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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The auxiliary base model class for other model classes. More...
#include <NPbase.h>
Inheritance diagram for NPbase:The auxiliary base model class for other model classes.
This is an auxiliary Model class containing the basic structure to compute new physics (NP) contributions to the electroweak precision observables. The NP contributions are described by the following quantities:
Using these quantities, the mass and width of the \(W\) boson and the NP contributions to the effective vector and axial-vector couplings of the \(Z\)-boson to leptons and quarks are computed:
In the model classes that are inherited from the current class (see the inheritance diagram above), some of these methods are reimplemented to account for the details of more specific scenarios.
This class is intended to be used with an inherited model class.
There is no model parameter in the current class.
There is no model flag in the current class.
The functions are explained above.
Public Member Functions | |
| virtual const double | A_f (const Particle f) const |
| The left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\mathcal{A}_f\). More... | |
| virtual const double | AFB (const Particle f) const |
| The forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(A^f_{FB}\). More... | |
| virtual const double | alphaMz () const |
| The electromagnetic coupling at the \(Z\)-mass scale, \(\alpha(M_Z^2)=\alpha/(1-\Delta\alpha(M_Z^2))\). More... | |
| virtual const double | alrmoller (const double q2, const double y) const |
| virtual const double | amuon () const |
| 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 | AuxObs_NP1 () const |
| Auxiliary observable AuxObs_NP1. More... | |
| virtual const double | AuxObs_NP10 () const |
| Auxiliary observable AuxObs_NP10. More... | |
| virtual const double | AuxObs_NP11 () const |
| Auxiliary observable AuxObs_NP11. More... | |
| virtual const double | AuxObs_NP12 () const |
| Auxiliary observable AuxObs_NP12. More... | |
| virtual const double | AuxObs_NP13 () const |
| Auxiliary observable AuxObs_NP13. More... | |
| virtual const double | AuxObs_NP14 () const |
| Auxiliary observable AuxObs_NP14. More... | |
| virtual const double | AuxObs_NP15 () const |
| Auxiliary observable AuxObs_NP15. More... | |
| virtual const double | AuxObs_NP16 () const |
| Auxiliary observable AuxObs_NP16. More... | |
| virtual const double | AuxObs_NP17 () const |
| Auxiliary observable AuxObs_NP17. More... | |
| virtual const double | AuxObs_NP18 () const |
| Auxiliary observable AuxObs_NP18. More... | |
| virtual const double | AuxObs_NP19 () const |
| Auxiliary observable AuxObs_NP19. More... | |
| virtual const double | AuxObs_NP2 () const |
| Auxiliary observable AuxObs_NP2. More... | |
| virtual const double | AuxObs_NP20 () const |
| Auxiliary observable AuxObs_NP20. More... | |
| virtual const double | AuxObs_NP21 () const |
| Auxiliary observable AuxObs_NP21. More... | |
| virtual const double | AuxObs_NP22 () const |
| Auxiliary observable AuxObs_NP22. More... | |
| virtual const double | AuxObs_NP23 () const |
| Auxiliary observable AuxObs_NP23. More... | |
| virtual const double | AuxObs_NP24 () const |
| Auxiliary observable AuxObs_NP24. More... | |
| virtual const double | AuxObs_NP25 () const |
| Auxiliary observable AuxObs_NP25. More... | |
| virtual const double | AuxObs_NP26 () const |
| Auxiliary observable AuxObs_NP26. More... | |
| virtual const double | AuxObs_NP27 () const |
| Auxiliary observable AuxObs_NP27. More... | |
| virtual const double | AuxObs_NP28 () const |
| Auxiliary observable AuxObs_NP28. More... | |
| virtual const double | AuxObs_NP29 () const |
| Auxiliary observable AuxObs_NP29. More... | |
| virtual const double | AuxObs_NP3 () const |
| Auxiliary observable AuxObs_NP3. More... | |
| virtual const double | AuxObs_NP30 () const |
| Auxiliary observable AuxObs_NP30. More... | |
| virtual const double | AuxObs_NP4 () const |
| Auxiliary observable AuxObs_NP4. More... | |
| virtual const double | AuxObs_NP5 () const |
| Auxiliary observable AuxObs_NP5. More... | |
| virtual const double | AuxObs_NP6 () const |
| Auxiliary observable AuxObs_NP6. More... | |
| virtual const double | AuxObs_NP7 () const |
| Auxiliary observable AuxObs_NP7. More... | |
| virtual const double | AuxObs_NP8 () const |
| Auxiliary observable AuxObs_NP8. More... | |
| virtual const double | AuxObs_NP9 () const |
| Auxiliary observable AuxObs_NP9. More... | |
| virtual const double | bPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More... | |
| virtual const double | Br_H_exo () const |
| The branching ratio of the of the Higgs into exotic particles. More... | |
| virtual const double | Br_H_inv () const |
| The branching ratio of the of the Higgs into invisible particles. More... | |
| virtual const double | Br_H_inv_NP () const |
| The branching ratio of the of the Higgs into invisible particles (only invisible new particles). More... | |
| virtual const double | BR_Zf (const Particle f) const |
| The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\). More... | |
| virtual const double | BrH2d2dRatio () const |
| The ratio of the Br \((H\to 2d2d)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2e2muRatio () const |
| The ratio of the Br \((H\to 2e 2\mu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2e2vRatio () const |
| The ratio of the Br \((H\to 2e2v)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2evRatio () const |
| The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2L2dRatio () const |
| The ratio of the Br \((H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2L2LRatio () const |
| The ratio of the Br \((H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2L2uRatio () const |
| The ratio of the Br \((H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2L2v2Ratio () const |
| The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2L2vRatio () const |
| The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2l2vRatio () const |
| The ratio of the Br \((H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2Lv2Ratio () const |
| The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2LvRatio () const |
| The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2mu2vRatio () const |
| The ratio of the Br \((H\to 2\mu 2v)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2muvRatio () const |
| The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2u2dRatio () const |
| The ratio of the Br \((H\to 2u2d)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2u2uRatio () const |
| The ratio of the Br \((H\to 2u2u)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2udRatio () const |
| The ratio of the Br \((H\to 2ud)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2v2dRatio () const |
| The ratio of the Br \((H\to 2v2d)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2v2uRatio () const |
| The ratio of the Br \((H\to 2v2u)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2v2vRatio () const |
| The ratio of the Br \((H\to 2v2v)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4dRatio () const |
| The ratio of the Br \((H\to 4d)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4eRatio () const |
| The ratio of the Br \((H\to 4e)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4fRatio () const |
| The ratio of the Br \((H\to 4f)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4L2Ratio () const |
| The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4LRatio () const |
| The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4lRatio () const |
| The ratio of the Br \((H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4muRatio () const |
| The ratio of the Br \((H\to 4\mu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4uRatio () const |
| The ratio of the Br \((H\to 4u)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4vRatio () const |
| The ratio of the Br \((H\to 4v)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHbbRatio () const |
| The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHccRatio () const |
| The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHevmuvRatio () const |
| The ratio of the Br \((H\to e\nu \mu\nu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHgagaRatio () const |
| The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHggRatio () const |
| The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHll_vvorjjRatio () const |
| The ratio of the Br \((H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHlljjRatio () const |
| The ratio of the Br \((H\to l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHlv_lvorjjRatio () const |
| The ratio of the Br \((H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHlvjjRatio () const |
| The ratio of the Br \((H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHLvudRatio () const |
| The ratio of the Br \((H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHLvvLRatio () const |
| The ratio of the Br \((H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHmumuRatio () const |
| The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHssRatio () const |
| The ratio of the Br \((H\to s\bar{s})\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHtautauRatio () const |
| The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHtoinvRatio () const |
| The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHudduRatio () const |
| The ratio of the Br \((H\to uddu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHvisRatio () const |
| The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHVVRatio () const |
| The ratio of the Br \((H\to VV)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHWWRatio () const |
| The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZgaeeRatio () const |
| The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZgallRatio () const |
| The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZgamumuRatio () const |
| The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZgaRatio () const |
| The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZZRatio () const |
| The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrW (const Particle fi, const Particle fj) const |
| The branching ratio of the \(W\) boson decaying into a SM fermion pair, \(Br(W\to f_i f_j)\). More... | |
| virtual const double | C1eeHvv (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| virtual const double | C1eettH (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| virtual const double | C1eeWBF (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| virtual const double | C1eeZBF (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| virtual const double | C1eeZH (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| const double | C1Htot () const |
| The C1 coefficient controlling the H^3 corrections to the total Higgs width from the Higgs trilinear coupling. More... | |
| virtual const double | cbminuscc () const |
| virtual const double | cbminusctau () const |
| virtual const double | cbW_TWG (const double mu) const |
| virtual const double | ccminusctau () const |
| virtual const double | CEWHd11 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{11}\). More... | |
| virtual const double | CEWHd22 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{22}\). More... | |
| virtual const double | CEWHd33 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{33}\). More... | |
| virtual const double | CEWHe11 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{11}\). More... | |
| virtual const double | CEWHe22 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{22}\). More... | |
| virtual const double | CEWHe33 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{33}\). More... | |
| virtual const double | CEWHL111 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{11}\). More... | |
| virtual const double | CEWHL122 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{22}\). More... | |
| virtual const double | CEWHL133 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{33}\). More... | |
| virtual const double | CEWHL311 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{11}\). More... | |
| virtual const double | CEWHL322 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{22}\). More... | |
| virtual const double | CEWHL333 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{33}\). More... | |
| virtual const double | CEWHQ111 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{11}\). More... | |
| virtual const double | CEWHQ122 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{22}\). More... | |
| virtual const double | CEWHQ133 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{33}\). More... | |
| virtual const double | CEWHQ311 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{11}\). More... | |
| virtual const double | CEWHQ322 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{22}\). More... | |
| virtual const double | CEWHQ333 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{33}\). More... | |
| virtual const double | CEWHQd33 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(d)})_{33}\). More... | |
| virtual const double | CEWHu11 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{11}\). More... | |
| virtual const double | CEWHu22 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{22}\). More... | |
| virtual const double | CEWHu33 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{33}\). More... | |
| virtual const double | cgaga_HB (const double mu) const |
| The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | cgaplusct () const |
| virtual const double | cgg_HB (const double mu) const |
| The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | cggEff_HB (const double mu) const |
| The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) More... | |
| virtual const double | cgminuscga () const |
| virtual const double | cgplusct () const |
| virtual const double | 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 | cVpluscb () const |
| virtual const double | cVplusctau () const |
| virtual const double | cZBox_HB (const double mu) const |
| The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | cZga_HB (const double mu) const |
| The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | cZZ_HB (const double mu) const |
| The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | 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 |
| virtual const double | delta_mubbH_2 (const double sqrt_s) const |
| virtual const double | delta_muggH_1 (const double sqrt_s) const |
| virtual const double | delta_muggH_2 (const double sqrt_s) const |
| virtual const double | delta_mutH_1 (const double sqrt_s) const |
| virtual const double | delta_mutH_2 (const double sqrt_s) const |
| virtual const double | delta_muttH_1 (const double sqrt_s) const |
| virtual const double | delta_muttH_2 (const double sqrt_s) const |
| virtual const double | delta_muVBF_1 (const double sqrt_s) const |
| virtual const double | delta_muVBF_2 (const double sqrt_s) const |
| virtual const double | delta_muVH_1 (const double sqrt_s) const |
| virtual const double | delta_muVH_2 (const double sqrt_s) const |
| virtual const double | delta_muWH_1 (const double sqrt_s) const |
| virtual const double | delta_muWH_2 (const double sqrt_s) const |
| virtual const double | delta_muZH_1 (const double sqrt_s) const |
| virtual const double | delta_muZH_2 (const double sqrt_s) const |
| virtual const double | 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 | deltaA_f (const Particle f) const |
| The new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta \mathcal{A}_f\). More... | |
| virtual const double | deltaA_f_2 (const Particle f) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\Delta \mathcal{A}_f^{(2)}\). More... | |
| virtual const double | deltaAFB (const Particle f) const |
| The new physics contribution to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta A^f_{FB}\). More... | |
| virtual const double | deltaAFB_2 (const Particle f) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\Delta A^f_{FB}\). More... | |
| virtual const double | deltacZ_HB (const double mu) const |
| The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | deltadxsdcoseeWWlvjjLEP2 (const double sqrt_s, const int bin) const |
| The new physics contribution to the differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph]. More... | |
| virtual const double | deltaeNP (const double mu) const |
| The new physics relative contribution to the EW coupling constant \(e\). More... | |
| virtual const double | deltaG1_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More... | |
| virtual const double | deltaG1_hWW_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More... | |
| virtual const double | deltaG1_hZA () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual const double | deltaG1_hZA_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual const double | deltaG1_hZARatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual const double | deltaG1_hZARatio_mu (const double mu) const |
| The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual const double | deltaG1_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More... | |
| virtual const double | deltaG1_hZZ_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More... | |
| virtual const double | deltag1gaNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More... | |
| virtual const double | deltag1ZNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More... | |
| virtual const double | deltag1ZNPEff () const |
| The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More... | |
| virtual const double | deltaG2_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More... | |
| virtual const double | deltaG2_hWW_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More... | |
