master
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a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models |
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master
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a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models |
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A model class for new physics in the form of the dimension-six effective Lagrangian. More...
#include <NPSMEFTd6General.h>
Inheritance diagram for NPSMEFTd6General:A model class for new physics in the form of the dimension-six effective Lagrangian.
This is a Model class containing parameters and functions associated with the general dimension-six effective Lagrangian. (Use the model "NPSMEFTd6_LFU_QFU" to assume lepton and quark flavour universality)
In this class we consider the dimension-six effective Lagrangian
\[ \mathcal{L}_\mathrm{eff} = \mathcal{L}_\mathrm{SM} + \sum_i \frac{C_i}{\Lambda^2} \mathcal{O}_i. \]
The implementation is written in the basis of [Grzadkowski:2010es]. For convenience, the parameterization also includes operators appearing in other common bases. In particular, the complete set of parameters contains 4 redundancies, given by the coefficients \(C_{2B,2W,DHB,DHW,DB,DW} \), which correspond to operators not included in the basis of [Grzadkowski:2010es]. For meaningful physical results one must make sure to include only a complete set of interactions in a given analysis.
After creating an instance of the current class with the constructor NPSMEFTd6General(), it is required to call the initialization method InitializeModel(). In the Monte Carlo run, the constructor as well as the initialization method are called in InputParser::ReadParameters().
The model parameters of NPSMEFTd6General are summarized below:
| Label | LaTeX symbol | Description |
|---|---|---|
| g1_LNP | \(g_1(\Lambda_\mathrm{NP})\) | The hypercharge coupling constant at the New Physics scale. |
| g2_LNP | \(g_2(\Lambda_\mathrm{NP})\) | The SU(2) \(_L\) coupling constant at the New Physics scale. |
| g1_LNP | \(g_3(\Lambda_\mathrm{NP})\) | The QCD coupling constant at the New Physics scale. |
| lambdaH_LNP | \(\lambda_H(\Lambda_\mathrm{NP})\) | The coefficient of the \((H^\dagger H)^2\) term at the New Physics scale. |
| muH_LNP | \(\mu_H(\Lambda_\mathrm{NP})\) | The square root of the coefficient of the \((H^\dagger H)\) term at the New Physics scale. |
| Ye_LNP | \(Y_e(\Lambda_\mathrm{NP})\) | The electron Yukawa coupling at the New Physics scale. |
| Ymu_LNP | \(Y_\mu(\Lambda_\mathrm{NP})\) | The muon Yukawa coupling at the New Physics scale. |
| Ytau_LNP | \(Y_\tau(\Lambda_\mathrm{NP})\) | The tau Yukawa coupling at the New Physics scale. |
| Yu_LNP | \(Y_u(\Lambda_\mathrm{NP})\) | The up quark Yukawa coupling at the New Physics scale in the up basis. |
| Yc_LNP | \(Y_c(\Lambda_\mathrm{NP})\) | The charm quark Yukawa coupling at the New Physics scale in the up basis. |
| Yt_LNP | \(Y_t(\Lambda_\mathrm{NP})\) | The top quark Yukawa coupling at the New Physics scale in the up basis. |
| Yd_LNP | \(Y_d(\Lambda_\mathrm{NP})\) | The down quark Yukawa coupling at the New Physics scale in the down basis. |
| Ys_LNP | \(Y_s(\Lambda_\mathrm{NP})\) | The strange quark Yukawa coupling at the New Physics scale in the down basis. |
| Yb_LNP | \(Y_b(\Lambda_\mathrm{NP})\) | The bottom quark Yukawa coupling at the New Physics scale in the down basis. |
| s12CKM_LNP | \(s_{12}(\Lambda_\mathrm{NP})\) | The sine of the \(\theta_{12}\) angle parameterizing the relative orientation of up and down Yukawa couplings at the New Physics scale. |
| s13CKM_LNP | \(s_{13}(\Lambda_\mathrm{NP})\) | The sine of the \(\theta_{13}\) angle parameterizing the relative orientation of up and down Yukawa couplings at the New Physics scale. |
| s23CKM_LNP | \(s_{23}(\Lambda_\mathrm{NP})\) | The sine of the \(\theta_{23}\) angle parameterizing the relative orientation of up and down Yukawa couplings at the New Physics scale. |
| dCKM_LNP | \(\delta(\Lambda_\mathrm{NP})\) | The CP-violating phase of the matrix describing the relative orientation of up and down Yukawa couplings at the New Physics scale. |
| CG | \(C_{G} \) | The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\). |
| CW | \(C_{W} \) | The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\). |
| CHG | \(C_{HG} \) | The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\). |
| CHW | \(C_{HW} \) | The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\). |
| CHB | \(C_{HB} \) | The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\). |
| CHWB | \(C_{HWB} \) | The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\sigma^a H\big)W_{\mu\nu}^a B^{\mu\nu}\). |
| CHD | \(C_{HD}\) | The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\). |
| CHbox | \(C_{H\Box}\) | The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\). |
| CH | \(C_{H}\) | The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\). |
| CHl1_kk, CHl1_klr, CHl1_kli | \( (C_{HL}^{(1)})_{kk}, \mbox{Re}\big[(C_{HL}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(1)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^j\big)\), for \(i,j=1,2,3\). |
| CHl3_kk, CHl3_klr, CHl3_kli | \( (C_{HL}^{(3)})_{kk}, \mbox{Re}\big[(C_{HL}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(3)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \sigma^a L^j\big)\), for \(i,j=1,2,3\). |
| CHe_kk, CHe_klr, CHe_kli | \( (C_{He})_{kk}, \mbox{Re}\big[(C_{He})_{kl}\big], \mbox{Im}\big[(C_{He})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^j\big)\), for \(i,j=1,2,3\). |
| CHq1_kk, CHq1_klr, CHq1_kli | \( (C_{HQ}^{(1)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(1)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^j\big)\), for \(i,j=1,2,3\). |
| CHq3_kk, CHq3_klr, CHq3_kli | \( (C_{HQ}^{(3)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(3)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \sigma^a Q^j\big)\), for \(i,j=1,2,3\). |
| CHu_kk, CHu_klr, CHu_kli | \( (C_{Hu})_{kk}, \mbox{Re}\big[(C_{Hu})_{kl}\big], \mbox{Im}\big[(C_{Hu})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hu})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^j\big)\), for \(i,j=1,2,3\). |
| CHd_kk, CHd_klr, CHd_kli | \( (C_{Hd})_{kk}, \mbox{Re}\big[(C_{Hd})_{kl}\big], \mbox{Im}\big[(C_{Hd})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hd})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\). |
| CHud_klr, CHud_kli | \(\mbox{Re}\big[(C_{Hud})_{kl}\big], \mbox{Im}\big[(C_{Hud})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ij} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\). |
| CeH_klr, CeH_kli | \(\mbox{Re}\big[(C_{eH})_{kl}\big], \mbox{Im}\big[(C_{eH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{ij} =\big(H^\dagger H\big) \big(\overline{L^i}\,H E^j\big)\), for \(i,j=1,2,3\). |
| CuH_klr, CuH_kli | \(\mbox{Re}\big[(C_{uH})_{kl}\big], \mbox{Im}\big[(C_{uH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,\widetilde{H} U^j\big)\), for \(i,j=1,2,3\). |
| CdH_klr, CdH_kli | \(\mbox{Re}\big[(C_{dH})_{kl}\big], \mbox{Im}\big[(C_{dH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,H D^j\big)\), for \(i,j=1,2,3\). |
| CuG_klr, CuG_kli | \(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\). |
| CuW_klr, CuW_kli | \(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\). |
| CuB_klr, CuB_kli | \(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\). |
| CdG_klr, CdG_kli | \(\mbox{Re}\big[(C_{dG})_{kl}\big], \mbox{Im}\big[(C_{dG})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A D^j\big)H G_{\mu\nu}^A\), for \(i,j=1,2,3\). |
| CdW_klr, CdW_kli | \(\mbox{Re}\big[(C_{dW})_{kl}\big], \mbox{Im}\big[(C_{dW})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a D^j\big)H W_{\mu\nu}^a\), for \(i,j=1,2,3\). |
| CdB_klr, CdB_kli | \(\mbox{Re}\big[(C_{dB})_{kl}\big], \mbox{Im}\big[(C_{dB})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} D^j\big)H B_{\mu\nu}\), for \(i,j=1,2,3\). |
| CeW_klr, CeW_kli | \(\mbox{Re}\big[(C_{eW})_{kl}\big], \mbox{Im}\big[(C_{eW})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eW})_{ij} =\big(\overline{L^i}\sigma^{\mu\nu} \sigma_a E^j\big)H W_{\mu\nu}^a\), for \(i,j=1,2,3\). |
| CeB_klr, CeB_kli | \(\mbox{Re}\big[(C_{eB})_{kl}\big], \mbox{Im}\big[(C_{eB})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eB})_{ij} =\big(\overline{L^i}\sigma^{\mu\nu} E^j\big)H B_{\mu\nu}\), for \(i,j=1,2,3\). |
| Cll_1221, Cll_2112 | \((C_{LL})_{1221,2112}\) | The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\). |
| Clq1 | \(C_{LQ}^{(1)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\). |
| Clq3 | \(C_{LQ}^{(3)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \sigma_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\). |
| Cee | \(C_{EE}\) | The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Ceu | \(C_{EU}\) | The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| Ced | \(C_{ED}\) | The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| Cle | \(C_{LE}\) | The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Clu | \(C_{LU}\) | The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| Cld | \(C_{LD}\) | The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| Cqe | \(C_{QE}\) | The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Cqq1_1133, Cqq1_1331, Cqq1_3333 | \(C_{QQ}^{(1)}\) | The coefficient of the operator \(({\cal O}_{QQ}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\). |
| Cqq3_1133, Cqq3_1331, Cqq3_3333 | \(C_{QQ}^{(3)}\) | The coefficient of the operator \(({\cal O}_{QQ}^{(3)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu \sigma_a Q^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\). |
| Cuu_1133, Cuu_1331, Cuu_3333 | \(C_{uu}\) | The coefficient of the operator \(({\cal O}_{uu})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu u^j\big) \big(\overline{u^k}\,\gamma_\mu u^l\big)\). |
| Cud1_3311, Cud1_3333 | \(C_{ud}^{(1)}\) | The coefficient of the operator \(({\cal O}_{ud}^{(1)})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu u^j\big) \big(\overline{d^k}\,\gamma_\mu d^l\big)\). |
| Cud8_3311, Cud8_3333 | \(C_{ud}^{(8)}\) | The coefficient of the operator \(({\cal O}_{ud}^{(8)})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu T^A u^j\big) \big(\overline{d^k}\,\gamma_\mu T^A d^l\big)\). |
| Cqu1_1133, Cqu1_3311, Cqu1_3333 | \(C_{Qu}^{(1)}\) | The coefficient of the operator \(({\cal O}_{Qu}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{u^k}\,\gamma_\mu u^l\big)\). |
| Cqu8_1133, Cqu8_3311, Cqu8_3333 | \(C_{Qu}^{(8)}\) | The coefficient of the operator \(({\cal O}_{Qu}^{(8)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu T^A Q^j\big) \big(\overline{u^k}\,\gamma_\mu T^A u^l\big)\). |
| Cqd1_3311, Cqd1_3333 | \(C_{Qd}^{(1)}\) | The coefficient of the operator \(({\cal O}_{Qd}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{d^k}\,\gamma_\mu d^l\big)\). |
| Cqd8_3311, Cqd8_3333 | \(C_{Qd}^{(8)}\) | The coefficient of the operator \(({\cal O}_{Qd}^{(8)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu T^A Q^j\big) \big(\overline{d^k}\,\gamma_\mu T^A d^l\big)\). |
| Cquqd1_3333 | \(C_{QuQd}^{(1)}\) | The coefficient of the operator \(({\cal O}_{QuQd}^{(1)})_{ijkl}=\big(\overline{Q^i}\, u^j\big) i\sigma_2 \big(\overline{Q^k}^T\, d^l\big)\). |
| Cquqd8_3333 | \(C_{QuQd}^{(8)}\) | The coefficient of the operator \(({\cal O}_{QuQd}^{(8)})_{ijkl}=\big(\overline{Q^i}\, T^A u^j\big) i\sigma_2 \big(\overline{Q^k}^T\, T^A d^l\big)\). |
| Lambda_NP | \(\Lambda \) | The new physics scale. |
| BrHinv | Br \((H\to invisible)\) | The branching ratio of invisible Higgs decays. Only the absolute value of this parameter is considered.(Not part of the EFT. Only for tests.) |
| BrHexo | Br \((H\to exotic)\) | The branching ratio of exotic Higgs decays. Only the absolute value of this parameter is considered. (Not part of the EFT. Only for tests.) |
| dg1Z | \(\delta g_{1Z}\) | Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.) |
| dKappaga | \(\delta \kappa_{\gamma}\) | Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.) |
| lambZ | \(\lambda_{Z}\) | Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.) |
Where the hermitian derivatives are defined as
\[ H^\dagger i \overset{\leftrightarrow}{D}_\mu H\equiv H^\dagger i(D_\mu - \overset{\leftarrow}{D}_\mu)H \]
and
\[ H^\dagger i \overset{\leftrightarrow}{D^a_\mu} H\equiv H^\dagger i (\sigma^a D_\mu - \overset{\leftarrow}{D}_\mu \sigma^a)H. \]
The Flags of NPSMEFTd6General are summarized below:
| Label | Value | Description |
|---|---|---|
| MWinput | TRUE / FALSE | This auxiliary flag is used for setting the W mass as a SM input, instead of the electromagnetic constant parameter dAle5Mz. The default value is FALSE. This flag will override the flag of the same name in StandardModel |
| QuadraticTerms | TRUE / FALSE | This flag is set to TRUE if the quadratic terms in Higgs cross sections and widths are switched on. The default value is FALSE; new physics contributions are linearized. |
| HiggsSM | TRUE / FALSE | This flag is set to TRUE if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. The default value is FALSE. |
| LoopHd6 | TRUE / FALSE | This flag is set to TRUE if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. The default value is FALSE. |
| LoopH3d6Quad | TRUE / FALSE | This flag is set to TRUE if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. Works independently of the flag QuadraticTerms (the quadratic contributions are also added if the latter is true). The default value is FALSE. |
| RGEci | TRUE / FALSE | This flag is set to TRUE if including the SMEFT RGE effects. The default value is TRUE. |
| finiteNLO | TRUE / FALSE | This flag is set to TRUE if including SMEFT finite NLO terms (where available). The default value is FALSE. |
| matchLEFT | TRUE / FALSE | This flag is set to TRUE if the matching between SMEFT and LEFT needs to be computed. The default value is TRUE. |
See the base classes of the current class.
