|
| | NPSMEFTd6U2 () |
| |
| virtual bool | PostUpdate () |
| | The post-update method for NPSMEFTd6General. More...
|
| |
| virtual const double | A_f (const Particle f) const |
| | The left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\mathcal{A}_f\). More...
|
| |
| virtual const double | AFB (const Particle f) const |
| | The forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(A^f_{FB}\). More...
|
| |
| virtual const double | alphaMz () const |
| | The electromagnetic coupling at the \(Z\)-mass scale. More...
|
| |
| virtual const double | aPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More...
|
| |
| virtual const double | bPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More...
|
| |
| virtual const double | Br_H_exo () const |
| | The branching ratio of the of the Higgs into exotic particles. More...
|
| |
| virtual const double | Br_H_inv () const |
| | The branching ratio of the of the Higgs into invisible particles. More...
|
| |
| virtual const double | Br_H_inv_NP () const |
| | The branching ratio of the of the Higgs into invisible particles (only invisible new particles). More...
|
| |
| virtual const double | BrH2d2dRatio () const |
| | The ratio of the Br \((H\to 2d2d)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2e2muRatio () const |
| | The ratio of the Br \((H\to 2e 2\mu)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2e2vRatio () const |
| | The ratio of the Br \((H\to 2e2v)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2evRatio () const |
| | The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2L2dRatio () const |
| | The ratio of the Br \((H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2L2LRatio () const |
| | The ratio of the Br \((H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2L2uRatio () const |
| | The ratio of the Br \((H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2L2v2Ratio () const |
| | The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2L2vRatio () const |
| | The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2l2vRatio () const |
| | The ratio of the Br \((H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2Lv2Ratio () const |
| | The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2LvRatio () const |
| | The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2mu2vRatio () const |
| | The ratio of the Br \((H\to 2\mu 2v)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2muvRatio () const |
| | The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2u2dRatio () const |
| | The ratio of the Br \((H\to 2u2d)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2u2uRatio () const |
| | The ratio of the Br \((H\to 2u2u)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2udRatio () const |
| | The ratio of the Br \((H\to 2ud)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2v2dRatio () const |
| | The ratio of the Br \((H\to 2v2d)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2v2uRatio () const |
| | The ratio of the Br \((H\to 2v2u)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH2v2vRatio () const |
| | The ratio of the Br \((H\to 2v2v)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH4dRatio () const |
| | The ratio of the Br \((H\to 4d)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH4eRatio () const |
| | The ratio of the Br \((H\to 4e)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH4fCCRatio () const |
| | The ratio of the Br \((H\to 4f, CC)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH4fNCRatio () const |
| | The ratio of the Br \((H\to 4f, NC)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH4fRatio () const |
| | The ratio of the Br \((H\to 4f)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH4L2Ratio () const |
| | The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH4LRatio () const |
| | The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH4lRatio () const |
| | The ratio of the Br \((H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH4muRatio () const |
| | The ratio of the Br \((H\to 4\mu)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH4uRatio () const |
| | The ratio of the Br \((H\to 4u)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrH4vRatio () const |
| | The ratio of the Br \((H\to 4v)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHbbRatio () const |
| | The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHccRatio () const |
| | The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHevmuvRatio () const |
| | The ratio of the Br \((H\to e\nu \mu\nu)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHgagaRatio () const |
| | The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHggRatio () const |
| | The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHll_vvorjjRatio () const |
| | The ratio of the Br \((H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHlv_lvorjjRatio () const |
| | The ratio of the Br \((H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHlvjjRatio () const |
| | The ratio of the Br \((H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHLvudRatio () const |
| | The ratio of the Br \((H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHLvvLRatio () const |
| | The ratio of the Br \((H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHmumuRatio () const |
| | The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHssRatio () const |
| | The ratio of the Br \((H\to s\bar{s})\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHtautauRatio () const |
| | The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHtoinvRatio () const |
| | The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHudduRatio () const |
| | The ratio of the Br \((H\to uddu)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHvisRatio () const |
| | The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHVVRatio () const |
| | The ratio of the Br \((H\to VV)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHWffRatio () const |
| | The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHWjjRatio () const |
| | The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHWlvRatio () const |
| | The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHWW2l2vRatio () const |
| | The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHWW4fRatio () const |
| | The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHWW4jRatio () const |
| | The ratio of the Br \((H\to WW^*\to 4j)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHWWRatio () const |
| | The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZddRatio () const |
| | The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZffRatio () const |
| | The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZgaeeRatio () const |
| | The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZgallRatio () const |
| | The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZgamumuRatio () const |
| | The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZgaRatio () const |
| | The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZllRatio () const |
| | The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZuuRatio () const |
| | The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZvvRatio () const |
| | The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZZ2e2muRatio () const |
| | The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZZ4dRatio () const |
| | The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZZ4eRatio () const |
| | The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZZ4fRatio () const |
| | The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZZ4lRatio () const |
| | The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZZ4muRatio () const |
| | The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZZ4uRatio () const |
| | The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZZ4vRatio () const |
| | The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrHZZRatio () const |
| | The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | BrW (const Particle fi, const Particle fj) const |
| | The branching ratio of the \(W\) boson decaying into a SM fermion pair, \(Br(W\to f_i f_j)\). More...
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| virtual const double | cbW_TWG (const double mu) const |
| |
| const double | CeeLL_bottom (const double mu) const |
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| const double | CeeLL_charm (const double mu) const |
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| const double | CeeLL_down (const double mu) const |
| |
| const double | CeeLL_e (const double mu) const |
| |
| const double | CeeLL_mu (const double mu) const |
| |
| const double | CeeLL_strange (const double mu) const |
| |
| const double | CeeLL_tau (const double mu) const |
| |
| const double | CeeLL_top (const double mu) const |
| |
| const double | CeeLL_up (const double mu) const |
| |
| const double | CeeLR_bottom (const double mu) const |
| |
| const double | CeeLR_charm (const double mu) const |
| |
| const double | CeeLR_down (const double mu) const |
| |
| const double | CeeLR_e (const double mu) const |
| |
| const double | CeeLR_mu (const double mu) const |
| |
| const double | CeeLR_strange (const double mu) const |
| |
| const double | CeeLR_tau (const double mu) const |
| |
| const double | CeeLR_top (const double mu) const |
| |
| const double | CeeLR_up (const double mu) const |
| |
| const double | CeeRL_bottom (const double mu) const |
| |
| const double | CeeRL_charm (const double mu) const |
| |
| const double | CeeRL_down (const double mu) const |
| |
| const double | CeeRL_e (const double mu) const |
| |
| const double | CeeRL_mu (const double mu) const |
| |
| const double | CeeRL_strange (const double mu) const |
| |
| const double | CeeRL_tau (const double mu) const |
| |
| const double | CeeRL_top (const double mu) const |
| |
| const double | CeeRL_up (const double mu) const |
| |
| const double | CeeRR_bottom (const double mu) const |
| |
| const double | CeeRR_charm (const double mu) const |
| |
| const double | CeeRR_down (const double mu) const |
| |
| const double | CeeRR_e (const double mu) const |
| |
| const double | CeeRR_mu (const double mu) const |
| |
| const double | CeeRR_strange (const double mu) const |
| |
| const double | CeeRR_tau (const double mu) const |
| |
| const double | CeeRR_top (const double mu) const |
| |
| const double | CeeRR_up (const double mu) const |
| |
| virtual const double | CEWHd11 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{11}\). More...
|
| |
| virtual const double | CEWHd22 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{22}\). More...
|
| |
| virtual const double | CEWHd33 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{33}\). More...
|
| |
| virtual const double | CEWHe11 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{11}\). More...
|
| |
| virtual const double | CEWHe22 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{22}\). More...
|
| |
| virtual const double | CEWHe33 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{33}\). More...
|
| |
| virtual const double | CEWHL111 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{11}\). More...
|
| |
| virtual const double | CEWHL122 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{22}\). More...
|
| |
| virtual const double | CEWHL133 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{33}\). More...
|
| |
| virtual const double | CEWHL311 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{11}\). More...
|
| |
| virtual const double | CEWHL322 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{22}\). More...
|
| |
| virtual const double | CEWHL333 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{33}\). More...
|
| |
| virtual const double | CEWHQ111 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{11}\). More...
|
| |
| virtual const double | CEWHQ122 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{22}\). More...
|
| |
| virtual const double | CEWHQ133 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{33}\). More...
|
| |
| virtual const double | CEWHQ311 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{11}\). More...
|
| |
| virtual const double | CEWHQ322 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{22}\). More...
|
| |
| virtual const double | CEWHQ333 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{33}\). More...
|
| |
| virtual const double | CEWHQd33 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(d)})_{33}\). More...
|
| |
| virtual const double | CEWHQu33 (const double mu) const |
| | Combination of coefficients of the Warsaw basis not constrained by EWPO (at LO) \((\hat{C}_{HQ}^{(u)})_{33}\). More...
|
| |
| virtual const double | CEWHu11 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{11}\). More...
|
| |
| virtual const double | CEWHu22 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{22}\). More...
|
| |
| virtual const double | CEWHu33 (const double mu) const |
| | Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{33}\). More...
|
| |
| virtual const double | cgaga_HB (const double mu) const |
| | The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
|
| |
| virtual const double | cgg_HB (const double mu) const |
| | The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
|
| |
| virtual const double | cggEff_HB (const double mu) const |
| | The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
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| |
| virtual const double | cHb_TWG (const double mu) const |
| |
| virtual const double | cHQ3_TWG (const double mu) const |
| |
| virtual const double | cHQm_TWG (const double mu) const |
| |
| virtual const double | cHQp_TWG (const double mu) const |
| |
| virtual const double | cHt_TWG (const double mu) const |
| |
| virtual const double | cHtb_TWG (const double mu) const |
| |
| virtual const double | computeGammaTotalRatio () const |
| | The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | cQd1_TWG (const double mu) const |
| |
| virtual const double | cQd8_TWG (const double mu) const |
| |
| virtual const double | cQe_TWG (const double mu) const |
| |
| virtual const double | cQl3_TWG (const double mu) const |
| |
| virtual const double | cQlM_TWG (const double mu) const |
| |
| virtual const double | cQlP_TWG (const double mu) const |
| |
| virtual const double | cQq11_TWG (const double mu) const |
| |
| virtual const double | cQq18_TWG (const double mu) const |
| |
| virtual const double | cQQ1_TWG (const double mu) const |
| |
| virtual const double | cQq31_TWG (const double mu) const |
| |
| virtual const double | cQq38_TWG (const double mu) const |
| |
| virtual const double | cQQ8_TWG (const double mu) const |
| |
| virtual const double | cQt1_TWG (const double mu) const |
| |
| virtual const double | cQt8_TWG (const double mu) const |
| |
| virtual const double | cQu1_TWG (const double mu) const |
| |
| virtual const double | cQu8_TWG (const double mu) const |
| |
| virtual const double | ctd1_TWG (const double mu) const |
| |
| virtual const double | ctd8_TWG (const double mu) const |
| |
| virtual const double | cte_TWG (const double mu) const |
| |
| virtual const double | ctG_TWG (const double mu) const |
| |
| virtual const double | ctH_TWG (const double mu) const |
| |
| virtual const double | ctl_TWG (const double mu) const |
| |
| virtual const double | ctlS_TWG (const double mu) const |
| |
| virtual const double | ctlT_TWG (const double mu) const |
| |
| virtual const double | ctq1_TWG (const double mu) const |
| |
| virtual const double | ctq8_TWG (const double mu) const |
| |
| virtual const double | ctt1_TWG (const double mu) const |
| |
| virtual const double | ctu1_TWG (const double mu) const |
| |
| virtual const double | ctu8_TWG (const double mu) const |
| |
| virtual const double | ctW_TWG (const double mu) const |
| |
| virtual const double | ctZ_TWG (const double mu) const |
| |
| virtual const double | cZBox_HB (const double mu) const |
| | The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
|
| |
| virtual const double | cZga_HB (const double mu) const |
| | The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
|
| |
| virtual const double | cZZ_HB (const double mu) const |
| | The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
|
| |
| virtual const double | del_A_mu (const double mu) const |
| | Correction to photon WF. More...
|
| |
| virtual const double | del_e_mu (const double mu) const |
| | Correction to electric charge. More...
|
| |
| virtual const double | del_sW2_mu (const double mu) const |
| | Correction to (sin squared of) weak mixing angle. More...
|
| |
| virtual const double | del_Z_mu (const double mu) const |
| | Correction to Z WF. More...
|
| |
| virtual const double | del_ZA_mu (const double mu) const |
| | Correction to Z-A mixing. More...
|
| |
| virtual const double | delQ_gNC (const double mu) const |
| | Separate, charge-proportional, indirect correction to EW neutral currents. More...
|
| |
| virtual const double | delta2sBRH3 (const double C1prod, const double C1Hxx) const |
| | Quadratic contribution from the Higgs self-couplings modifications to the signal strength for \(\sigma \times BR(H\to xx)\) in the current model. More...
|
| |
| virtual const double | delta2sH3 (const double C1) const |
| | Quadratic contribution from the Higgs self-couplings modifications to the signal strength for an observable \(\sigma\) in the current model. More...
