#include <NPSMEFTd6MFV.h>

Inheritance diagram for NPSMEFTd6MFV:

Detailed Description

Definition at line 14 of file NPSMEFTd6MFV.h.

Public Member Functions
	NPSMEFTd6MFV ()

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

virtual const double	CEWHQu33 (const double mu) const
	Combination of coefficients of the Warsaw basis not constrained by EWPO (at LO) $(\hat{C}_{HQ}^{(u)})_{33}$. More...

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

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

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

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

void	GenerateSMInitialConditions ()
	Generates the initial condition for the Standard Model parameters. More...

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

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

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

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...

	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...

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

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	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...

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

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

virtual const 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	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 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	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 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...

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

const double	Als (const double mu, const int Nf_in, const orders order=FULLNLO) const
	Computes the running strong coupling $\alpha_s(\mu)$ with $N_f$ active flavours in the $\overline{\mathrm{MS}}$ scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...

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

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

const double	Alstilde5 (const double mu) const
	The value of $\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}$ at any scale $\mu$ with the number of flavours $n_f = 4$ and full EW corrections. More...

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

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

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

virtual const double	BrHtobb () const
	The Br $(H\to b \bar{b})$ in the Standard Model. More...

virtual const double	BrHtocc () const
	The Br $(H\to c \bar{c})$ in the Standard Model. More...

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

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

virtual const double	BrHtomumu () const
	The Br $(H\to \mu^+ \mu^-)$ in the Standard Model. More...

virtual const double	BrHtoss () const
	The Br $(H\to s \bar{s})$ in the Standard Model. More...

virtual const double	BrHtotautau () const
	The Br $(H\to \tau^+ \tau^-)$ in the Standard Model. More...

virtual const double	BrHtoWWstar () const
	The Br $(H\to W W^*)$ in the Standard Model. More...

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

virtual const double	BrHtoZZstar () const
	The Br $(H\to Z Z^*)$ in the Standard Model. More...

const double	c02 () const
	The square of the cosine of the weak mixing angle $c_0^2$ defined without weak radiative corrections. More...

virtual bool	CheckFlags () const
	A method to check the sanity of the set of model flags. More...

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...

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

const double	eeffsigmaEbin (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const

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

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

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

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

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

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

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

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

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

gslpp::complex	f_triangle (const double tau) const
	Loop function entering in the calculation of the effective $Hgg$ and $H\gamma\gamma$ couplings. More...

gslpp::complex	g_triangle (const double tau) const
	Loop function entering in the calculation of the effective $HZ\gamma$ coupling. More...

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

virtual const double	Gamma_muon () const
	The computation of the muon decay. More...

virtual const double	Gamma_tau_l_nunu (const Particle l) const
	The computation of the leptonic tau decays. More...

virtual const double	GammaHtobb () const
	The $\Gamma(H\to b \bar{b})$ in the Standard Model. More...

virtual const double	GammaHtocc () const
	The $\Gamma(H\to c \bar{c})$ in the Standard Model. More...

virtual const double	GammaHtogaga () const
	The $\Gamma(H\to \gamma \gamma)$ in the Standard Model. More...

virtual const double	GammaHtogg () const
	The $\Gamma(H\to gg)$ in the Standard Model. More...

virtual const double	GammaHtomumu () const
	The $\Gamma(H\to \mu^+ \mu^-)$ in the Standard Model. More...

virtual const double	GammaHtoss () const
	The $\Gamma(H\to s \bar{s})$ in the Standard Model. More...

virtual const double	GammaHTot () const
	The total Higgs width $\Gamma(H)$ in the Standard Model. More...

virtual const double	GammaHtotautau () const
	The $\Gamma(H\to \tau^+ \tau^-)$ in the Standard Model. More...

virtual const double	GammaHtoWWstar () const
	The $\Gamma(H\to W W^*)$ in the Standard Model. More...

virtual const double	GammaHtoZga () const
	The $\Gamma(H\to Z \gamma)$ in the Standard Model. More...

virtual const double	GammaHtoZZstar () const
	The $\Gamma(H\to Z Z^*)$ in the Standard Model. More...

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

virtual const double	gAnue () const
	The effective (muon) neutrino-electron axial-vector coupling: gAnue. More...

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

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

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

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

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

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

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

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

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

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

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

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

const double	getDAle5Mz () const
	A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, $\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)$. More...

const double	getDelGammaWlv () const
	A get method to retrieve the theoretical uncertainty in $\Gamma_W_{l\nu}$, denoted as $\delta\,\Gamma_W_{l\nu}$. More...

const double	getDelGammaWqq () const
	A get method to retrieve the theoretical uncertainty in $\Gamma_W_{qq}$, denoted as $\delta\,\Gamma_W_{qq}$. More...

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

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

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

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

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

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

const double	getDelSin2th_b () const
	A get method to retrieve the theoretical uncertainty in $\sin^2\theta_{\rm eff}^{b}$, denoted as $\delta\sin^2\theta_{\rm eff}^{b}$. More...

const double	getDelSin2th_l () const
	A get method to retrieve the theoretical uncertainty in $\sin^2\theta_{\rm eff}^{\rm lept}$, denoted as $\delta\sin^2\theta_{\rm eff}^{\rm lept}$. More...

const double	getDelSin2th_q () const
	A get method to retrieve the theoretical uncertainty in $\sin^2\theta_{\rm eff}^{q\not = b,t}$, denoted as $\delta\sin^2\theta_{\rm eff}^{q\not = b,t}$. More...

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

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

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

const Flavour &	getFlavour () const

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

const int	getIterationNo () const

const Particle &	getLeptons (const QCD::lepton p) const
	A get method to retrieve the member object of a lepton. More...

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

virtual const double	getmq (const QCD::quark q, const double mu) const
	The MSbar running quark mass computed at NLO. More...

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

const double	getMw () const
	A get method to access the input value of the mass of the $W$ boson $M_W$. More...

EWSMApproximateFormulae *	getMyApproximateFormulae () const
	A get method to retrieve the member pointer of type EWSMApproximateFormulae. More...

EWSMcache *	getMyEWSMcache () const
	A get method to retrieve the member pointer of type EWSMcache. More...

LeptonFlavour *	getMyLeptonFlavour () const

EWSMOneLoopEW *	getMyOneLoopEW () const
	A get method to retrieve the member pointer of type EWSMOneLoopEW,. More...

EWSMThreeLoopEW *	getMyThreeLoopEW () const

EWSMThreeLoopEW2QCD *	getMyThreeLoopEW2QCD () const

EWSMThreeLoopQCD *	getMyThreeLoopQCD () const

EWSMTwoFermionsLEP2 *	getMyTwoFermionsLEP2 () const
	A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More...

EWSMTwoLoopEW *	getMyTwoLoopEW () const

EWSMTwoLoopQCD *	getMyTwoLoopQCD () const

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

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

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

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

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

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

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

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

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

virtual const double	gLnuN2 () const
	The effective neutrino nucleon LH coupling: gLnuN2. More...

virtual const double	gRnuN2 () const
	The effective neutrino nucleon RH coupling: gRnuN2. More...

virtual const double	gVnue () const
	The effective (muon) neutrino-electron vector coupling: gVnue. More...

gslpp::complex	I_triangle_1 (const double tau, const double lambda) const
	Loop function entering in the calculation of the effective $HZ\gamma$ coupling. More...

gslpp::complex	I_triangle_2 (const double tau, const double lambda) const
	Loop function entering in the calculation of the effective $HZ\gamma$ coupling. More...

virtual bool	InitializeModel ()
	A method to initialize the model. More...

const double	intMLL2eeeeus2 (const double s, const double t0, const double t1) const

const double	intMLR2eeeets2 (const double s, const double t0, const double t1) const

const double	intMLRtilde2eeeest2 (const double s, const double t0, const double t1) const

const double	intMRR2eeeeus2 (const double s, const double t0, const double t1) const

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

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

const bool	isSMSuccess () const
	A get method to retrieve the success status of the Standard Model update and matching. More...

virtual const double	LEP2AFBbottom (const double s) const

virtual const double	LEP2AFBcharm (const double s) const

virtual const double	LEP2AFBe (const double s) const

virtual const double	LEP2AFBmu (const double s) const

virtual const double	LEP2AFBtau (const double s) const

virtual const double	LEP2dsigmadcosBinE (const double s, const double cos, const double cosmin, const double cosmax) const

virtual const double	LEP2dsigmadcosBinMu (const double s, const double cos, const double cosmin, const double cosmax) const

virtual const double	LEP2dsigmadcosBinTau (const double s, const double cos, const double cosmin, const double cosmax) const

virtual const double	LEP2dsigmadcosE (const double s, const double cos) const

virtual const double	LEP2dsigmadcosMu (const double s, const double cos) const

virtual const double	LEP2dsigmadcosTau (const double s, const double cos) const

virtual const double	LEP2Rbottom (const double s) const

virtual const double	LEP2Rcharm (const double s) const

virtual const double	LEP2sigmaBottom (const double s) const

virtual const double	LEP2sigmaCharm (const double s) const

virtual const double	LEP2sigmaE (const double s) const

virtual const double	LEP2sigmaHadron (const double s) const

virtual const double	LEP2sigmaMu (const double s) const

virtual const double	LEP2sigmaTau (const double s) const

const double	MLL2eeff (const Particle f, const double s, const double t) const

const double	MLR2eeff (const Particle f, const double s) const

const double	MRL2eeff (const Particle f, const double s) const

const double	MRR2eeff (const Particle f, const double s, const double t) const

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

const double	MwbarFromMw (const double Mw) const
	A method to convert the $W$-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More...

const double	MwFromMwbar (const double Mwbar) const
	A method to convert the $W$-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More...

double	Mzbar () const
	The $Z$-boson mass $\overline{M}_Z$ in the complex-pole/fixed-width scheme. More...

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

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

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

virtual const double	rho_GammaW (const Particle fi, const Particle fj) const
	EW radiative corrections to the width of $W \to f_i \bar{f}_j$, denoted as $\rho^W_{ij}$. More...

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

void	setCKM (const CKM &CKMMatrix)
	A set method to change the CKM matrix. More...

void	setFlagCacheInStandardModel (bool FlagCacheInStandardModel)
	A set method to change the model flag CacheInStandardModel of StandardModel. More...

void	setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ)

bool	setFlagSigmaForAFB (const bool flagSigmaForAFB_i)

bool	setFlagSigmaForR (const bool flagSigmaForR_i)

void	setRequireCKM (bool requireCKM)
	A set method to change the value of requireCKM. More...

void	setSMSuccess (bool success) const
	A set method to change the success status of the Standard Model update and matching. More...

void	setYd (const gslpp::matrix< gslpp::complex > &Yd)
	A set method to set the Yukawa matrix of the down-type quarks, $Y_d$. More...

void	setYe (const gslpp::matrix< gslpp::complex > &Ye)
	A set method to set the Yukawa matrix of the charged leptons, $Y_e$. More...

void	setYu (const gslpp::matrix< gslpp::complex > &Yu)
	A set method to set the Yukawa matrix of the up-type quarks, $Y_u$. More...

virtual const double	SigmaeeHee (const double sqrt_s, const double Pe, const double Pp) const
	The $\sigma(e^+ e^- \to e^+ e^- H)$ in the Standard Model. More...

virtual const double	SigmaeeHvv (const double sqrt_s, const double Pe, const double Pp) const
	The $\sigma(e^+ e^- \to \nu \bar{\nu} H)$ in the Standard Model. More...

virtual const double	SigmaeeZH (const double sqrt_s, const double Pe, const double Pp) const
	The $\sigma(e^+ e^- \to Z H)$ in the Standard Model. More...

	StandardModel ()
	The default constructor. More...

const double	sW2 () const

virtual const double	sW2 (const double Mw_i) const
	The square of the sine of the weak mixing angle in the on-shell scheme, denoted as $s_W^2$. More...

const double	sW2_MSbar_Approx () const
	The (approximated formula for the) square of the sine of the weak mixing angle in the MSbar scheme, denoted as $\hat{s}_{W}^2$. See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) More...

const double	sW2_ND () const
	The square of the sine of the weak mixing angle in the MSbar-ND scheme (w/o decoupling $\alpha\ln(m_t/M_Z)$ terms), denoted as $\hat{s}_{ND}^2$. See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) (eq. 10.13a/10.13b) More...

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

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

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

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

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

virtual const double	ThetaLnuN () const
	The effective neutrino nucleon LH parameter: ThetaLnuN. More...

virtual const double	ThetaRnuN () const
	The effective neutrino nucleon RH parameter: ThetaRnuN. More...

const double	tovers2 (const double cosmin, const double cosmax) const

const double	uovers2 (const double cosmin, const double cosmax) const

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

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

Public Member Functions inherited from QCD
const double	AboveTh (const double mu) const
	The active flavour threshold above the scale $\mu$ as defined in QCD::Thresholds(). More...

void	addParameters (std::vector< std::string > params_i)
	A method to add parameters that are specific to only one set of observables. More...

const double	Als (const double mu, const int Nf_in, const orders order=FULLNLO) const
	Computes the running strong coupling $\alpha_s(\mu)$ with $N_f$ active flavours in the $\overline{\mathrm{MS}}$ scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...

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

const double	Als4 (const double mu) const
	The value of $\alpha_s^{\mathrm{FULLNLO}}$ at any scale $\mu$ with the number of flavours $n_f = 4$. More...

const double	AlsByOrder (const double mu, const int Nf_in, const orders order=FULLNLO) const

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

const double	AlsOLD (const double mu, const orders order=FULLNLO) const
	Computes the running strong coupling $\alpha_s(\mu)$ in the $\overline{\mathrm{MS}}$ scheme. In the cases of LO, NLO and FULLNNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...

const double	AlsWithInit (const double mu, const double alsi, const double mu_i, const int nf, const orders order) const
	Computes the running strong coupling $\alpha_s(\mu)$ from $\alpha_s(\mu_i)$ in the $\overline{\mathrm{MS}}$ scheme, where it is forbidden to across a flavour threshold in the RG running from $\mu_i$ to $\mu$. More...

const double	AlsWithLambda (const double mu, const orders order) const
	Computes the running strong coupling $\alpha_s(\mu)$ in the $\overline{\mathrm{MS}}$ scheme with the use of $\Lambda_{\rm QCD}$. More...

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

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

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

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

const double	Beta3 (const double nf) const
	The $\beta_3(n_f)$ coefficient for a certain number of flavours $n_f$. More...

void	CacheShift (double cache[][5], int n) const
	A member used to manage the caching for this class. More...

void	CacheShift (int cache[][5], int n) const

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

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

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

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

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

const BParameter &	getBBd () const
	For getting the bag parameters corresponding to the operator basis $O_1 -O_5$ in $\Delta b = 2$ process in the $B_d$ meson system. More...

const BParameter &	getBBd_subleading () const
	For getting the subleading bag parameters $R_2 - R_3$ in $\Delta b = 2$ process in the $B_d$ meson system. More...

const BParameter &	getBBs () const
	For getting the bag parameters corresponding to the operator basis $O_1 -O_5$ in $\Delta b = 2$ process in the $B_s$ meson system. More...

const BParameter &	getBBs_subleading () const
	For getting the subleading bag parameters $R_2 - R_3$ in $\Delta b = 2$ process in the $B_s$ meson system. More...

const BParameter &	getBD () const
	For getting the bag parameters corresponding to the operator basis $O_1 -O_5$ in $\Delta c = 2$ process in the $D^0$ meson system. More...

const BParameter &	getBK () const
	For getting the bag parameters corresponding to the operator basis $O_1 -O_5$ in $\Delta s = 2$ process in the $K^0$ meson system. More...

const BParameter &	getBKd1 () const

const BParameter &	getBKd3 () const

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

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

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

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

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

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

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

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

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

const Particle &	getQuarks (const QCD::quark q) const
	A get method to access a quark as an object of the type Particle. More...

std::vector< std::string >	getUnknownParameters ()
	A method to get the vector of the parameters that have been specified in the configuration file but not being used. More...

void	initializeBParameter (std::string name_i) const
	A method to initialize B Parameter and the corresponding meson. More...

void	initializeMeson (QCD::meson meson_i) const
	A method to initialize a meson. More...

bool	isQCDsuccess () const
	A getter for the QCDsuccess flag. More...

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

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

const double	Mofmu2Mbar (const double m, const double mu, const quark q) const
	Converts a quark running mass at an arbitrary scale to the corresponding $\overline{\mathrm{MS}}$ mass $m(m)$. More...

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

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

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

const double	Mrun4 (const double mu_f, const double mu_i, const double m) const
	The running of a mass with the number of flavours $n_f = 4$. More...

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

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

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

const double	NfThresholdCorrections (double mu, double M, double als, int nf, orders order) const
	Threshold corrections in matching $\alpha_s(n_f+1)$ with $\alpha_s(n_f)$ from eq. (34) of hep-ph/0512060. More...

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

	QCD ()
	Constructor. More...

void	setComputemt (bool computemt)
	A set method to change the value of computemt. More...

void	setMtpole (double mtpole_in)
	A method to set the pole mass of the top quark. More...

void	setNc (double Nc)
	A set method to change the number of colours $N_c$. More...

void	setOptionalParameter (std::string name, double value)
	A method to set the parameter value for the parameters that are specific to only one set of observables. More...

void	setQuarkMass (const quark q, const double mass)
	A set method to change the mass of a quark. More...

const double	Thresholds (const int i) const
	For accessing the active flavour threshold scales. More...

Public Member Functions inherited from Model
void	addMissingModelParameter (const std::string &missingParameterName)

std::vector< std::string >	getmissingModelParameters ()

unsigned int	getMissingModelParametersCount ()

std::string	getModelName () const
	A method to fetch the name of the model. More...

const double &	getModelParam (std::string name) const

bool	isModelFWC_DF2 () const

bool	isModelGeneralTHDM () const

bool	isModelGeorgiMachacek () const

bool	IsModelInitialized () const
	A method to check if the model is initialized. More...

bool	isModelLinearized () const

bool	isModelNPquadratic () const

bool	isModelParam (std::string name) const

bool	isModelSUSY () const

bool	isModelTHDM () const

bool	isModelTHDMW () const

bool	IsUpdateError () const
	A method to check if there was any error in the model update process. More...

	Model ()
	The default constructor. More...

void	raiseMissingModelParameterCount ()

void	setModelFWC_DF2 ()

void	setModelGeneralTHDM ()

void	setModelGeorgiMachacek ()

void	setModelInitialized (bool ModelInitialized)
	A set method to fix the failure or success of the initialization of the model. More...

void	setModelLinearized (bool linearized=true)

void	setModelName (const std::string name)
	A method to set the name of the model. More...

void	setModelNPquadratic (bool NPquadratic=true)

void	setModelSUSY ()

void	setModelTHDM ()

void	setModelTHDMW ()

void	setSliced (bool Sliced)

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

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

Static Public Attributes
static const int	NNPSMEFTd6MFVVars = 178+1

static std::string	NPSMEFTd6MFVVars [NNPSMEFTd6MFVVars]

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 = 28
	The number of the model parameters in StandardModel. More...

static const int	NumSMParamsForEWPO = 35
	The number of the SM parameters that are relevant to the EW precision observables. More...

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

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

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

Protected Member Functions
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 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	CdB_0_LNP = 0.

double	CdB_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{Hq}^{(1)})_{ij}$. More...

double	CdB_u_LNP = 0.

double	Cdd_00_LNP = 0.

double	Cdd_d0_LNP = 0.

double	Cdd_dd_LNP = 0.

double	Cddp_00_LNP = 0.

double	Cddp_d0_LNP = 0.

double	Cddp_dd_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ud}^{(1)})_{ijkm}$. More...

double	CdG_0_LNP = 0.

double	CdG_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{dW})_{ij}$. More...

double	CdG_u_LNP = 0.

double	CdH_0_LNP = 0.

double	CdH_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{dG})_{ij}$. More...

double	CdH_u_LNP = 0.

double	CdW_0_LNP = 0.

double	CdW_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{dB})_{ij}$. More...

double	CdW_u_LNP = 0.

double	Ced_0_LNP = 0.

double	Ced_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qq}^{(1)})_{ijkm}$. More...

double	Cee_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{le})_{ijkm}$. More...

double	Ceu_0_LNP = 0.

double	Ceu_u_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ld})_{ijkm}$. More...

double	CHd_0_LNP = 0.

double	CHd_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{Hud})_{ij}$. More...

double	CHe_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ll})_{ijkm}$. More...

double	CHl1_LNP = 0.
	< Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{Hl}^{(1)})_{ij}$. More...

double	CHl3_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{He})_{ij}$. More...

double	CHq1_0_LNP = 0.

double	CHq1_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{Hq}^{(3)})_{ij}$. More...

double	CHq1_u_LNP = 0.

double	CHq3_0_LNP = 0.

double	CHq3_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{Hu})_{ij}$. More...

double	CHq3_u_LNP = 0.

double	CHu_0_LNP = 0.

double	CHu_u_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{Hd})_{ij}$. More...

double	CHud_ud_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{lq}^{(1)})_{ijkm}$. More...

double	Cld_0_LNP = 0.

double	Cld_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ed})_{ijkm}$. More...

double	Cle_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{uH})_{ij}$. More...

double	Cll_aabb_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ll})_{ijkm}$. More...

double	Cll_abba_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ee})_{ijkm}$. More...

double	Clq1_0_LNP = 0.

double	Clq1_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{lq}^{(3)})_{ijkm}$. More...

double	Clq1_u_LNP = 0.

double	Clq3_0_LNP = 0.

double	Clq3_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qe})_{ijkm}$. More...

double	Clq3_u_LNP = 0.

double	Clu_0_LNP = 0.

double	Clu_u_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{eu})_{ijkm}$. More...

double	Cqd1_00_LNP = 0.

double	Cqd1_0d_LNP = 0.

double	Cqd1_d0_LNP = 0.

double	Cqd1_dd_LNP = 0.

double	Cqd1_dy_LNP = 0.

double	Cqd1_u0_LNP = 0.

double	Cqd1_ud_LNP = 0.

double	Cqd1_uy_LNP = 0.

double	Cqd1_y_LNP = 0.

double	Cqd1_yd_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qd}^{(8)})_{ijkm}$. More...

double	Cqd1_yu_LNP = 0.

double	Cqd8_00_LNP = 0.

double	Cqd8_0d_LNP = 0.

double	Cqd8_d0_LNP = 0.

double	Cqd8_dd_LNP = 0.

double	Cqd8_dy_LNP = 0.

double	Cqd8_u0_LNP = 0.

double	Cqd8_ud_LNP = 0.

double	Cqd8_uy_LNP = 0.

double	Cqd8_y_LNP = 0.

double	Cqd8_yd_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{quqd}^{(1)})_{ijkm}$. More...

double	Cqd8_yu_LNP = 0.

double	Cqe_0_LNP = 0.

double	Cqe_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{lu})_{ijkm}$. More...

double	Cqe_u_LNP = 0.

double	Cqq1_00_LNP = 0.

double	Cqq1_d0_LNP = 0.

double	Cqq1_dd_LNP = 0.

double	Cqq1_u0_LNP = 0.

double	Cqq1_ud_LNP = 0.

double	Cqq1_uu_LNP = 0.

double	Cqq1p_00_LNP = 0.

double	Cqq1p_d0_LNP = 0.

double	Cqq1p_dd_LNP = 0.

double	Cqq1p_u0_LNP = 0.

double	Cqq1p_ud_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qq}^{(3)})_{ijkm}$. More...

double	Cqq1p_uu_LNP = 0.

double	Cqq3_00_LNP = 0.

double	Cqq3_d0_LNP = 0.

double	Cqq3_dd_LNP = 0.

double	Cqq3_u0_LNP = 0.

double	Cqq3_ud_LNP = 0.

double	Cqq3_uu_LNP = 0.

double	Cqq3p_00_LNP = 0.

double	Cqq3p_d0_LNP = 0.

double	Cqq3p_dd_LNP = 0.

double	Cqq3p_u0_LNP = 0.

double	Cqq3p_ud_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{uu})_{ijkm}$. More...

double	Cqq3p_uu_LNP = 0.

double	Cqu1_00_LNP = 0.

double	Cqu1_0u_LNP = 0.

double	Cqu1_d0_LNP = 0.

double	Cqu1_du_LNP = 0.

double	Cqu1_dy_LNP = 0.

double	Cqu1_u0_LNP = 0.

double	Cqu1_uu_LNP = 0.

double	Cqu1_uy_LNP = 0.

double	Cqu1_y_LNP = 0.

double	Cqu1_yd_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qu}^{(8)})_{ijkm}$. More...

double	Cqu1_yu_LNP = 0.

double	Cqu8_00_LNP = 0.

double	Cqu8_0u_LNP = 0.

double	Cqu8_d0_LNP = 0.

double	Cqu8_du_LNP = 0.

double	Cqu8_dy_LNP = 0.

double	Cqu8_u0_LNP = 0.

double	Cqu8_uu_LNP = 0.

double	Cqu8_uy_LNP = 0.

double	Cqu8_y_LNP = 0.

double	Cqu8_yd_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qd}^{(1)})_{ijkm}$. More...

double	Cqu8_yu_LNP = 0.

double	Cquqd1_00_LNP = 0.

double	Cquqd1_0d_LNP = 0.

double	Cquqd1_0u_LNP = 0.

double	Cquqd1_d0_LNP = 0.

double	Cquqd1_u0_LNP = 0.

double	Cquqd1p_00_LNP = 0.

double	Cquqd1p_0d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{quqd}^{(8)})_{ijkm}$. More...

double	Cquqd1p_0u_LNP = 0.

double	Cquqd1p_d0_LNP = 0.

double	Cquqd1p_u0_LNP = 0.

double	Cquqd8_00_LNP = 0.

double	Cquqd8_0d_LNP = 0.

double	Cquqd8_0u_LNP = 0.

double	Cquqd8_d0_LNP = 0.

double	Cquqd8_u0_LNP = 0.

double	Cquqd8p_00_LNP = 0.

double	Cquqd8p_0d_LNP = 0.

double	Cquqd8p_0u_LNP = 0.

double	Cquqd8p_d0_LNP = 0.

double	Cquqd8p_u0_LNP = 0.

double	CuB_0_LNP = 0.

double	CuB_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{dH})_{ij}$. More...

double	CuB_u_LNP = 0.

double	Cud1_00_LNP = 0.

double	Cud1_0d_LNP = 0.

double	Cud1_u0_LNP = 0.

double	Cud1_ud_LNP = 0.

double	Cud1p_ud_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ud}^{(8)})_{ijkm}$. More...

double	Cud8_00_LNP = 0.

double	Cud8_0d_LNP = 0.

double	Cud8_u0_LNP = 0.

double	Cud8_ud_LNP = 0.

double	Cud8p_ud_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qu}^{(1)})_{ijkm}$. More...

double	CuG_0_LNP = 0.

double	CuG_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{uW})_{ij}$. More...

double	CuG_u_LNP = 0.

double	CuH_0_LNP = 0.

double	CuH_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{uG})_{ij}$. More...

double	CuH_u_LNP = 0.

double	Cuu_00_LNP = 0.

double	Cuu_u0_LNP = 0.

double	Cuu_uu_LNP = 0.

double	Cuup_00_LNP = 0.

double	Cuup_u0_LNP = 0.

double	Cuup_uu_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{dd})_{ijkm}$. More...

double	CuW_0_LNP = 0.

double	CuW_d_LNP = 0.
	Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{uB})_{ij}$. More...

double	CuW_u_LNP = 0.