Definition at line 593 of file NPSMEFTd6General.h.
Public Member Functions | |
| virtual const double | A_f (const Particle f) const |
| The left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\mathcal{A}_f\). 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. 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 | 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 | BrH4fCCRatio () const |
| The ratio of the Br \((H\to 4f, CC)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4fNCRatio () const |
| The ratio of the Br \((H\to 4f, NC)\) 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 | 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 | BrHWffRatio () const |
| The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| virtual const double | BrHWjjRatio () const |
| The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHWlvRatio () const |
| The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHWW2l2vRatio () const |
| The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHWW4fRatio () const |
| The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| virtual const double | BrHWW4jRatio () const |
| The ratio of the Br \((H\to WW^*\to 4j)\) 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 | BrHZddRatio () const |
| The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZffRatio () const |
| The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. 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 | BrHZllRatio () const |
| The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZuuRatio () const |
| The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZvvRatio () const |
| The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZZ2e2muRatio () const |
| The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZZ4dRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZZ4eRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZZ4fRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| virtual const double | BrHZZ4lRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZZ4muRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZZ4uRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZZ4vRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. 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 | cbW_TWG (const double mu) const |
| const double | CeeLL_bottom (const double mu) const |
| const double | CeeLL_charm (const double mu) const |
| const double | CeeLL_down (const double mu) const |
| const double | CeeLL_e (const double mu) const |
| const double | CeeLL_mu (const double mu) const |
| const double | CeeLL_strange (const double mu) const |
| const double | CeeLL_tau (const double mu) const |
| const double | CeeLL_top (const double mu) const |
| const double | CeeLL_up (const double mu) const |
| const double | CeeLR_bottom (const double mu) const |
| const double | CeeLR_charm (const double mu) const |
| const double | CeeLR_down (const double mu) const |
| const double | CeeLR_e (const double mu) const |
| const double | CeeLR_mu (const double mu) const |
| const double | CeeLR_strange (const double mu) const |
| const double | CeeLR_tau (const double mu) const |
| const double | CeeLR_top (const double mu) const |
| const double | CeeLR_up (const double mu) const |
| const double | CeeRL_bottom (const double mu) const |
| const double | CeeRL_charm (const double mu) const |
| const double | CeeRL_down (const double mu) const |
| const double | CeeRL_e (const double mu) const |
| const double | CeeRL_mu (const double mu) const |
| const double | CeeRL_strange (const double mu) const |
| const double | CeeRL_tau (const double mu) const |
| const double | CeeRL_top (const double mu) const |
| const double | CeeRL_up (const double mu) const |
| const double | CeeRR_bottom (const double mu) const |
| const double | CeeRR_charm (const double mu) const |
| const double | CeeRR_down (const double mu) const |
| const double | CeeRR_e (const double mu) const |
| const double | CeeRR_mu (const double mu) const |
| const double | CeeRR_strange (const double mu) const |
| const double | CeeRR_tau (const double mu) const |
| const double | CeeRR_top (const double mu) const |
| const double | CeeRR_up (const double mu) const |
| virtual const double | CEWHd11 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{11}\). 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.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | cgg_HB (const double mu) const |
| The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). 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.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | cHb_TWG (const double mu) const |
| virtual const double | cHQ3_TWG (const double mu) const |
| virtual const double | cHQm_TWG (const double mu) const |
| virtual const double | cHQp_TWG (const double mu) const |
| virtual const double | cHt_TWG (const double mu) const |
| virtual const double | cHtb_TWG (const double mu) const |
| virtual const double | computeGammaTotalRatio () const |
| The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More... | |
| virtual const double | cQd1_TWG (const double mu) const |
| virtual const double | cQd8_TWG (const double mu) const |
| virtual const double | cQe_TWG (const double mu) const |
| virtual const double | cQl3_TWG (const double mu) const |
| virtual const double | cQlM_TWG (const double mu) const |
| virtual const double | cQlP_TWG (const double mu) const |
| virtual const double | cQq11_TWG (const double mu) const |
| virtual const double | cQq18_TWG (const double mu) const |
| virtual const double | cQQ1_TWG (const double mu) const |
| virtual const double | cQq31_TWG (const double mu) const |
| virtual const double | cQq38_TWG (const double mu) const |
| virtual const double | cQQ8_TWG (const double mu) const |
| virtual const double | cQt1_TWG (const double mu) const |
| virtual const double | cQt8_TWG (const double mu) const |
| virtual const double | cQu1_TWG (const double mu) const |
| virtual const double | cQu8_TWG (const double mu) const |
| virtual const double | ctd1_TWG (const double mu) const |
| virtual const double | ctd8_TWG (const double mu) const |
| virtual const double | cte_TWG (const double mu) const |
| virtual const double | ctG_TWG (const double mu) const |
| virtual const double | ctH_TWG (const double mu) const |
| virtual const double | ctl_TWG (const double mu) const |
| virtual const double | ctlS_TWG (const double mu) const |
| virtual const double | ctlT_TWG (const double mu) const |
| virtual const double | ctq1_TWG (const double mu) const |
| virtual const double | ctq8_TWG (const double mu) const |
| virtual const double | ctt1_TWG (const double mu) const |
| virtual const double | ctu1_TWG (const double mu) const |
| virtual const double | ctu8_TWG (const double mu) const |
| virtual const double | ctW_TWG (const double mu) const |
| virtual const double | ctZ_TWG (const double mu) const |
| virtual const double | cZBox_HB (const double mu) const |
| The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | cZga_HB (const double mu) const |
| The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | cZZ_HB (const double mu) const |
| The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | del_A_mu (const double mu) const |
| Correction to photon WF. More... | |
| virtual const double | del_e_mu (const double mu) const |
| Correction to electric charge. More... | |
| virtual const double | del_sW2_mu (const double mu) const |
| Correction to (sin squared of) weak mixing angle. More... | |
| virtual const double | del_Z_mu (const double mu) const |
| Correction to Z WF. More... | |
| virtual const double | del_ZA_mu (const double mu) const |
| Correction to Z-A mixing. More... | |
| virtual const double | delQ_gNC (const double mu) const |
| Separate, charge-proportional, indirect correction to EW neutral currents. 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_AFB_ee (const double pol_e, const double pol_p, const double s) const |
| virtual const double | delta_AFB_f (const Particle f, const double pol_e, const double pol_p, const double s) const |
| virtual const double | delta_alrmoller (const double q2, const double y) const |
| The computation of the parity violating asymmetry in Moller scattering. More... | |
| virtual const double | delta_amuon () const |
| The computation of the anomalous magnetic moment of the muon \(a_\mu=(g_\mu-2)/2\). More... | |
| virtual const double | delta_Dsigma_f (const Particle f, const double pol_e, const double pol_p, const double s, const double cos) const |
| virtual const double | delta_gAnue () const |
| The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gAnue. More... | |
| virtual const double | delta_gLnuN2 () const |
| The computation of the correction to the effective neutrino nucleon LH coupling: delta_gLnuN2. More... | |
| virtual const double | delta_gRnuN2 () const |
| The computation of the correction to the effective neutrino nucleon RH coupling: delta_gRnuN2. More... | |
| virtual const double | delta_gVnue () const |
| The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gVnue. More... | |
| virtual const double | delta_mubbH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_mubbH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muggH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muggH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_mutH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_mutH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muttH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muttH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muVBF_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muVBF_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muVH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{VH}\) between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muVH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{VH}\) between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muWH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muWH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muZH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muZH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_Qwemoller (const double q2, const double y) const |
| The computation of the electron's weak charge. More... | |
| virtual const double | delta_Qwn () const |
| The computation of the neutron weak charge: Qwn. More... | |
| virtual const double | delta_Qwp () const |
| The computation of the proton weak charge: Qwp. More... | |
| virtual const double | delta_sigma_ee (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| virtual const double | delta_sigma_f (const Particle f, const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| virtual const double | delta_sigma_had (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| virtual const double | delta_sigmaTot_ee (const double pol_e, const double pol_p, const double s) const |
| virtual const double | delta_sigmaTot_f (const Particle f, const double pol_e, const double pol_p, const double s) const |
| virtual const double | delta_TauLFU_gmuge () const |
| The computation of the correction to the LFU ratio \(g_\mu/ g_e \). More... | |
| virtual const double | delta_TauLFU_gtauge () const |
| The computation of the correction to the LFU ratio \(g_\tau/ g_e \). More... | |
| virtual const double | delta_TauLFU_gtaugmu () const |
| The computation of the correction to the LFU ratio \(g_\tau/ g_\mu \). More... | |
| virtual const double | delta_TauLFU_gtaugmuK () const |
| The computation of the correction to the LFU ratio \(\left(g_\tau/ g_\mu\right)_K \). More... | |
| virtual const double | delta_TauLFU_gtaugmuPi () const |
| The computation of the correction to the LFU ratio \(\left(g_\tau/ g_\mu\right)_\pi \). More... | |
| virtual const double | deltaa0 () const |
| The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaa02 () const |
| The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| 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 | 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 | deltaaMZ () const |
| The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaaMZ2 () const |
| The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaaSMZ () const |
| The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaaSMZ2 () const |
| The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltacZ_HB (const double mu) const |
| The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). 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 \(g_{1,\gamma}\). 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... | |
| const double | deltag3G () const |
| The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\). More... | |
| gslpp::complex | deltaG_Aff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). More... | |
| gslpp::complex | deltaG_Gff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu}^A \bar{f}\sigma^{\mu\nu} T_A f\). 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... | |
| gslpp::complex | deltaG_hAff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). 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... | |
| gslpp::complex | deltaG_hGff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). 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... | |
| gslpp::complex | deltaG_hZff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). More... | |
| gslpp::complex | deltaG_Zff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). More... | |
| virtual const double | deltaGA_f (const Particle p) const |
| New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| 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_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... | |
| const double | deltaGammaH2d2dRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2d2dRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2e2muRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2e2muRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2e2vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2e2vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2evRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2evRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2dRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2dRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2LRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2LRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2uRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2uRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2v2Ratio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2v2Ratio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2l2vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2l2vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2Lv2Ratio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2Lv2Ratio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2LvRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2LvRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2mu2vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2mu2vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2muvRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2muvRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2u2dRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2u2dRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2u2uRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2u2uRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2udRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2udRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2v2dRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2v2dRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2v2uRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2v2uRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2v2vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2v2vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4dRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4dRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4eRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4eRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4fCCRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4f, CC)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4fCCRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4f, CC)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4fNCRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4f, NC)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4fNCRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4f, NC)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4fRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4fRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4L2Ratio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4L2Ratio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4LRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4lRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4LRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4lRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4muRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4muRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4uRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4uRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHbbRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHbbRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHccRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHccRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHevmuvRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHevmuvRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHffRatio1 (const double mf, const double CifH) const |
| The ratio of the \(\Gamma(H\to ff)\) in the current model and in the Standard Model. More... | |
| const double | deltaGammaHffRatio2 (const double mf, const double CifH) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the ratio of the \(\Gamma(H\to ff)\) in the current model and in the Standard Model at order Lambd. More... | |
