NPEffectiveGIMR Class Reference

A model class for new physics in the form of the dimension-six effective Lagrangian. More...

#include <NPEffectiveGIMR.h>

Inheritance diagram for NPEffectiveGIMR:

Collaboration diagram for NPEffectiveGIMR:

Detailed Description

A model class for new physics in the form of the dimension-six effective Lagrangian.

Author

HEPfit Collaboration

Copyright

GNU General Public License

This is a Model class containing parameters and functions associated with the general dimension-six effective Lagrangian. (Use the model name "NPEffectiveGIMR_LFU_QFU" to asumme lepton and quark flavour universality)

In this class we consider the dimension-six effective Lagrangian

\[ \mathcal{L}_\mathrm{eff} = \mathcal{L}_\mathrm{SM} + \sum_i \frac{C_i}{\Lambda^2} \mathcal{O}_i \]

as written in the basis of [84].

Initialization

After creating an instance of the current class with the constructor NPEffectiveGIMR(), it is required to call the initialization method InitializeModel(). In the Monte Carlo run, the constructor as well as the initialization method are called in InputParser::ReadParameters().

Model parameters

The model parameters of NPEffectiveGIMR are summarized below:

Label	LaTeX symbol	Description
CHG	\(C_{HG} \)	The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\).
CHW	\(C_{HW} \)	The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\).
CHB	\(C_{HB} \)	The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\).
CWB	\(C_{WB} \)	The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\tau^a H\big)W_{\mu\nu}^a B^{\mu\nu}\).
CHD	\(C_{HD}\)	The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\).
CHbox	\(C_{H\Box}\)	The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\).
CH	\(C_{H}\)	The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\).
CHL1_kk, CHL1_klr, CHL1_kli	\( (C_{HL}^{(1)})_{kk}, \mbox{Re}\big[(C_{HL}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(1)})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^j\big)\), for \(i,j=1,2,3\).
CHL3_kk, CHL3_klr, CHL3_kli	\( (C_{HL}^{(3)})_{kk}, \mbox{Re}\big[(C_{HL}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(3)})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \tau^a L^j\big)\), for \(i,j=1,2,3\).
CHe_kk, CHe_klr, CHe_kli	\( (C_{HE})_{kk}, \mbox{Re}\big[(C_{HE})_{kl}\big], \mbox{Im}\big[(C_{HE})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HE})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^j\big)\), for \(i,j=1,2,3\).
CHQ1_kk, CHQ1_klr, CHQ1_kli	\( (C_{HQ}^{(1)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(1)})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^j\big)\), for \(i,j=1,2,3\).
CHQ3_kk, CHQ3_klr, CHQ3_kli	\( (C_{HQ}^{(3)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(3)})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \tau^a Q^j\big)\), for \(i,j=1,2,3\).
CHu_kk, CHu_klr, CHu_kli	\( (C_{HU})_{kk}, \mbox{Re}\big[(C_{HU})_{kl}\big], \mbox{Im}\big[(C_{HU})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HU})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^j\big)\), for \(i,j=1,2,3\).
CHd_kk, CHd_klr, CHd_kli	\( (C_{HD})_{kk}, \mbox{Re}\big[(C_{HD})_{kl}\big], \mbox{Im}\big[(C_{HD})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HD})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\).
CHud_klr, CHud_kli	\(\mbox{Re}\big[(C_{HUD})_{kl}\big], \mbox{Im}\big[(C_{HUD})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HUD})_{ij} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\).
CeH_klr, CeH_kli	\(\mbox{Re}\big[(C_{EH})_{kl}\big], \mbox{Im}\big[(C_{EH})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{EH})_{ij} =\big(H^\dagger H\big) \big(\overline{L^i}\,H E^j\big)\), for \(i,j=1,2,3\).
CuH_klr, CuH_kli	\(\mbox{Re}\big[(C_{UH})_{kl}\big], \mbox{Im}\big[(C_{UH})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{UH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,\widetilde{H} U^j\big)\), for \(i,j=1,2,3\).
CdH_klr, CdH_kli	\(\mbox{Re}\big[(C_{DH})_{kl}\big], \mbox{Im}\big[(C_{DH})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{DH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,H D^j\big)\), for \(i,j=1,2,3\).
CLL_1221, CLL_2112	\((C_{LL})_{1221,2112}\)	The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\).
Lambda_NP	\(\Lambda \)	The new physics scale.
eVBFE_i	\(\varepsilon_{VBF}^i(E)\)	The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the VBF production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HAA}, g_{HWW}^{(1,2,3)}, g_{Hgg}, g_{HZuu,HZdd}^{L,R}, g_{HWud}^{L}, g_{Zuu,Zdd}^{L,R}, g_{Wud}^{L})\)
eWHE_i	\(\varepsilon_{WH}^i(E)\)	The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the WH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{HWW}^{(1,2,3)}, g_{HWud}^{L}, g_{Wud}^{L})\)
eZHE_i	\(\varepsilon_{ZH}^i(E)\)	The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ZH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HZuu,HZdd}^{L,R}, g_{Zuu,Zdd}^{L,R})\)
ettHE_i	\(\varepsilon_{ttH}^i(E)\)	The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ttH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{Htt}, g_{Hgg})\)

Where the hermitian derivatives are defined as

\[ H^\dagger i \overset{\leftrightarrow}{D}_\mu H\equiv H^\dagger i(D_\mu - \overset{\leftarrow}{D}_\mu)H \]

and

\[ H^\dagger i \overset{\leftrightarrow}{D^a_\mu} H\equiv H^\dagger i (\tau^a D_\mu - \overset{\leftarrow}{D}_\mu \tau^a)H. \]

Alternatively, when using the model name "NPEffectiveGIMR_LFU_QFU", where lepton and quark flavour universality are assumed, the parameters to be used as inputs for the dimension six coefficients are the following:

Label	LaTeX symbol	Description
CHG	\(C_{HG} \)	The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\).
CHW	\(C_{HW} \)	The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\).
CHB	\(C_{HB} \)	The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\).
CWB	\(C_{WB} \)	The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\tau^a H\big)W_{\mu\nu}^a B^{\mu\nu}\).
CHD	\(C_{HD}\)	The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\).
CHbox	\(C_{H\Box}\)	The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\).
CH	\(C_{H}\)	The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\).
CHL1	\( (C_{HL}^{(1)})_{ii} \)	The coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^i\big)\) (flavor universal).
CHL3	\( (C_{HL}^{(3)})_{ii} \)	The coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \tau^a L^i\big)\) (flavor universal).
CHe	\( (C_{HE})_{ii} \)	The coefficient of the operator \(({\cal O}_{HE})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^i\big)\) (flavor universal).
CHQ1	\( (C_{HQ}^{(1)})_{ii} \)	The coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^i\big)\) (flavor universal).
CHQ3	\( (C_{HQ}^{(3)})_{ii}\)	The coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \tau^a Q^i\big)\) (flavor universal).
CHu	\( (C_{HU})_{ii} \)	The coefficient of the operator \(({\cal O}_{HU})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^i\big)\) (flavor universal).
CHd	\( (C_{HD})_{ii} \)	The coefficient of the operator \(({\cal O}_{HD})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^i\big)\) (flavor universal).
CHud_r, CHud_i	\(\mbox{Re}\big[(C_{HUD})_{ii}\big], \mbox{Im}\big[(C_{HUD})_{ii}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HUD})_{ii} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^i\big)\) (flavor universal).
CeH_r, CeH_i	\(\mbox{Re}\big[(C_{EH})_{ii}\big], \mbox{Im}\big[(C_{EH})_{ii}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{EH})_{ii} =\big(H^\dagger H\big) \big(\overline{L^i}\,H E^i\big)\) (flavor universal).
CuH_r, CuH_i	\(\mbox{Re}\big[(C_{UH})_{ii}\big], \mbox{Im}\big[(C_{UH})_{ii}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{UH})_{ii} =\big(H^\dagger H\big) \big(\overline{Q^i}\,\widetilde{H} U^i\big)\) (flavor universal).
CdH_r, CdH_i	\(\mbox{Re}\big[(C_{DH})_{ii}\big], \mbox{Im}\big[(C_{DH})_{ii}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{DH})_{ii} =\big(H^\dagger H\big) \big(\overline{Q^i}\,H D^i\big)\) (flavor universal).
CLL	\((C_{LL})_{1221,2112}\)	The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\).
Lambda_NP	\(\Lambda \)	The new physics scale.

(The parameters associated to the theoretical uncertainties, \(\varepsilon_{X}^i(E)\), are the same for both "NPEffectiveGIMR" and "NPEffectiveGIMR_LFU_QFU".)

Finally, if the flag MwInput (see below) is set to TRUE, one must also specify the input value for the W mass via the following parameter (Warning: The W width is not implemented in this case):

Label	LaTeX symbol	Description
MwInput	\(M_{W} \)	The input value for the W mass in GeV.

Model flags

The Flags of NPEffectiveGIMR are summarized below:

Label	Value	Description
MwInput	TRUE / FALSE	This flag is set to TRUE if the W mass is taken as an input parameter. (Warning: The W width is not implemented in this case.) The default value is FALSE.
QuadraticTerms	TRUE / FALSE	This flag is set to TRUE if the quadratic terms in Higgs cross sections and widths are switched on. The default value is FALSE; new physics contributions are linearized.

Important member functions

See the base classes of the current class.

Definition at line 423 of file NPEffectiveGIMR.h.

Public Member Functions
gslpp::complex	AH_f (const double tau) const
	Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More...
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	BrHtautauRatio () const
	The ratio of the Br \((H\to \tau^+\tau^-)\) 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	BrHZgaRatio () const
	The ratio of the Br \((H\to Z\gamma)\) 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	computeGammaTotalRatio () const
	The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More...
double	deltaG1_hWW () const
	The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More...
double	deltaG1_hZA () const
	The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More...
double	deltaG1_hZZ () const
	The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More...
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...
double	deltaG2_hZA () const
	The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More...
double	deltaG2_hZZ () const
	The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More...
double	deltaG3_hWW () const
	The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More...
double	deltaG3_hZZ () const
	The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More...
double	deltaG_hAA () const
	The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More...
gslpp::complex	deltaG_hff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More...
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	deltaGA_f (const Particle p) const
	New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More...
double	deltaGammaHbbRatio1 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
double	deltaGammaHbbRatio2 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
double	deltaGammaHccRatio1 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
double	deltaGammaHccRatio2 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
double	deltaGammaHgagaRatio1 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
double	deltaGammaHgagaRatio2 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
double	deltaGammaHggRatio1 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...
double	deltaGammaHggRatio2 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
double	deltaGammaHtautauRatio1 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
double	deltaGammaHtautauRatio2 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
double	deltaGammaHWWRatio1 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
double	deltaGammaHWWRatio2 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
double	deltaGammaHZgaRatio1 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
double	deltaGammaHZgaRatio2 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
double	deltaGammaHZZRatio1 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
double	deltaGammaHZZRatio2 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
virtual double	deltaGammaTotalRatio1 () const
	The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...
virtual double	deltaGammaTotalRatio2 () const
	The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients. More...
virtual double	DeltaGF () const
	New physics contribution to the Fermi constant. More...
double	deltaGL_f (const Particle p) const
	New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More...
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...
gslpp::complex	deltaGL_Wffh (const Particle pbar, const Particle p) const
	The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\). More...
double	deltaGL_Zffh (const Particle p) const
	The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\). More...
double	deltaGR_f (const Particle p) const
	New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More...
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...
gslpp::complex	deltaGR_Wffh (const Particle pbar, const Particle p) const
	The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\). More...
double	deltaGR_Zffh (const Particle p) const
	The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\). More...
virtual double	deltaGV_f (const Particle p) const
	New physics contribution to the neutral-current vector coupling \(g_V^f\). More...
gslpp::complex	f_triangle (const double tau) const
	Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More...
double	GammaHbbRatio () const
	The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. More...
double	GammaHccRatio () const
	The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. More...
double	GammaHgagaRatio () const
	The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. More...
double	GammaHggRatio () const
	The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. More...
double	GammaHtautauRatio () const
	The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. More...
double	GammaHWWRatio () const
	The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. More...
double	GammaHZgaRatio () const
	The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. More...
double	GammaHZZRatio () const
	The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. More...
virtual double	GammaW () const
	The total width of the \(W\) boson, \(\Gamma_W\). 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	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	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	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	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	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	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	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	Mw () const
	The mass of the \(W\) boson, \(M_W\). More...
	NPEffectiveGIMR (const bool FlagLeptonUniversal_in=false, const bool FlagQuarkUniversal_in=false)
	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 bool	PostUpdate ()
	The post-update method for NPEffectiveGIMR. More...
virtual bool	setFlag (const std::string name, const bool value)
	A method to set a flag of NPEffectiveGIMR. More...
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	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	deltaGamma_Z () const
	The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\). More...
virtual double	deltaR0_f (const Particle f) const
	The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\) or \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\), for leptons or quarks, respectively. 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 leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. 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_Z () const
	The total decay width of the \(Z\) boson, \(\Gamma_Z\). 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 gslpp::complex	kappaZ_f (const Particle f) const
	The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions. More...
	NPbase ()
	The default constructor. More...
virtual double	R0_f (const Particle f) const
	The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\) or \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\), for leptons or quarks, respectively. 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...
Public Member Functions inherited from StandardModel
double	ale_OS (const double mu, orders order=FULLNLO) const
	The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell schem. 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	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	computeAlpha () const
	The CKM angle \(\alpha\). More...
double	computeBeta () const
	The CKM angle \(\beta\). More...
double	computeBetas () const
	The CKM angle \(\beta_s\). 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	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...
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	computeGamma () const
	The CKM angle \(\gamma\). 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. [89]. More...
gslpp::complex	computelamc () const
	The product of the CKM elements \(V_{cd} V_{cs}^*\). More...
gslpp::complex	computelamc_d () const
	The product of the CKM elements \(V_{cd} V_{cb}^*\). More...
gslpp::complex	computelamc_s () const
	The product of the CKM elements \(V_{cs} V_{cb}^*\). More...
gslpp::complex	computelamt () const
	The product of the CKM elements \(V_{td} V_{ts}^*\). More...
gslpp::complex	computelamt_d () const
	The product of the CKM elements \(V_{td} V_{tb}^*\). More...
gslpp::complex	computelamt_s () const
	The product of the CKM elements \(V_{ts} V_{tb}^*\). More...
gslpp::complex	computelamu () const
	The product of the CKM elements \(V_{ud} V_{us}^*\). More...
gslpp::complex	computelamu_d () const
	The product of the CKM elements \(V_{ud} V_{ub}^*\). More...
gslpp::complex	computelamu_s () const
	The product of the CKM elements \(V_{us} V_{ub}^*\). More...
double	computeRb () const
	\(R_b=|(V_{ud}V_{ub}^*)/(V_{ud}V_{ub}^*)|\). More...
double	computeRt () const
	\(R_t=|(V_{td} V_{tb}^*)/(V_{cd}V_{cb}^*)|\). More...
double	computeRts () const
	\(R_{ts}=|(V_{ts}V_{tb}^*)/(V_{cs}V_{cb}^*)|\). 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 double Mw_i) const
	The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as \(c_W^2\). More...
virtual double	cW2 () const
double	DeltaAlpha () const
	The total corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha(M_Z^2)\). More...
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_had () const
	The hadronic decay width of the \(Z\) boson, \(\Gamma_{h}\). More...
virtual double	Gamma_inv () const
	The invisible partial decay width of the \(Z\) boson, \(\Gamma_{\mathrm{inv}}\). 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 double	GammaZ (const Particle f) const
	The \(Z\to \ell\bar{\ell}\) partial decay width, \(\Gamma_\ell\). More...
double	getA () const
	A get method to retrieve the CKM element \(A\). 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...
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	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	getDeltaMK () const
double	getDmk () const
double	getEpsK () const
double	getEtab () const
	A get method to retrieve the CKM element \(\bar{\eta}\). 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...
double	getGF () const
	A get method to retrieve the Fermi constant \(G_\mu\). More...
int	getIterationNo () const
double	getKbarEpsK () const
double	getLambda () const
	A get method to retrieve the CKM element \(\lambda\). More...
Particle	getLeptons (const StandardModel::lepton p) const
	A get method to retrieve the member object of a lepton. More...
double	getMHl () const
	A get method to retrieve the Higgs mass \(m_h\). More...
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...
Flavour *	getMyFlavour () const
LeptonFlavour *	getMyLeptonFlavour () const
virtual StandardModelMatching *	getMyMatching () const
	A get method to access the member pointer of type StandardModelMatching. More...
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...
double	getphiEpsK () const
double	getRhob () const
	A get method to retrieve the CKM element \(\bar{\rho}\). More...
double	getSM_M12D () const
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	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...
void	setFlagCacheInStandardModel (bool FlagCacheInStandardModel)
	A set method to change the model flag CacheInStandardModel of StandardModel. More...
void	setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ)
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...
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...
double	sW2 () const
virtual bool	Update (const std::map< std::string, double > &DPars)
	The update method for StandardModel. More...
virtual double	v () const
	The Higgs vacuum expectation value. \[ v = \left(\frac{1}{\sqrt{2} G_\mu}\right)^{1/2}, \] where \(G_\mu\) is the Fermi constant, measured through muon decays. 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...
double	Als (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	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...
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	geta_0A0 () const
double	geta_0A0phi () const
double	geta_0A1 () const
double	geta_0A12 () const
double	geta_0A12phi () const
double	geta_0A1phi () const
double	geta_0T1 () const
double	geta_0T1phi () const
double	geta_0T2 () const
double	geta_0T23 () const
double	geta_0T23phi () const
double	geta_0T2phi () const
double	geta_0V () const
double	geta_0Vphi () const
double	geta_1A0 () const
double	geta_1A0phi () const
double	geta_1A1 () const
double	geta_1A12 () const
double	geta_1A12phi () const
double	geta_1A1phi () const
double	geta_1T1 () const
double	geta_1T1phi () const
double	geta_1T2 () const
double	geta_1T23 () const
double	geta_1T23phi () const
double	geta_1T2phi () const
double	geta_1V () const
double	geta_1Vphi () const
double	geta_2A0 () const
double	geta_2A0phi () const
double	geta_2A1 () const
double	geta_2A12 () const
double	geta_2A12phi () const
double	geta_2A1phi () const
double	geta_2T1 () const
double	geta_2T1phi () const
double	geta_2T2 () const
double	geta_2T23 () const
double	geta_2T23phi () const
double	geta_2T2phi () const
double	geta_2V () const
double	geta_2Vphi () const
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	getBLNPcorr () const
double	getBr_B_Xcenu () const
double	getBr_Kp_munu () const
double	getBr_Kp_P0enu () const
double	getbsgamma_E0 () const
double	getCF () const
	A get method to access the Casimir factor of QCD. More...
double	getDeltaP_cu () const
double	getFKstarp () const
double	getGambino_BRsem () const
double	getGambino_Mbkin () const
double	getGambino_Mcatmuc () const
double	getGambino_muG2 () const
double	getGambino_mukin () const
double	getGambino_mupi2 () const
double	getGambino_rhoD3 () const
double	getGambino_rhoLS3 () const
gslpp::complex	geth_0 () const
gslpp::complex	geth_0_1 () const
gslpp::complex	geth_0_1_MP () const
gslpp::complex	geth_0_2 () const
gslpp::complex	geth_0_MP () const
gslpp::complex	geth_m () const
gslpp::complex	geth_m_1 () const
gslpp::complex	geth_m_2 () const
gslpp::complex	geth_p () const
gslpp::complex	geth_p_1 () const
gslpp::complex	geth_p_2 () const
double	getIB_Kl () const
double	getIB_Kp () const
double	getm_fit2_f0 () const
double	getm_fit2_fplus () const
double	getm_fit2_fT () const
double	getMAls () const
	A get method to access the mass scale \(M_{\alpha_s}\) at which the strong coupling constant measurement is provided. More...
Meson	getMesons (const meson m) const
	A get method to access a meson as an object of the type Meson. More...
double	getMRA0 () const
double	getMRA0phi () const
double	getMRA1 () const
double	getMRA12 () const
double	getMRA12phi () const
double	getMRA1phi () const
double	getMRT1 () const
double	getMRT1phi () const
double	getMRT2 () const
double	getMRT23 () const
double	getMRT23phi () const
double	getMRT2phi () const
double	getMRV () const
double	getMRVphi () const
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	getOmega_eta_etap () const
Particle	getQuarks (const quark q) const
	A get method to access a quark as an object of the type Particle. More...
double	getr_1_fplus () const
double	getr_1_fT () const
double	getr_2_f0 () const
double	getr_2_fplus () const
double	getr_2_fT () const
double	getReA0_Kd () const
double	getReA2_Kd () const
double	logLambda (const double nf, orders order) const
	Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More...
double	Nf (const double mu) const
	The number of active flavour at scale \(\mu\). 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...
double	Thresholds (const int i) const
	For accessing the active flavour threshold scales. More...
Public Member Functions inherited from Model
const double &	getModelParam (std::string name) const
bool	IsModelInitialized () const
	A method to check if the model is initialized. More...
bool	isModelParam (std::string name) const
bool	isModelSUSY () const
bool	isModelTHDM () const
bool	IsUpdateError () const
	A method to check if there was any error in the model update process. More...
	Model ()
	The default constructor. More...
std::string	ModelName () const
	A method to fetch the name of the model. More...
void	setModelInitialized (bool ModelInitialized)
	A set method to fix the failure or success of the initialization of the model. More...
void	setModelName (const std::string name)
	A method to set the name of the model. More...
void	setModelSUSY ()
void	setModelTHDM ()
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	NNPEffectiveGIMRVars = 200
	The number of the model parameters in NPEffectiveGIMR. More...
static const int	NNPEffectiveGIMRVars_LFU_QFU = 104
	The number of the model parameters in NPEffectiveGIMR with lepton and quark flavour universalities. More...
static const std::string	NPEffectiveGIMRVars [NNPEffectiveGIMRVars]
	A string array containing the labels of the model parameters in NPEffectiveGIMR. More...
static const std::string	NPEffectiveGIMRVars_LFU_QFU [NNPEffectiveGIMRVars_LFU_QFU]
	A string array containing the labels of the model parameters in NPEffectiveGIMR with lepton and quark flavour universalities. 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 = 27
	The number of the SM parameters that are relevant to the EW precision observables. More...
static const 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 = 186
	The number of model parameters in QCD. More...
static const 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
gslpp::complex	CfH_diag (const Particle f) const
	The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f. More...
double	CHF1_diag (const Particle F) const
	The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F. More...
double	CHF3_diag (const Particle F) const
	The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F. More...
double	CHf_diag (const Particle f) const
	The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f. More...
gslpp::complex	CHud_diag (const Particle u) const
	The diagonal entry of the dimension-6 operator coefficient \(C_{HUD}\) corresponding to particle f. More...
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
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	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	taub () const
	Top-mass corrections to the \(Zb\bar{b}\) vertex, denoted by \(\tau_b\). More...