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

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

double	alpha21

double	alpha31

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

bool	bSigmaForAFB

bool	bSigmaForR

double	dAl5hMz
	The five-flavour hadronic contribution to the electromagnetic coupling, $\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)$. (Non-input parameter) More...

double	dAle5Mz
	The five-flavour hadronic contribution to the electromagnetic coupling, $\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)$, used as input for FlagMWinput = FALSE. More...

double	delGammaWlv
	The theoretical uncertainty in $\Gamma_W_{l\nu}$, denoted as $\delta\,\Gamma_W_{l\nu}$. More...

double	delGammaWqq
	The theoretical uncertainty in $\Gamma_W_{qq}$, denoted as $\delta\,\Gamma_W_{qq}$. More...

double	delGammaZ
	The theoretical uncertainty in $\Gamma_Z$, denoted as $\delta\,\Gamma_Z$, in GeV. More...

double	delMw
	The theoretical uncertainty in $M_W$, denoted as $\delta\,M_W$, in GeV. More...

double	delR0b
	The theoretical uncertainty in $R_b^0$, denoted as $\delta\,R_b^0$. More...

double	delR0c
	The theoretical uncertainty in $R_c^0$, denoted as $\delta\,R_c^0$. More...

double	delR0l
	The theoretical uncertainty in $R_l^0$, denoted as $\delta\,R_l^0$. More...

double	delsigma0H
	The theoretical uncertainty in $\sigma_{Hadron}^0$, denoted as $\delta\,\sigma_{Hadron}^0$ in nb. More...

double	delSin2th_b
	The theoretical uncertainty in $\sin^2\theta_{\rm eff}^{b}$, denoted as $\delta\sin^2\theta_{\rm eff}^{b}$. More...

double	delSin2th_l
	The theoretical uncertainty in $\sin^2\theta_{\rm eff}^{\rm lept}$, denoted as $\delta\sin^2\theta_{\rm eff}^{\rm lept}$. More...

double	delSin2th_q
	The theoretical uncertainty in $\sin^2\theta_{\rm eff}^{q\not = b,t}$, denoted as $\delta\sin^2\theta_{\rm eff}^{q\not = b,t}$. More...

double	delta

double	etab
	The CKM parameter $\bar{\eta}$ in the Wolfenstein parameterization. More...

bool	flag_order [orders_EW_size]
	An array of internal flags controlling the inclusions of higher-order corrections. More...

bool	FlagFixMuwMut
	A boolean for the model flag FixMuwMut. More...

bool	flagLEP2 [NUMofLEP2RCs]

double	gamma
	$\gamma $ used as an input for FlagWolfenstein = FALSE More...

double	GF
	The Fermi constant $G_\mu$ in ${\rm GeV}^{-2}$. More...

double	lambda
	The CKM parameter $\lambda$ in the Wolfenstein parameterization. More...

Particle	leptons [6]
	An array of Particle objects for the leptons. More...

double	mHl
	The Higgs mass $m_h$ in GeV. More...

double	muw
	A matching scale $\mu_W$ around the weak scale in GeV. More...

double	Mw_inp
	The mass of the $W$ boson in GeV used as input for FlagMWinput = TRUE. More...

CKM	myCKM
	An object of type CKM. More...

PMNS	myPMNS

double	Mz
	The mass of the $Z$ boson in GeV. More...

bool	requireCKM
	An internal flag to control whether the CKM matrix has to be recomputed. More...

bool	requireYe
	An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed. More...

bool	requireYn
	An internal flag to control whether the neutrino Yukawa matrix has to be recomputed. More...

double	rhob
	The CKM parameter $\bar{\rho}$ in the Wolfenstein parameterization. More...

double	s12

double	s13

double	s23

Flavour	SMFlavour
	An object of type Flavour. More...

Matching< StandardModelMatching, StandardModel >	SMM
	An object of type Matching. More...

double	Vcb
	$\vert V_{cb} \vert $ used as an input for FlagWolfenstein = FALSE More...

double	Vub
	$\vert V_{ub} \vert $ used as an input for FlagWolfenstein = FALSE More...

double	Vud
	$\vert V_{ud} \vert $ used as an input for FlagWolfenstein = FALSE and FlagUseVud = TRUE More...

double	Vus
	$\vert V_{us} \vert $ used as an input for FlagWolfenstein = FALSE More...

gslpp::matrix< gslpp::complex >	Yd
	The Yukawa matrix of the down-type quarks. More...

gslpp::matrix< gslpp::complex >	Ye
	The Yukawa matrix of the charged leptons. More...

gslpp::matrix< gslpp::complex >	Yn
	The Yukawa matrix of the neutrinos. More...

gslpp::matrix< gslpp::complex >	Yu
	The Yukawa matrix of the up-type quarks. More...

Protected Attributes inherited from QCD
double	AlsM
	The strong coupling constant at the mass scale MAls, $\alpha_s(M_{\alpha_s})$. More...

double	CA

double	CF

bool	computemt
	Switch for computing the $\overline{\mathrm{MS}}$ mass of the top quark. More...

double	dAdA_NA

double	dFdA_NA

double	dFdF_NA

bool	FlagMpole2MbarNumeric
	A flag to determine whether the pole mass to $\over \mathrm{MS}$ mass conversion is done numerically. More...

bool	FlagMtPole
	A flag to determine whether the pole mass of the top quark is used as input. More...

double	MAls
	The mass scale in GeV at which the strong coupling measurement is provided. More...

double	mtpole
	The pole mass of the top quark. More...

double	mub
	The threshold between five- and four-flavour theory in GeV. More...

double	muc
	The threshold between four- and three-flavour theory in GeV. More...

double	mut
	The threshold between six- and five-flavour theory in GeV. More...

double	NA

double	Nc
	The number of colours. More...

bool	QCDsuccess =true

Particle	quarks [6]
	The vector of all SM quarks. More...

bool	requireYd
	Switch for generating the Yukawa couplings to the down-type quarks. More...

bool	requireYu
	Switch for generating the Yukawa couplings to the up-type quarks. More...

double	TF

Protected Attributes inherited from Model
bool	isSliced = false
	A boolean set to true if the current istance is a slice of an extended object. More...

std::map< std::string, std::reference_wrapper< const double > >	ModelParamMap

bool	UpdateError = false
	A boolean set to false if update is successful. More...

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...

Constructor & Destructor Documentation

◆ NPSMEFTd6MFV()

NPSMEFTd6MFV::NPSMEFTd6MFV ( )

Definition at line 40 of file NPSMEFTd6MFV.cpp.

                          : NPSMEFTd6General() {
    setModelName("NPSMEFTd6MFV");
    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("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("Cee_LNP",std::cref(Cee_LNP)));
    ModelParamMap.insert(std::make_pair("Cle_LNP",std::cref(Cle_LNP)));
    ModelParamMap.insert(std::make_pair("CuH_0_LNP",std::cref(CuH_0_LNP)));
    ModelParamMap.insert(std::make_pair("CuH_u_LNP",std::cref(CuH_u_LNP)));
    ModelParamMap.insert(std::make_pair("CuH_d_LNP",std::cref(CuH_d_LNP)));
    ModelParamMap.insert(std::make_pair("CuG_0_LNP",std::cref(CuG_0_LNP)));
    ModelParamMap.insert(std::make_pair("CuG_u_LNP",std::cref(CuG_u_LNP)));
    ModelParamMap.insert(std::make_pair("CuG_d_LNP",std::cref(CuG_d_LNP)));
    ModelParamMap.insert(std::make_pair("CuW_0_LNP",std::cref(CuW_0_LNP)));
    ModelParamMap.insert(std::make_pair("CuW_u_LNP",std::cref(CuW_u_LNP)));
    ModelParamMap.insert(std::make_pair("CuW_d_LNP",std::cref(CuW_d_LNP)));
    ModelParamMap.insert(std::make_pair("CuB_0_LNP",std::cref(CuB_0_LNP)));
    ModelParamMap.insert(std::make_pair("CuB_u_LNP",std::cref(CuB_u_LNP)));
    ModelParamMap.insert(std::make_pair("CuB_d_LNP",std::cref(CuB_d_LNP)));
    ModelParamMap.insert(std::make_pair("CdH_0_LNP",std::cref(CdH_0_LNP)));
    ModelParamMap.insert(std::make_pair("CdH_u_LNP",std::cref(CdH_u_LNP)));
    ModelParamMap.insert(std::make_pair("CdH_d_LNP",std::cref(CdH_d_LNP)));
    ModelParamMap.insert(std::make_pair("CdG_0_LNP",std::cref(CdG_0_LNP)));
    ModelParamMap.insert(std::make_pair("CdG_u_LNP",std::cref(CdG_u_LNP)));
    ModelParamMap.insert(std::make_pair("CdG_d_LNP",std::cref(CdG_d_LNP)));
    ModelParamMap.insert(std::make_pair("CdW_0_LNP",std::cref(CdW_0_LNP)));
    ModelParamMap.insert(std::make_pair("CdW_u_LNP",std::cref(CdW_u_LNP)));
    ModelParamMap.insert(std::make_pair("CdW_d_LNP",std::cref(CdW_d_LNP)));
    ModelParamMap.insert(std::make_pair("CdB_0_LNP",std::cref(CdB_0_LNP)));
    ModelParamMap.insert(std::make_pair("CdB_u_LNP",std::cref(CdB_u_LNP)));
    ModelParamMap.insert(std::make_pair("CdB_d_LNP",std::cref(CdB_d_LNP)));
    ModelParamMap.insert(std::make_pair("CHq1_0_LNP",std::cref(CHq1_0_LNP)));
    ModelParamMap.insert(std::make_pair("CHq1_u_LNP",std::cref(CHq1_u_LNP)));
    ModelParamMap.insert(std::make_pair("CHq1_d_LNP",std::cref(CHq1_d_LNP)));
    ModelParamMap.insert(std::make_pair("CHq3_0_LNP",std::cref(CHq3_0_LNP)));
    ModelParamMap.insert(std::make_pair("CHq3_u_LNP",std::cref(CHq3_u_LNP)));
    ModelParamMap.insert(std::make_pair("CHq3_d_LNP",std::cref(CHq3_d_LNP)));
    ModelParamMap.insert(std::make_pair("CHu_0_LNP",std::cref(CHu_0_LNP)));
    ModelParamMap.insert(std::make_pair("CHu_u_LNP",std::cref(CHu_u_LNP)));
    ModelParamMap.insert(std::make_pair("CHd_0_LNP",std::cref(CHd_0_LNP)));
    ModelParamMap.insert(std::make_pair("CHd_d_LNP",std::cref(CHd_d_LNP)));
    ModelParamMap.insert(std::make_pair("CHud_ud_LNP",std::cref(CHud_ud_LNP)));
    ModelParamMap.insert(std::make_pair("Clq1_0_LNP",std::cref(Clq1_0_LNP)));
    ModelParamMap.insert(std::make_pair("Clq1_u_LNP",std::cref(Clq1_u_LNP)));
    ModelParamMap.insert(std::make_pair("Clq1_d_LNP",std::cref(Clq1_d_LNP)));
    ModelParamMap.insert(std::make_pair("Clq3_0_LNP",std::cref(Clq3_0_LNP)));
    ModelParamMap.insert(std::make_pair("Clq3_u_LNP",std::cref(Clq3_u_LNP)));
    ModelParamMap.insert(std::make_pair("Clq3_d_LNP",std::cref(Clq3_d_LNP)));
    ModelParamMap.insert(std::make_pair("Cqe_0_LNP",std::cref(Cqe_0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqe_u_LNP",std::cref(Cqe_u_LNP)));
    ModelParamMap.insert(std::make_pair("Cqe_d_LNP",std::cref(Cqe_d_LNP)));
    ModelParamMap.insert(std::make_pair("Clu_0_LNP",std::cref(Clu_0_LNP)));
    ModelParamMap.insert(std::make_pair("Clu_u_LNP",std::cref(Clu_u_LNP)));
    ModelParamMap.insert(std::make_pair("Ceu_0_LNP",std::cref(Ceu_0_LNP)));
    ModelParamMap.insert(std::make_pair("Ceu_u_LNP",std::cref(Ceu_u_LNP)));
    ModelParamMap.insert(std::make_pair("Cld_0_LNP",std::cref(Cld_0_LNP)));
    ModelParamMap.insert(std::make_pair("Cld_d_LNP",std::cref(Cld_d_LNP)));
    ModelParamMap.insert(std::make_pair("Ced_0_LNP",std::cref(Ced_0_LNP)));
    ModelParamMap.insert(std::make_pair("Ced_d_LNP",std::cref(Ced_d_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq1_00_LNP",std::cref(Cqq1_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq1_u0_LNP",std::cref(Cqq1_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq1_d0_LNP",std::cref(Cqq1_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq1_uu_LNP",std::cref(Cqq1_uu_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq1_dd_LNP",std::cref(Cqq1_dd_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq1_ud_LNP",std::cref(Cqq1_ud_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq1p_00_LNP",std::cref(Cqq1p_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq1p_u0_LNP",std::cref(Cqq1p_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq1p_d0_LNP",std::cref(Cqq1p_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq1p_uu_LNP",std::cref(Cqq1p_uu_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq1p_dd_LNP",std::cref(Cqq1p_dd_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq1p_ud_LNP",std::cref(Cqq1p_ud_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3_00_LNP",std::cref(Cqq3_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3_u0_LNP",std::cref(Cqq3_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3_d0_LNP",std::cref(Cqq3_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3_uu_LNP",std::cref(Cqq3_uu_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3_dd_LNP",std::cref(Cqq3_dd_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3_ud_LNP",std::cref(Cqq3_ud_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3p_00_LNP",std::cref(Cqq3p_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3p_u0_LNP",std::cref(Cqq3p_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3p_d0_LNP",std::cref(Cqq3p_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3p_uu_LNP",std::cref(Cqq3p_uu_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3p_dd_LNP",std::cref(Cqq3p_dd_LNP)));
    ModelParamMap.insert(std::make_pair("Cqq3p_ud_LNP",std::cref(Cqq3p_ud_LNP)));
    ModelParamMap.insert(std::make_pair("Cuu_00_LNP",std::cref(Cuu_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cuu_u0_LNP",std::cref(Cuu_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cuu_uu_LNP",std::cref(Cuu_uu_LNP)));
    ModelParamMap.insert(std::make_pair("Cuup_00_LNP",std::cref(Cuup_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cuup_u0_LNP",std::cref(Cuup_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cuup_uu_LNP",std::cref(Cuup_uu_LNP)));
    ModelParamMap.insert(std::make_pair("Cdd_00_LNP",std::cref(Cdd_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cdd_d0_LNP",std::cref(Cdd_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cdd_dd_LNP",std::cref(Cdd_dd_LNP)));
    ModelParamMap.insert(std::make_pair("Cddp_00_LNP",std::cref(Cddp_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cddp_d0_LNP",std::cref(Cddp_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cddp_dd_LNP",std::cref(Cddp_dd_LNP)));
    ModelParamMap.insert(std::make_pair("Cud1_00_LNP",std::cref(Cud1_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cud1_u0_LNP",std::cref(Cud1_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cud1_0d_LNP",std::cref(Cud1_0d_LNP)));
    ModelParamMap.insert(std::make_pair("Cud1_ud_LNP",std::cref(Cud1_ud_LNP)));
    ModelParamMap.insert(std::make_pair("Cud1p_ud_LNP",std::cref(Cud1p_ud_LNP)));
    ModelParamMap.insert(std::make_pair("Cud8_00_LNP",std::cref(Cud8_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cud8_u0_LNP",std::cref(Cud8_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cud8_0d_LNP",std::cref(Cud8_0d_LNP)));
    ModelParamMap.insert(std::make_pair("Cud8_ud_LNP",std::cref(Cud8_ud_LNP)));
    ModelParamMap.insert(std::make_pair("Cud8p_ud_LNP",std::cref(Cud8p_ud_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu1_00_LNP",std::cref(Cqu1_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu1_u0_LNP",std::cref(Cqu1_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu1_d0_LNP",std::cref(Cqu1_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu1_0u_LNP",std::cref(Cqu1_0u_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu1_uu_LNP",std::cref(Cqu1_uu_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu1_du_LNP",std::cref(Cqu1_du_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu1_y_LNP",std::cref(Cqu1_y_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu1_uy_LNP",std::cref(Cqu1_uy_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu1_dy_LNP",std::cref(Cqu1_dy_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu1_yu_LNP",std::cref(Cqu1_yu_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu1_yd_LNP",std::cref(Cqu1_yd_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu8_00_LNP",std::cref(Cqu8_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu8_u0_LNP",std::cref(Cqu8_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu8_d0_LNP",std::cref(Cqu8_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu8_0u_LNP",std::cref(Cqu8_0u_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu8_uu_LNP",std::cref(Cqu8_uu_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu8_du_LNP",std::cref(Cqu8_du_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu8_y_LNP",std::cref(Cqu8_y_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu8_uy_LNP",std::cref(Cqu8_uy_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu8_dy_LNP",std::cref(Cqu8_dy_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu8_yu_LNP",std::cref(Cqu8_yu_LNP)));
    ModelParamMap.insert(std::make_pair("Cqu8_yd_LNP",std::cref(Cqu8_yd_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd1_00_LNP",std::cref(Cqd1_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd1_u0_LNP",std::cref(Cqd1_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd1_d0_LNP",std::cref(Cqd1_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd1_0d_LNP",std::cref(Cqd1_0d_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd1_ud_LNP",std::cref(Cqd1_ud_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd1_dd_LNP",std::cref(Cqd1_dd_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd1_y_LNP",std::cref(Cqd1_y_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd1_uy_LNP",std::cref(Cqd1_uy_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd1_dy_LNP",std::cref(Cqd1_dy_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd1_yu_LNP",std::cref(Cqd1_yu_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd1_yd_LNP",std::cref(Cqd1_yd_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd8_00_LNP",std::cref(Cqd8_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd8_u0_LNP",std::cref(Cqd8_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd8_d0_LNP",std::cref(Cqd8_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd8_0d_LNP",std::cref(Cqd8_0d_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd8_ud_LNP",std::cref(Cqd8_ud_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd8_dd_LNP",std::cref(Cqd8_dd_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd8_y_LNP",std::cref(Cqd8_y_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd8_uy_LNP",std::cref(Cqd8_uy_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd8_dy_LNP",std::cref(Cqd8_dy_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd8_yu_LNP",std::cref(Cqd8_yu_LNP)));
    ModelParamMap.insert(std::make_pair("Cqd8_yd_LNP",std::cref(Cqd8_yd_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd1_00_LNP",std::cref(Cquqd1_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd1_u0_LNP",std::cref(Cquqd1_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd1_d0_LNP",std::cref(Cquqd1_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd1_0u_LNP",std::cref(Cquqd1_0u_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd1_0d_LNP",std::cref(Cquqd1_0d_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd1p_00_LNP",std::cref(Cquqd1p_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd1p_u0_LNP",std::cref(Cquqd1p_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd1p_d0_LNP",std::cref(Cquqd1p_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd1p_0u_LNP",std::cref(Cquqd1p_0u_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd1p_0d_LNP",std::cref(Cquqd1p_0d_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd8_00_LNP",std::cref(Cquqd8_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd8_u0_LNP",std::cref(Cquqd8_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd8_d0_LNP",std::cref(Cquqd8_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd8_0u_LNP",std::cref(Cquqd8_0u_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd8_0d_LNP",std::cref(Cquqd8_0d_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd8p_00_LNP",std::cref(Cquqd8p_00_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd8p_u0_LNP",std::cref(Cquqd8p_u0_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd8p_d0_LNP",std::cref(Cquqd8p_d0_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd8p_0u_LNP",std::cref(Cquqd8p_0u_LNP)));
    ModelParamMap.insert(std::make_pair("Cquqd8p_0d_LNP",std::cref(Cquqd8p_0d_LNP)));
 
}

Member Function Documentation

◆ PostUpdate()

bool NPSMEFTd6MFV::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 2080 of file NPSMEFTd6MFV.cpp.

                              {
 
    NPSMEFTd6General::GenerateSMInitialConditions();
    
    setNPSMEFTd6GeneralParameters();
    
    if (!NPSMEFTd6General::PostUpdate()) return (false);
    
    return (true);    
}

◆ setNPSMEFTd6GeneralParameters()

void NPSMEFTd6MFV::setNPSMEFTd6GeneralParameters ( )

protected

An auxiliary method to set the WC of the general class.

Definition at line 587 of file NPSMEFTd6MFV.cpp.

