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:

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 [132].

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
CG	\(C_{G} \)	The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\).
CW	\(C_{W} \)	The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\).
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 \(i,j=1,2,3\).
CuG_klr, CuG_kli	\(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\).
CuW_klr, CuW_kli	\(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \tau_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\).
CuB_klr, CuB_kli	\(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), 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 \(ijkl=1221,2112\).
CLQ1	\(C_{LQ}^{(1)}\)	The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\).
CLQ3	\(C_{LQ}^{(3)}\)	The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \tau_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \tau_a Q^l\big)\).
Cee	\(C_{EE}\)	The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Ceu	\(C_{EU}\)	The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
Ced	\(C_{ED}\)	The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CLe	\(C_{LE}\)	The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
CLu	\(C_{LU}\)	The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
CLd	\(C_{LD}\)	The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CQe	\(C_{QE}\)	The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
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
CG	\(C_{G} \)	The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\).
CW	\(C_{W} \)	The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\).
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).
CuG_klr, CuG_kli	\(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\).
CuW_klr, CuW_kli	\(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \tau_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\).
CuB_klr, CuB_kli	\(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \)	The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\).
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 \(ijkl=1221,2112\).
CLQ1	\(C_{LQ}^{(1)}\)	The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\).
CLQ3	\(C_{LQ}^{(3)}\)	The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \tau_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \tau_a Q^l\big)\).
Cee	\(C_{EE}\)	The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Ceu	\(C_{EU}\)	The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
Ced	\(C_{ED}\)	The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CLe	\(C_{LE}\)	The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
CLu	\(C_{LU}\)	The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
CLd	\(C_{LD}\)	The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CQe	\(C_{QE}\)	The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
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 610 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	BrHmumuRatio () const
	The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model. More...
virtual double	BrHtautauRatio () const
	The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More...
virtual double	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...
double	CLL_bottom () const
double	CLL_charm () const
double	CLL_down () const
double	CLL_mu () const
double	CLL_strange () const
double	CLL_tau () const
double	CLL_up () const
double	CLR_bottom () const
double	CLR_charm () const
double	CLR_down () const
double	CLR_mu () const
double	CLR_strange () const
double	CLR_tau () const
double	CLR_up () const
virtual double	computeGammaTotalRatio () const
	The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More...
double	CRL_bottom () const
double	CRL_charm () const
double	CRL_down () const
double	CRL_mu () const
double	CRL_strange () const
double	CRL_tau () const
double	CRL_up () const
double	CRR_bottom () const
double	CRR_charm () const
double	CRR_down () const
double	CRR_mu () const
double	CRR_strange () const
double	CRR_tau () const
double	CRR_up () const
virtual double	deltaG1_hWW () const
	The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More...
virtual double	deltaG1_hZA () const
	The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More...
virtual double	deltaG1_hZZ () const
	The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More...
virtual double	deltaG2_hWW () const
	The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More...
virtual double	deltaG2_hZA () const
	The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More...
virtual double	deltaG2_hZZ () const
	The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More...
virtual double	deltaG3_hWW () const
	The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More...
virtual double	deltaG3_hZZ () const
	The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More...
double	deltag3G () const
	The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\). More...
gslpp::complex	deltaG_Aff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
gslpp::complex	deltaG_Gff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
virtual double	deltaG_hAA () const
	The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More...
gslpp::complex	deltaG_hAff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
virtual gslpp::complex	deltaG_hff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More...
gslpp::complex	deltaG_hGff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
virtual double	deltaG_hgg () const
	The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More...
gslpp::complex	deltaG_hZff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
gslpp::complex	deltaG_Zff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). 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	deltaGammaHmumuRatio1 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
double	deltaGammaHmumuRatio2 () const
	The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
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...
virtual gslpp::complex	deltaGL_Wff (const Particle pbar, const Particle p) const
	New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More...
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...
virtual gslpp::complex	deltaGR_Wff (const Particle pbar, const Particle p) const
	New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More...
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...
virtual double	deltaMz2 () const
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	GammaHmumuRatio () const
	The ratio of the \(\Gamma(H\to \mu\mu)\) 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	LEP2AFBbottom (const double s) const
virtual double	LEP2AFBcharm (const double s) const
virtual double	LEP2AFBmu (const double s) const
virtual double	LEP2AFBtau (const double s) const
virtual double	LEP2Rbottom (const double s) const
virtual double	LEP2Rcharm (const double s) const
virtual double	LEP2sigmaHadron (const double s) const
virtual double	LEP2sigmaMu (const double s) const
virtual double	LEP2sigmaTau (const double s) const
virtual double	mueettH (const double sqrt_s) const
	The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More...
virtual double	mueeWBF (const double sqrt_s) const
	The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More...
virtual double	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	aPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More...
virtual double	AuxObs_NP1 () const
	Auxiliary observable AuxObs_NP1. More...
virtual double	AuxObs_NP10 () const
	Auxiliary observable AuxObs_NP10. More...
virtual double	AuxObs_NP11 () const
	Auxiliary observable AuxObs_NP11. More...
virtual double	AuxObs_NP12 () const
	Auxiliary observable AuxObs_NP12. More...
virtual double	AuxObs_NP13 () const
	Auxiliary observable AuxObs_NP13. More...
virtual double	AuxObs_NP14 () const
	Auxiliary observable AuxObs_NP14. More...
virtual double	AuxObs_NP15 () const
	Auxiliary observable AuxObs_NP15. More...
virtual double	AuxObs_NP16 () const
	Auxiliary observable AuxObs_NP16. More...
virtual double	AuxObs_NP17 () const
	Auxiliary observable AuxObs_NP17. More...
virtual double	AuxObs_NP18 () const
	Auxiliary observable AuxObs_NP18. More...
virtual double	AuxObs_NP19 () const
	Auxiliary observable AuxObs_NP19. More...
virtual double	AuxObs_NP2 () const
	Auxiliary observable AuxObs_NP2. More...
virtual double	AuxObs_NP20 () const
	Auxiliary observable AuxObs_NP20. More...
virtual double	AuxObs_NP3 () const
	Auxiliary observable AuxObs_NP3. More...
virtual double	AuxObs_NP4 () const
	Auxiliary observable AuxObs_NP4. More...
virtual double	AuxObs_NP5 () const
	Auxiliary observable AuxObs_NP5. More...
virtual double	AuxObs_NP6 () const
	Auxiliary observable AuxObs_NP6. More...
virtual double	AuxObs_NP7 () const
	Auxiliary observable AuxObs_NP7. More...
virtual double	AuxObs_NP8 () const
	Auxiliary observable AuxObs_NP8. More...
virtual double	AuxObs_NP9 () const
	Auxiliary observable AuxObs_NP9. More...
virtual double	bPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More...
virtual double	Br_H_exo () const
	The branching ratio of the of the Higgs into exotic particles. More...
virtual double	Br_H_inv () const
	The branching ratio of the of the Higgs into invisible particles. More...
virtual double	Br_H_inv_NP () const
	The branching ratio of the of the Higgs into invisible particles (only invisible new particles). More...
virtual double	BR_Zf (const Particle f) const
	The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\). More...
virtual double	BrHtoinvRatio () const
	The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model. More...
virtual double	BrHvisRatio () const
	The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model. More...
virtual double	BrHWlvRatio () const
	The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
virtual double	BrHWW2l2vRatio () const
	The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
virtual double	BrHZgaeeRatio () const
	The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model. More...
virtual double	BrHZgallRatio () const
	The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
virtual double	BrHZgamumuRatio () const
	The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model. More...
virtual double	BrHZllRatio () const
	The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
virtual double	BrHZZ2e2muRatio () const
	The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model. More...
virtual double	BrHZZ4eRatio () const
	The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More...
virtual double	BrHZZ4lRatio () const
	The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
virtual double	BrHZZ4muRatio () const
	The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More...
virtual double	cbminuscc () const
virtual double	cbminusctau () const
virtual double	ccminusctau () const
virtual double	cgaga_HB () const
	The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) More...
virtual double	cgaplusct () const
virtual double	cgg_HB () const
	The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) More...
virtual double	cggEff_HB () const
	The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) More...
virtual double	cgminuscga () const
virtual double	cgplusct () const
virtual double	cVpluscb () const
virtual double	cVplusctau () const
virtual double	cZBox_HB () const
	The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) More...
virtual double	cZga_HB () const
	The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) More...
virtual double	cZZ_HB () const
	The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) More...
virtual double	deltaA_f (const Particle f) const
	The new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta \mathcal{A}_f\). More...
virtual double	deltaAFB (const Particle f) const
	The new physics contribution to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta A^f_{FB}\). More...
virtual double	deltacZ_HB () const
	The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) More...
virtual double	deltaG1_hZARatio () const
	The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
virtual double	deltag1ZNP () const
	The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More...
virtual double	deltag1ZNPEff () const
	The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More...
virtual double	deltaG_hAARatio () const
	The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
virtual double	deltaG_hggRatio () const
	The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
virtual double	deltaG_hhhRatio () const
	The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More...
virtual double	deltaGamma_W () const
	The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\). More...
virtual double	deltaGamma_Wff (const Particle fi, const Particle fj) const
	The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More...
virtual double	deltaGamma_Z () const
	The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\). More...
virtual double	deltaGamma_Zf (const Particle f) const
	The new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More...
virtual double	deltaGamma_Zhad () const
	The new physics contribution to the hadronic decay width of the \(Z\) boson, \(\delta \Gamma_{Z,had}\). More...
virtual double	deltaKgammaNP () const
	The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\). More...
virtual double	deltaKgammaNPEff () const
	The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More...
virtual double	deltaN_nu () const
	The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements. More...
virtual double	deltaR0_f (const Particle f) const
	The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More...
virtual double	deltaR_inv () const
	The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the \(Z\) boson, \(\delta R_{inv}\). More...
virtual double	deltaSigmaHadron () const
	The new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\delta \sigma_h^0\). More...
virtual double	deltaSin2thetaEff_e () const
	The new physics contribution to the effective electron/leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. More...
virtual double	deltaSin2thetaEff_mu () const
	The new physics contribution to the effective muonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\mu\mu}\) at the \(Z\) pole. More...
virtual double	deltayb_HB () const
	The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) More...
virtual double	deltayc_HB () const
	The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) More...
virtual double	deltaymu_HB () const
	The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) More...
virtual double	deltayt_HB () const
	The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) More...
virtual double	deltaytau_HB () const
	The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) More...
virtual double	dxseeWWdcos (const double sqrt_s, const double cos) const
	The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle. More...
virtual double	dxseeWWdcosBin (const double sqrt_s, const double cos1, const double cos2) const
	The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle. More...
virtual gslpp::complex	gA_f (const Particle f) const
	The total (SM+NP) contribution to the neutral-current axial-vector coupling \(g_A^f\). More...
virtual double	Gamma_had () const
	The hadronic decay width of the \(Z\) boson, \(\Gamma_{Z,had}\). More...
virtual double	Gamma_Z () const
	The total decay width of the \(Z\) boson, \(\Gamma_Z\). More...
virtual double	Gamma_Zf (const Particle f) const
	The decay width of the \(Z\) boson into a given fermion pair, \(\Gamma_Z^{f}\). More...
virtual double	GammaW (const Particle fi, const Particle fj) const
	A partial decay width of the \(W\) boson decay into a SM fermion pair. More...
virtual StandardModel	getTrueSM () const
	A method to return a StandardModel object from NPbase. More...
virtual gslpp::complex	gV_f (const Particle f) const
	The total (SM+NP) contribution to the neutral-current vector coupling \(g_V^f\). More...
virtual double	kappaAeff () const
	The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\). More...
virtual double	kappabeff () const
	The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\). More...
virtual double	kappaceff () const
	The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\). More...
virtual double	kappaGeff () const
	The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\). More...
virtual double	kappamueff () const
	The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\). More...
virtual double	kappataueff () const
	The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\). More...
virtual double	kappaWeff () const
	The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\). More...
virtual gslpp::complex	kappaZ_f (const Particle f) const
	The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions. More...
virtual double	kappaZAeff () const
	The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\). More...
virtual double	kappaZeff () const
	The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\). More...
virtual double	lambdaZNP () const
	The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\). More...
virtual double	lambz_HB () const
	The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) More...
virtual double	mueeHvv (const double sqrt_s) const
	The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More...
virtual double	mueeHvvPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More...
virtual double	mueettHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More...
virtual double	mueeWBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More...
virtual double	mueeWW (const double sqrt_s) const
	The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More...
virtual double	mueeWWPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More...
virtual double	mueeZBF (const double sqrt_s) const
	The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More...
virtual double	mueeZBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More...
virtual double	mueeZHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More...
virtual double	mueeZllH (const double sqrt_s) const
	The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More...
virtual double	mueeZllHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More...
virtual double	mueeZqqH (const double sqrt_s) const
	The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More...
virtual double	mueeZqqHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More...
virtual double	muepWBF (const double sqrt_s) const
	The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model. More...
virtual double	muepZBF (const double sqrt_s) const
	The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model. More...
virtual double	muggHbb (const double sqrt_s) const
virtual double	muggHgaga (const double sqrt_s) const
virtual double	muggHgagaInt (const double sqrt_s) const
	The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259. More...
virtual double	muggHH (const double sqrt_s) const
	The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. More...
virtual double	muggHmumu (const double sqrt_s) const
virtual double	muggHtautau (const double sqrt_s) const
virtual double	muggHWW (const double sqrt_s) const
virtual double	muggHWW2l2v (const double sqrt_s) const
virtual double	muggHZga (const double sqrt_s) const
virtual double	muggHZZ (const double sqrt_s) const
virtual double	muggHZZ4l (const double sqrt_s) const
virtual double	mummH (const double sqrt_s) const
	The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model. More...
virtual double	muppHmumu (const double sqrt_s) const
virtual double	muppHZga (const double sqrt_s) const
virtual double	mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const
	The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class. More...
virtual double	mutHq (const double sqrt_s) const
	The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model. More...
virtual double	muTHUggHbb (const double sqrt_s) const
virtual double	muTHUggHgaga (const double sqrt_s) const
virtual double	muTHUggHmumu (const double sqrt_s) const
virtual double	muTHUggHtautau (const double sqrt_s) const
virtual double	muTHUggHWW (const double sqrt_s) const
virtual double	muTHUggHWW2l2v (const double sqrt_s) const
virtual double	muTHUggHZga (const double sqrt_s) const
virtual double	muTHUggHZgamumu (const double sqrt_s) const
virtual double	muTHUggHZZ (const double sqrt_s) const
virtual double	muTHUggHZZ4l (const double sqrt_s) const
virtual double	muTHUggHZZ4mu (const double sqrt_s) const
virtual double	muTHUttHbb (const double sqrt_s) const
virtual double	muTHUttHgaga (const double sqrt_s) const
virtual double	muTHUttHmumu (const double sqrt_s) const
virtual double	muTHUttHtautau (const double sqrt_s) const
virtual double	muTHUttHWW (const double sqrt_s) const
virtual double	muTHUttHWW2l2v (const double sqrt_s) const
virtual double	muTHUttHZga (const double sqrt_s) const
virtual double	muTHUttHZZ (const double sqrt_s) const
virtual double	muTHUttHZZ4l (const double sqrt_s) const
virtual double	muTHUVBFBRinv (const double sqrt_s) const
virtual double	muTHUVBFHbb (const double sqrt_s) const
virtual double	muTHUVBFHgaga (const double sqrt_s) const
virtual double	muTHUVBFHinv (const double sqrt_s) const
virtual double	muTHUVBFHmumu (const double sqrt_s) const
virtual double	muTHUVBFHtautau (const double sqrt_s) const
virtual double	muTHUVBFHWW (const double sqrt_s) const
virtual double	muTHUVBFHWW2l2v (const double sqrt_s) const
virtual double	muTHUVBFHZga (const double sqrt_s) const
virtual double	muTHUVBFHZZ (const double sqrt_s) const
virtual double	muTHUVBFHZZ4l (const double sqrt_s) const
virtual double	muTHUVHbb (const double sqrt_s) const
virtual double	muTHUVHBRinv (const double sqrt_s) const
virtual double	muTHUVHgaga (const double sqrt_s) const
virtual double	muTHUVHinv (const double sqrt_s) const
virtual double	muTHUVHmumu (const double sqrt_s) const
virtual double	muTHUVHtautau (const double sqrt_s) const
virtual double	muTHUVHWW (const double sqrt_s) const
virtual double	muTHUVHWW2l2v (const double sqrt_s) const
virtual double	muTHUVHZga (const double sqrt_s) const
virtual double	muTHUVHZZ (const double sqrt_s) const
virtual double	muTHUVHZZ4l (const double sqrt_s) const
virtual double	muTHUWHbb (const double sqrt_s) const
virtual double	muTHUWHgaga (const double sqrt_s) const
virtual double	muTHUWHmumu (const double sqrt_s) const
virtual double	muTHUWHtautau (const double sqrt_s) const
virtual double	muTHUWHWW (const double sqrt_s) const
virtual double	muTHUWHWW2l2v (const double sqrt_s) const
virtual double	muTHUWHZga (const double sqrt_s) const
virtual double	muTHUWHZZ (const double sqrt_s) const
virtual double	muTHUWHZZ4l (const double sqrt_s) const
virtual double	muTHUZHbb (const double sqrt_s) const
virtual double	muTHUZHgaga (const double sqrt_s) const
virtual double	muTHUZHmumu (const double sqrt_s) const
virtual double	muTHUZHtautau (const double sqrt_s) const
virtual double	muTHUZHWW (const double sqrt_s) const
virtual double	muTHUZHWW2l2v (const double sqrt_s) const
virtual double	muTHUZHZga (const double sqrt_s) const
virtual double	muTHUZHZZ (const double sqrt_s) const
virtual double	muTHUZHZZ4l (const double sqrt_s) const
virtual double	muttHbb (const double sqrt_s) const
virtual double	muttHgaga (const double sqrt_s) const
virtual double	muttHmumu (const double sqrt_s) const
virtual double	muttHtautau (const double sqrt_s) const
virtual double	muttHWW (const double sqrt_s) const
virtual double	muttHWW2l2v (const double sqrt_s) const
virtual double	muttHZbbboost (const double sqrt_s) const
	The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model. More...
virtual double	muttHZga (const double sqrt_s) const
virtual double	muttHZZ (const double sqrt_s) const
virtual double	muttHZZ4l (const double sqrt_s) const
virtual double	muVBFgamma (const double sqrt_s) const
	The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model. More...
virtual double	muVBFHbb (const double sqrt_s) const
virtual double	muVBFHgaga (const double sqrt_s) const
virtual double	muVBFHmumu (const double sqrt_s) const
virtual double	muVBFHtautau (const double sqrt_s) const
virtual double	muVBFHWW (const double sqrt_s) const
virtual double	muVBFHWW2l2v (const double sqrt_s) const
virtual double	muVBFHZga (const double sqrt_s) const
virtual double	muVBFHZZ (const double sqrt_s) const
virtual double	muVBFHZZ4l (const double sqrt_s) const
virtual double	muVHbb (const double sqrt_s) const
virtual double	muVHgaga (const double sqrt_s) const
virtual double	muVHmumu (const double sqrt_s) const
virtual double	muVHtautau (const double sqrt_s) const
virtual double	muVHWW (const double sqrt_s) const
virtual double	muVHWW2l2v (const double sqrt_s) const
virtual double	muVHZga (const double sqrt_s) const
virtual double	muVHZZ (const double sqrt_s) const
virtual double	muVHZZ4l (const double sqrt_s) const
virtual double	muWHbb (const double sqrt_s) const
virtual double	muWHgaga (const double sqrt_s) const
virtual double	muWHmumu (const double sqrt_s) const
virtual double	muWHtautau (const double sqrt_s) const
virtual double	muWHWW (const double sqrt_s) const
virtual double	muWHWW2l2v (const double sqrt_s) const
virtual double	muWHZga (const double sqrt_s) const
virtual double	muWHZZ (const double sqrt_s) const
virtual double	muWHZZ4l (const double sqrt_s) const
virtual double	muZHbb (const double sqrt_s) const
virtual double	muZHgaga (const double sqrt_s) const
virtual double	muZHmumu (const double sqrt_s) const
virtual double	muZHtautau (const double sqrt_s) const
virtual double	muZHWW (const double sqrt_s) const
virtual double	muZHWW2l2v (const double sqrt_s) const
virtual double	muZHZga (const double sqrt_s) const
virtual double	muZHZZ (const double sqrt_s) const
virtual double	muZHZZ4l (const double sqrt_s) const
virtual double	N_nu () const
	The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\). More...
	NPbase ()
	The default constructor. More...
virtual double	obliqueW () const
	The oblique parameter \(W\). More...
virtual double	obliqueY () const
	The oblique parameter \(Y\). More...
virtual double	ppZHprobe (const double sqrt_s) const
	The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class. More...
virtual double	R0_f (const Particle f) const
	The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More...
virtual double	R_inv () const
	The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\). More...
virtual gslpp::complex	rhoZ_f (const Particle f) const
	The effective neutral-current coupling \(\rho_Z^f\) including SM plus NP contributions. More...
virtual double	sigma0_had () const
	The cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\sigma_h^0\). More...
virtual double	sin2thetaEff (const Particle f) const
	The leptonic effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\rm lept}\) at the the \(Z\) pole. More...
virtual double	STXS_ggH0j (const double sqrt_s) const