Protected Attributes
double	CdH_11i
	The dimension-6 operator coefficient \((C_{DH})_{11}\) (imaginary part). More...
double	CdH_11r
	The dimension-6 operator coefficient \((C_{DH})_{11}\) (real part). More...
double	CdH_12i
	The dimension-6 operator coefficient \((C_{DH})_{12}\) (imaginary part). More...
double	CdH_12r
	The dimension-6 operator coefficient \((C_{DH})_{12}\) (real part). More...
double	CdH_13i
	The dimension-6 operator coefficient \((C_{DH})_{13}\) (imaginary part). More...
double	CdH_13r
	The dimension-6 operator coefficient \((C_{DH})_{13}\) (real part). More...
double	CdH_22i
	The dimension-6 operator coefficient \((C_{DH})_{22}\) (imaginary part). More...
double	CdH_22r
	The dimension-6 operator coefficient \((C_{DH})_{22}\) (real part). More...
double	CdH_23i
	The dimension-6 operator coefficient \((C_{DH})_{23}\) (imaginary part). More...
double	CdH_23r
	The dimension-6 operator coefficient \((C_{DH})_{23}\) (real part). More...
double	CdH_33i
	The dimension-6 operator coefficient \((C_{DH})_{33}\) (imaginary part). More...
double	CdH_33r
	The dimension-6 operator coefficient \((C_{DH})_{33}\) (real part). More...
double	CeH_11i
	The dimension-6 operator coefficient \((C_{EH})_{11}\) (imaginary part). More...
double	CeH_11r
	The dimension-6 operator coefficient \((C_{EH})_{11}\) (real part). More...
double	CeH_12i
	The dimension-6 operator coefficient \((C_{EH})_{12}\) (imaginary part). More...
double	CeH_12r
	The dimension-6 operator coefficient \((C_{EH})_{12}\) (real part). More...
double	CeH_13i
	The dimension-6 operator coefficient \((C_{EH})_{13}\) (imaginary part). More...
double	CeH_13r
	The dimension-6 operator coefficient \((C_{EH})_{13}\) (real part). More...
double	CeH_22i
	The dimension-6 operator coefficient \((C_{EH})_{22}\) (imaginary part). More...
double	CeH_22r
	The dimension-6 operator coefficient \((C_{EH})_{22}\) (real part). More...
double	CeH_23i
	The dimension-6 operator coefficient \((C_{EH})_{23}\) (imaginary part). More...
double	CeH_23r
	The dimension-6 operator coefficient \((C_{EH})_{23}\) (real part). More...
double	CeH_33i
	The dimension-6 operator coefficient \((C_{EH})_{33}\) (imaginary part). More...
double	CeH_33r
	The dimension-6 operator coefficient \((C_{EH})_{33}\) (real part). More...
double	CH
	The dimension-6 operator coefficient \(C_{H}\). More...
double	CHB
	The dimension-6 operator coefficient \(C_{HB}\). More...
double	CHbox
	The dimension-6 operator coefficient \(C_{H\Box}\). More...
double	CHD
	The dimension-6 operator coefficient \(C_{HD}\). More...
double	CHd_11
	The dimension-6 operator coefficient \((C_{HD})_{11}\). More...
double	CHd_12i
	The dimension-6 operator coefficient \((C_{HD})_{12}\) (imaginary part). More...
double	CHd_12r
	The dimension-6 operator coefficient \((C_{HD})_{12}\) (real part). More...
double	CHd_13i
	The dimension-6 operator coefficient \((C_{HD})_{13}\) (imaginary part). More...
double	CHd_13r
	The dimension-6 operator coefficient \((C_{HD})_{13}\) (real part). More...
double	CHd_22
	The dimension-6 operator coefficient \((C_{HD})_{22}\). More...
double	CHd_23i
	The dimension-6 operator coefficient \((C_{HD})_{23}\) (imaginary part). More...
double	CHd_23r
	The dimension-6 operator coefficient \((C_{HD})_{23}\) (real part). More...
double	CHd_33
	The dimension-6 operator coefficient \((C_{HD})_{33}\). More...
double	CHe_11
	The dimension-6 operator coefficient \((C_{HE})_{11}\). More...
double	CHe_12i
	The dimension-6 operator coefficient \((C_{HE})_{12}\) (imaginary part). More...
double	CHe_12r
	The dimension-6 operator coefficient \((C_{HE})_{12}\) (real part). More...
double	CHe_13i
	The dimension-6 operator coefficient \((C_{HE})_{13}\) (imaginary part). More...
double	CHe_13r
	The dimension-6 operator coefficient \((C_{HE})_{13}\) (real part). More...
double	CHe_22
	The dimension-6 operator coefficient \((C_{HE})_{22}\). More...
double	CHe_23i
	The dimension-6 operator coefficient \((C_{HE})_{23}\) (imaginary part). More...
double	CHe_23r
	The dimension-6 operator coefficient \((C_{HE})_{23}\) (real part). More...
double	CHe_33
	The dimension-6 operator coefficient \((C_{HE})_{33}\). More...
double	CHG
	The dimension-6 operator coefficient \(C_{HG}\). More...
double	CHL1_11
	The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\). More...
double	CHL1_12i
	The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part). More...
double	CHL1_12r
	The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part). More...
double	CHL1_13i
	The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part). More...
double	CHL1_13r
	The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part). More...
double	CHL1_22
	The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\). More...
double	CHL1_23i
	The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part). More...
double	CHL1_23r
	The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part). More...
double	CHL1_33
	The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\). More...
double	CHL3_11
	The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\). More...
double	CHL3_12i
	The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More...
double	CHL3_12r
	The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More...
double	CHL3_13i
	The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More...
double	CHL3_13r
	The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More...
double	CHL3_22
	The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\). More...
double	CHL3_23i
	The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More...
double	CHL3_23r
	The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More...
double	CHL3_33
	The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\). More...
double	CHQ1_11
	The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\). More...
double	CHQ1_12i
	The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part). More...
double	CHQ1_12r
	The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part). More...
double	CHQ1_13i
	The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part). More...
double	CHQ1_13r
	The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part). More...
double	CHQ1_22
	The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\). More...
double	CHQ1_23i
	The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part). More...
double	CHQ1_23r
	The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part). More...
double	CHQ1_33
	The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\). More...
double	CHQ3_11
	The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\). More...
double	CHQ3_12i
	The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part). More...
double	CHQ3_12r
	The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part). More...
double	CHQ3_13i
	The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part). More...
double	CHQ3_13r
	The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part). More...
double	CHQ3_22
	The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\). More...
double	CHQ3_23i
	The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part). More...
double	CHQ3_23r
	The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part). More...
double	CHQ3_33
	The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\). More...
double	CHu_11
	The dimension-6 operator coefficient \((C_{HU})_{11}\). More...
double	CHu_12i
	The dimension-6 operator coefficient \((C_{HU})_{12}\) (imaginary part). More...
double	CHu_12r
	The dimension-6 operator coefficient \((C_{HU})_{12}\) (real part). More...
double	CHu_13i
	The dimension-6 operator coefficient \((C_{HU})_{13}\) (imaginary part). More...
double	CHu_13r
	The dimension-6 operator coefficient \((C_{HU})_{13}\) (real part). More...
double	CHu_22
	The dimension-6 operator coefficient \((C_{HU})_{22}\). More...
double	CHu_23i
	The dimension-6 operator coefficient \((C_{HU})_{23}\) (imaginary part). More...
double	CHu_23r
	The dimension-6 operator coefficient \((C_{HU})_{23}\) (real part). More...
double	CHu_33
	The dimension-6 operator coefficient \((C_{HU})_{33}\). More...
double	CHud_11i
	The dimension-6 operator coefficient \((C_{HUD})_{11}\) (imaginary part). More...
double	CHud_11r
	The dimension-6 operator coefficient \((C_{HUD})_{11}\) (real part). More...
double	CHud_12i
	The dimension-6 operator coefficient \((C_{HUD})_{12}\) (imaginary part). More...
double	CHud_12r
	The dimension-6 operator coefficient \((C_{HUD})_{12}\) (real part). More...
double	CHud_13i
	The dimension-6 operator coefficient \((C_{HUD})_{13}\) (imaginary part). More...
double	CHud_13r
	The dimension-6 operator coefficient \((C_{HUD})_{13}\) (real part). More...
double	CHud_22i
	The dimension-6 operator coefficient \((C_{HUD})_{22}\) (imaginary part). More...
double	CHud_22r
	The dimension-6 operator coefficient \((C_{HUD})_{22}\) (real part). More...
double	CHud_23i
	The dimension-6 operator coefficient \((C_{HUD})_{23}\) (imaginary part). More...
double	CHud_23r
	The dimension-6 operator coefficient \((C_{HUD})_{23}\) (real part). More...
double	CHud_33i
	The dimension-6 operator coefficient \((C_{HUD})_{33}\) (imaginary part). More...
double	CHud_33r
	The dimension-6 operator coefficient \((C_{HUD})_{33}\) (real part). More...
double	CHW
	The dimension-6 operator coefficient \(C_{HW}\). More...
double	CHWB
	The dimension-6 operator coefficient \(C_{HWB}\). More...
double	CLL_1221
	The dimension-6 operator coefficient \((C_{LL})_{1221}\). More...
double	CLL_2112
	The dimension-6 operator coefficient \((C_{LL})_{2112}\). More...
double	CuH_11i
	The dimension-6 operator coefficient \((C_{UH})_{11}\) (imaginary part). More...
double	CuH_11r
	The dimension-6 operator coefficient \((C_{UH})_{11}\) (real part). More...
double	CuH_12i
	The dimension-6 operator coefficient \((C_{UH})_{12}\) (imaginary part). More...
double	CuH_12r
	The dimension-6 operator coefficient \((C_{UH})_{12}\) (real part). More...
double	CuH_13i
	The dimension-6 operator coefficient \((C_{UH})_{13}\) (imaginary part). More...
double	CuH_13r
	The dimension-6 operator coefficient \((C_{UH})_{13}\) (real part). More...
double	CuH_22i
	The dimension-6 operator coefficient \((C_{UH})_{22}\) (imaginary part). More...
double	CuH_22r
	The dimension-6 operator coefficient \((C_{UH})_{22}\) (real part). More...
double	CuH_23i
	The dimension-6 operator coefficient \((C_{UH})_{23}\) (imaginary part). More...
double	CuH_23r
	The dimension-6 operator coefficient \((C_{UH})_{23}\) (real part). More...
double	CuH_33i
	The dimension-6 operator coefficient \((C_{UH})_{33}\) (imaginary part). More...
double	CuH_33r
	The dimension-6 operator coefficient \((C_{UH})_{33}\) (real part). More...
double	cW2_tree
	The sqaure of the tree level values for the cosine of the weak angle. More...
double	cW_tree
	The tree level values for the cosine of the weak angle. More...
double	delta_AA
	Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More...
double	delta_AZ
	Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More...
double	delta_h
	Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition. More...
double	delta_ZZ
	Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition. More...
double	ettH2_Hgg
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to ttH production at Tevatron (1.96 TeV). More...
double	ettH2_Htt
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Htt}\) to ttH production at Tevatron (1.96 TeV). More...
double	ettH78_Hgg
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to ttH production at the LHC (7 & 8 TeV). More...
double	ettH78_Htt
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Htt}\) to ttH production at the LHC (7 & 8 TeV). More...
double	eVBF2_HAA
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HAA}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_Hgg
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_HWud
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_HWW1
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_HWW2
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_HWW3
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_HZA1
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_HZA2
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_HZdL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_HZdR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_HZuL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_HZuR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_HZZ1
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_HZZ2
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_HZZ3
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_Wud
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_ZdL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_ZdR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_ZuL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF2_ZuR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to VBF production at Tevatron (1.96 TeV). More...
double	eVBF78_HAA
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HAA}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_Hgg
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_HWud
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_HWW1
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_HWW2
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_HWW3
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_HZA1
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_HZA2
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_HZdL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_HZdR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_HZuL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_HZuR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_HZZ1
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_HZZ2
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_HZZ3
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_Wud
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_ZdL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_ZdR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_ZuL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eVBF78_ZuR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to VBF production at the LHC (7 & 8 TeV). More...
double	eWH2_HWud
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to WH production at Tevatron (1.96 TeV). More...
double	eWH2_HWW1
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to WH production at Tevatron (1.96 TeV). More...
double	eWH2_HWW2
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to WH production at Tevatron (1.96 TeV). More...
double	eWH2_HWW3
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to WH production at Tevatron (1.96 TeV). More...
double	eWH2_Wud
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to WH production at Tevatron (1.96 TeV). More...
double	eWH78_HWud
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to WH production at the LHC (7 & 8 TeV). More...
double	eWH78_HWW1
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to WH production at the LHC (7 & 8 TeV). More...
double	eWH78_HWW2
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to WH production at the LHC (7 & 8 TeV). More...
double	eWH78_HWW3
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to WH production at the LHC (7 & 8 TeV). More...
double	eWH78_Wud
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to WH production at the LHC (7 & 8 TeV). More...
double	eZH2_HZA1
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to ZH production at Tevatron (1.96 TeV). More...
double	eZH2_HZA2
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to ZH production at Tevatron (1.96 TeV). More...
double	eZH2_HZdL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to ZH production at Tevatron (1.96 TeV). More...
double	eZH2_HZdR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to ZH production at Tevatron (1.96 TeV). More...
double	eZH2_HZuL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to ZH production at Tevatron (1.96 TeV). More...
double	eZH2_HZuR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to ZH production at Tevatron (1.96 TeV). More...
double	eZH2_HZZ1
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to ZH production at Tevatron (1.96 TeV). More...
double	eZH2_HZZ2
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to ZH production at Tevatron (1.96 TeV). More...
double	eZH2_HZZ3
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to ZH production at Tevatron (1.96 TeV). More...
double	eZH2_ZdL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to ZH production at Tevatron (1.96 TeV). More...
double	eZH2_ZdR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to ZH production at Tevatron (1.96 TeV). More...
double	eZH2_ZuL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to ZH production at Tevatron (1.96 TeV). More...
double	eZH2_ZuR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to ZH production at Tevatron (1.96 TeV). More...
double	eZH78_HZA1
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to ZH production at the LHC (7 & 8 TeV). More...
double	eZH78_HZA2
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to ZH production at the LHC (7 & 8 TeV). More...
double	eZH78_HZdL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to ZH production at the LHC (7 & 8 TeV). More...
double	eZH78_HZdR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to ZH production at the LHC (7 & 8 TeV). More...
double	eZH78_HZuL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to ZH production at the LHC (7 & 8 TeV). More...
double	eZH78_HZuR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to ZH production at the LHC (7 & 8 TeV). More...
double	eZH78_HZZ1
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to ZH production at the LHC (7 & 8 TeV). More...
double	eZH78_HZZ2
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to ZH production at the LHC (7 & 8 TeV). More...
double	eZH78_HZZ3
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to ZH production at the LHC (7 & 8 TeV). More...
double	eZH78_ZdL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to ZH production at the LHC (7 & 8 TeV). More...
double	eZH78_ZdR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to ZH production at the LHC (7 & 8 TeV). More...
double	eZH78_ZuL
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to ZH production at the LHC (7 & 8 TeV). More...
double	eZH78_ZuR
	Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to ZH production at the LHC (7 & 8 TeV). More...
double	Lambda_NP
	The new physics scale [GeV]. More...
double	LambdaNP2
	The square of the new physics scale [GeV \(^2\)]. More...
double	MwInput
	The input value for the \(W\)-boson mass if FlagMwInput is true. More...
double	sW2_tree
	The sqaure of the tree level values for the sine of the weak angle. More...
double	sW_tree
	The tree level values for the sine of the weak angle. More...
double	v2_over_LambdaNP2
	The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\). 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	AlsMz
	The strong coupling constant at the Z-boson mass, \(\alpha_s(M_Z)\). More...
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	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	DeltaMK
double	Dmk
double	EpsK
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...
double	GF
	The Fermi constant \(G_\mu\) in \({\rm GeV}^{-2}\). More...
double	KbarEpsK
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...
double	Mz
	The mass of the \(Z\) boson in GeV. More...
double	phiEpsK
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	SM_M12D
gslpp::matrix< gslpp::complex >	UPMNS
	The PMNS matrix. More...
gslpp::matrix< gslpp::complex >	VCKM
	The CKM matrix. 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 Model
std::map< std::string, boost::reference_wrapper< const double > >	ModelParamMap
bool	UpdateError
	A boolean set to false if update is successful. More...

Private Attributes
const bool	FlagLeptonUniversal
	An internal boolean flag that is true if assuming lepton flavour universality. More...
bool	FlagMwInput
	A boolean flag that is true if the W mass is taken as an input parameter. (Warning: The W width is not implemented in this case.) More...
bool	FlagQuadraticTerms
	A boolean flag that is true if the quadratic terms in cross sections and widths are switched on. More...
const bool	FlagQuarkUniversal
	An internal boolean flag that is true if assuming quark flavour universality. More...

Additional Inherited Members
Public Types inherited from StandardModel
enum	lepton { NEUTRINO_1, ELECTRON, NEUTRINO_2, MU, NEUTRINO_3, TAU }
	An enum type for leptons. More...
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	meson { P_0, P_P, K_0, K_P, D_0, B_D, B_P, B_S, PHI, K_star, 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

NPEffectiveGIMR::NPEffectiveGIMR	(	const bool	FlagLeptonUniversal_in = false,
		const bool	FlagQuarkUniversal_in = false
	)

Constructor.

Parameters

[in]	FlagLeptonUniversal_in	an internal boolean flag that is true if assuming lepton flavour universality
[in]	FlagQuarkUniversal_in	an internal boolean flag that is true if assuming quark flavour universality

Definition at line 76 of file NPEffectiveGIMR.cpp.