                                                 {
    
    // Precomputing Yukawa matrices and matrix products 
 
    // Single Yukawa
    gslpp::matrix<gslpp::complex> YuL(3, 3, 0.), YucL(3, 3, 0.);
    gslpp::matrix<gslpp::complex> YdL(3, 3, 0.), YdcL(3, 3, 0.);
 
    for (int i = 0; i < 3; i++) {
        for (int j = 0; j < 3; j++) {
            YuL.assignre(i, j, getSMEFTCoeffEW("YuR", i, j));
            YuL.assignim(i, j, getSMEFTCoeffEW("YuI", i, j));
        }
    }
 
    for (int i = 0; i < 3; i++) {
        for (int j = 0; j < 3; j++) {
            YdL.assignre(i, j, getSMEFTCoeffEW("YdR", i, j));
            YdL.assignim(i, j, getSMEFTCoeffEW("YdI", i, j));
        }
    }
 
    YucL = YuL.hconjugate();
    YdcL = YdL.hconjugate();
 
    // Products of two Yukawas
    gslpp::matrix<gslpp::complex> SQUL(3, 3, 0.), SUL(3, 3, 0.);
    gslpp::matrix<gslpp::complex> SQDL(3, 3, 0.), SDL(3, 3, 0.);
    gslpp::matrix<gslpp::complex> SUDL(3, 3, 0.), SUDcL(3, 3, 0.);
 
    SQUL  = YucL * YuL;
    SQDL  = YdcL * YdL;
 
    SUL   = YuL * YucL;
    SDL   = YdL * YdcL;
 
    SUDL  = YuL * YdcL;
    SUDcL = YdL * YucL;
 
    // Products of three Yukawas
    gslpp::matrix<gslpp::complex> SQUYucL(3, 3, 0.), YuSQUL(3, 3, 0.);
    gslpp::matrix<gslpp::complex> SQUYdcL(3, 3, 0.), YdSQUL(3, 3, 0.);
    gslpp::matrix<gslpp::complex> SQDYucL(3, 3, 0.), YuSQDL(3, 3, 0.);
    gslpp::matrix<gslpp::complex> SQDYdcL(3, 3, 0.), YdSQDL(3, 3, 0.);
    
    SQUYucL = SQUL * YucL;
    YuSQUL  = YuL  * SQUL;
 
    SQUYdcL = SQUL * YdcL;
    YdSQUL  = YdL  * SQUL;
 
    SQDYucL = SQDL * YucL;
    YuSQDL  = YuL  * SQDL;
 
    SQDYdcL = SQDL * YdcL;
    YdSQDL  = YdL  * SQDL;
 
 
    // Operator assignments
 
    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;
 
    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;
 
    CuH_11r_LNP = (CuH_d_LNP*SQDYucL(0,0) + CuH_u_LNP*SQUYucL(0,0) + CuH_0_LNP*YucL(0,0)).real();
    CuH_11i_LNP = (CuH_d_LNP*SQDYucL(0,0) + CuH_u_LNP*SQUYucL(0,0) + CuH_0_LNP*YucL(0,0)).imag();
    CuH_12r_LNP = (CuH_d_LNP*SQDYucL(0,1) + CuH_u_LNP*SQUYucL(0,1) + CuH_0_LNP*YucL(0,1)).real();
    CuH_12i_LNP = (CuH_d_LNP*SQDYucL(0,1) + CuH_u_LNP*SQUYucL(0,1) + CuH_0_LNP*YucL(0,1)).imag();
    CuH_13r_LNP = (CuH_d_LNP*SQDYucL(0,2) + CuH_u_LNP*SQUYucL(0,2) + CuH_0_LNP*YucL(0,2)).real();
    CuH_13i_LNP = (CuH_d_LNP*SQDYucL(0,2) + CuH_u_LNP*SQUYucL(0,2) + CuH_0_LNP*YucL(0,2)).imag();
    CuH_21r_LNP = (CuH_d_LNP*SQDYucL(1,0) + CuH_u_LNP*SQUYucL(1,0) + CuH_0_LNP*YucL(1,0)).real();
    CuH_21i_LNP = (CuH_d_LNP*SQDYucL(1,0) + CuH_u_LNP*SQUYucL(1,0) + CuH_0_LNP*YucL(1,0)).imag();
    CuH_22r_LNP = (CuH_d_LNP*SQDYucL(1,1) + CuH_u_LNP*SQUYucL(1,1) + CuH_0_LNP*YucL(1,1)).real();
    CuH_22i_LNP = (CuH_d_LNP*SQDYucL(1,1) + CuH_u_LNP*SQUYucL(1,1) + CuH_0_LNP*YucL(1,1)).imag();
    CuH_23r_LNP = (CuH_d_LNP*SQDYucL(1,2) + CuH_u_LNP*SQUYucL(1,2) + CuH_0_LNP*YucL(1,2)).real();
    CuH_23i_LNP = (CuH_d_LNP*SQDYucL(1,2) + CuH_u_LNP*SQUYucL(1,2) + CuH_0_LNP*YucL(1,2)).imag();
    CuH_31r_LNP = (CuH_d_LNP*SQDYucL(2,0) + CuH_u_LNP*SQUYucL(2,0) + CuH_0_LNP*YucL(2,0)).real();
    CuH_31i_LNP = (CuH_d_LNP*SQDYucL(2,0) + CuH_u_LNP*SQUYucL(2,0) + CuH_0_LNP*YucL(2,0)).imag();
    CuH_32r_LNP = (CuH_d_LNP*SQDYucL(2,1) + CuH_u_LNP*SQUYucL(2,1) + CuH_0_LNP*YucL(2,1)).real();
    CuH_32i_LNP = (CuH_d_LNP*SQDYucL(2,1) + CuH_u_LNP*SQUYucL(2,1) + CuH_0_LNP*YucL(2,1)).imag();
    CuH_33r_LNP = (CuH_d_LNP*SQDYucL(2,2) + CuH_u_LNP*SQUYucL(2,2) + CuH_0_LNP*YucL(2,2)).real();
    CuH_33i_LNP = (CuH_d_LNP*SQDYucL(2,2) + CuH_u_LNP*SQUYucL(2,2) + CuH_0_LNP*YucL(2,2)).imag();
 
    CuG_11r_LNP = (CuG_d_LNP*SQDYucL(0,0) + CuG_u_LNP*SQUYucL(0,0) + CuG_0_LNP*YucL(0,0)).real();
    CuG_11i_LNP = (CuG_d_LNP*SQDYucL(0,0) + CuG_u_LNP*SQUYucL(0,0) + CuG_0_LNP*YucL(0,0)).imag();
    CuG_12r_LNP = (CuG_d_LNP*SQDYucL(0,1) + CuG_u_LNP*SQUYucL(0,1) + CuG_0_LNP*YucL(0,1)).real();
    CuG_12i_LNP = (CuG_d_LNP*SQDYucL(0,1) + CuG_u_LNP*SQUYucL(0,1) + CuG_0_LNP*YucL(0,1)).imag();
    CuG_13r_LNP = (CuG_d_LNP*SQDYucL(0,2) + CuG_u_LNP*SQUYucL(0,2) + CuG_0_LNP*YucL(0,2)).real();
    CuG_13i_LNP = (CuG_d_LNP*SQDYucL(0,2) + CuG_u_LNP*SQUYucL(0,2) + CuG_0_LNP*YucL(0,2)).imag();
    CuG_21r_LNP = (CuG_d_LNP*SQDYucL(1,0) + CuG_u_LNP*SQUYucL(1,0) + CuG_0_LNP*YucL(1,0)).real();
    CuG_21i_LNP = (CuG_d_LNP*SQDYucL(1,0) + CuG_u_LNP*SQUYucL(1,0) + CuG_0_LNP*YucL(1,0)).imag();
    CuG_22r_LNP = (CuG_d_LNP*SQDYucL(1,1) + CuG_u_LNP*SQUYucL(1,1) + CuG_0_LNP*YucL(1,1)).real();
    CuG_22i_LNP = (CuG_d_LNP*SQDYucL(1,1) + CuG_u_LNP*SQUYucL(1,1) + CuG_0_LNP*YucL(1,1)).imag();
    CuG_23r_LNP = (CuG_d_LNP*SQDYucL(1,2) + CuG_u_LNP*SQUYucL(1,2) + CuG_0_LNP*YucL(1,2)).real();
    CuG_23i_LNP = (CuG_d_LNP*SQDYucL(1,2) + CuG_u_LNP*SQUYucL(1,2) + CuG_0_LNP*YucL(1,2)).imag();
    CuG_31r_LNP = (CuG_d_LNP*SQDYucL(2,0) + CuG_u_LNP*SQUYucL(2,0) + CuG_0_LNP*YucL(2,0)).real();
    CuG_31i_LNP = (CuG_d_LNP*SQDYucL(2,0) + CuG_u_LNP*SQUYucL(2,0) + CuG_0_LNP*YucL(2,0)).imag();
    CuG_32r_LNP = (CuG_d_LNP*SQDYucL(2,1) + CuG_u_LNP*SQUYucL(2,1) + CuG_0_LNP*YucL(2,1)).real();
    CuG_32i_LNP = (CuG_d_LNP*SQDYucL(2,1) + CuG_u_LNP*SQUYucL(2,1) + CuG_0_LNP*YucL(2,1)).imag();
    CuG_33r_LNP = (CuG_d_LNP*SQDYucL(2,2) + CuG_u_LNP*SQUYucL(2,2) + CuG_0_LNP*YucL(2,2)).real();
    CuG_33i_LNP = (CuG_d_LNP*SQDYucL(2,2) + CuG_u_LNP*SQUYucL(2,2) + CuG_0_LNP*YucL(2,2)).imag();
 
    CuW_11r_LNP = (CuW_d_LNP*SQDYucL(0,0) + CuW_u_LNP*SQUYucL(0,0) + CuW_0_LNP*YucL(0,0)).real();
    CuW_11i_LNP = (CuW_d_LNP*SQDYucL(0,0) + CuW_u_LNP*SQUYucL(0,0) + CuW_0_LNP*YucL(0,0)).imag();
    CuW_12r_LNP = (CuW_d_LNP*SQDYucL(0,1) + CuW_u_LNP*SQUYucL(0,1) + CuW_0_LNP*YucL(0,1)).real();
    CuW_12i_LNP = (CuW_d_LNP*SQDYucL(0,1) + CuW_u_LNP*SQUYucL(0,1) + CuW_0_LNP*YucL(0,1)).imag();
    CuW_13r_LNP = (CuW_d_LNP*SQDYucL(0,2) + CuW_u_LNP*SQUYucL(0,2) + CuW_0_LNP*YucL(0,2)).real();
    CuW_13i_LNP = (CuW_d_LNP*SQDYucL(0,2) + CuW_u_LNP*SQUYucL(0,2) + CuW_0_LNP*YucL(0,2)).imag();
    CuW_21r_LNP = (CuW_d_LNP*SQDYucL(1,0) + CuW_u_LNP*SQUYucL(1,0) + CuW_0_LNP*YucL(1,0)).real();
    CuW_21i_LNP = (CuW_d_LNP*SQDYucL(1,0) + CuW_u_LNP*SQUYucL(1,0) + CuW_0_LNP*YucL(1,0)).imag();
    CuW_22r_LNP = (CuW_d_LNP*SQDYucL(1,1) + CuW_u_LNP*SQUYucL(1,1) + CuW_0_LNP*YucL(1,1)).real();
    CuW_22i_LNP = (CuW_d_LNP*SQDYucL(1,1) + CuW_u_LNP*SQUYucL(1,1) + CuW_0_LNP*YucL(1,1)).imag();
    CuW_23r_LNP = (CuW_d_LNP*SQDYucL(1,2) + CuW_u_LNP*SQUYucL(1,2) + CuW_0_LNP*YucL(1,2)).real();
    CuW_23i_LNP = (CuW_d_LNP*SQDYucL(1,2) + CuW_u_LNP*SQUYucL(1,2) + CuW_0_LNP*YucL(1,2)).imag();
    CuW_31r_LNP = (CuW_d_LNP*SQDYucL(2,0) + CuW_u_LNP*SQUYucL(2,0) + CuW_0_LNP*YucL(2,0)).real();
    CuW_31i_LNP = (CuW_d_LNP*SQDYucL(2,0) + CuW_u_LNP*SQUYucL(2,0) + CuW_0_LNP*YucL(2,0)).imag();
    CuW_32r_LNP = (CuW_d_LNP*SQDYucL(2,1) + CuW_u_LNP*SQUYucL(2,1) + CuW_0_LNP*YucL(2,1)).real();
    CuW_32i_LNP = (CuW_d_LNP*SQDYucL(2,1) + CuW_u_LNP*SQUYucL(2,1) + CuW_0_LNP*YucL(2,1)).imag();
    CuW_33r_LNP = (CuW_d_LNP*SQDYucL(2,2) + CuW_u_LNP*SQUYucL(2,2) + CuW_0_LNP*YucL(2,2)).real();
    CuW_33i_LNP = (CuW_d_LNP*SQDYucL(2,2) + CuW_u_LNP*SQUYucL(2,2) + CuW_0_LNP*YucL(2,2)).imag();
 
    CuB_11r_LNP = (CuB_d_LNP*SQDYucL(0,0) + CuB_u_LNP*SQUYucL(0,0) + CuB_0_LNP*YucL(0,0)).real();
    CuB_11i_LNP = (CuB_d_LNP*SQDYucL(0,0) + CuB_u_LNP*SQUYucL(0,0) + CuB_0_LNP*YucL(0,0)).imag();
    CuB_12r_LNP = (CuB_d_LNP*SQDYucL(0,1) + CuB_u_LNP*SQUYucL(0,1) + CuB_0_LNP*YucL(0,1)).real();
    CuB_12i_LNP = (CuB_d_LNP*SQDYucL(0,1) + CuB_u_LNP*SQUYucL(0,1) + CuB_0_LNP*YucL(0,1)).imag();
    CuB_13r_LNP = (CuB_d_LNP*SQDYucL(0,2) + CuB_u_LNP*SQUYucL(0,2) + CuB_0_LNP*YucL(0,2)).real();
    CuB_13i_LNP = (CuB_d_LNP*SQDYucL(0,2) + CuB_u_LNP*SQUYucL(0,2) + CuB_0_LNP*YucL(0,2)).imag();
    CuB_21r_LNP = (CuB_d_LNP*SQDYucL(1,0) + CuB_u_LNP*SQUYucL(1,0) + CuB_0_LNP*YucL(1,0)).real();
    CuB_21i_LNP = (CuB_d_LNP*SQDYucL(1,0) + CuB_u_LNP*SQUYucL(1,0) + CuB_0_LNP*YucL(1,0)).imag();
    CuB_22r_LNP = (CuB_d_LNP*SQDYucL(1,1) + CuB_u_LNP*SQUYucL(1,1) + CuB_0_LNP*YucL(1,1)).real();
    CuB_22i_LNP = (CuB_d_LNP*SQDYucL(1,1) + CuB_u_LNP*SQUYucL(1,1) + CuB_0_LNP*YucL(1,1)).imag();
    CuB_23r_LNP = (CuB_d_LNP*SQDYucL(1,2) + CuB_u_LNP*SQUYucL(1,2) + CuB_0_LNP*YucL(1,2)).real();
    CuB_23i_LNP = (CuB_d_LNP*SQDYucL(1,2) + CuB_u_LNP*SQUYucL(1,2) + CuB_0_LNP*YucL(1,2)).imag();
    CuB_31r_LNP = (CuB_d_LNP*SQDYucL(2,0) + CuB_u_LNP*SQUYucL(2,0) + CuB_0_LNP*YucL(2,0)).real();
    CuB_31i_LNP = (CuB_d_LNP*SQDYucL(2,0) + CuB_u_LNP*SQUYucL(2,0) + CuB_0_LNP*YucL(2,0)).imag();
    CuB_32r_LNP = (CuB_d_LNP*SQDYucL(2,1) + CuB_u_LNP*SQUYucL(2,1) + CuB_0_LNP*YucL(2,1)).real();
    CuB_32i_LNP = (CuB_d_LNP*SQDYucL(2,1) + CuB_u_LNP*SQUYucL(2,1) + CuB_0_LNP*YucL(2,1)).imag();
    CuB_33r_LNP = (CuB_d_LNP*SQDYucL(2,2) + CuB_u_LNP*SQUYucL(2,2) + CuB_0_LNP*YucL(2,2)).real();
    CuB_33i_LNP = (CuB_d_LNP*SQDYucL(2,2) + CuB_u_LNP*SQUYucL(2,2) + CuB_0_LNP*YucL(2,2)).imag();
 
    CdH_11r_LNP = (CdH_d_LNP*SQDYdcL(0,0) + CdH_u_LNP*SQUYdcL(0,0) + CdH_0_LNP*YdcL(0,0)).real();
    CdH_11i_LNP = (CdH_d_LNP*SQDYdcL(0,0) + CdH_u_LNP*SQUYdcL(0,0) + CdH_0_LNP*YdcL(0,0)).imag();
    CdH_12r_LNP = (CdH_d_LNP*SQDYdcL(0,1) + CdH_u_LNP*SQUYdcL(0,1) + CdH_0_LNP*YdcL(0,1)).real();
    CdH_12i_LNP = (CdH_d_LNP*SQDYdcL(0,1) + CdH_u_LNP*SQUYdcL(0,1) + CdH_0_LNP*YdcL(0,1)).imag();
    CdH_13r_LNP = (CdH_d_LNP*SQDYdcL(0,2) + CdH_u_LNP*SQUYdcL(0,2) + CdH_0_LNP*YdcL(0,2)).real();
    CdH_13i_LNP = (CdH_d_LNP*SQDYdcL(0,2) + CdH_u_LNP*SQUYdcL(0,2) + CdH_0_LNP*YdcL(0,2)).imag();
    CdH_21r_LNP = (CdH_d_LNP*SQDYdcL(1,0) + CdH_u_LNP*SQUYdcL(1,0) + CdH_0_LNP*YdcL(1,0)).real();
    CdH_21i_LNP = (CdH_d_LNP*SQDYdcL(1,0) + CdH_u_LNP*SQUYdcL(1,0) + CdH_0_LNP*YdcL(1,0)).imag();
    CdH_22r_LNP = (CdH_d_LNP*SQDYdcL(1,1) + CdH_u_LNP*SQUYdcL(1,1) + CdH_0_LNP*YdcL(1,1)).real();
    CdH_22i_LNP = (CdH_d_LNP*SQDYdcL(1,1) + CdH_u_LNP*SQUYdcL(1,1) + CdH_0_LNP*YdcL(1,1)).imag();
    CdH_23r_LNP = (CdH_d_LNP*SQDYdcL(1,2) + CdH_u_LNP*SQUYdcL(1,2) + CdH_0_LNP*YdcL(1,2)).real();
    CdH_23i_LNP = (CdH_d_LNP*SQDYdcL(1,2) + CdH_u_LNP*SQUYdcL(1,2) + CdH_0_LNP*YdcL(1,2)).imag();
    CdH_31r_LNP = (CdH_d_LNP*SQDYdcL(2,0) + CdH_u_LNP*SQUYdcL(2,0) + CdH_0_LNP*YdcL(2,0)).real();
    CdH_31i_LNP = (CdH_d_LNP*SQDYdcL(2,0) + CdH_u_LNP*SQUYdcL(2,0) + CdH_0_LNP*YdcL(2,0)).imag();
    CdH_32r_LNP = (CdH_d_LNP*SQDYdcL(2,1) + CdH_u_LNP*SQUYdcL(2,1) + CdH_0_LNP*YdcL(2,1)).real();
    CdH_32i_LNP = (CdH_d_LNP*SQDYdcL(2,1) + CdH_u_LNP*SQUYdcL(2,1) + CdH_0_LNP*YdcL(2,1)).imag();
    CdH_33r_LNP = (CdH_d_LNP*SQDYdcL(2,2) + CdH_u_LNP*SQUYdcL(2,2) + CdH_0_LNP*YdcL(2,2)).real();
    CdH_33i_LNP = (CdH_d_LNP*SQDYdcL(2,2) + CdH_u_LNP*SQUYdcL(2,2) + CdH_0_LNP*YdcL(2,2)).imag();
 
    CdG_11r_LNP = (CdG_d_LNP*SQDYdcL(0,0) + CdG_u_LNP*SQUYdcL(0,0) + CdG_0_LNP*YdcL(0,0)).real();
    CdG_11i_LNP = (CdG_d_LNP*SQDYdcL(0,0) + CdG_u_LNP*SQUYdcL(0,0) + CdG_0_LNP*YdcL(0,0)).imag();
    CdG_12r_LNP = (CdG_d_LNP*SQDYdcL(0,1) + CdG_u_LNP*SQUYdcL(0,1) + CdG_0_LNP*YdcL(0,1)).real();
    CdG_12i_LNP = (CdG_d_LNP*SQDYdcL(0,1) + CdG_u_LNP*SQUYdcL(0,1) + CdG_0_LNP*YdcL(0,1)).imag();
    CdG_13r_LNP = (CdG_d_LNP*SQDYdcL(0,2) + CdG_u_LNP*SQUYdcL(0,2) + CdG_0_LNP*YdcL(0,2)).real();
    CdG_13i_LNP = (CdG_d_LNP*SQDYdcL(0,2) + CdG_u_LNP*SQUYdcL(0,2) + CdG_0_LNP*YdcL(0,2)).imag();
    CdG_21r_LNP = (CdG_d_LNP*SQDYdcL(1,0) + CdG_u_LNP*SQUYdcL(1,0) + CdG_0_LNP*YdcL(1,0)).real();
    CdG_21i_LNP = (CdG_d_LNP*SQDYdcL(1,0) + CdG_u_LNP*SQUYdcL(1,0) + CdG_0_LNP*YdcL(1,0)).imag();
    CdG_22r_LNP = (CdG_d_LNP*SQDYdcL(1,1) + CdG_u_LNP*SQUYdcL(1,1) + CdG_0_LNP*YdcL(1,1)).real();
    CdG_22i_LNP = (CdG_d_LNP*SQDYdcL(1,1) + CdG_u_LNP*SQUYdcL(1,1) + CdG_0_LNP*YdcL(1,1)).imag();
    CdG_23r_LNP = (CdG_d_LNP*SQDYdcL(1,2) + CdG_u_LNP*SQUYdcL(1,2) + CdG_0_LNP*YdcL(1,2)).real();
    CdG_23i_LNP = (CdG_d_LNP*SQDYdcL(1,2) + CdG_u_LNP*SQUYdcL(1,2) + CdG_0_LNP*YdcL(1,2)).imag();
    CdG_31r_LNP = (CdG_d_LNP*SQDYdcL(2,0) + CdG_u_LNP*SQUYdcL(2,0) + CdG_0_LNP*YdcL(2,0)).real();
    CdG_31i_LNP = (CdG_d_LNP*SQDYdcL(2,0) + CdG_u_LNP*SQUYdcL(2,0) + CdG_0_LNP*YdcL(2,0)).imag();
    CdG_32r_LNP = (CdG_d_LNP*SQDYdcL(2,1) + CdG_u_LNP*SQUYdcL(2,1) + CdG_0_LNP*YdcL(2,1)).real();
    CdG_32i_LNP = (CdG_d_LNP*SQDYdcL(2,1) + CdG_u_LNP*SQUYdcL(2,1) + CdG_0_LNP*YdcL(2,1)).imag();
    CdG_33r_LNP = (CdG_d_LNP*SQDYdcL(2,2) + CdG_u_LNP*SQUYdcL(2,2) + CdG_0_LNP*YdcL(2,2)).real();
    CdG_33i_LNP = (CdG_d_LNP*SQDYdcL(2,2) + CdG_u_LNP*SQUYdcL(2,2) + CdG_0_LNP*YdcL(2,2)).imag();
 
    CdW_11r_LNP = (CdW_d_LNP*SQDYdcL(0,0) + CdW_u_LNP*SQUYdcL(0,0) + CdW_0_LNP*YdcL(0,0)).real();
    CdW_11i_LNP = (CdW_d_LNP*SQDYdcL(0,0) + CdW_u_LNP*SQUYdcL(0,0) + CdW_0_LNP*YdcL(0,0)).imag();
    CdW_12r_LNP = (CdW_d_LNP*SQDYdcL(0,1) + CdW_u_LNP*SQUYdcL(0,1) + CdW_0_LNP*YdcL(0,1)).real();
    CdW_12i_LNP = (CdW_d_LNP*SQDYdcL(0,1) + CdW_u_LNP*SQUYdcL(0,1) + CdW_0_LNP*YdcL(0,1)).imag();
    CdW_13r_LNP = (CdW_d_LNP*SQDYdcL(0,2) + CdW_u_LNP*SQUYdcL(0,2) + CdW_0_LNP*YdcL(0,2)).real();
    CdW_13i_LNP = (CdW_d_LNP*SQDYdcL(0,2) + CdW_u_LNP*SQUYdcL(0,2) + CdW_0_LNP*YdcL(0,2)).imag();
    CdW_21r_LNP = (CdW_d_LNP*SQDYdcL(1,0) + CdW_u_LNP*SQUYdcL(1,0) + CdW_0_LNP*YdcL(1,0)).real();
    CdW_21i_LNP = (CdW_d_LNP*SQDYdcL(1,0) + CdW_u_LNP*SQUYdcL(1,0) + CdW_0_LNP*YdcL(1,0)).imag();
    CdW_22r_LNP = (CdW_d_LNP*SQDYdcL(1,1) + CdW_u_LNP*SQUYdcL(1,1) + CdW_0_LNP*YdcL(1,1)).real();
    CdW_22i_LNP = (CdW_d_LNP*SQDYdcL(1,1) + CdW_u_LNP*SQUYdcL(1,1) + CdW_0_LNP*YdcL(1,1)).imag();
    CdW_23r_LNP = (CdW_d_LNP*SQDYdcL(1,2) + CdW_u_LNP*SQUYdcL(1,2) + CdW_0_LNP*YdcL(1,2)).real();
    CdW_23i_LNP = (CdW_d_LNP*SQDYdcL(1,2) + CdW_u_LNP*SQUYdcL(1,2) + CdW_0_LNP*YdcL(1,2)).imag();
    CdW_31r_LNP = (CdW_d_LNP*SQDYdcL(2,0) + CdW_u_LNP*SQUYdcL(2,0) + CdW_0_LNP*YdcL(2,0)).real();
    CdW_31i_LNP = (CdW_d_LNP*SQDYdcL(2,0) + CdW_u_LNP*SQUYdcL(2,0) + CdW_0_LNP*YdcL(2,0)).imag();
    CdW_32r_LNP = (CdW_d_LNP*SQDYdcL(2,1) + CdW_u_LNP*SQUYdcL(2,1) + CdW_0_LNP*YdcL(2,1)).real();
    CdW_32i_LNP = (CdW_d_LNP*SQDYdcL(2,1) + CdW_u_LNP*SQUYdcL(2,1) + CdW_0_LNP*YdcL(2,1)).imag();
    CdW_33r_LNP = (CdW_d_LNP*SQDYdcL(2,2) + CdW_u_LNP*SQUYdcL(2,2) + CdW_0_LNP*YdcL(2,2)).real();
    CdW_33i_LNP = (CdW_d_LNP*SQDYdcL(2,2) + CdW_u_LNP*SQUYdcL(2,2) + CdW_0_LNP*YdcL(2,2)).imag();
 
