#include <SigmaBR.h>

Inheritance diagram for SigmaBR:

Detailed Description

Definition at line 14 of file SigmaBR.h.

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

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

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

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

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

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

virtual double	BrHWW2l2vRatio () const
	The ratio of the Br $(H\to WW^*\to l\nu l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. More...

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

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

virtual double	BrHZZ2e2muRatio () const
	The ratio of the Br $(H\to ZZ* \to 2e 2\mu)$ in the current model and in the Standard Model. More...

virtual double	BrHZZ4eRatio () const
	The ratio of the Br $(H\to ZZ* \to 4e)$ in the current model and in the Standard Model. More...

virtual double	BrHZZ4lRatio () const
	The ratio of the Br $(H\to ZZ* \to 4l)$ ( $l=e,\mu $) in the current model and in the Standard Model. More...

virtual double	BrHZZ4muRatio () const
	The ratio of the Br $(H\to ZZ* \to 4\mu)$ in the current model and in the Standard Model. More...

virtual 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 NPEffectiveGIMR have been provided in model initialization. More...

virtual double	mueeHvv (const double sqrt_s) 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 double	mueeHvvPol (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 double	mueettH (const double sqrt_s) 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 double	mueettHPol (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 double	mueeZBF (const double sqrt_s) 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 double	mueeZBFPol (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 double	mueeZH (const double sqrt_s) 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 double	mueeZHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeZH}$ between the $ e^{+}e^{-}\to ZH $ associated production cross-section in the current model and in the Standard Model. More...

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

virtual 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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...

	SigmaBR ()

Public Member Functions inherited from NPbase
virtual 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 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 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 double	AuxObs_NP1 () const
	Auxiliary observable AuxObs_NP1. More...

virtual double	AuxObs_NP10 () const
	Auxiliary observable AuxObs_NP10. More...

virtual double	AuxObs_NP11 () const
	Auxiliary observable AuxObs_NP11. More...

virtual double	AuxObs_NP12 () const
	Auxiliary observable AuxObs_NP12. More...

virtual double	AuxObs_NP13 () const
	Auxiliary observable AuxObs_NP13. More...

virtual double	AuxObs_NP14 () const
	Auxiliary observable AuxObs_NP14. More...

virtual double	AuxObs_NP15 () const
	Auxiliary observable AuxObs_NP15. More...

virtual double	AuxObs_NP16 () const
	Auxiliary observable AuxObs_NP16. More...

virtual double	AuxObs_NP17 () const
	Auxiliary observable AuxObs_NP17. More...

virtual double	AuxObs_NP18 () const
	Auxiliary observable AuxObs_NP18. More...

virtual double	AuxObs_NP19 () const
	Auxiliary observable AuxObs_NP19. More...

virtual double	AuxObs_NP2 () const
	Auxiliary observable AuxObs_NP2. More...

virtual double	AuxObs_NP20 () const
	Auxiliary observable AuxObs_NP20. More...

virtual double	AuxObs_NP3 () const
	Auxiliary observable AuxObs_NP3. More...

virtual double	AuxObs_NP4 () const
	Auxiliary observable AuxObs_NP4. More...

virtual double	AuxObs_NP5 () const
	Auxiliary observable AuxObs_NP5. More...

virtual double	AuxObs_NP6 () const
	Auxiliary observable AuxObs_NP6. More...

virtual double	AuxObs_NP7 () const
	Auxiliary observable AuxObs_NP7. More...

virtual double	AuxObs_NP8 () const
	Auxiliary observable AuxObs_NP8. More...

virtual double	AuxObs_NP9 () const
	Auxiliary observable AuxObs_NP9. More...

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

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

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

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

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

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

virtual double	BrHWlvRatio () const
	The ratio of the Br $(H\to W l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. More...

virtual double	BrHZllRatio () const
	The ratio of the Br $(H\to Zll)$ ( $l=e,\mu $) in the current model and in the Standard Model. More...

virtual double	cbminuscc () const

virtual double	cbminusctau () const

virtual double	ccminusctau () const

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

virtual double	cgaplusct () const

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

virtual double	cggEff_HB () 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 double	cgminuscga () const

virtual double	cgplusct () const

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

virtual double	cVpluscb () const

virtual double	cVplusctau () const

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

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

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

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

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

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

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

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

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

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

virtual 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 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 double	deltaG_hggRatio () const
	The full new physics contribution to the coupling of the effective interaction $H G_{\mu\nu}^AG^{A \mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value. More...

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

virtual double	mueeWBF (const double sqrt_s) 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 double	mueeWBFPol (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 double	mueeWW (const double sqrt_s) 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 double	mueeWWPol (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 double	mueeZllH (const double sqrt_s) 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 double	mueeZllHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}$ between the $ e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- $ associated production cross-section in the current model and in the Standard Model. More...

virtual double	mueeZqqH (const double sqrt_s) 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 double	mueeZqqHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeZH, Z \to q \bar{q}}$ between the $ e^{+}e^{-}\to ZH, Z \to q \bar{q} $ associated production cross-section in the current model and in the Standard Model. More...

virtual 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 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 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 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 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 double	muppHmumu (const double sqrt_s) const

virtual double	muppHZga (const double sqrt_s) const

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

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

	NPbase ()
	The default constructor. More...

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

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

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

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

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

virtual bool	PostUpdate ()
	The postupdate method for NPbase. More...

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

virtual 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 double	UpperLimitZgammaA (const double sqrt_s) const

virtual double	UpperLimitZgammaA13 (const double sqrt_s) const

virtual double	UpperLimitZgammaC (const double sqrt_s) const

virtual double	UpperLimitZgammaC13 (const double sqrt_s) const

virtual 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...

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

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

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

double	Als (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const
	The running QCD coupling $\alpha(\mu)$ in the $\overline{MS}$ scheme including QED corrections. More...

double	AlsByOrder (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) 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...

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

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

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...

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

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

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

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

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

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

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

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

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

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

double	computeBrHtoZZinv () const
	The Br $(H\to ZZ \to inv)$ 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...

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

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

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

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

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

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

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

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

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

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. [138]. More...

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

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...

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

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...

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

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

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

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

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

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

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 double	cW2 () const

virtual 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...

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

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...

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

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

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

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

virtual 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 double	epsilon1 () const
	The SM contribution to the epsilon parameter $\varepsilon_1$. More...

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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...

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

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

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

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

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

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

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...

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...

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...

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

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

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

const Flavour &	getFlavour () const

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

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

virtual double	getmq (const QCD::quark q, const double mu) const

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

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

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

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

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

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

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

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

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

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

bool	IsFlagNoApproximateGammaZ () const
	A method to retrieve the model flag NoApproximateGammaZ. More...

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

virtual double	LEP2AFBbottom (const double s) const

virtual double	LEP2AFBcharm (const double s) const

virtual double	LEP2AFBmu (const double s) const

virtual double	LEP2AFBtau (const double s) const

virtual double	LEP2Rbottom (const double s) const

virtual double	LEP2Rcharm (const double s) const

virtual double	LEP2sigmaBottom (const double s) const

virtual double	LEP2sigmaCharm (const double s) const

virtual double	LEP2sigmaHadron (const double s) const

virtual double	LEP2sigmaMu (const double s) const

virtual double	LEP2sigmaTau (const double s) const

virtual double	Mw_tree () const
	The tree-level mass of the $W$ boson, $M_W^{\mathrm{tree}}$. More...

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...

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 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...

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

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

	StandardModel ()
	The default constructor. More...

double	sW2 () const

virtual 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...

virtual double	v () const
	The Higgs vacuum expectation value. More...

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

Public Member Functions inherited from QCD
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...

virtual double	Als (const double mu, const orders order=FULLNLO, bool Nf_thr=true) 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...

virtual double	AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) 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...

double	AlsWithInit (const double mu, const double alsi, const double mu_i, 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...

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...

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

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

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

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

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

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

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

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

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

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

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...

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...

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...

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...

BParameter	getBKd1 () const

BParameter	getBKd3 () const

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

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

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

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

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

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

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

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

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

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...

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

double	Mbar2Mp (const double mbar, const orders order=FULLNNLO) const
	Converts the $\overline{\mathrm{MS}}$ mass $m(m)$ to the pole mass. More...

double	Mp2Mbar (const double mp, const orders order=FULLNNLO) const
	Converts a quark pole mass to the corresponding $\overline{\mathrm{MS}}$ mass $m(m)$. More...

double	Mrun (const double mu, const double m, const orders order=FULLNNLO) const
	Computes a running quark mass $m(\mu)$ from $m(m)$. More...

double	Mrun (const double mu_f, const double mu_i, const double m, const orders order=FULLNNLO) const
	Runs a quark mass from $\mu_i$ to $\mu_f$. More...

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...

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

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...

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

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...

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

	QCD ()
	Constructor. 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...

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	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	setModelSUSY ()

void	setModelTHDM ()

void	setModelTHDMW ()

void	setSliced (bool Sliced)

void	setUpdateError (bool UpdateError)
	A set method to fix the update status as success or failure. More...

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

Static Public Attributes
static const int	NSigmaBRVars = 45
	The number of the model parameters in SigmaBR. More...

static const std::string	SigmaBRVars [NSigmaBRVars]
	A string array containing the labels of the model parameters in NPEffectiveGIMR. More...

Static Public Attributes inherited from StandardModel
static const double	GeVminus2_to_nb = 389379.338

static const double	Mw_error = 0.00001
	The target accuracy of the iterative calculation of the $W$-boson mass in units of GeV. More...

static const int	NSMvars = 26
	The number of the model parameters in StandardModel. More...

static const int	NumSMParamsForEWPO = 33
	The number of the SM parameters that are relevant to the EW precision observables. More...

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

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

static std::string	QCDvars [NQCDvars]
	An array containing the labels under which all QCD parameters are stored in a vector of ModelParameter via InputParser::ReadParameters(). More...