|
| |
| virtual const double | delta_AFB_ee (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | delta_AFB_f (const Particle f, const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | delta_alrmoller (const double q2, const double y) const |
| | The computation of the parity violating asymmetry in Moller scattering. More...
|
| |
| virtual const double | delta_amuon () const |
| | The computation of the anomalous magnetic moment of the muon \(a_\mu=(g_\mu-2)/2\). More...
|
| |
| virtual const double | delta_Dsigma_f (const Particle f, const double pol_e, const double pol_p, const double s, const double cos) const |
| |
| virtual const double | delta_gAnue () const |
| | The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gAnue. More...
|
| |
| virtual const double | delta_gLnuN2 () const |
| | The computation of the correction to the effective neutrino nucleon LH coupling: delta_gLnuN2. More...
|
| |
| virtual const double | delta_gRnuN2 () const |
| | The computation of the correction to the effective neutrino nucleon RH coupling: delta_gRnuN2. More...
|
| |
| virtual const double | delta_gVnue () const |
| | The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gVnue. More...
|
| |
| virtual const double | delta_mubbH_1 (const double sqrt_s) const |
| | The SMEFT linear correction to the ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_mubbH_2 (const double sqrt_s) const |
| | The SMEFT quadratic correction to the ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_muggH_1 (const double sqrt_s) const |
| | The SMEFT linear correction to the ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_muggH_2 (const double sqrt_s) const |
| | The SMEFT quadratic correction to the ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_mutH_1 (const double sqrt_s) const |
| | The SMEFT linear correction to the ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_mutH_2 (const double sqrt_s) const |
| | The SMEFT quadratic correction to the ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_muttH_1 (const double sqrt_s) const |
| | The SMEFT linear correction to the ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_muttH_2 (const double sqrt_s) const |
| | The SMEFT quadratic correction to the ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_muVBF_1 (const double sqrt_s) const |
| | The SMEFT linear correction to the ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_muVBF_2 (const double sqrt_s) const |
| | The SMEFT quadratic correction to the ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_muVH_1 (const double sqrt_s) const |
| | The SMEFT linear correction to the ratio \(\mu_{VH}\) between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_muVH_2 (const double sqrt_s) const |
| | The SMEFT quadratic correction to the ratio \(\mu_{VH}\) between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_muWH_1 (const double sqrt_s) const |
| | The SMEFT linear correction to the ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_muWH_2 (const double sqrt_s) const |
| | The SMEFT quadratic correction to the ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_muZH_1 (const double sqrt_s) const |
| | The SMEFT linear correction to the ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_muZH_2 (const double sqrt_s) const |
| | The SMEFT quadratic correction to the ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | delta_Qwemoller (const double q2, const double y) const |
| | The computation of the electron's weak charge. More...
|
| |
| virtual const double | delta_Qwn () const |
| | The computation of the neutron weak charge: Qwn. More...
|
| |
| virtual const double | delta_Qwp () const |
| | The computation of the proton weak charge: Qwp. More...
|
| |
| virtual const double | delta_sigma_ee (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| |
| virtual const double | delta_sigma_f (const Particle f, const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| |
| virtual const double | delta_sigma_had (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| |
| virtual const double | delta_sigmaTot_ee (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | delta_sigmaTot_f (const Particle f, const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | delta_TauLFU_gmuge () const |
| | The computation of the correction to the LFU ratio \(g_\mu/ g_e \). More...
|
| |
| virtual const double | delta_TauLFU_gtauge () const |
| | The computation of the correction to the LFU ratio \(g_\tau/ g_e \). More...
|
| |
| virtual const double | delta_TauLFU_gtaugmu () const |
| | The computation of the correction to the LFU ratio \(g_\tau/ g_\mu \). More...
|
| |
| virtual const double | delta_TauLFU_gtaugmuK () const |
| | The computation of the correction to the LFU ratio \(\left(g_\tau/ g_\mu\right)_K \). More...
|
| |
| virtual const double | delta_TauLFU_gtaugmuPi () const |
| | The computation of the correction to the LFU ratio \(\left(g_\tau/ g_\mu\right)_\pi \). More...
|
| |
| virtual const double | deltaa0 () const |
| | The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltaa02 () const |
| | The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltaA_f (const Particle f) const |
| | The new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta \mathcal{A}_f\). More...
|
| |
| virtual const double | deltaAFB (const Particle f) const |
| | The new physics contribution to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta A^f_{FB}\). More...
|
| |
| virtual const double | deltaaMZ () const |
| | The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltaaMZ2 () const |
| | The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltaaSMZ () const |
| | The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltaaSMZ2 () const |
| | The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltacZ_HB (const double mu) const |
| | The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
|
| |
| virtual const double | deltadxsdcoseeWWlvjjLEP2 (const double sqrt_s, const int bin) const |
| | The new physics contribution to the differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph]. More...
|
| |
| virtual const double | deltaeNP (const double mu) const |
| | The new physics relative contribution to the EW coupling constant \(e\). More...
|
| |
| virtual const double | deltaG1_hWW () const |
| | The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More...
|
| |
| virtual const double | deltaG1_hWW_mu (const double mu) const |
| | The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More...
|
| |
| virtual const double | deltaG1_hZA () const |
| | The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More...
|
| |
| virtual const double | deltaG1_hZA_mu (const double mu) const |
| | The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More...
|
| |
| virtual const double | deltaG1_hZARatio () const |
| | The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
|
| |
| virtual const double | deltaG1_hZARatio_mu (const double mu) const |
| | The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
|
| |
| virtual const double | deltaG1_hZZ () const |
| | The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More...
|
| |
| virtual const double | deltaG1_hZZ_mu (const double mu) const |
| | The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More...
|
| |
| virtual const double | deltag1gaNP (const double mu) const |
| | The new physics contribution to the anomalous triple gauge coupling \(g_{1,\gamma}\). More...
|
| |
| virtual const double | deltag1ZNP (const double mu) const |
| | The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More...
|
| |
| virtual const double | deltag1ZNPEff () const |
| | The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More...
|
| |
| virtual const double | deltaG2_hWW () const |
| | The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More...
|
| |
| virtual const double | deltaG2_hWW_mu (const double mu) const |
| | The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More...
|
| |
| virtual const double | deltaG2_hZA () const |
| | The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More...
|
| |
| virtual const double | deltaG2_hZA_mu (const double mu) const |
| | The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More...
|
| |
| virtual const double | deltaG2_hZZ () const |
| | The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More...
|
| |
| virtual const double | deltaG2_hZZ_mu (const double mu) const |
| | The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More...
|
| |
| virtual const double | deltaG3_hWW () const |
| | The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More...
|
| |
| virtual const double | deltaG3_hWW_mu (const double mu) const |
| | The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More...
|
| |
| virtual const double | deltaG3_hZZ () const |
| | The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More...
|
| |
| virtual const double | deltaG3_hZZ_mu (const double mu) const |
| | The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More...
|
| |
| const double | deltag3G () const |
| | The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\). More...
|
| |
| gslpp::complex | deltaG_Aff (const Particle p) const |
| | The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). More...
|
| |
| gslpp::complex | deltaG_Gff (const Particle p) const |
| | The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu}^A \bar{f}\sigma^{\mu\nu} T_A f\). More...
|
| |
| virtual const double | deltaG_hAA () const |
| | The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More...
|
| |
| virtual const double | deltaG_hAA_mu (const double mu) const |
| | The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More...
|
| |
| virtual const double | deltaG_hAARatio () const |
| | The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
|
| |
| virtual const double | deltaG_hAARatio_mu (const double mu) const |
| | The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
|
| |
| gslpp::complex | deltaG_hAff (const Particle p) const |
| | The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). More...
|
| |
| virtual gslpp::complex | deltaG_hff (const Particle p) const |
| | The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More...
|
| |
| virtual gslpp::complex | deltaG_hff_mu (const Particle p, const double mu) const |
| | The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More...
|
| |
| gslpp::complex | deltaG_hGff (const Particle p) const |
| | The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). More...
|
| |
| virtual const double | deltaG_hgg () const |
| | The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More...
|
| |
| virtual const double | deltaG_hgg_mu (const double mu) const |
| | The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More...
|
| |
| virtual const double | deltaG_hggRatio () const |
| | The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
|
| |
| virtual const double | deltaG_hggRatio_mu (const double mu) const |
| | The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
|
| |
| virtual const double | deltaG_hhhRatio () const |
| | The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More...
|
| |
| virtual const double | deltaG_hhhRatio_mu (const double mu) const |
| | The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More...
|
| |
| gslpp::complex | deltaG_hZff (const Particle p) const |
| | The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). More...
|
| |
| gslpp::complex | deltaG_Zff (const Particle p) const |
| | The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). More...
|
| |
| virtual const double | deltaGA_f (const Particle p) const |
| | New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More...
|
| |
| virtual const double | deltaGamma_W () const |
| | The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\). More...
|
| |
| virtual const double | deltaGamma_Wff (const Particle fi, const Particle fj) const |
| | The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More...
|
| |
| virtual const double | deltaGamma_Z () const |
| | The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\). More...
|
| |
| virtual const double | deltaGamma_Zf (const Particle f) const |
| | The new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More...
|
| |
| const double | deltaGammaH2d2dRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaH2d2dRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaH2e2muRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaH2e2muRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaH2e2vRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaH2e2vRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaH2evRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaH2evRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaH2L2dRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaH2L2dRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaH2L2LRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaH2L2LRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaH2L2uRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2L2uRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2L2v2Ratio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2L2v2Ratio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2L2vRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2l2vRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2L2vRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2l2vRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2Lv2Ratio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2Lv2Ratio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2LvRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2LvRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2mu2vRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2mu2vRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2muvRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2muvRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2u2dRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2u2dRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2u2uRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2u2uRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2udRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2udRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2v2dRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2v2dRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2v2uRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2v2uRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2v2vRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH2v2vRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4dRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4dRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4eRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4eRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4fCCRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4f, CC)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4fCCRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4f, CC)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4fNCRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4f, NC)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4fNCRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4f, NC)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4fRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4fRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4L2Ratio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4L2Ratio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4LRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4lRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4LRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4lRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4muRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4muRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4uRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4uRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4vRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaH4vRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHbbRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHbbRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHccRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHccRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHevmuvRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHevmuvRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHffRatio1 (const double mf, const double CifH) const |
| | The ratio of the \(\Gamma(H\to ff)\) in the current model and in the Standard Model. More...
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| const double | deltaGammaHffRatio2 (const double mf, const double CifH) const |
| | The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the ratio of the \(\Gamma(H\to ff)\) in the current model and in the Standard Model at order Lambd. More...
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| const double | deltaGammaHgagaRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHgagaRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHggRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...
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| const double | deltaGammaHggRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHll_vvorjjRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHll_vvorjjRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHlv_lvorjjRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHlv_lvorjjRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHlvjjRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHlvjjRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHLvudRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHLvudRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHLvvLRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHLvvLRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHmumuRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHmumuRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHssRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ss)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHssRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ss)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHtautauRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHtautauRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHudduRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHudduRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWffRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWffRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWjjRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWjjRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWlvRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWlvRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWW2l2vRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWW2l2vRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWW4fRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWW4fRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWW4jRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWW4jRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWWRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHWWRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHZddRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHZddRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHZeeRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHZeeRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHZffRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHZffRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHZgaRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHZgaRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHZllRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHZllRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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| const double | deltaGammaHZmumuRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
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| |
| const double | deltaGammaHZmumuRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZuuRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZuuRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZvvRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZvvRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ2e2muRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ2e2muRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4dRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4dRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4eRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4eRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4fRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4fRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4lRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4lRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4muRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4muRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4uRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4uRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4vRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZ4vRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
|
| |
| const double | deltaGammaHZZRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
|
| |
| virtual const double | deltaGammaTotalRatio1 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...
|
| |
| virtual const double | deltaGammaTotalRatio1noError () const |
| | The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors. More...
|
| |
| virtual const double | deltaGammaTotalRatio2 () const |
| | The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients. More...
|
| |
| virtual const double | DeltaGF () const |
| | New physics contribution to the Fermi constant. More...
|
| |
| const double | deltaGL_f (const Particle p) const |
| | New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More...
|
| |
| const double | deltaGL_f_mu (const Particle p, const double mu) const |
| | New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More...
|
| |
| virtual gslpp::complex | deltaGL_Wff (const Particle pbar, const Particle p) const |
| | New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More...
|
| |
| virtual gslpp::complex | deltaGL_Wff_mu (const Particle pbar, const Particle p, const double mu) const |
| | New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More...
|
| |
| gslpp::complex | deltaGL_Wffh (const Particle pbar, const Particle p) const |
| | The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\). More...
|
| |
| const double | deltaGL_Zffh (const Particle p) const |
| | The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\). More...
|
| |
| virtual const double | deltaGmu () const |
| | The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltaGmu2 () const |
| | The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| const double | deltaGR_f (const Particle p) const |
| | New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More...
|
| |
| const double | deltaGR_f_mu (const Particle p, const double mu) const |
| | New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More...
|
| |
| virtual gslpp::complex | deltaGR_Wff (const Particle pbar, const Particle p) const |
| | New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More...
|
| |
| virtual gslpp::complex | deltaGR_Wff_mu (const Particle pbar, const Particle p, const double mu) const |
| | New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More...
