#include <NPSMEFTd6U3.h>

Inheritance diagram for NPSMEFTd6U3:

Detailed Description

Definition at line 18 of file NPSMEFTd6U3.h.

Public Member Functions
	NPSMEFTd6U3 ()

virtual bool	PostUpdate ()
	The post-update method for NPSMEFTd6General. More...

Public Member Functions inherited from NPSMEFTd6General
virtual const double	A_f (const Particle f) const
	The left-right asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $\mathcal{A}_f$. More...

virtual const double	AFB (const Particle f) const
	The forward-backward asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $A^f_{FB}$. More...

virtual const double	alphaMz () const
	The electromagnetic coupling at the $Z$-mass scale. More...

virtual const double	aPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	the angular parameter $a$ from $\mu_{e^+e^- \to ZH}$ (arXiv:1708.09079 [hep-ph]). More...

virtual const double	AuxObs_NP1 () const
	Auxiliary observable AuxObs_NP1 (See code for details.) More...

virtual const double	AuxObs_NP10 () const
	Auxiliary observable AuxObs_NP10 (See code for details.) More...

virtual const double	AuxObs_NP11 () const
	Auxiliary observable AuxObs_NP11 (See code for details.) More...

virtual const double	AuxObs_NP12 () const
	Auxiliary observable AuxObs_NP12 (See code for details.) More...

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

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

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

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

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

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

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

virtual const double	AuxObs_NP2 () const
	Auxiliary observable AuxObs_NP2 (See code for details.) More...

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

virtual const double	AuxObs_NP21 () const
	Auxiliary observable AuxObs_NP21 (See code for details.) More...

virtual const double	AuxObs_NP22 () const
	Auxiliary observable AuxObs_NP22 (See code for details.) More...

virtual const double	AuxObs_NP23 () const
	Auxiliary observable AuxObs_NP23. More...

virtual const double	AuxObs_NP24 () const
	Auxiliary observable AuxObs_NP24. More...

virtual const double	AuxObs_NP25 () const
	Auxiliary observable AuxObs_NP25. More...

virtual const double	AuxObs_NP26 () const
	Auxiliary observable AuxObs_NP26. More...

virtual const double	AuxObs_NP27 () const
	Auxiliary observable AuxObs_NP27. More...

virtual const double	AuxObs_NP28 () const
	Auxiliary observable AuxObs_NP28. More...

virtual const double	AuxObs_NP29 () const
	Auxiliary observable AuxObs_NP29. More...

virtual const double	AuxObs_NP3 () const
	Auxiliary observable AuxObs_NP3 (See code for details.) More...

virtual const double	AuxObs_NP30 () const
	Auxiliary observable AuxObs_NP30. More...

virtual const double	AuxObs_NP4 () const
	Auxiliary observable AuxObs_NP4 (See code for details.) More...

virtual const double	AuxObs_NP5 () const
	Auxiliary observable AuxObs_NP5 (See code for details.) More...

virtual const double	AuxObs_NP6 () const
	Auxiliary observable AuxObs_NP6 (See code for details.) More...

virtual const double	AuxObs_NP7 () const
	Auxiliary observable AuxObs_NP7 (See code for details.) More...

virtual const double	AuxObs_NP8 () const
	Auxiliary observable AuxObs_NP8 (See code for details.) More...

virtual const double	AuxObs_NP9 () const
	Auxiliary observable AuxObs_NP9 (See code for details.) More...

virtual const double	bPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	the angular parameter $b$ from $\mu_{e^+e^- \to ZH}$ (arXiv:1708.09079 [hep-ph]). More...

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

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

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

virtual const double	BrH2d2dRatio () const
	The ratio of the Br $(H\to 2d2d)$ in the current model and in the Standard Model. More...

virtual const double	BrH2e2muRatio () const
	The ratio of the Br $(H\to 2e 2\mu)$ in the current model and in the Standard Model. More...

virtual const double	BrH2e2vRatio () const
	The ratio of the Br $(H\to 2e2v)$ in the current model and in the Standard Model. More...

virtual const double	BrH2evRatio () const
	The ratio of the Br $(H\to 2ev)$ in the current model and in the Standard Model. More...

virtual const double	BrH2L2dRatio () const
	The ratio of the Br $(H\to 2L2d)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

virtual const double	BrH2L2LRatio () const
	The ratio of the Br $(H\to 2L2L')$ ( $L,L'=e,\mu,\tau$) in the current model and in the Standard Model. More...

virtual const double	BrH2L2uRatio () const
	The ratio of the Br $(H\to 2L2u)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

virtual const double	BrH2L2v2Ratio () const
	The ratio of the Br $(H\to 2L2v)$ ( $L=e,\mu$) in the current model and in the Standard Model. More...

virtual const double	BrH2L2vRatio () const
	The ratio of the Br $(H\to 2L2v)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

virtual const double	BrH2l2vRatio () const
	The ratio of the Br $(H\to 2l2v)$ ( $l=e,\mu$) in the current model and in the Standard Model. More...

virtual const double	BrH2Lv2Ratio () const
	The ratio of the Br $(H\to 2Lv)$ ( $L=e,\mu$) in the current model and in the Standard Model. More...

virtual const double	BrH2LvRatio () const
	The ratio of the Br $(H\to 2Lv)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

virtual const double	BrH2mu2vRatio () const
	The ratio of the Br $(H\to 2\mu 2v)$ in the current model and in the Standard Model. More...

virtual const double	BrH2muvRatio () const
	The ratio of the Br $(H\to 2ev)$ in the current model and in the Standard Model. More...

virtual const double	BrH2u2dRatio () const
	The ratio of the Br $(H\to 2u2d)$ in the current model and in the Standard Model. More...

virtual const double	BrH2u2uRatio () const
	The ratio of the Br $(H\to 2u2u)$ in the current model and in the Standard Model. More...

virtual const double	BrH2udRatio () const
	The ratio of the Br $(H\to 2ud)$ in the current model and in the Standard Model. More...

virtual const double	BrH2v2dRatio () const
	The ratio of the Br $(H\to 2v2d)$ in the current model and in the Standard Model. More...

virtual const double	BrH2v2uRatio () const
	The ratio of the Br $(H\to 2v2u)$ in the current model and in the Standard Model. More...

virtual const double	BrH2v2vRatio () const
	The ratio of the Br $(H\to 2v2v)$ in the current model and in the Standard Model. More...

virtual const double	BrH4dRatio () const
	The ratio of the Br $(H\to 4d)$ in the current model and in the Standard Model. More...

virtual const double	BrH4eRatio () const
	The ratio of the Br $(H\to 4e)$ in the current model and in the Standard Model. More...

virtual const double	BrH4fCCRatio () const
	The ratio of the Br $(H\to 4f, CC)$ in the current model and in the Standard Model. More...

virtual const double	BrH4fNCRatio () const
	The ratio of the Br $(H\to 4f, NC)$ in the current model and in the Standard Model. More...

virtual const double	BrH4fRatio () const
	The ratio of the Br $(H\to 4f)$ in the current model and in the Standard Model. More...

virtual const double	BrH4L2Ratio () const
	The ratio of the Br $(H\to 4L)$ ( $L=e,\mu$) in the current model and in the Standard Model. More...

virtual const double	BrH4LRatio () const
	The ratio of the Br $(H\to 4L)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

virtual const double	BrH4lRatio () const
	The ratio of the Br $(H\to 4l)$ ( $l=e,\mu$) in the current model and in the Standard Model. More...

virtual const double	BrH4muRatio () const
	The ratio of the Br $(H\to 4\mu)$ in the current model and in the Standard Model. More...

virtual const double	BrH4uRatio () const
	The ratio of the Br $(H\to 4u)$ in the current model and in the Standard Model. More...

virtual const double	BrH4vRatio () const
	The ratio of the Br $(H\to 4v)$ in the current model and in the Standard Model. More...

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

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

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

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

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

virtual const double	BrHll_vvorjjRatio () const
	The ratio of the Br $(H\to l l \nu\nu, l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. More...

virtual const double	BrHlv_lvorjjRatio () const
	The ratio of the Br $(H\to l \nu l \nu, l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. More...

virtual const double	BrHlvjjRatio () const
	The ratio of the Br $(H\to l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. More...

virtual const double	BrHLvudRatio () const
	The ratio of the Br $(H\to Lvud)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

virtual const double	BrHLvvLRatio () const
	The ratio of the Br $(H\to LvvL)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

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

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

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

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

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

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

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

virtual const double	BrHWffRatio () const
	The ratio of the Br $(H\to W f f)$, with $f$ any fermion, in the current model and in the Standard Model. More...

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

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

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

virtual const double	BrHWW4fRatio () const
	The ratio of the Br $(H\to WW^*\to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. More...

virtual const double	BrHWW4jRatio () const
	The ratio of the Br $(H\to WW^*\to 4j)$ in the current model and in the Standard Model. More...

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

virtual const double	BrHZddRatio () const
	The ratio of the Br $(H\to Z d d)$ ( $d=d,s,b $) in the current model and in the Standard Model. More...

virtual const double	BrHZffRatio () const
	The ratio of the Br $(H\to Zff)$, with $f$ any fermion, in the current model and in the Standard Model. More...

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

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

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

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

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

virtual const double	BrHZuuRatio () const
	The ratio of the Br $(H\to Z u u)$ ( $u=u,c $) in the current model and in the Standard Model. More...

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

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

virtual const double	BrHZZ4dRatio () const
	The ratio of the Br $(H\to ZZ* \to 4 d)$ ( $d=d,s,b $) in the current model and in the Standard Model. More...

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

virtual const double	BrHZZ4fRatio () const
	The ratio of the Br $(H\to ZZ* \to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. More...

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

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

virtual const double	BrHZZ4uRatio () const
	The ratio of the Br $(H\to ZZ* \to 4 u)$ ( $u=u,c $) in the current model and in the Standard Model. More...

virtual const double	BrHZZ4vRatio () const
	The ratio of the Br $(H\to ZZ* \to 4\nu)$ in the current model and in the Standard Model. More...

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

virtual const double	BrW (const Particle fi, const Particle fj) const
	The branching ratio of the $W$ boson decaying into a SM fermion pair, $Br(W\to f_i f_j)$. More...

virtual const double	cbW_TWG (const double mu) const

const double	CeeLL_bottom (const double mu) const

const double	CeeLL_charm (const double mu) const

const double	CeeLL_down (const double mu) const

const double	CeeLL_e (const double mu) const

const double	CeeLL_mu (const double mu) const

const double	CeeLL_strange (const double mu) const

const double	CeeLL_tau (const double mu) const

const double	CeeLL_top (const double mu) const

const double	CeeLL_up (const double mu) const

const double	CeeLR_bottom (const double mu) const

const double	CeeLR_charm (const double mu) const

const double	CeeLR_down (const double mu) const

const double	CeeLR_e (const double mu) const

const double	CeeLR_mu (const double mu) const

const double	CeeLR_strange (const double mu) const

const double	CeeLR_tau (const double mu) const

const double	CeeLR_top (const double mu) const

const double	CeeLR_up (const double mu) const

const double	CeeRL_bottom (const double mu) const

const double	CeeRL_charm (const double mu) const

const double	CeeRL_down (const double mu) const

const double	CeeRL_e (const double mu) const

const double	CeeRL_mu (const double mu) const

const double	CeeRL_strange (const double mu) const

const double	CeeRL_tau (const double mu) const

const double	CeeRL_top (const double mu) const

const double	CeeRL_up (const double mu) const

const double	CeeRR_bottom (const double mu) const

const double	CeeRR_charm (const double mu) const

const double	CeeRR_down (const double mu) const

const double	CeeRR_e (const double mu) const

const double	CeeRR_mu (const double mu) const

const double	CeeRR_strange (const double mu) const

const double	CeeRR_tau (const double mu) const

const double	CeeRR_top (const double mu) const

const double	CeeRR_up (const double mu) const

virtual const double	CEWHd11 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hd})_{11}$. More...

virtual const double	CEWHd22 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hd})_{22}$. More...

virtual const double	CEWHd33 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hd})_{33}$. More...

virtual const double	CEWHe11 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{He})_{11}$. More...

virtual const double	CEWHe22 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{He})_{22}$. More...

virtual const double	CEWHe33 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{He})_{33}$. More...

virtual const double	CEWHL111 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(1)})_{11}$. More...

virtual const double	CEWHL122 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(1)})_{22}$. More...

virtual const double	CEWHL133 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(1)})_{33}$. More...

virtual const double	CEWHL311 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(3)})_{11}$. More...

virtual const double	CEWHL322 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(3)})_{22}$. More...

virtual const double	CEWHL333 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HL}^{(3)})_{33}$. More...

virtual const double	CEWHQ111 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(1)})_{11}$. More...

virtual const double	CEWHQ122 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(1)})_{22}$. More...

virtual const double	CEWHQ133 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(1)})_{33}$. More...

virtual const double	CEWHQ311 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(3)})_{11}$. More...

virtual const double	CEWHQ322 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(3)})_{22}$. More...

virtual const double	CEWHQ333 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(3)})_{33}$. More...

virtual const double	CEWHQd33 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{HQ}^{(d)})_{33}$. More...

virtual const double	CEWHu11 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hu})_{11}$. More...

virtual const double	CEWHu22 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hu})_{22}$. More...

virtual const double	CEWHu33 () const
	Combination of coefficients of the Warsaw basis constrained by EWPO $(\hat{C}_{Hu})_{33}$. More...

virtual const double	cgaga_HB (const double mu) const
	The Higgs-basis coupling $c_{\gamma\gamma}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	cgg_HB (const double mu) const
	The Higgs-basis coupling $c_{gg}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	cggEff_HB (const double mu) const
	The effective Higgs-basis coupling $c_{gg}^{Eff}$. (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	cHb_TWG (const double mu) const

virtual const double	cHQ3_TWG (const double mu) const

virtual const double	cHQm_TWG (const double mu) const

virtual const double	cHQp_TWG (const double mu) const

virtual const double	cHt_TWG (const double mu) const

virtual const double	cHtb_TWG (const double mu) const

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

virtual const double	cQd1_TWG (const double mu) const

virtual const double	cQd8_TWG (const double mu) const

virtual const double	cQe_TWG (const double mu) const

virtual const double	cQl3_TWG (const double mu) const

virtual const double	cQlM_TWG (const double mu) const

virtual const double	cQlP_TWG (const double mu) const

virtual const double	cQq11_TWG (const double mu) const

virtual const double	cQq18_TWG (const double mu) const

virtual const double	cQQ1_TWG (const double mu) const

virtual const double	cQq31_TWG (const double mu) const

virtual const double	cQq38_TWG (const double mu) const

virtual const double	cQQ8_TWG (const double mu) const

virtual const double	cQt1_TWG (const double mu) const

virtual const double	cQt8_TWG (const double mu) const

virtual const double	cQu1_TWG (const double mu) const

virtual const double	cQu8_TWG (const double mu) const

virtual const double	ctd1_TWG (const double mu) const

virtual const double	ctd8_TWG (const double mu) const

virtual const double	cte_TWG (const double mu) const

virtual const double	ctG_TWG (const double mu) const

virtual const double	ctH_TWG (const double mu) const

virtual const double	ctl_TWG (const double mu) const

virtual const double	ctlS_TWG (const double mu) const

virtual const double	ctlT_TWG (const double mu) const

virtual const double	ctq1_TWG (const double mu) const

virtual const double	ctq8_TWG (const double mu) const

virtual const double	ctt1_TWG (const double mu) const

virtual const double	ctu1_TWG (const double mu) const

virtual const double	ctu8_TWG (const double mu) const

virtual const double	ctW_TWG (const double mu) const

virtual const double	ctZ_TWG (const double mu) const

virtual const double	cZBox_HB (const double mu) const
	The Higgs-basis coupling $c_{z\Box}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	cZga_HB (const double mu) const
	The Higgs-basis coupling $c_{z\gamma}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	cZZ_HB (const double mu) const
	The Higgs-basis coupling $c_{zz}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	del_A_mu (const double mu) const
	Correction to photon WF. More...

virtual const double	del_e_mu (const double mu) const
	Correction to electric charge. More...

virtual const double	del_sW2_mu (const double mu) const
	Correction to (sin squared of) weak mixing angle. More...

virtual const double	del_Z_mu (const double mu) const
	Correction to Z WF. More...

virtual const double	del_ZA_mu (const double mu) const
	Correction to Z-A mixing. More...

virtual const double	delQ_gNC (const double mu) const
	Separate, charge-proportional, indirect correction to EW neutral currents. More...

virtual const double	delta2sBRH3 (const double C1prod, const double C1Hxx) const
	Quadratic contribution from the Higgs self-couplings modifications to the signal strength for $\sigma \times BR(H\to xx)$ in the current model. More...

virtual const double	delta2sH3 (const double C1) const
	Quadratic contribution from the Higgs self-couplings modifications to the signal strength for an observable $\sigma$ in the current model. More...

virtual const double	delta_AFB_ee (const double pol_e, const double pol_p, const double s) const

virtual const double	delta_AFB_f (const Particle f, const double pol_e, const double pol_p, const double s) const

virtual const double	delta_alrmoller (const double q2, const double y) const
	The computation of the parity violating asymmetry in Moller scattering. More...

virtual const double	delta_amuon () const
	The computation of the anomalous magnetic moment of the muon $a_\mu=(g_\mu-2)/2$. More...

virtual const double	delta_Dsigma_f (const Particle f, const double pol_e, const double pol_p, const double s, const double cos) const

virtual const double	delta_gAnue () const
	The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gAnue. More...

virtual const double	delta_gLnuN2 () const
	The computation of the correction to the effective neutrino nucleon LH coupling: delta_gLnuN2. More...

virtual const double	delta_gRnuN2 () const
	The computation of the correction to the effective neutrino nucleon RH coupling: delta_gRnuN2. More...

virtual const double	delta_gVnue () const
	The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gVnue. More...

virtual const double	delta_mubbH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{bbH}$ between the bbH production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_mubbH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{bbH}$ between the bbH production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_muggH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{ggH}$ between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_muggH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{ggH}$ between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_mutH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{tH}$ between the t-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_mutH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{tH}$ between the t-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_muttH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{ttH}$ between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_muttH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{ttH}$ between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_muVBF_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{VBF}$ between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_muVBF_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{VBF}$ between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_muVH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{VH}$ between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_muVH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{VH}$ between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_muWH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{WH}$ between the W-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_muWH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{WH}$ between the W-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_muZH_1 (const double sqrt_s) const
	The SMEFT linear correction to the ratio $\mu_{ZH}$ between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_muZH_2 (const double sqrt_s) const
	The SMEFT quadratic correction to the ratio $\mu_{ZH}$ between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	delta_Qwemoller (const double q2, const double y) const
	The computation of the electron's weak charge. More...

virtual const double	delta_Qwn () const
	The computation of the neutron weak charge: Qwn. More...

virtual const double	delta_Qwp () const
	The computation of the proton weak charge: Qwp. More...

virtual const double	delta_sigma_ee (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const

virtual const double	delta_sigma_f (const Particle f, const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const

virtual const double	delta_sigma_had (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const

virtual const double	delta_sigmaTot_ee (const double pol_e, const double pol_p, const double s) const

virtual const double	delta_sigmaTot_f (const Particle f, const double pol_e, const double pol_p, const double s) const

virtual const double	delta_TauLFU_gmuge () const
	The computation of the correction to the LFU ratio $g_\mu/ g_e $. More...

virtual const double	delta_TauLFU_gtauge () const
	The computation of the correction to the LFU ratio $g_\tau/ g_e $. More...

virtual const double	delta_TauLFU_gtaugmu () const
	The computation of the correction to the LFU ratio $g_\tau/ g_\mu $. More...

virtual const double	delta_TauLFU_gtaugmuK () const
	The computation of the correction to the LFU ratio $\left(g_\tau/ g_\mu\right)_K $. More...

virtual const double	delta_TauLFU_gtaugmuPi () const
	The computation of the correction to the LFU ratio $\left(g_\tau/ g_\mu\right)_\pi $. More...

virtual const double	deltaa0 () const
	The relative correction to the electromagnetic constant at zero momentum, $\delta \alpha(0)/\alpha(0)$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltaa02 () const
	The relative correction to the electromagnetic constant at zero momentum, $(\delta \alpha(0)/\alpha(0))^2$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltaA_f (const Particle f) const
	The new physics contribution to the left-right asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $\delta \mathcal{A}_f$. More...

virtual const double	deltaAFB (const Particle f) const
	The new physics contribution to the forward-backward asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $\delta A^f_{FB}$. More...

virtual const double	deltaaMZ () const
	The relative correction to the electromagnetic constant at the Z pole, $\delta \alpha(M_Z^2)/\alpha(M_Z^2)$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltaaMZ2 () const
	The relative correction to the electromagnetic constant at the Z pole, $(\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltaaSMZ () const
	The relative correction to the strong coupling constant at the Z pole, $\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltaaSMZ2 () const
	The relative correction to the strong coupling constant at the Z pole, $(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltacZ_HB (const double mu) const
	The Higgs-basis coupling $\delta c_z$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	deltadxsdcoseeWWlvjjLEP2 (const double sqrt_s, const int bin) const
	The new physics contribution to the differential cross section in pb for $e^+ e^- \to W^+ W^- \to lv jj $, with $ l= e,\mu $ for the 4 $ cos{\theta}$ bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph]. More...

virtual const double	deltaeNP (const double mu) const
	The new physics relative contribution to the EW coupling constant $e$. More...

virtual const double	deltaG1_hWW () const
	The new physics contribution to the coupling of the effective interaction $H W_{\mu\nu}^\dagger W^{\mu\nu}$. More...

virtual const double	deltaG1_hWW_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H W_{\mu\nu}^\dagger W^{\mu\nu}$. More...

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

virtual const double	deltaG1_hZA_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} F^{\mu\nu}$. More...

virtual const double	deltaG1_hZARatio () const
	The full new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} F^{A \mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value. More...

virtual const double	deltaG1_hZARatio_mu (const double mu) const
	The full new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} F^{A \mu\nu}$, including new local terms and modifications on the SM-loops. Normalized to the SM value. More...

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

virtual const double	deltaG1_hZZ_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} Z^{\mu\nu}$. More...

virtual const double	deltag1gaNP (const double mu) const
	The new physics contribution to the anomalous triple gauge coupling $g_{1,\gamma}$. More...

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

virtual const double	deltag1ZNPEff () const
	The new physics contribution to the effective anomalous triple gauge coupling $g_{1,Z}^{Eff}$ from arXiv: 1708.09079 [hep-ph]. More...

virtual const double	deltaG2_hWW () const
	The new physics contribution to the coupling of the effective interaction $H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}$. More...

virtual const double	deltaG2_hWW_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}$. More...

virtual const double	deltaG2_hZA () const
	The new physics contribution to the coupling of the effective interaction $H Z_{\nu} \partial^\mu F^{\mu\nu}$. More...

virtual const double	deltaG2_hZA_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H Z_{\nu} \partial^\mu F^{\mu\nu}$. More...

virtual const double	deltaG2_hZZ () const
	The new physics contribution to the coupling of the effective interaction $H Z_{\nu} \partial^\mu Z^{\mu\nu}$. More...

virtual const double	deltaG2_hZZ_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H Z_{\nu} \partial^\mu Z^{\mu\nu}$. More...

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

virtual const double	deltaG3_hWW_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H W_{\mu}^\dagger W^{\mu}$. More...

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

virtual const double	deltaG3_hZZ_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H Z_{\mu} Z^{\mu}$. More...

const double	deltag3G () const
	The new physics contribution to the coupling of the effective interaction $f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C$. More...

gslpp::complex	deltaG_Aff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$. More...

gslpp::complex	deltaG_Gff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $G_{\mu\nu}^A \bar{f}\sigma^{\mu\nu} T_A f$. More...

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

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

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

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

gslpp::complex	deltaG_hAff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$. More...

virtual gslpp::complex	deltaG_hff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H f\bar{f}$. More...

virtual gslpp::complex	deltaG_hff_mu (const Particle p, const double mu) const
	The new physics contribution to the coupling of the effective interaction $H f\bar{f}$. More...

gslpp::complex	deltaG_hGff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H G_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$. More...

virtual const double	deltaG_hgg () const
	The new physics contribution to the coupling of the effective interaction $H G_{\mu\nu}^AG^{A \mu\nu}$. More...

virtual const double	deltaG_hgg_mu (const double mu) const
	The new physics contribution to the coupling of the effective interaction $H G_{\mu\nu}^AG^{A \mu\nu}$. More...

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

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

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

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

gslpp::complex	deltaG_hZff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$. More...

gslpp::complex	deltaG_Zff (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f$. More...

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

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

virtual const double	deltaGamma_Wff (const Particle fi, const Particle fj) const
	The new physics contribution to the decay width of the $W$ boson into a given fermion pair, $\delta \Gamma_Z^{f}$. More...

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

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

const double	deltaGammaH2d2dRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2d2d)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2d2dRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2d2d)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2e2muRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2e 2\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2e2muRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2e 2\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2e2vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2e2v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2e2vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2e2v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2evRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2ev)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2evRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2ev)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2L2dRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2d)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2L2dRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2d)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2L2LRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2L')$ ( $L,L'=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2L2LRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2L')$ ( $L,L'=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2L2uRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2u)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2L2uRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2u)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2L2v2Ratio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2L2v2Ratio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2L2vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2l2vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2l2v)$ ( $l=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2L2vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2l2vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2l2v)$ ( $l=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2Lv2Ratio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2Lv2Ratio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2LvRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2LvRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2mu2vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2\mu 2v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2mu2vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2\mu 2v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2muvRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2\mu v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2muvRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2\mu v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2u2dRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2u2d)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2u2dRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2u2d)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2u2uRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2u2u)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2u2uRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2u2u)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2udRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2ud)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2udRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2ud)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2v2dRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2v2d)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2v2dRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2v2d)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2v2uRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2v2u)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2v2uRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2v2u)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2v2vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2v2v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH2v2vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 2v2v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4dRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4d)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4dRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4d)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4eRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4e)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4eRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4e)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4fCCRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4f, CC)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4fCCRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4f, CC)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4fNCRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4f, NC)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4fNCRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4f, NC)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4fRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4f)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4fRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4f)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4L2Ratio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4L2Ratio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4LRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4lRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4l)$ ( $l=e,\mu$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4LRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4lRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4l)$ ( $l=e,\mu$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4muRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4muRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4uRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4u)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4uRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4u)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4v)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaH4vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to 4v)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHbbRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to bb)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHbbRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to bb)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHccRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to cc)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHccRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to cc)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHevmuvRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to e\nu \mu\nu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHevmuvRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to e\nu \mu\nu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHffRatio1 (const double mf, const double CifH) const
	The ratio of the $\Gamma(H\to ff)$ in the current model and in the Standard Model. More...

const double	deltaGammaHffRatio2 (const double mf, const double CifH) const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the ratio of the $\Gamma(H\to ff)$ in the current model and in the Standard Model at order Lambd. More...

const double	deltaGammaHgagaRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to \gamma\gamma)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHgagaRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to \gamma\gamma)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHggRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to gg)$ in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...

const double	deltaGammaHggRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to gg)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHll_vvorjjRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to l l \nu\nu, l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHll_vvorjjRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to l l \nu\nu, l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHlv_lvorjjRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to l \nu l \nu, l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHlv_lvorjjRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to l \nu l \nu, l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHlvjjRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHlvjjRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHLvudRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Lvud)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHLvudRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Lvud)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHLvvLRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to LvvL)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHLvvLRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to LvvL)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHmumuRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to \mu\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHmumuRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to \mu\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHssRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ss)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHssRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ss)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHtautauRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to \tau\tau)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHtautauRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to \tau\tau)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHudduRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to uddu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHudduRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to uddu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWffRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to W f f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWffRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to W f f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWjjRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to W j j)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWjjRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to W j j)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWlvRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Wl\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWlvRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Wl\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWW2l2vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to l\nu l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWW2l2vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to l\nu l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWW4fRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWW4fRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWW4jRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to 4j)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWW4jRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW^*\to 4j)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWWRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHWWRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to WW)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZddRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z d d)$ ( $d=d,s,b $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZddRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z d d)$ ( $d=d,s,b $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZeeRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Zee)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZeeRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Zee)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZffRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z ff)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZffRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z ff)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZgaRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z\gamma)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZgaRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z\gamma)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZllRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Zll)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZllRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Zll)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZmumuRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z\mu\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZmumuRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z\mu\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZuuRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z u u)$ ( $u=u,c $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZuuRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z u u)$ ( $u=u,c $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZvvRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z\nu\nu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZvvRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to Z\nu\nu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ2e2muRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 2e2\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ2e2muRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 2e2\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4dRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4 d)$ ( $d=d,s,b $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4dRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4 d)$ ( $d=d,s,b $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4eRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4e)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4eRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4e)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4fRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4fRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4lRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4l)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4lRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4l)$ ( $l=e,\mu $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4muRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4\mu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4muRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4\mu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4uRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4 u)$ ( $u=u,c $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4uRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4 u)$ ( $u=u,c $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4vRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4\nu)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZ4vRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ* \to 4\nu)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ)$ in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...

const double	deltaGammaHZZRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H\to ZZ)$ in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...

virtual const double	deltaGammaTotalRatio1 () const
	The new physics contribution to the ratio of the $\Gamma(H)$ in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...

virtual const double	deltaGammaTotalRatio1noError () const
	The new physics contribution to the ratio of the $\Gamma(H)$ in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors. More...

virtual const double	deltaGammaTotalRatio2 () const
	The new physics contribution to the ratio of the $\Gamma(H)$ in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients. More...

virtual const double	DeltaGF () const
	New physics contribution to the Fermi constant. More...

const double	deltaGL_f (const Particle p) const
	New physics contribution to the neutral-current left-handed coupling $g_L^f$. More...

const double	deltaGL_f_mu (const Particle p, const double mu) const
	New physics contribution to the neutral-current left-handed coupling $g_L^f$. More...

virtual gslpp::complex	deltaGL_Wff (const Particle pbar, const Particle p) const
	New physics contribution to the charged current coupling $W_\mu \bar{f_L}\gamma^mu f_L$. More...

virtual gslpp::complex	deltaGL_Wff_mu (const Particle pbar, const Particle p, const double mu) const
	New physics contribution to the charged current coupling $W_\mu \bar{f_L}\gamma^mu f_L$. More...

gslpp::complex	deltaGL_Wffh (const Particle pbar, const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H W_\mu \bar{f_L}\gamma^mu f_L$. More...

const double	deltaGL_Zffh (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H Z_\mu \bar{f_L}\gamma^mu f_L$. More...

virtual const double	deltaGmu () const
	The relative correction to the muon decay constant, $\delta G_\mu/G_\mu$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltaGmu2 () const
	The relative correction to the muon decay constant, $(\delta G_\mu/G_\mu)^2$, with respect to ref. point used in the SM calculation of Higgs observables. More...

const double	deltaGR_f (const Particle p) const
	New physics contribution to the neutral-current right-handed coupling $g_R^f$. More...

const double	deltaGR_f_mu (const Particle p, const double mu) const
	New physics contribution to the neutral-current right-handed coupling $g_R^f$. More...

virtual gslpp::complex	deltaGR_Wff (const Particle pbar, const Particle p) const
	New physics contribution to the charged current coupling $W_\mu \bar{f_R}\gamma^mu f_R$. More...

virtual gslpp::complex	deltaGR_Wff_mu (const Particle pbar, const Particle p, const double mu) const
	New physics contribution to the charged current coupling $W_\mu \bar{f_R}\gamma^mu f_R$. More...

gslpp::complex	deltaGR_Wffh (const Particle pbar, const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H W_\mu \bar{f_R}\gamma^mu f_R$. More...

const double	deltaGR_Zffh (const Particle p) const
	The new physics contribution to the coupling of the effective interaction $H Z_\mu \bar{f_R}\gamma^mu f_R$. More...

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

virtual const double	deltaGwd6 () const
	The relative NP corrections to the width of the $W$ boson, $\delta \Gamma_W/\Gamma_W$. More...

virtual const double	deltaGwd62 () const
	The relative NP corrections to the width of the $W$ boson squared, $(\delta \Gamma_W/\Gamma_W)^2$. More...

virtual const double	deltaGzd6 () const
	The relative NP corrections to the width of the $Z$ boson, $\delta \Gamma_Z/\Gamma_Z$. More...

virtual const double	deltaGzd62 () const
	The relative NP corrections to the width of the $Z$ boson squared, $(\delta \Gamma_Z/\Gamma_Z)^2$. More...

virtual const double	deltaH3L1 (double C1) const
	The coefficient of the 1-loop linear term in the Higgs selfcoupling. More...

virtual const double	deltaH3L2 (double C1) const
	The coefficient of the 1-loop quadratic term in the Higgs selfcoupling. More...

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

virtual const double	deltaKgammaNPEff () const
	The new physics contribution to the effective anomalous triple gauge coupling $\kappa_{\gamma}^{Eff}$ from arXiv: 1708.09079 [hep-ph]. More...

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

virtual const double	deltamb () const
	The relative correction to the mass of the $b$ quark, $\delta m_b/m_b$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltamb2 () const
	The relative correction to the mass of the $b$ quark squared, $(\delta m_b/m_b)^2$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltamc () const
	The relative correction to the mass of the $c$ quark, $\delta m_c/m_c$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltamc2 () const
	The relative correction to the mass of the $c$ quark squared, $(\delta m_c/m_c)^2$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltaMh () const
	The relative correction to the mass of the $H$ boson, $\delta M_H/M_H$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltaMh2 () const
	The relative correction to the mass of the $H$ boson squared, $(\delta M_H/M_H)^2$, with respect to ref. point used in the SM calculation of Higgs observables. More...

const double	deltaMLL2_f (const Particle f, const double s, const double t) const

const double	deltaMLR2_f (const Particle f, const double s) const

const double	deltaMLR2t_e (const double s, const double t) const

const double	deltaMRL2_f (const Particle f, const double s) const

const double	deltaMRL2t_e (const double s, const double t) const

const double	deltaMRR2_f (const Particle f, const double s, const double t) const

virtual const double	deltamt () const
	The relative correction to the mass of the $t$ quark, $\delta m_t/m_t$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltamt2 () const
	The relative correction to the mass of the $t$ quark squared, $(\delta m_t/m_t)^2$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltamtau () const
	The relative correction to the mass of the $\tau$ lepton, $\delta m_\tau/m_\tau$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltamtau2 () const
	The relative correction to the mass of the $\tau$ lepton squared, $(\delta m_\tau/m_\tau)^2$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltaMw () const
	The relative correction to the mass of the $W$ boson, $\delta M_W/M_W$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltaMw2 () const
	The relative correction to the mass of the $W$ boson squared, $(\delta M_W/M_W)^2$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltaMwd6 () const
	The relative NP corrections to the mass of the $W$ boson, $\delta M_W/M_W$. More...

virtual const double	deltaMwd62 () const
	The relative NP corrections to the mass of the $W$ boson squared, $(\delta M_W/M_W)^2$. More...

virtual const double	deltaMz () const
	The relative correction to the mass of the $Z$ boson, $\delta M_Z/M_Z$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	deltaMz2 () const
	The relative correction to the mass of the $Z$ boson squared, $(\delta M_Z/M_Z)^2$, with respect to ref. point used in the SM calculation of Higgs observables. More...

virtual const double	DeltaOalphtoW (const double dOSMdalpha, const double mu) const
	Difference in prediction in $\alpha$ scheme and W mass scheme, computed from observable in $\alpha$ scheme. Difference at tree level. More...

virtual const double	DeltaOWtoalph (const double dOSMdMW, const double mu) const
	Difference in prediction in $\alpha$ scheme and W mass scheme, computed from observable in W mass scheme. Difference at tree level. More...

virtual const double	deltaR0_f (const Particle f) const
	The new physics contribution to the ratio $R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell$, $R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}$ and $R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}$, for charged leptons, quarks and neutrinos, respectively. More...

virtual const double	deltaSigmaHadron () const
	The new physics contribution to the cross section for the process $e^+ e^-\to Z\to \mathrm{hadrons}$ at the $Z$ pole, $\delta \sigma_h^0$. More...

virtual const double	deltaxseeWW4fLEP2 (const double sqrt_s, const int fstate) const
	The new physics contribution to the cross section in pb for $e^+ e^- \to W^+ W^- \to 4f $, with $ 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) $ the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More...

virtual const double	deltaxseeWWtotLEP2 (const double sqrt_s) const
	The new physics contribution to the total cross section in pb for $e^+ e^- \to W^+ W^-$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More...

virtual const double	deltayb_HB (const double mu) const
	The Higgs-basis coupling $\delta y_b$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	deltayc_HB (const double mu) const
	The Higgs-basis coupling $\delta y_c$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	deltaymu_HB (const double mu) const
	The Higgs-basis coupling $\delta y_\mu$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	deltays_HB (const double mu) const
	The Higgs-basis coupling $\delta y_s$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	deltayt_HB (const double mu) const
	The Higgs-basis coupling $\delta y_t$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	deltaytau_HB (const double mu) const
	The Higgs-basis coupling $\delta y_\tau$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	delU_gCC (const double mu) const
	Universal indirect correction to EW charged currents. More...

virtual const double	delU_gNC (const double mu) const
	Universal indirect correction to EW neutral currents. More...

virtual const double	dxsdcoseeWWlvjjLEP2 (const double sqrt_s, const int bin) const
	The differential cross section in pb for $e^+ e^- \to W^+ W^- \to lv jj $, with $ l= e,\mu $ for the 4 $ cos{\theta}$ bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph]. More...

virtual const double	dxseeWWdcos (const double sqrt_s, const double cos) const
	The differential distribution for $e^+ e^- \to W^+ W^- \to jj \ell \nu$, with $\ell= e, \mu$, as a function of the $W$ polar angle. More...

virtual const double	dxseeWWdcosBin (const double sqrt_s, const double cos1, const double cos2) const
	The integral of differential distribution for $e^+ e^- \to W^+ W^- \to jj \ell \nu$, with $\ell= e, \mu$ in a given bin of the $W$ polar angle. More...