: NPbase(), FlagLeptonUniversal(FlagLeptonUniversal_in), FlagQuarkUniversal(FlagQuarkUniversal_in)
{
    if ((!FlagLeptonUniversal && !FlagQuarkUniversal)
            || (!FlagLeptonUniversal && FlagQuarkUniversal)
            || (FlagLeptonUniversal && !FlagQuarkUniversal))
        throw std::runtime_error("Invalid arguments for NPEffectiveGIMR::NPEffectiveGIMR()");

    FlagMwInput = false;

    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHG", boost::cref(CHG)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHW", boost::cref(CHW)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHB", boost::cref(CHB)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHWB", boost::cref(CHWB)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHD", boost::cref(CHD)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHbox", boost::cref(CHbox)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CH", boost::cref(CH)));
    if (FlagLeptonUniversal) {
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1", boost::cref(CHL1_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3", boost::cref(CHL3_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe", boost::cref(CHe_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_r", boost::cref(CeH_11r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_i", boost::cref(CeH_11i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLL", boost::cref(CLL_1221)));
    } else {
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_11", boost::cref(CHL1_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_12r", boost::cref(CHL1_12r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_13r", boost::cref(CHL1_13r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_22", boost::cref(CHL1_22)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_23r", boost::cref(CHL1_23r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_33", boost::cref(CHL1_33)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_12i", boost::cref(CHL1_12i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_13i", boost::cref(CHL1_13i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL1_23i", boost::cref(CHL1_23i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_11", boost::cref(CHL3_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_12r", boost::cref(CHL3_12r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_13r", boost::cref(CHL3_13r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_22", boost::cref(CHL3_22)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_23r", boost::cref(CHL3_23r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_33", boost::cref(CHL3_33)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_12i", boost::cref(CHL3_12i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_13i", boost::cref(CHL3_13i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHL3_23i", boost::cref(CHL3_23i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_11", boost::cref(CHe_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_12r", boost::cref(CHe_12r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_13r", boost::cref(CHe_13r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_22", boost::cref(CHe_22)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_23r", boost::cref(CHe_23r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_33", boost::cref(CHe_33)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_12i", boost::cref(CHe_12i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_13i", boost::cref(CHe_13i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHe_23i", boost::cref(CHe_23i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_11r", boost::cref(CeH_11r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_12r", boost::cref(CeH_12r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_13r", boost::cref(CeH_13r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_22r", boost::cref(CeH_22r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_23r", boost::cref(CeH_23r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_33r", boost::cref(CeH_33r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_11i", boost::cref(CeH_11i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_12i", boost::cref(CeH_12i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_13i", boost::cref(CeH_13i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_22i", boost::cref(CeH_22i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_23i", boost::cref(CeH_23i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CeH_33i", boost::cref(CeH_33i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CLL_1221", boost::cref(CLL_1221)));
    }
    if (FlagQuarkUniversal) {
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1", boost::cref(CHQ1_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3", boost::cref(CHQ3_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu", boost::cref(CHu_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd", boost::cref(CHd_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_r", boost::cref(CHud_11r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_i", boost::cref(CHud_11i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_r", boost::cref(CuH_11r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_i", boost::cref(CuH_11i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_r", boost::cref(CdH_11r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_i", boost::cref(CdH_11i)));
    } else {
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_11", boost::cref(CHQ1_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_12r", boost::cref(CHQ1_12r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_13r", boost::cref(CHQ1_13r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_22", boost::cref(CHQ1_22)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_23r", boost::cref(CHQ1_23r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_33", boost::cref(CHQ1_33)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_12i", boost::cref(CHQ1_12i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_13i", boost::cref(CHQ1_13i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ1_23i", boost::cref(CHQ1_23i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_11", boost::cref(CHQ3_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_12r", boost::cref(CHQ3_12r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_13r", boost::cref(CHQ3_13r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_22", boost::cref(CHQ3_22)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_23r", boost::cref(CHQ3_23r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_33", boost::cref(CHQ3_33)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_12i", boost::cref(CHQ3_12i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_13i", boost::cref(CHQ3_13i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHQ3_23i", boost::cref(CHQ3_23i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_11", boost::cref(CHu_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_12r", boost::cref(CHu_12r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_13r", boost::cref(CHu_13r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_22", boost::cref(CHu_22)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_23r", boost::cref(CHu_23r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_33", boost::cref(CHu_33)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_12i", boost::cref(CHu_12i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_13i", boost::cref(CHu_13i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHu_23i", boost::cref(CHu_23i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_11", boost::cref(CHd_11)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_12r", boost::cref(CHd_12r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_13r", boost::cref(CHd_13r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_22", boost::cref(CHd_22)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_23r", boost::cref(CHd_23r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_33", boost::cref(CHd_33)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_12i", boost::cref(CHd_12i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_13i", boost::cref(CHd_13i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHd_23i", boost::cref(CHd_23i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_11r", boost::cref(CHud_11r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_12r", boost::cref(CHud_12r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_13r", boost::cref(CHud_13r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_22r", boost::cref(CHud_22r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_23r", boost::cref(CHud_23r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_33r", boost::cref(CHud_33r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_11i", boost::cref(CHud_11i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_12i", boost::cref(CHud_12i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_13i", boost::cref(CHud_13i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_22i", boost::cref(CHud_22i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_23i", boost::cref(CHud_23i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CHud_33i", boost::cref(CHud_33i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_11r", boost::cref(CuH_11r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_12r", boost::cref(CuH_12r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_13r", boost::cref(CuH_13r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_22r", boost::cref(CuH_22r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_23r", boost::cref(CuH_23r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_33r", boost::cref(CuH_33r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_11i", boost::cref(CuH_11i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_12i", boost::cref(CuH_12i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_13i", boost::cref(CuH_13i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_22i", boost::cref(CuH_22i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_23i", boost::cref(CuH_23i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CuH_33i", boost::cref(CuH_33i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_11r", boost::cref(CdH_11r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_12r", boost::cref(CdH_12r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_13r", boost::cref(CdH_13r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_22r", boost::cref(CdH_22r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_23r", boost::cref(CdH_23r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_33r", boost::cref(CdH_33r)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_11i", boost::cref(CdH_11i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_12i", boost::cref(CdH_12i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_13i", boost::cref(CdH_13i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_22i", boost::cref(CdH_22i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_23i", boost::cref(CdH_23i)));
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("CdH_33i", boost::cref(CdH_33i)));
    }
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("Lambda_NP", boost::cref(Lambda_NP)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HZZ1", boost::cref(eVBF2_HZZ1)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HZZ2", boost::cref(eVBF2_HZZ2)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HZZ3", boost::cref(eVBF2_HZZ3)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HZA1", boost::cref(eVBF2_HZA1)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HZA2", boost::cref(eVBF2_HZA2)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HAA", boost::cref(eVBF2_HAA)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HWW1", boost::cref(eVBF2_HWW1)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HWW2", boost::cref(eVBF2_HWW2)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HWW3", boost::cref(eVBF2_HWW3)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_Hgg", boost::cref(eVBF2_Hgg)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HZuL", boost::cref(eVBF2_HZuL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HZuR", boost::cref(eVBF2_HZuR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HZdL", boost::cref(eVBF2_HZdL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HZdR", boost::cref(eVBF2_HZdR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_HWud", boost::cref(eVBF2_HWud)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_ZuL", boost::cref(eVBF2_ZuL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_ZuR", boost::cref(eVBF2_ZuR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_ZdL", boost::cref(eVBF2_ZdL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_ZdR", boost::cref(eVBF2_ZdR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF2_Wud", boost::cref(eVBF2_Wud)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HZZ1", boost::cref(eVBF78_HZZ1)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HZZ2", boost::cref(eVBF78_HZZ2)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HZZ3", boost::cref(eVBF78_HZZ3)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HZA1", boost::cref(eVBF78_HZA1)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HZA2", boost::cref(eVBF78_HZA2)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HAA", boost::cref(eVBF78_HAA)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HWW1", boost::cref(eVBF78_HWW1)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HWW2", boost::cref(eVBF78_HWW2)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HWW3", boost::cref(eVBF78_HWW3)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_Hgg", boost::cref(eVBF78_Hgg)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HZuL", boost::cref(eVBF78_HZuL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HZuR", boost::cref(eVBF78_HZuR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HZdL", boost::cref(eVBF78_HZdL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HZdR", boost::cref(eVBF78_HZdR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_HWud", boost::cref(eVBF78_HWud)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_ZuL", boost::cref(eVBF78_ZuL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_ZuR", boost::cref(eVBF78_ZuR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_ZdL", boost::cref(eVBF78_ZdL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_ZdR", boost::cref(eVBF78_ZdR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eVBF78_Wud", boost::cref(eVBF78_Wud)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH2_HWW1", boost::cref(eWH2_HWW1)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH2_HWW2", boost::cref(eWH2_HWW2)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH2_HWW3", boost::cref(eWH2_HWW3)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH2_HWud", boost::cref(eWH2_HWud)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH2_Wud", boost::cref(eWH2_Wud)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH78_HWW1", boost::cref(eWH78_HWW1)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH78_HWW2", boost::cref(eWH78_HWW2)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH78_HWW3", boost::cref(eWH78_HWW3)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH78_HWud", boost::cref(eWH78_HWud)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eWH78_Wud", boost::cref(eWH78_Wud)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH2_HZZ1", boost::cref(eZH2_HZZ1)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH2_HZZ2", boost::cref(eZH2_HZZ2)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH2_HZZ3", boost::cref(eZH2_HZZ3)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH2_HZA1", boost::cref(eZH2_HZA1)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH2_HZA2", boost::cref(eZH2_HZA2)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH2_HZuL", boost::cref(eZH2_HZuL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH2_HZuR", boost::cref(eZH2_HZuR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH2_HZdL", boost::cref(eZH2_HZdL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH2_HZdR", boost::cref(eZH2_HZdR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH2_ZuL", boost::cref(eZH2_ZuL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH2_ZuR", boost::cref(eZH2_ZuR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH2_ZdL", boost::cref(eZH2_ZdL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH2_ZdR", boost::cref(eZH2_ZdR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH78_HZZ1", boost::cref(eZH78_HZZ1)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH78_HZZ2", boost::cref(eZH78_HZZ2)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH78_HZZ3", boost::cref(eZH78_HZZ3)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH78_HZA1", boost::cref(eZH78_HZA1)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH78_HZA2", boost::cref(eZH78_HZA2)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH78_HZuL", boost::cref(eZH78_HZuL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH78_HZuR", boost::cref(eZH78_HZuR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH78_HZdL", boost::cref(eZH78_HZdL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH78_HZdR", boost::cref(eZH78_HZdR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH78_ZuL", boost::cref(eZH78_ZuL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH78_ZuR", boost::cref(eZH78_ZuR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH78_ZdL", boost::cref(eZH78_ZdL)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("eZH78_ZdR", boost::cref(eZH78_ZdR)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH2_Htt", boost::cref(ettH2_Htt)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH2_Hgg", boost::cref(ettH2_Hgg)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH78_Htt", boost::cref(ettH78_Htt)));
    ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("ettH78_Hgg", boost::cref(ettH78_Hgg)));
    if (FlagMwInput)
        ModelParamMap.insert(std::pair<std::string, boost::reference_wrapper<const double> >("MwInput", boost::cref(MwInput)));
}

Member Function Documentation

gslpp::complex NPEffectiveGIMR::AH_f

(

const double

tau

)

const

Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.

\(A^H_f(\tau)=2\tau [1+(1-\tau)f(\tau)]\)

Parameters

[in]

Definition at line 1277 of file NPEffectiveGIMR.cpp.

{
    return (2.0 * tau * (1.0 + (1.0 - tau) * f_triangle(tau)));
}

double NPEffectiveGIMR::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 1886 of file NPEffectiveGIMR.cpp.

{
    double Br = 1.0;
    
    Br += deltaGammaHbbRatio1() - deltaGammaTotalRatio1();
    
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        //(Only valid under the assumptions of one dim 6 operator at a time)
        Br += - deltaGammaHbbRatio1() * deltaGammaTotalRatio1()
                + deltaGammaHbbRatio2() - deltaGammaTotalRatio2()
                + pow(deltaGammaTotalRatio1(),2.0);            
        }
    
    if (Br < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return Br;

}

double NPEffectiveGIMR::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 1866 of file NPEffectiveGIMR.cpp.

{
    double Br = 1.0;
    
    Br += deltaGammaHccRatio1() - deltaGammaTotalRatio1();
    
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        //(Only valid under the assumptions of one dim 6 operator at a time)
        Br += - deltaGammaHccRatio1() * deltaGammaTotalRatio1()
                + deltaGammaHccRatio2() - deltaGammaTotalRatio2()
                + pow(deltaGammaTotalRatio1(),2.0);            
        }
    
    if (Br < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return Br;

}

double NPEffectiveGIMR::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 1826 of file NPEffectiveGIMR.cpp.

{
    double Br = 1.0;
    
    Br += deltaGammaHgagaRatio1() - deltaGammaTotalRatio1();
    
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        //(Only valid under the assumptions of one dim 6 operator at a time)
        Br += - deltaGammaHgagaRatio1() * deltaGammaTotalRatio1()
                + deltaGammaHgagaRatio2() - deltaGammaTotalRatio2()
                + pow(deltaGammaTotalRatio1(),2.0);            
        }
    
    if (Br < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return Br;

}

double NPEffectiveGIMR::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 1746 of file NPEffectiveGIMR.cpp.

{
    double Br = 1.0;
    
    Br += deltaGammaHggRatio1() - deltaGammaTotalRatio1();
    
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        //(Only valid under the assumptions of one dim 6 operator at a time)
        Br += - deltaGammaHggRatio1() * deltaGammaTotalRatio1()
                + deltaGammaHggRatio2() - deltaGammaTotalRatio2()
                + pow(deltaGammaTotalRatio1(),2.0);            
        }
    
    if (Br < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return Br;

}

double NPEffectiveGIMR::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 1846 of file NPEffectiveGIMR.cpp.

{
    double Br = 1.0;
    
    Br += deltaGammaHtautauRatio1() - deltaGammaTotalRatio1();
    
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        //(Only valid under the assumptions of one dim 6 operator at a time)
        Br += - deltaGammaHtautauRatio1() * deltaGammaTotalRatio1()
                + deltaGammaHtautauRatio2() - deltaGammaTotalRatio2()
                + pow(deltaGammaTotalRatio1(),2.0);            
        }
    
    if (Br < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return Br;

}

double NPEffectiveGIMR::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 1766 of file NPEffectiveGIMR.cpp.

{
    double Br = 1.0;
    
    Br += deltaGammaHWWRatio1() - deltaGammaTotalRatio1();
    
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        //(Only valid under the assumptions of one dim 6 operator at a time)
        Br += - deltaGammaHWWRatio1() * deltaGammaTotalRatio1()
                + deltaGammaHWWRatio2() - deltaGammaTotalRatio2()
                + pow(deltaGammaTotalRatio1(),2.0);            
        }
    
    if (Br < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return Br;

}

double NPEffectiveGIMR::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 1806 of file NPEffectiveGIMR.cpp.

{
    double Br = 1.0;
    
    Br += deltaGammaHZgaRatio1() - deltaGammaTotalRatio1();
    
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        //(Only valid under the assumptions of one dim 6 operator at a time)
        Br += - deltaGammaHZgaRatio1() * deltaGammaTotalRatio1()
                + deltaGammaHZgaRatio2() - deltaGammaTotalRatio2()
                + pow(deltaGammaTotalRatio1(),2.0);            
        }
    
    if (Br < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return Br;

}

double NPEffectiveGIMR::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 1786 of file NPEffectiveGIMR.cpp.

{
    double Br = 1.0;
    
    Br += deltaGammaHZZRatio1() - deltaGammaTotalRatio1();
    
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        //(Only valid under the assumptions of one dim 6 operator at a time)
        Br += - deltaGammaHZZRatio1() * deltaGammaTotalRatio1()
                + deltaGammaHZZRatio2() - deltaGammaTotalRatio2()
                + pow(deltaGammaTotalRatio1(),2.0);            
        }
    
    if (Br < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return Br;

}

gslpp::complex NPEffectiveGIMR::CfH_diag ( const Particle  f ) const

protected

The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f.

Parameters

[in]

f

a lepton or quark

Returns

\((\)C_{fH})_{ff} \(\)

Definition at line 1006 of file NPEffectiveGIMR.cpp.

{
    if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
        return 0.0;
    else if (f.is("ELECTRON"))
        return gslpp::complex(CeH_11r, CeH_11i, false);
    else if (f.is("MU"))
        return gslpp::complex(CeH_22r, CeH_22i, false);
    else if (f.is("TAU"))
        return gslpp::complex(CeH_33r, CeH_33i, false);
    else if (f.is("UP"))
        return gslpp::complex(CuH_11r, CuH_11i, false);
    else if (f.is("CHARM"))
        return gslpp::complex(CuH_22r, CuH_22i, false);
    else if (f.is("TOP"))
        return gslpp::complex(CuH_33r, CuH_33i, false);
    else if (f.is("DOWN"))
        return gslpp::complex(CdH_11r, CdH_11i, false);
    else if (f.is("STRANGE"))
        return gslpp::complex(CdH_22r, CdH_22i, false);
    else if (f.is("BOTTOM"))
        return gslpp::complex(CdH_33r, CdH_33i, false);
    else
        throw std::runtime_error("NPEffectiveGIMR::CfH_diag(): wrong argument");
}

bool NPEffectiveGIMR::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 873 of file NPEffectiveGIMR.cpp.

{
    if (FlagLeptonUniversal && FlagQuarkUniversal) {
        if (FlagMwInput) {
            if (DPars.find("MwInput") == DPars.end()) {
                std::cout << "ERROR: Missing mandatory NPEffectiveGIMR_LFU_QFU parameter MwInput" << std::endl;
                return false;
            }
        }
        for (int i = 0; i < NNPEffectiveGIMRVars_LFU_QFU; i++) {
            if (DPars.find(NPEffectiveGIMRVars_LFU_QFU[i]) == DPars.end()) {
                std::cout << "ERROR: Missing mandatory NPEffectiveGIMR_LFU_QFU parameter "
                        << NPEffectiveGIMRVars_LFU_QFU[i] << std::endl;
                return false;
            }
        }
        //} else if (FlagLeptonUniversal && !FlagQuarkUniversal) {
        //} else if (!FlagLeptonUniversal && FlagQuarkUniversal) {
    } else if (!FlagLeptonUniversal && !FlagQuarkUniversal) {
        if (FlagMwInput) {
            if (DPars.find("MwInput") == DPars.end()) {
                std::cout << "ERROR: Missing mandatory NPEffectiveGIMR parameter MwInput" << std::endl;
                return false;
            }
        }
        for (int i = 0; i < NNPEffectiveGIMRVars; i++) {
            if (DPars.find(NPEffectiveGIMRVars[i]) == DPars.end()) {
                std::cout << "ERROR: Missing mandatory NPEffectiveGIMR parameter"
                        << NPEffectiveGIMRVars[i] << std::endl;
                return false;
            }
        }
    } else
        throw std::runtime_error("Error in NPEffectiveGIMR::CheckParameters()");

    return (NPbase::CheckParameters(DPars));
}

double NPEffectiveGIMR::CHF1_diag ( const Particle  F ) const

protected

The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F.

Parameters

[in]

F

a lepton or quark

Returns

\((\)C_{HF}^{(1)})_{FF} \(\)

Definition at line 929 of file NPEffectiveGIMR.cpp.

{
    if (F.is("NEUTRINO_1") || F.is("ELECTRON"))
        return CHL1_11;
    else if (F.is("NEUTRINO_2") || F.is("MU"))
        return CHL1_22;
    else if (F.is("NEUTRINO_3") || F.is("TAU"))
        return CHL1_33;
    else if (F.is("UP") || F.is("DOWN"))
        return CHQ1_11;
    else if (F.is("CHARM") || F.is("STRANGE"))
        return CHQ1_22;
    else if (F.is("TOP") || F.is("BOTTOM"))
        return CHQ1_33;
    else
        throw std::runtime_error("NPEffectiveGIMR::CHF1_diag(): wrong argument");
}

double NPEffectiveGIMR::CHF3_diag ( const Particle  F ) const

protected

The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F.

Parameters

[in]

F

a lepton or quark

Returns

\((\)C_{HF}^{(3)})_{FF} \(\)

Definition at line 947 of file NPEffectiveGIMR.cpp.

{
    if (F.is("NEUTRINO_1") || F.is("ELECTRON"))
        return CHL3_11;
    else if (F.is("NEUTRINO_2") || F.is("MU"))
        return CHL3_22;
    else if (F.is("NEUTRINO_3") || F.is("TAU"))
        return CHL3_33;
    else if (F.is("UP") || F.is("DOWN"))
        return CHQ3_11;
    else if (F.is("CHARM") || F.is("STRANGE"))
        return CHQ3_22;
    else if (F.is("TOP") || F.is("BOTTOM"))
        return CHQ3_33;
    else
        throw std::runtime_error("NPEffectiveGIMR::CHF3_diag(): wrong argument");
}

double NPEffectiveGIMR::CHf_diag ( const Particle  f ) const

protected

The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f.

Parameters

[in]

f

a lepton or quark

Returns

\((\)C_{Hf})_{ff} \(\)

Definition at line 965 of file NPEffectiveGIMR.cpp.

