master
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a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models |
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master
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a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models |
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A model class extending the StandardModel Higgs sector with seven flavour-universal couplings. More...
#include <HiggsKigen.h>
Inheritance diagram for HiggsKigen:A model class extending the StandardModel Higgs sector with seven flavour-universal couplings.
This is a Model class containing parameters and functions associated to rescaling the Higgs decay into vector bosons ( \(\kappa_W,\kappa_Z\)), gluons ( \(\kappa_g\)), photons ( \(\kappa_\gamma\)), Z and photons ( \(\kappa_{Z\gamma}\)) and fermions ( \(\kappa_{u,c,t}, \kappa_{d,s,b}, \kappa_{e\mu\tau}\)) (as well as the corresponding production mechanisms) with respect to the StandardModel. The possibility of extra decay width is also parametrized independently by Br \((H\to invisible)\) and Br \((H\to exotic)\). This class inherits from the NPbase class, which defines parameters related to generic extensions of the StandardModel Higgs sector.
After creating an instance of the current class, it is required to call the initialization method InitializeModel(), which is needed by the base class.
The initializations and updates of the model parameters are explained below.
The model parameters of HiggsKigen (in addition to the StandardModel ones) are summarized below:
| Label | LaTeX symbol | Description |
|---|---|---|
| Kw | \(\kappa_W\) | The factor rescaling all Higgs couplings to the W vector bosons with respect to the SM. |
| Kz | \(\kappa_Z\) | The factor rescaling all Higgs couplings to the Z vector bosons with respect to the SM. |
| Kg | \(\kappa_g\) | The factor rescaling all Higgs couplings to gluons with respect to the SM. |
| Kga | \(\kappa_ga\) | The factor rescaling all Higgs couplings to photons with respect to the SM. |
| Kzga | \(\kappa_{zga}\) | The factor rescaling all Higgs couplings to the Z and a photon with respect to the SM. |
| Ku | \(\kappa_u\) | The factor rescaling all Higgs couplings to the up quark with respect to the SM. |
| Kc | \(\kappa_c\) | The factor rescaling all Higgs couplings to the charm quark with respect to the SM. |
| Kt | \(\kappa_t\) | The factor rescaling all Higgs couplings to the top quark with respect to the SM. |
| Kd | \(\kappa_d\) | The factor rescaling all Higgs couplings to the down quark with respect to the SM. |
| Ks | \(\kappa_s\) | The factor rescaling all Higgs couplings to the strange quark with respect to the SM. |
| Kb | \(\kappa_b\) | The factor rescaling all Higgs couplings to the bottom quark with respect to the SM. |
| Ke | \(\kappa_e\) | The factor rescaling all Higgs couplings to electrons with respect to the SM. |
| Kmu | \(\kappa_\mu\) | The factor rescaling all Higgs couplings to muons with respect to the SM. |
| Ktau | \(\kappa_\tau\) | The factor rescaling all Higgs couplings to taus with respect to the SM. |
| KH | \(\kappa_H\) | The factor rescaling the Higgs total width with respect to the SM. (Only applies when flag UseKH is true. ) |
| BrHinv | Br \((H\to invisible)\) | The branching ratio of invisible Higgs decays. Only the absolute value of this parameter is considered. |
| BrHexo | Br \((H\to exotic (visible))\) | The branching ratio of exotic, not invisible, Higgs decays. Only the absolute value of this parameter is considered. (If flag UseKH is true this parameter is ignored and it is recomputed as a function of KH. ) |
| eXint | \(\varepsilon_{X}^{int}\) | The relative intrinsic theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.) |
| eXpar | \(\varepsilon_{X}^{par}\) | The relative parametric theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.) |
The Flags of HiggsKigen are summarized below:
| Label | Value | Description |
|---|---|---|
| KiLoop | TRUE / FALSE | This flag is set to TRUE if independent kappa's are used for the loop induced processes (g,ga,Zga). The default value is TRUE. |
| Custodial | TRUE / FALSE | This flag is set to TRUE if KZ=KW is assumed. The default value is FALSE. |
| UniversalKf | TRUE / FALSE | This flag is set to TRUE if all Kf are assumed to take the same universal value. The value is controlled by the parameter Kt. The default value is FALSE. |
| UniversalK | TRUE / FALSE | This flag is set to TRUE if all K are assumed to take the same universal value. The value is controlled by the parameter Kt. (It does not apply to the extra BR.) The default value is FALSE. |
| UseKH | TRUE / FALSE | This flag is set to TRUE if the total Higgs width is rescaled by KH. Otherwise, it is computed from the other SM decays, BrHinv and BrHexo. (If true BrHexo is ignored and computed from KH.) The default value is FALSE. |
Please read information about parameter initialization and update in the documentation of the StandardModel class.
Definition at line 198 of file HiggsKigen.h.
Public Member Functions | |
| virtual const double | Br_H_exo () const |
| The branching ratio of the of the Higgs into exotic particles (invisible or not). 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 | BrH4fRatio () const |
| The ratio of the Br \((H\to 4f)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4L2Ratio () const |
| The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4LRatio () const |
| The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4lRatio () const |
| The ratio of the Br \((H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4muRatio () const |
| The ratio of the Br \((H\to 4\mu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4uRatio () const |
| The ratio of the Br \((H\to 4u)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4vRatio () const |
| The ratio of the Br \((H\to 4v)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHbbRatio () const |
| The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHccRatio () const |
| The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHevmuvRatio () const |
| The ratio of the Br \((H\to e\nu \mu\nu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHgagaRatio () const |
| The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHggRatio () const |
| The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHll_vvorjjRatio () const |
| The ratio of the Br \((H\to l l \nu\nu, l l j j)\), \(l=e,\mu,~~j\not=b)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHlljjRatio () const |
| The ratio of the Br \((H\to l l j j)\), \(l=e,\mu,~~j\not=b)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHlv_lvorjjRatio () const |
| The ratio of the Br \((H\to l \nu l \nu, l \nu j j)\), \(l=e,\mu,~~j\not=b)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHlvjjRatio () const |
| The ratio of the Br \((H\to l \nu j j)\), \(l=e,\mu,~~j\not=b)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHLvudRatio () const |
| The ratio of the Br \((H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHLvvLRatio () const |
| The ratio of the Br \((H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHmumuRatio () const |
| The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHssRatio () const |
| The ratio of the Br \((H\to s\bar{s})\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHtautauRatio () const |
| The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHtoinvRatio () const |
| The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHudduRatio () const |
| The ratio of the Br \((H\to uddu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHvisRatio () const |
| The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHVVRatio () const |
| The ratio of the Br \((H\to VV)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHWWRatio () const |
| The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZgaeeRatio () const |
| The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZgallRatio () const |
| The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZgamumuRatio () const |
| The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZgaRatio () const |
| The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZZRatio () const |
| The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model. More... | |
| virtual bool | CheckParameters (const std::map< std::string, double > &DPars) |
| A method to check if all the mandatory parameters for HiggsKigen have been provided in model initialization. More... | |
| virtual const double | computeGammaTotalnoErrorRatio () const |
| The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model and neglecting theory errors. More... | |
| virtual const double | computeGammaTotalRatio () const |
| The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More... | |
| virtual const double | computeGammaTotalSMnoErrorRatio () const |
| The ratio of the \(\Gamma(H\to SM)\) in the current model and in the Standard Model, including only SM decays and neglecting theory errors. More... | |
| virtual const double | computeGammaTotalSMRatio () const |
| The ratio of the \(\Gamma(H\to SM)\) in the current model and in the Standard Model, including only SM decays. 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_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_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_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). 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_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_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 | 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_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More... | |
| virtual const double | deltaG_hAA () const |
| The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual const double | deltaG_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 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 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_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... | |
| double | getBrHexo () const |
| A get method to retrieve the exotic (not invisible) Higgs branching ratio. More... | |
| double | getBrHinv () const |
| A get method to retrieve the invisible Higgs branching ratio. More... | |
| double | getKb () const |
| A get method to retrieve the factor rescaling the Higgs coupling to b quarks with respect to the SM \(K_b\). More... | |
| double | getKc () const |
| A get method to retrieve the factor rescaling the Higgs coupling to c quarks with respect to the SM \(K_c\). More... | |
| double | getKd () const |
| A get method to retrieve the factor rescaling the Higgs coupling to d quarks with respect to the SM \(K_d\). More... | |
| double | getKe () const |
| A get method to retrieve the factor rescaling the Higgs coupling to electrons with respect to the SM \(K_e\). More... | |
| double | getKg () const |
| A get method to retrieve the factor rescaling the Higgs coupling to gluons with respect to the SM \(K_g\). More... | |
| double | getKga () const |
| A get method to retrieve the factor rescaling the Higgs coupling to photons with respect to the SM \(K_ga\). More... | |
| double | getKH () const |
| A get method to retrieve the factor rescaling the total Higgs width with respect to the SM \(K_H\). More... | |
| double | getKmu () const |
| A get method to retrieve the factor rescaling the Higgs coupling to muons with respect to the SM \(K_\mu\). More... | |
| double | getKs () const |
| A get method to retrieve the factor rescaling the Higgs coupling to s quarks with respect to the SM \(K_s\). More... | |
| double | getKt () const |
| A get method to retrieve the factor rescaling the Higgs coupling to t quarks with respect to the SM \(K_t\). More... | |
| double | getKtau () const |
| A get method to retrieve the factor rescaling the Higgs coupling to taus with respect to the SM \(K_\tau\). More... | |
| double | getKu () const |
| A get method to retrieve the factor rescaling the Higgs coupling to u quarks with respect to the SM \(K_u\). More... | |
| double | getKw () const |
| A get method to retrieve the factor rescaling the Higgs coupling to the W vector bosons with respect to the SM \(K_W\). More... | |
| double | getKz () const |
| A get method to retrieve the factor rescaling the Higgs coupling to the Z vector bosons with respect to the SM \(K_Z\). More... | |
| double | getKzga () const |
| A get method to retrieve the factor rescaling the Higgs coupling to Z and photon with respect to the SM \(K_{zga}\). More... | |
| HiggsKigen () | |
| The default constructor. More... | |
| virtual const double | kappaAeff () const |
| The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\). More... | |
| virtual const double | kappabeff () const |
| The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\). More... | |
| virtual const double | kappaceff () const |
| The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\). More... | |
| virtual const double | kappaGeff () const |
| The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\). More... | |
| virtual const double | kappamueff () const |
| The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\). More... | |
| virtual const double | kappataueff () const |
| The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\). More... | |
| virtual const double | kappaWeff () const |
| The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\). 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 | 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 | 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 | mueeZllH (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZqqH (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muepWBF (const double sqrt_s) const |
| The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muepZBF (const double sqrt_s) const |
| The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muggH (const double sqrt_s) const |
| The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muggHbb (const double sqrt_s) const |
| 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 | 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 | 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 | 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 | obliqueS () const |
| The oblique parameter \(S\). More... | |
| virtual const double | obliqueT () const |
| The oblique parameter \(T\). More... | |
| virtual const double | obliqueU () const |
| The oblique parameter \(U\). More... | |
| virtual bool | PostUpdate () |
| The post-update method for HiggsKigen. More... | |
| void | setBrHexo (double BrHexo) |
| A set method to change the exotic (not invisible) Higgs branching ratio. More... | |
| void | setBrHinv (double BrHinv) |
| A set method to change the invisible Higgs branching ratio. More... | |
| virtual bool | setFlag (const std::string name, const bool value) |
| A method to set a flag of HiggsKigen. More... | |
| void | setKb (double Kb) |
| A set method to change the factor rescaling the Higgs coupling to b quarks with respect to the SM \(K_b\). More... | |
| void | setKc (double Kc) |
| A set method to change the factor rescaling the Higgs coupling to c quarks with respect to the SM \(K_c\). More... | |
| void | setKd (double Kd) |
| A set method to change the factor rescaling the Higgs coupling to d quarks with respect to the SM \(K_d\). More... | |
| void | setKe (double Ke) |
| A set method to change the factor rescaling the Higgs coupling to electrons with respect to the SM \(K_e\). More... | |
| void | setKg (double Kg) |
| A set method to change the factor rescaling the Higgs coupling to gluons with respect to the SM \(K_g\). More... | |
| void | setKga (double Kga) |
| A set method to change the factor rescaling the Higgs coupling to photons with respect to the SM \(K_ga\). More... | |
| void | setKH (double KH) |
| A set method to change the factor rescaling the total Higgs width with respect to the SM \(K_H\). More... | |
| void | setKmu (double Kmu) |
| A set method to change the factor rescaling the Higgs coupling to muons with respect to the SM \(K_\mu\). More... | |
| void | setKs (double Ks) |
| A set method to change the factor rescaling the Higgs coupling to s quarks with respect to the SM \(K_s\). More... | |
| void | setKt (double Kt) |
| A set method to change the factor rescaling the Higgs coupling to t quarks with respect to the SM \(K_t\). More... | |
| void | setKtau (double Ktau) |
| A set method to change the factor rescaling the Higgs coupling to taus with respect to the SM \(K_\tau\). More... | |
| void | setKu (double Ku) |
| A set method to change the factor rescaling the Higgs coupling to u quarks with respect to the SM \(K_u\). More... | |
| void | setKw (double Kw) |
| A set method to change the factor rescaling the Higgs coupling to the W vector bosons with respect to the SM \(K_W\). More... | |
| void | setKz (double Kz) |
| A set method to change the factor rescaling the Higgs coupling to the Z vector bosons with respect to the SM \(K_Z\). More... | |
| void | setKzga (double Kzga) |
| A set method to change the factor rescaling the Higgs coupling to Z and photon with respect to the SM \(K_{zga}\). More... | |
| virtual | ~HiggsKigen () |
| The default destructor. More... | |
| Public Member Functions inherited from NPbase | |
| virtual const double | A_f (const Particle f) const |
| The left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\mathcal{A}_f\). More... | |
| virtual const double | AFB (const Particle f) const |
| The forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(A^f_{FB}\). More... | |
| virtual const double | alphaMz () const |
| The electromagnetic coupling at the \(Z\)-mass scale, \(\alpha(M_Z^2)=\alpha/(1-\Delta\alpha(M_Z^2))\). More... | |
| virtual const double | aPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More... | |
| virtual const double | bPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More... | |