| virtual const double | deltaG2_hZA () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More... | |
| virtual const double | deltaG2_hZA_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More... | |
| virtual const double | deltaG2_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More... | |
| virtual const double | deltaG2_hZZ_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More... | |
| virtual const double | deltaG3_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More... | |
| virtual const double | deltaG3_hWW_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More... | |
| virtual const double | deltaG3_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More... | |
| virtual const double | deltaG3_hZZ_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More... | |
| virtual const double | deltaG_hAA () const |
| The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual const double | deltaG_hAA_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual const double | deltaG_hAARatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual const double | deltaG_hAARatio_mu (const double mu) const |
| The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual gslpp::complex | deltaG_hff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More... | |
| virtual gslpp::complex | deltaG_hff_mu (const Particle p, const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More... | |
| virtual const double | deltaG_hgg () const |
| The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More... | |
| virtual const double | deltaG_hgg_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More... | |
| virtual const double | deltaG_hggRatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual const double | deltaG_hggRatio_mu (const double mu) const |
| The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual const double | deltaG_hhhRatio () const |
| The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More... | |
| virtual const double | deltaG_hhhRatio_mu (const double mu) const |
| The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More... | |
| virtual const double | deltaGA_f (const Particle f) const |
| New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| virtual const double | deltaGA_f_2 (const Particle f) const |
| virtual const double | deltaGamma_W () const |
| The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\). More... | |
| virtual const double | deltaGamma_Wff (const Particle fi, const Particle fj) const |
| The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More... | |
| virtual const double | deltaGamma_Z () const |
| The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\). More... | |
| virtual const double | deltaGamma_Z_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the total decay width of the \(Z\) boson, \(\Delta \Gamma_Z^{(2)}\). More... | |
| virtual const double | deltaGamma_Zf (const Particle f) const |
| The new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More... | |
| virtual const double | deltaGamma_Zf_2 (const Particle f) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\Delta \Gamma_{Z,f}^{(2)}\). More... | |
| virtual const double | deltaGamma_Zhad () const |
| The new physics contribution to the hadronic decay width of the \(Z\) boson, \(\delta \Gamma_{Z,had}\). More... | |
| virtual const double | deltaGamma_Zhad_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the hadronic decay width of the \(Z\) boson, \(\Delta \Gamma_{Z,had}^{(2)}\). More... | |
| virtual const double | deltaGammaHbbRatio1 () const |
| virtual const double | deltaGammaHbbRatio2 () const |
| virtual const double | deltaGammaHccRatio1 () const |
| virtual const double | deltaGammaHccRatio2 () const |
| virtual const double | deltaGammaHgagaRatio1 () const |
| virtual const double | deltaGammaHgagaRatio2 () const |
| virtual const double | deltaGammaHggRatio1 () const |
| virtual const double | deltaGammaHggRatio2 () const |
| virtual const double | deltaGammaHmumuRatio1 () const |
| virtual const double | deltaGammaHmumuRatio2 () const |
| virtual const double | deltaGammaHtautauRatio1 () const |
| virtual const double | deltaGammaHtautauRatio2 () const |
| virtual const double | deltaGammaHWWRatio1 () const |
| virtual const double | deltaGammaHWWRatio2 () const |
| virtual const double | deltaGammaHZgaRatio1 () const |
| virtual const double | deltaGammaHZgaRatio2 () const |
| virtual const double | deltaGammaHZZRatio1 () const |
| virtual const double | deltaGammaHZZRatio2 () const |
| virtual const double | deltaGammaTotalRatio1 () const |
| virtual const double | deltaGammaTotalRatio2 () const |
| virtual const double | DeltaGF () const |
| New physics contribution to the Fermi constant. More... | |
| const double | deltaGL_f_mu (const Particle p, const double mu) const |
| New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More... | |
| virtual gslpp::complex | deltaGL_Wff (const Particle pbar, const Particle p) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| virtual gslpp::complex | deltaGL_Wff_mu (const Particle pbar, const Particle p, const double mu) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| const double | deltaGR_f_mu (const Particle p, const double mu) const |
| New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More... | |
| virtual gslpp::complex | deltaGR_Wff (const Particle pbar, const Particle p) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| virtual gslpp::complex | deltaGR_Wff_mu (const Particle pbar, const Particle p, const double mu) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| virtual const double | deltaGV_f (const Particle f) const |
| New physics contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual const double | deltaGV_f_2 (const Particle f) const |
| virtual const double | deltaKgammaNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\). More... | |
| virtual const double | deltaKgammaNPEff () const |
| The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More... | |
| virtual const double | deltaN_nu () const |
| The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements. More... | |
| virtual const double | deltaR0_f (const Particle f) const |
| The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More... | |
| virtual const double | deltaR0_f_2 (const Particle f) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos: More... | |
| virtual const double | deltaR_inv () const |
| The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the \(Z\) boson, \(\delta R_{inv}\). More... | |
| virtual const double | deltaRuc () const |
| The new physics contribution to the ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width: More... | |
| virtual const double | deltaRuc_2 () const |
| The \(\mathcal{O}(1/\Lambda^4)\) new physics contribution to the ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width: More... | |
| virtual const double | deltaSigmaHadron () const |
| The new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\delta \sigma_h^0\). More... | |
| virtual const double | deltaSigmaHadron_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\Delta \sigma_h^{0,(2)}\). More... | |
| virtual const double | deltaSin2thetaEff_e () const |
| The new physics contribution to the effective electron/leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. More... | |
| virtual const double | deltaSin2thetaEff_e_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the effective electron weak angle \(\Delta \sin^2\theta_{eff,e}^{(2)}\) at the \(Z\) pole. More... | |
| virtual const double | deltaSin2thetaEff_mu () const |
| The new physics contribution to the effective muonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\mu\mu}\) at the \(Z\) pole. More... | |
| virtual const double | deltaSin2thetaEff_mu_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the effective muonic weak angle \(\Delta \sin^2\theta_{eff, \mu}^{(2)}\) at the \(Z\) pole. More... | |
| virtual const double | deltaxseeWW4fLEP2 (const double sqrt_s, const int fstate) const |
| The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More... | |
| virtual const double | deltaxseeWWhadLEP2 (const double sqrt_s) const |
| The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to j j j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | deltaxseeWWleptLEP2 (const double sqrt_s) const |
| The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | deltaxseeWWsemilLEP2 (const double sqrt_s) const |
| The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | deltaxseeWWtotLEP2 (const double sqrt_s) const |
| The new physics contribution to the total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More... | |
| virtual const double | deltayb_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | deltayc_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | deltaymu_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | deltays_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_s\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | deltayt_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | deltaytau_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | dxsdcoseeWWlvjjLEP2 (const double sqrt_s, const int bin) const |
| The differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | dxseeWWdcos (const double sqrt_s, const double cos) const |
| The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle. More... | |
| virtual const double | dxseeWWdcosBin (const double sqrt_s, const double cos1, const double cos2) const |
| The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle. More... | |
| virtual const 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 | 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 |
| 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 gslpp::complex | gA_f (const Particle f) const |
| The total (SM+NP) contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| virtual const double | Gamma_had () const |
| The hadronic decay width of the \(Z\) boson, \(\Gamma_{Z,had}\). More... | |
| virtual const double | Gamma_Z () const |
| The total decay width of the \(Z\) boson, \(\Gamma_Z\). More... | |
| virtual const double | Gamma_Zf (const Particle f) const |
| The decay width of the \(Z\) boson into a given fermion pair, \(\Gamma_Z^{f}\). More... | |
| virtual const double | GammaHbbRatio () const |
| The ratio of the \(\Gamma(H\to b\bar{b})\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHccRatio () const |
| The ratio of the \(\Gamma(H\to c\bar{c})\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHgagaRatio () const |
| The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHggRatio () const |
| The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHmumuRatio () const |
| The ratio of the \(\Gamma(H\to \mu^+\mu^-)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHssRatio () const |
| The ratio of the \(\Gamma(H\to s\bar{s})\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHtautauRatio () const |
| The ratio of the \(\Gamma(H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHWWRatio () const |
| The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHZgaRatio () const |
| The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHZZRatio () const |
| The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaW () const |
| The total width of the \(W\) boson, \(\Gamma_W\). More... | |
| virtual const double | GammaW (const Particle fi, const Particle fj) const |
| A partial decay width of the \(W\) boson decay into a SM fermion pair. More... | |
| virtual const double | gAnue () const |
| virtual const StandardModel & | getTrueSM () const |
| A method to return a StandardModel object from NPbase. More... | |
| virtual const double | gLnuN2 () const |
| virtual const double | gRnuN2 () const |
| virtual const gslpp::complex | gV_f (const Particle f) const |
| The total (SM+NP) contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual const double | gVnue () const |
| virtual const double | IctW_TWG (const double mu) const |
| virtual const double | IctZ_TWG (const double mu) 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 | kappataueff () const |
| The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\). More... | |
| virtual const double | kappaW4feff () const |
| The effective coupling \(\kappa_{W4f,eff}=\sqrt{\Gamma_{H4f, CC}/\Gamma_{H4f, CC}^{SM}}\). More... | |
| virtual const double | kappaWeff () const |
| The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\). More... | |
| virtual const double | kappaZ4feff () const |
| The effective coupling \(\kappa_{Z4f,eff}=\sqrt{\Gamma_{H4f, NC}/\Gamma_{H4f, NC}^{SM}}\). More... | |
| virtual const gslpp::complex | kappaZ_f (const Particle f) const |
| The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions. More... | |
| virtual const double | kappaZAeff () const |
| The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\). More... | |
| virtual const double | kappaZeff () const |
| The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\). More... | |
| virtual const double | lambdaZNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\). More... | |
| virtual const double | lambz_HB (const double mu) const |
| The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | 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 |
| virtual const double | mubbH (const double sqrt_s) const |
| The ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeHee (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{e^+e^- \to He^+e^-}\) between the \( e^+e^- \to H e^+e^- \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeHvv (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueettH (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeWBF (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeWW (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZBF (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZH (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZHGen (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZllH (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZqqH (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muepWBF (const double sqrt_s) const |
| The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muepZBF (const double sqrt_s) const |
| The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muggH (const double sqrt_s) const |
| The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muggHbb (const double sqrt_s) const |
| virtual const double | muggHgaga (const double sqrt_s) const |
| virtual const double | muggHgagaInt (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259. More... | |
| virtual const double | muggHH (const double sqrt_s) const |
| The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muggHmumu (const double sqrt_s) const |
| virtual const double | muggHpbbH_Hgaga (const double sqrt_s) const |
| virtual const double | muggHpbbH_Htautau (const double sqrt_s) const |
| virtual const double | muggHpbbH_HWW (const double sqrt_s) const |
| virtual const double | muggHpbbH_HZZ (const double sqrt_s) const |
| virtual const double | muggHpttH (const double sqrt_s) const |
| The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muggHpttHptHpbbH_Hmumu (const double sqrt_s) const |
| virtual const double | muggHpttHptHpbbH_HZga (const double sqrt_s) const |
| virtual const double | muggHpVBFpbbH_Hbb (const double sqrt_s) const |
| virtual const double | muggHtautau (const double sqrt_s) const |
| virtual const double | muggHWW (const double sqrt_s) const |
| virtual const double | muggHWW2l2v (const double sqrt_s) const |
| virtual const double | muggHZga (const double sqrt_s) const |
| virtual const double | muggHZZ (const double sqrt_s) const |
| virtual const double | muggHZZ4l (const double sqrt_s) const |
| virtual const double | mummH (const double sqrt_s) const |
| The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mummHmm (const double sqrt_s) const |
| The ratio \(\mu_{\mu\mu H\mu\mu}\) between the \(\sigma(\mu \mu \to H \mu \mu)}\) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mummHNWA (const double sqrt_s) const |
| The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model, in the narrow width approximation. More... | |
| virtual const double | mummHvv (const double sqrt_s) const |
| The ratio \(\mu_{\mu\mu H\nu\nu}\) between the \(\sigma(\mu \mu \to H \nu \nu)}\) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mummttH (const double sqrt_s) const |
| The ratio \(\mu_{\mu\mu ttH}\) between the \(\sigma(\mu \mu \to t\bar{t} H )}\) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mummZH (const double sqrt_s) const |
| The ratio \(\mu_{\mu\mu ZH}\) between the \(\sigma(\mu \mu \to Z H)}\) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muppHmumu (const double sqrt_s) const |
| virtual const double | muppHZga (const double sqrt_s) const |
| virtual const double | mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const |
| The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class. More... | |
| virtual const double | mutH (const double sqrt_s) const |
| The ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mutHgaga (const double sqrt_s) const |
| virtual const double | mutHq (const double sqrt_s) const |
| The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHbb (const double sqrt_s) const |
| virtual const double | muTHUggHgaga (const double sqrt_s) const |
| virtual const double | muTHUggHmumu (const double sqrt_s) const |
| virtual const double | muTHUggHtautau (const double sqrt_s) const |
| virtual const double | muTHUggHWW (const double sqrt_s) const |
| virtual const double | muTHUggHWW2l2v (const double sqrt_s) const |
| virtual const double | muTHUggHZga (const double sqrt_s) const |
| virtual const double | muTHUggHZgamumu (const double sqrt_s) const |
| virtual const double | muTHUggHZZ (const double sqrt_s) const |