	The STXS bin \(gg \to H\). More...
virtual double	STXS_ggH1j_pTH_0_60 (const double sqrt_s) const
	The STXS bin \(gg \to H\). More...
virtual double	STXS_ggH1j_pTH_120_200 (const double sqrt_s) const
	The STXS bin \(gg \to H\). More...
virtual double	STXS_ggH1j_pTH_200 (const double sqrt_s) const
	The STXS bin \(gg \to H\). More...
virtual double	STXS_ggH1j_pTH_60_120 (const double sqrt_s) const
	The STXS bin \(gg \to H\). More...
virtual double	STXS_ggH2j_pTH_0_200 (const double sqrt_s) const
	The STXS bin \(gg \to H\). More...
virtual double	STXS_ggH2j_pTH_0_60 (const double sqrt_s) const
	The STXS bin \(gg \to H\). More...
virtual double	STXS_ggH2j_pTH_120_200 (const double sqrt_s) const
	The STXS bin \(gg \to H\). More...
virtual double	STXS_ggH2j_pTH_200 (const double sqrt_s) const
	The STXS bin \(gg \to H\). More...
virtual double	STXS_ggH2j_pTH_60_120 (const double sqrt_s) const
	The STXS bin \(gg \to H\). More...
virtual double	STXS_ggH_VBFtopo_j3 (const double sqrt_s) const
	The STXS bin \(gg \to H\). More...
virtual double	STXS_ggH_VBFtopo_j3v (const double sqrt_s) const
	The STXS bin \(gg \to H\). More...
virtual double	STXS_qqHll_pTV_0_150 (const double sqrt_s) const
	The STXS bin \(qq \to H \ell \ell\). More...
virtual double	STXS_qqHll_pTV_150_250 (const double sqrt_s) const
	The STXS bin \(qq \to H \ell \ell\). More...
virtual double	STXS_qqHll_pTV_150_250_0j (const double sqrt_s) const
	The STXS bin \(qq \to H \ell \ell\). More...
virtual double	STXS_qqHll_pTV_150_250_1j (const double sqrt_s) const
	The STXS bin \(qq \to H \ell \ell\). More...
virtual double	STXS_qqHll_pTV_250 (const double sqrt_s) const
	The STXS bin \(qq \to H \ell \ell\). More...
virtual double	STXS_qqHlv_pTV_0_150 (const double sqrt_s) const
	The STXS bin \(qq \to H \ell \nu\). More...
virtual double	STXS_qqHlv_pTV_0_250 (const double sqrt_s) const
	The STXS bin \(qq \to H \ell \nu\). More...
virtual double	STXS_qqHlv_pTV_150_250_0j (const double sqrt_s) const
	The STXS bin \(qq \to H \ell \nu\). More...
virtual double	STXS_qqHlv_pTV_150_250_1j (const double sqrt_s) const
	The STXS bin \(qq \to H \ell \nu\). More...
virtual double	STXS_qqHlv_pTV_250 (const double sqrt_s) const
	The STXS bin \(qq \to H \ell \nu\). More...
virtual double	STXS_qqHqq_pTj_200 (const double sqrt_s) const
	The STXS bin \(qq \to H qq\). More...
virtual double	STXS_qqHqq_Rest (const double sqrt_s) const
	The STXS bin \(qq \to H qq\). More...
virtual double	STXS_qqHqq_VBFtopo_j3 (const double sqrt_s) const
	The STXS bin \(qq \to H qq\). More...
virtual double	STXS_qqHqq_VBFtopo_j3v (const double sqrt_s) const
	The STXS bin \(qq \to H qq\). More...
virtual double	STXS_qqHqq_VBFtopo_Rest (const double sqrt_s) const
	The STXS bin \(qq \to H qq\). More...
virtual double	STXS_qqHqq_VHtopo (const double sqrt_s) const
	The STXS bin \(qq \to H qq\). More...
virtual double	STXS_ttHtH (const double sqrt_s) const
	The STXS bin \( ttH + tH \). More...
virtual double	STXS_WHqqHqq_pTj1_200 (const double sqrt_s) const
	The STXS bin \( qq \to WH \to H qq \). More...
virtual double	STXS_WHqqHqq_Rest (const double sqrt_s) const
	The STXS bin \( qq \to WH \to H qq \). More...
virtual double	STXS_WHqqHqq_VBFtopo_j3 (const double sqrt_s) const
	The STXS bin \( qq \to WH \to H qq \). More...
virtual double	STXS_WHqqHqq_VBFtopo_j3v (const double sqrt_s) const
	The STXS bin \( qq \to WH \to H qq \). More...
virtual double	STXS_WHqqHqq_VH2j (const double sqrt_s) const
	The STXS bin \( qq \to WH \to H qq \). More...
virtual double	STXS_ZHqqHqq_pTj1_200 (const double sqrt_s) const
	The STXS bin \( qq \to ZH \to H qq \). More...
virtual double	STXS_ZHqqHqq_Rest (const double sqrt_s) const
	The STXS bin \( qq \to ZH \to H qq \). More...
virtual double	STXS_ZHqqHqq_VBFtopo_j3 (const double sqrt_s) const
	The STXS bin \( qq \to ZH \to H qq \). More...
virtual double	STXS_ZHqqHqq_VBFtopo_j3v (const double sqrt_s) const
	The STXS bin \( qq \to ZH \to H qq \). More...
virtual double	STXS_ZHqqHqq_VH2j (const double sqrt_s) const
	The STXS bin \( qq \to ZH \to H qq \). More...
virtual bool	Update (const std::map< std::string, double > &DPars)
	The update method for NPbase. More...
virtual double	UpperLimitZgammaA (const double sqrt_s) const
virtual double	UpperLimitZgammaA13 (const double sqrt_s) const
virtual double	UpperLimitZgammaC (const double sqrt_s) const
virtual double	UpperLimitZgammaC13 (const double sqrt_s) const
virtual double	xseeWW (const double sqrt_s) const
	Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\). More...
Public Member Functions inherited from StandardModel
double	Ale (double mu, orders order, bool Nf_thr=true) const
	The running electromagnetic coupling \(\alpha_e(\mu)\) in the \(\overline{MS}\) scheme. More...
double	ale_OS (const double mu, orders order=FULLNLO) const
	The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell scheme. More...
double	alphaMz () const
	The electromagnetic coupling at the \(Z\)-mass scale, \(\alpha(M_Z^2)=\alpha/(1-\Delta\alpha(M_Z^2))\). More...
double	Als (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const
	The running QCD coupling \(\alpha(\mu)\) in the \(\overline{MS}\) scheme including QED corrections. More...
double	AlsByOrder (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const
double	Alstilde5 (const double mu) const
	The value of \(\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\) and full EW corrections. More...
double	Beta_e (int nm, unsigned int nf) const
	QED beta function coefficients - eq. (36) hep-ph/0512066. More...
double	Beta_s (int nm, unsigned int nf) const
	QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066. More...
double	c02 () const
	The square of the cosine of the weak mixing angle \(c_0^2\) defined without weak radiative corrections. More...
virtual bool	CheckFlags () const
	A method to check the sanity of the set of model flags. More...
bool	checkSMparamsForEWPO ()
	A method to check whether the parameters relevant to the EWPO are updated. More...
double	computeBrHtobb () const
	The Br \((H\to bb)\) in the Standard Model. More...
double	computeBrHtocc () const
	The Br \((H\to cc)\) in the Standard Model. More...
double	computeBrHtogaga () const
	The Br \((H\to\gamma\gamma)\) in the Standard Model. More...
double	computeBrHtogg () const
	The Br \((H\to gg)\) in the Standard Model. More...
double	computeBrHtomumu () const
	The Br \((H\to \mu\mu)\) in the Standard Model. More...
double	computeBrHtoss () const
	The Br \((H\to ss)\) in the Standard Model. More...
double	computeBrHtotautau () const
	The Br \((H\to \tau\tau)\) in the Standard Model. More...
double	computeBrHtoWW () const
	The Br \((H\to WW)\) in the Standard Model. More...
double	computeBrHtoZga () const
	The Br \((H\to Z\gamma)\) in the Standard Model. More...
double	computeBrHtoZZ () const
	The Br \((H\to ZZ)\) in the Standard Model. More...
double	computeBrHtoZZinv () const
	The Br \((H\to ZZ \to inv)\) in the Standard Model. More...
void	ComputeDeltaR_rem (const double Mw_i, double DeltaR_rem[orders_EW_size]) const
	A method to collect \(\Delta r_{\mathrm{rem}}\) computed via subclasses. More...
void	ComputeDeltaRho (const double Mw_i, double DeltaRho[orders_EW_size]) const
	A method to collect \(\Delta\rho\) computed via subclasses. More...
double	computeGammaHgaga_tt () const
	The top loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
double	computeGammaHgaga_tW () const
	The mixed \(t-W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
double	computeGammaHgaga_WW () const
	The \(W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
double	computeGammaHgg_bb () const
	The bottom loop contribution to \(H\to gg\) in the Standard Model. More...
double	computeGammaHgg_tb () const
	The top-bottom interference contribution to \(H\to gg\) in the Standard Model. More...
double	computeGammaHgg_tt () const
	The top loop contribution to \(H\to gg\) in the Standard Model. More...
double	computeGammaHTotal () const
	The Higgs total width in the Standard Model. More...
double	computeGammaHZga_tt () const
	The top loop contribution to \(H\to Z\gamma\) in the Standard Model. More...
double	computeGammaHZga_tW () const
	The mixed \(t-W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. More...
double	computeGammaHZga_WW () const
	The \(W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. Currently it returns the value of tab 41 in ref. [138]. More...
double	computeSigmaggH (const double sqrt_s) const
	The ggH cross section in the Standard Model. More...
double	computeSigmaggH_bb (const double sqrt_s) const
	The square of the bottom-quark contribution to the ggH cross section in the Standard Model. More...
double	computeSigmaggH_tb (const double sqrt_s) const
	The top-bottom interference contribution to the ggH cross section in the Standard Model. More...
double	computeSigmaggH_tt (const double sqrt_s) const
	The square of the top-quark contribution to the ggH cross section in the Standard Model. More...
double	computeSigmattH (const double sqrt_s) const
	The ttH production cross section in the Standard Model. More...
double	computeSigmaVBF (const double sqrt_s) const
	The VBF cross section in the Standard Model. More...
double	computeSigmaWF (const double sqrt_s) const
	The W fusion contribution \(\sigma_{WF}\) to higgs-production cross section in the Standard Model. More...
double	computeSigmaWH (const double sqrt_s) const
	The WH production cross section in the Standard Model. More...
double	computeSigmaZF (const double sqrt_s) const
	The Z fusion contribution \(\sigma_{ZF}\) to higgs-production cross section in the Standard Model. More...
double	computeSigmaZH (const double sqrt_s) const
	The ZH production cross section in the Standard Model. More...
double	computeSigmaZWF (const double sqrt_s) const
	The Z W interference fusion contribution \(\sigma_{ZWF}\) to higgs-production cross section in the Standard Model. More...
virtual double	cW2 () const
virtual double	cW2 (const double Mw_i) const
	The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as \(c_W^2\). More...
double	DeltaAlpha () const
	The total corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha(M_Z^2)\). More...
double	DeltaAlphaL5q () const
	The sum of the leptonic and the five-flavour hadronic corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha^{\ell+5q}(M_Z^2)\). More...
double	DeltaAlphaLepton (const double s) const
	Leptonic contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{lept}}(s)\). More...
double	DeltaAlphaTop (const double s) const
	Top-quark contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{top}}(s)\). More...
virtual gslpp::complex	deltaKappaZ_f (const Particle f) const
	Flavour non-universal vertex corrections to \(\kappa_Z^l\), denoted by \(\Delta\kappa_Z^l\). More...
virtual double	DeltaR () const
	The SM prediction for \(\Delta r\) derived from that for the \(W\) boson mass. More...
virtual double	DeltaRbar () const
	The SM prediction for \(\Delta \overline{r}\) derived from that for the \(W\)-boson mass. More...
virtual gslpp::complex	deltaRhoZ_f (const Particle f) const
	Flavour non-universal vertex corrections to \(\rho_Z^l\), denoted by \(\Delta\rho_Z^l\). More...
virtual double	epsilon1 () const
	The SM contribution to the epsilon parameter \(\varepsilon_1\). More...
virtual double	epsilon2 () const
	The SM contribution to the epsilon parameter \(\varepsilon_2\). More...
virtual double	epsilon3 () const
	The SM contribution to the epsilon parameter \(\varepsilon_3\). More...
virtual double	epsilonb () const
	The SM contribution to the epsilon parameter \(\varepsilon_b\). More...
virtual double	Gamma_inv () const
	The invisible partial decay width of the \(Z\) boson, \(\Gamma_{\mathrm{inv}}\). More...
virtual double	GammaZ (const Particle f) const
	The \(Z\to \ell\bar{\ell}\) partial decay width, \(\Gamma_\ell\). More...
double	getAle () const
	A get method to retrieve the fine-structure constant \(\alpha\). More...
double	getAlsMz () const
	A get method to access the value of \(\alpha_s(M_Z)\). More...
virtual double	getCBd () const
	The ratio of the absolute value of the $B_d$ mixing amplitude over the Standard Model value. More...
virtual double	getCBs () const
	The ratio of the absolute value of the $B_s$ mixing amplitude over the Standard Model value. More...
virtual double	getCCC1 () const
	A virtual implementation for the RealWeakEFTCC class. More...
virtual double	getCCC2 () const
	A virtual implementation for the RealWeakEFTCC class. More...
virtual double	getCCC3 () const
	A virtual implementation for the RealWeakEFTCC class. More...
virtual double	getCCC4 () const
	A virtual implementation for the RealWeakEFTCC class. More...
virtual double	getCCC5 () const
	A virtual implementation for the RealWeakEFTCC class. More...
virtual double	getCDMK () const
	The ratio of the real part of the $K$ mixing amplitude over the Standard Model value. More...
virtual double	getCepsK () const
	The ratio of the imaginary part of the $K$ mixing amplitude over the Standard Model value. More...
CKM	getCKM () const
	A get method to retrieve the member object of type CKM. More...
double	getDAle5Mz () const
	A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More...
double	getDelGammaZ () const
	A get method to retrieve the theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\). More...
double	getDelMw () const
	A get method to retrieve the theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\). More...
double	getDelR0b () const
	A get method to retrieve the theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More...
double	getDelR0c () const
	A get method to retrieve the theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More...
double	getDelR0l () const
	A get method to retrieve the theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More...
double	getDelSigma0H () const
	A get method to retrieve the theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\). More...
double	getDelSin2th_b () const
	A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More...
double	getDelSin2th_l () const
	A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More...
double	getDelSin2th_q () const
	A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More...
std::string	getFlagKappaZ () const
	A method to retrieve the model flag KappaZ. More...
std::string	getFlagMw () const
	A method to retrieve the model flag Mw. More...
std::string	getFlagRhoZ () const
	A method to retrieve the model flag RhoZ. More...
const Flavour &	getFlavour () const
double	getGF () const
	A get method to retrieve the Fermi constant \(G_\mu\). More...
int	getIterationNo () const
Particle	getLeptons (const QCD::lepton p) const
	A get method to retrieve the member object of a lepton. More...
virtual StandardModelMatching &	getMatching () const
	A get method to access the member reference of type StandardModelMatching. More...
virtual double	getMHl () const
	A get method to retrieve the Higgs mass \(m_h\). More...
virtual double	getmq (const QCD::quark q, const double mu) const
double	getMuw () const
	A get method to retrieve the matching scale \(\mu_W\) around the weak scale. More...
EWSMApproximateFormulae *	getMyApproximateFormulae () const
	A get method to retrieve the member pointer of type EWSMApproximateFormulae. More...
EWSMcache *	getMyEWSMcache () const
	A get method to retrieve the member pointer of type EWSMcache. More...
LeptonFlavour *	getMyLeptonFlavour () const
EWSMOneLoopEW *	getMyOneLoopEW () const
	A get method to retrieve the member pointer of type EWSMOneLoopEW,. More...
EWSMThreeLoopEW *	getMyThreeLoopEW () const
EWSMThreeLoopEW2QCD *	getMyThreeLoopEW2QCD () const
EWSMThreeLoopQCD *	getMyThreeLoopQCD () const
EWSMTwoFermionsLEP2 *	getMyTwoFermionsLEP2 () const
	A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More...
EWSMTwoLoopEW *	getMyTwoLoopEW () const
EWSMTwoLoopQCD *	getMyTwoLoopQCD () const
double	getMz () const
	A get method to access the mass of the \(Z\) boson \(M_Z\). More...
virtual double	getPhiBd () const
	Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More...
virtual double	getPhiBs () const
	Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More...
gslpp::matrix< gslpp::complex >	getUPMNS () const
	A get method to retrieve the object of the PMNS matrix. More...
gslpp::matrix< gslpp::complex >	getVCKM () const
	A get method to retrieve the CKM matrix. More...
gslpp::matrix< gslpp::complex >	getYd () const
	A get method to retrieve the Yukawa matrix of the down-type quarks, \(Y_d\). More...
gslpp::matrix< gslpp::complex >	getYe () const
	A get method to retrieve the Yukawa matrix of the charged leptons, \(Y_e\). More...
gslpp::matrix< gslpp::complex >	getYn () const
	A get method to retrieve the Yukawa matrix of the neutrinos, \(Y_\nu\). More...
gslpp::matrix< gslpp::complex >	getYu () const
	A get method to retrieve the Yukawa matrix of the up-type quarks, \(Y_u\). More...
virtual bool	Init (const std::map< std::string, double > &DPars)
	A method to initialize the model parameters. More...
virtual bool	InitializeModel ()
	A method to initialize the model. More...
bool	IsFlagNoApproximateGammaZ () const
	A method to retrieve the model flag NoApproximateGammaZ. More...
bool	IsFlagWithoutNonUniversalVC () const
	A method to retrieve the model flag WithoutNonUniversalVC. More...
virtual double	LEP2sigmaBottom (const double s) const
virtual double	LEP2sigmaCharm (const double s) const
virtual double	Mw_tree () const
	The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). More...
double	MwbarFromMw (const double Mw) const
	A method to convert the \(W\)-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More...
double	MwFromMwbar (const double Mwbar) const
	A method to convert the \(W\)-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More...
double	Mzbar () const
	The \(Z\)-boson mass \(\overline{M}_Z\) in the complex-pole/fixed-width scheme. More...
virtual bool	PreUpdate ()
	The pre-update method for StandardModel. More...
virtual double	rho_GammaW (const Particle fi, const Particle fj) const
	EW radiative corrections to the width of \(W \to f_i \bar{f}_j\), denoted as \(\rho^W_{ij}\). More...
double	s02 () const
	The square of the sine of the weak mixing angle \(s_0^2\) defined without weak radiative corrections. More...
void	setFlagCacheInStandardModel (bool FlagCacheInStandardModel)
	A set method to change the model flag CacheInStandardModel of StandardModel. More...
void	setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ)
bool	setFlagSigmaForAFB (const bool flagSigmaForAFB_i)
bool	setFlagSigmaForR (const bool flagSigmaForR_i)
virtual bool	setFlagStr (const std::string name, const std::string value)
	A method to set a flag of StandardModel. More...
	StandardModel ()
	The default constructor. More...
double	sW2 () const
virtual double	sW2 (const double Mw_i) const
	The square of the sine of the weak mixing angle in the on-shell scheme, denoted as \(s_W^2\). More...
virtual double	v () const
	The Higgs vacuum expectation value. More...
virtual	~StandardModel ()
	The default destructor. More...
Public Member Functions inherited from QCD
double	AboveTh (const double mu) const
	The active flavour threshold above the scale \(\mu\) as defined in QCD::Thresholds(). More...
void	addParameters (std::vector< std::string > params_i)
	A method to add parameters that are specific to only one set of observables. More...
virtual double	Als (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const
double	Als4 (const double mu) const
	The value of \(\alpha_s^{\mathrm{FULLNLO}}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\). More...
virtual double	AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const
double	AlsOLD (const double mu, const orders order=FULLNLO) const
	Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...
double	AlsWithInit (const double mu, const double alsi, const double mu_i, const orders order) const
	Computes the running strong coupling \(\alpha_s(\mu)\) from \(\alpha_s(\mu_i)\) in the \(\overline{\mathrm{MS}}\) scheme, where it is forbidden to across a flavour threshold in the RG running from \(\mu_i\) to \(\mu\). More...
double	AlsWithLambda (const double mu, const orders order) const
	Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme with the use of \(\Lambda_{\rm QCD}\). More...
double	BelowTh (const double mu) const
	The active flavour threshold below the scale \(\mu\) as defined in QCD::Thresholds(). More...
double	Beta0 (const double nf) const
	The \(\beta_0(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
double	Beta1 (const double nf) const
	The \(\beta_1(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
double	Beta2 (const double nf) const
	The \(\beta_2(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
double	Beta3 (const double nf) const
	The \(\beta_3(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
void	CacheShift (double cache[][5], int n) const
	A member used to manage the caching for this class. More...
void	CacheShift (int cache[][5], int n) const
orders	FullOrder (orders order) const
	Return the FULLORDER enum corresponding to order. More...
double	Gamma0 (const double nf) const
	The \(\gamma_0\) coefficient used to compute the running of a mass. More...
double	Gamma1 (const double nf) const
	The \(\gamma_1\) coefficient used to compute the running of a mass. More...
double	Gamma2 (const double nf) const
	The \(\gamma_2\) coefficient used to compute the running of a mass. More...
double	getAlsM () const
	A get method to access the value of \(\alpha_s(M_{\alpha_s})\). More...
BParameter	getBBd () const
	For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More...
BParameter	getBBs () const
	For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More...
BParameter	getBD () const
	For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta c = 2\) process in the \(D^0\) meson system. More...
BParameter	getBK () const
	For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta s = 2\) process in the \(K^0\) meson system. More...
BParameter	getBKd1 () const
BParameter	getBKd3 () const
double	getCF () const
	A get method to access the Casimir factor of QCD. More...
double	getMAls () const
	A get method to access the mass scale \(M_{\alpha_s}\) at which the strong coupling constant measurement is provided. More...
Meson	getMesons (const QCD::meson m) const
	A get method to access a meson as an object of the type Meson. More...
double	getMtpole () const
	A get method to access the pole mass of the top quark. More...
double	getMub () const
	A get method to access the threshold between five- and four-flavour theory in GeV. More...
double	getMuc () const
	A get method to access the threshold between four- and three-flavour theory in GeV. More...
double	getMut () const
	A get method to access the threshold between six- and five-flavour theory in GeV. More...
double	getNc () const
	A get method to access the number of colours \(N_c\). More...
double	getOptionalParameter (std::string name) const
	A method to get parameters that are specific to only one set of observables. More...
Particle	getQuarks (const QCD::quark q) const
	A get method to access a quark as an object of the type Particle. More...
std::vector< std::string >	getUnknownParameters ()
	A method to get the vector of the parameters that have been specified in the configuration file but not being used. More...
void	initializeBParameter (std::string name_i) const
	A method to initialize B Parameter and the corresponding meson. More...
void	initializeMeson (QCD::meson meson_i) const
	A method to initialize a meson. More...
double	logLambda (const double nf, orders order) const
	Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More...
double	Mbar2Mp (const double mbar, const orders order=FULLNNLO) const
	Converts the \(\overline{\mathrm{MS}}\) mass \(m(m)\) to the pole mass. More...
double	Mp2Mbar (const double mp, const orders order=FULLNNLO) const
	Converts a quark pole mass to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More...
double	Mrun (const double mu, const double m, const orders order=FULLNNLO) const
	Computes a running quark mass \(m(\mu)\) from \(m(m)\). More...
double	Mrun (const double mu_f, const double mu_i, const double m, const orders order=FULLNNLO) const
	Runs a quark mass from \(\mu_i\) to \(\mu_f\). More...
double	Mrun4 (const double mu_f, const double mu_i, const double m) const
	The running of a mass with the number of flavours \(n_f = 4\). More...
double	MS2DRqmass (const double MSbar) const
	Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More...
double	MS2DRqmass (const double MSscale, const double MSbar) const
	Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More...
double	Nf (const double mu) const
	The number of active flavour at scale \(\mu\). More...
double	NfThresholdCorrections (double mu, double M, double als, int nf, orders order) const
	Threshold corrections in matching \(\alpha_s(n_f+1)\) with \(\alpha_s(n_f)\) from eq. (34) of hep-ph/0512060. More...
std::string	orderToString (const orders order) const
	Converts an object of the enum type "orders" to the corresponding string. More...
	QCD ()
	Constructor. More...
void	setNc (double Nc)
	A set method to change the number of colours \(N_c\). More...
void	setOptionalParameter (std::string name, double value)
	A method to set the parameter value for the parameters that are specific to only one set of observables. More...
double	Thresholds (const int i) const
	For accessing the active flavour threshold scales. More...
Public Member Functions inherited from Model
void	addMissingModelParameter (const std::string &missingParameterName)
std::vector< std::string >	getmissingModelParameters ()
unsigned int	getMissingModelParametersCount ()
std::string	getModelName () const
	A method to fetch the name of the model. More...
const double &	getModelParam (std::string name) const
bool	isModelFWC_DF2 () const
bool	isModelGeneralTHDM () const
bool	isModelGeorgiMachacek () const
bool	IsModelInitialized () const
	A method to check if the model is initialized. More...
bool	isModelLinearized () const
bool	isModelParam (std::string name) const
bool	isModelSUSY () const
bool	isModelTHDM () const
bool	isModelTHDMW () const
bool	IsUpdateError () const
	A method to check if there was any error in the model update process. More...
	Model ()
	The default constructor. More...
void	raiseMissingModelParameterCount ()
void	setModelFWC_DF2 ()
void	setModelGeneralTHDM ()
void	setModelGeorgiMachacek ()
void	setModelInitialized (bool ModelInitialized)
	A set method to fix the failure or success of the initialization of the model. More...
void	setModelLinearized (bool linearized=true)
void	setModelName (const std::string name)
	A method to set the name of the model. More...
void	setModelSUSY ()
void	setModelTHDM ()
void	setModelTHDMW ()
void	setSliced (bool Sliced)
void	setUpdateError (bool UpdateError)
	A set method to fix the update status as success or failure. More...
virtual	~Model ()
	The default destructor. More...