|
| |
| gslpp::complex | deltaGR_Wffh (const Particle pbar, const Particle p) const |
| | The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\). More...
|
| |
| const double | deltaGR_Zffh (const Particle p) const |
| | The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\). More...
|
| |
| virtual const double | deltaGV_f (const Particle p) const |
| | New physics contribution to the neutral-current vector coupling \(g_V^f\). More...
|
| |
| virtual const double | deltaGwd6 () const |
| | The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\). More...
|
| |
| virtual const double | deltaGwd62 () const |
| | The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\). More...
|
| |
| virtual const double | deltaGzd6 () const |
| | The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\). More...
|
| |
| virtual const double | deltaGzd62 () const |
| | The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\). More...
|
| |
| virtual const double | deltaH3L1 (double C1) const |
| | The coefficient of the 1-loop linear term in the Higgs selfcoupling. More...
|
| |
| virtual const double | deltaH3L2 (double C1) const |
| | The coefficient of the 1-loop quadratic term in the Higgs selfcoupling. More...
|
| |
| virtual const double | deltaKgammaNP (const double mu) const |
| | The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\). More...
|
| |
| virtual const double | deltaKgammaNPEff () const |
| | The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More...
|
| |
| virtual const double | deltaKZNP (const double mu) const |
| | The new physics contribution to the anomalous triple gauge coupling \(\kappa_{Z}\). More...
|
| |
| virtual const double | deltamb () const |
| | The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltamb2 () const |
| | The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltamc () const |
| | The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltamc2 () const |
| | The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltaMh () const |
| | The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltaMh2 () const |
| | The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| const double | deltaMLL2_f (const Particle f, const double s, const double t) const |
| |
| const double | deltaMLR2_f (const Particle f, const double s) const |
| |
| const double | deltaMLR2t_e (const double s, const double t) const |
| |
| const double | deltaMRL2_f (const Particle f, const double s) const |
| |
| const double | deltaMRL2t_e (const double s, const double t) const |
| |
| const double | deltaMRR2_f (const Particle f, const double s, const double t) const |
| |
| virtual const double | deltamt () const |
| | The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltamt2 () const |
| | The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltamtau () const |
| | The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltamtau2 () const |
| | The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltaMw () const |
| | The relative correction to the mass of the \(W\) boson, \(\delta M_W/M_W\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltaMw2 () const |
| | The relative correction to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltaMwd6 () const |
| | The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\). More...
|
| |
| virtual const double | deltaMwd62 () const |
| | The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\). More...
|
| |
| virtual const double | deltaMz () const |
| | The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | deltaMz2 () const |
| | The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
|
| |
| virtual const double | DeltaOalphtoW (const double dOSMdalpha, const double mu) const |
| | Difference in prediction in \(\alpha\) scheme and W mass scheme, computed from observable in \(\alpha\) scheme. Difference at tree level. More...
|
| |
| virtual const double | DeltaOWtoalph (const double dOSMdMW, const double mu) const |
| | Difference in prediction in \(\alpha\) scheme and W mass scheme, computed from observable in W mass scheme. Difference at tree level. More...
|
| |
| virtual const double | deltaR0_f (const Particle f) const |
| | The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More...
|
| |
| virtual const double | deltaSigmaHadron () const |
| | The new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\delta \sigma_h^0\). More...
|
| |
| virtual const double | deltaxseeWW4fLEP2 (const double sqrt_s, const int fstate) const |
| | The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More...
|
| |
| virtual const double | deltaxseeWWtotLEP2 (const double sqrt_s) const |
| | The new physics contribution to the total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More...
|
| |
| virtual const double | deltayb_HB (const double mu) const |
| | The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
|
| |
| virtual const double | deltayc_HB (const double mu) const |
| | The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
|
| |
| virtual const double | deltaymu_HB (const double mu) const |
| | The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
|
| |
| virtual const double | deltays_HB (const double mu) const |
| | The Higgs-basis coupling \(\delta y_s\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
|
| |
| virtual const double | deltayt_HB (const double mu) const |
| | The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
|
| |
| virtual const double | deltaytau_HB (const double mu) const |
| | The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
|
| |
| virtual const double | delU_gCC (const double mu) const |
| | Universal indirect correction to EW charged currents. More...
|
| |
| virtual const double | delU_gNC (const double mu) const |
| | Universal indirect correction to EW neutral currents. More...
|
| |
| virtual const double | dxsdcoseeWWlvjjLEP2 (const double sqrt_s, const int bin) const |
| | The differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph]. More...
|
| |
| virtual const double | dxseeWWdcos (const double sqrt_s, const double cos) const |
| | The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle. More...
|
| |
| virtual const double | dxseeWWdcosBin (const double sqrt_s, const double cos1, const double cos2) const |
| | The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle. More...
|
| |
| virtual const double | Gamma_Z () const |
| | The total decay width of the \(Z\) boson, \(\Gamma_Z\). More...
|
| |
| virtual const double | Gamma_Zf (const Particle f) const |
| | The decay width of the \(Z\) boson into a given fermion pair, \(\Gamma_Z^{f}\). More...
|
| |
| const double | GammaH2d2dRatio () const |
| | The ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2e2muRatio () const |
| | The ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2e2vRatio () const |
| | The ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2evRatio () const |
| | The ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2L2dRatio () const |
| | The ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2L2LRatio () const |
| | The ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2L2uRatio () const |
| | The ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2L2v2Ratio () const |
| | The ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2L2vRatio () const |
| | The ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2l2vRatio () const |
| | The ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2Lv2Ratio () const |
| | The ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2LvRatio () const |
| | The ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2mu2vRatio () const |
| | The ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2muvRatio () const |
| | The ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2u2dRatio () const |
| | The ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2u2uRatio () const |
| | The ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2udRatio () const |
| | The ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2v2dRatio () const |
| | The ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2v2uRatio () const |
| | The ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH2v2vRatio () const |
| | The ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH4dRatio () const |
| | The ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH4eRatio () const |
| | The ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH4fCCRatio () const |
| | The ratio of the \(\Gamma(H\to 4f)\) via CC in the current model and in the Standard Model. More...
|
| |
| const double | GammaH4fNCRatio () const |
| | The ratio of the \(\Gamma(H\to 4f)\) via NC in the current model and in the Standard Model. More...
|
| |
| const double | GammaH4fRatio () const |
| | The ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH4L2Ratio () const |
| | The ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH4LRatio () const |
| | The ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH4lRatio () const |
| | The ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH4muRatio () const |
| | The ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH4uRatio () const |
| | The ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaH4vRatio () const |
| | The ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHbbRatio () const |
| | The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHccRatio () const |
| | The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHevmuvRatio () const |
| | The ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHgagaRatio () const |
| | The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHggRatio () const |
| | The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHll_vvorjjRatio () const |
| | The ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHlv_lvorjjRatio () const |
| | The ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHlvjjRatio () const |
| | The ratio of the \(\Gamma(H\to l l j j)\) ( \(l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. @return \)\Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double GammaHlljjRatio() const; /** @brief The new physics contribution to the ratio of the \)\Gamma(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) @return \)\delta \Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double deltaGammaHlljjRatio1() const; /** @brief The new physics contribution to the ratio of the \)\Gamma(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) @return \)\delta \Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double deltaGammaHlljjRatio2() const; /** @brief The ratio of the Br\)(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. @return Br\)(H\to l l j j) \(/Br\)(H\to l l j j)_{\mathrm{SM}} \( */ virtual const double BrHlljjRatio() const; /** @brief The ratio of the \)\Gamma(H\to l \nu j j) \( (\)l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHLvudRatio () const |
| | The ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHLvvLRatio () const |
| | The ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHmumuRatio () const |
| | The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHssRatio () const |
| | The ratio of the \(\Gamma(H\to ss)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHtautauRatio () const |
| | The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHudduRatio () const |
| | The ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHWffRatio () const |
| | The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
|
| |
| const double | GammaHWjjRatio () const |
| | The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHWlvRatio () const |
| | The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHWW2l2vRatio () const |
| | The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHWW4fRatio () const |
| | The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
|
| |
| const double | GammaHWW4jRatio () const |
| | The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHWWRatio () const |
| | The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZddRatio () const |
| | The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZeeRatio () const |
| | The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZffRatio () const |
| | The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZgaRatio () const |
| | The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZllRatio () const |
| | The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZmumuRatio () const |
| | The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZuuRatio () const |
| | The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZvvRatio () const |
| | The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZZ2e2muRatio () const |
| | The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZZ4dRatio () const |
| | The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZZ4eRatio () const |
| | The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZZ4fRatio () const |
| | The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZZ4lRatio () const |
| | The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZZ4muRatio () const |
| | The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZZ4uRatio () const |
| | The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZZ4vRatio () const |
| | The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More...
|
| |
| const double | GammaHZZRatio () const |
| | The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | GammaW () const |
| | The total width of the \(W\) boson, \(\Gamma_W\). More...
|
| |
| virtual const double | GammaW (const Particle fi, const Particle fj) const |
| | A partial decay width of the \(W\) boson decay into a SM fermion pair. More...
|
| |
| void | GenerateSMInitialConditions () |
| | Generates the initial condition for the Standard Model parameters. More...
|
| |
| double | getCG_LNP () const |
| | Return CG_LNP. More...
|
| |
| double | getLambda_NP () const |
| | Return Lambda_NP. More...
|
| |
| virtual NPSMEFTd6GeneralMatching & | getMatching () const |
| | A method to get the Matching object for this model. More...
|
| |
| virtual const double | IctW_TWG (const double mu) const |
| |
| virtual const double | IctZ_TWG (const double mu) const |
| |
| virtual bool | Init (const std::map< std::string, double > &DPars) |
| | A method to initialize the model parameters. More...
|
| |
| virtual const double | intDMLL2eus2 (const double s, const double t0, const double t1) const |
| |
| virtual const double | intDMLR2etildest2 (const double s, const double t0, const double t1) const |
| |
| virtual const double | intDMLR2ets2 (const double s, const double t0, const double t1) const |
| |
| virtual const double | intDMRL2etildest2 (const double s, const double t0, const double t1) const |
| |
| virtual const double | intDMRL2ets2 (const double s, const double t0, const double t1) const |
| |
| virtual const double | intDMRR2eus2 (const double s, const double t0, const double t1) const |
| |
| virtual const double | kappaAeff () const |
| | The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\). More...
|
| |
| virtual const double | kappabeff () const |
| | The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\). More...
|
| |
| virtual const double | kappaceff () const |
| | The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\). More...
|
| |
| virtual const double | kappaGeff () const |
| | The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\). More...
|
| |
| virtual const double | kappamueff () const |
| | The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\). More...
|
| |
| virtual const double | kappaseff () const |
| | The effective coupling \(\kappa_{s,eff}=\sqrt{\Gamma_{Hss}/\Gamma_{Hss}^{SM}}\). More...
|
| |
| virtual const double | kappataueff () const |
| | The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\). More...
|
| |
| virtual const double | kappaW4feff () const |
| | The effective coupling \(\kappa_{W4f,eff}=\sqrt{\Gamma_{H4f, CC}/\Gamma_{H4f, CC}^{SM}}\). More...
|
| |
| virtual const double | kappaWeff () const |
| | The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\). More...
|
| |
| virtual const double | kappaZ4feff () const |
| | The effective coupling \(\kappa_{Z4f,eff}=\sqrt{\Gamma_{H4f, NC}/\Gamma_{H4f, NC}^{SM}}\). More...
|
| |
| virtual const double | kappaZAeff () const |
| | The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\). More...
|
| |
| virtual const double | kappaZeff () const |
| | The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\). More...
|
| |
| virtual const double | lambdaZNP (const double mu) const |
| | The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\). More...
|
| |
| virtual const double | lambz_HB (const double mu) const |
| | The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
|
| |
| virtual const double | mubbH (const double sqrt_s) const |
| | The ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mueeHee (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | The ratio \(\mu_{e^+e^- \to He^+e^-}\) between the \( e^+e^- \to H e^+e^- \) associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mueeHvv (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mueettH (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mueeWBF (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mueeWW (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mueeZBF (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mueeZH (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mueeZHGen (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mueeZHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mueeZllH (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mueeZllHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mueeZqqH (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mueeZqqHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| | The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | muepWBF (const double sqrt_s) const |
| | The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | muepZBF (const double sqrt_s) const |
| | The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | muggH (const double sqrt_s) const |
| | The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | muggHbb (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muggHgaga (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
|
| |
| virtual const double | muggHH (const double sqrt_s) const |
| | The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].) More...
|
| |
| virtual const double | muggHmumu (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muggHpttH (const double sqrt_s) const |
| | The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | muggHtautau (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muggHWW (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muggHWW2l2v (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muggHZga (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muggHZZ (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muggHZZ4l (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | mummH (const double sqrt_s) const |
| | The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mummHmm (const double sqrt_s) const |
| | The ratio \(\mu_{\mu\mu H\mu\mu}\) between the \(\sigma(\mu \mu \to H \mu \mu)}\) production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mummHNWA (const double sqrt_s) const |
| | The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model, in the narrow width approximation. More...