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

Protected Member Functions inherited from StandardModel
double	AFB_NoISR_l (const QCD::lepton l_flavor, const double s) 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 Yukawa matrices. 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...

double	getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const

double	getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const

double	getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const

double	getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const

double	getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const

double	getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const

double	getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const

double	getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const

double	getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const

double	getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const

double	getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const

double	getIntegrand_AFBnumeratorWithISR_charm133 (double x) const

double	getIntegrand_AFBnumeratorWithISR_charm167 (double x) const

double	getIntegrand_AFBnumeratorWithISR_charm172 (double x) const

double	getIntegrand_AFBnumeratorWithISR_charm183 (double x) const

double	getIntegrand_AFBnumeratorWithISR_charm189 (double x) const

double	getIntegrand_AFBnumeratorWithISR_charm192 (double x) const

double	getIntegrand_AFBnumeratorWithISR_charm196 (double x) const

double	getIntegrand_AFBnumeratorWithISR_charm200 (double x) const

double	getIntegrand_AFBnumeratorWithISR_charm202 (double x) const

double	getIntegrand_AFBnumeratorWithISR_charm205 (double x) const

double	getIntegrand_AFBnumeratorWithISR_charm207 (double x) const

double	getIntegrand_AFBnumeratorWithISR_mu130 (double x) const

double	getIntegrand_AFBnumeratorWithISR_mu136 (double x) const

double	getIntegrand_AFBnumeratorWithISR_mu161 (double x) const

double	getIntegrand_AFBnumeratorWithISR_mu172 (double x) const

double	getIntegrand_AFBnumeratorWithISR_mu183 (double x) const

double	getIntegrand_AFBnumeratorWithISR_mu189 (double x) const

double	getIntegrand_AFBnumeratorWithISR_mu192 (double x) const

double	getIntegrand_AFBnumeratorWithISR_mu196 (double x) const

double	getIntegrand_AFBnumeratorWithISR_mu200 (double x) const

double	getIntegrand_AFBnumeratorWithISR_mu202 (double x) const

double	getIntegrand_AFBnumeratorWithISR_mu205 (double x) const

double	getIntegrand_AFBnumeratorWithISR_mu207 (double x) const

double	getIntegrand_AFBnumeratorWithISR_tau130 (double x) const

double	getIntegrand_AFBnumeratorWithISR_tau136 (double x) const

double	getIntegrand_AFBnumeratorWithISR_tau161 (double x) const

double	getIntegrand_AFBnumeratorWithISR_tau172 (double x) const

double	getIntegrand_AFBnumeratorWithISR_tau183 (double x) const

double	getIntegrand_AFBnumeratorWithISR_tau189 (double x) const

double	getIntegrand_AFBnumeratorWithISR_tau192 (double x) const

double	getIntegrand_AFBnumeratorWithISR_tau196 (double x) const

double	getIntegrand_AFBnumeratorWithISR_tau200 (double x) const

double	getIntegrand_AFBnumeratorWithISR_tau202 (double x) const

double	getIntegrand_AFBnumeratorWithISR_tau205 (double x) const

double	getIntegrand_AFBnumeratorWithISR_tau207 (double x) const

double	getIntegrand_dsigmaBox_bottom130 (double x) const

double	getIntegrand_dsigmaBox_bottom133 (double x) const

double	getIntegrand_dsigmaBox_bottom136 (double x) const

double	getIntegrand_dsigmaBox_bottom161 (double x) const

double	getIntegrand_dsigmaBox_bottom167 (double x) const

double	getIntegrand_dsigmaBox_bottom172 (double x) const

double	getIntegrand_dsigmaBox_bottom183 (double x) const

double	getIntegrand_dsigmaBox_bottom189 (double x) const

double	getIntegrand_dsigmaBox_bottom192 (double x) const

double	getIntegrand_dsigmaBox_bottom196 (double x) const

double	getIntegrand_dsigmaBox_bottom200 (double x) const

double	getIntegrand_dsigmaBox_bottom202 (double x) const

double	getIntegrand_dsigmaBox_bottom205 (double x) const

double	getIntegrand_dsigmaBox_bottom207 (double x) const

double	getIntegrand_dsigmaBox_charm130 (double x) const

double	getIntegrand_dsigmaBox_charm133 (double x) const

double	getIntegrand_dsigmaBox_charm136 (double x) const

double	getIntegrand_dsigmaBox_charm161 (double x) const

double	getIntegrand_dsigmaBox_charm167 (double x) const

double	getIntegrand_dsigmaBox_charm172 (double x) const

double	getIntegrand_dsigmaBox_charm183 (double x) const

double	getIntegrand_dsigmaBox_charm189 (double x) const

double	getIntegrand_dsigmaBox_charm192 (double x) const

double	getIntegrand_dsigmaBox_charm196 (double x) const

double	getIntegrand_dsigmaBox_charm200 (double x) const

double	getIntegrand_dsigmaBox_charm202 (double x) const

double	getIntegrand_dsigmaBox_charm205 (double x) const

double	getIntegrand_dsigmaBox_charm207 (double x) const

double	getIntegrand_dsigmaBox_down130 (double x) const

double	getIntegrand_dsigmaBox_down133 (double x) const

double	getIntegrand_dsigmaBox_down136 (double x) const

double	getIntegrand_dsigmaBox_down161 (double x) const

double	getIntegrand_dsigmaBox_down167 (double x) const

double	getIntegrand_dsigmaBox_down172 (double x) const

double	getIntegrand_dsigmaBox_down183 (double x) const

double	getIntegrand_dsigmaBox_down189 (double x) const

double	getIntegrand_dsigmaBox_down192 (double x) const

double	getIntegrand_dsigmaBox_down196 (double x) const

double	getIntegrand_dsigmaBox_down200 (double x) const

double	getIntegrand_dsigmaBox_down202 (double x) const

double	getIntegrand_dsigmaBox_down205 (double x) const

double	getIntegrand_dsigmaBox_down207 (double x) const

double	getIntegrand_dsigmaBox_mu130 (double x) const

double	getIntegrand_dsigmaBox_mu133 (double x) const

double	getIntegrand_dsigmaBox_mu136 (double x) const

double	getIntegrand_dsigmaBox_mu161 (double x) const

double	getIntegrand_dsigmaBox_mu167 (double x) const

double	getIntegrand_dsigmaBox_mu172 (double x) const

double	getIntegrand_dsigmaBox_mu183 (double x) const

double	getIntegrand_dsigmaBox_mu189 (double x) const

double	getIntegrand_dsigmaBox_mu192 (double x) const

double	getIntegrand_dsigmaBox_mu196 (double x) const

double	getIntegrand_dsigmaBox_mu200 (double x) const

double	getIntegrand_dsigmaBox_mu202 (double x) const

double	getIntegrand_dsigmaBox_mu205 (double x) const

double	getIntegrand_dsigmaBox_mu207 (double x) const

double	getIntegrand_dsigmaBox_strange130 (double x) const

double	getIntegrand_dsigmaBox_strange133 (double x) const

double	getIntegrand_dsigmaBox_strange136 (double x) const

double	getIntegrand_dsigmaBox_strange161 (double x) const

double	getIntegrand_dsigmaBox_strange167 (double x) const

double	getIntegrand_dsigmaBox_strange172 (double x) const

double	getIntegrand_dsigmaBox_strange183 (double x) const

double	getIntegrand_dsigmaBox_strange189 (double x) const

double	getIntegrand_dsigmaBox_strange192 (double x) const

double	getIntegrand_dsigmaBox_strange196 (double x) const

double	getIntegrand_dsigmaBox_strange200 (double x) const

double	getIntegrand_dsigmaBox_strange202 (double x) const

double	getIntegrand_dsigmaBox_strange205 (double x) const

double	getIntegrand_dsigmaBox_strange207 (double x) const

double	getIntegrand_dsigmaBox_tau130 (double x) const

double	getIntegrand_dsigmaBox_tau133 (double x) const

double	getIntegrand_dsigmaBox_tau136 (double x) const

double	getIntegrand_dsigmaBox_tau161 (double x) const

double	getIntegrand_dsigmaBox_tau167 (double x) const

double	getIntegrand_dsigmaBox_tau172 (double x) const

double	getIntegrand_dsigmaBox_tau183 (double x) const

double	getIntegrand_dsigmaBox_tau189 (double x) const

double	getIntegrand_dsigmaBox_tau192 (double x) const

double	getIntegrand_dsigmaBox_tau196 (double x) const

double	getIntegrand_dsigmaBox_tau200 (double x) const

double	getIntegrand_dsigmaBox_tau202 (double x) const

double	getIntegrand_dsigmaBox_tau205 (double x) const

double	getIntegrand_dsigmaBox_tau207 (double x) const

double	getIntegrand_dsigmaBox_up130 (double x) const

double	getIntegrand_dsigmaBox_up133 (double x) const

double	getIntegrand_dsigmaBox_up136 (double x) const

double	getIntegrand_dsigmaBox_up161 (double x) const

double	getIntegrand_dsigmaBox_up167 (double x) const

double	getIntegrand_dsigmaBox_up172 (double x) const

double	getIntegrand_dsigmaBox_up183 (double x) const

double	getIntegrand_dsigmaBox_up189 (double x) const

double	getIntegrand_dsigmaBox_up192 (double x) const

double	getIntegrand_dsigmaBox_up196 (double x) const

double	getIntegrand_dsigmaBox_up200 (double x) const

double	getIntegrand_dsigmaBox_up202 (double x) const

double	getIntegrand_dsigmaBox_up205 (double x) const

double	getIntegrand_dsigmaBox_up207 (double x) const

double	getIntegrand_sigmaWithISR_bottom130 (double x) const

double	getIntegrand_sigmaWithISR_bottom133 (double x) const

double	getIntegrand_sigmaWithISR_bottom136 (double x) const

double	getIntegrand_sigmaWithISR_bottom161 (double x) const

double	getIntegrand_sigmaWithISR_bottom167 (double x) const

double	getIntegrand_sigmaWithISR_bottom172 (double x) const