| const double | deltaGammaHgagaRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHgagaRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHggRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More... | |
| const double | deltaGammaHggRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHll_vvorjjRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHll_vvorjjRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHlv_lvorjjRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHlv_lvorjjRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHlvjjRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHlvjjRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHLvudRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHLvudRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHLvvLRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHLvvLRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHmumuRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHmumuRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHssRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ss)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHssRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ss)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHtautauRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHtautauRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHudduRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHudduRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWffRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWffRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWjjRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWjjRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWlvRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWlvRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWW2l2vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWW2l2vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWW4fRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWW4fRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWW4jRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWW4jRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWWRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWWRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZddRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZddRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZeeRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZeeRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZffRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZffRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZgaRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZgaRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZllRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZllRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZmumuRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZmumuRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZuuRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZuuRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZvvRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZvvRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ2e2muRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ2e2muRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4dRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4dRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4eRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4eRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4fRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4fRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4lRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4lRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4muRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4muRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4uRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4uRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| virtual const double | deltaGammaTotalRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More... | |
| virtual const double | deltaGammaTotalRatio1noError () const |
| The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors. More... | |
| virtual const double | deltaGammaTotalRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients. More... | |
| virtual const double | DeltaGF () const |
| New physics contribution to the Fermi constant. More... | |
| const double | deltaGL_f (const Particle p) const |
| New physics contribution to the neutral-current left-handed coupling \(g_L^f\). 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... | |
| gslpp::complex | deltaGL_Wffh (const Particle pbar, const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| const double | deltaGL_Zffh (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| virtual const double | deltaGmu () const |
| The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaGmu2 () const |
| The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| const double | deltaGR_f (const Particle p) const |
| New physics contribution to the neutral-current right-handed coupling \(g_R^f\). 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... | |
| gslpp::complex | deltaGR_Wffh (const Particle pbar, const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| const double | deltaGR_Zffh (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| virtual const double | deltaGV_f (const Particle p) const |
| New physics contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual const double | deltaGwd6 () const |
| The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\). More... | |
| virtual const double | deltaGwd62 () const |
| The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\). More... | |
| virtual const double | deltaGzd6 () const |
| The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\). More... | |
| virtual const double | deltaGzd62 () const |
| The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\). More... | |
| virtual const double | deltaH3L1 (double C1) const |
| The coefficient of the 1-loop linear term in the Higgs selfcoupling. More... | |
| virtual const double | deltaH3L2 (double C1) const |
| The coefficient of the 1-loop quadratic term in the Higgs selfcoupling. More... | |
| 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 | deltaKZNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(\kappa_{Z}\). More... | |
| virtual const double | deltamb () const |
| The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltamb2 () const |
| The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltamc () const |
| The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltamc2 () const |
| The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaMh () const |
| The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaMh2 () const |
| The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| const double | deltaMLL2_f (const Particle f, const double s, const double t) const |
| const double | deltaMLR2_f (const Particle f, const double s) const |
| const double | deltaMLR2t_e (const double s, const double t) const |
| const double | deltaMRL2_f (const Particle f, const double s) const |
| const double | deltaMRL2t_e (const double s, const double t) const |
| const double | deltaMRR2_f (const Particle f, const double s, const double t) const |
| virtual const double | deltamt () const |
| The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltamt2 () const |
| The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltamtau () const |
| The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltamtau2 () const |
| The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaMw () const |
| The relative correction to the mass of the \(W\) boson, \(\delta M_W/M_W\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaMw2 () const |
| The relative correction to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaMwd6 () const |
| The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\). More... | |
| virtual const double | deltaMwd62 () const |
| The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\). More... | |
| virtual const double | deltaMz () const |
| The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaMz2 () const |
| The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | DeltaOalphtoW (const double dOSMdalpha, const double mu) const |
| Difference in prediction in \(\alpha\) scheme and W mass scheme, computed from observable in \(\alpha\) scheme. Difference at tree level. More... | |
| virtual const double | DeltaOWtoalph (const double dOSMdMW, const double mu) const |
| Difference in prediction in \(\alpha\) scheme and W mass scheme, computed from observable in W mass scheme. Difference at tree level. 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 | 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 | 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 | 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.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | deltayc_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | deltaymu_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | deltays_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_s\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | deltayt_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | deltaytau_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | delU_gCC (const double mu) const |
| Universal indirect correction to EW charged currents. More... | |
| virtual const double | delU_gNC (const double mu) const |
| Universal indirect correction to EW neutral currents. 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]. 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 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... | |
| const double | GammaH2d2dRatio () const |
| The ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2e2muRatio () const |
| The ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2e2vRatio () const |
| The ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2evRatio () const |
| The ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2L2dRatio () const |
| The ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2L2LRatio () const |
| The ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2L2uRatio () const |
| The ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2L2v2Ratio () const |
| The ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2L2vRatio () const |
| The ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2l2vRatio () const |
| The ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2Lv2Ratio () const |
| The ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2LvRatio () const |
| The ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2mu2vRatio () const |
| The ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2muvRatio () const |
| The ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2u2dRatio () const |
| The ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2u2uRatio () const |
| The ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2udRatio () const |
| The ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2v2dRatio () const |
| The ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2v2uRatio () const |
| The ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2v2vRatio () const |
| The ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. More... | |
| const double | GammaH4dRatio () const |
| The ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. More... | |
| const double | GammaH4eRatio () const |
| The ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. More... | |
| const double | GammaH4fCCRatio () const |
| The ratio of the \(\Gamma(H\to 4f)\) via CC in the current model and in the Standard Model. More... | |
| const double | GammaH4fNCRatio () const |
| The ratio of the \(\Gamma(H\to 4f)\) via NC in the current model and in the Standard Model. More... | |
| const double | GammaH4fRatio () const |
| The ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. More... | |
| const double | GammaH4L2Ratio () const |
| The ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More... | |
| const double | GammaH4LRatio () const |
| The ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaH4lRatio () const |
| The ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More... | |
| const double | GammaH4muRatio () const |
| The ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. More... | |
| const double | GammaH4uRatio () const |
| The ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. More... | |
| const double | GammaH4vRatio () const |
| The ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. More... | |
| const double | GammaHbbRatio () const |
| The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. More... | |
| const double | GammaHccRatio () const |
| The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. More... | |
| const double | GammaHevmuvRatio () const |
| The ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. More... | |
| const double | GammaHgagaRatio () const |
| The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. More... | |
| const double | GammaHggRatio () const |
| The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. More... | |
| const double | GammaHll_vvorjjRatio () const |
| The ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More... | |
| const double | GammaHlv_lvorjjRatio () const |
| The ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More... | |
| const double | GammaHlvjjRatio () const |
| The ratio of the \(\Gamma(H\to l l j j)\) ( \(l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. @return \)\Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double GammaHlljjRatio() const; /** @brief The new physics contribution to the ratio of the \)\Gamma(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) @return \)\delta \Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double deltaGammaHlljjRatio1() const; /** @brief The new physics contribution to the ratio of the \)\Gamma(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) @return \)\delta \Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double deltaGammaHlljjRatio2() const; /** @brief The ratio of the Br\)(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. @return Br\)(H\to l l j j) \(/Br\)(H\to l l j j)_{\mathrm{SM}} \( */ virtual const double BrHlljjRatio() const; /** @brief The ratio of the \)\Gamma(H\to l \nu j j) \( (\)l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. More... | |
| const double | GammaHLvudRatio () const |
| The ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaHLvvLRatio () const |
| The ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaHmumuRatio () const |
| The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. More... | |
| const double | GammaHssRatio () const |
| The ratio of the \(\Gamma(H\to ss)\) in the current model and in the Standard Model. More... | |
| const double | GammaHtautauRatio () const |
| The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. More... | |
| const double | GammaHudduRatio () const |
| The ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. More... | |
| const double | GammaHWffRatio () const |
| The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| const double | GammaHWjjRatio () const |
| The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. More... | |
| const double | GammaHWlvRatio () const |
| The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| const double | GammaHWW2l2vRatio () const |
| The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| const double | GammaHWW4fRatio () const |
| The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| const double | GammaHWW4jRatio () const |
| The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. More... | |
| const double | GammaHWWRatio () const |
| The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. More... | |
| const double | GammaHZddRatio () const |
| The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More... | |
| const double | GammaHZeeRatio () const |
| The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. More... | |
| const double | GammaHZffRatio () const |
| The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| const double | GammaHZgaRatio () const |
| The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. More... | |
| const double | GammaHZllRatio () const |
| The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| const double | GammaHZmumuRatio () const |
| The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. More... | |
| const double | GammaHZuuRatio () const |
| The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More... | |
| const double | GammaHZvvRatio () const |
| The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. More... | |
| const double | GammaHZZ2e2muRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. More... | |
| const double | GammaHZZ4dRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More... | |
| const double | GammaHZZ4eRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More... | |
| const double | GammaHZZ4fRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| const double | GammaHZZ4lRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| const double | GammaHZZ4muRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More... | |
| const double | GammaHZZ4uRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More... | |
| const double | GammaHZZ4vRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More... | |
| 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... | |
| void | GenerateSMInitialConditions () |
| Generates the initial condition for the Standard Model parameters. More... | |
| double | getCG_LNP () const |
| Return CG_LNP. More... | |
| double | getLambda_NP () const |
| Return Lambda_NP. More... | |
| virtual NPSMEFTd6GeneralMatching & | getMatching () const |