    CdB_11r_LNP = (CdB_d_LNP*SQDYdcL(0,0) + CdB_u_LNP*SQUYdcL(0,0) + CdB_0_LNP*YdcL(0,0)).real();
    CdB_11i_LNP = (CdB_d_LNP*SQDYdcL(0,0) + CdB_u_LNP*SQUYdcL(0,0) + CdB_0_LNP*YdcL(0,0)).imag();
    CdB_12r_LNP = (CdB_d_LNP*SQDYdcL(0,1) + CdB_u_LNP*SQUYdcL(0,1) + CdB_0_LNP*YdcL(0,1)).real();
    CdB_12i_LNP = (CdB_d_LNP*SQDYdcL(0,1) + CdB_u_LNP*SQUYdcL(0,1) + CdB_0_LNP*YdcL(0,1)).imag();
    CdB_13r_LNP = (CdB_d_LNP*SQDYdcL(0,2) + CdB_u_LNP*SQUYdcL(0,2) + CdB_0_LNP*YdcL(0,2)).real();
    CdB_13i_LNP = (CdB_d_LNP*SQDYdcL(0,2) + CdB_u_LNP*SQUYdcL(0,2) + CdB_0_LNP*YdcL(0,2)).imag();
    CdB_21r_LNP = (CdB_d_LNP*SQDYdcL(1,0) + CdB_u_LNP*SQUYdcL(1,0) + CdB_0_LNP*YdcL(1,0)).real();
    CdB_21i_LNP = (CdB_d_LNP*SQDYdcL(1,0) + CdB_u_LNP*SQUYdcL(1,0) + CdB_0_LNP*YdcL(1,0)).imag();
    CdB_22r_LNP = (CdB_d_LNP*SQDYdcL(1,1) + CdB_u_LNP*SQUYdcL(1,1) + CdB_0_LNP*YdcL(1,1)).real();
    CdB_22i_LNP = (CdB_d_LNP*SQDYdcL(1,1) + CdB_u_LNP*SQUYdcL(1,1) + CdB_0_LNP*YdcL(1,1)).imag();
    CdB_23r_LNP = (CdB_d_LNP*SQDYdcL(1,2) + CdB_u_LNP*SQUYdcL(1,2) + CdB_0_LNP*YdcL(1,2)).real();
    CdB_23i_LNP = (CdB_d_LNP*SQDYdcL(1,2) + CdB_u_LNP*SQUYdcL(1,2) + CdB_0_LNP*YdcL(1,2)).imag();
    CdB_31r_LNP = (CdB_d_LNP*SQDYdcL(2,0) + CdB_u_LNP*SQUYdcL(2,0) + CdB_0_LNP*YdcL(2,0)).real();
    CdB_31i_LNP = (CdB_d_LNP*SQDYdcL(2,0) + CdB_u_LNP*SQUYdcL(2,0) + CdB_0_LNP*YdcL(2,0)).imag();
    CdB_32r_LNP = (CdB_d_LNP*SQDYdcL(2,1) + CdB_u_LNP*SQUYdcL(2,1) + CdB_0_LNP*YdcL(2,1)).real();
    CdB_32i_LNP = (CdB_d_LNP*SQDYdcL(2,1) + CdB_u_LNP*SQUYdcL(2,1) + CdB_0_LNP*YdcL(2,1)).imag();
    CdB_33r_LNP = (CdB_d_LNP*SQDYdcL(2,2) + CdB_u_LNP*SQUYdcL(2,2) + CdB_0_LNP*YdcL(2,2)).real();
    CdB_33i_LNP = (CdB_d_LNP*SQDYdcL(2,2) + CdB_u_LNP*SQUYdcL(2,2) + CdB_0_LNP*YdcL(2,2)).imag();
 
    CHq1_11r_LNP = (CHq1_0_LNP + CHq1_d_LNP*SQDL(0,0) + CHq1_u_LNP*SQUL(0,0)).real();
    CHq1_12r_LNP = (CHq1_d_LNP*SQDL(0,1) + CHq1_u_LNP*SQUL(0,1)).real();
    CHq1_12i_LNP = (CHq1_d_LNP*SQDL(0,1) + CHq1_u_LNP*SQUL(0,1)).imag();
    CHq1_13r_LNP = (CHq1_d_LNP*SQDL(0,2) + CHq1_u_LNP*SQUL(0,2)).real();
    CHq1_13i_LNP = (CHq1_d_LNP*SQDL(0,2) + CHq1_u_LNP*SQUL(0,2)).imag();
    CHq1_22r_LNP = (CHq1_0_LNP + CHq1_d_LNP*SQDL(1,1) + CHq1_u_LNP*SQUL(1,1)).real();
    CHq1_23r_LNP = (CHq1_d_LNP*SQDL(1,2) + CHq1_u_LNP*SQUL(1,2)).real();
    CHq1_23i_LNP = (CHq1_d_LNP*SQDL(1,2) + CHq1_u_LNP*SQUL(1,2)).imag();
    CHq1_33r_LNP = (CHq1_0_LNP + CHq1_d_LNP*SQDL(2,2) + CHq1_u_LNP*SQUL(2,2)).real();
 
    CHq3_11r_LNP = (CHq3_0_LNP + CHq3_d_LNP*SQDL(0,0) + CHq3_u_LNP*SQUL(0,0)).real();
    CHq3_12r_LNP = (CHq3_d_LNP*SQDL(0,1) + CHq3_u_LNP*SQUL(0,1)).real();
    CHq3_12i_LNP = (CHq3_d_LNP*SQDL(0,1) + CHq3_u_LNP*SQUL(0,1)).imag();
    CHq3_13r_LNP = (CHq3_d_LNP*SQDL(0,2) + CHq3_u_LNP*SQUL(0,2)).real();
    CHq3_13i_LNP = (CHq3_d_LNP*SQDL(0,2) + CHq3_u_LNP*SQUL(0,2)).imag();
    CHq3_22r_LNP = (CHq3_0_LNP + CHq3_d_LNP*SQDL(1,1) + CHq3_u_LNP*SQUL(1,1)).real();
    CHq3_23r_LNP = (CHq3_d_LNP*SQDL(1,2) + CHq3_u_LNP*SQUL(1,2)).real();
    CHq3_23i_LNP = (CHq3_d_LNP*SQDL(1,2) + CHq3_u_LNP*SQUL(1,2)).imag();
    CHq3_33r_LNP = (CHq3_0_LNP + CHq3_d_LNP*SQDL(2,2) + CHq3_u_LNP*SQUL(2,2)).real();
 
    CHu_11r_LNP = (CHu_0_LNP + CHu_u_LNP*SUL(0,0)).real();
    CHu_12r_LNP = (CHu_u_LNP*SUL(0,1)).real();
    CHu_12i_LNP = (CHu_u_LNP*SUL(0,1)).imag();
    CHu_13r_LNP = (CHu_u_LNP*SUL(0,2)).real();
    CHu_13i_LNP = (CHu_u_LNP*SUL(0,2)).imag();
    CHu_22r_LNP = (CHu_0_LNP + CHu_u_LNP*SUL(1,1)).real();
    CHu_23r_LNP = (CHu_u_LNP*SUL(1,2)).real();
    CHu_23i_LNP = (CHu_u_LNP*SUL(1,2)).imag();
    CHu_33r_LNP = (CHu_0_LNP + CHu_u_LNP*SUL(2,2)).real();
 
    CHd_11r_LNP = (CHd_0_LNP + CHd_d_LNP*SDL(0,0)).real();
    CHd_12r_LNP = (CHd_d_LNP*SDL(0,1)).real();
    CHd_12i_LNP = (CHd_d_LNP*SDL(0,1)).imag();
    CHd_13r_LNP = (CHd_d_LNP*SDL(0,2)).real();
    CHd_13i_LNP = (CHd_d_LNP*SDL(0,2)).imag();
    CHd_22r_LNP = (CHd_0_LNP + CHd_d_LNP*SDL(1,1)).real();
    CHd_23r_LNP = (CHd_d_LNP*SDL(1,2)).real();
    CHd_23i_LNP = (CHd_d_LNP*SDL(1,2)).imag();
    CHd_33r_LNP = (CHd_0_LNP + CHd_d_LNP*SDL(2,2)).real();
 
    CHud_11r_LNP = (CHud_ud_LNP*SUDL(0,0)).real();
    CHud_11i_LNP = (CHud_ud_LNP*SUDL(0,0)).imag();
    CHud_12r_LNP = (CHud_ud_LNP*SUDL(0,1)).real();
    CHud_12i_LNP = (CHud_ud_LNP*SUDL(0,1)).imag();
    CHud_13r_LNP = (CHud_ud_LNP*SUDL(0,2)).real();
    CHud_13i_LNP = (CHud_ud_LNP*SUDL(0,2)).imag();
    CHud_21r_LNP = (CHud_ud_LNP*SUDL(1,0)).real();
    CHud_21i_LNP = (CHud_ud_LNP*SUDL(1,0)).imag();
    CHud_22r_LNP = (CHud_ud_LNP*SUDL(1,1)).real();
    CHud_22i_LNP = (CHud_ud_LNP*SUDL(1,1)).imag();
    CHud_23r_LNP = (CHud_ud_LNP*SUDL(1,2)).real();
    CHud_23i_LNP = (CHud_ud_LNP*SUDL(1,2)).imag();
    CHud_31r_LNP = (CHud_ud_LNP*SUDL(2,0)).real();
    CHud_31i_LNP = (CHud_ud_LNP*SUDL(2,0)).imag();
    CHud_32r_LNP = (CHud_ud_LNP*SUDL(2,1)).real();
    CHud_32i_LNP = (CHud_ud_LNP*SUDL(2,1)).imag();
    CHud_33r_LNP = (CHud_ud_LNP*SUDL(2,2)).real();
    CHud_33i_LNP = (CHud_ud_LNP*SUDL(2,2)).imag();
 
    Clq1_1111r_LNP = (Clq1_0_LNP + Clq1_d_LNP*SQDL(0,0) + Clq1_u_LNP*SQUL(0,0)).real();
    Clq1_1112r_LNP = (Clq1_d_LNP*SQDL(0,1) + Clq1_u_LNP*SQUL(0,1)).real();
    Clq1_1112i_LNP = (Clq1_d_LNP*SQDL(0,1) + Clq1_u_LNP*SQUL(0,1)).imag();
    Clq1_1113r_LNP = (Clq1_d_LNP*SQDL(0,2) + Clq1_u_LNP*SQUL(0,2)).real();
    Clq1_1113i_LNP = (Clq1_d_LNP*SQDL(0,2) + Clq1_u_LNP*SQUL(0,2)).imag();
    Clq1_1122r_LNP = (Clq1_0_LNP + Clq1_d_LNP*SQDL(1,1) + Clq1_u_LNP*SQUL(1,1)).real();
    Clq1_1123r_LNP = (Clq1_d_LNP*SQDL(1,2) + Clq1_u_LNP*SQUL(1,2)).real();
    Clq1_1123i_LNP = (Clq1_d_LNP*SQDL(1,2) + Clq1_u_LNP*SQUL(1,2)).imag();
    Clq1_1133r_LNP = (Clq1_0_LNP + Clq1_d_LNP*SQDL(2,2) + Clq1_u_LNP*SQUL(2,2)).real();
    Clq1_2211r_LNP = (Clq1_0_LNP + Clq1_d_LNP*SQDL(0,0) + Clq1_u_LNP*SQUL(0,0)).real();
    Clq1_2212r_LNP = (Clq1_d_LNP*SQDL(0,1) + Clq1_u_LNP*SQUL(0,1)).real();
    Clq1_2212i_LNP = (Clq1_d_LNP*SQDL(0,1) + Clq1_u_LNP*SQUL(0,1)).imag();
    Clq1_2213r_LNP = (Clq1_d_LNP*SQDL(0,2) + Clq1_u_LNP*SQUL(0,2)).real();
    Clq1_2213i_LNP = (Clq1_d_LNP*SQDL(0,2) + Clq1_u_LNP*SQUL(0,2)).imag();
    Clq1_2222r_LNP = (Clq1_0_LNP + Clq1_d_LNP*SQDL(1,1) + Clq1_u_LNP*SQUL(1,1)).real();
    Clq1_2223r_LNP = (Clq1_d_LNP*SQDL(1,2) + Clq1_u_LNP*SQUL(1,2)).real();
    Clq1_2223i_LNP = (Clq1_d_LNP*SQDL(1,2) + Clq1_u_LNP*SQUL(1,2)).imag();
    Clq1_2233r_LNP = (Clq1_0_LNP + Clq1_d_LNP*SQDL(2,2) + Clq1_u_LNP*SQUL(2,2)).real();
    Clq1_3311r_LNP = (Clq1_0_LNP + Clq1_d_LNP*SQDL(0,0) + Clq1_u_LNP*SQUL(0,0)).real();
    Clq1_3312r_LNP = (Clq1_d_LNP*SQDL(0,1) + Clq1_u_LNP*SQUL(0,1)).real();
    Clq1_3312i_LNP = (Clq1_d_LNP*SQDL(0,1) + Clq1_u_LNP*SQUL(0,1)).imag();
    Clq1_3313r_LNP = (Clq1_d_LNP*SQDL(0,2) + Clq1_u_LNP*SQUL(0,2)).real();
    Clq1_3313i_LNP = (Clq1_d_LNP*SQDL(0,2) + Clq1_u_LNP*SQUL(0,2)).imag();
    Clq1_3322r_LNP = (Clq1_0_LNP + Clq1_d_LNP*SQDL(1,1) + Clq1_u_LNP*SQUL(1,1)).real();
    Clq1_3323r_LNP = (Clq1_d_LNP*SQDL(1,2) + Clq1_u_LNP*SQUL(1,2)).real();
    Clq1_3323i_LNP = (Clq1_d_LNP*SQDL(1,2) + Clq1_u_LNP*SQUL(1,2)).imag();
    Clq1_3333r_LNP = (Clq1_0_LNP + Clq1_d_LNP*SQDL(2,2) + Clq1_u_LNP*SQUL(2,2)).real();
 
    Clq3_1111r_LNP = (Clq3_0_LNP + Clq3_d_LNP*SQDL(0,0) + Clq3_u_LNP*SQUL(0,0)).real();
    Clq3_1112r_LNP = (Clq3_d_LNP*SQDL(0,1) + Clq3_u_LNP*SQUL(0,1)).real();
    Clq3_1112i_LNP = (Clq3_d_LNP*SQDL(0,1) + Clq3_u_LNP*SQUL(0,1)).imag();
    Clq3_1113r_LNP = (Clq3_d_LNP*SQDL(0,2) + Clq3_u_LNP*SQUL(0,2)).real();
    Clq3_1113i_LNP = (Clq3_d_LNP*SQDL(0,2) + Clq3_u_LNP*SQUL(0,2)).imag();
    Clq3_1122r_LNP = (Clq3_0_LNP + Clq3_d_LNP*SQDL(1,1) + Clq3_u_LNP*SQUL(1,1)).real();
    Clq3_1123r_LNP = (Clq3_d_LNP*SQDL(1,2) + Clq3_u_LNP*SQUL(1,2)).real();
    Clq3_1123i_LNP = (Clq3_d_LNP*SQDL(1,2) + Clq3_u_LNP*SQUL(1,2)).imag();
    Clq3_1133r_LNP = (Clq3_0_LNP + Clq3_d_LNP*SQDL(2,2) + Clq3_u_LNP*SQUL(2,2)).real();
    Clq3_2211r_LNP = (Clq3_0_LNP + Clq3_d_LNP*SQDL(0,0) + Clq3_u_LNP*SQUL(0,0)).real();
    Clq3_2212r_LNP = (Clq3_d_LNP*SQDL(0,1) + Clq3_u_LNP*SQUL(0,1)).real();
    Clq3_2212i_LNP = (Clq3_d_LNP*SQDL(0,1) + Clq3_u_LNP*SQUL(0,1)).imag();
    Clq3_2213r_LNP = (Clq3_d_LNP*SQDL(0,2) + Clq3_u_LNP*SQUL(0,2)).real();
    Clq3_2213i_LNP = (Clq3_d_LNP*SQDL(0,2) + Clq3_u_LNP*SQUL(0,2)).imag();
    Clq3_2222r_LNP = (Clq3_0_LNP + Clq3_d_LNP*SQDL(1,1) + Clq3_u_LNP*SQUL(1,1)).real();
    Clq3_2223r_LNP = (Clq3_d_LNP*SQDL(1,2) + Clq3_u_LNP*SQUL(1,2)).real();
    Clq3_2223i_LNP = (Clq3_d_LNP*SQDL(1,2) + Clq3_u_LNP*SQUL(1,2)).imag();
    Clq3_2233r_LNP = (Clq3_0_LNP + Clq3_d_LNP*SQDL(2,2) + Clq3_u_LNP*SQUL(2,2)).real();
    Clq3_3311r_LNP = (Clq3_0_LNP + Clq3_d_LNP*SQDL(0,0) + Clq3_u_LNP*SQUL(0,0)).real();
    Clq3_3312r_LNP = (Clq3_d_LNP*SQDL(0,1) + Clq3_u_LNP*SQUL(0,1)).real();
    Clq3_3312i_LNP = (Clq3_d_LNP*SQDL(0,1) + Clq3_u_LNP*SQUL(0,1)).imag();
    Clq3_3313r_LNP = (Clq3_d_LNP*SQDL(0,2) + Clq3_u_LNP*SQUL(0,2)).real();
    Clq3_3313i_LNP = (Clq3_d_LNP*SQDL(0,2) + Clq3_u_LNP*SQUL(0,2)).imag();
    Clq3_3322r_LNP = (Clq3_0_LNP + Clq3_d_LNP*SQDL(1,1) + Clq3_u_LNP*SQUL(1,1)).real();
    Clq3_3323r_LNP = (Clq3_d_LNP*SQDL(1,2) + Clq3_u_LNP*SQUL(1,2)).real();
    Clq3_3323i_LNP = (Clq3_d_LNP*SQDL(1,2) + Clq3_u_LNP*SQUL(1,2)).imag();
    Clq3_3333r_LNP = (Clq3_0_LNP + Clq3_d_LNP*SQDL(2,2) + Clq3_u_LNP*SQUL(2,2)).real();
 
    Cqe_1111r_LNP = (Cqe_0_LNP + Cqe_d_LNP*SQDL(0,0) + Cqe_u_LNP*SQUL(0,0)).real();
    Cqe_1122r_LNP = (Cqe_0_LNP + Cqe_d_LNP*SQDL(0,0) + Cqe_u_LNP*SQUL(0,0)).real();
    Cqe_1133r_LNP = (Cqe_0_LNP + Cqe_d_LNP*SQDL(0,0) + Cqe_u_LNP*SQUL(0,0)).real();
    Cqe_1211r_LNP = (Cqe_d_LNP*SQDL(0,1) + Cqe_u_LNP*SQUL(0,1)).real();
    Cqe_1211i_LNP = (Cqe_d_LNP*SQDL(0,1) + Cqe_u_LNP*SQUL(0,1)).imag();
    Cqe_1222r_LNP = (Cqe_d_LNP*SQDL(0,1) + Cqe_u_LNP*SQUL(0,1)).real();
    Cqe_1222i_LNP = (Cqe_d_LNP*SQDL(0,1) + Cqe_u_LNP*SQUL(0,1)).imag();
    Cqe_1233r_LNP = (Cqe_d_LNP*SQDL(0,1) + Cqe_u_LNP*SQUL(0,1)).real();
    Cqe_1233i_LNP = (Cqe_d_LNP*SQDL(0,1) + Cqe_u_LNP*SQUL(0,1)).imag();
    Cqe_1311r_LNP = (Cqe_d_LNP*SQDL(0,2) + Cqe_u_LNP*SQUL(0,2)).real();
    Cqe_1311i_LNP = (Cqe_d_LNP*SQDL(0,2) + Cqe_u_LNP*SQUL(0,2)).imag();
    Cqe_1322r_LNP = (Cqe_d_LNP*SQDL(0,2) + Cqe_u_LNP*SQUL(0,2)).real();
    Cqe_1322i_LNP = (Cqe_d_LNP*SQDL(0,2) + Cqe_u_LNP*SQUL(0,2)).imag();
    Cqe_1333r_LNP = (Cqe_d_LNP*SQDL(0,2) + Cqe_u_LNP*SQUL(0,2)).real();
    Cqe_1333i_LNP = (Cqe_d_LNP*SQDL(0,2) + Cqe_u_LNP*SQUL(0,2)).imag();
    Cqe_2211r_LNP = (Cqe_0_LNP + Cqe_d_LNP*SQDL(1,1) + Cqe_u_LNP*SQUL(1,1)).real();
    Cqe_2222r_LNP = (Cqe_0_LNP + Cqe_d_LNP*SQDL(1,1) + Cqe_u_LNP*SQUL(1,1)).real();
    Cqe_2233r_LNP = (Cqe_0_LNP + Cqe_d_LNP*SQDL(1,1) + Cqe_u_LNP*SQUL(1,1)).real();
    Cqe_2311r_LNP = (Cqe_d_LNP*SQDL(1,2) + Cqe_u_LNP*SQUL(1,2)).real();
    Cqe_2311i_LNP = (Cqe_d_LNP*SQDL(1,2) + Cqe_u_LNP*SQUL(1,2)).imag();
    Cqe_2322r_LNP = (Cqe_d_LNP*SQDL(1,2) + Cqe_u_LNP*SQUL(1,2)).real();
    Cqe_2322i_LNP = (Cqe_d_LNP*SQDL(1,2) + Cqe_u_LNP*SQUL(1,2)).imag();
    Cqe_2333r_LNP = (Cqe_d_LNP*SQDL(1,2) + Cqe_u_LNP*SQUL(1,2)).real();
    Cqe_2333i_LNP = (Cqe_d_LNP*SQDL(1,2) + Cqe_u_LNP*SQUL(1,2)).imag();
    Cqe_3311r_LNP = (Cqe_0_LNP + Cqe_d_LNP*SQDL(2,2) + Cqe_u_LNP*SQUL(2,2)).real();
    Cqe_3322r_LNP = (Cqe_0_LNP + Cqe_d_LNP*SQDL(2,2) + Cqe_u_LNP*SQUL(2,2)).real();
    Cqe_3333r_LNP = (Cqe_0_LNP + Cqe_d_LNP*SQDL(2,2) + Cqe_u_LNP*SQUL(2,2)).real();
 
    Clu_1111r_LNP = (Clu_0_LNP + Clu_u_LNP*SUL(0,0)).real();
    Clu_1112r_LNP = (Clu_u_LNP*SUL(0,1)).real();
    Clu_1112i_LNP = (Clu_u_LNP*SUL(0,1)).imag();
    Clu_1113r_LNP = (Clu_u_LNP*SUL(0,2)).real();
    Clu_1113i_LNP = (Clu_u_LNP*SUL(0,2)).imag();
    Clu_1122r_LNP = (Clu_0_LNP + Clu_u_LNP*SUL(1,1)).real();
    Clu_1123r_LNP = (Clu_u_LNP*SUL(1,2)).real();
    Clu_1123i_LNP = (Clu_u_LNP*SUL(1,2)).imag();
    Clu_1133r_LNP = (Clu_0_LNP + Clu_u_LNP*SUL(2,2)).real();
    Clu_2211r_LNP = (Clu_0_LNP + Clu_u_LNP*SUL(0,0)).real();
    Clu_2212r_LNP = (Clu_u_LNP*SUL(0,1)).real();
    Clu_2212i_LNP = (Clu_u_LNP*SUL(0,1)).imag();
    Clu_2213r_LNP = (Clu_u_LNP*SUL(0,2)).real();
    Clu_2213i_LNP = (Clu_u_LNP*SUL(0,2)).imag();
    Clu_2222r_LNP = (Clu_0_LNP + Clu_u_LNP*SUL(1,1)).real();
    Clu_2223r_LNP = (Clu_u_LNP*SUL(1,2)).real();
    Clu_2223i_LNP = (Clu_u_LNP*SUL(1,2)).imag();
    Clu_2233r_LNP = (Clu_0_LNP + Clu_u_LNP*SUL(2,2)).real();
    Clu_3311r_LNP = (Clu_0_LNP + Clu_u_LNP*SUL(0,0)).real();
    Clu_3312r_LNP = (Clu_u_LNP*SUL(0,1)).real();
    Clu_3312i_LNP = (Clu_u_LNP*SUL(0,1)).imag();
    Clu_3313r_LNP = (Clu_u_LNP*SUL(0,2)).real();
    Clu_3313i_LNP = (Clu_u_LNP*SUL(0,2)).imag();
    Clu_3322r_LNP = (Clu_0_LNP + Clu_u_LNP*SUL(1,1)).real();
    Clu_3323r_LNP = (Clu_u_LNP*SUL(1,2)).real();
    Clu_3323i_LNP = (Clu_u_LNP*SUL(1,2)).imag();
    Clu_3333r_LNP = (Clu_0_LNP + Clu_u_LNP*SUL(2,2)).real();
 