double	getIntegrand_sigmaWithISR_bottom183 (double x) const

double	getIntegrand_sigmaWithISR_bottom189 (double x) const

double	getIntegrand_sigmaWithISR_bottom192 (double x) const

double	getIntegrand_sigmaWithISR_bottom196 (double x) const

double	getIntegrand_sigmaWithISR_bottom200 (double x) const

double	getIntegrand_sigmaWithISR_bottom202 (double x) const

double	getIntegrand_sigmaWithISR_bottom205 (double x) const

double	getIntegrand_sigmaWithISR_bottom207 (double x) const

double	getIntegrand_sigmaWithISR_charm130 (double x) const

double	getIntegrand_sigmaWithISR_charm133 (double x) const

double	getIntegrand_sigmaWithISR_charm136 (double x) const

double	getIntegrand_sigmaWithISR_charm161 (double x) const

double	getIntegrand_sigmaWithISR_charm167 (double x) const

double	getIntegrand_sigmaWithISR_charm172 (double x) const

double	getIntegrand_sigmaWithISR_charm183 (double x) const

double	getIntegrand_sigmaWithISR_charm189 (double x) const

double	getIntegrand_sigmaWithISR_charm192 (double x) const

double	getIntegrand_sigmaWithISR_charm196 (double x) const

double	getIntegrand_sigmaWithISR_charm200 (double x) const

double	getIntegrand_sigmaWithISR_charm202 (double x) const

double	getIntegrand_sigmaWithISR_charm205 (double x) const

double	getIntegrand_sigmaWithISR_charm207 (double x) const

double	getIntegrand_sigmaWithISR_down130 (double x) const

double	getIntegrand_sigmaWithISR_down133 (double x) const

double	getIntegrand_sigmaWithISR_down136 (double x) const

double	getIntegrand_sigmaWithISR_down161 (double x) const

double	getIntegrand_sigmaWithISR_down167 (double x) const

double	getIntegrand_sigmaWithISR_down172 (double x) const

double	getIntegrand_sigmaWithISR_down183 (double x) const

double	getIntegrand_sigmaWithISR_down189 (double x) const

double	getIntegrand_sigmaWithISR_down192 (double x) const

double	getIntegrand_sigmaWithISR_down196 (double x) const

double	getIntegrand_sigmaWithISR_down200 (double x) const

double	getIntegrand_sigmaWithISR_down202 (double x) const

double	getIntegrand_sigmaWithISR_down205 (double x) const

double	getIntegrand_sigmaWithISR_down207 (double x) const

double	getIntegrand_sigmaWithISR_mu130 (double x) const

double	getIntegrand_sigmaWithISR_mu136 (double x) const

double	getIntegrand_sigmaWithISR_mu161 (double x) const

double	getIntegrand_sigmaWithISR_mu172 (double x) const

double	getIntegrand_sigmaWithISR_mu183 (double x) const

double	getIntegrand_sigmaWithISR_mu189 (double x) const

double	getIntegrand_sigmaWithISR_mu192 (double x) const

double	getIntegrand_sigmaWithISR_mu196 (double x) const

double	getIntegrand_sigmaWithISR_mu200 (double x) const

double	getIntegrand_sigmaWithISR_mu202 (double x) const

double	getIntegrand_sigmaWithISR_mu205 (double x) const

double	getIntegrand_sigmaWithISR_mu207 (double x) const

double	getIntegrand_sigmaWithISR_strange130 (double x) const

double	getIntegrand_sigmaWithISR_strange133 (double x) const

double	getIntegrand_sigmaWithISR_strange136 (double x) const

double	getIntegrand_sigmaWithISR_strange161 (double x) const

double	getIntegrand_sigmaWithISR_strange167 (double x) const

double	getIntegrand_sigmaWithISR_strange172 (double x) const

double	getIntegrand_sigmaWithISR_strange183 (double x) const

double	getIntegrand_sigmaWithISR_strange189 (double x) const

double	getIntegrand_sigmaWithISR_strange192 (double x) const

double	getIntegrand_sigmaWithISR_strange196 (double x) const

double	getIntegrand_sigmaWithISR_strange200 (double x) const

double	getIntegrand_sigmaWithISR_strange202 (double x) const

double	getIntegrand_sigmaWithISR_strange205 (double x) const

double	getIntegrand_sigmaWithISR_strange207 (double x) const

double	getIntegrand_sigmaWithISR_tau130 (double x) const

double	getIntegrand_sigmaWithISR_tau136 (double x) const

double	getIntegrand_sigmaWithISR_tau161 (double x) const

double	getIntegrand_sigmaWithISR_tau172 (double x) const

double	getIntegrand_sigmaWithISR_tau183 (double x) const

double	getIntegrand_sigmaWithISR_tau189 (double x) const

double	getIntegrand_sigmaWithISR_tau192 (double x) const

double	getIntegrand_sigmaWithISR_tau196 (double x) const

double	getIntegrand_sigmaWithISR_tau200 (double x) const

double	getIntegrand_sigmaWithISR_tau202 (double x) const

double	getIntegrand_sigmaWithISR_tau205 (double x) const

double	getIntegrand_sigmaWithISR_tau207 (double x) const

double	getIntegrand_sigmaWithISR_up130 (double x) const

double	getIntegrand_sigmaWithISR_up133 (double x) const

double	getIntegrand_sigmaWithISR_up136 (double x) const

double	getIntegrand_sigmaWithISR_up161 (double x) const

double	getIntegrand_sigmaWithISR_up167 (double x) const

double	getIntegrand_sigmaWithISR_up172 (double x) const

double	getIntegrand_sigmaWithISR_up183 (double x) const

double	getIntegrand_sigmaWithISR_up189 (double x) const

double	getIntegrand_sigmaWithISR_up192 (double x) const

double	getIntegrand_sigmaWithISR_up196 (double x) const

double	getIntegrand_sigmaWithISR_up200 (double x) const

double	getIntegrand_sigmaWithISR_up202 (double x) const

double	getIntegrand_sigmaWithISR_up205 (double x) const

double	getIntegrand_sigmaWithISR_up207 (double x) const

double	Integrand_AFBnumeratorWithISR_l (double x, const QCD::lepton l_flavor, const double s) const

double	Integrand_AFBnumeratorWithISR_q (double x, const QCD::quark q_flavor, const double s) const

double	Integrand_dsigmaBox_l (double cosTheta, const QCD::lepton l_flavor, const double s) const

double	Integrand_dsigmaBox_q (double cosTheta, const QCD::quark q_flavor, const double s) const

double	Integrand_sigmaWithISR_l (double x, const QCD::lepton l_flavor, const double s) 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...

double	sigma_NoISR_l (const QCD::lepton l_flavor, const double s) 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
double	MassOfNf (int nf) const
	The Mbar mass of the heaviest quark in the theory with Nf active flavour. More...

Protected Attributes
double	brhbbratio
	The ratio of the Hbb BR in the current model w.r.t. the SM. More...

double	brhccratio
	The ratio of the Hcc BR in the current model w.r.t. the SM. More...

double	brhgagaratio
	The ratio of the Hgaga BR in the current model w.r.t. the SM. More...

double	brhggratio
	The ratio of the Hgg BR in the current model w.r.t. the SM. More...

double	brhmumuratio
	The ratio of the Hmumu BR in the current model w.r.t. the SM. More...

double	brhtautauratio
	The ratio of the Htautau BR in the current model w.r.t. the SM. More...

double	brhwwratio
	The ratio of the HWW BR in the current model w.r.t. the SM. More...

double	brhzgaratio
	The ratio of the HZga BR in the current model w.r.t. the SM. More...

double	brhzzratio
	The ratio of the HZZ BR in the current model w.r.t. the SM. More...

double	eeHee1000

double	eeHee1500

double	eeHee240

double	eeHee250

double	eeHee3000
	The eeHee cross section. More...

double	eeHee350

double	eeHee365

double	eeHee380

double	eeHee500

double	eeHvv1000

double	eeHvv1500

double	eeHvv240

double	eeHvv250

double	eeHvv3000
	The eeHvv cross section. More...

double	eeHvv350

double	eeHvv365

double	eeHvv380

double	eeHvv500

double	eettH1000

double	eettH1500

double	eettH3000
	The eettH cross section. More...

double	eettH500

double	eeZH1000

double	eeZH1500

double	eeZH240

double	eeZH250

double	eeZH3000
	The eeZH cross section. More...

double	eeZH350

double	eeZH365

double	eeZH380

double	eeZH500

double	ggh
	The ggH cross section. More...

double	tth
	The ttH cross section. More...

double	vbf
	The VBF cross section. More...

double	wh
	The WH cross section. More...

double	zh
	The ZH cross section. More...

Protected Attributes inherited from NPbase
StandardModel	trueSM

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

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

double	alpha21

double	alpha31

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

bool	bSigmaForAFB

bool	bSigmaForR

double	dAle5Mz
	The five-flavour hadronic contribution to the electromagnetic coupling, $\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)$. 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	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...

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	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

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...

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
	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
	A boolean set to false if update is successful. More...

Additional Inherited Members
Public Types inherited from StandardModel
enum	LEP2RCs { Weak = 0, WeakBox, ISR, QEDFSR, QCDFSR, NUMofLEP2RCs }

enum	orders_EW { EW1 = 0, EW1QCD1, EW1QCD2, EW2, EW2QCD1, EW3, orders_EW_size }
	An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More...

Public Types inherited from QCD
enum	lepton { NEUTRINO_1, ELECTRON, NEUTRINO_2, MU, NEUTRINO_3, TAU, NOLEPTON }
	An enum type for leptons. More...

enum	meson { P_0, P_P, K_0, K_P, D_0, D_P, B_D, B_P, B_S, B_C, PHI, K_star, K_star_P, 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...

Constructor & Destructor Documentation

◆ SigmaBR()

SigmaBR::SigmaBR ( )

Definition at line 17 of file SigmaBR.cpp.