{
    if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
        return 0.0;
    else if (f.is("ELECTRON"))
        return CHe_11;
    else if (f.is("MU"))
        return CHe_22;
    else if (f.is("TAU"))
        return CHe_33;
    else if (f.is("UP"))
        return CHu_11;
    else if (f.is("CHARM"))
        return CHu_22;
    else if (f.is("TOP"))
        return CHu_33;
    else if (f.is("DOWN"))
        return CHd_11;
    else if (f.is("STRANGE"))
        return CHd_22;
    else if (f.is("BOTTOM"))
        return CHd_33;
    else
        throw std::runtime_error("NPEffectiveGIMR::CHf_diag(): wrong argument");
}

gslpp::complex NPEffectiveGIMR::CHud_diag ( const Particle  u ) const

protected

The diagonal entry of the dimension-6 operator coefficient \(C_{HUD}\) corresponding to particle f.

Parameters

[in]

u

a quark

Returns

\((\)C_{HUD})_{ud} \(\)

Definition at line 991 of file NPEffectiveGIMR.cpp.

{
    if (!u.is("QUARK") || u.getIndex() % 2 != 0)
        throw std::runtime_error("NPEffectiveGIMR::CHud_diag(): wrong argument");

    if (u.is("UP"))
        return gslpp::complex(CHud_11r, CHud_11i, false);
    else if (u.is("CHARM"))
        return gslpp::complex(CHud_22r, CHud_22i, false);
    else if (u.is("TOP"))
        return gslpp::complex(CHud_22r, CHud_33i, false);
    else
        throw std::runtime_error("NPEffectiveGIMR::CHud_diag(): wrong argument");
}

double NPEffectiveGIMR::computeGammaTotalRatio ( ) const

virtual

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

Returns

\(\Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 1906 of file NPEffectiveGIMR.cpp.

{
    return (trueSM.computeBrHtogg() * GammaHggRatio()
            + trueSM.computeBrHtoWW() * GammaHWWRatio()
            + trueSM.computeBrHtoZZ() * GammaHZZRatio()
            + trueSM.computeBrHtoZga() * GammaHZgaRatio()
            + trueSM.computeBrHtogaga() * GammaHgagaRatio()
            + trueSM.computeBrHtotautau() * GammaHtautauRatio()
            + trueSM.computeBrHtocc() * GammaHccRatio()
            + trueSM.computeBrHtobb() * GammaHbbRatio());
}

double NPEffectiveGIMR::deltaG1_hWW

(

)

const

The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\).

Returns

\(\delta g_{HWW}^{(1)}\)

Definition at line 1161 of file NPEffectiveGIMR.cpp.

{
    return (2.0 * CHW * v2_over_LambdaNP2 / v());
}

double NPEffectiveGIMR::deltaG1_hZA

(

)

const

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\).

Returns

\(\delta g_{HZA}^{(1)}\)

Definition at line 1201 of file NPEffectiveGIMR.cpp.

{
    return (delta_AZ / v());
}

double NPEffectiveGIMR::deltaG1_hZZ

(

)

const

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\).

Returns

\(\delta g_{HZZ}^{(1)}\)

Definition at line 1184 of file NPEffectiveGIMR.cpp.

{
    return (delta_ZZ / v());
}

double NPEffectiveGIMR::deltaG2_hWW

(

)

const

The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\).

Returns

\(\delta g_{HWW}^{(2)}\)

Definition at line 1166 of file NPEffectiveGIMR.cpp.

{
    return 0.0;
}

double NPEffectiveGIMR::deltaG2_hZA

(

)

const

The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\).

Returns

\(\delta g_{HZA}^{(2)}\)

Definition at line 1206 of file NPEffectiveGIMR.cpp.

{
    return 0.0;
}

double NPEffectiveGIMR::deltaG2_hZZ

(

)

const

The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\).

Returns

\(\delta g_{HZZ}^{(2)}\)

Definition at line 1189 of file NPEffectiveGIMR.cpp.

{
    return 0.0;
}

double NPEffectiveGIMR::deltaG3_hWW

(

)

const

The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\).

Returns

\(\delta g_{HWW}^{(3)}\)

Definition at line 1171 of file NPEffectiveGIMR.cpp.

{
    double NPindirect;
    if (FlagMwInput) {
        NPindirect = 2.0 * MwInput * MwInput / v() * (delta_h - 0.5 * DeltaGF());
    } else {
        NPindirect = 2.0 * cW2_tree * Mz * Mz / v()
                * (delta_h - 1.0 / 2.0 / (cW2_tree - sW2_tree)
                * ((4.0 * sW_tree * cW_tree * CHWB + cW2_tree * CHD) * v2_over_LambdaNP2 + DeltaGF()));
    }
    return NPindirect;
}

double NPEffectiveGIMR::deltaG3_hZZ

(

)

const

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\).

Returns

\(\delta g_{HZZ}^{(3)}\)

Definition at line 1194 of file NPEffectiveGIMR.cpp.

{
    double NPindirect = Mz * Mz / v() * (-0.5 * CHD * v2_over_LambdaNP2 + delta_h - 0.5 * DeltaGF());
    double NPdirect = Mz * Mz / v() * CHD * v2_over_LambdaNP2;
    return (NPindirect + NPdirect);
}

double NPEffectiveGIMR::deltaG_hAA

(

)

const

The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\).

Returns

\(\delta g_{HAA}\)

Definition at line 1211 of file NPEffectiveGIMR.cpp.

{
    return (delta_AA / v());
}

gslpp::complex NPEffectiveGIMR::deltaG_hff

(

const Particle

p

)

const

The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\).

Parameters

[in]

p

a lepton or quark

Returns

\(\delta g_{Hff}\)

Definition at line 1216 of file NPEffectiveGIMR.cpp.

{
    /* The effects of the RG running are neglected. */
    double mf;
    if (p.is("TOP"))
        //mf = p.getMass(); // m_t(m_t)
        mf = mtpole; // pole mass
    else
        mf = p.getMass();
    gslpp::complex CfH = CfH_diag(p);
    return (-mf / v() * (delta_h - 0.5 * DeltaGF())
            + CfH * v2_over_LambdaNP2 / sqrt(2.0));
}

double NPEffectiveGIMR::deltaG_hgg

(

)

const

The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\).

Returns

\(\delta g_{HGG}\)

Definition at line 1156 of file NPEffectiveGIMR.cpp.

{
    return (CHG * v2_over_LambdaNP2 / v());
}

double NPEffectiveGIMR::deltaGA_f ( const Particle  p ) const

virtual

New physics contribution to the neutral-current axial-vector coupling \(g_A^f\).

Parameters

[in]

f

a lepton or quark

Returns

\(\delta g_A^f\)

Reimplemented from NPbase.

Definition at line 1087 of file NPEffectiveGIMR.cpp.

{
    return (deltaGL_f(p) - deltaGR_f(p));
}

double NPEffectiveGIMR::deltaGammaHbbRatio1

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to bb)\)/ \(\Gamma(H\to bb)_{\mathrm{SM}}\)

Definition at line 2200 of file NPEffectiveGIMR.cpp.

{    
    return ( -0.013 * deltaG_hff(quarks[TOP]).real()
            -117.431 * deltaG_hff(quarks[BOTTOM]).real() );
}

double NPEffectiveGIMR::deltaGammaHbbRatio2

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to bb)\)/ \(\Gamma(H\to bb)_{\mathrm{SM}}\)

Definition at line 2206 of file NPEffectiveGIMR.cpp.

{
    //Contributions that are quadratic in the effective coefficients
    //(Only valid under the assumptions of one dim 6 operator at a time)
    return ( +3443.96 * pow(deltaG_hff(quarks[BOTTOM]).real(),2.0) );        
    
}

double NPEffectiveGIMR::deltaGammaHccRatio1

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to cc)\)/ \(\Gamma(H\to cc)_{\mathrm{SM}}\)

Definition at line 2172 of file NPEffectiveGIMR.cpp.

{
    return ( -383.036 * deltaG_hff(quarks[CHARM]).real() );   
}

double NPEffectiveGIMR::deltaGammaHccRatio2

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to cc)\)/ \(\Gamma(H\to cc)_{\mathrm{SM}}\)

Definition at line 2177 of file NPEffectiveGIMR.cpp.

{
    //Contributions that are quadratic in the effective coefficients
    //(Only valid under the assumptions of one dim 6 operator at a time)
    return ( +36709.1 * pow(deltaG_hff(quarks[CHARM]).real(),2.0) );            
    
}

double NPEffectiveGIMR::deltaGammaHgagaRatio1

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to \gamma\gamma)\)/ \(\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}\)

Definition at line 2102 of file NPEffectiveGIMR.cpp.

{
    return ( -257366. * deltaG_hAA()
            +0.049 * deltaG3_hWW()
            +0.761 * deltaG_hff(quarks[TOP]).real()
            -0.441 * deltaG_hff(quarks[BOTTOM]).real()
            -1.087 * deltaG_hff(leptons[TAU]).real()
            -0.646 * deltaG_hff(quarks[CHARM]).real() );
    
}

double NPEffectiveGIMR::deltaGammaHgagaRatio2

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to \gamma\gamma)\)/ \(\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}\)

Definition at line 2113 of file NPEffectiveGIMR.cpp.

{
    //Contributions that are quadratic in the effective coefficients
    //(Only valid under the assumptions of one dim 6 operator at a time)
    return ( +16479108529. * pow(deltaG_hAA(),2.0)
            +0.001 * pow(deltaG3_hWW(),2.0)
            +0.146 * pow(deltaG_hff(quarks[TOP]).real(),2.0)
            +1.828 * pow(deltaG_hff(quarks[BOTTOM]).real(),2.0)
            +6.672 * pow(deltaG_hff(leptons[TAU]).real(),2.0)
            +9.962 * pow(deltaG_hff(quarks[CHARM]).real(),2.0) );            
    
}

double NPEffectiveGIMR::deltaGammaHggRatio1

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.

Returns

\(\delta \Gamma(H\to gg)\)/ \(\Gamma(H\to gg)_{\mathrm{SM}}\)

Definition at line 1958 of file NPEffectiveGIMR.cpp.

{
    return ( +151669. * deltaG_hgg()
            -3.006 * deltaG_hff(quarks[TOP]).real()
            +5.853 * deltaG_hff(quarks[BOTTOM]).real()
            +4.71 * deltaG_hff(quarks[CHARM]).real() );
}

double NPEffectiveGIMR::deltaGammaHggRatio2

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to gg)\)/ \(\Gamma(H\to gg)_{\mathrm{SM}}\)

Definition at line 1966 of file NPEffectiveGIMR.cpp.

{
    //Contributions that are quadratic in the effective coefficients
    //(Only valid under the assumptions of one dim 6 operator at a time)
    return ( +5879800851. * pow(deltaG_hgg(),2.0)
            +2.284 * pow(deltaG_hff(quarks[TOP]).real(),2.0)
            +40.881 * pow(deltaG_hff(quarks[BOTTOM]).real(),2.0)
            +2.17 * pow(deltaG_hff(quarks[CHARM]).real(),2.0) );            
    
}

double NPEffectiveGIMR::deltaGammaHtautauRatio1

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to \tau\tau)\)/ \(\Gamma(H\to \tau\tau)_{\mathrm{SM}}\)

Definition at line 2142 of file NPEffectiveGIMR.cpp.

{
    return ( -277.458 * deltaG_hff(leptons[TAU]).real() );
        
}

double NPEffectiveGIMR::deltaGammaHtautauRatio2

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to \tau\tau)\)/ \(\Gamma(H\to \tau\tau)_{\mathrm{SM}}\)

Definition at line 2148 of file NPEffectiveGIMR.cpp.

{
    //Contributions that are quadratic in the effective coefficients
    //(Only valid under the assumptions of one dim 6 operator at a time)
    return ( +19223. * pow(deltaG_hff(leptons[TAU]).real(),2.0) );            
    
}

double NPEffectiveGIMR::deltaGammaHWWRatio1

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to WW)\)/ \(\Gamma(H\to WW)_{\mathrm{SM}}\)

Definition at line 1993 of file NPEffectiveGIMR.cpp.

{

    return ( -183.404 * deltaG1_hWW()
            -274.568 * deltaG2_hWW()
            +0.039 * deltaG3_hWW() );
    
}

double NPEffectiveGIMR::deltaGammaHWWRatio2

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to WW)\)/ \(\Gamma(H\to WW)_{\mathrm{SM}}\)

Definition at line 2002 of file NPEffectiveGIMR.cpp.

{
    //Contributions that are quadratic in the effective coefficients
    //(Only valid under the assumptions of one dim 6 operator at a time)
    return ( +1267. * pow(deltaG1_hWW(),2.0)
            +868.393 * pow(deltaG2_hWW(),2.0) );
    
}

double NPEffectiveGIMR::deltaGammaHZgaRatio1

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to Z\gamma)\)/ \(\Gamma(H\to Z\gamma)_{\mathrm{SM}}\)

Definition at line 2062 of file NPEffectiveGIMR.cpp.

{

    return ( -71321.5 * deltaG1_hZA()
            +0.041 * deltaG3_hWW()
            +0.172 * deltaG_hff(quarks[TOP]).real()
            -0.301 * deltaG_hff(quarks[BOTTOM]).real()
            +0.196 * deltaG_hff(leptons[TAU]).real()
            +0.232 * deltaG_hff(quarks[CHARM]).real() );
    
}

double NPEffectiveGIMR::deltaGammaHZgaRatio2

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to Z\gamma)\)/ \(\Gamma(H\to Z\gamma)_{\mathrm{SM}}\)

Definition at line 2074 of file NPEffectiveGIMR.cpp.

{
    //Contributions that are quadratic in the effective coefficients
    //(Only valid under the assumptions of one dim 6 operator at a time)
    return ( +1271853409. * pow(deltaG1_hZA(),2.0)
            +0.003 * pow(deltaG_hff(quarks[TOP]).real(),2.0)
            +3.539 * pow(deltaG_hff(quarks[BOTTOM]).real(),2.0)
            -14.568 * pow(deltaG_hff(leptons[TAU]).real(),2.0)
            -31.197 * pow(deltaG_hff(quarks[CHARM]).real(),2.0) );            
    
}

double NPEffectiveGIMR::deltaGammaHZZRatio1

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to ZZ)\)/ \(\Gamma(H\to ZZ)_{\mathrm{SM}}\)

Definition at line 2027 of file NPEffectiveGIMR.cpp.

{

    return ( -246.654 * deltaG1_hZZ()
            -240.846 * deltaG2_hZZ()
            +0.059 * deltaG3_hZZ() );
    
}

double NPEffectiveGIMR::deltaGammaHZZRatio2

(

)

const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns

\(\delta \Gamma(H\to ZZ)\)/ \(\Gamma(H\to ZZ)_{\mathrm{SM}}\)

Definition at line 2036 of file NPEffectiveGIMR.cpp.

{
    //Contributions that are quadratic in the effective coefficients
    //(Only valid under the assumptions of one dim 6 operator at a time)
    return ( +6391.57 * pow(deltaG1_hZZ(),2.0)
            +2088.67 * pow(deltaG2_hZZ(),2.0)
            +0.001 * pow(deltaG3_hZZ(),2.0) );            
    
}

double NPEffectiveGIMR::deltaGammaTotalRatio1 ( ) const

virtual

The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.

Returns

\(\delta \Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Definition at line 1918 of file NPEffectiveGIMR.cpp.

{
    return (trueSM.computeBrHtogg() * deltaGammaHggRatio1()
            + trueSM.computeBrHtoWW() * deltaGammaHWWRatio1()
            + trueSM.computeBrHtoZZ() * deltaGammaHZZRatio1()
            + trueSM.computeBrHtoZga() * deltaGammaHZgaRatio1()
            + trueSM.computeBrHtogaga() * deltaGammaHgagaRatio1()
            + trueSM.computeBrHtotautau() * deltaGammaHtautauRatio1()
            + trueSM.computeBrHtocc() * deltaGammaHccRatio1()
            + trueSM.computeBrHtobb() * deltaGammaHbbRatio1());
}

double NPEffectiveGIMR::deltaGammaTotalRatio2 ( ) const

virtual

The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients.

Returns

\(\delta \Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Definition at line 1930 of file NPEffectiveGIMR.cpp.

{
    return (trueSM.computeBrHtogg() * deltaGammaHggRatio2()
            + trueSM.computeBrHtoWW() * deltaGammaHWWRatio2()
            + trueSM.computeBrHtoZZ() * deltaGammaHZZRatio2()
            + trueSM.computeBrHtoZga() * deltaGammaHZgaRatio2()
            + trueSM.computeBrHtogaga() * deltaGammaHgagaRatio2()
            + trueSM.computeBrHtotautau() * deltaGammaHtautauRatio2()
            + trueSM.computeBrHtocc() * deltaGammaHccRatio2()
            + trueSM.computeBrHtobb() * deltaGammaHbbRatio2());
}

double NPEffectiveGIMR::DeltaGF ( ) const

virtual

New physics contribution to the Fermi constant.

The new physics contribution \(\Delta G\) is defined as

\[ G_\mu = G_{\mu,\mathrm{SM}}(1+\Delta G)\,, \]

where \(G_\mu\) is the experimental value measured through muon decays, and \(G_{\mu,\mathrm{SM}}\) is the Fermi constant in the SM.

Returns

\(\Delta G\)

Reimplemented from NPbase.

Definition at line 1035 of file NPEffectiveGIMR.cpp.

{
    return ((CHL3_11 + CHL3_22 - 0.5 * (CLL_1221 + CLL_2112)) * v2_over_LambdaNP2);
}

double NPEffectiveGIMR::deltaGL_f

(

const Particle

p

)

const

New physics contribution to the neutral-current left-handed coupling \(g_L^f\).

Parameters

[in]

f

a lepton or quark

Returns

\(\delta g_L^f\)

Definition at line 1092 of file NPEffectiveGIMR.cpp.

{
    double I3p = p.getIsospin(), Qp = p.getCharge();
    double CHF1 = CHF1_diag(p);
    double CHF3 = CHF3_diag(p);
    double NPindirect;
    if (FlagMwInput) {
        NPindirect = -I3p / 4.0 * (CHD * v2_over_LambdaNP2 + 2.0 * DeltaGF())
                + Qp * sW2_tree
                * ((cW_tree / sW_tree * CHWB + (1.0 + cW2_tree) / 4.0 / sW2_tree * CHD) * v2_over_LambdaNP2 + 0.5 * DeltaGF());
    } else {
        NPindirect = -I3p / 4.0 * (CHD * v2_over_LambdaNP2 + 2.0 * DeltaGF())
                - Qp * sW2_tree / 4.0 / (cW2_tree - sW2_tree)
                *((4.0 * cW_tree / sW_tree * CHWB + CHD) * v2_over_LambdaNP2 + 2.0 * DeltaGF());
    }
    double NPdirect = -0.5 * (CHF1 - 2.0 * I3p * CHF3) * v2_over_LambdaNP2;
    return (NPindirect + NPdirect);
}

gslpp::complex NPEffectiveGIMR::deltaGL_Wff	(	const Particle	pbar,
		const Particle	p
	)		const

New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\).

Parameters

[in]	pbar	a lepton or quark
[in]	p	a lepton or quark

Returns

\(\delta g_{Wff}^{L}\)

Definition at line 1130 of file NPEffectiveGIMR.cpp.

{
    if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
        throw std::runtime_error("NPEffectiveGIMR::deltaGL_Wff(): Not implemented");

    double CHF3 = CHF3_diag(pbar);
    double NPindirect;
    if (FlagMwInput) {
        NPindirect = -0.5 * DeltaGF();
    } else {
        NPindirect = -cW2_tree / 4.0 / (cW2_tree - sW2_tree)
                * ((4.0 * sW_tree / cW_tree * CHWB + CHD) * v2_over_LambdaNP2 + 2.0 * DeltaGF());
    }
    double NPdirect = CHF3 * v2_over_LambdaNP2;
    return (NPindirect + NPdirect);
}

gslpp::complex NPEffectiveGIMR::deltaGL_Wffh	(	const Particle	pbar,
		const Particle	p
	)		const

The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\).

Parameters

[in]	pbar	a lepton or quark
[in]	p	a lepton or quark

Returns

\(\delta g_{WffH}^{L}\)

Definition at line 1230 of file NPEffectiveGIMR.cpp.

{
    if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
        throw std::runtime_error("NPEffectiveGIMR::deltaGL_Wffh(): Not implemented");

    double CHF3 = CHF3_diag(pbar);
    return (2.0 * sqrt(2.0) * Mz * cW_tree / v() / v() * CHF3 * v2_over_LambdaNP2);
}

double NPEffectiveGIMR::deltaGL_Zffh

(

const Particle

p

)

const

The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\).

Parameters

[in]

p

a lepton or quark

Returns

\(\delta g_{ZffH}^{L}\)

Definition at line 1248 of file NPEffectiveGIMR.cpp.