| A method to get the Matching object for this model. More... | |
| virtual const double | IctW_TWG (const double mu) const |
| virtual const double | IctZ_TWG (const double mu) const |
| virtual bool | Init (const std::map< std::string, double > &DPars) |
| A method to initialize the model parameters. More... | |
| virtual const double | intDMLL2eus2 (const double s, const double t0, const double t1) const |
| virtual const double | intDMLR2etildest2 (const double s, const double t0, const double t1) const |
| virtual const double | intDMLR2ets2 (const double s, const double t0, const double t1) const |
| virtual const double | intDMRL2etildest2 (const double s, const double t0, const double t1) const |
| virtual const double | intDMRL2ets2 (const double s, const double t0, const double t1) const |
| virtual const double | intDMRR2eus2 (const double s, const double t0, const double t1) const |
| virtual const double | kappaAeff () const |
| The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\). 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 | kappaseff () const |
| The effective coupling \(\kappa_{s,eff}=\sqrt{\Gamma_{Hss}/\Gamma_{Hss}^{SM}}\). 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 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.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). 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 | mueeZHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. 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 | mueeZllHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. 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 | mueeZqqHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. 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 |
| The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muggHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. 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. (From arXiv: 1502.00539 [hpe-ph].) More... | |
| virtual const double | muggHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| 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 | muggHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muggHWW (const double sqrt_s) const |
| The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muggHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muggHZga (const double sqrt_s) const |
| The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muggHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muggHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| 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 | mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const |
| The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6General class. 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 | 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 |
| The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHWW (const double sqrt_s) const |
| The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHZga (const double sqrt_s) const |
| The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHZgamumu (const double sqrt_s) const |
| The ratio \(\mu_{ggH,Z\gamma\to \gamma 2\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\to \gamma 2\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHZZ4mu (const double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ\to 4\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHbb (const double sqrt_s) const |
| The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHWW (const double sqrt_s) const |
| The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHZga (const double sqrt_s) const |
| The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFBRinv (const double sqrt_s) const |
| The ratio \(\mu_{VBF}\) between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More... | |
| virtual const double | muTHUVBFHbb (const double sqrt_s) const |
| The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHgaga (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHinv (const double sqrt_s) const |
| The ratio \(\mu_{VBF,inv}\) between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHmumu (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHtautau (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHWW (const double sqrt_s) const |
| The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHZga (const double sqrt_s) const |
| The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHZZ (const double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHbb (const double sqrt_s) const |
| The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHBRinv (const double sqrt_s) const |
| The ratio \(\mu_{VH}\) between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More... | |
| virtual const double | muTHUVHgaga (const double sqrt_s) const |
| The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHinv (const double sqrt_s) const |
| The ratio \(\mu_{VH,inv}\) between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHmumu (const double sqrt_s) const |
| The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHtautau (const double sqrt_s) const |
| The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHWW (const double sqrt_s) const |
| The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHZga (const double sqrt_s) const |
| The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHZZ (const double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHbb (const double sqrt_s) const |
| The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHgaga (const double sqrt_s) const |
| The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHmumu (const double sqrt_s) const |
| The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHtautau (const double sqrt_s) const |
| The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHWW (const double sqrt_s) const |
| The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHZga (const double sqrt_s) const |
| The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHZZ (const double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHbb (const double sqrt_s) const |
| The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHWW (const double sqrt_s) const |
| The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHZga (const double sqrt_s) const |
| The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| 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 |
| The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muttHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| 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 |
| The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muttHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muttHWW (const double sqrt_s) const |
| The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muttHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| 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 |
| The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muttHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muttHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| 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 |
| The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHgaga (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHmumu (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHtautau (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHWW (const double sqrt_s) const |
| The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHZga (const double sqrt_s) const |
| The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHZZ (const double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| 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 | 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 |
| The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muVHgaga (const double sqrt_s) const |
| The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muVHmumu (const double sqrt_s) const |
| The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| 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 |
| The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muVHWW (const double sqrt_s) const |
| The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muVHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muVHZga (const double sqrt_s) const |
| The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muVHZZ (const double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muVHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| 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 |
| The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muWHgaga (const double sqrt_s) const |
| The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muWHmumu (const double sqrt_s) const |
| The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| 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 |
| The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muWHWW (const double sqrt_s) const |
| The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muWHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muWHZga (const double sqrt_s) const |
| The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muWHZZ (const double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muWHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| 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 |
| The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muZHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muZHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| 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 |
| The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muZHWW (const double sqrt_s) const |
| The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muZHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muZHZga (const double sqrt_s) const |
| The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muZHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muZHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | Mw () const |
| The mass of the \(W\) boson, \(M_W\). More... | |
| NPSMEFTd6General () | |
| Constructor. More... | |
| virtual const double | obliqueS () const |
| The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).) More... | |
| virtual const double | obliqueT () const |
| The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).) More... | |
| virtual const double | obliqueU () const |
| The oblique parameter \(U\). More... | |
| virtual const double | obliqueW () const |
| The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).) More... | |
| virtual const double | obliqueY () const |
| The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).) More... | |
| virtual bool | PostUpdate () |
| The post-update method for NPSMEFTd6General. 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 NPSMEFTd6General class. More... | |
| virtual bool | PreUpdate () |
| The pre-update method for NPSMEFTd6General. 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 | 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 check if all the mandatory parameters for NPSMEFTd6General have been provided in model initialization. More... | |
| virtual bool | setFlagStr (const std::string name, const std::string value) |
| A method to set a flag of NPSMEFTd6General. 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 | 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 \(gg \to H\), \(N_j=0,~p_{TH} [GeV]<10\). 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 \(gg \to H\), \(,450<~p_{TH} [GeV]\). 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... | |
| const double | tovers2 (const double cosmin, const double cosmax) const |
| const double | uovers2 (const double cosmin, const double cosmax) const |
| virtual const double | xseeWW (const double sqrt_s) const |
| Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\). 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]. 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]. More... | |
| Public Member Functions inherited from NPbase | |
| virtual const double | BR_Zf (const Particle f) const |
| The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\). 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 | 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 | cgaplusct () const |
| virtual const double | cgminuscga () const |
| virtual const double | cgplusct () const |
| virtual const double | cVpluscb () const |
| virtual const double | cVplusctau () const |
| virtual const double | deltaA_f_2 (const Particle f) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\Delta \mathcal{A}_f^{(2)}\). 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 | deltaGA_f_2 (const Particle f) const |
| virtual const double | deltaGamma_Z_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the total decay width of the \(Z\) boson, \(\Delta \Gamma_Z^{(2)}\). 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... | |
| 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... | |
| 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 const double | deltaGV_f_2 (const Particle f) const |
| virtual const double | deltaN_nu () const |
| The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements. 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_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 | 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 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 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 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 | 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 | muggHpbbH_Hgaga (const double sqrt_s) const |
| virtual const double | muggHpbbH_Htautau (const double sqrt_s) const |
| virtual const double | muggHpbbH_HWW (const double sqrt_s) const |
| virtual const double | muggHpbbH_HZZ (const double sqrt_s) const |
| virtual const double | muggHpttHptHpbbH_Hmumu (const double sqrt_s) const |
| virtual const double | muggHpttHptHpbbH_HZga (const double sqrt_s) const |
| virtual const double | muggHpVBFpbbH_Hbb (const double sqrt_s) const |
| virtual const double | muppHmumu (const double sqrt_s) const |
| virtual const double | muppHZga (const double sqrt_s) const |
| virtual const double | mutHgaga (const double sqrt_s) const |
| virtual const double | muttHptH_Hbb (const double sqrt_s) const |
| virtual const double | muttHptH_Hgaga (const double sqrt_s) const |
| virtual const double | muttHptH_Hmumu (const double sqrt_s) const |
| virtual const double | muttHptH_Htautau (const double sqrt_s) const |
| virtual const double | muttHptH_HWW (const double sqrt_s) const |
| virtual const double | muttHptH_HZZ (const double sqrt_s) const |
| virtual const double | muVBFpVH_Hmumu (const double sqrt_s) const |
| virtual const double | muVBFpVH_HZga (const double sqrt_s) const |
| virtual const double | muVHcc (const double sqrt_s) const |
| virtual const double | N_nu () const |
| The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\). More... | |
| NPbase () | |
| The default constructor. 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 | 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 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 | 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... | |
| 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... | |
| 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... | |
| 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 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 | 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 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) |
| 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... | |
Static Public Attributes | |
| static const int | NNPSMEFTd6GeneralVars = 2708-208 + 79 |
| The number of the model parameters in NPSMEFTd6General (including the 18 parameters needed for the SM and 79 auxiliary parameters). More... | |
| static const std::string | NPSMEFTd6GeneralVars [NNPSMEFTd6GeneralVars] |
| A string array containing the labels of the model parameters in NPSMEFTd6General. 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... | |
Additional Inherited Members | |
| Public Types inherited from StandardModel | |
| enum | LEP2RCs { Weak = 0 , WeakBox , ISR , QEDFSR , QCDFSR , NUMofLEP2RCs } |
| enum | orders_EW { EW1 = 0 , EW1QCD1 , EW1QCD2 , EW2 , EW2QCD1 , EW3 , orders_EW_size } |
| An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More... | |
| Public Types inherited from QCD | |
| enum | lepton { NEUTRINO_1 , ELECTRON , NEUTRINO_2 , MU , NEUTRINO_3 , TAU , NOLEPTON } |
| An enum type for leptons. More... | |
| enum | meson { P_0 , P_P , K_0 , K_P , D_0 , D_P , D_S , B_D , B_P , B_S , B_C , PHI , K_star , K_star_P , K_S , D_star_P , RHO , RHO_P , OMEGA , MESON_END } |
| An enum type for mesons. More... | |
| enum | quark { UP , DOWN , CHARM , STRANGE , TOP , BOTTOM } |
| An enum type for quarks. More... | |
| Protected Member Functions inherited from StandardModel | |
| const double | AFB_NoISR_l (const QCD::lepton l_flavor, const double s) const |
| const double | AFB_NoISR_q (const QCD::quark q_flavor, const double s) const |
| bool | checkEWPOscheme (const std::string scheme) const |
| A method to check if a given scheme name in string form is valid. 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... | |
| NPSMEFTd6General::NPSMEFTd6General | ( | ) |
Constructor.
Definition at line 330 of file NPSMEFTd6General.cpp.
|
virtual |
The left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\mathcal{A}_f\).
\[ \mathcal{A}_f = \mathcal{A}_f^{SM} + \Delta \mathcal{A}_f^{(1)} + \Delta \mathcal{A}_f^{(2)} \]
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 16468 of file NPSMEFTd6General.cpp.
|
virtual |
The forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(A^f_{FB}\).
\[ A_{FB,f} = A_{FB,f}^{SM} + \Delta A_{FB,f}^{(1)} + \Delta A_{FB,f}^{(2)} \]
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 16696 of file NPSMEFTd6General.cpp.
|
virtual |
The electromagnetic coupling at the \(Z\)-mass scale.