 : NPbase()
 {
     
     ModelParamMap.insert(std::make_pair("ggH", std::cref(ggh)));
     ModelParamMap.insert(std::make_pair("VBF", std::cref(vbf)));
     ModelParamMap.insert(std::make_pair("WH", std::cref(wh)));
     ModelParamMap.insert(std::make_pair("ZH", std::cref(zh)));
     ModelParamMap.insert(std::make_pair("ttH", std::cref(tth)));
     ModelParamMap.insert(std::make_pair("eeZH240", std::cref(eeZH240)));
     ModelParamMap.insert(std::make_pair("eeZH250", std::cref(eeZH250)));
     ModelParamMap.insert(std::make_pair("eeZH350", std::cref(eeZH350)));
     ModelParamMap.insert(std::make_pair("eeZH365", std::cref(eeZH365)));
     ModelParamMap.insert(std::make_pair("eeZH380", std::cref(eeZH380)));    
     ModelParamMap.insert(std::make_pair("eeZH500", std::cref(eeZH500)));
     ModelParamMap.insert(std::make_pair("eeZH1000", std::cref(eeZH1000)));
     ModelParamMap.insert(std::make_pair("eeZH1500", std::cref(eeZH1500)));
     ModelParamMap.insert(std::make_pair("eeZH3000", std::cref(eeZH3000)));
     ModelParamMap.insert(std::make_pair("eeHvv240", std::cref(eeHvv240)));
     ModelParamMap.insert(std::make_pair("eeHvv250", std::cref(eeHvv250)));
     ModelParamMap.insert(std::make_pair("eeHvv350", std::cref(eeHvv350)));
     ModelParamMap.insert(std::make_pair("eeHvv365", std::cref(eeHvv365)));
     ModelParamMap.insert(std::make_pair("eeHvv380", std::cref(eeHvv380)));    
     ModelParamMap.insert(std::make_pair("eeHvv500", std::cref(eeHvv500)));
     ModelParamMap.insert(std::make_pair("eeHvv1000", std::cref(eeHvv1000)));
     ModelParamMap.insert(std::make_pair("eeHvv1500", std::cref(eeHvv1500)));
     ModelParamMap.insert(std::make_pair("eeHvv3000", std::cref(eeHvv3000)));   
     ModelParamMap.insert(std::make_pair("eeHee240", std::cref(eeHee240)));
     ModelParamMap.insert(std::make_pair("eeHee250", std::cref(eeHee250)));
     ModelParamMap.insert(std::make_pair("eeHee350", std::cref(eeHee350)));
     ModelParamMap.insert(std::make_pair("eeHee365", std::cref(eeHee365)));
     ModelParamMap.insert(std::make_pair("eeHee380", std::cref(eeHee380)));    
     ModelParamMap.insert(std::make_pair("eeHee500", std::cref(eeHee500)));
     ModelParamMap.insert(std::make_pair("eeHee1000", std::cref(eeHee1000)));
     ModelParamMap.insert(std::make_pair("eeHee1500", std::cref(eeHee1500)));
     ModelParamMap.insert(std::make_pair("eeHee3000", std::cref(eeHee3000))); 
     ModelParamMap.insert(std::make_pair("eettH500", std::cref(eettH500)));
     ModelParamMap.insert(std::make_pair("eettH1000", std::cref(eettH1000)));
     ModelParamMap.insert(std::make_pair("eettH1500", std::cref(eettH1500)));
     ModelParamMap.insert(std::make_pair("eettH3000", std::cref(eeHee3000)));
     ModelParamMap.insert(std::make_pair("BrHggRatio", std::cref(brhggratio)));
     ModelParamMap.insert(std::make_pair("BrHWWRatio", std::cref(brhwwratio)));
     ModelParamMap.insert(std::make_pair("BrHZZRatio", std::cref(brhzzratio)));
     ModelParamMap.insert(std::make_pair("BrHZgaRatio", std::cref(brhzgaratio)));
     ModelParamMap.insert(std::make_pair("BrHgagaRatio", std::cref(brhgagaratio)));
     ModelParamMap.insert(std::make_pair("BrHtautauRatio", std::cref(brhtautauratio)));
     ModelParamMap.insert(std::make_pair("BrHmumuRatio", std::cref(brhmumuratio)));
     ModelParamMap.insert(std::make_pair("BrHccRatio", std::cref(brhccratio)));
     ModelParamMap.insert(std::make_pair("BrHbbRatio", std::cref(brhbbratio)));
 }

Member Function Documentation

◆ BrHbbRatio()

double SigmaBR::BrHbbRatio ( ) const

virtual

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

Returns: Br $(H\to b\bar{b})$/Br $(H\to b\bar{b})_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 496 of file SigmaBR.cpp.

 {
     return brhbbratio;
 }

◆ BrHccRatio()

double SigmaBR::BrHccRatio ( ) const

virtual

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

Returns: Br $(H\to c\bar{c})$/Br $(H\to c\bar{c})_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 491 of file SigmaBR.cpp.

 {
     return brhccratio;
 }

◆ BrHgagaRatio()

double SigmaBR::BrHgagaRatio ( ) const

virtual

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

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

Reimplemented from NPbase.

Definition at line 476 of file SigmaBR.cpp.

 {
     return brhgagaratio;
 }

◆ BrHggRatio()

double SigmaBR::BrHggRatio ( ) const

virtual

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

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

Reimplemented from NPbase.

Definition at line 416 of file SigmaBR.cpp.

 {
     return brhggratio;
 }

◆ BrHmumuRatio()

double SigmaBR::BrHmumuRatio ( ) const

virtual

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

Returns: Br $(H\to \mu^+\mu^-)$/Br $(H\to \mu^+\mu^-)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 486 of file SigmaBR.cpp.

 {
     return brhmumuratio;
 }

◆ BrHtautauRatio()

double SigmaBR::BrHtautauRatio ( ) const

virtual

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

Returns: Br $(H\to \tau^+\tau^-)$/Br $(H\to \tau^+\tau^-)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 481 of file SigmaBR.cpp.

 {
     return brhtautauratio;
 }

◆ BrHWW2l2vRatio()

double SigmaBR::BrHWW2l2vRatio ( ) const

virtual

The ratio of the Br $(H\to WW^*\to l\nu l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model.

Returns: Br $(H\to WW^*\to l\nu l\nu)$/Br $(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 426 of file SigmaBR.cpp.

 {
     return BrHWWRatio();
 }

◆ BrHWWRatio()

double SigmaBR::BrHWWRatio ( ) const

virtual

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

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

Reimplemented from NPbase.

Definition at line 421 of file SigmaBR.cpp.

 {
     return brhwwratio;
 }

◆ BrHZgaeeRatio()

double SigmaBR::BrHZgaeeRatio ( ) const

virtual

The ratio of the Br $(H\to Z\gamma\to ee\gamma)$ in the current model and in the Standard Model.

Returns: Br $(H\to Z\gamma\to ee\gamma)$/Br $(H\to Z\gamma\to ee\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 466 of file SigmaBR.cpp.

 {
     return BrHZgaRatio();
 }

◆ BrHZgallRatio()

double SigmaBR::BrHZgallRatio ( ) const

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.

Returns: Br $(H\to Z\gamma\to ll\gamma)$/Br $(H\to Z\gamma\to ll\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 461 of file SigmaBR.cpp.

 {
     return BrHZgaRatio();
 }

◆ BrHZgamumuRatio()

double SigmaBR::BrHZgamumuRatio ( ) const

virtual

The ratio of the Br $(H\to Z\gamma\to \mu\mu\gamma)$ in the current model and in the Standard Model.

Returns: Br $(H\to Z\gamma\to \mu\mu\gamma)$/Br $(H\to Z\gamma\to \mu\mu\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 471 of file SigmaBR.cpp.

 {
     return BrHZgaRatio();
 }

◆ BrHZgaRatio()

double SigmaBR::BrHZgaRatio ( ) const

virtual

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

Returns: Br $(H\to Z\gamma)$/Br $(H\to Z\gamma)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 456 of file SigmaBR.cpp.

 {
     return brhzgaratio;
 }

◆ BrHZZ2e2muRatio()

double SigmaBR::BrHZZ2e2muRatio ( ) const

virtual

The ratio of the Br $(H\to ZZ* \to 2e 2\mu)$ in the current model and in the Standard Model.

Returns: Br $(H\to ZZ* \to 2e 2\mu)$/Br $(H\to ZZ* \to 2e 2\mu)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 446 of file SigmaBR.cpp.

 {
     return BrHZZRatio();
 }

◆ BrHZZ4eRatio()

double SigmaBR::BrHZZ4eRatio ( ) const

virtual

The ratio of the Br $(H\to ZZ* \to 4e)$ in the current model and in the Standard Model.

Returns: Br $(H\to ZZ* \to 4e)$/Br $(H\to ZZ* \to 4e)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 441 of file SigmaBR.cpp.

 {
     return BrHZZRatio();
 }

◆ BrHZZ4lRatio()

double SigmaBR::BrHZZ4lRatio ( ) const

virtual

The ratio of the Br $(H\to ZZ* \to 4l)$ ( $l=e,\mu $) in the current model and in the Standard Model.

Returns: Br $(H\to ZZ* \to 4l)$/Br $(H\to ZZ* \to 4l)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 436 of file SigmaBR.cpp.

 {
     return BrHZZRatio();
 }

◆ BrHZZ4muRatio()

double SigmaBR::BrHZZ4muRatio ( ) const

virtual

The ratio of the Br $(H\to ZZ* \to 4\mu)$ in the current model and in the Standard Model.

Returns: Br $(H\to ZZ* \to 4\mu)$/Br $(H\to ZZ* \to 4\mu)_{\mathrm{SM}}$

Reimplemented from NPbase.

Definition at line 451 of file SigmaBR.cpp.

 {
     return BrHZZRatio();
 }

◆ BrHZZRatio()

double SigmaBR::BrHZZRatio ( ) const

virtual

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

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

Reimplemented from NPbase.

Definition at line 431 of file SigmaBR.cpp.

 {
     return brhzzratio;
 }

◆ CheckParameters()

bool SigmaBR::CheckParameters ( const std::map< std::string, double > & DPars )

virtual

A method to check if all the mandatory parameters for NPEffectiveGIMR have been provided in model initialization.

Parameters

[in] DPars a map of the parameters that are being updated in the Monte Carlo run (including parameters that are varied and those that are held constant)

Returns: a boolean that is true if the execution is successful

Reimplemented from StandardModel.

Definition at line 164 of file SigmaBR.cpp.