| virtual const double | BR_Zf (const Particle f) const |
| The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\). More... | |
| virtual const double | BrW (const Particle fi, const Particle fj) const |
| The branching ratio of the \(W\) boson decaying into a SM fermion pair, \(Br(W\to f_i f_j)\). More... | |
| virtual const double | C1eeHvv (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| virtual const double | C1eettH (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| virtual const double | C1eeWBF (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| virtual const double | C1eeZBF (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| virtual const double | C1eeZH (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| virtual const double | cbminuscc () const |
| virtual const double | cbminusctau () const |
| virtual const double | ccminusctau () const |
| virtual const double | CEWHd11 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{11}\). More... | |
| virtual const double | CEWHd22 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{22}\). More... | |
| virtual const double | CEWHd33 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{33}\). More... | |
| virtual const double | CEWHe11 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{11}\). More... | |
| virtual const double | CEWHe22 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{22}\). More... | |
| virtual const double | CEWHe33 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{33}\). More... | |
| virtual const double | CEWHL111 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{11}\). More... | |
| virtual const double | CEWHL122 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{22}\). More... | |
| virtual const double | CEWHL133 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{33}\). More... | |
| virtual const double | CEWHL311 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{11}\). More... | |
| virtual const double | CEWHL322 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{22}\). More... | |
| virtual const double | CEWHL333 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{33}\). More... | |
| virtual const double | CEWHQ111 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{11}\). More... | |
| virtual const double | CEWHQ122 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{22}\). More... | |
| virtual const double | CEWHQ133 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{33}\). More... | |
| virtual const double | CEWHQ311 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{11}\). More... | |
| virtual const double | CEWHQ322 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{22}\). More... | |
| virtual const double | CEWHQ333 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{33}\). More... | |
| virtual const double | CEWHQd33 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(d)})_{33}\). More... | |
| virtual const double | CEWHQu33 (const double mu) const |
| Combination of coefficients of the Warsaw basis not constrained by EWPO (at LO) \((\hat{C}_{HQ}^{(u)})_{33}\). More... | |
| virtual const double | CEWHu11 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{11}\). More... | |
| virtual const double | CEWHu22 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{22}\). More... | |
| virtual const double | CEWHu33 (const double mu) const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{33}\). More... | |
| virtual const double | cgaga_HB (const double mu) const |
| The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | cgaplusct () const |
| virtual const double | cgg_HB (const double mu) const |
| The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | cggEff_HB (const double mu) const |
| The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) More... | |
| virtual const double | cgminuscga () const |
| virtual const double | cgplusct () const |
| virtual const double | cVpluscb () const |
| virtual const double | cVplusctau () const |
| virtual const double | cZBox_HB (const double mu) const |
| The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | cZga_HB (const double mu) const |
| The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | cZZ_HB (const double mu) const |
| The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | delta2sBRH3 (const double C1prod, const double C1Hxx) const |
| Quadratic contribution from the Higgs self-couplings modifications to the signal strength for \(\sigma \times BR(H\to xx)\) in the current model. More... | |
| virtual const double | delta2sH3 (const double C1) const |
| Quadratic contribution from the Higgs self-couplings modifications to the signal strength for an observable \(\sigma\) in the current model. More... | |
| virtual const double | delta_mubbH_1 (const double sqrt_s) const |
| virtual const double | delta_mubbH_2 (const double sqrt_s) const |
| virtual const double | delta_muggH_1 (const double sqrt_s) const |
| virtual const double | delta_muggH_2 (const double sqrt_s) const |
| virtual const double | delta_mutH_1 (const double sqrt_s) const |
| virtual const double | delta_mutH_2 (const double sqrt_s) const |
| virtual const double | delta_muttH_1 (const double sqrt_s) const |
| virtual const double | delta_muttH_2 (const double sqrt_s) const |
| virtual const double | delta_muVBF_1 (const double sqrt_s) const |
| virtual const double | delta_muVBF_2 (const double sqrt_s) const |
| virtual const double | delta_muVH_1 (const double sqrt_s) const |
| virtual const double | delta_muVH_2 (const double sqrt_s) const |
| virtual const double | delta_muWH_1 (const double sqrt_s) const |
| virtual const double | delta_muWH_2 (const double sqrt_s) const |
| virtual const double | delta_muZH_1 (const double sqrt_s) const |
| virtual const double | delta_muZH_2 (const double sqrt_s) const |
| virtual const double | deltaA_f (const Particle f) const |
| The new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta \mathcal{A}_f\). More... | |
| virtual const double | deltaA_f_2 (const Particle f) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\Delta \mathcal{A}_f^{(2)}\). More... | |
| virtual const double | deltaAFB (const Particle f) const |
| The new physics contribution to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta A^f_{FB}\). More... | |
| virtual const double | deltaAFB_2 (const Particle f) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\Delta A^f_{FB}\). More... | |
| virtual const double | deltacZ_HB (const double mu) const |
| The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | deltadxsdcoseeWWlvjjLEP2 (const double sqrt_s, const int bin) const |
| The new physics contribution to the differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph]. More... | |
| virtual const double | deltaeNP (const double mu) const |
| The new physics relative contribution to the EW coupling constant \(e\). More... | |
| virtual const double | deltaG1_hWW_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_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_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_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More... | |
| virtual const double | deltag1gaNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More... | |
| virtual const double | deltag1ZNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More... | |
| virtual const double | deltag1ZNPEff () const |
| The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More... | |
| virtual const double | deltaG2_hWW_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_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_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_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_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More... | |
| virtual const double | deltaG_hAA_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_mu (const double mu) const |
| The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual gslpp::complex | deltaG_hff_mu (const Particle p, const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More... | |
| virtual const double | deltaG_hgg_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_mu (const double mu) const |
| The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual const double | deltaG_hhhRatio () const |
| The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More... | |
| virtual const double | deltaG_hhhRatio_mu (const double mu) const |
| The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More... | |
| virtual const double | deltaGA_f (const Particle f) const |
| New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| virtual const double | deltaGA_f_2 (const Particle f) const |
| virtual const double | deltaGamma_W () const |
| The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\). More... | |
| virtual const double | deltaGamma_Wff (const Particle fi, const Particle fj) const |
| The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More... | |
| virtual const double | deltaGamma_Z () const |
| The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\). More... | |
| virtual const double | deltaGamma_Z_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the total decay width of the \(Z\) boson, \(\Delta \Gamma_Z^{(2)}\). More... | |
| virtual const double | deltaGamma_Zf (const Particle f) const |
| The new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More... | |
| virtual const double | deltaGamma_Zf_2 (const Particle f) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\Delta \Gamma_{Z,f}^{(2)}\). More... | |
| virtual const double | deltaGamma_Zhad () const |
| The new physics contribution to the hadronic decay width of the \(Z\) boson, \(\delta \Gamma_{Z,had}\). More... | |
| virtual const double | deltaGamma_Zhad_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the hadronic decay width of the \(Z\) boson, \(\Delta \Gamma_{Z,had}^{(2)}\). More... | |
| virtual const double | deltaGammaHbbRatio1 () const |
| virtual const double | deltaGammaHbbRatio2 () const |
| virtual const double | deltaGammaHccRatio1 () const |
| virtual const double | deltaGammaHccRatio2 () const |
| virtual const double | deltaGammaHgagaRatio1 () const |
| virtual const double | deltaGammaHgagaRatio2 () const |
| virtual const double | deltaGammaHggRatio1 () const |
| virtual const double | deltaGammaHggRatio2 () const |
| virtual const double | deltaGammaHmumuRatio1 () const |
| virtual const double | deltaGammaHmumuRatio2 () const |
| virtual const double | deltaGammaHtautauRatio1 () const |
| virtual const double | deltaGammaHtautauRatio2 () const |
| virtual const double | deltaGammaHWWRatio1 () const |
| virtual const double | deltaGammaHWWRatio2 () const |
| virtual const double | deltaGammaHZgaRatio1 () const |
| virtual const double | deltaGammaHZgaRatio2 () const |
| virtual const double | deltaGammaHZZRatio1 () const |
| virtual const double | deltaGammaHZZRatio2 () const |
| virtual const double | deltaGammaTotalRatio1 () const |
| virtual const double | deltaGammaTotalRatio2 () const |
| virtual const double | DeltaGF () const |
| New physics contribution to the Fermi constant. More... | |
| const double | deltaGL_f_mu (const Particle p, const double mu) const |
| New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More... | |
| virtual gslpp::complex | deltaGL_Wff (const Particle pbar, const Particle p) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| virtual gslpp::complex | deltaGL_Wff_mu (const Particle pbar, const Particle p, const double mu) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| const double | deltaGR_f_mu (const Particle p, const double mu) const |
| New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More... | |
| virtual gslpp::complex | deltaGR_Wff (const Particle pbar, const Particle p) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| virtual gslpp::complex | deltaGR_Wff_mu (const Particle pbar, const Particle p, const double mu) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| virtual const double | deltaGV_f (const Particle f) const |
| New physics contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual const double | deltaGV_f_2 (const Particle f) const |
| virtual const double | deltaKgammaNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\). More... | |
| virtual const double | deltaKgammaNPEff () const |
| The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More... | |
| virtual const double | deltaN_nu () const |
| The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements. More... | |
| virtual const double | deltaR0_f (const Particle f) const |
| The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More... | |
| virtual const double | deltaR0_f_2 (const Particle f) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos: More... | |
| virtual const double | deltaR_inv () const |
| The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the \(Z\) boson, \(\delta R_{inv}\). More... | |
| virtual const double | deltaRuc () const |
| The new physics contribution to the ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width: More... | |
| virtual const double | deltaRuc_2 () const |
| The \(\mathcal{O}(1/\Lambda^4)\) new physics contribution to the ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width: More... | |
| virtual const double | deltaSigmaHadron () const |
| The new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\delta \sigma_h^0\). More... | |
| virtual const double | deltaSigmaHadron_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\Delta \sigma_h^{0,(2)}\). More... | |
| virtual const double | deltaSin2thetaEff_e () const |
| The new physics contribution to the effective electron/leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. More... | |
| virtual const double | deltaSin2thetaEff_e_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the effective electron weak angle \(\Delta \sin^2\theta_{eff,e}^{(2)}\) at the \(Z\) pole. More... | |
| virtual const double | deltaSin2thetaEff_mu () const |
| The new physics contribution to the effective muonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\mu\mu}\) at the \(Z\) pole. More... | |
| virtual const double | deltaSin2thetaEff_mu_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the effective muonic weak angle \(\Delta \sin^2\theta_{eff, \mu}^{(2)}\) at the \(Z\) pole. More... | |
| virtual const double | deltaxseeWW4fLEP2 (const double sqrt_s, const int fstate) const |
| The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More... | |
| virtual const double | deltaxseeWWhadLEP2 (const double sqrt_s) const |
| The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to j j j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | deltaxseeWWleptLEP2 (const double sqrt_s) const |
| The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | deltaxseeWWsemilLEP2 (const double sqrt_s) const |
| The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | deltaxseeWWtotLEP2 (const double sqrt_s) const |
| The new physics contribution to the total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More... | |
| virtual const double | deltayb_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | deltayc_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | deltaymu_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | deltays_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_s\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | deltayt_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | deltaytau_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | dxsdcoseeWWlvjjLEP2 (const double sqrt_s, const int bin) const |
| The differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | dxseeWWdcos (const double sqrt_s, const double cos) const |
| The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle. More... | |
| virtual const double | dxseeWWdcosBin (const double sqrt_s, const double cos1, const double cos2) const |
| The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle. More... | |
| virtual const gslpp::complex | gA_f (const Particle f) const |
| The total (SM+NP) contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| virtual const double | Gamma_had () const |
| The hadronic decay width of the \(Z\) boson, \(\Gamma_{Z,had}\). More... | |
| virtual const double | Gamma_Z () const |
| The total decay width of the \(Z\) boson, \(\Gamma_Z\). More... | |
| virtual const double | Gamma_Zf (const Particle f) const |
| The decay width of the \(Z\) boson into a given fermion pair, \(\Gamma_Z^{f}\). More... | |
| virtual const double | GammaHbbRatio () const |
| The ratio of the \(\Gamma(H\to b\bar{b})\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHccRatio () const |
| The ratio of the \(\Gamma(H\to c\bar{c})\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHgagaRatio () const |
| The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHggRatio () const |
| The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHmumuRatio () const |
| The ratio of the \(\Gamma(H\to \mu^+\mu^-)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHssRatio () const |
| The ratio of the \(\Gamma(H\to s\bar{s})\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHtautauRatio () const |
| The ratio of the \(\Gamma(H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHWWRatio () const |
| The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHZgaRatio () const |
| The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaHZZRatio () const |
| The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaW () const |
| The total width of the \(W\) boson, \(\Gamma_W\). More... | |
| virtual const double | GammaW (const Particle fi, const Particle fj) const |
| A partial decay width of the \(W\) boson decay into a SM fermion pair. More... | |
| virtual const StandardModel & | getTrueSM () const |
| A method to return a StandardModel object from NPbase. More... | |
| virtual const gslpp::complex | gV_f (const Particle f) const |
