s})$ in the Standard Model. More...

virtual const double	GammaHTot () const
	The total Higgs width $\Gamma(H)$ in the Standard Model. More...

virtual const double	GammaHtotautau () const
	The $\Gamma(H\to \tau^+ \tau^-)$ in the Standard Model. More...

virtual const double	GammaHtoWWstar () const
	The $\Gamma(H\to W W^*)$ in the Standard Model. More...

virtual const double	GammaHtoZga () const
	The $\Gamma(H\to Z \gamma)$ in the Standard Model. More...

virtual const double	GammaHtoZZstar () const
	The $\Gamma(H\to Z Z^*)$ in the Standard Model. More...

virtual const double	GammaZ (const Particle f) const
	The $Z\to \ell\bar{\ell}$ partial decay width, $\Gamma_\ell$. More...

virtual const double	gAnue () const
	The effective (muon) neutrino-electron axial-vector coupling: gAnue. More...

const double	getAle () const
	A get method to retrieve the fine-structure constant $\alpha$. More...

const double	getAlsMz () const
	A get method to access the value of $\alpha_s(M_Z)$. More...

virtual const double	getCBd () const
	The ratio of the absolute value of the $B_d$ mixing amplitude over the Standard Model value. More...

virtual const double	getCBs () const
	The ratio of the absolute value of the $B_s$ mixing amplitude over the Standard Model value. More...

virtual const double	getCCC1 () const
	A virtual implementation for the RealWeakEFTCC class. More...

virtual const double	getCCC2 () const
	A virtual implementation for the RealWeakEFTCC class. More...

virtual const double	getCCC3 () const
	A virtual implementation for the RealWeakEFTCC class. More...

virtual const double	getCCC4 () const
	A virtual implementation for the RealWeakEFTCC class. More...

virtual const double	getCCC5 () const
	A virtual implementation for the RealWeakEFTCC class. More...

virtual const double	getCDMK () const
	The ratio of the real part of the $K$ mixing amplitude over the Standard Model value. More...

virtual const double	getCepsK () const
	The ratio of the imaginary part of the $K$ mixing amplitude over the Standard Model value. More...

const CKM &	getCKM () const
	A get method to retrieve the member object of type CKM. More...

const double	getDAle5Mz () const
	A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, $\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)$. More...

const double	getDelGammaWlv () const
	A get method to retrieve the theoretical uncertainty in $\Gamma_W_{l\nu}$, denoted as $\delta\,\Gamma_W_{l\nu}$. More...

const double	getDelGammaWqq () const
	A get method to retrieve the theoretical uncertainty in $\Gamma_W_{qq}$, denoted as $\delta\,\Gamma_W_{qq}$. More...

const double	getDelGammaZ () const
	A get method to retrieve the theoretical uncertainty in $\Gamma_Z$, denoted as $\delta\,\Gamma_Z$. More...

const double	getDelMw () const
	A get method to retrieve the theoretical uncertainty in $M_W$, denoted as $\delta\,M_W$. More...

const double	getDelR0b () const
	A get method to retrieve the theoretical uncertainty in $R_b^0$, denoted as $\delta\,R_b^0$. More...

const double	getDelR0c () const
	A get method to retrieve the theoretical uncertainty in $R_c^0$, denoted as $\delta\,R_c^0$. More...

const double	getDelR0l () const
	A get method to retrieve the theoretical uncertainty in $R_l^0$, denoted as $\delta\,R_l^0$. More...

const double	getDelSigma0H () const
	A get method to retrieve the theoretical uncertainty in $\sigma_{Hadron}^0$, denoted as $\delta\,\sigma_{Hadron}^0$. More...

const double	getDelSin2th_b () const
	A get method to retrieve the theoretical uncertainty in $\sin^2\theta_{\rm eff}^{b}$, denoted as $\delta\sin^2\theta_{\rm eff}^{b}$. More...

const double	getDelSin2th_l () const
	A get method to retrieve the theoretical uncertainty in $\sin^2\theta_{\rm eff}^{\rm lept}$, denoted as $\delta\sin^2\theta_{\rm eff}^{\rm lept}$. More...

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 $\delta\sin^2\theta_{\rm eff}^{q\not = b,t}$. More...

const std::string	getFlagKappaZ () const
	A method to retrieve the model flag KappaZ. More...

const std::string	getFlagMw () const
	A method to retrieve the model flag Mw. More...

const std::string	getFlagRhoZ () const
	A method to retrieve the model flag RhoZ. More...

const Flavour &	getFlavour () const

const double	getGF () const
	A get method to retrieve the Fermi constant $G_\mu$. More...

const int	getIterationNo () const

const Particle &	getLeptons (const QCD::lepton p) const
	A get method to retrieve the member object of a lepton. More...

virtual StandardModelMatching &	getMatching () const
	A get method to access the member reference of type StandardModelMatching. More...

virtual const double	getMHl () const
	A get method to retrieve the Higgs mass $m_h$. More...

virtual const double	getmq (const QCD::quark q, const double mu) const
	The MSbar running quark mass computed at NLO. More...

const double	getMuw () const
	A get method to retrieve the matching scale $\mu_W$ around the weak scale. More...

const double	getMw () const
	A get method to access the input value of the mass of the $W$ boson $M_W$. More...

EWSMApproximateFormulae *	getMyApproximateFormulae () const
	A get method to retrieve the member pointer of type EWSMApproximateFormulae. More...

EWSMcache *	getMyEWSMcache () const
	A get method to retrieve the member pointer of type EWSMcache. More...

LeptonFlavour *	getMyLeptonFlavour () const

EWSMOneLoopEW *	getMyOneLoopEW () const
	A get method to retrieve the member pointer of type EWSMOneLoopEW,. More...

EWSMThreeLoopEW *	getMyThreeLoopEW () const

EWSMThreeLoopEW2QCD *	getMyThreeLoopEW2QCD () const

EWSMThreeLoopQCD *	getMyThreeLoopQCD () const

EWSMTwoFermionsLEP2 *	getMyTwoFermionsLEP2 () const
	A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More...

EWSMTwoLoopEW *	getMyTwoLoopEW () const

EWSMTwoLoopQCD *	getMyTwoLoopQCD () const

const double	getMz () const
	A get method to access the mass of the $Z$ boson $M_Z$. More...

virtual const double	getPhiBd () const
	Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More...

virtual const double	getPhiBs () const
	Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More...

const gslpp::matrix< gslpp::complex >	getUPMNS () const
	A get method to retrieve the object of the PMNS matrix. More...

const gslpp::matrix< gslpp::complex >	getVCKM () const
	A get method to retrieve the CKM matrix. More...

const gslpp::matrix< gslpp::complex > &	getYd () const
	A get method to retrieve the Yukawa matrix of the down-type quarks, $Y_d$. More...

const gslpp::matrix< gslpp::complex > &	getYe () const
	A get method to retrieve the Yukawa matrix of the charged leptons, $Y_e$. More...

const gslpp::matrix< gslpp::complex > &	getYn () const
	A get method to retrieve the Yukawa matrix of the neutrinos, $Y_\nu$. More...

const gslpp::matrix< gslpp::complex > &	getYu () const
	A get method to retrieve the Yukawa matrix of the up-type quarks, $Y_u$. More...

virtual const double	gLnuN2 () const
	The effective neutrino nucleon LH coupling: gLnuN2. More...

virtual const double	gRnuN2 () const
	The effective neutrino nucleon RH coupling: gRnuN2. More...

virtual const double	gVnue () const
	The effective (muon) neutrino-electron vector coupling: gVnue. More...

gslpp::complex	I_triangle_1 (const double tau, const double lambda) const
	Loop function entering in the calculation of the effective $HZ\gamma$ coupling. More...

gslpp::complex	I_triangle_2 (const double tau, const double lambda) const
	Loop function entering in the calculation of the effective $HZ\gamma$ coupling. More...

virtual bool	Init (const std::map< std::string, double > &DPars)
	A method to initialize the model parameters. More...

virtual bool	InitializeModel ()
	A method to initialize the model. More...

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. More...

const bool	IsFlagWithoutNonUniversalVC () const
	A method to retrieve the model flag WithoutNonUniversalVC. More...

const bool	isSMSuccess () const
	A get method to retrieve the success status of the Standard Model update and matching. More...

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, $M_W^{\mathrm{tree}}$. More...

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. More...

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. More...

double	Mzbar () const
	The $Z$-boson mass $\overline{M}_Z$ in the complex-pole/fixed-width scheme. More...

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

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

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

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

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

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 $\rho^W_{ij}$. More...

const double	s02 () const
	The square of the sine of the weak mixing angle $s_0^2$ defined without weak radiative corrections. More...

void	setCKM (const CKM &CKMMatrix)
	A set method to change the CKM matrix. More...

void	setFlagCacheInStandardModel (bool FlagCacheInStandardModel)
	A set method to change the model flag CacheInStandardModel of StandardModel. More...

void	setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ)

bool	setFlagSigmaForAFB (const bool flagSigmaForAFB_i)

bool	setFlagSigmaForR (const bool flagSigmaForR_i)

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

void	setRequireCKM (bool requireCKM)
	A set method to change the value of requireCKM. More...

void	setSMSuccess (bool success) const
	A set method to change the success status of the Standard Model update and matching. More...

void	setYd (const gslpp::matrix< gslpp::complex > &Yd)
	A set method to set the Yukawa matrix of the down-type quarks, $Y_d$. More...

void	setYe (const gslpp::matrix< gslpp::complex > &Ye)
	A set method to set the Yukawa matrix of the charged leptons, $Y_e$. More...

void	setYu (const gslpp::matrix< gslpp::complex > &Yu)
	A set method to set the Yukawa matrix of the up-type quarks, $Y_u$. More...

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. More...

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. More...

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. More...

	StandardModel ()
	The default constructor. More...

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 $s_W^2$. More...

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) More...

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) More...

virtual const double	TauLFU_gmuge () const
	The computation of the LFU ratio $g_\mu/ g_e $. More...

virtual const double	TauLFU_gtauge () const
	The computation of the LFU ratio $g_\tau/ g_e $. More...

virtual const double	TauLFU_gtaugmu () const
	The computation of the LFU ratio $g_\tau/ g_\mu $. More...

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

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

virtual const double	ThetaLnuN () const
	The effective neutrino nucleon LH parameter: ThetaLnuN. More...

virtual const double	ThetaRnuN () const
	The effective neutrino nucleon RH parameter: ThetaRnuN. More...

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. More...

virtual	~StandardModel ()
	The default destructor. More...

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(). More...

void	addParameters (std::vector< std::string > params_i)
	A method to add parameters that are specific to only one set of observables. More...

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(). More...

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 $n_f = 4$. More...

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(). More...

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 $\mu$. More...

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 $\Lambda_{\rm QCD}$. More...

const double	BelowTh (const double mu) const
	The active flavour threshold below the scale $\mu$ as defined in QCD::Thresholds(). More...

const double	Beta0 (const double nf) const
	The $\beta_0(n_f)$ coefficient for a certain number of flavours $n_f$. More...

const double	Beta1 (const double nf) const
	The $\beta_1(n_f)$ coefficient for a certain number of flavours $n_f$. More...

const double	Beta2 (const double nf) const
	The $\beta_2(n_f)$ coefficient for a certain number of flavours $n_f$. More...

const double	Beta3 (const double nf) const
	The $\beta_3(n_f)$ coefficient for a certain number of flavours $n_f$. More...

void	CacheShift (double cache[][5], int n) const
	A member used to manage the caching for this class. More...

void	CacheShift (int cache[][5], int n) const

const orders	FullOrder (orders order) const
	Return the FULLORDER enum corresponding to order. More...

const double	Gamma0 (const double nf) const
	The $\gamma_0$ coefficient used to compute the running of a mass. More...

const double	Gamma1 (const double nf) const
	The $\gamma_1$ coefficient used to compute the running of a mass. More...

const double	Gamma2 (const double nf) const
	The $\gamma_2$ coefficient used to compute the running of a mass. More...

const double	getAlsM () const
	A get method to access the value of $\alpha_s(M_{\alpha_s})$. More...

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. More...

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. More...

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. More...

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. More...

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. More...

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. More...

const BParameter &	getBKd1 () const

const BParameter &	getBKd3 () const

const double	getCF () const
	A get method to access the Casimir factor of QCD. More...

const double	getMAls () const
	A get method to access the mass scale $M_{\alpha_s}$ at which the strong coupling constant measurement is provided. More...

const Meson &	getMesons (const QCD::meson m) const
	A get method to access a meson as an object of the type Meson. More...

const double	getMtpole () const
	A get method to access the pole mass of the top quark. More...

const double	getMub () const
	A get method to access the threshold between five- and four-flavour theory in GeV. More...

const double	getMuc () const
	A get method to access the threshold between four- and three-flavour theory in GeV. More...

const double	getMut () const
	A get method to access the threshold between six- and five-flavour theory in GeV. More...

const double	getNc () const
	A get method to access the number of colours $N_c$. More...

const double	getOptionalParameter (std::string name) const
	A method to get parameters that are specific to only one set of observables. More...

const Particle &	getQuarks (const QCD::quark q) const
	A get method to access a quark as an object of the type Particle. More...

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. More...

void	initializeBParameter (std::string name_i) const
	A method to initialize B Parameter and the corresponding meson. More...

void	initializeMeson (QCD::meson meson_i) const
	A method to initialize a meson. More...

bool	isQCDsuccess () const
	A getter for the QCDsuccess flag. More...

const double	logLambda (const double nf, orders order) const
	Computes $\ln\Lambda_\mathrm{QCD}$ with nf flavours in GeV. More...

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. More...

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 $m(m)$. More...

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 $m(m)$. More...

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 $m(m)$. More...

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 $\mu_f$. More...

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 $n_f = 4$. More...

const double	MS2DRqmass (const double MSbar) const
	Converts a quark mass from the $\overline{\mathrm{MS}}$ scheme to the $\overline{\mathrm{DR}}$ scheme. More...

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. More...

const double	Nf (const double mu) const
	The number of active flavour at scale $\mu$. More...

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. More...

const std::string	orderToString (const orders order) const
	Converts an object of the enum type "orders" to the corresponding string. More...

	QCD ()
	Constructor. More...

void	setComputemt (bool computemt)
	A set method to change the value of computemt. More...

void	setMtpole (double mtpole_in)
	A method to set the pole mass of the top quark. More...

void	setNc (double Nc)
	A set method to change the number of colours $N_c$. More...

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. More...

void	setQuarkMass (const quark q, const double mass)
	A set method to change the mass of a quark. More...

const double	Thresholds (const int i) const
	For accessing the active flavour threshold scales. More...

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. More...

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. More...

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. More...

	Model ()
	The default constructor. More...

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. More...

void	setModelLinearized (bool linearized=true)

void	setModelName (const std::string name)
	A method to set the name of the model. More...

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. More...

virtual	~Model ()
	The default destructor. More...

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...

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. More...

static const int	NSMvars = 28
	The number of the model parameters in StandardModel. More...

static const int	NumSMParamsForEWPO = 35
	The number of the SM parameters that are relevant to the EW precision observables. More...

static std::string	SMvars [NSMvars]
	A string array containing the labels of the model parameters in StandardModel. More...

Static Public Attributes inherited from QCD
static const int	NQCDvars = 11
	The number of model parameters in QCD. More...

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(). 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. More...

virtual void	computeCKM ()
	The method to compute the CKM matrix. More...

virtual void	computeYukawas ()
	The method to compute the Yukawas matrix. More...

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 $\Delta_{\mathrm{EW/QCD}}$. More...

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, $R_A^q(M_Z^2)$. More...

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 $\Delta r_{\mathrm{rem}}$. More...

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 $\Delta r_{\mathrm{rem}}$. More...

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 $\Delta r_{\mathrm{rem}}$. More...

double	RVh () const
	The singlet vector corrections to the hadronic $Z$-boson width, denoted as $R_V^h$. More...

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, $R_V^q(M_Z^2)$. More...

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. More...

virtual void	setParameter (const std::string name, const double &value)
	A method to set the value of a parameter of StandardModel. More...

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 $\tau_b$. More...

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. More...

Protected Attributes inherited from StandardModel
double	A
	The CKM parameter $A$ in the Wolfenstein parameterization. More...

double	ale
	The fine-structure constant $\alpha$. More...

double	alpha21

double	alpha31

double	AlsMz
	The strong coupling constant at the Z-boson mass, $\alpha_s(M_Z)$. More...

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) More...

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. More...

double	delGammaWlv
	The theoretical uncertainty in $\Gamma_W_{l\nu}$, denoted as $\delta\,\Gamma_W_{l\nu}$. More...

double	delGammaWqq
	The theoretical uncertainty in $\Gamma_W_{qq}$, denoted as $\delta\,\Gamma_W_{qq}$. More...

double	delGammaZ
	The theoretical uncertainty in $\Gamma_Z$, denoted as $\delta\,\Gamma_Z$, in GeV. More...

double	delMw
	The theoretical uncertainty in $M_W$, denoted as $\delta\,M_W$, in GeV. More...

double	delR0b
	The theoretical uncertainty in $R_b^0$, denoted as $\delta\,R_b^0$. More...

double	delR0c
	The theoretical uncertainty in $R_c^0$, denoted as $\delta\,R_c^0$. More...

double	delR0l
	The theoretical uncertainty in $R_l^0$, denoted as $\delta\,R_l^0$. More...

double	delsigma0H
	The theoretical uncertainty in $\sigma_{Hadron}^0$, denoted as $\delta\,\sigma_{Hadron}^0$ in nb. More...

double	delSin2th_b
	The theoretical uncertainty in $\sin^2\theta_{\rm eff}^{b}$, denoted as $\delta\sin^2\theta_{\rm eff}^{b}$. More...

double	delSin2th_l
	The theoretical uncertainty in $\sin^2\theta_{\rm eff}^{\rm lept}$, denoted as $\delta\sin^2\theta_{\rm eff}^{\rm lept}$. More...

double	delSin2th_q
	The theoretical uncertainty in $\sin^2\theta_{\rm eff}^{q\not = b,t}$, denoted as $\delta\sin^2\theta_{\rm eff}^{q\not = b,t}$. More...

double	delta

double	etab
	The CKM parameter $\bar{\eta}$ in the Wolfenstein parameterization. More...

bool	flag_order [orders_EW_size]
	An array of internal flags controlling the inclusions of higher-order corrections. More...

bool	FlagFixMuwMut
	A boolean for the model flag FixMuwMut. More...

bool	flagLEP2 [NUMofLEP2RCs]

double	gamma
	$\gamma $ used as an input for FlagWolfenstein = FALSE More...

double	GF
	The Fermi constant $G_\mu$ in ${\rm GeV}^{-2}$. More...

double	lambda
	The CKM parameter $\lambda$ in the Wolfenstein parameterization. More...

Particle	leptons [6]
	An array of Particle objects for the leptons. More...

double	mHl
	The Higgs mass $m_h$ in GeV. More...

double	muw
	A matching scale $\mu_W$ around the weak scale in GeV. More...

double	Mw_inp
	The mass of the $W$ boson in GeV used as input for FlagMWinput = TRUE. More...

CKM	myCKM
	An object of type CKM. More...

PMNS	myPMNS

double	Mz
	The mass of the $Z$ boson in GeV. More...

bool	requireCKM
	An internal flag to control whether the CKM matrix has to be recomputed. More...

bool	requireYe
	An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed. More...

bool	requireYn
	An internal flag to control whether the neutrino Yukawa matrix has to be recomputed. More...

double	rhob
	The CKM parameter $\bar{\rho}$ in the Wolfenstein parameterization. More...

double	s12

double	s13

double	s23

Flavour	SMFlavour
	An object of type Flavour. More...

Matching< StandardModelMatching, StandardModel >	SMM
	An object of type Matching. More...

double	Vcb
	$\vert V_{cb} \vert $ used as an input for FlagWolfenstein = FALSE More...

double	Vub
	$\vert V_{ub} \vert $ used as an input for FlagWolfenstein = FALSE More...

double	Vud
	$\vert V_{ud} \vert $ used as an input for FlagWolfenstein = FALSE and FlagUseVud = TRUE More...

double	Vus
	$\vert V_{us} \vert $ used as an input for FlagWolfenstein = FALSE More...

gslpp::matrix< gslpp::complex >	Yd
	The Yukawa matrix of the down-type quarks. More...

gslpp::matrix< gslpp::complex >	Ye
	The Yukawa matrix of the charged leptons. More...

gslpp::matrix< gslpp::complex >	Yn
	The Yukawa matrix of the neutrinos. More...

gslpp::matrix< gslpp::complex >	Yu
	The Yukawa matrix of the up-type quarks. More...

Protected Attributes inherited from QCD
double	AlsM
	The strong coupling constant at the mass scale MAls, $\alpha_s(M_{\alpha_s})$. More...

double	CA

double	CF

bool	computemt
	Switch for computing the $\overline{\mathrm{MS}}$ mass of the top quark. More...

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. More...

bool	FlagMtPole
	A flag to determine whether the pole mass of the top quark is used as input. More...

double	MAls
	The mass scale in GeV at which the strong coupling measurement is provided. More...

double	mtpole
	The pole mass of the top quark. More...

double	mub
	The threshold between five- and four-flavour theory in GeV. More...

double	muc
	The threshold between four- and three-flavour theory in GeV. More...

double	mut
	The threshold between six- and five-flavour theory in GeV. More...

double	NA

double	Nc
	The number of colours. More...

bool	QCDsuccess =true

Particle	quarks [6]
	The vector of all SM quarks. More...

bool	requireYd
	Switch for generating the Yukawa couplings to the down-type quarks. More...

bool	requireYu
	Switch for generating the Yukawa couplings to the up-type quarks. More...