    Ceu_1111r_LNP = (Ceu_0_LNP + Ceu_u_LNP*SUL(0,0)).real();
    Ceu_1112r_LNP = (Ceu_u_LNP*SUL(0,1)).real();
    Ceu_1112i_LNP = (Ceu_u_LNP*SUL(0,1)).imag();
    Ceu_1113r_LNP = (Ceu_u_LNP*SUL(0,2)).real();
    Ceu_1113i_LNP = (Ceu_u_LNP*SUL(0,2)).imag();
    Ceu_1122r_LNP = (Ceu_0_LNP + Ceu_u_LNP*SUL(1,1)).real();
    Ceu_1123r_LNP = (Ceu_u_LNP*SUL(1,2)).real();
    Ceu_1123i_LNP = (Ceu_u_LNP*SUL(1,2)).imag();
    Ceu_1133r_LNP = (Ceu_0_LNP + Ceu_u_LNP*SUL(2,2)).real();
    Ceu_2211r_LNP = (Ceu_0_LNP + Ceu_u_LNP*SUL(0,0)).real();
    Ceu_2212r_LNP = (Ceu_u_LNP*SUL(0,1)).real();
    Ceu_2212i_LNP = (Ceu_u_LNP*SUL(0,1)).imag();
    Ceu_2213r_LNP = (Ceu_u_LNP*SUL(0,2)).real();
    Ceu_2213i_LNP = (Ceu_u_LNP*SUL(0,2)).imag();
    Ceu_2222r_LNP = (Ceu_0_LNP + Ceu_u_LNP*SUL(1,1)).real();
    Ceu_2223r_LNP = (Ceu_u_LNP*SUL(1,2)).real();
    Ceu_2223i_LNP = (Ceu_u_LNP*SUL(1,2)).imag();
    Ceu_2233r_LNP = (Ceu_0_LNP + Ceu_u_LNP*SUL(2,2)).real();
    Ceu_3311r_LNP = (Ceu_0_LNP + Ceu_u_LNP*SUL(0,0)).real();
    Ceu_3312r_LNP = (Ceu_u_LNP*SUL(0,1)).real();
    Ceu_3312i_LNP = (Ceu_u_LNP*SUL(0,1)).imag();
    Ceu_3313r_LNP = (Ceu_u_LNP*SUL(0,2)).real();
    Ceu_3313i_LNP = (Ceu_u_LNP*SUL(0,2)).imag();
    Ceu_3322r_LNP = (Ceu_0_LNP + Ceu_u_LNP*SUL(1,1)).real();
    Ceu_3323r_LNP = (Ceu_u_LNP*SUL(1,2)).real();
    Ceu_3323i_LNP = (Ceu_u_LNP*SUL(1,2)).imag();
    Ceu_3333r_LNP = (Ceu_0_LNP + Ceu_u_LNP*SUL(2,2)).real();
 
    Cld_1111r_LNP = (Cld_0_LNP + Cld_d_LNP*SDL(0,0)).real();
    Cld_1112r_LNP = (Cld_d_LNP*SDL(0,1)).real();
    Cld_1112i_LNP = (Cld_d_LNP*SDL(0,1)).imag();
    Cld_1113r_LNP = (Cld_d_LNP*SDL(0,2)).real();
    Cld_1113i_LNP = (Cld_d_LNP*SDL(0,2)).imag();
    Cld_1122r_LNP = (Cld_0_LNP + Cld_d_LNP*SDL(1,1)).real();
    Cld_1123r_LNP = (Cld_d_LNP*SDL(1,2)).real();
    Cld_1123i_LNP = (Cld_d_LNP*SDL(1,2)).imag();
    Cld_1133r_LNP = (Cld_0_LNP + Cld_d_LNP*SDL(2,2)).real();
    Cld_2211r_LNP = (Cld_0_LNP + Cld_d_LNP*SDL(0,0)).real();
    Cld_2212r_LNP = (Cld_d_LNP*SDL(0,1)).real();
    Cld_2212i_LNP = (Cld_d_LNP*SDL(0,1)).imag();
    Cld_2213r_LNP = (Cld_d_LNP*SDL(0,2)).real();
    Cld_2213i_LNP = (Cld_d_LNP*SDL(0,2)).imag();
    Cld_2222r_LNP = (Cld_0_LNP + Cld_d_LNP*SDL(1,1)).real();
    Cld_2223r_LNP = (Cld_d_LNP*SDL(1,2)).real();
    Cld_2223i_LNP = (Cld_d_LNP*SDL(1,2)).imag();
    Cld_2233r_LNP = (Cld_0_LNP + Cld_d_LNP*SDL(2,2)).real();
    Cld_3311r_LNP = (Cld_0_LNP + Cld_d_LNP*SDL(0,0)).real();
    Cld_3312r_LNP = (Cld_d_LNP*SDL(0,1)).real();
    Cld_3312i_LNP = (Cld_d_LNP*SDL(0,1)).imag();
    Cld_3313r_LNP = (Cld_d_LNP*SDL(0,2)).real();
    Cld_3313i_LNP = (Cld_d_LNP*SDL(0,2)).imag();
    Cld_3322r_LNP = (Cld_0_LNP + Cld_d_LNP*SDL(1,1)).real();
    Cld_3323r_LNP = (Cld_d_LNP*SDL(1,2)).real();
    Cld_3323i_LNP = (Cld_d_LNP*SDL(1,2)).imag();
    Cld_3333r_LNP = (Cld_0_LNP + Cld_d_LNP*SDL(2,2)).real();
 
    Ced_1111r_LNP = (Ced_0_LNP + Ced_d_LNP*SDL(0,0)).real();
    Ced_1112r_LNP = (Ced_d_LNP*SDL(0,1)).real();
    Ced_1112i_LNP = (Ced_d_LNP*SDL(0,1)).imag();
    Ced_1113r_LNP = (Ced_d_LNP*SDL(0,2)).real();
    Ced_1113i_LNP = (Ced_d_LNP*SDL(0,2)).imag();
    Ced_1122r_LNP = (Ced_0_LNP + Ced_d_LNP*SDL(1,1)).real();
    Ced_1123r_LNP = (Ced_d_LNP*SDL(1,2)).real();
    Ced_1123i_LNP = (Ced_d_LNP*SDL(1,2)).imag();
    Ced_1133r_LNP = (Ced_0_LNP + Ced_d_LNP*SDL(2,2)).real();
    Ced_2211r_LNP = (Ced_0_LNP + Ced_d_LNP*SDL(0,0)).real();
    Ced_2212r_LNP = (Ced_d_LNP*SDL(0,1)).real();
    Ced_2212i_LNP = (Ced_d_LNP*SDL(0,1)).imag();
    Ced_2213r_LNP = (Ced_d_LNP*SDL(0,2)).real();
    Ced_2213i_LNP = (Ced_d_LNP*SDL(0,2)).imag();
    Ced_2222r_LNP = (Ced_0_LNP + Ced_d_LNP*SDL(1,1)).real();
    Ced_2223r_LNP = (Ced_d_LNP*SDL(1,2)).real();
    Ced_2223i_LNP = (Ced_d_LNP*SDL(1,2)).imag();
    Ced_2233r_LNP = (Ced_0_LNP + Ced_d_LNP*SDL(2,2)).real();
    Ced_3311r_LNP = (Ced_0_LNP + Ced_d_LNP*SDL(0,0)).real();
    Ced_3312r_LNP = (Ced_d_LNP*SDL(0,1)).real();
    Ced_3312i_LNP = (Ced_d_LNP*SDL(0,1)).imag();
    Ced_3313r_LNP = (Ced_d_LNP*SDL(0,2)).real();
    Ced_3313i_LNP = (Ced_d_LNP*SDL(0,2)).imag();
    Ced_3322r_LNP = (Ced_0_LNP + Ced_d_LNP*SDL(1,1)).real();
    Ced_3323r_LNP = (Ced_d_LNP*SDL(1,2)).real();
    Ced_3323i_LNP = (Ced_d_LNP*SDL(1,2)).imag();
    Ced_3333r_LNP = (Ced_0_LNP + Ced_d_LNP*SDL(2,2)).real();
 
    Cqq1_1111r_LNP = (Cqq1_00_LNP + 2*Cqq1_d0_LNP*SQDL(0,0) + Cqq1_dd_LNP*SQDL(0,0)*SQDL(0,0) + 2*Cqq1_u0_LNP*SQUL(0,0) + 2*Cqq1_ud_LNP*SQDL(0,0)*SQUL(0,0) + Cqq1_uu_LNP*SQUL(0,0)*SQUL(0,0) + Cqq1p_00_LNP + 2*Cqq1p_d0_LNP*SQDL(0,0) + Cqq1p_dd_LNP*SQDL(0,0)*SQDL(0,0) + 2*Cqq1p_u0_LNP*SQUL(0,0) + 2*Cqq1p_ud_LNP*SQDL(0,0)*SQUL(0,0) + Cqq1p_uu_LNP*SQUL(0,0)*SQUL(0,0)).real();
    Cqq1_1112r_LNP = (Cqq1_d0_LNP*SQDL(0,1) + Cqq1_dd_LNP*SQDL(0,0)*SQDL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(0,0) + Cqq1_u0_LNP*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,0)*SQUL(0,1) + Cqq1_uu_LNP*SQUL(0,0)*SQUL(0,1) + Cqq1p_d0_LNP*SQDL(0,1) + Cqq1p_dd_LNP*SQDL(0,0)*SQDL(0,1) + Cqq1p_ud_LNP*SQDL(0,1)*SQUL(0,0) + Cqq1p_u0_LNP*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(0,0)*SQUL(0,1) + Cqq1p_uu_LNP*SQUL(0,0)*SQUL(0,1)).real();
    Cqq1_1112i_LNP = (Cqq1_d0_LNP*SQDL(0,1) + Cqq1_dd_LNP*SQDL(0,0)*SQDL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(0,0) + Cqq1_u0_LNP*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,0)*SQUL(0,1) + Cqq1_uu_LNP*SQUL(0,0)*SQUL(0,1) + Cqq1p_d0_LNP*SQDL(0,1) + Cqq1p_dd_LNP*SQDL(0,0)*SQDL(0,1) + Cqq1p_ud_LNP*SQDL(0,1)*SQUL(0,0) + Cqq1p_u0_LNP*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(0,0)*SQUL(0,1) + Cqq1p_uu_LNP*SQUL(0,0)*SQUL(0,1)).imag();
    Cqq1_1113r_LNP = (Cqq1_d0_LNP*SQDL(0,2) + Cqq1_dd_LNP*SQDL(0,0)*SQDL(0,2) + Cqq1_ud_LNP*SQDL(0,2)*SQUL(0,0) + Cqq1_u0_LNP*SQUL(0,2) + Cqq1_ud_LNP*SQDL(0,0)*SQUL(0,2) + Cqq1_uu_LNP*SQUL(0,0)*SQUL(0,2) + Cqq1p_d0_LNP*SQDL(0,2) + Cqq1p_dd_LNP*SQDL(0,0)*SQDL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(0,0) + Cqq1p_u0_LNP*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(0,0)*SQUL(0,2) + Cqq1p_uu_LNP*SQUL(0,0)*SQUL(0,2)).real();
    Cqq1_1113i_LNP = (Cqq1_d0_LNP*SQDL(0,2) + Cqq1_dd_LNP*SQDL(0,0)*SQDL(0,2) + Cqq1_ud_LNP*SQDL(0,2)*SQUL(0,0) + Cqq1_u0_LNP*SQUL(0,2) + Cqq1_ud_LNP*SQDL(0,0)*SQUL(0,2) + Cqq1_uu_LNP*SQUL(0,0)*SQUL(0,2) + Cqq1p_d0_LNP*SQDL(0,2) + Cqq1p_dd_LNP*SQDL(0,0)*SQDL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(0,0) + Cqq1p_u0_LNP*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(0,0)*SQUL(0,2) + Cqq1p_uu_LNP*SQUL(0,0)*SQUL(0,2)).imag();
    Cqq1_1122r_LNP = (Cqq1_00_LNP + Cqq1_d0_LNP*SQDL(0,0) + Cqq1_d0_LNP*SQDL(1,1) + Cqq1_dd_LNP*SQDL(0,0)*SQDL(1,1) + Cqq1_u0_LNP*SQUL(0,0) + Cqq1_ud_LNP*SQDL(1,1)*SQUL(0,0) + Cqq1_u0_LNP*SQUL(1,1) + Cqq1_ud_LNP*SQDL(0,0)*SQUL(1,1) + Cqq1_uu_LNP*SQUL(0,0)*SQUL(1,1) + Cqq1p_dd_LNP*SQDL(0,1)*SQDL(1,0) + Cqq1p_ud_LNP*SQDL(1,0)*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(0,1)*SQUL(1,0) + Cqq1p_uu_LNP*SQUL(0,1)*SQUL(1,0)).real();
    Cqq1_1123r_LNP = (Cqq1_d0_LNP*SQDL(1,2) + Cqq1_dd_LNP*SQDL(0,0)*SQDL(1,2) + Cqq1_ud_LNP*SQDL(1,2)*SQUL(0,0) + Cqq1_u0_LNP*SQUL(1,2) + Cqq1_ud_LNP*SQDL(0,0)*SQUL(1,2) + Cqq1_uu_LNP*SQUL(0,0)*SQUL(1,2) + Cqq1p_dd_LNP*SQDL(0,2)*SQDL(1,0) + Cqq1p_ud_LNP*SQDL(1,0)*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(1,0) + Cqq1p_uu_LNP*SQUL(0,2)*SQUL(1,0)).real();
    Cqq1_1123i_LNP = (Cqq1_d0_LNP*SQDL(1,2) + Cqq1_dd_LNP*SQDL(0,0)*SQDL(1,2) + Cqq1_ud_LNP*SQDL(1,2)*SQUL(0,0) + Cqq1_u0_LNP*SQUL(1,2) + Cqq1_ud_LNP*SQDL(0,0)*SQUL(1,2) + Cqq1_uu_LNP*SQUL(0,0)*SQUL(1,2) + Cqq1p_dd_LNP*SQDL(0,2)*SQDL(1,0) + Cqq1p_ud_LNP*SQDL(1,0)*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(1,0) + Cqq1p_uu_LNP*SQUL(0,2)*SQUL(1,0)).imag();
    Cqq1_1133r_LNP = (Cqq1_00_LNP + Cqq1_d0_LNP*SQDL(0,0) + Cqq1_d0_LNP*SQDL(2,2) + Cqq1_dd_LNP*SQDL(0,0)*SQDL(2,2) + Cqq1_u0_LNP*SQUL(0,0) + Cqq1_ud_LNP*SQDL(2,2)*SQUL(0,0) + Cqq1_u0_LNP*SQUL(2,2) + Cqq1_ud_LNP*SQDL(0,0)*SQUL(2,2) + Cqq1_uu_LNP*SQUL(0,0)*SQUL(2,2) + Cqq1p_dd_LNP*SQDL(0,2)*SQDL(2,0) + Cqq1p_ud_LNP*SQDL(2,0)*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(2,0) + Cqq1p_uu_LNP*SQUL(0,2)*SQUL(2,0)).real();
    Cqq1_1212r_LNP = (Cqq1_dd_LNP*SQDL(0,1)*SQDL(0,1) + 2*Cqq1_ud_LNP*SQDL(0,1)*SQUL(0,1) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(0,1) + Cqq1p_dd_LNP*SQDL(0,1)*SQDL(0,1) + 2*Cqq1p_ud_LNP*SQDL(0,1)*SQUL(0,1) + Cqq1p_uu_LNP*SQUL(0,1)*SQUL(0,1)).real();
    Cqq1_1212i_LNP = (Cqq1_dd_LNP*SQDL(0,1)*SQDL(0,1) + 2*Cqq1_ud_LNP*SQDL(0,1)*SQUL(0,1) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(0,1) + Cqq1p_dd_LNP*SQDL(0,1)*SQDL(0,1) + 2*Cqq1p_ud_LNP*SQDL(0,1)*SQUL(0,1) + Cqq1p_uu_LNP*SQUL(0,1)*SQUL(0,1)).imag();
    Cqq1_1213r_LNP = (Cqq1_dd_LNP*SQDL(0,1)*SQDL(0,2) + Cqq1_ud_LNP*SQDL(0,2)*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(0,2) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(0,2) + Cqq1p_dd_LNP*SQDL(0,1)*SQDL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(0,1)*SQUL(0,2) + Cqq1p_uu_LNP*SQUL(0,1)*SQUL(0,2)).real();
    Cqq1_1213i_LNP = (Cqq1_dd_LNP*SQDL(0,1)*SQDL(0,2) + Cqq1_ud_LNP*SQDL(0,2)*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(0,2) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(0,2) + Cqq1p_dd_LNP*SQDL(0,1)*SQDL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(0,1)*SQUL(0,2) + Cqq1p_uu_LNP*SQUL(0,1)*SQUL(0,2)).imag();
    Cqq1_1221r_LNP = (Cqq1_dd_LNP*SQDL(0,1)*SQDL(1,0) + Cqq1_ud_LNP*SQDL(1,0)*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(1,0) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(1,0) + Cqq1p_00_LNP + Cqq1p_d0_LNP*SQDL(0,0) + Cqq1p_d0_LNP*SQDL(1,1) + Cqq1p_dd_LNP*SQDL(0,0)*SQDL(1,1) + Cqq1p_u0_LNP*SQUL(0,0) + Cqq1p_ud_LNP*SQDL(1,1)*SQUL(0,0) + Cqq1p_u0_LNP*SQUL(1,1) + Cqq1p_ud_LNP*SQDL(0,0)*SQUL(1,1) + Cqq1p_uu_LNP*SQUL(0,0)*SQUL(1,1)).real();
    Cqq1_1222r_LNP = (Cqq1_d0_LNP*SQDL(0,1) + Cqq1_dd_LNP*SQDL(0,1)*SQDL(1,1) + Cqq1_u0_LNP*SQUL(0,1) + Cqq1_ud_LNP*SQDL(1,1)*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(1,1) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(1,1) + Cqq1p_d0_LNP*SQDL(0,1) + Cqq1p_dd_LNP*SQDL(0,1)*SQDL(1,1) + Cqq1p_u0_LNP*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(1,1)*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(0,1)*SQUL(1,1) + Cqq1p_uu_LNP*SQUL(0,1)*SQUL(1,1)).real();
    Cqq1_1222i_LNP = (Cqq1_d0_LNP*SQDL(0,1) + Cqq1_dd_LNP*SQDL(0,1)*SQDL(1,1) + Cqq1_u0_LNP*SQUL(0,1) + Cqq1_ud_LNP*SQDL(1,1)*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(1,1) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(1,1) + Cqq1p_d0_LNP*SQDL(0,1) + Cqq1p_dd_LNP*SQDL(0,1)*SQDL(1,1) + Cqq1p_u0_LNP*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(1,1)*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(0,1)*SQUL(1,1) + Cqq1p_uu_LNP*SQUL(0,1)*SQUL(1,1)).imag();
    Cqq1_1223r_LNP = (Cqq1_dd_LNP*SQDL(0,1)*SQDL(1,2) + Cqq1_ud_LNP*SQDL(1,2)*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(1,2) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(1,2) + Cqq1p_d0_LNP*SQDL(0,2) + Cqq1p_dd_LNP*SQDL(0,2)*SQDL(1,1) + Cqq1p_u0_LNP*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(1,1)*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(1,1) + Cqq1p_uu_LNP*SQUL(0,2)*SQUL(1,1)).real();
    Cqq1_1223i_LNP = (Cqq1_dd_LNP*SQDL(0,1)*SQDL(1,2) + Cqq1_ud_LNP*SQDL(1,2)*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(1,2) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(1,2) + Cqq1p_d0_LNP*SQDL(0,2) + Cqq1p_dd_LNP*SQDL(0,2)*SQDL(1,1) + Cqq1p_u0_LNP*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(1,1)*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(1,1) + Cqq1p_uu_LNP*SQUL(0,2)*SQUL(1,1)).imag();
    Cqq1_1231r_LNP = (Cqq1_dd_LNP*SQDL(0,1)*SQDL(2,0) + Cqq1_ud_LNP*SQDL(2,0)*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(2,0) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(2,0) + Cqq1p_d0_LNP*SQDL(2,1) + Cqq1p_dd_LNP*SQDL(0,0)*SQDL(2,1) + Cqq1p_ud_LNP*SQDL(2,1)*SQUL(0,0) + Cqq1p_u0_LNP*SQUL(2,1) + Cqq1p_ud_LNP*SQDL(0,0)*SQUL(2,1) + Cqq1p_uu_LNP*SQUL(0,0)*SQUL(2,1)).real();
    Cqq1_1231i_LNP = (Cqq1_dd_LNP*SQDL(0,1)*SQDL(2,0) + Cqq1_ud_LNP*SQDL(2,0)*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(2,0) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(2,0) + Cqq1p_d0_LNP*SQDL(2,1) + Cqq1p_dd_LNP*SQDL(0,0)*SQDL(2,1) + Cqq1p_ud_LNP*SQDL(2,1)*SQUL(0,0) + Cqq1p_u0_LNP*SQUL(2,1) + Cqq1p_ud_LNP*SQDL(0,0)*SQUL(2,1) + Cqq1p_uu_LNP*SQUL(0,0)*SQUL(2,1)).imag();
    Cqq1_1232r_LNP = (Cqq1_dd_LNP*SQDL(0,1)*SQDL(2,1) + Cqq1_ud_LNP*SQDL(2,1)*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(2,1) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(2,1) + Cqq1p_dd_LNP*SQDL(0,1)*SQDL(2,1) + Cqq1p_ud_LNP*SQDL(2,1)*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(0,1)*SQUL(2,1) + Cqq1p_uu_LNP*SQUL(0,1)*SQUL(2,1)).real();
    Cqq1_1232i_LNP = (Cqq1_dd_LNP*SQDL(0,1)*SQDL(2,1) + Cqq1_ud_LNP*SQDL(2,1)*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(2,1) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(2,1) + Cqq1p_dd_LNP*SQDL(0,1)*SQDL(2,1) + Cqq1p_ud_LNP*SQDL(2,1)*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(0,1)*SQUL(2,1) + Cqq1p_uu_LNP*SQUL(0,1)*SQUL(2,1)).imag();
    Cqq1_1233r_LNP = (Cqq1_d0_LNP*SQDL(0,1) + Cqq1_dd_LNP*SQDL(0,1)*SQDL(2,2) + Cqq1_u0_LNP*SQUL(0,1) + Cqq1_ud_LNP*SQDL(2,2)*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(2,2) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(2,2) + Cqq1p_dd_LNP*SQDL(0,2)*SQDL(2,1) + Cqq1p_ud_LNP*SQDL(2,1)*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(2,1) + Cqq1p_uu_LNP*SQUL(0,2)*SQUL(2,1)).real();
    Cqq1_1233i_LNP = (Cqq1_d0_LNP*SQDL(0,1) + Cqq1_dd_LNP*SQDL(0,1)*SQDL(2,2) + Cqq1_u0_LNP*SQUL(0,1) + Cqq1_ud_LNP*SQDL(2,2)*SQUL(0,1) + Cqq1_ud_LNP*SQDL(0,1)*SQUL(2,2) + Cqq1_uu_LNP*SQUL(0,1)*SQUL(2,2) + Cqq1p_dd_LNP*SQDL(0,2)*SQDL(2,1) + Cqq1p_ud_LNP*SQDL(2,1)*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(2,1) + Cqq1p_uu_LNP*SQUL(0,2)*SQUL(2,1)).imag();
    Cqq1_1313r_LNP = (Cqq1_dd_LNP*SQDL(0,2)*SQDL(0,2) + 2*Cqq1_ud_LNP*SQDL(0,2)*SQUL(0,2) + Cqq1_uu_LNP*SQUL(0,2)*SQUL(0,2) + Cqq1p_dd_LNP*SQDL(0,2)*SQDL(0,2) + 2*Cqq1p_ud_LNP*SQDL(0,2)*SQUL(0,2) + Cqq1p_uu_LNP*SQUL(0,2)*SQUL(0,2)).real();
    Cqq1_1313i_LNP = (Cqq1_dd_LNP*SQDL(0,2)*SQDL(0,2) + 2*Cqq1_ud_LNP*SQDL(0,2)*SQUL(0,2) + Cqq1_uu_LNP*SQUL(0,2)*SQUL(0,2) + Cqq1p_dd_LNP*SQDL(0,2)*SQDL(0,2) + 2*Cqq1p_ud_LNP*SQDL(0,2)*SQUL(0,2) + Cqq1p_uu_LNP*SQUL(0,2)*SQUL(0,2)).imag();
    Cqq1_1322r_LNP = (Cqq1_d0_LNP*SQDL(0,2) + Cqq1_dd_LNP*SQDL(0,2)*SQDL(1,1) + Cqq1_u0_LNP*SQUL(0,2) + Cqq1_ud_LNP*SQDL(1,1)*SQUL(0,2) + Cqq1_ud_LNP*SQDL(0,2)*SQUL(1,1) + Cqq1_uu_LNP*SQUL(0,2)*SQUL(1,1) + Cqq1p_dd_LNP*SQDL(0,1)*SQDL(1,2) + Cqq1p_ud_LNP*SQDL(1,2)*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(0,1)*SQUL(1,2) + Cqq1p_uu_LNP*SQUL(0,1)*SQUL(1,2)).real();
    Cqq1_1322i_LNP = (Cqq1_d0_LNP*SQDL(0,2) + Cqq1_dd_LNP*SQDL(0,2)*SQDL(1,1) + Cqq1_u0_LNP*SQUL(0,2) + Cqq1_ud_LNP*SQDL(1,1)*SQUL(0,2) + Cqq1_ud_LNP*SQDL(0,2)*SQUL(1,1) + Cqq1_uu_LNP*SQUL(0,2)*SQUL(1,1) + Cqq1p_dd_LNP*SQDL(0,1)*SQDL(1,2) + Cqq1p_ud_LNP*SQDL(1,2)*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(0,1)*SQUL(1,2) + Cqq1p_uu_LNP*SQUL(0,1)*SQUL(1,2)).imag();
    Cqq1_1323r_LNP = (Cqq1_dd_LNP*SQDL(0,2)*SQDL(1,2) + Cqq1_ud_LNP*SQDL(1,2)*SQUL(0,2) + Cqq1_ud_LNP*SQDL(0,2)*SQUL(1,2) + Cqq1_uu_LNP*SQUL(0,2)*SQUL(1,2) + Cqq1p_dd_LNP*SQDL(0,2)*SQDL(1,2) + Cqq1p_ud_LNP*SQDL(1,2)*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(1,2) + Cqq1p_uu_LNP*SQUL(0,2)*SQUL(1,2)).real();
    Cqq1_1323i_LNP = (Cqq1_dd_LNP*SQDL(0,2)*SQDL(1,2) + Cqq1_ud_LNP*SQDL(1,2)*SQUL(0,2) + Cqq1_ud_LNP*SQDL(0,2)*SQUL(1,2) + Cqq1_uu_LNP*SQUL(0,2)*SQUL(1,2) + Cqq1p_dd_LNP*SQDL(0,2)*SQDL(1,2) + Cqq1p_ud_LNP*SQDL(1,2)*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(1,2) + Cqq1p_uu_LNP*SQUL(0,2)*SQUL(1,2)).imag();
    Cqq1_1331r_LNP = (Cqq1_dd_LNP*SQDL(0,2)*SQDL(2,0) + Cqq1_ud_LNP*SQDL(2,0)*SQUL(0,2) + Cqq1_ud_LNP*SQDL(0,2)*SQUL(2,0) + Cqq1_uu_LNP*SQUL(0,2)*SQUL(2,0) + Cqq1p_00_LNP + Cqq1p_d0_LNP*SQDL(0,0) + Cqq1p_d0_LNP*SQDL(2,2) + Cqq1p_dd_LNP*SQDL(0,0)*SQDL(2,2) + Cqq1p_u0_LNP*SQUL(0,0) + Cqq1p_ud_LNP*SQDL(2,2)*SQUL(0,0) + Cqq1p_u0_LNP*SQUL(2,2) + Cqq1p_ud_LNP*SQDL(0,0)*SQUL(2,2) + Cqq1p_uu_LNP*SQUL(0,0)*SQUL(2,2)).real();
    Cqq1_1332r_LNP = (Cqq1_dd_LNP*SQDL(0,2)*SQDL(2,1) + Cqq1_ud_LNP*SQDL(2,1)*SQUL(0,2) + Cqq1_ud_LNP*SQDL(0,2)*SQUL(2,1) + Cqq1_uu_LNP*SQUL(0,2)*SQUL(2,1) + Cqq1p_d0_LNP*SQDL(0,1) + Cqq1p_dd_LNP*SQDL(0,1)*SQDL(2,2) + Cqq1p_u0_LNP*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(2,2)*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(0,1)*SQUL(2,2) + Cqq1p_uu_LNP*SQUL(0,1)*SQUL(2,2)).real();
    Cqq1_1332i_LNP = (Cqq1_dd_LNP*SQDL(0,2)*SQDL(2,1) + Cqq1_ud_LNP*SQDL(2,1)*SQUL(0,2) + Cqq1_ud_LNP*SQDL(0,2)*SQUL(2,1) + Cqq1_uu_LNP*SQUL(0,2)*SQUL(2,1) + Cqq1p_d0_LNP*SQDL(0,1) + Cqq1p_dd_LNP*SQDL(0,1)*SQDL(2,2) + Cqq1p_u0_LNP*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(2,2)*SQUL(0,1) + Cqq1p_ud_LNP*SQDL(0,1)*SQUL(2,2) + Cqq1p_uu_LNP*SQUL(0,1)*SQUL(2,2)).imag();
    Cqq1_1333r_LNP = (Cqq1_d0_LNP*SQDL(0,2) + Cqq1_dd_LNP*SQDL(0,2)*SQDL(2,2) + Cqq1_u0_LNP*SQUL(0,2) + Cqq1_ud_LNP*SQDL(2,2)*SQUL(0,2) + Cqq1_ud_LNP*SQDL(0,2)*SQUL(2,2) + Cqq1_uu_LNP*SQUL(0,2)*SQUL(2,2) + Cqq1p_d0_LNP*SQDL(0,2) + Cqq1p_dd_LNP*SQDL(0,2)*SQDL(2,2) + Cqq1p_u0_LNP*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(2,2)*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(2,2) + Cqq1p_uu_LNP*SQUL(0,2)*SQUL(2,2)).real();
    Cqq1_1333i_LNP = (Cqq1_d0_LNP*SQDL(0,2) + Cqq1_dd_LNP*SQDL(0,2)*SQDL(2,2) + Cqq1_u0_LNP*SQUL(0,2) + Cqq1_ud_LNP*SQDL(2,2)*SQUL(0,2) + Cqq1_ud_LNP*SQDL(0,2)*SQUL(2,2) + Cqq1_uu_LNP*SQUL(0,2)*SQUL(2,2) + Cqq1p_d0_LNP*SQDL(0,2) + Cqq1p_dd_LNP*SQDL(0,2)*SQDL(2,2) + Cqq1p_u0_LNP*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(2,2)*SQUL(0,2) + Cqq1p_ud_LNP*SQDL(0,2)*SQUL(2,2) + Cqq1p_uu_LNP*SQUL(0,2)*SQUL(2,2)).imag();
    Cqq1_2222r_LNP = (Cqq1_00_LNP + 2*Cqq1_d0_LNP*SQDL(1,1) + Cqq1_dd_LNP*SQDL(1,1)*SQDL(1,1) + 2*Cqq1_u0_LNP*SQUL(1,1) + 2*Cqq1_ud_LNP*SQDL(1,1)*SQUL(1,1) + Cqq1_uu_LNP*SQUL(1,1)*SQUL(1,1) + Cqq1p_00_LNP + 2*Cqq1p_d0_LNP*SQDL(1,1) + Cqq1p_dd_LNP*SQDL(1,1)*SQDL(1,1) + 2*Cqq1p_u0_LNP*SQUL(1,1) + 2*Cqq1p_ud_LNP*SQDL(1,1)*SQUL(1,1) + Cqq1p_uu_LNP*SQUL(1,1)*SQUL(1,1)).real();
    Cqq1_2223r_LNP = (Cqq1_d0_LNP*SQDL(1,2) + Cqq1_dd_LNP*SQDL(1,1)*SQDL(1,2) + Cqq1_ud_LNP*SQDL(1,2)*SQUL(1,1) + Cqq1_u0_LNP*SQUL(1,2) + Cqq1_ud_LNP*SQDL(1,1)*SQUL(1,2) + Cqq1_uu_LNP*SQUL(1,1)*SQUL(1,2) + Cqq1p_d0_LNP*SQDL(1,2) + Cqq1p_dd_LNP*SQDL(1,1)*SQDL(1,2) + Cqq1p_ud_LNP*SQDL(1,2)*SQUL(1,1) + Cqq1p_u0_LNP*SQUL(1,2) + Cqq1p_ud_LNP*SQDL(1,1)*SQUL(1,2) + Cqq1p_uu_LNP*SQUL(1,1)*SQUL(1,2)).real();
    Cqq1_2223i_LNP = (Cqq1_d0_LNP*SQDL(1,2) + Cqq1_dd_LNP*SQDL(1,1)*SQDL(1,2) + Cqq1_ud_LNP*SQDL(1,2)*SQUL(1,1) + Cqq1_u0_LNP*SQUL(1,2) + Cqq1_ud_LNP*SQDL(1,1)*SQUL(1,2) + Cqq1_uu_LNP*SQUL(1,1)*SQUL(1,2) + Cqq1p_d0_LNP*SQDL(1,2) + Cqq1p_dd_LNP*SQDL(1,1)*SQDL(1,2) + Cqq1p_ud_LNP*SQDL(1,2)*SQUL(1,1) + Cqq1p_u0_LNP*SQUL(1,2) + Cqq1p_ud_LNP*SQDL(1,1)*SQUL(1,2) + Cqq1p_uu_LNP*SQUL(1,1)*SQUL(1,2)).imag();
    Cqq1_2233r_LNP = (Cqq1_00_LNP + Cqq1_d0_LNP*SQDL(1,1) + Cqq1_d0_LNP*SQDL(2,2) + Cqq1_dd_LNP*SQDL(1,1)*SQDL(2,2) + Cqq1_u0_LNP*SQUL(1,1) + Cqq1_ud_LNP*SQDL(2,2)*SQUL(1,1) + Cqq1_u0_LNP*SQUL(2,2) + Cqq1_ud_LNP*SQDL(1,1)*SQUL(2,2) + Cqq1_uu_LNP*SQUL(1,1)*SQUL(2,2) + Cqq1p_dd_LNP*SQDL(1,2)*SQDL(2,1) + Cqq1p_ud_LNP*SQDL(2,1)*SQUL(1,2) + Cqq1p_ud_LNP*SQDL(1,2)*SQUL(2,1) + Cqq1p_uu_LNP*SQUL(1,2)*SQUL(2,1)).real();
    Cqq1_2323r_LNP = (Cqq1_dd_LNP*SQDL(1,2)*SQDL(1,2) + 2*Cqq1_ud_LNP*SQDL(1,2)*SQUL(1,2) + Cqq1_uu_LNP*SQUL(1,2)*SQUL(1,2) + Cqq1p_dd_LNP*SQDL(1,2)*SQDL(1,2) + 2*Cqq1p_ud_LNP*SQDL(1,2)*SQUL(1,2) + Cqq1p_uu_LNP*SQUL(1,2)*SQUL(1,2)).real();
    Cqq1_2323i_LNP = (Cqq1_dd_LNP*SQDL(1,2)*SQDL(1,2) + 2*Cqq1_ud_LNP*SQDL(1,2)*SQUL(1,2) + Cqq1_uu_LNP*SQUL(1,2)*SQUL(1,2) + Cqq1p_dd_LNP*SQDL(1,2)*SQDL(1,2) + 2*Cqq1p_ud_LNP*SQDL(1,2)*SQUL(1,2) + Cqq1p_uu_LNP*SQUL(1,2)*SQUL(1,2)).imag();
    Cqq1_2332r_LNP = (Cqq1_dd_LNP*SQDL(1,2)*SQDL(2,1) + Cqq1_ud_LNP*SQDL(2,1)*SQUL(1,2) + Cqq1_ud_LNP*SQDL(1,2)*SQUL(2,1) + Cqq1_uu_LNP*SQUL(1,2)*SQUL(2,1) + Cqq1p_00_LNP + Cqq1p_d0_LNP*SQDL(1,1) + Cqq1p_d0_LNP*SQDL(2,2) + Cqq1p_dd_LNP*SQDL(1,1)*SQDL(2,2) + Cqq1p_u0_LNP*SQUL(1,1) + Cqq1p_ud_LNP*SQDL(2,2)*SQUL(1,1) + Cqq1p_u0_LNP*SQUL(2,2) + Cqq1p_ud_LNP*SQDL(1,1)*SQUL(2,2) + Cqq1p_uu_LNP*SQUL(1,1)*SQUL(2,2)).real();
    Cqq1_2333r_LNP = (Cqq1_d0_LNP*SQDL(1,2) + Cqq1_dd_LNP*SQDL(1,2)*SQDL(2,2) + Cqq1_u0_LNP*SQUL(1,2) + Cqq1_ud_LNP*SQDL(2,2)*SQUL(1,2) + Cqq1_ud_LNP*SQDL(1,2)*SQUL(2,2) + Cqq1_uu_LNP*SQUL(1,2)*SQUL(2,2) + Cqq1p_d0_LNP*SQDL(1,2) + Cqq1p_dd_LNP*SQDL(1,2)*SQDL(2,2) + Cqq1p_u0_LNP*SQUL(1,2) + Cqq1p_ud_LNP*SQDL(2,2)*SQUL(1,2) + Cqq1p_ud_LNP*SQDL(1,2)*SQUL(2,2) + Cqq1p_uu_LNP*SQUL(1,2)*SQUL(2,2)).real();
    Cqq1_2333i_LNP = (Cqq1_d0_LNP*SQDL(1,2) + Cqq1_dd_LNP*SQDL(1,2)*SQDL(2,2) + Cqq1_u0_LNP*SQUL(1,2) + Cqq1_ud_LNP*SQDL(2,2)*SQUL(1,2) + Cqq1_ud_LNP*SQDL(1,2)*SQUL(2,2) + Cqq1_uu_LNP*SQUL(1,2)*SQUL(2,2) + Cqq1p_d0_LNP*SQDL(1,2) + Cqq1p_dd_LNP*SQDL(1,2)*SQDL(2,2) + Cqq1p_u0_LNP*SQUL(1,2) + Cqq1p_ud_LNP*SQDL(2,2)*SQUL(1,2) + Cqq1p_ud_LNP*SQDL(1,2)*SQUL(2,2) + Cqq1p_uu_LNP*SQUL(1,2)*SQUL(2,2)).imag();
    Cqq1_3333r_LNP = (Cqq1_00_LNP + 2*Cqq1_d0_LNP*SQDL(2,2) + Cqq1_dd_LNP*SQDL(2,2)*SQDL(2,2) + 2*Cqq1_u0_LNP*SQUL(2,2) + 2*Cqq1_ud_LNP*SQDL(2,2)*SQUL(2,2) + Cqq1_uu_LNP*SQUL(2,2)*SQUL(2,2) + Cqq1p_00_LNP + 2*Cqq1p_d0_LNP*SQDL(2,2) + Cqq1p_dd_LNP*SQDL(2,2)*SQDL(2,2) + 2*Cqq1p_u0_LNP*SQUL(2,2) + 2*Cqq1p_ud_LNP*SQDL(2,2)*SQUL(2,2) + Cqq1p_uu_LNP*SQUL(2,2)*SQUL(2,2)).real();
 