{
    double I3p = p.getIsospin();
    double CHF1 = CHF1_diag(p);
    double CHF3 = CHF3_diag(p);
    return (-2.0 * Mz / v() / v() * (CHF1 - 2.0 * I3p * CHF3) * v2_over_LambdaNP2);
}

double NPEffectiveGIMR::deltaGR_f

(

const Particle

p

)

const

New physics contribution to the neutral-current right-handed coupling \(g_R^f\).

Parameters

[in]

f

a lepton or quark

Returns

\(\delta g_R^f\)

Definition at line 1111 of file NPEffectiveGIMR.cpp.

{
    double Qp = p.getCharge();
    double CHf = CHf_diag(p);
    double NPindirect;
    if (FlagMwInput) {
        NPindirect = Qp * sW2_tree
                * ((cW_tree / sW_tree * CHWB + (1.0 + cW2_tree) / 4.0 / sW2_tree * CHD) * v2_over_LambdaNP2 + 0.5 * DeltaGF());
    } else {
        NPindirect = -Qp * sW2_tree / 4.0 / (cW2_tree - sW2_tree)
                *((4.0 * cW_tree / sW_tree * CHWB + CHD) * v2_over_LambdaNP2 + 2.0 * DeltaGF());
    }
    double NPdirect = -0.5 * CHf*v2_over_LambdaNP2;
    return (NPindirect + NPdirect);
}

gslpp::complex NPEffectiveGIMR::deltaGR_Wff	(	const Particle	pbar,
		const Particle	p
	)		const

New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\).

Parameters

[in]	pbar	a lepton or quark
[in]	p	a lepton or quark

Returns

\(\delta g_{Wff}^{R}\)

Definition at line 1147 of file NPEffectiveGIMR.cpp.

{
    if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
        throw std::runtime_error("NPEffectiveGIMR::deltaGR_Wff(): Not implemented");

    gslpp::complex CHud = CHud_diag(pbar);
    return (0.5 * CHud * v2_over_LambdaNP2);
}

gslpp::complex NPEffectiveGIMR::deltaGR_Wffh	(	const Particle	pbar,
		const Particle	p
	)		const

The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\).

Parameters

[in]	pbar	a lepton or quark
[in]	p	a lepton or quark

Returns

\(\delta g_{WffH}^{R}\)

Definition at line 1239 of file NPEffectiveGIMR.cpp.

{
    if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
        throw std::runtime_error("NPEffectiveGIMR::deltaGR_Wffh(): Not implemented");

    gslpp::complex CHud = CHud_diag(pbar);
    return (sqrt(2.0) * Mz * cW_tree / v() / v() * CHud * v2_over_LambdaNP2);
}

double NPEffectiveGIMR::deltaGR_Zffh

(

const Particle

p

)

const

The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\).

Parameters

[in]

p

a lepton or quark

Returns

\(\delta g_{ZffH}^{R}\)

Definition at line 1256 of file NPEffectiveGIMR.cpp.

{
    double CHf = CHf_diag(p);
    return (-2.0 * Mz / v() / v() * CHf * v2_over_LambdaNP2);
}

double NPEffectiveGIMR::deltaGV_f ( const Particle  p ) const

virtual

New physics contribution to the neutral-current vector coupling \(g_V^f\).

Parameters

[in]

f

a lepton or quark

Returns

\(\delta g_V^f\)

Reimplemented from NPbase.

Definition at line 1082 of file NPEffectiveGIMR.cpp.

{
    return (deltaGL_f(p) + deltaGR_f(p));
}

gslpp::complex NPEffectiveGIMR::f_triangle

(

const double

tau

)

const

Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.

Parameters

[in]

Definition at line 1265 of file NPEffectiveGIMR.cpp.

{
    gslpp::complex tmp;
    if (tau >= 1.0) {
        tmp = asin(1.0 / sqrt(tau));
        return (tmp * tmp);
    } else {
        tmp = log((1.0 + sqrt(1.0 - tau)) / (1.0 - sqrt(1.0 - tau))) - M_PI * gslpp::complex::i();
        return (-0.25 * tmp * tmp);
    }
}

double NPEffectiveGIMR::GammaHbbRatio

(

)

const

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

Returns

\(\Gamma(H\to bb)\)/ \(\Gamma(H\to bb)_{\mathrm{SM}}\)

Definition at line 2185 of file NPEffectiveGIMR.cpp.

{
    double width = 1.0;
    
    width += deltaGammaHbbRatio1();
    
    if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
        width += deltaGammaHbbRatio2();        
        }
    
    return width;
}

double NPEffectiveGIMR::GammaHccRatio

(

)

const

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

Returns

\(\Gamma(H\to cc)\)/ \(\Gamma(H\to cc)_{\mathrm{SM}}\)

Definition at line 2156 of file NPEffectiveGIMR.cpp.

{
    double width = 1.0;

    width += deltaGammaHccRatio1();
    
    if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
        width += deltaGammaHccRatio2();            
        }
    
    return width;
    
}

double NPEffectiveGIMR::GammaHgagaRatio

(

)

const

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

Returns

\(\Gamma(H\to \gamma\gamma)\)/ \(\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}\)

Definition at line 2086 of file NPEffectiveGIMR.cpp.

{
    double width = 1.0;

    width += deltaGammaHgagaRatio1();
    
    if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
        width += deltaGammaHgagaRatio2();            
        }
    
    return width;
    
}

double NPEffectiveGIMR::GammaHggRatio

(

)

const

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

Returns

\(\Gamma(H\to gg)\)/ \(\Gamma(H\to gg)_{\mathrm{SM}}\)

Definition at line 1942 of file NPEffectiveGIMR.cpp.

{
    double width = 1.0;

    width += deltaGammaHggRatio1();
    
    if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
        width += deltaGammaHggRatio2();            
        }
    
    return width;
    
}

double NPEffectiveGIMR::GammaHtautauRatio

(

)

const

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

Returns

\(\Gamma(H\to \tau\tau)\)/ \(\Gamma(H\to \tau\tau)_{\mathrm{SM}}\)

Definition at line 2126 of file NPEffectiveGIMR.cpp.

{
    double width = 1.0;

    width += deltaGammaHtautauRatio1();
    
    if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
        width += deltaGammaHtautauRatio2();            
        }
    
    return width;
    
}

double NPEffectiveGIMR::GammaHWWRatio

(

)

const

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

Returns

\(\Gamma(H\to WW)\)/ \(\Gamma(H\to WW)_{\mathrm{SM}}\)

Definition at line 1977 of file NPEffectiveGIMR.cpp.

{
    double width = 1.0;

    width += deltaGammaHWWRatio1();
    
    if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
        width += deltaGammaHWWRatio2();
        }
    
    return width;
    
}

double NPEffectiveGIMR::GammaHZgaRatio

(

)

const

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

Returns

\(\Gamma(H\to Z\gamma)\)/ \(\Gamma(H\to Z\gamma)_{\mathrm{SM}}\)

Definition at line 2046 of file NPEffectiveGIMR.cpp.

{
    double width = 1.0;

    width += deltaGammaHZgaRatio1();
    
    if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
        width += deltaGammaHZgaRatio2();            
        }
    
    return width;
    
}

double NPEffectiveGIMR::GammaHZZRatio

(

)

const

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

Returns

\(\Gamma(H\to ZZ)\)/ \(\Gamma(H\to ZZ)_{\mathrm{SM}}\)

Definition at line 2011 of file NPEffectiveGIMR.cpp.

{
    double width = 1.0;

    width += deltaGammaHZZRatio1();
    
    if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
        width += deltaGammaHZZRatio2();            
        }
    
    return width;
    
}

double NPEffectiveGIMR::GammaW ( ) const

virtual

The total width of the \(W\) boson, \(\Gamma_W\).

Returns

\(\Gamma_W\) in GeV

Reimplemented from NPbase.

Definition at line 1066 of file NPEffectiveGIMR.cpp.

{
    double G0 = GF * pow(Mw(), 3.0) / 6.0 / sqrt(2.0) / M_PI;
    double GammaW_tree = (3.0 + 2.0 * Nc) * G0;

    if (FlagMwInput)
        throw std::runtime_error("Write codes in NPEffectiveGIMR::GammaW()!");
    else
        return (trueSM.GammaW()
            - 3.0 * GammaW_tree / 4.0 / (cW2_tree - sW2_tree)
            *(4.0 * sW_tree * cW_tree * CHWB * v2_over_LambdaNP2
            + cW2_tree * CHD * v2_over_LambdaNP2
            + 2.0 * (1.0 + cW2_tree) / 3.0 * DeltaGF())
            + 2.0 * GammaW_tree / 3.0 * (CHL3_11 + CHQ3_11 + CHQ3_22) * v2_over_LambdaNP2);
}

double NPEffectiveGIMR::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 1627 of file NPEffectiveGIMR.cpp.

{
    double mu = 1.0;

    mu += -4.243 * deltaGL_f(leptons[DOWN])
        +3.723 * deltaGR_f(leptons[DOWN])
        +2690.94  * deltaG1_hZZ()
        -1951.83  * deltaG2_hZZ()
        +0.059  * deltaG3_hZZ()
        +126.418  * deltaG1_hZA()
        -160.3  * deltaG2_hZA()
        -4179.8  * deltaGL_Zffh(leptons[DOWN])
        +3668.  * deltaGR_Zffh(leptons[DOWN]);
        
    if (FlagQuadraticTerms) {
        //Add contributions that are quadratic in the effective coefficients
        //(Only valid under the assumptions of one dim 6 operator at a time)
        mu += +7.966 * pow(deltaGL_f(leptons[DOWN]),2.0)
            +7.966 * pow(deltaGR_f(leptons[DOWN]),2.0)
            +1841343.  * pow(deltaG1_hZZ(),2.0)
            +952412.  * pow(deltaG2_hZZ(),2.0)
            +0.001  * pow(deltaG3_hZZ(),2.0)
            +961714.  * pow(deltaG1_hZA(),2.0)
            +1520521.  * pow(deltaG2_hZA(),2.0)
            +7731703.  * pow(deltaGL_Zffh(leptons[DOWN]),2.0)
            +7731703.  * pow(deltaGR_Zffh(leptons[DOWN]),2.0);
        }
    
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return mu;
}

double NPEffectiveGIMR::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 1282 of file NPEffectiveGIMR.cpp.

{
    double m_t = mtpole;
    //doulbe m_t = quarks[TOP].getMass();
    //double m_b = quarks[BOTTOM].getMass();

    gslpp::complex dKappa_t = deltaG_hff(quarks[TOP]) / (-m_t / v());
    //gslpp::complex dKappa_b = deltaG_hff(quarks[BOTTOM]) / (-m_b / v());

    /* L_eff = G_eff_t_SM*hGG */
    gslpp::complex G_eff_t_SM = AlsMz / 16.0 / M_PI / v() * AH_f(4.0 * m_t * m_t / mHl / mHl);

    //double sigma_tt_SM = trueSM.computeSigmaggH_tt(sqrt_s);
    //double sigma_bb_SM = trueSM.computeSigmaggH_bb(sqrt_s);
    //double sigma_tb_SM = trueSM.computeSigmaggH_tb(sqrt_s);
    //gslpp::complex tmp = (2.0 * dKappa_t * sigma_tt_SM
    //        + 2.0 * dKappa_b * sigma_bb_SM
    //        + (dKappa_t + dKappa_b) * sigma_tb_SM)
    //        / (sigma_tt_SM + sigma_bb_SM + sigma_tb_SM);
    gslpp::complex tmp = 2.0 * dKappa_t;

    gslpp::complex tmp2 = 2.0 * CHG / v() * v2_over_LambdaNP2 / G_eff_t_SM;
    
    double mu = (1.0 + tmp.real() + tmp2.real());
    
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return mu;
}

double NPEffectiveGIMR::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 1732 of file NPEffectiveGIMR.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));
    
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return mu;
} 

double NPEffectiveGIMR::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 1688 of file NPEffectiveGIMR.cpp.

{
    double mu = 1.0;
    if (sqrt_s == 1.96) {
        mu += -2.863 * (1. + ettH2_Htt ) * deltaG_hff(quarks[TOP]).real()
            +1737.35 * (1. + ettH2_Hgg ) * deltaG_hgg();
        
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
            mu += +2.036 * pow(deltaG_hff(quarks[TOP]).real(),2.0)
                +885586. * pow(deltaG_hgg(),2.0);            
        }
        
    } else if (sqrt_s == 7.0) {
        mu += -2.861 * (1. + ettH78_Htt ) * deltaG_hff(quarks[TOP]).real()
            +2583.3 * (1. + ettH78_Hgg ) * deltaG_hgg();
        
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
            mu += +2.073 * pow(deltaG_hff(quarks[TOP]).real(),2.0)
                +3909554. * pow(deltaG_hgg(),2.0);
        }
        
    } else if (sqrt_s == 8.0) {
        mu += -2.861 * (1. + ettH78_Htt ) * deltaG_hff(quarks[TOP]).real()
            +2636.88 * (1. + ettH78_Hgg ) * deltaG_hgg();
        
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
            mu += +1.963 * pow(deltaG_hff(quarks[TOP]).real(),2.0)
                +4367338. * pow(deltaG_hgg(),2.0);
        }
        
    } else
        throw std::runtime_error("Bad argument in NPEffectiveGIMR::muttH()");

    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return mu;
}

double NPEffectiveGIMR::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 1312 of file NPEffectiveGIMR.cpp.

{
    double mu = 1.0;
    if (sqrt_s == 1.96) {
        mu +=  +1.123 * (1. + eVBF2_ZuL ) * deltaGL_f(quarks[UP])
                -0.531 * (1. + eVBF2_ZuR ) * deltaGR_f(quarks[UP])
                -0.705 * (1. + eVBF2_ZdL ) * deltaGL_f(quarks[DOWN])
                +0.136 * (1. + eVBF2_ZdR ) * deltaGR_f(quarks[DOWN])
            +2.662 * (1. + eVBF2_Wud ) * deltaGL_Wff(quarks[UP],quarks[DOWN]).real()
                -1407.72 * (1. + eVBF2_HWud ) * deltaGL_Wffh(quarks[UP], quarks[DOWN]).real()
                +14928.1 * (1. + eVBF2_Hgg ) * deltaG_hgg()
                -12.451 * (1. + eVBF2_HAA ) * deltaG_hAA()
                -21.274 * (1. + eVBF2_HZA1 ) * deltaG1_hZA()
                +45.617 * (1. + eVBF2_HZA2 ) * deltaG2_hZA()
                -84.016 * (1. + eVBF2_HWW1 ) * deltaG1_hWW()
                +390.524 * (1. + eVBF2_HWW2 ) * deltaG2_hWW()
                +0.026 * (1. + eVBF2_HWW3 ) * deltaG3_hWW()
                -45.832 * (1. + eVBF2_HZZ1 ) * deltaG1_hZZ()
                +88.358 * (1. + eVBF2_HZZ2 ) * deltaG2_hZZ()
                +0.012 * (1. + eVBF2_HZZ3 ) * deltaG3_hZZ()
                -129.338 * (1. + eVBF2_HZuL ) * deltaGL_Zffh(quarks[UP])
                +84.325 * (1. + eVBF2_HZuR ) * deltaGR_Zffh(quarks[UP])
                +164.195 * (1. + eVBF2_HZdL ) * deltaGL_Zffh(quarks[DOWN])
                -32.751 * (1. + eVBF2_HZdR ) * deltaGR_Zffh(quarks[DOWN]);
        
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
            mu +=  +2.478 * pow(deltaGL_f(quarks[UP]),2.0)
                +1.878 * pow(deltaGR_f(quarks[UP]),2.0)
                +1.214 * pow(deltaGL_f(quarks[DOWN]),2.0)
                +0.898 * pow(deltaGR_f(quarks[DOWN]),2.0)
            +2.659 * pow(deltaGL_Wff(quarks[UP],quarks[DOWN]).real(),2.0)
                +1917816. * pow(deltaGL_Wffh(quarks[UP], quarks[DOWN]).real(),2.0)
                +524312994. * pow(deltaG_hgg(),2.0)
                +831253. * pow(deltaG_hAA(),2.0)
                +151140. * pow(deltaG1_hZA(),2.0)
                +58067.7 * pow(deltaG2_hZA(),2.0)
                +106835. * pow(deltaG1_hWW(),2.0)
                +219369. * pow(deltaG2_hWW(),2.0)
                +145840. * pow(deltaG1_hZZ(),2.0)
                +66461.2 * pow(deltaG2_hZZ(),2.0)
                +1608277. * pow(deltaGL_Zffh(quarks[UP]),2.0)
                +1449825. * pow(deltaGR_Zffh(quarks[UP]),2.0)
                +409700. * pow(deltaGL_Zffh(quarks[DOWN]),2.0)
                +385965. * pow(deltaGR_Zffh(quarks[DOWN]),2.0);            
        }
        
    } else if (sqrt_s == 7.0) {
        mu +=  +1.188 * (1. + eVBF78_ZuL ) * deltaGL_f(quarks[UP])
                -0.536 * (1. + eVBF78_ZuR ) * deltaGR_f(quarks[UP])
                -0.976 * (1. + eVBF78_ZdL ) * deltaGL_f(quarks[DOWN])
                +0.179 * (1. + eVBF78_ZdR ) * deltaGR_f(quarks[DOWN])
            +2.592 * (1. + eVBF78_Wud ) * deltaGL_Wff(quarks[UP],quarks[DOWN]).real()
                -1826.63 * (1. + eVBF78_HWud ) * deltaGL_Wffh(quarks[UP], quarks[DOWN]).real()
                +14265.8 * (1. + eVBF78_Hgg ) * deltaG_hgg()
                -40.051 * (1. + eVBF78_HAA ) * deltaG_hAA()
                -42.43 * (1. + eVBF78_HZA1 ) * deltaG1_hZA()
                +88.972 * (1. + eVBF78_HZA2 ) * deltaG2_hZA()
                -108.107 * (1. + eVBF78_HWW1 ) * deltaG1_hWW()
                +547.508 * (1. + eVBF78_HWW2 ) * deltaG2_hWW()
                +0.026 * (1. + eVBF78_HWW3 ) * deltaG3_hWW()
                -67.672 * (1. + eVBF78_HZZ1 ) * deltaG1_hZZ()
                +168.86 * (1. + eVBF78_HZZ2 ) * deltaG2_hZZ()
                +0.014 * (1. + eVBF78_HZZ3 ) * deltaG3_hZZ()
                -466.198 * (1. + eVBF78_HZuL ) * deltaGL_Zffh(quarks[UP])
                +211.308 * (1. + eVBF78_HZuR ) * deltaGR_Zffh(quarks[UP])
                +374.597 * (1. + eVBF78_HZdL ) * deltaGL_Zffh(quarks[DOWN])
                -69.916 * (1. + eVBF78_HZdR ) * deltaGR_Zffh(quarks[DOWN]);
        
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
            mu +=  +2.534 * pow(deltaGL_f(quarks[UP]),2.0)
                +1.9 * pow(deltaGR_f(quarks[UP]),2.0)
                +1.695 * pow(deltaGL_f(quarks[DOWN]),2.0)
                +1.177 * pow(deltaGR_f(quarks[DOWN]),2.0)
            +2.608 * pow(deltaGL_Wff(quarks[UP],quarks[DOWN]).real(),2.0)
                +2862580. * pow(deltaGL_Wffh(quarks[UP], quarks[DOWN]).real(),2.0)
                +519301209. * pow(deltaG_hgg(),2.0)
                +777159. * pow(deltaG_hAA(),2.0)
                +206157. * pow(deltaG1_hZA(),2.0)
                +94511.2 * pow(deltaG2_hZA(),2.0)
                +174828. * pow(deltaG1_hWW(),2.0)
                +414624. * pow(deltaG2_hWW(),2.0)
                +209132. * pow(deltaG1_hZZ(),2.0)
                +120250. * pow(deltaG2_hZZ(),2.0)
                +1311032. * pow(deltaGL_Zffh(quarks[UP]),2.0)
                +1130789. * pow(deltaGR_Zffh(quarks[UP]),2.0)
                +757088. * pow(deltaGL_Zffh(quarks[DOWN]),2.0)
                +651756. * pow(deltaGR_Zffh(quarks[DOWN]),2.0);            
        }
        