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

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

const double	GammaH2d2dRatio () const
	The ratio of the $\Gamma(H\to 2d2d)$ in the current model and in the Standard Model. More...

const double	GammaH2e2muRatio () const
	The ratio of the $\Gamma(H\to 2e 2\mu)$ in the current model and in the Standard Model. More...

const double	GammaH2e2vRatio () const
	The ratio of the $\Gamma(H\to 2e2v)$ in the current model and in the Standard Model. More...

const double	GammaH2evRatio () const
	The ratio of the $\Gamma(H\to 2ev)$ in the current model and in the Standard Model. More...

const double	GammaH2L2dRatio () const
	The ratio of the $\Gamma(H\to 2L2d)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

const double	GammaH2L2LRatio () const
	The ratio of the $\Gamma(H\to 2L2L')$ ( $L,L'=e,\mu,\tau$) in the current model and in the Standard Model. More...

const double	GammaH2L2uRatio () const
	The ratio of the $\Gamma(H\to 2L2u)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

const double	GammaH2L2v2Ratio () const
	The ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu$) in the current model and in the Standard Model. More...

const double	GammaH2L2vRatio () const
	The ratio of the $\Gamma(H\to 2L2v)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

const double	GammaH2l2vRatio () const
	The ratio of the $\Gamma(H\to 2l2v)$ ( $l=e,\mu$) in the current model and in the Standard Model. More...

const double	GammaH2Lv2Ratio () const
	The ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu$) in the current model and in the Standard Model. More...

const double	GammaH2LvRatio () const
	The ratio of the $\Gamma(H\to 2Lv)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

const double	GammaH2mu2vRatio () const
	The ratio of the $\Gamma(H\to 2\mu 2v)$ in the current model and in the Standard Model. More...

const double	GammaH2muvRatio () const
	The ratio of the $\Gamma(H\to 2\mu v)$ in the current model and in the Standard Model. More...

const double	GammaH2u2dRatio () const
	The ratio of the $\Gamma(H\to 2u2d)$ in the current model and in the Standard Model. More...

const double	GammaH2u2uRatio () const
	The ratio of the $\Gamma(H\to 2u2u)$ in the current model and in the Standard Model. More...

const double	GammaH2udRatio () const
	The ratio of the $\Gamma(H\to 2ud)$ in the current model and in the Standard Model. More...

const double	GammaH2v2dRatio () const
	The ratio of the $\Gamma(H\to 2v2d)$ in the current model and in the Standard Model. More...

const double	GammaH2v2uRatio () const
	The ratio of the $\Gamma(H\to 2v2u)$ in the current model and in the Standard Model. More...

const double	GammaH2v2vRatio () const
	The ratio of the $\Gamma(H\to 2v2v)$ in the current model and in the Standard Model. More...

const double	GammaH4dRatio () const
	The ratio of the $\Gamma(H\to 4d)$ in the current model and in the Standard Model. More...

const double	GammaH4eRatio () const
	The ratio of the $\Gamma(H\to 4e)$ in the current model and in the Standard Model. More...

const double	GammaH4fCCRatio () const
	The ratio of the $\Gamma(H\to 4f)$ via CC in the current model and in the Standard Model. More...

const double	GammaH4fNCRatio () const
	The ratio of the $\Gamma(H\to 4f)$ via NC in the current model and in the Standard Model. More...

const double	GammaH4fRatio () const
	The ratio of the $\Gamma(H\to 4f)$ in the current model and in the Standard Model. More...

const double	GammaH4L2Ratio () const
	The ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu$) in the current model and in the Standard Model. More...

const double	GammaH4LRatio () const
	The ratio of the $\Gamma(H\to 4L)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

const double	GammaH4lRatio () const
	The ratio of the $\Gamma(H\to 4l)$ ( $l=e,\mu$) in the current model and in the Standard Model. More...

const double	GammaH4muRatio () const
	The ratio of the $\Gamma(H\to 4\mu)$ in the current model and in the Standard Model. More...

const double	GammaH4uRatio () const
	The ratio of the $\Gamma(H\to 4u)$ in the current model and in the Standard Model. More...

const double	GammaH4vRatio () const
	The ratio of the $\Gamma(H\to 4v)$ in the current model and in the Standard Model. More...

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

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

const double	GammaHevmuvRatio () const
	The ratio of the $\Gamma(H\to e\nu \mu\nu)$ in the current model and in the Standard Model. More...

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

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

const double	GammaHll_vvorjjRatio () const
	The ratio of the $\Gamma(H\to l l \nu\nu, l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. More...

const double	GammaHlv_lvorjjRatio () const
	The ratio of the $\Gamma(H\to l \nu l \nu, l \nu j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. More...

const double	GammaHlvjjRatio () const
	The ratio of the $\Gamma(H\to l l j j)$ ( $l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. @return $\Gamma(H\to l l j j) $/$\Gamma(H\to l l j j)_{\mathrm{SM}} $ / const double GammaHlljjRatio() const; /* @brief The new physics contribution to the ratio of the $\Gamma(H\to l l j j) $ ($l=e,\mu,~~j\not=b $) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) @return $\delta \Gamma(H\to l l j j) $/$\Gamma(H\to l l j j)_{\mathrm{SM}} $ / const double deltaGammaHlljjRatio1() const; /* @brief The new physics contribution to the ratio of the $\Gamma(H\to l l j j) $ ($l=e,\mu,~~j\not=b $) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) @return $\delta \Gamma(H\to l l j j) $/$\Gamma(H\to l l j j)_{\mathrm{SM}} $ / const double deltaGammaHlljjRatio2() const; /* @brief The ratio of the Br$(H\to l l j j) $ ($l=e,\mu,~~j\not=b $) in the current model and in the Standard Model. @return Br$(H\to l l j j) $/Br$(H\to l l j j)_{\mathrm{SM}} $ / virtual const double BrHlljjRatio() const; /* @brief The ratio of the $\Gamma(H\to l \nu j j) $ ($l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. More...

const double	GammaHLvudRatio () const
	The ratio of the $\Gamma(H\to Lvud)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

const double	GammaHLvvLRatio () const
	The ratio of the $\Gamma(H\to LvvL)$ ( $L=e,\mu,\tau$) in the current model and in the Standard Model. More...

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

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

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

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

const double	GammaHWffRatio () const
	The ratio of the $\Gamma(H\to W f f)$, with $f$ any fermion, in the current model and in the Standard Model. More...

const double	GammaHWjjRatio () const
	The ratio of the $\Gamma(H\to W j j)$ in the current model and in the Standard Model. More...

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

const double	GammaHWW2l2vRatio () const
	The ratio of the $\Gamma(H\to WW^*\to l\nu l\nu)$ ( $l=e,\mu $) in the current model and in the Standard Model. More...

const double	GammaHWW4fRatio () const
	The ratio of the $\Gamma(H\to WW^*\to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. More...

const double	GammaHWW4jRatio () const
	The ratio of the $\Gamma(H\to WW^*\to 4j)$ in the current model and in the Standard Model. More...

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

const double	GammaHZddRatio () const
	The ratio of the $\Gamma(H\to Zd d)$ ( $d=d,s,b $) in the current model and in the Standard Model. More...

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

const double	GammaHZffRatio () const
	The ratio of the $\Gamma(H\to Zff)$, with $f$ any fermion, in the current model and in the Standard Model. More...

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

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

const double	GammaHZmumuRatio () const
	The ratio of the $\Gamma(H\to Z\mu\mu)$ in the current model and in the Standard Model. More...

const double	GammaHZuuRatio () const
	The ratio of the $\Gamma(H\to Zu u)$ ( $u=u,c $) in the current model and in the Standard Model. More...

const double	GammaHZvvRatio () const
	The ratio of the $\Gamma(H\to Z\nu\nu)$ in the current model and in the Standard Model. More...

const double	GammaHZZ2e2muRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 2e2\mu)$ in the current model and in the Standard Model. More...

const double	GammaHZZ4dRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4 d)$ ( $d=d,s,b $) in the current model and in the Standard Model. More...

const double	GammaHZZ4eRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4e)$ in the current model and in the Standard Model. More...

const double	GammaHZZ4fRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4f)$, with $f$ any fermion, in the current model and in the Standard Model. More...

const double	GammaHZZ4lRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4l)$ ( $l=e,\mu $) in the current model and in the Standard Model. More...

const double	GammaHZZ4muRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4\mu)$ in the current model and in the Standard Model. More...

const double	GammaHZZ4uRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4 u)$ ( $u=u,c $) in the current model and in the Standard Model. More...

const double	GammaHZZ4vRatio () const
	The ratio of the $\Gamma(H\to ZZ* \to 4\nu)$ in the current model and in the Standard Model. More...

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

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

virtual const double	GammaW (const Particle fi, const Particle fj) const
	A partial decay width of the $W$ boson decay into a SM fermion pair. More...

double	getCG_LNP () const
	Return CG_LNP. More...

const double	getCW_tree () const

const double	getDelta_ale () const

const double	getDelta_g1 () const

const double	getDelta_g2 () const

const double	getDelta_Mz2 () const

const double	getDelta_v () const

const double	getDelta_xBZ () const

const double	getDelta_xWZ () const

const double	getEeMz () const

const double	getG1_tree () const

const double	getG2_tree () const

const double	getG3_tree () const

const double	getGZdL () const

const double	getGZdR () const

const double	getGZlL () const

const double	getGZlR () const

const double	getGZuL () const

const double	getGZuR () const

const double	getGZvL () const

double	getLambda_NP () const
	Return Lambda_NP. More...

virtual NPSMEFTd6GeneralMatching &	getMatching () const
	A method to get the Matching object for this model. More...

const double	getMw_tree () const

double	getSMEFTCoeff (const std::string name, const double mu) const

double	getSMEFTCoeff (const std::string name, int i, int j, const double mu) const

double	getSMEFTCoeff (const std::string name, int i, int j, int k, int l, const double mu) const

double	getSMEFTCoeffEW (const std::string name) const

double	getSMEFTCoeffEW (const std::string name, int i, int j) const

double	getSMEFTCoeffEW (const std::string name, int i, int j, int k, int l) const

gslpp::complex	getSMEFTCoeffEWMB (const std::string name, int i, int j, gslpp::matrix< gslpp::complex > Vi, gslpp::matrix< gslpp::complex > Vj) const

gslpp::complex	getSMEFTCoeffEWMB (const std::string name, int i, int j, int k, int l, gslpp::matrix< gslpp::complex > Vi, gslpp::matrix< gslpp::complex > Vj, gslpp::matrix< gslpp::complex > Vk, gslpp::matrix< gslpp::complex > Vl) const

gslpp::complex	getSMEFTCoeffMB (const std::string name, int i, int j, gslpp::matrix< gslpp::complex > Vi, gslpp::matrix< gslpp::complex > Vj, const double mu) const

gslpp::complex	getSMEFTCoeffMB (const std::string name, int i, int j, int k, int l, gslpp::matrix< gslpp::complex > Vi, gslpp::matrix< gslpp::complex > Vj, gslpp::matrix< gslpp::complex > Vk, gslpp::matrix< gslpp::complex > Vl, const double mu) const

const RGESolver &	getSMEFTEvol () const

RGESolver	getSMEFTEvolEW () const

const double	getSW_tree () const

const gslpp::matrix< gslpp::complex > &	getVdL () const

const gslpp::matrix< gslpp::complex > &	getVdLd () const

const gslpp::matrix< gslpp::complex > &	getVdR () const

const gslpp::matrix< gslpp::complex > &	getVdRd () const

const gslpp::matrix< gslpp::complex > &	getVeL () const

const gslpp::matrix< gslpp::complex > &	getVeLd () const

const gslpp::matrix< gslpp::complex > &	getVeR () const

const gslpp::matrix< gslpp::complex > &	getVeRd () const

const gslpp::matrix< gslpp::complex > &	getVuL () const

const gslpp::matrix< gslpp::complex > &	getVuLd () const

const gslpp::matrix< gslpp::complex > &	getVuR () const

const gslpp::matrix< gslpp::complex > &	getVuRd () const

const double	getXBZ_tree () const

const double	getXWZ_tree () const

gslpp::matrix< gslpp::complex >	getYd () const

gslpp::matrix< gslpp::complex >	getYe () const

gslpp::matrix< gslpp::complex >	getYu () const

virtual const double	IctW_TWG (const double mu) const

virtual const double	IctZ_TWG (const double mu) const

virtual bool	Init (const std::map< std::string, double > &DPars)
	A method to initialize the model parameters. More...

virtual const double	intDMLL2eus2 (const double s, const double t0, const double t1) const

virtual const double	intDMLR2etildest2 (const double s, const double t0, const double t1) const

virtual const double	intDMLR2ets2 (const double s, const double t0, const double t1) const

virtual const double	intDMRL2etildest2 (const double s, const double t0, const double t1) const

virtual const double	intDMRL2ets2 (const double s, const double t0, const double t1) const

virtual const double	intDMRR2eus2 (const double s, const double t0, const double t1) const

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

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

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

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

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

virtual const double	kappaseff () const
	The effective coupling $\kappa_{s,eff}=\sqrt{\Gamma_{Hss}/\Gamma_{Hss}^{SM}}$. More...

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

virtual const double	kappaW4feff () const
	The effective coupling $\kappa_{W4f,eff}=\sqrt{\Gamma_{H4f, CC}/\Gamma_{H4f, CC}^{SM}}$. More...

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

virtual const double	kappaZ4feff () const
	The effective coupling $\kappa_{Z4f,eff}=\sqrt{\Gamma_{H4f, NC}/\Gamma_{H4f, NC}^{SM}}$. More...

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

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

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

virtual const double	lambz_HB (const double mu) const
	The Higgs-basis coupling $\lambda_{z}$. (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the $g_i, \delta g_i$ couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for $g_i, \delta g_i$. More...

virtual const double	mubbH (const double sqrt_s) const
	The ratio $\mu_{bbH}$ between the bbH production cross-section in the current model and in the Standard Model. More...

virtual const double	mueeHee (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{e^+e^- \to He^+e^-}$ between the $ e^+e^- \to H e^+e^- $ associated production cross-section in the current model and in the Standard Model. More...

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

virtual const double	mueettH (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eettH}$ between the $ e^{+}e^{-}\to t\bar{t} H $ production cross-section in the current model and in the Standard Model. More...

virtual const double	mueeWBF (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeWBF}$ between the $ e^{+}e^{-}\to \nu\bar{\nu} H $ production cross-section in the current model and in the Standard Model. More...

virtual const double	mueeWW (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeWW}$ between the $ e^{+}e^{-}\to W^{+}W^{-} $ production cross-section in the current model and in the Standard Model. More...

virtual const double	mueeZBF (const double sqrt_s, const double Pol_em, const double Pol_ep) const
	The ratio $\mu_{eeZBF}$ between the $ e^{+}e^{-}\to e^{+}e^{-} H $ production cross-section in the current model and in the Standard Model. More...

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

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

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

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

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

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

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

virtual const double	muepWBF (const double sqrt_s) const
	The ratio $\mu_{epWBF}$ between the $ e^{-} p\to \nu j H $ production cross-section in the current model and in the Standard Model. More...

virtual const double	muepZBF (const double sqrt_s) const
	The ratio $\mu_{epZBF}$ between the $ e^{-} p\to e^{-} j H $ production cross-section in the current model and in the Standard Model. More...

virtual const double	muggH (const double sqrt_s) const
	The ratio $\mu_{ggH}$ between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More...

virtual const double	muggHbb (const double sqrt_s) const
	The ratio $\mu_{ggH,bb}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model. More...

virtual const double	muggHgaga (const double sqrt_s) const
	The ratio $\mu_{ggH,\gamma\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...

virtual const double	muggHH (const double sqrt_s) const
	The ratio $\mu_{ggHH}$ between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].) More...

virtual const double	muggHmumu (const double sqrt_s) const
	The ratio $\mu_{ggH,\mu\mu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model. More...

virtual const double	muggHpttH (const double sqrt_s) const
	The ratio $\mu_{ggH+ttH}$ between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	muggHtautau (const double sqrt_s) const
	The ratio $\mu_{ggH,\tau\tau}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model. More...

virtual const double	muggHWW (const double sqrt_s) const
	The ratio $\mu_{ggH,WW}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model. More...

virtual const double	muggHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{ggH,WW\to 2l2\nu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model. More...

virtual const double	muggHZga (const double sqrt_s) const
	The ratio $\mu_{ggH,Z\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model. More...

virtual const double	muggHZZ (const double sqrt_s) const
	The ratio $\mu_{ggH,ZZ}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model. More...

virtual const double	muggHZZ4l (const double sqrt_s) const
	The ratio $\mu_{ggH,ZZ\to 4l}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model. More...

virtual const double	mummH (const double sqrt_s) const
	The ratio $\mu_{\mu\mu H}$ between the $\sigma(\mu \mu \to H)}$ production cross-section in the current model and in the Standard Model. More...

virtual const double	mummHmm (const double sqrt_s) const
	The ratio $\mu_{\mu\mu H\mu\mu}$ between the $\sigma(\mu \mu \to H \mu \mu)}$ production cross-section in the current model and in the Standard Model. More...

virtual const double	mummHNWA (const double sqrt_s) const
	The ratio $\mu_{\mu\mu H}$ between the $\sigma(\mu \mu \to H)}$ production cross-section in the current model and in the Standard Model, in the narrow width approximation. More...

virtual const double	mummHvv (const double sqrt_s) const
	The ratio $\mu_{\mu\mu H\nu\nu}$ between the $\sigma(\mu \mu \to H \nu \nu)}$ production cross-section in the current model and in the Standard Model. More...

virtual const double	mummttH (const double sqrt_s) const
	The ratio $\mu_{\mu\mu ttH}$ between the $\sigma(\mu \mu \to t\bar{t} H )}$ production cross-section in the current model and in the Standard Model. More...

virtual const double	mummZH (const double sqrt_s) const
	The ratio $\mu_{\mu\mu ZH}$ between the $\sigma(\mu \mu \to Z H)}$ production cross-section in the current model and in the Standard Model. More...

virtual const double	mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const
	The number of events in $ p p \to WZ$ in a given $p_{TV}$ bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6General class. More...

virtual const double	mutH (const double sqrt_s) const
	The ratio $\mu_{tH}$ between the t-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	mutHq (const double sqrt_s) const
	The ratio $\mu_{tHq}$ between the t-q-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	muTHUggHbb (const double sqrt_s) const
	The ratio $\mu_{ggH,bb}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model. More...

virtual const double	muTHUggHgaga (const double sqrt_s) const
	The ratio $\mu_{ggH,\gamma\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...

virtual const double	muTHUggHmumu (const double sqrt_s) const
	The ratio $\mu_{ggH,\mu\mu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model. More...

virtual const double	muTHUggHtautau (const double sqrt_s) const
	The ratio $\mu_{ggH,\tau\tau}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model. More...

virtual const double	muTHUggHWW (const double sqrt_s) const
	The ratio $\mu_{ggH,WW}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model. More...

virtual const double	muTHUggHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{ggH,WW\to 2l2\nu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model. More...

virtual const double	muTHUggHZga (const double sqrt_s) const
	The ratio $\mu_{ggH,Z\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model. More...

virtual const double	muTHUggHZgamumu (const double sqrt_s) const
	The ratio $\mu_{ggH,Z\gamma\to \gamma 2\mu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z \gamma\to \gamma 2\mu$ in the current model and in the Standard Model. More...

virtual const double	muTHUggHZZ (const double sqrt_s) const
	The ratio $\mu_{ggH,ZZ}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model. More...

virtual const double	muTHUggHZZ4l (const double sqrt_s) const
	The ratio $\mu_{ggH,ZZ\to 4l}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model. More...

virtual const double	muTHUggHZZ4mu (const double sqrt_s) const
	The ratio $\mu_{ggH,ZZ\to 4\mu}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into $Z Z^*\to 4\mu$ in the current model and in the Standard Model. More...

virtual const double	muTHUttHbb (const double sqrt_s) const
	The ratio $\mu_{ttH,bb}$ between the ttH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model. More...

virtual const double	muTHUttHgaga (const double sqrt_s) const
	The ratio $\mu_{ttH,\gamma\gamma}$ between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...

virtual const double	muTHUttHmumu (const double sqrt_s) const
	The ratio $\mu_{ttH,\mu\mu}$ between the ttH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model. More...

virtual const double	muTHUttHtautau (const double sqrt_s) const
	The ratio $\mu_{ttH,\tau\tau}$ between the ttH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model. More...

virtual const double	muTHUttHWW (const double sqrt_s) const
	The ratio $\mu_{ttH,WW}$ between the ttH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model. More...

virtual const double	muTHUttHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{ttH,WW\to 2l2\nu}$ between the ttH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model. More...

virtual const double	muTHUttHZga (const double sqrt_s) const
	The ratio $\mu_{ttH,Z\gamma}$ between the ttH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model. More...

virtual const double	muTHUttHZZ (const double sqrt_s) const
	The ratio $\mu_{ttH,ZZ}$ between the ttH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model. More...

virtual const double	muTHUttHZZ4l (const double sqrt_s) const
	The ratio $\mu_{ttH,ZZ\to 4l}$ between the ttH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model. More...

virtual const double	muTHUVBFBRinv (const double sqrt_s) const
	The ratio $\mu_{VBF}$ between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More...

virtual const double	muTHUVBFHbb (const double sqrt_s) const
	The ratio $\mu_{VBF,bb}$ between the VBF Higgs production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model. More...

virtual const double	muTHUVBFHgaga (const double sqrt_s) const
	The ratio $\mu_{VBF,\gamma\gamma}$ between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...

virtual const double	muTHUVBFHinv (const double sqrt_s) const
	The ratio $\mu_{VBF,inv}$ between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More...

virtual const double	muTHUVBFHmumu (const double sqrt_s) const
	The ratio $\mu_{VBF,\mu\mu}$ between the VBF Higgs production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model. More...

virtual const double	muTHUVBFHtautau (const double sqrt_s) const
	The ratio $\mu_{VBF,\tau\tau}$ between the VBF Higgs production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model. More...

virtual const double	muTHUVBFHWW (const double sqrt_s) const
	The ratio $\mu_{VBF,WW}$ between the VBF Higgs production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model. More...

virtual const double	muTHUVBFHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{VBF,WW\to 2l2\nu}$ between the VBF Higgs production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model. More...

virtual const double	muTHUVBFHZga (const double sqrt_s) const
	The ratio $\mu_{VBF,Z\gamma}$ between the VBF Higgs production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model. More...

virtual const double	muTHUVBFHZZ (const double sqrt_s) const
	The ratio $\mu_{VBF,ZZ}$ between the VBF Higgs production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model. More...

virtual const double	muTHUVBFHZZ4l (const double sqrt_s) const
	The ratio $\mu_{VBF,ZZ\to 4l}$ between the VBF Higgs production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model. More...

virtual const double	muTHUVHbb (const double sqrt_s) const
	The ratio $\mu_{VH,bb}$ between the VH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model. More...

virtual const double	muTHUVHBRinv (const double sqrt_s) const
	The ratio $\mu_{VH}$ between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More...

virtual const double	muTHUVHgaga (const double sqrt_s) const
	The ratio $\mu_{VH,\gamma\gamma}$ between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...

virtual const double	muTHUVHinv (const double sqrt_s) const
	The ratio $\mu_{VH,inv}$ between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More...

virtual const double	muTHUVHmumu (const double sqrt_s) const
	The ratio $\mu_{VH,\mu\mu}$ between the VH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model. More...

virtual const double	muTHUVHtautau (const double sqrt_s) const
	The ratio $\mu_{VH,\tau\tau}$ between the VH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model. More...

virtual const double	muTHUVHWW (const double sqrt_s) const
	The ratio $\mu_{VH,WW}$ between the VH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model. More...

virtual const double	muTHUVHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{VH,WW\to 2l2\nu}$ between the VH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model. More...

virtual const double	muTHUVHZga (const double sqrt_s) const
	The ratio $\mu_{VH,Z\gamma}$ between the VH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model. More...

virtual const double	muTHUVHZZ (const double sqrt_s) const
	The ratio $\mu_{VH,ZZ}$ between the VH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model. More...

virtual const double	muTHUVHZZ4l (const double sqrt_s) const
	The ratio $\mu_{VH,ZZ\to 4l}$ between the VH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model. More...

virtual const double	muTHUWHbb (const double sqrt_s) const
	The ratio $\mu_{WH,bb}$ between the WH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model. More...

virtual const double	muTHUWHgaga (const double sqrt_s) const
	The ratio $\mu_{WH,\gamma\gamma}$ between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...

virtual const double	muTHUWHmumu (const double sqrt_s) const
	The ratio $\mu_{WH,\mu\mu}$ between the WH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model. More...

virtual const double	muTHUWHtautau (const double sqrt_s) const
	The ratio $\mu_{WH,\tau\tau}$ between the WH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model. More...

virtual const double	muTHUWHWW (const double sqrt_s) const
	The ratio $\mu_{WH,WW}$ between the WH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model. More...

virtual const double	muTHUWHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{WH,WW\to 2l2\nu}$ between the WH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model. More...

virtual const double	muTHUWHZga (const double sqrt_s) const
	The ratio $\mu_{WH,Z\gamma}$ between the WH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model. More...

virtual const double	muTHUWHZZ (const double sqrt_s) const
	The ratio $\mu_{WH,ZZ}$ between the WH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model. More...

virtual const double	muTHUWHZZ4l (const double sqrt_s) const
	The ratio $\mu_{WH,ZZ\to 4l}$ between the WH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model. More...

virtual const double	muTHUZHbb (const double sqrt_s) const
	The ratio $\mu_{ZH,bb}$ between the ZH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model. More...

virtual const double	muTHUZHgaga (const double sqrt_s) const
	The ratio $\mu_{ZH,\gamma\gamma}$ between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...

virtual const double	muTHUZHmumu (const double sqrt_s) const
	The ratio $\mu_{ZH,\mu\mu}$ between the ZH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model. More...

virtual const double	muTHUZHtautau (const double sqrt_s) const
	The ratio $\mu_{ZH,\tau\tau}$ between the ZH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model. More...

virtual const double	muTHUZHWW (const double sqrt_s) const
	The ratio $\mu_{ZH,WW}$ between the ZH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model. More...

virtual const double	muTHUZHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{ZH,WW\to 2l2\nu}$ between the ZH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model. More...

virtual const double	muTHUZHZga (const double sqrt_s) const
	The ratio $\mu_{ZH,Z\gamma}$ between the ZH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model. More...

virtual const double	muTHUZHZZ (const double sqrt_s) const
	The ratio $\mu_{ZH,ZZ}$ between the ZH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model. More...

virtual const double	muTHUZHZZ4l (const double sqrt_s) const
	The ratio $\mu_{ZH,ZZ\to 4l}$ between the ZH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model. More...

virtual const double	muttH (const double sqrt_s) const
	The ratio $\mu_{ttH}$ between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	muttHbb (const double sqrt_s) const
	The ratio $\mu_{ttH,bb}$ between the ttH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model. More...

virtual const double	muttHgaga (const double sqrt_s) const
	The ratio $\mu_{ttH,\gamma\gamma}$ between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...

virtual const double	muttHgagaZeeboost (const double sqrt_s) const
	The ratio $\sigma(ttH)/\sigma(ttZ)$ in the $H\to b\bar{b}$, $Z\to e^+e^-$ channel channel in the current model and in the Standard Model. More...

virtual const double	muttHmumu (const double sqrt_s) const
	The ratio $\mu_{ttH,\mu\mu}$ between the ttH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model. More...

virtual const double	muttHtautau (const double sqrt_s) const
	The ratio $\mu_{ttH,\tau\tau}$ between the ttH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model. More...

virtual const double	muttHWW (const double sqrt_s) const
	The ratio $\mu_{ttH,WW}$ between the ttH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model. More...

virtual const double	muttHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{ttH,WW\to 2l2\nu}$ between the ttH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model. More...

virtual const double	muttHZbbboost (const double sqrt_s) const
	The ratio $\sigma(ttH)/\sigma(ttZ)$ in the $H,Z\to b\bar{b}$ channel in the current model and in the Standard Model. More...

virtual const double	muttHZga (const double sqrt_s) const
	The ratio $\mu_{ttH,Z\gamma}$ between the ttH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model. More...

virtual const double	muttHZZ (const double sqrt_s) const
	The ratio $\mu_{ttH,ZZ}$ between the ttH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model. More...

virtual const double	muttHZZ4l (const double sqrt_s) const
	The ratio $\mu_{ttH,ZZ\to 4l}$ between the ttH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model. More...

virtual const double	muVBF (const double sqrt_s) const
	The ratio $\mu_{VBF}$ between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More...

virtual const double	muVBFgamma (const double sqrt_s) const
	The ratio $\mu_{VBF+\gamma}$ between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model. More...

virtual const double	muVBFHbb (const double sqrt_s) const
	The ratio $\mu_{VBF,bb}$ between the VBF Higgs production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model. More...

virtual const double	muVBFHgaga (const double sqrt_s) const
	The ratio $\mu_{VBF,\gamma\gamma}$ between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...

virtual const double	muVBFHmumu (const double sqrt_s) const
	The ratio $\mu_{VBF,\mu\mu}$ between the VBF Higgs production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model. More...

virtual const double	muVBFHtautau (const double sqrt_s) const
	The ratio $\mu_{VBF,\tau\tau}$ between the VBF Higgs production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model. More...

virtual const double	muVBFHWW (const double sqrt_s) const
	The ratio $\mu_{VBF,WW}$ between the VBF Higgs production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model. More...

virtual const double	muVBFHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{VBF,WW\to 2l2\nu}$ between the VBF Higgs production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model. More...

virtual const double	muVBFHZga (const double sqrt_s) const
	The ratio $\mu_{VBF,Z\gamma}$ between the VBF Higgs production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model. More...

virtual const double	muVBFHZZ (const double sqrt_s) const
	The ratio $\mu_{VBF,ZZ}$ between the VBF Higgs production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model. More...

virtual const double	muVBFHZZ4l (const double sqrt_s) const
	The ratio $\mu_{VBF,ZZ\to 4l}$ between the VBF Higgs production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model. More...

virtual const double	muVBFpVH (const double sqrt_s) const
	The ratio $\mu_{VBF+VH}$ between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model. More...

virtual const double	muVH (const double sqrt_s) const
	The ratio $\mu_{VH}$ between the WH+ZH associated production cross-section in the current model and in the Standard Model. More...

virtual const double	muVHbb (const double sqrt_s) const
	The ratio $\mu_{VH,bb}$ between the VH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model. More...

virtual const double	muVHgaga (const double sqrt_s) const
	The ratio $\mu_{VH,\gamma\gamma}$ between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...

virtual const double	muVHmumu (const double sqrt_s) const
	The ratio $\mu_{VH,\mu\mu}$ between the VH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model. More...

virtual const double	muVHpT250 (const double sqrt_s) const
	The ratio $\mu_{VH}$ between the WH+ZH associated production cross-section in the current model and in the Standard Model, with $p_{T,H}>250$ GeV. More...

virtual const double	muVHtautau (const double sqrt_s) const
	The ratio $\mu_{VH,\tau\tau}$ between the VH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model. More...

virtual const double	muVHWW (const double sqrt_s) const
	The ratio $\mu_{VH,WW}$ between the VH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model. More...

virtual const double	muVHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{VH,WW\to 2l2\nu}$ between the VH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model. More...

virtual const double	muVHZga (const double sqrt_s) const
	The ratio $\mu_{VH,Z\gamma}$ between the VH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model. More...

virtual const double	muVHZZ (const double sqrt_s) const
	The ratio $\mu_{VH,ZZ}$ between the VH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model. More...

virtual const double	muVHZZ4l (const double sqrt_s) const
	The ratio $\mu_{VH,ZZ\to 4l}$ between the VH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model. More...

virtual const double	muWH (const double sqrt_s) const
	The ratio $\mu_{WH}$ between the W-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	muWHbb (const double sqrt_s) const
	The ratio $\mu_{WH,bb}$ between the WH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model. More...

virtual const double	muWHgaga (const double sqrt_s) const
	The ratio $\mu_{WH,\gamma\gamma}$ between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...

virtual const double	muWHmumu (const double sqrt_s) const
	The ratio $\mu_{WH,\mu\mu}$ between the WH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model. More...

virtual const double	muWHpT250 (const double sqrt_s) const
	The ratio $\mu_{WH}$ between the W-Higgs associated production cross-section in the current model and in the Standard Model, with $p_{T,H}>250$ GeV. More...

virtual const double	muWHtautau (const double sqrt_s) const
	The ratio $\mu_{WH,\tau\tau}$ between the WH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model. More...

virtual const double	muWHWW (const double sqrt_s) const
	The ratio $\mu_{WH,WW}$ between the WH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model. More...

virtual const double	muWHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{WH,WW\to 2l2\nu}$ between the WH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model. More...

virtual const double	muWHZga (const double sqrt_s) const
	The ratio $\mu_{WH,Z\gamma}$ between the WH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model. More...

virtual const double	muWHZZ (const double sqrt_s) const
	The ratio $\mu_{WH,ZZ}$ between the WH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model. More...

virtual const double	muWHZZ4l (const double sqrt_s) const
	The ratio $\mu_{WH,ZZ\to 4l}$ between the WH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model. More...

virtual const double	muZH (const double sqrt_s) const
	The ratio $\mu_{ZH}$ between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More...

virtual const double	muZHbb (const double sqrt_s) const
	The ratio $\mu_{ZH,bb}$ between the ZH production cross-section with subsequent decay into $bb$ in the current model and in the Standard Model. More...

virtual const double	muZHgaga (const double sqrt_s) const
	The ratio $\mu_{ZH,\gamma\gamma}$ between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...

virtual const double	muZHmumu (const double sqrt_s) const
	The ratio $\mu_{ZH,\mu\mu}$ between the ZH production cross-section with subsequent decay into $\mu\mu$ in the current model and in the Standard Model. More...

virtual const double	muZHpT250 (const double sqrt_s) const
	The ratio $\mu_{ZH}$ between the Z-Higgs associated production cross-section in the current model and in the Standard Model, with $p_{T,H}>250$ GeV. More...

virtual const double	muZHtautau (const double sqrt_s) const
	The ratio $\mu_{ZH,\tau\tau}$ between the ZH production cross-section with subsequent decay into $\tau\tau$ in the current model and in the Standard Model. More...

virtual const double	muZHWW (const double sqrt_s) const
	The ratio $\mu_{ZH,WW}$ between the ZH production cross-section with subsequent decay into $W W^*$ in the current model and in the Standard Model. More...

virtual const double	muZHWW2l2v (const double sqrt_s) const
	The ratio $\mu_{ZH,WW\to 2l2\nu}$ between the ZH production cross-section with subsequent decay into $W W^*\to 2l2\nu$ in the current model and in the Standard Model. More...

virtual const double	muZHZga (const double sqrt_s) const
	The ratio $\mu_{ZH,Z\gamma}$ between the ZH production cross-section with subsequent decay into $Z \gamma$ in the current model and in the Standard Model. More...

virtual const double	muZHZZ (const double sqrt_s) const
	The ratio $\mu_{ZH,ZZ}$ between the ZH production cross-section with subsequent decay into $Z Z^*$ in the current model and in the Standard Model. More...

virtual const double	muZHZZ4l (const double sqrt_s) const
	The ratio $\mu_{ZH,ZZ\to 4l}$ between the ZH production cross-section with subsequent decay into $Z Z^*\to 4l$ in the current model and in the Standard Model. More...

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

virtual const double	NevLHCppee13 (const int i_bin) const
	Number of di-electron events at the LHC at 13 TeV. More...

virtual const double	NevLHCppenu13 (const int i_bin) const
	Number of mono-electron events at the LHC at 13 TeV. More...

virtual const double	NevLHCppmumu13 (const int i_bin) const
	Number of di-muon events at the LHC at 13 TeV. More...

virtual const double	NevLHCppmunu13 (const int i_bin) const
	Number of mono-muon events at the LHC at 13 TeV. More...

virtual const double	NevLHCpptaunu13 (const int i_bin) const
	Number of mono-tau events at the LHC at 13 TeV. More...

virtual const double	NevLHCpptautau13 (const int i_bin) const
	Number of di-tau events at the LHC at 13 TeV. More...

	NPSMEFTd6General ()
	Constructor. More...

virtual const double	obliqueS () const
	The oblique parameter $S$. (Simplified implementation. Contribution only from $O_{HWB}$.) More...

virtual const double	obliqueT () const
	The oblique parameter $T$. (Simplified implementation. Contribution only from $O_{HD}$.) More...