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. More...

std::map< std::string, std::reference_wrapper< const double > >	ModelParamMap

bool	UpdateError = false
	A boolean set to false if update is successful. More...

Constructor & Destructor Documentation

◆ NPbase()

NPbase::NPbase ( )

The default constructor.

Definition at line 29 of file NPbase.cpp.

: StandardModel(), trueSM()
{
    trueSM.InitializeModel();
    trueSM.setSliced(true);
}

Member Function Documentation

◆ A_f()

const double NPbase::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 StandardModel.

Reimplemented in NPSMEFTd6General, NPZbbbar, and NPEpsilons.

Definition at line 826 of file NPbase.cpp.

{    
    //AG:begin
    if(OutputOrder()==0){ return (trueSM.A_f(f) ); }
    if(OutputOrder()==1){ return (trueSM.A_f(f) + deltaA_f(f)); }
    if(OutputOrder()==2){ return (trueSM.A_f(f) + deltaA_f(f) + deltaA_f_2(f) ); }
    if(OutputOrder()==3){ return ( deltaA_f_2(f) ); }
    else
    //AG:end
    //AG: deltaA_f_2(f) added below 
        return (trueSM.A_f(f) + deltaA_f(f) + deltaA_f_2(f));
}

◆ AFB()

const double NPbase::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 StandardModel.

Reimplemented in NPSMEFTd6General, NPZbbbar, and NPEpsilons.

Definition at line 923 of file NPbase.cpp.

{
    //AG: begin
    if(OutputOrder()==0){ return (trueSM.AFB(f) ); }
    if(OutputOrder()==1){ return (trueSM.AFB(f) + deltaAFB(f)); }
    if(OutputOrder()==2){ return (trueSM.AFB(f) + deltaAFB(f) + deltaAFB_2(f) ); }
    if(OutputOrder()==3){ return ( deltaAFB_2(f) ); }
    else
    //AG:end
    //AG: deltaAFB_2(f) added below
        return (trueSM.AFB(f) + deltaAFB(f) + deltaAFB_2(f));
}

◆ alphaMz()

const double NPbase::alphaMz ( ) const

virtual

The electromagnetic coupling at the $Z$-mass scale, $\alpha(M_Z^2)=\alpha/(1-\Delta\alpha(M_Z^2))$.

Returns: $\alpha(M_Z^2)$

Reimplemented from StandardModel.

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 51 of file NPbase.cpp.

{
    /*AG:begin
    // FlagMWinput flag to be implemented in NPbase, especially for alphaMz and Mw!
    double dalphaMz = 0.0;
    if(FlagMWinput){
        double alpha = trueSM.alphaMz();
        double c2 = trueSM.cW2();
        double s2 = trueSM.sW2();
        
        dalphaMz = sqrt(2.0)*GF*Mz*Mz/4.0/M_PI*c2*( alpha/2.0*(obliqueS() - 2.0*c2*obliqueT() - (c2-s2)/2.0/s2*obliqueU()) - s2/2.0/(c2-s2)*DeltaGF() );
    }
    return (trueSM.alphaMz() + dalphaMz);
    //AG:end */
    
    double myAlphaMz = trueSM.alphaMz();
    
    return myAlphaMz;
}

◆ aPskPol()

virtual const double NPbase::aPskPol	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1338 of file NPbase.h.

    {
        return 0.0;
    }

◆ bPskPol()

virtual const double NPbase::bPskPol	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1351 of file NPbase.h.

    {
        return 0.0;
    }

◆ Br_H_exo()

virtual const double NPbase::Br_H_exo ( ) const

inlinevirtual

The branching ratio of the of the Higgs into exotic particles.

Returns: Br $(H\to exotic)$

Reimplemented in HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2646 of file NPbase.h.

    {
        return 0.0;
    };

◆ Br_H_inv()

virtual const double NPbase::Br_H_inv ( ) const

inlinevirtual

The branching ratio of the of the Higgs into invisible particles.

Returns: Br $(H\to invisible)$

Reimplemented in HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2655 of file NPbase.h.

    {
        return 0.0;
    };

◆ Br_H_inv_NP()

virtual const double NPbase::Br_H_inv_NP ( ) const

inlinevirtual

The branching ratio of the of the Higgs into invisible particles (only invisible new particles).

Returns: Br $(H\to invisible,NP)$

Reimplemented in HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2665 of file NPbase.h.

    {
        return 0.0;
    };

◆ BR_Zf()

const double NPbase::BR_Zf ( const Particle f ) const

virtual

The Branching ratio of the $Z$ boson into a given fermion pair, $BR_Z^{f}$.

Parameters

[in] f a lepton or quark

Returns: $BR_Z^{f}$ including SM plus NP contributions

Attention: This function is applicable only to the NP model classes that are inherited from NPbase.

Definition at line 550 of file NPbase.cpp.

{
    double delGammaZTot = deltaGamma_Z();
    double delGammaZf = deltaGamma_Zf(f);
    
    double GammaZTotSM = trueSM.Gamma_Z();
    double GammaZfSM = trueSM.GammaZ(f);
    
    return (GammaZfSM/GammaZTotSM + delGammaZf/GammaZTotSM - GammaZfSM * delGammaZTot /GammaZTotSM/GammaZTotSM);
}

◆ BrH2d2dRatio()

virtual const double NPbase::BrH2d2dRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2376 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2e2muRatio()

virtual const double NPbase::BrH2e2muRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2313 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2e2vRatio()

virtual const double NPbase::BrH2e2vRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2349 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2evRatio()

virtual const double NPbase::BrH2evRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2556 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2L2dRatio()

virtual const double NPbase::BrH2L2dRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2403 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2L2LRatio()

virtual const double NPbase::BrH2L2LRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2304 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2L2uRatio()

virtual const double NPbase::BrH2L2uRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2394 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2L2v2Ratio()

virtual const double NPbase::BrH2L2v2Ratio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2340 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2L2vRatio()

virtual const double NPbase::BrH2L2vRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2331 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2l2vRatio()

virtual const double NPbase::BrH2l2vRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2595 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2Lv2Ratio()

virtual const double NPbase::BrH2Lv2Ratio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2547 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2LvRatio()

virtual const double NPbase::BrH2LvRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2538 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2mu2vRatio()

virtual const double NPbase::BrH2mu2vRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2358 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2muvRatio()

virtual const double NPbase::BrH2muvRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2565 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2u2dRatio()

virtual const double NPbase::BrH2u2dRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2385 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2u2uRatio()

virtual const double NPbase::BrH2u2uRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2367 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2udRatio()

virtual const double NPbase::BrH2udRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2529 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2v2dRatio()

virtual const double NPbase::BrH2v2dRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2421 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2v2uRatio()

virtual const double NPbase::BrH2v2uRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2412 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH2v2vRatio()

virtual const double NPbase::BrH2v2vRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2322 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH4dRatio()

virtual const double NPbase::BrH4dRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2484 of file NPbase.h.

    {
        return 1.0;
    }    

◆ BrH4eRatio()

virtual const double NPbase::BrH4eRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2448 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH4fRatio()

virtual const double NPbase::BrH4fRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2574 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH4L2Ratio()

virtual const double NPbase::BrH4L2Ratio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2439 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH4LRatio()

virtual const double NPbase::BrH4LRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2430 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH4lRatio()

virtual const double NPbase::BrH4lRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2586 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH4muRatio()

virtual const double NPbase::BrH4muRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2457 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrH4uRatio()

virtual const double NPbase::BrH4uRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2475 of file NPbase.h.

    {
        return 1.0;
    }   

◆ BrH4vRatio()

virtual const double NPbase::BrH4vRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2466 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHbbRatio()

virtual const double NPbase::BrHbbRatio ( ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.

Definition at line 2291 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHccRatio()

virtual const double NPbase::BrHccRatio ( ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.

Definition at line 2271 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHevmuvRatio()

virtual const double NPbase::BrHevmuvRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2502 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHgagaRatio()

virtual const double NPbase::BrHgagaRatio ( ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.

Definition at line 2238 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHggRatio()

virtual const double NPbase::BrHggRatio ( ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.

Definition at line 2158 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHll_vvorjjRatio()

virtual const double NPbase::BrHll_vvorjjRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2635 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHlljjRatio()

virtual const double NPbase::BrHlljjRatio ( ) const

inlinevirtual

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.

Returns: Br $(H\to l l j j)$/Br $(H\to l l j j)_{\mathrm{SM}}$

Reimplemented in HiggsChiral, and HiggsKigen.

Definition at line 2608 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHlv_lvorjjRatio()

virtual const double NPbase::BrHlv_lvorjjRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2626 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHlvjjRatio()

virtual const double NPbase::BrHlvjjRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2617 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHLvudRatio()

virtual const double NPbase::BrHLvudRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2520 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHLvvLRatio()

virtual const double NPbase::BrHLvvLRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2493 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHmumuRatio()

virtual const double NPbase::BrHmumuRatio ( ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.

Definition at line 2251 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHssRatio()

virtual const double NPbase::BrHssRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, and NPSMEFTd6General.

Definition at line 2281 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHtautauRatio()

virtual const double NPbase::BrHtautauRatio ( ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.

Definition at line 2261 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHtoinvRatio()

virtual const double NPbase::BrHtoinvRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2685 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHudduRatio()

virtual const double NPbase::BrHudduRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2511 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHvisRatio()

virtual const double NPbase::BrHvisRatio ( ) const

inlinevirtual

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 in HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2675 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHVVRatio()

virtual const double NPbase::BrHVVRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2188 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHWWRatio()

virtual const double NPbase::BrHWWRatio ( ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.

Definition at line 2168 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHZgaeeRatio()

virtual const double NPbase::BrHZgaeeRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, and SigmaBR.

Definition at line 2218 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHZgallRatio()

virtual const double NPbase::BrHZgallRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, and SigmaBR.

Definition at line 2208 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHZgamumuRatio()

virtual const double NPbase::BrHZgamumuRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, and SigmaBR.

Definition at line 2228 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHZgaRatio()

virtual const double NPbase::BrHZgaRatio ( ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.

Definition at line 2198 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrHZZRatio()

virtual const double NPbase::BrHZZRatio ( ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.

Definition at line 2178 of file NPbase.h.

    {
        return 1.0;
    }

◆ BrW()

const double NPbase::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 StandardModel.

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 137 of file NPbase.cpp.

{
    double GammW = GammaW();
    double GammWij = GammaW(fi, fj);
 
    return GammWij/GammW;
}

◆ C1eeHvv()

const double NPbase::C1eeHvv ( const double sqrt_s ) const

virtual

The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.

Definition at line 1745 of file NPbase.cpp.

{
    double C1;
    
    if (sqrt_s == 0.240) {
 
        C1 = 0.00639683;
        
    } else if (sqrt_s == 0.250) {
 
        C1 = 0.0064;
 
    } else if (sqrt_s == 0.350) {
 
        C1 = 0.0062;
 
    } else if (sqrt_s == 0.365) {
 
        C1 = 0.00618352; 
 
    } else if (sqrt_s == 0.380) {
 
        C1 = 0.0062;
 
    } else if (sqrt_s == 0.500) {
 
        C1 = 0.0061;
 
    } else if (sqrt_s == 1.0) {
 
        C1 = 0.0059;
 
    } else if (sqrt_s == 1.4) {
 
        C1 = 0.0058;
 
    } else if (sqrt_s == 1.5) {
 
        C1 = 0.0058;
 
    } else if (sqrt_s == 3.0) {
 
        C1 = 0.0057;
 
    } else
        throw std::runtime_error("Bad argument in NPbase::C1eeHvv");
    
    return C1;
}

◆ C1eettH()

const double NPbase::C1eettH ( const double sqrt_s ) const

virtual

The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.

Definition at line 1845 of file NPbase.cpp.

{
    double C1;
    
    if (sqrt_s == 0.500) {
 
        C1 = 0.086;
 
    } else if (sqrt_s == 1.0) {
 
        C1 = 0.017;
 
    } else if (sqrt_s == 1.4) {
 
        C1 = 0.0094;
 
    } else if (sqrt_s == 1.5) {
 
        C1 = 0.0094;
 
    } else if (sqrt_s == 3.0) {
 
        C1 = 0.0037;
 
    } else
        throw std::runtime_error("Bad argument in NPbase::C1eettH");
    
    return C1;
}

◆ C1eeWBF()

const double NPbase::C1eeWBF ( const double sqrt_s ) const

virtual

The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.

Definition at line 1695 of file NPbase.cpp.

{
    double C1;
    
    if (sqrt_s == 0.240) {
 
        C1 = 0.00639683;
        
    } else if (sqrt_s == 0.250) {
 
        C1 = 0.0064;
 
    } else if (sqrt_s == 0.350) {
 
        C1 = 0.0062;
 
    } else if (sqrt_s == 0.365) {
 
        C1 = 0.00618352; 
 
    } else if (sqrt_s == 0.380) {
 
        C1 = 0.0062;
 
    } else if (sqrt_s == 0.500) {
 
        C1 = 0.0061;
 
    } else if (sqrt_s == 1.0) {
 
        C1 = 0.0059;
 
    } else if (sqrt_s == 1.4) {
 
        C1 = 0.0058;
 
    } else if (sqrt_s == 1.5) {
 
        C1 = 0.0058;
 
    } else if (sqrt_s == 3.0) {
 
        C1 = 0.0057;
 
    } else
        throw std::runtime_error("Bad argument in NPbase::C1eeWBF");
    
    return C1;
}

◆ C1eeZBF()

const double NPbase::C1eeZBF ( const double sqrt_s ) const

virtual

The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.

Definition at line 1795 of file NPbase.cpp.

{
    double C1;
    
    if (sqrt_s == 0.240) {
 
        C1 = 0.0070;
        
    } else if (sqrt_s == 0.250) {
 
        C1 = 0.0070;
 
    } else if (sqrt_s == 0.350) {
 
        C1 = 0.0069;
 
    } else if (sqrt_s == 0.365) {
 
        C1 = 0.0069; 
 
    } else if (sqrt_s == 0.380) {
 
        C1 = 0.0069;
 
    } else if (sqrt_s == 0.500) {
 
        C1 = 0.0067;
 
    } else if (sqrt_s == 1.0) {
 
        C1 = 0.0065;
 
    } else if (sqrt_s == 1.4) {
 
        C1 = 0.0065;
 
    } else if (sqrt_s == 1.5) {
 
        C1 = 0.0065;
 
    } else if (sqrt_s == 3.0) {
 
        C1 = 0.0063;
 
    } else
        throw std::runtime_error("Bad argument in NPbase::C1eeZBF");
    
    return C1;
}

◆ C1eeZH()

const double NPbase::C1eeZH ( const double sqrt_s ) const

virtual

The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.

Definition at line 1645 of file NPbase.cpp.

{
    double C1;
    
    if (sqrt_s <= 0.240) {
 
        C1 = 0.0173302;
        
    } else if (sqrt_s == 0.250) {
 
        C1 = 0.015;
 
    } else if (sqrt_s == 0.350) {
 
        C1 = 0.0057;
 
    } else if (sqrt_s == 0.365) {
 
        C1 = 0.00493549; 
 
    } else if (sqrt_s == 0.380) {
 
        C1 = 0.0057; // Use same as 350 GeV
 
    } else if ((sqrt_s == 0.500)||(sqrt_s == 0.550) ) {
 
        C1 = 0.00099;
 
    } else if (sqrt_s == 1.0) {
 
        C1 = -0.0012;
 
    } else if (sqrt_s == 1.4) {
 
        C1 = -0.0011;
 
    } else if (sqrt_s == 1.5) {
 
        C1 = -0.0011; // Use the same as 1400 GeV
 
    } else if (sqrt_s == 3.0) {
 
        C1 = -0.00054;
 
    } else
        throw std::runtime_error("Bad argument in NPbase::C1eeZH");
    
    return C1;
}

◆ cbminuscc()

virtual const double NPbase::cbminuscc ( ) const

inlinevirtual

Returns

Reimplemented in HiggsChiral.

Definition at line 2823 of file NPbase.h.

    {
        return 0.0;
    }

◆ cbminusctau()

virtual const double NPbase::cbminusctau ( ) const

inlinevirtual

Returns

Reimplemented in HiggsChiral.

Definition at line 2832 of file NPbase.h.

    {
        return 0.0;
    }

◆ ccminusctau()

virtual const double NPbase::ccminusctau ( ) const

inlinevirtual

Returns

Reimplemented in HiggsChiral.

Definition at line 2841 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHd11()

virtual const double NPbase::CEWHd11 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{Hd})_{11}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4966 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHd22()

virtual const double NPbase::CEWHd22 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{Hd})_{22}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4976 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHd33()

virtual const double NPbase::CEWHd33 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{Hd})_{33}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4986 of file NPbase.h.

    {
        return 0.0;
    } 

◆ CEWHe11()

virtual const double NPbase::CEWHe11 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{He})_{11}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4904 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHe22()

virtual const double NPbase::CEWHe22 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{He})_{22}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4914 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHe33()

virtual const double NPbase::CEWHe33 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{He})_{33}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4924 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHL111()

virtual const double NPbase::CEWHL111 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{HL}^{(1)})_{11}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4762 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHL122()

virtual const double NPbase::CEWHL122 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{HL}^{(1)})_{22}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4772 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHL133()

virtual const double NPbase::CEWHL133 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{HL}^{(1)})_{33}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4782 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHL311()

virtual const double NPbase::CEWHL311 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{HL}^{(3)})_{11}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4792 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHL322()

virtual const double NPbase::CEWHL322 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{HL}^{(3)})_{22}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4802 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHL333()

virtual const double NPbase::CEWHL333 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{HL}^{(3)})_{33}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4812 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHQ111()

virtual const double NPbase::CEWHQ111 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{HQ}^{(1)})_{11}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4822 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHQ122()

virtual const double NPbase::CEWHQ122 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{HQ}^{(1)})_{22}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4832 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHQ133()

virtual const double NPbase::CEWHQ133 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{HQ}^{(1)})_{33}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4842 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHQ311()

virtual const double NPbase::CEWHQ311 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{HQ}^{(3)})_{11}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4852 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHQ322()

virtual const double NPbase::CEWHQ322 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{HQ}^{(3)})_{22}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4862 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHQ333()

virtual const double NPbase::CEWHQ333 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{HQ}^{(3)})_{33}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4872 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHQd33()

virtual const double NPbase::CEWHQd33 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{HQ}^{(d)})_{33}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4883 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHQu33()

virtual const double NPbase::CEWHQu33 ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4893 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHu11()

virtual const double NPbase::CEWHu11 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{Hu})_{11}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4935 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHu22()

virtual const double NPbase::CEWHu22 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{Hu})_{22}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4945 of file NPbase.h.

    {
        return 0.0;
    }

◆ CEWHu33()

virtual const double NPbase::CEWHu33 ( const double mu ) const

inlinevirtual

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

Returns: $(\hat{C}_{Hu})_{33}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4955 of file NPbase.h.

    {
        return 0.0;
    }

◆ cgaga_HB()

virtual const double NPbase::cgaga_HB ( const double mu ) const

inlinevirtual

The Higgs-basis coupling $c_{\gamma\gamma}$. (See LHCHXSWG-INT-2015-001 document.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $c_{\gamma\gamma}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4716 of file NPbase.h.

    {
        return 0.0;
    }

◆ cgaplusct()

virtual const double NPbase::cgaplusct ( ) const

inlinevirtual

Returns

Reimplemented in HiggsChiral.

Definition at line 2787 of file NPbase.h.

    {
        return 1.0;
    }

◆ cgg_HB()

virtual const double NPbase::cgg_HB ( const double mu ) const

inlinevirtual

The Higgs-basis coupling $c_{gg}$. (See LHCHXSWG-INT-2015-001 document.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $c_{gg}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4727 of file NPbase.h.

    {
        return 0.0;
    }

◆ cggEff_HB()

virtual const double NPbase::cggEff_HB ( const double mu ) const

inlinevirtual

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.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $c_{gg}^{Eff}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4738 of file NPbase.h.

    {
        return 0.0;
    }

◆ cgminuscga()

virtual const double NPbase::cgminuscga ( ) const

inlinevirtual

Returns

Reimplemented in HiggsChiral.

Definition at line 2796 of file NPbase.h.

    {
        return 0.0;
    }

◆ cgplusct()

virtual const double NPbase::cgplusct ( ) const

inlinevirtual

Returns

Reimplemented in HiggsChiral.

Definition at line 2778 of file NPbase.h.

    {
        return 1.0;
    }

◆ computeGammaTotalRatio()

virtual const double NPbase::computeGammaTotalRatio ( ) const

inlinevirtual

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

Returns: $\Gamma(H)$/ $\Gamma(H)_{\mathrm{SM}}$

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, THDMW, and THDMWSignalStrengths.

Definition at line 2146 of file NPbase.h.

    {
        return 1.0;
    }

◆ cVpluscb()

virtual const double NPbase::cVpluscb ( ) const

inlinevirtual

Returns

Reimplemented in HiggsChiral.

Definition at line 2805 of file NPbase.h.