    } else if (sqrt_s == 8.0) {
        mu +=  +1.179 * (1. + eVBF78_ZuL ) * deltaGL_f(quarks[UP])
                -0.532 * (1. + eVBF78_ZuR ) * deltaGR_f(quarks[UP])
                -0.984 * (1. + eVBF78_ZdL ) * deltaGL_f(quarks[DOWN])
                +0.181 * (1. + eVBF78_ZdR ) * deltaGR_f(quarks[DOWN])
                +2.591 * (1. + eVBF78_Wud ) * deltaGL_Wff(quarks[UP],quarks[DOWN]).real()
                -1858.03 * (1. + eVBF78_HWud ) * deltaGL_Wffh(quarks[UP], quarks[DOWN]).real()
                +14247.4 * (1. + eVBF78_Hgg ) * deltaG_hgg()
                -40.46 * (1. + eVBF78_HAA ) * deltaG_hAA()
                -41.713 * (1. + eVBF78_HZA1 ) * deltaG1_hZA()
                +90.462 * (1. + eVBF78_HZA2 ) * deltaG2_hZA()
                -106.576 * (1. + eVBF78_HWW1 ) * deltaG1_hWW()
                +562.98 * (1. + eVBF78_HWW2 ) * deltaG2_hWW()
                +0.026 * (1. + eVBF78_HWW3 ) * deltaG3_hWW()
                -67.57 * (1. + eVBF78_HZZ1 ) * deltaG1_hZZ()
                +174.474 * (1. + eVBF78_HZZ2 ) * deltaG2_hZZ()
                +0.014 * (1. + eVBF78_HZZ3 ) * deltaG3_hZZ()
                -472.887 * (1. + eVBF78_HZuL ) * deltaGL_Zffh(quarks[UP])
                +214.739 * (1. + eVBF78_HZuR ) * deltaGR_Zffh(quarks[UP])
                +386.582 * (1. + eVBF78_HZdL ) * deltaGL_Zffh(quarks[DOWN])
                -72.228 * (1. + eVBF78_HZdR ) * deltaGR_Zffh(quarks[DOWN]);
        
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
            mu +=  +2.503 * pow(deltaGL_f(quarks[UP]),2.0)
                +1.877 * pow(deltaGR_f(quarks[UP]),2.0)
                +1.712 * pow(deltaGL_f(quarks[DOWN]),2.0)
                +1.191 * pow(deltaGR_f(quarks[DOWN]),2.0)
            +2.606 * pow(deltaGL_Wff(quarks[UP],quarks[DOWN]).real(),2.0)
                +3057041. * pow(deltaGL_Wffh(quarks[UP], quarks[DOWN]).real(),2.0)
                +517064803. * pow(deltaG_hgg(),2.0)
                +766750. * pow(deltaG_hAA(),2.0)
                +207500. * pow(deltaG1_hZA(),2.0)
                +101779. * pow(deltaG2_hZA(),2.0)
                +177714. * pow(deltaG1_hWW(),2.0)
                +454117. * pow(deltaG2_hWW(),2.0)
                +210212. * pow(deltaG1_hZZ(),2.0)
                +131594. * pow(deltaG2_hZZ(),2.0)
                +1399281. * pow(deltaGL_Zffh(quarks[UP]),2.0)
                +1231240. * pow(deltaGR_Zffh(quarks[UP]),2.0)
                +820259. * pow(deltaGL_Zffh(quarks[DOWN]),2.0)
                +713820. * pow(deltaGR_Zffh(quarks[DOWN]),2.0);            
        }
        
    } else
        throw std::runtime_error("Bad argument in NPEffectiveGIMR::muVBF()");

    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return mu;
}

double NPEffectiveGIMR::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 1673 of file NPEffectiveGIMR.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));
    
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return mu;
}

double NPEffectiveGIMR::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 1660 of file NPEffectiveGIMR.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));
    
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return mu;
}

double NPEffectiveGIMR::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 1458 of file NPEffectiveGIMR.cpp.

{
    double mu = 1.0;
    if (sqrt_s == 1.96) {
        mu += +2.032 * (1. + eWH2_Wud ) * deltaGL_Wff(quarks[UP], quarks[DOWN]).real()
                +1738.87 * (1. + eWH2_HWW1 ) * deltaG1_hWW()
                -3432.64 * (1. + eWH2_HWW2 ) * deltaG2_hWW()
                +0.039 * (1. + eWH2_HWW3 ) * deltaG3_hWW()
                +6523.35 * (1. + eWH2_HWud ) * deltaGL_Wffh(quarks[UP], quarks[DOWN]).real();
        
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
            mu += +1.042 * pow(deltaGL_Wff(quarks[UP], quarks[DOWN]).real(),2.0)
                +1075949.  * pow(deltaG1_hWW(),2.0)
                +3978950.  * pow(deltaG2_hWW(),2.0)
                +15887131. * pow(deltaGL_Wffh(quarks[UP], quarks[DOWN]).real(),2.0);
        }
        
    } else if (sqrt_s == 7.0) {
        mu += +1.979 * (1. + eWH78_Wud ) * deltaGL_Wff(quarks[UP], quarks[DOWN]).real()
                +1777.77 * (1. + eWH78_HWW1 ) * deltaG1_hWW()
                -3890.65 * (1. + eWH78_HWW2 ) * deltaG2_hWW()
                +0.039 * (1. + eWH78_HWW3 ) * deltaG3_hWW()
                +7344.73 * (1. + eWH78_HWud ) * deltaGL_Wffh(quarks[UP], quarks[DOWN]).real();
        
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
        mu += +1.015 * pow(deltaGL_Wff(quarks[UP], quarks[DOWN]).real(),2.0)
                +1294405.  * pow(deltaG1_hWW(),2.0)
                +7356224.  * pow(deltaG2_hWW(),2.0)
                +31355627. * pow(deltaGL_Wffh(quarks[UP], quarks[DOWN]).real(),2.0);
        }
        
    } else if (sqrt_s == 8.0) {
        mu += +1.978 * (1. + eWH78_Wud ) * deltaGL_Wff(quarks[UP], quarks[DOWN]).real()
                +1784.47 * (1. + eWH78_HWW1 ) * deltaG1_hWW()
                -3967.38 * (1. + eWH78_HWW2 ) * deltaG2_hWW()
                +0.039 * (1. + eWH78_HWW3 ) * deltaG3_hWW()
                +7507.02 * (1. + eWH78_HWud ) * deltaGL_Wffh(quarks[UP], quarks[DOWN]).real();
        
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
            mu += +1.016 * pow(deltaGL_Wff(quarks[UP], quarks[DOWN]).real(),2.0)
                +1331512.  * pow(deltaG1_hWW(),2.0)
                +8168916.  * pow(deltaG2_hWW(),2.0)
                +35201222. * pow(deltaGL_Wffh(quarks[UP], quarks[DOWN]).real(),2.0);
        }
        
    } else
        throw std::runtime_error("Bad argument in NPEffectiveGIMR::muWH()");

    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return mu;
}

double NPEffectiveGIMR::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 1517 of file NPEffectiveGIMR.cpp.

{
    double mu = 1.0;
    if (sqrt_s == 1.96) {
        mu += +3.529 * (1. + eZH2_ZuL ) * deltaGL_f(quarks[UP])
                -1.598 * (1. + eZH2_ZuR ) * deltaGR_f(quarks[UP])
                -1.229 * (1. + eZH2_ZdL ) * deltaGL_f(quarks[DOWN])
                +0.227 * (1. + eZH2_ZdR ) * deltaGR_f(quarks[DOWN])
                +3215.38 * (1. + eZH2_HZZ1 ) * deltaG1_hZZ()
                -2922.42 * (1. + eZH2_HZZ2 ) * deltaG2_hZZ()
                +0.059 * (1. + eZH2_HZZ3 ) * deltaG3_hZZ()
                +495.399 * (1. + eZH2_HZA1 ) * deltaG1_hZA()
                -838.743 * (1. + eZH2_HZA2 ) * deltaG2_hZA()
                +5931.99 * (1. + eZH2_HZuL ) * deltaGL_Zffh(quarks[UP])
                -2684.23 * (1. + eZH2_HZuR ) * deltaGR_Zffh(quarks[UP])
                -1878.46 * (1. + eZH2_HZdL ) * deltaGL_Zffh(quarks[DOWN])
                +346.694 * (1. + eZH2_HZdR ) * deltaGR_Zffh(quarks[DOWN]);
        
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
            mu += +5.126 * pow(deltaGL_f(quarks[UP]),2.0)
                +5.126 * pow(deltaGR_f(quarks[UP]),2.0)
                +1.456 * pow(deltaGL_f(quarks[DOWN]),2.0)
                +1.454 * pow(deltaGR_f(quarks[DOWN]),2.0)
                +3525123.  * pow(deltaG1_hZZ(),2.0)
                +2844179.  * pow(deltaG2_hZZ(),2.0)
                +0.001  * pow(deltaG3_hZZ(),2.0)
                +662397.  * pow(deltaG1_hZA(),2.0)
                +2006248.  * pow(deltaG2_hZA(),2.0)
                +21799545.  * pow(deltaGL_Zffh(quarks[UP]),2.0)
                +21795795.  * pow(deltaGR_Zffh(quarks[UP]),2.0)
                +4723149.  * pow(deltaGL_Zffh(quarks[DOWN]),2.0)
                +4725123.  * pow(deltaGR_Zffh(quarks[DOWN]),2.0);
        }
        
    } else if (sqrt_s == 7.0) {
        mu += +2.583 * (1. + eZH78_ZuL ) * deltaGL_f(quarks[UP])
                -1.17 * (1. + eZH78_ZuR ) * deltaGR_f(quarks[UP])
                -2.127 * (1. + eZH78_ZdL ) * deltaGL_f(quarks[DOWN])
                +0.392 * (1. + eZH78_ZdR ) * deltaGR_f(quarks[DOWN])
                +3269.53 * (1. + eZH78_HZZ1 ) * deltaG1_hZZ()
                -3201.65 * (1. + eZH78_HZZ2 ) * deltaG2_hZZ()
                +0.059 * (1. + eZH78_HZZ3 ) * deltaG3_hZZ()
                +473.267 * (1. + eZH78_HZA1 ) * deltaG1_hZA()
                -873.421 * (1. + eZH78_HZA2 ) * deltaG2_hZA()
                +4763.44 * (1. + eZH78_HZuL ) * deltaGL_Zffh(quarks[UP])
                -2156.99 * (1. + eZH78_HZuR ) * deltaGR_Zffh(quarks[UP])
                -3853.2 * (1. + eZH78_HZdL ) * deltaGL_Zffh(quarks[DOWN])
                +712.124 * (1. + eZH78_HZdR ) * deltaGR_Zffh(quarks[DOWN]);
        
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
            mu +=  +3.752 * pow(deltaGL_f(quarks[UP]),2.0)
                +3.753 * pow(deltaGR_f(quarks[UP]),2.0)
                +2.519 * pow(deltaGL_f(quarks[DOWN]),2.0)
                +2.517 * pow(deltaGR_f(quarks[DOWN]),2.0)
                +4051505.  * pow(deltaG1_hZZ(),2.0)
                +4597749.  * pow(deltaG2_hZZ(),2.0)
                +0.001  * pow(deltaG3_hZZ(),2.0)
                +610510.  * pow(deltaG1_hZA(),2.0)
                +2766996.  * pow(deltaG2_hZA(),2.0)
                +27425400.  * pow(deltaGL_Zffh(quarks[UP]),2.0)
                +27416894.  * pow(deltaGR_Zffh(quarks[UP]),2.0)
                +17043782.  * pow(deltaGL_Zffh(quarks[DOWN]),2.0)
                +17039528.  * pow(deltaGR_Zffh(quarks[DOWN]),2.0);
        }
        
    } else if (sqrt_s == 8.0) {
        mu += +2.569 * (1. + eZH78_ZuL ) * deltaGL_f(quarks[UP])
                -1.163 * (1. + eZH78_ZuR ) * deltaGR_f(quarks[UP])
                -2.14 * (1. + eZH78_ZdL ) * deltaGL_f(quarks[DOWN])
                +0.395 * (1. + eZH78_ZdR ) * deltaGR_f(quarks[DOWN])
                +3282.79 * (1. + eZH78_HZZ1 ) * deltaG1_hZZ()
                -3262.46 * (1. + eZH78_HZZ2 ) * deltaG2_hZZ()
                +0.059 * (1. + eZH78_HZZ3 ) * deltaG3_hZZ()
                +475.044 * (1. + eZH78_HZA1 ) * deltaG1_hZA()
                -892.243 * (1. + eZH78_HZA2 ) * deltaG2_hZA()
                +4847.78 * (1. + eZH78_HZuL ) * deltaGL_Zffh(quarks[UP])
                -2193.61 * (1. + eZH78_HZuR ) * deltaGR_Zffh(quarks[UP])
                -3960.46 * (1. + eZH78_HZdL ) * deltaGL_Zffh(quarks[DOWN])
                +731.438 * (1. + eZH78_HZdR ) * deltaGR_Zffh(quarks[DOWN]);
        
        if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
            //(Only valid under the assumptions of one dim 6 operator at a time)
            mu += +3.732 * pow(deltaGL_f(quarks[UP]),2.0)
                +3.736 * pow(deltaGR_f(quarks[UP]),2.0)
                +2.535 * pow(deltaGL_f(quarks[DOWN]),2.0)
                +2.536 * pow(deltaGR_f(quarks[DOWN]),2.0)
                +4164701.  * pow(deltaG1_hZZ(),2.0)
                +5067698.  * pow(deltaG2_hZZ(),2.0)
                +0.001  * pow(deltaG3_hZZ(),2.0)
                +627966.  * pow(deltaG1_hZA(),2.0)
                +3087745.  * pow(deltaG2_hZA(),2.0)
                +30566228.  * pow(deltaGL_Zffh(quarks[UP]),2.0)
                +30559313.  * pow(deltaGR_Zffh(quarks[UP]),2.0)
                +19107837.  * pow(deltaGL_Zffh(quarks[DOWN]),2.0)
                +19109134.  * pow(deltaGR_Zffh(quarks[DOWN]),2.0);
        }
        
    } else
        throw std::runtime_error("Bad argument in NPEffectiveGIMR::muZH()");

    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return mu;
}

double NPEffectiveGIMR::Mw ( ) const

virtual

The mass of the \(W\) boson, \(M_W\).

Returns

\(M_W\) in GeV

Reimplemented from NPbase.

Definition at line 1055 of file NPEffectiveGIMR.cpp.

{
    if (FlagMwInput)
        return MwInput;
    else
        return (trueSM.Mw() - Mw_tree() / 4.0 / (cW2_tree - sW2_tree)
            *(4.0 * sW_tree * cW_tree * CHWB * v2_over_LambdaNP2
            + cW2_tree * CHD * v2_over_LambdaNP2
            + 2.0 * sW2_tree * DeltaGF()));
}

double NPEffectiveGIMR::obliqueS ( ) const

virtual

The oblique parameter \(S\).

Returns

the value of \(S\)

Reimplemented from NPbase.

Definition at line 1040 of file NPEffectiveGIMR.cpp.

{
    return (4.0 * sW2_tree * cW_tree * CHWB / alphaMz() * v2_over_LambdaNP2);
}

double NPEffectiveGIMR::obliqueT ( ) const

virtual

The oblique parameter \(T\).

Returns

the value of \(T\)

Reimplemented from NPbase.

Definition at line 1045 of file NPEffectiveGIMR.cpp.

{
    return (-CHD / 2.0 / alphaMz() * v2_over_LambdaNP2);
}

double NPEffectiveGIMR::obliqueU ( ) const

virtual

The oblique parameter \(U\).

Returns

the value of \(U\)

Reimplemented from NPbase.

Definition at line 1050 of file NPEffectiveGIMR.cpp.

{
    return 0.0;
}

bool NPEffectiveGIMR::PostUpdate ( )

virtual

The post-update method for NPEffectiveGIMR.

This method runs all the procedures that are need to be executed after the model is successfully updated.

Returns

a boolean that is true if the execution is successful

Reimplemented from NPbase.

Definition at line 312 of file NPEffectiveGIMR.cpp.

{
    if (!NPbase::PostUpdate()) return (false);

    LambdaNP2 = Lambda_NP * Lambda_NP;
    v2_over_LambdaNP2 = v() * v() / LambdaNP2;
    if (FlagMwInput)
        cW_tree = MwInput / Mz;
    else
        cW_tree = Mw_tree() / Mz;
    cW2_tree = cW_tree * cW_tree;
    sW2_tree = 1.0 - cW2_tree;
    sW_tree = sqrt(sW2_tree);

    delta_ZZ = (cW2_tree * CHW + sW2_tree * CHB + sW_tree * cW_tree * CHWB) * v2_over_LambdaNP2;
    delta_AA = (sW2_tree * CHW + cW2_tree * CHB - sW_tree * cW_tree * CHWB) * v2_over_LambdaNP2;
    delta_AZ = 2.0 * sW_tree * cW_tree * (CHW - CHB) * v2_over_LambdaNP2
            - (cW2_tree - sW2_tree) * CHWB * v2_over_LambdaNP2;
    delta_h = (-CHD / 4.0 + CHbox) * v2_over_LambdaNP2;

    return (true);
}

bool NPEffectiveGIMR::setFlag ( const std::string  name, const bool  value  )

virtual

A method to set a flag of NPEffectiveGIMR.

Parameters

[in]	name	name of a model flag
[in]	value	the boolean to be assigned to the flag specified by name

Returns

a boolean that is true if the execution is successful

Reimplemented from StandardModel.

Definition at line 911 of file NPEffectiveGIMR.cpp.

{
    bool res = false;
    if (name.compare("MwInput") == 0) {
        FlagMwInput = value;
        res = true;
    } else if (name.compare("QuadraticTerms") == 0) {
        FlagQuadraticTerms = value;
        res = true;
    } else
        res = NPbase::setFlag(name, value);

    return (res);
}

void NPEffectiveGIMR::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 335 of file NPEffectiveGIMR.cpp.