Static Public Attributes
static const int	NNPEffectiveGIMRVars = 331
	The number of the model parameters in NPEffectiveGIMR. More...
static const int	NNPEffectiveGIMRVars_LFU_QFU = 121
	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 = 33
	The number of the SM parameters that are relevant to the EW precision observables. More...
static std::string	SMvars [NSMvars]
	A string array containing the labels of the model parameters in StandardModel. More...
Static Public Attributes inherited from QCD
static const int	NQCDvars = 11
	The number of model parameters in QCD. More...
static std::string	QCDvars [NQCDvars]
	An array containing the labels under which all QCD parameters are stored in a vector of ModelParameter via InputParser::ReadParameters(). More...

Protected Member Functions
gslpp::complex	CfB_diag (const Particle f) const
	The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f. More...
gslpp::complex	CfG_diag (const Particle f) const
	The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f. More...
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...
gslpp::complex	CfW_diag (const Particle f) const
	The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) 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
double	AFB_NoISR_l (const QCD::lepton l_flavor, const double s) const
double	AFB_NoISR_q (const QCD::quark q_flavor, const double s) const
bool	checkEWPOscheme (const std::string scheme) const
	A method to check if a given scheme name in string form is valid. More...
virtual void	computeCKM ()
	The method to compute the CKM matrix. More...
virtual void	computeYukawas ()
	The method to compute the Yukawa matrices. More...
double	Delta_EWQCD (const QCD::quark q) const
	The non-factorizable EW-QCD corrections to the partial widths for \(Z\to q\bar{q}\), denoted as \(\Delta_{\mathrm{EW/QCD}}\). More...
double	getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const
double	getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const
double	getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const
double	getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const
double	getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const
double	getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const
double	getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const
double	getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const
double	getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const
double	getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const
double	getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const
double	getIntegrand_AFBnumeratorWithISR_charm133 (double x) const
double	getIntegrand_AFBnumeratorWithISR_charm167 (double x) const
double	getIntegrand_AFBnumeratorWithISR_charm172 (double x) const
double	getIntegrand_AFBnumeratorWithISR_charm183 (double x) const
double	getIntegrand_AFBnumeratorWithISR_charm189 (double x) const
double	getIntegrand_AFBnumeratorWithISR_charm192 (double x) const
double	getIntegrand_AFBnumeratorWithISR_charm196 (double x) const
double	getIntegrand_AFBnumeratorWithISR_charm200 (double x) const
double	getIntegrand_AFBnumeratorWithISR_charm202 (double x) const
double	getIntegrand_AFBnumeratorWithISR_charm205 (double x) const
double	getIntegrand_AFBnumeratorWithISR_charm207 (double x) const
double	getIntegrand_AFBnumeratorWithISR_mu130 (double x) const
double	getIntegrand_AFBnumeratorWithISR_mu136 (double x) const
double	getIntegrand_AFBnumeratorWithISR_mu161 (double x) const
double	getIntegrand_AFBnumeratorWithISR_mu172 (double x) const
double	getIntegrand_AFBnumeratorWithISR_mu183 (double x) const
double	getIntegrand_AFBnumeratorWithISR_mu189 (double x) const
double	getIntegrand_AFBnumeratorWithISR_mu192 (double x) const
double	getIntegrand_AFBnumeratorWithISR_mu196 (double x) const
double	getIntegrand_AFBnumeratorWithISR_mu200 (double x) const
double	getIntegrand_AFBnumeratorWithISR_mu202 (double x) const
double	getIntegrand_AFBnumeratorWithISR_mu205 (double x) const
double	getIntegrand_AFBnumeratorWithISR_mu207 (double x) const
double	getIntegrand_AFBnumeratorWithISR_tau130 (double x) const
double	getIntegrand_AFBnumeratorWithISR_tau136 (double x) const
double	getIntegrand_AFBnumeratorWithISR_tau161 (double x) const
double	getIntegrand_AFBnumeratorWithISR_tau172 (double x) const
double	getIntegrand_AFBnumeratorWithISR_tau183 (double x) const
double	getIntegrand_AFBnumeratorWithISR_tau189 (double x) const
double	getIntegrand_AFBnumeratorWithISR_tau192 (double x) const
double	getIntegrand_AFBnumeratorWithISR_tau196 (double x) const
double	getIntegrand_AFBnumeratorWithISR_tau200 (double x) const
double	getIntegrand_AFBnumeratorWithISR_tau202 (double x) const
double	getIntegrand_AFBnumeratorWithISR_tau205 (double x) const
double	getIntegrand_AFBnumeratorWithISR_tau207 (double x) const
double	getIntegrand_dsigmaBox_bottom130 (double x) const
double	getIntegrand_dsigmaBox_bottom133 (double x) const
double	getIntegrand_dsigmaBox_bottom136 (double x) const
double	getIntegrand_dsigmaBox_bottom161 (double x) const
double	getIntegrand_dsigmaBox_bottom167 (double x) const
double	getIntegrand_dsigmaBox_bottom172 (double x) const
double	getIntegrand_dsigmaBox_bottom183 (double x) const
double	getIntegrand_dsigmaBox_bottom189 (double x) const
double	getIntegrand_dsigmaBox_bottom192 (double x) const
double	getIntegrand_dsigmaBox_bottom196 (double x) const
double	getIntegrand_dsigmaBox_bottom200 (double x) const
double	getIntegrand_dsigmaBox_bottom202 (double x) const
double	getIntegrand_dsigmaBox_bottom205 (double x) const
double	getIntegrand_dsigmaBox_bottom207 (double x) const
double	getIntegrand_dsigmaBox_charm130 (double x) const
double	getIntegrand_dsigmaBox_charm133 (double x) const
double	getIntegrand_dsigmaBox_charm136 (double x) const
double	getIntegrand_dsigmaBox_charm161 (double x) const
double	getIntegrand_dsigmaBox_charm167 (double x) const
double	getIntegrand_dsigmaBox_charm172 (double x) const
double	getIntegrand_dsigmaBox_charm183 (double x) const
double	getIntegrand_dsigmaBox_charm189 (double x) const
double	getIntegrand_dsigmaBox_charm192 (double x) const
double	getIntegrand_dsigmaBox_charm196 (double x) const
double	getIntegrand_dsigmaBox_charm200 (double x) const
double	getIntegrand_dsigmaBox_charm202 (double x) const
double	getIntegrand_dsigmaBox_charm205 (double x) const
double	getIntegrand_dsigmaBox_charm207 (double x) const
double	getIntegrand_dsigmaBox_down130 (double x) const
double	getIntegrand_dsigmaBox_down133 (double x) const
double	getIntegrand_dsigmaBox_down136 (double x) const
double	getIntegrand_dsigmaBox_down161 (double x) const
double	getIntegrand_dsigmaBox_down167 (double x) const
double	getIntegrand_dsigmaBox_down172 (double x) const
double	getIntegrand_dsigmaBox_down183 (double x) const
double	getIntegrand_dsigmaBox_down189 (double x) const
double	getIntegrand_dsigmaBox_down192 (double x) const
double	getIntegrand_dsigmaBox_down196 (double x) const
double	getIntegrand_dsigmaBox_down200 (double x) const
double	getIntegrand_dsigmaBox_down202 (double x) const
double	getIntegrand_dsigmaBox_down205 (double x) const
double	getIntegrand_dsigmaBox_down207 (double x) const
double	getIntegrand_dsigmaBox_mu130 (double x) const
double	getIntegrand_dsigmaBox_mu133 (double x) const
double	getIntegrand_dsigmaBox_mu136 (double x) const
double	getIntegrand_dsigmaBox_mu161 (double x) const
double	getIntegrand_dsigmaBox_mu167 (double x) const
double	getIntegrand_dsigmaBox_mu172 (double x) const
double	getIntegrand_dsigmaBox_mu183 (double x) const
double	getIntegrand_dsigmaBox_mu189 (double x) const
double	getIntegrand_dsigmaBox_mu192 (double x) const
double	getIntegrand_dsigmaBox_mu196 (double x) const
double	getIntegrand_dsigmaBox_mu200 (double x) const
double	getIntegrand_dsigmaBox_mu202 (double x) const
double	getIntegrand_dsigmaBox_mu205 (double x) const
double	getIntegrand_dsigmaBox_mu207 (double x) const
double	getIntegrand_dsigmaBox_strange130 (double x) const
double	getIntegrand_dsigmaBox_strange133 (double x) const
double	getIntegrand_dsigmaBox_strange136 (double x) const
double	getIntegrand_dsigmaBox_strange161 (double x) const
double	getIntegrand_dsigmaBox_strange167 (double x) const
double	getIntegrand_dsigmaBox_strange172 (double x) const
double	getIntegrand_dsigmaBox_strange183 (double x) const
double	getIntegrand_dsigmaBox_strange189 (double x) const
double	getIntegrand_dsigmaBox_strange192 (double x) const
double	getIntegrand_dsigmaBox_strange196 (double x) const
double	getIntegrand_dsigmaBox_strange200 (double x) const
double	getIntegrand_dsigmaBox_strange202 (double x) const
double	getIntegrand_dsigmaBox_strange205 (double x) const
double	getIntegrand_dsigmaBox_strange207 (double x) const
double	getIntegrand_dsigmaBox_tau130 (double x) const
double	getIntegrand_dsigmaBox_tau133 (double x) const
double	getIntegrand_dsigmaBox_tau136 (double x) const
double	getIntegrand_dsigmaBox_tau161 (double x) const
double	getIntegrand_dsigmaBox_tau167 (double x) const
double	getIntegrand_dsigmaBox_tau172 (double x) const
double	getIntegrand_dsigmaBox_tau183 (double x) const
double	getIntegrand_dsigmaBox_tau189 (double x) const
double	getIntegrand_dsigmaBox_tau192 (double x) const
double	getIntegrand_dsigmaBox_tau196 (double x) const
double	getIntegrand_dsigmaBox_tau200 (double x) const
double	getIntegrand_dsigmaBox_tau202 (double x) const
double	getIntegrand_dsigmaBox_tau205 (double x) const
double	getIntegrand_dsigmaBox_tau207 (double x) const
double	getIntegrand_dsigmaBox_up130 (double x) const
double	getIntegrand_dsigmaBox_up133 (double x) const
double	getIntegrand_dsigmaBox_up136 (double x) const
double	getIntegrand_dsigmaBox_up161 (double x) const
double	getIntegrand_dsigmaBox_up167 (double x) const
double	getIntegrand_dsigmaBox_up172 (double x) const
double	getIntegrand_dsigmaBox_up183 (double x) const
double	getIntegrand_dsigmaBox_up189 (double x) const
double	getIntegrand_dsigmaBox_up192 (double x) const
double	getIntegrand_dsigmaBox_up196 (double x) const
double	getIntegrand_dsigmaBox_up200 (double x) const
double	getIntegrand_dsigmaBox_up202 (double x) const
double	getIntegrand_dsigmaBox_up205 (double x) const
double	getIntegrand_dsigmaBox_up207 (double x) const
double	getIntegrand_sigmaWithISR_bottom130 (double x) const
double	getIntegrand_sigmaWithISR_bottom133 (double x) const
double	getIntegrand_sigmaWithISR_bottom136 (double x) const
double	getIntegrand_sigmaWithISR_bottom161 (double x) const
double	getIntegrand_sigmaWithISR_bottom167 (double x) const
double	getIntegrand_sigmaWithISR_bottom172 (double x) const
double	getIntegrand_sigmaWithISR_bottom183 (double x) const
double	getIntegrand_sigmaWithISR_bottom189 (double x) const
double	getIntegrand_sigmaWithISR_bottom192 (double x) const
double	getIntegrand_sigmaWithISR_bottom196 (double x) const
double	getIntegrand_sigmaWithISR_bottom200 (double x) const
double	getIntegrand_sigmaWithISR_bottom202 (double x) const
double	getIntegrand_sigmaWithISR_bottom205 (double x) const
double	getIntegrand_sigmaWithISR_bottom207 (double x) const
double	getIntegrand_sigmaWithISR_charm130 (double x) const
double	getIntegrand_sigmaWithISR_charm133 (double x) const
double	getIntegrand_sigmaWithISR_charm136 (double x) const
double	getIntegrand_sigmaWithISR_charm161 (double x) const
double	getIntegrand_sigmaWithISR_charm167 (double x) const
double	getIntegrand_sigmaWithISR_charm172 (double x) const
double	getIntegrand_sigmaWithISR_charm183 (double x) const
double	getIntegrand_sigmaWithISR_charm189 (double x) const
double	getIntegrand_sigmaWithISR_charm192 (double x) const
double	getIntegrand_sigmaWithISR_charm196 (double x) const
double	getIntegrand_sigmaWithISR_charm200 (double x) const
double	getIntegrand_sigmaWithISR_charm202 (double x) const
double	getIntegrand_sigmaWithISR_charm205 (double x) const
double	getIntegrand_sigmaWithISR_charm207 (double x) const
double	getIntegrand_sigmaWithISR_down130 (double x) const
double	getIntegrand_sigmaWithISR_down133 (double x) const
double	getIntegrand_sigmaWithISR_down136 (double x) const
double	getIntegrand_sigmaWithISR_down161 (double x) const
double	getIntegrand_sigmaWithISR_down167 (double x) const
double	getIntegrand_sigmaWithISR_down172 (double x) const
double	getIntegrand_sigmaWithISR_down183 (double x) const
double	getIntegrand_sigmaWithISR_down189 (double x) const
double	getIntegrand_sigmaWithISR_down192 (double x) const
double	getIntegrand_sigmaWithISR_down196 (double x) const
double	getIntegrand_sigmaWithISR_down200 (double x) const
double	getIntegrand_sigmaWithISR_down202 (double x) const
double	getIntegrand_sigmaWithISR_down205 (double x) const
double	getIntegrand_sigmaWithISR_down207 (double x) const
double	getIntegrand_sigmaWithISR_mu130 (double x) const
double	getIntegrand_sigmaWithISR_mu136 (double x) const
double	getIntegrand_sigmaWithISR_mu161 (double x) const
double	getIntegrand_sigmaWithISR_mu172 (double x) const
double	getIntegrand_sigmaWithISR_mu183 (double x) const
double	getIntegrand_sigmaWithISR_mu189 (double x) const
double	getIntegrand_sigmaWithISR_mu192 (double x) const
double	getIntegrand_sigmaWithISR_mu196 (double x) const
double	getIntegrand_sigmaWithISR_mu200 (double x) const
double	getIntegrand_sigmaWithISR_mu202 (double x) const
double	getIntegrand_sigmaWithISR_mu205 (double x) const
double	getIntegrand_sigmaWithISR_mu207 (double x) const
double	getIntegrand_sigmaWithISR_strange130 (double x) const
double	getIntegrand_sigmaWithISR_strange133 (double x) const
double	getIntegrand_sigmaWithISR_strange136 (double x) const
double	getIntegrand_sigmaWithISR_strange161 (double x) const
double	getIntegrand_sigmaWithISR_strange167 (double x) const
double	getIntegrand_sigmaWithISR_strange172 (double x) const
double	getIntegrand_sigmaWithISR_strange183 (double x) const
double	getIntegrand_sigmaWithISR_strange189 (double x) const
double	getIntegrand_sigmaWithISR_strange192 (double x) const
double	getIntegrand_sigmaWithISR_strange196 (double x) const
double	getIntegrand_sigmaWithISR_strange200 (double x) const
double	getIntegrand_sigmaWithISR_strange202 (double x) const
double	getIntegrand_sigmaWithISR_strange205 (double x) const
double	getIntegrand_sigmaWithISR_strange207 (double x) const
double	getIntegrand_sigmaWithISR_tau130 (double x) const
double	getIntegrand_sigmaWithISR_tau136 (double x) const
double	getIntegrand_sigmaWithISR_tau161 (double x) const
double	getIntegrand_sigmaWithISR_tau172 (double x) const
double	getIntegrand_sigmaWithISR_tau183 (double x) const
double	getIntegrand_sigmaWithISR_tau189 (double x) const
double	getIntegrand_sigmaWithISR_tau192 (double x) const
double	getIntegrand_sigmaWithISR_tau196 (double x) const
double	getIntegrand_sigmaWithISR_tau200 (double x) const
double	getIntegrand_sigmaWithISR_tau202 (double x) const
double	getIntegrand_sigmaWithISR_tau205 (double x) const
double	getIntegrand_sigmaWithISR_tau207 (double x) const
double	getIntegrand_sigmaWithISR_up130 (double x) const
double	getIntegrand_sigmaWithISR_up133 (double x) const
double	getIntegrand_sigmaWithISR_up136 (double x) const
double	getIntegrand_sigmaWithISR_up161 (double x) const
double	getIntegrand_sigmaWithISR_up167 (double x) const
double	getIntegrand_sigmaWithISR_up172 (double x) const
double	getIntegrand_sigmaWithISR_up183 (double x) const
double	getIntegrand_sigmaWithISR_up189 (double x) const
double	getIntegrand_sigmaWithISR_up192 (double x) const
double	getIntegrand_sigmaWithISR_up196 (double x) const
double	getIntegrand_sigmaWithISR_up200 (double x) const
double	getIntegrand_sigmaWithISR_up202 (double x) const
double	getIntegrand_sigmaWithISR_up205 (double x) const
double	getIntegrand_sigmaWithISR_up207 (double x) const
double	Integrand_AFBnumeratorWithISR_l (double x, const QCD::lepton l_flavor, const double s) const
double	Integrand_AFBnumeratorWithISR_q (double x, const QCD::quark q_flavor, const double s) const
double	Integrand_dsigmaBox_l (double cosTheta, const QCD::lepton l_flavor, const double s) const
double	Integrand_dsigmaBox_q (double cosTheta, const QCD::quark q_flavor, const double s) const
double	Integrand_sigmaWithISR_l (double x, const QCD::lepton l_flavor, const double s) const
double	Integrand_sigmaWithISR_q (double x, const QCD::quark q_flavor, const double s) const
double	m_q (const QCD::quark q, const double mu, const orders order=FULLNLO) const
double	RAq (const QCD::quark q) const
	The radiator factor associated with the final-state QED and QCD corrections to the the axial-vector-current interactions, \(R_A^q(M_Z^2)\). More...
double	resumKappaZ (const double DeltaRho[orders_EW_size], const double deltaKappa_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
	A method to compute the real part of the effetvive coupling \(\kappa_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More...
double	resumMw (const double Mw_i, const double DeltaRho[orders_EW_size], const double DeltaR_rem[orders_EW_size]) const
	A method to compute the \(W\)-boson mass from \(\Delta\rho\) and \(\Delta r_{\mathrm{rem}}\). More...
double	resumRhoZ (const double DeltaRho[orders_EW_size], const double deltaRho_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
	A method to compute the real part of the effective coupling \(\rho_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More...
double	RVh () const
	The singlet vector corrections to the hadronic \(Z\)-boson width, denoted as \(R_V^h\). More...
double	RVq (const QCD::quark q) const
	The radiator factor associated with the final-state QED and QCD corrections to the the vector-current interactions, \(R_V^q(M_Z^2)\). More...
double	SchemeToDouble (const std::string scheme) const
	A method to convert a given scheme name in string form into a floating-point number with double precision. More...
double	sigma_NoISR_l (const QCD::lepton l_flavor, const double s) const
double	sigma_NoISR_q (const QCD::quark q_flavor, const double s) const
double	taub () const
	Top-mass corrections to the \(Zb\bar{b}\) vertex, denoted by \(\tau_b\). More...
Protected Member Functions inherited from QCD
double	MassOfNf (int nf) const
	The Mbar mass of the heaviest quark in the theory with Nf active flavour. More...

Protected Attributes
double	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	Ced_1111
double	Ced_1122
double	Ced_1123
double	Ced_1132
double	Ced_1133
double	Ced_2211
double	Ced_2223
double	Ced_2232
double	Ced_3311
double	Ced_3323
double	Ced_3332
double	Cee_1111
double	Cee_1122
double	Cee_1133
double	Cee_2211
double	Cee_3311
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	Ceu_1111
double	Ceu_1122
double	Ceu_1133
double	Ceu_2211
double	Ceu_3311
double	CG
	The dimension-6 operator coefficient \(C_{G}\). 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	CLd_1111
double	CLd_1122
double	CLd_1123
double	CLd_1132
double	CLd_1133
double	CLd_2211
double	CLd_2223
double	CLd_2232
double	CLd_3311
double	CLd_3323
double	CLd_3332
double	CLe_1111
double	CLe_1122
double	CLe_1133
double	CLe_2211
double	CLe_3311
double	CLL_1111
double	CLL_1122
double	CLL_1133
double	CLL_1221
double	CLL_1331
double	CLL_2112
double	CLL_2211
double	CLL_3113
double	CLL_3311
double	CLQ1_1111
double	CLQ1_1122
double	CLQ1_1123
double	CLQ1_1132
double	CLQ1_1133
double	CLQ1_1221
double	CLQ1_1331
double	CLQ1_2112
double	CLQ1_2211
double	CLQ1_2223
double	CLQ1_2232
double	CLQ1_3113
double	CLQ1_3311
double	CLQ1_3323
double	CLQ1_3332
double	CLQ3_1111
double	CLQ3_1122
double	CLQ3_1123
double	CLQ3_1132
double	CLQ3_1133
double	CLQ3_1221
double	CLQ3_1331
double	CLQ3_2112
double	CLQ3_2211
double	CLQ3_2223
double	CLQ3_2232
double	CLQ3_3113
double	CLQ3_3311
double	CLQ3_3323
double	CLQ3_3332
double	CLu_1111
double	CLu_1122
double	CLu_1133
double	CLu_2211
double	CLu_3311
double	CQe_1111
double	CQe_1122
double	CQe_1133
double	CQe_2211
double	CQe_2311
double	CQe_2322
double	CQe_2333
double	CQe_3211
double	CQe_3222
double	CQe_3233
double	CQe_3311
double	CuB_11i
	The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part). More...
double	CuB_11r
	The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part). More...
double	CuB_12i
	The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part). More...
double	CuB_12r
	The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part). More...
double	CuB_13i
	The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part). More...
double	CuB_13r
	The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part). More...
double	CuB_22i
	The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part). More...
double	CuB_22r
	The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part). More...
double	CuB_23i
	The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part). More...
double	CuB_23r
	The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part). More...
double	CuB_33i
	The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part). More...
double	CuB_33r
	The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part). More...
double	CuG_11i
	The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part). More...
double	CuG_11r
	The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part). More...
double	CuG_12i
	The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part). More...
double	CuG_12r
	The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part). More...
double	CuG_13i
	The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part). More...
double	CuG_13r
	The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part). More...
double	CuG_22i
	The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part). More...
double	CuG_22r
	The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part). More...
double	CuG_23i
	The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part). More...
double	CuG_23r
	The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part). More...
double	CuG_33i
	The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part). More...
double	CuG_33r
	The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part). 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	CuW_11i
	The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part). More...
double	CuW_11r
	The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part). More...
double	CuW_12i
	The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part). More...
double	CuW_12r
	The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part). More...
double	CuW_13i
	The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part). More...
double	CuW_13r
	The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part). More...
double	CuW_22i
	The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part). More...
double	CuW_22r
	The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part). More...
double	CuW_23i
	The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part). More...
double	CuW_23r
	The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part). More...
double	CuW_33i
	The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part). More...
double	CuW_33r
	The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part). More...
double	CW
	The dimension-6 operator coefficient \(C_{W}\). 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...
const LEP2GIMR	myLEP2GIMR
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	alpha21
double	alpha31
double	AlsMz
	The strong coupling constant at the Z-boson mass, \(\alpha_s(M_Z)\). More...
bool	bSigmaForAFB
bool	bSigmaForR
double	dAle5Mz
	The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More...
double	delGammaZ
	The theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\), in GeV. More...
double	delMw
	The theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\), in GeV. More...
double	delR0b
	The theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More...
double	delR0c
	The theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More...
double	delR0l
	The theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More...
double	delsigma0H
	The theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\) in nb. More...
double	delSin2th_b
	The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More...
double	delSin2th_l
	The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More...
double	delSin2th_q
	The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More...
double	delta
double	etab
	The CKM parameter \(\bar{\eta}\) in the Wolfenstein parameterization. More...
bool	flag_order [orders_EW_size]
	An array of internal flags controlling the inclusions of higher-order corrections. More...
bool	flagLEP2 [NUMofLEP2RCs]
double	gamma
	\(\gamma \) used as an input for FlagWolfenstein = FALSE More...
double	GF
	The Fermi constant \(G_\mu\) in \({\rm GeV}^{-2}\). More...
double	lambda
	The CKM parameter \(\lambda\) in the Wolfenstein parameterization. More...
Particle	leptons [6]
	An array of Particle objects for the leptons. More...
double	mHl
	The Higgs mass \(m_h\) in GeV. More...
double	muw
	A matching scale \(\mu_W\) around the weak scale in GeV. More...
CKM	myCKM
	An object of type CKM. More...
PMNS	myPMNS
double	Mz
	The mass of the \(Z\) boson in GeV. More...
bool	requireCKM
	An internal flag to control whether the CKM matrix has to be recomputed. More...
bool	requireYe
	An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed. More...
bool	requireYn
	An internal flag to control whether the neutrino Yukawa matrix has to be recomputed. More...
double	rhob
	The CKM parameter \(\bar{\rho}\) in the Wolfenstein parameterization. More...
double	s12
double	s13
double	s23
Flavour	SMFlavour
	An object of type Flavour. More...
Matching< StandardModelMatching, StandardModel >	SMM
	An object of type Matching. More...
double	Vcb
	\(\vert V_{cb} \vert \) used as an input for FlagWolfenstein = FALSE More...
double	Vub
	\(\vert V_{ub} \vert \) used as an input for FlagWolfenstein = FALSE More...
double	Vus
	\(\vert V_{us} \vert \) used as an input for FlagWolfenstein = FALSE More...
gslpp::matrix< gslpp::complex >	Yd
	The Yukawa matrix of the down-type quarks. More...
gslpp::matrix< gslpp::complex >	Ye
	The Yukawa matrix of the charged leptons. More...
gslpp::matrix< gslpp::complex >	Yn
	The Yukawa matrix of the neutrinos. More...
gslpp::matrix< gslpp::complex >	Yu
	The Yukawa matrix of the up-type quarks. More...
Protected Attributes inherited from QCD
double	AlsM
	The strong coupling constant at the mass scale MAls, \(\alpha_s(M_{\alpha_s})\). More...
double	CA
double	CF
bool	computemt
	Switch for computing the \(\overline{\mathrm{MS}}\) mass of the top quark. More...
double	dAdA_NA
double	dFdA_NA
double	dFdF_NA
double	MAls
	The mass scale in GeV at which the strong coupling measurement is provided. More...
double	mtpole
	The pole mass of the top quark. More...
double	mub
	The threshold between five- and four-flavour theory in GeV. More...
double	muc
	The threshold between four- and three-flavour theory in GeV. More...
double	mut
	The threshold between six- and five-flavour theory in GeV. More...
double	NA
double	Nc
	The number of colours. More...
Particle	quarks [6]
	The vector of all SM quarks. More...
bool	requireYd
	Switch for generating the Yukawa couplings to the down-type quarks. More...
bool	requireYu
	Switch for generating the Yukawa couplings to the up-type quarks. More...
double	TF
Protected Attributes inherited from Model
bool	isSliced
	A boolean set to true if the current istance is a slice of an extended object. More...
std::map< std::string, std::reference_wrapper< const double > >	ModelParamMap
bool	UpdateError
	A boolean set to false if update is successful. More...

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	LEP2RCs { Weak = 0, WeakBox, ISR, QEDFSR, QCDFSR, NUMofLEP2RCs }
enum	orders_EW { EW1 = 0, EW1QCD1, EW1QCD2, EW2, EW2QCD1, EW3, orders_EW_size }
	An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More...
Public Types inherited from QCD
enum	lepton { NEUTRINO_1, ELECTRON, NEUTRINO_2, MU, NEUTRINO_3, TAU, NOLEPTON }
	An enum type for leptons. More...
enum	meson { P_0, P_P, K_0, K_P, D_0, D_P, B_D, B_P, B_S, B_C, PHI, K_star, K_star_P, D_star_P, RHO, RHO_P, OMEGA, MESON_END }
	An enum type for mesons. More...
enum	quark { UP, DOWN, CHARM, STRANGE, TOP, BOTTOM }
	An enum type for quarks. More...

Constructor & Destructor Documentation

NPEffectiveGIMR()

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 106 of file NPEffectiveGIMR.cpp.

: NPbase(), myLEP2GIMR(trueSM), FlagLeptonUniversal(FlagLeptonUniversal_in), FlagQuarkUniversal(FlagQuarkUniversal_in)
{
    if ((!FlagLeptonUniversal && FlagQuarkUniversal)
            || (FlagLeptonUniversal && !FlagQuarkUniversal))
        throw std::runtime_error("Invalid arguments for NPEffectiveGIMR::NPEffectiveGIMR()");
 
    FlagMwInput = false;
    FlagQuadraticTerms = false;
    setModelLinearized();
 