    Cqq3_1111r_LNP = (Cqq3_00_LNP + 2*Cqq3_d0_LNP*SQDL(0,0) + Cqq3_dd_LNP*SQDL(0,0)*SQDL(0,0) + 2*Cqq3_u0_LNP*SQUL(0,0) + 2*Cqq3_ud_LNP*SQDL(0,0)*SQUL(0,0) + Cqq3_uu_LNP*SQUL(0,0)*SQUL(0,0) + Cqq3p_00_LNP + 2*Cqq3p_d0_LNP*SQDL(0,0) + Cqq3p_dd_LNP*SQDL(0,0)*SQDL(0,0) + 2*Cqq3p_u0_LNP*SQUL(0,0) + 2*Cqq3p_ud_LNP*SQDL(0,0)*SQUL(0,0) + Cqq3p_uu_LNP*SQUL(0,0)*SQUL(0,0)).real();
    Cqq3_1112r_LNP = (Cqq3_d0_LNP*SQDL(0,1) + Cqq3_dd_LNP*SQDL(0,0)*SQDL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(0,0) + Cqq3_u0_LNP*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,0)*SQUL(0,1) + Cqq3_uu_LNP*SQUL(0,0)*SQUL(0,1) + Cqq3p_d0_LNP*SQDL(0,1) + Cqq3p_dd_LNP*SQDL(0,0)*SQDL(0,1) + Cqq3p_ud_LNP*SQDL(0,1)*SQUL(0,0) + Cqq3p_u0_LNP*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(0,0)*SQUL(0,1) + Cqq3p_uu_LNP*SQUL(0,0)*SQUL(0,1)).real();
    Cqq3_1112i_LNP = (Cqq3_d0_LNP*SQDL(0,1) + Cqq3_dd_LNP*SQDL(0,0)*SQDL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(0,0) + Cqq3_u0_LNP*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,0)*SQUL(0,1) + Cqq3_uu_LNP*SQUL(0,0)*SQUL(0,1) + Cqq3p_d0_LNP*SQDL(0,1) + Cqq3p_dd_LNP*SQDL(0,0)*SQDL(0,1) + Cqq3p_ud_LNP*SQDL(0,1)*SQUL(0,0) + Cqq3p_u0_LNP*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(0,0)*SQUL(0,1) + Cqq3p_uu_LNP*SQUL(0,0)*SQUL(0,1)).imag();
    Cqq3_1113r_LNP = (Cqq3_d0_LNP*SQDL(0,2) + Cqq3_dd_LNP*SQDL(0,0)*SQDL(0,2) + Cqq3_ud_LNP*SQDL(0,2)*SQUL(0,0) + Cqq3_u0_LNP*SQUL(0,2) + Cqq3_ud_LNP*SQDL(0,0)*SQUL(0,2) + Cqq3_uu_LNP*SQUL(0,0)*SQUL(0,2) + Cqq3p_d0_LNP*SQDL(0,2) + Cqq3p_dd_LNP*SQDL(0,0)*SQDL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(0,0) + Cqq3p_u0_LNP*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(0,0)*SQUL(0,2) + Cqq3p_uu_LNP*SQUL(0,0)*SQUL(0,2)).real();
    Cqq3_1113i_LNP = (Cqq3_d0_LNP*SQDL(0,2) + Cqq3_dd_LNP*SQDL(0,0)*SQDL(0,2) + Cqq3_ud_LNP*SQDL(0,2)*SQUL(0,0) + Cqq3_u0_LNP*SQUL(0,2) + Cqq3_ud_LNP*SQDL(0,0)*SQUL(0,2) + Cqq3_uu_LNP*SQUL(0,0)*SQUL(0,2) + Cqq3p_d0_LNP*SQDL(0,2) + Cqq3p_dd_LNP*SQDL(0,0)*SQDL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(0,0) + Cqq3p_u0_LNP*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(0,0)*SQUL(0,2) + Cqq3p_uu_LNP*SQUL(0,0)*SQUL(0,2)).imag();
    Cqq3_1122r_LNP = (Cqq3_00_LNP + Cqq3_d0_LNP*SQDL(0,0) + Cqq3_d0_LNP*SQDL(1,1) + Cqq3_dd_LNP*SQDL(0,0)*SQDL(1,1) + Cqq3_u0_LNP*SQUL(0,0) + Cqq3_ud_LNP*SQDL(1,1)*SQUL(0,0) + Cqq3_u0_LNP*SQUL(1,1) + Cqq3_ud_LNP*SQDL(0,0)*SQUL(1,1) + Cqq3_uu_LNP*SQUL(0,0)*SQUL(1,1) + Cqq3p_dd_LNP*SQDL(0,1)*SQDL(1,0) + Cqq3p_ud_LNP*SQDL(1,0)*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(0,1)*SQUL(1,0) + Cqq3p_uu_LNP*SQUL(0,1)*SQUL(1,0)).real();
    Cqq3_1123r_LNP = (Cqq3_d0_LNP*SQDL(1,2) + Cqq3_dd_LNP*SQDL(0,0)*SQDL(1,2) + Cqq3_ud_LNP*SQDL(1,2)*SQUL(0,0) + Cqq3_u0_LNP*SQUL(1,2) + Cqq3_ud_LNP*SQDL(0,0)*SQUL(1,2) + Cqq3_uu_LNP*SQUL(0,0)*SQUL(1,2) + Cqq3p_dd_LNP*SQDL(0,2)*SQDL(1,0) + Cqq3p_ud_LNP*SQDL(1,0)*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(1,0) + Cqq3p_uu_LNP*SQUL(0,2)*SQUL(1,0)).real();
    Cqq3_1123i_LNP = (Cqq3_d0_LNP*SQDL(1,2) + Cqq3_dd_LNP*SQDL(0,0)*SQDL(1,2) + Cqq3_ud_LNP*SQDL(1,2)*SQUL(0,0) + Cqq3_u0_LNP*SQUL(1,2) + Cqq3_ud_LNP*SQDL(0,0)*SQUL(1,2) + Cqq3_uu_LNP*SQUL(0,0)*SQUL(1,2) + Cqq3p_dd_LNP*SQDL(0,2)*SQDL(1,0) + Cqq3p_ud_LNP*SQDL(1,0)*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(1,0) + Cqq3p_uu_LNP*SQUL(0,2)*SQUL(1,0)).imag();
    Cqq3_1133r_LNP = (Cqq3_00_LNP + Cqq3_d0_LNP*SQDL(0,0) + Cqq3_d0_LNP*SQDL(2,2) + Cqq3_dd_LNP*SQDL(0,0)*SQDL(2,2) + Cqq3_u0_LNP*SQUL(0,0) + Cqq3_ud_LNP*SQDL(2,2)*SQUL(0,0) + Cqq3_u0_LNP*SQUL(2,2) + Cqq3_ud_LNP*SQDL(0,0)*SQUL(2,2) + Cqq3_uu_LNP*SQUL(0,0)*SQUL(2,2) + Cqq3p_dd_LNP*SQDL(0,2)*SQDL(2,0) + Cqq3p_ud_LNP*SQDL(2,0)*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(2,0) + Cqq3p_uu_LNP*SQUL(0,2)*SQUL(2,0)).real();
    Cqq3_1212r_LNP = (Cqq3_dd_LNP*SQDL(0,1)*SQDL(0,1) + 2*Cqq3_ud_LNP*SQDL(0,1)*SQUL(0,1) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(0,1) + Cqq3p_dd_LNP*SQDL(0,1)*SQDL(0,1) + 2*Cqq3p_ud_LNP*SQDL(0,1)*SQUL(0,1) + Cqq3p_uu_LNP*SQUL(0,1)*SQUL(0,1)).real();
    Cqq3_1212i_LNP = (Cqq3_dd_LNP*SQDL(0,1)*SQDL(0,1) + 2*Cqq3_ud_LNP*SQDL(0,1)*SQUL(0,1) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(0,1) + Cqq3p_dd_LNP*SQDL(0,1)*SQDL(0,1) + 2*Cqq3p_ud_LNP*SQDL(0,1)*SQUL(0,1) + Cqq3p_uu_LNP*SQUL(0,1)*SQUL(0,1)).imag();
    Cqq3_1213r_LNP = (Cqq3_dd_LNP*SQDL(0,1)*SQDL(0,2) + Cqq3_ud_LNP*SQDL(0,2)*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(0,2) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(0,2) + Cqq3p_dd_LNP*SQDL(0,1)*SQDL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(0,1)*SQUL(0,2) + Cqq3p_uu_LNP*SQUL(0,1)*SQUL(0,2)).real();
    Cqq3_1213i_LNP = (Cqq3_dd_LNP*SQDL(0,1)*SQDL(0,2) + Cqq3_ud_LNP*SQDL(0,2)*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(0,2) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(0,2) + Cqq3p_dd_LNP*SQDL(0,1)*SQDL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(0,1)*SQUL(0,2) + Cqq3p_uu_LNP*SQUL(0,1)*SQUL(0,2)).imag();
    Cqq3_1221r_LNP = (Cqq3_dd_LNP*SQDL(0,1)*SQDL(1,0) + Cqq3_ud_LNP*SQDL(1,0)*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(1,0) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(1,0) + Cqq3p_00_LNP + Cqq3p_d0_LNP*SQDL(0,0) + Cqq3p_d0_LNP*SQDL(1,1) + Cqq3p_dd_LNP*SQDL(0,0)*SQDL(1,1) + Cqq3p_u0_LNP*SQUL(0,0) + Cqq3p_ud_LNP*SQDL(1,1)*SQUL(0,0) + Cqq3p_u0_LNP*SQUL(1,1) + Cqq3p_ud_LNP*SQDL(0,0)*SQUL(1,1) + Cqq3p_uu_LNP*SQUL(0,0)*SQUL(1,1)).real();
    Cqq3_1222r_LNP = (Cqq3_d0_LNP*SQDL(0,1) + Cqq3_dd_LNP*SQDL(0,1)*SQDL(1,1) + Cqq3_u0_LNP*SQUL(0,1) + Cqq3_ud_LNP*SQDL(1,1)*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(1,1) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(1,1) + Cqq3p_d0_LNP*SQDL(0,1) + Cqq3p_dd_LNP*SQDL(0,1)*SQDL(1,1) + Cqq3p_u0_LNP*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(1,1)*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(0,1)*SQUL(1,1) + Cqq3p_uu_LNP*SQUL(0,1)*SQUL(1,1)).real();
    Cqq3_1222i_LNP = (Cqq3_d0_LNP*SQDL(0,1) + Cqq3_dd_LNP*SQDL(0,1)*SQDL(1,1) + Cqq3_u0_LNP*SQUL(0,1) + Cqq3_ud_LNP*SQDL(1,1)*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(1,1) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(1,1) + Cqq3p_d0_LNP*SQDL(0,1) + Cqq3p_dd_LNP*SQDL(0,1)*SQDL(1,1) + Cqq3p_u0_LNP*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(1,1)*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(0,1)*SQUL(1,1) + Cqq3p_uu_LNP*SQUL(0,1)*SQUL(1,1)).imag();
    Cqq3_1223r_LNP = (Cqq3_dd_LNP*SQDL(0,1)*SQDL(1,2) + Cqq3_ud_LNP*SQDL(1,2)*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(1,2) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(1,2) + Cqq3p_d0_LNP*SQDL(0,2) + Cqq3p_dd_LNP*SQDL(0,2)*SQDL(1,1) + Cqq3p_u0_LNP*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(1,1)*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(1,1) + Cqq3p_uu_LNP*SQUL(0,2)*SQUL(1,1)).real();
    Cqq3_1223i_LNP = (Cqq3_dd_LNP*SQDL(0,1)*SQDL(1,2) + Cqq3_ud_LNP*SQDL(1,2)*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(1,2) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(1,2) + Cqq3p_d0_LNP*SQDL(0,2) + Cqq3p_dd_LNP*SQDL(0,2)*SQDL(1,1) + Cqq3p_u0_LNP*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(1,1)*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(1,1) + Cqq3p_uu_LNP*SQUL(0,2)*SQUL(1,1)).imag();
    Cqq3_1231r_LNP = (Cqq3_dd_LNP*SQDL(0,1)*SQDL(2,0) + Cqq3_ud_LNP*SQDL(2,0)*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(2,0) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(2,0) + Cqq3p_d0_LNP*SQDL(2,1) + Cqq3p_dd_LNP*SQDL(0,0)*SQDL(2,1) + Cqq3p_ud_LNP*SQDL(2,1)*SQUL(0,0) + Cqq3p_u0_LNP*SQUL(2,1) + Cqq3p_ud_LNP*SQDL(0,0)*SQUL(2,1) + Cqq3p_uu_LNP*SQUL(0,0)*SQUL(2,1)).real();
    Cqq3_1231i_LNP = (Cqq3_dd_LNP*SQDL(0,1)*SQDL(2,0) + Cqq3_ud_LNP*SQDL(2,0)*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(2,0) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(2,0) + Cqq3p_d0_LNP*SQDL(2,1) + Cqq3p_dd_LNP*SQDL(0,0)*SQDL(2,1) + Cqq3p_ud_LNP*SQDL(2,1)*SQUL(0,0) + Cqq3p_u0_LNP*SQUL(2,1) + Cqq3p_ud_LNP*SQDL(0,0)*SQUL(2,1) + Cqq3p_uu_LNP*SQUL(0,0)*SQUL(2,1)).imag();
    Cqq3_1232r_LNP = (Cqq3_dd_LNP*SQDL(0,1)*SQDL(2,1) + Cqq3_ud_LNP*SQDL(2,1)*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(2,1) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(2,1) + Cqq3p_dd_LNP*SQDL(0,1)*SQDL(2,1) + Cqq3p_ud_LNP*SQDL(2,1)*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(0,1)*SQUL(2,1) + Cqq3p_uu_LNP*SQUL(0,1)*SQUL(2,1)).real();
    Cqq3_1232i_LNP = (Cqq3_dd_LNP*SQDL(0,1)*SQDL(2,1) + Cqq3_ud_LNP*SQDL(2,1)*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(2,1) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(2,1) + Cqq3p_dd_LNP*SQDL(0,1)*SQDL(2,1) + Cqq3p_ud_LNP*SQDL(2,1)*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(0,1)*SQUL(2,1) + Cqq3p_uu_LNP*SQUL(0,1)*SQUL(2,1)).imag();
    Cqq3_1233r_LNP = (Cqq3_d0_LNP*SQDL(0,1) + Cqq3_dd_LNP*SQDL(0,1)*SQDL(2,2) + Cqq3_u0_LNP*SQUL(0,1) + Cqq3_ud_LNP*SQDL(2,2)*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(2,2) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(2,2) + Cqq3p_dd_LNP*SQDL(0,2)*SQDL(2,1) + Cqq3p_ud_LNP*SQDL(2,1)*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(2,1) + Cqq3p_uu_LNP*SQUL(0,2)*SQUL(2,1)).real();
    Cqq3_1233i_LNP = (Cqq3_d0_LNP*SQDL(0,1) + Cqq3_dd_LNP*SQDL(0,1)*SQDL(2,2) + Cqq3_u0_LNP*SQUL(0,1) + Cqq3_ud_LNP*SQDL(2,2)*SQUL(0,1) + Cqq3_ud_LNP*SQDL(0,1)*SQUL(2,2) + Cqq3_uu_LNP*SQUL(0,1)*SQUL(2,2) + Cqq3p_dd_LNP*SQDL(0,2)*SQDL(2,1) + Cqq3p_ud_LNP*SQDL(2,1)*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(2,1) + Cqq3p_uu_LNP*SQUL(0,2)*SQUL(2,1)).imag();
    Cqq3_1313r_LNP = (Cqq3_dd_LNP*SQDL(0,2)*SQDL(0,2) + 2*Cqq3_ud_LNP*SQDL(0,2)*SQUL(0,2) + Cqq3_uu_LNP*SQUL(0,2)*SQUL(0,2) + Cqq3p_dd_LNP*SQDL(0,2)*SQDL(0,2) + 2*Cqq3p_ud_LNP*SQDL(0,2)*SQUL(0,2) + Cqq3p_uu_LNP*SQUL(0,2)*SQUL(0,2)).real();
    Cqq3_1313i_LNP = (Cqq3_dd_LNP*SQDL(0,2)*SQDL(0,2) + 2*Cqq3_ud_LNP*SQDL(0,2)*SQUL(0,2) + Cqq3_uu_LNP*SQUL(0,2)*SQUL(0,2) + Cqq3p_dd_LNP*SQDL(0,2)*SQDL(0,2) + 2*Cqq3p_ud_LNP*SQDL(0,2)*SQUL(0,2) + Cqq3p_uu_LNP*SQUL(0,2)*SQUL(0,2)).imag();
    Cqq3_1322r_LNP = (Cqq3_d0_LNP*SQDL(0,2) + Cqq3_dd_LNP*SQDL(0,2)*SQDL(1,1) + Cqq3_u0_LNP*SQUL(0,2) + Cqq3_ud_LNP*SQDL(1,1)*SQUL(0,2) + Cqq3_ud_LNP*SQDL(0,2)*SQUL(1,1) + Cqq3_uu_LNP*SQUL(0,2)*SQUL(1,1) + Cqq3p_dd_LNP*SQDL(0,1)*SQDL(1,2) + Cqq3p_ud_LNP*SQDL(1,2)*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(0,1)*SQUL(1,2) + Cqq3p_uu_LNP*SQUL(0,1)*SQUL(1,2)).real();
    Cqq3_1322i_LNP = (Cqq3_d0_LNP*SQDL(0,2) + Cqq3_dd_LNP*SQDL(0,2)*SQDL(1,1) + Cqq3_u0_LNP*SQUL(0,2) + Cqq3_ud_LNP*SQDL(1,1)*SQUL(0,2) + Cqq3_ud_LNP*SQDL(0,2)*SQUL(1,1) + Cqq3_uu_LNP*SQUL(0,2)*SQUL(1,1) + Cqq3p_dd_LNP*SQDL(0,1)*SQDL(1,2) + Cqq3p_ud_LNP*SQDL(1,2)*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(0,1)*SQUL(1,2) + Cqq3p_uu_LNP*SQUL(0,1)*SQUL(1,2)).imag();
    Cqq3_1323r_LNP = (Cqq3_dd_LNP*SQDL(0,2)*SQDL(1,2) + Cqq3_ud_LNP*SQDL(1,2)*SQUL(0,2) + Cqq3_ud_LNP*SQDL(0,2)*SQUL(1,2) + Cqq3_uu_LNP*SQUL(0,2)*SQUL(1,2) + Cqq3p_dd_LNP*SQDL(0,2)*SQDL(1,2) + Cqq3p_ud_LNP*SQDL(1,2)*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(1,2) + Cqq3p_uu_LNP*SQUL(0,2)*SQUL(1,2)).real();
    Cqq3_1323i_LNP = (Cqq3_dd_LNP*SQDL(0,2)*SQDL(1,2) + Cqq3_ud_LNP*SQDL(1,2)*SQUL(0,2) + Cqq3_ud_LNP*SQDL(0,2)*SQUL(1,2) + Cqq3_uu_LNP*SQUL(0,2)*SQUL(1,2) + Cqq3p_dd_LNP*SQDL(0,2)*SQDL(1,2) + Cqq3p_ud_LNP*SQDL(1,2)*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(1,2) + Cqq3p_uu_LNP*SQUL(0,2)*SQUL(1,2)).imag();
    Cqq3_1331r_LNP = (Cqq3_dd_LNP*SQDL(0,2)*SQDL(2,0) + Cqq3_ud_LNP*SQDL(2,0)*SQUL(0,2) + Cqq3_ud_LNP*SQDL(0,2)*SQUL(2,0) + Cqq3_uu_LNP*SQUL(0,2)*SQUL(2,0) + Cqq3p_00_LNP + Cqq3p_d0_LNP*SQDL(0,0) + Cqq3p_d0_LNP*SQDL(2,2) + Cqq3p_dd_LNP*SQDL(0,0)*SQDL(2,2) + Cqq3p_u0_LNP*SQUL(0,0) + Cqq3p_ud_LNP*SQDL(2,2)*SQUL(0,0) + Cqq3p_u0_LNP*SQUL(2,2) + Cqq3p_ud_LNP*SQDL(0,0)*SQUL(2,2) + Cqq3p_uu_LNP*SQUL(0,0)*SQUL(2,2)).real();
    Cqq3_1332r_LNP = (Cqq3_dd_LNP*SQDL(0,2)*SQDL(2,1) + Cqq3_ud_LNP*SQDL(2,1)*SQUL(0,2) + Cqq3_ud_LNP*SQDL(0,2)*SQUL(2,1) + Cqq3_uu_LNP*SQUL(0,2)*SQUL(2,1) + Cqq3p_d0_LNP*SQDL(0,1) + Cqq3p_dd_LNP*SQDL(0,1)*SQDL(2,2) + Cqq3p_u0_LNP*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(2,2)*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(0,1)*SQUL(2,2) + Cqq3p_uu_LNP*SQUL(0,1)*SQUL(2,2)).real();
    Cqq3_1332i_LNP = (Cqq3_dd_LNP*SQDL(0,2)*SQDL(2,1) + Cqq3_ud_LNP*SQDL(2,1)*SQUL(0,2) + Cqq3_ud_LNP*SQDL(0,2)*SQUL(2,1) + Cqq3_uu_LNP*SQUL(0,2)*SQUL(2,1) + Cqq3p_d0_LNP*SQDL(0,1) + Cqq3p_dd_LNP*SQDL(0,1)*SQDL(2,2) + Cqq3p_u0_LNP*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(2,2)*SQUL(0,1) + Cqq3p_ud_LNP*SQDL(0,1)*SQUL(2,2) + Cqq3p_uu_LNP*SQUL(0,1)*SQUL(2,2)).imag();
    Cqq3_1333r_LNP = (Cqq3_d0_LNP*SQDL(0,2) + Cqq3_dd_LNP*SQDL(0,2)*SQDL(2,2) + Cqq3_u0_LNP*SQUL(0,2) + Cqq3_ud_LNP*SQDL(2,2)*SQUL(0,2) + Cqq3_ud_LNP*SQDL(0,2)*SQUL(2,2) + Cqq3_uu_LNP*SQUL(0,2)*SQUL(2,2) + Cqq3p_d0_LNP*SQDL(0,2) + Cqq3p_dd_LNP*SQDL(0,2)*SQDL(2,2) + Cqq3p_u0_LNP*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(2,2)*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(2,2) + Cqq3p_uu_LNP*SQUL(0,2)*SQUL(2,2)).real();
    Cqq3_1333i_LNP = (Cqq3_d0_LNP*SQDL(0,2) + Cqq3_dd_LNP*SQDL(0,2)*SQDL(2,2) + Cqq3_u0_LNP*SQUL(0,2) + Cqq3_ud_LNP*SQDL(2,2)*SQUL(0,2) + Cqq3_ud_LNP*SQDL(0,2)*SQUL(2,2) + Cqq3_uu_LNP*SQUL(0,2)*SQUL(2,2) + Cqq3p_d0_LNP*SQDL(0,2) + Cqq3p_dd_LNP*SQDL(0,2)*SQDL(2,2) + Cqq3p_u0_LNP*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(2,2)*SQUL(0,2) + Cqq3p_ud_LNP*SQDL(0,2)*SQUL(2,2) + Cqq3p_uu_LNP*SQUL(0,2)*SQUL(2,2)).imag();
    Cqq3_2222r_LNP = (Cqq3_00_LNP + 2*Cqq3_d0_LNP*SQDL(1,1) + Cqq3_dd_LNP*SQDL(1,1)*SQDL(1,1) + 2*Cqq3_u0_LNP*SQUL(1,1) + 2*Cqq3_ud_LNP*SQDL(1,1)*SQUL(1,1) + Cqq3_uu_LNP*SQUL(1,1)*SQUL(1,1) + Cqq3p_00_LNP + 2*Cqq3p_d0_LNP*SQDL(1,1) + Cqq3p_dd_LNP*SQDL(1,1)*SQDL(1,1) + 2*Cqq3p_u0_LNP*SQUL(1,1) + 2*Cqq3p_ud_LNP*SQDL(1,1)*SQUL(1,1) + Cqq3p_uu_LNP*SQUL(1,1)*SQUL(1,1)).real();
    Cqq3_2223r_LNP = (Cqq3_d0_LNP*SQDL(1,2) + Cqq3_dd_LNP*SQDL(1,1)*SQDL(1,2) + Cqq3_ud_LNP*SQDL(1,2)*SQUL(1,1) + Cqq3_u0_LNP*SQUL(1,2) + Cqq3_ud_LNP*SQDL(1,1)*SQUL(1,2) + Cqq3_uu_LNP*SQUL(1,1)*SQUL(1,2) + Cqq3p_d0_LNP*SQDL(1,2) + Cqq3p_dd_LNP*SQDL(1,1)*SQDL(1,2) + Cqq3p_ud_LNP*SQDL(1,2)*SQUL(1,1) + Cqq3p_u0_LNP*SQUL(1,2) + Cqq3p_ud_LNP*SQDL(1,1)*SQUL(1,2) + Cqq3p_uu_LNP*SQUL(1,1)*SQUL(1,2)).real();
    Cqq3_2223i_LNP = (Cqq3_d0_LNP*SQDL(1,2) + Cqq3_dd_LNP*SQDL(1,1)*SQDL(1,2) + Cqq3_ud_LNP*SQDL(1,2)*SQUL(1,1) + Cqq3_u0_LNP*SQUL(1,2) + Cqq3_ud_LNP*SQDL(1,1)*SQUL(1,2) + Cqq3_uu_LNP*SQUL(1,1)*SQUL(1,2) + Cqq3p_d0_LNP*SQDL(1,2) + Cqq3p_dd_LNP*SQDL(1,1)*SQDL(1,2) + Cqq3p_ud_LNP*SQDL(1,2)*SQUL(1,1) + Cqq3p_u0_LNP*SQUL(1,2) + Cqq3p_ud_LNP*SQDL(1,1)*SQUL(1,2) + Cqq3p_uu_LNP*SQUL(1,1)*SQUL(1,2)).imag();
    Cqq3_2233r_LNP = (Cqq3_00_LNP + Cqq3_d0_LNP*SQDL(1,1) + Cqq3_d0_LNP*SQDL(2,2) + Cqq3_dd_LNP*SQDL(1,1)*SQDL(2,2) + Cqq3_u0_LNP*SQUL(1,1) + Cqq3_ud_LNP*SQDL(2,2)*SQUL(1,1) + Cqq3_u0_LNP*SQUL(2,2) + Cqq3_ud_LNP*SQDL(1,1)*SQUL(2,2) + Cqq3_uu_LNP*SQUL(1,1)*SQUL(2,2) + Cqq3p_dd_LNP*SQDL(1,2)*SQDL(2,1) + Cqq3p_ud_LNP*SQDL(2,1)*SQUL(1,2) + Cqq3p_ud_LNP*SQDL(1,2)*SQUL(2,1) + Cqq3p_uu_LNP*SQUL(1,2)*SQUL(2,1)).real();
    Cqq3_2323r_LNP = (Cqq3_dd_LNP*SQDL(1,2)*SQDL(1,2) + 2*Cqq3_ud_LNP*SQDL(1,2)*SQUL(1,2) + Cqq3_uu_LNP*SQUL(1,2)*SQUL(1,2) + Cqq3p_dd_LNP*SQDL(1,2)*SQDL(1,2) + 2*Cqq3p_ud_LNP*SQDL(1,2)*SQUL(1,2) + Cqq3p_uu_LNP*SQUL(1,2)*SQUL(1,2)).real();
    Cqq3_2323i_LNP = (Cqq3_dd_LNP*SQDL(1,2)*SQDL(1,2) + 2*Cqq3_ud_LNP*SQDL(1,2)*SQUL(1,2) + Cqq3_uu_LNP*SQUL(1,2)*SQUL(1,2) + Cqq3p_dd_LNP*SQDL(1,2)*SQDL(1,2) + 2*Cqq3p_ud_LNP*SQDL(1,2)*SQUL(1,2) + Cqq3p_uu_LNP*SQUL(1,2)*SQUL(1,2)).imag();
    Cqq3_2332r_LNP = (Cqq3_dd_LNP*SQDL(1,2)*SQDL(2,1) + Cqq3_ud_LNP*SQDL(2,1)*SQUL(1,2) + Cqq3_ud_LNP*SQDL(1,2)*SQUL(2,1) + Cqq3_uu_LNP*SQUL(1,2)*SQUL(2,1) + Cqq3p_00_LNP + Cqq3p_d0_LNP*SQDL(1,1) + Cqq3p_d0_LNP*SQDL(2,2) + Cqq3p_dd_LNP*SQDL(1,1)*SQDL(2,2) + Cqq3p_u0_LNP*SQUL(1,1) + Cqq3p_ud_LNP*SQDL(2,2)*SQUL(1,1) + Cqq3p_u0_LNP*SQUL(2,2) + Cqq3p_ud_LNP*SQDL(1,1)*SQUL(2,2) + Cqq3p_uu_LNP*SQUL(1,1)*SQUL(2,2)).real();
    Cqq3_2333r_LNP = (Cqq3_d0_LNP*SQDL(1,2) + Cqq3_dd_LNP*SQDL(1,2)*SQDL(2,2) + Cqq3_u0_LNP*SQUL(1,2) + Cqq3_ud_LNP*SQDL(2,2)*SQUL(1,2) + Cqq3_ud_LNP*SQDL(1,2)*SQUL(2,2) + Cqq3_uu_LNP*SQUL(1,2)*SQUL(2,2) + Cqq3p_d0_LNP*SQDL(1,2) + Cqq3p_dd_LNP*SQDL(1,2)*SQDL(2,2) + Cqq3p_u0_LNP*SQUL(1,2) + Cqq3p_ud_LNP*SQDL(2,2)*SQUL(1,2) + Cqq3p_ud_LNP*SQDL(1,2)*SQUL(2,2) + Cqq3p_uu_LNP*SQUL(1,2)*SQUL(2,2)).real();
    Cqq3_2333i_LNP = (Cqq3_d0_LNP*SQDL(1,2) + Cqq3_dd_LNP*SQDL(1,2)*SQDL(2,2) + Cqq3_u0_LNP*SQUL(1,2) + Cqq3_ud_LNP*SQDL(2,2)*SQUL(1,2) + Cqq3_ud_LNP*SQDL(1,2)*SQUL(2,2) + Cqq3_uu_LNP*SQUL(1,2)*SQUL(2,2) + Cqq3p_d0_LNP*SQDL(1,2) + Cqq3p_dd_LNP*SQDL(1,2)*SQDL(2,2) + Cqq3p_u0_LNP*SQUL(1,2) + Cqq3p_ud_LNP*SQDL(2,2)*SQUL(1,2) + Cqq3p_ud_LNP*SQDL(1,2)*SQUL(2,2) + Cqq3p_uu_LNP*SQUL(1,2)*SQUL(2,2)).imag();
    Cqq3_3333r_LNP = (Cqq3_00_LNP + 2*Cqq3_d0_LNP*SQDL(2,2) + Cqq3_dd_LNP*SQDL(2,2)*SQDL(2,2) + 2*Cqq3_u0_LNP*SQUL(2,2) + 2*Cqq3_ud_LNP*SQDL(2,2)*SQUL(2,2) + Cqq3_uu_LNP*SQUL(2,2)*SQUL(2,2) + Cqq3p_00_LNP + 2*Cqq3p_d0_LNP*SQDL(2,2) + Cqq3p_dd_LNP*SQDL(2,2)*SQDL(2,2) + 2*Cqq3p_u0_LNP*SQUL(2,2) + 2*Cqq3p_ud_LNP*SQDL(2,2)*SQUL(2,2) + Cqq3p_uu_LNP*SQUL(2,2)*SQUL(2,2)).real();
 