| virtual const double | muTHUggHZZ4l (const double sqrt_s) const |
| virtual const double | muTHUggHZZ4mu (const double sqrt_s) const |
| virtual const double | muTHUttHbb (const double sqrt_s) const |
| virtual const double | muTHUttHgaga (const double sqrt_s) const |
| virtual const double | muTHUttHmumu (const double sqrt_s) const |
| virtual const double | muTHUttHtautau (const double sqrt_s) const |
| virtual const double | muTHUttHWW (const double sqrt_s) const |
| virtual const double | muTHUttHWW2l2v (const double sqrt_s) const |
| virtual const double | muTHUttHZga (const double sqrt_s) const |
| virtual const double | muTHUttHZZ (const double sqrt_s) const |
| virtual const double | muTHUttHZZ4l (const double sqrt_s) const |
| virtual const double | muTHUVBFBRinv (const double sqrt_s) const |
| virtual const double | muTHUVBFHbb (const double sqrt_s) const |
| virtual const double | muTHUVBFHgaga (const double sqrt_s) const |
| virtual const double | muTHUVBFHinv (const double sqrt_s) const |
| virtual const double | muTHUVBFHmumu (const double sqrt_s) const |
| virtual const double | muTHUVBFHtautau (const double sqrt_s) const |
| virtual const double | muTHUVBFHWW (const double sqrt_s) const |
| virtual const double | muTHUVBFHWW2l2v (const double sqrt_s) const |
| virtual const double | muTHUVBFHZga (const double sqrt_s) const |
| virtual const double | muTHUVBFHZZ (const double sqrt_s) const |
| virtual const double | muTHUVBFHZZ4l (const double sqrt_s) const |
| virtual const double | muTHUVHbb (const double sqrt_s) const |
| virtual const double | muTHUVHBRinv (const double sqrt_s) const |
| virtual const double | muTHUVHgaga (const double sqrt_s) const |
| virtual const double | muTHUVHinv (const double sqrt_s) const |
| virtual const double | muTHUVHmumu (const double sqrt_s) const |
| virtual const double | muTHUVHtautau (const double sqrt_s) const |
| virtual const double | muTHUVHWW (const double sqrt_s) const |
| virtual const double | muTHUVHWW2l2v (const double sqrt_s) const |
| virtual const double | muTHUVHZga (const double sqrt_s) const |
| virtual const double | muTHUVHZZ (const double sqrt_s) const |
| virtual const double | muTHUVHZZ4l (const double sqrt_s) const |
| virtual const double | muTHUWHbb (const double sqrt_s) const |
| virtual const double | muTHUWHgaga (const double sqrt_s) const |
| virtual const double | muTHUWHmumu (const double sqrt_s) const |
| virtual const double | muTHUWHtautau (const double sqrt_s) const |
| virtual const double | muTHUWHWW (const double sqrt_s) const |
| virtual const double | muTHUWHWW2l2v (const double sqrt_s) const |
| virtual const double | muTHUWHZga (const double sqrt_s) const |
| virtual const double | muTHUWHZZ (const double sqrt_s) const |
| virtual const double | muTHUWHZZ4l (const double sqrt_s) const |
| virtual const double | muTHUZHbb (const double sqrt_s) const |
| virtual const double | muTHUZHgaga (const double sqrt_s) const |
| virtual const double | muTHUZHmumu (const double sqrt_s) const |
| virtual const double | muTHUZHtautau (const double sqrt_s) const |
| virtual const double | muTHUZHWW (const double sqrt_s) const |
| virtual const double | muTHUZHWW2l2v (const double sqrt_s) const |
| virtual const double | muTHUZHZga (const double sqrt_s) const |
| virtual const double | muTHUZHZZ (const double sqrt_s) const |
| virtual const double | muTHUZHZZ4l (const double sqrt_s) const |
| virtual const double | muttH (const double sqrt_s) const |
| The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muttHbb (const double sqrt_s) const |
| virtual const double | muttHgaga (const double sqrt_s) const |
| virtual const double | muttHgagaZeeboost (const double sqrt_s) const |
| The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H\to b\bar{b}\), \(Z\to e^+e^-\) channel channel in the current model and in the Standard Model. More... | |
| virtual const double | muttHmumu (const double sqrt_s) const |
| virtual const double | muttHptH_Hbb (const double sqrt_s) const |
| virtual const double | muttHptH_Hgaga (const double sqrt_s) const |
| virtual const double | muttHptH_Hmumu (const double sqrt_s) const |
| virtual const double | muttHptH_Htautau (const double sqrt_s) const |
| virtual const double | muttHptH_HWW (const double sqrt_s) const |
| virtual const double | muttHptH_HZZ (const double sqrt_s) const |
| virtual const double | muttHtautau (const double sqrt_s) const |
| virtual const double | muttHWW (const double sqrt_s) const |
| virtual const double | muttHWW2l2v (const double sqrt_s) const |
| virtual const double | muttHZbbboost (const double sqrt_s) const |
| The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model. More... | |
| virtual const double | muttHZga (const double sqrt_s) const |
| virtual const double | muttHZZ (const double sqrt_s) const |
| virtual const double | muttHZZ4l (const double sqrt_s) const |
| virtual const double | muVBF (const double sqrt_s) const |
| The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muVBFgamma (const double sqrt_s) const |
| The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHbb (const double sqrt_s) const |
| virtual const double | muVBFHgaga (const double sqrt_s) const |
| virtual const double | muVBFHmumu (const double sqrt_s) const |
| virtual const double | muVBFHtautau (const double sqrt_s) const |
| virtual const double | muVBFHWW (const double sqrt_s) const |
| virtual const double | muVBFHWW2l2v (const double sqrt_s) const |
| virtual const double | muVBFHZga (const double sqrt_s) const |
| virtual const double | muVBFHZZ (const double sqrt_s) const |
| virtual const double | muVBFHZZ4l (const double sqrt_s) const |
| virtual const double | muVBFpVH (const double sqrt_s) const |
| The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muVBFpVH_Hmumu (const double sqrt_s) const |
| virtual const double | muVBFpVH_HZga (const double sqrt_s) const |
| virtual const double | muVH (const double sqrt_s) const |
| The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muVHbb (const double sqrt_s) const |
| virtual const double | muVHcc (const double sqrt_s) const |
| virtual const double | muVHgaga (const double sqrt_s) const |
| virtual const double | muVHmumu (const double sqrt_s) const |
| virtual const double | muVHpT250 (const double sqrt_s) const |
| The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV. More... | |
| virtual const double | muVHtautau (const double sqrt_s) const |
| virtual const double | muVHWW (const double sqrt_s) const |
| virtual const double | muVHWW2l2v (const double sqrt_s) const |
| virtual const double | muVHZga (const double sqrt_s) const |
| virtual const double | muVHZZ (const double sqrt_s) const |
| virtual const double | muVHZZ4l (const double sqrt_s) const |
| virtual const double | muWH (const double sqrt_s) const |
| The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muWHbb (const double sqrt_s) const |
| virtual const double | muWHgaga (const double sqrt_s) const |
| virtual const double | muWHmumu (const double sqrt_s) const |
| virtual const double | muWHpT250 (const double sqrt_s) const |
| The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV. More... | |
| virtual const double | muWHtautau (const double sqrt_s) const |
| virtual const double | muWHWW (const double sqrt_s) const |
| virtual const double | muWHWW2l2v (const double sqrt_s) const |
| virtual const double | muWHZga (const double sqrt_s) const |
| virtual const double | muWHZZ (const double sqrt_s) const |
| virtual const double | muWHZZ4l (const double sqrt_s) const |
| virtual const double | muZH (const double sqrt_s) const |
| The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muZHbb (const double sqrt_s) const |
| virtual const double | muZHgaga (const double sqrt_s) const |
| virtual const double | muZHmumu (const double sqrt_s) const |
| virtual const double | muZHpT250 (const double sqrt_s) const |
| The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV. More... | |
| virtual const double | muZHtautau (const double sqrt_s) const |
| virtual const double | muZHWW (const double sqrt_s) const |
| virtual const double | muZHWW2l2v (const double sqrt_s) const |
| virtual const double | muZHZga (const double sqrt_s) const |
| virtual const double | muZHZZ (const double sqrt_s) const |
| virtual const double | muZHZZ4l (const double sqrt_s) const |
| virtual const double | Mw () const |
| The mass of the \(W\) boson, \(M_W\). More... | |
| virtual const double | N_nu () const |
| The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\). More... | |
| virtual const double | NevLHCppee13 (const int i_bin) const |
| Number of di-electron events at the LHC at 13 TeV. More... | |
| virtual const double | NevLHCppenu13 (const int i_bin) const |
| Number of mono-electron events at the LHC at 13 TeV. More... | |
| virtual const double | NevLHCppmumu13 (const int i_bin) const |
| Number of di-muon events at the LHC at 13 TeV. More... | |
| virtual const double | NevLHCppmunu13 (const int i_bin) const |
| Number of mono-muon events at the LHC at 13 TeV. More... | |
| virtual const double | NevLHCpptaunu13 (const int i_bin) const |
| Number of mono-tau events at the LHC at 13 TeV. More... | |
| virtual const double | NevLHCpptautau13 (const int i_bin) const |
| Number of di-tau events at the LHC at 13 TeV. More... | |
| NPbase () | |
| The default constructor. More... | |
| virtual const double | obliqueS () const |
| The oblique parameter \(S\). More... | |
| virtual const double | obliqueT () const |
| The oblique parameter \(T\). More... | |
| virtual const double | obliqueU () const |
| The oblique parameter \(U\). More... | |
| virtual const double | obliqueW () const |
| The oblique parameter \(W\). More... | |
| virtual const double | obliqueY () const |
| The oblique parameter \(Y\). More... | |
| virtual int | OutputOrder () const |
| virtual const double | ppZHprobe (const double sqrt_s) const |
| The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class. More... | |
| virtual const double | Qwemoller (const double q2, const double y) const |
| virtual const double | Qwn () const |
| virtual const double | Qwp () const |
| virtual const double | R0_f (const Particle f) const |
| The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More... | |
| virtual const double | R_inv () const |
| The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\). More... | |
| virtual const gslpp::complex | rhoZ_f (const Particle f) const |
| The effective neutral-current coupling \(\rho_Z^f\) including SM plus NP contributions. More... | |
| virtual const double | Ruc () const |
| The ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width. More... | |
| virtual const double | RWc () const |
| The ratio \(R_{W,c)=\Gamma(W\to c + X)/\Gamma(W\to had)\). More... | |
| virtual const double | RWlilj (const Particle li, const Particle lj) const |
| The lepton universality ratio \(R_{W,l_i/l_j)=\Gamma(W\to l_i \nu_i)/\Gamma(W\to l_j \nu_j)\). More... | |
| virtual const double | RZlilj (const Particle li, const Particle lj) const |
| The lepton universality ratio \(R_{Z,l_i/l_j)=\Gamma(Z\to l_i^+ l_i^-)/\Gamma(Z\to l_j^+ l_j^-)\). More... | |
| virtual bool | setFlag (const std::string name, const bool value) |
| A method to set a flag of NPbase. More... | |
| virtual const double | sigma0_had () const |
| The cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\sigma_h^0\). More... | |
| virtual const double | sigmaSM_ee (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| virtual const double | sin2thetaEff (const Particle f) const |
| The leptonic effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\rm lept}\) at the the \(Z\) pole. More... | |
| virtual const double | STXS0_qqH (const double sqrt_s) const |
| The STXS0 bin \(pp \to H qq\). More... | |
| virtual const double | STXS12_BrH4lRatio () const |
| The STXS BR \( H \to 4l \), \(l=e,\mu\). More... | |
| virtual const double | STXS12_BrHbbRatio () const |
| The STXS BR \( H \to bb \). More... | |
| virtual const double | STXS12_BrHevmuvRatio () const |
| The STXS BR \( H \to e\nu \mu\nu \). More... | |
| virtual const double | STXS12_BrHgagaRatio () const |
| The STXS BR \( H \to \gamma \gamma \). More... | |
| virtual const double | STXS12_ggH_mjj0_350_pTH0_60_Nj1 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 1,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60\). More... | |
| virtual const double | STXS12_ggH_mjj0_350_pTH0_60_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60\). More... | |
| virtual const double | STXS12_ggH_mjj0_350_pTH120_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~120<p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_mjj0_350_pTH60_120_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~60<p_{TH} [GeV]<120\). More... | |
| virtual const double | STXS12_ggH_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\). More... | |
| virtual const double | STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\). More... | |
| virtual const double | STXS12_ggH_mjj700_Inf_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\). More... | |
| virtual const double | STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\). More... | |
| virtual const double | STXS12_ggH_pTH0_10_Nj0 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j=0,~p_{TH} [GeV]<10\). More... | |
| virtual const double | STXS12_ggH_pTH0_60_Nj1 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j = 1,~p_{TH} [GeV]<60\). More... | |
| virtual const double | STXS12_ggH_pTH10_200_Nj0 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j = 0, 10<~p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_pTH10_Inf_Nj0 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j=0,~10<p_{TH} [GeV]\). More... | |
| virtual const double | STXS12_ggH_pTH120_200_Nj1 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j = 1,~120<p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_pTH200_300 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(~200<p_{TH} [GeV]<300\). More... | |
| virtual const double | STXS12_ggH_pTH200_300_Nj01 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j\leq 1,~200<p_{TH} [GeV]<300\). More... | |
| virtual const double | STXS12_ggH_pTH300_450 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(~300<p_{TH} [GeV]<450\). More... | |
| virtual const double | STXS12_ggH_pTH300_450_Nj01 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j\leq 1,~300<p_{TH} [GeV]<450\). More... | |
| virtual const double | STXS12_ggH_pTH450_650 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(450<~p_{TH} [GeV]<650\). More... | |
| virtual const double | STXS12_ggH_pTH450_650_Nj01 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j\leq 1,~450<p_{TH} [GeV]<650\). More... | |
| virtual const double | STXS12_ggH_pTH450_Inf (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(~p_{TH} [GeV]>450\). More... | |
| virtual const double | STXS12_ggH_pTH60_120_Nj1 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j = 1,~60<p_{TH} [GeV]<120\). More... | |
| virtual const double | STXS12_ggH_pTH650_Inf (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(~p_{TH} [GeV]>650\). More... | |
| virtual const double | STXS12_ggH_pTH650_Inf_Nj01 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j\leq 1,650<p_{TH} [GeV]\). More... | |
| virtual const double | STXS12_ggHll_pTV0_75 (const double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(p_{TV}[GeV]<75\). More... | |
| virtual const double | STXS12_ggHll_pTV150_250_Nj0 (const double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_ggHll_pTV150_250_Nj1 (const double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(N_j = 1,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_ggHll_pTV250_Inf (const double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(250 < p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_ggHll_pTV75_150 (const double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(75<p_{TV}[GeV]<150\). More... | |
| virtual const double | STXS12_qqHll_pTV0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(0<p_{TV}<150[GeV]\). More... | |
| virtual const double | STXS12_qqHll_pTV0_75 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(p_{TV}[GeV]<75\). More... | |
| virtual const double | STXS12_qqHll_pTV150_250_Nj0 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_qqHll_pTV150_250_Nj1 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_qqHll_pTV250_400 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}<400[GeV]\). More... | |
| virtual const double | STXS12_qqHll_pTV250_Inf (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_qqHll_pTV400_Inf (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(400<p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_qqHll_pTV75_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(75<p_{TV}[GeV]<150\). More... | |
| virtual const double | STXS12_qqHlv_pTV0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(0<p_{TV}<150[GeV]\). More... | |
| virtual const double | STXS12_qqHlv_pTV0_75 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(p_{TV}[GeV]<75\). More... | |
| virtual const double | STXS12_qqHlv_pTV150_250_Nj0 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_qqHlv_pTV150_250_Nj1 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_qqHlv_pTV250_400 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}<400[GeV]\). More... | |
| virtual const double | STXS12_qqHlv_pTV250_Inf (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_qqHlv_pTV400_Inf (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(400<p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_qqHlv_pTV75_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(75<p_{TV}[GeV]<150\). More... | |
| virtual const double | STXS12_qqHqq_mjj0_60_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~m_{jj}[GeV]<60\). More... | |