 {
         for (int i = 0; i < NSigmaBRVars; i++) 
             if (DPars.find(SigmaBRVars[i]) == DPars.end()) {
                 std::cout << "ERROR: Missing mandatory SigmaBR parameter"
                         << SigmaBRVars[i] << std::endl;
                 raiseMissingModelParameterCount();
                 addMissingModelParameter(SigmaBRVars[i]);
             }
     return (NPbase::CheckParameters(DPars));
 }

◆ mueeHvv()

double SigmaBR::mueeHvv ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{e^+e^- \to H\nu\bar{\nu}}$

Reimplemented from NPbase.

Definition at line 289 of file SigmaBR.cpp.

 {
     if (sqrt_s == 0.240) {
         
         return eeHvv240;
         
     } else if (sqrt_s == 0.250) {
         
         return eeHvv250;
         
     } else if (sqrt_s == 0.350) {
  
         return eeHvv350;        
         
     } else if (sqrt_s == 0.365) {
         
         return eeHvv365;
         
     } else if (sqrt_s == 0.380) {
         
         return eeHvv380;
         
     } else if (sqrt_s == 0.500) {
         
         return eeHvv500;
         
     } else if (sqrt_s == 1.0) {
         
         return eeHvv1000;
         
     } else if (sqrt_s == 1.5) {
         
         return eeHvv1500;
         
     } else if (sqrt_s == 3.0) {
         
         return eeHvv3000;
         
     } else
         throw std::runtime_error("Bad argument in SigmaBR::mueeHvv()");
     
     return 1.0;
 }

◆ mueeHvvPol()

double SigmaBR::mueeHvvPol	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{e^+e^- \to H\nu\bar{\nu}}$

Reimplemented from NPbase.

Definition at line 333 of file SigmaBR.cpp.

 {
     return mueeHvv(sqrt_s);
 }

◆ mueettH()

double SigmaBR::mueettH ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{eettH}$

Reimplemented from NPbase.

Definition at line 387 of file SigmaBR.cpp.

 {
     if (sqrt_s == 0.500) {
         
         return eettH500;
         
     } else if (sqrt_s == 1.0) {
         
         return eettH1000;
         
     } else if (sqrt_s == 1.5) {
         
         return eettH1500;
         
     } else if (sqrt_s == 3.0) {
         
         return eettH3000;
         
     } else
         throw std::runtime_error("Bad argument in SigmaBR::mueettH()");
     
     return 1.0;
 }

◆ mueettHPol()

double SigmaBR::mueettHPol	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eettH}$

Reimplemented from NPbase.

Definition at line 411 of file SigmaBR.cpp.

 {
     return mueettH(sqrt_s);
 }

◆ mueeZBF()

double SigmaBR::mueeZBF ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{eeZBF}$

Reimplemented from NPbase.

Definition at line 338 of file SigmaBR.cpp.

 {
     if (sqrt_s == 0.240) {
         
         return eeHee240;
         
     } else if (sqrt_s == 0.250) {
         
         return eeHee250;
         
     } else if (sqrt_s == 0.350) {
  
         return eeHee350;        
         
     } else if (sqrt_s == 0.365) {
         
         return eeHee365;
         
     } else if (sqrt_s == 0.380) {
         
         return eeHee380;
         
     } else if (sqrt_s == 0.500) {
         
         return eeHee500;
         
     } else if (sqrt_s == 1.0) {
         
         return eeHee1000;
         
     } else if (sqrt_s == 1.5) {
         
         return eeHee1500;
         
     } else if (sqrt_s == 3.0) {
         
         return eeHee3000;
         
     } else
         throw std::runtime_error("Bad argument in SigmaBR::mueeHee()");
     
     return 1.0;
 }

◆ mueeZBFPol()

double SigmaBR::mueeZBFPol	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eeZBF}$

Reimplemented from NPbase.

Definition at line 382 of file SigmaBR.cpp.

 {
     return mueeZBF(sqrt_s);
 }

◆ mueeZH()

double SigmaBR::mueeZH ( const double sqrt_s ) const

virtual

The ratio $\mu_{eeZH}$ between the $e^{+}e^{-}\to ZH$ associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{eeZH}$

Reimplemented from NPbase.

Definition at line 237 of file SigmaBR.cpp.

 {
     
     if (sqrt_s == 0.240) {
         
         return eeZH240;
         
     } else if (sqrt_s == 0.250) {
         
         return eeZH250;
         
     } else if (sqrt_s == 0.350) {
  
         return eeZH350;        
         
     } else if (sqrt_s == 0.365) {
         
         return eeZH365;
         
     } else if (sqrt_s == 0.380) {
         
         return eeZH380;
         
     } else if (sqrt_s == 0.500) {
         
         return eeZH500;
         
     } else if (sqrt_s == 1.0) {
         
         return eeZH1000;
         
     } else if (sqrt_s == 1.5) {
         
         return eeZH1500;
         
     } else if (sqrt_s == 3.0) {
         
         return eeZH3000;
         
     } else
         throw std::runtime_error("Bad argument in SigmaBR::mueeZH()");
     
     return 1.0;
  
 }

◆ mueeZHPol()

double SigmaBR::mueeZHPol	(	const double	sqrt_s,
		const double	Pol_em,
		const double	Pol_ep
	)		const

virtual

The ratio $\mu_{eeZH}$ between the $ e^{+}e^{-}\to ZH $ associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively

Returns: $\mu_{eeZH}$

Reimplemented from NPbase.

Definition at line 283 of file SigmaBR.cpp.

 {
     return mueeZH(sqrt_s);
 }

◆ muggH()

double SigmaBR::muggH ( const double sqrt_s ) const

virtual

The ratio $\mu_{ggH}$ between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH}$

Reimplemented from NPbase.

Definition at line 176 of file SigmaBR.cpp.

 {    
     return ggh;
 }

◆ muggHbb()

double SigmaBR::muggHbb ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,bb}$

Reimplemented from NPbase.

Definition at line 741 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHbbRatio();
 }

◆ muggHgaga()

double SigmaBR::muggHgaga ( const double sqrt_s ) const

virtual

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

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

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 501 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHgagaRatio();
 }

◆ muggHmumu()

double SigmaBR::muggHmumu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 681 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHmumuRatio();
 }

◆ muggHpttH()

double SigmaBR::muggHpttH ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH+ttH}$

Reimplemented from NPbase.

Definition at line 225 of file SigmaBR.cpp.

 {
     double sigmaggH_SM = computeSigmaggH(sqrt_s);
     double sigmattH_SM = computeSigmattH(sqrt_s);
     double sigmaggH = muggH(sqrt_s) * sigmaggH_SM;
     double sigmattH = muttH(sqrt_s) * sigmattH_SM;
  
     double mu = ((sigmaggH + sigmattH) / (sigmaggH_SM + sigmattH_SM));
         
     return mu;
 } 

◆ muggHtautau()

double SigmaBR::muggHtautau ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 711 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHtautauRatio();
 }

◆ muggHWW()

double SigmaBR::muggHWW ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,WW}$

Reimplemented from NPbase.

Definition at line 621 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHWWRatio();
 }

◆ muggHWW2l2v()

double SigmaBR::muggHWW2l2v ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 651 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHWW2l2vRatio();
 }

◆ muggHZga()

double SigmaBR::muggHZga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 531 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHZgaRatio();
 }

◆ muggHZZ()

double SigmaBR::muggHZZ ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,ZZ}$

Reimplemented from NPbase.

Definition at line 561 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHZZRatio();
 }

◆ muggHZZ4l()

double SigmaBR::muggHZZ4l ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 591 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHZZ4lRatio();
 }

◆ muTHUggHbb()

double SigmaBR::muTHUggHbb ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,bb}$

Reimplemented from NPbase.

Definition at line 1017 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHbbRatio();
 }

◆ muTHUggHgaga()

double SigmaBR::muTHUggHgaga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 777 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHgagaRatio();
 }

◆ muTHUggHmumu()

double SigmaBR::muTHUggHmumu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 957 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHmumuRatio();
 }

◆ muTHUggHtautau()

double SigmaBR::muTHUggHtautau ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 987 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHtautauRatio();
 }

◆ muTHUggHWW()

double SigmaBR::muTHUggHWW ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,WW}$

Reimplemented from NPbase.

Definition at line 897 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHWWRatio();
 }

◆ muTHUggHWW2l2v()

double SigmaBR::muTHUggHWW2l2v ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 927 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHWW2l2vRatio();
 }

◆ muTHUggHZga()

double SigmaBR::muTHUggHZga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 807 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHZgaRatio();
 }

◆ muTHUggHZgamumu()

double SigmaBR::muTHUggHZgamumu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,Z\gamma\to \gamma 2\mu}$

Reimplemented from NPbase.

Definition at line 1072 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHZgamumuRatio();
 }

◆ muTHUggHZZ()

double SigmaBR::muTHUggHZZ ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,ZZ}$

Reimplemented from NPbase.

Definition at line 837 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHZZRatio();
 }

◆ muTHUggHZZ4l()

double SigmaBR::muTHUggHZZ4l ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 867 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHZZ4lRatio();
 }

◆ muTHUggHZZ4mu()

double SigmaBR::muTHUggHZZ4mu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ggH,ZZ\to 4\mu}$

Reimplemented from NPbase.

Definition at line 1067 of file SigmaBR.cpp.

 {
     return muggH(sqrt_s)*BrHZZ4muRatio();
 }

◆ muTHUttHbb()

double SigmaBR::muTHUttHbb ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,bb}$

Reimplemented from NPbase.

Definition at line 1042 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHbbRatio();
 }

◆ muTHUttHgaga()

double SigmaBR::muTHUttHgaga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 802 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHgagaRatio();
 }

◆ muTHUttHmumu()

double SigmaBR::muTHUttHmumu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 982 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHmumuRatio();
 }

◆ muTHUttHtautau()

double SigmaBR::muTHUttHtautau ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 1012 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHtautauRatio();
 }

◆ muTHUttHWW()

double SigmaBR::muTHUttHWW ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,WW}$

Reimplemented from NPbase.