    Cuu_1111r_LNP = (Cuu_00_LNP + 2*Cuu_u0_LNP*SUL(0,0) + Cuu_uu_LNP*SUL(0,0)*SUL(0,0) + Cuup_00_LNP + 2*Cuup_u0_LNP*SUL(0,0) + Cuup_uu_LNP*SUL(0,0)*SUL(0,0)).real();
    Cuu_1112r_LNP = (Cuu_u0_LNP*SUL(0,1) + Cuu_uu_LNP*SUL(0,0)*SUL(0,1) + Cuup_u0_LNP*SUL(0,1) + Cuup_uu_LNP*SUL(0,0)*SUL(0,1)).real();
    Cuu_1112i_LNP = (Cuu_u0_LNP*SUL(0,1) + Cuu_uu_LNP*SUL(0,0)*SUL(0,1) + Cuup_u0_LNP*SUL(0,1) + Cuup_uu_LNP*SUL(0,0)*SUL(0,1)).imag();
    Cuu_1113r_LNP = (Cuu_u0_LNP*SUL(0,2) + Cuu_uu_LNP*SUL(0,0)*SUL(0,2) + Cuup_u0_LNP*SUL(0,2) + Cuup_uu_LNP*SUL(0,0)*SUL(0,2)).real();
    Cuu_1113i_LNP = (Cuu_u0_LNP*SUL(0,2) + Cuu_uu_LNP*SUL(0,0)*SUL(0,2) + Cuup_u0_LNP*SUL(0,2) + Cuup_uu_LNP*SUL(0,0)*SUL(0,2)).imag();
    Cuu_1122r_LNP = (Cuu_00_LNP + Cuu_u0_LNP*SUL(0,0) + Cuu_u0_LNP*SUL(1,1) + Cuu_uu_LNP*SUL(0,0)*SUL(1,1) + Cuup_uu_LNP*SUL(0,1)*SUL(1,0)).real();
    Cuu_1123r_LNP = (Cuu_u0_LNP*SUL(1,2) + Cuu_uu_LNP*SUL(0,0)*SUL(1,2) + Cuup_uu_LNP*SUL(0,2)*SUL(1,0)).real();
    Cuu_1123i_LNP = (Cuu_u0_LNP*SUL(1,2) + Cuu_uu_LNP*SUL(0,0)*SUL(1,2) + Cuup_uu_LNP*SUL(0,2)*SUL(1,0)).imag();
    Cuu_1133r_LNP = (Cuu_00_LNP + Cuu_u0_LNP*SUL(0,0) + Cuu_u0_LNP*SUL(2,2) + Cuu_uu_LNP*SUL(0,0)*SUL(2,2) + Cuup_uu_LNP*SUL(0,2)*SUL(2,0)).real();
    Cuu_1212r_LNP = (Cuu_uu_LNP*SUL(0,1)*SUL(0,1) + Cuup_uu_LNP*SUL(0,1)*SUL(0,1)).real();
    Cuu_1212i_LNP = (Cuu_uu_LNP*SUL(0,1)*SUL(0,1) + Cuup_uu_LNP*SUL(0,1)*SUL(0,1)).imag();
    Cuu_1213r_LNP = (Cuu_uu_LNP*SUL(0,1)*SUL(0,2) + Cuup_uu_LNP*SUL(0,1)*SUL(0,2)).real();
    Cuu_1213i_LNP = (Cuu_uu_LNP*SUL(0,1)*SUL(0,2) + Cuup_uu_LNP*SUL(0,1)*SUL(0,2)).imag();
    Cuu_1221r_LNP = (Cuu_uu_LNP*SUL(0,1)*SUL(1,0) + Cuup_00_LNP + Cuup_u0_LNP*SUL(0,0) + Cuup_u0_LNP*SUL(1,1) + Cuup_uu_LNP*SUL(0,0)*SUL(1,1)).real();
    Cuu_1222r_LNP = (Cuu_u0_LNP*SUL(0,1) + Cuu_uu_LNP*SUL(0,1)*SUL(1,1) + Cuup_u0_LNP*SUL(0,1) + Cuup_uu_LNP*SUL(0,1)*SUL(1,1)).real();
    Cuu_1222i_LNP = (Cuu_u0_LNP*SUL(0,1) + Cuu_uu_LNP*SUL(0,1)*SUL(1,1) + Cuup_u0_LNP*SUL(0,1) + Cuup_uu_LNP*SUL(0,1)*SUL(1,1)).imag();
    Cuu_1223r_LNP = (Cuu_uu_LNP*SUL(0,1)*SUL(1,2) + Cuup_u0_LNP*SUL(0,2) + Cuup_uu_LNP*SUL(0,2)*SUL(1,1)).real();
    Cuu_1223i_LNP = (Cuu_uu_LNP*SUL(0,1)*SUL(1,2) + Cuup_u0_LNP*SUL(0,2) + Cuup_uu_LNP*SUL(0,2)*SUL(1,1)).imag();
    Cuu_1231r_LNP = (Cuu_uu_LNP*SUL(0,1)*SUL(2,0) + Cuup_u0_LNP*SUL(2,1) + Cuup_uu_LNP*SUL(0,0)*SUL(2,1)).real();
    Cuu_1231i_LNP = (Cuu_uu_LNP*SUL(0,1)*SUL(2,0) + Cuup_u0_LNP*SUL(2,1) + Cuup_uu_LNP*SUL(0,0)*SUL(2,1)).imag();
    Cuu_1232r_LNP = (Cuu_uu_LNP*SUL(0,1)*SUL(2,1) + Cuup_uu_LNP*SUL(0,1)*SUL(2,1)).real();
    Cuu_1232i_LNP = (Cuu_uu_LNP*SUL(0,1)*SUL(2,1) + Cuup_uu_LNP*SUL(0,1)*SUL(2,1)).imag();
    Cuu_1233r_LNP = (Cuu_u0_LNP*SUL(0,1) + Cuu_uu_LNP*SUL(0,1)*SUL(2,2) + Cuup_uu_LNP*SUL(0,2)*SUL(2,1)).real();
    Cuu_1233i_LNP = (Cuu_u0_LNP*SUL(0,1) + Cuu_uu_LNP*SUL(0,1)*SUL(2,2) + Cuup_uu_LNP*SUL(0,2)*SUL(2,1)).imag();
    Cuu_1313r_LNP = (Cuu_uu_LNP*SUL(0,2)*SUL(0,2) + Cuup_uu_LNP*SUL(0,2)*SUL(0,2)).real();
    Cuu_1313i_LNP = (Cuu_uu_LNP*SUL(0,2)*SUL(0,2) + Cuup_uu_LNP*SUL(0,2)*SUL(0,2)).imag();
    Cuu_1322r_LNP = (Cuu_u0_LNP*SUL(0,2) + Cuu_uu_LNP*SUL(0,2)*SUL(1,1) + Cuup_uu_LNP*SUL(0,1)*SUL(1,2)).real();
    Cuu_1322i_LNP = (Cuu_u0_LNP*SUL(0,2) + Cuu_uu_LNP*SUL(0,2)*SUL(1,1) + Cuup_uu_LNP*SUL(0,1)*SUL(1,2)).imag();
    Cuu_1323r_LNP = (Cuu_uu_LNP*SUL(0,2)*SUL(1,2) + Cuup_uu_LNP*SUL(0,2)*SUL(1,2)).real();
    Cuu_1323i_LNP = (Cuu_uu_LNP*SUL(0,2)*SUL(1,2) + Cuup_uu_LNP*SUL(0,2)*SUL(1,2)).imag();
    Cuu_1331r_LNP = (Cuu_uu_LNP*SUL(0,2)*SUL(2,0) + Cuup_00_LNP + Cuup_u0_LNP*SUL(0,0) + Cuup_u0_LNP*SUL(2,2) + Cuup_uu_LNP*SUL(0,0)*SUL(2,2)).real();
    Cuu_1332r_LNP = (Cuu_uu_LNP*SUL(0,2)*SUL(2,1) + Cuup_u0_LNP*SUL(0,1) + Cuup_uu_LNP*SUL(0,1)*SUL(2,2)).real();
    Cuu_1332i_LNP = (Cuu_uu_LNP*SUL(0,2)*SUL(2,1) + Cuup_u0_LNP*SUL(0,1) + Cuup_uu_LNP*SUL(0,1)*SUL(2,2)).imag();
    Cuu_1333r_LNP = (Cuu_u0_LNP*SUL(0,2) + Cuu_uu_LNP*SUL(0,2)*SUL(2,2) + Cuup_u0_LNP*SUL(0,2) + Cuup_uu_LNP*SUL(0,2)*SUL(2,2)).real();
    Cuu_1333i_LNP = (Cuu_u0_LNP*SUL(0,2) + Cuu_uu_LNP*SUL(0,2)*SUL(2,2) + Cuup_u0_LNP*SUL(0,2) + Cuup_uu_LNP*SUL(0,2)*SUL(2,2)).imag();
    Cuu_2222r_LNP = (Cuu_00_LNP + 2*Cuu_u0_LNP*SUL(1,1) + Cuu_uu_LNP*SUL(1,1)*SUL(1,1) + Cuup_00_LNP + 2*Cuup_u0_LNP*SUL(1,1) + Cuup_uu_LNP*SUL(1,1)*SUL(1,1)).real();
    Cuu_2223r_LNP = (Cuu_u0_LNP*SUL(1,2) + Cuu_uu_LNP*SUL(1,1)*SUL(1,2) + Cuup_u0_LNP*SUL(1,2) + Cuup_uu_LNP*SUL(1,1)*SUL(1,2)).real();
    Cuu_2223i_LNP = (Cuu_u0_LNP*SUL(1,2) + Cuu_uu_LNP*SUL(1,1)*SUL(1,2) + Cuup_u0_LNP*SUL(1,2) + Cuup_uu_LNP*SUL(1,1)*SUL(1,2)).imag();
    Cuu_2233r_LNP = (Cuu_00_LNP + Cuu_u0_LNP*SUL(1,1) + Cuu_u0_LNP*SUL(2,2) + Cuu_uu_LNP*SUL(1,1)*SUL(2,2) + Cuup_uu_LNP*SUL(1,2)*SUL(2,1)).real();
    Cuu_2323r_LNP = (Cuu_uu_LNP*SUL(1,2)*SUL(1,2) + Cuup_uu_LNP*SUL(1,2)*SUL(1,2)).real();
    Cuu_2323i_LNP = (Cuu_uu_LNP*SUL(1,2)*SUL(1,2) + Cuup_uu_LNP*SUL(1,2)*SUL(1,2)).imag();
    Cuu_2332r_LNP = (Cuu_uu_LNP*SUL(1,2)*SUL(2,1) + Cuup_00_LNP + Cuup_u0_LNP*SUL(1,1) + Cuup_u0_LNP*SUL(2,2) + Cuup_uu_LNP*SUL(1,1)*SUL(2,2)).real();
    Cuu_2333r_LNP = (Cuu_u0_LNP*SUL(1,2) + Cuu_uu_LNP*SUL(1,2)*SUL(2,2) + Cuup_u0_LNP*SUL(1,2) + Cuup_uu_LNP*SUL(1,2)*SUL(2,2)).real();
    Cuu_2333i_LNP = (Cuu_u0_LNP*SUL(1,2) + Cuu_uu_LNP*SUL(1,2)*SUL(2,2) + Cuup_u0_LNP*SUL(1,2) + Cuup_uu_LNP*SUL(1,2)*SUL(2,2)).imag();
    Cuu_3333r_LNP = (Cuu_00_LNP + 2*Cuu_u0_LNP*SUL(2,2) + Cuu_uu_LNP*SUL(2,2)*SUL(2,2) + Cuup_00_LNP + 2*Cuup_u0_LNP*SUL(2,2) + Cuup_uu_LNP*SUL(2,2)*SUL(2,2)).real();
 