| virtual const double | STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1000<m_{jj}[GeV]<1500,~p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1000<m_{jj}[GeV],~p_{TH}[GeV]>200\). More... | |
| virtual const double | STXS12_qqHqq_mjj120_350_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~120<m_{jj}[GeV]<350\). More... | |
| virtual const double | STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1500<m_{jj}[GeV],~p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<1000,~p_{TH}[GeV]>200\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV],~200<p_{TH}[GeV]\). More... | |
| virtual const double | STXS12_qqHqq_mjj60_120_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~60<m_{jj}[GeV]<120\). More... | |
| virtual const double | STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV]<1000,~p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\). More... | |
| virtual const double | STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\). More... | |
| virtual const double | STXS12_qqHqq_Nj0 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j = 0\). More... | |
| virtual const double | STXS12_qqHqq_Nj1 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j = 1\). More... | |
| virtual const double | STXS12_qqHqq_VH_veto_Nj01 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j = 0,1\) VH-veto Ref. 2402.05742. More... | |
| virtual const double | STXS12_tH (const double sqrt_s) const |
| The STXS bin \(pp \to tH\). More... | |
| virtual const double | STXS12_ttH_pTH0_60 (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(p_{TH}[GeV]<60\). More... | |
| virtual const double | STXS12_ttH_pTH120_200 (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(120<p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_ttH_pTH200_300 (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(200<p_{TH}[GeV]<300\). More... | |
| virtual const double | STXS12_ttH_pTH300_450 (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]<450\). More... | |
| virtual const double | STXS12_ttH_pTH300_Inf (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]\). More... | |
| virtual const double | STXS12_ttH_pTH450_Inf (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(450<p_{TH}[GeV]\). More... | |
| virtual const double | STXS12_ttH_pTH60_120 (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(60<p_{TH}[GeV]<120\). More... | |
| virtual const double | STXS_ggH0j (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH1j_pTH_0_60 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH1j_pTH_120_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH1j_pTH_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH1j_pTH_60_120 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_0_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_0_60 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_120_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_60_120 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_qqHll_pTV_0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHll_pTV_150_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHll_pTV_150_250_0j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHll_pTV_150_250_1j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHll_pTV_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHlv_pTV_0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHlv_pTV_0_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHlv_pTV_150_250_0j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHlv_pTV_150_250_1j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHlv_pTV_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHqq_nonVHtopo (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_pTj_200 (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_Rest (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_VBFtopo_Rest (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_VHtopo (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_ttHtH (const double sqrt_s) const |
| The STXS bin \( ttH + tH \). More... | |
| virtual const double | STXS_WHqqHqq_pTj1_200 (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_WHqqHqq_Rest (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_WHqqHqq_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_WHqqHqq_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_WHqqHqq_VH2j (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_pTj1_200 (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_Rest (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_VH2j (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual const double | TauLFU_gmuge () const |
| virtual const double | TauLFU_gtauge () const |
| virtual const double | TauLFU_gtaugmu () const |
| virtual const double | TauLFU_gtaugmuK () const |
| virtual const double | TauLFU_gtaugmuPi () const |
| virtual bool | Update (const std::map< std::string, double > &DPars) |
| The update method for NPbase. More... | |
| virtual const double | UpperLimitZgammaA (const double sqrt_s) const |
| virtual const double | UpperLimitZgammaA13 (const double sqrt_s) const |
| virtual const double | UpperLimitZgammaC (const double sqrt_s) const |
| virtual const double | UpperLimitZgammaC13 (const double sqrt_s) const |
| virtual const double | xseeWW (const double sqrt_s) const |
| Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\). More... | |
| virtual const double | xseeWW4fLEP2 (const double sqrt_s, const int fstate) const |
| The cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | xseeWWhadLEP2 (const double sqrt_s) const |
| The cross section in pb for \(e^+ e^- \to W^+ W^- \to j j j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | xseeWWleptLEP2 (const double sqrt_s) const |
| The cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | xseeWWsemilLEP2 (const double sqrt_s) const |
| The cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | xseeWWtotLEP2 (const double sqrt_s) const |
| The total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| Public Member Functions inherited from StandardModel | |
| gslpp::complex | AH_f (const double tau) const |
| Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More... | |
| gslpp::complex | AH_W (const double tau) const |
| W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling. More... | |
| gslpp::complex | AHZga_f (const double tau, const double lambda) const |
| Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | AHZga_W (const double tau, const double lambda) const |
| W loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| const double | Ale (double mu, orders order, bool Nf_thr=true) const |
| The running electromagnetic coupling \(\alpha_e(\mu)\) in the \(\overline{MS}\) scheme. More... | |
| const double | ale_OS (const double mu, orders order=FULLNLO) const |
| The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell scheme. More... | |
| 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... | |
| 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... | |
| const double | eeffsigma (const Particle f, const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) 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 | 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... | |
| 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 | getDelGammaZ () const |
| A get method to retrieve the theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\). More... | |
| const double | getDelMw () const |
| A get method to retrieve the theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\). More... | |
| const double | getDelR0b () const |
| A get method to retrieve the theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More... | |
| const double | getDelR0c () const |
| A get method to retrieve the theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More... | |
| const double | getDelR0l () const |
| A get method to retrieve the theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More... | |
| const double | getDelSigma0H () const |
| A get method to retrieve the theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\). More... | |
| const double | getDelSin2th_b () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More... | |
| const double | getDelSin2th_l () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More... | |
| const double | getDelSin2th_q () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More... | |
| const std::string | getFlagKappaZ () const |
| A method to retrieve the model flag KappaZ. More... | |
| const std::string | getFlagMw () const |
| A method to retrieve the model flag Mw. More... | |
| const std::string | getFlagRhoZ () const |
| A method to retrieve the model flag RhoZ. More... | |
| const Flavour & | getFlavour () const |
| const double | getGF () const |
| A get method to retrieve the Fermi constant \(G_\mu\). More... | |
| const int | getIterationNo () const |
| const Particle & | getLeptons (const QCD::lepton p) const |
| A get method to retrieve the member object of a lepton. More... | |
| virtual StandardModelMatching & | getMatching () const |
| A get method to access the member reference of type StandardModelMatching. More... | |
| virtual const double | getMHl () const |
| A get method to retrieve the Higgs mass \(m_h\). More... | |
| virtual const double | getmq (const QCD::quark q, const double mu) const |
| The MSbar running quark mass computed at NLO. More... | |
| const double | getMuw () const |
| A get method to retrieve the matching scale \(\mu_W\) around the weak scale. More... | |
| const double | getMw () const |
| A get method to access the input value of the mass of the \(W\) boson \(M_W\). More... | |
| EWSMApproximateFormulae * | getMyApproximateFormulae () const |
| A get method to retrieve the member pointer of type EWSMApproximateFormulae. More... | |
| EWSMcache * | getMyEWSMcache () const |
| A get method to retrieve the member pointer of type EWSMcache. More... | |
| LeptonFlavour * | getMyLeptonFlavour () const |
| EWSMOneLoopEW * | getMyOneLoopEW () const |
| A get method to retrieve the member pointer of type EWSMOneLoopEW,. More... | |
| EWSMThreeLoopEW * | getMyThreeLoopEW () const |
| EWSMThreeLoopEW2QCD * | getMyThreeLoopEW2QCD () const |
| EWSMThreeLoopQCD * | getMyThreeLoopQCD () const |
| EWSMTwoFermionsLEP2 * | getMyTwoFermionsLEP2 () const |
| A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More... | |
| EWSMTwoLoopEW * | getMyTwoLoopEW () const |
| EWSMTwoLoopQCD * | getMyTwoLoopQCD () const |
| const double | getMz () const |
| A get method to access the mass of the \(Z\) boson \(M_Z\). More... | |
| virtual const double | getPhiBd () const |
| Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More... | |
| virtual const double | getPhiBs () const |
| Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More... | |
| const gslpp::matrix< gslpp::complex > | getUPMNS () const |
| A get method to retrieve the object of the PMNS matrix. More... | |
| const gslpp::matrix< gslpp::complex > | getVCKM () const |
| A get method to retrieve the CKM matrix. More... | |
| const gslpp::matrix< gslpp::complex > & | getYd () const |
| A get method to retrieve the Yukawa matrix of the down-type quarks, \(Y_d\). More... | |
| const gslpp::matrix< gslpp::complex > & | getYe () const |
| A get method to retrieve the Yukawa matrix of the charged leptons, \(Y_e\). More... | |
| const gslpp::matrix< gslpp::complex > & | getYn () const |
| A get method to retrieve the Yukawa matrix of the neutrinos, \(Y_\nu\). More... | |
| const gslpp::matrix< gslpp::complex > & | getYu () const |
| A get method to retrieve the Yukawa matrix of the up-type quarks, \(Y_u\). More... | |
| gslpp::complex | I_triangle_1 (const double tau, const double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | I_triangle_2 (const double tau, const double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| virtual bool | Init (const std::map< std::string, double > &DPars) |
| A method to initialize the model parameters. More... | |
| virtual bool | InitializeModel () |
| A method to initialize the model. More... | |
| const double | intMLL2eeeeus2 (const double s, const double t0, const double t1) const |
| const double | intMLR2eeeets2 (const double s, const double t0, const double t1) const |
| const double | intMLRtilde2eeeest2 (const double s, const double t0, const double t1) const |
| const double | intMRR2eeeeus2 (const double s, const double t0, const double t1) const |
| const bool | IsFlagNoApproximateGammaZ () const |
| A method to retrieve the model flag NoApproximateGammaZ. More... | |
| const bool | IsFlagWithoutNonUniversalVC () const |
| A method to retrieve the model flag WithoutNonUniversalVC. More... | |
| const bool | isSMSuccess () const |
| A get method to retrieve the success status of the Standard Model update and matching. More... | |
| const double | MLL2eeff (const Particle f, const double s, const double t) const |
| const double | MLR2eeff (const Particle f, const double s) const |
| const double | MRL2eeff (const Particle f, const double s) const |
| const double | MRR2eeff (const Particle f, const double s, const double t) const |
| const double | Mw_tree () const |
| The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). More... | |
| const double | MwbarFromMw (const double Mw) const |
| A method to convert the \(W\)-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More... | |
| const double | MwFromMwbar (const double Mwbar) const |
| A method to convert the \(W\)-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More... | |
| double | Mzbar () const |
| The \(Z\)-boson mass \(\overline{M}_Z\) in the complex-pole/fixed-width scheme. More... | |
| virtual bool | PostUpdate () |
| The post-update method for StandardModel. More... | |
| virtual bool | PreUpdate () |
| The pre-update method for StandardModel. More... | |
| virtual const double | rho_GammaW (const Particle fi, const Particle fj) const |
| EW radiative corrections to the width of \(W \to f_i \bar{f}_j\), denoted as \(\rho^W_{ij}\). More... | |
| const double | s02 () const |
| The square of the sine of the weak mixing angle \(s_0^2\) defined without weak radiative corrections. More... | |
| void | setCKM (const CKM &CKMMatrix) |
| A set method to change the CKM matrix. More... | |
| void | setFlagCacheInStandardModel (bool FlagCacheInStandardModel) |
| A set method to change the model flag CacheInStandardModel of StandardModel. More... | |
| void | setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ) |
| bool | setFlagSigmaForAFB (const bool flagSigmaForAFB_i) |
| bool | setFlagSigmaForR (const bool flagSigmaForR_i) |
| virtual bool | setFlagStr (const std::string name, const std::string value) |
| A method to set a flag of StandardModel. More... | |
| void | setRequireCKM (bool requireCKM) |
| A set method to change the value of requireCKM. More... | |
| void | setSMSuccess (bool success) const |
| A set method to change the success status of the Standard Model update and matching. More... | |
| void | setYd (const gslpp::matrix< gslpp::complex > &Yd) |
| A set method to set the Yukawa matrix of the down-type quarks, \(Y_d\). More... | |
| void | setYe (const gslpp::matrix< gslpp::complex > &Ye) |
| A set method to set the Yukawa matrix of the charged leptons, \(Y_e\). More... | |
| void | setYu (const gslpp::matrix< gslpp::complex > &Yu) |
| A set method to set the Yukawa matrix of the up-type quarks, \(Y_u\). More... | |
| virtual const double | SigmaeeHee (const double sqrt_s, const double Pe, const double Pp) const |
| The \(\sigma(e^+ e^- \to e^+ e^- H)\) in the Standard Model. More... | |
| virtual const double | SigmaeeHvv (const double sqrt_s, const double Pe, const double Pp) const |
| The \(\sigma(e^+ e^- \to \nu \bar{\nu} H)\) in the Standard Model. More... | |
| virtual const double | SigmaeeZH (const double sqrt_s, const double Pe, const double Pp) const |
| The \(\sigma(e^+ e^- \to Z H)\) in the Standard Model. More... | |
| StandardModel () | |
| The default constructor. More... | |
| const double | sW2 () const |
| virtual const double | sW2 (const double Mw_i) const |
| The square of the sine of the weak mixing angle in the on-shell scheme, denoted as \(s_W^2\). More... | |
| const double | sW2_MSbar_Approx () const |
| The (approximated formula for the) square of the sine of the weak mixing angle in the MSbar scheme, denoted as \(\hat{s}_{W}^2\). See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) More... | |
| const double | sW2_ND () const |
| The square of the sine of the weak mixing angle in the MSbar-ND scheme (w/o decoupling $\alpha\ln(m_t/M_Z)$ terms), denoted as \(\hat{s}_{ND}^2\). See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) (eq. 10.13a/10.13b) More... | |
| virtual const double | 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... | |
Public Attributes | |
| double | C1Hbb = 0.0 |
| double | C1Hcc = 0.0 |
| double | C1Hgaga = 0.0049 |
| double | C1Hgg = 0.0066 |
| double | C1Hmumu = 0.0 |
| The C1 coefficient controlling the H^3 corrections to the Higgs partial width from the Higgs trilinear coupling. More... | |
| double | C1Hss = 0.0 |
| double | C1Htautau = 0.0 |
| double | C1HWW = 0.0073 |
| double | C1HZga = 0.0 |
| The C1 coefficient controlling the H^3 corrections to the Higgs partial width from the Higgs trilinear coupling. More... | |
| double | C1HZZ = 0.0083 |
Protected Attributes | |
| StandardModel | trueSM |
| 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 | 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... | |
Additional Inherited Members | |
| Public Types inherited from StandardModel | |
| enum | LEP2RCs { Weak = 0 , WeakBox , ISR , QEDFSR , QCDFSR , NUMofLEP2RCs } |
| enum | orders_EW { EW1 = 0 , EW1QCD1 , EW1QCD2 , EW2 , EW2QCD1 , EW3 , orders_EW_size } |
| An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More... | |
| Public Types inherited from QCD | |