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

virtual const double	obliqueW () const
	The oblique parameter $W$. (Simplified implementation. Contribution only from $O_{2W}$.) More...

virtual const double	obliqueY () const
	The oblique parameter $Y$. (Simplified implementation. Contribution only from $O_{2B}$.) More...

virtual const double	ppZHprobe (const double sqrt_s) const
	The direction constrained by $ p p \to Z H$ in the boosted regime, $g_p^Z$. From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6General class. More...

virtual bool	PreUpdate ()
	The pre-update method for NPSMEFTd6General. More...

void	printNonVanishingSMEFTCoeffEW () const

virtual const double	R0_f (const Particle f) const
	The ratio $R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell$, $R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}$ and $R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}$, for charged leptons, quarks and neutrinos, respectively. More...

virtual const double	RWc () const
	The ratio $R_{W,c)=\Gamma(W\to c + X)/\Gamma(W\to had)$. More...

virtual const double	RWlilj (const Particle li, const Particle lj) const
	The lepton universality ratio $R_{W,l_i/l_j)=\Gamma(W\to l_i \nu_i)/\Gamma(W\to l_j \nu_j)$. More...

virtual const double	RZlilj (const Particle li, const Particle lj) const
	The lepton universality ratio $R_{Z,l_i/l_j)=\Gamma(Z\to l_i^+ l_i^-)/\Gamma(Z\to l_j^+ l_j^-)$. More...

virtual bool	setFlag (const std::string name, const bool value)
	A method to check if all the mandatory parameters for NPSMEFTd6General have been provided in model initialization. More...

virtual bool	setFlagStr (const std::string name, const std::string value)
	A method to set a flag of NPSMEFTd6General. More...

virtual const double	sigma0_had () const
	The cross section for the process $e^+ e^-\to Z\to \mathrm{hadrons}$ at the $Z$ pole, $\sigma_h^0$. More...

virtual const double	STXS0_qqH (const double sqrt_s) const
	The STXS0 bin $pp \to H qq$. More...

virtual const double	STXS12_BrH4lRatio () const
	The STXS BR $ H \to 4l $, $l=e,\mu$. More...

virtual const double	STXS12_BrHbbRatio () const
	The STXS BR $ H \to bb $. More...

virtual const double	STXS12_BrHevmuvRatio () const
	The STXS BR $ H \to e\nu \mu\nu $. More...

virtual const double	STXS12_BrHgagaRatio () const
	The STXS BR $ H \to \gamma \gamma $. More...

virtual const double	STXS12_ggH_mjj0_350_pTH0_60_Nj1 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 1,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60$. More...

virtual const double	STXS12_ggH_mjj0_350_pTH0_60_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60$. More...

virtual const double	STXS12_ggH_mjj0_350_pTH120_200_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~m_{jj}[GeV]<350,~120<p_{TH} [GeV]<200$. More...

virtual const double	STXS12_ggH_mjj0_350_pTH60_120_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~m_{jj}[GeV]<350,~60<p_{TH} [GeV]<120$. More...

virtual const double	STXS12_ggH_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~<p_{TH} [GeV]<200$. More...

virtual const double	STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25$. More...

virtual const double	STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]$. More...

virtual const double	STXS12_ggH_mjj700_Inf_pTH0_200_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200$. More...

virtual const double	STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25$. More...

virtual const double	STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]$. More...

virtual const double	STXS12_ggH_pTH0_10_Nj0 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j=0,~p_{TH} [GeV]<10$. More...

virtual const double	STXS12_ggH_pTH0_60_Nj1 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j = 1,~p_{TH} [GeV]<60$. More...

virtual const double	STXS12_ggH_pTH10_200_Nj0 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j=0,~p_{TH} [GeV]<10$. More...

virtual const double	STXS12_ggH_pTH10_Inf_Nj0 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j=0,~10<p_{TH} [GeV]$. More...

virtual const double	STXS12_ggH_pTH120_200_Nj1 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j = 1,~120<p_{TH} [GeV]<200$. More...

virtual const double	STXS12_ggH_pTH200_300 (const double sqrt_s) const
	The STXS bin $gg \to H$, $,200<~p_{TH} [GeV]<300$. More...

virtual const double	STXS12_ggH_pTH200_300_Nj01 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j\leq 1,~200<p_{TH} [GeV]<300$. More...

virtual const double	STXS12_ggH_pTH300_450 (const double sqrt_s) const
	The STXS bin $gg \to H$, $,300<~p_{TH} [GeV]<450$. More...

virtual const double	STXS12_ggH_pTH300_450_Nj01 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j\leq 1,~300<p_{TH} [GeV]<450$. More...

virtual const double	STXS12_ggH_pTH450_650 (const double sqrt_s) const
	The STXS bin $gg \to H$, $450<~p_{TH} [GeV]<650$. More...

virtual const double	STXS12_ggH_pTH450_650_Nj01 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j\leq 1,~450<p_{TH} [GeV]<650$. More...

virtual const double	STXS12_ggH_pTH450_Inf (const double sqrt_s) const
	The STXS bin $gg \to H$, $,450<~p_{TH} [GeV]$. More...

virtual const double	STXS12_ggH_pTH60_120_Nj1 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j = 1,~60<p_{TH} [GeV]<120$. More...

virtual const double	STXS12_ggH_pTH650_Inf (const double sqrt_s) const
	The STXS bin $gg \to H$, $~p_{TH} [GeV]>650$. More...

virtual const double	STXS12_ggH_pTH650_Inf_Nj01 (const double sqrt_s) const
	The STXS bin $gg \to H$, $N_j\leq 1,650<p_{TH} [GeV]$. More...

virtual const double	STXS12_ggHll_pTV0_75 (const double sqrt_s) const
	The STXS bin $gg \to H\ell\ell$, $p_{TV}[GeV]<75$. More...

virtual const double	STXS12_ggHll_pTV150_250_Nj0 (const double sqrt_s) const
	The STXS bin $gg \to H\ell\ell$, $N_j = 0,~150<p_{TV}[GeV]<250$. More...

virtual const double	STXS12_ggHll_pTV150_250_Nj1 (const double sqrt_s) const
	The STXS bin $gg \to H\ell\ell$, $N_j = 1,~150<p_{TV}[GeV]<250$. More...

virtual const double	STXS12_ggHll_pTV250_Inf (const double sqrt_s) const
	The STXS bin $gg \to H\ell\ell$, $250 < p_{TV}[GeV]$. More...

virtual const double	STXS12_ggHll_pTV75_150 (const double sqrt_s) const
	The STXS bin $gg \to H\ell\ell$, $75<p_{TV}[GeV]<150$. More...

virtual const double	STXS12_qqHll_pTV0_150 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $0<p_{TV}<150[GeV]$. More...

virtual const double	STXS12_qqHll_pTV0_75 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $p_{TV}[GeV]<75$. More...

virtual const double	STXS12_qqHll_pTV150_250_Nj0 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $N_j = 0,~150<p_{TV}[GeV]<250$. More...

virtual const double	STXS12_qqHll_pTV150_250_Nj1 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $N_j \geq 1,~150<p_{TV}[GeV]<250$. More...

virtual const double	STXS12_qqHll_pTV250_400 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $250<p_{TV}<400[GeV]$. More...

virtual const double	STXS12_qqHll_pTV250_Inf (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $250<p_{TV}[GeV]$. More...

virtual const double	STXS12_qqHll_pTV400_Inf (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $400<p_{TV}[GeV]$. More...

virtual const double	STXS12_qqHll_pTV75_150 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\ell$, $75<p_{TV}[GeV]<150$. More...

virtual const double	STXS12_qqHlv_pTV0_150 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $0<p_{TV}<150[GeV]$. More...

virtual const double	STXS12_qqHlv_pTV0_75 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $p_{TV}[GeV]<75$. More...

virtual const double	STXS12_qqHlv_pTV150_250_Nj0 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $N_j = 0,~150<p_{TV}[GeV]<250$. More...

virtual const double	STXS12_qqHlv_pTV150_250_Nj1 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $N_j \geq 1,~150<p_{TV}[GeV]<250$. More...

virtual const double	STXS12_qqHlv_pTV250_400 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $250<p_{TV}<400[GeV]$. More...

virtual const double	STXS12_qqHlv_pTV250_Inf (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $250<p_{TV}[GeV]$. More...

virtual const double	STXS12_qqHlv_pTV400_Inf (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $400<p_{TV}[GeV]$. More...

virtual const double	STXS12_qqHlv_pTV75_150 (const double sqrt_s) const
	The STXS bin $qq \to H\ell\nu$, $75<p_{TV}[GeV]<150$. More...

virtual const double	STXS12_qqHqq_mjj0_60_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~m_{jj}[GeV]<60$. More...

virtual const double	STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~1000<m_{jj}[GeV]<1500,~p_{TH}[GeV]<200$. More...

virtual const double	STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~1000<m_{jj}[GeV],~p_{TH}[GeV]>200$. More...

virtual const double	STXS12_qqHqq_mjj120_350_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~120<m_{jj}[GeV]<350$. More...

virtual const double	STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~1500<m_{jj}[GeV],~p_{TH}[GeV]<200$. More...

virtual const double	STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV]<1000,~p_{TH}[GeV]>200$. More...

virtual const double	STXS12_qqHqq_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200$. More...

virtual const double	STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25$. More...

virtual const double	STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]$. More...

virtual const double	STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~350<m_{jj}[GeV],~200<p_{TH}[GeV]$. More...

virtual const double	STXS12_qqHqq_mjj60_120_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~60<m_{jj}[GeV]<120$. More...

virtual const double	STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~700<m_{jj}[GeV]<1000,~p_{TH}[GeV]<200$. More...

virtual const double	STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25$. More...

virtual const double	STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]$. More...

virtual const double	STXS12_qqHqq_Nj0 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j = 0$. More...

virtual const double	STXS12_qqHqq_Nj1 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j = 1$. More...

virtual const double	STXS12_qqHqq_VH_veto_Nj01 (const double sqrt_s) const
	The STXS bin $qq \to Hqq$, $N_j = 0,1$ VH-veto Ref. 2402.05742. More...

virtual const double	STXS12_tH (const double sqrt_s) const
	The STXS bin $pp \to tH$. More...

virtual const double	STXS12_ttH_pTH0_60 (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $p_{TH}[GeV]<60$. More...

virtual const double	STXS12_ttH_pTH120_200 (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $120<p_{TH}[GeV]<200$. More...

virtual const double	STXS12_ttH_pTH200_300 (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $200<p_{TH}[GeV]<300$. More...

virtual const double	STXS12_ttH_pTH300_450 (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $300<p_{TH}[GeV]<450$. More...

virtual const double	STXS12_ttH_pTH300_Inf (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $300<p_{TH}[GeV]$. More...

virtual const double	STXS12_ttH_pTH450_Inf (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $450<p_{TH}[GeV]$. More...

virtual const double	STXS12_ttH_pTH60_120 (const double sqrt_s) const
	The STXS bin $pp \to ttH$, $60<p_{TH}[GeV]<120$. More...

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

virtual const double	STXS_ZHqqHqq_VH2j (const double sqrt_s) const
	The STXS bin $ qq \to ZH \to H qq $. More...

const double	tovers2 (const double cosmin, const double cosmax) const

const double	uovers2 (const double cosmin, const double cosmax) const

double	xlog1 (const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const

double	xlog2 (const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const

double	xlog3 (const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const

double	xlog4 (const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const

double	xlog5 (const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const

virtual const double	xseeWW (const double sqrt_s) const
	Total $e^+ e^- \to W^+ W^- \to jj \ell \nu$ cross section in pb, with $\ell= e, \mu$. More...

virtual const double	xseeWW4fLEP2 (const double sqrt_s, const int fstate) const
	The cross section in pb for $e^+ e^- \to W^+ W^- \to 4f $, with $ 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) $ the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More...

virtual const double	xseeWWtotLEP2 (const double sqrt_s) const
	The total cross section in pb for $e^+ e^- \to W^+ W^-$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More...

Public Member Functions inherited from NPbase
virtual const double	alrmoller (const double q2, const double y) const

virtual const double	amuon () const

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

virtual const double	BrHlljjRatio () const
	The ratio of the Br $(H\to l l j j)$ ( $l=e,\mu,~~j\not=b$) in the current model and in the Standard Model. More...

virtual const double	C1eeHvv (const double sqrt_s) const
	The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...

virtual const double	C1eettH (const double sqrt_s) const
	The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...

virtual const double	C1eeWBF (const double sqrt_s) const
	The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...

virtual const double	C1eeZBF (const double sqrt_s) const
	The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...

virtual const double	C1eeZH (const double sqrt_s) const
	The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...

const double	C1Htot () const
	The C1 coefficient controlling the H^3 corrections to the total Higgs width from the Higgs trilinear coupling. More...

virtual const double	cbminuscc () const

virtual const double	cbminusctau () const

virtual const double	ccminusctau () const

virtual const double	cgaplusct () const

virtual const double	cgminuscga () const

virtual const double	cgplusct () const

virtual const double	cVpluscb () const

virtual const double	cVplusctau () const

virtual const double	deltaA_f_2 (const Particle f) const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the left-right asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $\Delta \mathcal{A}_f^{(2)}$. More...

virtual const double	deltaAFB_2 (const Particle f) const
	The $\mathcal{O}(\Lambda^{-4})$ new physics to the forward-backward asymmetry in $e^+e^-\to Z\to f \bar{f}$ at the $Z$-pole, $\Delta A^f_{FB}$. More...

virtual const double	deltaGA_f_2 (const Particle f) const

virtual const double	deltaGamma_Z_2 () const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the total decay width of the $Z$ boson, $\Delta \Gamma_Z^{(2)}$. More...

virtual const double	deltaGamma_Zf_2 (const Particle f) const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the decay width of the $Z$ boson into a given fermion pair, $\Delta \Gamma_{Z,f}^{(2)}$. More...

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

virtual const double	deltaGamma_Zhad_2 () const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the hadronic decay width of the $Z$ boson, $\Delta \Gamma_{Z,had}^{(2)}$. More...

const double	deltaGL_f_mu (const Particle p, const double mu) const
	New physics contribution to the neutral-current left-handed coupling $g_L^f$. More...

const double	deltaGR_f_mu (const Particle p, const double mu) const
	New physics contribution to the neutral-current right-handed coupling $g_R^f$. More...

virtual const double	deltaGV_f_2 (const Particle f) const

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

virtual const double	deltaR0_f_2 (const Particle f) const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the ratio $R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell$, $R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}$ and $R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}$, for charged leptons, quarks and neutrinos: More...

virtual const double	deltaR_inv () const
	The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the $Z$ boson, $\delta R_{inv}$. More...

virtual const double	deltaRuc () const
	The new physics contribution to the ratio of the $Z\to u\bar{u} + Z\to c\bar{c}$ width to the $Z$-boson hadronic width: More...

virtual const double	deltaRuc_2 () const
	The $\mathcal{O}(1/\Lambda^4)$ new physics contribution to the ratio of the $Z\to u\bar{u} + Z\to c\bar{c}$ width to the $Z$-boson hadronic width: More...

virtual const double	deltaSigmaHadron_2 () const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the cross section for the process $e^+ e^-\to Z\to \mathrm{hadrons}$ at the $Z$ pole, $\Delta \sigma_h^{0,(2)}$. More...

virtual const double	deltaSin2thetaEff_e () const
	The new physics contribution to the effective electron/leptonic weak angle $\delta \sin^2\theta_{\rm eff}^{\rm lept}$ at the $Z$ pole. More...

virtual const double	deltaSin2thetaEff_e_2 () const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the effective electron weak angle $\Delta \sin^2\theta_{eff,e}^{(2)}$ at the $Z$ pole. More...

virtual const double	deltaSin2thetaEff_mu () const
	The new physics contribution to the effective muonic weak angle $\delta \sin^2\theta_{\rm eff}^{\mu\mu}$ at the $Z$ pole. More...

virtual const double	deltaSin2thetaEff_mu_2 () const
	The $\mathcal{O}(\Lambda^{-4})$ new physics contribution to the effective muonic weak angle $\Delta \sin^2\theta_{eff, \mu}^{(2)}$ at the $Z$ pole. More...

virtual const double	deltaxseeWWhadLEP2 (const double sqrt_s) const
	The new physics contribution to the cross section in pb for $e^+ e^- \to W^+ W^- \to j j j j$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...

virtual const double	deltaxseeWWleptLEP2 (const double sqrt_s) const
	The new physics contribution to the cross section in pb for $e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...

virtual const double	deltaxseeWWsemilLEP2 (const double sqrt_s) const
	The new physics contribution to the cross section in pb for $e^+ e^- \to W^+ W^- \to \ell \nu j j$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...

virtual const double	eeffAFBbottom (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffAFBcharm (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffAFBe (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffAFBetsub (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffAFBmu (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffAFBstrange (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffAFBtau (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRbottom (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRcharm (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRelectron (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRelectrontsub (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRmuon (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRstrange (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffRtau (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaBottom (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaCharm (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaE (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaEtsub (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaHadron (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaMu (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaStrange (const double pol_e, const double pol_p, const double s) const

virtual const double	eeffsigmaTau (const double pol_e, const double pol_p, const double s) const

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

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

virtual const double	gAnue () const

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

virtual const double	gLnuN2 () const

virtual const double	gRnuN2 () const

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

virtual const double	gVnue () const

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

virtual const double	LEP2AFBbottom (const double s) const

virtual const double	LEP2AFBcharm (const double s) const

virtual const double	LEP2AFBe (const double s) const

virtual const double	LEP2AFBmu (const double s) const

virtual const double	LEP2AFBtau (const double s) const

virtual const double	LEP2dsigmadcosBinE (const double s, const double cos, const double cosmin, const double cosmax) const

virtual const double	LEP2dsigmadcosBinMu (const double s, const double cos, const double cosmin, const double cosmax) const

virtual const double	LEP2dsigmadcosBinTau (const double s, const double cos, const double cosmin, const double cosmax) const

virtual const double	LEP2dsigmadcosE (const double s, const double cos) const

virtual const double	LEP2dsigmadcosMu (const double s, const double cos) const

virtual const double	LEP2dsigmadcosTau (const double s, const double cos) const

virtual const double	LEP2Rbottom (const double s) const

virtual const double	LEP2Rcharm (const double s) const

virtual const double	LEP2sigmaBottom (const double s) const

virtual const double	LEP2sigmaCharm (const double s) const

virtual const double	LEP2sigmaE (const double s) const

virtual const double	LEP2sigmaHadron (const double s) const

virtual const double	LEP2sigmaMu (const double s) const

virtual const double	LEP2sigmaTau (const double s) const

virtual const double	muggHgagaInt (const double sqrt_s) const
	The ratio $\mu_{ggH,\gamma\gamma}$ between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259. More...

virtual const double	muggHpbbH_Hgaga (const double sqrt_s) const

virtual const double	muggHpbbH_Htautau (const double sqrt_s) const

virtual const double	muggHpbbH_HWW (const double sqrt_s) const

virtual const double	muggHpbbH_HZZ (const double sqrt_s) const

virtual const double	muggHpttHptHpbbH_Hmumu (const double sqrt_s) const

virtual const double	muggHpttHptHpbbH_HZga (const double sqrt_s) const

virtual const double	muggHpVBFpbbH_Hbb (const double sqrt_s) const

virtual const double	muppHmumu (const double sqrt_s) const

virtual const double	muppHZga (const double sqrt_s) const

virtual const double	mutHgaga (const double sqrt_s) const

virtual const double	muttHptH_Hbb (const double sqrt_s) const

virtual const double	muttHptH_Hgaga (const double sqrt_s) const

virtual const double	muttHptH_Hmumu (const double sqrt_s) const

virtual const double	muttHptH_Htautau (const double sqrt_s) const

virtual const double	muttHptH_HWW (const double sqrt_s) const

virtual const double	muttHptH_HZZ (const double sqrt_s) const

virtual const double	muVBFpVH_Hmumu (const double sqrt_s) const

virtual const double	muVBFpVH_HZga (const double sqrt_s) const

virtual const double	muVHcc (const double sqrt_s) const

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

	NPbase ()
	The default constructor. More...

virtual int	OutputOrder () const

virtual const double	Qwemoller (const double q2, const double y) const

virtual const double	Qwn () const

virtual const double	Qwp () const

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

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

virtual const double	Ruc () const
	The ratio of the $Z\to u\bar{u} + Z\to c\bar{c}$ width to the $Z$-boson hadronic width. More...

virtual const double	sigmaSM_ee (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const

virtual const double	sin2thetaEff (const Particle f) const
	The leptonic effective weak mixing angle $\sin^2\theta_{\rm eff}^{\rm lept}$ at the the $Z$ pole. More...

virtual const double	TauLFU_gmuge () const

virtual const double	TauLFU_gtauge () const

virtual const double	TauLFU_gtaugmu () const

virtual const double	TauLFU_gtaugmuK () const

virtual const double	TauLFU_gtaugmuPi () const

virtual bool	Update (const std::map< std::string, double > &DPars)
	The update method for NPbase. More...

virtual const double	UpperLimitZgammaA (const double sqrt_s) const

virtual const double	UpperLimitZgammaA13 (const double sqrt_s) const

virtual const double	UpperLimitZgammaC (const double sqrt_s) const

virtual const double	UpperLimitZgammaC13 (const double sqrt_s) const

virtual const double	xseeWWhadLEP2 (const double sqrt_s) const
	The cross section in pb for $e^+ e^- \to W^+ W^- \to j j j j$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...

virtual const double	xseeWWleptLEP2 (const double sqrt_s) const
	The cross section in pb for $e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...

virtual const double	xseeWWsemilLEP2 (const double sqrt_s) const
	The cross section in pb for $e^+ e^- \to W^+ W^- \to \ell \nu j j$, summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...

Public Member Functions inherited from StandardModel
gslpp::complex	AH_f (const double tau) const
	Fermionic loop function entering in the calculation of the effective $Hgg$ and $H\gamma\gamma$ couplings. More...

gslpp::complex	AH_W (const double tau) const
	W loop function entering in the calculation of the effective $H\gamma\gamma$ coupling. More...

gslpp::complex	AHZga_f (const double tau, const double lambda) const
	Fermionic loop function entering in the calculation of the effective $HZ\gamma$ coupling. More...

gslpp::complex	AHZga_W (const double tau, const double lambda) const
	W loop function entering in the calculation of the effective $HZ\gamma$ coupling. More...

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

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

const double	Als (const double mu, const int Nf_in, const orders order=FULLNLO) const
	Computes the running strong coupling $\alpha_s(\mu)$ with $N_f$ active flavours in the $\overline{\mathrm{MS}}$ scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...

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

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

const double	Alstilde5 (const double mu) const
	The value of $\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}$ at any scale $\mu$ with the number of flavours $n_f = 4$ and full EW corrections. More...

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

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

virtual const double	BrHtobb () const
	The Br $(H\to b \bar{b})$ in the Standard Model. More...

virtual const double	BrHtocc () const
	The Br $(H\to c \bar{c})$ in the Standard Model. More...

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

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

virtual const double	BrHtomumu () const
	The Br $(H\to \mu^+ \mu^-)$ in the Standard Model. More...

virtual const double	BrHtoss () const
	The Br $(H\to s \bar{s})$ in the Standard Model. More...

virtual const double	BrHtotautau () const
	The Br $(H\to \tau^+ \tau^-)$ in the Standard Model. More...

virtual const double	BrHtoWWstar () const
	The Br $(H\to W W^*)$ in the Standard Model. More...

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

virtual const double	BrHtoZZstar () const
	The Br $(H\to Z Z^*)$ in the Standard Model. More...

const double	c02 () const
	The square of the cosine of the weak mixing angle $c_0^2$ defined without weak radiative corrections. More...

virtual bool	CheckFlags () const
	A method to check the sanity of the set of model flags. More...

virtual bool	CheckParameters (const std::map< std::string, double > &DPars)
	A method to check if all the mandatory parameters for StandardModel have been provided in model initialization. More...

bool	checkSMparamsForEWPO ()
	A method to check whether the parameters relevant to the EWPO are updated. More...

const double	computeBrHto4f () const
	The Br $(H\to 4f)$ in the Standard Model. More...

const double	computeBrHto4l2 () const
	The Br $(H\to 4l)$ $l=e,\mu$ in the Standard Model. More...

const double	computeBrHto4l3 () const
	The Br $(H\to 4l)$ $l=e,\mu,\tau$ in the Standard Model. More...

const double	computeBrHto4q () const
	The Br $(H\to 4q)$ in the Standard Model. More...

const double	computeBrHto4v () const
	The Br $(H\to 4\nu)$ in the Standard Model. More...

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

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

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

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

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

const double	computeBrHtollvv2 () const
	The Br $(H\to l^+ l^- \nu \nu)$ $l=e,\mu$ in the Standard Model. More...

const double	computeBrHtollvv3 () const
	The Br $(H\to l^+ l^- \nu \nu)$ $l=e,\mu,\tau$ in the Standard Model. More...

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

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

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

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

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

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

void	ComputeDeltaR_rem (const double Mw_i, double DeltaR_rem[orders_EW_size]) const
	A method to collect $\Delta r_{\mathrm{rem}}$ computed via subclasses. More...

void	ComputeDeltaRho (const double Mw_i, double DeltaRho[orders_EW_size]) const
	A method to collect $\Delta\rho$ computed via subclasses. More...

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

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

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

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

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

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

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

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

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

const double	computeGammaHZga_WW () const
	The $W$ loop contribution to $H\to Z\gamma$ in the Standard Model. Currently it returns the value of tab 41 in ref. [Heinemeyer:2013tqa]. More...

const double	computeSigmabbH (const double sqrt_s) const
	The bbH production cross section in the Standard Model. More...

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

const double	computeSigmaggH_bb (const double sqrt_s) const
	The square of the bottom-quark contribution to the ggH cross section in the Standard Model. More...

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

const double	computeSigmaggH_tt (const double sqrt_s) const
	The square of the top-quark contribution to the ggH cross section in the Standard Model. More...

const double	computeSigmatHq (const double sqrt_s) const
	The tHq production cross section in the Standard Model. More...

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

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

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

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

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

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

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

virtual const double	cW2 () const

virtual const double	cW2 (const double Mw_i) const
	The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as $c_W^2$. More...

virtual const double	Dalpha5hMz () const
	The 5-quark contribution to the running of the em constant to the $Z$ pole. $\Delta\alpha_{had}^{(5)}(M_Z)$. More...

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

const double	DeltaAlphaL5q () const
	The sum of the leptonic and the five-flavour hadronic corrections to the electromagnetic coupling $\alpha$ at the $Z$-mass scale, denoted as $\Delta\alpha^{\ell+5q}(M_Z^2)$. More...

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

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

virtual const gslpp::complex	deltaKappaZ_f (const Particle f) const
	Flavour non-universal vertex corrections to $\kappa_Z^l$, denoted by $\Delta\kappa_Z^l$. More...

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

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

virtual const gslpp::complex	deltaRhoZ_f (const Particle f) const
	Flavour non-universal vertex corrections to $\rho_Z^l$, denoted by $\Delta\rho_Z^l$. More...

const double	eeffsigma (const Particle f, const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const

const double	eeffsigmaEbin (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const

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

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

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

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

gslpp::complex	f_triangle (const double tau) const
	Loop function entering in the calculation of the effective $Hgg$ and $H\gamma\gamma$ couplings. More...

gslpp::complex	g_triangle (const double tau) const
	Loop function entering in the calculation of the effective $HZ\gamma$ coupling. More...

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

virtual const double	Gamma_muon () const
	The computation of the muon decay. More...

virtual const double	Gamma_tau_l_nunu (const Particle l) const
	The computation of the leptonic tau decays. More...

virtual const double	GammaHtobb () const
	The $\Gamma(H\to b \bar{b})$ in the Standard Model. More...

virtual const double	GammaHtocc () const
	The $\Gamma(H\to c \bar{c})$ in the Standard Model. More...

virtual const double	GammaHtogaga () const
	The $\Gamma(H\to \gamma \gamma)$ in the Standard Model. More...

virtual const double	GammaHtogg () const
	The $\Gamma(H\to gg)$ in the Standard Model. More...

virtual const double	GammaHtomumu () const
	The $\Gamma(H\to \mu^+ \mu^-)$ in the Standard Model. More...

virtual const double	GammaHtoss () const
	The $\Gamma(H\to s \bar{s})$ in the Standard Model. More...

virtual const double	GammaHTot () const
	The total Higgs width $\Gamma(H)$ in the Standard Model. More...

virtual const double	GammaHtotautau () const
	The $\Gamma(H\to \tau^+ \tau^-)$ in the Standard Model. More...

virtual const double	GammaHtoWWstar () const
	The $\Gamma(H\to W W^*)$ in the Standard Model. More...

virtual const double	GammaHtoZga () const
	The $\Gamma(H\to Z \gamma)$ in the Standard Model. More...

virtual const double	GammaHtoZZstar () const
	The $\Gamma(H\to Z Z^*)$ in the Standard Model. More...

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

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

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

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

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

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

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

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

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

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

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

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

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

const double	getDAle5Mz () const
	A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, $\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)$. More...

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

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

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

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

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

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

const double	getDelSin2th_b () const
	A get method to retrieve the theoretical uncertainty in $\sin^2\theta_{\rm eff}^{b}$, denoted as $\delta\sin^2\theta_{\rm eff}^{b}$. More...

const double	getDelSin2th_l () const
	A get method to retrieve the theoretical uncertainty in $\sin^2\theta_{\rm eff}^{\rm lept}$, denoted as $\delta\sin^2\theta_{\rm eff}^{\rm lept}$. More...

const double	getDelSin2th_q () const
	A get method to retrieve the theoretical uncertainty in $\sin^2\theta_{\rm eff}^{q\not = b,t}$, denoted as $\delta\sin^2\theta_{\rm eff}^{q\not = b,t}$. More...

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

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

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

const Flavour &	getFlavour () const

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

const int	getIterationNo () const

const Particle &	getLeptons (const QCD::lepton p) const
	A get method to retrieve the member object of a lepton. More...

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

virtual const double	getmq (const QCD::quark q, const double mu) const
	The MSbar running quark mass computed at NLO. More...

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

const double	getMw () const
	A get method to access the input value of the mass of the $W$ boson $M_W$. More...

EWSMApproximateFormulae *	getMyApproximateFormulae () const
	A get method to retrieve the member pointer of type EWSMApproximateFormulae. More...

EWSMcache *	getMyEWSMcache () const
	A get method to retrieve the member pointer of type EWSMcache. More...

LeptonFlavour *	getMyLeptonFlavour () const

EWSMOneLoopEW *	getMyOneLoopEW () const
	A get method to retrieve the member pointer of type EWSMOneLoopEW,. More...

EWSMThreeLoopEW *	getMyThreeLoopEW () const

EWSMThreeLoopEW2QCD *	getMyThreeLoopEW2QCD () const

EWSMThreeLoopQCD *	getMyThreeLoopQCD () const

EWSMTwoFermionsLEP2 *	getMyTwoFermionsLEP2 () const
	A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More...

EWSMTwoLoopEW *	getMyTwoLoopEW () const

EWSMTwoLoopQCD *	getMyTwoLoopQCD () const

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

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

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

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

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

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

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

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

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

gslpp::complex	I_triangle_1 (const double tau, const double lambda) const
	Loop function entering in the calculation of the effective $HZ\gamma$ coupling. More...

gslpp::complex	I_triangle_2 (const double tau, const double lambda) const
	Loop function entering in the calculation of the effective $HZ\gamma$ coupling. More...

virtual bool	InitializeModel ()
	A method to initialize the model. More...

const double	intMLL2eeeeus2 (const double s, const double t0, const double t1) const

const double	intMLR2eeeets2 (const double s, const double t0, const double t1) const

const double	intMLRtilde2eeeest2 (const double s, const double t0, const double t1) const

const double	intMRR2eeeeus2 (const double s, const double t0, const double t1) const

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

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

const bool	isSMSuccess () const
	A get method to retrieve the success status of the Standard Model update and matching. More...

const double	MLL2eeff (const Particle f, const double s, const double t) const

const double	MLR2eeff (const Particle f, const double s) const

const double	MRL2eeff (const Particle f, const double s) const

const double	MRR2eeff (const Particle f, const double s, const double t) const

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

const double	MwbarFromMw (const double Mw) const
	A method to convert the $W$-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More...

const double	MwFromMwbar (const double Mwbar) const
	A method to convert the $W$-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More...

double	Mzbar () const
	The $Z$-boson mass $\overline{M}_Z$ in the complex-pole/fixed-width scheme. More...

virtual const double	rho_GammaW (const Particle fi, const Particle fj) const
	EW radiative corrections to the width of $W \to f_i \bar{f}_j$, denoted as $\rho^W_{ij}$. More...

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

void	setCKM (const CKM &CKMMatrix)
	A set method to change the CKM matrix. More...

void	setFlagCacheInStandardModel (bool FlagCacheInStandardModel)
	A set method to change the model flag CacheInStandardModel of StandardModel. More...

void	setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ)

bool	setFlagSigmaForAFB (const bool flagSigmaForAFB_i)

bool	setFlagSigmaForR (const bool flagSigmaForR_i)

void	setRequireCKM (bool requireCKM)
	A set method to change the value of requireCKM. More...

void	setSMSuccess (bool success) const
	A set method to change the success status of the Standard Model update and matching. More...

void	setYd (const gslpp::matrix< gslpp::complex > &Yd)
	A set method to set the Yukawa matrix of the down-type quarks, $Y_d$. More...

void	setYe (const gslpp::matrix< gslpp::complex > &Ye)
	A set method to set the Yukawa matrix of the charged leptons, $Y_e$. More...

void	setYu (const gslpp::matrix< gslpp::complex > &Yu)
	A set method to set the Yukawa matrix of the up-type quarks, $Y_u$. More...

virtual const double	SigmaeeHee (const double sqrt_s, const double Pe, const double Pp) const
	The $\sigma(e^+ e^- \to e^+ e^- H)$ in the Standard Model. More...

virtual const double	SigmaeeHvv (const double sqrt_s, const double Pe, const double Pp) const
	The $\sigma(e^+ e^- \to \nu \bar{\nu} H)$ in the Standard Model. More...

virtual const double	SigmaeeZH (const double sqrt_s, const double Pe, const double Pp) const
	The $\sigma(e^+ e^- \to Z H)$ in the Standard Model. More...

	StandardModel ()
	The default constructor. More...

const double	sW2 () const

virtual const double	sW2 (const double Mw_i) const
	The square of the sine of the weak mixing angle in the on-shell scheme, denoted as $s_W^2$. More...

const double	sW2_MSbar_Approx () const
	The (approximated formula for the) square of the sine of the weak mixing angle in the MSbar scheme, denoted as $\hat{s}_{W}^2$. See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) More...

const double	sW2_ND () const
	The square of the sine of the weak mixing angle in the MSbar-ND scheme (w/o decoupling $\alpha\ln(m_t/M_Z)$ terms), denoted as $\hat{s}_{ND}^2$. See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) (eq. 10.13a/10.13b) More...

virtual const double	ThetaLnuN () const
	The effective neutrino nucleon LH parameter: ThetaLnuN. More...

virtual const double	ThetaRnuN () const
	The effective neutrino nucleon RH parameter: ThetaRnuN. More...

const double	tovers2 (const double cosmin, const double cosmax) const

const double	uovers2 (const double cosmin, const double cosmax) const

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

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

Public Member Functions inherited from QCD
const double	AboveTh (const double mu) const
	The active flavour threshold above the scale $\mu$ as defined in QCD::Thresholds(). More...

void	addParameters (std::vector< std::string > params_i)
	A method to add parameters that are specific to only one set of observables. More...

const double	Als (const double mu, const int Nf_in, const orders order=FULLNLO) const
	Computes the running strong coupling $\alpha_s(\mu)$ with $N_f$ active flavours in the $\overline{\mathrm{MS}}$ scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...

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

const double	Als4 (const double mu) const
	The value of $\alpha_s^{\mathrm{FULLNLO}}$ at any scale $\mu$ with the number of flavours $n_f = 4$. More...

const double	AlsByOrder (const double mu, const int Nf_in, const orders order=FULLNLO) const

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

const double	AlsOLD (const double mu, const orders order=FULLNLO) const
	Computes the running strong coupling $\alpha_s(\mu)$ in the $\overline{\mathrm{MS}}$ scheme. In the cases of LO, NLO and FULLNNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...

const double	AlsWithInit (const double mu, const double alsi, const double mu_i, const int nf, const orders order) const
	Computes the running strong coupling $\alpha_s(\mu)$ from $\alpha_s(\mu_i)$ in the $\overline{\mathrm{MS}}$ scheme, where it is forbidden to across a flavour threshold in the RG running from $\mu_i$ to $\mu$. More...

const double	AlsWithLambda (const double mu, const orders order) const
	Computes the running strong coupling $\alpha_s(\mu)$ in the $\overline{\mathrm{MS}}$ scheme with the use of $\Lambda_{\rm QCD}$. More...

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

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

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

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

const double	Beta3 (const double nf) const
	The $\beta_3(n_f)$ coefficient for a certain number of flavours $n_f$. More...

void	CacheShift (double cache[][5], int n) const
	A member used to manage the caching for this class. More...

void	CacheShift (int cache[][5], int n) const

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

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

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

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

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

const BParameter &	getBBd () const
	For getting the bag parameters corresponding to the operator basis $O_1 -O_5$ in $\Delta b = 2$ process in the $B_d$ meson system. More...

const BParameter &	getBBd_subleading () const
	For getting the subleading bag parameters $R_2 - R_3$ in $\Delta b = 2$ process in the $B_d$ meson system. More...

const BParameter &	getBBs () const
	For getting the bag parameters corresponding to the operator basis $O_1 -O_5$ in $\Delta b = 2$ process in the $B_s$ meson system. More...

const BParameter &	getBBs_subleading () const
	For getting the subleading bag parameters $R_2 - R_3$ in $\Delta b = 2$ process in the $B_s$ meson system. More...

const BParameter &	getBD () const
	For getting the bag parameters corresponding to the operator basis $O_1 -O_5$ in $\Delta c = 2$ process in the $D^0$ meson system. More...

const BParameter &	getBK () const
	For getting the bag parameters corresponding to the operator basis $O_1 -O_5$ in $\Delta s = 2$ process in the $K^0$ meson system. More...

const BParameter &	getBKd1 () const

const BParameter &	getBKd3 () const

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

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

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

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

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

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

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

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

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

const Particle &	getQuarks (const QCD::quark q) const
	A get method to access a quark as an object of the type Particle. More...

std::vector< std::string >	getUnknownParameters ()
	A method to get the vector of the parameters that have been specified in the configuration file but not being used. More...

void	initializeBParameter (std::string name_i) const
	A method to initialize B Parameter and the corresponding meson. More...

void	initializeMeson (QCD::meson meson_i) const
	A method to initialize a meson. More...

bool	isQCDsuccess () const
	A getter for the QCDsuccess flag. More...

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

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

const double	Mofmu2Mbar (const double m, const double mu, const quark q) const
	Converts a quark running mass at an arbitrary scale to the corresponding $\overline{\mathrm{MS}}$ mass $m(m)$. More...

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

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

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

const double	Mrun4 (const double mu_f, const double mu_i, const double m) const
	The running of a mass with the number of flavours $n_f = 4$. More...

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

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

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

const double	NfThresholdCorrections (double mu, double M, double als, int nf, orders order) const
	Threshold corrections in matching $\alpha_s(n_f+1)$ with $\alpha_s(n_f)$ from eq. (34) of hep-ph/0512060. More...

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

	QCD ()
	Constructor. More...

void	setComputemt (bool computemt)
	A set method to change the value of computemt. More...

void	setMtpole (double mtpole_in)
	A method to set the pole mass of the top quark. More...

void	setNc (double Nc)
	A set method to change the number of colours $N_c$. More...

void	setOptionalParameter (std::string name, double value)
	A method to set the parameter value for the parameters that are specific to only one set of observables. More...

void	setQuarkMass (const quark q, const double mass)
	A set method to change the mass of a quark. More...

const double	Thresholds (const int i) const
	For accessing the active flavour threshold scales. More...

Public Member Functions inherited from Model
void	addMissingModelParameter (const std::string &missingParameterName)

std::vector< std::string >	getmissingModelParameters ()

unsigned int	getMissingModelParametersCount ()

std::string	getModelName () const
	A method to fetch the name of the model. More...

const double &	getModelParam (std::string name) const

bool	isModelFWC_DF2 () const

bool	isModelGeneralTHDM () const

bool	isModelGeorgiMachacek () const

bool	IsModelInitialized () const
	A method to check if the model is initialized. More...

bool	isModelLinearized () const

bool	isModelNPquadratic () const

bool	isModelParam (std::string name) const

bool	isModelSUSY () const

bool	isModelTHDM () const

bool	isModelTHDMW () const

bool	IsUpdateError () const
	A method to check if there was any error in the model update process. More...

	Model ()
	The default constructor. More...

void	raiseMissingModelParameterCount ()

void	setModelFWC_DF2 ()

void	setModelGeneralTHDM ()

void	setModelGeorgiMachacek ()

void	setModelInitialized (bool ModelInitialized)
	A set method to fix the failure or success of the initialization of the model. More...

void	setModelLinearized (bool linearized=true)

void	setModelName (const std::string name)
	A method to set the name of the model. More...

void	setModelNPquadratic (bool NPquadratic=true)

void	setModelSUSY ()

void	setModelTHDM ()

void	setModelTHDMW ()

void	setSliced (bool Sliced)

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

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

Static Public Attributes
static const int	NNPSMEFTd6U3Vars = 41+1

static const std::string	NPSMEFTd6U3Vars [NNPSMEFTd6U3Vars]

Static Public Attributes inherited from NPSMEFTd6General
static const int	NNPSMEFTd6GeneralVars = 2708-208 + 79
	The number of the model parameters in NPSMEFTd6General (including the 18 parameters needed for the SM and 79 auxiliary parameters). More...

static const std::string	NPSMEFTd6GeneralVars [NNPSMEFTd6GeneralVars]
	A string array containing the labels of the model parameters in NPSMEFTd6General. 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
void	setNPSMEFTd6GeneralParameters ()
	An auxiliary method to set the WC of the general class. More...

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

Protected Member Functions inherited from NPSMEFTd6General
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	CfH_diag_mu (const Particle f, const double mu) 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...

void	ChangeToEvolutorsBasisPureSM ()
	This function computes the SM parameters needed for the evolutor, neglecting any NP contribution. More...

void	ChangeToEvolutorsBasisSMEFTtoSM ()
	This function computes the SM parameters needed for the evolutor, including a LO approximation to NP contributions where the Wilson coefficients are evaluated at the UV. 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...

gslpp::complex	CHF3CC_diag (const Particle F) const
	The diagonal entry of the dimension-6 operator coefficient $C_{HL,HQ}^{(3)}$ corresponding to charged-current modification, e.g. quarks u d (family diagonal). 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...

void	computeQuarkMassesAndCKMFromYukawas ()
	The method to compute the Yukawas matrix. More...

void	setSMEFTEvolWC (RGESolver &RGevol)
	An auxiliary method to set the WC on the evolutor. More...