    ModelParamMap.insert(std::make_pair("CG", std::cref(CG)));
    ModelParamMap.insert(std::make_pair("CW", std::cref(CW)));
    ModelParamMap.insert(std::make_pair("CHG", std::cref(CHG)));
    ModelParamMap.insert(std::make_pair("CHW", std::cref(CHW)));
    ModelParamMap.insert(std::make_pair("CHB", std::cref(CHB)));
    ModelParamMap.insert(std::make_pair("CHWB", std::cref(CHWB)));
    ModelParamMap.insert(std::make_pair("CHD", std::cref(CHD)));
    ModelParamMap.insert(std::make_pair("CHbox", std::cref(CHbox)));
    ModelParamMap.insert(std::make_pair("CH", std::cref(CH)));
    if (FlagLeptonUniversal) {
        ModelParamMap.insert(std::make_pair("CHL1", std::cref(CHL1_11)));
        ModelParamMap.insert(std::make_pair("CHL3", std::cref(CHL3_11)));
        ModelParamMap.insert(std::make_pair("CHe", std::cref(CHe_11)));
        ModelParamMap.insert(std::make_pair("CeH_r", std::cref(CeH_11r)));
        ModelParamMap.insert(std::make_pair("CeH_i", std::cref(CeH_11i)));
        ModelParamMap.insert(std::make_pair("CLL", std::cref(CLL_1221)));
        ModelParamMap.insert(std::make_pair("Cee", std::cref(Cee_1111)));
        ModelParamMap.insert(std::make_pair("CLe", std::cref(CLe_1111)));
    } else {
        ModelParamMap.insert(std::make_pair("CHL1_11", std::cref(CHL1_11)));
        ModelParamMap.insert(std::make_pair("CHL1_12r", std::cref(CHL1_12r)));
        ModelParamMap.insert(std::make_pair("CHL1_13r", std::cref(CHL1_13r)));
        ModelParamMap.insert(std::make_pair("CHL1_22", std::cref(CHL1_22)));
        ModelParamMap.insert(std::make_pair("CHL1_23r", std::cref(CHL1_23r)));
        ModelParamMap.insert(std::make_pair("CHL1_33", std::cref(CHL1_33)));
        ModelParamMap.insert(std::make_pair("CHL1_12i", std::cref(CHL1_12i)));
        ModelParamMap.insert(std::make_pair("CHL1_13i", std::cref(CHL1_13i)));
        ModelParamMap.insert(std::make_pair("CHL1_23i", std::cref(CHL1_23i)));
        ModelParamMap.insert(std::make_pair("CHL3_11", std::cref(CHL3_11)));
        ModelParamMap.insert(std::make_pair("CHL3_12r", std::cref(CHL3_12r)));
        ModelParamMap.insert(std::make_pair("CHL3_13r", std::cref(CHL3_13r)));
        ModelParamMap.insert(std::make_pair("CHL3_22", std::cref(CHL3_22)));
        ModelParamMap.insert(std::make_pair("CHL3_23r", std::cref(CHL3_23r)));
        ModelParamMap.insert(std::make_pair("CHL3_33", std::cref(CHL3_33)));
        ModelParamMap.insert(std::make_pair("CHL3_12i", std::cref(CHL3_12i)));
        ModelParamMap.insert(std::make_pair("CHL3_13i", std::cref(CHL3_13i)));
        ModelParamMap.insert(std::make_pair("CHL3_23i", std::cref(CHL3_23i)));
        ModelParamMap.insert(std::make_pair("CHe_11", std::cref(CHe_11)));
        ModelParamMap.insert(std::make_pair("CHe_12r", std::cref(CHe_12r)));
        ModelParamMap.insert(std::make_pair("CHe_13r", std::cref(CHe_13r)));
        ModelParamMap.insert(std::make_pair("CHe_22", std::cref(CHe_22)));
        ModelParamMap.insert(std::make_pair("CHe_23r", std::cref(CHe_23r)));
        ModelParamMap.insert(std::make_pair("CHe_33", std::cref(CHe_33)));
        ModelParamMap.insert(std::make_pair("CHe_12i", std::cref(CHe_12i)));
        ModelParamMap.insert(std::make_pair("CHe_13i", std::cref(CHe_13i)));
        ModelParamMap.insert(std::make_pair("CHe_23i", std::cref(CHe_23i)));
        ModelParamMap.insert(std::make_pair("CeH_11r", std::cref(CeH_11r)));
        ModelParamMap.insert(std::make_pair("CeH_12r", std::cref(CeH_12r)));
        ModelParamMap.insert(std::make_pair("CeH_13r", std::cref(CeH_13r)));
        ModelParamMap.insert(std::make_pair("CeH_22r", std::cref(CeH_22r)));
        ModelParamMap.insert(std::make_pair("CeH_23r", std::cref(CeH_23r)));
        ModelParamMap.insert(std::make_pair("CeH_33r", std::cref(CeH_33r)));
        ModelParamMap.insert(std::make_pair("CeH_11i", std::cref(CeH_11i)));
        ModelParamMap.insert(std::make_pair("CeH_12i", std::cref(CeH_12i)));
        ModelParamMap.insert(std::make_pair("CeH_13i", std::cref(CeH_13i)));
        ModelParamMap.insert(std::make_pair("CeH_22i", std::cref(CeH_22i)));
        ModelParamMap.insert(std::make_pair("CeH_23i", std::cref(CeH_23i)));
        ModelParamMap.insert(std::make_pair("CeH_33i", std::cref(CeH_33i)));
        ModelParamMap.insert(std::make_pair("CLL_1111", std::cref(CLL_1111)));
        ModelParamMap.insert(std::make_pair("CLL_1221", std::cref(CLL_1221)));
        ModelParamMap.insert(std::make_pair("CLL_2112", std::cref(CLL_2112)));
        ModelParamMap.insert(std::make_pair("CLL_2211", std::cref(CLL_2211)));
        ModelParamMap.insert(std::make_pair("CLL_1122", std::cref(CLL_1122)));
        ModelParamMap.insert(std::make_pair("CLL_1331", std::cref(CLL_1331)));
        ModelParamMap.insert(std::make_pair("CLL_3113", std::cref(CLL_3113)));
        ModelParamMap.insert(std::make_pair("CLL_3311", std::cref(CLL_3311)));
        ModelParamMap.insert(std::make_pair("CLL_1133", std::cref(CLL_1133)));
        ModelParamMap.insert(std::make_pair("Cee_1111", std::cref(Cee_1111)));
        ModelParamMap.insert(std::make_pair("Cee_1122", std::cref(Cee_1122)));
        ModelParamMap.insert(std::make_pair("Cee_2211", std::cref(Cee_2211)));
        ModelParamMap.insert(std::make_pair("Cee_1133", std::cref(Cee_1133)));
        ModelParamMap.insert(std::make_pair("Cee_3311", std::cref(Cee_3311)));
        ModelParamMap.insert(std::make_pair("CLe_1111", std::cref(CLe_1111)));
        ModelParamMap.insert(std::make_pair("CLe_1122", std::cref(CLe_1122)));
        ModelParamMap.insert(std::make_pair("CLe_2211", std::cref(CLe_2211)));
        ModelParamMap.insert(std::make_pair("CLe_1133", std::cref(CLe_1133)));
        ModelParamMap.insert(std::make_pair("CLe_3311", std::cref(CLe_3311)));
        ModelParamMap.insert(std::make_pair("CLQ1_1123", std::cref(CLQ1_1123)));
        ModelParamMap.insert(std::make_pair("CLQ1_2223", std::cref(CLQ1_2223)));
        ModelParamMap.insert(std::make_pair("CLQ1_3323", std::cref(CLQ1_3323)));
        ModelParamMap.insert(std::make_pair("CLQ1_1132", std::cref(CLQ1_1132)));
        ModelParamMap.insert(std::make_pair("CLQ1_2232", std::cref(CLQ1_2232)));       
        ModelParamMap.insert(std::make_pair("CLQ1_3332", std::cref(CLQ1_3332)));
        ModelParamMap.insert(std::make_pair("CLQ3_1123", std::cref(CLQ3_1123)));
        ModelParamMap.insert(std::make_pair("CLQ3_2223", std::cref(CLQ3_2223)));
        ModelParamMap.insert(std::make_pair("CLQ3_3323", std::cref(CLQ3_3323)));
        ModelParamMap.insert(std::make_pair("CLQ3_1132", std::cref(CLQ3_1132)));
        ModelParamMap.insert(std::make_pair("CLQ3_2232", std::cref(CLQ3_2232)));       
        ModelParamMap.insert(std::make_pair("CLQ3_3332", std::cref(CLQ3_3332)));
        ModelParamMap.insert(std::make_pair("Ced_1123", std::cref(Ced_1123)));
        ModelParamMap.insert(std::make_pair("Ced_2223", std::cref(Ced_2223)));
        ModelParamMap.insert(std::make_pair("Ced_3323", std::cref(Ced_3323)));
        ModelParamMap.insert(std::make_pair("Ced_1132", std::cref(Ced_1132)));
        ModelParamMap.insert(std::make_pair("Ced_2232", std::cref(Ced_2232)));       
        ModelParamMap.insert(std::make_pair("Ced_3332", std::cref(Ced_3332)));
        ModelParamMap.insert(std::make_pair("CLd_1123", std::cref(CLd_1123)));
        ModelParamMap.insert(std::make_pair("CLd_2223", std::cref(CLd_2223)));
        ModelParamMap.insert(std::make_pair("CLd_3323", std::cref(CLd_3323)));
        ModelParamMap.insert(std::make_pair("CLd_1132", std::cref(CLd_1132)));
        ModelParamMap.insert(std::make_pair("CLd_2232", std::cref(CLd_2232)));       
        ModelParamMap.insert(std::make_pair("CLd_3332", std::cref(CLd_3332)));
        ModelParamMap.insert(std::make_pair("CQe_2311", std::cref(CQe_2311)));
        ModelParamMap.insert(std::make_pair("CQe_2322", std::cref(CQe_2322)));
        ModelParamMap.insert(std::make_pair("CQe_2333", std::cref(CQe_2333)));
        ModelParamMap.insert(std::make_pair("CQe_3211", std::cref(CQe_3211)));
        ModelParamMap.insert(std::make_pair("CQe_3222", std::cref(CQe_3222)));
        ModelParamMap.insert(std::make_pair("CQe_3233", std::cref(CQe_3233)));
    }
    if (FlagQuarkUniversal) {
        ModelParamMap.insert(std::make_pair("CHQ1", std::cref(CHQ1_11)));
        ModelParamMap.insert(std::make_pair("CHQ3", std::cref(CHQ3_11)));
        ModelParamMap.insert(std::make_pair("CHu", std::cref(CHu_11)));
        ModelParamMap.insert(std::make_pair("CHd", std::cref(CHd_11)));
        ModelParamMap.insert(std::make_pair("CHud_r", std::cref(CHud_11r)));
        ModelParamMap.insert(std::make_pair("CHud_i", std::cref(CHud_11i)));
        ModelParamMap.insert(std::make_pair("CuH_r", std::cref(CuH_11r)));
        ModelParamMap.insert(std::make_pair("CuH_i", std::cref(CuH_11i)));
        ModelParamMap.insert(std::make_pair("CdH_r", std::cref(CdH_11r)));
        ModelParamMap.insert(std::make_pair("CdH_i", std::cref(CdH_11i)));
        ModelParamMap.insert(std::make_pair("CuG_r", std::cref(CuG_11r)));
        ModelParamMap.insert(std::make_pair("CuG_i", std::cref(CuG_11i)));
        ModelParamMap.insert(std::make_pair("CuW_r", std::cref(CuW_11r)));
        ModelParamMap.insert(std::make_pair("CuW_i", std::cref(CuW_11i)));
        ModelParamMap.insert(std::make_pair("CuB_r", std::cref(CuB_11r)));
        ModelParamMap.insert(std::make_pair("CuB_i", std::cref(CuB_11i)));
    } else {
        ModelParamMap.insert(std::make_pair("CHQ1_11", std::cref(CHQ1_11)));
        ModelParamMap.insert(std::make_pair("CHQ1_12r", std::cref(CHQ1_12r)));
        ModelParamMap.insert(std::make_pair("CHQ1_13r", std::cref(CHQ1_13r)));
        ModelParamMap.insert(std::make_pair("CHQ1_22", std::cref(CHQ1_22)));
        ModelParamMap.insert(std::make_pair("CHQ1_23r", std::cref(CHQ1_23r)));
        ModelParamMap.insert(std::make_pair("CHQ1_33", std::cref(CHQ1_33)));
        ModelParamMap.insert(std::make_pair("CHQ1_12i", std::cref(CHQ1_12i)));
        ModelParamMap.insert(std::make_pair("CHQ1_13i", std::cref(CHQ1_13i)));
        ModelParamMap.insert(std::make_pair("CHQ1_23i", std::cref(CHQ1_23i)));
        ModelParamMap.insert(std::make_pair("CHQ3_11", std::cref(CHQ3_11)));
        ModelParamMap.insert(std::make_pair("CHQ3_12r", std::cref(CHQ3_12r)));
        ModelParamMap.insert(std::make_pair("CHQ3_13r", std::cref(CHQ3_13r)));
        ModelParamMap.insert(std::make_pair("CHQ3_22", std::cref(CHQ3_22)));
        ModelParamMap.insert(std::make_pair("CHQ3_23r", std::cref(CHQ3_23r)));
        ModelParamMap.insert(std::make_pair("CHQ3_33", std::cref(CHQ3_33)));
        ModelParamMap.insert(std::make_pair("CHQ3_12i", std::cref(CHQ3_12i)));
        ModelParamMap.insert(std::make_pair("CHQ3_13i", std::cref(CHQ3_13i)));
        ModelParamMap.insert(std::make_pair("CHQ3_23i", std::cref(CHQ3_23i)));
        ModelParamMap.insert(std::make_pair("CHu_11", std::cref(CHu_11)));
        ModelParamMap.insert(std::make_pair("CHu_12r", std::cref(CHu_12r)));
        ModelParamMap.insert(std::make_pair("CHu_13r", std::cref(CHu_13r)));
        ModelParamMap.insert(std::make_pair("CHu_22", std::cref(CHu_22)));
        ModelParamMap.insert(std::make_pair("CHu_23r", std::cref(CHu_23r)));
        ModelParamMap.insert(std::make_pair("CHu_33", std::cref(CHu_33)));
        ModelParamMap.insert(std::make_pair("CHu_12i", std::cref(CHu_12i)));
        ModelParamMap.insert(std::make_pair("CHu_13i", std::cref(CHu_13i)));
        ModelParamMap.insert(std::make_pair("CHu_23i", std::cref(CHu_23i)));
        ModelParamMap.insert(std::make_pair("CHd_11", std::cref(CHd_11)));
        ModelParamMap.insert(std::make_pair("CHd_12r", std::cref(CHd_12r)));
        ModelParamMap.insert(std::make_pair("CHd_13r", std::cref(CHd_13r)));
        ModelParamMap.insert(std::make_pair("CHd_22", std::cref(CHd_22)));
        ModelParamMap.insert(std::make_pair("CHd_23r", std::cref(CHd_23r)));
        ModelParamMap.insert(std::make_pair("CHd_33", std::cref(CHd_33)));
        ModelParamMap.insert(std::make_pair("CHd_12i", std::cref(CHd_12i)));
        ModelParamMap.insert(std::make_pair("CHd_13i", std::cref(CHd_13i)));
        ModelParamMap.insert(std::make_pair("CHd_23i", std::cref(CHd_23i)));
        ModelParamMap.insert(std::make_pair("CHud_11r", std::cref(CHud_11r)));
        ModelParamMap.insert(std::make_pair("CHud_12r", std::cref(CHud_12r)));
        ModelParamMap.insert(std::make_pair("CHud_13r", std::cref(CHud_13r)));
        ModelParamMap.insert(std::make_pair("CHud_22r", std::cref(CHud_22r)));
        ModelParamMap.insert(std::make_pair("CHud_23r", std::cref(CHud_23r)));
        ModelParamMap.insert(std::make_pair("CHud_33r", std::cref(CHud_33r)));
        ModelParamMap.insert(std::make_pair("CHud_11i", std::cref(CHud_11i)));
        ModelParamMap.insert(std::make_pair("CHud_12i", std::cref(CHud_12i)));
        ModelParamMap.insert(std::make_pair("CHud_13i", std::cref(CHud_13i)));
        ModelParamMap.insert(std::make_pair("CHud_22i", std::cref(CHud_22i)));
        ModelParamMap.insert(std::make_pair("CHud_23i", std::cref(CHud_23i)));
        ModelParamMap.insert(std::make_pair("CHud_33i", std::cref(CHud_33i)));
        ModelParamMap.insert(std::make_pair("CuH_11r", std::cref(CuH_11r)));
        ModelParamMap.insert(std::make_pair("CuH_12r", std::cref(CuH_12r)));
        ModelParamMap.insert(std::make_pair("CuH_13r", std::cref(CuH_13r)));
        ModelParamMap.insert(std::make_pair("CuH_22r", std::cref(CuH_22r)));
        ModelParamMap.insert(std::make_pair("CuH_23r", std::cref(CuH_23r)));
        ModelParamMap.insert(std::make_pair("CuH_33r", std::cref(CuH_33r)));
        ModelParamMap.insert(std::make_pair("CuH_11i", std::cref(CuH_11i)));
        ModelParamMap.insert(std::make_pair("CuH_12i", std::cref(CuH_12i)));
        ModelParamMap.insert(std::make_pair("CuH_13i", std::cref(CuH_13i)));
        ModelParamMap.insert(std::make_pair("CuH_22i", std::cref(CuH_22i)));
        ModelParamMap.insert(std::make_pair("CuH_23i", std::cref(CuH_23i)));
        ModelParamMap.insert(std::make_pair("CuH_33i", std::cref(CuH_33i)));
        ModelParamMap.insert(std::make_pair("CdH_11r", std::cref(CdH_11r)));
        ModelParamMap.insert(std::make_pair("CdH_12r", std::cref(CdH_12r)));
        ModelParamMap.insert(std::make_pair("CdH_13r", std::cref(CdH_13r)));
        ModelParamMap.insert(std::make_pair("CdH_22r", std::cref(CdH_22r)));
        ModelParamMap.insert(std::make_pair("CdH_23r", std::cref(CdH_23r)));
        ModelParamMap.insert(std::make_pair("CdH_33r", std::cref(CdH_33r)));
        ModelParamMap.insert(std::make_pair("CdH_11i", std::cref(CdH_11i)));
        ModelParamMap.insert(std::make_pair("CdH_12i", std::cref(CdH_12i)));
        ModelParamMap.insert(std::make_pair("CdH_13i", std::cref(CdH_13i)));
        ModelParamMap.insert(std::make_pair("CdH_22i", std::cref(CdH_22i)));
        ModelParamMap.insert(std::make_pair("CdH_23i", std::cref(CdH_23i)));
        ModelParamMap.insert(std::make_pair("CdH_33i", std::cref(CdH_33i)));
        ModelParamMap.insert(std::make_pair("CuG_11r", std::cref(CuG_11r)));
        ModelParamMap.insert(std::make_pair("CuG_12r", std::cref(CuG_12r)));
        ModelParamMap.insert(std::make_pair("CuG_13r", std::cref(CuG_13r)));
        ModelParamMap.insert(std::make_pair("CuG_22r", std::cref(CuG_22r)));
        ModelParamMap.insert(std::make_pair("CuG_23r", std::cref(CuG_23r)));
        ModelParamMap.insert(std::make_pair("CuG_33r", std::cref(CuG_33r)));
        ModelParamMap.insert(std::make_pair("CuG_11i", std::cref(CuG_11i)));
        ModelParamMap.insert(std::make_pair("CuG_12i", std::cref(CuG_12i)));
        ModelParamMap.insert(std::make_pair("CuG_13i", std::cref(CuG_13i)));
        ModelParamMap.insert(std::make_pair("CuG_22i", std::cref(CuG_22i)));
        ModelParamMap.insert(std::make_pair("CuG_23i", std::cref(CuG_23i)));
        ModelParamMap.insert(std::make_pair("CuG_33i", std::cref(CuG_33i)));
        ModelParamMap.insert(std::make_pair("CuW_11r", std::cref(CuW_11r)));
        ModelParamMap.insert(std::make_pair("CuW_12r", std::cref(CuW_12r)));
        ModelParamMap.insert(std::make_pair("CuW_13r", std::cref(CuW_13r)));
        ModelParamMap.insert(std::make_pair("CuW_22r", std::cref(CuW_22r)));
        ModelParamMap.insert(std::make_pair("CuW_23r", std::cref(CuW_23r)));
        ModelParamMap.insert(std::make_pair("CuW_33r", std::cref(CuW_33r)));
        ModelParamMap.insert(std::make_pair("CuW_11i", std::cref(CuW_11i)));
        ModelParamMap.insert(std::make_pair("CuW_12i", std::cref(CuW_12i)));
        ModelParamMap.insert(std::make_pair("CuW_13i", std::cref(CuW_13i)));
        ModelParamMap.insert(std::make_pair("CuW_22i", std::cref(CuW_22i)));
        ModelParamMap.insert(std::make_pair("CuW_23i", std::cref(CuW_23i)));
        ModelParamMap.insert(std::make_pair("CuW_33i", std::cref(CuW_33i)));
        ModelParamMap.insert(std::make_pair("CuB_11r", std::cref(CuB_11r)));
        ModelParamMap.insert(std::make_pair("CuB_12r", std::cref(CuB_12r)));
        ModelParamMap.insert(std::make_pair("CuB_13r", std::cref(CuB_13r)));
        ModelParamMap.insert(std::make_pair("CuB_22r", std::cref(CuB_22r)));
        ModelParamMap.insert(std::make_pair("CuB_23r", std::cref(CuB_23r)));
        ModelParamMap.insert(std::make_pair("CuB_33r", std::cref(CuB_33r)));
        ModelParamMap.insert(std::make_pair("CuB_11i", std::cref(CuB_11i)));
        ModelParamMap.insert(std::make_pair("CuB_12i", std::cref(CuB_12i)));
        ModelParamMap.insert(std::make_pair("CuB_13i", std::cref(CuB_13i)));
        ModelParamMap.insert(std::make_pair("CuB_22i", std::cref(CuB_22i)));
        ModelParamMap.insert(std::make_pair("CuB_23i", std::cref(CuB_23i)));
        ModelParamMap.insert(std::make_pair("CuB_33i", std::cref(CuB_33i)));
    }
    if(FlagLeptonUniversal && FlagQuarkUniversal){
        ModelParamMap.insert(std::make_pair("CLQ1", std::cref(CLQ1_1111)));  
        ModelParamMap.insert(std::make_pair("CLQ3", std::cref(CLQ3_1111))); 
        ModelParamMap.insert(std::make_pair("Ceu", std::cref(Ceu_1111)));
        ModelParamMap.insert(std::make_pair("Ced", std::cref(Ced_1111)));
        ModelParamMap.insert(std::make_pair("CLu", std::cref(CLu_1111)));
        ModelParamMap.insert(std::make_pair("CLd", std::cref(CLd_1111)));
        ModelParamMap.insert(std::make_pair("CQe", std::cref(CQe_1111)));
    } else {
        ModelParamMap.insert(std::make_pair("CLQ1_1111", std::cref(CLQ1_1111)));
        ModelParamMap.insert(std::make_pair("CLQ1_1122", std::cref(CLQ1_1122)));
        ModelParamMap.insert(std::make_pair("CLQ1_2211", std::cref(CLQ1_2211)));
        ModelParamMap.insert(std::make_pair("CLQ1_1221", std::cref(CLQ1_1221)));
        ModelParamMap.insert(std::make_pair("CLQ1_2112", std::cref(CLQ1_2112)));
        ModelParamMap.insert(std::make_pair("CLQ1_1133", std::cref(CLQ1_1133)));
        ModelParamMap.insert(std::make_pair("CLQ1_3311", std::cref(CLQ1_3311)));
        ModelParamMap.insert(std::make_pair("CLQ1_1331", std::cref(CLQ1_1331)));
        ModelParamMap.insert(std::make_pair("CLQ1_3113", std::cref(CLQ1_3113)));
        ModelParamMap.insert(std::make_pair("CLQ3_1111", std::cref(CLQ3_1111)));
        ModelParamMap.insert(std::make_pair("CLQ3_1122", std::cref(CLQ3_1122)));
        ModelParamMap.insert(std::make_pair("CLQ3_2211", std::cref(CLQ3_2211)));
        ModelParamMap.insert(std::make_pair("CLQ3_1221", std::cref(CLQ3_1221)));
        ModelParamMap.insert(std::make_pair("CLQ3_2112", std::cref(CLQ3_2112)));
        ModelParamMap.insert(std::make_pair("CLQ3_1133", std::cref(CLQ3_1133)));
        ModelParamMap.insert(std::make_pair("CLQ3_3311", std::cref(CLQ3_3311)));
        ModelParamMap.insert(std::make_pair("CLQ3_1331", std::cref(CLQ3_1331)));
        ModelParamMap.insert(std::make_pair("CLQ3_3113", std::cref(CLQ3_3113)));
        ModelParamMap.insert(std::make_pair("Ceu_1111", std::cref(Ceu_1111)));
        ModelParamMap.insert(std::make_pair("Ceu_1122", std::cref(Ceu_1122)));
        ModelParamMap.insert(std::make_pair("Ceu_2211", std::cref(Ceu_2211)));
        ModelParamMap.insert(std::make_pair("Ceu_1133", std::cref(Ceu_1133)));
        ModelParamMap.insert(std::make_pair("Ceu_3311", std::cref(Ceu_3311)));
        ModelParamMap.insert(std::make_pair("Ced_1111", std::cref(Ced_1111)));
        ModelParamMap.insert(std::make_pair("Ced_1122", std::cref(Ced_1122)));
        ModelParamMap.insert(std::make_pair("Ced_2211", std::cref(Ced_2211)));
        ModelParamMap.insert(std::make_pair("Ced_1133", std::cref(Ced_1133)));
        ModelParamMap.insert(std::make_pair("Ced_3311", std::cref(Ced_3311)));
        ModelParamMap.insert(std::make_pair("CLe_1111", std::cref(CLe_1111)));
        ModelParamMap.insert(std::make_pair("CLe_1122", std::cref(CLe_1122)));
        ModelParamMap.insert(std::make_pair("CLe_2211", std::cref(CLe_2211)));
        ModelParamMap.insert(std::make_pair("CLe_1133", std::cref(CLe_1133)));
        ModelParamMap.insert(std::make_pair("CLe_3311", std::cref(CLe_3311)));
        ModelParamMap.insert(std::make_pair("CLu_1111", std::cref(CLu_1111)));
        ModelParamMap.insert(std::make_pair("CLu_1122", std::cref(CLu_1122)));
        ModelParamMap.insert(std::make_pair("CLu_2211", std::cref(CLu_2211)));
        ModelParamMap.insert(std::make_pair("CLu_1133", std::cref(CLu_1133)));
        ModelParamMap.insert(std::make_pair("CLu_3311", std::cref(CLu_3311)));
        ModelParamMap.insert(std::make_pair("CLd_1111", std::cref(CLd_1111)));
        ModelParamMap.insert(std::make_pair("CLd_1122", std::cref(CLd_1122)));
        ModelParamMap.insert(std::make_pair("CLd_2211", std::cref(CLd_2211)));
        ModelParamMap.insert(std::make_pair("CLd_1133", std::cref(CLd_1133)));
        ModelParamMap.insert(std::make_pair("CLd_3311", std::cref(CLd_3311)));
        ModelParamMap.insert(std::make_pair("CQe_1111", std::cref(CQe_1111)));
        ModelParamMap.insert(std::make_pair("CQe_1122", std::cref(CQe_1122)));
        ModelParamMap.insert(std::make_pair("CQe_2211", std::cref(CQe_2211)));
        ModelParamMap.insert(std::make_pair("CQe_1133", std::cref(CQe_1133)));
        ModelParamMap.insert(std::make_pair("CQe_3311", std::cref(CQe_3311)));
    }
    ModelParamMap.insert(std::make_pair("Lambda_NP", std::cref(Lambda_NP)));
    ModelParamMap.insert(std::make_pair("eVBF2_HZZ1", std::cref(eVBF2_HZZ1)));
    ModelParamMap.insert(std::make_pair("eVBF2_HZZ2", std::cref(eVBF2_HZZ2)));
    ModelParamMap.insert(std::make_pair("eVBF2_HZZ3", std::cref(eVBF2_HZZ3)));
    ModelParamMap.insert(std::make_pair("eVBF2_HZA1", std::cref(eVBF2_HZA1)));
    ModelParamMap.insert(std::make_pair("eVBF2_HZA2", std::cref(eVBF2_HZA2)));
    ModelParamMap.insert(std::make_pair("eVBF2_HAA", std::cref(eVBF2_HAA)));
    ModelParamMap.insert(std::make_pair("eVBF2_HWW1", std::cref(eVBF2_HWW1)));
    ModelParamMap.insert(std::make_pair("eVBF2_HWW2", std::cref(eVBF2_HWW2)));
    ModelParamMap.insert(std::make_pair("eVBF2_HWW3", std::cref(eVBF2_HWW3)));
    ModelParamMap.insert(std::make_pair("eVBF2_Hgg", std::cref(eVBF2_Hgg)));
    ModelParamMap.insert(std::make_pair("eVBF2_HZuL", std::cref(eVBF2_HZuL)));
    ModelParamMap.insert(std::make_pair("eVBF2_HZuR", std::cref(eVBF2_HZuR)));
    ModelParamMap.insert(std::make_pair("eVBF2_HZdL", std::cref(eVBF2_HZdL)));
    ModelParamMap.insert(std::make_pair("eVBF2_HZdR", std::cref(eVBF2_HZdR)));
    ModelParamMap.insert(std::make_pair("eVBF2_HWud", std::cref(eVBF2_HWud)));
    ModelParamMap.insert(std::make_pair("eVBF2_ZuL", std::cref(eVBF2_ZuL)));
    ModelParamMap.insert(std::make_pair("eVBF2_ZuR", std::cref(eVBF2_ZuR)));
    ModelParamMap.insert(std::make_pair("eVBF2_ZdL", std::cref(eVBF2_ZdL)));
    ModelParamMap.insert(std::make_pair("eVBF2_ZdR", std::cref(eVBF2_ZdR)));
    ModelParamMap.insert(std::make_pair("eVBF2_Wud", std::cref(eVBF2_Wud)));
    ModelParamMap.insert(std::make_pair("eVBF78_HZZ1", std::cref(eVBF78_HZZ1)));
    ModelParamMap.insert(std::make_pair("eVBF78_HZZ2", std::cref(eVBF78_HZZ2)));
    ModelParamMap.insert(std::make_pair("eVBF78_HZZ3", std::cref(eVBF78_HZZ3)));
    ModelParamMap.insert(std::make_pair("eVBF78_HZA1", std::cref(eVBF78_HZA1)));
    ModelParamMap.insert(std::make_pair("eVBF78_HZA2", std::cref(eVBF78_HZA2)));
    ModelParamMap.insert(std::make_pair("eVBF78_HAA", std::cref(eVBF78_HAA)));
    ModelParamMap.insert(std::make_pair("eVBF78_HWW1", std::cref(eVBF78_HWW1)));
    ModelParamMap.insert(std::make_pair("eVBF78_HWW2", std::cref(eVBF78_HWW2)));
    ModelParamMap.insert(std::make_pair("eVBF78_HWW3", std::cref(eVBF78_HWW3)));
    ModelParamMap.insert(std::make_pair("eVBF78_Hgg", std::cref(eVBF78_Hgg)));
    ModelParamMap.insert(std::make_pair("eVBF78_HZuL", std::cref(eVBF78_HZuL)));
    ModelParamMap.insert(std::make_pair("eVBF78_HZuR", std::cref(eVBF78_HZuR)));
    ModelParamMap.insert(std::make_pair("eVBF78_HZdL", std::cref(eVBF78_HZdL)));
    ModelParamMap.insert(std::make_pair("eVBF78_HZdR", std::cref(eVBF78_HZdR)));
    ModelParamMap.insert(std::make_pair("eVBF78_HWud", std::cref(eVBF78_HWud)));
    ModelParamMap.insert(std::make_pair("eVBF78_ZuL", std::cref(eVBF78_ZuL)));
    ModelParamMap.insert(std::make_pair("eVBF78_ZuR", std::cref(eVBF78_ZuR)));
    ModelParamMap.insert(std::make_pair("eVBF78_ZdL", std::cref(eVBF78_ZdL)));
    ModelParamMap.insert(std::make_pair("eVBF78_ZdR", std::cref(eVBF78_ZdR)));
    ModelParamMap.insert(std::make_pair("eVBF78_Wud", std::cref(eVBF78_Wud)));
    ModelParamMap.insert(std::make_pair("eWH2_HWW1", std::cref(eWH2_HWW1)));
    ModelParamMap.insert(std::make_pair("eWH2_HWW2", std::cref(eWH2_HWW2)));
    ModelParamMap.insert(std::make_pair("eWH2_HWW3", std::cref(eWH2_HWW3)));
    ModelParamMap.insert(std::make_pair("eWH2_HWud", std::cref(eWH2_HWud)));
    ModelParamMap.insert(std::make_pair("eWH2_Wud", std::cref(eWH2_Wud)));
    ModelParamMap.insert(std::make_pair("eWH78_HWW1", std::cref(eWH78_HWW1)));
    ModelParamMap.insert(std::make_pair("eWH78_HWW2", std::cref(eWH78_HWW2)));
    ModelParamMap.insert(std::make_pair("eWH78_HWW3", std::cref(eWH78_HWW3)));
    ModelParamMap.insert(std::make_pair("eWH78_HWud", std::cref(eWH78_HWud)));
    ModelParamMap.insert(std::make_pair("eWH78_Wud", std::cref(eWH78_Wud)));
    ModelParamMap.insert(std::make_pair("eZH2_HZZ1", std::cref(eZH2_HZZ1)));
    ModelParamMap.insert(std::make_pair("eZH2_HZZ2", std::cref(eZH2_HZZ2)));
    ModelParamMap.insert(std::make_pair("eZH2_HZZ3", std::cref(eZH2_HZZ3)));
    ModelParamMap.insert(std::make_pair("eZH2_HZA1", std::cref(eZH2_HZA1)));
    ModelParamMap.insert(std::make_pair("eZH2_HZA2", std::cref(eZH2_HZA2)));
    ModelParamMap.insert(std::make_pair("eZH2_HZuL", std::cref(eZH2_HZuL)));
    ModelParamMap.insert(std::make_pair("eZH2_HZuR", std::cref(eZH2_HZuR)));
    ModelParamMap.insert(std::make_pair("eZH2_HZdL", std::cref(eZH2_HZdL)));
    ModelParamMap.insert(std::make_pair("eZH2_HZdR", std::cref(eZH2_HZdR)));
    ModelParamMap.insert(std::make_pair("eZH2_ZuL", std::cref(eZH2_ZuL)));
    ModelParamMap.insert(std::make_pair("eZH2_ZuR", std::cref(eZH2_ZuR)));
    ModelParamMap.insert(std::make_pair("eZH2_ZdL", std::cref(eZH2_ZdL)));
    ModelParamMap.insert(std::make_pair("eZH2_ZdR", std::cref(eZH2_ZdR)));
    ModelParamMap.insert(std::make_pair("eZH78_HZZ1", std::cref(eZH78_HZZ1)));
    ModelParamMap.insert(std::make_pair("eZH78_HZZ2", std::cref(eZH78_HZZ2)));
    ModelParamMap.insert(std::make_pair("eZH78_HZZ3", std::cref(eZH78_HZZ3)));
    ModelParamMap.insert(std::make_pair("eZH78_HZA1", std::cref(eZH78_HZA1)));
    ModelParamMap.insert(std::make_pair("eZH78_HZA2", std::cref(eZH78_HZA2)));
    ModelParamMap.insert(std::make_pair("eZH78_HZuL", std::cref(eZH78_HZuL)));
    ModelParamMap.insert(std::make_pair("eZH78_HZuR", std::cref(eZH78_HZuR)));
    ModelParamMap.insert(std::make_pair("eZH78_HZdL", std::cref(eZH78_HZdL)));
    ModelParamMap.insert(std::make_pair("eZH78_HZdR", std::cref(eZH78_HZdR)));
    ModelParamMap.insert(std::make_pair("eZH78_ZuL", std::cref(eZH78_ZuL)));
    ModelParamMap.insert(std::make_pair("eZH78_ZuR", std::cref(eZH78_ZuR)));
    ModelParamMap.insert(std::make_pair("eZH78_ZdL", std::cref(eZH78_ZdL)));
    ModelParamMap.insert(std::make_pair("eZH78_ZdR", std::cref(eZH78_ZdR)));
    ModelParamMap.insert(std::make_pair("ettH2_Htt", std::cref(ettH2_Htt)));
    ModelParamMap.insert(std::make_pair("ettH2_Hgg", std::cref(ettH2_Hgg)));
    ModelParamMap.insert(std::make_pair("ettH78_Htt", std::cref(ettH78_Htt)));
    ModelParamMap.insert(std::make_pair("ettH78_Hgg", std::cref(ettH78_Hgg)));
    if (FlagMwInput) {
        ModelParamMap.insert(std::make_pair("MwInput", std::cref(MwInput)));
    }
 
    if (FlagLeptonUniversal) {        
//  bsll/sbll entries only interesting (for the moment) if non-lepton universal. Set to 0 otherwise
        CLQ1_1123 = 0.0;
        CLQ1_2223 = 0.0;
        CLQ1_3323 = 0.0;
        CLQ1_1132 = 0.0;
        CLQ1_2232 = 0.0;
        CLQ1_3332 = 0.0;
        
        CLQ3_1123 = 0.0;
        CLQ3_2223 = 0.0;
        CLQ3_3323 = 0.0;
        CLQ3_1132 = 0.0;
        CLQ3_2232 = 0.0;
        CLQ3_3332 = 0.0;
        
        Ced_1123 = 0.0;
        Ced_2223 = 0.0;
        Ced_3323 = 0.0;
        Ced_1132 = 0.0;
        Ced_2232 = 0.0;
        Ced_3332 = 0.0;  
        
        CLd_1123 = 0.0;
        CLd_2223 = 0.0;
        CLd_3323 = 0.0;
        CLd_1132 = 0.0;
        CLd_2232 = 0.0;
        CLd_3332 = 0.0;
        
        CQe_2311 = 0.0;
        CQe_2322 = 0.0;
        CQe_2333 = 0.0;
        CQe_3211 = 0.0;
        CQe_3222 = 0.0;
        CQe_3233 = 0.0;
    }
    
}

Member Function Documentation

AH_f()

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 1985 of file NPEffectiveGIMR.cpp.