|
| |
| virtual const double | mummHvv (const double sqrt_s) const |
| | The ratio \(\mu_{\mu\mu H\nu\nu}\) between the \(\sigma(\mu \mu \to H \nu \nu)}\) production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mummttH (const double sqrt_s) const |
| | The ratio \(\mu_{\mu\mu ttH}\) between the \(\sigma(\mu \mu \to t\bar{t} H )}\) production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mummZH (const double sqrt_s) const |
| | The ratio \(\mu_{\mu\mu ZH}\) between the \(\sigma(\mu \mu \to Z H)}\) production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const |
| | The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6General class. More...
|
| |
| virtual const double | mutH (const double sqrt_s) const |
| | The ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | mutHq (const double sqrt_s) const |
| | The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUggHbb (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUggHgaga (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUggHmumu (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUggHtautau (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUggHWW (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUggHWW2l2v (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUggHZga (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUggHZgamumu (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,Z\gamma\to \gamma 2\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\to \gamma 2\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUggHZZ (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUggHZZ4l (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUggHZZ4mu (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,ZZ\to 4\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUttHbb (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUttHgaga (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUttHmumu (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUttHtautau (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUttHWW (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUttHWW2l2v (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUttHZga (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUttHZZ (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUttHZZ4l (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVBFBRinv (const double sqrt_s) const |
| | The ratio \(\mu_{VBF}\) between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More...
|
| |
| virtual const double | muTHUVBFHbb (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVBFHgaga (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVBFHinv (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,inv}\) between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVBFHmumu (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVBFHtautau (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVBFHWW (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVBFHWW2l2v (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVBFHZga (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVBFHZZ (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVBFHZZ4l (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVHbb (const double sqrt_s) const |
| | The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVHBRinv (const double sqrt_s) const |
| | The ratio \(\mu_{VH}\) between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More...
|
| |
| virtual const double | muTHUVHgaga (const double sqrt_s) const |
| | The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVHinv (const double sqrt_s) const |
| | The ratio \(\mu_{VH,inv}\) between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVHmumu (const double sqrt_s) const |
| | The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVHtautau (const double sqrt_s) const |
| | The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVHWW (const double sqrt_s) const |
| | The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVHWW2l2v (const double sqrt_s) const |
| | The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVHZga (const double sqrt_s) const |
| | The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVHZZ (const double sqrt_s) const |
| | The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUVHZZ4l (const double sqrt_s) const |
| | The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUWHbb (const double sqrt_s) const |
| | The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUWHgaga (const double sqrt_s) const |
| | The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUWHmumu (const double sqrt_s) const |
| | The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUWHtautau (const double sqrt_s) const |
| | The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUWHWW (const double sqrt_s) const |
| | The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUWHWW2l2v (const double sqrt_s) const |
| | The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUWHZga (const double sqrt_s) const |
| | The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUWHZZ (const double sqrt_s) const |
| | The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUWHZZ4l (const double sqrt_s) const |
| | The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUZHbb (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUZHgaga (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUZHmumu (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUZHtautau (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUZHWW (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUZHWW2l2v (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUZHZga (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUZHZZ (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muTHUZHZZ4l (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muttH (const double sqrt_s) const |
| | The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | muttHbb (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muttHgaga (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
|
| |
| virtual const double | muttHgagaZeeboost (const double sqrt_s) const |
| | The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H\to b\bar{b}\), \(Z\to e^+e^-\) channel channel in the current model and in the Standard Model. More...
|
| |
| virtual const double | muttHmumu (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muttHtautau (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muttHWW (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muttHWW2l2v (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muttHZbbboost (const double sqrt_s) const |
| | The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model. More...
|
| |
| virtual const double | muttHZga (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muttHZZ (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muttHZZ4l (const double sqrt_s) const |
| | The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVBF (const double sqrt_s) const |
| | The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVBFgamma (const double sqrt_s) const |
| | The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVBFHbb (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVBFHgaga (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVBFHmumu (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVBFHtautau (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVBFHWW (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVBFHWW2l2v (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVBFHZga (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVBFHZZ (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVBFHZZ4l (const double sqrt_s) const |
| | The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVBFpVH (const double sqrt_s) const |
| | The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVH (const double sqrt_s) const |
| | The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVHbb (const double sqrt_s) const |
| | The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVHgaga (const double sqrt_s) const |
| | The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVHmumu (const double sqrt_s) const |
| | The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVHpT250 (const double sqrt_s) const |
| | The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV. More...
|
| |
| virtual const double | muVHtautau (const double sqrt_s) const |
| | The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVHWW (const double sqrt_s) const |
| | The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVHWW2l2v (const double sqrt_s) const |
| | The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVHZga (const double sqrt_s) const |
| | The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVHZZ (const double sqrt_s) const |
| | The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muVHZZ4l (const double sqrt_s) const |
| | The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muWH (const double sqrt_s) const |
| | The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | muWHbb (const double sqrt_s) const |
| | The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muWHgaga (const double sqrt_s) const |
| | The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
|
| |
| virtual const double | muWHmumu (const double sqrt_s) const |
| | The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muWHpT250 (const double sqrt_s) const |
| | The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV. More...
|
| |
| virtual const double | muWHtautau (const double sqrt_s) const |
| | The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muWHWW (const double sqrt_s) const |
| | The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muWHWW2l2v (const double sqrt_s) const |
| | The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muWHZga (const double sqrt_s) const |
| | The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muWHZZ (const double sqrt_s) const |
| | The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muWHZZ4l (const double sqrt_s) const |
| | The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muZH (const double sqrt_s) const |
| | The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More...
|
| |
| virtual const double | muZHbb (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muZHgaga (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
|
| |
| virtual const double | muZHmumu (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muZHpT250 (const double sqrt_s) const |
| | The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV. More...
|
| |
| virtual const double | muZHtautau (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muZHWW (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muZHWW2l2v (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muZHZga (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muZHZZ (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | muZHZZ4l (const double sqrt_s) const |
| | The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
|
| |
| virtual const double | Mw () const |
| | The mass of the \(W\) boson, \(M_W\). More...
|
| |
| | NPSMEFTd6General () |
| | Constructor. More...
|
| |
| virtual const double | obliqueS () const |
| | The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).) More...
|
| |
| virtual const double | obliqueT () const |
| | The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).) More...
|
| |
| virtual const double | obliqueU () const |
| | The oblique parameter \(U\). More...
|
| |
| virtual const double | obliqueW () const |
| | The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).) More...
|
| |
| virtual const double | obliqueY () const |
| | The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).) More...
|
| |
| virtual const double | ppZHprobe (const double sqrt_s) const |
| | The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6General class. More...
|
| |
| virtual bool | PreUpdate () |
| | The pre-update method for NPSMEFTd6General. More...
|
| |
| virtual const double | R0_f (const Particle f) const |
| | The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More...
|
| |
| virtual const double | RWc () const |
| | The ratio \(R_{W,c)=\Gamma(W\to c + X)/\Gamma(W\to had)\). More...
|
| |
| virtual const double | RWlilj (const Particle li, const Particle lj) const |
| | The lepton universality ratio \(R_{W,l_i/l_j)=\Gamma(W\to l_i \nu_i)/\Gamma(W\to l_j \nu_j)\). More...
|
| |
| virtual const double | RZlilj (const Particle li, const Particle lj) const |
| | The lepton universality ratio \(R_{Z,l_i/l_j)=\Gamma(Z\to l_i^+ l_i^-)/\Gamma(Z\to l_j^+ l_j^-)\). More...
|
| |
| virtual bool | setFlag (const std::string name, const bool value) |
| | A method to check if all the mandatory parameters for NPSMEFTd6General have been provided in model initialization. More...
|
| |
| virtual bool | setFlagStr (const std::string name, const std::string value) |
| | A method to set a flag of NPSMEFTd6General. More...
|
| |
| virtual const double | sigma0_had () const |
| | The cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\sigma_h^0\). More...
|
| |
| virtual const double | STXS0_qqH (const double sqrt_s) const |
| | The STXS0 bin \(pp \to H qq\). More...
|
| |
| virtual const double | STXS12_BrH4lRatio () const |
| | The STXS BR \( H \to 4l \), \(l=e,\mu\). More...
|
| |
| virtual const double | STXS12_BrHbbRatio () const |
| | The STXS BR \( H \to bb \). More...
|
| |
| virtual const double | STXS12_BrHevmuvRatio () const |
| | The STXS BR \( H \to e\nu \mu\nu \). More...
|
| |
| virtual const double | STXS12_BrHgagaRatio () const |
| | The STXS BR \( H \to \gamma \gamma \). More...
|
| |
| virtual const double | STXS12_ggH_mjj0_350_pTH0_60_Nj1 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j \geq 1,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60\). More...
|
| |
| virtual const double | STXS12_ggH_mjj0_350_pTH0_60_Nj2 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60\). More...
|
| |
| virtual const double | STXS12_ggH_mjj0_350_pTH120_200_Nj2 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~120<p_{TH} [GeV]<200\). More...
|
| |
| virtual const double | STXS12_ggH_mjj0_350_pTH60_120_Nj2 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~60<p_{TH} [GeV]<120\). More...
|
| |
| virtual const double | STXS12_ggH_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~<p_{TH} [GeV]<200\). More...
|
| |
| virtual const double | STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\). More...
|
| |
| virtual const double | STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\). More...
|
| |
| virtual const double | STXS12_ggH_mjj700_Inf_pTH0_200_Nj2 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200\). More...
|
| |
| virtual const double | STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\). More...
|
| |
| virtual const double | STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\). More...
|
| |
| virtual const double | STXS12_ggH_pTH0_10_Nj0 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j=0,~p_{TH} [GeV]<10\). More...
|
| |
| virtual const double | STXS12_ggH_pTH0_60_Nj1 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j = 1,~p_{TH} [GeV]<60\). More...
|
| |
| virtual const double | STXS12_ggH_pTH10_200_Nj0 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j=0,~p_{TH} [GeV]<10\). More...
|
| |
| virtual const double | STXS12_ggH_pTH10_Inf_Nj0 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j=0,~10<p_{TH} [GeV]\). More...
|
| |
| virtual const double | STXS12_ggH_pTH120_200_Nj1 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j = 1,~120<p_{TH} [GeV]<200\). More...
|
| |
| virtual const double | STXS12_ggH_pTH200_300 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(,200<~p_{TH} [GeV]<300\). More...
|
| |
| virtual const double | STXS12_ggH_pTH200_300_Nj01 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j\leq 1,~200<p_{TH} [GeV]<300\). More...
|
| |
| virtual const double | STXS12_ggH_pTH300_450 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(,300<~p_{TH} [GeV]<450\). More...
|
| |
| virtual const double | STXS12_ggH_pTH300_450_Nj01 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j\leq 1,~300<p_{TH} [GeV]<450\). More...
|
| |
| virtual const double | STXS12_ggH_pTH450_650 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(450<~p_{TH} [GeV]<650\). More...
|
| |
| virtual const double | STXS12_ggH_pTH450_650_Nj01 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j\leq 1,~450<p_{TH} [GeV]<650\). More...
|
| |
| virtual const double | STXS12_ggH_pTH450_Inf (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(,450<~p_{TH} [GeV]\). More...
|
| |
| virtual const double | STXS12_ggH_pTH60_120_Nj1 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j = 1,~60<p_{TH} [GeV]<120\). More...
|
| |
| virtual const double | STXS12_ggH_pTH650_Inf (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(~p_{TH} [GeV]>650\). More...
|
| |
| virtual const double | STXS12_ggH_pTH650_Inf_Nj01 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\), \(N_j\leq 1,650<p_{TH} [GeV]\). More...
|
| |
| virtual const double | STXS12_ggHll_pTV0_75 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\ell\ell\), \(p_{TV}[GeV]<75\). More...
|
| |
| virtual const double | STXS12_ggHll_pTV150_250_Nj0 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More...
|
| |
| virtual const double | STXS12_ggHll_pTV150_250_Nj1 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\ell\ell\), \(N_j = 1,~150<p_{TV}[GeV]<250\). More...
|
| |
| virtual const double | STXS12_ggHll_pTV250_Inf (const double sqrt_s) const |
| | The STXS bin \(gg \to H\ell\ell\), \(250 < p_{TV}[GeV]\). More...
|
| |
| virtual const double | STXS12_ggHll_pTV75_150 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\ell\ell\), \(75<p_{TV}[GeV]<150\). More...
|
| |
| virtual const double | STXS12_qqHll_pTV0_150 (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\ell\), \(0<p_{TV}<150[GeV]\). More...
|
| |
| virtual const double | STXS12_qqHll_pTV0_75 (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\ell\), \(p_{TV}[GeV]<75\). More...
|
| |
| virtual const double | STXS12_qqHll_pTV150_250_Nj0 (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More...
|
| |
| virtual const double | STXS12_qqHll_pTV150_250_Nj1 (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\ell\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\). More...
|
| |
| virtual const double | STXS12_qqHll_pTV250_400 (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}<400[GeV]\). More...
|
| |
| virtual const double | STXS12_qqHll_pTV250_Inf (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}[GeV]\). More...
|
| |
| virtual const double | STXS12_qqHll_pTV400_Inf (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\ell\), \(400<p_{TV}[GeV]\). More...
|
| |
| virtual const double | STXS12_qqHll_pTV75_150 (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\ell\), \(75<p_{TV}[GeV]<150\). More...