Definition at line 922 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHWWRatio();
 }

◆ muTHUttHWW2l2v()

double SigmaBR::muTHUttHWW2l2v ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 952 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHWW2l2vRatio();
 }

◆ muTHUttHZga()

double SigmaBR::muTHUttHZga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 832 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHZgaRatio();
 }

◆ muTHUttHZZ()

double SigmaBR::muTHUttHZZ ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,ZZ}$

Reimplemented from NPbase.

Definition at line 862 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHZZRatio();
 }

◆ muTHUttHZZ4l()

double SigmaBR::muTHUttHZZ4l ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 892 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHZZ4lRatio();
 }

◆ muTHUVBFBRinv()

double SigmaBR::muTHUVBFBRinv ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF}BR_{inv}$

Reimplemented from NPbase.

Definition at line 1047 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*Br_H_inv();
 }

◆ muTHUVBFHbb()

double SigmaBR::muTHUVBFHbb ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,bb}$

Reimplemented from NPbase.

Definition at line 1022 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHbbRatio();
 }

◆ muTHUVBFHgaga()

double SigmaBR::muTHUVBFHgaga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 782 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHgagaRatio();
 }

◆ muTHUVBFHinv()

double SigmaBR::muTHUVBFHinv ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,inv}$

Reimplemented from NPbase.

Definition at line 1052 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHtoinvRatio();
 }

◆ muTHUVBFHmumu()

double SigmaBR::muTHUVBFHmumu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,\mu\mu}$

Reimplemented from NPbase.

Definition at line 962 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHmumuRatio();
 }

◆ muTHUVBFHtautau()

double SigmaBR::muTHUVBFHtautau ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,\tau\tau}$

Reimplemented from NPbase.

Definition at line 992 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHtautauRatio();
 }

◆ muTHUVBFHWW()

double SigmaBR::muTHUVBFHWW ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,WW}$

Reimplemented from NPbase.

Definition at line 902 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHWWRatio();
 }

◆ muTHUVBFHWW2l2v()

double SigmaBR::muTHUVBFHWW2l2v ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 932 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHWW2l2vRatio();
 }

◆ muTHUVBFHZga()

double SigmaBR::muTHUVBFHZga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,Z\gamma}$

Reimplemented from NPbase.

Definition at line 812 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHZgaRatio();
 }

◆ muTHUVBFHZZ()

double SigmaBR::muTHUVBFHZZ ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,ZZ}$

Reimplemented from NPbase.

Definition at line 842 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHZZRatio();
 }

◆ muTHUVBFHZZ4l()

double SigmaBR::muTHUVBFHZZ4l ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 872 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHZZ4lRatio();
 }

◆ muTHUVHbb()

double SigmaBR::muTHUVHbb ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,bb}$

Reimplemented from NPbase.

Definition at line 1037 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHbbRatio();
 }

◆ muTHUVHBRinv()

double SigmaBR::muTHUVHBRinv ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH}BR_{inv}$

Reimplemented from NPbase.

Definition at line 1057 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*Br_H_inv();
 }

◆ muTHUVHgaga()

double SigmaBR::muTHUVHgaga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 797 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHgagaRatio();
 }

◆ muTHUVHinv()

double SigmaBR::muTHUVHinv ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,inv}$

Reimplemented from NPbase.

Definition at line 1062 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHtoinvRatio();
 }

◆ muTHUVHmumu()

double SigmaBR::muTHUVHmumu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 977 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHmumuRatio();
 }

◆ muTHUVHtautau()

double SigmaBR::muTHUVHtautau ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 1007 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHtautauRatio();
 }

◆ muTHUVHWW()

double SigmaBR::muTHUVHWW ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,WW}$

Reimplemented from NPbase.

Definition at line 917 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHWWRatio();
 }

◆ muTHUVHWW2l2v()

double SigmaBR::muTHUVHWW2l2v ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 947 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHWW2l2vRatio();
 }

◆ muTHUVHZga()

double SigmaBR::muTHUVHZga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 827 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHZgaRatio();
 }

◆ muTHUVHZZ()

double SigmaBR::muTHUVHZZ ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,ZZ}$

Reimplemented from NPbase.

Definition at line 857 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHZZRatio();
 }

◆ muTHUVHZZ4l()

double SigmaBR::muTHUVHZZ4l ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 887 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHZZ4lRatio();
 }

◆ muTHUWHbb()

double SigmaBR::muTHUWHbb ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,bb}$

Reimplemented from NPbase.

Definition at line 1032 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHbbRatio();
 }

◆ muTHUWHgaga()

double SigmaBR::muTHUWHgaga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 792 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHgagaRatio();
 }

◆ muTHUWHmumu()

double SigmaBR::muTHUWHmumu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 972 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHmumuRatio();
 }

◆ muTHUWHtautau()

double SigmaBR::muTHUWHtautau ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 1002 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHtautauRatio();
 }

◆ muTHUWHWW()

double SigmaBR::muTHUWHWW ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,WW}$

Reimplemented from NPbase.

Definition at line 912 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHWWRatio();
 }

◆ muTHUWHWW2l2v()

double SigmaBR::muTHUWHWW2l2v ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 942 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHWW2l2vRatio();
 }

◆ muTHUWHZga()

double SigmaBR::muTHUWHZga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 822 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHZgaRatio();
 }

◆ muTHUWHZZ()

double SigmaBR::muTHUWHZZ ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,ZZ}$

Reimplemented from NPbase.

Definition at line 852 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHZZRatio();
 }

◆ muTHUWHZZ4l()

double SigmaBR::muTHUWHZZ4l ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 882 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHZZ4lRatio();
 }

◆ muTHUZHbb()

double SigmaBR::muTHUZHbb ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,bb}$

Reimplemented from NPbase.

Definition at line 1027 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHbbRatio();
 }

◆ muTHUZHgaga()

double SigmaBR::muTHUZHgaga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 787 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHgagaRatio();
 }

◆ muTHUZHmumu()

double SigmaBR::muTHUZHmumu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 967 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHmumuRatio();
 }

◆ muTHUZHtautau()

double SigmaBR::muTHUZHtautau ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 997 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHtautauRatio();
 }

◆ muTHUZHWW()

double SigmaBR::muTHUZHWW ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,WW}$

Reimplemented from NPbase.

Definition at line 907 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHWWRatio();
 }

◆ muTHUZHWW2l2v()

double SigmaBR::muTHUZHWW2l2v ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 937 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHWW2l2vRatio();
 }

◆ muTHUZHZga()

double SigmaBR::muTHUZHZga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 817 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHZgaRatio();
 }

◆ muTHUZHZZ()

double SigmaBR::muTHUZHZZ ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,ZZ}$

Reimplemented from NPbase.

Definition at line 847 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHZZRatio();
 }

◆ muTHUZHZZ4l()

double SigmaBR::muTHUZHZZ4l ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 877 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHZZ4lRatio();
 }

◆ muttH()

double SigmaBR::muttH ( const double sqrt_s ) const

virtual

The ratio $\mu_{ttH}$ between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH}$

Reimplemented from NPbase.

Definition at line 220 of file SigmaBR.cpp.

 {
     return tth;
 }

◆ muttHbb()

double SigmaBR::muttHbb ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,bb}$

Reimplemented from NPbase.

Definition at line 766 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHbbRatio();
 }

◆ muttHgaga()

double SigmaBR::muttHgaga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 526 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHgagaRatio();
 }

◆ muttHmumu()

double SigmaBR::muttHmumu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 706 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHmumuRatio();
 }

◆ muttHtautau()

double SigmaBR::muttHtautau ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 736 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHtautauRatio();
 }

◆ muttHWW()

double SigmaBR::muttHWW ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,WW}$

Reimplemented from NPbase.

Definition at line 646 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHWWRatio();
 }

◆ muttHWW2l2v()

double SigmaBR::muttHWW2l2v ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 676 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHWW2l2vRatio();
 }

◆ muttHZga()

double SigmaBR::muttHZga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 556 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHZgaRatio();
 }

◆ muttHZZ()

double SigmaBR::muttHZZ ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,ZZ}$

Reimplemented from NPbase.

Definition at line 586 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHZZRatio();
 }

◆ muttHZZ4l()

double SigmaBR::muttHZZ4l ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ttH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 616 of file SigmaBR.cpp.

 {
     return muttH(sqrt_s)*BrHZZ4lRatio();
 }

◆ muVBF()

double SigmaBR::muVBF ( const double sqrt_s ) const

virtual

The ratio $\mu_{VBF}$ between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF}$

Reimplemented from NPbase.

Definition at line 181 of file SigmaBR.cpp.

 {
     return vbf;
 }

◆ muVBFHbb()

double SigmaBR::muVBFHbb ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,bb}$

Reimplemented from NPbase.

Definition at line 746 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHbbRatio();
 }

◆ muVBFHgaga()

double SigmaBR::muVBFHgaga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 506 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHgagaRatio();
 }

◆ muVBFHmumu()

double SigmaBR::muVBFHmumu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,\mu\mu}$

Reimplemented from NPbase.

Definition at line 686 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHmumuRatio();
 }

◆ muVBFHtautau()

double SigmaBR::muVBFHtautau ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,\tau\tau}$

Reimplemented from NPbase.

Definition at line 716 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHtautauRatio();
 }

◆ muVBFHWW()

double SigmaBR::muVBFHWW ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,WW}$

Reimplemented from NPbase.

Definition at line 626 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHWWRatio();
 }

◆ muVBFHWW2l2v()

double SigmaBR::muVBFHWW2l2v ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 656 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHWW2l2vRatio();
 }

◆ muVBFHZga()

double SigmaBR::muVBFHZga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,Z\gamma}$

Reimplemented from NPbase.

Definition at line 536 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHZgaRatio();
 }

◆ muVBFHZZ()

double SigmaBR::muVBFHZZ ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,ZZ}$

Reimplemented from NPbase.

Definition at line 566 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHZZRatio();
 }

◆ muVBFHZZ4l()

double SigmaBR::muVBFHZZ4l ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 596 of file SigmaBR.cpp.

 {
     return muVBF(sqrt_s)*BrHZZ4lRatio();
 }

◆ muVBFpVH()

double SigmaBR::muVBFpVH ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VBF+VH}$

Reimplemented from NPbase.