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

const double	AFB_NoISR_q (const QCD::quark q_flavor, const double s) const

bool	checkEWPOscheme (const std::string scheme) const
	A method to check if a given scheme name in string form is valid. More...

virtual void	computeCKM ()
	The method to compute the CKM matrix. More...

virtual void	computeYukawas ()
	The method to compute the Yukawas matrix. More...

double	Delta_EWQCD (const QCD::quark q) const
	The non-factorizable EW-QCD corrections to the partial widths for $Z\to q\bar{q}$, denoted as $\Delta_{\mathrm{EW/QCD}}$. More...

const double	getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm133 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm167 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm172 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm183 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm189 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm192 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm196 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm200 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm202 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm205 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_charm207 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu130 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu136 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu161 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu172 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu183 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu189 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu192 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu196 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu200 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu202 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu205 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_mu207 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau130 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau136 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau161 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau172 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau183 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau189 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau192 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau196 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau200 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau202 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau205 (double x) const

const double	getIntegrand_AFBnumeratorWithISR_tau207 (double x) const

const double	getIntegrand_dsigmaBox_bottom130 (double x) const

const double	getIntegrand_dsigmaBox_bottom133 (double x) const

const double	getIntegrand_dsigmaBox_bottom136 (double x) const

const double	getIntegrand_dsigmaBox_bottom161 (double x) const

const double	getIntegrand_dsigmaBox_bottom167 (double x) const

const double	getIntegrand_dsigmaBox_bottom172 (double x) const

const double	getIntegrand_dsigmaBox_bottom183 (double x) const

const double	getIntegrand_dsigmaBox_bottom189 (double x) const

const double	getIntegrand_dsigmaBox_bottom192 (double x) const

const double	getIntegrand_dsigmaBox_bottom196 (double x) const

const double	getIntegrand_dsigmaBox_bottom200 (double x) const

const double	getIntegrand_dsigmaBox_bottom202 (double x) const

const double	getIntegrand_dsigmaBox_bottom205 (double x) const

const double	getIntegrand_dsigmaBox_bottom207 (double x) const

const double	getIntegrand_dsigmaBox_charm130 (double x) const

const double	getIntegrand_dsigmaBox_charm133 (double x) const

const double	getIntegrand_dsigmaBox_charm136 (double x) const

const double	getIntegrand_dsigmaBox_charm161 (double x) const

const double	getIntegrand_dsigmaBox_charm167 (double x) const

const double	getIntegrand_dsigmaBox_charm172 (double x) const

const double	getIntegrand_dsigmaBox_charm183 (double x) const

const double	getIntegrand_dsigmaBox_charm189 (double x) const

const double	getIntegrand_dsigmaBox_charm192 (double x) const

const double	getIntegrand_dsigmaBox_charm196 (double x) const

const double	getIntegrand_dsigmaBox_charm200 (double x) const

const double	getIntegrand_dsigmaBox_charm202 (double x) const

const double	getIntegrand_dsigmaBox_charm205 (double x) const

const double	getIntegrand_dsigmaBox_charm207 (double x) const

const double	getIntegrand_dsigmaBox_down130 (double x) const

const double	getIntegrand_dsigmaBox_down133 (double x) const

const double	getIntegrand_dsigmaBox_down136 (double x) const

const double	getIntegrand_dsigmaBox_down161 (double x) const

const double	getIntegrand_dsigmaBox_down167 (double x) const

const double	getIntegrand_dsigmaBox_down172 (double x) const

const double	getIntegrand_dsigmaBox_down183 (double x) const

const double	getIntegrand_dsigmaBox_down189 (double x) const

const double	getIntegrand_dsigmaBox_down192 (double x) const

const double	getIntegrand_dsigmaBox_down196 (double x) const

const double	getIntegrand_dsigmaBox_down200 (double x) const

const double	getIntegrand_dsigmaBox_down202 (double x) const

const double	getIntegrand_dsigmaBox_down205 (double x) const

const double	getIntegrand_dsigmaBox_down207 (double x) const

const double	getIntegrand_dsigmaBox_mu130 (double x) const

const double	getIntegrand_dsigmaBox_mu133 (double x) const

const double	getIntegrand_dsigmaBox_mu136 (double x) const

const double	getIntegrand_dsigmaBox_mu161 (double x) const

const double	getIntegrand_dsigmaBox_mu167 (double x) const

const double	getIntegrand_dsigmaBox_mu172 (double x) const

const double	getIntegrand_dsigmaBox_mu183 (double x) const

const double	getIntegrand_dsigmaBox_mu189 (double x) const

const double	getIntegrand_dsigmaBox_mu192 (double x) const

const double	getIntegrand_dsigmaBox_mu196 (double x) const

const double	getIntegrand_dsigmaBox_mu200 (double x) const

const double	getIntegrand_dsigmaBox_mu202 (double x) const

const double	getIntegrand_dsigmaBox_mu205 (double x) const

const double	getIntegrand_dsigmaBox_mu207 (double x) const

const double	getIntegrand_dsigmaBox_strange130 (double x) const

const double	getIntegrand_dsigmaBox_strange133 (double x) const

const double	getIntegrand_dsigmaBox_strange136 (double x) const

const double	getIntegrand_dsigmaBox_strange161 (double x) const

const double	getIntegrand_dsigmaBox_strange167 (double x) const

const double	getIntegrand_dsigmaBox_strange172 (double x) const

const double	getIntegrand_dsigmaBox_strange183 (double x) const

const double	getIntegrand_dsigmaBox_strange189 (double x) const

const double	getIntegrand_dsigmaBox_strange192 (double x) const

const double	getIntegrand_dsigmaBox_strange196 (double x) const

const double	getIntegrand_dsigmaBox_strange200 (double x) const

const double	getIntegrand_dsigmaBox_strange202 (double x) const

const double	getIntegrand_dsigmaBox_strange205 (double x) const

const double	getIntegrand_dsigmaBox_strange207 (double x) const

const double	getIntegrand_dsigmaBox_tau130 (double x) const

const double	getIntegrand_dsigmaBox_tau133 (double x) const

const double	getIntegrand_dsigmaBox_tau136 (double x) const

const double	getIntegrand_dsigmaBox_tau161 (double x) const

const double	getIntegrand_dsigmaBox_tau167 (double x) const

const double	getIntegrand_dsigmaBox_tau172 (double x) const

const double	getIntegrand_dsigmaBox_tau183 (double x) const

const double	getIntegrand_dsigmaBox_tau189 (double x) const

const double	getIntegrand_dsigmaBox_tau192 (double x) const

const double	getIntegrand_dsigmaBox_tau196 (double x) const

const double	getIntegrand_dsigmaBox_tau200 (double x) const

const double	getIntegrand_dsigmaBox_tau202 (double x) const

const double	getIntegrand_dsigmaBox_tau205 (double x) const

const double	getIntegrand_dsigmaBox_tau207 (double x) const

const double	getIntegrand_dsigmaBox_up130 (double x) const

const double	getIntegrand_dsigmaBox_up133 (double x) const

const double	getIntegrand_dsigmaBox_up136 (double x) const

const double	getIntegrand_dsigmaBox_up161 (double x) const

const double	getIntegrand_dsigmaBox_up167 (double x) const

const double	getIntegrand_dsigmaBox_up172 (double x) const

const double	getIntegrand_dsigmaBox_up183 (double x) const

const double	getIntegrand_dsigmaBox_up189 (double x) const

const double	getIntegrand_dsigmaBox_up192 (double x) const

const double	getIntegrand_dsigmaBox_up196 (double x) const

const double	getIntegrand_dsigmaBox_up200 (double x) const

const double	getIntegrand_dsigmaBox_up202 (double x) const

const double	getIntegrand_dsigmaBox_up205 (double x) const

const double	getIntegrand_dsigmaBox_up207 (double x) const

const double	getIntegrand_sigmaWithISR_bottom130 (double x) const

const double	getIntegrand_sigmaWithISR_bottom133 (double x) const

const double	getIntegrand_sigmaWithISR_bottom136 (double x) const

const double	getIntegrand_sigmaWithISR_bottom161 (double x) const

const double	getIntegrand_sigmaWithISR_bottom167 (double x) const

const double	getIntegrand_sigmaWithISR_bottom172 (double x) const

const double	getIntegrand_sigmaWithISR_bottom183 (double x) const

const double	getIntegrand_sigmaWithISR_bottom189 (double x) const

const double	getIntegrand_sigmaWithISR_bottom192 (double x) const

const double	getIntegrand_sigmaWithISR_bottom196 (double x) const

const double	getIntegrand_sigmaWithISR_bottom200 (double x) const

const double	getIntegrand_sigmaWithISR_bottom202 (double x) const

const double	getIntegrand_sigmaWithISR_bottom205 (double x) const

const double	getIntegrand_sigmaWithISR_bottom207 (double x) const

const double	getIntegrand_sigmaWithISR_charm130 (double x) const

const double	getIntegrand_sigmaWithISR_charm133 (double x) const

const double	getIntegrand_sigmaWithISR_charm136 (double x) const

const double	getIntegrand_sigmaWithISR_charm161 (double x) const

const double	getIntegrand_sigmaWithISR_charm167 (double x) const

const double	getIntegrand_sigmaWithISR_charm172 (double x) const

const double	getIntegrand_sigmaWithISR_charm183 (double x) const

const double	getIntegrand_sigmaWithISR_charm189 (double x) const

const double	getIntegrand_sigmaWithISR_charm192 (double x) const

const double	getIntegrand_sigmaWithISR_charm196 (double x) const

const double	getIntegrand_sigmaWithISR_charm200 (double x) const

const double	getIntegrand_sigmaWithISR_charm202 (double x) const

const double	getIntegrand_sigmaWithISR_charm205 (double x) const

const double	getIntegrand_sigmaWithISR_charm207 (double x) const

const double	getIntegrand_sigmaWithISR_down130 (double x) const

const double	getIntegrand_sigmaWithISR_down133 (double x) const

const double	getIntegrand_sigmaWithISR_down136 (double x) const

const double	getIntegrand_sigmaWithISR_down161 (double x) const

const double	getIntegrand_sigmaWithISR_down167 (double x) const

const double	getIntegrand_sigmaWithISR_down172 (double x) const

const double	getIntegrand_sigmaWithISR_down183 (double x) const

const double	getIntegrand_sigmaWithISR_down189 (double x) const

const double	getIntegrand_sigmaWithISR_down192 (double x) const

const double	getIntegrand_sigmaWithISR_down196 (double x) const

const double	getIntegrand_sigmaWithISR_down200 (double x) const

const double	getIntegrand_sigmaWithISR_down202 (double x) const

const double	getIntegrand_sigmaWithISR_down205 (double x) const

const double	getIntegrand_sigmaWithISR_down207 (double x) const

const double	getIntegrand_sigmaWithISR_mu130 (double x) const

const double	getIntegrand_sigmaWithISR_mu136 (double x) const

const double	getIntegrand_sigmaWithISR_mu161 (double x) const

const double	getIntegrand_sigmaWithISR_mu172 (double x) const

const double	getIntegrand_sigmaWithISR_mu183 (double x) const

const double	getIntegrand_sigmaWithISR_mu189 (double x) const

const double	getIntegrand_sigmaWithISR_mu192 (double x) const

const double	getIntegrand_sigmaWithISR_mu196 (double x) const

const double	getIntegrand_sigmaWithISR_mu200 (double x) const

const double	getIntegrand_sigmaWithISR_mu202 (double x) const

const double	getIntegrand_sigmaWithISR_mu205 (double x) const

const double	getIntegrand_sigmaWithISR_mu207 (double x) const

const double	getIntegrand_sigmaWithISR_strange130 (double x) const

const double	getIntegrand_sigmaWithISR_strange133 (double x) const

const double	getIntegrand_sigmaWithISR_strange136 (double x) const

const double	getIntegrand_sigmaWithISR_strange161 (double x) const

const double	getIntegrand_sigmaWithISR_strange167 (double x) const

const double	getIntegrand_sigmaWithISR_strange172 (double x) const

const double	getIntegrand_sigmaWithISR_strange183 (double x) const

const double	getIntegrand_sigmaWithISR_strange189 (double x) const

const double	getIntegrand_sigmaWithISR_strange192 (double x) const

const double	getIntegrand_sigmaWithISR_strange196 (double x) const

const double	getIntegrand_sigmaWithISR_strange200 (double x) const

const double	getIntegrand_sigmaWithISR_strange202 (double x) const

const double	getIntegrand_sigmaWithISR_strange205 (double x) const

const double	getIntegrand_sigmaWithISR_strange207 (double x) const

const double	getIntegrand_sigmaWithISR_tau130 (double x) const

const double	getIntegrand_sigmaWithISR_tau136 (double x) const

const double	getIntegrand_sigmaWithISR_tau161 (double x) const

const double	getIntegrand_sigmaWithISR_tau172 (double x) const

const double	getIntegrand_sigmaWithISR_tau183 (double x) const

const double	getIntegrand_sigmaWithISR_tau189 (double x) const

const double	getIntegrand_sigmaWithISR_tau192 (double x) const

const double	getIntegrand_sigmaWithISR_tau196 (double x) const

const double	getIntegrand_sigmaWithISR_tau200 (double x) const

const double	getIntegrand_sigmaWithISR_tau202 (double x) const

const double	getIntegrand_sigmaWithISR_tau205 (double x) const

const double	getIntegrand_sigmaWithISR_tau207 (double x) const

const double	getIntegrand_sigmaWithISR_up130 (double x) const

const double	getIntegrand_sigmaWithISR_up133 (double x) const

const double	getIntegrand_sigmaWithISR_up136 (double x) const

const double	getIntegrand_sigmaWithISR_up161 (double x) const

const double	getIntegrand_sigmaWithISR_up167 (double x) const

const double	getIntegrand_sigmaWithISR_up172 (double x) const

const double	getIntegrand_sigmaWithISR_up183 (double x) const

const double	getIntegrand_sigmaWithISR_up189 (double x) const

const double	getIntegrand_sigmaWithISR_up192 (double x) const

const double	getIntegrand_sigmaWithISR_up196 (double x) const

const double	getIntegrand_sigmaWithISR_up200 (double x) const

const double	getIntegrand_sigmaWithISR_up202 (double x) const

const double	getIntegrand_sigmaWithISR_up205 (double x) const

const double	getIntegrand_sigmaWithISR_up207 (double x) const

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

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

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

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

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

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

double	m_q (const QCD::quark q, const double mu, const orders order=FULLNLO) const

double	RAq (const QCD::quark q) const
	The radiator factor associated with the final-state QED and QCD corrections to the the axial-vector-current interactions, $R_A^q(M_Z^2)$. More...

double	resumKappaZ (const double DeltaRho[orders_EW_size], const double deltaKappa_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
	A method to compute the real part of the effetvive coupling $\kappa_Z^f$ from $\Delta\rho$, $\delta\rho_{\rm rem}^{f}$ and $\Delta r_{\mathrm{rem}}$. More...

double	resumMw (const double Mw_i, const double DeltaRho[orders_EW_size], const double DeltaR_rem[orders_EW_size]) const
	A method to compute the $W$-boson mass from $\Delta\rho$ and $\Delta r_{\mathrm{rem}}$. More...

double	resumRhoZ (const double DeltaRho[orders_EW_size], const double deltaRho_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
	A method to compute the real part of the effective coupling $\rho_Z^f$ from $\Delta\rho$, $\delta\rho_{\rm rem}^{f}$ and $\Delta r_{\mathrm{rem}}$. More...

double	RVh () const
	The singlet vector corrections to the hadronic $Z$-boson width, denoted as $R_V^h$. More...

double	RVq (const QCD::quark q) const
	The radiator factor associated with the final-state QED and QCD corrections to the the vector-current interactions, $R_V^q(M_Z^2)$. More...

double	SchemeToDouble (const std::string scheme) const
	A method to convert a given scheme name in string form into a floating-point number with double precision. More...

const double	sigma_NoISR_l (const QCD::lepton l_flavor, const double s) const

const double	sigma_NoISR_q (const QCD::quark q_flavor, const double s) const

double	taub () const
	Top-mass corrections to the $Zb\bar{b}$ vertex, denoted by $\tau_b$. More...

Protected Member Functions inherited from QCD
const double	MassOfNf (int nf) const
	The Mbar mass of the heaviest quark in the theory with Nf active flavour. More...

Protected Attributes
double	Cdd_aabb_LNP = 0.
	The dimension-6 operator coefficient $(C_{dd})_{ijkm}$ (Real part and pure real operator). More...

double	Cdd_abba_LNP = 0.
	The dimension-6 operator coefficient $(C_{dd})_{ijkm}$ (Real part and pure real operator). More...

double	Ced_LNP = 0.
	The dimension-6 operator coefficient $(C_{ed})_{ijkm}$ (Imaginary part). More...

double	Cee_LNP = 0.
	The dimension-6 operator coefficient $(C_{ee})_{ijkm}$ (Imaginary part). More...

double	Ceu_LNP = 0.
	The dimension-6 operator coefficient $(C_{eu})_{ijkm}$ (Real part and pure real operator). More...

double	CHd_LNP = 0.
	The dimension-6 operator coefficient $(C_{Hd})_{ij}$. More...

double	CHe_LNP = 0.
	The dimension-6 operator coefficient $(C_{He})_{ij}$. More...

double	CHl1_LNP = 0.
	The dimension-6 operator coefficient $(C_{HL}^{(1)})_{ij}$. More...

double	CHl3_LNP = 0.
	The dimension-6 operator coefficient $(C_{HL}^{(3)})_{ij}$. More...

double	CHq1_LNP = 0.
	The dimension-6 operator coefficient $(C_{HQ}^{(1)})_{ij}$. More...

double	CHq3_LNP = 0.
	The dimension-6 operator coefficient $(C_{HQ}^{(3)})_{ij}$. More...

double	CHu_LNP = 0.
	The dimension-6 operator coefficient $(C_{Hu})_{ij}$. More...

double	Cld_LNP = 0.
	The dimension-6 operator coefficient $(C_{ld})_{ijkm}$ (Real part and pure real operator). More...

double	Cle_LNP = 0.
	The dimension-6 operator coefficient $(C_{le})_{ijkm}$ (Real part and pure real operator). More...

double	Cll_aabb_LNP = 0.
	The dimension-6 operator coefficient $(C_{ll})_{ijkm}$ (Real part and pure real operator). More...

double	Cll_abba_LNP = 0.
	The dimension-6 operator coefficient $(C_{ll})_{ijkm}$ (Real part and pure real operator). More...

double	Clq1_LNP = 0.
	The dimension-6 operator coefficient $(C_{lq}^{(1)})_{ijkm}$ (Imaginary part). More...

double	Clq3_LNP = 0.
	The dimension-6 operator coefficient $(C_{lq}^{(3)})_{ijkm}$ (Real part and pure real operator). More...

double	Clu_LNP = 0.
	The dimension-6 operator coefficient $(C_{lu})_{ijkm}$ (Imaginary part). More...

double	Cqd1_LNP = 0.
	The dimension-6 operator coefficient $(C_{qd}^{(1)})_{ijkm}$ (Imaginary part). More...

double	Cqd8_LNP = 0.
	The dimension-6 operator coefficient $(C_{qd}^{(8)})_{ijkm}$ (Real part and pure real operator). More...

double	Cqe_LNP = 0.
	The dimension-6 operator coefficient $(C_{qe})_{ijkm}$ (Imaginary part). More...

double	Cqq1_aabb_LNP = 0.
	The dimension-6 operator coefficient $(C_{qq}^{(1)})_{ijkm}$ (Imaginary part). More...

double	Cqq1_abba_LNP = 0.
	The dimension-6 operator coefficient $(C_{qq}^{(1)})_{ijkm}$ (Imaginary part). More...

double	Cqq3_aabb_LNP = 0.
	The dimension-6 operator coefficient $(C_{qq}^{(3)})_{ijkm}$ (Real part and pure real operator). More...

double	Cqq3_abba_LNP = 0.
	The dimension-6 operator coefficient $(C_{qq}^{(3)})_{ijkm}$ (Real part and pure real operator). More...

double	Cqu1_LNP = 0.
	The dimension-6 operator coefficient $(C_{qu}^{(1)})_{ijkm}$ (Imaginary part). More...

double	Cqu8_LNP = 0.
	The dimension-6 operator coefficient $(C_{qu}^{(8)})_{ijkm}$ (Real part and pure real operator). More...

double	Cud1_LNP = 0.
	The dimension-6 operator coefficient $(C_{ud}^{(1)})_{ijkm}$ (Imaginary part). More...

double	Cud8_LNP = 0.
	The dimension-6 operator coefficient $(C_{ud}^{(8)})_{ijkm}$ (Real part and pure real operator). More...

double	Cuu_aabb_LNP = 0.
	The dimension-6 operator coefficient $(C_{uu})_{ijkm}$ (Imaginary part). More...

double	Cuu_abba_LNP = 0.
	The dimension-6 operator coefficient $(C_{uu})_{ijkm}$ (Imaginary part). More...

Protected Attributes inherited from NPSMEFTd6General
double	ai2G

double	ai3G

double	aiA

double	aiB

double	aiG

double	aiH

double	aiHB

double	aiHd

double	aiHe

double	aiHL

double	aiHQ

double	aiHu

double	aiHW

double	aipHL

double	aipHQ

double	aiT

double	aiu

double	aiuG

double	aiWW

double	aleMz
	The em constant at Mz. More...

double	BrHexo = 0.
	The branching ratio of exotic (not invisible) Higgs decays. More...

double	BrHinv = 0.
	The branching ratio of invisible Higgs decays. More...

double	C1Htotal
	The C1 coefficient controlling the H^3 corrections to the total Higgs width from the Higgs trilinear coupling. More...

double	cAsch

double	CdB_11i_LNP = 0.

double	CdB_11r_LNP = 0.

double	CdB_12i_LNP = 0.

double	CdB_12r_LNP = 0.

double	CdB_13i_LNP = 0.

double	CdB_13r_LNP = 0.

double	CdB_21i_LNP = 0.

double	CdB_21r_LNP = 0.

double	CdB_22i_LNP = 0.

double	CdB_22r_LNP = 0.

double	CdB_23i_LNP = 0.

double	CdB_23r_LNP = 0.

double	CdB_31i_LNP = 0.

double	CdB_31r_LNP = 0.

double	CdB_32i_LNP = 0.

double	CdB_32r_LNP = 0.

double	CdB_33i_LNP = 0.
	The dimension-6 operator coefficient $(C_{dB})_{ij}$ (Imaginary part). More...

double	CdB_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{dB})_{ij}$ (Real part and pure real operator). More...

double	CDB_LNP = 0
	The dimension-6 operator coefficient $C_{DB}$. More...

double	Cdd_1111r_LNP = 0.

double	Cdd_1112i_LNP = 0.

double	Cdd_1112r_LNP = 0.

double	Cdd_1113i_LNP = 0.

double	Cdd_1113r_LNP = 0.

double	Cdd_1122r_LNP = 0.

double	Cdd_1123i_LNP = 0.

double	Cdd_1123r_LNP = 0.

double	Cdd_1133r_LNP = 0.

double	Cdd_1212i_LNP = 0.

double	Cdd_1212r_LNP = 0.

double	Cdd_1213i_LNP = 0.

double	Cdd_1213r_LNP = 0.

double	Cdd_1221r_LNP = 0.

double	Cdd_1222i_LNP = 0.

double	Cdd_1222r_LNP = 0.

double	Cdd_1223i_LNP = 0.

double	Cdd_1223r_LNP = 0.

double	Cdd_1231i_LNP = 0.

double	Cdd_1231r_LNP = 0.

double	Cdd_1232i_LNP = 0.

double	Cdd_1232r_LNP = 0.

double	Cdd_1233i_LNP = 0.

double	Cdd_1233r_LNP = 0.

double	Cdd_1313i_LNP = 0.

double	Cdd_1313r_LNP = 0.

double	Cdd_1322i_LNP = 0.

double	Cdd_1322r_LNP = 0.

double	Cdd_1323i_LNP = 0.

double	Cdd_1323r_LNP = 0.

double	Cdd_1331r_LNP = 0.

double	Cdd_1332i_LNP = 0.

double	Cdd_1332r_LNP = 0.

double	Cdd_1333i_LNP = 0.

double	Cdd_1333r_LNP = 0.

double	Cdd_2222r_LNP = 0.

double	Cdd_2223i_LNP = 0.

double	Cdd_2223r_LNP = 0.

double	Cdd_2233r_LNP = 0.

double	Cdd_2323i_LNP = 0.

double	Cdd_2323r_LNP = 0.

double	Cdd_2332r_LNP = 0.

double	Cdd_2333i_LNP = 0.
	The dimension-6 operator coefficient $(C_{dd})_{ijkm}$ (Imaginary part). More...

double	Cdd_2333r_LNP = 0.

double	Cdd_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{dd})_{ijkm}$ (Real part and pure real operator). More...

double	CdG_11i_LNP = 0.

double	CdG_11r_LNP = 0.

double	CdG_12i_LNP = 0.

double	CdG_12r_LNP = 0.

double	CdG_13i_LNP = 0.

double	CdG_13r_LNP = 0.

double	CdG_21i_LNP = 0.

double	CdG_21r_LNP = 0.

double	CdG_22i_LNP = 0.

double	CdG_22r_LNP = 0.

double	CdG_23i_LNP = 0.

double	CdG_23r_LNP = 0.

double	CdG_31i_LNP = 0.

double	CdG_31r_LNP = 0.

double	CdG_32i_LNP = 0.

double	CdG_32r_LNP = 0.

double	CdG_33i_LNP = 0.
	The dimension-6 operator coefficient $(C_{dG})_{ij}$ (Imaginary part). More...

double	CdG_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{dG})_{ij}$ (Real part and pure real operator). More...

double	CdH_11i_LNP = 0.

double	CdH_11r_LNP = 0.

double	CdH_12i_LNP = 0.

double	CdH_12r_LNP = 0.

double	CdH_13i_LNP = 0.

double	CdH_13r_LNP = 0.

double	CdH_21i_LNP = 0.

double	CdH_21r_LNP = 0.

double	CdH_22i_LNP = 0.

double	CdH_22r_LNP = 0.

double	CdH_23i_LNP = 0.

double	CdH_23r_LNP = 0.

double	CdH_31i_LNP = 0.

double	CdH_31r_LNP = 0.

double	CdH_32i_LNP = 0.

double	CdH_32r_LNP = 0.

double	CdH_33i_LNP = 0.
	The dimension-6 operator coefficient $(C_{dH})_{ij}$ (Imaginary part). More...

double	CdH_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{dH})_{ij}$ (Real part and pure real operator). More...

double	CdW_11i_LNP = 0.

double	CdW_11r_LNP = 0.

double	CdW_12i_LNP = 0.

double	CdW_12r_LNP = 0.

double	CdW_13i_LNP = 0.

double	CdW_13r_LNP = 0.

double	CdW_21i_LNP = 0.

double	CdW_21r_LNP = 0.

double	CdW_22i_LNP = 0.

double	CdW_22r_LNP = 0.

double	CdW_23i_LNP = 0.

double	CdW_23r_LNP = 0.

double	CdW_31i_LNP = 0.

double	CdW_31r_LNP = 0.

double	CdW_32i_LNP = 0.

double	CdW_32r_LNP = 0.

double	CdW_33i_LNP = 0.
	The dimension-6 operator coefficient $(C_{dW})_{ij}$ (Imaginary part). More...

double	CdW_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{dW})_{ij}$ (Real part and pure real operator). More...

double	CDW_LNP = 0
	The dimension-6 operator coefficient $C_{DW}$. More...

double	CeB_11i_LNP = 0.

double	CeB_11r_LNP = 0.

double	CeB_12i_LNP = 0.

double	CeB_12r_LNP = 0.

double	CeB_13i_LNP = 0.

double	CeB_13r_LNP = 0.

double	CeB_21i_LNP = 0.

double	CeB_21r_LNP = 0.

double	CeB_22i_LNP = 0.

double	CeB_22r_LNP = 0.

double	CeB_23i_LNP = 0.

double	CeB_23r_LNP = 0.

double	CeB_31i_LNP = 0.

double	CeB_31r_LNP = 0.

double	CeB_32i_LNP = 0.

double	CeB_32r_LNP = 0.

double	CeB_33i_LNP = 0.
	The dimension-6 operator coefficient $(C_{eB})_{ij}$ (Imaginary part). More...

double	CeB_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{eB})_{ij}$ (Real part and pure real operator). More...

double	Ced_1111r_LNP = 0.

double	Ced_1112i_LNP = 0.

double	Ced_1112r_LNP = 0.

double	Ced_1113i_LNP = 0.

double	Ced_1113r_LNP = 0.

double	Ced_1122r_LNP = 0.

double	Ced_1123i_LNP = 0.

double	Ced_1123r_LNP = 0.

double	Ced_1133r_LNP = 0.

double	Ced_1211i_LNP = 0.

double	Ced_1211r_LNP = 0.

double	Ced_1212i_LNP = 0.

double	Ced_1212r_LNP = 0.

double	Ced_1213i_LNP = 0.

double	Ced_1213r_LNP = 0.

double	Ced_1221i_LNP = 0.

double	Ced_1221r_LNP = 0.

double	Ced_1222i_LNP = 0.

double	Ced_1222r_LNP = 0.

double	Ced_1223i_LNP = 0.

double	Ced_1223r_LNP = 0.

double	Ced_1231i_LNP = 0.

double	Ced_1231r_LNP = 0.

double	Ced_1232i_LNP = 0.

double	Ced_1232r_LNP = 0.

double	Ced_1233i_LNP = 0.

double	Ced_1233r_LNP = 0.

double	Ced_1311i_LNP = 0.

double	Ced_1311r_LNP = 0.

double	Ced_1312i_LNP = 0.

double	Ced_1312r_LNP = 0.

double	Ced_1313i_LNP = 0.

double	Ced_1313r_LNP = 0.

double	Ced_1321i_LNP = 0.

double	Ced_1321r_LNP = 0.

double	Ced_1322i_LNP = 0.

double	Ced_1322r_LNP = 0.

double	Ced_1323i_LNP = 0.

double	Ced_1323r_LNP = 0.

double	Ced_1331i_LNP = 0.

double	Ced_1331r_LNP = 0.

double	Ced_1332i_LNP = 0.

double	Ced_1332r_LNP = 0.

double	Ced_1333i_LNP = 0.

double	Ced_1333r_LNP = 0.

double	Ced_2211r_LNP = 0.

double	Ced_2212i_LNP = 0.

double	Ced_2212r_LNP = 0.

double	Ced_2213i_LNP = 0.

double	Ced_2213r_LNP = 0.

double	Ced_2222r_LNP = 0.

double	Ced_2223i_LNP = 0.

double	Ced_2223r_LNP = 0.

double	Ced_2233r_LNP = 0.

double	Ced_2311i_LNP = 0.

double	Ced_2311r_LNP = 0.

double	Ced_2312i_LNP = 0.

double	Ced_2312r_LNP = 0.

double	Ced_2313i_LNP = 0.

double	Ced_2313r_LNP = 0.

double	Ced_2321i_LNP = 0.

double	Ced_2321r_LNP = 0.

double	Ced_2322i_LNP = 0.

double	Ced_2322r_LNP = 0.

double	Ced_2323i_LNP = 0.

double	Ced_2323r_LNP = 0.

double	Ced_2331i_LNP = 0.

double	Ced_2331r_LNP = 0.

double	Ced_2332i_LNP = 0.

double	Ced_2332r_LNP = 0.

double	Ced_2333i_LNP = 0.

double	Ced_2333r_LNP = 0.

double	Ced_3311r_LNP = 0.

double	Ced_3312i_LNP = 0.

double	Ced_3312r_LNP = 0.

double	Ced_3313i_LNP = 0.

double	Ced_3313r_LNP = 0.

double	Ced_3322r_LNP = 0.

double	Ced_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{ed})_{ijkm}$ (Imaginary part). More...

double	Ced_3323r_LNP = 0.

double	Ced_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{ed})_{ijkm}$ (Real part and pure real operator). More...

double	Cee_1111r_LNP = 0.

double	Cee_1112i_LNP = 0.

double	Cee_1112r_LNP = 0.

double	Cee_1113i_LNP = 0.

double	Cee_1113r_LNP = 0.

double	Cee_1122r_LNP = 0.

double	Cee_1123i_LNP = 0.

double	Cee_1123r_LNP = 0.

double	Cee_1133r_LNP = 0.

double	Cee_1212i_LNP = 0.

double	Cee_1212r_LNP = 0.

double	Cee_1213i_LNP = 0.

double	Cee_1213r_LNP = 0.

double	Cee_1222i_LNP = 0.

double	Cee_1222r_LNP = 0.

double	Cee_1223i_LNP = 0.

double	Cee_1223r_LNP = 0.

double	Cee_1232i_LNP = 0.

double	Cee_1232r_LNP = 0.

double	Cee_1233i_LNP = 0.

double	Cee_1233r_LNP = 0.

double	Cee_1313i_LNP = 0.

double	Cee_1313r_LNP = 0.

double	Cee_1323i_LNP = 0.

double	Cee_1323r_LNP = 0.

double	Cee_1333i_LNP = 0.

double	Cee_1333r_LNP = 0.

double	Cee_2222r_LNP = 0.

double	Cee_2223i_LNP = 0.

double	Cee_2223r_LNP = 0.

double	Cee_2233r_LNP = 0.

double	Cee_2323i_LNP = 0.

double	Cee_2323r_LNP = 0.

double	Cee_2333i_LNP = 0.
	The dimension-6 operator coefficient $(C_{ee})_{ijkm}$ (Imaginary part). More...

double	Cee_2333r_LNP = 0.

double	Cee_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{ee})_{ijkm}$ (Real part and pure real operator). More...

double	CeH_11i_LNP = 0.

double	CeH_11r_LNP = 0.

double	CeH_12i_LNP = 0.

double	CeH_12r_LNP = 0.

double	CeH_13i_LNP = 0.

double	CeH_13r_LNP = 0.

double	CeH_21i_LNP = 0.

double	CeH_21r_LNP = 0.

double	CeH_22i_LNP = 0.

double	CeH_22r_LNP = 0.

double	CeH_23i_LNP = 0.

double	CeH_23r_LNP = 0.

double	CeH_31i_LNP = 0.

double	CeH_31r_LNP = 0.

double	CeH_32i_LNP = 0.

double	CeH_32r_LNP = 0.

double	CeH_33i_LNP = 0.
	The dimension-6 operator coefficient $(C_{eH})_{ij}$ (Imaginary part). More...

double	CeH_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{eH})_{ij}$ (Real part and pure real operator). More...

double	Ceu_1111r_LNP = 0.

double	Ceu_1112i_LNP = 0.

double	Ceu_1112r_LNP = 0.

double	Ceu_1113i_LNP = 0.

double	Ceu_1113r_LNP = 0.

double	Ceu_1122r_LNP = 0.

double	Ceu_1123i_LNP = 0.

double	Ceu_1123r_LNP = 0.

double	Ceu_1133r_LNP = 0.

double	Ceu_1211i_LNP = 0.

double	Ceu_1211r_LNP = 0.

double	Ceu_1212i_LNP = 0.

double	Ceu_1212r_LNP = 0.

double	Ceu_1213i_LNP = 0.

double	Ceu_1213r_LNP = 0.

double	Ceu_1221i_LNP = 0.

double	Ceu_1221r_LNP = 0.

double	Ceu_1222i_LNP = 0.

double	Ceu_1222r_LNP = 0.

double	Ceu_1223i_LNP = 0.

double	Ceu_1223r_LNP = 0.

double	Ceu_1231i_LNP = 0.

double	Ceu_1231r_LNP = 0.

double	Ceu_1232i_LNP = 0.

double	Ceu_1232r_LNP = 0.

double	Ceu_1233i_LNP = 0.

double	Ceu_1233r_LNP = 0.

double	Ceu_1311i_LNP = 0.

double	Ceu_1311r_LNP = 0.

double	Ceu_1312i_LNP = 0.

double	Ceu_1312r_LNP = 0.

double	Ceu_1313i_LNP = 0.

double	Ceu_1313r_LNP = 0.

double	Ceu_1321i_LNP = 0.

double	Ceu_1321r_LNP = 0.

double	Ceu_1322i_LNP = 0.

double	Ceu_1322r_LNP = 0.

double	Ceu_1323i_LNP = 0.

double	Ceu_1323r_LNP = 0.

double	Ceu_1331i_LNP = 0.

double	Ceu_1331r_LNP = 0.

double	Ceu_1332i_LNP = 0.

double	Ceu_1332r_LNP = 0.

double	Ceu_1333i_LNP = 0.

double	Ceu_1333r_LNP = 0.

double	Ceu_2211r_LNP = 0.

double	Ceu_2212i_LNP = 0.

double	Ceu_2212r_LNP = 0.

double	Ceu_2213i_LNP = 0.

double	Ceu_2213r_LNP = 0.

double	Ceu_2222r_LNP = 0.

double	Ceu_2223i_LNP = 0.

double	Ceu_2223r_LNP = 0.

double	Ceu_2233r_LNP = 0.

double	Ceu_2311i_LNP = 0.

double	Ceu_2311r_LNP = 0.

double	Ceu_2312i_LNP = 0.

double	Ceu_2312r_LNP = 0.

double	Ceu_2313i_LNP = 0.

double	Ceu_2313r_LNP = 0.

double	Ceu_2321i_LNP = 0.

double	Ceu_2321r_LNP = 0.

double	Ceu_2322i_LNP = 0.

double	Ceu_2322r_LNP = 0.

double	Ceu_2323i_LNP = 0.

double	Ceu_2323r_LNP = 0.

double	Ceu_2331i_LNP = 0.

double	Ceu_2331r_LNP = 0.

double	Ceu_2332i_LNP = 0.

double	Ceu_2332r_LNP = 0.

double	Ceu_2333i_LNP = 0.

double	Ceu_2333r_LNP = 0.

double	Ceu_3311r_LNP = 0.

double	Ceu_3312i_LNP = 0.

double	Ceu_3312r_LNP = 0.

double	Ceu_3313i_LNP = 0.

double	Ceu_3313r_LNP = 0.

double	Ceu_3322r_LNP = 0.

double	Ceu_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{eu})_{ijkm}$ (Imaginary part). More...

double	Ceu_3323r_LNP = 0.

double	Ceu_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{eu})_{ijkm}$ (Real part and pure real operator). More...

double	CeW_11i_LNP = 0.

double	CeW_11r_LNP = 0.

double	CeW_12i_LNP = 0.

double	CeW_12r_LNP = 0.

double	CeW_13i_LNP = 0.

double	CeW_13r_LNP = 0.

double	CeW_21i_LNP = 0.

double	CeW_21r_LNP = 0.

double	CeW_22i_LNP = 0.

double	CeW_22r_LNP = 0.

double	CeW_23i_LNP = 0.

double	CeW_23r_LNP = 0.

double	CeW_31i_LNP = 0.

double	CeW_31r_LNP = 0.

double	CeW_32i_LNP = 0.

double	CeW_32r_LNP = 0.

double	CeW_33i_LNP = 0.
	The dimension-6 operator coefficient $(C_{eW})_{ij}$ (Imaginary part). More...

double	CeW_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{eW})_{ij}$ (Real part and pure real operator). More...

double	CG_LNP = 0.
	The dimension-6 operator coefficient $C_{G}$. More...

double	CGtilde_LNP = 0.
	The dimension-6 operator coefficient $C_{\tilde{G}}$. More...

double	CH_LNP = 0.
	The dimension-6 operator coefficient $C_{H}$. More...

double	CHB_LNP = 0.
	The dimension-6 operator coefficient $C_{HB}$. More...

double	CHbox_LNP = 0.
	The dimension-6 operator coefficient $C_{H\Box}$. More...

double	CHBtilde_LNP = 0.
	The dimension-6 operator coefficient $C_{H\tilde{B}}$. More...

double	CHd_11r_LNP = 0.

double	CHd_12i_LNP = 0.

double	CHd_12r_LNP = 0.

double	CHd_13i_LNP = 0.

double	CHd_13r_LNP = 0.

double	CHd_22r_LNP = 0.

double	CHd_23i_LNP = 0.
	The dimension-6 operator coefficient $(C_{Hd})_{ij}$ (Imaginary part). More...

double	CHd_23r_LNP = 0.

double	CHd_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{Hd})_{ij}$ (Real part and pure real operator). More...

double	CHD_LNP = 0.
	The dimension-6 operator coefficient $C_{HD}$. More...

double	CHdEWbb = 0.
	CHd operators at the EW scale in the down-quark mass basis More...