| enum | lepton { NEUTRINO_1 , ELECTRON , NEUTRINO_2 , MU , NEUTRINO_3 , TAU , NOLEPTON } |
| An enum type for leptons. More... | |
| enum | meson { P_0 , P_P , K_0 , K_P , D_0 , D_P , D_S , B_D , B_P , B_S , B_C , PHI , K_star , K_star_P , K_S , D_star_P , RHO , RHO_P , OMEGA , MESON_END } |
| An enum type for mesons. More... | |
| enum | quark { UP , DOWN , CHARM , STRANGE , TOP , BOTTOM } |
| An enum type for quarks. More... | |
| Static Public Attributes inherited from StandardModel | |
| static const double | GeVminus2_to_nb = 389379.338 |
| static const double | Mw_error = 0.00001 |
| The target accuracy of the iterative calculation of the \(W\)-boson mass in units of GeV. More... | |
| static const int | NSMvars = 26 |
| The number of the model parameters in StandardModel. More... | |
| static const int | NumSMParamsForEWPO = 33 |
| The number of the SM parameters that are relevant to the EW precision observables. More... | |
| static std::string | SMvars [NSMvars] |
| A string array containing the labels of the model parameters in StandardModel. More... | |
| Static Public Attributes inherited from QCD | |
| static const int | NQCDvars = 11 |
| The number of model parameters in QCD. More... | |
| static std::string | QCDvars [NQCDvars] |
| An array containing the labels under which all QCD parameters are stored in a vector of ModelParameter via InputParser::ReadParameters(). More... | |
| Protected Member Functions inherited from StandardModel | |
| const double | AFB_NoISR_l (const QCD::lepton l_flavor, const double s) const |
| const double | AFB_NoISR_q (const QCD::quark q_flavor, const double s) const |
| bool | checkEWPOscheme (const std::string scheme) const |
| A method to check if a given scheme name in string form is valid. More... | |
| virtual void | computeCKM () |
| The method to compute the CKM matrix. More... | |
| virtual void | computeYukawas () |
| The method to compute the Yukawas matrix. More... | |
| double | Delta_EWQCD (const QCD::quark q) const |
| The non-factorizable EW-QCD corrections to the partial widths for \(Z\to q\bar{q}\), denoted as \(\Delta_{\mathrm{EW/QCD}}\). More... | |
| const double | getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm133 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm167 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm207 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu130 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu136 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu161 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu207 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau130 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau136 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau161 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau207 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom130 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom133 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom136 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom161 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom167 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom172 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom183 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom189 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom192 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom196 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom200 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom202 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom205 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom207 (double x) const |
| const double | getIntegrand_dsigmaBox_charm130 (double x) const |
| const double | getIntegrand_dsigmaBox_charm133 (double x) const |
| const double | getIntegrand_dsigmaBox_charm136 (double x) const |
| const double | getIntegrand_dsigmaBox_charm161 (double x) const |
| const double | getIntegrand_dsigmaBox_charm167 (double x) const |
| const double | getIntegrand_dsigmaBox_charm172 (double x) const |
| const double | getIntegrand_dsigmaBox_charm183 (double x) const |
| const double | getIntegrand_dsigmaBox_charm189 (double x) const |
| const double | getIntegrand_dsigmaBox_charm192 (double x) const |
| const double | getIntegrand_dsigmaBox_charm196 (double x) const |
| const double | getIntegrand_dsigmaBox_charm200 (double x) const |
| const double | getIntegrand_dsigmaBox_charm202 (double x) const |
| const double | getIntegrand_dsigmaBox_charm205 (double x) const |
| const double | getIntegrand_dsigmaBox_charm207 (double x) const |
| const double | getIntegrand_dsigmaBox_down130 (double x) const |
| const double | getIntegrand_dsigmaBox_down133 (double x) const |
| const double | getIntegrand_dsigmaBox_down136 (double x) const |
| const double | getIntegrand_dsigmaBox_down161 (double x) const |
| const double | getIntegrand_dsigmaBox_down167 (double x) const |
| const double | getIntegrand_dsigmaBox_down172 (double x) const |
| const double | getIntegrand_dsigmaBox_down183 (double x) const |
| const double | getIntegrand_dsigmaBox_down189 (double x) const |
| const double | getIntegrand_dsigmaBox_down192 (double x) const |
| const double | getIntegrand_dsigmaBox_down196 (double x) const |
| const double | getIntegrand_dsigmaBox_down200 (double x) const |
| const double | getIntegrand_dsigmaBox_down202 (double x) const |
| const double | getIntegrand_dsigmaBox_down205 (double x) const |
| const double | getIntegrand_dsigmaBox_down207 (double x) const |
| const double | getIntegrand_dsigmaBox_mu130 (double x) const |
| const double | getIntegrand_dsigmaBox_mu133 (double x) const |
| const double | getIntegrand_dsigmaBox_mu136 (double x) const |
| const double | getIntegrand_dsigmaBox_mu161 (double x) const |
| const double | getIntegrand_dsigmaBox_mu167 (double x) const |
| const double | getIntegrand_dsigmaBox_mu172 (double x) const |
| const double | getIntegrand_dsigmaBox_mu183 (double x) const |
| const double | getIntegrand_dsigmaBox_mu189 (double x) const |
| const double | getIntegrand_dsigmaBox_mu192 (double x) const |
| const double | getIntegrand_dsigmaBox_mu196 (double x) const |
| const double | getIntegrand_dsigmaBox_mu200 (double x) const |
| const double | getIntegrand_dsigmaBox_mu202 (double x) const |
| const double | getIntegrand_dsigmaBox_mu205 (double x) const |
| const double | getIntegrand_dsigmaBox_mu207 (double x) const |
| const double | getIntegrand_dsigmaBox_strange130 (double x) const |
| const double | getIntegrand_dsigmaBox_strange133 (double x) const |
| const double | getIntegrand_dsigmaBox_strange136 (double x) const |
| const double | getIntegrand_dsigmaBox_strange161 (double x) const |
| const double | getIntegrand_dsigmaBox_strange167 (double x) const |
| const double | getIntegrand_dsigmaBox_strange172 (double x) const |
| const double | getIntegrand_dsigmaBox_strange183 (double x) const |
| const double | getIntegrand_dsigmaBox_strange189 (double x) const |
| const double | getIntegrand_dsigmaBox_strange192 (double x) const |
| const double | getIntegrand_dsigmaBox_strange196 (double x) const |
| const double | getIntegrand_dsigmaBox_strange200 (double x) const |
| const double | getIntegrand_dsigmaBox_strange202 (double x) const |
| const double | getIntegrand_dsigmaBox_strange205 (double x) const |
| const double | getIntegrand_dsigmaBox_strange207 (double x) const |
| const double | getIntegrand_dsigmaBox_tau130 (double x) const |
| const double | getIntegrand_dsigmaBox_tau133 (double x) const |
| const double | getIntegrand_dsigmaBox_tau136 (double x) const |
| const double | getIntegrand_dsigmaBox_tau161 (double x) const |
| const double | getIntegrand_dsigmaBox_tau167 (double x) const |
| const double | getIntegrand_dsigmaBox_tau172 (double x) const |
| const double | getIntegrand_dsigmaBox_tau183 (double x) const |
| const double | getIntegrand_dsigmaBox_tau189 (double x) const |
| const double | getIntegrand_dsigmaBox_tau192 (double x) const |
| const double | getIntegrand_dsigmaBox_tau196 (double x) const |
| const double | getIntegrand_dsigmaBox_tau200 (double x) const |
| const double | getIntegrand_dsigmaBox_tau202 (double x) const |
| const double | getIntegrand_dsigmaBox_tau205 (double x) const |
| const double | getIntegrand_dsigmaBox_tau207 (double x) const |
| const double | getIntegrand_dsigmaBox_up130 (double x) const |
| const double | getIntegrand_dsigmaBox_up133 (double x) const |
| const double | getIntegrand_dsigmaBox_up136 (double x) const |
| const double | getIntegrand_dsigmaBox_up161 (double x) const |
| const double | getIntegrand_dsigmaBox_up167 (double x) const |
| const double | getIntegrand_dsigmaBox_up172 (double x) const |
| const double | getIntegrand_dsigmaBox_up183 (double x) const |
| const double | getIntegrand_dsigmaBox_up189 (double x) const |
| const double | getIntegrand_dsigmaBox_up192 (double x) const |
| const double | getIntegrand_dsigmaBox_up196 (double x) const |
| const double | getIntegrand_dsigmaBox_up200 (double x) const |
| const double | getIntegrand_dsigmaBox_up202 (double x) const |
| const double | getIntegrand_dsigmaBox_up205 (double x) const |
| const double | getIntegrand_dsigmaBox_up207 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom130 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom133 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom136 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom161 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom167 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom172 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom183 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom189 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom192 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom196 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom200 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom202 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom205 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom207 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm130 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm133 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm136 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm161 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm167 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm172 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm183 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm189 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm192 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm196 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm200 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm202 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm205 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm207 (double x) const |
| const double | getIntegrand_sigmaWithISR_down130 (double x) const |
| const double | getIntegrand_sigmaWithISR_down133 (double x) const |
| const double | getIntegrand_sigmaWithISR_down136 (double x) const |
| const double | getIntegrand_sigmaWithISR_down161 (double x) const |
| const double | getIntegrand_sigmaWithISR_down167 (double x) const |
| const double | getIntegrand_sigmaWithISR_down172 (double x) const |
| const double | getIntegrand_sigmaWithISR_down183 (double x) const |
| const double | getIntegrand_sigmaWithISR_down189 (double x) const |
| const double | getIntegrand_sigmaWithISR_down192 (double x) const |
| const double | getIntegrand_sigmaWithISR_down196 (double x) const |
| const double | getIntegrand_sigmaWithISR_down200 (double x) const |
| const double | getIntegrand_sigmaWithISR_down202 (double x) const |
| const double | getIntegrand_sigmaWithISR_down205 (double x) const |
| const double | getIntegrand_sigmaWithISR_down207 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu130 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu136 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu161 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu172 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu183 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu189 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu192 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu196 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu200 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu202 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu205 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu207 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange130 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange133 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange136 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange161 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange167 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange172 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange183 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange189 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange192 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange196 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange200 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange202 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange205 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange207 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau130 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau136 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau161 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau172 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau183 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau189 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau192 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau196 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau200 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau202 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau205 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau207 (double x) const |
| const double | getIntegrand_sigmaWithISR_up130 (double x) const |
| const double | getIntegrand_sigmaWithISR_up133 (double x) const |
| const double | getIntegrand_sigmaWithISR_up136 (double x) const |
| const double | getIntegrand_sigmaWithISR_up161 (double x) const |
| const double | getIntegrand_sigmaWithISR_up167 (double x) const |
| const double | getIntegrand_sigmaWithISR_up172 (double x) const |
| const double | getIntegrand_sigmaWithISR_up183 (double x) const |
| const double | getIntegrand_sigmaWithISR_up189 (double x) const |
| const double | getIntegrand_sigmaWithISR_up192 (double x) const |
| const double | getIntegrand_sigmaWithISR_up196 (double x) const |
| const double | getIntegrand_sigmaWithISR_up200 (double x) const |
| const double | getIntegrand_sigmaWithISR_up202 (double x) const |
| const double | getIntegrand_sigmaWithISR_up205 (double x) const |
| const double | getIntegrand_sigmaWithISR_up207 (double x) const |
| const double | Integrand_AFBnumeratorWithISR_l (double x, const QCD::lepton l_flavor, const double s) const |
| const double | Integrand_AFBnumeratorWithISR_q (double x, const QCD::quark q_flavor, const double s) const |
| const double | Integrand_dsigmaBox_l (double cosTheta, const QCD::lepton l_flavor, const double s) const |
| const double | Integrand_dsigmaBox_q (double cosTheta, const QCD::quark q_flavor, const double s) const |
| const double | Integrand_sigmaWithISR_l (double x, const QCD::lepton l_flavor, const double s) const |
| const double | Integrand_sigmaWithISR_q (double x, const QCD::quark q_flavor, const double s) const |
| double | m_q (const QCD::quark q, const double mu, const orders order=FULLNLO) const |
| double | RAq (const QCD::quark q) const |
| The radiator factor associated with the final-state QED and QCD corrections to the the axial-vector-current interactions, \(R_A^q(M_Z^2)\). More... | |
| double | resumKappaZ (const double DeltaRho[orders_EW_size], const double deltaKappa_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const |
| A method to compute the real part of the effetvive coupling \(\kappa_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | resumMw (const double Mw_i, const double DeltaRho[orders_EW_size], const double DeltaR_rem[orders_EW_size]) const |
| A method to compute the \(W\)-boson mass from \(\Delta\rho\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | resumRhoZ (const double DeltaRho[orders_EW_size], const double deltaRho_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const |
| A method to compute the real part of the effective coupling \(\rho_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | RVh () const |
| The singlet vector corrections to the hadronic \(Z\)-boson width, denoted as \(R_V^h\). More... | |
| double | RVq (const QCD::quark q) const |
| The radiator factor associated with the final-state QED and QCD corrections to the the vector-current interactions, \(R_V^q(M_Z^2)\). More... | |
| double | SchemeToDouble (const std::string scheme) const |
| A method to convert a given scheme name in string form into a floating-point number with double precision. More... | |
| virtual void | setParameter (const std::string name, const double &value) |
| A method to set the value of a parameter of StandardModel. More... | |
| const double | sigma_NoISR_l (const QCD::lepton l_flavor, const double s) const |
| const double | sigma_NoISR_q (const QCD::quark q_flavor, const double s) const |
| double | taub () const |
| Top-mass corrections to the \(Zb\bar{b}\) vertex, denoted by \(\tau_b\). More... | |
| Protected Member Functions inherited from QCD | |
| const double | MassOfNf (int nf) const |
| The Mbar mass of the heaviest quark in the theory with Nf active flavour. More... | |
| NPbase::NPbase | ( | ) |
The default constructor.