    {
        return 2.0;
    }

◆ cVplusctau()

virtual const double NPbase::cVplusctau ( ) const

inlinevirtual

Returns

Reimplemented in HiggsChiral.

Definition at line 2814 of file NPbase.h.

    {
        return 2.0;
    }

◆ cZBox_HB()

virtual const double NPbase::cZBox_HB ( const double mu ) const

inlinevirtual

The Higgs-basis coupling $c_{z\Box}$. (See LHCHXSWG-INT-2015-001 document.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $c_{z\Box}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4683 of file NPbase.h.

    {
        return 0.0;
    }

◆ cZga_HB()

virtual const double NPbase::cZga_HB ( const double mu ) const

inlinevirtual

The Higgs-basis coupling $c_{z\gamma}$. (See LHCHXSWG-INT-2015-001 document.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $c_{z\gamma}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4705 of file NPbase.h.

    {
        return 0.0;
    }

◆ cZZ_HB()

virtual const double NPbase::cZZ_HB ( const double mu ) const

inlinevirtual

The Higgs-basis coupling $c_{zz}$. (See LHCHXSWG-INT-2015-001 document.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $c_{zz}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4694 of file NPbase.h.

    {
        return 0.0;
    }

◆ Dalpha5hMz()

const double NPbase::Dalpha5hMz ( ) const

virtual

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

Depending on the flag MWinput this is given by the input parameter dAle5Mz (MWinput=false) or it is computed from Mw (MWinput=true)

Returns: $\Delta\alpha_{had}^{(5)}(M_Z)$

Reimplemented from StandardModel.

Reimplemented in NPSMEFTd6General.

Definition at line 72 of file NPbase.cpp.

{
    double myDalpha5hMz = trueSM.Dalpha5hMz();
    
    return myDalpha5hMz;
}

◆ delta2sBRH3()

virtual const double NPbase::delta2sBRH3	(	const double	C1prod,
		const double	C1Hxx
	)		const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2706 of file NPbase.h.

    {
        return 0.0;
    }

◆ delta2sH3()

virtual const double NPbase::delta2sH3 ( const double C1 ) const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2697 of file NPbase.h.

    {
        return 0.0;
    }

◆ delta_mubbH_1()

virtual const double NPbase::delta_mubbH_1 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1935 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_mubbH_2()

virtual const double NPbase::delta_mubbH_2 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1939 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_muggH_1()

virtual const double NPbase::delta_muggH_1 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1872 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_muggH_2()

virtual const double NPbase::delta_muggH_2 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1876 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_mutH_1()

virtual const double NPbase::delta_mutH_1 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1926 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_mutH_2()

virtual const double NPbase::delta_mutH_2 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1930 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_muttH_1()

virtual const double NPbase::delta_muttH_1 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1917 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_muttH_2()

virtual const double NPbase::delta_muttH_2 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1921 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_muVBF_1()

virtual const double NPbase::delta_muVBF_1 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1881 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_muVBF_2()

virtual const double NPbase::delta_muVBF_2 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1885 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_muVH_1()

virtual const double NPbase::delta_muVH_1 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1908 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_muVH_2()

virtual const double NPbase::delta_muVH_2 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1912 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_muWH_1()

virtual const double NPbase::delta_muWH_1 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1890 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_muWH_2()

virtual const double NPbase::delta_muWH_2 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1894 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_muZH_1()

virtual const double NPbase::delta_muZH_1 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1899 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ delta_muZH_2()

virtual const double NPbase::delta_muZH_2 ( const double sqrt_s ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1903 of file NPbase.h.

    { 
        return 0.0 ;
    }

◆ deltaA_f()

const double NPbase::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 in NPSMEFTd6General.

Definition at line 809 of file NPbase.cpp.

{
    double dAf = 0.;
    double delGVf = deltaGV_f(f);
    double delGAf = deltaGA_f(f);
    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;
    }
 
    return dAf;
}

◆ deltaA_f_2()

const double NPbase::deltaA_f_2 ( const Particle f ) const

virtual

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, $\Delta \mathcal{A}_f^{(2)}$.

$\newcommand{\nc}{\newcommand}$ $\nc{\gVfSM}{g_{V,f}^{SM}}$ $\nc{\gAfSM}{g_{A,f}^{SM}}$ $\nc{\gVfL}{\Delta g_{V,f}^{(1)}}$ $\nc{\gAfL}{\Delta g_{A,f}^{(1)}}$ $\nc{\gVfQ}{\Delta g_{V,f}^{(2)}}$ $\nc{\gAfQ}{\Delta g_{A,f}^{(2)}}$

\begin{eqnarray*} \Delta \mathcal{A}_f^{(2)} &=& 2~ \frac{ \gVfSM ~\gAfSM }{ \left[(g_{V,f}^{SM})^2+(g_{A,f}^{SM})^2\right]^3 } \left( \left[(\gAfSM)^2 -3 (\gVfSM)^2\right] (\gAfL)^2 + \left[(\gVfSM)^2 -3 (\gAfSM)^2\right] (\gVfL)^2 \right) \\ &-& ~ 2~ \frac{ (\gAfSM)^4 - 6(\gAfSM)^2(\gVfSM)^2 + (\gVfSM)^4 }{\left[(g_{V,f}^{SM})^2+(g_{A,f}^{SM})^2\right]^3} ~\gVfL ~\gAfL +~ 2~ \frac{ (g_{V,f}^{SM})^2-(g_{A,f}^{SM})^2 }{ \left[(g_{V,f}^{SM})^2+(g_{A,f}^{SM})^2\right]^2 } \left[ \gVfSM ~\gAfQ - \gAfSM ~\gVfQ \right] \end{eqnarray*}

Parameters

[in] f a lepton or quark

Returns: $\Delta \mathcal{A}_f^{(2)}$

Definition at line 781 of file NPbase.cpp.

{     
    //AG:added
    double dA_2 = 0.0;
   
    bool nonZeroNP = false;
    double delGVf = deltaGV_f(f);
    double delGAf = deltaGA_f(f);
    double delGVf2 = deltaGV_f_2(f);
    double delGAf2 = deltaGA_f_2(f);
    if (delGVf2!=0.0 || delGAf2!=0.0) {nonZeroNP = true;}
    
    if (nonZeroNP) {
        double gVf = trueSM.gV_f(f).real();
        double gAf = trueSM.gA_f(f).real();
        double Gf = gVf*gVf + gAf*gAf;
 
        double f2 = -2.0 * ( gVf*gVf - gAf*gAf ) * ( gAf*delGVf2 - gVf*delGAf2) / Gf / Gf;
        double f1 =  2.0 * ( gVf*gAf*( gAf*gAf - 3.0*gVf*gVf )*delGAf*delGAf 
                    + gVf*gAf*( gVf*gVf - 3.0*gAf*gAf )*delGVf*delGVf 
                    - ( pow(gAf,4.0) - 6.0*pow(gAf,2.0)*pow(gVf,2.0) + pow(gVf,4.0) )*delGVf*delGAf 
                    ) / pow(Gf,3.0);
 
        dA_2 = f1+f2;
    }
    return dA_2;
}

◆ deltaAFB()

const double NPbase::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 in NPSMEFTd6General.

Definition at line 888 of file NPbase.cpp.

{
    double dAFB = 0.;
    double delGVf = deltaGV_f(f);
    double delGAf = deltaGA_f(f);
    if (f.is("ELECTRON")) {
        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 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);
        }
    }
 
    return dAFB;
}

◆ deltaAFB_2()

const double NPbase::deltaAFB_2 ( const Particle f ) const

virtual

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, $\Delta A^f_{FB}$.

\[ \Delta A_{FB,f}^{(2)} = \frac{3}{4} \left( \Delta A_e^{(1)} \Delta A_f^{(1)} + A_e^{SM} \Delta A_f^{(2)} + A_f^{SM} \Delta A_e^{(2)} \right) \]

Parameters

[in] f a lepton or quark

Returns: $\Delta A^{f (2)}_{FB}$

Definition at line 839 of file NPbase.cpp.

{
    //AG:added
    double dAFB_2=0.0;
    
    bool nonZeroNP = false;
    double delGVf2 = deltaGV_f_2(f);
    double delGAf2 = deltaGA_f_2(f);
    if (delGVf2!=0.0 || delGAf2!=0.0) {nonZeroNP = true;}
    
    if (nonZeroNP) {
        /*
        double gVe = trueSM.gV_f(leptons[ELECTRON]).real();
        double gAe = trueSM.gA_f(leptons[ELECTRON]).real();
        double gVf = trueSM.gV_f(f).real();
        double gAf = trueSM.gA_f(f).real();
        
        double Ge = gVe*gVe + gAe*gAe;
        double delGVeOverGAe = (gVe*delGAe-gAe*delGVe) ;
        double Gf = gVf*gVf + gAf*gAf;
        double delGVfOverGAf = (gVf*delGAf-gAf*delGVf) ;
        
        double Ae = 2.0*gVe*gAe/(gVe*gVe+gAe*gAe);
        double deltaAe = deltaA_f(leptons[ELECTRON]);
        double Af = 2.0*gVf*gAf/(gVf*gVf+gAf*gAf);
        double deltaAf = deltaA_f(f);
        
        dAFB_Test = 3.0 * Af/2.0 * deltaAe/2.0 + 3.0 * Ae/2.0 * deltaAf/2.0 ;*/
        
        double gVe = trueSM.gV_f(leptons[ELECTRON]).real();
        double gAe = trueSM.gA_f(leptons[ELECTRON]).real();
        double gVf = trueSM.gV_f(f).real();
        double gAf = trueSM.gA_f(f).real();
        
        double Ae = 2.0*gVe*gAe/(gVe*gVe+gAe*gAe);
        double deltaAe = deltaA_f(leptons[ELECTRON]);
        double deltaAe2 = deltaA_f_2(leptons[ELECTRON]);
        double Af = 2.0*gVf*gAf/(gVf*gVf+gAf*gAf);
        double deltaAf = deltaA_f(f);
        double deltaAf2 = deltaA_f_2(f);
        
        if (f.is("ELECTRON")) 
            dAFB_2 = 3.0/4.0 * ( deltaAe*deltaAe + 2.0*Ae*deltaAe2 );
        else 
            dAFB_2 = 3.0/4.0 * ( deltaAe*deltaAf + Ae*deltaAf2 + Af*deltaAe2 );
    }
    return dAFB_2;
}

◆ deltacZ_HB()

virtual const double NPbase::deltacZ_HB ( const double mu ) const

inlinevirtual

The Higgs-basis coupling $\delta c_z$. (See LHCHXSWG-INT-2015-001 document.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta c_z$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4672 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltadxsdcoseeWWlvjjLEP2()

virtual const double NPbase::deltadxsdcoseeWWlvjjLEP2	(	const double	sqrt_s,
		const int	bin
	)		const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3314 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaeNP()

virtual const double NPbase::deltaeNP ( const double mu ) const

inlinevirtual

The new physics relative contribution to the EW coupling constant $e$.

Returns: $\delta e$

Reimplemented in NPSMEFTd6General.

Definition at line 3111 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaG1_hWW()

virtual const double NPbase::deltaG1_hWW ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 859 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG1_hWW_mu()

virtual const double NPbase::deltaG1_hWW_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 990 of file NPbase.h.

    {
        return deltaG1_hWW();
    };

◆ deltaG1_hZA()

virtual const double NPbase::deltaG1_hZA ( ) const

inlinevirtual

The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} F^{\mu\nu}$.

Returns: $\delta g_{HZA}^{(1)}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 907 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG1_hZA_mu()

virtual const double NPbase::deltaG1_hZA_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1044 of file NPbase.h.

    {
        return deltaG1_hZA();
    };

◆ deltaG1_hZARatio()

virtual const double NPbase::deltaG1_hZARatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 916 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG1_hZARatio_mu()

virtual const double NPbase::deltaG1_hZARatio_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1054 of file NPbase.h.

    {
        return deltaG1_hZARatio();
    };

◆ deltaG1_hZZ()

virtual const double NPbase::deltaG1_hZZ ( ) const

inlinevirtual

The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} Z^{\mu\nu}$.

Returns: $\delta g_{HZZ}^{(1)}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 883 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG1_hZZ_mu()

virtual const double NPbase::deltaG1_hZZ_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1017 of file NPbase.h.

    {
        return deltaG1_hZZ();
    };

◆ deltag1gaNP()

virtual const double NPbase::deltag1gaNP ( const double mu ) const

inlinevirtual

The new physics contribution to the anomalous triple gauge coupling $g_{1,Z}$.

Returns: $\delta g_{1,\gamma}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 3131 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltag1ZNP()

virtual const double NPbase::deltag1ZNP ( const double mu ) const

inlinevirtual

The new physics contribution to the anomalous triple gauge coupling $g_{1,Z}$.

Returns: $\delta g_{1,Z}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 3122 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltag1ZNPEff()

virtual const double NPbase::deltag1ZNPEff ( ) const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 3162 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaG2_hWW()

virtual const double NPbase::deltaG2_hWW ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 867 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG2_hWW_mu()

virtual const double NPbase::deltaG2_hWW_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 999 of file NPbase.h.

    {
        return deltaG2_hWW();
    };

◆ deltaG2_hZA()

virtual const double NPbase::deltaG2_hZA ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 924 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG2_hZA_mu()

virtual const double NPbase::deltaG2_hZA_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1063 of file NPbase.h.

    {
        return deltaG2_hZA();
    };

◆ deltaG2_hZZ()

virtual const double NPbase::deltaG2_hZZ ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 891 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG2_hZZ_mu()

virtual const double NPbase::deltaG2_hZZ_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1026 of file NPbase.h.

    {
        return deltaG2_hZZ();
    };

◆ deltaG3_hWW()

virtual const double NPbase::deltaG3_hWW ( ) const

inlinevirtual

The new physics contribution to the coupling of the effective interaction $H W_{\mu}^\dagger W^{\mu}$.

Returns: $\delta g_{HWW}^{(3)}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 875 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG3_hWW_mu()

virtual const double NPbase::deltaG3_hWW_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1008 of file NPbase.h.

    {
        return deltaG3_hWW();
    };

◆ deltaG3_hZZ()

virtual const double NPbase::deltaG3_hZZ ( ) const

inlinevirtual

The new physics contribution to the coupling of the effective interaction $H Z_{\mu} Z^{\mu}$.

Returns: $\delta g_{HZZ}^{(3)}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 899 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG3_hZZ_mu()

virtual const double NPbase::deltaG3_hZZ_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1035 of file NPbase.h.

    {
        return deltaG3_hZZ();
    };

◆ deltaG_hAA()

virtual const double NPbase::deltaG_hAA ( ) const

inlinevirtual

The new physics contribution to the coupling of the effective interaction $H F_{\mu\nu} F^{\mu\nu}$.

Returns: $\delta g_{HAA}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 932 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG_hAA_mu()

virtual const double NPbase::deltaG_hAA_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1072 of file NPbase.h.

    {
        return deltaG_hAA();
    };

◆ deltaG_hAARatio()

virtual const double NPbase::deltaG_hAARatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 941 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG_hAARatio_mu()

virtual const double NPbase::deltaG_hAARatio_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1082 of file NPbase.h.

    {
        return deltaG_hAARatio();
    };

◆ deltaG_hff()

virtual gslpp::complex NPbase::deltaG_hff ( const Particle p ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 951 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG_hff_mu()

virtual gslpp::complex NPbase::deltaG_hff_mu	(	const Particle	p,
		const double	mu
	)		const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1093 of file NPbase.h.

    {
        return deltaG_hff(p);
    };

◆ deltaG_hgg()

virtual const double NPbase::deltaG_hgg ( ) const

inlinevirtual

The new physics contribution to the coupling of the effective interaction $H G_{\mu\nu}^AG^{A \mu\nu}$.

Returns: $\delta g_{HGG}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 842 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG_hgg_mu()

virtual const double NPbase::deltaG_hgg_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 971 of file NPbase.h.

    {
        return deltaG_hgg();
    };

◆ deltaG_hggRatio()

virtual const double NPbase::deltaG_hggRatio ( ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 851 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG_hggRatio_mu()

virtual const double NPbase::deltaG_hggRatio_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 981 of file NPbase.h.

    {
        return deltaG_hggRatio();
    };

◆ deltaG_hhhRatio()

virtual const double NPbase::deltaG_hhhRatio ( ) const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 959 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaG_hhhRatio_mu()

virtual const double NPbase::deltaG_hhhRatio_mu ( const double mu ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1102 of file NPbase.h.

    {
        return deltaG_hhhRatio();
    };

◆ deltaGA_f()

const double NPbase::deltaGA_f ( const Particle f ) const

virtual

New physics contribution to the neutral-current axial-vector coupling $g_A^f$.

The neutral-current axial-vector coupling $g_A^f$ receives the new physics contribution via the oblique parameter $T$ and the shift in the Fermi constant, $\Delta G$:

\[ \delta g_A^f = \frac{g_{A,\mathrm{SM}}^f}{2} \left[ \alpha(M_Z^2)\, T - \Delta G \right]. \]

See [Ciuchini:2013pca] and references therein.

Parameters

[in] f a lepton or quark

Returns: $\delta g_A^f$

Reimplemented in NPEpsilons_pureNP, NPSTUZbbbarLR, NPZbbbar, NPZbbbarLinearized, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 213 of file NPbase.cpp.

{
    if (f.is("TOP")) return 0.;
    /* SM values */
    double alpha = trueSM.alphaMz();
    double gASM = trueSM.gA_f(f).real();
 
    return ( gASM * (alpha * obliqueT() - DeltaGF()) / 2.0);
}

◆ deltaGA_f_2()

virtual const double NPbase::deltaGA_f_2 ( const Particle f ) const

inlinevirtual

Reimplemented in NPSMEFTd6.

Definition at line 229 of file NPbase.h.

                                                             {
        return 0.0;
    }  //AG:added    

◆ deltaGamma_W()

virtual const double NPbase::deltaGamma_W ( ) const

inlinevirtual

The new physics contribution to the total decay width of the $W$ boson, $\delta \Gamma_W$.

Returns: $\delta \Gamma_W$ in GeV

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 394 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaGamma_Wff()

virtual const double NPbase::deltaGamma_Wff	(	const Particle	fi,
		const Particle	fj
	)		const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 363 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaGamma_Z()

const double NPbase::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 in NPSMEFTd6General.

Definition at line 372 of file NPbase.cpp.

{
    double deltaGamma_Z = 0.;
    bool nonZeroNP = false;
 
    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;
    }
 
    return deltaGamma_Z;
}

◆ deltaGamma_Z_2()

const double NPbase::deltaGamma_Z_2 ( ) const

virtual

The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the total decay width of the $Z$ boson, $\Delta \Gamma_Z^{(2)}$.

\[ \Delta \Gamma_{Z}^{(2)} = \Delta \Gamma_{Z,fer}^{(2)} + \Delta \Gamma_{Z,had}^{(2)} \]

Returns: $\Delta \Gamma_Z^{(2)}$ in GeV

Definition at line 347 of file NPbase.cpp.

{
    //AG:added
    double deltaGamma_Z_2 = 0.;
    
    bool nonZeroNP = false;
    double delGVl2[6], delGAl2[6], delGVq2[6], delGAq2[6];
    for (int p = 0; p < 6; ++p) {
        delGVl2[p] = deltaGV_f_2(leptons[p]);
        delGAl2[p] = deltaGA_f_2(leptons[p]);
        delGVq2[p] = deltaGV_f_2(quarks[p]);
        delGAq2[p] = deltaGA_f_2(quarks[p]);
        if (delGVq2[p]!=0.0 or delGAq2[p]!=0.0 or delGVl2[p]!=0.0 or delGAl2[p]!=0.0)
            nonZeroNP = true;
    }
 
    if (nonZeroNP) {
        for(int p=0; p<6; p++){
            deltaGamma_Z_2 += deltaGamma_Zf_2(leptons[p]) + deltaGamma_Zf_2(quarks[p]);
        }
    }
 
    return deltaGamma_Z_2;
}

◆ deltaGamma_Zf()

const double NPbase::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 in NPSMEFTd6General.

Definition at line 298 of file NPbase.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;
    
    if (f.is("LEPTON")) {
        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;
    }
 
    return deltaGamma_Zf;
}

◆ deltaGamma_Zf_2()

const double NPbase::deltaGamma_Zf_2 ( const Particle f ) const

virtual

The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the decay width of the $Z$ boson into a given fermion pair, $\Delta \Gamma_{Z,f}^{(2)}$.

$\newcommand{\nc}{\newcommand}$ $\nc{\gVfSM}{g_{V,f}^{SM}}$ $\nc{\gAfSM}{g_{A,f}^{SM}}$ $\nc{\gVfL}{\Delta g_{V,f}^{(1)}}$ $\nc{\gAfL}{\Delta g_{A,f}^{(1)}}$ $\nc{\gVfQ}{\Delta g_{V,f}^{(2)}}$ $\nc{\gAfQ}{\Delta g_{A,f}^{(2)}}$

\[ \Delta \Gamma_{Z,f}^{(2)} = N_f \frac{\alpha(M_Z)^{SM} M_Z}{6 s_W^2 c_w^2} \left[ (\gVfL)^2 + (\gAfL)^2 + 2 \left( \gAfSM ~\gAfQ + \gVfSM ~\gVfQ \right) \right] \]

Parameters

[in] f a lepton or quark

Returns: $\Delta \Gamma_{Z,f}^{(2)}$ in GeV

Definition at line 265 of file NPbase.cpp.