| The total (SM+NP) contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual const double | kappaW4feff () const |
| The effective coupling \(\kappa_{W4f,eff}=\sqrt{\Gamma_{H4f, CC}/\Gamma_{H4f, CC}^{SM}}\). More... | |
| virtual const double | kappaZ4feff () const |
| The effective coupling \(\kappa_{Z4f,eff}=\sqrt{\Gamma_{H4f, NC}/\Gamma_{H4f, NC}^{SM}}\). More... | |
| virtual const gslpp::complex | kappaZ_f (const Particle f) const |
| The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions. More... | |
| virtual const double | lambdaZNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\). More... | |
| virtual const double | lambz_HB (const double mu) const |
| The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) More... | |
| virtual const double | mubbH (const double sqrt_s) const |
| The ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeHee (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{e^+e^- \to He^+e^-}\) between the \( e^+e^- \to H e^+e^- \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | 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 | 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 | muggHH (const double sqrt_s) const |
| The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | 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 | mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const |
| The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class. More... | |
| virtual const double | mutH (const double sqrt_s) const |
| The ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mutHgaga (const double sqrt_s) const |
| virtual const double | 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 | Mw () const |
| The mass of the \(W\) boson, \(M_W\). More... | |
| virtual const double | N_nu () const |
| The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\). More... | |
| NPbase () | |
| The default constructor. More... | |
| virtual const double | obliqueW () const |
| The oblique parameter \(W\). More... | |
| virtual const double | obliqueY () const |
| The oblique parameter \(Y\). More... | |
| virtual const double | ppZHprobe (const double sqrt_s) const |
| The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class. More... | |
| virtual const double | R0_f (const Particle f) const |
| The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More... | |
| virtual const double | R_inv () const |
| The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\). More... | |
| virtual const gslpp::complex | rhoZ_f (const Particle f) const |
| The effective neutral-current coupling \(\rho_Z^f\) including SM plus NP contributions. More... | |
| virtual const double | Ruc () const |
| The ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width. More... | |
| virtual const double | RWc () const |
| The ratio \(R_{W,c)=\Gamma(W\to c + X)/\Gamma(W\to had)\). More... | |
| virtual const double | RWlilj (const Particle li, const Particle lj) const |
| The lepton universality ratio \(R_{W,l_i/l_j)=\Gamma(W\to l_i \nu_i)/\Gamma(W\to l_j \nu_j)\). More... | |
| virtual const double | RZlilj (const Particle li, const Particle lj) const |
| The lepton universality ratio \(R_{Z,l_i/l_j)=\Gamma(Z\to l_i^+ l_i^-)/\Gamma(Z\to l_j^+ l_j^-)\). More... | |
| virtual const double | sigma0_had () const |
| The cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\sigma_h^0\). More... | |
| virtual const double | sin2thetaEff (const Particle f) const |
| The leptonic effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\rm lept}\) at the the \(Z\) pole. More... | |
| virtual const double | STXS0_qqH (const double sqrt_s) const |
| The STXS0 bin \(pp \to H qq\). More... | |
| virtual const double | STXS12_BrH4lRatio () const |
| The STXS BR \( H \to 4l \), \(l=e,\mu\). More... | |
| virtual const double | STXS12_BrHbbRatio () const |
| The STXS BR \( H \to bb \). More... | |
| virtual const double | STXS12_BrHevmuvRatio () const |
| The STXS BR \( H \to e\nu \mu\nu \). More... | |
| virtual const double | STXS12_BrHgagaRatio () const |
| The STXS BR \( H \to \gamma \gamma \). More... | |
| virtual const double | STXS12_ggH_mjj0_350_pTH0_60_Nj1 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 1,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60\). More... | |
| virtual const double | STXS12_ggH_mjj0_350_pTH0_60_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60\). More... | |
| virtual const double | STXS12_ggH_mjj0_350_pTH120_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~120<p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_mjj0_350_pTH60_120_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~60<p_{TH} [GeV]<120\). More... | |
| virtual const double | STXS12_ggH_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\). More... | |
| virtual const double | STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\). More... | |
| virtual const double | STXS12_ggH_mjj700_Inf_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\). More... | |
| virtual const double | STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\). More... | |
| virtual const double | STXS12_ggH_pTH0_10_Nj0 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j=0,~p_{TH} [GeV]<10\). More... | |
| virtual const double | STXS12_ggH_pTH0_60_Nj1 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j = 1,~p_{TH} [GeV]<60\). More... | |
| virtual const double | STXS12_ggH_pTH10_200_Nj0 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j = 0, 10<~p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_pTH10_Inf_Nj0 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j=0,~10<p_{TH} [GeV]\). More... | |
| virtual const double | STXS12_ggH_pTH120_200_Nj1 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j = 1,~120<p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_pTH200_300 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(~200<p_{TH} [GeV]<300\). More... | |
| virtual const double | STXS12_ggH_pTH200_300_Nj01 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j\leq 1,~200<p_{TH} [GeV]<300\). More... | |
| virtual const double | STXS12_ggH_pTH300_450 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(~300<p_{TH} [GeV]<450\). More... | |
| virtual const double | STXS12_ggH_pTH300_450_Nj01 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j\leq 1,~300<p_{TH} [GeV]<450\). More... | |
| virtual const double | STXS12_ggH_pTH450_650 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(450<~p_{TH} [GeV]<650\). More... | |
| virtual const double | STXS12_ggH_pTH450_650_Nj01 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j\leq 1,~450<p_{TH} [GeV]<650\). More... | |
| virtual const double | STXS12_ggH_pTH450_Inf (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(~p_{TH} [GeV]>450\). More... | |
| virtual const double | STXS12_ggH_pTH60_120_Nj1 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j = 1,~60<p_{TH} [GeV]<120\). More... | |
| virtual const double | STXS12_ggH_pTH650_Inf (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(~p_{TH} [GeV]>650\). More... | |
| virtual const double | STXS12_ggH_pTH650_Inf_Nj01 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j\leq 1,650<p_{TH} [GeV]\). More... | |
| virtual const double | STXS12_ggHll_pTV0_75 (const double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(p_{TV}[GeV]<75\). More... | |
| virtual const double | STXS12_ggHll_pTV150_250_Nj0 (const double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_ggHll_pTV150_250_Nj1 (const double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(N_j = 1,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_ggHll_pTV250_Inf (const double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(250 < p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_ggHll_pTV75_150 (const double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(75<p_{TV}[GeV]<150\). More... | |
| virtual const double | STXS12_qqHll_pTV0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(0<p_{TV}<150[GeV]\). More... | |
| virtual const double | STXS12_qqHll_pTV0_75 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(p_{TV}[GeV]<75\). More... | |
| virtual const double | STXS12_qqHll_pTV150_250_Nj0 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_qqHll_pTV150_250_Nj1 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_qqHll_pTV250_400 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}<400[GeV]\). More... | |
| virtual const double | STXS12_qqHll_pTV250_Inf (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_qqHll_pTV400_Inf (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(400<p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_qqHll_pTV75_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(75<p_{TV}[GeV]<150\). More... | |
| virtual const double | STXS12_qqHlv_pTV0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(0<p_{TV}<150[GeV]\). More... | |
| virtual const double | STXS12_qqHlv_pTV0_75 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(p_{TV}[GeV]<75\). More... | |
| virtual const double | STXS12_qqHlv_pTV150_250_Nj0 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_qqHlv_pTV150_250_Nj1 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_qqHlv_pTV250_400 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}<400[GeV]\). More... | |
| virtual const double | STXS12_qqHlv_pTV250_Inf (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_qqHlv_pTV400_Inf (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(400<p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_qqHlv_pTV75_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(75<p_{TV}[GeV]<150\). More... | |
| virtual const double | STXS12_qqHqq_mjj0_60_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~m_{jj}[GeV]<60\). More... | |
| virtual const double | STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1000<m_{jj}[GeV]<1500,~p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1000<m_{jj}[GeV],~p_{TH}[GeV]>200\). More... | |
| virtual const double | STXS12_qqHqq_mjj120_350_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~120<m_{jj}[GeV]<350\). More... | |
| virtual const double | STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1500<m_{jj}[GeV],~p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<1000,~p_{TH}[GeV]>200\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV],~200<p_{TH}[GeV]\). More... | |
| virtual const double | STXS12_qqHqq_mjj60_120_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~60<m_{jj}[GeV]<120\). More... | |
| virtual const double | STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV]<1000,~p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\). More... | |
| virtual const double | STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\). More... | |
| virtual const double | STXS12_qqHqq_Nj0 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j = 0\). More... | |
| virtual const double | STXS12_qqHqq_Nj1 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j = 1\). More... | |
| virtual const double | STXS12_qqHqq_VH_veto_Nj01 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j = 0,1\) VH-veto Ref. 2402.05742. More... | |
| virtual const double | STXS12_tH (const double sqrt_s) const |
| The STXS bin \(pp \to tH\). More... | |
| virtual const double | STXS12_ttH_pTH0_60 (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(p_{TH}[GeV]<60\). More... | |
| virtual const double | STXS12_ttH_pTH120_200 (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(120<p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_ttH_pTH200_300 (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(200<p_{TH}[GeV]<300\). More... | |
| virtual const double | STXS12_ttH_pTH300_450 (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]<450\). More... | |
| virtual const double | STXS12_ttH_pTH300_Inf (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]\). More... | |
| virtual const double | STXS12_ttH_pTH450_Inf (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(450<p_{TH}[GeV]\). More... | |
| virtual const double | STXS12_ttH_pTH60_120 (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(60<p_{TH}[GeV]<120\). More... | |
| virtual const double | STXS_ggH0j (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH1j_pTH_0_60 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH1j_pTH_120_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH1j_pTH_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH1j_pTH_60_120 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_0_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_0_60 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_120_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_60_120 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_qqHll_pTV_0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHll_pTV_150_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHll_pTV_150_250_0j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHll_pTV_150_250_1j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHll_pTV_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHlv_pTV_0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHlv_pTV_0_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHlv_pTV_150_250_0j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHlv_pTV_150_250_1j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHlv_pTV_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHqq_nonVHtopo (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_pTj_200 (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_Rest (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_VBFtopo_Rest (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_VHtopo (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_ttHtH (const double sqrt_s) const |
| The STXS bin \( ttH + tH \). More... | |
| virtual const double | STXS_WHqqHqq_pTj1_200 (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_WHqqHqq_Rest (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_WHqqHqq_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_WHqqHqq_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_WHqqHqq_VH2j (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_pTj1_200 (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_Rest (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_VH2j (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual bool | Update (const std::map< std::string, double > &DPars) |
| The update method for NPbase. More... | |
| virtual const double | UpperLimitZgammaA (const double sqrt_s) const |
| virtual const double | UpperLimitZgammaA13 (const double sqrt_s) const |
| virtual const double | UpperLimitZgammaC (const double sqrt_s) const |
| virtual const double | UpperLimitZgammaC13 (const double sqrt_s) const |
| virtual const double | xseeWW (const double sqrt_s) const |
| Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\). More... | |
| virtual const double | xseeWW4fLEP2 (const double sqrt_s, const int fstate) const |
| The cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | xseeWWhadLEP2 (const double sqrt_s) const |
| The cross section in pb for \(e^+ e^- \to W^+ W^- \to j j j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | xseeWWleptLEP2 (const double sqrt_s) const |
| The cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | xseeWWsemilLEP2 (const double sqrt_s) const |
| The cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | xseeWWtotLEP2 (const double sqrt_s) const |
| The total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| Public Member Functions inherited from StandardModel | |
| gslpp::complex | AH_f (const double tau) const |
| Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More... | |
| gslpp::complex | AH_W (const double tau) const |
| W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling. More... | |
| gslpp::complex | AHZga_f (const double tau, const double lambda) const |
| Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | AHZga_W (const double tau, const double lambda) const |
| W loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| const double | Ale (double mu, orders order, bool Nf_thr=true) const |
| The running electromagnetic coupling \(\alpha_e(\mu)\) in the \(\overline{MS}\) scheme. More... | |
| const double | ale_OS (const double mu, orders order=FULLNLO) const |
| The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell scheme. More... | |
| virtual const double | alrmoller (const double q2, const double y) const |
| The computation of the parity violating asymmetry in Moller scattering. More... | |
| const double | Als (const double mu, const int Nf_in, const orders order=FULLNLO) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) with \(N_f\) active flavours in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More... | |
| const double | Als (const double mu, const orders order, const bool Nf_thr, const bool qed_flag) const |
| The running QCD coupling \(\alpha(\mu)\) in the \(\overline{MS}\) scheme including QED corrections. More... | |
| const double | Als (const double mu, const orders order=FULLNLO, const bool Nf_thr=true) const |
| const double | Alstilde5 (const double mu) const |
| The value of \(\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\) and full EW corrections. More... | |
| virtual const double | amuon () const |
| The computation of the anomalous magnetic moment of the muon \(a_\mu=(g_\mu-2)/2\). More... | |
| const double | Beta_e (int nm, unsigned int nf) const |
| QED beta function coefficients - eq. (36) hep-ph/0512066. More... | |
| const double | Beta_s (int nm, unsigned int nf) const |
| QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066. More... | |
| virtual const double | BrHtobb () const |
| The Br \((H\to b \bar{b})\) in the Standard Model. More... | |
| virtual const double | BrHtocc () const |
| The Br \((H\to c \bar{c})\) in the Standard Model. More... | |
| virtual const double | BrHtogaga () const |
| The Br \((H\to \gamma \gamma)\) in the Standard Model. More... | |