Reimplemented from NPbase.
Definition at line 15552 of file NPSMEFTd6General.cpp.
|
virtual |
the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]).
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 24852 of file NPSMEFTd6General.cpp.
|
virtual |
the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]).
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 24934 of file NPSMEFTd6General.cpp.
|
virtual |
The branching ratio of the of the Higgs into exotic particles.
Reimplemented from NPbase.
Definition at line 35175 of file NPSMEFTd6General.cpp.
|
virtual |
The branching ratio of the of the Higgs into invisible particles.
Reimplemented from NPbase.
Definition at line 35181 of file NPSMEFTd6General.cpp.
|
virtual |
The branching ratio of the of the Higgs into invisible particles (only invisible new particles).
Reimplemented from NPbase.
Definition at line 35194 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2d2d)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 30389 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2e 2\mu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 29158 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2e2v)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 29792 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 34337 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 31339 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 29065 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 30995 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 29699 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 29604 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 34831 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 34242 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 34143 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2\mu 2v)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 29884 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 34432 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2u2d)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 30684 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2u2u)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 30119 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2ud)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 33941 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2v2d)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 31912 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2v2u)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 31606 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 2v2v)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 29362 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 4d)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 33155 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 4e)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 32336 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 4f, CC)\) in the current model and in the Standard Model.
Definition at line 34703 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 4f, NC)\) in the current model and in the Standard Model.
Definition at line 34628 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 4f)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 34539 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 32246 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 32153 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 34767 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 4\mu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 32426 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 4u)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 32876 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to 4v)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 32628 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28812 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28613 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to e\nu \mu\nu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 33390 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28311 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 26042 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 35148 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 35086 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 35023 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 33712 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 33299 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28424 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to s\bar{s})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28712 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28511 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 35252 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to uddu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 33545 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 35203 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to VV)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 27891 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 26489 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model.
Definition at line 26330 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 26171 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 26253 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 26632 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to WW^*\to 4j)\) in the current model and in the Standard Model.
Definition at line 26411 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 26111 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.
Definition at line 27546 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 27646 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28074 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28060 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28084 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28035 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 26760 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model.
Definition at line 27453 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model.
Definition at line 27291 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model.
Definition at line 27130 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.
Definition at line 27570 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model.
Definition at line 27047 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 27867 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 26964 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model.
Definition at line 27213 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model.
Definition at line 27477 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model.
Definition at line 27374 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 26700 of file NPSMEFTd6General.cpp.
The branching ratio of the \(W\) boson decaying into a SM fermion pair, \(Br(W\to f_i f_j)\).
Reimplemented from NPbase.
Definition at line 16122 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47504 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLL_bottom | ( | const double | mu | ) | const |
Definition at line 45845 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLL_charm | ( | const double | mu | ) | const |
Definition at line 45829 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLL_down | ( | const double | mu | ) | const |
Definition at line 45837 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLL_e | ( | const double | mu | ) | const |
Definition at line 45813 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLL_mu | ( | const double | mu | ) | const |
Definition at line 45817 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLL_strange | ( | const double | mu | ) | const |
Definition at line 45841 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLL_tau | ( | const double | mu | ) | const |
Definition at line 45821 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLL_top | ( | const double | mu | ) | const |
Definition at line 45833 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLL_up | ( | const double | mu | ) | const |
Definition at line 45825 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLR_bottom | ( | const double | mu | ) | const |
Definition at line 45881 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLR_charm | ( | const double | mu | ) | const |
Definition at line 45865 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLR_down | ( | const double | mu | ) | const |
Definition at line 45873 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLR_e | ( | const double | mu | ) | const |
Definition at line 45849 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLR_mu | ( | const double | mu | ) | const |
Definition at line 45853 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLR_strange | ( | const double | mu | ) | const |
Definition at line 45877 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLR_tau | ( | const double | mu | ) | const |
Definition at line 45857 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLR_top | ( | const double | mu | ) | const |
Definition at line 45869 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeLR_up | ( | const double | mu | ) | const |
Definition at line 45861 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRL_bottom | ( | const double | mu | ) | const |
Definition at line 45918 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRL_charm | ( | const double | mu | ) | const |
Definition at line 45902 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRL_down | ( | const double | mu | ) | const |
Definition at line 45910 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRL_e | ( | const double | mu | ) | const |
Definition at line 45885 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRL_mu | ( | const double | mu | ) | const |
Definition at line 45890 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRL_strange | ( | const double | mu | ) | const |
Definition at line 45914 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRL_tau | ( | const double | mu | ) | const |
Definition at line 45894 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRL_top | ( | const double | mu | ) | const |
Definition at line 45906 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRL_up | ( | const double | mu | ) | const |
Definition at line 45898 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRR_bottom | ( | const double | mu | ) | const |
Definition at line 45954 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRR_charm | ( | const double | mu | ) | const |
Definition at line 45938 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRR_down | ( | const double | mu | ) | const |
Definition at line 45946 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRR_e | ( | const double | mu | ) | const |
Definition at line 45922 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRR_mu | ( | const double | mu | ) | const |
Definition at line 45926 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRR_strange | ( | const double | mu | ) | const |
Definition at line 45950 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRR_tau | ( | const double | mu | ) | const |
Definition at line 45930 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRR_top | ( | const double | mu | ) | const |
Definition at line 45942 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::CeeRR_up | ( | const double | mu | ) | const |
Definition at line 45934 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{11}\).
Reimplemented from NPbase.
Definition at line 43298 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{22}\).
Reimplemented from NPbase.
Definition at line 43302 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{33}\).
Reimplemented from NPbase.
Definition at line 43306 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{11}\).
Reimplemented from NPbase.
Definition at line 43274 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{22}\).
Reimplemented from NPbase.
Definition at line 43278 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{33}\).
Reimplemented from NPbase.
Definition at line 43282 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{11}\).
Reimplemented from NPbase.
Definition at line 43218 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{22}\).
Reimplemented from NPbase.
Definition at line 43222 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{33}\).
Reimplemented from NPbase.
Definition at line 43226 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{11}\).
Reimplemented from NPbase.
Definition at line 43230 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{22}\).
Reimplemented from NPbase.
Definition at line 43234 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{33}\).
Reimplemented from NPbase.
Definition at line 43238 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{11}\).
Reimplemented from NPbase.
Definition at line 43242 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{22}\).
Reimplemented from NPbase.
Definition at line 43246 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{33}\).
Reimplemented from NPbase.
Definition at line 43250 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{11}\).
Reimplemented from NPbase.
Definition at line 43254 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{22}\).
Reimplemented from NPbase.
Definition at line 43258 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{33}\).
Reimplemented from NPbase.
Definition at line 43262 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(d)})_{33}\).
Reimplemented from NPbase.
Definition at line 43266 of file NPSMEFTd6General.cpp.
|
virtual |
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{11}\).
Reimplemented from NPbase.
Definition at line 43286 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{22}\).
Reimplemented from NPbase.
Definition at line 43290 of file NPSMEFTd6General.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{33}\).
Reimplemented from NPbase.
Definition at line 43294 of file NPSMEFTd6General.cpp.
|
virtual |
The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43175 of file NPSMEFTd6General.cpp.
|
virtual |
The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43183 of file NPSMEFTd6General.cpp.
|
virtual |
The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43191 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47429 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47409 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47389 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47399 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47419 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47439 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 25849 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47291 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47302 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47548 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47537 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47515 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47526 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47247 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47258 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47175 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47225 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47236 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47185 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47205 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47215 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47269 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47280 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47357 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47368 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47570 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47493 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47379 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47559 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47581 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47592 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47313 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47324 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47195 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47335 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47346 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47449 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47471 of file NPSMEFTd6General.cpp.
|
virtual |
The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43148 of file NPSMEFTd6General.cpp.
|
virtual |
The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43167 of file NPSMEFTd6General.cpp.
|
virtual |
The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43159 of file NPSMEFTd6General.cpp.
|
virtual |
Correction to photon WF.
| [in] | mu | the RG scale associated to the observable where the function is used |
Definition at line 15329 of file NPSMEFTd6General.cpp.
|
virtual |
Correction to electric charge.
| [in] | mu | the RG scale associated to the observable where the function is used |
Definition at line 15357 of file NPSMEFTd6General.cpp.
|
virtual |
Correction to (sin squared of) weak mixing angle.
| [in] | mu | the RG scale associated to the observable where the function is used |
Definition at line 15371 of file NPSMEFTd6General.cpp.
|
virtual |
Correction to Z WF.
| [in] | mu | the RG scale associated to the observable where the function is used |
Definition at line 15338 of file NPSMEFTd6General.cpp.
|
virtual |
Correction to Z-A mixing.
| [in] | mu | the RG scale associated to the observable where the function is used |
Definition at line 15347 of file NPSMEFTd6General.cpp.
|
virtual |
Separate, charge-proportional, indirect correction to EW neutral currents.
| [in] | mu | the RG scale associated to the observable where the function is used |
Definition at line 15404 of file NPSMEFTd6General.cpp.
|
virtual |
Quadratic contribution from the Higgs self-couplings modifications to the signal strength for \(\sigma \times BR(H\to xx)\) in the current model.
Reimplemented from NPbase.
Definition at line 15305 of file NPSMEFTd6General.cpp.
|
virtual |
Quadratic contribution from the Higgs self-couplings modifications to the signal strength for an observable \(\sigma\) in the current model.
Reimplemented from NPbase.
Definition at line 15293 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46878 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46559 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the parity violating asymmetry in Moller scattering.
| [in] | q2 | the \(Q^2\) of the process |
| [in] | y |
Definition at line 46943 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the anomalous magnetic moment of the muon \(a_\mu=(g_\mu-2)/2\).
Definition at line 46908 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46475 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gAnue.
Definition at line 47057 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the correction to the effective neutrino nucleon LH coupling: delta_gLnuN2.
Definition at line 47001 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the correction to the effective neutrino nucleon RH coupling: delta_gRnuN2.
Definition at line 47023 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gVnue.
Definition at line 47045 of file NPSMEFTd6General.cpp.
|
inlinevirtual |
The SMEFT linear correction to the ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2249 of file NPSMEFTd6General.h.
|
inlinevirtual |
The SMEFT quadratic correction to the ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2253 of file NPSMEFTd6General.h.
|
virtual |
The SMEFT linear correction to the ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 17878 of file NPSMEFTd6General.cpp.
|
virtual |
The SMEFT quadratic correction to the ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 17993 of file NPSMEFTd6General.cpp.
|
virtual |
The SMEFT linear correction to the ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 20071 of file NPSMEFTd6General.cpp.
|
virtual |
The SMEFT quadratic correction to the ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 20125 of file NPSMEFTd6General.cpp.
|
virtual |
The SMEFT linear correction to the ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 19218 of file NPSMEFTd6General.cpp.
|
virtual |
The SMEFT quadratic correction to the ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 19668 of file NPSMEFTd6General.cpp.
|
virtual |
The SMEFT linear correction to the ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 18029 of file NPSMEFTd6General.cpp.
|
virtual |
The SMEFT quadratic correction to the ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 18345 of file NPSMEFTd6General.cpp.
|
virtual |
The SMEFT linear correction to the ratio \(\mu_{VH}\) between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 20235 of file NPSMEFTd6General.cpp.
|
virtual |
The SMEFT quadratic correction to the ratio \(\mu_{VH}\) between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 20248 of file NPSMEFTd6General.cpp.
|
virtual |
The SMEFT linear correction to the ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 18496 of file NPSMEFTd6General.cpp.
|
virtual |
The SMEFT quadratic correction to the ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 18696 of file NPSMEFTd6General.cpp.
|
virtual |
The SMEFT linear correction to the ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 18781 of file NPSMEFTd6General.cpp.
|
virtual |
The SMEFT quadratic correction to the ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 19056 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the electron's weak charge.
| [in] | q2 | the \(Q^2\) at which the weak charge is measured |
| [in] | y |
Definition at line 46914 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the neutron weak charge: Qwn.