{
    if (name.compare("CHG") == 0)
        CHG = value;
    else if (name.compare("CHW") == 0)
        CHW = value;
    else if (name.compare("CHB") == 0)
        CHB = value;
    else if (name.compare("CHWB") == 0)
        CHWB = value;
    else if (name.compare("CHD") == 0)
        CHD = value;
    else if (name.compare("CHbox") == 0)
        CHbox = value;
    else if (name.compare("CH") == 0)
        CH = value;
    else if (name.compare("CHL1_11") == 0)
        CHL1_11 = value;
    else if (name.compare("CHL1_12r") == 0)
        CHL1_12r = value;
    else if (name.compare("CHL1_13r") == 0)
        CHL1_13r = value;
    else if (name.compare("CHL1_22") == 0)
        CHL1_22 = value;
    else if (name.compare("CHL1_23r") == 0)
        CHL1_23r = value;
    else if (name.compare("CHL1_33") == 0)
        CHL1_33 = value;
    else if (name.compare("CHL1_12i") == 0)
        CHL1_12i = value;
    else if (name.compare("CHL1_13i") == 0)
        CHL1_13i = value;
    else if (name.compare("CHL1_23i") == 0)
        CHL1_23i = value;
    else if (name.compare("CHL1") == 0) {
        CHL1_11 = value;
        CHL1_12r = 0.0;
        CHL1_13r = 0.0;
        CHL1_22 = value;
        CHL1_23r = 0.0;
        CHL1_33 = value;
        CHL1_12i = 0.0;
        CHL1_13i = 0.0;
        CHL1_23i = 0.0;
    } else if (name.compare("CHL3_11") == 0)
        CHL3_11 = value;
    else if (name.compare("CHL3_12r") == 0)
        CHL3_12r = value;
    else if (name.compare("CHL3_13r") == 0)
        CHL3_13r = value;
    else if (name.compare("CHL3_22") == 0)
        CHL3_22 = value;
    else if (name.compare("CHL3_23r") == 0)
        CHL3_23r = value;
    else if (name.compare("CHL3_33") == 0)
        CHL3_33 = value;
    else if (name.compare("CHL3_12i") == 0)
        CHL3_12i = value;
    else if (name.compare("CHL3_13i") == 0)
        CHL3_13i = value;
    else if (name.compare("CHL3_23i") == 0)
        CHL3_23i = value;
    else if (name.compare("CHL3") == 0) {
        CHL3_11 = value;
        CHL3_12r = 0.0;
        CHL3_13r = 0.0;
        CHL3_22 = value;
        CHL3_23r = 0.0;
        CHL3_33 = value;
        CHL3_12i = 0.0;
        CHL3_13i = 0.0;
        CHL3_23i = 0.0;
    } else if (name.compare("CHe_11") == 0)
        CHe_11 = value;
    else if (name.compare("CHe_12r") == 0)
        CHe_12r = value;
    else if (name.compare("CHe_13r") == 0)
        CHe_13r = value;
    else if (name.compare("CHe_22") == 0)
        CHe_22 = value;
    else if (name.compare("CHe_23r") == 0)
        CHe_23r = value;
    else if (name.compare("CHe_33") == 0)
        CHe_33 = value;
    else if (name.compare("CHe_12i") == 0)
        CHe_12i = value;
    else if (name.compare("CHe_13i") == 0)
        CHe_13i = value;
    else if (name.compare("CHe_23i") == 0)
        CHe_23i = value;
    else if (name.compare("CHe") == 0) {
        CHe_11 = value;
        CHe_12r = 0.0;
        CHe_13r = 0.0;
        CHe_22 = value;
        CHe_23r = 0.0;
        CHe_33 = value;
        CHe_12i = 0.0;
        CHe_13i = 0.0;
        CHe_23i = 0.0;
    } else if (name.compare("CHQ1_11") == 0)
        CHQ1_11 = value;
    else if (name.compare("CHQ1_12r") == 0)
        CHQ1_12r = value;
    else if (name.compare("CHQ1_13r") == 0)
        CHQ1_13r = value;
    else if (name.compare("CHQ1_22") == 0)
        CHQ1_22 = value;
    else if (name.compare("CHQ1_23r") == 0)
        CHQ1_23r = value;
    else if (name.compare("CHQ1_33") == 0)
        CHQ1_33 = value;
    else if (name.compare("CHQ1_12i") == 0)
        CHQ1_12i = value;
    else if (name.compare("CHQ1_13i") == 0)
        CHQ1_13i = value;
    else if (name.compare("CHQ1_23i") == 0)
        CHQ1_23i = value;
    else if (name.compare("CHQ1") == 0) {
        CHQ1_11 = value;
        CHQ1_12r = 0.0;
        CHQ1_13r = 0.0;
        CHQ1_22 = value;
        CHQ1_23r = 0.0;
        CHQ1_33 = value;
        CHQ1_12i = 0.0;
        CHQ1_13i = 0.0;
        CHQ1_23i = 0.0;
    } else if (name.compare("CHQ3_11") == 0)
        CHQ3_11 = value;
    else if (name.compare("CHQ3_12r") == 0)
        CHQ3_12r = value;
    else if (name.compare("CHQ3_13r") == 0)
        CHQ3_13r = value;
    else if (name.compare("CHQ3_22") == 0)
        CHQ3_22 = value;
    else if (name.compare("CHQ3_23r") == 0)
        CHQ3_23r = value;
    else if (name.compare("CHQ3_33") == 0)
        CHQ3_33 = value;
    else if (name.compare("CHQ3_12i") == 0)
        CHQ3_12i = value;
    else if (name.compare("CHQ3_13i") == 0)
        CHQ3_13i = value;
    else if (name.compare("CHQ3_23i") == 0)
        CHQ3_23i = value;
    else if (name.compare("CHQ3") == 0) {
        CHQ3_11 = value;
        CHQ3_12r = 0.0;
        CHQ3_13r = 0.0;
        CHQ3_22 = value;
        CHQ3_23r = 0.0;
        CHQ3_33 = value;
        CHQ3_12i = 0.0;
        CHQ3_13i = 0.0;
        CHQ3_23i = 0.0;
    } else if (name.compare("CHu_11") == 0)
        CHu_11 = value;
    else if (name.compare("CHu_12r") == 0)
        CHu_12r = value;
    else if (name.compare("CHu_13r") == 0)
        CHu_13r = value;
    else if (name.compare("CHu_22") == 0)
        CHu_22 = value;
    else if (name.compare("CHu_23r") == 0)
        CHu_23r = value;
    else if (name.compare("CHu_33") == 0)
        CHu_33 = value;
    else if (name.compare("CHu_12i") == 0)
        CHu_12i = value;
    else if (name.compare("CHu_13i") == 0)
        CHu_13i = value;
    else if (name.compare("CHu_23i") == 0)
        CHu_23i = value;
    else if (name.compare("CHu") == 0) {
        CHu_11 = value;
        CHu_12r = 0.0;
        CHu_13r = 0.0;
        CHu_22 = value;
        CHu_23r = 0.0;
        CHu_33 = value;
        CHu_12i = 0.0;
        CHu_13i = 0.0;
        CHu_23i = 0.0;
    } else if (name.compare("CHd_11") == 0)
        CHd_11 = value;
    else if (name.compare("CHd_12r") == 0)
        CHd_12r = value;
    else if (name.compare("CHd_13r") == 0)
        CHd_13r = value;
    else if (name.compare("CHd_22") == 0)
        CHd_22 = value;
    else if (name.compare("CHd_23r") == 0)
        CHd_23r = value;
    else if (name.compare("CHd_33") == 0)
        CHd_33 = value;
    else if (name.compare("CHd_12i") == 0)
        CHd_12i = value;
    else if (name.compare("CHd_13i") == 0)
        CHd_13i = value;
    else if (name.compare("CHd_23i") == 0)
        CHd_23i = value;
    else if (name.compare("CHd") == 0) {
        CHd_11 = value;
        CHd_12r = 0.0;
        CHd_13r = 0.0;
        CHd_22 = value;
        CHd_23r = 0.0;
        CHd_33 = value;
        CHd_12i = 0.0;
        CHd_13i = 0.0;
        CHd_23i = 0.0;
    } else if (name.compare("CHud_11r") == 0)
        CHud_11r = value;
    else if (name.compare("CHud_12r") == 0)
        CHud_12r = value;
    else if (name.compare("CHud_13r") == 0)
        CHud_13r = value;
    else if (name.compare("CHud_22r") == 0)
        CHud_22r = value;
    else if (name.compare("CHud_23r") == 0)
        CHud_23r = value;
    else if (name.compare("CHud_33r") == 0)
        CHud_33r = value;
    else if (name.compare("CHud_r") == 0) {
        CHud_11r = value;
        CHud_12r = 0.0;
        CHud_13r = 0.0;
        CHud_22r = value;
        CHud_23r = 0.0;
        CHud_33r = value;
    } else if (name.compare("CHud_11i") == 0)
        CHud_11i = value;
    else if (name.compare("CHud_12i") == 0)
        CHud_12i = value;
    else if (name.compare("CHud_13i") == 0)
        CHud_13i = value;
    else if (name.compare("CHud_22i") == 0)
        CHud_22i = value;
    else if (name.compare("CHud_23i") == 0)
        CHud_23i = value;
    else if (name.compare("CHud_33i") == 0)
        CHud_33i = value;
    else if (name.compare("CHud_i") == 0) {
        CHud_11i = value;
        CHud_12i = 0.0;
        CHud_13i = 0.0;
        CHud_22i = value;
        CHud_23i = 0.0;
        CHud_33i = value;
    } else if (name.compare("CeH_11r") == 0)
        CeH_11r = value;
    else if (name.compare("CeH_12r") == 0)
        CeH_12r = value;
    else if (name.compare("CeH_13r") == 0)
        CeH_13r = value;
    else if (name.compare("CeH_22r") == 0)
        CeH_22r = value;
    else if (name.compare("CeH_23r") == 0)
        CeH_23r = value;
    else if (name.compare("CeH_33r") == 0)
        CeH_33r = value;
    else if (name.compare("CeH_r") == 0) {
        CeH_11r = value;
        CeH_12r = 0.0;
        CeH_13r = 0.0;
        CeH_22r = value;
        CeH_23r = 0.0;
        CeH_33r = value;
    } else if (name.compare("CeH_11i") == 0)
        CeH_11i = value;
    else if (name.compare("CeH_12i") == 0)
        CeH_12i = value;
    else if (name.compare("CeH_13i") == 0)
        CeH_13i = value;
    else if (name.compare("CeH_22i") == 0)
        CeH_22i = value;
    else if (name.compare("CeH_23i") == 0)
        CeH_23i = value;
    else if (name.compare("CeH_33i") == 0)
        CeH_33i = value;
    else if (name.compare("CeH_i") == 0) {
        CeH_11i = value;
        CeH_12i = 0.0;
        CeH_13i = 0.0;
        CeH_22i = value;
        CeH_23i = 0.0;
        CeH_33i = value;
    } else if (name.compare("CuH_11r") == 0)
        CuH_11r = value;
    else if (name.compare("CuH_12r") == 0)
        CuH_12r = value;
    else if (name.compare("CuH_13r") == 0)
        CuH_13r = value;
    else if (name.compare("CuH_22r") == 0)
        CuH_22r = value;
    else if (name.compare("CuH_23r") == 0)
        CuH_23r = value;
    else if (name.compare("CuH_33r") == 0)
        CuH_33r = value;
    else if (name.compare("CuH_r") == 0) {
        CuH_11r = value;
        CuH_12r = 0.0;
        CuH_13r = 0.0;
        CuH_22r = value;
        CuH_23r = 0.0;
        CuH_33r = value;
    } else if (name.compare("CuH_11i") == 0)
        CuH_11i = value;
    else if (name.compare("CuH_12i") == 0)
        CuH_12i = value;
    else if (name.compare("CuH_13i") == 0)
        CuH_13i = value;
    else if (name.compare("CuH_22i") == 0)
        CuH_22i = value;
    else if (name.compare("CuH_23i") == 0)
        CuH_23i = value;
    else if (name.compare("CuH_33i") == 0)
        CuH_33i = value;
    else if (name.compare("CuH_i") == 0) {
        CuH_11i = value;
        CuH_12i = 0.0;
        CuH_13i = 0.0;
        CuH_22i = value;
        CuH_23i = 0.0;
        CuH_33i = value;
    } else if (name.compare("CdH_11r") == 0)
        CdH_11r = value;
    else if (name.compare("CdH_12r") == 0)
        CdH_12r = value;
    else if (name.compare("CdH_13r") == 0)
        CdH_13r = value;
    else if (name.compare("CdH_22r") == 0)
        CdH_22r = value;
    else if (name.compare("CdH_23r") == 0)
        CdH_23r = value;
    else if (name.compare("CdH_33r") == 0)
        CdH_33r = value;
    else if (name.compare("CdH_r") == 0) {
        CdH_11r = value;
        CdH_12r = 0.0;
        CdH_13r = 0.0;
        CdH_22r = value;
        CdH_23r = 0.0;
        CdH_33r = value;
    } else if (name.compare("CdH_11i") == 0)
        CdH_11i = value;
    else if (name.compare("CdH_12i") == 0)
        CdH_12i = value;
    else if (name.compare("CdH_13i") == 0)
        CdH_13i = value;
    else if (name.compare("CdH_22i") == 0)
        CdH_22i = value;
    else if (name.compare("CdH_23i") == 0)
        CdH_23i = value;
    else if (name.compare("CdH_33i") == 0)
        CdH_33i = value;
    else if (name.compare("CdH_i") == 0) {
        CdH_11i = value;
        CdH_12i = 0.0;
        CdH_13i = 0.0;
        CdH_22i = value;
        CdH_23i = 0.0;
        CdH_33i = value;
    } else if (name.compare("CLL_1221") == 0) {
        CLL_1221 = value;
        CLL_2112 = value;
    } else if (name.compare("CLL") == 0) {
        CLL_1221 = value;
        CLL_2112 = value;
    } else if (name.compare("Lambda_NP") == 0) {
        Lambda_NP = value;
    } else if (name.compare("eVBF2_HZZ1") == 0) {
         eVBF2_HZZ1 = value;
    } else if (name.compare("eVBF2_HZZ2") == 0) {
         eVBF2_HZZ2 = value;
    } else if (name.compare("eVBF2_HZZ3") == 0) {
         eVBF2_HZZ3 = value;
    } else if (name.compare("eVBF2_HZA1") == 0) {
         eVBF2_HZA1 = value;
    } else if (name.compare("eVBF2_HZA2") == 0) {
         eVBF2_HZA2 = value;
    } else if (name.compare("eVBF2_HAA") == 0) {
         eVBF2_HAA = value;
    } else if (name.compare("eVBF2_HWW1") == 0) {
         eVBF2_HWW1 = value;
    } else if (name.compare("eVBF2_HWW2") == 0) {
         eVBF2_HWW2 = value;
    } else if (name.compare("eVBF2_HWW3") == 0) {
         eVBF2_HWW3 = value;
    } else if (name.compare("eVBF2_Hgg") == 0) {
         eVBF2_Hgg = value;
    } else if (name.compare("eVBF2_HZuL") == 0) {
         eVBF2_HZuL = value;
    } else if (name.compare("eVBF2_HZuR") == 0) {
         eVBF2_HZuR = value;
    } else if (name.compare("eVBF2_HZdL") == 0) {
         eVBF2_HZdL = value;
    } else if (name.compare("eVBF2_HZdR") == 0) {
         eVBF2_HZdR = value;
    } else if (name.compare("eVBF2_HWud") == 0) {
         eVBF2_HWud = value;
    } else if (name.compare("eVBF2_ZuL") == 0) {
         eVBF2_ZuL = value;
    } else if (name.compare("eVBF2_ZuR") == 0) {
         eVBF2_ZuR = value;
    } else if (name.compare("eVBF2_ZdL") == 0) {
         eVBF2_ZdL = value;
    } else if (name.compare("eVBF2_ZdR") == 0) {
         eVBF2_ZdR = value;
    } else if (name.compare("eVBF2_Wud") == 0) {
         eVBF2_Wud = value;
    } else if (name.compare("eVBF78_HZZ1") == 0) {
         eVBF78_HZZ1 = value;
    } else if (name.compare("eVBF78_HZZ2") == 0) {
         eVBF78_HZZ2 = value;
    } else if (name.compare("eVBF78_HZZ3") == 0) {
         eVBF78_HZZ3 = value;
    } else if (name.compare("eVBF78_HZA1") == 0) {
         eVBF78_HZA1 = value;
    } else if (name.compare("eVBF78_HZA2") == 0) {
         eVBF78_HZA2 = value;
    } else if (name.compare("eVBF78_HAA") == 0) {
         eVBF78_HAA = value;
    } else if (name.compare("eVBF78_HWW1") == 0) {
         eVBF78_HWW1 = value;
    } else if (name.compare("eVBF78_HWW2") == 0) {
         eVBF78_HWW2 = value;
    } else if (name.compare("eVBF78_HWW3") == 0) {
         eVBF78_HWW3 = value;
    } else if (name.compare("eVBF78_Hgg") == 0) {
         eVBF78_Hgg = value;
    } else if (name.compare("eVBF78_HZuL") == 0) {
         eVBF78_HZuL = value;
    } else if (name.compare("eVBF78_HZuR") == 0) {
         eVBF78_HZuR = value;
    } else if (name.compare("eVBF78_HZdL") == 0) {
         eVBF78_HZdL = value;
    } else if (name.compare("eVBF78_HZdR") == 0) {
         eVBF78_HZdR = value;
    } else if (name.compare("eVBF78_HWud") == 0) {
         eVBF78_HWud = value;
    } else if (name.compare("eVBF78_ZuL") == 0) {
         eVBF78_ZuL = value;
    } else if (name.compare("eVBF78_ZuR") == 0) {
         eVBF78_ZuR = value;
    } else if (name.compare("eVBF78_ZdL") == 0) {
         eVBF78_ZdL = value;
    } else if (name.compare("eVBF78_ZdR") == 0) {
         eVBF78_ZdR = value;
    } else if (name.compare("eVBF78_Wud") == 0) {
         eVBF78_Wud = value;
    } else if (name.compare("eWH2_HWW1") == 0) {
         eWH2_HWW1 = value;
    } else if (name.compare("eWH2_HWW2") == 0) {
         eWH2_HWW2 = value;
    } else if (name.compare("eWH2_HWW3") == 0) {
         eWH2_HWW3 = value;
    } else if (name.compare("eWH2_HWud") == 0) {
         eWH2_HWud = value;
    } else if (name.compare("eWH2_Wud") == 0) {
         eWH2_Wud = value;
    } else if (name.compare("eWH78_HWW1") == 0) {
         eWH78_HWW1 = value;
    } else if (name.compare("eWH78_HWW2") == 0) {
         eWH78_HWW2 = value;
    } else if (name.compare("eWH78_HWW3") == 0) {
         eWH78_HWW3 = value;
    } else if (name.compare("eWH78_HWud") == 0) {
         eWH78_HWud = value;
    } else if (name.compare("eWH78_Wud") == 0) {
         eWH78_Wud = value;
    } else if (name.compare("eZH2_HZZ1") == 0) {
         eZH2_HZZ1 = value;
    } else if (name.compare("eZH2_HZZ2") == 0) {
         eZH2_HZZ2 = value;
    } else if (name.compare("eZH2_HZZ3") == 0) {
         eZH2_HZZ3 = value;
    } else if (name.compare("eZH2_HZA1") == 0) {
         eZH2_HZA1 = value;
    } else if (name.compare("eZH2_HZA2") == 0) {
         eZH2_HZA2 = value;
    } else if (name.compare("eZH2_HZuL") == 0) {
         eZH2_HZuL = value;
    } else if (name.compare("eZH2_HZuR") == 0) {
         eZH2_HZuR = value;
    } else if (name.compare("eZH2_HZdL") == 0) {
         eZH2_HZdL = value;
    } else if (name.compare("eZH2_HZdR") == 0) {
         eZH2_HZdR = value;
    } else if (name.compare("eZH2_ZuL") == 0) {
         eZH2_ZuL = value;
    } else if (name.compare("eZH2_ZuR") == 0) {
         eZH2_ZuR = value;
    } else if (name.compare("eZH2_ZdL") == 0) {
         eZH2_ZdL = value;
    } else if (name.compare("eZH2_ZdR") == 0) {
         eZH2_ZdR = value;   
    } else if (name.compare("eZH78_HZZ1") == 0) {
         eZH78_HZZ1 = value;
    } else if (name.compare("eZH78_HZZ2") == 0) {
         eZH78_HZZ2 = value;
    } else if (name.compare("eZH78_HZZ3") == 0) {
         eZH78_HZZ3 = value;
    } else if (name.compare("eZH78_HZA1") == 0) {
         eZH78_HZA1 = value;
    } else if (name.compare("eZH78_HZA2") == 0) {
         eZH78_HZA2 = value;
    } else if (name.compare("eZH78_HZuL") == 0) {
         eZH78_HZuL = value;
    } else if (name.compare("eZH78_HZuR") == 0) {
         eZH78_HZuR = value;
    } else if (name.compare("eZH78_HZdL") == 0) {
         eZH78_HZdL = value;
    } else if (name.compare("eZH78_HZdR") == 0) {
         eZH78_HZdR = value;
    } else if (name.compare("eZH78_ZuL") == 0) {
         eZH78_ZuL = value;
    } else if (name.compare("eZH78_ZuR") == 0) {
         eZH78_ZuR = value;
    } else if (name.compare("eZH78_ZdL") == 0) {
         eZH78_ZdL = value;
    } else if (name.compare("eZH78_ZdR") == 0) {
         eZH78_ZdR = value;     
    } else if (name.compare("ettH2_Htt") == 0) {
         ettH2_Htt = value;
    } else if (name.compare("ettH2_Hgg") == 0) {
         ettH2_Hgg = value;
    } else if (name.compare("ettH78_Htt") == 0) {
         ettH78_Htt = value;
    } else if (name.compare("ettH78_Hgg") == 0) {
         ettH78_Hgg = value;
    } else if (name.compare("MwInput") == 0)
        MwInput = value;
    else
        NPbase::setParameter(name, value);
}

Member Data Documentation

double NPEffectiveGIMR::CdH_11i

protected

The dimension-6 operator coefficient \((C_{DH})_{11}\) (imaginary part).

Definition at line 1102 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CdH_11r

protected

The dimension-6 operator coefficient \((C_{DH})_{11}\) (real part).

Definition at line 1096 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CdH_12i

protected

The dimension-6 operator coefficient \((C_{DH})_{12}\) (imaginary part).

Definition at line 1103 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CdH_12r

protected

The dimension-6 operator coefficient \((C_{DH})_{12}\) (real part).

Definition at line 1097 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CdH_13i

protected

The dimension-6 operator coefficient \((C_{DH})_{13}\) (imaginary part).

Definition at line 1104 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CdH_13r

protected

The dimension-6 operator coefficient \((C_{DH})_{13}\) (real part).

Definition at line 1098 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CdH_22i

protected

The dimension-6 operator coefficient \((C_{DH})_{22}\) (imaginary part).

Definition at line 1105 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CdH_22r

protected

The dimension-6 operator coefficient \((C_{DH})_{22}\) (real part).

Definition at line 1099 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CdH_23i

protected

The dimension-6 operator coefficient \((C_{DH})_{23}\) (imaginary part).

Definition at line 1106 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CdH_23r

protected

The dimension-6 operator coefficient \((C_{DH})_{23}\) (real part).

Definition at line 1100 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CdH_33i

protected

The dimension-6 operator coefficient \((C_{DH})_{33}\) (imaginary part).

Definition at line 1107 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CdH_33r

protected

The dimension-6 operator coefficient \((C_{DH})_{33}\) (real part).

Definition at line 1101 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CeH_11i

protected

The dimension-6 operator coefficient \((C_{EH})_{11}\) (imaginary part).

Definition at line 1078 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CeH_11r

protected

The dimension-6 operator coefficient \((C_{EH})_{11}\) (real part).

Definition at line 1072 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CeH_12i

protected

The dimension-6 operator coefficient \((C_{EH})_{12}\) (imaginary part).