Definition at line 29 of file NPbase.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 StandardModel.
Reimplemented in NPSMEFTd6General, NPZbbbar, and NPEpsilons.
Definition at line 817 of file NPbase.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 StandardModel.
Reimplemented in NPSMEFTd6General, NPZbbbar, and NPEpsilons.
Definition at line 914 of file NPbase.cpp.
|
virtual |
The electromagnetic coupling at the \(Z\)-mass scale, \(\alpha(M_Z^2)=\alpha/(1-\Delta\alpha(M_Z^2))\).
Reimplemented from StandardModel.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 51 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1530 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1520 of file NPbase.cpp.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
Auxiliary observable AuxObs_NP1.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP10.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP11.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP12.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP13.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP14.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP15.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP16.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP17.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP18.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP19.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP2.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP20.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP21.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP22.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP23.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP24.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP25.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP26.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP27.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP28.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP29.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP3.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP30.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP4.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP5.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP6.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP7.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP8.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Auxiliary observable AuxObs_NP9.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The branching ratio of the of the Higgs into exotic particles.
Reimplemented in HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The branching ratio of the of the Higgs into invisible particles.
Reimplemented in HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The branching ratio of the of the Higgs into invisible particles (only invisible new particles).
Reimplemented in HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
virtual |
The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\).
| [in] | f | a lepton or quark |
Definition at line 541 of file NPbase.cpp.
|
inlinevirtual |
The ratio of the Br \((H\to 2d2d)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2e 2\mu)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2e2v)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2\mu 2v)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2u2d)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2u2u)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2ud)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2v2d)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2v2u)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 2v2v)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 4d)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 4e)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 4f)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 4\mu)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 4u)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to 4v)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model.
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.
|
inlinevirtual |
The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model.
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.
|
inlinevirtual |
The ratio of the Br \((H\to e\nu \mu\nu)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model.
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.
|
inlinevirtual |
The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model.
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.
|
inlinevirtual |
The ratio of the Br \((H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, and HiggsKigen.
|
inlinevirtual |
The ratio of the Br \((H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model.
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.
|
inlinevirtual |
The ratio of the Br \((H\to s\bar{s})\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model.
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.
|
inlinevirtual |
The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to uddu)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model.
Reimplemented in HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to VV)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model.
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.
|
inlinevirtual |
The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, and SigmaBR.
|
inlinevirtual |
The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, and SigmaBR.
|
inlinevirtual |
The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, and SigmaBR.
|
inlinevirtual |
The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model.
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.
|
inlinevirtual |
The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model.
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, SigmaBR, THDMW, and THDMWSignalStrengths.
The branching ratio of the \(W\) boson decaying into a SM fermion pair, \(Br(W\to f_i f_j)\).
Reimplemented from StandardModel.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 128 of file NPbase.cpp.
|
virtual |
The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.
Definition at line 1730 of file NPbase.cpp.
|
virtual |
The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.
Definition at line 1830 of file NPbase.cpp.
|
virtual |
The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.
Definition at line 1680 of file NPbase.cpp.
|
virtual |
The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.
Definition at line 1780 of file NPbase.cpp.
|
virtual |
The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH.
Definition at line 1630 of file NPbase.cpp.
| const double NPbase::C1Htot | ( | ) | const |
The C1 coefficient controlling the H^3 corrections to the total Higgs width from the Higgs trilinear coupling.
Definition at line 1624 of file NPbase.cpp.
|
inlinevirtual |
Reimplemented in HiggsChiral.
|
inlinevirtual |
Reimplemented in HiggsChiral.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in HiggsChiral.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{11}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{22}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{33}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{11}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{22}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{33}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{11}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{22}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{33}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{11}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{22}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{33}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{11}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{22}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{33}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{11}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{22}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{33}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(d)})_{33}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{11}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{22}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{33}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in HiggsChiral.
|
inlinevirtual |
The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in HiggsChiral.
|
inlinevirtual |
Reimplemented in HiggsChiral.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model.
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6, NPSMEFTd6General, THDMW, and THDMWSignalStrengths.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in HiggsChiral.
|
inlinevirtual |
Reimplemented in HiggsChiral.
|
inlinevirtual |
The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Quadratic contribution from the Higgs self-couplings modifications to the signal strength for \(\sigma \times BR(H\to xx)\) in the current model.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Quadratic contribution from the Higgs self-couplings modifications to the signal strength for an observable \(\sigma\) in the current model.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
virtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 1201 of file NPbase.cpp.
|
virtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 1179 of file NPbase.cpp.
|
virtual |
The computation of the parity violating asymmetry in Moller scattering.
| [in] | q2 | the \(Q^2\) of the process |
| [in] | y |
Reimplemented in NPSMEFTd6General.
Definition at line 1481 of file NPbase.cpp.
|
virtual |
The computation of the anomalous magnetic moment of the muon \(a_\mu=(g_\mu-2)/2\).
Reimplemented in NPSMEFTd6General.
Definition at line 1468 of file NPbase.cpp.
|
virtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 1157 of file NPbase.cpp.
|
virtual |
The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gAnue.
Reimplemented in NPSMEFTd6General.
Definition at line 1513 of file NPbase.cpp.
|
virtual |
The computation of the correction to the effective neutrino nucleon LH coupling: delta_gLnuN2.
Reimplemented in NPSMEFTd6General.
Definition at line 1498 of file NPbase.cpp.
|
virtual |
The computation of the correction to the effective neutrino nucleon RH coupling: delta_gRnuN2.
Reimplemented in NPSMEFTd6General.
Definition at line 1503 of file NPbase.cpp.
|
virtual |
The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gVnue.
Reimplemented in NPSMEFTd6General.
Definition at line 1508 of file NPbase.cpp.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
virtual |
The computation of the electron's weak charge.
| [in] | q2 | the \(Q^2\) at which the weak charge is measured |
| [in] | y |
Reimplemented in NPSMEFTd6General.
Definition at line 1475 of file NPbase.cpp.
|
virtual |
The computation of the neutron weak charge: Qwn.
Reimplemented in NPSMEFTd6General.
Definition at line 1493 of file NPbase.cpp.
|
virtual |
The computation of the proton weak charge: Qwp.
Reimplemented in NPSMEFTd6General.
Definition at line 1487 of file NPbase.cpp.
|
virtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 1191 of file NPbase.cpp.
|
virtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 1162 of file NPbase.cpp.
|
virtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 1167 of file NPbase.cpp.
|
virtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 1196 of file NPbase.cpp.
|
virtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 1173 of file NPbase.cpp.
|
virtual |
The computation of the correction to the LFU ratio \(g_\mu/ g_e \).
Reimplemented in NPSMEFTd6General.
Definition at line 1570 of file NPbase.cpp.
|
virtual |
The computation of the correction to the LFU ratio \(g_\tau/ g_e \).
Reimplemented in NPSMEFTd6General.
Definition at line 1580 of file NPbase.cpp.
|
virtual |
The computation of the correction to the LFU ratio \(g_\tau/ g_\mu \).
Reimplemented in NPSMEFTd6General.
Definition at line 1575 of file NPbase.cpp.
|
virtual |
The computation of the correction to the LFU ratio \(\left(g_\tau/ g_\mu\right)_K \).
Reimplemented in NPSMEFTd6General.
Definition at line 1590 of file NPbase.cpp.
|
virtual |
The computation of the correction to the LFU ratio \(\left(g_\tau/ g_\mu\right)_\pi \).
Reimplemented in NPSMEFTd6General.
Definition at line 1585 of file NPbase.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 in NPSMEFTd6General.
Definition at line 800 of file NPbase.cpp.
|
virtual |
The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\Delta \mathcal{A}_f^{(2)}\).
\(\newcommand{\nc}{\newcommand}\) \(\nc{\gVfSM}{g_{V,f}^{SM}}\) \(\nc{\gAfSM}{g_{A,f}^{SM}}\) \(\nc{\gVfL}{\Delta g_{V,f}^{(1)}}\) \(\nc{\gAfL}{\Delta g_{A,f}^{(1)}}\) \(\nc{\gVfQ}{\Delta g_{V,f}^{(2)}}\) \(\nc{\gAfQ}{\Delta g_{A,f}^{(2)}}\)
\begin{eqnarray*} \Delta \mathcal{A}_f^{(2)} &=& 2~ \frac{ \gVfSM ~\gAfSM }{ \left[(g_{V,f}^{SM})^2+(g_{A,f}^{SM})^2\right]^3 } \left( \left[(\gAfSM)^2 -3 (\gVfSM)^2\right] (\gAfL)^2 + \left[(\gVfSM)^2 -3 (\gAfSM)^2\right] (\gVfL)^2 \right) \\ &-& ~ 2~ \frac{ (\gAfSM)^4 - 6(\gAfSM)^2(\gVfSM)^2 + (\gVfSM)^4 }{\left[(g_{V,f}^{SM})^2+(g_{A,f}^{SM})^2\right]^3} ~\gVfL ~\gAfL +~ 2~ \frac{ (g_{V,f}^{SM})^2-(g_{A,f}^{SM})^2 }{ \left[(g_{V,f}^{SM})^2+(g_{A,f}^{SM})^2\right]^2 } \left[ \gVfSM ~\gAfQ - \gAfSM ~\gVfQ \right] \end{eqnarray*}
| [in] | f | a lepton or quark |
Definition at line 772 of file NPbase.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 in NPSMEFTd6General.
Definition at line 879 of file NPbase.cpp.
|
virtual |
The \(\mathcal{O}(\Lambda^{-4})\) new physics to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\Delta A^f_{FB}\).
\[ \Delta A_{FB,f}^{(2)} = \frac{3}{4} \left( \Delta A_e^{(1)} \Delta A_f^{(1)} + A_e^{SM} \Delta A_f^{(2)} + A_f^{SM} \Delta A_e^{(2)} \right) \]
| [in] | f | a lepton or quark |
Definition at line 830 of file NPbase.cpp.
|
inlinevirtual |
The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The new physics contribution to the differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The new physics relative contribution to the EW coupling constant \(e\).
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
Definition at line 980 of file NPbase.h.
|
inlinevirtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
Definition at line 1034 of file NPbase.h.
|
inlinevirtual |
The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6General.
Definition at line 1044 of file NPbase.h.
|
inlinevirtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
Definition at line 1007 of file NPbase.h.
|
inlinevirtual |
The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph].
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
Definition at line 989 of file NPbase.h.
|
inlinevirtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
Definition at line 1053 of file NPbase.h.
|
inlinevirtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
Definition at line 1016 of file NPbase.h.
|
inlinevirtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
Definition at line 998 of file NPbase.h.
|
inlinevirtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
Definition at line 1025 of file NPbase.h.
|
inlinevirtual |
The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
Definition at line 1062 of file NPbase.h.
|
inlinevirtual |
The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6General.
Definition at line 1072 of file NPbase.h.
|
inlinevirtual |
The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\).
| [in] | p | a lepton or quark |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
Definition at line 1083 of file NPbase.h.
|
inlinevirtual |
The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
Definition at line 961 of file NPbase.h.
|
inlinevirtual |
The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6General.
Definition at line 971 of file NPbase.h.
|
inlinevirtual |
The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
Definition at line 1092 of file NPbase.h.
|
virtual |
New physics contribution to the neutral-current axial-vector coupling \(g_A^f\).