Definition at line 46974 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the proton weak charge: Qwp.
Definition at line 46947 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46838 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46517 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46545 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46872 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46555 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the correction to the LFU ratio \(g_\mu/ g_e \).
Definition at line 47074 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the correction to the LFU ratio \(g_\tau/ g_e \).
Definition at line 47098 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the correction to the LFU ratio \(g_\tau/ g_\mu \).
Definition at line 47086 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the correction to the LFU ratio \(\left(g_\tau/ g_\mu\right)_K \).
Definition at line 47139 of file NPSMEFTd6General.cpp.
|
virtual |
The computation of the correction to the LFU ratio \(\left(g_\tau/ g_\mu\right)_\pi \).
Definition at line 47110 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15521 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15526 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta \mathcal{A}_f\).
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 16321 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta A^f_{FB}\).
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 16474 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15512 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15517 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15530 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15535 of file NPSMEFTd6General.cpp.
|
virtual |
The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43136 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented from NPbase.
Definition at line 37646 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics relative contribution to the EW coupling constant \(e\).
Reimplemented from NPbase.
Definition at line 36448 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 17276 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17525 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 17313 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17574 of file NPSMEFTd6General.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 17317 of file NPSMEFTd6General.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17585 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 17297 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17547 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(g_{1,\gamma}\).
Reimplemented from NPbase.
Definition at line 36481 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\).
Reimplemented from NPbase.
Definition at line 36459 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph].
Reimplemented from NPbase.
Definition at line 36511 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 17280 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17529 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 17406 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17674 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 17301 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17557 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\).
Reimplemented from NPbase.
Definition at line 17284 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17533 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\).
Reimplemented from NPbase.
Definition at line 17305 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17561 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltag3G | ( | ) | const |
The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\).
Definition at line 17854 of file NPSMEFTd6General.cpp.
| gslpp::complex NPSMEFTd6General::deltaG_Aff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 17848 of file NPSMEFTd6General.cpp.
| gslpp::complex NPSMEFTd6General::deltaG_Gff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu}^A \bar{f}\sigma^{\mu\nu} T_A f\).
| [in] | p | a lepton or quark |
Definition at line 17836 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 17410 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17678 of file NPSMEFTd6General.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 17414 of file NPSMEFTd6General.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17688 of file NPSMEFTd6General.cpp.
| gslpp::complex NPSMEFTd6General::deltaG_hAff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 17828 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\).
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 17472 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\).
| [in] | p | a lepton or quark |
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17746 of file NPSMEFTd6General.cpp.
| gslpp::complex NPSMEFTd6General::deltaG_hGff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 17816 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\).
Reimplemented from NPbase.
Definition at line 17247 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17496 of file NPSMEFTd6General.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 17251 of file NPSMEFTd6General.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17500 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 17485 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value.
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 17767 of file NPSMEFTd6General.cpp.
| gslpp::complex NPSMEFTd6General::deltaG_hZff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 17822 of file NPSMEFTd6General.cpp.
| gslpp::complex NPSMEFTd6General::deltaG_Zff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 17842 of file NPSMEFTd6General.cpp.
|
virtual |
New physics contribution to the neutral-current axial-vector coupling \(g_A^f\).
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 16993 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\).
Reimplemented from NPbase.
Definition at line 15697 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\).
| [in] | fi | a lepton or quark |
| [in] | fj | a lepton or quark |
Reimplemented from NPbase.
Definition at line 15599 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\).
Reimplemented from NPbase.
Definition at line 16016 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\).
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 15742 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2d2dRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 30158 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2d2dRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 30229 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2e2muRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 29104 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2e2muRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 29148 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2e2vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 29738 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2e2vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 29782 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2evRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 34281 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2evRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 34327 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2L2dRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 31034 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2L2dRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 31118 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2L2LRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 28851 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2L2LRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 28921 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2L2uRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 30723 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2L2uRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 30802 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2L2v2Ratio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 29643 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2L2v2Ratio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 29691 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2L2vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 29401 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2l2vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 34806 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2L2vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 29473 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2l2vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 34821 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2Lv2Ratio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 34182 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2Lv2Ratio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 34232 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2LvRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 33980 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2LvRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 34057 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2mu2vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 29831 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2mu2vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 29874 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2muvRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 34376 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2muvRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 34422 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2u2dRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 30428 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2u2dRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 30506 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2u2uRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 29923 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2u2uRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 29989 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2udRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 33751 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2udRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 33828 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2v2dRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 31645 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2v2dRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 31723 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2v2uRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 31378 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2v2uRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 31451 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2v2vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 29197 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH2v2vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 29260 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4dRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 32915 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4dRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 32988 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4eRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 32285 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4eRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 32326 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4fCCRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4f, CC)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 34668 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4fCCRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4f, CC)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 34684 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4fNCRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4f, NC)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 34579 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4fNCRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4f, NC)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 34602 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4fRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 34471 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4fRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 34508 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4L2Ratio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 32192 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4L2Ratio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 32236 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4LRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 31951 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4lRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 34743 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4LRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 32020 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4lRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 34757 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4muRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 32375 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4muRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 32416 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4uRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 32667 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4uRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 32735 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 32465 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaH4vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 32528 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 28752 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 28798 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 28551 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 28598 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHevmuvRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 33338 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHevmuvRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 33380 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHffRatio1 | ( | const double | mf, |
| const double | CifH | ||
| ) | const |
The ratio of the \(\Gamma(H\to ff)\) in the current model and in the Standard Model.
Definition at line 28336 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHffRatio2 | ( | const double | mf, |
| const double | CifH | ||
| ) | const |
The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the ratio of the \(\Gamma(H\to ff)\) in the current model and in the Standard Model at order Lambd.
Definition at line 28346 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 28109 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 28301 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.
Reimplemented from NPbase.
Definition at line 25960 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 26032 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHll_vvorjjRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 35125 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHll_vvorjjRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 35140 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHlv_lvorjjRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 35062 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHlv_lvorjjRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 35078 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHlvjjRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 34971 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHlvjjRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 35015 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHLvudRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 33584 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHLvudRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 33646 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHLvvLRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 33194 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHLvvLRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 33252 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 28377 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 28409 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHssRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ss)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 28654 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHssRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ss)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 28699 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 28464 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 28496 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHudduRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 33429 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHudduRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 33487 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHWffRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 26450 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHWffRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 26479 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHWjjRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 26292 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHWjjRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 26320 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHWlvRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 26133 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHWlvRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 26161 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHWW2l2vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 26210 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHWW2l2vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 26243 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHWW4fRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 26528 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHWW4fRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 26588 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHWW4jRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 26369 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHWW4jRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 26401 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 26082 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 26101 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZddRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 27506 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZddRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 27536 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZeeRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 26799 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZeeRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 26831 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZffRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 27602 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZffRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 27636 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 27912 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 28025 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZllRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 26720 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZllRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 26750 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZmumuRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 26856 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZmumuRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 26888 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZuuRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 27413 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZuuRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 27443 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZvvRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 27252 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZvvRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 27281 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZZ2e2muRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 27086 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZZ2e2muRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 27120 of file NPSMEFTd6General.cpp.
|
inline |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 2867 of file NPSMEFTd6General.h.
|
inline |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 2877 of file NPSMEFTd6General.h.
| const double NPSMEFTd6General::deltaGammaHZZ4eRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 27003 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZZ4eRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 27037 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZZ4fRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 27685 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZZ4fRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 27765 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZZ4lRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 26913 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZZ4lRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 26954 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZZ4muRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 27169 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZZ4muRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 27203 of file NPSMEFTd6General.cpp.
|
inline |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 2805 of file NPSMEFTd6General.h.
|
inline |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 2815 of file NPSMEFTd6General.h.
| const double NPSMEFTd6General::deltaGammaHZZ4vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 27330 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGammaHZZ4vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 27364 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 26671 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 26690 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.
Reimplemented from NPbase.
Definition at line 25865 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors.
Definition at line 25897 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients.
Reimplemented from NPbase.
Definition at line 25922 of file NPSMEFTd6General.cpp.
|
virtual |
New physics contribution to the Fermi constant.
The new physics contribution \(\Delta G\) is defined as
\[ G_\mu = G_{\mu,\mathrm{SM}}(1+\Delta G)\,, \]
where \(G_\mu\) is the experimental value measured through muon decays, and \(G_{\mu,\mathrm{SM}}\) is the Fermi constant in the SM.
Reimplemented from NPbase.
Definition at line 15322 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGL_f | ( | const Particle | p | ) | const |
New physics contribution to the neutral-current left-handed coupling \(g_L^f\).
| [in] | f | a lepton or quark |
Definition at line 16997 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGL_f_mu | ( | const Particle | p, |
| const double | mu | ||
| ) | const |
New physics contribution to the neutral-current left-handed coupling \(g_L^f\).
| [in] | f | a lepton or quark |
| [in] | mu | the RG scale to be used in the evaluation |
Definition at line 17028 of file NPSMEFTd6General.cpp.
|
virtual |
New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 17168 of file NPSMEFTd6General.cpp.
|
virtual |
New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\).
| [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) |
Reimplemented from NPbase.
Definition at line 17194 of file NPSMEFTd6General.cpp.
The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Definition at line 17784 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGL_Zffh | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | p | a lepton or quark |
Definition at line 17802 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15503 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15508 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGR_f | ( | const Particle | p | ) | const |
New physics contribution to the neutral-current right-handed coupling \(g_R^f\).
| [in] | f | a lepton or quark |
Definition at line 17013 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGR_f_mu | ( | const Particle | p, |
| const double | mu | ||
| ) | const |
New physics contribution to the neutral-current right-handed coupling \(g_R^f\).
| [in] | f | a lepton or quark |
| [in] | mu | the RG scale to be used in the evaluation |
Definition at line 17099 of file NPSMEFTd6General.cpp.
|
virtual |
New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 17185 of file NPSMEFTd6General.cpp.
|
virtual |
New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\).
| [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) |
Reimplemented from NPbase.
Definition at line 17224 of file NPSMEFTd6General.cpp.
The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Definition at line 17794 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaGR_Zffh | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | p | a lepton or quark |
Definition at line 17809 of file NPSMEFTd6General.cpp.
|
virtual |
New physics contribution to the neutral-current vector coupling \(g_V^f\).
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 16989 of file NPSMEFTd6General.cpp.
|
virtual |
The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\).
Definition at line 15732 of file NPSMEFTd6General.cpp.
|
virtual |
The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\).
Definition at line 15736 of file NPSMEFTd6General.cpp.
|
virtual |
The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\).
Definition at line 16112 of file NPSMEFTd6General.cpp.
|
virtual |
The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\).
Definition at line 16116 of file NPSMEFTd6General.cpp.
|
virtual |
The coefficient of the 1-loop linear term in the Higgs selfcoupling.
Definition at line 15270 of file NPSMEFTd6General.cpp.
|
virtual |
The coefficient of the 1-loop quadratic term in the Higgs selfcoupling.
Definition at line 15282 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\).
Reimplemented from NPbase.
Definition at line 36489 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph].
Reimplemented from NPbase.
Definition at line 36523 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(\kappa_{Z}\).