Definition at line 1079 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CeH_12r

protected

The dimension-6 operator coefficient \((C_{EH})_{12}\) (real part).

Definition at line 1073 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CeH_13i

protected

The dimension-6 operator coefficient \((C_{EH})_{13}\) (imaginary part).

Definition at line 1080 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CeH_13r

protected

The dimension-6 operator coefficient \((C_{EH})_{13}\) (real part).

Definition at line 1074 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CeH_22i

protected

The dimension-6 operator coefficient \((C_{EH})_{22}\) (imaginary part).

Definition at line 1081 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CeH_22r

protected

The dimension-6 operator coefficient \((C_{EH})_{22}\) (real part).

Definition at line 1075 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CeH_23i

protected

The dimension-6 operator coefficient \((C_{EH})_{23}\) (imaginary part).

Definition at line 1082 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CeH_23r

protected

The dimension-6 operator coefficient \((C_{EH})_{23}\) (real part).

Definition at line 1076 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CeH_33i

protected

The dimension-6 operator coefficient \((C_{EH})_{33}\) (imaginary part).

Definition at line 1083 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CeH_33r

protected

The dimension-6 operator coefficient \((C_{EH})_{33}\) (real part).

Definition at line 1077 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CH

protected

The dimension-6 operator coefficient \(C_{H}\).

Definition at line 996 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHB

protected

The dimension-6 operator coefficient \(C_{HB}\).

Definition at line 992 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHbox

protected

The dimension-6 operator coefficient \(C_{H\Box}\).

Definition at line 995 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHD

protected

The dimension-6 operator coefficient \(C_{HD}\).

Definition at line 994 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHd_11

protected

The dimension-6 operator coefficient \((C_{HD})_{11}\).

Definition at line 1051 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHd_12i

protected

The dimension-6 operator coefficient \((C_{HD})_{12}\) (imaginary part).

Definition at line 1057 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHd_12r

protected

The dimension-6 operator coefficient \((C_{HD})_{12}\) (real part).

Definition at line 1052 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHd_13i

protected

The dimension-6 operator coefficient \((C_{HD})_{13}\) (imaginary part).

Definition at line 1058 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHd_13r

protected

The dimension-6 operator coefficient \((C_{HD})_{13}\) (real part).

Definition at line 1053 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHd_22

protected

The dimension-6 operator coefficient \((C_{HD})_{22}\).

Definition at line 1054 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHd_23i

protected

The dimension-6 operator coefficient \((C_{HD})_{23}\) (imaginary part).

Definition at line 1059 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHd_23r

protected

The dimension-6 operator coefficient \((C_{HD})_{23}\) (real part).

Definition at line 1055 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHd_33

protected

The dimension-6 operator coefficient \((C_{HD})_{33}\).

Definition at line 1056 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHe_11

protected

The dimension-6 operator coefficient \((C_{HE})_{11}\).

Definition at line 1015 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHe_12i

protected

The dimension-6 operator coefficient \((C_{HE})_{12}\) (imaginary part).

Definition at line 1021 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHe_12r

protected

The dimension-6 operator coefficient \((C_{HE})_{12}\) (real part).

Definition at line 1016 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHe_13i

protected

The dimension-6 operator coefficient \((C_{HE})_{13}\) (imaginary part).

Definition at line 1022 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHe_13r

protected

The dimension-6 operator coefficient \((C_{HE})_{13}\) (real part).

Definition at line 1017 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHe_22

protected

The dimension-6 operator coefficient \((C_{HE})_{22}\).

Definition at line 1018 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHe_23i

protected

The dimension-6 operator coefficient \((C_{HE})_{23}\) (imaginary part).

Definition at line 1023 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHe_23r

protected

The dimension-6 operator coefficient \((C_{HE})_{23}\) (real part).

Definition at line 1019 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHe_33

protected

The dimension-6 operator coefficient \((C_{HE})_{33}\).

Definition at line 1020 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHG

protected

The dimension-6 operator coefficient \(C_{HG}\).

Definition at line 990 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL1_11

protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\).

Definition at line 997 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL1_12i

protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part).

Definition at line 1003 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL1_12r

protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part).

Definition at line 998 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL1_13i

protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part).

Definition at line 1004 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL1_13r

protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part).

Definition at line 999 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL1_22

protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\).

Definition at line 1000 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL1_23i

protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part).

Definition at line 1005 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL1_23r

protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part).

Definition at line 1001 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL1_33

protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\).

Definition at line 1002 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL3_11

protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\).

Definition at line 1006 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL3_12i

protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).

Definition at line 1012 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL3_12r

protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).

Definition at line 1007 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL3_13i

protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).

Definition at line 1013 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL3_13r

protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).

Definition at line 1008 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL3_22

protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\).

Definition at line 1009 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL3_23i

protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).

Definition at line 1014 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL3_23r

protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).

Definition at line 1010 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHL3_33

protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\).

Definition at line 1011 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ1_11

protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\).

Definition at line 1024 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ1_12i

protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part).

Definition at line 1030 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ1_12r

protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part).

Definition at line 1025 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ1_13i

protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part).

Definition at line 1031 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ1_13r

protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part).

Definition at line 1026 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ1_22

protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\).

Definition at line 1027 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ1_23i

protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part).

Definition at line 1032 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ1_23r

protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part).

Definition at line 1028 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ1_33

protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\).

Definition at line 1029 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ3_11

protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\).

Definition at line 1033 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ3_12i

protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part).

Definition at line 1039 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ3_12r

protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part).

Definition at line 1034 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ3_13i

protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part).

Definition at line 1040 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ3_13r

protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part).

Definition at line 1035 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ3_22

protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\).

Definition at line 1036 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ3_23i

protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part).

Definition at line 1041 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ3_23r

protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part).

Definition at line 1037 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHQ3_33

protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\).

Definition at line 1038 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHu_11

protected

The dimension-6 operator coefficient \((C_{HU})_{11}\).

Definition at line 1042 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHu_12i

protected

The dimension-6 operator coefficient \((C_{HU})_{12}\) (imaginary part).

Definition at line 1048 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHu_12r

protected

The dimension-6 operator coefficient \((C_{HU})_{12}\) (real part).

Definition at line 1043 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHu_13i

protected

The dimension-6 operator coefficient \((C_{HU})_{13}\) (imaginary part).

Definition at line 1049 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHu_13r

protected

The dimension-6 operator coefficient \((C_{HU})_{13}\) (real part).

Definition at line 1044 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHu_22

protected

The dimension-6 operator coefficient \((C_{HU})_{22}\).

Definition at line 1045 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHu_23i

protected

The dimension-6 operator coefficient \((C_{HU})_{23}\) (imaginary part).

Definition at line 1050 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHu_23r

protected

The dimension-6 operator coefficient \((C_{HU})_{23}\) (real part).

Definition at line 1046 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHu_33

protected

The dimension-6 operator coefficient \((C_{HU})_{33}\).

Definition at line 1047 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHud_11i

protected

The dimension-6 operator coefficient \((C_{HUD})_{11}\) (imaginary part).

Definition at line 1066 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHud_11r

protected

The dimension-6 operator coefficient \((C_{HUD})_{11}\) (real part).

Definition at line 1060 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHud_12i

protected

The dimension-6 operator coefficient \((C_{HUD})_{12}\) (imaginary part).

Definition at line 1067 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHud_12r

protected

The dimension-6 operator coefficient \((C_{HUD})_{12}\) (real part).

Definition at line 1061 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHud_13i

protected

The dimension-6 operator coefficient \((C_{HUD})_{13}\) (imaginary part).

Definition at line 1068 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHud_13r

protected

The dimension-6 operator coefficient \((C_{HUD})_{13}\) (real part).

Definition at line 1062 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHud_22i

protected

The dimension-6 operator coefficient \((C_{HUD})_{22}\) (imaginary part).

Definition at line 1069 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHud_22r

protected

The dimension-6 operator coefficient \((C_{HUD})_{22}\) (real part).

Definition at line 1063 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHud_23i

protected

The dimension-6 operator coefficient \((C_{HUD})_{23}\) (imaginary part).

Definition at line 1070 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHud_23r

protected

The dimension-6 operator coefficient \((C_{HUD})_{23}\) (real part).

Definition at line 1064 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHud_33i

protected

The dimension-6 operator coefficient \((C_{HUD})_{33}\) (imaginary part).

Definition at line 1071 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHud_33r

protected

The dimension-6 operator coefficient \((C_{HUD})_{33}\) (real part).

Definition at line 1065 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHW

protected

The dimension-6 operator coefficient \(C_{HW}\).

Definition at line 991 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CHWB

protected

The dimension-6 operator coefficient \(C_{HWB}\).

Definition at line 993 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CLL_1221

protected

The dimension-6 operator coefficient \((C_{LL})_{1221}\).

Definition at line 1108 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CLL_2112

protected

The dimension-6 operator coefficient \((C_{LL})_{2112}\).

Definition at line 1109 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CuH_11i

protected

The dimension-6 operator coefficient \((C_{UH})_{11}\) (imaginary part).

Definition at line 1090 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CuH_11r

protected

The dimension-6 operator coefficient \((C_{UH})_{11}\) (real part).

Definition at line 1084 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CuH_12i

protected

The dimension-6 operator coefficient \((C_{UH})_{12}\) (imaginary part).

Definition at line 1091 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CuH_12r

protected

The dimension-6 operator coefficient \((C_{UH})_{12}\) (real part).

Definition at line 1085 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CuH_13i

protected

The dimension-6 operator coefficient \((C_{UH})_{13}\) (imaginary part).

Definition at line 1092 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CuH_13r

protected

The dimension-6 operator coefficient \((C_{UH})_{13}\) (real part).

Definition at line 1086 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CuH_22i

protected

The dimension-6 operator coefficient \((C_{UH})_{22}\) (imaginary part).

Definition at line 1093 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CuH_22r

protected

The dimension-6 operator coefficient \((C_{UH})_{22}\) (real part).

Definition at line 1087 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CuH_23i

protected

The dimension-6 operator coefficient \((C_{UH})_{23}\) (imaginary part).

Definition at line 1094 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CuH_23r

protected

The dimension-6 operator coefficient \((C_{UH})_{23}\) (real part).

Definition at line 1088 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CuH_33i

protected

The dimension-6 operator coefficient \((C_{UH})_{33}\) (imaginary part).

Definition at line 1095 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::CuH_33r

protected

The dimension-6 operator coefficient \((C_{UH})_{33}\) (real part).

Definition at line 1089 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::cW2_tree

protected

The sqaure of the tree level values for the cosine of the weak angle.

Definition at line 1202 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::cW_tree

protected

The tree level values for the cosine of the weak angle.

Definition at line 1200 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::delta_AA

protected

Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.

Definition at line 1205 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::delta_AZ

protected

Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.

Definition at line 1206 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::delta_h

protected

Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition.

Definition at line 1207 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::delta_ZZ

protected

Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition.

Definition at line 1204 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::ettH2_Hgg

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to ttH production at Tevatron (1.96 TeV).

Definition at line 1192 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::ettH2_Htt

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Htt}\) to ttH production at Tevatron (1.96 TeV).

Definition at line 1191 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::ettH78_Hgg

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to ttH production at the LHC (7 & 8 TeV).

Definition at line 1194 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::ettH78_Htt

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Htt}\) to ttH production at the LHC (7 & 8 TeV).

Definition at line 1193 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HAA

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HAA}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1117 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_Hgg

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1121 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HWud

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1126 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HWW1

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1118 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HWW2

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1119 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HWW3

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1120 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HZA1

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1115 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HZA2

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1116 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HZdL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1124 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HZdR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1125 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HZuL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1122 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HZuR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1123 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HZZ1

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1112 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HZZ2

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1113 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_HZZ3

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1114 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_Wud

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1131 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_ZdL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1129 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_ZdR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1130 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_ZuL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1127 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF2_ZuR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 1128 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HAA

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HAA}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1137 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_Hgg

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Hgg}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1141 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HWud

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1146 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HWW1

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1138 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HWW2

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1139 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HWW3

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1140 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HZA1

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1135 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HZA2

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1136 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HZdL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1144 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HZdR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1145 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HZuL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1142 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HZuR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1143 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HZZ1

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1132 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HZZ2

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1133 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_HZZ3

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1134 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_Wud

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1151 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_ZdL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1149 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_ZdR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1150 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_ZuL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1147 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eVBF78_ZuR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to VBF production at the LHC (7 & 8 TeV).

Definition at line 1148 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eWH2_HWud

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to WH production at Tevatron (1.96 TeV).

Definition at line 1156 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eWH2_HWW1

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to WH production at Tevatron (1.96 TeV).

Definition at line 1153 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eWH2_HWW2

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to WH production at Tevatron (1.96 TeV).

Definition at line 1154 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eWH2_HWW3

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to WH production at Tevatron (1.96 TeV).

Definition at line 1155 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eWH2_Wud

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to WH production at Tevatron (1.96 TeV).

Definition at line 1157 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eWH78_HWud

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWud}^{L}\) to WH production at the LHC (7 & 8 TeV).

Definition at line 1161 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eWH78_HWW1

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(1)}\) to WH production at the LHC (7 & 8 TeV).

Definition at line 1158 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eWH78_HWW2

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(2)}\) to WH production at the LHC (7 & 8 TeV).

Definition at line 1159 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eWH78_HWW3

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HWW}^{(3)}\) to WH production at the LHC (7 & 8 TeV).

Definition at line 1160 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eWH78_Wud

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Wud}^{L}\) to WH production at the LHC (7 & 8 TeV).

Definition at line 1162 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH2_HZA1

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 1167 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH2_HZA2

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 1168 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH2_HZdL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 1171 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH2_HZdR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 1172 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH2_HZuL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 1169 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH2_HZuR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 1170 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH2_HZZ1

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 1164 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH2_HZZ2

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 1165 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH2_HZZ3

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 1166 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH2_ZdL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 1175 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH2_ZdR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 1176 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH2_ZuL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 1173 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH2_ZuR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 1174 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH78_HZA1

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(1)}\) to ZH production at the LHC (7 & 8 TeV).

Definition at line 1180 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH78_HZA2

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZA}^{(2)}\) to ZH production at the LHC (7 & 8 TeV).

Definition at line 1181 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH78_HZdL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{L}\) to ZH production at the LHC (7 & 8 TeV).

Definition at line 1184 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH78_HZdR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZdd}^{R}\) to ZH production at the LHC (7 & 8 TeV).

Definition at line 1185 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH78_HZuL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{L}\) to ZH production at the LHC (7 & 8 TeV).

Definition at line 1182 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH78_HZuR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZuu}^{R}\) to ZH production at the LHC (7 & 8 TeV).

Definition at line 1183 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH78_HZZ1

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(1)}\) to ZH production at the LHC (7 & 8 TeV).

Definition at line 1177 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH78_HZZ2

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(2)}\) to ZH production at the LHC (7 & 8 TeV).

Definition at line 1178 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH78_HZZ3

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{HZZ}^{(3)}\) to ZH production at the LHC (7 & 8 TeV).

Definition at line 1179 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH78_ZdL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{L}\) to ZH production at the LHC (7 & 8 TeV).

Definition at line 1188 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH78_ZdR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zdd}^{R}\) to ZH production at the LHC (7 & 8 TeV).

Definition at line 1189 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH78_ZuL

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{L}\) to ZH production at the LHC (7 & 8 TeV).

Definition at line 1186 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::eZH78_ZuR

protected

Theoretical uncertainty in the (linear) new physics contribution from \(g_{Zuu}^{R}\) to ZH production at the LHC (7 & 8 TeV).

Definition at line 1187 of file NPEffectiveGIMR.h.

const bool NPEffectiveGIMR::FlagLeptonUniversal

private

An internal boolean flag that is true if assuming lepton flavour universality.

Definition at line 1255 of file NPEffectiveGIMR.h.

bool NPEffectiveGIMR::FlagMwInput

private

A boolean flag that is true if the W mass is taken as an input parameter. (Warning: The W width is not implemented in this case.)

Definition at line 1248 of file NPEffectiveGIMR.h.

bool NPEffectiveGIMR::FlagQuadraticTerms

private

A boolean flag that is true if the quadratic terms in cross sections and widths are switched on.

Definition at line 1249 of file NPEffectiveGIMR.h.

const bool NPEffectiveGIMR::FlagQuarkUniversal

private

An internal boolean flag that is true if assuming quark flavour universality.

Definition at line 1261 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::Lambda_NP

protected

The new physics scale [GeV].

Definition at line 1110 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::LambdaNP2

protected

The square of the new physics scale [GeV \(^2\)].

Definition at line 1198 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::MwInput

protected

The input value for the \(W\)-boson mass if FlagMwInput is true.

Definition at line 1196 of file NPEffectiveGIMR.h.

const int NPEffectiveGIMR::NNPEffectiveGIMRVars = 200

static

The number of the model parameters in NPEffectiveGIMR.

　

Definition at line 429 of file NPEffectiveGIMR.h.

const int NPEffectiveGIMR::NNPEffectiveGIMRVars_LFU_QFU = 104

static

The number of the model parameters in NPEffectiveGIMR with lepton and quark flavour universalities.

　

Definition at line 441 of file NPEffectiveGIMR.h.

const std::string NPEffectiveGIMR::NPEffectiveGIMRVars

static

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

Definition at line 435 of file NPEffectiveGIMR.h.

const std::string NPEffectiveGIMR::NPEffectiveGIMRVars_LFU_QFU

static

Initial value:

= {"CHG", "CHW", "CHB", "CHWB", "CHD", "CHbox", "CH",
    "CHL1", "CHL3", "CHe", "CHQ1", "CHQ3", "CHu", "CHd", "CHud_r", "CHud_i",
    "CeH_r", "CeH_i", "CuH_r", "CuH_i", "CdH_r", "CdH_i", "CLL",
    "Lambda_NP",
    "eVBF2_HZZ1", "eVBF2_HZZ2", "eVBF2_HZZ3", "eVBF2_HZA1", "eVBF2_HZA2", "eVBF2_HAA",
    "eVBF2_HWW1", "eVBF2_HWW2", "eVBF2_HWW3", "eVBF2_Hgg", "eVBF2_HZuL", "eVBF2_HZuR",
    "eVBF2_HZdL", "eVBF2_HZdR", "eVBF2_HWud", "eVBF2_ZuL", "eVBF2_ZuR", "eVBF2_ZdL",
    "eVBF2_ZdR", "eVBF2_Wud",
    "eVBF78_HZZ1", "eVBF78_HZZ2", "eVBF78_HZZ3", "eVBF78_HZA1", "eVBF78_HZA2", "eVBF78_HAA",
    "eVBF78_HWW1", "eVBF78_HWW2", "eVBF78_HWW3", "eVBF78_Hgg", "eVBF78_HZuL", "eVBF78_HZuR",
    "eVBF78_HZdL", "eVBF78_HZdR", "eVBF78_HWud", "eVBF78_ZuL", "eVBF78_ZuR", "eVBF78_ZdL",
    "eVBF78_ZdR", "eVBF78_Wud",
    "eWH2_HWW1", "eWH2_HWW2", "eWH2_HWW3", "eWH2_HWud", "eWH2_Wud",
    "eWH78_HWW1", "eWH78_HWW2", "eWH78_HWW3", "eWH78_HWud", "eWH78_Wud",
    "eZH2_HZZ1", "eZH2_HZZ2", "eZH2_HZZ3", "eZH2_HZA1", "eZH2_HZA2", "eZH2_HZuL", "eZH2_HZuR",
    "eZH2_HZdL", "eZH2_HZdR", "eZH2_ZuL", "eZH2_ZuR", "eZH2_ZdL", "eZH2_ZdR",
    "eZH78_HZZ1", "eZH78_HZZ2", "eZH78_HZZ3", "eZH78_HZA1", "eZH78_HZA2", "eZH78_HZuL", "eZH78_HZuR",
    "eZH78_HZdL", "eZH78_HZdR", "eZH78_ZuL", "eZH78_ZuR", "eZH78_ZdL", "eZH78_ZdR",
    "ettH2_Htt", "ettH2_Hgg",
    "ettH78_Htt", "ettH78_Hgg"}

A string array containing the labels of the model parameters in NPEffectiveGIMR with lepton and quark flavour universalities.

Definition at line 447 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::sW2_tree

protected

The sqaure of the tree level values for the sine of the weak angle.

Definition at line 1203 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::sW_tree

protected

The tree level values for the sine of the weak angle.

Definition at line 1201 of file NPEffectiveGIMR.h.

double NPEffectiveGIMR::v2_over_LambdaNP2

protected

The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\).

Definition at line 1199 of file NPEffectiveGIMR.h.

---

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

• NPEffectiveGIMR.h
• NPEffectiveGIMR.cpp