| virtual const double | BrHtogg () const |
| The Br \(\(H\to gg)\) in the Standard Model. More... | |
| virtual const double | BrHtomumu () const |
| The Br \((H\to \mu^+ \mu^-)\) in the Standard Model. More... | |
| virtual const double | BrHtoss () const |
| The Br \((H\to s \bar{s})\) in the Standard Model. More... | |
| virtual const double | BrHtotautau () const |
| The Br \((H\to \tau^+ \tau^-)\) in the Standard Model. More... | |
| virtual const double | BrHtoWWstar () const |
| The Br \((H\to W W^*)\) in the Standard Model. More... | |
| virtual const double | BrHtoZga () const |
| The Br \((H\to Z \gamma)\) in the Standard Model. More... | |
| virtual const double | BrHtoZZstar () const |
| The Br \((H\to Z Z^*)\) in the Standard Model. More... | |
| const double | c02 () const |
| The square of the cosine of the weak mixing angle \(c_0^2\) defined without weak radiative corrections. More... | |
| virtual bool | CheckFlags () const |
| A method to check the sanity of the set of model flags. More... | |
| 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 StandardModelMatching & | getMatching () const |
| A get method to access the member reference of type StandardModelMatching. More... | |
| virtual const double | getMHl () const |
| A get method to retrieve the Higgs mass \(m_h\). More... | |
| virtual const double | getmq (const QCD::quark q, const double mu) const |
| The MSbar running quark mass computed at NLO. More... | |
| const double | getMuw () const |
| A get method to retrieve the matching scale \(\mu_W\) around the weak scale. More... | |
| const double | getMw () const |
| A get method to access the input value of the mass of the \(W\) boson \(M_W\). More... | |
| EWSMApproximateFormulae * | getMyApproximateFormulae () const |
| A get method to retrieve the member pointer of type EWSMApproximateFormulae. More... | |
| EWSMcache * | getMyEWSMcache () const |
| A get method to retrieve the member pointer of type EWSMcache. More... | |
| LeptonFlavour * | getMyLeptonFlavour () const |
| EWSMOneLoopEW * | getMyOneLoopEW () const |
| A get method to retrieve the member pointer of type EWSMOneLoopEW,. More... | |
| EWSMThreeLoopEW * | getMyThreeLoopEW () const |
| EWSMThreeLoopEW2QCD * | getMyThreeLoopEW2QCD () const |
| EWSMThreeLoopQCD * | getMyThreeLoopQCD () const |
| EWSMTwoFermionsLEP2 * | getMyTwoFermionsLEP2 () const |
| A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More... | |
| EWSMTwoLoopEW * | getMyTwoLoopEW () const |
| EWSMTwoLoopQCD * | getMyTwoLoopQCD () const |
| const double | getMz () const |
| A get method to access the mass of the \(Z\) boson \(M_Z\). More... | |
| virtual const double | getPhiBd () const |
| Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More... | |
| virtual const double | getPhiBs () const |
| Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More... | |
| const gslpp::matrix< gslpp::complex > | getUPMNS () const |
| A get method to retrieve the object of the PMNS matrix. More... | |
| const gslpp::matrix< gslpp::complex > | getVCKM () const |
| A get method to retrieve the CKM matrix. More... | |
| const gslpp::matrix< gslpp::complex > & | getYd () const |
| A get method to retrieve the Yukawa matrix of the down-type quarks, \(Y_d\). More... | |
| const gslpp::matrix< gslpp::complex > & | getYe () const |
| A get method to retrieve the Yukawa matrix of the charged leptons, \(Y_e\). More... | |
| const gslpp::matrix< gslpp::complex > & | getYn () const |
| A get method to retrieve the Yukawa matrix of the neutrinos, \(Y_\nu\). More... | |
| const gslpp::matrix< gslpp::complex > & | getYu () const |
| A get method to retrieve the Yukawa matrix of the up-type quarks, \(Y_u\). More... | |
| virtual const double | gLnuN2 () const |
| The effective neutrino nucleon LH coupling: gLnuN2. More... | |
| virtual const double | gRnuN2 () const |
| The effective neutrino nucleon RH coupling: gRnuN2. More... | |
| virtual const double | gVnue () const |
| The effective (muon) neutrino-electron vector coupling: gVnue. More... | |
| gslpp::complex | I_triangle_1 (const double tau, const double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | I_triangle_2 (const double tau, const double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| virtual bool | Init (const std::map< std::string, double > &DPars) |
| A method to initialize the model parameters. More... | |
| virtual bool | InitializeModel () |
| A method to initialize the model. More... | |
| const double | intMLL2eeeeus2 (const double s, const double t0, const double t1) const |
| const double | intMLR2eeeets2 (const double s, const double t0, const double t1) const |
| const double | intMLRtilde2eeeest2 (const double s, const double t0, const double t1) const |
| const double | intMRR2eeeeus2 (const double s, const double t0, const double t1) const |
| const bool | IsFlagNoApproximateGammaZ () const |
| A method to retrieve the model flag NoApproximateGammaZ. More... | |
| const bool | IsFlagWithoutNonUniversalVC () const |
| A method to retrieve the model flag WithoutNonUniversalVC. More... | |
| const bool | isSMSuccess () const |
| A get method to retrieve the success status of the Standard Model update and matching. More... | |
| virtual const double | LEP2AFBbottom (const double s) const |
| virtual const double | LEP2AFBcharm (const double s) const |
| virtual const double | LEP2AFBe (const double s) const |
| virtual const double | LEP2AFBmu (const double s) const |
| virtual const double | LEP2AFBtau (const double s) const |
| virtual const double | LEP2dsigmadcosBinE (const double s, const double cos, const double cosmin, const double cosmax) const |
| virtual const double | LEP2dsigmadcosBinMu (const double s, const double cos, const double cosmin, const double cosmax) const |
| virtual const double | LEP2dsigmadcosBinTau (const double s, const double cos, const double cosmin, const double cosmax) const |
| virtual const double | LEP2dsigmadcosE (const double s, const double cos) const |
| virtual const double | LEP2dsigmadcosMu (const double s, const double cos) const |
| virtual const double | LEP2dsigmadcosTau (const double s, const double cos) const |
| virtual const double | LEP2Rbottom (const double s) const |
| virtual const double | LEP2Rcharm (const double s) const |
| virtual const double | LEP2sigmaBottom (const double s) const |
| virtual const double | LEP2sigmaCharm (const double s) const |
| virtual const double | LEP2sigmaE (const double s) const |
| virtual const double | LEP2sigmaHadron (const double s) const |
| virtual const double | LEP2sigmaMu (const double s) const |
| virtual const double | LEP2sigmaTau (const double s) const |
| const double | MLL2eeff (const Particle f, const double s, const double t) const |
| const double | MLR2eeff (const Particle f, const double s) const |
| const double | MRL2eeff (const Particle f, const double s) const |
| const double | MRR2eeff (const Particle f, const double s, const double t) const |
| const double | Mw_tree () const |
| The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). More... | |
| const double | MwbarFromMw (const double Mw) const |
| A method to convert the \(W\)-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More... | |
| const double | MwFromMwbar (const double Mwbar) const |
| A method to convert the \(W\)-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More... | |
| double | Mzbar () const |
| The \(Z\)-boson mass \(\overline{M}_Z\) in the complex-pole/fixed-width scheme. More... | |
| virtual bool | PreUpdate () |
| The pre-update method for StandardModel. More... | |
| virtual const double | Qwemoller (const double q2, const double y) const |
| The computation of the electron's weak charge. More... | |
| virtual const double | Qwn () const |
| The computation of the neutron weak charge: Qwn. More... | |
| virtual const double | Qwp () const |
| The computation of the proton weak charge: Qwp. More... | |
| virtual const double | rho_GammaW (const Particle fi, const Particle fj) const |
| EW radiative corrections to the width of \(W \to f_i \bar{f}_j\), denoted as \(\rho^W_{ij}\). More... | |
| const double | s02 () const |
| The square of the sine of the weak mixing angle \(s_0^2\) defined without weak radiative corrections. More... | |
| void | setCKM (const CKM &CKMMatrix) |
| A set method to change the CKM matrix. More... | |
| void | setFlagCacheInStandardModel (bool FlagCacheInStandardModel) |
| A set method to change the model flag CacheInStandardModel of StandardModel. More... | |
| void | setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ) |
| bool | setFlagSigmaForAFB (const bool flagSigmaForAFB_i) |
| bool | setFlagSigmaForR (const bool flagSigmaForR_i) |
| virtual bool | setFlagStr (const std::string name, const std::string value) |
| A method to set a flag of StandardModel. More... | |
| void | setRequireCKM (bool requireCKM) |
| A set method to change the value of requireCKM. More... | |
| void | setSMSuccess (bool success) const |
| A set method to change the success status of the Standard Model update and matching. More... | |
| void | setYd (const gslpp::matrix< gslpp::complex > &Yd) |
| A set method to set the Yukawa matrix of the down-type quarks, \(Y_d\). More... | |
| void | setYe (const gslpp::matrix< gslpp::complex > &Ye) |
| A set method to set the Yukawa matrix of the charged leptons, \(Y_e\). More... | |
| void | setYu (const gslpp::matrix< gslpp::complex > &Yu) |
| A set method to set the Yukawa matrix of the up-type quarks, \(Y_u\). More... | |
| virtual const double | SigmaeeHee (const double sqrt_s, const double Pe, const double Pp) const |
| The \(\sigma(e^+ e^- \to e^+ e^- H)\) in the Standard Model. More... | |
| virtual const double | SigmaeeHvv (const double sqrt_s, const double Pe, const double Pp) const |
| The \(\sigma(e^+ e^- \to \nu \bar{\nu} H)\) in the Standard Model. More... | |
| virtual const double | SigmaeeZH (const double sqrt_s, const double Pe, const double Pp) const |
| The \(\sigma(e^+ e^- \to Z H)\) in the Standard Model. More... | |
| StandardModel () | |
| The default constructor. More... | |
| const double | sW2 () const |
| virtual const double | sW2 (const double Mw_i) const |
| The square of the sine of the weak mixing angle in the on-shell scheme, denoted as \(s_W^2\). More... | |
| const double | sW2_MSbar_Approx () const |
| The (approximated formula for the) square of the sine of the weak mixing angle in the MSbar scheme, denoted as \(\hat{s}_{W}^2\). See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) More... | |
| const double | sW2_ND () const |
| The square of the sine of the weak mixing angle in the MSbar-ND scheme (w/o decoupling $\alpha\ln(m_t/M_Z)$ terms), denoted as \(\hat{s}_{ND}^2\). See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) (eq. 10.13a/10.13b) More... | |
| virtual const double | TauLFU_gmuge () const |
| The computation of the LFU ratio \(g_\mu/ g_e \). More... | |
| virtual const double | TauLFU_gtauge () const |
| The computation of the LFU ratio \(g_\tau/ g_e \). More... | |
| virtual const double | TauLFU_gtaugmu () const |
| The computation of the LFU ratio \(g_\tau/ g_\mu \). More... | |
| virtual const double | TauLFU_gtaugmuK () const |
| The computation of the LFU ratio \(\left(g_\tau/ g_\mu\right)_K \). More... | |
| virtual const double | TauLFU_gtaugmuPi () const |
| The computation of the LFU ratio \(\left(g_\tau/ g_\mu\right)_\pi \). More... | |
| virtual const double | ThetaLnuN () const |
| The effective neutrino nucleon LH parameter: ThetaLnuN. More... | |
| virtual const double | ThetaRnuN () const |
| The effective neutrino nucleon RH parameter: ThetaRnuN. More... | |
| const double | tovers2 (const double cosmin, const double cosmax) const |
| const double | uovers2 (const double cosmin, const double cosmax) const |
| const double | v () const |
| The Higgs vacuum expectation value. More... | |
| virtual | ~StandardModel () |
| The default destructor. More... | |
| Public Member Functions inherited from QCD | |
| const double | AboveTh (const double mu) const |
| The active flavour threshold above the scale \(\mu\) as defined in QCD::Thresholds(). More... | |
| void | addParameters (std::vector< std::string > params_i) |
| A method to add parameters that are specific to only one set of observables. More... | |
| const double | Als (const double mu, const int Nf_in, const orders order=FULLNLO) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) with \(N_f\) active flavours in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More... | |
| const double | Als (const double mu, const orders order=FULLNLO, const bool Nf_thr=true) const |
| const double | Als4 (const double mu) const |
| The value of \(\alpha_s^{\mathrm{FULLNLO}}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\). More... | |
| const double | AlsByOrder (const double mu, const int Nf_in, const orders order=FULLNLO) const |
| const double | AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const |
| const double | AlsOLD (const double mu, const orders order=FULLNLO) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More... | |
| const double | AlsWithInit (const double mu, const double alsi, const double mu_i, const int nf, const orders order) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) from \(\alpha_s(\mu_i)\) in the \(\overline{\mathrm{MS}}\) scheme, where it is forbidden to across a flavour threshold in the RG running from \(\mu_i\) to \(\mu\). More... | |
| const double | AlsWithLambda (const double mu, const orders order) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme with the use of \(\Lambda_{\rm QCD}\). More... | |
| const double | BelowTh (const double mu) const |
| The active flavour threshold below the scale \(\mu\) as defined in QCD::Thresholds(). More... | |
| const double | Beta0 (const double nf) const |
| The \(\beta_0(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| const double | Beta1 (const double nf) const |
| The \(\beta_1(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| const double | Beta2 (const double nf) const |
| The \(\beta_2(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| const double | Beta3 (const double nf) const |
| The \(\beta_3(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| void | CacheShift (double cache[][5], int n) const |
| A member used to manage the caching for this class. More... | |
| void | CacheShift (int cache[][5], int n) const |
| const orders | FullOrder (orders order) const |
| Return the FULLORDER enum corresponding to order. More... | |
| const double | Gamma0 (const double nf) const |
| The \(\gamma_0\) coefficient used to compute the running of a mass. More... | |
| const double | Gamma1 (const double nf) const |
| The \(\gamma_1\) coefficient used to compute the running of a mass. More... | |
| const double | Gamma2 (const double nf) const |
| The \(\gamma_2\) coefficient used to compute the running of a mass. More... | |
| const double | getAlsM () const |
| A get method to access the value of \(\alpha_s(M_{\alpha_s})\). More... | |
| const BParameter & | getBBd () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More... | |
| const BParameter & | getBBd_subleading () const |
| For getting the subleading bag parameters \(R_2 - R_3\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More... | |
| const BParameter & | getBBs () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More... | |
| const BParameter & | getBBs_subleading () const |
| For getting the subleading bag parameters \(R_2 - R_3\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More... | |
| const BParameter & | getBD () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta c = 2\) process in the \(D^0\) meson system. More... | |
| const BParameter & | getBK () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta s = 2\) process in the \(K^0\) meson system. More... | |
| const BParameter & | getBKd1 () const |
| const BParameter & | getBKd3 () const |
| const double | getCF () const |
| A get method to access the Casimir factor of QCD. More... | |
| const double | getMAls () const |
| A get method to access the mass scale \(M_{\alpha_s}\) at which the strong coupling constant measurement is provided. More... | |
| const Meson & | getMesons (const QCD::meson m) const |
| A get method to access a meson as an object of the type Meson. More... | |
| const double | getMtpole () const |
| A get method to access the pole mass of the top quark. More... | |
| const double | getMub () const |
| A get method to access the threshold between five- and four-flavour theory in GeV. More... | |
| const double | getMuc () const |
| A get method to access the threshold between four- and three-flavour theory in GeV. More... | |
| const double | getMut () const |
| A get method to access the threshold between six- and five-flavour theory in GeV. More... | |
| const double | getNc () const |
| A get method to access the number of colours \(N_c\). More... | |
| const double | getOptionalParameter (std::string name) const |
| A method to get parameters that are specific to only one set of observables. More... | |
| const Particle & | getQuarks (const QCD::quark q) const |
| A get method to access a quark as an object of the type Particle. More... | |
| std::vector< std::string > | getUnknownParameters () |
| A method to get the vector of the parameters that have been specified in the configuration file but not being used. More... | |
| void | initializeBParameter (std::string name_i) const |
| A method to initialize B Parameter and the corresponding meson. More... | |
| void | initializeMeson (QCD::meson meson_i) const |
| A method to initialize a meson. More... | |
| bool | isQCDsuccess () const |
| A getter for the QCDsuccess flag. More... | |
| const double | logLambda (const double nf, orders order) const |
| Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More... | |