The neutral-current axial-vector coupling \(g_A^f\) receives the new physics contribution via the oblique parameter \(T\) and the shift in the Fermi constant, \(\Delta G\):
\[ \delta g_A^f = \frac{g_{A,\mathrm{SM}}^f}{2} \left[ \alpha(M_Z^2)\, T - \Delta G \right]. \]
See [Ciuchini:2013pca] and references therein.
| [in] | f | a lepton or quark |
Reimplemented in NPEpsilons_pureNP, NPSTUZbbbarLR, NPZbbbar, NPZbbbarLinearized, NPSMEFTd6, and NPSMEFTd6General.
Definition at line 204 of file NPbase.cpp.
|
inlinevirtual |
|
inlinevirtual |
The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6, and NPSMEFTd6General.
|
virtual |
The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\).
Reimplemented in NPSMEFTd6General.
Definition at line 363 of file NPbase.cpp.
|
virtual |
The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the total decay width of the \(Z\) boson, \(\Delta \Gamma_Z^{(2)}\).
\[ \Delta \Gamma_{Z}^{(2)} = \Delta \Gamma_{Z,fer}^{(2)} + \Delta \Gamma_{Z,had}^{(2)} \]
Definition at line 338 of file NPbase.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 in NPSMEFTd6General.
Definition at line 289 of file NPbase.cpp.
|
virtual |
The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\Delta \Gamma_{Z,f}^{(2)}\).
\(\newcommand{\nc}{\newcommand}\) \(\nc{\gVfSM}{g_{V,f}^{SM}}\) \(\nc{\gAfSM}{g_{A,f}^{SM}}\) \(\nc{\gVfL}{\Delta g_{V,f}^{(1)}}\) \(\nc{\gAfL}{\Delta g_{A,f}^{(1)}}\) \(\nc{\gVfQ}{\Delta g_{V,f}^{(2)}}\) \(\nc{\gAfQ}{\Delta g_{A,f}^{(2)}}\)
\[ \Delta \Gamma_{Z,f}^{(2)} = N_f \frac{\alpha(M_Z)^{SM} M_Z}{6 s_W^2 c_w^2} \left[ (\gVfL)^2 + (\gAfL)^2 + 2 \left( \gAfSM ~\gAfQ + \gVfSM ~\gVfQ \right) \right] \]
| [in] | f | a lepton or quark |
Definition at line 256 of file NPbase.cpp.
|
virtual |
The new physics contribution to the hadronic decay width of the \(Z\) boson, \(\delta \Gamma_{Z,had}\).
Definition at line 499 of file NPbase.cpp.
|
virtual |
The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the hadronic decay width of the \(Z\) boson, \(\Delta \Gamma_{Z,had}^{(2)}\).
\[ \Delta \Gamma_{Z,had}^{(2)} = \Delta \Gamma_{Z,u}^{(2)} + \Delta \Gamma_{Z,d}^{(2)} + \Delta \Gamma_{Z,c}^{(2)} + \Delta \Gamma_{Z,s}^{(2)} + \Delta \Gamma_{Z,b}^{(2)} \]
Definition at line 478 of file NPbase.cpp.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
New physics contribution to the Fermi constant.
The new physics contribution \(\Delta G\) is defined as
\[ G_\mu = G_{\mu,\mathrm{SM}}(1+\Delta G)\,, \]
where \(G_\mu\) is the experimental value measured through muon decays, and \(G_{\mu,\mathrm{SM}}\) is the Fermi constant in the SM.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
| const double NPbase::deltaGL_f_mu | ( | const Particle | p, |
| const double | mu | ||
| ) | const |
New physics contribution to the neutral-current left-handed coupling \(g_L^f\).
| [in] | f | a lepton or quark |
| [in] | mu | the RG scale to be used in the evaluation (for those models where it is available) |
Definition at line 231 of file NPbase.cpp.
|
inlinevirtual |
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 in NPSMEFTd6, and NPSMEFTd6General.
|
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 in NPSMEFTd6General.
Definition at line 244 of file NPbase.cpp.
| const double NPbase::deltaGR_f_mu | ( | const Particle | p, |
| const double | mu | ||
| ) | const |
New physics contribution to the neutral-current right-handed coupling \(g_R^f\).
| [in] | f | a lepton or quark |
| [in] | mu | the RG scale to be used in the evaluation (for those models where it is available) |
Definition at line 238 of file NPbase.cpp.
|
inlinevirtual |
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 in NPSMEFTd6, and NPSMEFTd6General.
|
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 in NPSMEFTd6General.
Definition at line 250 of file NPbase.cpp.
|
virtual |
New physics contribution to the neutral-current vector coupling \(g_V^f\).
The neutral-current vector coupling \(g_V^f\) receives the new physics contribution via the oblique parameters \(S\) and \(T\) and the shift in the Fermi constant, \(\Delta G\):
\[ \delta g_V^f = \frac{g_{V,\mathrm{SM}}^f}{2} \left[ \alpha(M_Z^2)\, T - \Delta G \right] + \frac{\big( g_{V,\mathrm{SM}}^f - g_{A,\mathrm{SM}}^f \big) \left[ \alpha(M_Z^2)\left( S - 4\,c_W^2s_W^2\, T \right) + 4\,c_W^2s_W^2\, \Delta G \right]}{4s_W^2\,(c_W^2-s_W^2)}\,. \]
See [Ciuchini:2013pca] and references therein.
| [in] | f | a lepton or quark |
Reimplemented in NPEpsilons_pureNP, NPSTUZbbbarLR, NPZbbbar, NPZbbbarLinearized, NPSMEFTd6, and NPSMEFTd6General.
Definition at line 181 of file NPbase.cpp.
|
inlinevirtual |
|
inlinevirtual |
The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph].
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
virtual |
The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements.
Definition at line 1097 of file NPbase.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 in NPSMEFTd6General.
Definition at line 983 of file NPbase.cpp.
|
virtual |
The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos:
\[ \Delta R_l^{(2)} = \frac{ \Gamma_{had}^{SM}~(\Delta \Gamma_l^{(1)})^2}{(\Gamma_l^{SM})^3} - \frac{\Delta \Gamma_{had}^{(1)}~\Delta \Gamma_l^{(1)}}{(\Gamma_l^{SM})^2} + \frac{ \Gamma_l^{SM} ~\Delta \Gamma_{had}^{(2)} - \Gamma_{had}^{SM} ~\Delta \Gamma_l^{(2)}}{(\Gamma_l^{SM})^2} \]
\[ \Delta R_q^{(2)} = \frac{ \Gamma_{q}^{SM}~(\Delta \Gamma_{had}^{(1)})^2}{(\Gamma_{had}^{SM})^3} - \frac{\Delta \Gamma_q^{(1)}~\Delta \Gamma_{had}^{(1)}}{(\Gamma_{had}^{SM})^2} + \frac{ \Gamma_{had}^{SM} ~\Delta \Gamma_q^{(2)} - \Gamma_q^{SM} ~\Delta \Gamma_{had}^{(2)}}{(\Gamma_{had}^{SM})^2} \]
\[ \Delta R_{\nu}^{(2)} = \frac{ \Gamma_{\nu}^{SM}~(\Delta \Gamma_{had}^{(1)})^2}{(\Gamma_{had}^{SM})^3} - \frac{\Delta \Gamma_{\nu}^{(1)}~\Delta \Gamma_{had}^{(1)}}{(\Gamma_{had}^{SM})^2} + \frac{ \Gamma_{had}^{SM} ~\Delta \Gamma_{\nu}^{(2)} - \Gamma_{\nu}^{SM} ~\Delta \Gamma_{had}^{(2)}}{(\Gamma_{had}^{SM})^2} \]
| f | a lepton or quark |
Definition at line 927 of file NPbase.cpp.
|
virtual |
The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the \(Z\) boson, \(\delta R_{inv}\).
Definition at line 1047 of file NPbase.cpp.
|
virtual |
The new physics contribution to the ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width:
\[ \Delta R_{uc} = \frac{1}{2} \left(\Delta R_u^{(1)} + \Delta R_c^{(1)} \right) \]
Definition at line 434 of file NPbase.cpp.
|
virtual |
The \(\mathcal{O}(1/\Lambda^4)\) new physics contribution to the ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width:
\[ \Delta R_{uc}^{(2)} = \frac{1}{2} \left(\Delta R_u^{(2)} + \Delta R_c^{(2)} \right) \]
Definition at line 418 of file NPbase.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 in NPSMEFTd6General.
Definition at line 608 of file NPbase.cpp.
|
virtual |
The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\Delta \sigma_h^{0,(2)}\).
\(\nc{\MZt}{\widetilde{M}_Z}\)
\[ \Delta\sigma_{h}^{0,(2)} = \frac{12\pi}{\MZt^2} ~\frac{\Gamma_e^{SM} \Gamma_{had}^{SM}}{(\Gamma_Z^{SM})^2} ~ \left( \frac{\Delta\Gamma_e^{(2)}}{\Gamma_e^{SM}} + \frac{\Delta\Gamma_{had}^{(2)}}{\Gamma_{had}^{SM}} - 2 \frac{\Delta\Gamma_Z^{(2)}}{\Gamma_Z^{SM}} + \frac{\Delta\Gamma_e^{(1)} \Delta\Gamma_{had}^{(1)}}{\Gamma_e^{SM} \Gamma_{had}^{SM}} - 2 \frac{\Delta\Gamma_e^{(1)} \Delta\Gamma_Z^{(1)}}{\Gamma_e^{SM} \Gamma_Z^{SM}} - 2 \frac{\Delta\Gamma_{had}^{(1)} \Delta\Gamma_Z^{(1)}}{\Gamma_{had}^{SM} \Gamma_Z^{SM}} + 3 \frac{(\Delta\Gamma_Z^{(1)})^2}{(\Gamma_Z^{SM})^2} \right) \]
Definition at line 552 of file NPbase.cpp.
|
virtual |
The new physics contribution to the effective electron/leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole.
Definition at line 691 of file NPbase.cpp.
|
virtual |
The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the effective electron weak angle \(\Delta \sin^2\theta_{eff,e}^{(2)}\) at the \(Z\) pole.
\(\nc{\gVlSM}{g_{V,e}^{SM}}\) \(\nc{\gAlSM}{g_{A,e}^{SM}}\) \(\nc{\gVlL}{\Delta g_{V,e}^{(1)}}\) \(\nc{\gAlL}{\Delta g_{A,e}^{(1)}}\) \(\nc{\gVlQ}{\Delta g_{V,e}^{(2)}}\) \(\nc{\gAlQ}{\Delta g_{A,e}^{(2)}}\)
\[ \Delta sin^2\theta_{eff,e}^{(2)} = \frac{1}{4}\frac{\gVlL ~\gAlL}{(\gAlSM)^2} -\frac{1}{4}\frac{\gVlSM ~(\gAlL)^2}{(\gAlSM)^3} - \frac{1}{4} \frac{ \gAlSM ~\gVlQ - \gVlSM ~\gAlQ}{(\gAlSM)^2} \]
Definition at line 668 of file NPbase.cpp.
|
virtual |
The new physics contribution to the effective muonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\mu\mu}\) at the \(Z\) pole.
Definition at line 729 of file NPbase.cpp.
|
virtual |
The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the effective muonic weak angle \(\Delta \sin^2\theta_{eff, \mu}^{(2)}\) at the \(Z\) pole.
\(\nc{\gVlSM}{g_{V,\mu}^{SM}}\) \(\nc{\gAlSM}{g_{A,\mu}^{SM}}\) \(\nc{\gVlL}{\Delta g_{V,\mu}^{(1)}}\) \(\nc{\gAlL}{\Delta g_{A,\mu}^{(1)}}\) \(\nc{\gVlQ}{\Delta g_{V,\mu}^{(2)}}\) \(\nc{\gAlQ}{\Delta g_{A,\mu}^{(2)}}\)
\[ \Delta sin^2\theta_{eff,\mu}^{(2)} = \frac{1}{4}\frac{\gVlL ~\gAlL}{(\gAlSM)^2} -\frac{1}{4}\frac{\gVlSM ~(\gAlL)^2}{(\gAlSM)^3} - \frac{1}{4} \frac{ \gAlSM ~\gVlQ - \gVlSM ~\gAlQ}{(\gAlSM)^2} \]
Definition at line 706 of file NPbase.cpp.
|
inlinevirtual |
The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to j j j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.
Definition at line 3258 of file NPbase.h.
|
inlinevirtual |
The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.
|
inlinevirtual |
The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.
|
inlinevirtual |
The new physics contribution to the total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The Higgs-basis coupling \(\delta y_s\). (See LHCHXSWG-INT-2015-001 document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle.
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle.
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1354 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1350 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1330 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1334 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1338 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1346 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1342 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1315 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1303 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1243 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1255 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1267 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1291 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1279 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1237 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1233 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1209 of file NPbase.cpp.
|
virtual |
|
virtual |
Reimplemented from StandardModel.
Definition at line 1225 of file NPbase.cpp.
|
virtual |
|
virtual |
Reimplemented from StandardModel.
Definition at line 1229 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1221 of file NPbase.cpp.
|
virtual |
The total (SM+NP) contribution to the neutral-current axial-vector coupling \(g_A^f\).
| [in] | f | a lepton or quark |
Reimplemented from StandardModel.
Reimplemented in NPEpsilons.
Definition at line 214 of file NPbase.cpp.
|
virtual |
The hadronic decay width of the \(Z\) boson, \(\Gamma_{Z,had}\).
\Gamma_{Z,had} = \Gamma_Z,had}^{SM} + \Delta \Gamma_{Z,had}^{(1)} + \Delta \Gamma_{Z,had}^{(2)}
Reimplemented from StandardModel.
Definition at line 535 of file NPbase.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 StandardModel.
Reimplemented in NPEpsilons, NPSMEFTd6General, and NPZbbbar.
Definition at line 405 of file NPbase.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 in NPSMEFTd6General.