double	CHdEWdd = 0.

double	CHdEWss = 0.

double	CHe_11r_LNP = 0.

double	CHe_12i_LNP = 0.

double	CHe_12r_LNP = 0.

double	CHe_13i_LNP = 0.

double	CHe_13r_LNP = 0.

double	CHe_22r_LNP = 0.

double	CHe_23i_LNP = 0.
	The dimension-6 operator coefficient $(C_{He})_{ij}$ (Imaginary part). More...

double	CHe_23r_LNP = 0.

double	CHe_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{He})_{ij}$ (Real part and pure real operator). More...

double	CHG_LNP = 0.
	The dimension-6 operator coefficient $C_{HG}$. More...

double	CHGtilde_LNP = 0.
	The dimension-6 operator coefficient $C_{H\tilde{G}}$. More...

double	CHl1_11r_LNP = 0.

double	CHl1_12i_LNP = 0.

double	CHl1_12r_LNP = 0.

double	CHl1_13i_LNP = 0.

double	CHl1_13r_LNP = 0.

double	CHl1_22r_LNP = 0.

double	CHl1_23i_LNP = 0.
	The dimension-6 operator coefficient $(C_{HL}^{(1)})_{ij}$ (Imaginary part). More...

double	CHl1_23r_LNP = 0.

double	CHl1_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{HL}^{(1)})_{ij}$ (Real part and pure real operator). More...

double	CHl3_11r_LNP = 0.

double	CHl3_12i_LNP = 0.

double	CHl3_12r_LNP = 0.

double	CHl3_13i_LNP = 0.

double	CHl3_13r_LNP = 0.

double	CHl3_22r_LNP = 0.

double	CHl3_23i_LNP = 0.
	The dimension-6 operator coefficient $(C_{HL}^{(3)})_{ij}$ (Imaginary part). More...

double	CHl3_23r_LNP = 0.

double	CHl3_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{HL}^{(3)})_{ij}$ (Real part and pure real operator). More...

double	CHq1_11r_LNP = 0.

double	CHq1_12i_LNP = 0.

double	CHq1_12r_LNP = 0.

double	CHq1_13i_LNP = 0.

double	CHq1_13r_LNP = 0.

double	CHq1_22r_LNP = 0.

double	CHq1_23i_LNP = 0.
	The dimension-6 operator coefficient $(C_{HQ}^{(1)})_{ij}$ (Imaginary part). More...

double	CHq1_23r_LNP = 0.

double	CHq1_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{HQ}^{(1)})_{ij}$ (Real part and pure real operator). More...

double	CHq1EWbb = 0.
	CHq1 operators at the EW scale in the down-quark mass basis More...

double	CHq1EWcc = 0.

double	CHq1EWdd = 0.

double	CHq1EWss = 0.

double	CHq1EWtt = 0.
	CHq1 operators at the EW scale in the up-quark mass basis. More...

double	CHq1EWuu = 0.

double	CHq3_11r_LNP = 0.

double	CHq3_12i_LNP = 0.

double	CHq3_12r_LNP = 0.

double	CHq3_13i_LNP = 0.

double	CHq3_13r_LNP = 0.

double	CHq3_22r_LNP = 0.

double	CHq3_23i_LNP = 0.
	The dimension-6 operator coefficient $(C_{HQ}^{(3)})_{ij}$ (Imaginary part). More...

double	CHq3_23r_LNP = 0.

double	CHq3_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{HQ}^{(3)})_{ij}$ (Real part and pure real operator). More...

double	CHq3EWbb = 0.
	CHq3 operators at the EW scale in the down-quark mass basis More...

double	CHq3EWcc = 0.

gslpp::complex	CHq3EWcs = gslpp::complex(0., 0., false)

double	CHq3EWdd = 0.

double	CHq3EWss = 0.

gslpp::complex	CHq3EWtb = gslpp::complex(0., 0., false)
	CHq3 operators at the EW scale in the up-down-quark mass basis More...

double	CHq3EWtt = 0.
	CHq3 operators at the EW scale in the up-quark mass basis. More...

gslpp::complex	CHq3EWud = gslpp::complex(0., 0., false)

double	CHq3EWuu = 0.

double	cHSM
	Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes. More...

double	CHu_11r_LNP = 0.

double	CHu_12i_LNP = 0.

double	CHu_12r_LNP = 0.

double	CHu_13i_LNP = 0.

double	CHu_13r_LNP = 0.

double	CHu_22r_LNP = 0.

double	CHu_23i_LNP = 0.
	The dimension-6 operator coefficient $(C_{Hu})_{ij}$ (Imaginary part). More...

double	CHu_23r_LNP = 0.

double	CHu_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{Hu})_{ij}$ (Real part and pure real operator). More...

double	CHud_11i_LNP = 0.

double	CHud_11r_LNP = 0.

double	CHud_12i_LNP = 0.

double	CHud_12r_LNP = 0.

double	CHud_13i_LNP = 0.

double	CHud_13r_LNP = 0.

double	CHud_21i_LNP = 0.

double	CHud_21r_LNP = 0.

double	CHud_22i_LNP = 0.

double	CHud_22r_LNP = 0.

double	CHud_23i_LNP = 0.

double	CHud_23r_LNP = 0.

double	CHud_31i_LNP = 0.

double	CHud_31r_LNP = 0.

double	CHud_32i_LNP = 0.

double	CHud_32r_LNP = 0.

double	CHud_33i_LNP = 0.
	The dimension-6 operator coefficient $(C_{Hud})_{ij}$ (Imaginary part). More...

double	CHud_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{Hud})_{ij}$ (Real part and pure real operator). More...

double	CHuEWcc = 0.

double	CHuEWtt = 0.
	CHu operators at the EW scale in the up-quark mass basis. More...

double	CHuEWuu = 0.

double	CHW_LNP = 0.
	The dimension-6 operator coefficient $C_{HW}$. More...

double	CHWB_LNP = 0.
	The dimension-6 operator coefficient $C_{HWB}$. More...

double	CHWtilde_LNP = 0.
	The dimension-6 operator coefficient $C_{H\tilde{W}}$. More...

double	CHWtildeB_LNP = 0.
	The dimension-6 operator coefficient $C_{H\tilde{W}B}$. More...

double	Cld_1111r_LNP = 0.

double	Cld_1112i_LNP = 0.

double	Cld_1112r_LNP = 0.

double	Cld_1113i_LNP = 0.

double	Cld_1113r_LNP = 0.

double	Cld_1122r_LNP = 0.

double	Cld_1123i_LNP = 0.

double	Cld_1123r_LNP = 0.

double	Cld_1133r_LNP = 0.

double	Cld_1211i_LNP = 0.

double	Cld_1211r_LNP = 0.

double	Cld_1212i_LNP = 0.

double	Cld_1212r_LNP = 0.

double	Cld_1213i_LNP = 0.

double	Cld_1213r_LNP = 0.

double	Cld_1221i_LNP = 0.

double	Cld_1221r_LNP = 0.

double	Cld_1222i_LNP = 0.

double	Cld_1222r_LNP = 0.

double	Cld_1223i_LNP = 0.

double	Cld_1223r_LNP = 0.

double	Cld_1231i_LNP = 0.

double	Cld_1231r_LNP = 0.

double	Cld_1232i_LNP = 0.

double	Cld_1232r_LNP = 0.

double	Cld_1233i_LNP = 0.

double	Cld_1233r_LNP = 0.

double	Cld_1311i_LNP = 0.

double	Cld_1311r_LNP = 0.

double	Cld_1312i_LNP = 0.

double	Cld_1312r_LNP = 0.

double	Cld_1313i_LNP = 0.

double	Cld_1313r_LNP = 0.

double	Cld_1321i_LNP = 0.

double	Cld_1321r_LNP = 0.

double	Cld_1322i_LNP = 0.

double	Cld_1322r_LNP = 0.

double	Cld_1323i_LNP = 0.

double	Cld_1323r_LNP = 0.

double	Cld_1331i_LNP = 0.

double	Cld_1331r_LNP = 0.

double	Cld_1332i_LNP = 0.

double	Cld_1332r_LNP = 0.

double	Cld_1333i_LNP = 0.

double	Cld_1333r_LNP = 0.

double	Cld_2211r_LNP = 0.

double	Cld_2212i_LNP = 0.

double	Cld_2212r_LNP = 0.

double	Cld_2213i_LNP = 0.

double	Cld_2213r_LNP = 0.

double	Cld_2222r_LNP = 0.

double	Cld_2223i_LNP = 0.

double	Cld_2223r_LNP = 0.

double	Cld_2233r_LNP = 0.

double	Cld_2311i_LNP = 0.

double	Cld_2311r_LNP = 0.

double	Cld_2312i_LNP = 0.

double	Cld_2312r_LNP = 0.

double	Cld_2313i_LNP = 0.

double	Cld_2313r_LNP = 0.

double	Cld_2321i_LNP = 0.

double	Cld_2321r_LNP = 0.

double	Cld_2322i_LNP = 0.

double	Cld_2322r_LNP = 0.

double	Cld_2323i_LNP = 0.

double	Cld_2323r_LNP = 0.

double	Cld_2331i_LNP = 0.

double	Cld_2331r_LNP = 0.

double	Cld_2332i_LNP = 0.

double	Cld_2332r_LNP = 0.

double	Cld_2333i_LNP = 0.

double	Cld_2333r_LNP = 0.

double	Cld_3311r_LNP = 0.

double	Cld_3312i_LNP = 0.

double	Cld_3312r_LNP = 0.

double	Cld_3313i_LNP = 0.

double	Cld_3313r_LNP = 0.

double	Cld_3322r_LNP = 0.

double	Cld_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{ld})_{ijkm}$ (Imaginary part). More...

double	Cld_3323r_LNP = 0.

double	Cld_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{ld})_{ijkm}$ (Real part and pure real operator). More...

double	Cle_1111r_LNP = 0.

double	Cle_1112i_LNP = 0.

double	Cle_1112r_LNP = 0.

double	Cle_1113i_LNP = 0.

double	Cle_1113r_LNP = 0.

double	Cle_1122r_LNP = 0.

double	Cle_1123i_LNP = 0.

double	Cle_1123r_LNP = 0.

double	Cle_1133r_LNP = 0.

double	Cle_1211i_LNP = 0.

double	Cle_1211r_LNP = 0.

double	Cle_1212i_LNP = 0.

double	Cle_1212r_LNP = 0.

double	Cle_1213i_LNP = 0.

double	Cle_1213r_LNP = 0.

double	Cle_1221i_LNP = 0.

double	Cle_1221r_LNP = 0.

double	Cle_1222i_LNP = 0.

double	Cle_1222r_LNP = 0.

double	Cle_1223i_LNP = 0.

double	Cle_1223r_LNP = 0.

double	Cle_1231i_LNP = 0.

double	Cle_1231r_LNP = 0.

double	Cle_1232i_LNP = 0.

double	Cle_1232r_LNP = 0.

double	Cle_1233i_LNP = 0.

double	Cle_1233r_LNP = 0.

double	Cle_1311i_LNP = 0.

double	Cle_1311r_LNP = 0.

double	Cle_1312i_LNP = 0.

double	Cle_1312r_LNP = 0.

double	Cle_1313i_LNP = 0.

double	Cle_1313r_LNP = 0.

double	Cle_1321i_LNP = 0.

double	Cle_1321r_LNP = 0.

double	Cle_1322i_LNP = 0.

double	Cle_1322r_LNP = 0.

double	Cle_1323i_LNP = 0.

double	Cle_1323r_LNP = 0.

double	Cle_1331i_LNP = 0.

double	Cle_1331r_LNP = 0.

double	Cle_1332i_LNP = 0.

double	Cle_1332r_LNP = 0.

double	Cle_1333i_LNP = 0.

double	Cle_1333r_LNP = 0.

double	Cle_2211r_LNP = 0.

double	Cle_2212i_LNP = 0.

double	Cle_2212r_LNP = 0.

double	Cle_2213i_LNP = 0.

double	Cle_2213r_LNP = 0.

double	Cle_2222r_LNP = 0.

double	Cle_2223i_LNP = 0.

double	Cle_2223r_LNP = 0.

double	Cle_2233r_LNP = 0.

double	Cle_2311i_LNP = 0.

double	Cle_2311r_LNP = 0.

double	Cle_2312i_LNP = 0.

double	Cle_2312r_LNP = 0.

double	Cle_2313i_LNP = 0.

double	Cle_2313r_LNP = 0.

double	Cle_2321i_LNP = 0.

double	Cle_2321r_LNP = 0.

double	Cle_2322i_LNP = 0.

double	Cle_2322r_LNP = 0.

double	Cle_2323i_LNP = 0.

double	Cle_2323r_LNP = 0.

double	Cle_2331i_LNP = 0.

double	Cle_2331r_LNP = 0.

double	Cle_2332i_LNP = 0.

double	Cle_2332r_LNP = 0.

double	Cle_2333i_LNP = 0.

double	Cle_2333r_LNP = 0.

double	Cle_3311r_LNP = 0.

double	Cle_3312i_LNP = 0.

double	Cle_3312r_LNP = 0.

double	Cle_3313i_LNP = 0.

double	Cle_3313r_LNP = 0.

double	Cle_3322r_LNP = 0.

double	Cle_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{le})_{ijkm}$ (Imaginary part). More...

double	Cle_3323r_LNP = 0.

double	Cle_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{le})_{ijkm}$ (Real part and pure real operator). More...

double	Cledq_1111i_LNP = 0.

double	Cledq_1111r_LNP = 0.

double	Cledq_1112i_LNP = 0.

double	Cledq_1112r_LNP = 0.

double	Cledq_1113i_LNP = 0.

double	Cledq_1113r_LNP = 0.

double	Cledq_1121i_LNP = 0.

double	Cledq_1121r_LNP = 0.

double	Cledq_1122i_LNP = 0.

double	Cledq_1122r_LNP = 0.

double	Cledq_1123i_LNP = 0.

double	Cledq_1123r_LNP = 0.

double	Cledq_1131i_LNP = 0.

double	Cledq_1131r_LNP = 0.

double	Cledq_1132i_LNP = 0.

double	Cledq_1132r_LNP = 0.

double	Cledq_1133i_LNP = 0.

double	Cledq_1133r_LNP = 0.

double	Cledq_1211i_LNP = 0.

double	Cledq_1211r_LNP = 0.

double	Cledq_1212i_LNP = 0.

double	Cledq_1212r_LNP = 0.

double	Cledq_1213i_LNP = 0.

double	Cledq_1213r_LNP = 0.

double	Cledq_1221i_LNP = 0.

double	Cledq_1221r_LNP = 0.

double	Cledq_1222i_LNP = 0.

double	Cledq_1222r_LNP = 0.

double	Cledq_1223i_LNP = 0.

double	Cledq_1223r_LNP = 0.

double	Cledq_1231i_LNP = 0.

double	Cledq_1231r_LNP = 0.

double	Cledq_1232i_LNP = 0.

double	Cledq_1232r_LNP = 0.

double	Cledq_1233i_LNP = 0.

double	Cledq_1233r_LNP = 0.

double	Cledq_1311i_LNP = 0.

double	Cledq_1311r_LNP = 0.

double	Cledq_1312i_LNP = 0.

double	Cledq_1312r_LNP = 0.

double	Cledq_1313i_LNP = 0.

double	Cledq_1313r_LNP = 0.

double	Cledq_1321i_LNP = 0.

double	Cledq_1321r_LNP = 0.

double	Cledq_1322i_LNP = 0.

double	Cledq_1322r_LNP = 0.

double	Cledq_1323i_LNP = 0.

double	Cledq_1323r_LNP = 0.

double	Cledq_1331i_LNP = 0.

double	Cledq_1331r_LNP = 0.

double	Cledq_1332i_LNP = 0.

double	Cledq_1332r_LNP = 0.

double	Cledq_1333i_LNP = 0.

double	Cledq_1333r_LNP = 0.

double	Cledq_2111i_LNP = 0.

double	Cledq_2111r_LNP = 0.

double	Cledq_2112i_LNP = 0.

double	Cledq_2112r_LNP = 0.

double	Cledq_2113i_LNP = 0.

double	Cledq_2113r_LNP = 0.

double	Cledq_2121i_LNP = 0.

double	Cledq_2121r_LNP = 0.

double	Cledq_2122i_LNP = 0.

double	Cledq_2122r_LNP = 0.

double	Cledq_2123i_LNP = 0.

double	Cledq_2123r_LNP = 0.

double	Cledq_2131i_LNP = 0.

double	Cledq_2131r_LNP = 0.

double	Cledq_2132i_LNP = 0.

double	Cledq_2132r_LNP = 0.

double	Cledq_2133i_LNP = 0.

double	Cledq_2133r_LNP = 0.

double	Cledq_2211i_LNP = 0.

double	Cledq_2211r_LNP = 0.

double	Cledq_2212i_LNP = 0.

double	Cledq_2212r_LNP = 0.

double	Cledq_2213i_LNP = 0.

double	Cledq_2213r_LNP = 0.

double	Cledq_2221i_LNP = 0.

double	Cledq_2221r_LNP = 0.

double	Cledq_2222i_LNP = 0.

double	Cledq_2222r_LNP = 0.

double	Cledq_2223i_LNP = 0.

double	Cledq_2223r_LNP = 0.

double	Cledq_2231i_LNP = 0.

double	Cledq_2231r_LNP = 0.

double	Cledq_2232i_LNP = 0.

double	Cledq_2232r_LNP = 0.

double	Cledq_2233i_LNP = 0.

double	Cledq_2233r_LNP = 0.

double	Cledq_2311i_LNP = 0.

double	Cledq_2311r_LNP = 0.

double	Cledq_2312i_LNP = 0.

double	Cledq_2312r_LNP = 0.

double	Cledq_2313i_LNP = 0.

double	Cledq_2313r_LNP = 0.

double	Cledq_2321i_LNP = 0.

double	Cledq_2321r_LNP = 0.

double	Cledq_2322i_LNP = 0.

double	Cledq_2322r_LNP = 0.

double	Cledq_2323i_LNP = 0.

double	Cledq_2323r_LNP = 0.

double	Cledq_2331i_LNP = 0.

double	Cledq_2331r_LNP = 0.

double	Cledq_2332i_LNP = 0.

double	Cledq_2332r_LNP = 0.

double	Cledq_2333i_LNP = 0.

double	Cledq_2333r_LNP = 0.

double	Cledq_3111i_LNP = 0.

double	Cledq_3111r_LNP = 0.

double	Cledq_3112i_LNP = 0.

double	Cledq_3112r_LNP = 0.

double	Cledq_3113i_LNP = 0.

double	Cledq_3113r_LNP = 0.

double	Cledq_3121i_LNP = 0.

double	Cledq_3121r_LNP = 0.

double	Cledq_3122i_LNP = 0.

double	Cledq_3122r_LNP = 0.

double	Cledq_3123i_LNP = 0.

double	Cledq_3123r_LNP = 0.

double	Cledq_3131i_LNP = 0.

double	Cledq_3131r_LNP = 0.

double	Cledq_3132i_LNP = 0.

double	Cledq_3132r_LNP = 0.

double	Cledq_3133i_LNP = 0.

double	Cledq_3133r_LNP = 0.

double	Cledq_3211i_LNP = 0.

double	Cledq_3211r_LNP = 0.

double	Cledq_3212i_LNP = 0.

double	Cledq_3212r_LNP = 0.

double	Cledq_3213i_LNP = 0.

double	Cledq_3213r_LNP = 0.

double	Cledq_3221i_LNP = 0.

double	Cledq_3221r_LNP = 0.

double	Cledq_3222i_LNP = 0.

double	Cledq_3222r_LNP = 0.

double	Cledq_3223i_LNP = 0.

double	Cledq_3223r_LNP = 0.

double	Cledq_3231i_LNP = 0.

double	Cledq_3231r_LNP = 0.

double	Cledq_3232i_LNP = 0.

double	Cledq_3232r_LNP = 0.

double	Cledq_3233i_LNP = 0.

double	Cledq_3233r_LNP = 0.

double	Cledq_3311i_LNP = 0.

double	Cledq_3311r_LNP = 0.

double	Cledq_3312i_LNP = 0.

double	Cledq_3312r_LNP = 0.

double	Cledq_3313i_LNP = 0.

double	Cledq_3313r_LNP = 0.

double	Cledq_3321i_LNP = 0.

double	Cledq_3321r_LNP = 0.

double	Cledq_3322i_LNP = 0.

double	Cledq_3322r_LNP = 0.

double	Cledq_3323i_LNP = 0.

double	Cledq_3323r_LNP = 0.

double	Cledq_3331i_LNP = 0.

double	Cledq_3331r_LNP = 0.

double	Cledq_3332i_LNP = 0.

double	Cledq_3332r_LNP = 0.

double	Cledq_3333i_LNP = 0.
	The dimension-6 operator coefficient $(C_{ledq})_{ijkm}$ (Imaginary part). More...

double	Cledq_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{ledq})_{ijkm}$ (Real part and pure real operator). More...

double	Clequ1_1111i_LNP = 0.

double	Clequ1_1111r_LNP = 0.

double	Clequ1_1112i_LNP = 0.

double	Clequ1_1112r_LNP = 0.

double	Clequ1_1113i_LNP = 0.

double	Clequ1_1113r_LNP = 0.

double	Clequ1_1121i_LNP = 0.

double	Clequ1_1121r_LNP = 0.

double	Clequ1_1122i_LNP = 0.

double	Clequ1_1122r_LNP = 0.

double	Clequ1_1123i_LNP = 0.

double	Clequ1_1123r_LNP = 0.

double	Clequ1_1131i_LNP = 0.

double	Clequ1_1131r_LNP = 0.

double	Clequ1_1132i_LNP = 0.

double	Clequ1_1132r_LNP = 0.

double	Clequ1_1133i_LNP = 0.

double	Clequ1_1133r_LNP = 0.

double	Clequ1_1211i_LNP = 0.

double	Clequ1_1211r_LNP = 0.

double	Clequ1_1212i_LNP = 0.

double	Clequ1_1212r_LNP = 0.

double	Clequ1_1213i_LNP = 0.

double	Clequ1_1213r_LNP = 0.

double	Clequ1_1221i_LNP = 0.

double	Clequ1_1221r_LNP = 0.

double	Clequ1_1222i_LNP = 0.

double	Clequ1_1222r_LNP = 0.

double	Clequ1_1223i_LNP = 0.

double	Clequ1_1223r_LNP = 0.

double	Clequ1_1231i_LNP = 0.

double	Clequ1_1231r_LNP = 0.

double	Clequ1_1232i_LNP = 0.

double	Clequ1_1232r_LNP = 0.

double	Clequ1_1233i_LNP = 0.

double	Clequ1_1233r_LNP = 0.

double	Clequ1_1311i_LNP = 0.

double	Clequ1_1311r_LNP = 0.

double	Clequ1_1312i_LNP = 0.

double	Clequ1_1312r_LNP = 0.

double	Clequ1_1313i_LNP = 0.

double	Clequ1_1313r_LNP = 0.

double	Clequ1_1321i_LNP = 0.

double	Clequ1_1321r_LNP = 0.

double	Clequ1_1322i_LNP = 0.

double	Clequ1_1322r_LNP = 0.

double	Clequ1_1323i_LNP = 0.

double	Clequ1_1323r_LNP = 0.

double	Clequ1_1331i_LNP = 0.

double	Clequ1_1331r_LNP = 0.

double	Clequ1_1332i_LNP = 0.

double	Clequ1_1332r_LNP = 0.

double	Clequ1_1333i_LNP = 0.

double	Clequ1_1333r_LNP = 0.

double	Clequ1_2111i_LNP = 0.

double	Clequ1_2111r_LNP = 0.

double	Clequ1_2112i_LNP = 0.

double	Clequ1_2112r_LNP = 0.

double	Clequ1_2113i_LNP = 0.

double	Clequ1_2113r_LNP = 0.

double	Clequ1_2121i_LNP = 0.

double	Clequ1_2121r_LNP = 0.

double	Clequ1_2122i_LNP = 0.

double	Clequ1_2122r_LNP = 0.

double	Clequ1_2123i_LNP = 0.

double	Clequ1_2123r_LNP = 0.

double	Clequ1_2131i_LNP = 0.

double	Clequ1_2131r_LNP = 0.

double	Clequ1_2132i_LNP = 0.

double	Clequ1_2132r_LNP = 0.

double	Clequ1_2133i_LNP = 0.

double	Clequ1_2133r_LNP = 0.

double	Clequ1_2211i_LNP = 0.

double	Clequ1_2211r_LNP = 0.

double	Clequ1_2212i_LNP = 0.

double	Clequ1_2212r_LNP = 0.

double	Clequ1_2213i_LNP = 0.

double	Clequ1_2213r_LNP = 0.

double	Clequ1_2221i_LNP = 0.

double	Clequ1_2221r_LNP = 0.

double	Clequ1_2222i_LNP = 0.

double	Clequ1_2222r_LNP = 0.

double	Clequ1_2223i_LNP = 0.

double	Clequ1_2223r_LNP = 0.

double	Clequ1_2231i_LNP = 0.

double	Clequ1_2231r_LNP = 0.

double	Clequ1_2232i_LNP = 0.

double	Clequ1_2232r_LNP = 0.

double	Clequ1_2233i_LNP = 0.

double	Clequ1_2233r_LNP = 0.

double	Clequ1_2311i_LNP = 0.

double	Clequ1_2311r_LNP = 0.

double	Clequ1_2312i_LNP = 0.

double	Clequ1_2312r_LNP = 0.

double	Clequ1_2313i_LNP = 0.

double	Clequ1_2313r_LNP = 0.

double	Clequ1_2321i_LNP = 0.

double	Clequ1_2321r_LNP = 0.

double	Clequ1_2322i_LNP = 0.

double	Clequ1_2322r_LNP = 0.

double	Clequ1_2323i_LNP = 0.

double	Clequ1_2323r_LNP = 0.

double	Clequ1_2331i_LNP = 0.

double	Clequ1_2331r_LNP = 0.

double	Clequ1_2332i_LNP = 0.

double	Clequ1_2332r_LNP = 0.

double	Clequ1_2333i_LNP = 0.

double	Clequ1_2333r_LNP = 0.

double	Clequ1_3111i_LNP = 0.

double	Clequ1_3111r_LNP = 0.

double	Clequ1_3112i_LNP = 0.

double	Clequ1_3112r_LNP = 0.

double	Clequ1_3113i_LNP = 0.

double	Clequ1_3113r_LNP = 0.

double	Clequ1_3121i_LNP = 0.

double	Clequ1_3121r_LNP = 0.

double	Clequ1_3122i_LNP = 0.

double	Clequ1_3122r_LNP = 0.

double	Clequ1_3123i_LNP = 0.

double	Clequ1_3123r_LNP = 0.

double	Clequ1_3131i_LNP = 0.

double	Clequ1_3131r_LNP = 0.

double	Clequ1_3132i_LNP = 0.

double	Clequ1_3132r_LNP = 0.

double	Clequ1_3133i_LNP = 0.

double	Clequ1_3133r_LNP = 0.

double	Clequ1_3211i_LNP = 0.

double	Clequ1_3211r_LNP = 0.

double	Clequ1_3212i_LNP = 0.

double	Clequ1_3212r_LNP = 0.

double	Clequ1_3213i_LNP = 0.

double	Clequ1_3213r_LNP = 0.

double	Clequ1_3221i_LNP = 0.

double	Clequ1_3221r_LNP = 0.

double	Clequ1_3222i_LNP = 0.

double	Clequ1_3222r_LNP = 0.

double	Clequ1_3223i_LNP = 0.

double	Clequ1_3223r_LNP = 0.

double	Clequ1_3231i_LNP = 0.

double	Clequ1_3231r_LNP = 0.

double	Clequ1_3232i_LNP = 0.

double	Clequ1_3232r_LNP = 0.

double	Clequ1_3233i_LNP = 0.

double	Clequ1_3233r_LNP = 0.

double	Clequ1_3311i_LNP = 0.

double	Clequ1_3311r_LNP = 0.

double	Clequ1_3312i_LNP = 0.

double	Clequ1_3312r_LNP = 0.

double	Clequ1_3313i_LNP = 0.

double	Clequ1_3313r_LNP = 0.

double	Clequ1_3321i_LNP = 0.

double	Clequ1_3321r_LNP = 0.

double	Clequ1_3322i_LNP = 0.

double	Clequ1_3322r_LNP = 0.

double	Clequ1_3323i_LNP = 0.

double	Clequ1_3323r_LNP = 0.

double	Clequ1_3331i_LNP = 0.

double	Clequ1_3331r_LNP = 0.

double	Clequ1_3332i_LNP = 0.

double	Clequ1_3332r_LNP = 0.

double	Clequ1_3333i_LNP = 0.
	The dimension-6 operator coefficient $(C_{lequ}^{(1)})_{ijkm}$ (Imaginary part). More...

double	Clequ1_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{lequ}^{(1)})_{ijkm}$ (Real part and pure real operator). More...

double	Clequ3_1111i_LNP = 0.

double	Clequ3_1111r_LNP = 0.

double	Clequ3_1112i_LNP = 0.

double	Clequ3_1112r_LNP = 0.

double	Clequ3_1113i_LNP = 0.

double	Clequ3_1113r_LNP = 0.

double	Clequ3_1121i_LNP = 0.

double	Clequ3_1121r_LNP = 0.

double	Clequ3_1122i_LNP = 0.

double	Clequ3_1122r_LNP = 0.

double	Clequ3_1123i_LNP = 0.

double	Clequ3_1123r_LNP = 0.

double	Clequ3_1131i_LNP = 0.

double	Clequ3_1131r_LNP = 0.

double	Clequ3_1132i_LNP = 0.

double	Clequ3_1132r_LNP = 0.

double	Clequ3_1133i_LNP = 0.

double	Clequ3_1133r_LNP = 0.

double	Clequ3_1211i_LNP = 0.

double	Clequ3_1211r_LNP = 0.

double	Clequ3_1212i_LNP = 0.

double	Clequ3_1212r_LNP = 0.

double	Clequ3_1213i_LNP = 0.

double	Clequ3_1213r_LNP = 0.

double	Clequ3_1221i_LNP = 0.

double	Clequ3_1221r_LNP = 0.

double	Clequ3_1222i_LNP = 0.

double	Clequ3_1222r_LNP = 0.

double	Clequ3_1223i_LNP = 0.

double	Clequ3_1223r_LNP = 0.

double	Clequ3_1231i_LNP = 0.

double	Clequ3_1231r_LNP = 0.

double	Clequ3_1232i_LNP = 0.

double	Clequ3_1232r_LNP = 0.

double	Clequ3_1233i_LNP = 0.

double	Clequ3_1233r_LNP = 0.

double	Clequ3_1311i_LNP = 0.

double	Clequ3_1311r_LNP = 0.

double	Clequ3_1312i_LNP = 0.

double	Clequ3_1312r_LNP = 0.

double	Clequ3_1313i_LNP = 0.

double	Clequ3_1313r_LNP = 0.

double	Clequ3_1321i_LNP = 0.

double	Clequ3_1321r_LNP = 0.

double	Clequ3_1322i_LNP = 0.

double	Clequ3_1322r_LNP = 0.

double	Clequ3_1323i_LNP = 0.

double	Clequ3_1323r_LNP = 0.

double	Clequ3_1331i_LNP = 0.

double	Clequ3_1331r_LNP = 0.

double	Clequ3_1332i_LNP = 0.

double	Clequ3_1332r_LNP = 0.

double	Clequ3_1333i_LNP = 0.

double	Clequ3_1333r_LNP = 0.

double	Clequ3_2111i_LNP = 0.

double	Clequ3_2111r_LNP = 0.

double	Clequ3_2112i_LNP = 0.

double	Clequ3_2112r_LNP = 0.

double	Clequ3_2113i_LNP = 0.

double	Clequ3_2113r_LNP = 0.

double	Clequ3_2121i_LNP = 0.

double	Clequ3_2121r_LNP = 0.

double	Clequ3_2122i_LNP = 0.

double	Clequ3_2122r_LNP = 0.

double	Clequ3_2123i_LNP = 0.

double	Clequ3_2123r_LNP = 0.

double	Clequ3_2131i_LNP = 0.

double	Clequ3_2131r_LNP = 0.

double	Clequ3_2132i_LNP = 0.

double	Clequ3_2132r_LNP = 0.

double	Clequ3_2133i_LNP = 0.

double	Clequ3_2133r_LNP = 0.

double	Clequ3_2211i_LNP = 0.

double	Clequ3_2211r_LNP = 0.

double	Clequ3_2212i_LNP = 0.

double	Clequ3_2212r_LNP = 0.

double	Clequ3_2213i_LNP = 0.

double	Clequ3_2213r_LNP = 0.

double	Clequ3_2221i_LNP = 0.

double	Clequ3_2221r_LNP = 0.

double	Clequ3_2222i_LNP = 0.

double	Clequ3_2222r_LNP = 0.

double	Clequ3_2223i_LNP = 0.

double	Clequ3_2223r_LNP = 0.

double	Clequ3_2231i_LNP = 0.

double	Clequ3_2231r_LNP = 0.

double	Clequ3_2232i_LNP = 0.

double	Clequ3_2232r_LNP = 0.

double	Clequ3_2233i_LNP = 0.

double	Clequ3_2233r_LNP = 0.

double	Clequ3_2311i_LNP = 0.

double	Clequ3_2311r_LNP = 0.

double	Clequ3_2312i_LNP = 0.

double	Clequ3_2312r_LNP = 0.

double	Clequ3_2313i_LNP = 0.

double	Clequ3_2313r_LNP = 0.

double	Clequ3_2321i_LNP = 0.

double	Clequ3_2321r_LNP = 0.

double	Clequ3_2322i_LNP = 0.

double	Clequ3_2322r_LNP = 0.

double	Clequ3_2323i_LNP = 0.

double	Clequ3_2323r_LNP = 0.

double	Clequ3_2331i_LNP = 0.

double	Clequ3_2331r_LNP = 0.

double	Clequ3_2332i_LNP = 0.

double	Clequ3_2332r_LNP = 0.

double	Clequ3_2333i_LNP = 0.

double	Clequ3_2333r_LNP = 0.

double	Clequ3_3111i_LNP = 0.

double	Clequ3_3111r_LNP = 0.

double	Clequ3_3112i_LNP = 0.

double	Clequ3_3112r_LNP = 0.

double	Clequ3_3113i_LNP = 0.

double	Clequ3_3113r_LNP = 0.

double	Clequ3_3121i_LNP = 0.

double	Clequ3_3121r_LNP = 0.

double	Clequ3_3122i_LNP = 0.

double	Clequ3_3122r_LNP = 0.

double	Clequ3_3123i_LNP = 0.

double	Clequ3_3123r_LNP = 0.

double	Clequ3_3131i_LNP = 0.

double	Clequ3_3131r_LNP = 0.

double	Clequ3_3132i_LNP = 0.

double	Clequ3_3132r_LNP = 0.

double	Clequ3_3133i_LNP = 0.

double	Clequ3_3133r_LNP = 0.

double	Clequ3_3211i_LNP = 0.

double	Clequ3_3211r_LNP = 0.

double	Clequ3_3212i_LNP = 0.

double	Clequ3_3212r_LNP = 0.

double	Clequ3_3213i_LNP = 0.

double	Clequ3_3213r_LNP = 0.

double	Clequ3_3221i_LNP = 0.

double	Clequ3_3221r_LNP = 0.

double	Clequ3_3222i_LNP = 0.

double	Clequ3_3222r_LNP = 0.

double	Clequ3_3223i_LNP = 0.

double	Clequ3_3223r_LNP = 0.

double	Clequ3_3231i_LNP = 0.

double	Clequ3_3231r_LNP = 0.

double	Clequ3_3232i_LNP = 0.

double	Clequ3_3232r_LNP = 0.

double	Clequ3_3233i_LNP = 0.

double	Clequ3_3233r_LNP = 0.

double	Clequ3_3311i_LNP = 0.

double	Clequ3_3311r_LNP = 0.

double	Clequ3_3312i_LNP = 0.

double	Clequ3_3312r_LNP = 0.

double	Clequ3_3313i_LNP = 0.

double	Clequ3_3313r_LNP = 0.

double	Clequ3_3321i_LNP = 0.

double	Clequ3_3321r_LNP = 0.

double	Clequ3_3322i_LNP = 0.

double	Clequ3_3322r_LNP = 0.

double	Clequ3_3323i_LNP = 0.

double	Clequ3_3323r_LNP = 0.

double	Clequ3_3331i_LNP = 0.

double	Clequ3_3331r_LNP = 0.

double	Clequ3_3332i_LNP = 0.

double	Clequ3_3332r_LNP = 0.

double	Clequ3_3333i_LNP = 0.
	The dimension-6 operator coefficient $(C_{lequ}^{(3)})_{ijkm}$ (Imaginary part). More...

double	Clequ3_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{lequ}^{(3)})_{ijkm}$ (Real part and pure real operator). More...

double	cLH3d62
	Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms). More...

double	cLHd6
	Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions. More...

double	Cll_1111r_LNP = 0.

double	Cll_1112i_LNP = 0.

double	Cll_1112r_LNP = 0.

double	Cll_1113i_LNP = 0.

double	Cll_1113r_LNP = 0.

double	Cll_1122r_LNP = 0.

double	Cll_1123i_LNP = 0.

double	Cll_1123r_LNP = 0.

double	Cll_1133r_LNP = 0.

double	Cll_1212i_LNP = 0.

double	Cll_1212r_LNP = 0.

double	Cll_1213i_LNP = 0.

double	Cll_1213r_LNP = 0.

double	Cll_1221r_LNP = 0.

double	Cll_1222i_LNP = 0.

double	Cll_1222r_LNP = 0.

double	Cll_1223i_LNP = 0.

double	Cll_1223r_LNP = 0.

double	Cll_1231i_LNP = 0.

double	Cll_1231r_LNP = 0.

double	Cll_1232i_LNP = 0.

double	Cll_1232r_LNP = 0.

double	Cll_1233i_LNP = 0.

double	Cll_1233r_LNP = 0.

double	Cll_1313i_LNP = 0.

double	Cll_1313r_LNP = 0.

double	Cll_1322i_LNP = 0.

double	Cll_1322r_LNP = 0.

double	Cll_1323i_LNP = 0.

double	Cll_1323r_LNP = 0.

double	Cll_1331r_LNP = 0.

double	Cll_1332i_LNP = 0.

double	Cll_1332r_LNP = 0.

double	Cll_1333i_LNP = 0.

double	Cll_1333r_LNP = 0.

double	Cll_2222r_LNP = 0.

double	Cll_2223i_LNP = 0.

double	Cll_2223r_LNP = 0.

double	Cll_2233r_LNP = 0.

double	Cll_2323i_LNP = 0.

double	Cll_2323r_LNP = 0.

double	Cll_2332r_LNP = 0.

double	Cll_2333i_LNP = 0.
	The dimension-6 operator coefficient $(C_{ll})_{ijkm}$ (Imaginary part). More...

double	Cll_2333r_LNP = 0.

double	Cll_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{ll})_{ijkm}$ (Real part and pure real operator). More...

double	Clq1_1111r_LNP = 0.

double	Clq1_1112i_LNP = 0.

double	Clq1_1112r_LNP = 0.

double	Clq1_1113i_LNP = 0.

double	Clq1_1113r_LNP = 0.

double	Clq1_1122r_LNP = 0.

double	Clq1_1123i_LNP = 0.

double	Clq1_1123r_LNP = 0.

double	Clq1_1133r_LNP = 0.

double	Clq1_1211i_LNP = 0.