| const double | Mbar2Mp (const double mbar, const quark q, const orders order=FULLNNLO) const |
| Converts the \(\overline{\mathrm{MS}}\) mass \(m(m)\) to the pole mass. More... | |
| const double | Mofmu2Mbar (const double m, const double mu, const quark q) const |
| Converts a quark running mass at an arbitrary scale to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More... | |
| const double | Mp2Mbar (const double mp, const quark q, orders order=FULLNNLO) const |
| Converts a quark pole mass to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More... | |
| const double | Mrun (const double mu, const double m, const quark q, const orders order=FULLNNLO) const |
| Computes a running quark mass \(m(\mu)\) from \(m(m)\). More... | |
| const double | Mrun (const double mu_f, const double mu_i, const double m, const quark q, const orders order=FULLNNLO) const |
| Runs a quark mass from \(\mu_i\) to \(\mu_f\). More... | |
| const double | Mrun4 (const double mu_f, const double mu_i, const double m) const |
| The running of a mass with the number of flavours \(n_f = 4\). More... | |
| const double | MS2DRqmass (const double MSbar) const |
| Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More... | |
| const double | MS2DRqmass (const double MSscale, const double MSbar) const |
| Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More... | |
| const double | Nf (const double mu) const |
| The number of active flavour at scale \(\mu\). More... | |
| const double | NfThresholdCorrections (double mu, double M, double als, int nf, orders order) const |
| Threshold corrections in matching \(\alpha_s(n_f+1)\) with \(\alpha_s(n_f)\) from eq. (34) of hep-ph/0512060. More... | |
| const std::string | orderToString (const orders order) const |
| Converts an object of the enum type "orders" to the corresponding string. More... | |
| QCD () | |
| Constructor. More... | |
| void | setComputemt (bool computemt) |
| A set method to change the value of computemt. More... | |
| void | setMtpole (double mtpole_in) |
| A method to set the pole mass of the top quark. More... | |
| void | setNc (double Nc) |
| A set method to change the number of colours \(N_c\). More... | |
| void | setOptionalParameter (std::string name, double value) |
| A method to set the parameter value for the parameters that are specific to only one set of observables. More... | |
| void | setQuarkMass (const quark q, const double mass) |
| A set method to change the mass of a quark. More... | |
| const double | Thresholds (const int i) const |
| For accessing the active flavour threshold scales. More... | |
| Public Member Functions inherited from Model | |
| void | addMissingModelParameter (const std::string &missingParameterName) |
| std::vector< std::string > | getmissingModelParameters () |
| unsigned int | getMissingModelParametersCount () |
| std::string | getModelName () const |
| A method to fetch the name of the model. More... | |
| const double & | getModelParam (std::string name) const |
| bool | isModelFWC_DF2 () const |
| bool | isModelGeneralTHDM () const |
| bool | isModelGeorgiMachacek () const |
| bool | IsModelInitialized () const |
| A method to check if the model is initialized. More... | |
| bool | isModelLinearized () const |
| bool | isModelNPquadratic () const |
| bool | isModelParam (std::string name) const |
| bool | isModelSUSY () const |
| bool | isModelTHDM () const |
| bool | isModelTHDMW () const |
| bool | IsUpdateError () const |
| A method to check if there was any error in the model update process. More... | |
| Model () | |
| The default constructor. More... | |
| void | raiseMissingModelParameterCount () |
| void | setModelFWC_DF2 () |
| void | setModelGeneralTHDM () |
| void | setModelGeorgiMachacek () |
| void | setModelInitialized (bool ModelInitialized) |
| A set method to fix the failure or success of the initialization of the model. More... | |
| void | setModelLinearized (bool linearized=true) |
| void | setModelName (const std::string name) |
| A method to set the name of the model. More... | |
| void | setModelNPquadratic (bool NPquadratic=true) |
| void | setModelSUSY () |
| void | setModelTHDM () |
| void | setModelTHDMW () |
| void | setSliced (bool Sliced) |
| void | setUpdateError (bool UpdateError) |
| A set method to fix the update status as success or failure. More... | |
| virtual | ~Model () |
| The default destructor. More... | |
Static Public Attributes | |
| static const std::string | HKvKfgenvars [NHKvKfgenvars] |
| A string array containing the labels of the model parameters in HiggsKigen. More... | |
| static const int | NHKvKfgenvars = 94 |
| The number of the model parameters in HiggsKigen: 17 modelpars + 39 + 38 th. err. pars. More... | |
| Static Public Attributes inherited from StandardModel | |
| static const double | GeVminus2_to_nb = 389379.338 |
| static const double | Mw_error = 0.00001 |
| The target accuracy of the iterative calculation of the \(W\)-boson mass in units of GeV. More... | |
| static const int | NSMvars = 28 |
| The number of the model parameters in StandardModel. More... | |
| static const int | NumSMParamsForEWPO = 35 |
| The number of the SM parameters that are relevant to the EW precision observables. More... | |
| static std::string | SMvars [NSMvars] |
| A string array containing the labels of the model parameters in StandardModel. More... | |
| Static Public Attributes inherited from QCD | |
| static const int | NQCDvars = 11 |
| The number of model parameters in QCD. More... | |
| static std::string | QCDvars [NQCDvars] |
| An array containing the labels under which all QCD parameters are stored in a vector of ModelParameter via InputParser::ReadParameters(). More... | |
Protected Member Functions | |
| virtual const double | computeKb () const |
| A method to compute the ratio of the \(Hbb\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKc () const |
| A method to compute the ratio of the \(Hcc\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKd () const |
| A method to compute the ratio of the \(Hdd\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKe () const |
| A method to compute the ratio of the \(Hee\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKg () const |
| A method to compute the ratio of the \(Hgg\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKgaga () const |
| A method to compute the ratio of the \(H\gamma\gamma\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKgagaLoop () const |
| A method to compute the ratio of the \(H\gamma\gamma\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKgLoop () const |
| A method to compute the ratio of the \(Hgg\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKmu () const |
| A method to compute the ratio of the \(H\mu\mu\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKs () const |
| A method to compute the ratio of the \(Hss\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKt () const |
| A method to compute the ratio of the \(Htt\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKtau () const |
| A method to compute the ratio of the \(H\tau\tau\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKu () const |
| A method to compute the ratio of the \(Huu\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKW () const |
| A method to compute the ratio of the \(HWW\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKZ () const |
| A method to compute the ratio of the \(HZZ\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKZga () const |
| A method to compute the ratio of the \(HZ\gamma\) coupling in the current model and in the SM. More... | |
| virtual const double | computeKZgaLoop () const |
| A method to compute the ratio of the \(HZ\gamma\) coupling in the current model and in the SM. More... | |
| virtual void | setParameter (const std::string name, const double &value) |
| A method to set the value of a parameter of HiggsKigen. More... | |
| Protected Member Functions inherited from StandardModel | |
| const double | AFB_NoISR_l (const QCD::lepton l_flavor, const double s) const |
| const double | AFB_NoISR_q (const QCD::quark q_flavor, const double s) const |
| bool | checkEWPOscheme (const std::string scheme) const |
| A method to check if a given scheme name in string form is valid. More... | |
| virtual void | computeCKM () |
| The method to compute the CKM matrix. More... | |
| virtual void | computeYukawas () |
| The method to compute the Yukawas matrix. More... | |
| double | Delta_EWQCD (const QCD::quark q) const |
| The non-factorizable EW-QCD corrections to the partial widths for \(Z\to q\bar{q}\), denoted as \(\Delta_{\mathrm{EW/QCD}}\). More... | |
| const double | getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm133 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm167 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm207 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu130 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu136 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu161 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu207 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau130 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau136 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau161 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau207 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom130 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom133 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom136 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom161 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom167 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom172 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom183 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom189 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom192 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom196 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom200 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom202 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom205 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom207 (double x) const |
| const double | getIntegrand_dsigmaBox_charm130 (double x) const |
| const double | getIntegrand_dsigmaBox_charm133 (double x) const |
| const double | getIntegrand_dsigmaBox_charm136 (double x) const |
| const double | getIntegrand_dsigmaBox_charm161 (double x) const |
| const double | getIntegrand_dsigmaBox_charm167 (double x) const |
| const double | getIntegrand_dsigmaBox_charm172 (double x) const |
| const double | getIntegrand_dsigmaBox_charm183 (double x) const |
| const double | getIntegrand_dsigmaBox_charm189 (double x) const |
| const double | getIntegrand_dsigmaBox_charm192 (double x) const |
| const double | getIntegrand_dsigmaBox_charm196 (double x) const |
| const double | getIntegrand_dsigmaBox_charm200 (double x) const |
| const double | getIntegrand_dsigmaBox_charm202 (double x) const |
| const double | getIntegrand_dsigmaBox_charm205 (double x) const |
| const double | getIntegrand_dsigmaBox_charm207 (double x) const |
| const double | getIntegrand_dsigmaBox_down130 (double x) const |
| const double | getIntegrand_dsigmaBox_down133 (double x) const |
| const double | getIntegrand_dsigmaBox_down136 (double x) const |
| const double | getIntegrand_dsigmaBox_down161 (double x) const |
| const double | getIntegrand_dsigmaBox_down167 (double x) const |
| const double | getIntegrand_dsigmaBox_down172 (double x) const |
| const double | getIntegrand_dsigmaBox_down183 (double x) const |
| const double | getIntegrand_dsigmaBox_down189 (double x) const |
| const double | getIntegrand_dsigmaBox_down192 (double x) const |
| const double | getIntegrand_dsigmaBox_down196 (double x) const |
| const double | getIntegrand_dsigmaBox_down200 (double x) const |
| const double | getIntegrand_dsigmaBox_down202 (double x) const |
| const double | getIntegrand_dsigmaBox_down205 (double x) const |
| const double | getIntegrand_dsigmaBox_down207 (double x) const |
| const double | getIntegrand_dsigmaBox_mu130 (double x) const |
| const double | getIntegrand_dsigmaBox_mu133 (double x) const |
| const double | getIntegrand_dsigmaBox_mu136 (double x) const |
| const double | getIntegrand_dsigmaBox_mu161 (double x) const |
| const double | getIntegrand_dsigmaBox_mu167 (double x) const |
| const double | getIntegrand_dsigmaBox_mu172 (double x) const |
| const double | getIntegrand_dsigmaBox_mu183 (double x) const |
| const double | getIntegrand_dsigmaBox_mu189 (double x) const |
| const double | getIntegrand_dsigmaBox_mu192 (double x) const |
| const double | getIntegrand_dsigmaBox_mu196 (double x) const |
| const double | getIntegrand_dsigmaBox_mu200 (double x) const |
| const double | getIntegrand_dsigmaBox_mu202 (double x) const |
| const double | getIntegrand_dsigmaBox_mu205 (double x) const |
| const double | getIntegrand_dsigmaBox_mu207 (double x) const |
| const double | getIntegrand_dsigmaBox_strange130 (double x) const |
| const double | getIntegrand_dsigmaBox_strange133 (double x) const |
| const double | getIntegrand_dsigmaBox_strange136 (double x) const |
| const double | getIntegrand_dsigmaBox_strange161 (double x) const |
| const double | getIntegrand_dsigmaBox_strange167 (double x) const |
| const double | getIntegrand_dsigmaBox_strange172 (double x) const |
| const double | getIntegrand_dsigmaBox_strange183 (double x) const |
| const double | getIntegrand_dsigmaBox_strange189 (double x) const |
| const double | getIntegrand_dsigmaBox_strange192 (double x) const |
| const double | getIntegrand_dsigmaBox_strange196 (double x) const |
| const double | getIntegrand_dsigmaBox_strange200 (double x) const |
| const double | getIntegrand_dsigmaBox_strange202 (double x) const |
| const double | getIntegrand_dsigmaBox_strange205 (double x) const |
| const double | getIntegrand_dsigmaBox_strange207 (double x) const |
| const double | getIntegrand_dsigmaBox_tau130 (double x) const |
| const double | getIntegrand_dsigmaBox_tau133 (double x) const |
| const double | getIntegrand_dsigmaBox_tau136 (double x) const |
| const double | getIntegrand_dsigmaBox_tau161 (double x) const |
| const double | getIntegrand_dsigmaBox_tau167 (double x) const |
| const double | getIntegrand_dsigmaBox_tau172 (double x) const |
| const double | getIntegrand_dsigmaBox_tau183 (double x) const |
| const double | getIntegrand_dsigmaBox_tau189 (double x) const |
| const double | getIntegrand_dsigmaBox_tau192 (double x) const |
| const double | getIntegrand_dsigmaBox_tau196 (double x) const |
| const double | getIntegrand_dsigmaBox_tau200 (double x) const |
| const double | getIntegrand_dsigmaBox_tau202 (double x) const |
| const double | getIntegrand_dsigmaBox_tau205 (double x) const |
| const double | getIntegrand_dsigmaBox_tau207 (double x) const |
| const double | getIntegrand_dsigmaBox_up130 (double x) const |
| const double | getIntegrand_dsigmaBox_up133 (double x) const |
| const double | getIntegrand_dsigmaBox_up136 (double x) const |
| const double | getIntegrand_dsigmaBox_up161 (double x) const |
| const double | getIntegrand_dsigmaBox_up167 (double x) const |
| const double | getIntegrand_dsigmaBox_up172 (double x) const |
| const double | getIntegrand_dsigmaBox_up183 (double x) const |
| const double | getIntegrand_dsigmaBox_up189 (double x) const |
| const double | getIntegrand_dsigmaBox_up192 (double x) const |
| const double | getIntegrand_dsigmaBox_up196 (double x) const |
| const double | getIntegrand_dsigmaBox_up200 (double x) const |
| const double | getIntegrand_dsigmaBox_up202 (double x) const |
| const double | getIntegrand_dsigmaBox_up205 (double x) const |
| const double | getIntegrand_dsigmaBox_up207 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom130 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom133 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom136 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom161 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom167 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom172 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom183 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom189 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom192 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom196 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom200 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom202 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom205 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom207 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm130 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm133 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm136 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm161 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm167 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm172 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm183 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm189 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm192 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm196 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm200 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm202 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm205 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm207 (double x) const |
| const double | getIntegrand_sigmaWithISR_down130 (double x) const |
| const double | getIntegrand_sigmaWithISR_down133 (double x) const |
| const double | getIntegrand_sigmaWithISR_down136 (double x) const |
| const double | getIntegrand_sigmaWithISR_down161 (double x) const |
| const double | getIntegrand_sigmaWithISR_down167 (double x) const |
| const double | getIntegrand_sigmaWithISR_down172 (double x) const |
| const double | getIntegrand_sigmaWithISR_down183 (double x) const |
| const double | getIntegrand_sigmaWithISR_down189 (double x) const |