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

BrHbbRatio()

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 2994 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;
 
}

BrHccRatio()

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 2974 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;
 
}

BrHgagaRatio()

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 2914 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;
 
}

BrHggRatio()

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 2834 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;
 
}

BrHmumuRatio()

double NPEffectiveGIMR::BrHmumuRatio ( ) const

virtual

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

Returns

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

Reimplemented from NPbase.

Definition at line 2934 of file NPEffectiveGIMR.cpp.

{
    double Br = 1.0;
    
    Br += deltaGammaHmumuRatio1() - 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 += - deltaGammaHmumuRatio1() * deltaGammaTotalRatio1()
                + deltaGammaHmumuRatio2() - deltaGammaTotalRatio2()
                + pow(deltaGammaTotalRatio1(),2.0);            
        }
    
    if (Br < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return Br;
 
}

BrHtautauRatio()

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 2954 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;
 
}

BrHWWRatio()

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 2854 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;
 
}

BrHZgaRatio()

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 2894 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;
 
}

BrHZZRatio()

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 2874 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;
 
}

CfB_diag()

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

protected

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

Parameters

[in]

f

a lepton or quark

Returns

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

Definition at line 1660 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 0.0;
    else if (f.is("MU"))
        return 0.0;
    else if (f.is("TAU"))
        return 0.0;
    else if (f.is("UP"))
        return gslpp::complex(CuB_11r, CuB_11i, false);
    else if (f.is("CHARM"))
        return gslpp::complex(CuB_22r, CuB_22i, false);
    else if (f.is("TOP"))
        return gslpp::complex(CuB_33r, CuB_33i, false);
    else if (f.is("DOWN"))
        return 0.0;
    else if (f.is("STRANGE"))
        return 0.0;
    else if (f.is("BOTTOM"))
        return 0.0;
    else
        throw std::runtime_error("NPEffectiveGIMR::CfB_diag(): wrong argument");
}

CfG_diag()

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

protected

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

Parameters

[in]

f

a lepton or quark

Returns

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

Definition at line 1608 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 0.0;
    else if (f.is("MU"))
        return 0.0;
    else if (f.is("TAU"))
        return 0.0;
    else if (f.is("UP"))
        return gslpp::complex(CuG_11r, CuG_11i, false);
    else if (f.is("CHARM"))
        return gslpp::complex(CuG_22r, CuG_22i, false);
    else if (f.is("TOP"))
        return gslpp::complex(CuG_33r, CuG_33i, false);
    else if (f.is("DOWN"))
        return 0.0;
    else if (f.is("STRANGE"))
        return 0.0;
    else if (f.is("BOTTOM"))
        return 0.0;
    else
        throw std::runtime_error("NPEffectiveGIMR::CfG_diag(): wrong argument");
}

CfH_diag()

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 1582 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");
}

CfW_diag()

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

protected

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

Parameters

[in]

f

a lepton or quark

Returns

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

Definition at line 1634 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 0.0;
    else if (f.is("MU"))
        return 0.0;
    else if (f.is("TAU"))
        return 0.0;
    else if (f.is("UP"))
        return gslpp::complex(CuW_11r, CuW_11i, false);
    else if (f.is("CHARM"))
        return gslpp::complex(CuW_22r, CuW_22i, false);
    else if (f.is("TOP"))
        return gslpp::complex(CuW_33r, CuW_33i, false);
    else if (f.is("DOWN"))
        return 0.0;
    else if (f.is("STRANGE"))
        return 0.0;
    else if (f.is("BOTTOM"))
        return 0.0;
    else
        throw std::runtime_error("NPEffectiveGIMR::CfW_diag(): wrong argument");
}

CheckParameters()

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 1444 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;
                raiseMissingModelParameterCount();
                addMissingModelParameter("MwInput");
            }
        }
        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;
                raiseMissingModelParameterCount();
                addMissingModelParameter(NPEffectiveGIMRVars_LFU_QFU[i]);
            }
        }
        //} 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;
                raiseMissingModelParameterCount();
                addMissingModelParameter("MwInput");
            }
        }
        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;
                raiseMissingModelParameterCount();
                addMissingModelParameter(NPEffectiveGIMRVars[i]);
            }
        }
    } else
        throw std::runtime_error("Error in NPEffectiveGIMR::CheckParameters()");
 
    return (NPbase::CheckParameters(DPars));
}

CHF1_diag()

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 1505 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");
}

CHF3_diag()

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 1523 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");
}

CHf_diag()

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 1541 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");
}

CHud_diag()

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 1567 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");
}

CLL_bottom()

double NPEffectiveGIMR::CLL_bottom

(

)

const

Definition at line 3387 of file NPEffectiveGIMR.cpp.

{
    return ((CLQ1_1133 + CLQ3_1133) / LambdaNP2);
}

CLL_charm()

double NPEffectiveGIMR::CLL_charm

(

)

const

Definition at line 3377 of file NPEffectiveGIMR.cpp.

{
    return ((CLQ1_1122 - CLQ3_1122) / LambdaNP2);
}

CLL_down()

double NPEffectiveGIMR::CLL_down

(

)

const

Definition at line 3372 of file NPEffectiveGIMR.cpp.

{
    return ((CLQ1_1111 + CLQ3_1111) / LambdaNP2);
}

CLL_mu()

double NPEffectiveGIMR::CLL_mu

(

)

const

Definition at line 3357 of file NPEffectiveGIMR.cpp.

{
    return ((CLL_1122 + CLL_1221) / LambdaNP2);
}

CLL_strange()

double NPEffectiveGIMR::CLL_strange

(

)

const

Definition at line 3382 of file NPEffectiveGIMR.cpp.

{
    return ((CLQ1_1122 + CLQ3_1122) / LambdaNP2);
}

CLL_tau()

double NPEffectiveGIMR::CLL_tau

(

)

const

Definition at line 3362 of file NPEffectiveGIMR.cpp.

{
    return ((CLL_1133 + CLL_1331) / LambdaNP2);
}

CLL_up()

double NPEffectiveGIMR::CLL_up

(

)

const

Definition at line 3367 of file NPEffectiveGIMR.cpp.

{
    return ((CLQ1_1111 - CLQ3_1111) / LambdaNP2);
}

CLR_bottom()

double NPEffectiveGIMR::CLR_bottom

(

)

const

Definition at line 3422 of file NPEffectiveGIMR.cpp.

{
    return (CLd_1133 / LambdaNP2);
}

CLR_charm()

double NPEffectiveGIMR::CLR_charm

(

)

const

Definition at line 3412 of file NPEffectiveGIMR.cpp.

{
    return (CLu_1122 / LambdaNP2);
}

CLR_down()

double NPEffectiveGIMR::CLR_down

(

)

const

Definition at line 3407 of file NPEffectiveGIMR.cpp.

{
    return (CLd_1111 / LambdaNP2);
}

CLR_mu()

double NPEffectiveGIMR::CLR_mu

(

)

const

Definition at line 3392 of file NPEffectiveGIMR.cpp.

{
    return ((CLe_1122 + CLe_2211) / LambdaNP2);
}

CLR_strange()

double NPEffectiveGIMR::CLR_strange

(

)

const

Definition at line 3417 of file NPEffectiveGIMR.cpp.

{
    return (CLd_1122 / LambdaNP2);
}

CLR_tau()

double NPEffectiveGIMR::CLR_tau

(

)

const

Definition at line 3397 of file NPEffectiveGIMR.cpp.

{
    return ((CLe_1133 + CLe_3311) / LambdaNP2);
}

CLR_up()

double NPEffectiveGIMR::CLR_up

(

)

const

Definition at line 3402 of file NPEffectiveGIMR.cpp.

{
    return (CLu_1111 / LambdaNP2);
}

computeGammaTotalRatio()

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 3014 of file NPEffectiveGIMR.cpp.

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

CRL_bottom()

double NPEffectiveGIMR::CRL_bottom

(

)

const

Definition at line 3457 of file NPEffectiveGIMR.cpp.

{
    return (CQe_1133 / LambdaNP2);
}

CRL_charm()

double NPEffectiveGIMR::CRL_charm

(

)

const

Definition at line 3447 of file NPEffectiveGIMR.cpp.

{
    return (CQe_1122 / LambdaNP2);
}

CRL_down()

double NPEffectiveGIMR::CRL_down

(

)

const

Definition at line 3442 of file NPEffectiveGIMR.cpp.

{
    return (CQe_1111 / LambdaNP2);
}

CRL_mu()

double NPEffectiveGIMR::CRL_mu

(

)

const

Definition at line 3427 of file NPEffectiveGIMR.cpp.

{
    return (CLe_1122 / LambdaNP2);
}

CRL_strange()

double NPEffectiveGIMR::CRL_strange

(

)

const

Definition at line 3452 of file NPEffectiveGIMR.cpp.

{
    return (CQe_1122 / LambdaNP2);
}

CRL_tau()

double NPEffectiveGIMR::CRL_tau

(

)

const

Definition at line 3432 of file NPEffectiveGIMR.cpp.

{
    return (CLe_1133 / LambdaNP2);
}

CRL_up()

double NPEffectiveGIMR::CRL_up

(

)

const

Definition at line 3437 of file NPEffectiveGIMR.cpp.

{
    return (CQe_1111 / LambdaNP2);
}

CRR_bottom()

double NPEffectiveGIMR::CRR_bottom

(

)

const

Definition at line 3493 of file NPEffectiveGIMR.cpp.

{
    return (Ced_1133 / LambdaNP2);
}

CRR_charm()

double NPEffectiveGIMR::CRR_charm

(

)

const

Definition at line 3483 of file NPEffectiveGIMR.cpp.

{
    return (Ceu_1122 / LambdaNP2);
}

CRR_down()

double NPEffectiveGIMR::CRR_down

(

)

const

Definition at line 3478 of file NPEffectiveGIMR.cpp.

{
    return (Ced_1111 / LambdaNP2);
}

CRR_mu()

double NPEffectiveGIMR::CRR_mu

(

)

const

Definition at line 3462 of file NPEffectiveGIMR.cpp.

{
    return (Cee_1122 / LambdaNP2);
}

CRR_strange()

double NPEffectiveGIMR::CRR_strange

(

)

const

Definition at line 3488 of file NPEffectiveGIMR.cpp.

{
    return (Ced_1122 / LambdaNP2);
}

CRR_tau()

double NPEffectiveGIMR::CRR_tau

(

)

const

Definition at line 3467 of file NPEffectiveGIMR.cpp.

{
    return (Cee_1133 / LambdaNP2);
}

CRR_up()

double NPEffectiveGIMR::CRR_up

(

)

const

Definition at line 3473 of file NPEffectiveGIMR.cpp.

{
    return (Ceu_1111 / LambdaNP2);
}

deltaG1_hWW()

double NPEffectiveGIMR::deltaG1_hWW ( ) const

virtual

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

Returns

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

Reimplemented from NPbase.

Definition at line 1820 of file NPEffectiveGIMR.cpp.

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

deltaG1_hZA()

double NPEffectiveGIMR::deltaG1_hZA ( ) const

virtual

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

Returns

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

Reimplemented from NPbase.

Definition at line 1860 of file NPEffectiveGIMR.cpp.

{
    return (delta_AZ / v());
}

deltaG1_hZZ()

double NPEffectiveGIMR::deltaG1_hZZ ( ) const

virtual

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

Returns

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

Reimplemented from NPbase.

Definition at line 1843 of file NPEffectiveGIMR.cpp.

{
    return (delta_ZZ / v());
}

deltaG2_hWW()

double NPEffectiveGIMR::deltaG2_hWW ( ) const

virtual

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

Returns

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

Reimplemented from NPbase.

Definition at line 1825 of file NPEffectiveGIMR.cpp.

{
    return 0.0;
}

deltaG2_hZA()

double NPEffectiveGIMR::deltaG2_hZA ( ) const

virtual

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

Returns

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

Reimplemented from NPbase.

Definition at line 1865 of file NPEffectiveGIMR.cpp.

{
    return 0.0;
}

deltaG2_hZZ()

double NPEffectiveGIMR::deltaG2_hZZ ( ) const

virtual

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

Returns

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

Reimplemented from NPbase.

Definition at line 1848 of file NPEffectiveGIMR.cpp.

{
    return 0.0;
}

deltaG3_hWW()

double NPEffectiveGIMR::deltaG3_hWW ( ) const

virtual

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

Returns

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

Reimplemented from NPbase.

Definition at line 1830 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;
}

deltaG3_hZZ()

double NPEffectiveGIMR::deltaG3_hZZ ( ) const

virtual

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

Returns

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

Reimplemented from NPbase.

Definition at line 1853 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);
}

deltag3G()

double NPEffectiveGIMR::deltag3G

(

)

const

The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\).

Returns

\(\delta g_{3G}\)

Definition at line 1963 of file NPEffectiveGIMR.cpp.

{
    /* Set to 0. for the moment */
 
    return 0.;
}

deltaG_Aff()

gslpp::complex NPEffectiveGIMR::deltaG_Aff

(

const Particle

p

)

const

The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters

[in]

p

a lepton or quark

Returns

\(\delta g_{Aff}\)

Definition at line 1956 of file NPEffectiveGIMR.cpp.

{
    /* Set to 0. for the moment */
 
    return 0.;
}

deltaG_Gff()

gslpp::complex NPEffectiveGIMR::deltaG_Gff

(

const Particle

p

)

const

The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters

[in]

p

a lepton or quark

Returns

\(\delta g_{Gff}\)

Definition at line 1942 of file NPEffectiveGIMR.cpp.

{
    /* Set to 0. for the moment */
 
    return 0.;
}

deltaG_hAA()

double NPEffectiveGIMR::deltaG_hAA ( ) const

virtual

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

Returns

\(\delta g_{HAA}\)

Reimplemented from NPbase.

Definition at line 1870 of file NPEffectiveGIMR.cpp.

{
    return (delta_AA / v());
}

deltaG_hAff()

gslpp::complex NPEffectiveGIMR::deltaG_hAff

(

const Particle

p

)

const

The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters

[in]

p

a lepton or quark

Returns

\(\delta g_{hAff}\)

Definition at line 1935 of file NPEffectiveGIMR.cpp.

{
    /* Set to 0. for the moment */
 
    return 0.;
}

deltaG_hff()

gslpp::complex NPEffectiveGIMR::deltaG_hff ( const Particle  p ) const

virtual

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

Parameters

[in]

p

a lepton or quark

Returns

\(\delta g_{Hff}\)

Reimplemented from NPbase.

Definition at line 1875 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));
}

deltaG_hGff()

gslpp::complex NPEffectiveGIMR::deltaG_hGff

(

const Particle

p

)

const

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

Parameters

[in]

p

a lepton or quark

Returns

\(\delta g_{hGff}\)

Definition at line 1921 of file NPEffectiveGIMR.cpp.

{
    /* Set to 0. for the moment */
 
    return 0.;
}

deltaG_hgg()

double NPEffectiveGIMR::deltaG_hgg ( ) const

virtual

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

Returns

\(\delta g_{HGG}\)

Reimplemented from NPbase.

Definition at line 1815 of file NPEffectiveGIMR.cpp.

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

deltaG_hZff()

gslpp::complex NPEffectiveGIMR::deltaG_hZff

(

const Particle

p

)

const

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

Parameters

[in]

p

a lepton or quark

Returns

\(\delta g_{hZff}\)

Definition at line 1928 of file NPEffectiveGIMR.cpp.

{
    /* Set to 0. for the moment */
 
    return 0.;
}

deltaG_Zff()

gslpp::complex NPEffectiveGIMR::deltaG_Zff

(

const Particle

p

)

const

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

Parameters

[in]

p

a lepton or quark

Returns

\(\delta g_{Zff}\)

Definition at line 1949 of file NPEffectiveGIMR.cpp.

{
    /* Set to 0. for the moment */
 
    return 0.;
}

deltaGA_f()

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 1746 of file NPEffectiveGIMR.cpp.

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

deltaGammaHbbRatio1()

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 3341 of file NPEffectiveGIMR.cpp.

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

deltaGammaHbbRatio2()

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 3347 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) );        
    
}

deltaGammaHccRatio1()

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 3313 of file NPEffectiveGIMR.cpp.

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

deltaGammaHccRatio2()

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 3318 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) );            
    
}

deltaGammaHgagaRatio1()

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 3213 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() );
    
}

deltaGammaHgagaRatio2()

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 3224 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) );            
    
}

deltaGammaHggRatio1()

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 3069 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() );
}

deltaGammaHggRatio2()

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 3077 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) );            
    
}

deltaGammaHmumuRatio1()

double NPEffectiveGIMR::deltaGammaHmumuRatio1

(

)

const

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

Returns

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

Definition at line 3253 of file NPEffectiveGIMR.cpp.

{
    return ( -4653.43 * deltaG_hff(leptons[MU]).real() );
        
}

deltaGammaHmumuRatio2()

double NPEffectiveGIMR::deltaGammaHmumuRatio2

(

)

const

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

Returns

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

Definition at line 3259 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 0.0;
    
}

deltaGammaHtautauRatio1()

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 3283 of file NPEffectiveGIMR.cpp.

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

deltaGammaHtautauRatio2()

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 3289 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) );            
    
}

deltaGammaHWWRatio1()

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 3104 of file NPEffectiveGIMR.cpp.

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

deltaGammaHWWRatio2()

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 3113 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) );
    
}

deltaGammaHZgaRatio1()

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 3173 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() );
    
}

deltaGammaHZgaRatio2()

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 3185 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) );            
    
}

deltaGammaHZZRatio1()

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 3138 of file NPEffectiveGIMR.cpp.

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

deltaGammaHZZRatio2()

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 3147 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) );            
    
}

deltaGammaTotalRatio1()

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 3027 of file NPEffectiveGIMR.cpp.

{
    return (trueSM.computeBrHtogg() * deltaGammaHggRatio1()
            + trueSM.computeBrHtoWW() * deltaGammaHWWRatio1()
            + trueSM.computeBrHtoZZ() * deltaGammaHZZRatio1()
            + trueSM.computeBrHtoZga() * deltaGammaHZgaRatio1()
            + trueSM.computeBrHtogaga() * deltaGammaHgagaRatio1()
            + trueSM.computeBrHtomumu() * deltaGammaHmumuRatio1()
            + trueSM.computeBrHtotautau() * deltaGammaHtautauRatio1()
            + trueSM.computeBrHtocc() * deltaGammaHccRatio1()
            + trueSM.computeBrHtobb() * deltaGammaHbbRatio1());
}

deltaGammaTotalRatio2()

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 3040 of file NPEffectiveGIMR.cpp.

{
    return (trueSM.computeBrHtogg() * deltaGammaHggRatio2()
            + trueSM.computeBrHtoWW() * deltaGammaHWWRatio2()
            + trueSM.computeBrHtoZZ() * deltaGammaHZZRatio2()
            + trueSM.computeBrHtoZga() * deltaGammaHZgaRatio2()
            + trueSM.computeBrHtogaga() * deltaGammaHgagaRatio2()
            + trueSM.computeBrHtomumu() * deltaGammaHmumuRatio2()
            + trueSM.computeBrHtotautau() * deltaGammaHtautauRatio2()
            + trueSM.computeBrHtocc() * deltaGammaHccRatio2()
            + trueSM.computeBrHtobb() * deltaGammaHbbRatio2());
}

DeltaGF()

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 1689 of file NPEffectiveGIMR.cpp.

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

deltaGL_f()

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 1751 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);
}

deltaGL_Wff()

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

virtual

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

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

Reimplemented from NPbase.

Definition at line 1789 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);
}

deltaGL_Wffh()

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 1889 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);
}

deltaGL_Zffh()

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 1907 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);
}

deltaGR_f()

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 1770 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);
}

deltaGR_Wff()

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

virtual

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

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

Reimplemented from NPbase.

Definition at line 1806 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);
}

deltaGR_Wffh()

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 1898 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);
}

deltaGR_Zffh()

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 1915 of file NPEffectiveGIMR.cpp.

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

deltaGV_f()

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 1741 of file NPEffectiveGIMR.cpp.

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

deltaMz2()

double NPEffectiveGIMR::deltaMz2 ( ) const

virtual

Definition at line 1709 of file NPEffectiveGIMR.cpp.

{
    return (2.0*(cW2_tree*CHW+sW2_tree*CHB+cW_tree*sW_tree*CHWB)*v2_over_LambdaNP2);
}

f_triangle()

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 1973 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);
    }
}

GammaHbbRatio()

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 3326 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;
}

GammaHccRatio()

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 3297 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;
    
}

GammaHgagaRatio()

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 3197 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;
    
}

GammaHggRatio()

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 3053 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;
    
}

GammaHmumuRatio()

double NPEffectiveGIMR::GammaHmumuRatio

(

)

const

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

Returns

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

Definition at line 3237 of file NPEffectiveGIMR.cpp.

{
    double width = 1.0;
 
    width += deltaGammaHmumuRatio1();
    
    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 += deltaGammaHmumuRatio2();
        }
    
    return width;
    
}

GammaHtautauRatio()

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 3267 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;
    
}

GammaHWWRatio()

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 3088 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;
    
}

GammaHZgaRatio()

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 3157 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;
    
}

GammaHZZRatio()

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 3122 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;
    
}

GammaW()

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 1725 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);
}

LEP2AFBbottom()

double NPEffectiveGIMR::LEP2AFBbottom ( const double  s ) const

virtual

Reimplemented from StandardModel.

Definition at line 3637 of file NPEffectiveGIMR.cpp.

{
   double AFB_bottom, sigma = 0.0,dFminusB =0.0;;
   double GIMRParam[10] = {CLL_bottom(), CLR_bottom(), CRL_bottom(), CRR_bottom(), deltaGamma_Z(), 
                          deltaGR_f(quarks[BOTTOM]), 
                          deltaGL_f(quarks[BOTTOM]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
   sigma = trueSM.LEP2sigmaBottom(s);
   dFminusB = myLEP2GIMR.sigmaFminusB_q_LEP2_GIMR(QCD::quark(BOTTOM), s, GIMRParam);
   
   AFB_bottom = trueSM.LEP2AFBbottom(s) * (1. - myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::quark(BOTTOM), s, GIMRParam) / sigma)
                   + dFminusB / sigma;
   
   return AFB_bottom;
}

LEP2AFBcharm()

double NPEffectiveGIMR::LEP2AFBcharm ( const double  s ) const

virtual

Reimplemented from StandardModel.

Definition at line 3619 of file NPEffectiveGIMR.cpp.

{
   double AFB_charm, sigma = 0.0,dFminusB =0.0;
   double GIMRParam[10] = {CLL_charm(), CLR_charm(), CRL_charm(), CRR_charm(), deltaGamma_Z(), 
                          deltaGR_f(quarks[CHARM]), 
                          deltaGL_f(quarks[CHARM]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
   sigma = trueSM.LEP2sigmaCharm(s);
   dFminusB = myLEP2GIMR.sigmaFminusB_q_LEP2_GIMR(QCD::quark(CHARM), s, GIMRParam);
   
   AFB_charm = trueSM.LEP2AFBcharm(s) * (1. - myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::quark(CHARM), s, GIMRParam) / sigma)
                   + dFminusB / sigma;
   
   return AFB_charm;
}

LEP2AFBmu()

double NPEffectiveGIMR::LEP2AFBmu ( const double  s ) const

virtual

Reimplemented from StandardModel.

Definition at line 3582 of file NPEffectiveGIMR.cpp.

{
   double AFB_mu = 0., sigma = 0.0,dFminusB =0.0;
   double GIMRParam[10] = {CLL_mu(), CLR_mu(), CRL_mu(), CRR_mu(), deltaGamma_Z(), 
                          deltaGR_f(leptons[MU]), 
                          deltaGL_f(leptons[MU]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
   
   sigma = trueSM.LEP2sigmaMu(s);
   dFminusB = myLEP2GIMR.sigmaFminusB_l_LEP2_GIMR(QCD::lepton(MU), s, GIMRParam);
   
   AFB_mu = trueSM.LEP2AFBmu(s) * (1. - myLEP2GIMR.sigma_l_LEP2_GIMR(QCD::lepton(MU), s, GIMRParam) / sigma)
                   + dFminusB / sigma;
   
   return AFB_mu;
}

LEP2AFBtau()

double NPEffectiveGIMR::LEP2AFBtau ( const double  s ) const

virtual

Reimplemented from StandardModel.

Definition at line 3601 of file NPEffectiveGIMR.cpp.

{
   double AFB_tau, sigma = 0.0,dFminusB =0.0;
   double GIMRParam[10] = {CLL_tau(), CLR_tau(), CRL_tau(), CRR_tau(), deltaGamma_Z(), 
                          deltaGR_f(leptons[TAU]), 
                          deltaGL_f(leptons[TAU]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
   sigma = trueSM.LEP2sigmaTau(s);
   dFminusB = myLEP2GIMR.sigmaFminusB_l_LEP2_GIMR(QCD::lepton(TAU), s, GIMRParam);
 
   AFB_tau = trueSM.LEP2AFBtau(s) * (1. - myLEP2GIMR.sigma_l_LEP2_GIMR(QCD::lepton(TAU), s, GIMRParam) / sigma)
                   + dFminusB / sigma;
   
   return AFB_tau;
}

LEP2Rbottom()

double NPEffectiveGIMR::LEP2Rbottom ( const double  s ) const

virtual

Reimplemented from StandardModel.

Definition at line 3709 of file NPEffectiveGIMR.cpp.