Definition at line 207 of file SigmaBR.cpp.

 {
     double sigmaWH_SM = computeSigmaWH(sqrt_s);
     double sigmaZH_SM = computeSigmaZH(sqrt_s);
     double sigmaVBF_SM = computeSigmaVBF(sqrt_s);
     double sigmaWH = muWH(sqrt_s) * sigmaWH_SM;
     double sigmaZH = muZH(sqrt_s) * sigmaZH_SM;
     double sigmaVBF = muVBF(sqrt_s) * sigmaVBF_SM;
     double mu = ((sigmaWH + sigmaZH + sigmaVBF) / (sigmaWH_SM + sigmaZH_SM + sigmaVBF_SM));
         
     return mu;
 }

◆ muVH()

double SigmaBR::muVH ( const double sqrt_s ) const

virtual

The ratio $\mu_{VH}$ between the WH+ZH associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH}$

Reimplemented from NPbase.

Definition at line 196 of file SigmaBR.cpp.

 {
     double sigmaWH_SM = computeSigmaWH(sqrt_s);
     double sigmaZH_SM = computeSigmaZH(sqrt_s);
     double sigmaWH = muWH(sqrt_s) * sigmaWH_SM;
     double sigmaZH = muZH(sqrt_s) * sigmaZH_SM;
     double mu = ((sigmaWH + sigmaZH) / (sigmaWH_SM + sigmaZH_SM));
         
     return mu;
 }

◆ muVHbb()

double SigmaBR::muVHbb ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,bb}$

Reimplemented from NPbase.

Definition at line 761 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHbbRatio();
 }

◆ muVHgaga()

double SigmaBR::muVHgaga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 521 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHgagaRatio();
 }

◆ muVHmumu()

double SigmaBR::muVHmumu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 701 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHmumuRatio();
 }

◆ muVHtautau()

double SigmaBR::muVHtautau ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 731 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHtautauRatio();
 }

◆ muVHWW()

double SigmaBR::muVHWW ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,WW}$

Reimplemented from NPbase.

Definition at line 641 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHWWRatio();
 }

◆ muVHWW2l2v()

double SigmaBR::muVHWW2l2v ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 671 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHWW2l2vRatio();
 }

◆ muVHZga()

double SigmaBR::muVHZga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 551 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHZgaRatio();
 }

◆ muVHZZ()

double SigmaBR::muVHZZ ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,ZZ}$

Reimplemented from NPbase.

Definition at line 581 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHZZRatio();
 }

◆ muVHZZ4l()

double SigmaBR::muVHZZ4l ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{VH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 611 of file SigmaBR.cpp.

 {
     return muVH(sqrt_s)*BrHZZ4lRatio();
 }

◆ muWH()

double SigmaBR::muWH ( const double sqrt_s ) const

virtual

The ratio $\mu_{WH}$ between the W-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH}$

Reimplemented from NPbase.

Definition at line 186 of file SigmaBR.cpp.

 {
     return wh;
 }

◆ muWHbb()

double SigmaBR::muWHbb ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,bb}$

Reimplemented from NPbase.

Definition at line 756 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHbbRatio();
 }

◆ muWHgaga()

double SigmaBR::muWHgaga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 516 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHgagaRatio();
 }

◆ muWHmumu()

double SigmaBR::muWHmumu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 696 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHmumuRatio();
 }

◆ muWHtautau()

double SigmaBR::muWHtautau ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 726 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHtautauRatio();
 }

◆ muWHWW()

double SigmaBR::muWHWW ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,WW}$

Reimplemented from NPbase.

Definition at line 636 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHWWRatio();
 }

◆ muWHWW2l2v()

double SigmaBR::muWHWW2l2v ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 666 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHWW2l2vRatio();
 }

◆ muWHZga()

double SigmaBR::muWHZga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 546 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHZgaRatio();
 }

◆ muWHZZ()

double SigmaBR::muWHZZ ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,ZZ}$

Reimplemented from NPbase.

Definition at line 576 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHZZRatio();
 }

◆ muWHZZ4l()

double SigmaBR::muWHZZ4l ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{WH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 606 of file SigmaBR.cpp.

 {
     return muWH(sqrt_s)*BrHZZ4lRatio();
 }

◆ muZH()

double SigmaBR::muZH ( const double sqrt_s ) const

virtual

The ratio $\mu_{ZH}$ between the Z-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH}$

Reimplemented from NPbase.

Definition at line 191 of file SigmaBR.cpp.

 {
     return zh;
 }

◆ muZHbb()

double SigmaBR::muZHbb ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,bb}$

Reimplemented from NPbase.

Definition at line 751 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHbbRatio();
 }

◆ muZHgaga()

double SigmaBR::muZHgaga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,\gamma\gamma}$

Reimplemented from NPbase.

Definition at line 511 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHgagaRatio();
 }

◆ muZHmumu()

double SigmaBR::muZHmumu ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,\mu\mu}$

Reimplemented from NPbase.

Definition at line 691 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHmumuRatio();
 }

◆ muZHtautau()

double SigmaBR::muZHtautau ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,\tau\tau}$

Reimplemented from NPbase.

Definition at line 721 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHtautauRatio();
 }

◆ muZHWW()

double SigmaBR::muZHWW ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,WW}$

Reimplemented from NPbase.

Definition at line 631 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHWWRatio();
 }

◆ muZHWW2l2v()

double SigmaBR::muZHWW2l2v ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,WW\to 2l2\nu}$

Reimplemented from NPbase.

Definition at line 661 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHWW2l2vRatio();
 }

◆ muZHZga()

double SigmaBR::muZHZga ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,Z\gamma}$

Reimplemented from NPbase.

Definition at line 541 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHZgaRatio();
 }

◆ muZHZZ()

double SigmaBR::muZHZZ ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,ZZ}$

Reimplemented from NPbase.

Definition at line 571 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHZZRatio();
 }

◆ muZHZZ4l()

double SigmaBR::muZHZZ4l ( const double sqrt_s ) const

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.

Parameters

[in] sqrt_s the center-of-mass energy in TeV

Returns: $\mu_{ZH,ZZ\to 4l}$

Reimplemented from NPbase.

Definition at line 601 of file SigmaBR.cpp.

 {
     return muZH(sqrt_s)*BrHZZ4lRatio();
 }

◆ setParameter()

void SigmaBR::setParameter	(	const std::string	name,
		const double &	value
	)

protectedvirtual

A method to set the value of a parameter of the model.

Parameters

[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 68 of file SigmaBR.cpp.

 {
     if (name.compare("ggH") == 0)
         ggh = value;
     else if (name.compare("VBF") == 0)
         vbf = value;
     else if (name.compare("WH") == 0)
         wh = value;
     else if (name.compare("ZH") == 0)
         zh = value;
     else if (name.compare("ttH") == 0)
         tth = value;
     else if (name.compare("eeZH240") == 0)
         eeZH240 = value; 
     else if (name.compare("eeZH250") == 0)
         eeZH250 = value; 
     else if (name.compare("eeZH350") == 0)
         eeZH350 = value;     
     else if (name.compare("eeZH365") == 0)
         eeZH365 = value; 
     else if (name.compare("eeZH380") == 0)
         eeZH380 = value; 
     else if (name.compare("eeZH500") == 0)
         eeZH500 = value; 
     else if (name.compare("eeZH1000") == 0)
         eeZH1000 = value; 
     else if (name.compare("eeZH1500") == 0)
         eeZH1500 = value; 
     else if (name.compare("eeZH3000") == 0)
         eeZH3000 = value; 
     else if (name.compare("eeHvv240") == 0)
         eeHvv240 = value; 
     else if (name.compare("eeHvv250") == 0)
         eeHvv250 = value; 
     else if (name.compare("eeHvv350") == 0)
         eeHvv350 = value;     
     else if (name.compare("eeHvv365") == 0)
         eeHvv365 = value; 
     else if (name.compare("eeHvv380") == 0)
         eeHvv380 = value; 
     else if (name.compare("eeHvv500") == 0)
         eeHvv500 = value; 
     else if (name.compare("eeHvv1000") == 0)
         eeHvv1000 = value; 
     else if (name.compare("eeHvv1500") == 0)
         eeHvv1500 = value; 
     else if (name.compare("eeHvv3000") == 0)
         eeHvv3000 = value;
     else if (name.compare("eeHee240") == 0)
         eeHee240 = value; 
     else if (name.compare("eeHee250") == 0)
         eeHee250 = value; 
     else if (name.compare("eeHee350") == 0)
         eeHee350 = value;     
     else if (name.compare("eeHee365") == 0)
         eeHee365 = value; 
     else if (name.compare("eeHee380") == 0)
         eeHee380 = value; 
     else if (name.compare("eeHee500") == 0)
         eeHee500 = value; 
     else if (name.compare("eeHee1000") == 0)
         eeHee1000 = value; 
     else if (name.compare("eeHee1500") == 0)
         eeHee1500 = value; 
     else if (name.compare("eeHee3000") == 0)
         eeHee3000 = value;
     else if (name.compare("eettH500") == 0)
         eettH500 = value; 
     else if (name.compare("eettH1000") == 0)
         eettH1000 = value; 
     else if (name.compare("eettH1500") == 0)
         eettH1500 = value; 
     else if (name.compare("eettH3000") == 0)
         eettH3000 = value; 
     else if (name.compare("BrHggRatio") == 0)
         brhggratio = value;
     else if (name.compare("BrHWWRatio") == 0)
         brhwwratio = value;
     else if (name.compare("BrHZZRatio") == 0)
         brhzzratio = value;
     else if (name.compare("BrHZgaRatio") == 0)
         brhzgaratio = value;
     else if (name.compare("BrHgagaRatio") == 0)
         brhgagaratio = value;
     else if (name.compare("BrHtautauRatio") == 0)
         brhtautauratio = value;
     else if (name.compare("BrHmumuRatio") == 0)
         brhmumuratio = value;
     else if (name.compare("BrHccRatio") == 0)
         brhccratio = value;
     else if (name.compare("BrHbbRatio") == 0)
         brhbbratio = value;
     else
         NPbase::setParameter(name, value);
 }

Member Data Documentation

◆ brhbbratio

double SigmaBR::brhbbratio

protected

The ratio of the Hbb BR in the current model w.r.t. the SM.