double	Clq1_1211r_LNP = 0.

double	Clq1_1212i_LNP = 0.

double	Clq1_1212r_LNP = 0.

double	Clq1_1213i_LNP = 0.

double	Clq1_1213r_LNP = 0.

double	Clq1_1221i_LNP = 0.

double	Clq1_1221r_LNP = 0.

double	Clq1_1222i_LNP = 0.

double	Clq1_1222r_LNP = 0.

double	Clq1_1223i_LNP = 0.

double	Clq1_1223r_LNP = 0.

double	Clq1_1231i_LNP = 0.

double	Clq1_1231r_LNP = 0.

double	Clq1_1232i_LNP = 0.

double	Clq1_1232r_LNP = 0.

double	Clq1_1233i_LNP = 0.

double	Clq1_1233r_LNP = 0.

double	Clq1_1311i_LNP = 0.

double	Clq1_1311r_LNP = 0.

double	Clq1_1312i_LNP = 0.

double	Clq1_1312r_LNP = 0.

double	Clq1_1313i_LNP = 0.

double	Clq1_1313r_LNP = 0.

double	Clq1_1321i_LNP = 0.

double	Clq1_1321r_LNP = 0.

double	Clq1_1322i_LNP = 0.

double	Clq1_1322r_LNP = 0.

double	Clq1_1323i_LNP = 0.

double	Clq1_1323r_LNP = 0.

double	Clq1_1331i_LNP = 0.

double	Clq1_1331r_LNP = 0.

double	Clq1_1332i_LNP = 0.

double	Clq1_1332r_LNP = 0.

double	Clq1_1333i_LNP = 0.

double	Clq1_1333r_LNP = 0.

double	Clq1_2211r_LNP = 0.

double	Clq1_2212i_LNP = 0.

double	Clq1_2212r_LNP = 0.

double	Clq1_2213i_LNP = 0.

double	Clq1_2213r_LNP = 0.

double	Clq1_2222r_LNP = 0.

double	Clq1_2223i_LNP = 0.

double	Clq1_2223r_LNP = 0.

double	Clq1_2233r_LNP = 0.

double	Clq1_2311i_LNP = 0.

double	Clq1_2311r_LNP = 0.

double	Clq1_2312i_LNP = 0.

double	Clq1_2312r_LNP = 0.

double	Clq1_2313i_LNP = 0.

double	Clq1_2313r_LNP = 0.

double	Clq1_2321i_LNP = 0.

double	Clq1_2321r_LNP = 0.

double	Clq1_2322i_LNP = 0.

double	Clq1_2322r_LNP = 0.

double	Clq1_2323i_LNP = 0.

double	Clq1_2323r_LNP = 0.

double	Clq1_2331i_LNP = 0.

double	Clq1_2331r_LNP = 0.

double	Clq1_2332i_LNP = 0.

double	Clq1_2332r_LNP = 0.

double	Clq1_2333i_LNP = 0.

double	Clq1_2333r_LNP = 0.

double	Clq1_3311r_LNP = 0.

double	Clq1_3312i_LNP = 0.

double	Clq1_3312r_LNP = 0.

double	Clq1_3313i_LNP = 0.

double	Clq1_3313r_LNP = 0.

double	Clq1_3322r_LNP = 0.

double	Clq1_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{lq}^{(1)})_{ijkm}$ (Imaginary part). More...

double	Clq1_3323r_LNP = 0.

double	Clq1_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{lq}^{(1)})_{ijkm}$ (Real part and pure real operator). More...

double	Clq3_1111r_LNP = 0.

double	Clq3_1112i_LNP = 0.

double	Clq3_1112r_LNP = 0.

double	Clq3_1113i_LNP = 0.

double	Clq3_1113r_LNP = 0.

double	Clq3_1122r_LNP = 0.

double	Clq3_1123i_LNP = 0.

double	Clq3_1123r_LNP = 0.

double	Clq3_1133r_LNP = 0.

double	Clq3_1211i_LNP = 0.

double	Clq3_1211r_LNP = 0.

double	Clq3_1212i_LNP = 0.

double	Clq3_1212r_LNP = 0.

double	Clq3_1213i_LNP = 0.

double	Clq3_1213r_LNP = 0.

double	Clq3_1221i_LNP = 0.

double	Clq3_1221r_LNP = 0.

double	Clq3_1222i_LNP = 0.

double	Clq3_1222r_LNP = 0.

double	Clq3_1223i_LNP = 0.

double	Clq3_1223r_LNP = 0.

double	Clq3_1231i_LNP = 0.

double	Clq3_1231r_LNP = 0.

double	Clq3_1232i_LNP = 0.

double	Clq3_1232r_LNP = 0.

double	Clq3_1233i_LNP = 0.

double	Clq3_1233r_LNP = 0.

double	Clq3_1311i_LNP = 0.

double	Clq3_1311r_LNP = 0.

double	Clq3_1312i_LNP = 0.

double	Clq3_1312r_LNP = 0.

double	Clq3_1313i_LNP = 0.

double	Clq3_1313r_LNP = 0.

double	Clq3_1321i_LNP = 0.

double	Clq3_1321r_LNP = 0.

double	Clq3_1322i_LNP = 0.

double	Clq3_1322r_LNP = 0.

double	Clq3_1323i_LNP = 0.

double	Clq3_1323r_LNP = 0.

double	Clq3_1331i_LNP = 0.

double	Clq3_1331r_LNP = 0.

double	Clq3_1332i_LNP = 0.

double	Clq3_1332r_LNP = 0.

double	Clq3_1333i_LNP = 0.

double	Clq3_1333r_LNP = 0.

double	Clq3_2211r_LNP = 0.

double	Clq3_2212i_LNP = 0.

double	Clq3_2212r_LNP = 0.

double	Clq3_2213i_LNP = 0.

double	Clq3_2213r_LNP = 0.

double	Clq3_2222r_LNP = 0.

double	Clq3_2223i_LNP = 0.

double	Clq3_2223r_LNP = 0.

double	Clq3_2233r_LNP = 0.

double	Clq3_2311i_LNP = 0.

double	Clq3_2311r_LNP = 0.

double	Clq3_2312i_LNP = 0.

double	Clq3_2312r_LNP = 0.

double	Clq3_2313i_LNP = 0.

double	Clq3_2313r_LNP = 0.

double	Clq3_2321i_LNP = 0.

double	Clq3_2321r_LNP = 0.

double	Clq3_2322i_LNP = 0.

double	Clq3_2322r_LNP = 0.

double	Clq3_2323i_LNP = 0.

double	Clq3_2323r_LNP = 0.

double	Clq3_2331i_LNP = 0.

double	Clq3_2331r_LNP = 0.

double	Clq3_2332i_LNP = 0.

double	Clq3_2332r_LNP = 0.

double	Clq3_2333i_LNP = 0.

double	Clq3_2333r_LNP = 0.

double	Clq3_3311r_LNP = 0.

double	Clq3_3312i_LNP = 0.

double	Clq3_3312r_LNP = 0.

double	Clq3_3313i_LNP = 0.

double	Clq3_3313r_LNP = 0.

double	Clq3_3322r_LNP = 0.

double	Clq3_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{lq}^{(3)})_{ijkm}$ (Imaginary part). More...

double	Clq3_3323r_LNP = 0.

double	Clq3_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{lq}^{(3)})_{ijkm}$ (Real part and pure real operator). More...

double	Clu_1111r_LNP = 0.

double	Clu_1112i_LNP = 0.

double	Clu_1112r_LNP = 0.

double	Clu_1113i_LNP = 0.

double	Clu_1113r_LNP = 0.

double	Clu_1122r_LNP = 0.

double	Clu_1123i_LNP = 0.

double	Clu_1123r_LNP = 0.

double	Clu_1133r_LNP = 0.

double	Clu_1211i_LNP = 0.

double	Clu_1211r_LNP = 0.

double	Clu_1212i_LNP = 0.

double	Clu_1212r_LNP = 0.

double	Clu_1213i_LNP = 0.

double	Clu_1213r_LNP = 0.

double	Clu_1221i_LNP = 0.

double	Clu_1221r_LNP = 0.

double	Clu_1222i_LNP = 0.

double	Clu_1222r_LNP = 0.

double	Clu_1223i_LNP = 0.

double	Clu_1223r_LNP = 0.

double	Clu_1231i_LNP = 0.

double	Clu_1231r_LNP = 0.

double	Clu_1232i_LNP = 0.

double	Clu_1232r_LNP = 0.

double	Clu_1233i_LNP = 0.

double	Clu_1233r_LNP = 0.

double	Clu_1311i_LNP = 0.

double	Clu_1311r_LNP = 0.

double	Clu_1312i_LNP = 0.

double	Clu_1312r_LNP = 0.

double	Clu_1313i_LNP = 0.

double	Clu_1313r_LNP = 0.

double	Clu_1321i_LNP = 0.

double	Clu_1321r_LNP = 0.

double	Clu_1322i_LNP = 0.

double	Clu_1322r_LNP = 0.

double	Clu_1323i_LNP = 0.

double	Clu_1323r_LNP = 0.

double	Clu_1331i_LNP = 0.

double	Clu_1331r_LNP = 0.

double	Clu_1332i_LNP = 0.

double	Clu_1332r_LNP = 0.

double	Clu_1333i_LNP = 0.

double	Clu_1333r_LNP = 0.

double	Clu_2211r_LNP = 0.

double	Clu_2212i_LNP = 0.

double	Clu_2212r_LNP = 0.

double	Clu_2213i_LNP = 0.

double	Clu_2213r_LNP = 0.

double	Clu_2222r_LNP = 0.

double	Clu_2223i_LNP = 0.

double	Clu_2223r_LNP = 0.

double	Clu_2233r_LNP = 0.

double	Clu_2311i_LNP = 0.

double	Clu_2311r_LNP = 0.

double	Clu_2312i_LNP = 0.

double	Clu_2312r_LNP = 0.

double	Clu_2313i_LNP = 0.

double	Clu_2313r_LNP = 0.

double	Clu_2321i_LNP = 0.

double	Clu_2321r_LNP = 0.

double	Clu_2322i_LNP = 0.

double	Clu_2322r_LNP = 0.

double	Clu_2323i_LNP = 0.

double	Clu_2323r_LNP = 0.

double	Clu_2331i_LNP = 0.

double	Clu_2331r_LNP = 0.

double	Clu_2332i_LNP = 0.

double	Clu_2332r_LNP = 0.

double	Clu_2333i_LNP = 0.

double	Clu_2333r_LNP = 0.

double	Clu_3311r_LNP = 0.

double	Clu_3312i_LNP = 0.

double	Clu_3312r_LNP = 0.

double	Clu_3313i_LNP = 0.

double	Clu_3313r_LNP = 0.

double	Clu_3322r_LNP = 0.

double	Clu_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{lu})_{ijkm}$ (Imaginary part). More...

double	Clu_3323r_LNP = 0.

double	Clu_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{lu})_{ijkm}$ (Real part and pure real operator). More...

double	cNLOd6
	Parameter to control the inclusion of finite NLO corrections, when available. More...

double	Cqd1_1111r_LNP = 0.

double	Cqd1_1112i_LNP = 0.

double	Cqd1_1112r_LNP = 0.

double	Cqd1_1113i_LNP = 0.

double	Cqd1_1113r_LNP = 0.

double	Cqd1_1122r_LNP = 0.

double	Cqd1_1123i_LNP = 0.

double	Cqd1_1123r_LNP = 0.

double	Cqd1_1133r_LNP = 0.

double	Cqd1_1211i_LNP = 0.

double	Cqd1_1211r_LNP = 0.

double	Cqd1_1212i_LNP = 0.

double	Cqd1_1212r_LNP = 0.

double	Cqd1_1213i_LNP = 0.

double	Cqd1_1213r_LNP = 0.

double	Cqd1_1221i_LNP = 0.

double	Cqd1_1221r_LNP = 0.

double	Cqd1_1222i_LNP = 0.

double	Cqd1_1222r_LNP = 0.

double	Cqd1_1223i_LNP = 0.

double	Cqd1_1223r_LNP = 0.

double	Cqd1_1231i_LNP = 0.

double	Cqd1_1231r_LNP = 0.

double	Cqd1_1232i_LNP = 0.

double	Cqd1_1232r_LNP = 0.

double	Cqd1_1233i_LNP = 0.

double	Cqd1_1233r_LNP = 0.

double	Cqd1_1311i_LNP = 0.

double	Cqd1_1311r_LNP = 0.

double	Cqd1_1312i_LNP = 0.

double	Cqd1_1312r_LNP = 0.

double	Cqd1_1313i_LNP = 0.

double	Cqd1_1313r_LNP = 0.

double	Cqd1_1321i_LNP = 0.

double	Cqd1_1321r_LNP = 0.

double	Cqd1_1322i_LNP = 0.

double	Cqd1_1322r_LNP = 0.

double	Cqd1_1323i_LNP = 0.

double	Cqd1_1323r_LNP = 0.

double	Cqd1_1331i_LNP = 0.

double	Cqd1_1331r_LNP = 0.

double	Cqd1_1332i_LNP = 0.

double	Cqd1_1332r_LNP = 0.

double	Cqd1_1333i_LNP = 0.

double	Cqd1_1333r_LNP = 0.

double	Cqd1_2211r_LNP = 0.

double	Cqd1_2212i_LNP = 0.

double	Cqd1_2212r_LNP = 0.

double	Cqd1_2213i_LNP = 0.

double	Cqd1_2213r_LNP = 0.

double	Cqd1_2222r_LNP = 0.

double	Cqd1_2223i_LNP = 0.

double	Cqd1_2223r_LNP = 0.

double	Cqd1_2233r_LNP = 0.

double	Cqd1_2311i_LNP = 0.

double	Cqd1_2311r_LNP = 0.

double	Cqd1_2312i_LNP = 0.

double	Cqd1_2312r_LNP = 0.

double	Cqd1_2313i_LNP = 0.

double	Cqd1_2313r_LNP = 0.

double	Cqd1_2321i_LNP = 0.

double	Cqd1_2321r_LNP = 0.

double	Cqd1_2322i_LNP = 0.

double	Cqd1_2322r_LNP = 0.

double	Cqd1_2323i_LNP = 0.

double	Cqd1_2323r_LNP = 0.

double	Cqd1_2331i_LNP = 0.

double	Cqd1_2331r_LNP = 0.

double	Cqd1_2332i_LNP = 0.

double	Cqd1_2332r_LNP = 0.

double	Cqd1_2333i_LNP = 0.

double	Cqd1_2333r_LNP = 0.

double	Cqd1_3311r_LNP = 0.

double	Cqd1_3312i_LNP = 0.

double	Cqd1_3312r_LNP = 0.

double	Cqd1_3313i_LNP = 0.

double	Cqd1_3313r_LNP = 0.

double	Cqd1_3322r_LNP = 0.

double	Cqd1_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{qd}^{(1)})_{ijkm}$ (Imaginary part). More...

double	Cqd1_3323r_LNP = 0.

double	Cqd1_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{qd}^{(1)})_{ijkm}$ (Real part and pure real operator). More...

double	Cqd8_1111r_LNP = 0.

double	Cqd8_1112i_LNP = 0.

double	Cqd8_1112r_LNP = 0.

double	Cqd8_1113i_LNP = 0.

double	Cqd8_1113r_LNP = 0.

double	Cqd8_1122r_LNP = 0.

double	Cqd8_1123i_LNP = 0.

double	Cqd8_1123r_LNP = 0.

double	Cqd8_1133r_LNP = 0.

double	Cqd8_1211i_LNP = 0.

double	Cqd8_1211r_LNP = 0.

double	Cqd8_1212i_LNP = 0.

double	Cqd8_1212r_LNP = 0.

double	Cqd8_1213i_LNP = 0.

double	Cqd8_1213r_LNP = 0.

double	Cqd8_1221i_LNP = 0.

double	Cqd8_1221r_LNP = 0.

double	Cqd8_1222i_LNP = 0.

double	Cqd8_1222r_LNP = 0.

double	Cqd8_1223i_LNP = 0.

double	Cqd8_1223r_LNP = 0.

double	Cqd8_1231i_LNP = 0.

double	Cqd8_1231r_LNP = 0.

double	Cqd8_1232i_LNP = 0.

double	Cqd8_1232r_LNP = 0.

double	Cqd8_1233i_LNP = 0.

double	Cqd8_1233r_LNP = 0.

double	Cqd8_1311i_LNP = 0.

double	Cqd8_1311r_LNP = 0.

double	Cqd8_1312i_LNP = 0.

double	Cqd8_1312r_LNP = 0.

double	Cqd8_1313i_LNP = 0.

double	Cqd8_1313r_LNP = 0.

double	Cqd8_1321i_LNP = 0.

double	Cqd8_1321r_LNP = 0.

double	Cqd8_1322i_LNP = 0.

double	Cqd8_1322r_LNP = 0.

double	Cqd8_1323i_LNP = 0.

double	Cqd8_1323r_LNP = 0.

double	Cqd8_1331i_LNP = 0.

double	Cqd8_1331r_LNP = 0.

double	Cqd8_1332i_LNP = 0.

double	Cqd8_1332r_LNP = 0.

double	Cqd8_1333i_LNP = 0.

double	Cqd8_1333r_LNP = 0.

double	Cqd8_2211r_LNP = 0.

double	Cqd8_2212i_LNP = 0.

double	Cqd8_2212r_LNP = 0.

double	Cqd8_2213i_LNP = 0.

double	Cqd8_2213r_LNP = 0.

double	Cqd8_2222r_LNP = 0.

double	Cqd8_2223i_LNP = 0.

double	Cqd8_2223r_LNP = 0.

double	Cqd8_2233r_LNP = 0.

double	Cqd8_2311i_LNP = 0.

double	Cqd8_2311r_LNP = 0.

double	Cqd8_2312i_LNP = 0.

double	Cqd8_2312r_LNP = 0.

double	Cqd8_2313i_LNP = 0.

double	Cqd8_2313r_LNP = 0.

double	Cqd8_2321i_LNP = 0.

double	Cqd8_2321r_LNP = 0.

double	Cqd8_2322i_LNP = 0.

double	Cqd8_2322r_LNP = 0.

double	Cqd8_2323i_LNP = 0.

double	Cqd8_2323r_LNP = 0.

double	Cqd8_2331i_LNP = 0.

double	Cqd8_2331r_LNP = 0.

double	Cqd8_2332i_LNP = 0.

double	Cqd8_2332r_LNP = 0.

double	Cqd8_2333i_LNP = 0.

double	Cqd8_2333r_LNP = 0.

double	Cqd8_3311r_LNP = 0.

double	Cqd8_3312i_LNP = 0.

double	Cqd8_3312r_LNP = 0.

double	Cqd8_3313i_LNP = 0.

double	Cqd8_3313r_LNP = 0.

double	Cqd8_3322r_LNP = 0.

double	Cqd8_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{qd}^{(8)})_{ijkm}$ (Imaginary part). More...

double	Cqd8_3323r_LNP = 0.

double	Cqd8_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{qd}^{(8)})_{ijkm}$ (Real part and pure real operator). More...

double	Cqe_1111r_LNP = 0.

double	Cqe_1112i_LNP = 0.

double	Cqe_1112r_LNP = 0.

double	Cqe_1113i_LNP = 0.

double	Cqe_1113r_LNP = 0.

double	Cqe_1122r_LNP = 0.

double	Cqe_1123i_LNP = 0.

double	Cqe_1123r_LNP = 0.

double	Cqe_1133r_LNP = 0.

double	Cqe_1211i_LNP = 0.

double	Cqe_1211r_LNP = 0.

double	Cqe_1212i_LNP = 0.

double	Cqe_1212r_LNP = 0.

double	Cqe_1213i_LNP = 0.

double	Cqe_1213r_LNP = 0.

double	Cqe_1221i_LNP = 0.

double	Cqe_1221r_LNP = 0.

double	Cqe_1222i_LNP = 0.

double	Cqe_1222r_LNP = 0.

double	Cqe_1223i_LNP = 0.

double	Cqe_1223r_LNP = 0.

double	Cqe_1231i_LNP = 0.

double	Cqe_1231r_LNP = 0.

double	Cqe_1232i_LNP = 0.

double	Cqe_1232r_LNP = 0.

double	Cqe_1233i_LNP = 0.

double	Cqe_1233r_LNP = 0.

double	Cqe_1311i_LNP = 0.

double	Cqe_1311r_LNP = 0.

double	Cqe_1312i_LNP = 0.

double	Cqe_1312r_LNP = 0.

double	Cqe_1313i_LNP = 0.

double	Cqe_1313r_LNP = 0.

double	Cqe_1321i_LNP = 0.

double	Cqe_1321r_LNP = 0.

double	Cqe_1322i_LNP = 0.

double	Cqe_1322r_LNP = 0.

double	Cqe_1323i_LNP = 0.

double	Cqe_1323r_LNP = 0.

double	Cqe_1331i_LNP = 0.

double	Cqe_1331r_LNP = 0.

double	Cqe_1332i_LNP = 0.

double	Cqe_1332r_LNP = 0.

double	Cqe_1333i_LNP = 0.

double	Cqe_1333r_LNP = 0.

double	Cqe_2211r_LNP = 0.

double	Cqe_2212i_LNP = 0.

double	Cqe_2212r_LNP = 0.

double	Cqe_2213i_LNP = 0.

double	Cqe_2213r_LNP = 0.

double	Cqe_2222r_LNP = 0.

double	Cqe_2223i_LNP = 0.

double	Cqe_2223r_LNP = 0.

double	Cqe_2233r_LNP = 0.

double	Cqe_2311i_LNP = 0.

double	Cqe_2311r_LNP = 0.

double	Cqe_2312i_LNP = 0.

double	Cqe_2312r_LNP = 0.

double	Cqe_2313i_LNP = 0.

double	Cqe_2313r_LNP = 0.

double	Cqe_2321i_LNP = 0.

double	Cqe_2321r_LNP = 0.

double	Cqe_2322i_LNP = 0.

double	Cqe_2322r_LNP = 0.

double	Cqe_2323i_LNP = 0.

double	Cqe_2323r_LNP = 0.

double	Cqe_2331i_LNP = 0.

double	Cqe_2331r_LNP = 0.

double	Cqe_2332i_LNP = 0.

double	Cqe_2332r_LNP = 0.

double	Cqe_2333i_LNP = 0.

double	Cqe_2333r_LNP = 0.

double	Cqe_3311r_LNP = 0.

double	Cqe_3312i_LNP = 0.

double	Cqe_3312r_LNP = 0.

double	Cqe_3313i_LNP = 0.

double	Cqe_3313r_LNP = 0.

double	Cqe_3322r_LNP = 0.

double	Cqe_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{qe})_{ijkm}$ (Imaginary part). More...

double	Cqe_3323r_LNP = 0.

double	Cqe_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{qe})_{ijkm}$ (Real part and pure real operator). More...

double	Cqq1_1111r_LNP = 0.

double	Cqq1_1112i_LNP = 0.

double	Cqq1_1112r_LNP = 0.

double	Cqq1_1113i_LNP = 0.

double	Cqq1_1113r_LNP = 0.

double	Cqq1_1122r_LNP = 0.

double	Cqq1_1123i_LNP = 0.

double	Cqq1_1123r_LNP = 0.

double	Cqq1_1133r_LNP = 0.

double	Cqq1_1212i_LNP = 0.

double	Cqq1_1212r_LNP = 0.

double	Cqq1_1213i_LNP = 0.

double	Cqq1_1213r_LNP = 0.

double	Cqq1_1221r_LNP = 0.

double	Cqq1_1222i_LNP = 0.

double	Cqq1_1222r_LNP = 0.

double	Cqq1_1223i_LNP = 0.

double	Cqq1_1223r_LNP = 0.

double	Cqq1_1231i_LNP = 0.

double	Cqq1_1231r_LNP = 0.

double	Cqq1_1232i_LNP = 0.

double	Cqq1_1232r_LNP = 0.

double	Cqq1_1233i_LNP = 0.

double	Cqq1_1233r_LNP = 0.

double	Cqq1_1313i_LNP = 0.

double	Cqq1_1313r_LNP = 0.

double	Cqq1_1322i_LNP = 0.

double	Cqq1_1322r_LNP = 0.

double	Cqq1_1323i_LNP = 0.

double	Cqq1_1323r_LNP = 0.

double	Cqq1_1331r_LNP = 0.

double	Cqq1_1332i_LNP = 0.

double	Cqq1_1332r_LNP = 0.

double	Cqq1_1333i_LNP = 0.

double	Cqq1_1333r_LNP = 0.

double	Cqq1_2222r_LNP = 0.

double	Cqq1_2223i_LNP = 0.

double	Cqq1_2223r_LNP = 0.

double	Cqq1_2233r_LNP = 0.

double	Cqq1_2323i_LNP = 0.

double	Cqq1_2323r_LNP = 0.

double	Cqq1_2332r_LNP = 0.

double	Cqq1_2333i_LNP = 0.
	The dimension-6 operator coefficient $(C_{qq}^{(1)})_{ijkm}$ (Imaginary part). More...

double	Cqq1_2333r_LNP = 0.

double	Cqq1_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{qq}^{(1)})_{ijkm}$ (Real part and pure real operator). More...

double	Cqq3_1111r_LNP = 0.

double	Cqq3_1112i_LNP = 0.

double	Cqq3_1112r_LNP = 0.

double	Cqq3_1113i_LNP = 0.

double	Cqq3_1113r_LNP = 0.

double	Cqq3_1122r_LNP = 0.

double	Cqq3_1123i_LNP = 0.

double	Cqq3_1123r_LNP = 0.

double	Cqq3_1133r_LNP = 0.

double	Cqq3_1212i_LNP = 0.

double	Cqq3_1212r_LNP = 0.

double	Cqq3_1213i_LNP = 0.

double	Cqq3_1213r_LNP = 0.

double	Cqq3_1221r_LNP = 0.

double	Cqq3_1222i_LNP = 0.

double	Cqq3_1222r_LNP = 0.

double	Cqq3_1223i_LNP = 0.

double	Cqq3_1223r_LNP = 0.

double	Cqq3_1231i_LNP = 0.

double	Cqq3_1231r_LNP = 0.

double	Cqq3_1232i_LNP = 0.

double	Cqq3_1232r_LNP = 0.

double	Cqq3_1233i_LNP = 0.

double	Cqq3_1233r_LNP = 0.

double	Cqq3_1313i_LNP = 0.

double	Cqq3_1313r_LNP = 0.

double	Cqq3_1322i_LNP = 0.

double	Cqq3_1322r_LNP = 0.

double	Cqq3_1323i_LNP = 0.

double	Cqq3_1323r_LNP = 0.

double	Cqq3_1331r_LNP = 0.

double	Cqq3_1332i_LNP = 0.

double	Cqq3_1332r_LNP = 0.

double	Cqq3_1333i_LNP = 0.

double	Cqq3_1333r_LNP = 0.

double	Cqq3_2222r_LNP = 0.

double	Cqq3_2223i_LNP = 0.

double	Cqq3_2223r_LNP = 0.

double	Cqq3_2233r_LNP = 0.

double	Cqq3_2323i_LNP = 0.

double	Cqq3_2323r_LNP = 0.

double	Cqq3_2332r_LNP = 0.

double	Cqq3_2333i_LNP = 0.
	The dimension-6 operator coefficient $(C_{qq}^{(3)})_{ijkm}$ (Imaginary part). More...

double	Cqq3_2333r_LNP = 0.

double	Cqq3_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{qq}^{(3)})_{ijkm}$ (Real part and pure real operator). More...

double	Cqu1_1111r_LNP = 0.

double	Cqu1_1112i_LNP = 0.

double	Cqu1_1112r_LNP = 0.

double	Cqu1_1113i_LNP = 0.

double	Cqu1_1113r_LNP = 0.

double	Cqu1_1122r_LNP = 0.

double	Cqu1_1123i_LNP = 0.

double	Cqu1_1123r_LNP = 0.

double	Cqu1_1133r_LNP = 0.

double	Cqu1_1211i_LNP = 0.

double	Cqu1_1211r_LNP = 0.

double	Cqu1_1212i_LNP = 0.

double	Cqu1_1212r_LNP = 0.

double	Cqu1_1213i_LNP = 0.

double	Cqu1_1213r_LNP = 0.

double	Cqu1_1221i_LNP = 0.

double	Cqu1_1221r_LNP = 0.

double	Cqu1_1222i_LNP = 0.

double	Cqu1_1222r_LNP = 0.

double	Cqu1_1223i_LNP = 0.

double	Cqu1_1223r_LNP = 0.

double	Cqu1_1231i_LNP = 0.

double	Cqu1_1231r_LNP = 0.

double	Cqu1_1232i_LNP = 0.

double	Cqu1_1232r_LNP = 0.

double	Cqu1_1233i_LNP = 0.

double	Cqu1_1233r_LNP = 0.

double	Cqu1_1311i_LNP = 0.

double	Cqu1_1311r_LNP = 0.

double	Cqu1_1312i_LNP = 0.

double	Cqu1_1312r_LNP = 0.

double	Cqu1_1313i_LNP = 0.

double	Cqu1_1313r_LNP = 0.

double	Cqu1_1321i_LNP = 0.

double	Cqu1_1321r_LNP = 0.

double	Cqu1_1322i_LNP = 0.

double	Cqu1_1322r_LNP = 0.

double	Cqu1_1323i_LNP = 0.

double	Cqu1_1323r_LNP = 0.

double	Cqu1_1331i_LNP = 0.

double	Cqu1_1331r_LNP = 0.

double	Cqu1_1332i_LNP = 0.

double	Cqu1_1332r_LNP = 0.

double	Cqu1_1333i_LNP = 0.

double	Cqu1_1333r_LNP = 0.

double	Cqu1_2211r_LNP = 0.

double	Cqu1_2212i_LNP = 0.

double	Cqu1_2212r_LNP = 0.

double	Cqu1_2213i_LNP = 0.

double	Cqu1_2213r_LNP = 0.

double	Cqu1_2222r_LNP = 0.

double	Cqu1_2223i_LNP = 0.

double	Cqu1_2223r_LNP = 0.

double	Cqu1_2233r_LNP = 0.

double	Cqu1_2311i_LNP = 0.

double	Cqu1_2311r_LNP = 0.

double	Cqu1_2312i_LNP = 0.

double	Cqu1_2312r_LNP = 0.

double	Cqu1_2313i_LNP = 0.

double	Cqu1_2313r_LNP = 0.

double	Cqu1_2321i_LNP = 0.

double	Cqu1_2321r_LNP = 0.

double	Cqu1_2322i_LNP = 0.

double	Cqu1_2322r_LNP = 0.

double	Cqu1_2323i_LNP = 0.

double	Cqu1_2323r_LNP = 0.

double	Cqu1_2331i_LNP = 0.

double	Cqu1_2331r_LNP = 0.

double	Cqu1_2332i_LNP = 0.

double	Cqu1_2332r_LNP = 0.

double	Cqu1_2333i_LNP = 0.

double	Cqu1_2333r_LNP = 0.

double	Cqu1_3311r_LNP = 0.

double	Cqu1_3312i_LNP = 0.

double	Cqu1_3312r_LNP = 0.

double	Cqu1_3313i_LNP = 0.

double	Cqu1_3313r_LNP = 0.

double	Cqu1_3322r_LNP = 0.

double	Cqu1_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{qu}^{(1)})_{ijkm}$ (Imaginary part). More...

double	Cqu1_3323r_LNP = 0.

double	Cqu1_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{qu}^{(1)})_{ijkm}$ (Real part and pure real operator). More...

double	Cqu8_1111r_LNP = 0.

double	Cqu8_1112i_LNP = 0.

double	Cqu8_1112r_LNP = 0.

double	Cqu8_1113i_LNP = 0.

double	Cqu8_1113r_LNP = 0.

double	Cqu8_1122r_LNP = 0.

double	Cqu8_1123i_LNP = 0.

double	Cqu8_1123r_LNP = 0.

double	Cqu8_1133r_LNP = 0.

double	Cqu8_1211i_LNP = 0.

double	Cqu8_1211r_LNP = 0.

double	Cqu8_1212i_LNP = 0.

double	Cqu8_1212r_LNP = 0.

double	Cqu8_1213i_LNP = 0.

double	Cqu8_1213r_LNP = 0.

double	Cqu8_1221i_LNP = 0.

double	Cqu8_1221r_LNP = 0.

double	Cqu8_1222i_LNP = 0.

double	Cqu8_1222r_LNP = 0.

double	Cqu8_1223i_LNP = 0.

double	Cqu8_1223r_LNP = 0.

double	Cqu8_1231i_LNP = 0.

double	Cqu8_1231r_LNP = 0.

double	Cqu8_1232i_LNP = 0.

double	Cqu8_1232r_LNP = 0.

double	Cqu8_1233i_LNP = 0.

double	Cqu8_1233r_LNP = 0.

double	Cqu8_1311i_LNP = 0.

double	Cqu8_1311r_LNP = 0.

double	Cqu8_1312i_LNP = 0.

double	Cqu8_1312r_LNP = 0.

double	Cqu8_1313i_LNP = 0.

double	Cqu8_1313r_LNP = 0.

double	Cqu8_1321i_LNP = 0.

double	Cqu8_1321r_LNP = 0.

double	Cqu8_1322i_LNP = 0.

double	Cqu8_1322r_LNP = 0.

double	Cqu8_1323i_LNP = 0.

double	Cqu8_1323r_LNP = 0.

double	Cqu8_1331i_LNP = 0.

double	Cqu8_1331r_LNP = 0.

double	Cqu8_1332i_LNP = 0.

double	Cqu8_1332r_LNP = 0.

double	Cqu8_1333i_LNP = 0.

double	Cqu8_1333r_LNP = 0.

double	Cqu8_2211r_LNP = 0.

double	Cqu8_2212i_LNP = 0.

double	Cqu8_2212r_LNP = 0.

double	Cqu8_2213i_LNP = 0.

double	Cqu8_2213r_LNP = 0.

double	Cqu8_2222r_LNP = 0.

double	Cqu8_2223i_LNP = 0.

double	Cqu8_2223r_LNP = 0.

double	Cqu8_2233r_LNP = 0.

double	Cqu8_2311i_LNP = 0.

double	Cqu8_2311r_LNP = 0.

double	Cqu8_2312i_LNP = 0.

double	Cqu8_2312r_LNP = 0.

double	Cqu8_2313i_LNP = 0.

double	Cqu8_2313r_LNP = 0.

double	Cqu8_2321i_LNP = 0.

double	Cqu8_2321r_LNP = 0.

double	Cqu8_2322i_LNP = 0.

double	Cqu8_2322r_LNP = 0.

double	Cqu8_2323i_LNP = 0.

double	Cqu8_2323r_LNP = 0.

double	Cqu8_2331i_LNP = 0.

double	Cqu8_2331r_LNP = 0.

double	Cqu8_2332i_LNP = 0.

double	Cqu8_2332r_LNP = 0.

double	Cqu8_2333i_LNP = 0.

double	Cqu8_2333r_LNP = 0.

double	Cqu8_3311r_LNP = 0.

double	Cqu8_3312i_LNP = 0.

double	Cqu8_3312r_LNP = 0.

double	Cqu8_3313i_LNP = 0.

double	Cqu8_3313r_LNP = 0.

double	Cqu8_3322r_LNP = 0.

double	Cqu8_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{qu}^{(8)})_{ijkm}$ (Imaginary part). More...

double	Cqu8_3323r_LNP = 0.

double	Cqu8_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{qu}^{(8)})_{ijkm}$ (Real part and pure real operator). More...

double	Cquqd1_1111i_LNP = 0.

double	Cquqd1_1111r_LNP = 0.

double	Cquqd1_1112i_LNP = 0.

double	Cquqd1_1112r_LNP = 0.

double	Cquqd1_1113i_LNP = 0.

double	Cquqd1_1113r_LNP = 0.

double	Cquqd1_1121i_LNP = 0.

double	Cquqd1_1121r_LNP = 0.

double	Cquqd1_1122i_LNP = 0.

double	Cquqd1_1122r_LNP = 0.

double	Cquqd1_1123i_LNP = 0.

double	Cquqd1_1123r_LNP = 0.

double	Cquqd1_1131i_LNP = 0.

double	Cquqd1_1131r_LNP = 0.

double	Cquqd1_1132i_LNP = 0.

double	Cquqd1_1132r_LNP = 0.

double	Cquqd1_1133i_LNP = 0.

double	Cquqd1_1133r_LNP = 0.

double	Cquqd1_1211i_LNP = 0.

double	Cquqd1_1211r_LNP = 0.

double	Cquqd1_1212i_LNP = 0.

double	Cquqd1_1212r_LNP = 0.

double	Cquqd1_1213i_LNP = 0.

double	Cquqd1_1213r_LNP = 0.

double	Cquqd1_1221i_LNP = 0.

double	Cquqd1_1221r_LNP = 0.

double	Cquqd1_1222i_LNP = 0.

double	Cquqd1_1222r_LNP = 0.

double	Cquqd1_1223i_LNP = 0.

double	Cquqd1_1223r_LNP = 0.

double	Cquqd1_1231i_LNP = 0.

double	Cquqd1_1231r_LNP = 0.

double	Cquqd1_1232i_LNP = 0.

double	Cquqd1_1232r_LNP = 0.

double	Cquqd1_1233i_LNP = 0.

double	Cquqd1_1233r_LNP = 0.

double	Cquqd1_1311i_LNP = 0.

double	Cquqd1_1311r_LNP = 0.

double	Cquqd1_1312i_LNP = 0.

double	Cquqd1_1312r_LNP = 0.

double	Cquqd1_1313i_LNP = 0.

double	Cquqd1_1313r_LNP = 0.

double	Cquqd1_1321i_LNP = 0.

double	Cquqd1_1321r_LNP = 0.

double	Cquqd1_1322i_LNP = 0.

double	Cquqd1_1322r_LNP = 0.

double	Cquqd1_1323i_LNP = 0.

double	Cquqd1_1323r_LNP = 0.

double	Cquqd1_1331i_LNP = 0.

double	Cquqd1_1331r_LNP = 0.

double	Cquqd1_1332i_LNP = 0.

double	Cquqd1_1332r_LNP = 0.

double	Cquqd1_1333i_LNP = 0.

double	Cquqd1_1333r_LNP = 0.

double	Cquqd1_2111i_LNP = 0.

double	Cquqd1_2111r_LNP = 0.

double	Cquqd1_2112i_LNP = 0.

double	Cquqd1_2112r_LNP = 0.

double	Cquqd1_2113i_LNP = 0.

double	Cquqd1_2113r_LNP = 0.

double	Cquqd1_2121i_LNP = 0.

double	Cquqd1_2121r_LNP = 0.

double	Cquqd1_2122i_LNP = 0.

double	Cquqd1_2122r_LNP = 0.

double	Cquqd1_2123i_LNP = 0.

double	Cquqd1_2123r_LNP = 0.

double	Cquqd1_2131i_LNP = 0.

double	Cquqd1_2131r_LNP = 0.

double	Cquqd1_2132i_LNP = 0.

double	Cquqd1_2132r_LNP = 0.

double	Cquqd1_2133i_LNP = 0.

double	Cquqd1_2133r_LNP = 0.

double	Cquqd1_2211i_LNP = 0.

double	Cquqd1_2211r_LNP = 0.

double	Cquqd1_2212i_LNP = 0.

double	Cquqd1_2212r_LNP = 0.

double	Cquqd1_2213i_LNP = 0.

double	Cquqd1_2213r_LNP = 0.

double	Cquqd1_2221i_LNP = 0.

double	Cquqd1_2221r_LNP = 0.

double	Cquqd1_2222i_LNP = 0.