|
| |
| virtual const double | STXS12_qqHlv_pTV0_150 (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\nu\), \(0<p_{TV}<150[GeV]\). More...
|
| |
| virtual const double | STXS12_qqHlv_pTV0_75 (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\nu\), \(p_{TV}[GeV]<75\). More...
|
| |
| virtual const double | STXS12_qqHlv_pTV150_250_Nj0 (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\nu\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More...
|
| |
| virtual const double | STXS12_qqHlv_pTV150_250_Nj1 (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\nu\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\). More...
|
| |
| virtual const double | STXS12_qqHlv_pTV250_400 (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}<400[GeV]\). More...
|
| |
| virtual const double | STXS12_qqHlv_pTV250_Inf (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}[GeV]\). More...
|
| |
| virtual const double | STXS12_qqHlv_pTV400_Inf (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\nu\), \(400<p_{TV}[GeV]\). More...
|
| |
| virtual const double | STXS12_qqHlv_pTV75_150 (const double sqrt_s) const |
| | The STXS bin \(qq \to H\ell\nu\), \(75<p_{TV}[GeV]<150\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj0_60_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~m_{jj}[GeV]<60\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1000<m_{jj}[GeV]<1500,~p_{TH}[GeV]<200\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1000<m_{jj}[GeV],~p_{TH}[GeV]>200\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj120_350_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~120<m_{jj}[GeV]<350\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1500<m_{jj}[GeV],~p_{TH}[GeV]<200\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<1000,~p_{TH}[GeV]>200\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV],~200<p_{TH}[GeV]\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj60_120_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~60<m_{jj}[GeV]<120\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV]<1000,~p_{TH}[GeV]<200\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\). More...
|
| |
| virtual const double | STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\). More...
|
| |
| virtual const double | STXS12_qqHqq_Nj0 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j = 0\). More...
|
| |
| virtual const double | STXS12_qqHqq_Nj1 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j = 1\). More...
|
| |
| virtual const double | STXS12_qqHqq_VH_veto_Nj01 (const double sqrt_s) const |
| | The STXS bin \(qq \to Hqq\), \(N_j = 0,1\) VH-veto Ref. 2402.05742. More...
|
| |
| virtual const double | STXS12_tH (const double sqrt_s) const |
| | The STXS bin \(pp \to tH\). More...
|
| |
| virtual const double | STXS12_ttH_pTH0_60 (const double sqrt_s) const |
| | The STXS bin \(pp \to ttH\), \(p_{TH}[GeV]<60\). More...
|
| |
| virtual const double | STXS12_ttH_pTH120_200 (const double sqrt_s) const |
| | The STXS bin \(pp \to ttH\), \(120<p_{TH}[GeV]<200\). More...
|
| |
| virtual const double | STXS12_ttH_pTH200_300 (const double sqrt_s) const |
| | The STXS bin \(pp \to ttH\), \(200<p_{TH}[GeV]<300\). More...
|
| |
| virtual const double | STXS12_ttH_pTH300_450 (const double sqrt_s) const |
| | The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]<450\). More...
|
| |
| virtual const double | STXS12_ttH_pTH300_Inf (const double sqrt_s) const |
| | The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]\). More...
|
| |
| virtual const double | STXS12_ttH_pTH450_Inf (const double sqrt_s) const |
| | The STXS bin \(pp \to ttH\), \(450<p_{TH}[GeV]\). More...
|
| |
| virtual const double | STXS12_ttH_pTH60_120 (const double sqrt_s) const |
| | The STXS bin \(pp \to ttH\), \(60<p_{TH}[GeV]<120\). More...
|
| |
| virtual const double | STXS_ggH0j (const double sqrt_s) const |
| | The STXS bin \(gg \to H\). More...
|
| |
| virtual const double | STXS_ggH1j_pTH_0_60 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\). More...
|
| |
| virtual const double | STXS_ggH1j_pTH_120_200 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\). More...
|
| |
| virtual const double | STXS_ggH1j_pTH_200 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\). More...
|
| |
| virtual const double | STXS_ggH1j_pTH_60_120 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\). More...
|
| |
| virtual const double | STXS_ggH2j_pTH_0_200 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\). More...
|
| |
| virtual const double | STXS_ggH2j_pTH_0_60 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\). More...
|
| |
| virtual const double | STXS_ggH2j_pTH_120_200 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\). More...
|
| |
| virtual const double | STXS_ggH2j_pTH_200 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\). More...
|
| |
| virtual const double | STXS_ggH2j_pTH_60_120 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\). More...
|
| |
| virtual const double | STXS_ggH_VBFtopo_j3 (const double sqrt_s) const |
| | The STXS bin \(gg \to H\). More...
|
| |
| virtual const double | STXS_ggH_VBFtopo_j3v (const double sqrt_s) const |
| | The STXS bin \(gg \to H\). More...
|
| |
| virtual const double | STXS_qqHll_pTV_0_150 (const double sqrt_s) const |
| | The STXS bin \(qq \to H \ell \ell\). More...
|
| |
| virtual const double | STXS_qqHll_pTV_150_250 (const double sqrt_s) const |
| | The STXS bin \(qq \to H \ell \ell\). More...
|
| |
| virtual const double | STXS_qqHll_pTV_150_250_0j (const double sqrt_s) const |
| | The STXS bin \(qq \to H \ell \ell\). More...
|
| |
| virtual const double | STXS_qqHll_pTV_150_250_1j (const double sqrt_s) const |
| | The STXS bin \(qq \to H \ell \ell\). More...
|
| |
| virtual const double | STXS_qqHll_pTV_250 (const double sqrt_s) const |
| | The STXS bin \(qq \to H \ell \ell\). More...
|
| |
| virtual const double | STXS_qqHlv_pTV_0_150 (const double sqrt_s) const |
| | The STXS bin \(qq \to H \ell \nu\). More...
|
| |
| virtual const double | STXS_qqHlv_pTV_0_250 (const double sqrt_s) const |
| | The STXS bin \(qq \to H \ell \nu\). More...
|
| |
| virtual const double | STXS_qqHlv_pTV_150_250_0j (const double sqrt_s) const |
| | The STXS bin \(qq \to H \ell \nu\). More...
|
| |
| virtual const double | STXS_qqHlv_pTV_150_250_1j (const double sqrt_s) const |
| | The STXS bin \(qq \to H \ell \nu\). More...
|
| |
| virtual const double | STXS_qqHlv_pTV_250 (const double sqrt_s) const |
| | The STXS bin \(qq \to H \ell \nu\). More...
|
| |
| virtual const double | STXS_qqHqq_nonVHtopo (const double sqrt_s) const |
| | The STXS bin \(qq \to H qq\). More...
|
| |
| virtual const double | STXS_qqHqq_pTj_200 (const double sqrt_s) const |
| | The STXS bin \(qq \to H qq\). More...
|
| |
| virtual const double | STXS_qqHqq_Rest (const double sqrt_s) const |
| | The STXS bin \(qq \to H qq\). More...
|
| |
| virtual const double | STXS_qqHqq_VBFtopo_j3 (const double sqrt_s) const |
| | The STXS bin \(qq \to H qq\). More...
|
| |
| virtual const double | STXS_qqHqq_VBFtopo_j3v (const double sqrt_s) const |
| | The STXS bin \(qq \to H qq\). More...
|
| |
| virtual const double | STXS_qqHqq_VBFtopo_Rest (const double sqrt_s) const |
| | The STXS bin \(qq \to H qq\). More...
|
| |
| virtual const double | STXS_qqHqq_VHtopo (const double sqrt_s) const |
| | The STXS bin \(qq \to H qq\). More...
|
| |
| virtual const double | STXS_ttHtH (const double sqrt_s) const |
| | The STXS bin \( ttH + tH \). More...
|
| |
| virtual const double | STXS_WHqqHqq_pTj1_200 (const double sqrt_s) const |
| | The STXS bin \( qq \to WH \to H qq \). More...
|
| |
| virtual const double | STXS_WHqqHqq_Rest (const double sqrt_s) const |
| | The STXS bin \( qq \to WH \to H qq \). More...
|
| |
| virtual const double | STXS_WHqqHqq_VBFtopo_j3 (const double sqrt_s) const |
| | The STXS bin \( qq \to WH \to H qq \). More...
|
| |
| virtual const double | STXS_WHqqHqq_VBFtopo_j3v (const double sqrt_s) const |
| | The STXS bin \( qq \to WH \to H qq \). More...
|
| |
| virtual const double | STXS_WHqqHqq_VH2j (const double sqrt_s) const |
| | The STXS bin \( qq \to WH \to H qq \). More...
|
| |
| virtual const double | STXS_ZHqqHqq_pTj1_200 (const double sqrt_s) const |
| | The STXS bin \( qq \to ZH \to H qq \). More...
|
| |
| virtual const double | STXS_ZHqqHqq_Rest (const double sqrt_s) const |
| | The STXS bin \( qq \to ZH \to H qq \). More...
|
| |
| virtual const double | STXS_ZHqqHqq_VBFtopo_j3 (const double sqrt_s) const |
| | The STXS bin \( qq \to ZH \to H qq \). More...
|
| |
| virtual const double | STXS_ZHqqHqq_VBFtopo_j3v (const double sqrt_s) const |
| | The STXS bin \( qq \to ZH \to H qq \). More...
|
| |
| virtual const double | STXS_ZHqqHqq_VH2j (const double sqrt_s) const |
| | The STXS bin \( qq \to ZH \to H qq \). More...
|
| |
| const double | tovers2 (const double cosmin, const double cosmax) const |
| |
| const double | uovers2 (const double cosmin, const double cosmax) const |
| |
| virtual const double | xseeWW (const double sqrt_s) const |
| | Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\). More...
|
| |
| virtual const double | xseeWW4fLEP2 (const double sqrt_s, const int fstate) const |
| | The cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More...
|
| |
| virtual const double | xseeWWtotLEP2 (const double sqrt_s) const |
| | The total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More...
|
| |
| virtual const double | BR_Zf (const Particle f) const |
| | The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\). More...
|
| |
| virtual const double | BrHlljjRatio () const |
| | The ratio of the Br \((H\to l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More...
|
| |
| virtual const double | C1eeHvv (const double sqrt_s) const |
| | The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...
|
| |
| virtual const double | C1eettH (const double sqrt_s) const |
| | The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...
|
| |
| virtual const double | C1eeWBF (const double sqrt_s) const |
| | The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...
|
| |
| virtual const double | C1eeZBF (const double sqrt_s) const |
| | The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...
|
| |
| virtual const double | C1eeZH (const double sqrt_s) const |
| | The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...
|
| |
| virtual const double | cbminuscc () const |
| |
| virtual const double | cbminusctau () const |
| |
| virtual const double | ccminusctau () const |
| |
| virtual const double | cgaplusct () const |
| |
| virtual const double | cgminuscga () const |
| |
| virtual const double | cgplusct () const |
| |
| virtual const double | cVpluscb () const |
| |
| virtual const double | cVplusctau () const |
| |
| virtual const double | deltaA_f_2 (const Particle f) const |
| | The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\Delta \mathcal{A}_f^{(2)}\). More...
|
| |
| virtual const double | deltaAFB_2 (const Particle f) const |
| | The \(\mathcal{O}(\Lambda^{-4})\) new physics to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\Delta A^f_{FB}\). More...
|
| |
| virtual const double | deltaGA_f_2 (const Particle f) const |
| |
| virtual const double | deltaGamma_Z_2 () const |
| | The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the total decay width of the \(Z\) boson, \(\Delta \Gamma_Z^{(2)}\). More...
|
| |
| virtual const double | deltaGamma_Zf_2 (const Particle f) const |
| | The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\Delta \Gamma_{Z,f}^{(2)}\). More...
|
| |
| virtual const double | deltaGamma_Zhad () const |
| | The new physics contribution to the hadronic decay width of the \(Z\) boson, \(\delta \Gamma_{Z,had}\). More...
|
| |
| virtual const double | deltaGamma_Zhad_2 () const |
| | The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the hadronic decay width of the \(Z\) boson, \(\Delta \Gamma_{Z,had}^{(2)}\). More...
|
| |
| const double | deltaGL_f_mu (const Particle p, const double mu) const |
| | New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More...
|
| |
| const double | deltaGR_f_mu (const Particle p, const double mu) const |
| | New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More...
|
| |
| virtual const double | deltaGV_f_2 (const Particle f) const |
| |
| virtual const double | deltaN_nu () const |
| | The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements. More...
|
| |
| virtual const double | deltaR0_f_2 (const Particle f) const |
| | The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos: More...
|
| |
| virtual const double | deltaR_inv () const |
| | The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the \(Z\) boson, \(\delta R_{inv}\). More...
|
| |
| virtual const double | deltaRuc () const |
| | The new physics contribution to the ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width: More...
|
| |
| virtual const double | deltaRuc_2 () const |
| | The \(\mathcal{O}(1/\Lambda^4)\) new physics contribution to the ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width: More...
|
| |
| virtual const double | deltaSigmaHadron_2 () const |
| | The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\Delta \sigma_h^{0,(2)}\). More...
|
| |
| virtual const double | deltaSin2thetaEff_e () const |
| | The new physics contribution to the effective electron/leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. More...