{   
    //AG:added
    double DeltaGamma_Zf_2=0.0;
    
    double delGVf = deltaGV_f(f);
    double delGAf = deltaGA_f(f);  
    double delGVf2 = deltaGV_f_2(f);
    double delGAf2 = deltaGA_f_2(f);
    
    bool nonZeroNP = false;
    if (delGVf2!=0.0 || delGAf2!=0.0) {nonZeroNP = true;}
    
    if (nonZeroNP) {
        double Nf;
        if (f.is("LEPTON")) {
            Nf = 1.0;
        } else {
            Nf = 3.0;
        }
 
        double gVf = trueSM.gV_f(f).real();
        double gAf = trueSM.gA_f(f).real(); 
        double DelGammaZf2;
        
        DelGammaZf2 = Nf * ( 2.0*(gVf*delGVf2 + gAf*delGAf2) + delGVf*delGVf + delGAf*delGAf );
        //DeltaGamma_Zf_2 = 4.0 * GF * pow(Mz,3.0) / 24.0 / pow(2,0.5) / M_PI * DelGammaZf2;
        DeltaGamma_Zf_2 = alphaMz()*Mz / 12.0 / trueSM.sW2()/trueSM.cW2() * DelGammaZf2;
    }
 
    return DeltaGamma_Zf_2;
}

◆ deltaGamma_Zhad()

const double NPbase::deltaGamma_Zhad ( ) const

virtual

The new physics contribution to the hadronic decay width of the $Z$ boson, $\delta \Gamma_{Z,had}$.

Returns: $\delta \Gamma_{Z,had}$ in GeV

Definition at line 508 of file NPbase.cpp.

{
    double deltaGamma_Zhad = 0.;
    bool nonZeroNP = false;
 
    double delGVq[6], delGAq[6];
    for (int p = 0; p < 6; ++p) {
        delGVq[p] = deltaGV_f(quarks[p]);
        delGAq[p] = deltaGA_f(quarks[p]);
        if (delGVq[p] != 0.0 || delGAq[p] != 0.0)
            nonZeroNP = true;
    }
 
    if (nonZeroNP) {
        double gVf, gAf;
        double deltaGq[6];
        double delGammaZhad = 0.0;
        for (int p = 0; p < 6; ++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]);
 
            delGammaZhad += 3.0 * deltaGq[p];
        }
 
        double alpha = trueSM.alphaMz();
        double sW2_SM = trueSM.sW2();
        double cW2_SM = trueSM.cW2();
        deltaGamma_Zhad = alpha * Mz / 12.0 / sW2_SM / cW2_SM
                * delGammaZhad;
    }
 
    return deltaGamma_Zhad;
}

◆ deltaGamma_Zhad_2()

const double NPbase::deltaGamma_Zhad_2 ( ) const

virtual

The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the hadronic decay width of the $Z$ boson, $\Delta \Gamma_{Z,had}^{(2)}$.

\[ \Delta \Gamma_{Z,had}^{(2)} = \Delta \Gamma_{Z,u}^{(2)} + \Delta \Gamma_{Z,d}^{(2)} + \Delta \Gamma_{Z,c}^{(2)} + \Delta \Gamma_{Z,s}^{(2)} + \Delta \Gamma_{Z,b}^{(2)} \]

Returns: $\Delta \Gamma_{Z,had}^{(2)}$ in GeV

Definition at line 487 of file NPbase.cpp.

{
    //AG:added
    double DeltaGamma_Zhad_2 = 0.;
    bool nonZeroNP = false;
    double delGVq2[6], delGAq2[6];
    for (int p = 0; p < 6; ++p) {
        delGVq2[p] = deltaGV_f_2(quarks[p]);
        delGAq2[p] = deltaGA_f_2(quarks[p]);
        if (delGVq2[p] != 0.0 || delGAq2[p] != 0.0) {nonZeroNP = true;}
    }
    
    if (nonZeroNP) {
        for(int p=0; p<6; p++){
            DeltaGamma_Zhad_2 += deltaGamma_Zf_2(quarks[p]);
        }
    }
    
    return DeltaGamma_Zhad_2;
}

◆ deltaGammaHbbRatio1()

virtual const double NPbase::deltaGammaHbbRatio1 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1989 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHbbRatio2()

virtual const double NPbase::deltaGammaHbbRatio2 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1993 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHccRatio1()

virtual const double NPbase::deltaGammaHccRatio1 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2016 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHccRatio2()

virtual const double NPbase::deltaGammaHccRatio2 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2020 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHgagaRatio1()

virtual const double NPbase::deltaGammaHgagaRatio1 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1971 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHgagaRatio2()

virtual const double NPbase::deltaGammaHgagaRatio2 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1975 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHggRatio1()

virtual const double NPbase::deltaGammaHggRatio1 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1944 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHggRatio2()

virtual const double NPbase::deltaGammaHggRatio2 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1948 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHmumuRatio1()

virtual const double NPbase::deltaGammaHmumuRatio1 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1998 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHmumuRatio2()

virtual const double NPbase::deltaGammaHmumuRatio2 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2002 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHtautauRatio1()

virtual const double NPbase::deltaGammaHtautauRatio1 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2007 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHtautauRatio2()

virtual const double NPbase::deltaGammaHtautauRatio2 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2011 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHWWRatio1()

virtual const double NPbase::deltaGammaHWWRatio1 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1953 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHWWRatio2()

virtual const double NPbase::deltaGammaHWWRatio2 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1957 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHZgaRatio1()

virtual const double NPbase::deltaGammaHZgaRatio1 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1980 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHZgaRatio2()

virtual const double NPbase::deltaGammaHZgaRatio2 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1984 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHZZRatio1()

virtual const double NPbase::deltaGammaHZZRatio1 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1962 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaHZZRatio2()

virtual const double NPbase::deltaGammaHZZRatio2 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1966 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaTotalRatio1()

virtual const double NPbase::deltaGammaTotalRatio1 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2025 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaGammaTotalRatio2()

virtual const double NPbase::deltaGammaTotalRatio2 ( ) const

inlinevirtual

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2029 of file NPbase.h.

    {
        return 0.0;
    }

◆ DeltaGF()

virtual const double NPbase::DeltaGF ( ) const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 117 of file NPbase.h.

    {
        return 0.;
    }

◆ deltaGL_f_mu()

const double NPbase::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 (for those models where it is available)

Returns: $\delta g_L^f(\mu)$

Definition at line 240 of file NPbase.cpp.

{
    // Default: No scale dependence
    return 0.5 * ( deltaGV_f(p) + deltaGA_f(p) );
}

◆ deltaGL_Wff()

virtual gslpp::complex NPbase::deltaGL_Wff	(	const Particle	pbar,
		const Particle	p
	)		const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 300 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaGL_Wff_mu()

gslpp::complex NPbase::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 in NPSMEFTd6General.

Definition at line 253 of file NPbase.cpp.

{
    // Default: No scale dependence
    return deltaGL_Wff(pbar, p);
}

◆ deltaGR_f_mu()

const double NPbase::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 (for those models where it is available)

Returns: $\delta g_R^f(\mu)$

Definition at line 247 of file NPbase.cpp.

{
    // Default: No scale dependence
    return 0.5 * ( deltaGV_f(p) - deltaGA_f(p) );
}

◆ deltaGR_Wff()

virtual gslpp::complex NPbase::deltaGR_Wff	(	const Particle	pbar,
		const Particle	p
	)		const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 311 of file NPbase.h.

    {
        return 0.0;
    };

◆ deltaGR_Wff_mu()

gslpp::complex NPbase::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 in NPSMEFTd6General.

Definition at line 259 of file NPbase.cpp.

{
    // Default: No scale dependence
    return deltaGR_Wff(pbar, p);
}

◆ deltaGV_f()

const double NPbase::deltaGV_f ( const Particle f ) const

virtual

New physics contribution to the neutral-current vector coupling $g_V^f$.

The neutral-current vector coupling $g_V^f$ receives the new physics contribution via the oblique parameters $S$ and $T$ and the shift in the Fermi constant, $\Delta G$:

\[ \delta g_V^f = \frac{g_{V,\mathrm{SM}}^f}{2} \left[ \alpha(M_Z^2)\, T - \Delta G \right] + \frac{\big( g_{V,\mathrm{SM}}^f - g_{A,\mathrm{SM}}^f \big) \left[ \alpha(M_Z^2)\left( S - 4\,c_W^2s_W^2\, T \right) + 4\,c_W^2s_W^2\, \Delta G \right]}{4s_W^2\,(c_W^2-s_W^2)}\,. \]

See [Ciuchini:2013pca] and references therein.

Parameters

[in] f a lepton or quark

Returns: $\delta g_V^f$

Reimplemented in NPEpsilons_pureNP, NPSTUZbbbarLR, NPZbbbar, NPZbbbarLinearized, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 190 of file NPbase.cpp.

{
    if (f.is("TOP")) return 0.;
 
    /* SM values */
    double alpha = trueSM.alphaMz();
    double sW2SM = trueSM.sW2();
    double cW2SM = trueSM.cW2();
    double gVSM = trueSM.gV_f(f).real();
    double gASM = trueSM.gA_f(f).real();
 
    return ( gVSM * (alpha * obliqueT() - DeltaGF()) / 2.0
            + (gVSM - gASM) / 4.0 / sW2SM / (cW2SM - sW2SM)
            *(alpha * (obliqueS() - 4.0 * cW2SM * sW2SM * obliqueT())
            + 4.0 * cW2SM * sW2SM * DeltaGF()));
}

◆ deltaGV_f_2()

virtual const double NPbase::deltaGV_f_2 ( const Particle f ) const

inlinevirtual

Reimplemented in NPSMEFTd6.

Definition at line 191 of file NPbase.h.

                                                             {
        return 0.0;
    }  //AG:added

◆ deltaKgammaNP()

virtual const double NPbase::deltaKgammaNP ( const double mu ) const

inlinevirtual

The new physics contribution to the anomalous triple gauge coupling $\kappa_{\gamma}$.

Returns: $\delta \kappa_{\gamma}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 3140 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaKgammaNPEff()

virtual const double NPbase::deltaKgammaNPEff ( ) const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 3172 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaN_nu()

const double NPbase::deltaN_nu ( ) const

virtual

The new physics contribution to the number of neutrinos dervied from the $Z$ pole measurements.

Returns: $\delta N_{\nu}$

Definition at line 1106 of file NPbase.cpp.

{   
    double dNnu = 0.0;
    double dGl1, dGl2, dGl3, dGl, dGinv;
    double Gl1, Gl2, Gl3, Gl, Ginv;
    double dRl1, dRl2, dRl3, dRl;
    double Rl1, Rl2, Rl3, Rl;
    double shad0;
    
    dGl1 = deltaGamma_Zf(leptons[ELECTRON]);
    dGl2 = deltaGamma_Zf(leptons[MU]);
    dGl3 = deltaGamma_Zf(leptons[TAU]);
    
    dGl = (1.0/3.0) * (dGl1 + dGl2 + dGl3);
    
    Gl1 = trueSM.GammaZ(leptons[ELECTRON]);
    Gl2 = trueSM.GammaZ(leptons[MU]);
    Gl3 = trueSM.GammaZ(leptons[TAU]);
    
    Gl = (1.0/3.0) * (Gl1 + Gl2 + Gl3);
    
    dGinv = deltaGamma_Zf(leptons[NEUTRINO_1]) + 
            deltaGamma_Zf(leptons[NEUTRINO_2]) +
            deltaGamma_Zf(leptons[NEUTRINO_3]);
    
    Ginv = trueSM.GammaZ(leptons[NEUTRINO_1]) + 
            trueSM.GammaZ(leptons[NEUTRINO_2]) +
            trueSM.GammaZ(leptons[NEUTRINO_3]);
    
    dRl1 = deltaR0_f(leptons[ELECTRON]);
    dRl2 = deltaR0_f(leptons[MU]);
    dRl3 = deltaR0_f(leptons[TAU]);
    
    dRl = (1.0/3.0) * (dRl1 + dRl2 + dRl3);
    
    Rl1 = trueSM.R0_f(leptons[ELECTRON]);
    Rl2 = trueSM.R0_f(leptons[MU]);
    Rl3 = trueSM.R0_f(leptons[TAU]);
    
    Rl = (1.0/3.0) * (Rl1 + Rl2 + Rl3);
    
    shad0 = trueSM.sigma0_had();
    
    dNnu = (trueSM.N_nu())*( dGl/Gl - dGinv/Ginv ) -
            3.0*(Gl/Ginv)*dRl +
            (Gl/Ginv)*sqrt(3.0*M_PI*Rl/Mz/Mz/shad0)*(-3.0*deltaSigmaHadron()/shad0 + 3.0* dRl/Rl);
 
    return dNnu;
}

◆ deltaR0_f()

const double NPbase::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 in NPSMEFTd6General.

Definition at line 992 of file NPbase.cpp.

{
    double dR0_f = 0., delGVl = 0., delGAl = 0., deltaGl = 0., Gl = 0.;
    bool nonZeroNP = false;
    if (f.is("LEPTON")) {
        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")) {
            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 ( 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;
    }
    return dR0_f;
}

◆ deltaR0_f_2()

const double NPbase::deltaR0_f_2 ( const Particle f ) const

virtual

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:

\[ \Delta R_l^{(2)} = \frac{ \Gamma_{had}^{SM}~(\Delta \Gamma_l^{(1)})^2}{(\Gamma_l^{SM})^3} - \frac{\Delta \Gamma_{had}^{(1)}~\Delta \Gamma_l^{(1)}}{(\Gamma_l^{SM})^2} + \frac{ \Gamma_l^{SM} ~\Delta \Gamma_{had}^{(2)} - \Gamma_{had}^{SM} ~\Delta \Gamma_l^{(2)}}{(\Gamma_l^{SM})^2} \]

\[ \Delta R_q^{(2)} = \frac{ \Gamma_{q}^{SM}~(\Delta \Gamma_{had}^{(1)})^2}{(\Gamma_{had}^{SM})^3} - \frac{\Delta \Gamma_q^{(1)}~\Delta \Gamma_{had}^{(1)}}{(\Gamma_{had}^{SM})^2} + \frac{ \Gamma_{had}^{SM} ~\Delta \Gamma_q^{(2)} - \Gamma_q^{SM} ~\Delta \Gamma_{had}^{(2)}}{(\Gamma_{had}^{SM})^2} \]

\[ \Delta R_{\nu}^{(2)} = \frac{ \Gamma_{\nu}^{SM}~(\Delta \Gamma_{had}^{(1)})^2}{(\Gamma_{had}^{SM})^3} - \frac{\Delta \Gamma_{\nu}^{(1)}~\Delta \Gamma_{had}^{(1)}}{(\Gamma_{had}^{SM})^2} + \frac{ \Gamma_{had}^{SM} ~\Delta \Gamma_{\nu}^{(2)} - \Gamma_{\nu}^{SM} ~\Delta \Gamma_{had}^{(2)}}{(\Gamma_{had}^{SM})^2} \]

Parameters

f	a lepton or quark

Returns: $\Delta R_f^{0 (2)}$

Definition at line 936 of file NPbase.cpp.

{
    //AG:added
    double dR0_f_2 = 0.;
    double delGVl2=0.0, delGAl2=0.0, delGVq2[6], delGAq2[6];
    bool nonZeroNP = false;
    if (f.is("LEPTON")) {
        delGAl2 = deltaGA_f_2(f);
        delGVl2 = deltaGV_f_2(f);
        if (delGVl2!=0.0 || delGAl2!=0.0) {nonZeroNP = true;}
    }
    for (int q = 0; q < 6; ++q) {
        delGVq2[q] = deltaGV_f_2(quarks[q]);
        delGAq2[q] = deltaGA_f_2(quarks[q]);
        if (delGVq2[q]!=0.0 || delGAq2[q]!=0.0) {nonZeroNP = true;}
    }
   
    if (nonZeroNP) {
        //double prefactor = 4.0 * GF*pow(Mz,3.0)/24.0/sqrt(2.0)/M_PI; // It will cancel in the ratio either way
        double prefactor = alphaMz()*Mz / 12.0 / trueSM.sW2()/trueSM.cW2();
        
        double Gamma_l_SMtree = 1.0 * prefactor * ( pow(trueSM.gV_f(f).real(),2.0) + pow(trueSM.gA_f(f).real(),2.0) );
        double Gamma_q_SMtree = 3.0 * prefactor * ( pow(trueSM.gV_f(f).real(),2.0) + pow(trueSM.gA_f(f).real(),2.0) );
        
        double Gamma_had_SMtree = 0.0;
        for (int q = 0; q < 6; ++q) {
            Gamma_had_SMtree += 3.0 * prefactor * ( pow(trueSM.gV_f(quarks[q]).real(),2.0) + pow(trueSM.gA_f(quarks[q]).real(),2.0) );
        };
        
        double deltaGamma_f = deltaGamma_Zf(f);        
        double deltaGamma_had = deltaGamma_Zhad();
        
        double deltaGamma_f_2 = deltaGamma_Zf_2(f);        
        double deltaGamma_had_2 = deltaGamma_Zhad_2();
        
        // There may be s mistake in the charged leptons case:
        if(f.is("ELECTRON") || f.is("MU") || f.is("TAU")){
            dR0_f_2 =  Gamma_had_SMtree*pow(deltaGamma_f,2.0) / pow(Gamma_l_SMtree,3.0)
                     - deltaGamma_had*deltaGamma_f / pow(Gamma_l_SMtree,2.0)
                     + (Gamma_l_SMtree*deltaGamma_had_2-Gamma_had_SMtree*deltaGamma_f_2) / pow(Gamma_l_SMtree,2.0);
        }
        if(f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3")){
            dR0_f_2 = Gamma_l_SMtree*pow(deltaGamma_had,2.0) / pow(Gamma_had_SMtree,3.0)
                     - deltaGamma_f*deltaGamma_had / pow(Gamma_had_SMtree,2.0)
                     + (Gamma_had_SMtree*deltaGamma_f_2-Gamma_l_SMtree*deltaGamma_had_2) / pow(Gamma_had_SMtree,2.0);
        }
        if(f.is("QUARK")){
            dR0_f_2 = Gamma_q_SMtree*pow(deltaGamma_had,2.0) / pow(Gamma_had_SMtree,3.0)
                     - deltaGamma_f*deltaGamma_had / pow(Gamma_had_SMtree,2.0)
                     + (Gamma_had_SMtree*deltaGamma_f_2-Gamma_q_SMtree*deltaGamma_had_2) / pow(Gamma_had_SMtree,2.0);
        }
    }
    
    return dR0_f_2;
}

◆ deltaR_inv()

const double NPbase::deltaR_inv ( ) const

virtual

The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the $Z$ boson, $\delta R_{inv}$.

Returns: $\delta R_{inv}$

Definition at line 1056 of file NPbase.cpp.

{
    double dR_inv = 0., delGVe = 0., delGAe = 0., deltaGe = 0., Ge = 0.;
    bool nonZeroNP = false;
 
    delGVe = deltaGV_f(leptons[ELECTRON]);
    delGAe = deltaGA_f(leptons[ELECTRON]);
    if (delGVe != 0.0 || delGAe != 0.0) nonZeroNP = true;
 
    double delGVnu[3], delGAnu[3];
    for (int p = 0; p < 3; ++p) {
        delGVnu[p] = deltaGV_f(leptons[2*p]);
        delGAnu[p] = deltaGA_f(leptons[2*p]);
        if (delGVnu[p] != 0.0 || delGAnu[p] != 0.0 ) nonZeroNP = true;
    }
 
    if (nonZeroNP) {
 
        double gVe = trueSM.gV_f(leptons[ELECTRON]).real();
        double gAe = trueSM.gA_f(leptons[ELECTRON]).real();
        Ge = gVe * gVe + gAe * gAe;
        deltaGe = 2.0 * (gVe * delGVe + gAe * delGAe);
 
        double Gnu[3], deltaGnu[3];
        double gVnu, gAnu;
        double Gnu_sum = 0.0, delGnu_sum = 0.0;
        for (int p = 0; p < 3; ++p) {
            gVnu = trueSM.gV_f(leptons[2*p]).real();
            gAnu = trueSM.gA_f(leptons[2*p]).real();
              
 
            Gnu[p] = gVnu * gVnu + gAnu * gAnu;
 
            deltaGnu[p] = 2.0 * (gVnu * delGVnu[p] + gAnu * delGAnu[p]);
 
            Gnu_sum += Gnu[p];
            delGnu_sum += deltaGnu[p];
        }
 
        dR_inv = delGnu_sum / Ge - Gnu_sum * deltaGe / Ge / Ge;
    }
    return dR_inv;
}

◆ deltaRuc()

const double NPbase::deltaRuc ( ) const

virtual

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:

\[ \Delta R_{uc} = \frac{1}{2} \left(\Delta R_u^{(1)} + \Delta R_c^{(1)} \right) \]

Returns: $\Delta R_{uc}^{(1)}$

Definition at line 443 of file NPbase.cpp.