double	Cquqd1_2222r_LNP = 0.

double	Cquqd1_2223i_LNP = 0.

double	Cquqd1_2223r_LNP = 0.

double	Cquqd1_2231i_LNP = 0.

double	Cquqd1_2231r_LNP = 0.

double	Cquqd1_2232i_LNP = 0.

double	Cquqd1_2232r_LNP = 0.

double	Cquqd1_2233i_LNP = 0.

double	Cquqd1_2233r_LNP = 0.

double	Cquqd1_2311i_LNP = 0.

double	Cquqd1_2311r_LNP = 0.

double	Cquqd1_2312i_LNP = 0.

double	Cquqd1_2312r_LNP = 0.

double	Cquqd1_2313i_LNP = 0.

double	Cquqd1_2313r_LNP = 0.

double	Cquqd1_2321i_LNP = 0.

double	Cquqd1_2321r_LNP = 0.

double	Cquqd1_2322i_LNP = 0.

double	Cquqd1_2322r_LNP = 0.

double	Cquqd1_2323i_LNP = 0.

double	Cquqd1_2323r_LNP = 0.

double	Cquqd1_2331i_LNP = 0.

double	Cquqd1_2331r_LNP = 0.

double	Cquqd1_2332i_LNP = 0.

double	Cquqd1_2332r_LNP = 0.

double	Cquqd1_2333i_LNP = 0.

double	Cquqd1_2333r_LNP = 0.

double	Cquqd1_3111i_LNP = 0.

double	Cquqd1_3111r_LNP = 0.

double	Cquqd1_3112i_LNP = 0.

double	Cquqd1_3112r_LNP = 0.

double	Cquqd1_3113i_LNP = 0.

double	Cquqd1_3113r_LNP = 0.

double	Cquqd1_3121i_LNP = 0.

double	Cquqd1_3121r_LNP = 0.

double	Cquqd1_3122i_LNP = 0.

double	Cquqd1_3122r_LNP = 0.

double	Cquqd1_3123i_LNP = 0.

double	Cquqd1_3123r_LNP = 0.

double	Cquqd1_3131i_LNP = 0.

double	Cquqd1_3131r_LNP = 0.

double	Cquqd1_3132i_LNP = 0.

double	Cquqd1_3132r_LNP = 0.

double	Cquqd1_3133i_LNP = 0.

double	Cquqd1_3133r_LNP = 0.

double	Cquqd1_3211i_LNP = 0.

double	Cquqd1_3211r_LNP = 0.

double	Cquqd1_3212i_LNP = 0.

double	Cquqd1_3212r_LNP = 0.

double	Cquqd1_3213i_LNP = 0.

double	Cquqd1_3213r_LNP = 0.

double	Cquqd1_3221i_LNP = 0.

double	Cquqd1_3221r_LNP = 0.

double	Cquqd1_3222i_LNP = 0.

double	Cquqd1_3222r_LNP = 0.

double	Cquqd1_3223i_LNP = 0.

double	Cquqd1_3223r_LNP = 0.

double	Cquqd1_3231i_LNP = 0.

double	Cquqd1_3231r_LNP = 0.

double	Cquqd1_3232i_LNP = 0.

double	Cquqd1_3232r_LNP = 0.

double	Cquqd1_3233i_LNP = 0.

double	Cquqd1_3233r_LNP = 0.

double	Cquqd1_3311i_LNP = 0.

double	Cquqd1_3311r_LNP = 0.

double	Cquqd1_3312i_LNP = 0.

double	Cquqd1_3312r_LNP = 0.

double	Cquqd1_3313i_LNP = 0.

double	Cquqd1_3313r_LNP = 0.

double	Cquqd1_3321i_LNP = 0.

double	Cquqd1_3321r_LNP = 0.

double	Cquqd1_3322i_LNP = 0.

double	Cquqd1_3322r_LNP = 0.

double	Cquqd1_3323i_LNP = 0.

double	Cquqd1_3323r_LNP = 0.

double	Cquqd1_3331i_LNP = 0.

double	Cquqd1_3331r_LNP = 0.

double	Cquqd1_3332i_LNP = 0.

double	Cquqd1_3332r_LNP = 0.

double	Cquqd1_3333i_LNP = 0.
	The dimension-6 operator coefficient $(C_{quqd}^{(1)})_{ijkm}$ (Imaginary part). More...

double	Cquqd1_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{quqd}^{(1)})_{ijkm}$ (Real part and pure real operator). More...

double	Cquqd8_1111i_LNP = 0.

double	Cquqd8_1111r_LNP = 0.

double	Cquqd8_1112i_LNP = 0.

double	Cquqd8_1112r_LNP = 0.

double	Cquqd8_1113i_LNP = 0.

double	Cquqd8_1113r_LNP = 0.

double	Cquqd8_1121i_LNP = 0.

double	Cquqd8_1121r_LNP = 0.

double	Cquqd8_1122i_LNP = 0.

double	Cquqd8_1122r_LNP = 0.

double	Cquqd8_1123i_LNP = 0.

double	Cquqd8_1123r_LNP = 0.

double	Cquqd8_1131i_LNP = 0.

double	Cquqd8_1131r_LNP = 0.

double	Cquqd8_1132i_LNP = 0.

double	Cquqd8_1132r_LNP = 0.

double	Cquqd8_1133i_LNP = 0.

double	Cquqd8_1133r_LNP = 0.

double	Cquqd8_1211i_LNP = 0.

double	Cquqd8_1211r_LNP = 0.

double	Cquqd8_1212i_LNP = 0.

double	Cquqd8_1212r_LNP = 0.

double	Cquqd8_1213i_LNP = 0.

double	Cquqd8_1213r_LNP = 0.

double	Cquqd8_1221i_LNP = 0.

double	Cquqd8_1221r_LNP = 0.

double	Cquqd8_1222i_LNP = 0.

double	Cquqd8_1222r_LNP = 0.

double	Cquqd8_1223i_LNP = 0.

double	Cquqd8_1223r_LNP = 0.

double	Cquqd8_1231i_LNP = 0.

double	Cquqd8_1231r_LNP = 0.

double	Cquqd8_1232i_LNP = 0.

double	Cquqd8_1232r_LNP = 0.

double	Cquqd8_1233i_LNP = 0.

double	Cquqd8_1233r_LNP = 0.

double	Cquqd8_1311i_LNP = 0.

double	Cquqd8_1311r_LNP = 0.

double	Cquqd8_1312i_LNP = 0.

double	Cquqd8_1312r_LNP = 0.

double	Cquqd8_1313i_LNP = 0.

double	Cquqd8_1313r_LNP = 0.

double	Cquqd8_1321i_LNP = 0.

double	Cquqd8_1321r_LNP = 0.

double	Cquqd8_1322i_LNP = 0.

double	Cquqd8_1322r_LNP = 0.

double	Cquqd8_1323i_LNP = 0.

double	Cquqd8_1323r_LNP = 0.

double	Cquqd8_1331i_LNP = 0.

double	Cquqd8_1331r_LNP = 0.

double	Cquqd8_1332i_LNP = 0.

double	Cquqd8_1332r_LNP = 0.

double	Cquqd8_1333i_LNP = 0.

double	Cquqd8_1333r_LNP = 0.

double	Cquqd8_2111i_LNP = 0.

double	Cquqd8_2111r_LNP = 0.

double	Cquqd8_2112i_LNP = 0.

double	Cquqd8_2112r_LNP = 0.

double	Cquqd8_2113i_LNP = 0.

double	Cquqd8_2113r_LNP = 0.

double	Cquqd8_2121i_LNP = 0.

double	Cquqd8_2121r_LNP = 0.

double	Cquqd8_2122i_LNP = 0.

double	Cquqd8_2122r_LNP = 0.

double	Cquqd8_2123i_LNP = 0.

double	Cquqd8_2123r_LNP = 0.

double	Cquqd8_2131i_LNP = 0.

double	Cquqd8_2131r_LNP = 0.

double	Cquqd8_2132i_LNP = 0.

double	Cquqd8_2132r_LNP = 0.

double	Cquqd8_2133i_LNP = 0.

double	Cquqd8_2133r_LNP = 0.

double	Cquqd8_2211i_LNP = 0.

double	Cquqd8_2211r_LNP = 0.

double	Cquqd8_2212i_LNP = 0.

double	Cquqd8_2212r_LNP = 0.

double	Cquqd8_2213i_LNP = 0.

double	Cquqd8_2213r_LNP = 0.

double	Cquqd8_2221i_LNP = 0.

double	Cquqd8_2221r_LNP = 0.

double	Cquqd8_2222i_LNP = 0.

double	Cquqd8_2222r_LNP = 0.

double	Cquqd8_2223i_LNP = 0.

double	Cquqd8_2223r_LNP = 0.

double	Cquqd8_2231i_LNP = 0.

double	Cquqd8_2231r_LNP = 0.

double	Cquqd8_2232i_LNP = 0.

double	Cquqd8_2232r_LNP = 0.

double	Cquqd8_2233i_LNP = 0.

double	Cquqd8_2233r_LNP = 0.

double	Cquqd8_2311i_LNP = 0.

double	Cquqd8_2311r_LNP = 0.

double	Cquqd8_2312i_LNP = 0.

double	Cquqd8_2312r_LNP = 0.

double	Cquqd8_2313i_LNP = 0.

double	Cquqd8_2313r_LNP = 0.

double	Cquqd8_2321i_LNP = 0.

double	Cquqd8_2321r_LNP = 0.

double	Cquqd8_2322i_LNP = 0.

double	Cquqd8_2322r_LNP = 0.

double	Cquqd8_2323i_LNP = 0.

double	Cquqd8_2323r_LNP = 0.

double	Cquqd8_2331i_LNP = 0.

double	Cquqd8_2331r_LNP = 0.

double	Cquqd8_2332i_LNP = 0.

double	Cquqd8_2332r_LNP = 0.

double	Cquqd8_2333i_LNP = 0.

double	Cquqd8_2333r_LNP = 0.

double	Cquqd8_3111i_LNP = 0.

double	Cquqd8_3111r_LNP = 0.

double	Cquqd8_3112i_LNP = 0.

double	Cquqd8_3112r_LNP = 0.

double	Cquqd8_3113i_LNP = 0.

double	Cquqd8_3113r_LNP = 0.

double	Cquqd8_3121i_LNP = 0.

double	Cquqd8_3121r_LNP = 0.

double	Cquqd8_3122i_LNP = 0.

double	Cquqd8_3122r_LNP = 0.

double	Cquqd8_3123i_LNP = 0.

double	Cquqd8_3123r_LNP = 0.

double	Cquqd8_3131i_LNP = 0.

double	Cquqd8_3131r_LNP = 0.

double	Cquqd8_3132i_LNP = 0.

double	Cquqd8_3132r_LNP = 0.

double	Cquqd8_3133i_LNP = 0.

double	Cquqd8_3133r_LNP = 0.

double	Cquqd8_3211i_LNP = 0.

double	Cquqd8_3211r_LNP = 0.

double	Cquqd8_3212i_LNP = 0.

double	Cquqd8_3212r_LNP = 0.

double	Cquqd8_3213i_LNP = 0.

double	Cquqd8_3213r_LNP = 0.

double	Cquqd8_3221i_LNP = 0.

double	Cquqd8_3221r_LNP = 0.

double	Cquqd8_3222i_LNP = 0.

double	Cquqd8_3222r_LNP = 0.

double	Cquqd8_3223i_LNP = 0.

double	Cquqd8_3223r_LNP = 0.

double	Cquqd8_3231i_LNP = 0.

double	Cquqd8_3231r_LNP = 0.

double	Cquqd8_3232i_LNP = 0.

double	Cquqd8_3232r_LNP = 0.

double	Cquqd8_3233i_LNP = 0.

double	Cquqd8_3233r_LNP = 0.

double	Cquqd8_3311i_LNP = 0.

double	Cquqd8_3311r_LNP = 0.

double	Cquqd8_3312i_LNP = 0.

double	Cquqd8_3312r_LNP = 0.

double	Cquqd8_3313i_LNP = 0.

double	Cquqd8_3313r_LNP = 0.

double	Cquqd8_3321i_LNP = 0.

double	Cquqd8_3321r_LNP = 0.

double	Cquqd8_3322i_LNP = 0.

double	Cquqd8_3322r_LNP = 0.

double	Cquqd8_3323i_LNP = 0.

double	Cquqd8_3323r_LNP = 0.

double	Cquqd8_3331i_LNP = 0.

double	Cquqd8_3331r_LNP = 0.

double	Cquqd8_3332i_LNP = 0.

double	Cquqd8_3332r_LNP = 0.

double	Cquqd8_3333i_LNP = 0.
	The dimension-6 operator coefficient $(C_{quqd}^{(8)})_{ijkm}$ (Imaginary part). More...

double	Cquqd8_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{quqd}^{(8)})_{ijkm}$ (Real part and pure real operator). More...

double	CuB_11i_LNP = 0.

double	CuB_11r_LNP = 0.

double	CuB_12i_LNP = 0.

double	CuB_12r_LNP = 0.

double	CuB_13i_LNP = 0.

double	CuB_13r_LNP = 0.

double	CuB_21i_LNP = 0.

double	CuB_21r_LNP = 0.

double	CuB_22i_LNP = 0.

double	CuB_22r_LNP = 0.

double	CuB_23i_LNP = 0.

double	CuB_23r_LNP = 0.

double	CuB_31i_LNP = 0.

double	CuB_31r_LNP = 0.

double	CuB_32i_LNP = 0.

double	CuB_32r_LNP = 0.

double	CuB_33i_LNP = 0.
	The dimension-6 operator coefficient $(C_{uB})_{ij}$ (Imaginary part). More...

double	CuB_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{uB})_{ij}$ (Real part and pure real operator). More...

double	Cud1_1111r_LNP = 0.

double	Cud1_1112i_LNP = 0.

double	Cud1_1112r_LNP = 0.

double	Cud1_1113i_LNP = 0.

double	Cud1_1113r_LNP = 0.

double	Cud1_1122r_LNP = 0.

double	Cud1_1123i_LNP = 0.

double	Cud1_1123r_LNP = 0.

double	Cud1_1133r_LNP = 0.

double	Cud1_1211i_LNP = 0.

double	Cud1_1211r_LNP = 0.

double	Cud1_1212i_LNP = 0.

double	Cud1_1212r_LNP = 0.

double	Cud1_1213i_LNP = 0.

double	Cud1_1213r_LNP = 0.

double	Cud1_1221i_LNP = 0.

double	Cud1_1221r_LNP = 0.

double	Cud1_1222i_LNP = 0.

double	Cud1_1222r_LNP = 0.

double	Cud1_1223i_LNP = 0.

double	Cud1_1223r_LNP = 0.

double	Cud1_1231i_LNP = 0.

double	Cud1_1231r_LNP = 0.

double	Cud1_1232i_LNP = 0.

double	Cud1_1232r_LNP = 0.

double	Cud1_1233i_LNP = 0.

double	Cud1_1233r_LNP = 0.

double	Cud1_1311i_LNP = 0.

double	Cud1_1311r_LNP = 0.

double	Cud1_1312i_LNP = 0.

double	Cud1_1312r_LNP = 0.

double	Cud1_1313i_LNP = 0.

double	Cud1_1313r_LNP = 0.

double	Cud1_1321i_LNP = 0.

double	Cud1_1321r_LNP = 0.

double	Cud1_1322i_LNP = 0.

double	Cud1_1322r_LNP = 0.

double	Cud1_1323i_LNP = 0.

double	Cud1_1323r_LNP = 0.

double	Cud1_1331i_LNP = 0.

double	Cud1_1331r_LNP = 0.

double	Cud1_1332i_LNP = 0.

double	Cud1_1332r_LNP = 0.

double	Cud1_1333i_LNP = 0.

double	Cud1_1333r_LNP = 0.

double	Cud1_2211r_LNP = 0.

double	Cud1_2212i_LNP = 0.

double	Cud1_2212r_LNP = 0.

double	Cud1_2213i_LNP = 0.

double	Cud1_2213r_LNP = 0.

double	Cud1_2222r_LNP = 0.

double	Cud1_2223i_LNP = 0.

double	Cud1_2223r_LNP = 0.

double	Cud1_2233r_LNP = 0.

double	Cud1_2311i_LNP = 0.

double	Cud1_2311r_LNP = 0.

double	Cud1_2312i_LNP = 0.

double	Cud1_2312r_LNP = 0.

double	Cud1_2313i_LNP = 0.

double	Cud1_2313r_LNP = 0.

double	Cud1_2321i_LNP = 0.

double	Cud1_2321r_LNP = 0.

double	Cud1_2322i_LNP = 0.

double	Cud1_2322r_LNP = 0.

double	Cud1_2323i_LNP = 0.

double	Cud1_2323r_LNP = 0.

double	Cud1_2331i_LNP = 0.

double	Cud1_2331r_LNP = 0.

double	Cud1_2332i_LNP = 0.

double	Cud1_2332r_LNP = 0.

double	Cud1_2333i_LNP = 0.

double	Cud1_2333r_LNP = 0.

double	Cud1_3311r_LNP = 0.

double	Cud1_3312i_LNP = 0.

double	Cud1_3312r_LNP = 0.

double	Cud1_3313i_LNP = 0.

double	Cud1_3313r_LNP = 0.

double	Cud1_3322r_LNP = 0.

double	Cud1_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{ud}^{(1)})_{ijkm}$ (Imaginary part). More...

double	Cud1_3323r_LNP = 0.

double	Cud1_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{ud}^{(1)})_{ijkm}$ (Real part and pure real operator). More...

double	Cud8_1111r_LNP = 0.

double	Cud8_1112i_LNP = 0.

double	Cud8_1112r_LNP = 0.

double	Cud8_1113i_LNP = 0.

double	Cud8_1113r_LNP = 0.

double	Cud8_1122r_LNP = 0.

double	Cud8_1123i_LNP = 0.

double	Cud8_1123r_LNP = 0.

double	Cud8_1133r_LNP = 0.

double	Cud8_1211i_LNP = 0.

double	Cud8_1211r_LNP = 0.

double	Cud8_1212i_LNP = 0.

double	Cud8_1212r_LNP = 0.

double	Cud8_1213i_LNP = 0.

double	Cud8_1213r_LNP = 0.

double	Cud8_1221i_LNP = 0.

double	Cud8_1221r_LNP = 0.

double	Cud8_1222i_LNP = 0.

double	Cud8_1222r_LNP = 0.

double	Cud8_1223i_LNP = 0.

double	Cud8_1223r_LNP = 0.

double	Cud8_1231i_LNP = 0.

double	Cud8_1231r_LNP = 0.

double	Cud8_1232i_LNP = 0.

double	Cud8_1232r_LNP = 0.

double	Cud8_1233i_LNP = 0.

double	Cud8_1233r_LNP = 0.

double	Cud8_1311i_LNP = 0.

double	Cud8_1311r_LNP = 0.

double	Cud8_1312i_LNP = 0.

double	Cud8_1312r_LNP = 0.

double	Cud8_1313i_LNP = 0.

double	Cud8_1313r_LNP = 0.

double	Cud8_1321i_LNP = 0.

double	Cud8_1321r_LNP = 0.

double	Cud8_1322i_LNP = 0.

double	Cud8_1322r_LNP = 0.

double	Cud8_1323i_LNP = 0.

double	Cud8_1323r_LNP = 0.

double	Cud8_1331i_LNP = 0.

double	Cud8_1331r_LNP = 0.

double	Cud8_1332i_LNP = 0.

double	Cud8_1332r_LNP = 0.

double	Cud8_1333i_LNP = 0.

double	Cud8_1333r_LNP = 0.

double	Cud8_2211r_LNP = 0.

double	Cud8_2212i_LNP = 0.

double	Cud8_2212r_LNP = 0.

double	Cud8_2213i_LNP = 0.

double	Cud8_2213r_LNP = 0.

double	Cud8_2222r_LNP = 0.

double	Cud8_2223i_LNP = 0.

double	Cud8_2223r_LNP = 0.

double	Cud8_2233r_LNP = 0.

double	Cud8_2311i_LNP = 0.

double	Cud8_2311r_LNP = 0.

double	Cud8_2312i_LNP = 0.

double	Cud8_2312r_LNP = 0.

double	Cud8_2313i_LNP = 0.

double	Cud8_2313r_LNP = 0.

double	Cud8_2321i_LNP = 0.

double	Cud8_2321r_LNP = 0.

double	Cud8_2322i_LNP = 0.

double	Cud8_2322r_LNP = 0.

double	Cud8_2323i_LNP = 0.

double	Cud8_2323r_LNP = 0.

double	Cud8_2331i_LNP = 0.

double	Cud8_2331r_LNP = 0.

double	Cud8_2332i_LNP = 0.

double	Cud8_2332r_LNP = 0.

double	Cud8_2333i_LNP = 0.

double	Cud8_2333r_LNP = 0.

double	Cud8_3311r_LNP = 0.

double	Cud8_3312i_LNP = 0.

double	Cud8_3312r_LNP = 0.

double	Cud8_3313i_LNP = 0.

double	Cud8_3313r_LNP = 0.

double	Cud8_3322r_LNP = 0.

double	Cud8_3323i_LNP = 0.
	The dimension-6 operator coefficient $(C_{ud}^{(8)})_{ijkm}$ (Imaginary part). More...

double	Cud8_3323r_LNP = 0.

double	Cud8_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{ud}^{(8)})_{ijkm}$ (Real part and pure real operator). More...

double	CuG_11i_LNP = 0.

double	CuG_11r_LNP = 0.

double	CuG_12i_LNP = 0.

double	CuG_12r_LNP = 0.

double	CuG_13i_LNP = 0.

double	CuG_13r_LNP = 0.

double	CuG_21i_LNP = 0.

double	CuG_21r_LNP = 0.

double	CuG_22i_LNP = 0.

double	CuG_22r_LNP = 0.

double	CuG_23i_LNP = 0.

double	CuG_23r_LNP = 0.

double	CuG_31i_LNP = 0.

double	CuG_31r_LNP = 0.

double	CuG_32i_LNP = 0.

double	CuG_32r_LNP = 0.

double	CuG_33i_LNP = 0.
	The dimension-6 operator coefficient $(C_{uG})_{ij}$ (Imaginary part). More...

double	CuG_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{uG})_{ij}$ (Real part and pure real operator). More...

double	CuH_11i_LNP = 0.

double	CuH_11r_LNP = 0.

double	CuH_12i_LNP = 0.

double	CuH_12r_LNP = 0.

double	CuH_13i_LNP = 0.

double	CuH_13r_LNP = 0.

double	CuH_21i_LNP = 0.

double	CuH_21r_LNP = 0.

double	CuH_22i_LNP = 0.

double	CuH_22r_LNP = 0.

double	CuH_23i_LNP = 0.

double	CuH_23r_LNP = 0.

double	CuH_31i_LNP = 0.

double	CuH_31r_LNP = 0.

double	CuH_32i_LNP = 0.

double	CuH_32r_LNP = 0.

double	CuH_33i_LNP = 0.
	The dimension-6 operator coefficient $(C_{uH})_{ij}$ (Imaginary part). More...

double	CuH_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{uH})_{ij}$ (Real part and pure real operator). More...

double	Cuu_1111r_LNP = 0.

double	Cuu_1112i_LNP = 0.

double	Cuu_1112r_LNP = 0.

double	Cuu_1113i_LNP = 0.

double	Cuu_1113r_LNP = 0.

double	Cuu_1122r_LNP = 0.

double	Cuu_1123i_LNP = 0.

double	Cuu_1123r_LNP = 0.

double	Cuu_1133r_LNP = 0.

double	Cuu_1212i_LNP = 0.

double	Cuu_1212r_LNP = 0.

double	Cuu_1213i_LNP = 0.

double	Cuu_1213r_LNP = 0.

double	Cuu_1221r_LNP = 0.

double	Cuu_1222i_LNP = 0.

double	Cuu_1222r_LNP = 0.

double	Cuu_1223i_LNP = 0.

double	Cuu_1223r_LNP = 0.

double	Cuu_1231i_LNP = 0.

double	Cuu_1231r_LNP = 0.

double	Cuu_1232i_LNP = 0.

double	Cuu_1232r_LNP = 0.

double	Cuu_1233i_LNP = 0.

double	Cuu_1233r_LNP = 0.

double	Cuu_1313i_LNP = 0.

double	Cuu_1313r_LNP = 0.

double	Cuu_1322i_LNP = 0.

double	Cuu_1322r_LNP = 0.

double	Cuu_1323i_LNP = 0.

double	Cuu_1323r_LNP = 0.

double	Cuu_1331r_LNP = 0.

double	Cuu_1332i_LNP = 0.

double	Cuu_1332r_LNP = 0.

double	Cuu_1333i_LNP = 0.

double	Cuu_1333r_LNP = 0.

double	Cuu_2222r_LNP = 0.

double	Cuu_2223i_LNP = 0.

double	Cuu_2223r_LNP = 0.

double	Cuu_2233r_LNP = 0.

double	Cuu_2323i_LNP = 0.

double	Cuu_2323r_LNP = 0.

double	Cuu_2332r_LNP = 0.

double	Cuu_2333i_LNP = 0.
	The dimension-6 operator coefficient $(C_{uu})_{ijkm}$ (Imaginary part). More...

double	Cuu_2333r_LNP = 0.

double	Cuu_3333r_LNP = 0.
	The dimension-6 operator coefficient $(C_{uu})_{ijkm}$ (Real part and pure real operator). More...

double	CuW_11i_LNP = 0.

double	CuW_11r_LNP = 0.

double	CuW_12i_LNP = 0.

double	CuW_12r_LNP = 0.

double	CuW_13i_LNP = 0.

double	CuW_13r_LNP = 0.

double	CuW_21i_LNP = 0.

double	CuW_21r_LNP = 0.

double	CuW_22i_LNP = 0.

double	CuW_22r_LNP = 0.

double	CuW_23i_LNP = 0.

double	CuW_23r_LNP = 0.

double	CuW_31i_LNP = 0.

double	CuW_31r_LNP = 0.

double	CuW_32i_LNP = 0.

double	CuW_32r_LNP = 0.

double	CuW_33i_LNP = 0.
	The dimension-6 operator coefficient $(C_{uW})_{ij}$ (Imaginary part). More...

double	CuW_33r_LNP = 0.
	The dimension-6 operator coefficient $(C_{uW})_{ij}$ (Real part and pure real operator). More...

double	cW2_tree
	The square of the tree level values for the cosine of the weak angle. More...

double	CW_LNP = 0.
	The dimension-6 operator coefficient $C_{W}$. More...

double	cW_tree
	The tree level values for the cosine of the weak angle. More...

double	cWsch
	Parameters to control the SM EW input scheme: Alpha or MW. More...

double	CWtilde_LNP = 0.
	The dimension-6 operator coefficient $C_{\tilde{W}}$. More...

double	dCKM_LEW = 0.

double	delta_A
	Combination of dimension 6 coefficients modifying the $A_\mu$ canonical field definition for EWPO. More...

double	delta_AA
	Combination of dimension 6 coefficients modifying the $A_\mu$ canonical field definition. More...

double	delta_ale
	The $\mathcal{O}(\Lambda^{-2})$ dimension 6 correction to the electromagnetic coupling. More...

double	delta_ale_2
	The $\mathcal{O}(\Lambda^{-4})$ dimension 6 correction to the electromagnetic coupling. More...

double	delta_AZ
	Combination of dimension 6 coefficients modifying the $A_\mu$ canonical field definition. More...

double	delta_e
	The dimension 6 correction to the electric constant parameter. More...

double	delta_em
	The relative dimension 6 correction to the QED interaction vertex. More...

double	delta_g1
	The $\mathcal{O}(\Lambda^{-2})$ dimension 6 correction to the $U(1)_Y$ gauge coupling, for the Alpha-Scheme (cAsch=1, cWsch=0) or the Mw-Scheme (cAsch=0, cWsch=1). More...

double	delta_g1_2
	The $\mathcal{O}(\Lambda^{-4})$ dimension 6 correction to the $U(1)_Y$ gauge coupling. More...

double	delta_g2
	The $\mathcal{O}(\Lambda^{-2})$ dimension 6 correction to the $SU(2)_L$ gauge coupling, for the Alpha-Scheme (cAsch=1, cWsch=0) or the Mw-Scheme (cAsch=0, cWsch=1). More...

double	delta_g2_2
	The $\mathcal{O}(\Lambda^{-4})$ dimension 6 correction to the $SU(2)_L$ gauge coupling. More...

double	delta_GF
	The dimension 6 correction to the Fermi constant, as extracted from muon decay. More...

double	delta_GF_2
	The $\mathcal{O}(\Lambda^{-4})$ dimension 6 correction to the Fermi constant. More...

double	delta_h
	Combinations of dimension 6 coefficients modifying the $H$ canonical field definition. More...

double	delta_MW
	The dimension 6 correction to W mass Lagrangian parameter. More...

double	delta_MZ
	The dimension 6 correction to Z mass Lagrangian parameter. More...

double	delta_Mz2
	The $\mathcal{O}(\Lambda^{-2})$ dimension 6 correction to the Z-boson mass squared. More...

double	delta_Mz2_2
	The $\mathcal{O}(\Lambda^{-4})$ dimension 6 correction to the Z-boson mass squared. More...

double	delta_QgNC
	The dimension 6 charge correction to neutral current EW couplings. More...

double	delta_sW2
	The dimension 6 correction to the weak mixing angle. More...

double	delta_UgCC
	The dimension 6 universal correction to charged current EW couplings. More...

double	delta_UgNC
	The dimension 6 universal correction to neutral current EW couplings. More...

double	delta_v
	The dimension 6 correction to the vev, as extracted from GF. More...

double	delta_xBZ
	The $\mathcal{O}(\Lambda^{-2})$ dimension 6 correction to the component of the matrix that transform the gauge field $B_{\mu}$ into $Z_{\mu}$. More...

double	delta_xBZ_2
	The $\mathcal{O}(\Lambda^{-4})$ dimension 6 correction to the component of the matrix that transform the gauge field $B_{\mu}$ into $Z_{\mu}$. More...

double	delta_xWZ
	The $\mathcal{O}(\Lambda^{-2})$ dimension 6 correction to the component of the matrix that transform the gauge field $W_{\mu}^3$ into $Z_{\mu}$. More...

double	delta_xWZ_2
	The $\mathcal{O}(\Lambda^{-4})$ dimension 6 correction to the component of the matrix that transform the gauge field $W_{\mu}^3$ into $Z_{\mu}$. More...

double	delta_Z
	Combination of dimension 6 coefficients modifying the $Z_\mu$ canonical field definition for EWPO. More...

double	delta_ZA
	Combination of dimension 6 coefficients modifying the $A_\mu$ canonical field definition for EWPO. More...

double	delta_ZZ
	Combination of dimension 6 coefficients modifying the $Z_\mu$ canonical field definition. More...

double	dGammaHTotR1

double	dGammaHTotR2

double	dZH

double	dZH1

double	dZH2
	Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization and combinations entering in the linear and quadratic pieces. More...

double	edeeWWdcint = 0.
	Intrinsic relative theoretical error in $e^+ e^- \to W^+ W^-$: total cross section and $d/d\cos{\theta}$ distribution. More...

double	eeettHint = 0.
	Intrinsic relative theoretical error in $e^+ e^- \to t \bar{t} H$. (Assumed to be constant in energy.) More...

double	eeettHpar = 0.
	Parametric relative theoretical error in $e^+ e^- \to t \bar{t} H$. (Assumed to be constant in energy.) More...

double	eeeWBFint = 0.
	Intrinsic relative theoretical error in $e^+ e^- \to H \bar{\nu} \nu$. (Assumed to be constant in energy.) More...

double	eeeWBFpar = 0.
	Parametric relative theoretical error in $e^+ e^- \to H \bar{\nu} \nu$. (Assumed to be constant in energy.) More...

double	eeeWWint = 0.

double	eeeZHint = 0.
	Intrinsic relative theoretical error in $e^+ e^- \to Z H$. (Assumed to be constant in energy.) More...

double	eeeZHpar = 0.
	Parametric relative theoretical error in $e^+ e^- \to Z H$. (Assumed to be constant in energy.) More...

double	eeMz
	The em coupling at Mz. More...

double	eeMz2
	The em coupling squared (at Mz). More...

double	eepWBFint = 0.
	Intrinsic relative theoretical error in $e^- p \to H e^- j$ via WBF. (Assumed to be constant in energy.) More...

double	eepWBFpar = 0.
	Parametric relative theoretical error in $e^- p \to H e^- j$ via WBF. (Assumed to be constant in energy.) More...

double	eepZBFint = 0.
	Intrinsic relative theoretical error in $e^- p \to H e^- j$ via ZBF. (Assumed to be constant in energy.) More...

double	eepZBFpar = 0.
	Parametric relative theoretical error in $e^- p \to H e^- j$ via ZBF. (Assumed to be constant in energy.) More...

double	eggFHbb = 0.

double	eggFHgaga = 0.

double	eggFHmumu = 0.
	Total relative theoretical error in $gg \to H \to X$. More...

double	eggFHtautau = 0.

double	eggFHWW = 0.

double	eggFHZga = 0.

double	eggFHZZ = 0.

double	eggFint = 0.
	Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.) More...

double	eggFpar = 0.
	Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.) More...

double	eHbbint = 0.
	Intrinsic relative theoretical error in $H \to b\bar{b}$. More...

double	eHbbpar = 0.
	Parametric relative theoretical error in $H \to b\bar{b}$. More...

double	eHccint = 0.
	Intrinsic relative theoretical error in $H \to c\bar{c}$. More...

double	eHccpar = 0.
	Parametric relative theoretical error in $H \to c\bar{c}$. More...

double	eHgagaint = 0.
	Intrinsic relative theoretical error in $H \to \gamma\gamma$. More...

double	eHgagapar = 0.
	Parametric relative theoretical error in $H \to \gamma\gamma$. More...

double	eHggint = 0.
	Intrinsic relative theoretical error in $H \to g g$. More...

double	eHggpar = 0.
	Parametric relative theoretical error in $H \to g g$. More...

double	eHmumuint = 0.
	Intrinsic relative theoretical error in $H \to \mu^+ \mu^-$. More...

double	eHmumupar = 0.
	Parametric relative theoretical error in $H \to \mu^+ \mu^-$. More...

double	eHssint = 0.
	Intrinsic relative theoretical error in $H \to s\bar{s}$. More...

double	eHsspar = 0.
	Parametric relative theoretical error in $H \to s\bar{s}$. More...

double	eHtautauint = 0.
	Intrinsic relative theoretical error in $H \to \tau^+ \tau^-$. More...

double	eHtautaupar = 0.
	Parametric relative theoretical error in $H \to \tau^+ \tau^-$. More...

double	eHwidth = 0.
	Total relative theoretical error in the Higgs width. More...

double	eHWWint = 0.
	Intrinsic relative theoretical error in $H \to W W$. More...

double	eHWWpar = 0.
	Parametric relative theoretical error in $H \to W W$. More...

double	eHZgaint = 0.
	Intrinsic relative theoretical error in $H \to Z \gamma$. More...

double	eHZgapar = 0.
	Parametric relative theoretical error in $H \to Z \gamma$. More...

double	eHZZint = 0.
	Intrinsic relative theoretical error in $H \to Z Z$. More...

double	eHZZpar = 0.
	Parametric relative theoretical error in $H \to Z Z$. More...

double	ettHbb = 0.

double	ettHgaga = 0.

double	ettHint = 0.
	Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.) More...

double	ettHmumu = 0.
	Total relative theoretical error in $pp \to ttH \to tt X$. More...

double	ettHpar = 0.
	Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.) More...

double	ettHtautau = 0.

double	ettHWW = 0.

double	ettHZga = 0.

double	ettHZZ = 0.

double	eVBFHbb = 0.

double	eVBFHgaga = 0.

double	eVBFHinv = 0.

double	eVBFHmumu = 0.
	Total relative theoretical error in $pp \to Hjj (VBF) \to X jj$. More...

double	eVBFHtautau = 0.

double	eVBFHWW = 0.

double	eVBFHZga = 0.

double	eVBFHZZ = 0.

double	eVBFint = 0.
	Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.) More...

double	eVBFpar = 0.
	Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.) More...

double	eVHinv = 0.
	Total relative theoretical error in $pp \to X H \to X + invisible$. More...

double	eWHbb = 0.

double	eWHgaga = 0.

double	eWHint = 0.
	Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.) More...

double	eWHmumu = 0.
	Total relative theoretical error in $pp \to WH \to W X$. More...

double	eWHpar = 0.
	Parametric relative theoretical error in WH production. (Assumed to be constant in energy.) More...

double	eWHtautau = 0.

double	eWHWW = 0.

double	eWHZga = 0.

double	eWHZZ = 0.

double	eZHbb = 0.

double	eZHgaga = 0.

double	eZHint = 0.
	Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.) More...

double	eZHmumu = 0.
	Total relative theoretical error in $pp \to ZH \to Z X$. More...

double	eZHpar = 0.
	Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.) More...

double	eZHtautau = 0.

double	eZHWW = 0.

double	eZHZga = 0.

double	eZHZZ = 0.

int	flavBas = 1

double	g1_LEW = 0

double	g1_tree
	The tree level value of the $U(1)_Y$ gauge coupling contant (at the $Z$ pole). More...

double	g2_LEW = 0

double	g2_tree
	The tree level value of the $SU(2)_L$ gauge coupling contant (at the $Z$ pole). More...

double	g3_LEW = 0

double	g3_tree
	The tree level value of the $SU(3)_c$ gauge coupling contant (at the $Z$ pole). More...

double	GammaHTotR
	NP contributions and Total to Higgs width ratio with SM. More...

double	gZdL

double	gZdR
	The tree level value of the $Z\bar{d}d$ couplings in the SM. More...

double	gZlL

double	gZlR
	The tree level value of the $Z\ell^+\ell^-$ couplings in the SM. More...

double	gZuL

double	gZuR
	The tree level value of the $Z\bar{u}u$ couplings in the SM. More...

double	gZvL
	The tree level value of the $Z\bar{\nu}\nu$ couplings in the SM. More...

double	Lambda_NP
	The new physics scale [GeV]. More...

double	lambdaH_LEW = 0

double	lambdaH_tree
	The SM tree level value of the scalar quartic coupling in the potential. More...

double	LambdaNP2
	The square of the new physics scale [GeV $^2$]. More...

double	LambdaNPm2
	The inverse square of the new physics scale [GeV $^{-2}$]. More...

double	mb_LEW = 0

double	mc_LEW = 0

double	md_LEW = 0

double	me_LEW = 0

double	mH2_LEW = 0

double	mmu_LEW = 0

double	ms_LEW = 0

double	mt_LEW = 0

double	mtau_LEW = 0

double	mu_LEW = 0

double	Mw_tree
	The tree level value of the $W$ boson mass. More...