{
   double R_bottom = 0., dsigma_b = 0.0, dsigma_had =0.0, sigma_hSM = 0.0;
   double GIMRParamUP[10] = {CLL_up(), CLR_up(), CRL_up(), CRR_up(), deltaGamma_Z(), 
                          deltaGR_f(quarks[UP]), 
                          deltaGL_f(quarks[UP]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
   
   double GIMRParamDOWN[10] = {CLL_down(), CLR_down(), CRL_down(), CRR_down(), deltaGamma_Z(), 
                          deltaGR_f(quarks[DOWN]), 
                          deltaGL_f(quarks[DOWN]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
      
   double GIMRParamSTRANGE[10] = {CLL_strange(), CLR_strange(), CRL_strange(), CRR_strange(), deltaGamma_Z(), 
                          deltaGR_f(quarks[STRANGE]), 
                          deltaGL_f(quarks[STRANGE]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
         
   double GIMRParamCHARM[10] = {CLL_charm(), CLR_charm(), CRL_charm(), CRR_charm(), deltaGamma_Z(), 
                          deltaGR_f(quarks[CHARM]), 
                          deltaGL_f(quarks[CHARM]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
            
   double GIMRParamBOTTOM[10] = {CLL_bottom(), CLR_bottom(), CRL_bottom(), CRR_bottom(), deltaGamma_Z(), 
                          deltaGR_f(quarks[BOTTOM]), 
                          deltaGL_f(quarks[BOTTOM]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
   
   sigma_hSM = trueSM.LEP2sigmaHadron(s);
   
   dsigma_had = myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::UP, s, GIMRParamUP) +
                myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::DOWN, s, GIMRParamDOWN) +
                myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::CHARM, s, GIMRParamCHARM) +
                myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::STRANGE, s, GIMRParamSTRANGE) +
                myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::BOTTOM, s, GIMRParamBOTTOM);
   
   dsigma_b = myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::BOTTOM, s, GIMRParamCHARM);
 
   R_bottom = trueSM.LEP2Rbottom(s) * (1 - dsigma_had / sigma_hSM) + dsigma_b / sigma_hSM;
   
   return R_bottom;
}

LEP2Rcharm()

double NPEffectiveGIMR::LEP2Rcharm ( const double  s ) const

virtual

Reimplemented from StandardModel.

Definition at line 3656 of file NPEffectiveGIMR.cpp.

{
   double R_charm = 0., dsigma_c = 0.0, dsigma_had =0.0, sigma_hSM = 0.0;
   double GIMRParamUP[10] = {CLL_up(), CLR_up(), CRL_up(), CRR_up(), deltaGamma_Z(), 
                          deltaGR_f(quarks[UP]), 
                          deltaGL_f(quarks[UP]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
   
   double GIMRParamDOWN[10] = {CLL_down(), CLR_down(), CRL_down(), CRR_down(), deltaGamma_Z(), 
                          deltaGR_f(quarks[DOWN]), 
                          deltaGL_f(quarks[DOWN]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
      
   double GIMRParamSTRANGE[10] = {CLL_strange(), CLR_strange(), CRL_strange(), CRR_strange(), deltaGamma_Z(), 
                          deltaGR_f(quarks[STRANGE]), 
                          deltaGL_f(quarks[STRANGE]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
         
   double GIMRParamCHARM[10] = {CLL_charm(), CLR_charm(), CRL_charm(), CRR_charm(), deltaGamma_Z(), 
                          deltaGR_f(quarks[CHARM]), 
                          deltaGL_f(quarks[CHARM]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
            
   double GIMRParamBOTTOM[10] = {CLL_bottom(), CLR_bottom(), CRL_bottom(), CRR_bottom(), deltaGamma_Z(), 
                          deltaGR_f(quarks[BOTTOM]), 
                          deltaGL_f(quarks[BOTTOM]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
   
   sigma_hSM = trueSM.LEP2sigmaHadron(s);
   
   dsigma_had = myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::UP, s, GIMRParamUP) +
                myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::DOWN, s, GIMRParamDOWN) +
                myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::CHARM, s, GIMRParamCHARM) +
                myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::STRANGE, s, GIMRParamSTRANGE) +
                myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::BOTTOM, s, GIMRParamBOTTOM);
   
   dsigma_c = myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::CHARM, s, GIMRParamCHARM);
           
   R_charm = trueSM.LEP2Rcharm(s) * (1 - dsigma_had / sigma_hSM) + dsigma_c / sigma_hSM;
   
   return R_charm;
}

LEP2sigmaHadron()

double NPEffectiveGIMR::LEP2sigmaHadron ( const double  s ) const

virtual

Reimplemented from StandardModel.

Definition at line 3532 of file NPEffectiveGIMR.cpp.

{
   double sigma_had;
   double GIMRParamUP[10] = {CLL_up(), CLR_up(), CRL_up(), CRR_up(), deltaGamma_Z(), 
                          deltaGR_f(quarks[UP]), 
                          deltaGL_f(quarks[UP]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
   
   double GIMRParamDOWN[10] = {CLL_down(), CLR_down(), CRL_down(), CRR_down(), deltaGamma_Z(), 
                          deltaGR_f(quarks[DOWN]), 
                          deltaGL_f(quarks[DOWN]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
      
   double GIMRParamSTRANGE[10] = {CLL_strange(), CLR_strange(), CRL_strange(), CRR_strange(), deltaGamma_Z(), 
                          deltaGR_f(quarks[STRANGE]), 
                          deltaGL_f(quarks[STRANGE]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
         
   double GIMRParamCHARM[10] = {CLL_charm(), CLR_charm(), CRL_charm(), CRR_charm(), deltaGamma_Z(), 
                          deltaGR_f(quarks[CHARM]), 
                          deltaGL_f(quarks[CHARM]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
            
   double GIMRParamBOTTOM[10] = {CLL_bottom(), CLR_bottom(), CRL_bottom(), CRR_bottom(), deltaGamma_Z(), 
                          deltaGR_f(quarks[BOTTOM]), 
                          deltaGL_f(quarks[BOTTOM]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
           
           
   sigma_had = trueSM.LEP2sigmaHadron(s) + 
              myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::UP, s, GIMRParamUP) +
              myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::DOWN, s, GIMRParamDOWN) +
              myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::CHARM, s, GIMRParamCHARM) +
              myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::STRANGE, s, GIMRParamSTRANGE) +
              myLEP2GIMR.sigma_q_LEP2_GIMR(QCD::BOTTOM, s, GIMRParamBOTTOM);
   
   return sigma_had;
}

LEP2sigmaMu()

double NPEffectiveGIMR::LEP2sigmaMu ( const double  s ) const

virtual

Reimplemented from StandardModel.

Definition at line 3500 of file NPEffectiveGIMR.cpp.

{
   double sigma_mu;
   double GIMRParam[10] = {CLL_mu(), CLR_mu(), CRL_mu(), CRR_mu(), deltaGamma_Z(), 
                          deltaGR_f(leptons[MU]), 
                          deltaGL_f(leptons[MU]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
   
   sigma_mu = trueSM.LEP2sigmaMu(s) + 
              myLEP2GIMR.sigma_l_LEP2_GIMR(QCD::lepton(MU), s, GIMRParam);
   
   return sigma_mu;
}

LEP2sigmaTau()

double NPEffectiveGIMR::LEP2sigmaTau ( const double  s ) const

virtual

Reimplemented from StandardModel.

Definition at line 3516 of file NPEffectiveGIMR.cpp.

{
   double sigma_tau;
   double GIMRParam[10] = {CLL_tau(), CLR_tau(), CRL_tau(), CRR_tau(), deltaGamma_Z(), 
                          deltaGR_f(leptons[TAU]), 
                          deltaGL_f(leptons[TAU]),
                          deltaGR_f(leptons[ELECTRON]),
                          deltaGL_f(leptons[ELECTRON]),
                          deltaMz2()};
   
   sigma_tau = trueSM.LEP2sigmaTau(s) + 
               myLEP2GIMR.sigma_l_LEP2_GIMR(QCD::lepton(TAU), s, GIMRParam);   
   
   return sigma_tau;
}

mueettH()

double NPEffectiveGIMR::mueettH ( const double  sqrt_s ) const

virtual

The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.

Parameters

[in]

sqrt_s

the center-of-mass energy in TeV

Returns

\(\mu_{eettH}\)

Reimplemented from NPbase.

Definition at line 2769 of file NPEffectiveGIMR.cpp.

{
    double mu = 1.0;
    if (sqrt_s == 0.5) {
        mu +=  85.139 * deltaG1_hZZ()
                -51.41 * deltaG2_hZZ()
                +0. * deltaG3_hZZ()
                +276.673 * deltaG1_hZA()
                -159.708 * deltaG2_hZA()
                +1017.44 * deltaG_hAA()
                -2.833 * deltaG_hff(quarks[TOP]).real()
                -287.92 * deltaGL_Zffh(leptons[ELECTRON])
                -132.849 * deltaGR_Zffh(leptons[ELECTRON])
                +84.883 * deltaGL_Zffh(quarks[TOP])
                +72.935 * deltaGR_Zffh(quarks[TOP])
                +863716. * deltaG_hAff(quarks[TOP]).real()
                +154393. * deltaG_hZff(quarks[TOP]).real()
                -1.046 * deltaGL_f(leptons[ELECTRON])
                -0.608 * deltaGR_f(leptons[ELECTRON])
                +0.663 * deltaGL_f(quarks[TOP])
                +0.585 * deltaGR_f(quarks[TOP])
                +8833.35 * deltaG_Aff(quarks[TOP]).real()
                +1650.94 * deltaG_Zff(quarks[TOP]).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 +=  +0.0;
        }
        
    } else if (sqrt_s == 1.0) {
        mu +=  446.758 * deltaG1_hZZ()
                -1500.92 * deltaG2_hZZ()
                +0.003 * deltaG3_hZZ()
                +657.283 * deltaG1_hZA()
                -572.102 * deltaG2_hZA()
                +2443.18 * deltaG_hAA()
                -2.701 * deltaG_hff(quarks[TOP]).real()
                -4591.53 * deltaGL_Zffh(leptons[ELECTRON])
                +2945.96 * deltaGR_Zffh(leptons[ELECTRON])
                +251.003 * deltaGL_Zffh(quarks[TOP])
                +49.581 * deltaGR_Zffh(quarks[TOP])
                +3025550. * deltaG_hAff(quarks[TOP]).real()
                +519896. * deltaG_hZff(quarks[TOP]).real()
                -1.426 * deltaGL_f(leptons[ELECTRON])
                -0.041 * deltaGR_f(leptons[ELECTRON])
                +1.066 * deltaGL_f(quarks[TOP])
                -0.038 * deltaGR_f(quarks[TOP])
                +12745.4 * deltaG_Aff(quarks[TOP]).real()
                +2238.61 * deltaG_Zff(quarks[TOP]).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 +=  +0.0;
        }
        
    } else
        throw std::runtime_error("Bad argument in NPEffectiveGIMR::mueettH()");
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return mu;
}

mueeWBF()

double NPEffectiveGIMR::mueeWBF ( const double  sqrt_s ) const

virtual

The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.

Parameters

[in]

sqrt_s

the center-of-mass energy in TeV

Returns

\(\mu_{eeWBF}\)

Reimplemented from NPbase.

Definition at line 2219 of file NPEffectiveGIMR.cpp.

{
    double mu = 1.0;
    if (sqrt_s == 0.24) {
        mu +=  985.974 * deltaG1_hZZ()
                +23.622 * deltaG2_hZZ()
                +0. * deltaG3_hZZ()
                +377.441 * deltaG1_hZA()
                -394.144 * deltaG2_hZA()
                -30.997 * deltaG1_hWW()
                +273.526 * deltaG2_hWW()
                +0.038 * deltaG3_hWW()
                -62.505 * deltaGL_Zffh(leptons[NEUTRINO_1])
                -1781.02 * deltaGL_Zffh(leptons[ELECTRON])
                +183.495 * deltaGR_Zffh(leptons[ELECTRON])
                -4.991 * deltaGL_Wffh(leptons[NEUTRINO_1],leptons[ELECTRON]).real()
                -0.062 * deltaGL_f(leptons[NEUTRINO_1])
                -1.436 * deltaGL_f(leptons[ELECTRON])
                +0.004 * deltaGR_f(leptons[ELECTRON])
                +4.07 * deltaGL_Wff(leptons[NEUTRINO_1],leptons[ELECTRON]).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 +=  +0.0;            
        }
          
    } else if (sqrt_s == 0.25) {
        mu +=  903.947 * deltaG1_hZZ()
                +93.416 * deltaG2_hZZ()
                -0.002 * deltaG3_hZZ()
                +277.754 * deltaG1_hZA()
                -271.135 * deltaG2_hZA()
                -29.647 * deltaG1_hWW()
                +298.034 * deltaG2_hWW()
                +0.039 * deltaG3_hWW()
                -61.73 * deltaGL_Zffh(leptons[NEUTRINO_1])
                -1409.1 * deltaGL_Zffh(leptons[ELECTRON])
                +182.068 * deltaGR_Zffh(leptons[ELECTRON])
                -5.518 * deltaGL_Wffh(leptons[NEUTRINO_1],leptons[ELECTRON]).real()
                -0.174 * deltaGL_f(leptons[NEUTRINO_1])
                -1.003 * deltaGL_f(leptons[ELECTRON])
                +0. * deltaGR_f(leptons[ELECTRON])
                +4.203 * deltaGL_Wff(leptons[NEUTRINO_1],leptons[ELECTRON]).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 +=  +0.0;
        }
        
    } else if (sqrt_s == 0.35) {
        mu +=  -63.056 * deltaG1_hZZ()
                +99.834 * deltaG2_hZZ()
                -0.001 * deltaG3_hZZ()
                -100.006 * deltaG1_hZA()
                +120.858 * deltaG2_hZA()
                -77.085 * deltaG1_hWW()
                +424.21 * deltaG2_hWW()
                +0.039 * deltaG3_hWW()
                -36.176 * deltaGL_Zffh(leptons[NEUTRINO_1])
                +108.441 * deltaGL_Zffh(leptons[ELECTRON])
                +137.702 * deltaGR_Zffh(leptons[ELECTRON])
                -8.003 * deltaGL_Wffh(leptons[NEUTRINO_1],leptons[ELECTRON]).real()
                -0.091 * deltaGL_f(leptons[NEUTRINO_1])
                +0.074 * deltaGL_f(leptons[ELECTRON])
                +0.033 * deltaGR_f(leptons[ELECTRON])
                +4.102 * deltaGL_Wff(leptons[NEUTRINO_1],leptons[ELECTRON]).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 +=  +0.0;
        }
        
    } else if (sqrt_s == 0.5) {
        mu +=  -82.771 * deltaG1_hZZ()
                +48.73 * deltaG2_hZZ()
                +0. * deltaG3_hZZ()
                -78.056 * deltaG1_hZA()
                +78.264 * deltaG2_hZA()
                -98.794 * deltaG1_hWW()
                +579.5 * deltaG2_hWW()
                +0.039 * deltaG3_hWW()
                -26.448 * deltaGL_Zffh(leptons[NEUTRINO_1])
                +163.236 * deltaGL_Zffh(leptons[ELECTRON])
                +56.583 * deltaGR_Zffh(leptons[ELECTRON])
                -9.491 * deltaGL_Wffh(leptons[NEUTRINO_1],leptons[ELECTRON]).real()
                -0.02 * deltaGL_f(leptons[NEUTRINO_1])
                +0.037 * deltaGL_f(leptons[ELECTRON])
                +0.009 * deltaGR_f(leptons[ELECTRON])
                +4.025 * deltaGL_Wff(leptons[NEUTRINO_1],leptons[ELECTRON]).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 +=  +0.0;
        }
        
    } else if (sqrt_s == 1.0) {
        mu +=  -32.198 * deltaG1_hZZ()
                +13.389 * deltaG2_hZZ()
                +0. * deltaG3_hZZ()
                -27.018 * deltaG1_hZA()
                +18.957 * deltaG2_hZA()
                -100.42 * deltaG1_hWW()
                +884.402 * deltaG2_hWW()
                +0.039 * deltaG3_hWW()
                -11.556 * deltaGL_Zffh(leptons[NEUTRINO_1])
                +56.187 * deltaGL_Zffh(leptons[ELECTRON])
                +16.258 * deltaGR_Zffh(leptons[ELECTRON])
                -12.168 * deltaGL_Wffh(leptons[NEUTRINO_1],leptons[ELECTRON]).real()
                -0.001 * deltaGL_f(leptons[NEUTRINO_1])
                +0.004 * deltaGL_f(leptons[ELECTRON])
                +0.002 * deltaGR_f(leptons[ELECTRON])
                +4.003 * deltaGL_Wff(leptons[NEUTRINO_1],leptons[ELECTRON]).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 +=  +0.0;
        }
        
    } else
        throw std::runtime_error("Bad argument in NPEffectiveGIMR::mueeWBF()");
 
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return mu;
}

mueeZH()

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 2567 of file NPEffectiveGIMR.cpp.

{
    double mu = 1.0;
 
    if (sqrt_s == 0.24) {
        mu += 2690.84 * deltaG1_hZZ()
                -1951.93 * deltaG2_hZZ()
                +0.059 * deltaG3_hZZ()
                +147.761 * deltaG1_hZA()
                -185.735 * deltaG2_hZA()
                -4217.73 * deltaGL_Zffh(leptons[ELECTRON])
                +3619.82 * deltaGR_Zffh(leptons[ELECTRON])
                -4.282 * deltaGL_f(leptons[ELECTRON])
                +3.674 * deltaGR_f(leptons[ELECTRON]);
        
        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);
            }
 
    } else if (sqrt_s == 0.25) {
        mu +=  2829.45 * deltaG1_hZZ()
                -2097.01 * deltaG2_hZZ()
                +0.059 * deltaG3_hZZ()
                +156.787 * deltaG1_hZA()
                -204.357 * deltaG2_hZA()
                -4635.23 * deltaGL_Zffh(leptons[ELECTRON])
                +3979.84 * deltaGR_Zffh(leptons[ELECTRON])
                -4.282 * deltaGL_f(leptons[ELECTRON])
                +3.674 * deltaGR_f(leptons[ELECTRON]);
        
        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 +=  +0.0;
        }
        
    } else if (sqrt_s == 0.35) {
        mu +=  3893.41 * deltaG1_hZZ()
                -3873.83 * deltaG2_hZZ()
                +0.059 * deltaG3_hZZ()
                +231.963 * deltaG1_hZA()
                -424.266 * deltaG2_hZA()
                -9763.89 * deltaGL_Zffh(leptons[ELECTRON])
                +8387.72 * deltaGR_Zffh(leptons[ELECTRON])
                -4.282 * deltaGL_f(leptons[ELECTRON])
                +3.674 * deltaGR_f(leptons[ELECTRON]);
        
        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 +=  +0.0;
        }
          
    } else if (sqrt_s == 0.5) {
        mu +=  4747.11 * deltaG1_hZZ()
                -7649.28 * deltaG2_hZZ()
                +0.059 * deltaG3_hZZ()
                +291.854 * deltaG1_hZA()
                -902.663 * deltaG2_hZA()
                -20668.9 * deltaGL_Zffh(leptons[ELECTRON])
                +17754.2 * deltaGR_Zffh(leptons[ELECTRON])
                -4.282 * deltaGL_f(leptons[ELECTRON])
                +3.674 * deltaGR_f(leptons[ELECTRON]);
        
        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 +=  +0.0;
        }
        
    } else if (sqrt_s == 1.0) {
        mu +=  5576.18 * deltaG1_hZZ()
                -29856.9 * deltaG2_hZZ()
                +0.059 * deltaG3_hZZ()
                +351.186 * deltaG1_hZA()
                -3727.98 * deltaG2_hZA()
                -84814.3 * deltaGL_Zffh(leptons[ELECTRON])
                +72844.9 * deltaGR_Zffh(leptons[ELECTRON])
                -4.282 * deltaGL_f(leptons[ELECTRON])
                +3.673 * deltaGR_f(leptons[ELECTRON]);
        
        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 +=  +0.0;
        }
        
    } else
        throw std::runtime_error("Bad argument in NPEffectiveGIMR::mueeZH()");
    
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return mu;
}

muggH()

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 1990 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 = CHG / v() * v2_over_LambdaNP2 / G_eff_t_SM;
    
    double mu = (1.0 + 2.0 * ( dKappa_t.real() + tmp.real() ) );
    
    if (FlagQuadraticTerms) {
            //Add contributions that are quadratic in the effective coefficients
        gslpp::complex tmp2 = dKappa_t + tmp;
        
        mu += tmp2.abs2();
        
    }
    
    if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
    
    return mu;
}

muggHpttH()

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 2755 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;
} 

muttH()

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 2700 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 if (sqrt_s == 14.0) {
        mu += -2.861 * deltaG_hff(quarks[TOP]).real()
            +2769.79 * 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 +=  +2.012 * pow(deltaG_hff(quarks[TOP]).real(),2.0)
            +5689423. * 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;
}

muVBF()

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 2026 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 if (sqrt_s == 14.0) {
        mu +=  +1.129 * deltaGL_f(quarks[UP])
                -0.505 * deltaGR_f(quarks[UP])
                -1.05 * deltaGL_f(quarks[DOWN])
                +0.191 * deltaGR_f(quarks[DOWN])
            +2.586 * deltaGL_Wff(quarks[UP],quarks[DOWN]).real()
                -1989.34 * deltaGL_Wffh(quarks[UP], quarks[DOWN]).real()
                +14228.8 * deltaG_hgg()
                -35.554 * deltaG_hAA()
                -39.847 * deltaG1_hZA()
                +98.522 * deltaG2_hZA()
                -99.287 * deltaG1_hWW()
                +622.352 * deltaG2_hWW()
                +0.026 * deltaG3_hWW()
                -66.196 * deltaG1_hZZ()
                +196.676 * deltaG2_hZZ()
                +0.014 * deltaG3_hZZ()
                -493.198 * deltaGL_Zffh(quarks[UP])
                +217.017 * deltaGR_Zffh(quarks[UP])
                +447.396 * deltaGL_Zffh(quarks[DOWN])
                -82.396 * 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 +=  +2.319 * pow(deltaGL_f(quarks[UP]),2.0)
                +1.783 * pow(deltaGR_f(quarks[UP]),2.0)
                +1.849 * pow(deltaGL_f(quarks[DOWN]),2.0)
                +1.263 * pow(deltaGR_f(quarks[DOWN]),2.0)
            +2.592 * pow(deltaGL_Wff(quarks[UP],quarks[DOWN]).real(),2.0)
                +4077238. * pow(deltaGL_Wffh(quarks[UP], quarks[DOWN]).real(),2.0)
                +507787376. * pow(deltaG_hgg(),2.0)
                +702353. * pow(deltaG_hAA(),2.0)
                +212082. * pow(deltaG1_hZA(),2.0)
                +141422. * pow(deltaG2_hZA(),2.0)
                +195770. * pow(deltaG1_hWW(),2.0)
                +655804. * pow(deltaG2_hWW(),2.0)
                +0. * pow(deltaG3_hWW(),2.0)
                +240333. * pow(deltaG1_hZZ(),2.0)
                +192371. * pow(deltaG2_hZZ(),2.0)
                +0. * pow(deltaG3_hZZ(),2.0)
                +1904757. * pow(deltaGL_Zffh(quarks[UP]),2.0)
                +1743849. * pow(deltaGR_Zffh(quarks[UP]),2.0)
                +1185212. * pow(deltaGL_Zffh(quarks[DOWN]),2.0)
                +1061826. * 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;
}

muVBFpVH()

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 2685 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;
}

muVH()

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 2672 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;
}

muWH()

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 2350 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 if (sqrt_s == 14.0) {
        mu += +1.963 * deltaGL_Wff(quarks[UP], quarks[DOWN]).real()
                +1799.45 * deltaG1_hWW()
                -4252.03 * deltaG2_hWW()
                +0.039 * deltaG3_hWW()
                +8047.59 * 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 +=  +1.007 * pow(deltaGL_Wff(quarks[UP], quarks[DOWN]).real(),2.0)
                +1467903.  * pow(deltaG1_hWW(),2.0)
                +13173439.  * pow(deltaG2_hWW(),2.0)
                +58780336.  * 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;
}

muZH()

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 2425 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 if (sqrt_s == 14.0) {
        mu += +2.477 * deltaGL_f(quarks[UP])
                -1.103 * deltaGR_f(quarks[UP])
                -2.226 * deltaGL_f(quarks[DOWN])
                +0.405 * deltaGR_f(quarks[DOWN])
                +3321.75 * deltaG1_hZZ()
                -3494.38 * deltaG2_hZZ()
                +0.059 * deltaG3_hZZ()
                +481.727 * deltaG1_hZA()
                -967.239 * deltaG2_hZA()
                +5106.92 * deltaGL_Zffh(quarks[UP])
                -2270.81 * deltaGR_Zffh(quarks[UP])
                -4434.64 * deltaGL_Zffh(quarks[DOWN])
                +807.186 * 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 +=  +3.579 * pow(deltaGL_f(quarks[UP]),2.0)
                +3.58  * pow(deltaGR_f(quarks[UP]),2.0)
                +2.631  * pow(deltaGL_f(quarks[DOWN]),2.0)
                +2.629  * pow(deltaGR_f(quarks[DOWN]),2.0)
                +4609160.  * pow(deltaG1_hZZ(),2.0)
                +7946470.  * pow(deltaG2_hZZ(),2.0)
                +0.001  * pow(deltaG3_hZZ(),2.0)
                +683466.  * pow(deltaG1_hZA(),2.0)
                +5019397.  * pow(deltaG2_hZA(),2.0)
                +50036976.  * pow(deltaGL_Zffh(quarks[UP]),2.0)
                +50008570.  * pow(deltaGR_Zffh(quarks[UP]),2.0)
                +31660707.  * pow(deltaGL_Zffh(quarks[DOWN]),2.0)
                +31666009.  * 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;
}

Mw()

double NPEffectiveGIMR::Mw ( ) const

virtual

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

Returns

\(M_W\) in GeV

Reimplemented from NPbase.

Definition at line 1714 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()));
}

obliqueS()

double NPEffectiveGIMR::obliqueS ( ) const

virtual

The oblique parameter \(S\).

Returns

the value of \(S\)

Reimplemented from NPbase.

Definition at line 1694 of file NPEffectiveGIMR.cpp.

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

obliqueT()

double NPEffectiveGIMR::obliqueT ( ) const

virtual

The oblique parameter \(T\).

Returns

the value of \(T\)

Reimplemented from NPbase.

Definition at line 1699 of file NPEffectiveGIMR.cpp.

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

obliqueU()

double NPEffectiveGIMR::obliqueU ( ) const

virtual

The oblique parameter \(U\).

Returns

the value of \(U\)

Reimplemented from NPbase.

Definition at line 1704 of file NPEffectiveGIMR.cpp.

{
    return 0.0;
}

PostUpdate()

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 535 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);
}

setFlag()

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 1486 of file NPEffectiveGIMR.cpp.

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

setParameter()

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 558 of file NPEffectiveGIMR.cpp.