|
| |
| virtual const double | deltaSin2thetaEff_e_2 () const |
| | The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the effective electron weak angle \(\Delta \sin^2\theta_{eff,e}^{(2)}\) at the \(Z\) pole. More...
|
| |
| virtual const double | deltaSin2thetaEff_mu () const |
| | The new physics contribution to the effective muonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\mu\mu}\) at the \(Z\) pole. More...
|
| |
| virtual const double | deltaSin2thetaEff_mu_2 () const |
| | The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the effective muonic weak angle \(\Delta \sin^2\theta_{eff, \mu}^{(2)}\) at the \(Z\) pole. More...
|
| |
| virtual const double | deltaxseeWWhadLEP2 (const double sqrt_s) const |
| | The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to j j j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...
|
| |
| virtual const double | deltaxseeWWleptLEP2 (const double sqrt_s) const |
| | The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...
|
| |
| virtual const double | deltaxseeWWsemilLEP2 (const double sqrt_s) const |
| | The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...
|
| |
| virtual const gslpp::complex | gA_f (const Particle f) const |
| | The total (SM+NP) contribution to the neutral-current axial-vector coupling \(g_A^f\). More...
|
| |
| virtual const double | Gamma_had () const |
| | The hadronic decay width of the \(Z\) boson, \(\Gamma_{Z,had}\). More...
|
| |
| virtual const StandardModel & | getTrueSM () const |
| | A method to return a StandardModel object from NPbase. More...
|
| |
| virtual const gslpp::complex | gV_f (const Particle f) const |
| | The total (SM+NP) contribution to the neutral-current vector coupling \(g_V^f\). More...
|
| |
| virtual const gslpp::complex | kappaZ_f (const Particle f) const |
| | The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions. More...
|
| |
| virtual const double | muggHgagaInt (const double sqrt_s) const |
| | The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259. More...
|
| |
| virtual const double | muggHpbbH_Hgaga (const double sqrt_s) const |
| |
| virtual const double | muggHpbbH_Htautau (const double sqrt_s) const |
| |
| virtual const double | muggHpbbH_HWW (const double sqrt_s) const |
| |
| virtual const double | muggHpbbH_HZZ (const double sqrt_s) const |
| |
| virtual const double | muggHpttHptHpbbH_Hmumu (const double sqrt_s) const |
| |
| virtual const double | muggHpttHptHpbbH_HZga (const double sqrt_s) const |
| |
| virtual const double | muggHpVBFpbbH_Hbb (const double sqrt_s) const |
| |
| virtual const double | muppHmumu (const double sqrt_s) const |
| |
| virtual const double | muppHZga (const double sqrt_s) const |
| |
| virtual const double | mutHgaga (const double sqrt_s) const |
| |
| virtual const double | muttHptH_Hbb (const double sqrt_s) const |
| |
| virtual const double | muttHptH_Hgaga (const double sqrt_s) const |
| |
| virtual const double | muttHptH_Hmumu (const double sqrt_s) const |
| |
| virtual const double | muttHptH_Htautau (const double sqrt_s) const |
| |
| virtual const double | muttHptH_HWW (const double sqrt_s) const |
| |
| virtual const double | muttHptH_HZZ (const double sqrt_s) const |
| |
| virtual const double | muVBFpVH_Hmumu (const double sqrt_s) const |
| |
| virtual const double | muVBFpVH_HZga (const double sqrt_s) const |
| |
| virtual const double | muVHcc (const double sqrt_s) const |
| |
| virtual const double | N_nu () const |
| | The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\). More...
|
| |
| | NPbase () |
| | The default constructor. More...
|
| |
| virtual const double | R_inv () const |
| | The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\). More...
|
| |
| virtual const gslpp::complex | rhoZ_f (const Particle f) const |
| | The effective neutral-current coupling \(\rho_Z^f\) including SM plus NP contributions. More...
|
| |
| virtual const double | Ruc () const |
| | The ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width. More...
|
| |
| virtual const double | sin2thetaEff (const Particle f) const |
| | The leptonic effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\rm lept}\) at the the \(Z\) pole. More...
|
| |
| virtual bool | Update (const std::map< std::string, double > &DPars) |
| | The update method for NPbase. More...
|
| |
| virtual const double | UpperLimitZgammaA (const double sqrt_s) const |
| |
| virtual const double | UpperLimitZgammaA13 (const double sqrt_s) const |
| |
| virtual const double | UpperLimitZgammaC (const double sqrt_s) const |
| |
| virtual const double | UpperLimitZgammaC13 (const double sqrt_s) const |
| |
| virtual const double | xseeWWhadLEP2 (const double sqrt_s) const |
| | The cross section in pb for \(e^+ e^- \to W^+ W^- \to j j j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...
|
| |
| virtual const double | xseeWWleptLEP2 (const double sqrt_s) const |
| | The cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...
|
| |
| virtual const double | xseeWWsemilLEP2 (const double sqrt_s) const |
| | The cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...
|
| |
 Public Member Functions inherited from StandardModel |
| gslpp::complex | AH_f (const double tau) const |
| | Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More...
|
| |
| gslpp::complex | AH_W (const double tau) const |
| | W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling. More...
|
| |
| gslpp::complex | AHZga_f (const double tau, const double lambda) const |
| | Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
|
| |
| gslpp::complex | AHZga_W (const double tau, const double lambda) const |
| | W loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
|
| |
| const double | Ale (double mu, orders order, bool Nf_thr=true) const |
| | The running electromagnetic coupling \(\alpha_e(\mu)\) in the \(\overline{MS}\) scheme. More...
|
| |
| const double | ale_OS (const double mu, orders order=FULLNLO) const |
| | The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell scheme. More...
|
| |
| virtual const double | alrmoller (const double q2, const double y) const |
| | The computation of the parity violating asymmetry in Moller scattering. More...
|
| |
| const double | Als (const double mu, const int Nf_in, const orders order=FULLNLO) const |
| | Computes the running strong coupling \(\alpha_s(\mu)\) with \(N_f\) active flavours in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...
|
| |
| const double | Als (const double mu, const orders order, const bool Nf_thr, const bool qed_flag) const |
| | The running QCD coupling \(\alpha(\mu)\) in the \(\overline{MS}\) scheme including QED corrections. More...
|
| |
| const double | Als (const double mu, const orders order=FULLNLO, const bool Nf_thr=true) const |
| |
| const double | Alstilde5 (const double mu) const |
| | The value of \(\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\) and full EW corrections. More...
|
| |
| virtual const double | amuon () const |
| | The computation of the anomalous magnetic moment of the muon \(a_\mu=(g_\mu-2)/2\). More...
|
| |
| const double | Beta_e (int nm, unsigned int nf) const |
| | QED beta function coefficients - eq. (36) hep-ph/0512066. More...
|
| |
| const double | Beta_s (int nm, unsigned int nf) const |
| | QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066. More...
|
| |
| virtual const double | BrHtobb () const |
| | The Br \((H\to b \bar{b})\) in the Standard Model. More...
|
| |
| virtual const double | BrHtocc () const |
| | The Br \((H\to c \bar{c})\) in the Standard Model. More...
|
| |
| virtual const double | BrHtogaga () const |
| | The Br \((H\to \gamma \gamma)\) in the Standard Model. More...
|
| |
| virtual const double | BrHtogg () const |
| | The Br \(\(H\to gg)\) in the Standard Model. More...
|
| |
| virtual const double | BrHtomumu () const |
| | The Br \((H\to \mu^+ \mu^-)\) in the Standard Model. More...
|
| |
| virtual const double | BrHtoss () const |
| | The Br \((H\to s \bar{s})\) in the Standard Model. More...
|
| |
| virtual const double | BrHtotautau () const |
| | The Br \((H\to \tau^+ \tau^-)\) in the Standard Model. More...
|
| |
| virtual const double | BrHtoWWstar () const |
| | The Br \((H\to W W^*)\) in the Standard Model. More...
|
| |
| virtual const double | BrHtoZga () const |
| | The Br \((H\to Z \gamma)\) in the Standard Model. More...
|
| |
| virtual const double | BrHtoZZstar () const |
| | The Br \((H\to Z Z^*)\) in the Standard Model. More...
|
| |
| const double | c02 () const |
| | The square of the cosine of the weak mixing angle \(c_0^2\) defined without weak radiative corrections. More...
|
| |
| virtual bool | CheckFlags () const |
| | A method to check the sanity of the set of model flags. More...
|
| |
| virtual bool | CheckParameters (const std::map< std::string, double > &DPars) |
| | A method to check if all the mandatory parameters for StandardModel have been provided in model initialization. More...
|
| |
| bool | checkSMparamsForEWPO () |
| | A method to check whether the parameters relevant to the EWPO are updated. More...
|
| |
| const double | computeBrHto4f () const |
| | The Br \((H\to 4f)\) in the Standard Model. More...
|
| |
| const double | computeBrHto4l2 () const |
| | The Br \((H\to 4l)\) \(l=e,\mu\) in the Standard Model. More...
|
| |
| const double | computeBrHto4l3 () const |
| | The Br \((H\to 4l)\) \(l=e,\mu,\tau\) in the Standard Model. More...
|
| |
| const double | computeBrHto4q () const |
| | The Br \((H\to 4q)\) in the Standard Model. More...
|
| |
| const double | computeBrHto4v () const |
| | The Br \((H\to 4\nu)\) in the Standard Model. More...
|
| |
| const double | computeBrHtobb () const |
| | The Br \((H\to bb)\) in the Standard Model. More...
|
| |
| const double | computeBrHtocc () const |
| | The Br \((H\to cc)\) in the Standard Model. More...
|
| |
| const double | computeBrHtoevmuv () const |
| | The Br \((H\to e \nu \mu \nu)\) in the Standard Model. More...
|
| |
| const double | computeBrHtogaga () const |
| | The Br \((H\to\gamma\gamma)\) in the Standard Model. More...
|
| |
| const double | computeBrHtogg () const |
| | The Br \((H\to gg)\) in the Standard Model. More...
|
| |
| const double | computeBrHtollvv2 () const |
| | The Br \((H\to l^+ l^- \nu \nu)\) \(l=e,\mu\) in the Standard Model. More...
|
| |
| const double | computeBrHtollvv3 () const |
| | The Br \((H\to l^+ l^- \nu \nu)\) \(l=e,\mu,\tau\) in the Standard Model. More...
|
| |
| const double | computeBrHtomumu () const |
| | The Br \((H\to \mu\mu)\) in the Standard Model. More...
|
| |
| const double | computeBrHtoss () const |
| | The Br \((H\to ss)\) in the Standard Model. More...
|
| |
| const double | computeBrHtotautau () const |
| | The Br \((H\to \tau\tau)\) in the Standard Model. More...
|
| |
| const double | computeBrHtoWW () const |
| | The Br \((H\to WW)\) in the Standard Model. More...
|
| |
| const double | computeBrHtoZga () const |
| | The Br \((H\to Z\gamma)\) in the Standard Model. More...
|
| |
| const double | computeBrHtoZZ () const |
| | The Br \((H\to ZZ)\) in the Standard Model. More...
|
| |
| void | ComputeDeltaR_rem (const double Mw_i, double DeltaR_rem[orders_EW_size]) const |
| | A method to collect \(\Delta r_{\mathrm{rem}}\) computed via subclasses. More...
|
| |
| void | ComputeDeltaRho (const double Mw_i, double DeltaRho[orders_EW_size]) const |
| | A method to collect \(\Delta\rho\) computed via subclasses. More...
|
| |
| const double | computeGammaHgaga_tt () const |
| | The top loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
|
| |
| const double | computeGammaHgaga_tW () const |
| | The mixed \(t-W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
|
| |
| const double | computeGammaHgaga_WW () const |
| | The \(W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
|
| |
| const double | computeGammaHgg_bb () const |
| | The bottom loop contribution to \(H\to gg\) in the Standard Model. More...
|
| |
| const double | computeGammaHgg_tb () const |
| | The top-bottom interference contribution to \(H\to gg\) in the Standard Model. More...
|
| |
| const double | computeGammaHgg_tt () const |
| | The top loop contribution to \(H\to gg\) in the Standard Model. More...
|
| |
| const double | computeGammaHTotal () const |
| | The Higgs total width in the Standard Model. More...
|
| |
| const double | computeGammaHZga_tt () const |
| | The top loop contribution to \(H\to Z\gamma\) in the Standard Model. More...
|
| |
| const double | computeGammaHZga_tW () const |
| | The mixed \(t-W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. More...
|
| |
| const double | computeGammaHZga_WW () const |
| | The \(W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. Currently it returns the value of tab 41 in ref. [Heinemeyer:2013tqa]. More...
|
| |
| const double | computeSigmabbH (const double sqrt_s) const |
| | The bbH production cross section in the Standard Model. More...
|
| |
| const double | computeSigmaggH (const double sqrt_s) const |
| | The ggH cross section in the Standard Model. More...
|
| |
| const double | computeSigmaggH_bb (const double sqrt_s) const |
| | The square of the bottom-quark contribution to the ggH cross section in the Standard Model. More...
|
| |
| const double | computeSigmaggH_tb (const double sqrt_s) const |
| | The top-bottom interference contribution to the ggH cross section in the Standard Model. More...
|
| |
| const double | computeSigmaggH_tt (const double sqrt_s) const |
| | The square of the top-quark contribution to the ggH cross section in the Standard Model. More...