| const double | getIntegrand_sigmaWithISR_down192 (double x) const |
| const double | getIntegrand_sigmaWithISR_down196 (double x) const |
| const double | getIntegrand_sigmaWithISR_down200 (double x) const |
| const double | getIntegrand_sigmaWithISR_down202 (double x) const |
| const double | getIntegrand_sigmaWithISR_down205 (double x) const |
| const double | getIntegrand_sigmaWithISR_down207 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu130 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu136 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu161 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu172 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu183 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu189 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu192 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu196 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu200 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu202 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu205 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu207 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange130 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange133 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange136 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange161 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange167 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange172 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange183 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange189 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange192 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange196 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange200 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange202 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange205 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange207 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau130 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau136 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau161 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau172 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau183 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau189 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau192 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau196 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau200 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau202 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau205 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau207 (double x) const |
| const double | getIntegrand_sigmaWithISR_up130 (double x) const |
| const double | getIntegrand_sigmaWithISR_up133 (double x) const |
| const double | getIntegrand_sigmaWithISR_up136 (double x) const |
| const double | getIntegrand_sigmaWithISR_up161 (double x) const |
| const double | getIntegrand_sigmaWithISR_up167 (double x) const |
| const double | getIntegrand_sigmaWithISR_up172 (double x) const |
| const double | getIntegrand_sigmaWithISR_up183 (double x) const |
| const double | getIntegrand_sigmaWithISR_up189 (double x) const |
| const double | getIntegrand_sigmaWithISR_up192 (double x) const |
| const double | getIntegrand_sigmaWithISR_up196 (double x) const |
| const double | getIntegrand_sigmaWithISR_up200 (double x) const |
| const double | getIntegrand_sigmaWithISR_up202 (double x) const |
| const double | getIntegrand_sigmaWithISR_up205 (double x) const |
| const double | getIntegrand_sigmaWithISR_up207 (double x) const |
| const double | Integrand_AFBnumeratorWithISR_l (double x, const QCD::lepton l_flavor, const double s) const |
| const double | Integrand_AFBnumeratorWithISR_q (double x, const QCD::quark q_flavor, const double s) const |
| const double | Integrand_dsigmaBox_l (double cosTheta, const QCD::lepton l_flavor, const double s) const |
| const double | Integrand_dsigmaBox_q (double cosTheta, const QCD::quark q_flavor, const double s) const |
| const double | Integrand_sigmaWithISR_l (double x, const QCD::lepton l_flavor, const double s) const |
| const double | Integrand_sigmaWithISR_q (double x, const QCD::quark q_flavor, const double s) const |
| double | m_q (const QCD::quark q, const double mu, const orders order=FULLNLO) const |
| double | RAq (const QCD::quark q) const |
| The radiator factor associated with the final-state QED and QCD corrections to the the axial-vector-current interactions, \(R_A^q(M_Z^2)\). More... | |
| double | resumKappaZ (const double DeltaRho[orders_EW_size], const double deltaKappa_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const |
| A method to compute the real part of the effetvive coupling \(\kappa_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | resumMw (const double Mw_i, const double DeltaRho[orders_EW_size], const double DeltaR_rem[orders_EW_size]) const |
| A method to compute the \(W\)-boson mass from \(\Delta\rho\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | resumRhoZ (const double DeltaRho[orders_EW_size], const double deltaRho_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const |
| A method to compute the real part of the effective coupling \(\rho_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | RVh () const |
| The singlet vector corrections to the hadronic \(Z\)-boson width, denoted as \(R_V^h\). More... | |
| double | RVq (const QCD::quark q) const |
| The radiator factor associated with the final-state QED and QCD corrections to the the vector-current interactions, \(R_V^q(M_Z^2)\). More... | |
| double | SchemeToDouble (const std::string scheme) const |
| A method to convert a given scheme name in string form into a floating-point number with double precision. More... | |
| const double | sigma_NoISR_l (const QCD::lepton l_flavor, const double s) const |
| const double | sigma_NoISR_q (const QCD::quark q_flavor, const double s) const |
| double | taub () const |
| Top-mass corrections to the \(Zb\bar{b}\) vertex, denoted by \(\tau_b\). More... | |
| Protected Member Functions inherited from QCD | |
| const double | MassOfNf (int nf) const |
| The Mbar mass of the heaviest quark in the theory with Nf active flavour. More... | |
Private Member Functions | |
| gslpp::complex | f_func (const double x) const |
| gslpp::complex | g_func (const double x) const |
| gslpp::complex | Int1 (const double tau, const double lambda) const |
| gslpp::complex | Int2 (const double tau, const double lambda) const |
Private Attributes | |
| double | BrHexo |
| The branching ratio of exotic (not invisible) Higgs decays. More... | |
| double | BrHinv |
| The branching ratio of invisible Higgs decays. More... | |
| double | eeettHint |
| Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More... | |
| double | eeettHpar |
| Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More... | |
| double | eeeWBFint |
| Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More... | |
| double | eeeWBFpar |
| Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More... | |
| double | eeeZHint |
| Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More... | |
| double | eeeZHpar |
| Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More... | |
| double | eepWBFint |
| Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.) More... | |
| double | eepWBFpar |
| Parametric relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.) More... | |
| double | eepZBFint |
| Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.) More... | |
| double | eepZBFpar |
| Parametric relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.) More... | |
| double | eggFHbb |
| double | eggFHgaga |
| double | eggFHmumu |
| Total relative theoretical error in \(gg \to H \to X\). More... | |
| double | eggFHtautau |
| double | eggFHWW |
| double | eggFHZga |
| double | eggFHZZ |
| double | eggFint |
| Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.) More... | |
| double | eggFpar |
| Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.) More... | |
| double | eHbbint |
| Intrinsic relative theoretical error in \(H \to b\bar{b}\). More... | |
| double | eHbbpar |
| Parametric relative theoretical error in \(H \to b\bar{b}\). More... | |
| double | eHccint |
| Intrinsic relative theoretical error in \(H \to c\bar{c}\). More... | |
| double | eHccpar |
| Parametric relative theoretical error in \(H \to c\bar{c}\). More... | |
| double | eHgagaint |
| Intrinsic relative theoretical error in \(H \to \gamma\gamma\). More... | |
| double | eHgagapar |
| Parametric relative theoretical error in \(H \to \gamma\gamma\). More... | |
| double | eHggint |
| Intrinsic relative theoretical error in \(H \to g g\). More... | |
| double | eHggpar |
| Parametric relative theoretical error in \(H \to g g\). More... | |
| double | eHmumuint |
| Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\). More... | |
| double | eHmumupar |
| Parametric relative theoretical error in \(H \to \mu^+ \mu^-\). More... | |
| double | eHssint |
| Intrinsic relative theoretical error in \(H \to s\bar{s}\). More... | |
| double | eHsspar |
| Parametric relative theoretical error in \(H \to s\bar{s}\). More... | |
| double | eHtautauint |
| Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\). More... | |
| double | eHtautaupar |
| Parametric relative theoretical error in \(H \to \tau^+ \tau^-\). More... | |
| double | eHwidth |
| Total relative theoretical error in the Higgs width. More... | |
| double | eHWWint |
| Intrinsic relative theoretical error in \(H \to W W\). More... | |
| double | eHWWpar |
| Parametric relative theoretical error in \(H \to W W\). More... | |
| double | eHZgaint |
| Intrinsic relative theoretical error in \(H \to Z \gamma\). More... | |
| double | eHZgapar |
| Parametric relative theoretical error in \(H \to Z \gamma\). More... | |
| double | eHZZint |
| Intrinsic relative theoretical error in \(H \to Z Z\). More... | |
| double | eHZZpar |
| Parametric relative theoretical error in \(H \to Z Z\). More... | |
| double | ettHbb |
| double | ettHgaga |
| double | ettHint |
| Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.) More... | |
| double | ettHmumu |
| Total relative theoretical error in \(pp \to ttH \to tt X\). More... | |
| double | ettHpar |
| Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.) More... | |
| double | ettHtautau |
| double | ettHWW |
| double | ettHZga |
| double | ettHZZ |
| double | eVBFHbb |
| double | eVBFHgaga |
| double | eVBFHinv |
| double | eVBFHmumu |
| Total relative theoretical error in \(pp \to Hjj (VBF) \to X jj\). More... | |
| double | eVBFHtautau |
| double | eVBFHWW |
| double | eVBFHZga |
| double | eVBFHZZ |
| double | eVBFint |
| Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.) More... | |
| double | eVBFpar |
| Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.) More... | |
| double | eVHinv |
| Total relative theoretical error in \(pp \to X H \to X + invisible\). More... | |
| double | eWHbb |
| double | eWHgaga |
| double | eWHint |
| Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.) More... | |
| double | eWHmumu |
| Total relative theoretical error in \(pp \to WH \to W X\). More... | |
| double | eWHpar |
| Parametric relative theoretical error in WH production. (Assumed to be constant in energy.) More... | |
| double | eWHtautau |
| double | eWHWW |
| double | eWHZga |
| double | eWHZZ |
| double | eZHbb |
| double | eZHgaga |
| double | eZHint |
| Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.) More... | |
| double | eZHmumu |
| Total relative theoretical error in \(pp \to ZH \to Z X\). More... | |
| double | eZHpar |
| Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.) More... | |
| double | eZHtautau |
| double | eZHWW |
| double | eZHZga |
| double | eZHZZ |
| bool | FlagCustodial |
| A boolean flag that is true if KZ=KW. More... | |
| bool | FlagKiLoop |
| A boolean flag that is true if one allows independent kappa's for the loop induced processes (g,ga,Zga) More... | |
| bool | FlagUniversalK |
| A boolean flag that is true if all K take the same universal value. More... | |
| bool | FlagUniversalKf |
| A boolean flag that is true if all Kf take the same universal value. More... | |
| bool | FlagUseKH |
| A boolean flag that is true if the Higgs width is rescaled by KH. (See above for the description of flag.) More... | |
| double | GammaHTotnoER |
| Total Higgs width ratio with respect to SM, neglecting theory errors. More... | |
| double | GammaHTotR |
| Total Higgs width ratio with respect to SM. More... | |
| double | GammaHTotSMnoER |
| Total Higgs width ratio with respect to SM, neglecting theory errors (only SM channels) More... | |
| double | GammaHTotSMR |
| Total Higgs width ratio with respect to SM (only SM channels) More... | |
| double | Kb |
| The factor rescaling the Higgs couplings to the bottom quark with respect to the SM. More... | |
| double | Kc |
| The factor rescaling the Higgs couplings to the charm quark with respect to the SM. More... | |
| double | Kd |
| The factor rescaling the Higgs couplings to the down quark with respect to the SM. More... | |
| double | Ke |
| The factor rescaling the Higgs couplings to electrons with respect to the SM. More... | |
| double | Kg |
| The factor rescaling the effective Higgs couplings to gluons with respect to the SM. More... | |
| double | Kga |
| The factor rescaling the effective Higgs couplings to photons with respect to the SM. More... | |
| double | KH |
| The factor rescaling the total Higgs width with respect to the SM. More... | |
| double | Kmu |
| The factor rescaling the Higgs couplings to muons with respect to the SM. More... | |
| double | Ks |
| The factor rescaling the Higgs couplings to the strange quark with respect to the SM. More... | |
| double | Kt |
| The factor rescaling the Higgs couplings to the top quark with respect to the SM. More... | |
| double | Ktau |
| The factor rescaling the Higgs couplings to taus with respect to the SM. More... | |
| double | Ku |
| The factor rescaling the Higgs couplings to the up quark with respect to the SM. More... | |
| double | Kw |
| The factor rescaling the SM-like Higgs couplings to the W vector bosons with respect to the SM. More... | |
| double | Kz |
| The factor rescaling the SM-like Higgs couplings to the Z vector bosons with respect to the SM. More... | |
| double | Kzga |
| The factor rescaling the effective Higgs couplings to the Z and a photon with respect to the SM. More... | |
Additional Inherited Members | |
| Public Types inherited from StandardModel | |
| enum | LEP2RCs { Weak = 0 , WeakBox , ISR , QEDFSR , QCDFSR , NUMofLEP2RCs } |
| enum | orders_EW { EW1 = 0 , EW1QCD1 , EW1QCD2 , EW2 , EW2QCD1 , EW3 , orders_EW_size } |
| An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More... | |
| Public Types inherited from QCD | |
| enum | lepton { NEUTRINO_1 , ELECTRON , NEUTRINO_2 , MU , NEUTRINO_3 , TAU , NOLEPTON } |
| An enum type for leptons. More... | |
| enum | meson { P_0 , P_P , K_0 , K_P , D_0 , D_P , D_S , B_D , B_P , B_S , B_C , PHI , K_star , K_star_P , K_S , D_star_P , RHO , RHO_P , OMEGA , MESON_END } |
| An enum type for mesons. More... | |
| enum | quark { UP , DOWN , CHARM , STRANGE , TOP , BOTTOM } |
| An enum type for quarks. More... | |
| Protected Attributes inherited from StandardModel | |
| double | A |
| The CKM parameter \(A\) in the Wolfenstein parameterization. More... | |
| double | ale |
| The fine-structure constant \(\alpha\). More... | |
| double | alpha21 |
| double | alpha31 |
| double | AlsMz |
| The strong coupling constant at the Z-boson mass, \(\alpha_s(M_Z)\). More... | |
| bool | bSigmaForAFB |
| bool | bSigmaForR |
| double | dAl5hMz |
| The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). (Non-input parameter) More... | |
| double | dAle5Mz |
| The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\), used as input for FlagMWinput = FALSE. More... | |
| double | delGammaWlv |
| The theoretical uncertainty in \(\Gamma_W_{l\nu}\), denoted as \(\delta\,\Gamma_W_{l\nu}\). More... | |
| double | delGammaWqq |
| The theoretical uncertainty in \(\Gamma_W_{qq}\), denoted as \(\delta\,\Gamma_W_{qq}\). More... | |
| double | delGammaZ |
| The theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\), in GeV. More... | |
| double | delMw |
| The theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\), in GeV. More... | |
| double | delR0b |
| The theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More... | |
| double | delR0c |
| The theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More... | |
| double | delR0l |
| The theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More... | |
| double | delsigma0H |
| The theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\) in nb. More... | |
| double | delSin2th_b |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More... | |
| double | delSin2th_l |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More... | |
| double | delSin2th_q |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More... | |
| double | delta |
| double | etab |
| The CKM parameter \(\bar{\eta}\) in the Wolfenstein parameterization. More... | |
| bool | flag_order [orders_EW_size] |
| An array of internal flags controlling the inclusions of higher-order corrections. More... | |
| bool | FlagFixMuwMut |
| A boolean for the model flag FixMuwMut. More... | |
| bool | flagLEP2 [NUMofLEP2RCs] |
| double | gamma |
| \(\gamma \) used as an input for FlagWolfenstein = FALSE More... | |
| double | GF |
| The Fermi constant \(G_\mu\) in \({\rm GeV}^{-2}\). More... | |
| double | lambda |
| The CKM parameter \(\lambda\) in the Wolfenstein parameterization. More... | |
| Particle | leptons [6] |
| An array of Particle objects for the leptons. More... | |
| double | mHl |
| The Higgs mass \(m_h\) in GeV. More... | |
| double | muw |
| A matching scale \(\mu_W\) around the weak scale in GeV. More... | |
| double | Mw_inp |