{
    //AG:added
    double DeltaRuc = 0.0;
    
    bool nonZeroNP=false;
    if(deltaR0_f(quarks[UP])!=0.0 || deltaR0_f(quarks[CHARM])!=0.0) { nonZeroNP = true;}
    
    if(nonZeroNP){
        // This keeps the same structure in SM. Should it be modified with a more general CKM assumption?
        DeltaRuc = 0.5 * ( deltaR0_f(quarks[UP]) + deltaR0_f(quarks[CHARM]) );
    }
    
    return DeltaRuc;
}

◆ deltaRuc_2()

const double NPbase::deltaRuc_2 ( ) const

virtual

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:

\[ \Delta R_{uc}^{(2)} = \frac{1}{2} \left(\Delta R_u^{(2)} + \Delta R_c^{(2)} \right) \]

Returns: $\Delta R_{uc}^{(2)}$

Definition at line 427 of file NPbase.cpp.

{
    //AG:added
    double DeltaRuc_2 = 0.0;
    
    bool nonZeroNP=false;
    if(deltaR0_f_2(quarks[UP])!=0.0 || deltaR0_f_2(quarks[CHARM])!=0.0) { nonZeroNP = true;}
    
    if(nonZeroNP){
        // This keeps the same structure in SM. Should it be modified with a more general CKM assumption?
        DeltaRuc_2 = 0.5 * ( deltaR0_f_2(quarks[UP]) + deltaR0_f_2(quarks[CHARM]) );
    }
    
    return DeltaRuc_2;
}

◆ deltaSigmaHadron()

const double NPbase::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 in NPSMEFTd6General.

Definition at line 617 of file NPbase.cpp.

{
    double sigma_had = 0.;
    bool nonZeroNP = false;
 
    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);
    }
 
    return sigma_had;
}

◆ deltaSigmaHadron_2()

const double NPbase::deltaSigmaHadron_2 ( ) const

virtual

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, $\Delta \sigma_h^{0,(2)}$.

$\nc{\MZt}{\widetilde{M}_Z}$

\[ \Delta\sigma_{h}^{0,(2)} = \frac{12\pi}{\MZt^2} ~\frac{\Gamma_e^{SM} \Gamma_{had}^{SM}}{(\Gamma_Z^{SM})^2} ~ \left( \frac{\Delta\Gamma_e^{(2)}}{\Gamma_e^{SM}} + \frac{\Delta\Gamma_{had}^{(2)}}{\Gamma_{had}^{SM}} - 2 \frac{\Delta\Gamma_Z^{(2)}}{\Gamma_Z^{SM}} + \frac{\Delta\Gamma_e^{(1)} \Delta\Gamma_{had}^{(1)}}{\Gamma_e^{SM} \Gamma_{had}^{SM}} - 2 \frac{\Delta\Gamma_e^{(1)} \Delta\Gamma_Z^{(1)}}{\Gamma_e^{SM} \Gamma_Z^{SM}} - 2 \frac{\Delta\Gamma_{had}^{(1)} \Delta\Gamma_Z^{(1)}}{\Gamma_{had}^{SM} \Gamma_Z^{SM}} + 3 \frac{(\Delta\Gamma_Z^{(1)})^2}{(\Gamma_Z^{SM})^2} \right) \]

Returns: $\Delta \sigma_h^{0,(2)}$ in GeV $^{-2}$

Definition at line 561 of file NPbase.cpp.

{
    //AG:added
    double sigma_had_2 = 0.;
 
    bool nonZeroNP = false;
    double delGVl2[6], delGAl2[6], delGVq2[6], delGAq2[6];
    for (int p = 0; p < 6; ++p) {
        delGVl2[p] = deltaGV_f_2(leptons[p]);
        delGAl2[p] = deltaGA_f_2(leptons[p]);
        delGVq2[p] = deltaGV_f_2(quarks[p]);
        delGAq2[p] = deltaGA_f_2(quarks[p]);
        if (delGVl2[p]!=0.0 || delGAl2[p]!=0.0 || delGVq2[p]!=0.0 || delGAq2[p]!=0.0) 
            nonZeroNP = true;
    }
 
    if (nonZeroNP) {
        //double prefactor = 4.0 * GF*pow(Mz,3.0)/24.0/sqrt(2.0)/M_PI; // It will cancel in the ratio either way
        double prefactor = alphaMz()*Mz / 12.0 / trueSM.sW2()/trueSM.cW2();
        
        // tree-level SM:
        double Gamma_e_SM = 1.0 * prefactor * ( pow(trueSM.gV_f(leptons[ELECTRON]).real(),2.0) + pow(trueSM.gA_f(leptons[ELECTRON]).real(),2.0) );
        
        double Gamma_lep_SM = 0.0;
        double Gamma_had_SM = 0.0;
        for (int p = 0; p < 6; ++p) {
            Gamma_lep_SM += 1.0 * prefactor * ( pow(trueSM.gV_f(leptons[p]).real(),2.0) + pow(trueSM.gA_f(leptons[p]).real(),2.0) );
            if (quarks[p].getName()!="TOP") {
                Gamma_had_SM += 3.0 * prefactor * ( pow(trueSM.gV_f(quarks[p]).real(),2.0) + pow(trueSM.gA_f(quarks[p]).real(),2.0) );
            }
        };      
        double Gamma_Z_SM = Gamma_had_SM + Gamma_lep_SM;
        
        double dGamma_e = deltaGamma_Zf(leptons[ELECTRON]);        
        double dGamma_had = deltaGamma_Zhad();
        double dGamma_Z = deltaGamma_Z();
        
        double dGamma_e_2 = deltaGamma_Zf_2(leptons[ELECTRON]);        
        double dGamma_had_2 = deltaGamma_Zhad_2();
        double dGamma_Z_2 = deltaGamma_Z_2();
       
        // Then,
        sigma_had_2 = 12.0*M_PI/pow(Mz,2.0) * Gamma_e_SM*Gamma_had_SM/pow(Gamma_Z_SM,2.0) * (
                  dGamma_e_2/Gamma_e_SM 
                + dGamma_had_2/Gamma_had_SM 
                - 2.0*dGamma_Z_2/Gamma_Z_SM
                + dGamma_e*dGamma_had/Gamma_e_SM/Gamma_had_SM
                - 2.0*dGamma_e*dGamma_Z/Gamma_e_SM/Gamma_Z_SM
                - 2.0*dGamma_had*dGamma_Z/Gamma_had_SM/Gamma_Z_SM
                + 3.0*pow(dGamma_Z,2.0)/pow(Gamma_Z_SM,2.0)
                );
    }
 
    return sigma_had_2;
}

◆ deltaSin2thetaEff_e()

const double NPbase::deltaSin2thetaEff_e ( ) const

virtual

The new physics contribution to the effective electron/leptonic weak angle $\delta \sin^2\theta_{\rm eff}^{\rm lept}$ at the $Z$ pole.

Returns: $\delta \sin^2\theta_{\rm eff}^{\rm lept}$

Definition at line 700 of file NPbase.cpp.

{
    double sin2_theta_eff = 0.;
    double delGVf = deltaGV_f(leptons[ELECTRON]);
    double delGAf = deltaGA_f(leptons[ELECTRON]);
    if (delGVf != 0.0 || delGAf != 0.0) {
        double gVf = trueSM.gV_f(leptons[ELECTRON]).real();
        double gAf = trueSM.gA_f(leptons[ELECTRON]).real();
        double delGVfOverGAf = (gAf * delGVf - gVf * delGAf) / gAf / gAf;
 
        sin2_theta_eff = -delGVfOverGAf / 4.0;
    }
    return sin2_theta_eff;
}

◆ deltaSin2thetaEff_e_2()

const double NPbase::deltaSin2thetaEff_e_2 ( ) const

virtual

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.

$\nc{\gVlSM}{g_{V,e}^{SM}}$ $\nc{\gAlSM}{g_{A,e}^{SM}}$ $\nc{\gVlL}{\Delta g_{V,e}^{(1)}}$ $\nc{\gAlL}{\Delta g_{A,e}^{(1)}}$ $\nc{\gVlQ}{\Delta g_{V,e}^{(2)}}$ $\nc{\gAlQ}{\Delta g_{A,e}^{(2)}}$

\[ \Delta sin^2\theta_{eff,e}^{(2)} = \frac{1}{4}\frac{\gVlL ~\gAlL}{(\gAlSM)^2} -\frac{1}{4}\frac{\gVlSM ~(\gAlL)^2}{(\gAlSM)^3} - \frac{1}{4} \frac{ \gAlSM ~\gVlQ - \gVlSM ~\gAlQ}{(\gAlSM)^2} \]

Returns: $\Delta \sin^2\theta_{eff,e}^{(2)}$

Definition at line 677 of file NPbase.cpp.

{
    //AG:added
    double sin2_theta_eff_2=0.0;
    double delGVf = deltaGV_f(leptons[ELECTRON]);
    double delGAf = deltaGA_f(leptons[ELECTRON]);
    double delGVf2 = deltaGV_f_2(leptons[ELECTRON]);
    double delGAf2 = deltaGA_f_2(leptons[ELECTRON]);
    
    bool nonZeroNP = false;
    if (delGVf2!=0.0 || delGAf2!=0.0) {nonZeroNP = true;}
    
    if (nonZeroNP) {
        double gVf = trueSM.gV_f(leptons[ELECTRON]).real();
        double gAf = trueSM.gA_f(leptons[ELECTRON]).real();
        sin2_theta_eff_2 = 1.0/4.0 * delGVf * delGAf / pow(gAf,2.0)
                           - 1.0/4.0 * gVf * pow(delGAf,2.0) / pow(gAf,3.0)
                           - 1.0/4.0 * ( gAf*delGVf2 - gVf*delGAf2) / pow(gAf,2.0) ; 
    }
    
    return sin2_theta_eff_2;
}

◆ deltaSin2thetaEff_mu()

const double NPbase::deltaSin2thetaEff_mu ( ) const

virtual

The new physics contribution to the effective muonic weak angle $\delta \sin^2\theta_{\rm eff}^{\mu\mu}$ at the $Z$ pole.

Returns: $\delta \sin^2\theta_{\rm eff}^{\mu\mu}$

Definition at line 738 of file NPbase.cpp.

{
    double sin2_theta_eff = 0.;
    double delGVf = deltaGV_f(leptons[MU]);
    double delGAf = deltaGA_f(leptons[MU]);
    if (delGVf != 0.0 || delGAf != 0.0) {
        double gVf = trueSM.gV_f(leptons[MU]).real();
        double gAf = trueSM.gA_f(leptons[MU]).real();
        double delGVfOverGAf = (gAf * delGVf - gVf * delGAf) / gAf / gAf;
 
        sin2_theta_eff = -delGVfOverGAf / 4.0;
    }
    return sin2_theta_eff;
}

◆ deltaSin2thetaEff_mu_2()

const double NPbase::deltaSin2thetaEff_mu_2 ( ) const

virtual

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.

$\nc{\gVlSM}{g_{V,\mu}^{SM}}$ $\nc{\gAlSM}{g_{A,\mu}^{SM}}$ $\nc{\gVlL}{\Delta g_{V,\mu}^{(1)}}$ $\nc{\gAlL}{\Delta g_{A,\mu}^{(1)}}$ $\nc{\gVlQ}{\Delta g_{V,\mu}^{(2)}}$ $\nc{\gAlQ}{\Delta g_{A,\mu}^{(2)}}$

\[ \Delta sin^2\theta_{eff,\mu}^{(2)} = \frac{1}{4}\frac{\gVlL ~\gAlL}{(\gAlSM)^2} -\frac{1}{4}\frac{\gVlSM ~(\gAlL)^2}{(\gAlSM)^3} - \frac{1}{4} \frac{ \gAlSM ~\gVlQ - \gVlSM ~\gAlQ}{(\gAlSM)^2} \]

Returns: $\Delta \sin^2\theta_{eff,\mu}^{(2)}$

Definition at line 715 of file NPbase.cpp.

{
    //AG:added
    double sin2_theta_eff_2=0.0;
    double delGVf = deltaGV_f(leptons[MU]);
    double delGAf = deltaGA_f(leptons[MU]);
    double delGVf2 = deltaGV_f_2(leptons[MU]);
    double delGAf2 = deltaGA_f_2(leptons[MU]);
    
    bool nonZeroNP = false;
    if (delGVf2!=0.0 || delGAf2!=0.0) {nonZeroNP = true;}
    
    if (nonZeroNP) {
        double gVf = trueSM.gV_f(leptons[MU]).real();
        double gAf = trueSM.gA_f(leptons[MU]).real();
        sin2_theta_eff_2 = 1.0/4.0 * delGVf * delGAf / pow(gAf,2.0)
                           - 1.0/4.0 * gVf * pow(delGAf,2.0) / pow(gAf,3.0)
                           - 1.0/4.0 * ( gAf*delGVf2 - gVf*delGAf2) / pow(gAf,2.0) ; 
    }
    
    return sin2_theta_eff_2;
}

◆ deltaxseeWW4fLEP2()

virtual const double NPbase::deltaxseeWW4fLEP2	(	const double	sqrt_s,
		const int	fstate
	)		const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3202 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaxseeWWhadLEP2()

virtual const double NPbase::deltaxseeWWhadLEP2 ( const double sqrt_s ) const

inlinevirtual

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.

Returns: $\delta sigma$ [pb]

Definition at line 3268 of file NPbase.h.

    {
        return deltaxseeWW4fLEP2(sqrt_s, 0);
    }

◆ deltaxseeWWleptLEP2()

virtual const double NPbase::deltaxseeWWleptLEP2 ( const double sqrt_s ) const

inlinevirtual

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.

Returns: $\delta sigma$ [pb]

Definition at line 3224 of file NPbase.h.

    {
        return deltaxseeWW4fLEP2(sqrt_s, 11);
    }

◆ deltaxseeWWsemilLEP2()

virtual const double NPbase::deltaxseeWWsemilLEP2 ( const double sqrt_s ) const

inlinevirtual

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.

Returns: $\delta sigma$ [pb]

Definition at line 3246 of file NPbase.h.

    {
        return deltaxseeWW4fLEP2(sqrt_s, 10);
    } 

◆ deltaxseeWWtotLEP2()

virtual const double NPbase::deltaxseeWWtotLEP2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3290 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltayb_HB()

virtual const double NPbase::deltayb_HB ( const double mu ) const

inlinevirtual

The Higgs-basis coupling $\delta y_b$. (See LHCHXSWG-INT-2015-001 document.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta y_b$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4617 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltayc_HB()

virtual const double NPbase::deltayc_HB ( const double mu ) const

inlinevirtual

The Higgs-basis coupling $\delta y_c$. (See LHCHXSWG-INT-2015-001 document.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta y_c$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4639 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaymu_HB()

virtual const double NPbase::deltaymu_HB ( const double mu ) const

inlinevirtual

The Higgs-basis coupling $\delta y_\mu$. (See LHCHXSWG-INT-2015-001 document.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta y_\mu$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4661 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltays_HB()

virtual const double NPbase::deltays_HB ( const double mu ) const

inlinevirtual

The Higgs-basis coupling $\delta y_s$. (See LHCHXSWG-INT-2015-001 document.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta y_s$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4650 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltayt_HB()

virtual const double NPbase::deltayt_HB ( const double mu ) const

inlinevirtual

The Higgs-basis coupling $\delta y_t$. (See LHCHXSWG-INT-2015-001 document.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta y_t$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4606 of file NPbase.h.

    {
        return 0.0;
    }

◆ deltaytau_HB()

virtual const double NPbase::deltaytau_HB ( const double mu ) const

inlinevirtual

The Higgs-basis coupling $\delta y_\tau$. (See LHCHXSWG-INT-2015-001 document.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\delta y_\tau$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4628 of file NPbase.h.

    {
        return 0.0;
    }

◆ dxsdcoseeWWlvjjLEP2()

virtual const double NPbase::dxsdcoseeWWlvjjLEP2	(	const double	sqrt_s,
		const int	bin
	)		const

inlinevirtual

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]. Defined only for the NPSMEFTd6 class.

Returns: $d\sigma/d\cos{\theta}$ [pb]

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3302 of file NPbase.h.

    {
        return 0.0;
    }

◆ dxseeWWdcos()

virtual const double NPbase::dxseeWWdcos	(	const double	sqrt_s,
		const double	cos
	)		const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3324 of file NPbase.h.

    {
        return 0.0;
    }

◆ dxseeWWdcosBin()

virtual const double NPbase::dxseeWWdcosBin	(	const double	sqrt_s,
		const double	cos1,
		const double	cos2
	)		const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3334 of file NPbase.h.

    {
        return 0.0;
    }

◆ gA_f()

const gslpp::complex NPbase::gA_f ( const Particle f ) const

virtual

The total (SM+NP) contribution to the neutral-current axial-vector coupling $g_A^f$.

Parameters

[in] f a lepton or quark

Returns: $g_A^f$, including SM plus NP contributions

Reimplemented from StandardModel.

Reimplemented in NPEpsilons.

Definition at line 223 of file NPbase.cpp.

{
    //AG: deltaGA_f_2(f) added below
    return ( trueSM.gA_f(f) + deltaGA_f(f) + deltaGA_f_2(f) );
}

◆ Gamma_had()

const double NPbase::Gamma_had ( ) const

virtual

The hadronic decay width of the $Z$ boson, $\Gamma_{Z,had}$.

\Gamma_{Z,had} = \Gamma_Z,had}^{SM} + \Delta \Gamma_{Z,had}^{(1)} + \Delta \Gamma_{Z,had}^{(2)}

Returns: $\Gamma_{Z,had}$ 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 StandardModel.

Definition at line 544 of file NPbase.cpp.

{
    //AG: deltaGamma_Zhad_2() added below
    return (trueSM.Gamma_had() + deltaGamma_Zhad() + deltaGamma_Zhad_2());
}

◆ Gamma_Z()

const double NPbase::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 StandardModel.

Reimplemented in NPEpsilons, NPSMEFTd6General, and NPZbbbar.

Definition at line 414 of file NPbase.cpp.

{
    //AG:begin
    if(OutputOrder()==0){ return (trueSM.Gamma_Z() ); }
    if(OutputOrder()==1){ return (trueSM.Gamma_Z() + deltaGamma_Z()); }
    if(OutputOrder()==2){ return (trueSM.Gamma_Z() + deltaGamma_Z() + deltaGamma_Z_2() ); }
    if(OutputOrder()==3){ return (trueSM.Gamma_Z() + deltaGamma_Z_2() ); }
    else
    //AG:end
    //AG: deltaGamma_Z_2() added below
        return (trueSM.Gamma_Z() + deltaGamma_Z() + deltaGamma_Z_2());
}

◆ Gamma_Zf()

const double NPbase::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 in NPSMEFTd6General.

Definition at line 334 of file NPbase.cpp.

{
    //AG:begin
    if(OutputOrder()==0){ return (trueSM.GammaZ(f) ); }
    if(OutputOrder()==1){ return (trueSM.GammaZ(f) + deltaGamma_Zf(f)); }
    if(OutputOrder()==2){ return (trueSM.GammaZ(f) + deltaGamma_Zf(f) + deltaGamma_Zf_2(f) ); }
    if(OutputOrder()==3){ return (trueSM.GammaZ(f) + deltaGamma_Zf_2(f) ); }
    else
    //AG:end
    //AG: deltaGamma_Zf_2(f) added below
        return (trueSM.GammaZ(f) + deltaGamma_Zf(f) + deltaGamma_Zf_2(f));
}

◆ GammaHbbRatio()

virtual const double NPbase::GammaHbbRatio ( ) const

inlinevirtual

The ratio of the $\Gamma(H\to b\bar{b})$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to b\bar{b})$/ $\Gamma(H\to b\bar{b})_{\mathrm{SM}}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2136 of file NPbase.h.

    {
        return 1.0;
    }

◆ GammaHccRatio()

virtual const double NPbase::GammaHccRatio ( ) const

inlinevirtual

The ratio of the $\Gamma(H\to c\bar{c})$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to c\bar{c})$/ $\Gamma(H\to c\bar{c})_{\mathrm{SM}}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2116 of file NPbase.h.

    {
        return 1.0;
    }

◆ GammaHgagaRatio()

virtual const double NPbase::GammaHgagaRatio ( ) const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2083 of file NPbase.h.

    {
        return 1.0;
    }

◆ GammaHggRatio()

virtual const double NPbase::GammaHggRatio ( ) const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2043 of file NPbase.h.

    {
        return 1.0;
    }

◆ GammaHmumuRatio()

virtual const double NPbase::GammaHmumuRatio ( ) const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2096 of file NPbase.h.

    {
        return 1.0;
    }

◆ GammaHssRatio()

virtual const double NPbase::GammaHssRatio ( ) const

inlinevirtual

The ratio of the $\Gamma(H\to s\bar{s})$ in the current model and in the Standard Model.

Returns: $\Gamma(H\to s\bar{s})$/ $\Gamma(H\to s\bar{s})_{\mathrm{SM}}$

Reimplemented in NPSMEFTd6General.

Definition at line 2126 of file NPbase.h.

    {
        return 1.0;
    }

◆ GammaHtautauRatio()

virtual const double NPbase::GammaHtautauRatio ( ) const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2106 of file NPbase.h.

    {
        return 1.0;
    }

◆ GammaHWWRatio()

virtual const double NPbase::GammaHWWRatio ( ) const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2053 of file NPbase.h.

    {
        return 1.0;
    }

◆ GammaHZgaRatio()

virtual const double NPbase::GammaHZgaRatio ( ) const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2073 of file NPbase.h.

    {
        return 1.0;
    }

◆ GammaHZZRatio()

virtual const double NPbase::GammaHZZRatio ( ) const

inlinevirtual

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 in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 2063 of file NPbase.h.