{
    if (name.compare("CG") == 0)
        CG = value;
    else if (name.compare("CW") == 0)
        CW = value;
    else 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("CuG_11r") == 0)
        CuG_11r = value;
    else if (name.compare("CuG_12r") == 0)
        CuG_12r = value;
    else if (name.compare("CuG_13r") == 0)
        CuG_13r = value;
    else if (name.compare("CuG_22r") == 0)
        CuG_22r = value;
    else if (name.compare("CuG_23r") == 0)
        CuG_23r = value;
    else if (name.compare("CuG_33r") == 0)
        CuG_33r = value;
    else if (name.compare("CuG_r") == 0) {
        CuG_11r = value;
        CuG_12r = 0.0;
        CuG_13r = 0.0;
        CuG_22r = value;
        CuG_23r = 0.0;
        CuG_33r = value;
    } else if (name.compare("CuG_11i") == 0)
        CuG_11i = value;
    else if (name.compare("CuG_12i") == 0)
        CuG_12i = value;
    else if (name.compare("CuG_13i") == 0)
        CuG_13i = value;
    else if (name.compare("CuG_22i") == 0)
        CuG_22i = value;
    else if (name.compare("CuG_23i") == 0)
        CuG_23i = value;
    else if (name.compare("CuG_33i") == 0)
        CuG_33i = value;
    else if (name.compare("CuG_i") == 0) {
        CuG_11i = value;
        CuG_12i = 0.0;
        CuG_13i = 0.0;
        CuG_22i = value;
        CuG_23i = 0.0;
        CuG_33i = value;
    } else if (name.compare("CuW_11r") == 0)
        CuW_11r = value;
    else if (name.compare("CuW_12r") == 0)
        CuW_12r = value;
    else if (name.compare("CuW_13r") == 0)
        CuW_13r = value;
    else if (name.compare("CuW_22r") == 0)
        CuW_22r = value;
    else if (name.compare("CuW_23r") == 0)
        CuW_23r = value;
    else if (name.compare("CuW_33r") == 0)
        CuW_33r = value;
    else if (name.compare("CuW_r") == 0) {
        CuW_11r = value;
        CuW_12r = 0.0;
        CuW_13r = 0.0;
        CuW_22r = value;
        CuW_23r = 0.0;
        CuW_33r = value;
    } else if (name.compare("CuW_11i") == 0)
        CuW_11i = value;
    else if (name.compare("CuW_12i") == 0)
        CuW_12i = value;
    else if (name.compare("CuW_13i") == 0)
        CuW_13i = value;
    else if (name.compare("CuW_22i") == 0)
        CuW_22i = value;
    else if (name.compare("CuW_23i") == 0)
        CuW_23i = value;
    else if (name.compare("CuW_33i") == 0)
        CuW_33i = value;
    else if (name.compare("CuW_i") == 0) {
        CuW_11i = value;
        CuW_12i = 0.0;
        CuW_13i = 0.0;
        CuW_22i = value;
        CuW_23i = 0.0;
        CuW_33i = value;
    } else if (name.compare("CuB_11r") == 0)
        CuB_11r = value;
    else if (name.compare("CuB_12r") == 0)
        CuB_12r = value;
    else if (name.compare("CuB_13r") == 0)
        CuB_13r = value;
    else if (name.compare("CuB_22r") == 0)
        CuB_22r = value;
    else if (name.compare("CuB_23r") == 0)
        CuB_23r = value;
    else if (name.compare("CuB_33r") == 0)
        CuB_33r = value;
    else if (name.compare("CuB_r") == 0) {
        CuB_11r = value;
        CuB_12r = 0.0;
        CuB_13r = 0.0;
        CuB_22r = value;
        CuB_23r = 0.0;
        CuB_33r = value;
    } else if (name.compare("CuB_11i") == 0)
        CuB_11i = value;
    else if (name.compare("CuB_12i") == 0)
        CuB_12i = value;
    else if (name.compare("CuB_13i") == 0)
        CuB_13i = value;
    else if (name.compare("CuB_22i") == 0)
        CuB_22i = value;
    else if (name.compare("CuB_23i") == 0)
        CuB_23i = value;
    else if (name.compare("CuB_33i") == 0)
        CuB_33i = value;
    else if (name.compare("CuB_i") == 0) {
        CuB_11i = value;
        CuB_12i = 0.0;
        CuB_13i = 0.0;
        CuB_22i = value;
        CuB_23i = 0.0;
        CuB_33i = value;
    } else if (name.compare("CLL_1111") == 0) {
        CLL_1111 = value;
    } else if (name.compare("CLL_1221") == 0) {
        CLL_1221 = value;
        CLL_2112 = value;
        CLL_2211 = value;
        CLL_1122 = value;
    } else if (name.compare("CLL_1133") == 0) {
        CLL_1331 = value;
        CLL_3113 = value;
        CLL_3311 = value;
        CLL_1133 = value;
    } else if (name.compare("CLL") == 0) {
        CLL_1111 = value;
        CLL_1221 = value;
        CLL_2112 = value;
        CLL_2211 = value;
        CLL_1122 = value;
        CLL_3311 = value;
        CLL_1133 = value;
        CLL_1331 = value;
        CLL_3113 = value;
    } else if (name.compare("CLQ1_1111") == 0) {
        CLQ1_1111 = value;
    } else if (name.compare("CLQ1_1122") == 0) {
        CLQ1_1122 = value;
        CLQ1_2211 = value;
        CLQ1_1221 = value;
        CLQ1_2112 = value;
    } else if (name.compare("CLQ1_1133") == 0) {
        CLQ1_1133 = value;
        CLQ1_3311 = value;
        CLQ1_1331 = value;
        CLQ1_3113 = value;
    } else if (name.compare("CLQ1") == 0) {
        CLQ1_1111 = value;
        CLQ1_1122 = value;
        CLQ1_2211 = value;
        CLQ1_1221 = value;
        CLQ1_2112 = value;
        CLQ1_1133 = value;
        CLQ1_3311 = value;
        CLQ1_1331 = value;
        CLQ1_3113 = value;
    } else if (name.compare("CLQ1_1111") == 0) {
        CLQ1_1111 = value;
    } else if (name.compare("CLQ1_1122") == 0) {
        CLQ1_1122 = value;
        CLQ1_2211 = value;
        CLQ1_2112 = value;
        CLQ1_1221 = value;
    } else if (name.compare("CLQ1_1133") == 0) {
        CLQ1_1133 = value;
        CLQ1_3311 = value;
        CLQ1_3113 = value;
        CLQ1_1331 = value;
    } else if (name.compare("CLQ1_1123") == 0) {
        CLQ1_1123 = value;
    } else if (name.compare("CLQ1_2223") == 0) {
        CLQ1_2223 = value;
    } else if (name.compare("CLQ1_3323") == 0) {
        CLQ1_3323 = value;
    } else if (name.compare("CLQ1_1132") == 0) {
        CLQ1_1132 = value;
    } else if (name.compare("CLQ1_2232") == 0) {
        CLQ1_2232 = value;
    } else if (name.compare("CLQ1_3332") == 0) {
        CLQ1_3332 = value;
    } else if (name.compare("CLQ3") == 0) {
        CLQ3_1111 = value;
        CLQ3_1122 = value;
        CLQ3_2211 = value;
        CLQ3_1221 = value;
        CLQ3_2112 = value;
        CLQ3_1133 = value;
        CLQ3_3311 = value;
        CLQ3_1331 = value;
        CLQ3_3113 = value;
    } else if (name.compare("CLQ3_1111") == 0) {
        CLQ3_1111 = value;
    } else if (name.compare("CLQ3_1122") == 0) {
        CLQ3_1122 = value;
        CLQ3_2211 = value;
        CLQ3_2112 = value;
        CLQ3_1221 = value;
    } else if (name.compare("CLQ3_1133") == 0) {
        CLQ3_1133 = value;
        CLQ3_3311 = value;
        CLQ3_3113 = value;
        CLQ3_1331 = value;
    } else if (name.compare("CLQ3_1123") == 0) {
        CLQ3_1123 = value;
    } else if (name.compare("CLQ3_2223") == 0) {
        CLQ3_2223 = value;
    } else if (name.compare("CLQ3_3323") == 0) {
        CLQ3_3323 = value;
    } else if (name.compare("CLQ3_1132") == 0) {
        CLQ3_1132 = value;
    } else if (name.compare("CLQ3_2232") == 0) {
        CLQ3_2232 = value;
    } else if (name.compare("CLQ3_3332") == 0) {
        CLQ3_3332 = value;
    } else if (name.compare("Cee") == 0) {
        Cee_1111 = value;
        Cee_1122 = value;
        Cee_2211 = value;
        Cee_1133 = value;
        Cee_3311 = value;
    } else if (name.compare("Cee_1111") == 0) {
        Cee_1111 = value;
    } else if (name.compare("Cee_1122") == 0) {
        Cee_1122 = value;
        Cee_2211 = value;
    } else if (name.compare("Cee_1133") == 0) {
        Cee_1133 = value;
        Cee_3311 = value;
    } else if (name.compare("Ceu") == 0) {
        Ceu_1111 = value;
        Ceu_1122 = value;
        Ceu_2211 = value;
        Ceu_1133 = value;
        Ceu_3311 = value;
    } else if (name.compare("Ceu_1111") == 0) {
        Ceu_1111 = value;
    } else if (name.compare("Ceu_1122") == 0) {
        Ceu_1122 = value;
        Ceu_2211 = value;
    } else if (name.compare("Ceu_1133") == 0) {
        Ceu_1133 = value;
        Ceu_3311 = value;
    } else if (name.compare("Ced") == 0) {
        Ced_1111 = value;
        Ced_1122 = value;
        Ced_2211 = value;
        Ced_1133 = value;
        Ced_3311 = value;
    } else if (name.compare("Ced_1111") == 0) {
        Ced_1111 = value;
    } else if (name.compare("Ced_1122") == 0) {
        Ced_1122 = value;
        Ced_2211 = value;
    } else if (name.compare("Ced_1133") == 0) {
        Ced_1133 = value;
        Ced_3311 = value;
    } else if (name.compare("Ced_1123") == 0) {
        Ced_1123 = value;
    } else if (name.compare("Ced_2223") == 0) {
        Ced_2223 = value;
    } else if (name.compare("Ced_3323") == 0) {
        Ced_3323 = value;
    } else if (name.compare("Ced_1132") == 0) {
        Ced_1132 = value;
    } else if (name.compare("Ced_2232") == 0) {
        Ced_2232 = value;
    } else if (name.compare("Ced_3332") == 0) {
        Ced_3332 = value;
    } else if (name.compare("CLe") == 0) {
        CLe_1111 = value;
        CLe_1122 = value;
        CLe_2211 = value;
        CLe_1133 = value;
        CLe_3311 = value;
    } else if (name.compare("CLe_1111") == 0) {
        CLe_1111 = value;
    } else if (name.compare("CLe_1122") == 0) {
        CLe_1122 = value;
        CLe_2211 = value;
    } else if (name.compare("CLe_1133") == 0) {
        CLe_1133 = value;
        CLe_3311 = value;
    } else if (name.compare("CLu") == 0) {
        CLu_1111 = value;
        CLu_1122 = value;
        CLu_2211 = value;
        CLu_1133 = value;
        CLu_3311 = value;
    } else if (name.compare("CLu_1111") == 0) {
        CLu_1111 = value;
    } else if (name.compare("CLu_1122") == 0) {
        CLu_1122 = value;
        CLu_2211 = value;
    } else if (name.compare("CLu_1133") == 0) {
        CLu_1133 = value;
        CLu_3311 = value;
    } else if (name.compare("CLd") == 0) {
        CLd_1111 = value;
        CLd_1122 = value;
        CLd_2211 = value;
        CLd_1133 = value;
        CLd_3311 = value;
    } else if (name.compare("CLd_1111") == 0) {
        CLd_1111 = value;
    } else if (name.compare("CLd_1122") == 0) {
        CLd_1122 = value;
        CLd_2211 = value;
    } else if (name.compare("CLd_1133") == 0) {
        CLd_1133 = value;
        CLd_3311 = value;
    } else if (name.compare("CLd_1123") == 0) {
        CLd_1123 = value;
    } else if (name.compare("CLd_2223") == 0) {
        CLd_2223 = value;
    } else if (name.compare("CLd_3323") == 0) {
        CLd_3323 = value;
    } else if (name.compare("CLd_1132") == 0) {
        CLd_1132 = value;
    } else if (name.compare("CLd_2232") == 0) {
        CLd_2232 = value;
    } else if (name.compare("CLd_3332") == 0) {
        CLd_3332 = value;
    } else if (name.compare("CQe") == 0) {
        CQe_1111 = value;
        CQe_1122 = value;
        CQe_2211 = value;
        CQe_1133 = value;
        CQe_3311 = value;
    } else if (name.compare("CQe_1111") == 0) {
        CQe_1111 = value;
    } else if (name.compare("CQe_1122") == 0) {
        CQe_1122 = value;
        CQe_2211 = value;
    } else if (name.compare("CQe_1133") == 0) {
        CQe_1133 = value;
        CQe_3311 = value;
    } else if (name.compare("CQe_2311") == 0) {
        CQe_2311 = value;
    } else if (name.compare("CQe_2322") == 0) {
        CQe_2322 = value;
    } else if (name.compare("CQe_2333") == 0) {
        CQe_2333 = value;
    } else if (name.compare("CQe_3211") == 0) {
        CQe_3211 = value;
    } else if (name.compare("CQe_3222") == 0) {
        CQe_3222 = value;
    } else if (name.compare("CQe_3233") == 0) {
        CQe_3233 = 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

CdH_11i

double NPEffectiveGIMR::CdH_11i

protected

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

Definition at line 1436 of file NPEffectiveGIMR.h.

CdH_11r

double NPEffectiveGIMR::CdH_11r

protected

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

Definition at line 1430 of file NPEffectiveGIMR.h.

CdH_12i

double NPEffectiveGIMR::CdH_12i

protected

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

Definition at line 1437 of file NPEffectiveGIMR.h.

CdH_12r

double NPEffectiveGIMR::CdH_12r

protected

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

Definition at line 1431 of file NPEffectiveGIMR.h.

CdH_13i

double NPEffectiveGIMR::CdH_13i

protected

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

Definition at line 1438 of file NPEffectiveGIMR.h.

CdH_13r

double NPEffectiveGIMR::CdH_13r

protected

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

Definition at line 1432 of file NPEffectiveGIMR.h.

CdH_22i

double NPEffectiveGIMR::CdH_22i

protected

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

Definition at line 1439 of file NPEffectiveGIMR.h.

CdH_22r

double NPEffectiveGIMR::CdH_22r

protected

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

Definition at line 1433 of file NPEffectiveGIMR.h.

CdH_23i

double NPEffectiveGIMR::CdH_23i

protected

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

Definition at line 1440 of file NPEffectiveGIMR.h.

CdH_23r

double NPEffectiveGIMR::CdH_23r

protected

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

Definition at line 1434 of file NPEffectiveGIMR.h.

CdH_33i

double NPEffectiveGIMR::CdH_33i

protected

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

Definition at line 1441 of file NPEffectiveGIMR.h.

CdH_33r

double NPEffectiveGIMR::CdH_33r

protected

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

Definition at line 1435 of file NPEffectiveGIMR.h.

Ced_1111

double NPEffectiveGIMR::Ced_1111

protected

Definition at line 1497 of file NPEffectiveGIMR.h.

Ced_1122

double NPEffectiveGIMR::Ced_1122

protected

Definition at line 1498 of file NPEffectiveGIMR.h.

Ced_1123

double NPEffectiveGIMR::Ced_1123

protected

Definition at line 1500 of file NPEffectiveGIMR.h.

Ced_1132

double NPEffectiveGIMR::Ced_1132

protected

Definition at line 1501 of file NPEffectiveGIMR.h.

Ced_1133

double NPEffectiveGIMR::Ced_1133

protected

Definition at line 1499 of file NPEffectiveGIMR.h.

Ced_2211

double NPEffectiveGIMR::Ced_2211

protected

Definition at line 1498 of file NPEffectiveGIMR.h.

Ced_2223

double NPEffectiveGIMR::Ced_2223

protected

Definition at line 1500 of file NPEffectiveGIMR.h.

Ced_2232

double NPEffectiveGIMR::Ced_2232

protected

Definition at line 1501 of file NPEffectiveGIMR.h.

Ced_3311

double NPEffectiveGIMR::Ced_3311

protected

Definition at line 1499 of file NPEffectiveGIMR.h.

Ced_3323

double NPEffectiveGIMR::Ced_3323

protected

Definition at line 1500 of file NPEffectiveGIMR.h.

Ced_3332

double NPEffectiveGIMR::Ced_3332

protected

Definition at line 1501 of file NPEffectiveGIMR.h.

Cee_1111

double NPEffectiveGIMR::Cee_1111

protected

Definition at line 1491 of file NPEffectiveGIMR.h.

Cee_1122

double NPEffectiveGIMR::Cee_1122

protected

Definition at line 1492 of file NPEffectiveGIMR.h.

Cee_1133

double NPEffectiveGIMR::Cee_1133

protected

Definition at line 1493 of file NPEffectiveGIMR.h.

Cee_2211

double NPEffectiveGIMR::Cee_2211

protected

Definition at line 1492 of file NPEffectiveGIMR.h.

Cee_3311

double NPEffectiveGIMR::Cee_3311

protected

Definition at line 1493 of file NPEffectiveGIMR.h.

CeH_11i

double NPEffectiveGIMR::CeH_11i

protected

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

Definition at line 1412 of file NPEffectiveGIMR.h.

CeH_11r

double NPEffectiveGIMR::CeH_11r

protected

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

Definition at line 1406 of file NPEffectiveGIMR.h.

CeH_12i

double NPEffectiveGIMR::CeH_12i

protected

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

Definition at line 1413 of file NPEffectiveGIMR.h.

CeH_12r

double NPEffectiveGIMR::CeH_12r

protected

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

Definition at line 1407 of file NPEffectiveGIMR.h.

CeH_13i

double NPEffectiveGIMR::CeH_13i

protected

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

Definition at line 1414 of file NPEffectiveGIMR.h.

CeH_13r

double NPEffectiveGIMR::CeH_13r

protected

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

Definition at line 1408 of file NPEffectiveGIMR.h.

CeH_22i

double NPEffectiveGIMR::CeH_22i

protected

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

Definition at line 1415 of file NPEffectiveGIMR.h.

CeH_22r

double NPEffectiveGIMR::CeH_22r

protected

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

Definition at line 1409 of file NPEffectiveGIMR.h.

CeH_23i

double NPEffectiveGIMR::CeH_23i

protected

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

Definition at line 1416 of file NPEffectiveGIMR.h.

CeH_23r

double NPEffectiveGIMR::CeH_23r

protected

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

Definition at line 1410 of file NPEffectiveGIMR.h.

CeH_33i

double NPEffectiveGIMR::CeH_33i

protected

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

Definition at line 1417 of file NPEffectiveGIMR.h.

CeH_33r

double NPEffectiveGIMR::CeH_33r

protected

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

Definition at line 1411 of file NPEffectiveGIMR.h.

Ceu_1111

double NPEffectiveGIMR::Ceu_1111

protected

Definition at line 1494 of file NPEffectiveGIMR.h.

Ceu_1122

double NPEffectiveGIMR::Ceu_1122

protected

Definition at line 1495 of file NPEffectiveGIMR.h.

Ceu_1133

double NPEffectiveGIMR::Ceu_1133

protected

Definition at line 1496 of file NPEffectiveGIMR.h.

Ceu_2211

double NPEffectiveGIMR::Ceu_2211

protected

Definition at line 1495 of file NPEffectiveGIMR.h.

Ceu_3311

double NPEffectiveGIMR::Ceu_3311

protected

Definition at line 1496 of file NPEffectiveGIMR.h.

CG

double NPEffectiveGIMR::CG

protected

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

Definition at line 1322 of file NPEffectiveGIMR.h.

CH

double NPEffectiveGIMR::CH

protected

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

Definition at line 1330 of file NPEffectiveGIMR.h.

CHB

double NPEffectiveGIMR::CHB

protected

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

Definition at line 1326 of file NPEffectiveGIMR.h.

CHbox

double NPEffectiveGIMR::CHbox

protected

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

Definition at line 1329 of file NPEffectiveGIMR.h.

CHD

double NPEffectiveGIMR::CHD

protected

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

Definition at line 1328 of file NPEffectiveGIMR.h.

CHd_11

double NPEffectiveGIMR::CHd_11

protected

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

Definition at line 1385 of file NPEffectiveGIMR.h.

CHd_12i

double NPEffectiveGIMR::CHd_12i

protected

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

Definition at line 1391 of file NPEffectiveGIMR.h.

CHd_12r

double NPEffectiveGIMR::CHd_12r

protected

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

Definition at line 1386 of file NPEffectiveGIMR.h.

CHd_13i

double NPEffectiveGIMR::CHd_13i

protected

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

Definition at line 1392 of file NPEffectiveGIMR.h.

CHd_13r

double NPEffectiveGIMR::CHd_13r

protected

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

Definition at line 1387 of file NPEffectiveGIMR.h.

CHd_22

double NPEffectiveGIMR::CHd_22

protected

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

Definition at line 1388 of file NPEffectiveGIMR.h.

CHd_23i

double NPEffectiveGIMR::CHd_23i

protected

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

Definition at line 1393 of file NPEffectiveGIMR.h.

CHd_23r

double NPEffectiveGIMR::CHd_23r

protected

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

Definition at line 1389 of file NPEffectiveGIMR.h.

CHd_33

double NPEffectiveGIMR::CHd_33

protected

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

Definition at line 1390 of file NPEffectiveGIMR.h.

CHe_11

double NPEffectiveGIMR::CHe_11

protected

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

Definition at line 1349 of file NPEffectiveGIMR.h.

CHe_12i

double NPEffectiveGIMR::CHe_12i

protected

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

Definition at line 1355 of file NPEffectiveGIMR.h.

CHe_12r

double NPEffectiveGIMR::CHe_12r

protected

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

Definition at line 1350 of file NPEffectiveGIMR.h.

CHe_13i

double NPEffectiveGIMR::CHe_13i

protected

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

Definition at line 1356 of file NPEffectiveGIMR.h.

CHe_13r

double NPEffectiveGIMR::CHe_13r

protected

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

Definition at line 1351 of file NPEffectiveGIMR.h.

CHe_22

double NPEffectiveGIMR::CHe_22

protected

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

Definition at line 1352 of file NPEffectiveGIMR.h.

CHe_23i

double NPEffectiveGIMR::CHe_23i

protected

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

Definition at line 1357 of file NPEffectiveGIMR.h.

CHe_23r

double NPEffectiveGIMR::CHe_23r

protected

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

Definition at line 1353 of file NPEffectiveGIMR.h.

CHe_33

double NPEffectiveGIMR::CHe_33

protected

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

Definition at line 1354 of file NPEffectiveGIMR.h.

CHG

double NPEffectiveGIMR::CHG

protected

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

Definition at line 1324 of file NPEffectiveGIMR.h.

CHL1_11

double NPEffectiveGIMR::CHL1_11

protected

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

Definition at line 1331 of file NPEffectiveGIMR.h.

CHL1_12i

double NPEffectiveGIMR::CHL1_12i

protected

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

Definition at line 1337 of file NPEffectiveGIMR.h.

CHL1_12r

double NPEffectiveGIMR::CHL1_12r

protected

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

Definition at line 1332 of file NPEffectiveGIMR.h.

CHL1_13i

double NPEffectiveGIMR::CHL1_13i

protected

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

Definition at line 1338 of file NPEffectiveGIMR.h.

CHL1_13r

double NPEffectiveGIMR::CHL1_13r

protected

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

Definition at line 1333 of file NPEffectiveGIMR.h.

CHL1_22

double NPEffectiveGIMR::CHL1_22

protected

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

Definition at line 1334 of file NPEffectiveGIMR.h.

CHL1_23i

double NPEffectiveGIMR::CHL1_23i

protected

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

Definition at line 1339 of file NPEffectiveGIMR.h.

CHL1_23r

double NPEffectiveGIMR::CHL1_23r

protected

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

Definition at line 1335 of file NPEffectiveGIMR.h.

CHL1_33

double NPEffectiveGIMR::CHL1_33

protected

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

Definition at line 1336 of file NPEffectiveGIMR.h.

CHL3_11

double NPEffectiveGIMR::CHL3_11

protected

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

Definition at line 1340 of file NPEffectiveGIMR.h.

CHL3_12i

double NPEffectiveGIMR::CHL3_12i

protected

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

Definition at line 1346 of file NPEffectiveGIMR.h.

CHL3_12r

double NPEffectiveGIMR::CHL3_12r

protected

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

Definition at line 1341 of file NPEffectiveGIMR.h.

CHL3_13i

double NPEffectiveGIMR::CHL3_13i

protected

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

Definition at line 1347 of file NPEffectiveGIMR.h.

CHL3_13r

double NPEffectiveGIMR::CHL3_13r

protected

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

Definition at line 1342 of file NPEffectiveGIMR.h.

CHL3_22

double NPEffectiveGIMR::CHL3_22

protected

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

Definition at line 1343 of file NPEffectiveGIMR.h.

CHL3_23i

double NPEffectiveGIMR::CHL3_23i

protected

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

Definition at line 1348 of file NPEffectiveGIMR.h.

CHL3_23r

double NPEffectiveGIMR::CHL3_23r

protected

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

Definition at line 1344 of file NPEffectiveGIMR.h.

CHL3_33

double NPEffectiveGIMR::CHL3_33

protected

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

Definition at line 1345 of file NPEffectiveGIMR.h.

CHQ1_11

double NPEffectiveGIMR::CHQ1_11

protected

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

Definition at line 1358 of file NPEffectiveGIMR.h.

CHQ1_12i

double NPEffectiveGIMR::CHQ1_12i

protected

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

Definition at line 1364 of file NPEffectiveGIMR.h.

CHQ1_12r

double NPEffectiveGIMR::CHQ1_12r

protected

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

Definition at line 1359 of file NPEffectiveGIMR.h.

CHQ1_13i

double NPEffectiveGIMR::CHQ1_13i

protected

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

Definition at line 1365 of file NPEffectiveGIMR.h.

CHQ1_13r

double NPEffectiveGIMR::CHQ1_13r

protected

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

Definition at line 1360 of file NPEffectiveGIMR.h.

CHQ1_22

double NPEffectiveGIMR::CHQ1_22

protected

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

Definition at line 1361 of file NPEffectiveGIMR.h.

CHQ1_23i

double NPEffectiveGIMR::CHQ1_23i

protected

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

Definition at line 1366 of file NPEffectiveGIMR.h.

CHQ1_23r

double NPEffectiveGIMR::CHQ1_23r

protected

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

Definition at line 1362 of file NPEffectiveGIMR.h.

CHQ1_33

double NPEffectiveGIMR::CHQ1_33

protected

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

Definition at line 1363 of file NPEffectiveGIMR.h.

CHQ3_11

double NPEffectiveGIMR::CHQ3_11

protected

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

Definition at line 1367 of file NPEffectiveGIMR.h.

CHQ3_12i

double NPEffectiveGIMR::CHQ3_12i

protected

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

Definition at line 1373 of file NPEffectiveGIMR.h.

CHQ3_12r

double NPEffectiveGIMR::CHQ3_12r

protected

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

Definition at line 1368 of file NPEffectiveGIMR.h.

CHQ3_13i

double NPEffectiveGIMR::CHQ3_13i

protected

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

Definition at line 1374 of file NPEffectiveGIMR.h.

CHQ3_13r

double NPEffectiveGIMR::CHQ3_13r

protected

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

Definition at line 1369 of file NPEffectiveGIMR.h.

CHQ3_22

double NPEffectiveGIMR::CHQ3_22

protected

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

Definition at line 1370 of file NPEffectiveGIMR.h.

CHQ3_23i

double NPEffectiveGIMR::CHQ3_23i

protected

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

Definition at line 1375 of file NPEffectiveGIMR.h.

CHQ3_23r

double NPEffectiveGIMR::CHQ3_23r

protected

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

Definition at line 1371 of file NPEffectiveGIMR.h.

CHQ3_33

double NPEffectiveGIMR::CHQ3_33

protected

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

Definition at line 1372 of file NPEffectiveGIMR.h.

CHu_11

double NPEffectiveGIMR::CHu_11

protected

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

Definition at line 1376 of file NPEffectiveGIMR.h.

CHu_12i

double NPEffectiveGIMR::CHu_12i

protected

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

Definition at line 1382 of file NPEffectiveGIMR.h.

CHu_12r

double NPEffectiveGIMR::CHu_12r

protected

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

Definition at line 1377 of file NPEffectiveGIMR.h.

CHu_13i

double NPEffectiveGIMR::CHu_13i

protected

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

Definition at line 1383 of file NPEffectiveGIMR.h.

CHu_13r

double NPEffectiveGIMR::CHu_13r

protected

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

Definition at line 1378 of file NPEffectiveGIMR.h.

CHu_22

double NPEffectiveGIMR::CHu_22

protected

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

Definition at line 1379 of file NPEffectiveGIMR.h.

CHu_23i

double NPEffectiveGIMR::CHu_23i

protected

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

Definition at line 1384 of file NPEffectiveGIMR.h.

CHu_23r

double NPEffectiveGIMR::CHu_23r

protected

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

Definition at line 1380 of file NPEffectiveGIMR.h.

CHu_33

double NPEffectiveGIMR::CHu_33

protected

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

Definition at line 1381 of file NPEffectiveGIMR.h.

CHud_11i

double NPEffectiveGIMR::CHud_11i

protected

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

Definition at line 1400 of file NPEffectiveGIMR.h.

CHud_11r

double NPEffectiveGIMR::CHud_11r

protected

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

Definition at line 1394 of file NPEffectiveGIMR.h.

CHud_12i

double NPEffectiveGIMR::CHud_12i

protected

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

Definition at line 1401 of file NPEffectiveGIMR.h.