| The mass of the \(W\) boson in GeV used as input for FlagMWinput = TRUE. More... | |
| CKM | myCKM |
| An object of type CKM. More... | |
| PMNS | myPMNS |
| double | Mz |
| The mass of the \(Z\) boson in GeV. More... | |
| bool | requireCKM |
| An internal flag to control whether the CKM matrix has to be recomputed. More... | |
| bool | requireYe |
| An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed. More... | |
| bool | requireYn |
| An internal flag to control whether the neutrino Yukawa matrix has to be recomputed. More... | |
| double | rhob |
| The CKM parameter \(\bar{\rho}\) in the Wolfenstein parameterization. More... | |
| double | s12 |
| double | s13 |
| double | s23 |
| Flavour | SMFlavour |
| An object of type Flavour. More... | |
| Matching< StandardModelMatching, StandardModel > | SMM |
| An object of type Matching. More... | |
| double | Vcb |
| \(\vert V_{cb} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| double | Vub |
| \(\vert V_{ub} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| double | Vud |
| \(\vert V_{ud} \vert \) used as an input for FlagWolfenstein = FALSE and FlagUseVud = TRUE More... | |
| double | Vus |
| \(\vert V_{us} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| gslpp::matrix< gslpp::complex > | Yd |
| The Yukawa matrix of the down-type quarks. More... | |
| gslpp::matrix< gslpp::complex > | Ye |
| The Yukawa matrix of the charged leptons. More... | |
| gslpp::matrix< gslpp::complex > | Yn |
| The Yukawa matrix of the neutrinos. More... | |
| gslpp::matrix< gslpp::complex > | Yu |
| The Yukawa matrix of the up-type quarks. More... | |
| Protected Attributes inherited from QCD | |
| double | AlsM |
| The strong coupling constant at the mass scale MAls, \(\alpha_s(M_{\alpha_s})\). More... | |
| double | CA |
| double | CF |
| bool | computemt |
| Switch for computing the \(\overline{\mathrm{MS}}\) mass of the top quark. More... | |
| double | dAdA_NA |
| double | dFdA_NA |
| double | dFdF_NA |
| bool | FlagMpole2MbarNumeric |
| A flag to determine whether the pole mass to \(\over \mathrm{MS}\) mass conversion is done numerically. More... | |
| bool | FlagMtPole |
| A flag to determine whether the pole mass of the top quark is used as input. More... | |
| double | MAls |
| The mass scale in GeV at which the strong coupling measurement is provided. More... | |
| double | mtpole |
| The pole mass of the top quark. More... | |
| double | mub |
| The threshold between five- and four-flavour theory in GeV. More... | |
| double | muc |
| The threshold between four- and three-flavour theory in GeV. More... | |
| double | mut |
| The threshold between six- and five-flavour theory in GeV. More... | |
| double | NA |
| double | Nc |
| The number of colours. More... | |
| bool | QCDsuccess =true |
| Particle | quarks [6] |
| The vector of all SM quarks. More... | |
| bool | requireYd |
| Switch for generating the Yukawa couplings to the down-type quarks. More... | |
| bool | requireYu |
| Switch for generating the Yukawa couplings to the up-type quarks. More... | |
| double | TF |
| Protected Attributes inherited from Model | |
| bool | isSliced = false |
| A boolean set to true if the current istance is a slice of an extended object. More... | |
| std::map< std::string, std::reference_wrapper< const double > > | ModelParamMap |
| bool | UpdateError = false |
| A boolean set to false if update is successful. More... | |
| HiggsKigen::HiggsKigen | ( | ) |
The default constructor.
Definition at line 27 of file HiggsKigen.cpp.
|
inlinevirtual |
|
virtual |
The branching ratio of the of the Higgs into exotic particles (invisible or not).
Reimplemented from NPbase.
Definition at line 1957 of file HiggsKigen.cpp.
|
virtual |
The branching ratio of the of the Higgs into invisible particles.
Reimplemented from NPbase.
Definition at line 1963 of file HiggsKigen.cpp.
|
virtual |
The branching ratio of the of the Higgs into invisible particles (only invisible new particles).
Reimplemented from NPbase.
Definition at line 1968 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2d2d)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 973 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2e 2\mu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 938 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2e2v)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 958 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1076 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 988 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 933 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 983 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 953 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 948 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1124 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1070 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1064 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2\mu 2v)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 963 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1082 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2u2d)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 978 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2u2u)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 968 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2ud)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1058 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2v2d)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 998 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2v2u)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 993 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 2v2v)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 943 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 4d)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1033 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 4e)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1013 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 4f)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1088 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1008 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1003 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1119 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 4\mu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1018 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 4u)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1028 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to 4v)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1023 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 924 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 910 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to e\nu \mu\nu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1043 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 889 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 839 of file HiggsKigen.cpp.
|
inlinevirtual |
The ratio of the Br \((H\to l l \nu\nu, l l j j)\), \(l=e,\mu,~~j\not=b)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1705 of file HiggsKigen.h.
|
inlinevirtual |
The ratio of the Br \((H\to l l j j)\), \(l=e,\mu,~~j\not=b)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1675 of file HiggsKigen.h.
|
inlinevirtual |
The ratio of the Br \((H\to l \nu l \nu, l \nu j j)\), \(l=e,\mu,~~j\not=b)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1695 of file HiggsKigen.h.
|
inlinevirtual |
The ratio of the Br \((H\to l \nu j j)\), \(l=e,\mu,~~j\not=b)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1685 of file HiggsKigen.h.
|
virtual |
The ratio of the Br \((H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1053 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1038 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 896 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to s\bar{s})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 917 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 903 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1979 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to uddu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1048 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1974 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to VV)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 860 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 846 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 879 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 874 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 884 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 867 of file HiggsKigen.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 853 of file HiggsKigen.cpp.
|
virtual |
A method to check if all the mandatory parameters for HiggsKigen have been provided in model initialization.
| [in] | DPars | a map of the parameters that are being updated in the Monte Carlo run (including parameters that are varied and those that are held constant) |
Reimplemented from StandardModel.
Definition at line 433 of file HiggsKigen.cpp.
|
virtual |
The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model and neglecting theory errors.
Definition at line 1889 of file HiggsKigen.cpp.
|
virtual |
The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 1879 of file HiggsKigen.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to SM)\) in the current model and in the Standard Model, including only SM decays and neglecting theory errors.
Definition at line 1928 of file HiggsKigen.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to SM)\) in the current model and in the Standard Model, including only SM decays.
Definition at line 1899 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(Hbb\) coupling in the current model and in the SM.
Definition at line 2052 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(Hcc\) coupling in the current model and in the SM.
Definition at line 2032 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(Hdd\) coupling in the current model and in the SM.
Definition at line 2042 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(Hee\) coupling in the current model and in the SM.
Definition at line 2012 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(Hgg\) coupling in the current model and in the SM.
Definition at line 1987 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(H\gamma\gamma\) coupling in the current model and in the SM.
Definition at line 2007 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(H\gamma\gamma\) coupling in the current model and in the SM.
Definition at line 2132 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(Hgg\) coupling in the current model and in the SM.
Definition at line 2059 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(H\mu\mu\) coupling in the current model and in the SM.
Definition at line 2017 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(Hss\) coupling in the current model and in the SM.
Definition at line 2047 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(Htt\) coupling in the current model and in the SM.
Definition at line 2037 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(H\tau\tau\) coupling in the current model and in the SM.
Definition at line 2022 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(Huu\) coupling in the current model and in the SM.
Definition at line 2027 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(HWW\) coupling in the current model and in the SM.
Definition at line 1992 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(HZZ\) coupling in the current model and in the SM.
Definition at line 1997 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(HZ\gamma\) coupling in the current model and in the SM.
Definition at line 2002 of file HiggsKigen.cpp.
|
protectedvirtual |
A method to compute the ratio of the \(HZ\gamma\) coupling in the current model and in the SM.
Definition at line 2084 of file HiggsKigen.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2181 of file HiggsKigen.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2211 of file HiggsKigen.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 2216 of file HiggsKigen.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2196 of file HiggsKigen.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2185 of file HiggsKigen.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2220 of file HiggsKigen.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2200 of file HiggsKigen.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\).
Reimplemented from NPbase.
Definition at line 2189 of file HiggsKigen.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\).
Reimplemented from NPbase.
Definition at line 2204 of file HiggsKigen.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2224 of file HiggsKigen.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 2229 of file HiggsKigen.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\).
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 2233 of file HiggsKigen.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\).
Reimplemented from NPbase.
Definition at line 2171 of file HiggsKigen.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 2177 of file HiggsKigen.cpp.
|
private |
Definition at line 2309 of file HiggsKigen.cpp.
|
private |
Definition at line 2319 of file HiggsKigen.cpp.
|
inline |
A get method to retrieve the exotic (not invisible) Higgs branching ratio.
Definition at line 559 of file HiggsKigen.h.
|
inline |
A get method to retrieve the invisible Higgs branching ratio.
Definition at line 541 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to b quarks with respect to the SM \(K_b\).
Definition at line 381 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to c quarks with respect to the SM \(K_c\).
Definition at line 481 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to d quarks with respect to the SM \(K_d\).
Definition at line 341 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to electrons with respect to the SM \(K_e\).
Definition at line 401 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to gluons with respect to the SM \(K_g\).
Definition at line 281 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to photons with respect to the SM \(K_ga\).
Definition at line 301 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the total Higgs width with respect to the SM \(K_H\).
Definition at line 521 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to muons with respect to the SM \(K_\mu\).
Definition at line 421 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to s quarks with respect to the SM \(K_s\).
Definition at line 361 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to t quarks with respect to the SM \(K_t\).
Definition at line 501 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to taus with respect to the SM \(K_\tau\).
Definition at line 441 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to u quarks with respect to the SM \(K_u\).
Definition at line 461 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to the W vector bosons with respect to the SM \(K_W\).
Definition at line 241 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to the Z vector bosons with respect to the SM \(K_Z\).
Definition at line 261 of file HiggsKigen.h.
|
inline |
A get method to retrieve the factor rescaling the Higgs coupling to Z and photon with respect to the SM \(K_{zga}\).
Definition at line 321 of file HiggsKigen.h.
|
private |
Definition at line 2331 of file HiggsKigen.cpp.
|
private |
|
virtual |
The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\).
Reimplemented from NPbase.
Definition at line 2297 of file HiggsKigen.cpp.
|
virtual |
The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\).
Reimplemented from NPbase.
Definition at line 2277 of file HiggsKigen.cpp.
|
virtual |
The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\).
Reimplemented from NPbase.
Definition at line 2272 of file HiggsKigen.cpp.
|
virtual |
The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\).
Reimplemented from NPbase.
Definition at line 2282 of file HiggsKigen.cpp.
|
virtual |
The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\).
Reimplemented from NPbase.
Definition at line 2262 of file HiggsKigen.cpp.
|
virtual |
The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\).
Reimplemented from NPbase.
Definition at line 2267 of file HiggsKigen.cpp.
|
virtual |
The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\).
Reimplemented from NPbase.
Definition at line 2292 of file HiggsKigen.cpp.
|
virtual |
The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\).
Reimplemented from NPbase.
Definition at line 2302 of file HiggsKigen.cpp.
|
virtual |
The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\).
Reimplemented from NPbase.
Definition at line 2287 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
| [in] | Pol_em | polarization of electrons |
| [in] |
polarization of positrons
Reimplemented from NPbase.
Definition at line 589 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 751 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
| [in] | Pol_em | polarization of electrons |
| [in] |
polarization of positrons
Reimplemented from NPbase.
Definition at line 571 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
| [in] | Pol_em | polarization of electrons |
| [in] |
polarization of positrons
Reimplemented from NPbase.
Definition at line 609 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 665 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
| [in] | Pol_em | polarization of electrons |
| [in] |
polarization of positrons
Reimplemented from NPbase.
Definition at line 672 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
| [in] | Pol_em | polarization of electrons |
| [in] |
polarization of positrons
Reimplemented from NPbase.