Matching< NPSMEFTd6GeneralMatching, NPSMEFTd6General >	NPSMEFTd6GM
	An auxiliary method to get the WC from the evolutor. More...

double	s12CKM_LEW = 0.

double	s13CKM_LEW = 0.

double	s23CKM_LEW = 0.

std::string	SMEFTBasisFlag

RGESolver	SMEFTEvol1000

RGESolver	SMEFTEvol1500

RGESolver	SMEFTEvol240

RGESolver	SMEFTEvol3000

RGESolver	SMEFTEvol365

RGESolver	SMEFTEvol5000

RGESolver	SMEFTEvol550

RGESolver	SMEFTEvolEW

RGESolver	SMEFTEvolMH

RGESolver	SMEFTEvolUV

double	sW2_tree
	The square 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	tmu2 = 0.

double	tmu3 = 0.

double	tmu4 = 0.

double	tmu5 = 0.

double	tmuw = 0.

double	UevL
	The tree level value of the $W^-\bar{\ell}\nu$ couplings in the SM. (Neglecting PMNS effects.) More...

double	v2
	The square of the EW vev. More...

double	v2_over_LambdaNP2
	The ratio between the EW vev and the new physics scale, squared $v^2/\Lambda^2$. More...

double	VudL
	The tree level value of the $W^+\bar{u}d$ couplings in the SM. (Neglecting CKM effects.) More...

double	xBZ_tree
	The tree level component of the matrix that transform the gauge field $B_{\mu}$ into $Z_{\mu}$. More...

double	xWZ_tree
	The tree level component of the matrix that transform the gauge field $W_{\mu}^3$ into $Z_{\mu}$. More...

double	Yukc

double	Yukt
	SM u-quark Yukawas. More...

double	Yuku

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	dAl5hMz
	The five-flavour hadronic contribution to the electromagnetic coupling, $\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)$. (Non-input parameter) More...

double	dAle5Mz
	The five-flavour hadronic contribution to the electromagnetic coupling, $\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)$, used as input for FlagMWinput = FALSE. More...

double	delGammaZ
	The theoretical uncertainty in $\Gamma_Z$, denoted as $\delta\,\Gamma_Z$, in GeV. More...

double	delMw
	The theoretical uncertainty in $M_W$, denoted as $\delta\,M_W$, in GeV. More...

double	delR0b
	The theoretical uncertainty in $R_b^0$, denoted as $\delta\,R_b^0$. More...

double	delR0c
	The theoretical uncertainty in $R_c^0$, denoted as $\delta\,R_c^0$. More...

double	delR0l
	The theoretical uncertainty in $R_l^0$, denoted as $\delta\,R_l^0$. More...

double	delsigma0H
	The theoretical uncertainty in $\sigma_{Hadron}^0$, denoted as $\delta\,\sigma_{Hadron}^0$ in nb. More...

double	delSin2th_b
	The theoretical uncertainty in $\sin^2\theta_{\rm eff}^{b}$, denoted as $\delta\sin^2\theta_{\rm eff}^{b}$. More...

double	delSin2th_l
	The theoretical uncertainty in $\sin^2\theta_{\rm eff}^{\rm lept}$, denoted as $\delta\sin^2\theta_{\rm eff}^{\rm lept}$. More...

double	delSin2th_q
	The theoretical uncertainty in $\sin^2\theta_{\rm eff}^{q\not = b,t}$, denoted as $\delta\sin^2\theta_{\rm eff}^{q\not = b,t}$. More...

double	delta

double	etab
	The CKM parameter $\bar{\eta}$ in the Wolfenstein parameterization. More...

bool	flag_order [orders_EW_size]
	An array of internal flags controlling the inclusions of higher-order corrections. More...

bool	FlagFixMuwMut
	A boolean for the model flag FixMuwMut. More...

bool	flagLEP2 [NUMofLEP2RCs]

double	gamma
	$\gamma $ used as an input for FlagWolfenstein = FALSE More...

double	GF
	The Fermi constant $G_\mu$ in ${\rm GeV}^{-2}$. More...

double	lambda
	The CKM parameter $\lambda$ in the Wolfenstein parameterization. More...

Particle	leptons [6]
	An array of Particle objects for the leptons. More...

double	mHl
	The Higgs mass $m_h$ in GeV. More...

double	muw
	A matching scale $\mu_W$ around the weak scale in GeV. More...

double	Mw_inp
	The mass of the $W$ boson in GeV used as input for FlagMWinput = TRUE. More...

CKM	myCKM
	An object of type CKM. More...

PMNS	myPMNS

double	Mz
	The mass of the $Z$ boson in GeV. More...

bool	requireCKM
	An internal flag to control whether the CKM matrix has to be recomputed. More...

bool	requireYe
	An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed. More...

bool	requireYn
	An internal flag to control whether the neutrino Yukawa matrix has to be recomputed. More...

double	rhob
	The CKM parameter $\bar{\rho}$ in the Wolfenstein parameterization. More...

double	s12

double	s13

double	s23

Flavour	SMFlavour
	An object of type Flavour. More...

Matching< StandardModelMatching, StandardModel >	SMM
	An object of type Matching. More...

double	Vcb
	$\vert V_{cb} \vert $ used as an input for FlagWolfenstein = FALSE More...

double	Vub
	$\vert V_{ub} \vert $ used as an input for FlagWolfenstein = FALSE More...

double	Vud
	$\vert V_{ud} \vert $ used as an input for FlagWolfenstein = FALSE and FlagUseVud = TRUE More...

double	Vus
	$\vert V_{us} \vert $ used as an input for FlagWolfenstein = FALSE More...

gslpp::matrix< gslpp::complex >	Yd
	The Yukawa matrix of the down-type quarks. More...

gslpp::matrix< gslpp::complex >	Ye
	The Yukawa matrix of the charged leptons. More...

gslpp::matrix< gslpp::complex >	Yn
	The Yukawa matrix of the neutrinos. More...

gslpp::matrix< gslpp::complex >	Yu
	The Yukawa matrix of the up-type quarks. More...

Protected Attributes inherited from QCD
double	AlsM
	The strong coupling constant at the mass scale MAls, $\alpha_s(M_{\alpha_s})$. More...

double	CA

double	CF

bool	computemt
	Switch for computing the $\overline{\mathrm{MS}}$ mass of the top quark. More...

double	dAdA_NA

double	dFdA_NA

double	dFdF_NA

bool	FlagMpole2MbarNumeric
	A flag to determine whether the pole mass to $\over \mathrm{MS}$ mass conversion is done numerically. More...

bool	FlagMtPole
	A flag to determine whether the pole mass of the top quark is used as input. More...

double	MAls
	The mass scale in GeV at which the strong coupling measurement is provided. More...

double	mtpole
	The pole mass of the top quark. More...

double	mub
	The threshold between five- and four-flavour theory in GeV. More...

double	muc
	The threshold between four- and three-flavour theory in GeV. More...

double	mut
	The threshold between six- and five-flavour theory in GeV. More...

double	NA

double	Nc
	The number of colours. More...

bool	QCDsuccess =true

Particle	quarks [6]
	The vector of all SM quarks. More...

bool	requireYd
	Switch for generating the Yukawa couplings to the down-type quarks. More...

bool	requireYu
	Switch for generating the Yukawa couplings to the up-type quarks. More...

double	TF

Protected Attributes inherited from Model
bool	isSliced = false
	A boolean set to true if the current istance is a slice of an extended object. More...

std::map< std::string, std::reference_wrapper< const double > >	ModelParamMap

bool	UpdateError = false
	A boolean set to false if update is successful. More...

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

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

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

enum	meson { P_0 , P_P , K_0 , K_P , D_0 , D_P , D_S , B_D , B_P , B_S , B_C , PHI , K_star , K_star_P , K_S , D_star_P , RHO , RHO_P , OMEGA , MESON_END }
	An enum type for mesons. More...

enum	quark { UP , DOWN , CHARM , STRANGE , TOP , BOTTOM }
	An enum type for quarks. More...

Public Attributes inherited from NPbase
double	C1Hbb = 0.0

double	C1Hcc = 0.0

double	C1Hgaga = 0.0049

double	C1Hgg = 0.0066

double	C1Hmumu = 0.0
	The C1 coefficient controlling the H^3 corrections to the Higgs partial width from the Higgs trilinear coupling. More...

double	C1Hss = 0.0

double	C1Htautau = 0.0

double	C1HWW = 0.0073

double	C1HZga = 0.0
	The C1 coefficient controlling the H^3 corrections to the Higgs partial width from the Higgs trilinear coupling. More...

double	C1HZZ = 0.0083

Constructor & Destructor Documentation

◆ NPSMEFTd6U3()

NPSMEFTd6U3::NPSMEFTd6U3 ( )

Definition at line 19 of file NPSMEFTd6U3.cpp.

: NPSMEFTd6General()
{
    setModelName("NPSMEFTd6U3");
   
    ModelParamMap.insert(std::make_pair("CG_LNP", std::cref(CG_LNP)));
    ModelParamMap.insert(std::make_pair("CW_LNP", std::cref(CW_LNP)));
    ModelParamMap.insert(std::make_pair("CHG_LNP", std::cref(CHG_LNP)));
    ModelParamMap.insert(std::make_pair("CHW_LNP", std::cref(CHW_LNP)));
    ModelParamMap.insert(std::make_pair("CHB_LNP", std::cref(CHB_LNP)));
    ModelParamMap.insert(std::make_pair("CHWB_LNP", std::cref(CHWB_LNP)));
    ModelParamMap.insert(std::make_pair("CHD_LNP", std::cref(CHD_LNP)));
    ModelParamMap.insert(std::make_pair("CHbox_LNP", std::cref(CHbox_LNP)));
    ModelParamMap.insert(std::make_pair("CH_LNP", std::cref(CH_LNP)));
    
    ModelParamMap.insert(std::make_pair("CHl1_LNP", std::cref(CHl1_LNP)));
    ModelParamMap.insert(std::make_pair("CHl3_LNP", std::cref(CHl3_LNP)));
    ModelParamMap.insert(std::make_pair("CHe_LNP", std::cref(CHe_LNP)));
    ModelParamMap.insert(std::make_pair("CHq1_LNP", std::cref(CHq1_LNP)));
    ModelParamMap.insert(std::make_pair("CHq3_LNP", std::cref(CHq3_LNP)));
    ModelParamMap.insert(std::make_pair("CHu_LNP", std::cref(CHu_LNP)));
    ModelParamMap.insert(std::make_pair("CHd_LNP", std::cref(CHd_LNP)));
 
    
    
    ModelParamMap.insert(std::make_pair("Cll_aabb_LNP", std::cref(Cll_aabb_LNP)));
    ModelParamMap.insert(std::make_pair("Cll_abba_LNP", std::cref(Cll_abba_LNP)));
    ModelParamMap.insert(std::make_pair("Clq1_LNP", std::cref(Clq1_LNP)));
    ModelParamMap.insert(std::make_pair("Clq3_LNP", std::cref(Clq3_LNP)));
    ModelParamMap.insert(std::make_pair("Cee_LNP", std::cref(Cee_LNP)));
    ModelParamMap.insert(std::make_pair("Ceu_LNP", std::cref(Ceu_LNP)));
    ModelParamMap.insert(std::make_pair("Ced_LNP", std::cref(Ced_LNP)));
    ModelParamMap.insert(std::make_pair("Cle_LNP", std::cref(Cle_LNP)));
    ModelParamMap.insert(std::make_pair("Clu_LNP", std::cref(Clu_LNP)));
    ModelParamMap.insert(std::make_pair("Cld_LNP", std::cref(Cld_LNP)));
    ModelParamMap.insert(std::make_pair("Cqe_LNP", std::cref(Cqe_LNP)));
    
    
    ModelParamMap.insert(std::make_pair("Cqq1_aabb_LNP", std::cref(Cqq1_aabb_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq1_abba_LNP", std::cref(Cqq1_abba_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3_aabb_LNP", std::cref(Cqq3_aabb_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3_abba_LNP", std::cref(Cqq3_abba_LNP)));
    ModelParamMap.insert(std::make_pair("Cuu_aabb_LNP", std::cref(Cuu_aabb_LNP)));
    ModelParamMap.insert(std::make_pair("Cuu_abba_LNP", std::cref(Cuu_abba_LNP)));
    ModelParamMap.insert(std::make_pair("Cdd_aabb_LNP", std::cref(Cdd_aabb_LNP)));
    ModelParamMap.insert(std::make_pair("Cdd_abba_LNP", std::cref(Cdd_abba_LNP)));
 
    ModelParamMap.insert(std::make_pair("Cud1_LNP", std::cref(Cud1_LNP)));
    ModelParamMap.insert(std::make_pair("Cud8_LNP", std::cref(Cud8_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu1_LNP", std::cref(Cqu1_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu8_LNP", std::cref(Cqu8_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd1_LNP", std::cref(Cqd1_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd8_LNP", std::cref(Cqd8_LNP)));
    
    
}

Member Function Documentation

◆ PostUpdate()

bool NPSMEFTd6U3::PostUpdate ( )

virtual

The post-update method for NPSMEFTd6General.

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 NPSMEFTd6General.

Definition at line 568 of file NPSMEFTd6U3.cpp.

{
    
    setNPSMEFTd6GeneralParameters();
    
    if (!NPSMEFTd6General::PostUpdate()) return (false);
    
    return (true);
        
}

◆ setNPSMEFTd6GeneralParameters()

void NPSMEFTd6U3::setNPSMEFTd6GeneralParameters ( )

protected

An auxiliary method to set the WC of the general class.

Definition at line 258 of file NPSMEFTd6U3.cpp.

{
 
    
    CHl1_11r_LNP = CHl1_LNP;
    CHl1_22r_LNP = CHl1_LNP;
    CHl1_33r_LNP = CHl1_LNP;
    
    CHl3_11r_LNP = CHl3_LNP;
    CHl3_22r_LNP = CHl3_LNP;
    CHl3_33r_LNP = CHl3_LNP;
    
    CHe_11r_LNP = CHe_LNP;
    CHe_22r_LNP = CHe_LNP;
    CHe_33r_LNP = CHe_LNP;
    
    CHq1_11r_LNP = CHq1_LNP;
    CHq1_22r_LNP = CHq1_LNP;
    CHq1_33r_LNP = CHq1_LNP;
    
    CHq3_11r_LNP = CHq3_LNP;
    CHq3_22r_LNP = CHq3_LNP;
    CHq3_33r_LNP = CHq3_LNP;
    
    CHu_11r_LNP = CHu_LNP;
    CHu_22r_LNP = CHu_LNP;
    CHu_33r_LNP = CHu_LNP;
    
    CHd_11r_LNP = CHd_LNP;
    CHd_22r_LNP = CHd_LNP;
    CHd_33r_LNP = CHd_LNP;
    
    
    
    
    
    
    Cll_1111r_LNP = Cll_aabb_LNP+Cll_abba_LNP;
    Cll_2222r_LNP = Cll_aabb_LNP+Cll_abba_LNP;
    Cll_3333r_LNP = Cll_aabb_LNP+Cll_abba_LNP;
 
    Cll_1122r_LNP = Cll_aabb_LNP;
    Cll_1133r_LNP = Cll_aabb_LNP;
    Cll_2233r_LNP = Cll_aabb_LNP;
    
    Cll_1221r_LNP = Cll_abba_LNP;
    Cll_1331r_LNP = Cll_abba_LNP;
    Cll_2332r_LNP = Cll_abba_LNP;
    
    
    
    Clq1_1111r_LNP = Clq1_LNP;
    Clq1_1122r_LNP = Clq1_LNP;
    Clq1_1133r_LNP = Clq1_LNP;
    Clq1_2211r_LNP = Clq1_LNP;
    Clq1_2222r_LNP = Clq1_LNP;
    Clq1_2233r_LNP = Clq1_LNP;
    Clq1_3311r_LNP = Clq1_LNP;
    Clq1_3322r_LNP = Clq1_LNP;
    Clq1_3333r_LNP = Clq1_LNP;
    
    
    
    Clq3_1111r_LNP = Clq3_LNP;
    Clq3_1122r_LNP = Clq3_LNP;
    Clq3_1133r_LNP = Clq3_LNP;
    Clq3_2211r_LNP = Clq3_LNP;
    Clq3_2222r_LNP = Clq3_LNP;
    Clq3_2233r_LNP = Clq3_LNP;
    Clq3_3311r_LNP = Clq3_LNP;
    Clq3_3322r_LNP = Clq3_LNP;
    Clq3_3333r_LNP = Clq3_LNP;
    
    
    
    Cee_1111r_LNP = Cee_LNP;
    Cee_1122r_LNP = Cee_LNP;
    Cee_1133r_LNP = Cee_LNP;
    Cee_2222r_LNP = Cee_LNP;
    Cee_2233r_LNP = Cee_LNP;
    Cee_3333r_LNP = Cee_LNP;
    
    
    
    Ceu_1111r_LNP = Ceu_LNP;
    Ceu_1122r_LNP = Ceu_LNP;
    Ceu_1133r_LNP = Ceu_LNP;
    Ceu_2211r_LNP = Ceu_LNP;
    Ceu_2222r_LNP = Ceu_LNP;
    Ceu_2233r_LNP = Ceu_LNP;
    Ceu_3311r_LNP = Ceu_LNP;
    Ceu_3322r_LNP = Ceu_LNP;
    Ceu_3333r_LNP = Ceu_LNP;
 
    
    
    Ced_1111r_LNP = Ced_LNP;
    Ced_1122r_LNP = Ced_LNP;
    Ced_1133r_LNP = Ced_LNP;
    Ced_2211r_LNP = Ced_LNP;
    Ced_2222r_LNP = Ced_LNP;
    Ced_2233r_LNP = Ced_LNP;
    Ced_3311r_LNP = Ced_LNP;
    Ced_3322r_LNP = Ced_LNP;
    Ced_3333r_LNP = Ced_LNP;
 
    
    
    Cle_1111r_LNP = Cle_LNP;
    Cle_1122r_LNP = Cle_LNP;
    Cle_1133r_LNP = Cle_LNP;
    Cle_2211r_LNP = Cle_LNP;
    Cle_2222r_LNP = Cle_LNP;
    Cle_2233r_LNP = Cle_LNP;
    Cle_3311r_LNP = Cle_LNP;
    Cle_3322r_LNP = Cle_LNP;
    Cle_3333r_LNP = Cle_LNP; 
 
    
    
    Clu_1111r_LNP = Clu_LNP;
    Clu_1122r_LNP = Clu_LNP;
    Clu_1133r_LNP = Clu_LNP;
    Clu_2211r_LNP = Clu_LNP;
    Clu_2222r_LNP = Clu_LNP;
    Clu_2233r_LNP = Clu_LNP;
    Clu_3311r_LNP = Clu_LNP;
    Clu_3322r_LNP = Clu_LNP;
    Clu_3333r_LNP = Clu_LNP; 
    
 
    
    
    Cld_1111r_LNP = Cld_LNP;
    Cld_1122r_LNP = Cld_LNP;
    Cld_1133r_LNP = Cld_LNP;
    Cld_2211r_LNP = Cld_LNP;
    Cld_2222r_LNP = Cld_LNP;
    Cld_2233r_LNP = Cld_LNP;
    Cld_3311r_LNP = Cld_LNP;
    Cld_3322r_LNP = Cld_LNP;
    Cld_3333r_LNP = Cld_LNP; 
    
 
    
    
    Cqe_1111r_LNP = Cqe_LNP;
    Cqe_1122r_LNP = Cqe_LNP;
    Cqe_1133r_LNP = Cqe_LNP;
    Cqe_2211r_LNP = Cqe_LNP;
    Cqe_2222r_LNP = Cqe_LNP;
    Cqe_2233r_LNP = Cqe_LNP;
    Cqe_3311r_LNP = Cqe_LNP;
    Cqe_3322r_LNP = Cqe_LNP;
    Cqe_3333r_LNP = Cqe_LNP; 
    
    
    
    
    
    
    
    
    Cqq1_1111r_LNP = Cqq1_aabb_LNP+Cqq1_abba_LNP;
    Cqq1_2222r_LNP = Cqq1_aabb_LNP+Cqq1_abba_LNP;
    Cqq1_3333r_LNP = Cqq1_aabb_LNP+Cqq1_abba_LNP;
 
    Cqq1_1122r_LNP = Cqq1_aabb_LNP;
    Cqq1_1133r_LNP = Cqq1_aabb_LNP;
    Cqq1_2233r_LNP = Cqq1_aabb_LNP;
    
    Cqq1_1221r_LNP = Cqq1_abba_LNP;
    Cqq1_1331r_LNP = Cqq1_abba_LNP;
    Cqq1_2332r_LNP = Cqq1_abba_LNP;
    
    
    
    
    
    Cqq3_1111r_LNP = Cqq3_aabb_LNP+Cqq3_abba_LNP;
    Cqq3_2222r_LNP = Cqq3_aabb_LNP+Cqq3_abba_LNP;
    Cqq3_3333r_LNP = Cqq3_aabb_LNP+Cqq3_abba_LNP;
 
    Cqq3_1122r_LNP = Cqq3_aabb_LNP;
    Cqq3_1133r_LNP = Cqq3_aabb_LNP;
    Cqq3_2233r_LNP = Cqq3_aabb_LNP;
    
    Cqq3_1221r_LNP = Cqq3_abba_LNP;
    Cqq3_1331r_LNP = Cqq3_abba_LNP;
    Cqq3_2332r_LNP = Cqq3_abba_LNP;
   
    
    
    
    
    Cuu_1111r_LNP = Cuu_aabb_LNP+Cuu_abba_LNP;
    Cuu_2222r_LNP = Cuu_aabb_LNP+Cuu_abba_LNP;
    Cuu_3333r_LNP = Cuu_aabb_LNP+Cuu_abba_LNP;
 
    Cuu_1122r_LNP = Cuu_aabb_LNP;
    Cuu_1133r_LNP = Cuu_aabb_LNP;
    Cuu_2233r_LNP = Cuu_aabb_LNP;
    
    Cuu_1221r_LNP = Cuu_abba_LNP;
    Cuu_1331r_LNP = Cuu_abba_LNP;
    Cuu_2332r_LNP = Cuu_abba_LNP;
    
    
    
    
    
    
    Cdd_1111r_LNP = Cdd_aabb_LNP+Cdd_abba_LNP;
    Cdd_2222r_LNP = Cdd_aabb_LNP+Cdd_abba_LNP;
    Cdd_3333r_LNP = Cdd_aabb_LNP+Cdd_abba_LNP;
 
    Cdd_1122r_LNP = Cdd_aabb_LNP;
    Cdd_1133r_LNP = Cdd_aabb_LNP;
    Cdd_2233r_LNP = Cdd_aabb_LNP;
    
    Cdd_1221r_LNP = Cdd_abba_LNP;
    Cdd_1331r_LNP = Cdd_abba_LNP;
    Cdd_2332r_LNP = Cdd_abba_LNP;
    
    
    
    
    Cud1_1111r_LNP = Cud1_LNP;
    Cud1_1122r_LNP = Cud1_LNP;
    Cud1_1133r_LNP = Cud1_LNP;
    Cud1_2211r_LNP = Cud1_LNP;
    Cud1_2222r_LNP = Cud1_LNP;
    Cud1_2233r_LNP = Cud1_LNP;
    Cud1_3311r_LNP = Cud1_LNP;
    Cud1_3322r_LNP = Cud1_LNP;
    Cud1_3333r_LNP = Cud1_LNP; 
    
    
    
    
    Cud8_1111r_LNP = Cud8_LNP;
    Cud8_1122r_LNP = Cud8_LNP;
    Cud8_1133r_LNP = Cud8_LNP;
    Cud8_2211r_LNP = Cud8_LNP;
    Cud8_2222r_LNP = Cud8_LNP;
    Cud8_2233r_LNP = Cud8_LNP;
    Cud8_3311r_LNP = Cud8_LNP;
    Cud8_3322r_LNP = Cud8_LNP;
    Cud8_3333r_LNP = Cud8_LNP; 
    
    
    
    
    Cqu1_1111r_LNP = Cqu1_LNP;
    Cqu1_1122r_LNP = Cqu1_LNP;
    Cqu1_1133r_LNP = Cqu1_LNP;
    Cqu1_2211r_LNP = Cqu1_LNP;
    Cqu1_2222r_LNP = Cqu1_LNP;
    Cqu1_2233r_LNP = Cqu1_LNP;
    Cqu1_3311r_LNP = Cqu1_LNP;
    Cqu1_3322r_LNP = Cqu1_LNP;
    Cqu1_3333r_LNP = Cqu1_LNP; 
    
    
    
    
    Cqu8_1111r_LNP = Cqu8_LNP;
    Cqu8_1122r_LNP = Cqu8_LNP;
    Cqu8_1133r_LNP = Cqu8_LNP;
    Cqu8_2211r_LNP = Cqu8_LNP;
    Cqu8_2222r_LNP = Cqu8_LNP;
    Cqu8_2233r_LNP = Cqu8_LNP;
    Cqu8_3311r_LNP = Cqu8_LNP;
    Cqu8_3322r_LNP = Cqu8_LNP;
    Cqu8_3333r_LNP = Cqu8_LNP; 
    
    
    
    
    
    
    
    Cqd1_1111r_LNP = Cqd1_LNP;
    Cqd1_1122r_LNP = Cqd1_LNP;
    Cqd1_1133r_LNP = Cqd1_LNP;
    Cqd1_2211r_LNP = Cqd1_LNP;
    Cqd1_2222r_LNP = Cqd1_LNP;
    Cqd1_2233r_LNP = Cqd1_LNP;
    Cqd1_3311r_LNP = Cqd1_LNP;
    Cqd1_3322r_LNP = Cqd1_LNP;
    Cqd1_3333r_LNP = Cqd1_LNP; 
    
    
    
    
    Cqd8_1111r_LNP = Cqd8_LNP;
    Cqd8_1122r_LNP = Cqd8_LNP;
    Cqd8_1133r_LNP = Cqd8_LNP;
    Cqd8_2211r_LNP = Cqd8_LNP;
    Cqd8_2222r_LNP = Cqd8_LNP;
    Cqd8_2233r_LNP = Cqd8_LNP;
    Cqd8_3311r_LNP = Cqd8_LNP;
    Cqd8_3322r_LNP = Cqd8_LNP;
    Cqd8_3333r_LNP = Cqd8_LNP; 
    
}

◆ setParameter()

void NPSMEFTd6U3::setParameter	(	const std::string	name,
		const double &	value
	)

protectedvirtual

Reimplemented from NPSMEFTd6General.

Definition at line 79 of file NPSMEFTd6U3.cpp.

{
 
    if (name.compare("CG_LNP") == 0) {
        CG_LNP = value;
 
    } else if (name.compare("CW_LNP") == 0) {
        CW_LNP = value;
 
    } else if (name.compare("CHG_LNP") == 0) {
        CHG_LNP = value;
 
    } else if (name.compare("CHW_LNP") == 0) {
        CHW_LNP = value;
 
    } else if (name.compare("CHB_LNP") == 0) {
        CHB_LNP = value;
 
    } else if (name.compare("CHWB_LNP") == 0) {
        CHWB_LNP = value;
 
    } else if (name.compare("CHD_LNP") == 0) {
        CHD_LNP = value;
 
    } else if (name.compare("CHbox_LNP") == 0) {
        CHbox_LNP = value;
 
    } else if (name.compare("CH_LNP") == 0) {
        CH_LNP = value;
 
    } else if (name.compare("CHl1_LNP") == 0) {
        
        //std::cout<<"\033[1;33m   LambdaNPm2 =  \033[0m "<< LambdaNPm2 <<std::endl;
                
        CHl1_LNP = value;
 
    } else if (name.compare("CHl3_LNP") == 0) {
        
        CHl3_LNP = value;
 
    } else if (name.compare("CHe_LNP") == 0) {
        
        CHe_LNP = value;
 
    } else if (name.compare("CHq1_LNP") == 0) {
        
        CHq1_LNP = value;
 
    } else if (name.compare("CHq3_LNP") == 0) {
        
        CHq3_LNP = value;
 
    } else if (name.compare("CHu_LNP") == 0) {
        
        CHu_LNP = value;
 
    } else if (name.compare("CHd_LNP") == 0) {
        
        CHd_LNP = value;
  
    } else if (name.compare("Cll_aabb_LNP") == 0) {
        
        Cll_aabb_LNP = value; 
        
    } else if (name.compare("Cll_abba_LNP") == 0) {
        
        Cll_abba_LNP = value;   
        
    } else if (name.compare("Clq1_LNP") == 0) {
        
        Clq1_LNP = value;
 
    } else if (name.compare("Clq3_LNP") == 0) {
        
        Clq3_LNP = value;
     
    } else if (name.compare("Cee_LNP") == 0) {
        
        Cee_LNP = value;
    
    } else if (name.compare("Ceu_LNP") == 0) {
        
        Ceu_LNP = value;
                       
    } else if (name.compare("Ced_LNP") == 0) {
        
        Ced_LNP = value;
                       
    }  else if (name.compare("Cle_LNP") == 0) {
        
        Cle_LNP = value;
                       
    }  else if (name.compare("Clu_LNP") == 0) {
        
        Clu_LNP = value;
                       
    }  else if (name.compare("Cld_LNP") == 0) {
        
        Cld_LNP = value;
                       
    }  else if (name.compare("Cqe_LNP") == 0) {
        
        Cqe_LNP = value;
                       
    } else if (name.compare("Cqq1_aabb_LNP") == 0) {
        
        Cqq1_aabb_LNP = value;
        
    } else if (name.compare("Cqq1_abba_LNP") == 0) {
        
        Cqq1_abba_LNP = value;
        
    } else if (name.compare("Cqq3_aabb_LNP") == 0) {
        
        Cqq3_aabb_LNP = value;
        
    } else if (name.compare("Cqq3_abba_LNP") == 0) {
        
        Cqq3_abba_LNP = value;
        
    } else if (name.compare("Cuu_aabb_LNP") == 0) {
        
        Cuu_aabb_LNP = value;
        
    } else if (name.compare("Cuu_abba_LNP") == 0) {
        
        Cuu_abba_LNP = value;
        
    } else if (name.compare("Cdd_aabb_LNP") == 0) {
        
        Cdd_aabb_LNP = value;
        
    } else if (name.compare("Cdd_abba_LNP") == 0) {
        
        Cdd_abba_LNP = value;
        
    } else if (name.compare("Cud1_LNP") == 0) {
        
        Cud1_LNP = value;
                       
    } else if (name.compare("Cud8_LNP") == 0) {
        
        Cud8_LNP = value;
                       
    } else if (name.compare("Cqu1_LNP") == 0) {
        
        Cqu1_LNP = value;
        
    } else if (name.compare("Cqu8_LNP") == 0) {
        
        Cqu8_LNP = value;
        
    } else if (name.compare("Cqd1_LNP") == 0) {
        
        Cqd1_LNP = value;
                       
    } else if (name.compare("Cqd8_LNP") == 0) {
        
        Cqd8_LNP = value;
                              
    } else if (name.compare("Lambda_NP") == 0)
        Lambda_NP = value;
    else
        NPSMEFTd6General::setParameter(name, value);
 
}

Member Data Documentation

◆ Cdd_aabb_LNP

double NPSMEFTd6U3::Cdd_aabb_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{dd})_{ijkm}$ (Real part and pure real operator).

Definition at line 80 of file NPSMEFTd6U3.h.

◆ Cdd_abba_LNP

double NPSMEFTd6U3::Cdd_abba_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{dd})_{ijkm}$ (Real part and pure real operator).

Definition at line 81 of file NPSMEFTd6U3.h.

◆ Ced_LNP

double NPSMEFTd6U3::Ced_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{ed})_{ijkm}$ (Imaginary part).

Definition at line 68 of file NPSMEFTd6U3.h.

◆ Cee_LNP

double NPSMEFTd6U3::Cee_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{ee})_{ijkm}$ (Imaginary part).

Definition at line 66 of file NPSMEFTd6U3.h.

◆ Ceu_LNP

double NPSMEFTd6U3::Ceu_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{eu})_{ijkm}$ (Real part and pure real operator).

Definition at line 67 of file NPSMEFTd6U3.h.

◆ CHd_LNP

double NPSMEFTd6U3::CHd_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{Hd})_{ij}$.

Definition at line 59 of file NPSMEFTd6U3.h.

◆ CHe_LNP

double NPSMEFTd6U3::CHe_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{He})_{ij}$.

Definition at line 55 of file NPSMEFTd6U3.h.

◆ CHl1_LNP

double NPSMEFTd6U3::CHl1_LNP = 0.

protected

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

Definition at line 53 of file NPSMEFTd6U3.h.

◆ CHl3_LNP

double NPSMEFTd6U3::CHl3_LNP = 0.

protected

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

Definition at line 54 of file NPSMEFTd6U3.h.

◆ CHq1_LNP

double NPSMEFTd6U3::CHq1_LNP = 0.

protected

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

Definition at line 56 of file NPSMEFTd6U3.h.

◆ CHq3_LNP

double NPSMEFTd6U3::CHq3_LNP = 0.

protected

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

Definition at line 57 of file NPSMEFTd6U3.h.

◆ CHu_LNP

double NPSMEFTd6U3::CHu_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{Hu})_{ij}$.

Definition at line 58 of file NPSMEFTd6U3.h.

◆ Cld_LNP

double NPSMEFTd6U3::Cld_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{ld})_{ijkm}$ (Real part and pure real operator).

Definition at line 71 of file NPSMEFTd6U3.h.

◆ Cle_LNP

double NPSMEFTd6U3::Cle_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{le})_{ijkm}$ (Real part and pure real operator).

Definition at line 69 of file NPSMEFTd6U3.h.

◆ Cll_aabb_LNP

double NPSMEFTd6U3::Cll_aabb_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{ll})_{ijkm}$ (Real part and pure real operator).

Definition at line 61 of file NPSMEFTd6U3.h.

◆ Cll_abba_LNP

double NPSMEFTd6U3::Cll_abba_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{ll})_{ijkm}$ (Real part and pure real operator).

Definition at line 62 of file NPSMEFTd6U3.h.

◆ Clq1_LNP

double NPSMEFTd6U3::Clq1_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{lq}^{(1)})_{ijkm}$ (Imaginary part).

Definition at line 64 of file NPSMEFTd6U3.h.

◆ Clq3_LNP

double NPSMEFTd6U3::Clq3_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{lq}^{(3)})_{ijkm}$ (Real part and pure real operator).

Definition at line 65 of file NPSMEFTd6U3.h.

◆ Clu_LNP

double NPSMEFTd6U3::Clu_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{lu})_{ijkm}$ (Imaginary part).

Definition at line 70 of file NPSMEFTd6U3.h.

◆ Cqd1_LNP

double NPSMEFTd6U3::Cqd1_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{qd}^{(1)})_{ijkm}$ (Imaginary part).

Definition at line 87 of file NPSMEFTd6U3.h.

◆ Cqd8_LNP

double NPSMEFTd6U3::Cqd8_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{qd}^{(8)})_{ijkm}$ (Real part and pure real operator).

Definition at line 88 of file NPSMEFTd6U3.h.

◆ Cqe_LNP

double NPSMEFTd6U3::Cqe_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{qe})_{ijkm}$ (Imaginary part).

Definition at line 72 of file NPSMEFTd6U3.h.

◆ Cqq1_aabb_LNP

double NPSMEFTd6U3::Cqq1_aabb_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{qq}^{(1)})_{ijkm}$ (Imaginary part).

Definition at line 74 of file NPSMEFTd6U3.h.

◆ Cqq1_abba_LNP

double NPSMEFTd6U3::Cqq1_abba_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{qq}^{(1)})_{ijkm}$ (Imaginary part).

Definition at line 75 of file NPSMEFTd6U3.h.

◆ Cqq3_aabb_LNP

double NPSMEFTd6U3::Cqq3_aabb_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{qq}^{(3)})_{ijkm}$ (Real part and pure real operator).

Definition at line 76 of file NPSMEFTd6U3.h.

◆ Cqq3_abba_LNP

double NPSMEFTd6U3::Cqq3_abba_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{qq}^{(3)})_{ijkm}$ (Real part and pure real operator).

Definition at line 77 of file NPSMEFTd6U3.h.

◆ Cqu1_LNP

double NPSMEFTd6U3::Cqu1_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{qu}^{(1)})_{ijkm}$ (Imaginary part).

Definition at line 85 of file NPSMEFTd6U3.h.

◆ Cqu8_LNP

double NPSMEFTd6U3::Cqu8_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{qu}^{(8)})_{ijkm}$ (Real part and pure real operator).

Definition at line 86 of file NPSMEFTd6U3.h.

◆ Cud1_LNP

double NPSMEFTd6U3::Cud1_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{ud}^{(1)})_{ijkm}$ (Imaginary part).

Definition at line 83 of file NPSMEFTd6U3.h.

◆ Cud8_LNP

double NPSMEFTd6U3::Cud8_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{ud}^{(8)})_{ijkm}$ (Real part and pure real operator).

Definition at line 84 of file NPSMEFTd6U3.h.

◆ Cuu_aabb_LNP

double NPSMEFTd6U3::Cuu_aabb_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{uu})_{ijkm}$ (Imaginary part).

Definition at line 78 of file NPSMEFTd6U3.h.

◆ Cuu_abba_LNP

double NPSMEFTd6U3::Cuu_abba_LNP = 0.

protected

The dimension-6 operator coefficient $(C_{uu})_{ijkm}$ (Imaginary part).

Definition at line 79 of file NPSMEFTd6U3.h.

◆ NNPSMEFTd6U3Vars

const int NPSMEFTd6U3::NNPSMEFTd6U3Vars = 41+1

static

Definition at line 21 of file NPSMEFTd6U3.h.

◆ NPSMEFTd6U3Vars

const std::string NPSMEFTd6U3::NPSMEFTd6U3Vars

static

Initial value:

= {
    "CG_LNP", "CW_LNP", "CHG_LNP", "CHW_LNP", "CHB_LNP",
    "CHWB_LNP", "CHD_LNP", "CHbox_LNP", "CH_LNP",
    "CHl1_LNP","CHl3_LNP","CHe_LNP","CHq1_LNP","CHq3_LNP","CHu_LNP","CHd_LNP",
    "Cll_aabb_LNP","Cll_abba_LNP","Clq1_LNP","Clq3_LNP","Cee_LNP","Ceu_LNP","Ced_LNP","Cle_LNP","Clu_LNP","Cld_LNP","Cqe_LNP",
    "Cqq1_aabb_LNP","Cqq1_abba_LNP", "Cqq3_aabb_LNP", "Cqq3_abba_LNP", "Cuu_aabb_LNP", "Cuu_abba_LNP", "Cdd_aabb_LNP", "Cdd_abba_LNP",
    "Cud1_LNP", "Cud8_LNP", "Cqu1_LNP", "Cqu8_LNP", "Cqd1_LNP", "Cqd8_LNP", "Lambda_NP"
}

Definition at line 23 of file NPSMEFTd6U3.h.

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

Detailed Description

Public Member Functions

Static Public Attributes

Protected Member Functions

Protected Attributes

Additional Inherited Members

Constructor & Destructor Documentation

◆ NPSMEFTd6U3()

Member Function Documentation

◆ PostUpdate()

◆ setNPSMEFTd6GeneralParameters()

◆ setParameter()

Member Data Documentation

◆ Cdd_aabb_LNP

◆ Cdd_abba_LNP

◆ Ced_LNP

◆ Cee_LNP

◆ Ceu_LNP

◆ CHd_LNP

◆ CHe_LNP

◆ CHl1_LNP

◆ CHl3_LNP

◆ CHq1_LNP

◆ CHq3_LNP

◆ CHu_LNP

◆ Cld_LNP

◆ Cle_LNP

◆ Cll_aabb_LNP

◆ Cll_abba_LNP

◆ Clq1_LNP

◆ Clq3_LNP

◆ Clu_LNP

◆ Cqd1_LNP

◆ Cqd8_LNP

◆ Cqe_LNP

◆ Cqq1_aabb_LNP

◆ Cqq1_abba_LNP

◆ Cqq3_aabb_LNP

◆ Cqq3_abba_LNP

◆ Cqu1_LNP

◆ Cqu8_LNP

◆ Cud1_LNP

◆ Cud8_LNP

◆ Cuu_aabb_LNP

◆ Cuu_abba_LNP

◆ NNPSMEFTd6U3Vars

◆ NPSMEFTd6U3Vars