    {
        return 1.0;
    }

◆ GammaW() [1/2]

const double NPbase::GammaW ( ) const

virtual

The total width of the $W$ boson, $\Gamma_W$.

The $W$-boson width receives the new physics contribution via the oblique parameters $S$, $T$ and $U$ and the shift in the Fermi constant, $\Delta G$:

\[ \Gamma_W = \Gamma_{W,\mathrm{SM}} \left[ 1 - \frac{3\alpha(M_Z^2)}{4(c_W^2-s_W^2)} \left( S - 2c_W^2\,T - \frac{c_W^2-s_W^2}{2s_W^2}\,U \right) - \frac{1+c_W^2}{2(c_W^2-s_W^2)}\, \Delta G \right]. \]

See [Ciuchini:2013pca] and references therein.

Returns: $\Gamma_W$ in GeV

Reimplemented from StandardModel.

Reimplemented in NPEpsilons, NPEpsilons_pureNP, NPSMEFTd6, NPSMEFTd6General, NPSTUVWXY, and NPZbbbar.

Definition at line 118 of file NPbase.cpp.

{
    double Gamma_W = trueSM.GammaW();
 
    double alpha = trueSM.alphaMz();
    double c2 = trueSM.cW2();
    double s2 = trueSM.sW2();
 
    Gamma_W *= 1.0 - 3.0 * alpha / 4.0 / (c2 - s2)
            *(obliqueS() - 2.0 * c2 * obliqueT() - (c2 - s2) * obliqueU() / 2.0 / s2)
            - (1.0 + c2) / 2.0 / (c2 - s2) * DeltaGF();
 
    //std::cout << "Gw: c_S=" << - 3.0*alpha/4.0/(c2-s2) << std::endl;
    //std::cout << "Gw: c_T=" << - 3.0*alpha/4.0/(c2-s2)*(- 2.0*c2) << std::endl;
    //std::cout << "Gw: c_U=" << - 3.0*alpha/4.0/(c2-s2)*(- (c2-s2)/2.0/s2) << std::endl;
 
    return Gamma_W;
}

◆ GammaW() [2/2]

const double NPbase::GammaW	(	const Particle	fi,
		const Particle	fj
	)		const

virtual

A partial decay width of the $W$ boson decay into a SM fermion pair.

The partial $W$-boson widths receives the new physics contribution via the oblique parameters $S$, $T$ and $U$ and the shift in the Fermi constant, $\Delta G$:

\[ \Gamma_W^{ij} = \Gamma_{W,\mathrm{SM}} \left[ 1 - \frac{3\alpha(M_Z^2)}{4(c_W^2-s_W^2)} \left( S - 2c_W^2\,T - \frac{c_W^2-s_W^2}{2s_W^2}\,U \right) - \frac{1+c_W^2}{2(c_W^2-s_W^2)}\, \Delta G \right]. \]

Parameters

[in]	fi	a lepton or quark
[in]	fj	a lepton or quark

Returns: $\Gamma^W_{ij}$

Attention: Fermion masses are neglected.

Reimplemented from StandardModel.

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 99 of file NPbase.cpp.

{
    double Gamma_Wij = trueSM.GammaW(fi, fj);
 
    double alpha = trueSM.alphaMz();
    double c2 = trueSM.cW2();
    double s2 = trueSM.sW2();
 
    Gamma_Wij *= 1.0 - 3.0 * alpha / 4.0 / (c2 - s2)
            *(obliqueS() - 2.0 * c2 * obliqueT() - (c2 - s2) * obliqueU() / 2.0 / s2)
            - (1.0 + c2) / 2.0 / (c2 - s2) * DeltaGF();
 
    //std::cout << "Gw: c_S=" << - 3.0*alpha/4.0/(c2-s2) << std::endl;
    //std::cout << "Gw: c_T=" << - 3.0*alpha/4.0/(c2-s2)*(- 2.0*c2) << std::endl;
    //std::cout << "Gw: c_U=" << - 3.0*alpha/4.0/(c2-s2)*(- (c2-s2)/2.0/s2) << std::endl;
 
    return Gamma_Wij;
}

◆ getTrueSM()

virtual const StandardModel & NPbase::getTrueSM ( ) const

inlinevirtual

A method to return a StandardModel object from NPbase.

Returns: an StandardModel object

Reimplemented from StandardModel.

Definition at line 86 of file NPbase.h.

    {
        return trueSM;
    }

◆ gV_f()

const gslpp::complex NPbase::gV_f ( const Particle f ) const

virtual

The total (SM+NP) contribution to the neutral-current vector coupling $g_V^f$.

Parameters

[in] f a lepton or quark

Returns: $g_V^f$, including SM plus NP contributions

Reimplemented from StandardModel.

Reimplemented in NPEpsilons.

Definition at line 207 of file NPbase.cpp.

{
    //AG: deltaGV_f_2(f) added below.
    return ( trueSM.gV_f(f) + deltaGV_f(f) + deltaGV_f_2(f) );
}

◆ kappaAeff()

virtual const double NPbase::kappaAeff ( ) const

inlinevirtual

The effective coupling $\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}$.

Returns: $\kappa_{A,eff}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4584 of file NPbase.h.

    {
        return 1.0;
    }

◆ kappabeff()

virtual const double NPbase::kappabeff ( ) const

inlinevirtual

The effective coupling $\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}$.

Returns: $\kappa_{b,eff}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4530 of file NPbase.h.

    {
        return 1.0;
    }

◆ kappaceff()

virtual const double NPbase::kappaceff ( ) const

inlinevirtual

The effective coupling $\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}$.

Returns: $\kappa_{c,eff}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4521 of file NPbase.h.

    {
        return 1.0;
    }

◆ kappaGeff()

virtual const double NPbase::kappaGeff ( ) const

inlinevirtual

The effective coupling $\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}$.

Returns: $\kappa_{G,eff}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4539 of file NPbase.h.

    {
        return 1.0;
    }

◆ kappamueff()

virtual const double NPbase::kappamueff ( ) const

inlinevirtual

The effective coupling $\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}$.

Returns: $\kappa_{\mu,eff}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4503 of file NPbase.h.

    {
        return 1.0;
    }

◆ kappataueff()

virtual const double NPbase::kappataueff ( ) const

inlinevirtual

The effective coupling $\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}$.

Returns: $\kappa_{\tau,eff}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4512 of file NPbase.h.

    {
        return 1.0;
    }

◆ kappaW4feff()

virtual const double NPbase::kappaW4feff ( ) const

inlinevirtual

The effective coupling $\kappa_{W4f,eff}=\sqrt{\Gamma_{H4f, CC}/\Gamma_{H4f, CC}^{SM}}$.

Returns: $\kappa_{W4f,eff}$

Reimplemented in NPSMEFTd6General.

Definition at line 4575 of file NPbase.h.

    {
        return 1.0;
    }

◆ kappaWeff()

virtual const double NPbase::kappaWeff ( ) const

inlinevirtual

The effective coupling $\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}$.

Returns: $\kappa_{W,eff}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4557 of file NPbase.h.

    {
        return 1.0;
    }

◆ kappaZ4feff()

virtual const double NPbase::kappaZ4feff ( ) const

inlinevirtual

The effective coupling $\kappa_{Z4f,eff}=\sqrt{\Gamma_{H4f, NC}/\Gamma_{H4f, NC}^{SM}}$.

Returns: $\kappa_{Z4f,eff}$

Reimplemented in NPSMEFTd6General.

Definition at line 4566 of file NPbase.h.

    {
        return 1.0;
    }

◆ kappaZ_f()

const gslpp::complex NPbase::kappaZ_f ( const Particle f ) const

virtual

The effective neutral-current coupling $\kappa_Z^f$ including SM plus NP contributions.

Parameters

[in] f a lepton or quark

Returns: $\kappa_Z^f$, including SM plus NP contributions

Reimplemented from StandardModel.

Reimplemented in NPEpsilons.

Definition at line 235 of file NPbase.cpp.

{
    return ( (1.0 - gV_f(f) / gA_f(f)) / (4.0 * fabs(f.getCharge()) * sW2()));
}

◆ kappaZAeff()

virtual const double NPbase::kappaZAeff ( ) const

inlinevirtual

The effective coupling $\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}$.

Returns: $\kappa_{ZA,eff}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4593 of file NPbase.h.

    {
        return 1.0;
    }

◆ kappaZeff()

virtual const double NPbase::kappaZeff ( ) const

inlinevirtual

The effective coupling $\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}$.

Returns: $\kappa_{Z,eff}$

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4548 of file NPbase.h.

    {
        return 1.0;
    }

◆ lambdaZNP()

virtual const double NPbase::lambdaZNP ( const double mu ) const

inlinevirtual

The new physics contribution to the anomalous triple gauge coupling $\lambda_{Z}$.

Returns: $\lambda_{Z}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 3149 of file NPbase.h.

    {
        return 0.0;
    }

◆ lambz_HB()

virtual const double NPbase::lambz_HB ( const double mu ) const

inlinevirtual

The Higgs-basis coupling $\lambda_{z}$. (See LHCHXSWG-INT-2015-001 document.)

Parameters

[in] mu the RG scale to be used in the evaluation

Returns: $\lambda_{z}$

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 4749 of file NPbase.h.

    {
        return 0.0;
    }

◆ mubbH()

virtual const double NPbase::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 in NPSMEFTd6General.

Definition at line 1420 of file NPbase.h.

    {
        return 1.0;
    }

◆ mueeHee()

virtual const double NPbase::mueeHee	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1203 of file NPbase.h.

    {
        return 1.0;
    }

◆ mueeHvv()

virtual const double NPbase::mueeHvv	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1176 of file NPbase.h.

    {
        return 1.0;
    }

◆ mueettH()

virtual const double NPbase::mueettH	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1456 of file NPbase.h.

    {
        return 1.0;
    }

◆ mueeWBF()

virtual const double NPbase::mueeWBF	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, THDMW, THDMWSignalStrengths, and NPSMEFTd6.

Definition at line 1162 of file NPbase.h.

    {
        return 1.0;
    }

◆ mueeWW()

virtual const double NPbase::mueeWW	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3357 of file NPbase.h.

    {
        return 1.0;
    }

◆ mueeZBF()

virtual const double NPbase::mueeZBF	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1190 of file NPbase.h.

    {
        return 1.0;
    }

◆ mueeZH()

virtual const double NPbase::mueeZH	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

inlinevirtual

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
[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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.

Definition at line 1299 of file NPbase.h.

    {
        return 1.0;
    }

◆ mueeZHGen()

virtual const double NPbase::mueeZHGen	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1285 of file NPbase.h.

    {
        return 1.0;
    }

◆ mueeZllH()

virtual const double NPbase::mueeZllH	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1312 of file NPbase.h.

    {
        return 1.0;
    }

◆ mueeZqqH()

virtual const double NPbase::mueeZqqH	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1325 of file NPbase.h.

    {
        return 1.0;
    }

◆ muepWBF()

virtual const double NPbase::muepWBF ( const double sqrt_s ) const

inlinevirtual

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 in HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1216 of file NPbase.h.

    {
        return 1.0;
    }

◆ muepZBF()

virtual const double NPbase::muepZBF ( const double sqrt_s ) const

inlinevirtual

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 in HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1228 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggH()

virtual const double NPbase::muggH ( const double sqrt_s ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.

Definition at line 1115 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHbb()

virtual const double NPbase::muggHbb ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1826 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHgaga()

virtual const double NPbase::muggHgaga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1555 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHgagaInt()

virtual const double NPbase::muggHgagaInt ( const double sqrt_s ) const

inlinevirtual

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,\gamma\gamma}$

Reimplemented in HiggsChiral, and HiggsKigen.

Definition at line 1588 of file NPbase.h.

    {
        return 1.0;        
    };

◆ muggHH()

virtual const double NPbase::muggHH ( const double sqrt_s ) const

inlinevirtual

The ratio $\mu_{ggHH}$ between the gluon-gluon fusion di-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: $\mu_{ggHH}$

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1126 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHmumu()

virtual const double NPbase::muggHmumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1758 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHpbbH_Hgaga()

virtual const double NPbase::muggHpbbH_Hgaga ( const double sqrt_s ) const

inlinevirtual

Definition at line 1567 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHpbbH_Htautau()

virtual const double NPbase::muggHpbbH_Htautau ( const double sqrt_s ) const

inlinevirtual

Definition at line 1798 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHpbbH_HWW()

virtual const double NPbase::muggHpbbH_HWW ( const double sqrt_s ) const

inlinevirtual

Definition at line 1706 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHpbbH_HZZ()

virtual const double NPbase::muggHpbbH_HZZ ( const double sqrt_s ) const

inlinevirtual

Definition at line 1649 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHpttH()

virtual const double NPbase::muggHpttH ( const double sqrt_s ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1443 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHpttHptHpbbH_Hmumu()

virtual const double NPbase::muggHpttHptHpbbH_Hmumu ( const double sqrt_s ) const

inlinevirtual

Definition at line 1786 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHpttHptHpbbH_HZga()

virtual const double NPbase::muggHpttHptHpbbH_HZga ( const double sqrt_s ) const

inlinevirtual

Definition at line 1637 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHpVBFpbbH_Hbb()

virtual const double NPbase::muggHpVBFpbbH_Hbb ( const double sqrt_s ) const

inlinevirtual

Definition at line 1830 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHtautau()

virtual const double NPbase::muggHtautau ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1794 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHWW()

virtual const double NPbase::muggHWW ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1702 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHWW2l2v()

virtual const double NPbase::muggHWW2l2v ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1734 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHZga()

virtual const double NPbase::muggHZga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1613 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHZZ()

virtual const double NPbase::muggHZZ ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1645 of file NPbase.h.

    {
        return 1.0;
    }

◆ muggHZZ4l()

virtual const double NPbase::muggHZZ4l ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1677 of file NPbase.h.

    {
        return 1.0;
    }

◆ mummH()

virtual const double NPbase::mummH ( const double sqrt_s ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1467 of file NPbase.h.

    {
        return 1.0;
    }

◆ mummHmm()

virtual const double NPbase::mummHmm ( const double sqrt_s ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1515 of file NPbase.h.

    {
        return 1.0;
    }

◆ mummHNWA()

virtual const double NPbase::mummHNWA ( const double sqrt_s ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1479 of file NPbase.h.

    {
        return 1.0;
    }

◆ mummHvv()

virtual const double NPbase::mummHvv ( const double sqrt_s ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1503 of file NPbase.h.

    {
        return 1.0;
    }

◆ mummttH()

virtual const double NPbase::mummttH ( const double sqrt_s ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1527 of file NPbase.h.

    {
        return 1.0;
    }

◆ mummZH()

virtual const double NPbase::mummZH ( const double sqrt_s ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1491 of file NPbase.h.

    {
        return 1.0;
    }

◆ muppHmumu()

virtual const double NPbase::muppHmumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, and THDMW.

Definition at line 1862 of file NPbase.h.

    {
        return 1.0;
    }

◆ muppHZga()

virtual const double NPbase::muppHZga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, and THDMW.

Definition at line 1866 of file NPbase.h.

    {
        return 1.0;
    }

◆ mupTVppWZ()

virtual const double NPbase::mupTVppWZ	(	const double	sqrt_s,
		const double	pTV1,
		const double	pTV2
	)		const

inlinevirtual

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 NPSMEFTd6 class.

Returns: $N_{ev}^{p_{TV}}/N_{ev,SM}^{p_{TV}}$

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3384 of file NPbase.h.

    {
        return 1.0;
    }

◆ mutH()

virtual const double NPbase::mutH ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 1409 of file NPbase.h.

    {
        return 1.0;
    }

◆ mutHgaga()

virtual const double NPbase::mutHgaga ( const double sqrt_s ) const

inlinevirtual

Definition at line 1561 of file NPbase.h.

    {
        return 1.0;
    }

◆ mutHq()

virtual const double NPbase::mutHq ( const double sqrt_s ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1431 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUggHbb()

virtual const double NPbase::muTHUggHbb ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3049 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUggHgaga()

virtual const double NPbase::muTHUggHgaga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2854 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUggHmumu()

virtual const double NPbase::muTHUggHmumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3001 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUggHtautau()

virtual const double NPbase::muTHUggHtautau ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3025 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUggHWW()

virtual const double NPbase::muTHUggHWW ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2953 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUggHWW2l2v()

virtual const double NPbase::muTHUggHWW2l2v ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2977 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUggHZga()

virtual const double NPbase::muTHUggHZga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2879 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUggHZgamumu()

virtual const double NPbase::muTHUggHZgamumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3099 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUggHZZ()

virtual const double NPbase::muTHUggHZZ ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2903 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUggHZZ4l()

virtual const double NPbase::muTHUggHZZ4l ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2928 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUggHZZ4mu()

virtual const double NPbase::muTHUggHZZ4mu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3094 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUttHbb()

virtual const double NPbase::muTHUttHbb ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3069 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUttHgaga()

virtual const double NPbase::muTHUttHgaga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2875 of file NPbase.h.

    {
        return 1.0;
    }   

◆ muTHUttHmumu()

virtual const double NPbase::muTHUttHmumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3021 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUttHtautau()

virtual const double NPbase::muTHUttHtautau ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3045 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUttHWW()

virtual const double NPbase::muTHUttHWW ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2973 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUttHWW2l2v()

virtual const double NPbase::muTHUttHWW2l2v ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2997 of file NPbase.h.

    {
        return 1.0;
    }   

◆ muTHUttHZga()

virtual const double NPbase::muTHUttHZga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2899 of file NPbase.h.

    {
        return 1.0;
    }  

◆ muTHUttHZZ()

virtual const double NPbase::muTHUttHZZ ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2923 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUttHZZ4l()

virtual const double NPbase::muTHUttHZZ4l ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2948 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVBFBRinv()

virtual const double NPbase::muTHUVBFBRinv ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3074 of file NPbase.h.

    {
        return 0.0;
    }

◆ muTHUVBFHbb()

virtual const double NPbase::muTHUVBFHbb ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3053 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVBFHgaga()

virtual const double NPbase::muTHUVBFHgaga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2859 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVBFHinv()

virtual const double NPbase::muTHUVBFHinv ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3079 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVBFHmumu()

virtual const double NPbase::muTHUVBFHmumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3005 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVBFHtautau()

virtual const double NPbase::muTHUVBFHtautau ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3029 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVBFHWW()

virtual const double NPbase::muTHUVBFHWW ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2957 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVBFHWW2l2v()

virtual const double NPbase::muTHUVBFHWW2l2v ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2981 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVBFHZga()

virtual const double NPbase::muTHUVBFHZga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2883 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVBFHZZ()

virtual const double NPbase::muTHUVBFHZZ ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2907 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVBFHZZ4l()

virtual const double NPbase::muTHUVBFHZZ4l ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2932 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVHbb()

virtual const double NPbase::muTHUVHbb ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3065 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVHBRinv()

virtual const double NPbase::muTHUVHBRinv ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3084 of file NPbase.h.

    {
        return 0.0;
    }

◆ muTHUVHgaga()

virtual const double NPbase::muTHUVHgaga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2871 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVHinv()

virtual const double NPbase::muTHUVHinv ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3089 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVHmumu()

virtual const double NPbase::muTHUVHmumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3017 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVHtautau()

virtual const double NPbase::muTHUVHtautau ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3041 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVHWW()

virtual const double NPbase::muTHUVHWW ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2969 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVHWW2l2v()

virtual const double NPbase::muTHUVHWW2l2v ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2993 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVHZga()

virtual const double NPbase::muTHUVHZga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2895 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVHZZ()

virtual const double NPbase::muTHUVHZZ ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2919 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUVHZZ4l()

virtual const double NPbase::muTHUVHZZ4l ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2944 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUWHbb()

virtual const double NPbase::muTHUWHbb ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3061 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUWHgaga()

virtual const double NPbase::muTHUWHgaga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2867 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUWHmumu()

virtual const double NPbase::muTHUWHmumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3013 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUWHtautau()

virtual const double NPbase::muTHUWHtautau ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3037 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUWHWW()

virtual const double NPbase::muTHUWHWW ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2965 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUWHWW2l2v()

virtual const double NPbase::muTHUWHWW2l2v ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2989 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUWHZga()

virtual const double NPbase::muTHUWHZga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2891 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUWHZZ()

virtual const double NPbase::muTHUWHZZ ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2915 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUWHZZ4l()

virtual const double NPbase::muTHUWHZZ4l ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2940 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUZHbb()

virtual const double NPbase::muTHUZHbb ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3057 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUZHgaga()

virtual const double NPbase::muTHUZHgaga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2863 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUZHmumu()

virtual const double NPbase::muTHUZHmumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3009 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUZHtautau()

virtual const double NPbase::muTHUZHtautau ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 3033 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUZHWW()

virtual const double NPbase::muTHUZHWW ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2961 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUZHWW2l2v()

virtual const double NPbase::muTHUZHWW2l2v ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2985 of file NPbase.h.

    {
        return 1.0;
    }

◆ muTHUZHZga()

virtual const double NPbase::muTHUZHZga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2887 of file NPbase.h.

    {
        return 1.0;
    }    

◆ muTHUZHZZ()

virtual const double NPbase::muTHUZHZZ ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2911 of file NPbase.h.

    {
        return 1.0;
    }    

◆ muTHUZHZZ4l()

virtual const double NPbase::muTHUZHZZ4l ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 2936 of file NPbase.h.