Definition at line 679 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 627 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 634 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 517 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1441 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1144 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1149 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1381 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 740 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1411 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1321 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1351 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1231 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1261 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1291 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 759 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H\mu\mu}\) between the \(\sigma(\mu \mu \to H \mu \mu)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 813 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model, in the narrow width approximation.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 776 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H\nu\nu}\) between the \(\sigma(\mu \mu \to H \nu \nu)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 793 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu ttH}\) between the \(\sigma(\mu \mu \to t\bar{t} H )}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 831 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu ZH}\) between the \(\sigma(\mu \mu \to Z H)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 785 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 728 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1790 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1478 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1712 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1751 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1634 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1673 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1517 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,Z\gamma\to \gamma 2\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\to \gamma 2\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1868 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1556 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1595 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ\to 4\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1863 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1824 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1512 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1746 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1785 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1668 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1707 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1551 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1590 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1629 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF}\) between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1829 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1795 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1483 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,inv}\) between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1834 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1717 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1756 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1639 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1678 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1522 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1561 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1600 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1810 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH}\) between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1839 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1498 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,inv}\) between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1851 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1732 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1771 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1654 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1693 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1537 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1576 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1615 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1805 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1493 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1727 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1766 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1649 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1688 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1532 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1571 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1610 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1800 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1488 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1722 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1761 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1644 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1683 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1527 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1566 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1605 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 721 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1466 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1226 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H\to b\bar{b}\), \(Z\to e^+e^-\) channel channel in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1138 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1406 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1436 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1346 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1376 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1132 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1256 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1286 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1316 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 550 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 563 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1446 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1206 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1386 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1416 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1326 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1356 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1236 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1266 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1296 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 705 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 686 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1461 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1221 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1401 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 695 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1431 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1341 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1371 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1251 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1281 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1311 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 641 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1456 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1216 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1396 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 648 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1426 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1336 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1366 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1246 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1276 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1306 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 653 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1451 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1211 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1391 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 660 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1421 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1331 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1361 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1241 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1271 of file HiggsKigen.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 1301 of file HiggsKigen.cpp.
|
virtual |
The oblique parameter \(S\).
Reimplemented from NPbase.
Definition at line 471 of file HiggsKigen.cpp.
|
virtual |
The oblique parameter \(T\).
Reimplemented from NPbase.
Definition at line 490 of file HiggsKigen.cpp.
|
virtual |
The oblique parameter \(U\).
Reimplemented from NPbase.
Definition at line 510 of file HiggsKigen.cpp.
|
virtual |
The post-update method for HiggsKigen.
This method runs all the procedures that are need to be executed after the model is successfully updated.
Reimplemented from StandardModel.
Definition at line 132 of file HiggsKigen.cpp.
|
inline |
A set method to change the exotic (not invisible) Higgs branching ratio.
| [in] | BrHexo | \(BR_{exo}\) the exotic (not invisible) Higgs branching ratio. |
Definition at line 568 of file HiggsKigen.h.
|
inline |
A set method to change the invisible Higgs branching ratio.
| [in] | BrHinv | \(BR_{inv}\) the invisible Higgs branching ratio. |
Definition at line 550 of file HiggsKigen.h.
|
virtual |
A method to set a flag of HiggsKigen.
| [in] | name | name of a model flag |
| [in] | value | the boolean to be assigned to the flag specified by name |
Reimplemented from NPbase.
Definition at line 445 of file HiggsKigen.cpp.
|
inline |
A set method to change the factor rescaling the Higgs coupling to b quarks with respect to the SM \(K_b\).
| [in] | Kb | \(K_b\) the factor rescaling the Higgs coupling to b quarks. |
Definition at line 391 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the Higgs coupling to c quarks with respect to the SM \(K_c\).
| [in] | Kc | \(K_c\) the factor rescaling the Higgs coupling to c quarks. |
Definition at line 491 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the Higgs coupling to d quarks with respect to the SM \(K_d\).
| [in] | Kd | \(K_d\) the factor rescaling the Higgs coupling to d quarks. |
Definition at line 351 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the Higgs coupling to electrons with respect to the SM \(K_e\).
| [in] | Ke | \(K_e\) the factor rescaling the Higgs coupling to electrons. |
Definition at line 411 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the Higgs coupling to gluons with respect to the SM \(K_g\).
| [in] | Kg | \(K_g\) the factor rescaling the Higgs coupling to gluons. |
Definition at line 291 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the Higgs coupling to photons with respect to the SM \(K_ga\).
| [in] | Kga | \(K_ga\) the factor rescaling the Higgs coupling to photons. |
Definition at line 311 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the total Higgs width with respect to the SM \(K_H\).
| [in] | KH | \(K_H\) the factor rescaling the total Higgs width. |
Definition at line 531 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the Higgs coupling to muons with respect to the SM \(K_\mu\).
| [in] | Kmu | \(K_\mu\) the factor rescaling the Higgs coupling to muons. |
Definition at line 431 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the Higgs coupling to s quarks with respect to the SM \(K_s\).
| [in] | Ks | \(K_s\) the factor rescaling the Higgs coupling to s quarks. |
Definition at line 371 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the Higgs coupling to t quarks with respect to the SM \(K_t\).
| [in] | Kt | \(K_t\) the factor rescaling the Higgs coupling to t quarks. |
Definition at line 511 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the Higgs coupling to taus with respect to the SM \(K_\tau\).
| [in] | Ktau | \(K_\tau\) the factor rescaling the Higgs coupling to taus. |
Definition at line 451 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the Higgs coupling to u quarks with respect to the SM \(K_u\).
| [in] | Ku | \(K_u\) the factor rescaling the Higgs coupling to u quarks. |
Definition at line 471 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the Higgs coupling to the W vector bosons with respect to the SM \(K_W\).
| [in] | Kw | \(K_W\) the factor rescaling the Higgs coupling to the W vector bosons. |
Definition at line 251 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the Higgs coupling to the Z vector bosons with respect to the SM \(K_Z\).
| [in] | Kz | \(K_Z\) the factor rescaling the Higgs coupling to the Z vector bosons. |
Definition at line 271 of file HiggsKigen.h.
|
inline |
A set method to change the factor rescaling the Higgs coupling to Z and photon with respect to the SM \(K_{zga}\).
| [in] | Kzga | \(K_{zga}\) the factor rescaling the Higgs coupling to photons. |
Definition at line 331 of file HiggsKigen.h.
|
protectedvirtual |
A method to set the value of a parameter of HiggsKigen.
| [in] | name | name of a model parameter |
| [in] | value | the value to be assigned to the parameter specified by name |
Reimplemented from StandardModel.
Definition at line 237 of file HiggsKigen.cpp.
|
private |
The branching ratio of exotic (not invisible) Higgs decays.
Definition at line 2473 of file HiggsKigen.h.
|
private |
The branching ratio of invisible Higgs decays.
Definition at line 2472 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)
Definition at line 2489 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)
Definition at line 2490 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)
Definition at line 2485 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)
Definition at line 2486 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)
Definition at line 2487 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)
Definition at line 2488 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.)
Definition at line 2491 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.)
Definition at line 2492 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.)
Definition at line 2493 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.)
Definition at line 2494 of file HiggsKigen.h.
|
private |
Definition at line 2516 of file HiggsKigen.h.
|
private |
Definition at line 2516 of file HiggsKigen.h.
|
private |
Total relative theoretical error in \(gg \to H \to X\).
Definition at line 2516 of file HiggsKigen.h.
|
private |
Definition at line 2516 of file HiggsKigen.h.
|
private |
Definition at line 2516 of file HiggsKigen.h.
|
private |
Definition at line 2516 of file HiggsKigen.h.
|
private |
Definition at line 2516 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.)
Definition at line 2475 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.)
Definition at line 2476 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(H \to b\bar{b}\).
Definition at line 2513 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(H \to b\bar{b}\).
Definition at line 2514 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(H \to c\bar{c}\).
Definition at line 2509 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(H \to c\bar{c}\).
Definition at line 2510 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(H \to \gamma\gamma\).
Definition at line 2503 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(H \to \gamma\gamma\).
Definition at line 2504 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(H \to g g\).
Definition at line 2495 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(H \to g g\).
Definition at line 2496 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\).
Definition at line 2505 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(H \to \mu^+ \mu^-\).
Definition at line 2506 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(H \to s\bar{s}\).
Definition at line 2511 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(H \to s\bar{s}\).
Definition at line 2512 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\).
Definition at line 2507 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(H \to \tau^+ \tau^-\).
Definition at line 2508 of file HiggsKigen.h.
|
private |
Total relative theoretical error in the Higgs width.
Definition at line 2523 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(H \to W W\).
Definition at line 2497 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(H \to W W\).
Definition at line 2498 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(H \to Z \gamma\).
Definition at line 2501 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(H \to Z \gamma\).
Definition at line 2502 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in \(H \to Z Z\).
Definition at line 2499 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in \(H \to Z Z\).
Definition at line 2500 of file HiggsKigen.h.
|
private |
Definition at line 2520 of file HiggsKigen.h.
|
private |
Definition at line 2520 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.)
Definition at line 2477 of file HiggsKigen.h.
|
private |
Total relative theoretical error in \(pp \to ttH \to tt X\).
Definition at line 2520 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.)
Definition at line 2478 of file HiggsKigen.h.
|
private |
Definition at line 2520 of file HiggsKigen.h.
|
private |
Definition at line 2520 of file HiggsKigen.h.
|
private |
Definition at line 2520 of file HiggsKigen.h.
|
private |
Definition at line 2520 of file HiggsKigen.h.
|
private |
Definition at line 2517 of file HiggsKigen.h.
|
private |
Definition at line 2517 of file HiggsKigen.h.
|
private |
Definition at line 2521 of file HiggsKigen.h.
|
private |
Total relative theoretical error in \(pp \to Hjj (VBF) \to X jj\).
Definition at line 2517 of file HiggsKigen.h.
|
private |
Definition at line 2517 of file HiggsKigen.h.
|
private |
Definition at line 2517 of file HiggsKigen.h.
|
private |
Definition at line 2517 of file HiggsKigen.h.
|
private |
Definition at line 2517 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.)
Definition at line 2479 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.)
Definition at line 2480 of file HiggsKigen.h.
|
private |
Total relative theoretical error in \(pp \to X H \to X + invisible\).
Definition at line 2521 of file HiggsKigen.h.
|
private |
Definition at line 2518 of file HiggsKigen.h.
|
private |
Definition at line 2518 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.)
Definition at line 2481 of file HiggsKigen.h.
|
private |
Total relative theoretical error in \(pp \to WH \to W X\).
Definition at line 2518 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in WH production. (Assumed to be constant in energy.)
Definition at line 2482 of file HiggsKigen.h.
|
private |
Definition at line 2518 of file HiggsKigen.h.
|
private |
Definition at line 2518 of file HiggsKigen.h.
|
private |
Definition at line 2518 of file HiggsKigen.h.
|
private |
Definition at line 2518 of file HiggsKigen.h.
|
private |
Definition at line 2519 of file HiggsKigen.h.
|
private |
Definition at line 2519 of file HiggsKigen.h.
|
private |
Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.)
Definition at line 2483 of file HiggsKigen.h.
|
private |
Total relative theoretical error in \(pp \to ZH \to Z X\).
Definition at line 2519 of file HiggsKigen.h.
|
private |
Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.)
Definition at line 2484 of file HiggsKigen.h.
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Definition at line 2519 of file HiggsKigen.h.
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Definition at line 2519 of file HiggsKigen.h.
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private |
Definition at line 2519 of file HiggsKigen.h.
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private |
Definition at line 2519 of file HiggsKigen.h.
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A boolean flag that is true if KZ=KW.
Definition at line 2534 of file HiggsKigen.h.
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A boolean flag that is true if one allows independent kappa's for the loop induced processes (g,ga,Zga)
Definition at line 2533 of file HiggsKigen.h.
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A boolean flag that is true if all K take the same universal value.
Definition at line 2536 of file HiggsKigen.h.
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A boolean flag that is true if all Kf take the same universal value.
Definition at line 2535 of file HiggsKigen.h.
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A boolean flag that is true if the Higgs width is rescaled by KH. (See above for the description of flag.)
Definition at line 2537 of file HiggsKigen.h.
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Total Higgs width ratio with respect to SM, neglecting theory errors.
Definition at line 2529 of file HiggsKigen.h.
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Total Higgs width ratio with respect to SM.
Definition at line 2526 of file HiggsKigen.h.
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Total Higgs width ratio with respect to SM, neglecting theory errors (only SM channels)
Definition at line 2530 of file HiggsKigen.h.
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Total Higgs width ratio with respect to SM (only SM channels)
Definition at line 2527 of file HiggsKigen.h.
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A string array containing the labels of the model parameters in HiggsKigen.
Definition at line 206 of file HiggsKigen.h.
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The factor rescaling the Higgs couplings to the bottom quark with respect to the SM.
Definition at line 2467 of file HiggsKigen.h.
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The factor rescaling the Higgs couplings to the charm quark with respect to the SM.
Definition at line 2463 of file HiggsKigen.h.
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The factor rescaling the Higgs couplings to the down quark with respect to the SM.
Definition at line 2465 of file HiggsKigen.h.
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The factor rescaling the Higgs couplings to electrons with respect to the SM.
Definition at line 2468 of file HiggsKigen.h.
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The factor rescaling the effective Higgs couplings to gluons with respect to the SM.
Definition at line 2459 of file HiggsKigen.h.
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The factor rescaling the effective Higgs couplings to photons with respect to the SM.
Definition at line 2460 of file HiggsKigen.h.
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The factor rescaling the total Higgs width with respect to the SM.
Definition at line 2471 of file HiggsKigen.h.
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The factor rescaling the Higgs couplings to muons with respect to the SM.
Definition at line 2469 of file HiggsKigen.h.
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The factor rescaling the Higgs couplings to the strange quark with respect to the SM.
Definition at line 2466 of file HiggsKigen.h.
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private |
The factor rescaling the Higgs couplings to the top quark with respect to the SM.
Definition at line 2464 of file HiggsKigen.h.
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private |
The factor rescaling the Higgs couplings to taus with respect to the SM.
Definition at line 2470 of file HiggsKigen.h.
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The factor rescaling the Higgs couplings to the up quark with respect to the SM.
Definition at line 2462 of file HiggsKigen.h.
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The factor rescaling the SM-like Higgs couplings to the W vector bosons with respect to the SM.
Definition at line 2457 of file HiggsKigen.h.
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The factor rescaling the SM-like Higgs couplings to the Z vector bosons with respect to the SM.
Definition at line 2458 of file HiggsKigen.h.
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The factor rescaling the effective Higgs couplings to the Z and a photon with respect to the SM.
Definition at line 2461 of file HiggsKigen.h.
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The number of the model parameters in HiggsKigen: 17 modelpars + 39 + 38 th. err. pars.
Definition at line 201 of file HiggsKigen.h.
1.9.2 