Definition at line 36475 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15476 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15481 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15485 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15490 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15458 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15463 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaMLL2_f | ( | const Particle | f, |
| const double | s, | ||
| const double | t | ||
| ) | const |
Definition at line 46228 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaMLR2_f | ( | const Particle | f, |
| const double | s | ||
| ) | const |
Definition at line 45958 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaMLR2t_e | ( | const double | s, |
| const double | t | ||
| ) | const |
Definition at line 46176 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaMRL2_f | ( | const Particle | f, |
| const double | s | ||
| ) | const |
Definition at line 46067 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaMRL2t_e | ( | const double | s, |
| const double | t | ||
| ) | const |
Definition at line 46224 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::deltaMRR2_f | ( | const Particle | f, |
| const double | s, | ||
| const double | t | ||
| ) | const |
Definition at line 46346 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15467 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15472 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15494 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15499 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(W\) boson, \(\delta M_W/M_W\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15539 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15545 of file NPSMEFTd6General.cpp.
|
virtual |
The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\).
Definition at line 15579 of file NPSMEFTd6General.cpp.
|
virtual |
The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\).
Definition at line 15593 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15449 of file NPSMEFTd6General.cpp.
|
virtual |
The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 15454 of file NPSMEFTd6General.cpp.
|
virtual |
Difference in prediction in \(\alpha\) scheme and W mass scheme, computed from observable in \(\alpha\) scheme. Difference at tree level.
The difference \(\Delta O\) is defined as
\[ \Delta O = O_{\alpha} - O_{W} \,, \]
where \(O\) is a given observable in the SMEFT.
| [in] | dOSMdalpha | the derivative with respect to \(\alpha\) of the SM tree-level prediction of \(O\) (in the \(\alpha\) scheme) |
| [in] | mu | the RG scale associated to the observable |
Definition at line 15225 of file NPSMEFTd6General.cpp.
|
virtual |
Difference in prediction in \(\alpha\) scheme and W mass scheme, computed from observable in W mass scheme. Difference at tree level.
The difference \(\Delta O\) is defined as
\[ \Delta O = O_{\alpha} - O_{W} \,, \]
where \(O\) is a given observable in the SMEFT.
| [in] | dOSMdMW | the derivative with respect to \(M_W\) of the SM tree-level prediction of \(O\) (in the \(M_W\) scheme) |
| [in] | mu | the RG scale associated to the observable |
Definition at line 15244 of file NPSMEFTd6General.cpp.
|
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.
| f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 16702 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\delta \sigma_h^0\).
Reimplemented from NPbase.
Definition at line 16216 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented from NPbase.
Definition at line 36536 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented from NPbase.
Definition at line 37638 of file NPSMEFTd6General.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43071 of file NPSMEFTd6General.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43097 of file NPSMEFTd6General.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43123 of file NPSMEFTd6General.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_s\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43110 of file NPSMEFTd6General.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43058 of file NPSMEFTd6General.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43084 of file NPSMEFTd6General.cpp.
|
virtual |
Universal indirect correction to EW charged currents.
| [in] | mu | the RG scale associated to the observable where the function is used |
Definition at line 15415 of file NPSMEFTd6General.cpp.
|
virtual |
Universal indirect correction to EW neutral currents.
| [in] | mu | the RG scale associated to the observable where the function is used |
Definition at line 15386 of file NPSMEFTd6General.cpp.
|
virtual |
The differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented from NPbase.
Definition at line 38029 of file NPSMEFTd6General.cpp.
|
virtual |
The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle.
Reimplemented from NPbase.
Definition at line 38422 of file NPSMEFTd6General.cpp.
|
virtual |
The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle.
Reimplemented from NPbase.
Definition at line 38720 of file NPSMEFTd6General.cpp.
|
virtual |
The total decay width of the \(Z\) boson, \(\Gamma_Z\).
\[ \Gamma_Z = \Gamma_Z^{SM} + \Delta \Gamma_Z^{(1)} + \Delta \Gamma_Z^{(2)} \]
Reimplemented from NPbase.
Definition at line 16107 of file NPSMEFTd6General.cpp.
|
virtual |
The decay width of the \(Z\) boson into a given fermion pair, \(\Gamma_Z^{f}\).
\[ \Gamma_Z^{f} = \Gamma_{Z,f}^{SM} + \Delta \Gamma_{Z,f}^{(1)} + \Delta \Gamma_{Z,f}^{(2)} \]
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 16010 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2d2dRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model.
Definition at line 30144 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2e2muRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model.
Definition at line 29090 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2e2vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model.
Definition at line 29724 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2evRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model.
Definition at line 34267 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2L2dRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 31020 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2L2LRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 28837 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2L2uRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 30709 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2L2v2Ratio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Definition at line 29629 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2L2vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 29387 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2l2vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model.
Definition at line 34792 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2Lv2Ratio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Definition at line 34168 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2LvRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 33966 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2mu2vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model.
Definition at line 29817 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2muvRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model.
Definition at line 34362 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2u2dRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model.
Definition at line 30414 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2u2uRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model.
Definition at line 29909 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2udRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model.
Definition at line 33737 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2v2dRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model.
Definition at line 31631 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2v2uRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model.
Definition at line 31364 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH2v2vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model.
Definition at line 29183 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH4dRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model.
Definition at line 32901 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH4eRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model.
Definition at line 32271 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH4fCCRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4f)\) via CC in the current model and in the Standard Model.
Definition at line 34654 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH4fNCRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4f)\) via NC in the current model and in the Standard Model.
Definition at line 34565 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH4fRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model.
Definition at line 34457 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH4L2Ratio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Definition at line 32178 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH4LRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 31937 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH4lRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model.
Definition at line 34729 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH4muRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model.
Definition at line 32361 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH4uRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model.
Definition at line 32653 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaH4vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model.
Definition at line 32451 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28738 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28536 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHevmuvRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model.
Definition at line 33324 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28094 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 25945 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHll_vvorjjRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Definition at line 35111 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHlv_lvorjjRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Definition at line 35048 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHlvjjRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to l l j j)\) ( \(l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. @return \)\Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double GammaHlljjRatio() const; /** @brief The new physics contribution to the ratio of the \)\Gamma(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) @return \)\delta \Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double deltaGammaHlljjRatio1() const; /** @brief The new physics contribution to the ratio of the \)\Gamma(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) @return \)\delta \Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double deltaGammaHlljjRatio2() const; /** @brief The ratio of the Br\)(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. @return Br\)(H\to l l j j) \(/Br\)(H\to l l j j)_{\mathrm{SM}} \( */ virtual const double BrHlljjRatio() const; /** @brief The ratio of the \)\Gamma(H\to l \nu j j) \( (\)l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model.
Definition at line 34957 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHLvudRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 33570 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHLvvLRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 33180 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28362 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to ss)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28639 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 28449 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHudduRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model.
Definition at line 33415 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHWffRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 26435 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHWjjRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model.
Definition at line 26277 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHWlvRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 26118 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHWW2l2vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 26195 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHWW4fRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 26513 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHWW4jRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model.
Definition at line 26354 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 26067 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHZddRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.
Definition at line 27491 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHZeeRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model.
Definition at line 26784 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHZffRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 27587 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 27897 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHZllRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 26705 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHZmumuRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model.
Definition at line 26841 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHZuuRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model.
Definition at line 27398 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHZvvRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model.
Definition at line 27237 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHZZ2e2muRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model.
Definition at line 27071 of file NPSMEFTd6General.cpp.
|
inline |
The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.
Definition at line 2857 of file NPSMEFTd6General.h.
| const double NPSMEFTd6General::GammaHZZ4eRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model.
Definition at line 26988 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHZZ4fRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 27670 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHZZ4lRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 26898 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::GammaHZZ4muRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model.
Definition at line 27154 of file NPSMEFTd6General.cpp.
|
inline |
The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model.
Definition at line 2795 of file NPSMEFTd6General.h.
| const double NPSMEFTd6General::GammaHZZ4vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model.
Definition at line 27315 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 26656 of file NPSMEFTd6General.cpp.
|
virtual |
The total width of the \(W\) boson, \(\Gamma_W\).
Reimplemented from NPbase.
Definition at line 15728 of file NPSMEFTd6General.cpp.
A partial decay width of the \(W\) boson decay into a SM fermion pair.
| [in] | fi | a lepton or quark |
| [in] | fj | a lepton or quark |
Reimplemented from NPbase.
Definition at line 15693 of file NPSMEFTd6General.cpp.
| void NPSMEFTd6General::GenerateSMInitialConditions | ( | ) |
Generates the initial condition for the Standard Model parameters.
This method sets all the Standard Model parameters to their values and RG evolves them up to the New Physics scale.
Definition at line 8355 of file NPSMEFTd6General.cpp.
|
inline |
|
inline |
|
inlinevirtual |
A method to get the Matching object for this model.
Reimplemented from StandardModel.
Definition at line 678 of file NPSMEFTd6General.h.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47460 of file NPSMEFTd6General.cpp.
|
virtual |
< To change C/Lambda^2 from GeV to TeV
Definition at line 47482 of file NPSMEFTd6General.cpp.
|
virtual |
A method to initialize the model parameters.
| [in] | DPars | a map of the parameters that are being updated in the Monte Carlo run (including parameters that are varied and those that are held constant) |
Reimplemented from StandardModel.
Definition at line 2998 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46687 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46775 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46757 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46806 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46766 of file NPSMEFTd6General.cpp.
|
virtual |
Definition at line 46722 of file NPSMEFTd6General.cpp.
|
virtual |
The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\).
Reimplemented from NPbase.
Definition at line 43047 of file NPSMEFTd6General.cpp.
|
virtual |
The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\).
Reimplemented from NPbase.
Definition at line 43023 of file NPSMEFTd6General.cpp.
|
virtual |
The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\).
Reimplemented from NPbase.
Definition at line 43015 of file NPSMEFTd6General.cpp.
|
virtual |
The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\).
Reimplemented from NPbase.
Definition at line 43027 of file NPSMEFTd6General.cpp.
|
virtual |
The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\).
Reimplemented from NPbase.
Definition at line 43007 of file NPSMEFTd6General.cpp.
|
virtual |
The effective coupling \(\kappa_{s,eff}=\sqrt{\Gamma_{Hss}/\Gamma_{Hss}^{SM}}\).
Definition at line 43019 of file NPSMEFTd6General.cpp.
|
virtual |
The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\).
Reimplemented from NPbase.
Definition at line 43011 of file NPSMEFTd6General.cpp.
|
virtual |
The effective coupling \(\kappa_{W4f,eff}=\sqrt{\Gamma_{H4f, CC}/\Gamma_{H4f, CC}^{SM}}\).
Reimplemented from NPbase.
Definition at line 43043 of file NPSMEFTd6General.cpp.
|
virtual |
The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\).
Reimplemented from NPbase.
Definition at line 43035 of file NPSMEFTd6General.cpp.
|
virtual |
The effective coupling \(\kappa_{Z4f,eff}=\sqrt{\Gamma_{H4f, NC}/\Gamma_{H4f, NC}^{SM}}\).
Reimplemented from NPbase.
Definition at line 43039 of file NPSMEFTd6General.cpp.
|
virtual |
The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\).
Reimplemented from NPbase.
Definition at line 43051 of file NPSMEFTd6General.cpp.
|
virtual |
The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\).
Reimplemented from NPbase.
Definition at line 43031 of file NPSMEFTd6General.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\).
Reimplemented from NPbase.