    {
        return 1.0;
    }    

◆ muttH()

virtual const double NPbase::muttH ( const double sqrt_s ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.

Definition at line 1398 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHbb()

virtual const double NPbase::muttHbb ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1850 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHgaga()

virtual const double NPbase::muttHgaga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1609 of file NPbase.h.

    {
        return 1.0;
    }   

◆ muttHgagaZeeboost()

virtual const double NPbase::muttHgagaZeeboost ( const double sqrt_s ) const

inlinevirtual

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 in HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.

Definition at line 1550 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHmumu()

virtual const double NPbase::muttHmumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1778 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHptH_Hbb()

virtual const double NPbase::muttHptH_Hbb ( const double sqrt_s ) const

inlinevirtual

Definition at line 1854 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHptH_Hgaga()

virtual const double NPbase::muttHptH_Hgaga ( const double sqrt_s ) const

inlinevirtual

Definition at line 1573 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHptH_Hmumu()

virtual const double NPbase::muttHptH_Hmumu ( const double sqrt_s ) const

inlinevirtual

Definition at line 1782 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHptH_Htautau()

virtual const double NPbase::muttHptH_Htautau ( const double sqrt_s ) const

inlinevirtual

Definition at line 1822 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHptH_HWW()

virtual const double NPbase::muttHptH_HWW ( const double sqrt_s ) const

inlinevirtual

Definition at line 1730 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHptH_HZZ()

virtual const double NPbase::muttHptH_HZZ ( const double sqrt_s ) const

inlinevirtual

Definition at line 1673 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHtautau()

virtual const double NPbase::muttHtautau ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1818 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHWW()

virtual const double NPbase::muttHWW ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1726 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHWW2l2v()

virtual const double NPbase::muttHWW2l2v ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1754 of file NPbase.h.

    {
        return 1.0;
    }   

◆ muttHZbbboost()

virtual const double NPbase::muttHZbbboost ( const double sqrt_s ) const

inlinevirtual

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 in HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1539 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHZga()

virtual const double NPbase::muttHZga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1633 of file NPbase.h.

    {
        return 1.0;
    }  

◆ muttHZZ()

virtual const double NPbase::muttHZZ ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1669 of file NPbase.h.

    {
        return 1.0;
    }

◆ muttHZZ4l()

virtual const double NPbase::muttHZZ4l ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1697 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBF()

virtual const double NPbase::muVBF ( const double sqrt_s ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.

Definition at line 1137 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBFgamma()

virtual const double NPbase::muVBFgamma ( const double sqrt_s ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1149 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBFHbb()

virtual const double NPbase::muVBFHbb ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1834 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBFHgaga()

virtual const double NPbase::muVBFHgaga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1593 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBFHmumu()

virtual const double NPbase::muVBFHmumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1762 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBFHtautau()

virtual const double NPbase::muVBFHtautau ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1802 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBFHWW()

virtual const double NPbase::muVBFHWW ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1710 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBFHWW2l2v()

virtual const double NPbase::muVBFHWW2l2v ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1738 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBFHZga()

virtual const double NPbase::muVBFHZga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1617 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBFHZZ()

virtual const double NPbase::muVBFHZZ ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1653 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBFHZZ4l()

virtual const double NPbase::muVBFHZZ4l ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1681 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBFpVH()

virtual const double NPbase::muVBFpVH ( const double sqrt_s ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.

Definition at line 1387 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBFpVH_Hmumu()

virtual const double NPbase::muVBFpVH_Hmumu ( const double sqrt_s ) const

inlinevirtual

Definition at line 1790 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVBFpVH_HZga()

virtual const double NPbase::muVBFpVH_HZga ( const double sqrt_s ) const

inlinevirtual

Definition at line 1641 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVH()

virtual const double NPbase::muVH ( const double sqrt_s ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.

Definition at line 1363 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVHbb()

virtual const double NPbase::muVHbb ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1846 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVHcc()

virtual const double NPbase::muVHcc ( const double sqrt_s ) const

inlinevirtual

Definition at line 1858 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVHgaga()

virtual const double NPbase::muVHgaga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1605 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVHmumu()

virtual const double NPbase::muVHmumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1774 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVHpT250()

virtual const double NPbase::muVHpT250 ( const double sqrt_s ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1375 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVHtautau()

virtual const double NPbase::muVHtautau ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1814 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVHWW()

virtual const double NPbase::muVHWW ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1722 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVHWW2l2v()

virtual const double NPbase::muVHWW2l2v ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1750 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVHZga()

virtual const double NPbase::muVHZga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1629 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVHZZ()

virtual const double NPbase::muVHZZ ( const double sqrt_s ) const

inlinevirtual

Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.

Definition at line 1665 of file NPbase.h.

    {
        return 1.0;
    }

◆ muVHZZ4l()

virtual const double NPbase::muVHZZ4l ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1693 of file NPbase.h.

    {
        return 1.0;
    }

◆ muWH()

virtual const double NPbase::muWH ( const double sqrt_s ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.

Definition at line 1239 of file NPbase.h.

    {
        return 1.0;
    }

◆ muWHbb()

virtual const double NPbase::muWHbb ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1842 of file NPbase.h.

    {
        return 1.0;
    }

◆ muWHgaga()

virtual const double NPbase::muWHgaga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1601 of file NPbase.h.

    {
        return 1.0;
    }

◆ muWHmumu()

virtual const double NPbase::muWHmumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1770 of file NPbase.h.

    {
        return 1.0;
    }

◆ muWHpT250()

virtual const double NPbase::muWHpT250 ( const double sqrt_s ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1250 of file NPbase.h.

    {
        return 1.0;
    }

◆ muWHtautau()

virtual const double NPbase::muWHtautau ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1810 of file NPbase.h.

    {
        return 1.0;
    }

◆ muWHWW()

virtual const double NPbase::muWHWW ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1718 of file NPbase.h.

    {
        return 1.0;
    }

◆ muWHWW2l2v()

virtual const double NPbase::muWHWW2l2v ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1746 of file NPbase.h.

    {
        return 1.0;
    }

◆ muWHZga()

virtual const double NPbase::muWHZga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1625 of file NPbase.h.

    {
        return 1.0;
    }

◆ muWHZZ()

virtual const double NPbase::muWHZZ ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1661 of file NPbase.h.

    {
        return 1.0;
    }

◆ muWHZZ4l()

virtual const double NPbase::muWHZZ4l ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1689 of file NPbase.h.

    {
        return 1.0;
    }

◆ muZH()

virtual const double NPbase::muZH ( const double sqrt_s ) const

inlinevirtual

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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.

Definition at line 1261 of file NPbase.h.

    {
        return 1.0;
    }

◆ muZHbb()

virtual const double NPbase::muZHbb ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1838 of file NPbase.h.

    {
        return 1.0;
    }

◆ muZHgaga()

virtual const double NPbase::muZHgaga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1597 of file NPbase.h.

    {
        return 1.0;
    }

◆ muZHmumu()

virtual const double NPbase::muZHmumu ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1766 of file NPbase.h.

    {
        return 1.0;
    }

◆ muZHpT250()

virtual const double NPbase::muZHpT250 ( const double sqrt_s ) const

inlinevirtual

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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.

Definition at line 1272 of file NPbase.h.

    {
        return 1.0;
    }

◆ muZHtautau()

virtual const double NPbase::muZHtautau ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1806 of file NPbase.h.

    {
        return 1.0;
    }

◆ muZHWW()

virtual const double NPbase::muZHWW ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1714 of file NPbase.h.

    {
        return 1.0;
    }

◆ muZHWW2l2v()

virtual const double NPbase::muZHWW2l2v ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1742 of file NPbase.h.

    {
        return 1.0;
    }

◆ muZHZga()

virtual const double NPbase::muZHZga ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1621 of file NPbase.h.

    {
        return 1.0;
    }    

◆ muZHZZ()

virtual const double NPbase::muZHZZ ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1657 of file NPbase.h.

    {
        return 1.0;
    }    

◆ muZHZZ4l()

virtual const double NPbase::muZHZZ4l ( const double sqrt_s ) const

inlinevirtual

Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.

Definition at line 1685 of file NPbase.h.

    {
        return 1.0;
    }    

◆ Mw()

const double NPbase::Mw ( ) const

virtual

The mass of the $W$ boson, $M_W$.

The $W$-boson mass receives the new physics contribution via the oblique parameters $S$, $T$ and $U$ and the shift in the Fermi constant, $\Delta G$:

\[ M_W = M_{W,\mathrm{SM}} \left[ 1 - \frac{\alpha(M_Z^2)}{4(c_W^2-s_W^2)} \left( S - 2c_W^2\,T - \frac{c_W^2-s_W^2}{2s_W^2}\,U \right) - \frac{s_W^2}{2(c_W^2-s_W^2)}\,\Delta G \right]. \]

See [Ciuchini:2013pca] and references therein.

Returns: $M_W$ in GeV

Reimplemented from StandardModel.

Reimplemented in GeorgiMachacek, NPEpsilons, NPEpsilons_pureNP, NPSMEFTd6, NPSMEFTd6General, NPZbbbar, and THDMW.

Definition at line 80 of file NPbase.cpp.

{
    double myMw = trueSM.Mw();
 
    double alpha = trueSM.alphaMz();
    double c2 = trueSM.cW2();
    double s2 = trueSM.sW2();
 
    myMw *= 1.0 - alpha / 4.0 / (c2 - s2)
            *(obliqueS() - 2.0 * c2 * obliqueT() - (c2 - s2) * obliqueU() / 2.0 / s2)
            - s2 / 2.0 / (c2 - s2) * DeltaGF();
 
    //std::cout << "Mw: c_S=" << - alpha/4.0/(c2-s2) << std::endl;
    //std::cout << "Mw: c_T=" << - alpha/4.0/(c2-s2)*(- 2.0*c2) << std::endl;
    //std::cout << "Mw: c_U=" << - alpha/4.0/(c2-s2)*(- (c2-s2)/2.0/s2) << std::endl;
 
    return myMw;
}

◆ N_nu()

const double NPbase::N_nu ( ) const

virtual

The number of neutrinos dervied from the $Z$ pole measurements, $N_{\nu}$.

Returns: $N_{\nu}$, including SM plus NP contributions

Attention: This function is applicable only to the NP model classes that are inherited from NPbase.

Reimplemented from StandardModel.

Definition at line 1156 of file NPbase.cpp.

{
    return ( trueSM.N_nu() + deltaN_nu() );
}

◆ obliqueS()

virtual const double NPbase::obliqueS ( ) const

inlinevirtual

The oblique parameter $S$.

Returns: the value of $S$

Reimplemented in HiggsChiral, HiggsKigen, NPd6SILH, NPHiggs, NPSMEFTd6, NPSMEFTd6General, NPSTU, and NPSTUVWXY.

Definition at line 128 of file NPbase.h.

    {
        return 0.;
    }

◆ obliqueT()

virtual const double NPbase::obliqueT ( ) const

inlinevirtual

The oblique parameter $T$.

Returns: the value of $T$

Reimplemented in HiggsChiral, HiggsKigen, NPd6SILH, NPHiggs, NPSMEFTd6, NPSMEFTd6General, NPSTU, and NPSTUVWXY.

Definition at line 137 of file NPbase.h.

    {
        return 0.;
    }

◆ obliqueU()

virtual const double NPbase::obliqueU ( ) const

inlinevirtual

The oblique parameter $U$.

Returns: the value of $U$

Reimplemented in HiggsChiral, HiggsKigen, NPHiggs, NPSMEFTd6, NPSMEFTd6General, NPSTU, and NPSTUVWXY.

Definition at line 146 of file NPbase.h.

    {
        return 0.;
    }

◆ obliqueW()

virtual const double NPbase::obliqueW ( ) const

inlinevirtual

The oblique parameter $W$.

Returns: the value of $W$

Reimplemented in NPd6SILH, NPSMEFTd6, NPSMEFTd6General, and NPSTUVWXY.

Definition at line 155 of file NPbase.h.

    {
        return 0.;
    }

◆ obliqueY()

virtual const double NPbase::obliqueY ( ) const

inlinevirtual

The oblique parameter $Y$.

Returns: the value of $Y$

Reimplemented in NPd6SILH, NPSMEFTd6, NPSMEFTd6General, and NPSTUVWXY.

Definition at line 164 of file NPbase.h.

    {
        return 0.;
    }

◆ ppZHprobe()

virtual const double NPbase::ppZHprobe ( const double sqrt_s ) const

inlinevirtual

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 NPSMEFTd6 class.

Returns: $g_p^Z$

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3372 of file NPbase.h.

    {
        return 0.0;
    }

◆ R0_f()

const double NPbase::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 StandardModel.

Reimplemented in NPSMEFTd6General, NPZbbbar, and NPEpsilons.

Definition at line 1043 of file NPbase.cpp.

{
    //AG:begin
    if(OutputOrder()==0){ return (trueSM.R0_f(f) ); }
    if(OutputOrder()==1){ return (trueSM.R0_f(f) + deltaR0_f(f)); }
    if(OutputOrder()==2){ return (trueSM.R0_f(f) + deltaR0_f(f) + deltaR0_f_2(f) ); }
    if(OutputOrder()==3){ return ( deltaR0_f_2(f) ); }
    else
    //AG:end
    //AG: deltaR0_f_2(f) added below
        return (trueSM.R0_f(f) + deltaR0_f(f) + deltaR0_f_2(f));
}

◆ R_inv()

const double NPbase::R_inv ( ) const

virtual

The ratio of the invisible and leptonic (electron) decay widths of the $Z$ boson, $R_{inv}$.

Returns: $R_{inv}$, including SM plus NP contributions

Attention: This function is applicable only to the NP model classes that are inherited from NPbase.

Reimplemented from StandardModel.

Definition at line 1100 of file NPbase.cpp.

{
    return ( trueSM.R_inv() + deltaR_inv() );
}

◆ rhoZ_f()

const gslpp::complex NPbase::rhoZ_f ( const Particle f ) const

virtual

The effective neutral-current coupling $\rho_Z^f$ including SM plus NP contributions.

Parameters

[in] f a lepton or quark

Returns: $\rho_Z^f$, including SM plus NP contributions

Reimplemented from StandardModel.

Reimplemented in NPEpsilons.

Definition at line 229 of file NPbase.cpp.

{
    return ( gA_f(f) * gA_f(f) / f.getIsospin() / f.getIsospin());
 
}

◆ Ruc()

const double NPbase::Ruc ( ) const

virtual

The ratio of the $Z\to u\bar{u} + Z\to c\bar{c}$ width to the $Z$-boson hadronic width.

Returns: $\Delta R_{uc}^{0 (2)}$, including SM plus NP contributions

Reimplemented from StandardModel.

Definition at line 459 of file NPbase.cpp.

{
    //AG:added
    if(OutputOrder()==0){ return (trueSM.Ruc() ); }
    if(OutputOrder()==1){ return (trueSM.Ruc() + deltaRuc()); }
    if(OutputOrder()==2){ return (trueSM.Ruc() + deltaRuc() + deltaRuc_2() ); }
    if(OutputOrder()==3){ return ( deltaRuc_2() ); }
    else
        return ( trueSM.Ruc() + deltaRuc() + deltaRuc_2() );
}

◆ RWc()

const double NPbase::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 StandardModel.

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 171 of file NPbase.cpp.

{  
    double GammWcX, GammWhad;
    
//  Basic NPBase implementation is only NP universal and respects CKM unitarity.
//  As it directly uses SM implementation of W width, use same definition here
//  (with the modified NPBase implementation of GammaW)
 
//  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
    GammWcX = GammaW(quarks[CHARM], quarks[STRANGE]);
    
//  For the same reasons, I only need to add the W-> ud decays into the hadronic part
    GammWhad = GammWcX
            + GammaW(quarks[UP], quarks[DOWN]);
 
    return GammWcX/GammWhad;
}

◆ RWlilj()

const double NPbase::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 StandardModel.

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 146 of file NPbase.cpp.

{
    double GammWli, GammWlj;
    
    if (li.is("ELECTRON"))
        GammWli = GammaW(leptons[NEUTRINO_1],li);
    else if (li.is("MU"))
        GammWli = GammaW(leptons[NEUTRINO_2],li);        
    else if (li.is("TAU"))
        GammWli = GammaW(leptons[NEUTRINO_3],li);        
    else
        throw std::runtime_error("Error in NPbase::RWlilj. li must be a charged lepton");
    
    if (lj.is("ELECTRON"))
        GammWlj = GammaW(leptons[NEUTRINO_1],lj);
    else if (lj.is("MU"))
        GammWlj = GammaW(leptons[NEUTRINO_2],lj);        
    else if (lj.is("TAU"))
        GammWlj = GammaW(leptons[NEUTRINO_3],lj);        
    else
        throw std::runtime_error("Error in NPbase::RWlilj. lj must be a charged lepton");
    
    return GammWli/GammWlj;
}

◆ RZlilj()

const double NPbase::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 StandardModel.

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 470 of file NPbase.cpp.

{
    double GammZli, GammZlj;
    
    if ( li.is("ELECTRON") || li.is("MU") || li.is("TAU") )
        GammZli = Gamma_Zf(li);        
    else
        throw std::runtime_error("Error in NPbase::RZlilj. li must be a charged lepton");
    
    if ( lj.is("ELECTRON") || lj.is("MU") || lj.is("TAU") )
        GammZlj = Gamma_Zf(lj);        
    else
        throw std::runtime_error("Error in NPbase::RZlilj. lj must be a charged lepton");
    
    return GammZli/GammZlj;
}

◆ setFlag()

virtual bool NPbase::setFlag	(	const std::string	name,
		const bool	value
	)

inlinevirtual

A method to set a flag of NPbase.

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 StandardModel.

Reimplemented in HiggsChiral, HiggsKigen, NPd6SILH, NPEpsilons, NPSMEFTd6, NPSMEFTd6General, GeorgiMachacek, and NPSMEFT6dtopquark.

Definition at line 97 of file NPbase.h.

    {
        bool result = false;
        result = trueSM.setFlag(name, value) && StandardModel::setFlag(name, value);
        return result;
    }

◆ sigma0_had()

const double NPbase::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

Attention: This function is applicable only to the NP model classes that are inherited from NPbase.

Reimplemented from StandardModel.

Reimplemented in NPEpsilons, NPSMEFTd6General, and NPZbbbar.

Definition at line 664 of file NPbase.cpp.

{
    //AG:begin    
    if(OutputOrder()==0){ return (trueSM.sigma0_had() ); }
    if(OutputOrder()==1){ return (trueSM.sigma0_had() + deltaSigmaHadron()); }
    if(OutputOrder()==2){ return (trueSM.sigma0_had() + deltaSigmaHadron() + deltaSigmaHadron_2() ); }
    if(OutputOrder()==3){ return ( deltaSigmaHadron_2() ); }
    else
    //AG:end
    //AG: deltaSigmaHadron_2() added below
        return (trueSM.sigma0_had() + deltaSigmaHadron() + deltaSigmaHadron_2());
}

◆ sin2thetaEff()

const double NPbase::sin2thetaEff ( const Particle f ) const

virtual

The leptonic effective weak mixing angle $\sin^2\theta_{\rm eff}^{\rm lept}$ at the the $Z$ pole.

\[ \sin^2\theta_{eff} = \sin^2\theta_{eff}^{SM} + \Delta \sin^2\theta_{eff}^{(1)} + \Delta \sin^2\theta_{eff}^{(2)} \]

Parameters

[in] f a lepton or quark

Returns: $\sin^2\theta_{\rm eff}^{\rm lept}$, 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 StandardModel.

Reimplemented in NPZbbbar, and NPEpsilons.

Definition at line 753 of file NPbase.cpp.

{    
    if (f.is("ELECTRON")){
        //AG:begin
        if(OutputOrder()==0){ return (trueSM.sin2thetaEff(f)); }        
        if(OutputOrder()==1){ return (trueSM.sin2thetaEff(f) + deltaSin2thetaEff_e()); }
        if(OutputOrder()==2){ return (trueSM.sin2thetaEff(f) + deltaSin2thetaEff_e() + deltaSin2thetaEff_e_2() ); }
        if(OutputOrder()==3){ return ( deltaSin2thetaEff_e_2() ); }
        else
        //AG:end
        //AG: deltaSin2thetaEff_e_2() added below
            return (trueSM.sin2thetaEff(f) + deltaSin2thetaEff_e() + deltaSin2thetaEff_e_2());
    }
    else if (f.is("MU")){
        //AG:begin
        if(OutputOrder()==0){ return (trueSM.sin2thetaEff(f) ); }
        if(OutputOrder()==1){ return (trueSM.sin2thetaEff(f) + deltaSin2thetaEff_mu()); }
        if(OutputOrder()==2){ return (trueSM.sin2thetaEff(f) + deltaSin2thetaEff_mu() + deltaSin2thetaEff_mu_2() ); }
        if(OutputOrder()==3){ return (deltaSin2thetaEff_mu_2() ); }
        else
        //AG:end
        //AG: deltaSin2thetaEff_mu_2() added below
            return (trueSM.sin2thetaEff(f) + deltaSin2thetaEff_mu() + deltaSin2thetaEff_mu_2());
    }
    else
        return (trueSM.sin2thetaEff(f));
}

◆ STXS0_qqH()

virtual const double NPbase::STXS0_qqH ( const double sqrt_s ) const

inlinevirtual

The STXS0 bin $pp \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3401 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_BrH4lRatio()

virtual const double NPbase::STXS12_BrH4lRatio ( ) const

inlinevirtual

The STXS BR $ H \to 4l $, $l=e,\mu$.