Definition at line 325 of file NPbase.cpp.
|
inlinevirtual |
The ratio of the \(\Gamma(H\to b\bar{b})\) in the current model and in the Standard Model.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the \(\Gamma(H\to c\bar{c})\) in the current model and in the Standard Model.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the \(\Gamma(H\to \mu^+\mu^-)\) in the current model and in the Standard Model.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the \(\Gamma(H\to s\bar{s})\) in the current model and in the Standard Model.
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The ratio of the \(\Gamma(H\to \tau^+\tau^-)\) in the current model and in the Standard Model.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
virtual |
The total width of the \(W\) boson, \(\Gamma_W\).
The \(W\)-boson width receives the new physics contribution via the oblique parameters \(S\), \(T\) and \(U\) and the shift in the Fermi constant, \(\Delta G\):
\[ \Gamma_W = \Gamma_{W,\mathrm{SM}} \left[ 1 - \frac{3\alpha(M_Z^2)}{4(c_W^2-s_W^2)} \left( S - 2c_W^2\,T - \frac{c_W^2-s_W^2}{2s_W^2}\,U \right) - \frac{1+c_W^2}{2(c_W^2-s_W^2)}\, \Delta G \right]. \]
See [Ciuchini:2013pca] and references therein.
Reimplemented from StandardModel.
Reimplemented in NPEpsilons, NPEpsilons_pureNP, NPSMEFTd6, NPSMEFTd6General, NPSTUVWXY, and NPZbbbar.
Definition at line 109 of file NPbase.cpp.
A partial decay width of the \(W\) boson decay into a SM fermion pair.
The partial \(W\)-boson widths receives the new physics contribution via the oblique parameters \(S\), \(T\) and \(U\) and the shift in the Fermi constant, \(\Delta G\):
\[ \Gamma_W^{ij} = \Gamma_{W,\mathrm{SM}} \left[ 1 - \frac{3\alpha(M_Z^2)}{4(c_W^2-s_W^2)} \left( S - 2c_W^2\,T - \frac{c_W^2-s_W^2}{2s_W^2}\,U \right) - \frac{1+c_W^2}{2(c_W^2-s_W^2)}\, \Delta G \right]. \]
| [in] | fi | a lepton or quark |
| [in] | fj | a lepton or quark |
Reimplemented from StandardModel.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 90 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1560 of file NPbase.cpp.
|
inlinevirtual |
A method to return a StandardModel object from NPbase.
Reimplemented from StandardModel.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1545 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1550 of file NPbase.cpp.
|
virtual |
The total (SM+NP) contribution to the neutral-current vector coupling \(g_V^f\).
| [in] | f | a lepton or quark |
Reimplemented from StandardModel.
Reimplemented in NPEpsilons.
Definition at line 198 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1555 of file NPbase.cpp.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The effective coupling \(\kappa_{W4f,eff}=\sqrt{\Gamma_{H4f, CC}/\Gamma_{H4f, CC}^{SM}}\).
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The effective coupling \(\kappa_{Z4f,eff}=\sqrt{\Gamma_{H4f, NC}/\Gamma_{H4f, NC}^{SM}}\).
Reimplemented in NPSMEFTd6General.
|
virtual |
The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions.
| [in] | f | a lepton or quark |
Reimplemented from StandardModel.
Reimplemented in NPEpsilons.
Definition at line 226 of file NPbase.cpp.
|
inlinevirtual |
The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\).
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.)
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
virtual |
Reimplemented from StandardModel.
Reimplemented in NPSTUVWXY.
Definition at line 1411 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Reimplemented in NPSTUVWXY.
Definition at line 1406 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1391 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Reimplemented in NPSTUVWXY.
Definition at line 1396 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Reimplemented in NPSTUVWXY.
Definition at line 1401 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1441 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1449 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1457 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1426 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1431 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1436 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Reimplemented in NPSTUVWXY.
Definition at line 1421 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Reimplemented in NPSTUVWXY.
Definition at line 1416 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Reimplemented in NPSTUVWXY.
Definition at line 1386 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Reimplemented in NPSTUVWXY.
Definition at line 1381 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1361 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Reimplemented in NPSTUVWXY.
Definition at line 1376 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Reimplemented in NPSTUVWXY.
Definition at line 1366 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Reimplemented in NPSTUVWXY.
Definition at line 1371 of file NPbase.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 in NPSMEFTd6General.
|
inlinevirtual |
The ratio \(\mu_{e^+e^- \to He^+e^-}\) between the \( e^+e^- \to H e^+e^- \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, THDMW, THDMWSignalStrengths, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
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 |
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General.
|
inlinevirtual |
The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsChiral, and HiggsKigen.
|
inlinevirtual |
The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
|
inlinevirtual |
|
inlinevirtual |
|
inlinevirtual |
|
inlinevirtual |
The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
|
inlinevirtual |
|
inlinevirtual |
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{\mu\mu H\mu\mu}\) between the \(\sigma(\mu \mu \to H \mu \mu)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model, in the narrow width approximation.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{\mu\mu H\nu\nu}\) between the \(\sigma(\mu \mu \to H \nu \nu)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{\mu\mu ttH}\) between the \(\sigma(\mu \mu \to t\bar{t} H )}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{\mu\mu ZH}\) between the \(\sigma(\mu \mu \to Z H)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, and THDMW.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, and THDMW.
|
inlinevirtual |
The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class.
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General.
|
inlinevirtual |
|
inlinevirtual |
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 in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H\to b\bar{b}\), \(Z\to e^+e^-\) channel channel in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsKigen, NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
|
inlinevirtual |
|
inlinevirtual |
|
inlinevirtual |
|
inlinevirtual |
|
inlinevirtual |
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.
|
inlinevirtual |
|
inlinevirtual |
|
inlinevirtual |
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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
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 in GeorgiMachacek, HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, THDMW, THDMWSignalStrengths, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
inlinevirtual |
Reimplemented in HiggsChiral, HiggsKigen, NPSMEFTd6General, SigmaBR, and NPSMEFTd6.
|
virtual |
The mass of the \(W\) boson, \(M_W\).
The \(W\)-boson mass receives the new physics contribution via the oblique parameters \(S\), \(T\) and \(U\) and the shift in the Fermi constant, \(\Delta G\):
\[ M_W = M_{W,\mathrm{SM}} \left[ 1 - \frac{\alpha(M_Z^2)}{4(c_W^2-s_W^2)} \left( S - 2c_W^2\,T - \frac{c_W^2-s_W^2}{2s_W^2}\,U \right) - \frac{s_W^2}{2(c_W^2-s_W^2)}\,\Delta G \right]. \]
See [Ciuchini:2013pca] and references therein.
Reimplemented from StandardModel.
Reimplemented in GeorgiMachacek, NPEpsilons, NPEpsilons_pureNP, NPSMEFTd6, NPSMEFTd6General, NPZbbbar, and THDMW.
Definition at line 71 of file NPbase.cpp.
|
virtual |
The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\).
Reimplemented from StandardModel.
Definition at line 1147 of file NPbase.cpp.
|
inlinevirtual |
Number of di-electron events at the LHC at 13 TeV.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Number of mono-electron events at the LHC at 13 TeV.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Number of di-muon events at the LHC at 13 TeV.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Number of mono-muon events at the LHC at 13 TeV.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Number of mono-tau events at the LHC at 13 TeV.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
Number of di-tau events at the LHC at 13 TeV.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The oblique parameter \(S\).
Reimplemented in HiggsChiral, HiggsKigen, NPHiggs, NPSMEFTd6, NPSMEFTd6General, NPSTU, and NPSTUVWXY.
|
inlinevirtual |
The oblique parameter \(T\).
Reimplemented in HiggsChiral, HiggsKigen, NPHiggs, NPSMEFTd6, NPSMEFTd6General, NPSTU, and NPSTUVWXY.
|
inlinevirtual |
The oblique parameter \(U\).
Reimplemented in HiggsChiral, HiggsKigen, NPHiggs, NPSMEFTd6, NPSMEFTd6General, NPSTU, and NPSTUVWXY.
|
inlinevirtual |
The oblique parameter \(W\).
Reimplemented in NPSMEFTd6, NPSMEFTd6General, and NPSTUVWXY.
|
inlinevirtual |
The oblique parameter \(Y\).
Reimplemented in NPSMEFTd6, NPSMEFTd6General, and NPSTUVWXY.
|
virtual |
Reimplemented in NPSMEFTd6.
Definition at line 42 of file NPbase.cpp.
|
inlinevirtual |
The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class.
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1525 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1540 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1535 of file NPbase.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 StandardModel.
Reimplemented in NPSMEFTd6General, NPZbbbar, and NPEpsilons.
Definition at line 1034 of file NPbase.cpp.
|
virtual |
The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\).
Reimplemented from StandardModel.
Definition at line 1091 of file NPbase.cpp.
|
virtual |
The effective neutral-current coupling \(\rho_Z^f\) including SM plus NP contributions.
| [in] | f | a lepton or quark |
Reimplemented from StandardModel.
Reimplemented in NPEpsilons.
Definition at line 220 of file NPbase.cpp.
|
virtual |
The ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width.
Reimplemented from StandardModel.
Definition at line 450 of file NPbase.cpp.
|
virtual |
The ratio \(R_{W,c)=\Gamma(W\to c + X)/\Gamma(W\to had)\).
Reimplemented from StandardModel.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 162 of file NPbase.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 StandardModel.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 137 of file NPbase.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 StandardModel.
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
Definition at line 461 of file NPbase.cpp.
|
inlinevirtual |
A method to set a flag of NPbase.
| [in] | name | name of a model flag |
| [in] | value | the boolean to be assigned to the flag specified by name |
Reimplemented from StandardModel.
Reimplemented in HiggsChiral, HiggsKigen, NPd6SILH, NPEpsilons, NPSMEFTd6, NPSMEFTd6General, GeorgiMachacek, and NPSMEFT6dtopquark.
Definition at line 97 of file NPbase.h.
|
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 StandardModel.
Reimplemented in NPEpsilons, NPSMEFTd6General, and NPZbbbar.
Definition at line 655 of file NPbase.cpp.
|
virtual |
Reimplemented in NPSMEFTd6.
Definition at line 1186 of file NPbase.cpp.
|
virtual |
The leptonic effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\rm lept}\) at the the \(Z\) pole.
\[ \sin^2\theta_{eff} = \sin^2\theta_{eff}^{SM} + \Delta \sin^2\theta_{eff}^{(1)} + \Delta \sin^2\theta_{eff}^{(2)} \]
| [in] | f | a lepton or quark |
Reimplemented from StandardModel.
Reimplemented in NPZbbbar, and NPEpsilons.
Definition at line 744 of file NPbase.cpp.
|
inlinevirtual |
The STXS0 bin \(pp \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS BR \( H \to 4l \), \(l=e,\mu\).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The STXS BR \( H \to bb \).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The STXS BR \( H \to e\nu \mu\nu \).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
The STXS BR \( H \to \gamma \gamma \).
Reimplemented in NPSMEFTd6, and NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\), \(N_j=0,~p_{TH} [GeV]<10\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\), \(N_j = 1,~p_{TH} [GeV]<60\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\), \(N_j = 0, 10<~p_{TH} [GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The STXS bin \(gg \to H\), \(N_j=0,~10<p_{TH} [GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\), \(~200<p_{TH} [GeV]<300\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\), \(~300<p_{TH} [GeV]<450\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\), \(450<~p_{TH} [GeV]<650\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\), \(~p_{TH} [GeV]>450\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\), \(~p_{TH} [GeV]>650\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\ell\ell\), \(p_{TV}[GeV]<75\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\ell\ell\), \(250 < p_{TV}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\ell\ell\), \(75<p_{TV}[GeV]<150\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H\ell\ell\), \(0<p_{TV}<150[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The STXS bin \(qq \to H\ell\ell\), \(p_{TV}[GeV]<75\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}<400[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H\ell\ell\), \(400<p_{TV}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The STXS bin \(qq \to H\ell\ell\), \(75<p_{TV}[GeV]<150\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H\ell\nu\), \(0<p_{TV}<150[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The STXS bin \(qq \to H\ell\nu\), \(p_{TV}[GeV]<75\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}<400[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H\ell\nu\), \(400<p_{TV}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The STXS bin \(qq \to H\ell\nu\), \(75<p_{TV}[GeV]<150\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to Hqq\), \(N_j = 0\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to Hqq\), \(N_j = 1\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
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 in NPSMEFTd6General.
|
inlinevirtual |
The STXS bin \(pp \to tH\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(pp \to ttH\), \(p_{TH}[GeV]<60\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(pp \to ttH\), \(120<p_{TH}[GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(pp \to ttH\), \(200<p_{TH}[GeV]<300\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]<450\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(pp \to ttH\), \(450<p_{TH}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General.
|
inlinevirtual |
The STXS bin \(pp \to ttH\), \(60<p_{TH}[GeV]<120\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \( ttH + tH \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1596 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1606 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1601 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1616 of file NPbase.cpp.
|
virtual |
Reimplemented from StandardModel.
Definition at line 1611 of file NPbase.cpp.
|
virtual |
The update method for NPbase.
Reimplemented from StandardModel.
Reimplemented in GeorgiMachacek, and THDMW.
Definition at line 36 of file NPbase.cpp.
|
inlinevirtual |
Reimplemented in HiggsChiral.
|
inlinevirtual |
Reimplemented in HiggsChiral.
|
inlinevirtual |
Reimplemented in HiggsChiral.
|
inlinevirtual |
Reimplemented in HiggsChiral.
|
inlinevirtual |
Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\).
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
|
inlinevirtual |
The cross section in pb for \(e^+ e^- \to W^+ W^- \to j j j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.
Definition at line 3247 of file NPbase.h.
|
inlinevirtual |
The cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.
|
inlinevirtual |
The cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.
|
inlinevirtual |
The total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class.
Reimplemented in NPSMEFTd6General, and NPSMEFTd6.
| double NPbase::C1Hmumu = 0.0 |
| double NPbase::C1HZga = 0.0 |
|
protected |
1.9.2 