Definition at line 36501 of file NPSMEFTd6General.cpp.
|
virtual |
The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 43207 of file NPSMEFTd6General.cpp.
|
inlinevirtual |
The ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 2154 of file NPSMEFTd6General.h.
|
virtual |
The ratio \(\mu_{e^+e^- \to He^+e^-}\) between the \( e^+e^- \to H e^+e^- \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 22017 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 20632 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 25093 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 20406 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 38768 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 21511 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 23130 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 23556 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Definition at line 23903 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 23856 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Definition at line 24809 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 23877 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Definition at line 24828 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22744 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22867 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18011 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35841 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35601 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].)
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 20283 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35781 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 25080 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35811 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35721 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35751 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35631 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35661 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35691 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 25451 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H\mu\mu}\) between the \(\sigma(\mu \mu \to H \mu \mu)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 25661 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model, in the narrow width approximation.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 25468 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H\nu\nu}\) between the \(\sigma(\mu \mu \to H \nu \nu)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 25571 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu ttH}\) between the \(\sigma(\mu \mu \to t\bar{t} H )}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 25750 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu ZH}\) between the \(\sigma(\mu \mu \to Z H)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 25487 of file NPSMEFTd6General.cpp.
|
virtual |
The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6General class.
Reimplemented from NPbase.
Definition at line 39263 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 20217 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 24988 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36333 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35877 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36219 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36276 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36105 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36162 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35934 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,Z\gamma\to \gamma 2\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\to \gamma 2\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36436 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35991 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36048 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ\to 4\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36428 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36382 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35926 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36268 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36325 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36154 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36211 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35983 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36040 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36097 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF}\) between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36390 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36341 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35885 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,inv}\) between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36394 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36227 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36284 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36113 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36170 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35942 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35999 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36056 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36365 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH}\) between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36402 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35909 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,inv}\) between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36413 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36251 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36308 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36137 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36194 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35966 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36023 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36080 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36357 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35901 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36243 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36300 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36129 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36186 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35958 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36015 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36072 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36349 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35893 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36235 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36292 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36121 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36178 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35950 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36007 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 36064 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 20053 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35866 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35626 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H\to b\bar{b}\), \(Z\to e^+e^-\) channel channel in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35429 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35806 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35836 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35746 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35776 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35260 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35656 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35686 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35716 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18478 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 20361 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35846 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35606 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35786 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35816 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35726 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35756 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35636 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35666 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35696 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 24974 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 20263 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35861 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35621 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35801 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 24961 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35831 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35741 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35771 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35651 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35681 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35711 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18763 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35856 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35616 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35796 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23035 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35826 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35736 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35766 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35646 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35676 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35706 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 19200 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35851 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35611 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35791 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23079 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35821 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35731 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35761 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35641 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35671 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 35701 of file NPSMEFTd6General.cpp.
|
virtual |
The mass of the \(W\) boson, \(M_W\).
Reimplemented from NPbase.
Definition at line 15570 of file NPSMEFTd6General.cpp.
|
virtual |
The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).)
Reimplemented from NPbase.
Reimplemented in NPd6SILH.
Definition at line 15427 of file NPSMEFTd6General.cpp.
|
virtual |
The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).)
Reimplemented from NPbase.
Reimplemented in NPd6SILH.
Definition at line 15431 of file NPSMEFTd6General.cpp.
|
virtual |
The oblique parameter \(U\).
Reimplemented from NPbase.
Definition at line 15435 of file NPSMEFTd6General.cpp.
|
virtual |
The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).)
Reimplemented from NPbase.
Reimplemented in NPd6SILH.
Definition at line 15439 of file NPSMEFTd6General.cpp.
|
virtual |
The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).)
Reimplemented from NPbase.
Reimplemented in NPd6SILH.
Definition at line 15443 of file NPSMEFTd6General.cpp.
|
virtual |
The post-update method for NPSMEFTd6General.
This method runs all the procedures that are need to be executed after the model is successfully updated.
Reimplemented from StandardModel.
Reimplemented in NPd6SILH, NPSMEFTd6MFV, NPSMEFTd6U2, NPSMEFTd6U2qU1le, and NPSMEFTd6U3.
Definition at line 8450 of file NPSMEFTd6General.cpp.
|
virtual |
The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6General class.
Reimplemented from NPbase.
Definition at line 39228 of file NPSMEFTd6General.cpp.
|
virtual |
The pre-update method for NPSMEFTd6General.
This method runs all the procedures that are need to be executed before the model is successfully updated.
Reimplemented from StandardModel.
Definition at line 3008 of file NPSMEFTd6General.cpp.
|
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.
\[ R^0_f = R_f^{SM} + \Delta R_f^{(1)} + \Delta R_f^{(2)} \]
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 16982 of file NPSMEFTd6General.cpp.
|
virtual |
The ratio \(R_{W,c)=\Gamma(W\to c + X)/\Gamma(W\to had)\).
Reimplemented from NPbase.
Definition at line 16165 of file NPSMEFTd6General.cpp.
The lepton universality ratio \(R_{W,l_i/l_j)=\Gamma(W\to l_i \nu_i)/\Gamma(W\to l_j \nu_j)\).
Reimplemented from NPbase.
Definition at line 16132 of file NPSMEFTd6General.cpp.
The lepton universality ratio \(R_{Z,l_i/l_j)=\Gamma(Z\to l_i^+ l_i^-)/\Gamma(Z\to l_j^+ l_j^-)\).
Reimplemented from NPbase.
Definition at line 16194 of file NPSMEFTd6General.cpp.
|
virtual |
A method to check if all the mandatory parameters for NPSMEFTd6General have been provided in model initialization.
| [in] | DPars | a map of the parameters that are being updated in the Monte Carlo run (including parameters that are varied and those that are held constant) |
A method to set a flag of NPSMEFTd6General.
| [in] | name | name of a model flag |
| [in] | value | the boolean to be assigned to the flag specified by name |
Reimplemented from NPbase.
Reimplemented in NPd6SILH.
Definition at line 14082 of file NPSMEFTd6General.cpp.
|
virtual |
A method to set a flag of NPSMEFTd6General.
| [in] | name | name of a model flag |
| [in] | value | the value to be assigned to the flag specified by name |
Reimplemented from StandardModel.
Definition at line 14162 of file NPSMEFTd6General.cpp.
|
virtual |
The cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\sigma_h^0\).
\[ \sigma_h = \sigma_h^{SM} + \Delta \sigma_h^{(1)} + \Delta \sigma_h^{(2)} \]
Reimplemented from NPbase.
Definition at line 16315 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS0 bin \(pp \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39380 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS BR \( H \to 4l \), \(l=e,\mu\).
Reimplemented from NPbase.
Definition at line 39999 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS BR \( H \to bb \).
Reimplemented from NPbase.
Definition at line 40071 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS BR \( H \to e\nu \mu\nu \).
Reimplemented from NPbase.
Definition at line 40023 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS BR \( H \to \gamma \gamma \).
Reimplemented from NPbase.
Definition at line 40046 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 1,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40471 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40620 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~120<p_{TH} [GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40697 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~60<p_{TH} [GeV]<120\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40658 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~<p_{TH} [GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40852 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40735 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40763 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40885 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40793 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40824 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j=0,~p_{TH} [GeV]<10\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40196 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j = 1,~p_{TH} [GeV]<60\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40505 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j=0,~p_{TH} [GeV]<10\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40236 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j=0,~10<p_{TH} [GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40443 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j = 1,~120<p_{TH} [GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40582 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(,200<~p_{TH} [GeV]<300\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40272 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j\leq 1,~200<p_{TH} [GeV]<300\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40095 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(,300<~p_{TH} [GeV]<450\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40306 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j\leq 1,~300<p_{TH} [GeV]<450\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40120 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(450<~p_{TH} [GeV]<650\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40374 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j\leq 1,~450<p_{TH} [GeV]<650\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40145 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(,450<~p_{TH} [GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40340 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j = 1,~60<p_{TH} [GeV]<120\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40544 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(~p_{TH} [GeV]>650\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40408 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j\leq 1,650<p_{TH} [GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40169 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\ell\ell\), \(p_{TV}[GeV]<75\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40918 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40988 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\ell\ell\), \(N_j = 1,~150<p_{TV}[GeV]<250\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41022 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\ell\ell\), \(250 < p_{TV}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41056 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\ell\ell\), \(75<p_{TV}[GeV]<150\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 40953 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\ell\), \(0<p_{TV}<150[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42315 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\ell\), \(p_{TV}[GeV]<75\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42025 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42144 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\ell\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42204 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}<400[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42360 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42263 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\ell\), \(400<p_{TV}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42405 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\ell\), \(75<p_{TV}[GeV]<150\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42085 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\nu\), \(0<p_{TV}<150[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41932 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\nu\), \(p_{TV}[GeV]<75\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41749 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\nu\), \(N_j = 0,~150<p_{TV}[GeV]<250\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41829 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\nu\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41869 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}<400[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41964 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41909 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\nu\), \(400<p_{TV}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41994 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\nu\), \(75<p_{TV}[GeV]<150\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41789 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~m_{jj}[GeV]<60\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41186 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1000<m_{jj}[GeV]<1500,~p_{TH}[GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41589 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1000<m_{jj}[GeV],~p_{TH}[GeV]>200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41709 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~120<m_{jj}[GeV]<350\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41266 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1500<m_{jj}[GeV],~p_{TH}[GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41629 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<1000,~p_{TH}[GeV]>200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41669 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41509 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41360 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41398 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV],~200<p_{TH}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41301 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~60<m_{jj}[GeV]<120\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41224 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV]<1000,~p_{TH}[GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41549 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41435 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41472 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j = 0\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41123 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j = 1\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41155 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j = 0,1\) VH-veto Ref. 2402.05742.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 41091 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(pp \to tH\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42976 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(pp \to ttH\), \(p_{TH}[GeV]<60\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42451 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(pp \to ttH\), \(120<p_{TH}[GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42625 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(pp \to ttH\), \(200<p_{TH}[GeV]<300\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42713 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]<450\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42843 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42802 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(pp \to ttH\), \(450<p_{TH}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42913 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(pp \to ttH\), \(60<p_{TH}[GeV]<120\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 42539 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39463 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39477 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39505 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39519 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39491 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39533 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39544 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39566 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39577 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39555 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39452 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39441 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39757 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39780 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39799 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39812 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39825 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39705 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39689 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39716 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39727 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39738 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39618 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39669 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39658 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39607 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39596 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39591 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39638 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \( ttH + tH \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39848 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39922 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39911 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39889 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39878 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39900 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39981 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39969 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39945 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39933 of file NPSMEFTd6General.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 39957 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::tovers2 | ( | const double | cosmin, |
| const double | cosmax | ||
| ) | const |
Definition at line 46467 of file NPSMEFTd6General.cpp.
| const double NPSMEFTd6General::uovers2 | ( | const double | cosmin, |
| const double | cosmax | ||
| ) | const |
Definition at line 46471 of file NPSMEFTd6General.cpp.
|
virtual |
Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\).
Reimplemented from NPbase.
Definition at line 38764 of file NPSMEFTd6General.cpp.
|
virtual |
The cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented from NPbase.
Definition at line 37099 of file NPSMEFTd6General.cpp.
|
virtual |
The total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented from NPbase.
Definition at line 37642 of file NPSMEFTd6General.cpp.
|
static |
The number of the model parameters in NPSMEFTd6General (including the 18 parameters needed for the SM and 79 auxiliary parameters).
Definition at line 600 of file NPSMEFTd6General.h.
|
static |
A string array containing the labels of the model parameters in NPSMEFTd6General.
Definition at line 607 of file NPSMEFTd6General.h.
1.9.2 