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 3796 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_BrHbbRatio()

virtual const double NPbase::STXS12_BrHbbRatio ( ) const

inlinevirtual

The STXS BR $ H \to bb $.

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 3820 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_BrHevmuvRatio()

virtual const double NPbase::STXS12_BrHevmuvRatio ( ) const

inlinevirtual

The STXS BR $ H \to e\nu \mu\nu $.

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 3804 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_BrHgagaRatio()

virtual const double NPbase::STXS12_BrHgagaRatio ( ) const

inlinevirtual

The STXS BR $ H \to \gamma \gamma $.

Reimplemented in NPSMEFTd6, and NPSMEFTd6General.

Definition at line 3812 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_mjj0_350_pTH0_60_Nj1()

virtual const double NPbase::STXS12_ggH_mjj0_350_pTH0_60_Nj1 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 3895 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_mjj0_350_pTH0_60_Nj2()

virtual const double NPbase::STXS12_ggH_mjj0_350_pTH0_60_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3934 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_mjj0_350_pTH120_200_Nj2()

virtual const double NPbase::STXS12_ggH_mjj0_350_pTH120_200_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3952 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_mjj0_350_pTH60_120_Nj2()

virtual const double NPbase::STXS12_ggH_mjj0_350_pTH60_120_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3943 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_mjj350_700_pTH0_200_Nj2()

virtual const double NPbase::STXS12_ggH_mjj350_700_pTH0_200_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 3997 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2()

virtual const double NPbase::STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3961 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2()

virtual const double NPbase::STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3970 of file NPbase.h.

    {
        return 1.0;
    }    

◆ STXS12_ggH_mjj700_Inf_pTH0_200_Nj2()

virtual const double NPbase::STXS12_ggH_mjj700_Inf_pTH0_200_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 4006 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2()

virtual const double NPbase::STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3979 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2()

virtual const double NPbase::STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3988 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH0_10_Nj0()

virtual const double NPbase::STXS12_ggH_pTH0_10_Nj0 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3865 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH0_60_Nj1()

virtual const double NPbase::STXS12_ggH_pTH0_60_Nj1 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3907 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH10_200_Nj0()

virtual const double NPbase::STXS12_ggH_pTH10_200_Nj0 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$, $N_j = 0, 10<~p_{TH} [GeV]<200$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General.

Definition at line 3884 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH10_Inf_Nj0()

virtual const double NPbase::STXS12_ggH_pTH10_Inf_Nj0 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3874 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH120_200_Nj1()

virtual const double NPbase::STXS12_ggH_pTH120_200_Nj1 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3925 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH200_300()

virtual const double NPbase::STXS12_ggH_pTH200_300 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$, $~200<p_{TH} [GeV]<300$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General.

Definition at line 4017 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH200_300_Nj01()

virtual const double NPbase::STXS12_ggH_pTH200_300_Nj01 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3829 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH300_450()

virtual const double NPbase::STXS12_ggH_pTH300_450 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$, $~300<p_{TH} [GeV]<450$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General.

Definition at line 4028 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH300_450_Nj01()

virtual const double NPbase::STXS12_ggH_pTH300_450_Nj01 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3838 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH450_650()

virtual const double NPbase::STXS12_ggH_pTH450_650 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$, $450<~p_{TH} [GeV]<650$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General.

Definition at line 4049 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH450_650_Nj01()

virtual const double NPbase::STXS12_ggH_pTH450_650_Nj01 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3847 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH450_Inf()

virtual const double NPbase::STXS12_ggH_pTH450_Inf ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$, $~p_{TH} [GeV]>450$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General.

Definition at line 4038 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH60_120_Nj1()

virtual const double NPbase::STXS12_ggH_pTH60_120_Nj1 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3916 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH650_Inf()

virtual const double NPbase::STXS12_ggH_pTH650_Inf ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$, $~p_{TH} [GeV]>650$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General.

Definition at line 4061 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggH_pTH650_Inf_Nj01()

virtual const double NPbase::STXS12_ggH_pTH650_Inf_Nj01 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3856 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggHll_pTV0_75()

virtual const double NPbase::STXS12_ggHll_pTV0_75 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H\ell\ell$, $p_{TV}[GeV]<75$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4074 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggHll_pTV150_250_Nj0()

virtual const double NPbase::STXS12_ggHll_pTV150_250_Nj0 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4092 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggHll_pTV150_250_Nj1()

virtual const double NPbase::STXS12_ggHll_pTV150_250_Nj1 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4101 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggHll_pTV250_Inf()

virtual const double NPbase::STXS12_ggHll_pTV250_Inf ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H\ell\ell$, $250 < p_{TV}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4110 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ggHll_pTV75_150()

virtual const double NPbase::STXS12_ggHll_pTV75_150 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4083 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHll_pTV0_150()

virtual const double NPbase::STXS12_qqHll_pTV0_150 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 4401 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHll_pTV0_75()

virtual const double NPbase::STXS12_qqHll_pTV0_75 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H\ell\ell$, $p_{TV}[GeV]<75$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4356 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHll_pTV150_250_Nj0()

virtual const double NPbase::STXS12_qqHll_pTV150_250_Nj0 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4374 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHll_pTV150_250_Nj1()

virtual const double NPbase::STXS12_qqHll_pTV150_250_Nj1 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4383 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHll_pTV250_400()

virtual const double NPbase::STXS12_qqHll_pTV250_400 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 4410 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHll_pTV250_Inf()

virtual const double NPbase::STXS12_qqHll_pTV250_Inf ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H\ell\ell$, $250<p_{TV}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4392 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHll_pTV400_Inf()

virtual const double NPbase::STXS12_qqHll_pTV400_Inf ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H\ell\ell$, $400<p_{TV}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General.

Definition at line 4419 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHll_pTV75_150()

virtual const double NPbase::STXS12_qqHll_pTV75_150 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4365 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHlv_pTV0_150()

virtual const double NPbase::STXS12_qqHlv_pTV0_150 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 4329 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHlv_pTV0_75()

virtual const double NPbase::STXS12_qqHlv_pTV0_75 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H\ell\nu$, $p_{TV}[GeV]<75$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4284 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHlv_pTV150_250_Nj0()

virtual const double NPbase::STXS12_qqHlv_pTV150_250_Nj0 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4302 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHlv_pTV150_250_Nj1()

virtual const double NPbase::STXS12_qqHlv_pTV150_250_Nj1 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4311 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHlv_pTV250_400()

virtual const double NPbase::STXS12_qqHlv_pTV250_400 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 4338 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHlv_pTV250_Inf()

virtual const double NPbase::STXS12_qqHlv_pTV250_Inf ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H\ell\nu$, $250<p_{TV}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4320 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHlv_pTV400_Inf()

virtual const double NPbase::STXS12_qqHlv_pTV400_Inf ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H\ell\nu$, $400<p_{TV}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General.

Definition at line 4347 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHlv_pTV75_150()

virtual const double NPbase::STXS12_qqHlv_pTV75_150 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4293 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_mjj0_60_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj0_60_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4152 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 4248 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 4275 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_mjj120_350_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj120_350_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4170 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 4257 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 4266 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_mjj350_700_pTH0_200_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj350_700_pTH0_200_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 4230 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4194 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4203 of file NPbase.h.

    {
        return 1.0;
    }    

◆ STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4179 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_mjj60_120_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj60_120_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4161 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 4239 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4212 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2()

virtual const double NPbase::STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4221 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_Nj0()

virtual const double NPbase::STXS12_qqHqq_Nj0 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to Hqq$, $N_j = 0$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4134 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_Nj1()

virtual const double NPbase::STXS12_qqHqq_Nj1 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to Hqq$, $N_j = 1$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4143 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_qqHqq_VH_veto_Nj01()

virtual const double NPbase::STXS12_qqHqq_VH_veto_Nj01 ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General.

Definition at line 4121 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_tH()

virtual const double NPbase::STXS12_tH ( const double sqrt_s ) const

inlinevirtual

The STXS bin $pp \to tH$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4491 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ttH_pTH0_60()

virtual const double NPbase::STXS12_ttH_pTH0_60 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $pp \to ttH$, $p_{TH}[GeV]<60$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4428 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ttH_pTH120_200()

virtual const double NPbase::STXS12_ttH_pTH120_200 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $pp \to ttH$, $120<p_{TH}[GeV]<200$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4446 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ttH_pTH200_300()

virtual const double NPbase::STXS12_ttH_pTH200_300 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $pp \to ttH$, $200<p_{TH}[GeV]<300$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4455 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ttH_pTH300_450()

virtual const double NPbase::STXS12_ttH_pTH300_450 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $pp \to ttH$, $300<p_{TH}[GeV]<450$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General.

Definition at line 4473 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ttH_pTH300_Inf()

virtual const double NPbase::STXS12_ttH_pTH300_Inf ( const double sqrt_s ) const

inlinevirtual

The STXS bin $pp \to ttH$, $300<p_{TH}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4464 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ttH_pTH450_Inf()

virtual const double NPbase::STXS12_ttH_pTH450_Inf ( const double sqrt_s ) const

inlinevirtual

The STXS bin $pp \to ttH$, $450<p_{TH}[GeV]$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General.

Definition at line 4482 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS12_ttH_pTH60_120()

virtual const double NPbase::STXS12_ttH_pTH60_120 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $pp \to ttH$, $60<p_{TH}[GeV]<120$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 4437 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ggH0j()

virtual const double NPbase::STXS_ggH0j ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3433 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ggH1j_pTH_0_60()

virtual const double NPbase::STXS_ggH1j_pTH_0_60 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3442 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ggH1j_pTH_120_200()

virtual const double NPbase::STXS_ggH1j_pTH_120_200 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3460 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ggH1j_pTH_200()

virtual const double NPbase::STXS_ggH1j_pTH_200 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3469 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ggH1j_pTH_60_120()

virtual const double NPbase::STXS_ggH1j_pTH_60_120 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3451 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ggH2j_pTH_0_200()

virtual const double NPbase::STXS_ggH2j_pTH_0_200 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3478 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ggH2j_pTH_0_60()

virtual const double NPbase::STXS_ggH2j_pTH_0_60 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3488 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ggH2j_pTH_120_200()

virtual const double NPbase::STXS_ggH2j_pTH_120_200 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3508 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ggH2j_pTH_200()

virtual const double NPbase::STXS_ggH2j_pTH_200 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3518 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ggH2j_pTH_60_120()

virtual const double NPbase::STXS_ggH2j_pTH_60_120 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3498 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ggH_VBFtopo_j3()

virtual const double NPbase::STXS_ggH_VBFtopo_j3 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3423 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ggH_VBFtopo_j3v()

virtual const double NPbase::STXS_ggH_VBFtopo_j3v ( const double sqrt_s ) const

inlinevirtual

The STXS bin $gg \to H$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3413 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHll_pTV_0_150()

virtual const double NPbase::STXS_qqHll_pTV_0_150 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H \ell \ell$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3643 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHll_pTV_150_250()

virtual const double NPbase::STXS_qqHll_pTV_150_250 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H \ell \ell$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3652 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHll_pTV_150_250_0j()

virtual const double NPbase::STXS_qqHll_pTV_150_250_0j ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H \ell \ell$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3662 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHll_pTV_150_250_1j()

virtual const double NPbase::STXS_qqHll_pTV_150_250_1j ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H \ell \ell$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3672 of file NPbase.h.

    {
        return 1.0;
    }   

◆ STXS_qqHll_pTV_250()

virtual const double NPbase::STXS_qqHll_pTV_250 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H \ell \ell$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3682 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHlv_pTV_0_150()

virtual const double NPbase::STXS_qqHlv_pTV_0_150 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H \ell \nu$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3604 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHlv_pTV_0_250()

virtual const double NPbase::STXS_qqHlv_pTV_0_250 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H \ell \nu$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3594 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHlv_pTV_150_250_0j()

virtual const double NPbase::STXS_qqHlv_pTV_150_250_0j ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H \ell \nu$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3614 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHlv_pTV_150_250_1j()

virtual const double NPbase::STXS_qqHlv_pTV_150_250_1j ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H \ell \nu$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3624 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHlv_pTV_250()

virtual const double NPbase::STXS_qqHlv_pTV_250 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H \ell \nu$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3634 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHqq_nonVHtopo()

virtual const double NPbase::STXS_qqHqq_nonVHtopo ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3557 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHqq_pTj_200()

virtual const double NPbase::STXS_qqHqq_pTj_200 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3585 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHqq_Rest()

virtual const double NPbase::STXS_qqHqq_Rest ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3576 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHqq_VBFtopo_j3()

virtual const double NPbase::STXS_qqHqq_VBFtopo_j3 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3548 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHqq_VBFtopo_j3v()

virtual const double NPbase::STXS_qqHqq_VBFtopo_j3v ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3538 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHqq_VBFtopo_Rest()

virtual const double NPbase::STXS_qqHqq_VBFtopo_Rest ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3528 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_qqHqq_VHtopo()

virtual const double NPbase::STXS_qqHqq_VHtopo ( const double sqrt_s ) const

inlinevirtual

The STXS bin $qq \to H qq$.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3566 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ttHtH()

virtual const double NPbase::STXS_ttHtH ( const double sqrt_s ) const

inlinevirtual

The STXS bin $ ttH + tH $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3692 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_WHqqHqq_pTj1_200()

virtual const double NPbase::STXS_WHqqHqq_pTj1_200 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $ qq \to WH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3738 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_WHqqHqq_Rest()

virtual const double NPbase::STXS_WHqqHqq_Rest ( const double sqrt_s ) const

inlinevirtual

The STXS bin $ qq \to WH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3729 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_WHqqHqq_VBFtopo_j3()

virtual const double NPbase::STXS_WHqqHqq_VBFtopo_j3 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $ qq \to WH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3711 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_WHqqHqq_VBFtopo_j3v()

virtual const double NPbase::STXS_WHqqHqq_VBFtopo_j3v ( const double sqrt_s ) const

inlinevirtual

The STXS bin $ qq \to WH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3702 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_WHqqHqq_VH2j()

virtual const double NPbase::STXS_WHqqHqq_VH2j ( const double sqrt_s ) const

inlinevirtual

The STXS bin $ qq \to WH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3720 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ZHqqHqq_pTj1_200()

virtual const double NPbase::STXS_ZHqqHqq_pTj1_200 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $ qq \to ZH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3783 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ZHqqHqq_Rest()

virtual const double NPbase::STXS_ZHqqHqq_Rest ( const double sqrt_s ) const

inlinevirtual

The STXS bin $ qq \to ZH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3774 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ZHqqHqq_VBFtopo_j3()

virtual const double NPbase::STXS_ZHqqHqq_VBFtopo_j3 ( const double sqrt_s ) const

inlinevirtual

The STXS bin $ qq \to ZH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3756 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ZHqqHqq_VBFtopo_j3v()

virtual const double NPbase::STXS_ZHqqHqq_VBFtopo_j3v ( const double sqrt_s ) const

inlinevirtual

The STXS bin $ qq \to ZH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3747 of file NPbase.h.

    {
        return 1.0;
    }

◆ STXS_ZHqqHqq_VH2j()

virtual const double NPbase::STXS_ZHqqHqq_VH2j ( const double sqrt_s ) const

inlinevirtual

The STXS bin $ qq \to ZH \to H qq $.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3765 of file NPbase.h.

    {
        return 1.0;
    }

◆ Update()

bool NPbase::Update ( const std::map< std::string, double > & DPars )

virtual

The update method for NPbase.

Returns: a boolean that is true if the execution is successful

Reimplemented from StandardModel.

Reimplemented in GeorgiMachacek, and THDMW.

Definition at line 36 of file NPbase.cpp.

{
    if (!trueSM.Update(DPars)) return (false);
    return StandardModel::Update(DPars);
}

◆ UpperLimitZgammaA()

virtual const double NPbase::UpperLimitZgammaA ( const double sqrt_s ) const

inlinevirtual

Returns

Reimplemented in HiggsChiral.

Definition at line 2760 of file NPbase.h.

    {
        return 1.0;
    }

◆ UpperLimitZgammaA13()

virtual const double NPbase::UpperLimitZgammaA13 ( const double sqrt_s ) const

inlinevirtual

Returns

Reimplemented in HiggsChiral.

Definition at line 2742 of file NPbase.h.

    {
        return 1.0;
    }

◆ UpperLimitZgammaC()

virtual const double NPbase::UpperLimitZgammaC ( const double sqrt_s ) const

inlinevirtual

Returns

Reimplemented in HiggsChiral.

Definition at line 2769 of file NPbase.h.

    {
        return 1.0;
    }

◆ UpperLimitZgammaC13()

virtual const double NPbase::UpperLimitZgammaC13 ( const double sqrt_s ) const

inlinevirtual

Returns

Reimplemented in HiggsChiral.

Definition at line 2751 of file NPbase.h.

    {
        return 1.0;
    }

◆ xseeWW()

virtual const double NPbase::xseeWW ( const double sqrt_s ) const

inlinevirtual

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 in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3344 of file NPbase.h.

    {
        return 0.0;
    }

◆ xseeWW4fLEP2()

virtual const double NPbase::xseeWW4fLEP2	(	const double	sqrt_s,
		const int	fstate
	)		const

inlinevirtual

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]. Defined only for the NPSMEFTd6 class.

Returns: $sigma$ [pb]

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3188 of file NPbase.h.

    {
        return 0.0;
    }

◆ xseeWWhadLEP2()

virtual const double NPbase::xseeWWhadLEP2 ( const double sqrt_s ) const

inlinevirtual

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.

Returns: $sigma$ [pb]

Definition at line 3257 of file NPbase.h.

    {
        return xseeWW4fLEP2(sqrt_s, 0);
    }

◆ xseeWWleptLEP2()

virtual const double NPbase::xseeWWleptLEP2 ( const double sqrt_s ) const

inlinevirtual

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.

Returns: $sigma$ [pb]

Definition at line 3213 of file NPbase.h.

    {
        return xseeWW4fLEP2(sqrt_s, 11);
    }

◆ xseeWWsemilLEP2()

virtual const double NPbase::xseeWWsemilLEP2 ( const double sqrt_s ) const

inlinevirtual

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.

Returns: $sigma$ [pb]

Definition at line 3235 of file NPbase.h.

    {
        return xseeWW4fLEP2(sqrt_s, 10);
    }  

◆ xseeWWtotLEP2()

virtual const double NPbase::xseeWWtotLEP2 ( const double sqrt_s ) const

inlinevirtual

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]. Defined only for the NPSMEFTd6 class.

Returns: $sigma$ [pb]

Reimplemented in NPSMEFTd6General, and NPSMEFTd6.

Definition at line 3279 of file NPbase.h.

    {
        return 0.0;
    }

The documentation for this class was generated from the following files:

Detailed Description

Initialization

Model parameters

Model flags

Important member functions

Public Member Functions

Additional Inherited Members

Constructor & Destructor Documentation

◆ NPbase()

Member Function Documentation

◆ A_f()

◆ AFB()

◆ alphaMz()

◆ aPskPol()

◆ bPskPol()

◆ Br_H_exo()

◆ Br_H_inv()

◆ Br_H_inv_NP()

◆ BR_Zf()

◆ BrH2d2dRatio()

◆ BrH2e2muRatio()

◆ BrH2e2vRatio()

◆ BrH2evRatio()

◆ BrH2L2dRatio()

◆ BrH2L2LRatio()

◆ BrH2L2uRatio()

◆ BrH2L2v2Ratio()

◆ BrH2L2vRatio()

◆ BrH2l2vRatio()

◆ BrH2Lv2Ratio()

◆ BrH2LvRatio()

◆ BrH2mu2vRatio()

◆ BrH2muvRatio()

◆ BrH2u2dRatio()

◆ BrH2u2uRatio()

◆ BrH2udRatio()

◆ BrH2v2dRatio()

◆ BrH2v2uRatio()

◆ BrH2v2vRatio()

◆ BrH4dRatio()

◆ BrH4eRatio()

◆ BrH4fRatio()

◆ BrH4L2Ratio()

◆ BrH4LRatio()

◆ BrH4lRatio()

◆ BrH4muRatio()

◆ BrH4uRatio()

◆ BrH4vRatio()

◆ BrHbbRatio()

◆ BrHccRatio()

◆ BrHevmuvRatio()

◆ BrHgagaRatio()

◆ BrHggRatio()

◆ BrHll_vvorjjRatio()

◆ BrHlljjRatio()

◆ BrHlv_lvorjjRatio()

◆ BrHlvjjRatio()

◆ BrHLvudRatio()

◆ BrHLvvLRatio()

◆ BrHmumuRatio()

◆ BrHssRatio()

◆ BrHtautauRatio()

◆ BrHtoinvRatio()

◆ BrHudduRatio()

◆ BrHvisRatio()

◆ BrHVVRatio()

◆ BrHWWRatio()

◆ BrHZgaeeRatio()

◆ BrHZgallRatio()

◆ BrHZgamumuRatio()

◆ BrHZgaRatio()

◆ BrHZZRatio()

◆ BrW()

◆ C1eeHvv()

◆ C1eettH()

◆ C1eeWBF()

◆ C1eeZBF()

◆ C1eeZH()

◆ cbminuscc()

◆ cbminusctau()