|
| |
| const double | computeSigmatHq (const double sqrt_s) const |
| | The tHq production cross section in the Standard Model. More...
|
| |
| const double | computeSigmattH (const double sqrt_s) const |
| | The ttH production cross section in the Standard Model. More...
|
| |
| const double | computeSigmaVBF (const double sqrt_s) const |
| | The VBF cross section in the Standard Model. More...
|
| |
| const double | computeSigmaWF (const double sqrt_s) const |
| | The W fusion contribution \(\sigma_{WF}\) to higgs-production cross section in the Standard Model. More...
|
| |
| const double | computeSigmaWH (const double sqrt_s) const |
| | The WH production cross section in the Standard Model. More...
|
| |
| const double | computeSigmaZF (const double sqrt_s) const |
| | The Z fusion contribution \(\sigma_{ZF}\) to higgs-production cross section in the Standard Model. More...
|
| |
| const double | computeSigmaZH (const double sqrt_s) const |
| | The ZH production cross section in the Standard Model. More...
|
| |
| const double | computeSigmaZWF (const double sqrt_s) const |
| | The Z W interference fusion contribution \(\sigma_{ZWF}\) to higgs-production cross section in the Standard Model. More...
|
| |
| virtual const double | cW2 () const |
| |
| virtual const double | cW2 (const double Mw_i) const |
| | The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as \(c_W^2\). More...
|
| |
| virtual const double | Dalpha5hMz () const |
| | The 5-quark contribution to the running of the em constant to the \(Z\) pole. \(\Delta\alpha_{had}^{(5)}(M_Z)\). More...
|
| |
| const double | DeltaAlpha () const |
| | The total corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha(M_Z^2)\). More...
|
| |
| const double | DeltaAlphaL5q () const |
| | The sum of the leptonic and the five-flavour hadronic corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha^{\ell+5q}(M_Z^2)\). More...
|
| |
| const double | DeltaAlphaLepton (const double s) const |
| | Leptonic contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{lept}}(s)\). More...
|
| |
| const double | DeltaAlphaTop (const double s) const |
| | Top-quark contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{top}}(s)\). More...
|
| |
| virtual const gslpp::complex | deltaKappaZ_f (const Particle f) const |
| | Flavour non-universal vertex corrections to \(\kappa_Z^l\), denoted by \(\Delta\kappa_Z^l\). More...
|
| |
| virtual const double | DeltaR () const |
| | The SM prediction for \(\Delta r\) derived from that for the \(W\) boson mass. More...
|
| |
| virtual const double | DeltaRbar () const |
| | The SM prediction for \(\Delta \overline{r}\) derived from that for the \(W\)-boson mass. More...
|
| |
| virtual const gslpp::complex | deltaRhoZ_f (const Particle f) const |
| | Flavour non-universal vertex corrections to \(\rho_Z^l\), denoted by \(\Delta\rho_Z^l\). More...
|
| |
| virtual const double | eeffAFBbottom (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffAFBcharm (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffAFBe (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffAFBetsub (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffAFBmu (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffAFBstrange (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffAFBtau (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffRbottom (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffRcharm (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffRelectron (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffRelectrontsub (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffRmuon (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffRstrange (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffRtau (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffsigma (const Particle f, const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| |
| virtual const double | eeffsigmaBottom (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffsigmaCharm (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffsigmaE (const double pol_e, const double pol_p, const double s) const |
| |
| const double | eeffsigmaEbin (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| |
| virtual const double | eeffsigmaEtsub (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffsigmaHadron (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffsigmaMu (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffsigmaStrange (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | eeffsigmaTau (const double pol_e, const double pol_p, const double s) const |
| |
| virtual const double | epsilon1 () const |
| | The SM contribution to the epsilon parameter \(\varepsilon_1\). More...
|
| |
| virtual const double | epsilon2 () const |
| | The SM contribution to the epsilon parameter \(\varepsilon_2\). More...
|
| |
| virtual const double | epsilon3 () const |
| | The SM contribution to the epsilon parameter \(\varepsilon_3\). More...
|
| |
| virtual const double | epsilonb () const |
| | The SM contribution to the epsilon parameter \(\varepsilon_b\). More...
|
| |
| gslpp::complex | f_triangle (const double tau) const |
| | Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More...
|
| |
| gslpp::complex | g_triangle (const double tau) const |
| | Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
|
| |
| virtual const double | Gamma_inv () const |
| | The invisible partial decay width of the \(Z\) boson, \(\Gamma_{\mathrm{inv}}\). More...
|
| |
| virtual const double | Gamma_muon () const |
| | The computation of the muon decay. More...
|
| |
| virtual const double | Gamma_tau_l_nunu (const Particle l) const |
| | The computation of the leptonic tau decays. More...
|
| |
| virtual const double | GammaHtobb () const |
| | The \(\Gamma(H\to b \bar{b})\) in the Standard Model. More...
|
| |
| virtual const double | GammaHtocc () const |
| | The \(\Gamma(H\to c \bar{c})\) in the Standard Model. More...
|
| |
| virtual const double | GammaHtogaga () const |
| | The \(\Gamma(H\to \gamma \gamma)\) in the Standard Model. More...
|
| |
| virtual const double | GammaHtogg () const |
| | The \(\Gamma(H\to gg)\) in the Standard Model. More...
|
| |
| virtual const double | GammaHtomumu () const |
| | The \(\Gamma(H\to \mu^+ \mu^-)\) in the Standard Model. More...
|
| |
| virtual const double | GammaHtoss () const |
| | The \(\Gamma(H\to s \bar{s})\) in the Standard Model. More...
|
| |
| virtual const double | GammaHTot () const |
| | The total Higgs width \(\Gamma(H)\) in the Standard Model. More...
|
| |
| virtual const double | GammaHtotautau () const |
| | The \(\Gamma(H\to \tau^+ \tau^-)\) in the Standard Model. More...
|
| |
| virtual const double | GammaHtoWWstar () const |
| | The \(\Gamma(H\to W W^*)\) in the Standard Model. More...
|
| |
| virtual const double | GammaHtoZga () const |
| | The \(\Gamma(H\to Z \gamma)\) in the Standard Model. More...
|
| |
| virtual const double | GammaHtoZZstar () const |
| | The \(\Gamma(H\to Z Z^*)\) in the Standard Model. More...
|
| |
| virtual const double | GammaZ (const Particle f) const |
| | The \(Z\to \ell\bar{\ell}\) partial decay width, \(\Gamma_\ell\). More...
|
| |
| virtual const double | gAnue () const |
| | The effective (muon) neutrino-electron axial-vector coupling: gAnue. More...
|
| |
| const double | getAle () const |
| | A get method to retrieve the fine-structure constant \(\alpha\). More...
|
| |
| const double | getAlsMz () const |
| | A get method to access the value of \(\alpha_s(M_Z)\). More...
|
| |
| virtual const double | getCBd () const |
| | The ratio of the absolute value of the $B_d$ mixing amplitude over the Standard Model value. More...
|
| |
| virtual const double | getCBs () const |
| | The ratio of the absolute value of the $B_s$ mixing amplitude over the Standard Model value. More...
|
| |
| virtual const double | getCCC1 () const |
| | A virtual implementation for the RealWeakEFTCC class. More...
|
| |
| virtual const double | getCCC2 () const |
| | A virtual implementation for the RealWeakEFTCC class. More...
|
| |
| virtual const double | getCCC3 () const |
| | A virtual implementation for the RealWeakEFTCC class. More...
|
| |
| virtual const double | getCCC4 () const |
| | A virtual implementation for the RealWeakEFTCC class. More...
|
| |
| virtual const double | getCCC5 () const |
| | A virtual implementation for the RealWeakEFTCC class. More...
|
| |
| virtual const double | getCDMK () const |
| | The ratio of the real part of the $K$ mixing amplitude over the Standard Model value. More...
|
| |
| virtual const double | getCepsK () const |
| | The ratio of the imaginary part of the $K$ mixing amplitude over the Standard Model value. More...
|
| |
| const CKM & | getCKM () const |
| | A get method to retrieve the member object of type CKM. More...
|
| |
| const double | getDAle5Mz () const |
| | A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More...
|
| |
| const double | getDelGammaWlv () const |
| | A get method to retrieve the theoretical uncertainty in \(\Gamma_W_{l\nu}\), denoted as \(\delta\,\Gamma_W_{l\nu}\). More...
|
| |
| const double | getDelGammaWqq () const |
| | A get method to retrieve the theoretical uncertainty in \(\Gamma_W_{qq}\), denoted as \(\delta\,\Gamma_W_{qq}\). More...
|
| |
| const double | getDelGammaZ () const |
| | A get method to retrieve the theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\). More...
|
| |
| const double | getDelMw () const |
| | A get method to retrieve the theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\). More...
|
| |
| const double | getDelR0b () const |
| | A get method to retrieve the theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More...
|
| |
| const double | getDelR0c () const |
| | A get method to retrieve the theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More...
|
| |
| const double | getDelR0l () const |
| | A get method to retrieve the theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More...
|
| |
| const double | getDelSigma0H () const |
| | A get method to retrieve the theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\). More...
|
| |
| const double | getDelSin2th_b () const |
| | A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More...
|
| |
| const double | getDelSin2th_l () const |
| | A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More...
|
| |
| const double | getDelSin2th_q () const |
| | A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More...
|
| |
| const std::string | getFlagKappaZ () const |
| | A method to retrieve the model flag KappaZ. More...
|
| |
| const std::string | getFlagMw () const |
| | A method to retrieve the model flag Mw. More...
|
| |
| const std::string | getFlagRhoZ () const |
| | A method to retrieve the model flag RhoZ. More...
|
| |
| const Flavour & | getFlavour () const |
| |
| const double | getGF () const |
| | A get method to retrieve the Fermi constant \(G_\mu\). More...
|
| |
| const int | getIterationNo () const |
| |
| const Particle & | getLeptons (const QCD::lepton p) const |
| | A get method to retrieve the member object of a lepton. More...
|
| |
| virtual const double | getMHl () const |
| | A get method to retrieve the Higgs mass \(m_h\). More...
|
| |
| virtual const double | getmq (const QCD::quark q, const double mu) const |
| | The MSbar running quark mass computed at NLO. More...
|
| |
| const double | getMuw () const |
| | A get method to retrieve the matching scale \(\mu_W\) around the weak scale. More...
|
| |
| const double | getMw () const |
| | A get method to access the input value of the mass of the \(W\) boson \(M_W\). More...
|
| |
| EWSMApproximateFormulae * | getMyApproximateFormulae () const |
| | A get method to retrieve the member pointer of type EWSMApproximateFormulae. More...
|
| |
| EWSMcache * | getMyEWSMcache () const |
| | A get method to retrieve the member pointer of type EWSMcache. More...
|
| |
| LeptonFlavour * | getMyLeptonFlavour () const |
| |
| EWSMOneLoopEW * | getMyOneLoopEW () const |
| | A get method to retrieve the member pointer of type EWSMOneLoopEW,. More...
|
| |
| EWSMThreeLoopEW * | getMyThreeLoopEW () const |
| |
| EWSMThreeLoopEW2QCD * | getMyThreeLoopEW2QCD () const |
| |
| EWSMThreeLoopQCD * | getMyThreeLoopQCD () const |
| |
| EWSMTwoFermionsLEP2 * | getMyTwoFermionsLEP2 () const |
| | A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More...
|
| |
| EWSMTwoLoopEW * | getMyTwoLoopEW () const |
| |
| EWSMTwoLoopQCD * | getMyTwoLoopQCD () const |
| |
| const double | getMz () const |
| | A get method to access the mass of the \(Z\) boson \(M_Z\). More...
|
| |
| virtual const double | getPhiBd () const |
| | Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More...
|
| |
| virtual const double | getPhiBs () const |
| | Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More...
|
| |
| const gslpp::matrix< gslpp::complex > | getUPMNS () const |
| | A get method to retrieve the object of the PMNS matrix. More...
|
| |
| const gslpp::matrix< gslpp::complex > | getVCKM () const |
| | A get method to retrieve the CKM matrix. More...
|
| |
| const gslpp::matrix< gslpp::complex > & | getYd () const |
| | A get method to retrieve the Yukawa matrix of the down-type quarks, \(Y_d\). More...
|
| |
| const gslpp::matrix< gslpp::complex > & | getYe () const |
| | A get method to retrieve the Yukawa matrix of the charged leptons, \(Y_e\). More...
|
| |
| const gslpp::matrix< gslpp::complex > & | getYn () const |
| | A get method to retrieve the Yukawa matrix of the neutrinos, \(Y_\nu\). More...
|
| |
| const gslpp::matrix< gslpp::complex > & | getYu () const |
| | A get method to retrieve the Yukawa matrix of the up-type quarks, \(Y_u\). More...
|
| |
| virtual const double | gLnuN2 () const |
| | The effective neutrino nucleon LH coupling: gLnuN2. More...
|
| |
| virtual const double | gRnuN2 () const |
| | The effective neutrino nucleon RH coupling: gRnuN2. More...
|
| |
| virtual const double | gVnue () const |
| | The effective (muon) neutrino-electron vector coupling: gVnue. More...