Definition at line 1226 of file SigmaBR.h.

◆ brhccratio

double SigmaBR::brhccratio

protected

The ratio of the Hcc BR in the current model w.r.t. the SM.

Definition at line 1225 of file SigmaBR.h.

◆ brhgagaratio

double SigmaBR::brhgagaratio

protected

The ratio of the Hgaga BR in the current model w.r.t. the SM.

Definition at line 1222 of file SigmaBR.h.

◆ brhggratio

double SigmaBR::brhggratio

protected

The ratio of the Hgg BR in the current model w.r.t. the SM.

Definition at line 1218 of file SigmaBR.h.

◆ brhmumuratio

double SigmaBR::brhmumuratio

protected

The ratio of the Hmumu BR in the current model w.r.t. the SM.

Definition at line 1224 of file SigmaBR.h.

◆ brhtautauratio

double SigmaBR::brhtautauratio

protected

The ratio of the Htautau BR in the current model w.r.t. the SM.

Definition at line 1223 of file SigmaBR.h.

◆ brhwwratio

double SigmaBR::brhwwratio

protected

The ratio of the HWW BR in the current model w.r.t. the SM.

Definition at line 1219 of file SigmaBR.h.

◆ brhzgaratio

double SigmaBR::brhzgaratio

protected

The ratio of the HZga BR in the current model w.r.t. the SM.

Definition at line 1221 of file SigmaBR.h.

◆ brhzzratio

double SigmaBR::brhzzratio

protected

The ratio of the HZZ BR in the current model w.r.t. the SM.

Definition at line 1220 of file SigmaBR.h.

◆ eeHee1000

double SigmaBR::eeHee1000

protected

Definition at line 1216 of file SigmaBR.h.

◆ eeHee1500

double SigmaBR::eeHee1500

protected

Definition at line 1216 of file SigmaBR.h.

◆ eeHee240

double SigmaBR::eeHee240

protected

Definition at line 1216 of file SigmaBR.h.

◆ eeHee250

double SigmaBR::eeHee250

protected

Definition at line 1216 of file SigmaBR.h.

◆ eeHee3000

double SigmaBR::eeHee3000

protected

The eeHee cross section.

Definition at line 1216 of file SigmaBR.h.

◆ eeHee350

double SigmaBR::eeHee350

protected

Definition at line 1216 of file SigmaBR.h.

◆ eeHee365

double SigmaBR::eeHee365

protected

Definition at line 1216 of file SigmaBR.h.

◆ eeHee380

double SigmaBR::eeHee380

protected

Definition at line 1216 of file SigmaBR.h.

◆ eeHee500

double SigmaBR::eeHee500

protected

Definition at line 1216 of file SigmaBR.h.

◆ eeHvv1000

double SigmaBR::eeHvv1000

protected

Definition at line 1215 of file SigmaBR.h.

◆ eeHvv1500

double SigmaBR::eeHvv1500

protected

Definition at line 1215 of file SigmaBR.h.

◆ eeHvv240

double SigmaBR::eeHvv240

protected

Definition at line 1215 of file SigmaBR.h.

◆ eeHvv250

double SigmaBR::eeHvv250

protected

Definition at line 1215 of file SigmaBR.h.

◆ eeHvv3000

double SigmaBR::eeHvv3000

protected

The eeHvv cross section.

Definition at line 1215 of file SigmaBR.h.

◆ eeHvv350

double SigmaBR::eeHvv350

protected

Definition at line 1215 of file SigmaBR.h.

◆ eeHvv365

double SigmaBR::eeHvv365

protected

Definition at line 1215 of file SigmaBR.h.

◆ eeHvv380

double SigmaBR::eeHvv380

protected

Definition at line 1215 of file SigmaBR.h.

◆ eeHvv500

double SigmaBR::eeHvv500

protected

Definition at line 1215 of file SigmaBR.h.

◆ eettH1000

double SigmaBR::eettH1000

protected

Definition at line 1217 of file SigmaBR.h.

◆ eettH1500

double SigmaBR::eettH1500

protected

Definition at line 1217 of file SigmaBR.h.

◆ eettH3000

double SigmaBR::eettH3000

protected

The eettH cross section.

Definition at line 1217 of file SigmaBR.h.

◆ eettH500

double SigmaBR::eettH500

protected

Definition at line 1217 of file SigmaBR.h.

◆ eeZH1000

double SigmaBR::eeZH1000

protected

Definition at line 1214 of file SigmaBR.h.

◆ eeZH1500

double SigmaBR::eeZH1500

protected

Definition at line 1214 of file SigmaBR.h.

◆ eeZH240

double SigmaBR::eeZH240

protected

Definition at line 1214 of file SigmaBR.h.

◆ eeZH250

double SigmaBR::eeZH250

protected

Definition at line 1214 of file SigmaBR.h.

◆ eeZH3000

double SigmaBR::eeZH3000

protected

The eeZH cross section.

Definition at line 1214 of file SigmaBR.h.

◆ eeZH350

double SigmaBR::eeZH350

protected

Definition at line 1214 of file SigmaBR.h.

◆ eeZH365

double SigmaBR::eeZH365

protected

Definition at line 1214 of file SigmaBR.h.

◆ eeZH380

double SigmaBR::eeZH380

protected

Definition at line 1214 of file SigmaBR.h.

◆ eeZH500

double SigmaBR::eeZH500

protected

Definition at line 1214 of file SigmaBR.h.

◆ ggh

double SigmaBR::ggh

protected

The ggH cross section.

Definition at line 1209 of file SigmaBR.h.

◆ NSigmaBRVars

const int SigmaBR::NSigmaBRVars = 45

static

The number of the model parameters in SigmaBR.

Definition at line 20 of file SigmaBR.h.

◆ SigmaBRVars

const std::string SigmaBR::SigmaBRVars

static

Initial value:

= {"ggH", "VBF", "WH", "ZH", "ttH", 
        "eeZH240","eeZH250","eeZH350","eeZH365","eeZH380","eeZH500","eeZH1000","eeZH1500","eeZH3000",
        "eeHvv240","eeHvv250","eeHvv350","eeHvv365","eeHvv380","eeHvv500","eeHvv1000","eeHvv1500","eeHvv3000",
        "eeHee240","eeHee250","eeHee350","eeHee365","eeHee380","eeHee500","eeHee1000","eeHee1500","eeHee3000",
        "eettH500","eettH1000","eettH1500","eettH3000",
        "BrHggRatio", "BrHWWRatio", "BrHZZRatio","BrHZgaRatio", "BrHgagaRatio", "BrHtautauRatio", "BrHmumuRatio", "BrHccRatio", "BrHbbRatio"}

A string array containing the labels of the model parameters in NPEffectiveGIMR.

Definition at line 26 of file SigmaBR.h.

◆ tth

double SigmaBR::tth

protected

The ttH cross section.

Definition at line 1213 of file SigmaBR.h.

◆ vbf

double SigmaBR::vbf

protected

The VBF cross section.

Definition at line 1210 of file SigmaBR.h.

◆ wh

double SigmaBR::wh

protected

The WH cross section.

Definition at line 1211 of file SigmaBR.h.

◆ zh

double SigmaBR::zh

protected

The ZH cross section.

Definition at line 1212 of file SigmaBR.h.

The documentation for this class was generated from the following files:

Detailed Description

Public Member Functions

Static Public Attributes

Protected Member Functions

Protected Attributes

Additional Inherited Members

Constructor & Destructor Documentation

◆ SigmaBR()

Member Function Documentation

◆ BrHbbRatio()

◆ BrHccRatio()

◆ BrHgagaRatio()

◆ BrHggRatio()

◆ BrHmumuRatio()

◆ BrHtautauRatio()

◆ BrHWW2l2vRatio()

◆ BrHWWRatio()

◆ BrHZgaeeRatio()

◆ BrHZgallRatio()

◆ BrHZgamumuRatio()

◆ BrHZgaRatio()

◆ BrHZZ2e2muRatio()

◆ BrHZZ4eRatio()

◆ BrHZZ4lRatio()

◆ BrHZZ4muRatio()

◆ BrHZZRatio()

◆ CheckParameters()

◆ mueeHvv()

◆ mueeHvvPol()

◆ mueettH()

◆ mueettHPol()

◆ mueeZBF()

◆ mueeZBFPol()

◆ mueeZH()

◆ mueeZHPol()

◆ muggH()

◆ muggHbb()

◆ muggHgaga()

◆ muggHmumu()

◆ muggHpttH()

◆ muggHtautau()

◆ muggHWW()

◆ muggHWW2l2v()

◆ muggHZga()

◆ muggHZZ()

◆ muggHZZ4l()

◆ muTHUggHbb()

◆ muTHUggHgaga()

◆ muTHUggHmumu()

◆ muTHUggHtautau()

◆ muTHUggHWW()

◆ muTHUggHWW2l2v()

◆ muTHUggHZga()

◆ muTHUggHZgamumu()

◆ muTHUggHZZ()

◆ muTHUggHZZ4l()

◆ muTHUggHZZ4mu()

◆ muTHUttHbb()

◆ muTHUttHgaga()

◆ muTHUttHmumu()

◆ muTHUttHtautau()

◆ muTHUttHWW()

◆ muTHUttHWW2l2v()

◆ muTHUttHZga()

◆ muTHUttHZZ()

◆ muTHUttHZZ4l()

◆ muTHUVBFBRinv()

◆ muTHUVBFHbb()

◆ muTHUVBFHgaga()

◆ muTHUVBFHinv()

◆ muTHUVBFHmumu()

◆ muTHUVBFHtautau()

◆ muTHUVBFHWW()

◆ muTHUVBFHWW2l2v()

◆ muTHUVBFHZga()

◆ muTHUVBFHZZ()

◆ muTHUVBFHZZ4l()

◆ muTHUVHbb()

◆ muTHUVHBRinv()

◆ muTHUVHgaga()