CHud_12r

double NPEffectiveGIMR::CHud_12r

protected

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

Definition at line 1395 of file NPEffectiveGIMR.h.

CHud_13i

double NPEffectiveGIMR::CHud_13i

protected

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

Definition at line 1402 of file NPEffectiveGIMR.h.

CHud_13r

double NPEffectiveGIMR::CHud_13r

protected

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

Definition at line 1396 of file NPEffectiveGIMR.h.

CHud_22i

double NPEffectiveGIMR::CHud_22i

protected

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

Definition at line 1403 of file NPEffectiveGIMR.h.

CHud_22r

double NPEffectiveGIMR::CHud_22r

protected

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

Definition at line 1397 of file NPEffectiveGIMR.h.

CHud_23i

double NPEffectiveGIMR::CHud_23i

protected

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

Definition at line 1404 of file NPEffectiveGIMR.h.

CHud_23r

double NPEffectiveGIMR::CHud_23r

protected

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

Definition at line 1398 of file NPEffectiveGIMR.h.

CHud_33i

double NPEffectiveGIMR::CHud_33i

protected

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

Definition at line 1405 of file NPEffectiveGIMR.h.

CHud_33r

double NPEffectiveGIMR::CHud_33r

protected

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

Definition at line 1399 of file NPEffectiveGIMR.h.

CHW

double NPEffectiveGIMR::CHW

protected

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

Definition at line 1325 of file NPEffectiveGIMR.h.

CHWB

double NPEffectiveGIMR::CHWB

protected

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

Definition at line 1327 of file NPEffectiveGIMR.h.

CLd_1111

double NPEffectiveGIMR::CLd_1111

protected

Definition at line 1508 of file NPEffectiveGIMR.h.

CLd_1122

double NPEffectiveGIMR::CLd_1122

protected

Definition at line 1509 of file NPEffectiveGIMR.h.

CLd_1123

double NPEffectiveGIMR::CLd_1123

protected

Definition at line 1511 of file NPEffectiveGIMR.h.

CLd_1132

double NPEffectiveGIMR::CLd_1132

protected

Definition at line 1512 of file NPEffectiveGIMR.h.

CLd_1133

double NPEffectiveGIMR::CLd_1133

protected

Definition at line 1510 of file NPEffectiveGIMR.h.

CLd_2211

double NPEffectiveGIMR::CLd_2211

protected

Definition at line 1509 of file NPEffectiveGIMR.h.

CLd_2223

double NPEffectiveGIMR::CLd_2223

protected

Definition at line 1511 of file NPEffectiveGIMR.h.

CLd_2232

double NPEffectiveGIMR::CLd_2232

protected

Definition at line 1512 of file NPEffectiveGIMR.h.

CLd_3311

double NPEffectiveGIMR::CLd_3311

protected

Definition at line 1510 of file NPEffectiveGIMR.h.

CLd_3323

double NPEffectiveGIMR::CLd_3323

protected

Definition at line 1511 of file NPEffectiveGIMR.h.

CLd_3332

double NPEffectiveGIMR::CLd_3332

protected

Definition at line 1512 of file NPEffectiveGIMR.h.

CLe_1111

double NPEffectiveGIMR::CLe_1111

protected

Definition at line 1502 of file NPEffectiveGIMR.h.

CLe_1122

double NPEffectiveGIMR::CLe_1122

protected

Definition at line 1503 of file NPEffectiveGIMR.h.

CLe_1133

double NPEffectiveGIMR::CLe_1133

protected

Definition at line 1504 of file NPEffectiveGIMR.h.

CLe_2211

double NPEffectiveGIMR::CLe_2211

protected

Definition at line 1503 of file NPEffectiveGIMR.h.

CLe_3311

double NPEffectiveGIMR::CLe_3311

protected

Definition at line 1504 of file NPEffectiveGIMR.h.

CLL_1111

double NPEffectiveGIMR::CLL_1111

protected

Definition at line 1478 of file NPEffectiveGIMR.h.

CLL_1122

double NPEffectiveGIMR::CLL_1122

protected

Definition at line 1479 of file NPEffectiveGIMR.h.

CLL_1133

double NPEffectiveGIMR::CLL_1133

protected

Definition at line 1480 of file NPEffectiveGIMR.h.

CLL_1221

double NPEffectiveGIMR::CLL_1221

protected

Definition at line 1479 of file NPEffectiveGIMR.h.

CLL_1331

double NPEffectiveGIMR::CLL_1331

protected

Definition at line 1480 of file NPEffectiveGIMR.h.

CLL_2112

double NPEffectiveGIMR::CLL_2112

protected

Definition at line 1479 of file NPEffectiveGIMR.h.

CLL_2211

double NPEffectiveGIMR::CLL_2211

protected

Definition at line 1479 of file NPEffectiveGIMR.h.

CLL_3113

double NPEffectiveGIMR::CLL_3113

protected

Definition at line 1480 of file NPEffectiveGIMR.h.

CLL_3311

double NPEffectiveGIMR::CLL_3311

protected

Definition at line 1480 of file NPEffectiveGIMR.h.

CLQ1_1111

double NPEffectiveGIMR::CLQ1_1111

protected

Definition at line 1481 of file NPEffectiveGIMR.h.

CLQ1_1122

double NPEffectiveGIMR::CLQ1_1122

protected

Definition at line 1482 of file NPEffectiveGIMR.h.

CLQ1_1123

double NPEffectiveGIMR::CLQ1_1123

protected

Definition at line 1484 of file NPEffectiveGIMR.h.

CLQ1_1132

double NPEffectiveGIMR::CLQ1_1132

protected

Definition at line 1485 of file NPEffectiveGIMR.h.

CLQ1_1133

double NPEffectiveGIMR::CLQ1_1133

protected

Definition at line 1483 of file NPEffectiveGIMR.h.

CLQ1_1221

double NPEffectiveGIMR::CLQ1_1221

protected

Definition at line 1482 of file NPEffectiveGIMR.h.

CLQ1_1331

double NPEffectiveGIMR::CLQ1_1331

protected

Definition at line 1483 of file NPEffectiveGIMR.h.

CLQ1_2112

double NPEffectiveGIMR::CLQ1_2112

protected

Definition at line 1482 of file NPEffectiveGIMR.h.

CLQ1_2211

double NPEffectiveGIMR::CLQ1_2211

protected

Definition at line 1482 of file NPEffectiveGIMR.h.

CLQ1_2223

double NPEffectiveGIMR::CLQ1_2223

protected

Definition at line 1484 of file NPEffectiveGIMR.h.

CLQ1_2232

double NPEffectiveGIMR::CLQ1_2232

protected

Definition at line 1485 of file NPEffectiveGIMR.h.

CLQ1_3113

double NPEffectiveGIMR::CLQ1_3113

protected

Definition at line 1483 of file NPEffectiveGIMR.h.

CLQ1_3311

double NPEffectiveGIMR::CLQ1_3311

protected

Definition at line 1483 of file NPEffectiveGIMR.h.

CLQ1_3323

double NPEffectiveGIMR::CLQ1_3323

protected

Definition at line 1484 of file NPEffectiveGIMR.h.

CLQ1_3332

double NPEffectiveGIMR::CLQ1_3332

protected

Definition at line 1485 of file NPEffectiveGIMR.h.

CLQ3_1111

double NPEffectiveGIMR::CLQ3_1111

protected

Definition at line 1486 of file NPEffectiveGIMR.h.

CLQ3_1122

double NPEffectiveGIMR::CLQ3_1122

protected

Definition at line 1487 of file NPEffectiveGIMR.h.

CLQ3_1123

double NPEffectiveGIMR::CLQ3_1123

protected

Definition at line 1489 of file NPEffectiveGIMR.h.

CLQ3_1132

double NPEffectiveGIMR::CLQ3_1132

protected

Definition at line 1490 of file NPEffectiveGIMR.h.

CLQ3_1133

double NPEffectiveGIMR::CLQ3_1133

protected

Definition at line 1488 of file NPEffectiveGIMR.h.

CLQ3_1221

double NPEffectiveGIMR::CLQ3_1221

protected

Definition at line 1487 of file NPEffectiveGIMR.h.

CLQ3_1331

double NPEffectiveGIMR::CLQ3_1331

protected

Definition at line 1488 of file NPEffectiveGIMR.h.

CLQ3_2112

double NPEffectiveGIMR::CLQ3_2112

protected

Definition at line 1487 of file NPEffectiveGIMR.h.

CLQ3_2211

double NPEffectiveGIMR::CLQ3_2211

protected

Definition at line 1487 of file NPEffectiveGIMR.h.

CLQ3_2223

double NPEffectiveGIMR::CLQ3_2223

protected

Definition at line 1489 of file NPEffectiveGIMR.h.

CLQ3_2232

double NPEffectiveGIMR::CLQ3_2232

protected

Definition at line 1490 of file NPEffectiveGIMR.h.

CLQ3_3113

double NPEffectiveGIMR::CLQ3_3113

protected

Definition at line 1488 of file NPEffectiveGIMR.h.

CLQ3_3311

double NPEffectiveGIMR::CLQ3_3311

protected

Definition at line 1488 of file NPEffectiveGIMR.h.

CLQ3_3323

double NPEffectiveGIMR::CLQ3_3323

protected

Definition at line 1489 of file NPEffectiveGIMR.h.

CLQ3_3332

double NPEffectiveGIMR::CLQ3_3332

protected

Definition at line 1490 of file NPEffectiveGIMR.h.

CLu_1111

double NPEffectiveGIMR::CLu_1111

protected

Definition at line 1505 of file NPEffectiveGIMR.h.

CLu_1122

double NPEffectiveGIMR::CLu_1122

protected

Definition at line 1506 of file NPEffectiveGIMR.h.

CLu_1133

double NPEffectiveGIMR::CLu_1133

protected

Definition at line 1507 of file NPEffectiveGIMR.h.

CLu_2211

double NPEffectiveGIMR::CLu_2211

protected

Definition at line 1506 of file NPEffectiveGIMR.h.

CLu_3311

double NPEffectiveGIMR::CLu_3311

protected

Definition at line 1507 of file NPEffectiveGIMR.h.

CQe_1111

double NPEffectiveGIMR::CQe_1111

protected

Definition at line 1513 of file NPEffectiveGIMR.h.

CQe_1122

double NPEffectiveGIMR::CQe_1122

protected

Definition at line 1514 of file NPEffectiveGIMR.h.

CQe_1133

double NPEffectiveGIMR::CQe_1133

protected

Definition at line 1515 of file NPEffectiveGIMR.h.

CQe_2211

double NPEffectiveGIMR::CQe_2211

protected

Definition at line 1514 of file NPEffectiveGIMR.h.

CQe_2311

double NPEffectiveGIMR::CQe_2311

protected

Definition at line 1516 of file NPEffectiveGIMR.h.

CQe_2322

double NPEffectiveGIMR::CQe_2322

protected

Definition at line 1516 of file NPEffectiveGIMR.h.

CQe_2333

double NPEffectiveGIMR::CQe_2333

protected

Definition at line 1516 of file NPEffectiveGIMR.h.

CQe_3211

double NPEffectiveGIMR::CQe_3211

protected

Definition at line 1517 of file NPEffectiveGIMR.h.

CQe_3222

double NPEffectiveGIMR::CQe_3222

protected

Definition at line 1517 of file NPEffectiveGIMR.h.

CQe_3233

double NPEffectiveGIMR::CQe_3233

protected

Definition at line 1517 of file NPEffectiveGIMR.h.

CQe_3311

double NPEffectiveGIMR::CQe_3311

protected

Definition at line 1515 of file NPEffectiveGIMR.h.

CuB_11i

double NPEffectiveGIMR::CuB_11i

protected

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

Definition at line 1472 of file NPEffectiveGIMR.h.

CuB_11r

double NPEffectiveGIMR::CuB_11r

protected

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

Definition at line 1466 of file NPEffectiveGIMR.h.

CuB_12i

double NPEffectiveGIMR::CuB_12i

protected

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

Definition at line 1473 of file NPEffectiveGIMR.h.

CuB_12r

double NPEffectiveGIMR::CuB_12r

protected

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

Definition at line 1467 of file NPEffectiveGIMR.h.

CuB_13i

double NPEffectiveGIMR::CuB_13i

protected

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

Definition at line 1474 of file NPEffectiveGIMR.h.

CuB_13r

double NPEffectiveGIMR::CuB_13r

protected

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

Definition at line 1468 of file NPEffectiveGIMR.h.

CuB_22i

double NPEffectiveGIMR::CuB_22i

protected

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

Definition at line 1475 of file NPEffectiveGIMR.h.

CuB_22r

double NPEffectiveGIMR::CuB_22r

protected

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

Definition at line 1469 of file NPEffectiveGIMR.h.

CuB_23i

double NPEffectiveGIMR::CuB_23i

protected

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

Definition at line 1476 of file NPEffectiveGIMR.h.

CuB_23r

double NPEffectiveGIMR::CuB_23r

protected

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

Definition at line 1470 of file NPEffectiveGIMR.h.

CuB_33i

double NPEffectiveGIMR::CuB_33i

protected

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

Definition at line 1477 of file NPEffectiveGIMR.h.

CuB_33r

double NPEffectiveGIMR::CuB_33r

protected

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

Definition at line 1471 of file NPEffectiveGIMR.h.

CuG_11i

double NPEffectiveGIMR::CuG_11i

protected

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

Definition at line 1448 of file NPEffectiveGIMR.h.

CuG_11r

double NPEffectiveGIMR::CuG_11r

protected

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

Definition at line 1442 of file NPEffectiveGIMR.h.

CuG_12i

double NPEffectiveGIMR::CuG_12i

protected

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

Definition at line 1449 of file NPEffectiveGIMR.h.

CuG_12r

double NPEffectiveGIMR::CuG_12r

protected

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

Definition at line 1443 of file NPEffectiveGIMR.h.

CuG_13i

double NPEffectiveGIMR::CuG_13i

protected

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

Definition at line 1450 of file NPEffectiveGIMR.h.

CuG_13r

double NPEffectiveGIMR::CuG_13r

protected

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

Definition at line 1444 of file NPEffectiveGIMR.h.

CuG_22i

double NPEffectiveGIMR::CuG_22i

protected

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

Definition at line 1451 of file NPEffectiveGIMR.h.

CuG_22r

double NPEffectiveGIMR::CuG_22r

protected

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

Definition at line 1445 of file NPEffectiveGIMR.h.

CuG_23i

double NPEffectiveGIMR::CuG_23i

protected

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

Definition at line 1452 of file NPEffectiveGIMR.h.

CuG_23r

double NPEffectiveGIMR::CuG_23r

protected

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

Definition at line 1446 of file NPEffectiveGIMR.h.

CuG_33i

double NPEffectiveGIMR::CuG_33i

protected

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

Definition at line 1453 of file NPEffectiveGIMR.h.

CuG_33r

double NPEffectiveGIMR::CuG_33r

protected

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

Definition at line 1447 of file NPEffectiveGIMR.h.

CuH_11i

double NPEffectiveGIMR::CuH_11i

protected

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

Definition at line 1424 of file NPEffectiveGIMR.h.

CuH_11r

double NPEffectiveGIMR::CuH_11r

protected

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

Definition at line 1418 of file NPEffectiveGIMR.h.

CuH_12i

double NPEffectiveGIMR::CuH_12i

protected

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

Definition at line 1425 of file NPEffectiveGIMR.h.

CuH_12r

double NPEffectiveGIMR::CuH_12r

protected

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

Definition at line 1419 of file NPEffectiveGIMR.h.

CuH_13i

double NPEffectiveGIMR::CuH_13i

protected

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

Definition at line 1426 of file NPEffectiveGIMR.h.

CuH_13r

double NPEffectiveGIMR::CuH_13r

protected

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

Definition at line 1420 of file NPEffectiveGIMR.h.

CuH_22i

double NPEffectiveGIMR::CuH_22i

protected

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

Definition at line 1427 of file NPEffectiveGIMR.h.

CuH_22r

double NPEffectiveGIMR::CuH_22r

protected

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

Definition at line 1421 of file NPEffectiveGIMR.h.

CuH_23i

double NPEffectiveGIMR::CuH_23i

protected

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

Definition at line 1428 of file NPEffectiveGIMR.h.

CuH_23r

double NPEffectiveGIMR::CuH_23r

protected

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

Definition at line 1422 of file NPEffectiveGIMR.h.

CuH_33i

double NPEffectiveGIMR::CuH_33i

protected

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

Definition at line 1429 of file NPEffectiveGIMR.h.

CuH_33r

double NPEffectiveGIMR::CuH_33r

protected

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

Definition at line 1423 of file NPEffectiveGIMR.h.

CuW_11i

double NPEffectiveGIMR::CuW_11i

protected

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

Definition at line 1460 of file NPEffectiveGIMR.h.

CuW_11r

double NPEffectiveGIMR::CuW_11r

protected

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

Definition at line 1454 of file NPEffectiveGIMR.h.

CuW_12i

double NPEffectiveGIMR::CuW_12i

protected

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

Definition at line 1461 of file NPEffectiveGIMR.h.

CuW_12r

double NPEffectiveGIMR::CuW_12r

protected

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

Definition at line 1455 of file NPEffectiveGIMR.h.

CuW_13i

double NPEffectiveGIMR::CuW_13i

protected

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

Definition at line 1462 of file NPEffectiveGIMR.h.

CuW_13r

double NPEffectiveGIMR::CuW_13r

protected

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

Definition at line 1456 of file NPEffectiveGIMR.h.

CuW_22i

double NPEffectiveGIMR::CuW_22i

protected

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

Definition at line 1463 of file NPEffectiveGIMR.h.

CuW_22r

double NPEffectiveGIMR::CuW_22r

protected

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

Definition at line 1457 of file NPEffectiveGIMR.h.

CuW_23i

double NPEffectiveGIMR::CuW_23i

protected

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

Definition at line 1464 of file NPEffectiveGIMR.h.

CuW_23r

double NPEffectiveGIMR::CuW_23r

protected

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

Definition at line 1458 of file NPEffectiveGIMR.h.

CuW_33i

double NPEffectiveGIMR::CuW_33i

protected

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

Definition at line 1465 of file NPEffectiveGIMR.h.

CuW_33r

double NPEffectiveGIMR::CuW_33r

protected

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

Definition at line 1459 of file NPEffectiveGIMR.h.

CW

double NPEffectiveGIMR::CW

protected

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

Definition at line 1323 of file NPEffectiveGIMR.h.

cW2_tree

double NPEffectiveGIMR::cW2_tree

protected

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

Definition at line 1610 of file NPEffectiveGIMR.h.

cW_tree

double NPEffectiveGIMR::cW_tree

protected

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

Definition at line 1608 of file NPEffectiveGIMR.h.

delta_AA

double NPEffectiveGIMR::delta_AA

protected

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

Definition at line 1613 of file NPEffectiveGIMR.h.

delta_AZ

double NPEffectiveGIMR::delta_AZ

protected

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

Definition at line 1614 of file NPEffectiveGIMR.h.

delta_h

double NPEffectiveGIMR::delta_h

protected

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

Definition at line 1615 of file NPEffectiveGIMR.h.

delta_ZZ

double NPEffectiveGIMR::delta_ZZ

protected

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

Definition at line 1612 of file NPEffectiveGIMR.h.

ettH2_Hgg

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 1600 of file NPEffectiveGIMR.h.

ettH2_Htt

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 1599 of file NPEffectiveGIMR.h.

ettH78_Hgg

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 1602 of file NPEffectiveGIMR.h.

ettH78_Htt

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 1601 of file NPEffectiveGIMR.h.

eVBF2_HAA

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 1525 of file NPEffectiveGIMR.h.

eVBF2_Hgg

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 1529 of file NPEffectiveGIMR.h.

eVBF2_HWud

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 1534 of file NPEffectiveGIMR.h.

eVBF2_HWW1

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 1526 of file NPEffectiveGIMR.h.

eVBF2_HWW2

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 1527 of file NPEffectiveGIMR.h.

eVBF2_HWW3

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 1528 of file NPEffectiveGIMR.h.

eVBF2_HZA1

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 1523 of file NPEffectiveGIMR.h.

eVBF2_HZA2

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 1524 of file NPEffectiveGIMR.h.

eVBF2_HZdL

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 1532 of file NPEffectiveGIMR.h.

eVBF2_HZdR

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 1533 of file NPEffectiveGIMR.h.

eVBF2_HZuL

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 1530 of file NPEffectiveGIMR.h.

eVBF2_HZuR

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 1531 of file NPEffectiveGIMR.h.

eVBF2_HZZ1

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 1520 of file NPEffectiveGIMR.h.

eVBF2_HZZ2

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 1521 of file NPEffectiveGIMR.h.

eVBF2_HZZ3

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 1522 of file NPEffectiveGIMR.h.

eVBF2_Wud

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 1539 of file NPEffectiveGIMR.h.

eVBF2_ZdL

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 1537 of file NPEffectiveGIMR.h.

eVBF2_ZdR

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 1538 of file NPEffectiveGIMR.h.

eVBF2_ZuL

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 1535 of file NPEffectiveGIMR.h.

eVBF2_ZuR

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 1536 of file NPEffectiveGIMR.h.

eVBF78_HAA

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 1545 of file NPEffectiveGIMR.h.

eVBF78_Hgg

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 1549 of file NPEffectiveGIMR.h.

eVBF78_HWud

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 1554 of file NPEffectiveGIMR.h.

eVBF78_HWW1

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 1546 of file NPEffectiveGIMR.h.

eVBF78_HWW2

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 1547 of file NPEffectiveGIMR.h.

eVBF78_HWW3

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 1548 of file NPEffectiveGIMR.h.

eVBF78_HZA1

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 1543 of file NPEffectiveGIMR.h.

eVBF78_HZA2

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 1544 of file NPEffectiveGIMR.h.

eVBF78_HZdL

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 1552 of file NPEffectiveGIMR.h.

eVBF78_HZdR

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 1553 of file NPEffectiveGIMR.h.

eVBF78_HZuL

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 1550 of file NPEffectiveGIMR.h.

eVBF78_HZuR

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 1551 of file NPEffectiveGIMR.h.

eVBF78_HZZ1

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 1540 of file NPEffectiveGIMR.h.

eVBF78_HZZ2

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 1541 of file NPEffectiveGIMR.h.

eVBF78_HZZ3

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 1542 of file NPEffectiveGIMR.h.

eVBF78_Wud

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 1559 of file NPEffectiveGIMR.h.

eVBF78_ZdL

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 1557 of file NPEffectiveGIMR.h.

eVBF78_ZdR

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 1558 of file NPEffectiveGIMR.h.

eVBF78_ZuL

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 1555 of file NPEffectiveGIMR.h.

eVBF78_ZuR

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 1556 of file NPEffectiveGIMR.h.

eWH2_HWud

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 1564 of file NPEffectiveGIMR.h.

eWH2_HWW1

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 1561 of file NPEffectiveGIMR.h.

eWH2_HWW2

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 1562 of file NPEffectiveGIMR.h.

eWH2_HWW3

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 1563 of file NPEffectiveGIMR.h.

eWH2_Wud

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 1565 of file NPEffectiveGIMR.h.

eWH78_HWud

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 1569 of file NPEffectiveGIMR.h.

eWH78_HWW1

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 1566 of file NPEffectiveGIMR.h.

eWH78_HWW2

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 1567 of file NPEffectiveGIMR.h.

eWH78_HWW3

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 1568 of file NPEffectiveGIMR.h.

eWH78_Wud

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 1570 of file NPEffectiveGIMR.h.

eZH2_HZA1

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 1575 of file NPEffectiveGIMR.h.

eZH2_HZA2

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 1576 of file NPEffectiveGIMR.h.

eZH2_HZdL

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 1579 of file NPEffectiveGIMR.h.

eZH2_HZdR

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 1580 of file NPEffectiveGIMR.h.

eZH2_HZuL

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 1577 of file NPEffectiveGIMR.h.

eZH2_HZuR

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 1578 of file NPEffectiveGIMR.h.

eZH2_HZZ1

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 1572 of file NPEffectiveGIMR.h.

eZH2_HZZ2

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 1573 of file NPEffectiveGIMR.h.

eZH2_HZZ3

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 1574 of file NPEffectiveGIMR.h.

eZH2_ZdL

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 1583 of file NPEffectiveGIMR.h.

eZH2_ZdR

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 1584 of file NPEffectiveGIMR.h.

eZH2_ZuL

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 1581 of file NPEffectiveGIMR.h.

eZH2_ZuR

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 1582 of file NPEffectiveGIMR.h.

eZH78_HZA1

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 1588 of file NPEffectiveGIMR.h.

eZH78_HZA2

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 1589 of file NPEffectiveGIMR.h.

eZH78_HZdL

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 1592 of file NPEffectiveGIMR.h.

eZH78_HZdR

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 1593 of file NPEffectiveGIMR.h.

eZH78_HZuL

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 1590 of file NPEffectiveGIMR.h.

eZH78_HZuR

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 1591 of file NPEffectiveGIMR.h.

eZH78_HZZ1

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 1585 of file NPEffectiveGIMR.h.

eZH78_HZZ2

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 1586 of file NPEffectiveGIMR.h.

eZH78_HZZ3

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 1587 of file NPEffectiveGIMR.h.

eZH78_ZdL

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 1596 of file NPEffectiveGIMR.h.

eZH78_ZdR

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 1597 of file NPEffectiveGIMR.h.

eZH78_ZuL

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 1594 of file NPEffectiveGIMR.h.

eZH78_ZuR

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 1595 of file NPEffectiveGIMR.h.

FlagLeptonUniversal

const bool NPEffectiveGIMR::FlagLeptonUniversal

private

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

Definition at line 1685 of file NPEffectiveGIMR.h.

FlagMwInput

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 1678 of file NPEffectiveGIMR.h.

FlagQuadraticTerms

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 1679 of file NPEffectiveGIMR.h.

FlagQuarkUniversal

const bool NPEffectiveGIMR::FlagQuarkUniversal

private

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

Definition at line 1691 of file NPEffectiveGIMR.h.

Lambda_NP

double NPEffectiveGIMR::Lambda_NP

protected

The new physics scale [GeV].

Definition at line 1518 of file NPEffectiveGIMR.h.

LambdaNP2

double NPEffectiveGIMR::LambdaNP2

protected

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

Definition at line 1606 of file NPEffectiveGIMR.h.

MwInput

double NPEffectiveGIMR::MwInput

protected

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

Definition at line 1604 of file NPEffectiveGIMR.h.

myLEP2GIMR

const LEP2GIMR NPEffectiveGIMR::myLEP2GIMR

protected

Definition at line 1673 of file NPEffectiveGIMR.h.

NNPEffectiveGIMRVars

const int NPEffectiveGIMR::NNPEffectiveGIMRVars = 331

static

The number of the model parameters in NPEffectiveGIMR.

　

Definition at line 616 of file NPEffectiveGIMR.h.

NNPEffectiveGIMRVars_LFU_QFU

const int NPEffectiveGIMR::NNPEffectiveGIMRVars_LFU_QFU = 121

static

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

　

Definition at line 628 of file NPEffectiveGIMR.h.

NPEffectiveGIMRVars

const std::string NPEffectiveGIMR::NPEffectiveGIMRVars

static

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

Definition at line 622 of file NPEffectiveGIMR.h.

NPEffectiveGIMRVars_LFU_QFU

const std::string NPEffectiveGIMR::NPEffectiveGIMRVars_LFU_QFU

static

Initial value:

= {"CG", "CW", "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",
    "CuG_r", "CuG_i", "CuW_r", "CuW_i", "CuB_r", "CuB_i",
    "CLL", "CLQ1", "CLQ3",
    "Cee", "Ceu", "Ced", "CLe", "CLu", "CLd", "CQe","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 634 of file NPEffectiveGIMR.h.

sW2_tree

double NPEffectiveGIMR::sW2_tree

protected

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

Definition at line 1611 of file NPEffectiveGIMR.h.

sW_tree

double NPEffectiveGIMR::sW_tree

protected

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

Definition at line 1609 of file NPEffectiveGIMR.h.

v2_over_LambdaNP2

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 1607 of file NPEffectiveGIMR.h.

---

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

• NPEffectiveGIMR.h
• NPEffectiveGIMR.cpp