|
| |
| gslpp::complex | I_triangle_1 (const double tau, const double lambda) const |
| | Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
|
| |
| gslpp::complex | I_triangle_2 (const double tau, const double lambda) const |
| | Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
|
| |
| virtual bool | InitializeModel () |
| | A method to initialize the model. More...
|
| |
| const double | intMLL2eeeeus2 (const double s, const double t0, const double t1) const |
| |
| const double | intMLR2eeeets2 (const double s, const double t0, const double t1) const |
| |
| const double | intMLRtilde2eeeest2 (const double s, const double t0, const double t1) const |
| |
| const double | intMRR2eeeeus2 (const double s, const double t0, const double t1) const |
| |
| const bool | IsFlagNoApproximateGammaZ () const |
| | A method to retrieve the model flag NoApproximateGammaZ. More...
|
| |
| const bool | IsFlagWithoutNonUniversalVC () const |
| | A method to retrieve the model flag WithoutNonUniversalVC. More...
|
| |
| const bool | isSMSuccess () const |
| | A get method to retrieve the success status of the Standard Model update and matching. More...
|
| |
| virtual const double | LEP2AFBbottom (const double s) const |
| |
| virtual const double | LEP2AFBcharm (const double s) const |
| |
| virtual const double | LEP2AFBe (const double s) const |
| |
| virtual const double | LEP2AFBmu (const double s) const |
| |
| virtual const double | LEP2AFBtau (const double s) const |
| |
| virtual const double | LEP2dsigmadcosBinE (const double s, const double cos, const double cosmin, const double cosmax) const |
| |
| virtual const double | LEP2dsigmadcosBinMu (const double s, const double cos, const double cosmin, const double cosmax) const |
| |
| virtual const double | LEP2dsigmadcosBinTau (const double s, const double cos, const double cosmin, const double cosmax) const |
| |
| virtual const double | LEP2dsigmadcosE (const double s, const double cos) const |
| |
| virtual const double | LEP2dsigmadcosMu (const double s, const double cos) const |
| |
| virtual const double | LEP2dsigmadcosTau (const double s, const double cos) const |
| |
| virtual const double | LEP2Rbottom (const double s) const |
| |
| virtual const double | LEP2Rcharm (const double s) const |
| |
| virtual const double | LEP2sigmaBottom (const double s) const |
| |
| virtual const double | LEP2sigmaCharm (const double s) const |
| |
| virtual const double | LEP2sigmaE (const double s) const |
| |
| virtual const double | LEP2sigmaHadron (const double s) const |
| |
| virtual const double | LEP2sigmaMu (const double s) const |
| |
| virtual const double | LEP2sigmaTau (const double s) const |
| |
| const double | MLL2eeff (const Particle f, const double s, const double t) const |
| |
| const double | MLR2eeff (const Particle f, const double s) const |
| |
| const double | MRL2eeff (const Particle f, const double s) const |
| |
| const double | MRR2eeff (const Particle f, const double s, const double t) const |
| |
| const double | Mw_tree () const |
| | The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). More...
|
| |
| const double | MwbarFromMw (const double Mw) const |
| | A method to convert the \(W\)-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More...
|
| |
| const double | MwFromMwbar (const double Mwbar) const |
| | A method to convert the \(W\)-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More...
|
| |
| double | Mzbar () const |
| | The \(Z\)-boson mass \(\overline{M}_Z\) in the complex-pole/fixed-width scheme. More...
|
| |
| virtual const double | Qwemoller (const double q2, const double y) const |
| | The computation of the electron's weak charge. More...
|
| |
| virtual const double | Qwn () const |
| | The computation of the neutron weak charge: Qwn. More...
|
| |
| virtual const double | Qwp () const |
| | The computation of the proton weak charge: Qwp. More...
|
| |
| virtual const double | rho_GammaW (const Particle fi, const Particle fj) const |
| | EW radiative corrections to the width of \(W \to f_i \bar{f}_j\), denoted as \(\rho^W_{ij}\). More...
|
| |
| const double | s02 () const |
| | The square of the sine of the weak mixing angle \(s_0^2\) defined without weak radiative corrections. More...
|
| |
| void | setCKM (const CKM &CKMMatrix) |
| | A set method to change the CKM matrix. More...
|
| |
| void | setFlagCacheInStandardModel (bool FlagCacheInStandardModel) |
| | A set method to change the model flag CacheInStandardModel of StandardModel. More...
|
| |
| void | setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ) |
| |
| bool | setFlagSigmaForAFB (const bool flagSigmaForAFB_i) |
| |
| bool | setFlagSigmaForR (const bool flagSigmaForR_i) |
| |
| void | setRequireCKM (bool requireCKM) |
| | A set method to change the value of requireCKM. More...
|
| |
| void | setSMSuccess (bool success) const |
| | A set method to change the success status of the Standard Model update and matching. More...
|
| |
| void | setYd (const gslpp::matrix< gslpp::complex > &Yd) |
| | A set method to set the Yukawa matrix of the down-type quarks, \(Y_d\). More...
|
| |
| void | setYe (const gslpp::matrix< gslpp::complex > &Ye) |
| | A set method to set the Yukawa matrix of the charged leptons, \(Y_e\). More...
|
| |
| void | setYu (const gslpp::matrix< gslpp::complex > &Yu) |
| | A set method to set the Yukawa matrix of the up-type quarks, \(Y_u\). More...
|
| |
| virtual const double | SigmaeeHee (const double sqrt_s, const double Pe, const double Pp) const |
| | The \(\sigma(e^+ e^- \to e^+ e^- H)\) in the Standard Model. More...
|
| |
| virtual const double | SigmaeeHvv (const double sqrt_s, const double Pe, const double Pp) const |
| | The \(\sigma(e^+ e^- \to \nu \bar{\nu} H)\) in the Standard Model. More...
|
| |
| virtual const double | SigmaeeZH (const double sqrt_s, const double Pe, const double Pp) const |
| | The \(\sigma(e^+ e^- \to Z H)\) in the Standard Model. More...
|
| |
| | StandardModel () |
| | The default constructor. More...
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| const double | sW2 () const |
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| 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...
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| 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...
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| 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...
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| virtual const double | TauLFU_gmuge () const |
| | The computation of the LFU ratio \(g_\mu/ g_e \). More...
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| virtual const double | TauLFU_gtauge () const |
| | The computation of the LFU ratio \(g_\tau/ g_e \). More...
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| virtual const double | TauLFU_gtaugmu () const |
| | The computation of the LFU ratio \(g_\tau/ g_\mu \). More...
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| virtual const double | TauLFU_gtaugmuK () const |
| | The computation of the LFU ratio \(\left(g_\tau/ g_\mu\right)_K \). More...
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| virtual const double | TauLFU_gtaugmuPi () const |
| | The computation of the LFU ratio \(\left(g_\tau/ g_\mu\right)_\pi \). More...
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| virtual const double | ThetaLnuN () const |
| | The effective neutrino nucleon LH parameter: ThetaLnuN. More...
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| virtual const double | ThetaRnuN () const |
| | The effective neutrino nucleon RH parameter: ThetaRnuN. More...
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| const double | tovers2 (const double cosmin, const double cosmax) const |
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| const double | uovers2 (const double cosmin, const double cosmax) const |
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| const double | v () const |
| | The Higgs vacuum expectation value. More...
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| virtual | ~StandardModel () |
| | The default destructor. More...
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| const double | AboveTh (const double mu) const |
| | The active flavour threshold above the scale \(\mu\) as defined in QCD::Thresholds(). More...
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| void | addParameters (std::vector< std::string > params_i) |
| | A method to add parameters that are specific to only one set of observables. More...
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| 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...
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| const double | Als (const double mu, const orders order=FULLNLO, const bool Nf_thr=true) const |
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| 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...
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| const double | AlsByOrder (const double mu, const int Nf_in, const orders order=FULLNLO) const |
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| const double | AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const |
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| 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...
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| 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...
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| 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...
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| const double | BelowTh (const double mu) const |
| | The active flavour threshold below the scale \(\mu\) as defined in QCD::Thresholds(). More...
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| const double | Beta0 (const double nf) const |
| | The \(\beta_0(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
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| const double | Beta1 (const double nf) const |
| | The \(\beta_1(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
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| const double | Beta2 (const double nf) const |
| | The \(\beta_2(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
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| const double | Beta3 (const double nf) const |
| | The \(\beta_3(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
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| void | CacheShift (double cache[][5], int n) const |
| | A member used to manage the caching for this class. More...
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| void | CacheShift (int cache[][5], int n) const |
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| const orders | FullOrder (orders order) const |
| | Return the FULLORDER enum corresponding to order. More...
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| const double | Gamma0 (const double nf) const |
| | The \(\gamma_0\) coefficient used to compute the running of a mass. More...
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| const double | Gamma1 (const double nf) const |
| | The \(\gamma_1\) coefficient used to compute the running of a mass. More...
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| const double | Gamma2 (const double nf) const |
| | The \(\gamma_2\) coefficient used to compute the running of a mass. More...
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| const double | getAlsM () const |
| | A get method to access the value of \(\alpha_s(M_{\alpha_s})\). More...
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| 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...
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| 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...
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| 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...
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| 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...
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| 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...
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| 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...
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| const BParameter & | getBKd1 () const |
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| const BParameter & | getBKd3 () const |
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| const double | getCF () const |
| | A get method to access the Casimir factor of QCD. More...
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| 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...
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| const Meson & | getMesons (const QCD::meson m) const |
| | A get method to access a meson as an object of the type Meson. More...
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| const double | getMtpole () const |
| | A get method to access the pole mass of the top quark. More...
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| const double | getMub () const |
| | A get method to access the threshold between five- and four-flavour theory in GeV. More...
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| const double | getMuc () const |
| | A get method to access the threshold between four- and three-flavour theory in GeV. More...
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| const double | getMut () const |
| | A get method to access the threshold between six- and five-flavour theory in GeV. More...
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| const double | getNc () const |
| | A get method to access the number of colours \(N_c\). More...
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| const double | getOptionalParameter (std::string name) const |
| | A method to get parameters that are specific to only one set of observables. More...
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| const Particle & | getQuarks (const QCD::quark q) const |
| | A get method to access a quark as an object of the type Particle. More...
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| 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...
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| void | initializeBParameter (std::string name_i) const |
| | A method to initialize B Parameter and the corresponding meson. More...
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| void | initializeMeson (QCD::meson meson_i) const |
| | A method to initialize a meson. More...
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| bool | isQCDsuccess () const |
| | A getter for the QCDsuccess flag. More...
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| const double | logLambda (const double nf, orders order) const |
| | Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More...
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| 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...
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| 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...
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| 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...
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| 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...
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| 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...
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| 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...
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| const double | MS2DRqmass (const double MSbar) const |
| | Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More...
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| 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...
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| const double | Nf (const double mu) const |
| | The number of active flavour at scale \(\mu\). More...
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| 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...
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| const std::string | orderToString (const orders order) const |
| | Converts an object of the enum type "orders" to the corresponding string. More...
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| | QCD () |
| | Constructor. More...
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| void | setComputemt (bool computemt) |
| | A set method to change the value of computemt. More...
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| void | setMtpole (double mtpole_in) |
| | A method to set the pole mass of the top quark. More...
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| void | setNc (double Nc) |
| | A set method to change the number of colours \(N_c\). More...
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| 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...
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| void | setQuarkMass (const quark q, const double mass) |
| | A set method to change the mass of a quark. More...
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| const double | Thresholds (const int i) const |
| | For accessing the active flavour threshold scales. More...
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| void | addMissingModelParameter (const std::string &missingParameterName) |
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| std::vector< std::string > | getmissingModelParameters () |
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| unsigned int | getMissingModelParametersCount () |
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| std::string | getModelName () const |
| | A method to fetch the name of the model. More...
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| const double & | getModelParam (std::string name) const |
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| bool | isModelFWC_DF2 () const |
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| bool | isModelGeneralTHDM () const |
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| bool | isModelGeorgiMachacek () const |
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| bool | IsModelInitialized () const |
| | A method to check if the model is initialized. More...
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| bool | isModelLinearized () const |
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| bool | isModelNPquadratic () const |
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| bool | isModelParam (std::string name) const |
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| bool | isModelSUSY () const |
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| bool | isModelTHDM () const |
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| bool | isModelTHDMW () const |
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| bool | IsUpdateError () const |
| | A method to check if there was any error in the model update process. More...
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| | Model () |
| | The default constructor. More...
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| void | raiseMissingModelParameterCount () |
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| void | setModelFWC_DF2 () |
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| void | setModelGeneralTHDM () |
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| void | setModelGeorgiMachacek () |
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| void | setModelInitialized (bool ModelInitialized) |
| | A set method to fix the failure or success of the initialization of the model. More...
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| void | setModelLinearized (bool linearized=true) |
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| void | setModelName (const std::string name) |
| | A method to set the name of the model. More...
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| void | setModelNPquadratic (bool NPquadratic=true) |
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| void | setModelSUSY () |
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| void | setModelTHDM () |
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| void | setModelTHDMW () |
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| void | setSliced (bool Sliced) |
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| void | setUpdateError (bool UpdateError) |
| | A set method to fix the update status as success or failure. More...
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| virtual | ~Model () |
| | The default destructor. More...
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master
1.9.2 