    Cdd_1111r_LNP = (Cdd_00_LNP + 2*Cdd_d0_LNP*SDL(0,0) + Cdd_dd_LNP*SDL(0,0)*SDL(0,0) + Cddp_00_LNP + 2*Cddp_d0_LNP*SDL(0,0) + Cddp_dd_LNP*SDL(0,0)*SDL(0,0)).real();
    Cdd_1112r_LNP = (Cdd_d0_LNP*SDL(0,1) + Cdd_dd_LNP*SDL(0,0)*SDL(0,1) + Cddp_d0_LNP*SDL(0,1) + Cddp_dd_LNP*SDL(0,0)*SDL(0,1)).real();
    Cdd_1112i_LNP = (Cdd_d0_LNP*SDL(0,1) + Cdd_dd_LNP*SDL(0,0)*SDL(0,1) + Cddp_d0_LNP*SDL(0,1) + Cddp_dd_LNP*SDL(0,0)*SDL(0,1)).imag();
    Cdd_1113r_LNP = (Cdd_d0_LNP*SDL(0,2) + Cdd_dd_LNP*SDL(0,0)*SDL(0,2) + Cddp_d0_LNP*SDL(0,2) + Cddp_dd_LNP*SDL(0,0)*SDL(0,2)).real();
    Cdd_1113i_LNP = (Cdd_d0_LNP*SDL(0,2) + Cdd_dd_LNP*SDL(0,0)*SDL(0,2) + Cddp_d0_LNP*SDL(0,2) + Cddp_dd_LNP*SDL(0,0)*SDL(0,2)).imag();
    Cdd_1122r_LNP = (Cdd_00_LNP + Cdd_d0_LNP*SDL(0,0) + Cdd_d0_LNP*SDL(1,1) + Cdd_dd_LNP*SDL(0,0)*SDL(1,1) + Cddp_dd_LNP*SDL(0,1)*SDL(1,0)).real();
    Cdd_1123r_LNP = (Cdd_d0_LNP*SDL(1,2) + Cdd_dd_LNP*SDL(0,0)*SDL(1,2) + Cddp_dd_LNP*SDL(0,2)*SDL(1,0)).real();
    Cdd_1123i_LNP = (Cdd_d0_LNP*SDL(1,2) + Cdd_dd_LNP*SDL(0,0)*SDL(1,2) + Cddp_dd_LNP*SDL(0,2)*SDL(1,0)).imag();
    Cdd_1133r_LNP = (Cdd_00_LNP + Cdd_d0_LNP*SDL(0,0) + Cdd_d0_LNP*SDL(2,2) + Cdd_dd_LNP*SDL(0,0)*SDL(2,2) + Cddp_dd_LNP*SDL(0,2)*SDL(2,0)).real();
    Cdd_1212r_LNP = (Cdd_dd_LNP*SDL(0,1)*SDL(0,1) + Cddp_dd_LNP*SDL(0,1)*SDL(0,1)).real();
    Cdd_1212i_LNP = (Cdd_dd_LNP*SDL(0,1)*SDL(0,1) + Cddp_dd_LNP*SDL(0,1)*SDL(0,1)).imag();
    Cdd_1213r_LNP = (Cdd_dd_LNP*SDL(0,1)*SDL(0,2) + Cddp_dd_LNP*SDL(0,1)*SDL(0,2)).real();
    Cdd_1213i_LNP = (Cdd_dd_LNP*SDL(0,1)*SDL(0,2) + Cddp_dd_LNP*SDL(0,1)*SDL(0,2)).imag();
    Cdd_1221r_LNP = (Cdd_dd_LNP*SDL(0,1)*SDL(1,0) + Cddp_00_LNP + Cddp_d0_LNP*SDL(0,0) + Cddp_d0_LNP*SDL(1,1) + Cddp_dd_LNP*SDL(0,0)*SDL(1,1)).real();
    Cdd_1222r_LNP = (Cdd_d0_LNP*SDL(0,1) + Cdd_dd_LNP*SDL(0,1)*SDL(1,1) + Cddp_d0_LNP*SDL(0,1) + Cddp_dd_LNP*SDL(0,1)*SDL(1,1)).real();
    Cdd_1222i_LNP = (Cdd_d0_LNP*SDL(0,1) + Cdd_dd_LNP*SDL(0,1)*SDL(1,1) + Cddp_d0_LNP*SDL(0,1) + Cddp_dd_LNP*SDL(0,1)*SDL(1,1)).imag();
    Cdd_1223r_LNP = (Cdd_dd_LNP*SDL(0,1)*SDL(1,2) + Cddp_d0_LNP*SDL(0,2) + Cddp_dd_LNP*SDL(0,2)*SDL(1,1)).real();
    Cdd_1223i_LNP = (Cdd_dd_LNP*SDL(0,1)*SDL(1,2) + Cddp_d0_LNP*SDL(0,2) + Cddp_dd_LNP*SDL(0,2)*SDL(1,1)).imag();
    Cdd_1231r_LNP = (Cdd_dd_LNP*SDL(0,1)*SDL(2,0) + Cddp_d0_LNP*SDL(2,1) + Cddp_dd_LNP*SDL(0,0)*SDL(2,1)).real();
    Cdd_1231i_LNP = (Cdd_dd_LNP*SDL(0,1)*SDL(2,0) + Cddp_d0_LNP*SDL(2,1) + Cddp_dd_LNP*SDL(0,0)*SDL(2,1)).imag();
    Cdd_1232r_LNP = (Cdd_dd_LNP*SDL(0,1)*SDL(2,1) + Cddp_dd_LNP*SDL(0,1)*SDL(2,1)).real();
    Cdd_1232i_LNP = (Cdd_dd_LNP*SDL(0,1)*SDL(2,1) + Cddp_dd_LNP*SDL(0,1)*SDL(2,1)).imag();
    Cdd_1233r_LNP = (Cdd_d0_LNP*SDL(0,1) + Cdd_dd_LNP*SDL(0,1)*SDL(2,2) + Cddp_dd_LNP*SDL(0,2)*SDL(2,1)).real();
    Cdd_1233i_LNP = (Cdd_d0_LNP*SDL(0,1) + Cdd_dd_LNP*SDL(0,1)*SDL(2,2) + Cddp_dd_LNP*SDL(0,2)*SDL(2,1)).imag();
    Cdd_1313r_LNP = (Cdd_dd_LNP*SDL(0,2)*SDL(0,2) + Cddp_dd_LNP*SDL(0,2)*SDL(0,2)).real();
    Cdd_1313i_LNP = (Cdd_dd_LNP*SDL(0,2)*SDL(0,2) + Cddp_dd_LNP*SDL(0,2)*SDL(0,2)).imag();
    Cdd_1322r_LNP = (Cdd_d0_LNP*SDL(0,2) + Cdd_dd_LNP*SDL(0,2)*SDL(1,1) + Cddp_dd_LNP*SDL(0,1)*SDL(1,2)).real();
    Cdd_1322i_LNP = (Cdd_d0_LNP*SDL(0,2) + Cdd_dd_LNP*SDL(0,2)*SDL(1,1) + Cddp_dd_LNP*SDL(0,1)*SDL(1,2)).imag();
    Cdd_1323r_LNP = (Cdd_dd_LNP*SDL(0,2)*SDL(1,2) + Cddp_dd_LNP*SDL(0,2)*SDL(1,2)).real();
    Cdd_1323i_LNP = (Cdd_dd_LNP*SDL(0,2)*SDL(1,2) + Cddp_dd_LNP*SDL(0,2)*SDL(1,2)).imag();
    Cdd_1331r_LNP = (Cdd_dd_LNP*SDL(0,2)*SDL(2,0) + Cddp_00_LNP + Cddp_d0_LNP*SDL(0,0) + Cddp_d0_LNP*SDL(2,2) + Cddp_dd_LNP*SDL(0,0)*SDL(2,2)).real();
    Cdd_1332r_LNP = (Cdd_dd_LNP*SDL(0,2)*SDL(2,1) + Cddp_d0_LNP*SDL(0,1) + Cddp_dd_LNP*SDL(0,1)*SDL(2,2)).real();
    Cdd_1332i_LNP = (Cdd_dd_LNP*SDL(0,2)*SDL(2,1) + Cddp_d0_LNP*SDL(0,1) + Cddp_dd_LNP*SDL(0,1)*SDL(2,2)).imag();
    Cdd_1333r_LNP = (Cdd_d0_LNP*SDL(0,2) + Cdd_dd_LNP*SDL(0,2)*SDL(2,2) + Cddp_d0_LNP*SDL(0,2) + Cddp_dd_LNP*SDL(0,2)*SDL(2,2)).real();
    Cdd_1333i_LNP = (Cdd_d0_LNP*SDL(0,2) + Cdd_dd_LNP*SDL(0,2)*SDL(2,2) + Cddp_d0_LNP*SDL(0,2) + Cddp_dd_LNP*SDL(0,2)*SDL(2,2)).imag();
    Cdd_2222r_LNP = (Cdd_00_LNP + 2*Cdd_d0_LNP*SDL(1,1) + Cdd_dd_LNP*SDL(1,1)*SDL(1,1) + Cddp_00_LNP + 2*Cddp_d0_LNP*SDL(1,1) + Cddp_dd_LNP*SDL(1,1)*SDL(1,1)).real();
    Cdd_2223r_LNP = (Cdd_d0_LNP*SDL(1,2) + Cdd_dd_LNP*SDL(1,1)*SDL(1,2) + Cddp_d0_LNP*SDL(1,2) + Cddp_dd_LNP*SDL(1,1)*SDL(1,2)).real();
    Cdd_2223i_LNP = (Cdd_d0_LNP*SDL(1,2) + Cdd_dd_LNP*SDL(1,1)*SDL(1,2) + Cddp_d0_LNP*SDL(1,2) + Cddp_dd_LNP*SDL(1,1)*SDL(1,2)).imag();
    Cdd_2233r_LNP = (Cdd_00_LNP + Cdd_d0_LNP*SDL(1,1) + Cdd_d0_LNP*SDL(2,2) + Cdd_dd_LNP*SDL(1,1)*SDL(2,2) + Cddp_dd_LNP*SDL(1,2)*SDL(2,1)).real();
    Cdd_2323r_LNP = (Cdd_dd_LNP*SDL(1,2)*SDL(1,2) + Cddp_dd_LNP*SDL(1,2)*SDL(1,2)).real();
    Cdd_2323i_LNP = (Cdd_dd_LNP*SDL(1,2)*SDL(1,2) + Cddp_dd_LNP*SDL(1,2)*SDL(1,2)).imag();
    Cdd_2332r_LNP = (Cdd_dd_LNP*SDL(1,2)*SDL(2,1) + Cddp_00_LNP + Cddp_d0_LNP*SDL(1,1) + Cddp_d0_LNP*SDL(2,2) + Cddp_dd_LNP*SDL(1,1)*SDL(2,2)).real();
    Cdd_2333r_LNP = (Cdd_d0_LNP*SDL(1,2) + Cdd_dd_LNP*SDL(1,2)*SDL(2,2) + Cddp_d0_LNP*SDL(1,2) + Cddp_dd_LNP*SDL(1,2)*SDL(2,2)).real();
    Cdd_2333i_LNP = (Cdd_d0_LNP*SDL(1,2) + Cdd_dd_LNP*SDL(1,2)*SDL(2,2) + Cddp_d0_LNP*SDL(1,2) + Cddp_dd_LNP*SDL(1,2)*SDL(2,2)).imag();
    Cdd_3333r_LNP = (Cdd_00_LNP + 2*Cdd_d0_LNP*SDL(2,2) + Cdd_dd_LNP*SDL(2,2)*SDL(2,2) + Cddp_00_LNP + 2*Cddp_d0_LNP*SDL(2,2) + Cddp_dd_LNP*SDL(2,2)*SDL(2,2)).real();
 
    Cud1_1111r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*SDL(0,0) + Cud1p_ud_LNP*SUDcL(0,0)*SUDL(0,0) + Cud1_u0_LNP*SUL(0,0) + Cud1_ud_LNP*SDL(0,0)*SUL(0,0)).real();
    Cud1_1112r_LNP = (Cud1_0d_LNP*SDL(0,1) + Cud1p_ud_LNP*SUDcL(0,0)*SUDL(0,1) + Cud1_ud_LNP*SDL(0,1)*SUL(0,0)).real();
    Cud1_1112i_LNP = (Cud1_0d_LNP*SDL(0,1) + Cud1p_ud_LNP*SUDcL(0,0)*SUDL(0,1) + Cud1_ud_LNP*SDL(0,1)*SUL(0,0)).imag();
    Cud1_1113r_LNP = (Cud1_0d_LNP*SDL(0,2) + Cud1p_ud_LNP*SUDcL(0,0)*SUDL(0,2) + Cud1_ud_LNP*SDL(0,2)*SUL(0,0)).real();
    Cud1_1113i_LNP = (Cud1_0d_LNP*SDL(0,2) + Cud1p_ud_LNP*SUDcL(0,0)*SUDL(0,2) + Cud1_ud_LNP*SDL(0,2)*SUL(0,0)).imag();
    Cud1_1122r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*SDL(1,1) + Cud1p_ud_LNP*SUDcL(1,0)*SUDL(0,1) + Cud1_u0_LNP*SUL(0,0) + Cud1_ud_LNP*SDL(1,1)*SUL(0,0)).real();
    Cud1_1123r_LNP = (Cud1_0d_LNP*SDL(1,2) + Cud1p_ud_LNP*SUDcL(1,0)*SUDL(0,2) + Cud1_ud_LNP*SDL(1,2)*SUL(0,0)).real();
    Cud1_1123i_LNP = (Cud1_0d_LNP*SDL(1,2) + Cud1p_ud_LNP*SUDcL(1,0)*SUDL(0,2) + Cud1_ud_LNP*SDL(1,2)*SUL(0,0)).imag();
    Cud1_1133r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*SDL(2,2) + Cud1p_ud_LNP*SUDcL(2,0)*SUDL(0,2) + Cud1_u0_LNP*SUL(0,0) + Cud1_ud_LNP*SDL(2,2)*SUL(0,0)).real();
    Cud1_1211r_LNP = (Cud1p_ud_LNP*SUDcL(0,1)*SUDL(0,0) + Cud1_u0_LNP*SUL(0,1) + Cud1_ud_LNP*SDL(0,0)*SUL(0,1)).real();
    Cud1_1211i_LNP = (Cud1p_ud_LNP*SUDcL(0,1)*SUDL(0,0) + Cud1_u0_LNP*SUL(0,1) + Cud1_ud_LNP*SDL(0,0)*SUL(0,1)).imag();
    Cud1_1212r_LNP = (Cud1p_ud_LNP*SUDcL(0,1)*SUDL(0,1) + Cud1_ud_LNP*SDL(0,1)*SUL(0,1)).real();
    Cud1_1212i_LNP = (Cud1p_ud_LNP*SUDcL(0,1)*SUDL(0,1) + Cud1_ud_LNP*SDL(0,1)*SUL(0,1)).imag();
    Cud1_1213r_LNP = (Cud1p_ud_LNP*SUDcL(0,1)*SUDL(0,2) + Cud1_ud_LNP*SDL(0,2)*SUL(0,1)).real();
    Cud1_1213i_LNP = (Cud1p_ud_LNP*SUDcL(0,1)*SUDL(0,2) + Cud1_ud_LNP*SDL(0,2)*SUL(0,1)).imag();
    Cud1_1221r_LNP = (Cud1p_ud_LNP*SUDcL(1,1)*SUDL(0,0) + Cud1_ud_LNP*SDL(1,0)*SUL(0,1)).real();
    Cud1_1221i_LNP = (Cud1p_ud_LNP*SUDcL(1,1)*SUDL(0,0) + Cud1_ud_LNP*SDL(1,0)*SUL(0,1)).imag();
    Cud1_1222r_LNP = (Cud1p_ud_LNP*SUDcL(1,1)*SUDL(0,1) + Cud1_u0_LNP*SUL(0,1) + Cud1_ud_LNP*SDL(1,1)*SUL(0,1)).real();
    Cud1_1222i_LNP = (Cud1p_ud_LNP*SUDcL(1,1)*SUDL(0,1) + Cud1_u0_LNP*SUL(0,1) + Cud1_ud_LNP*SDL(1,1)*SUL(0,1)).imag();
    Cud1_1223r_LNP = (Cud1p_ud_LNP*SUDcL(1,1)*SUDL(0,2) + Cud1_ud_LNP*SDL(1,2)*SUL(0,1)).real();
    Cud1_1223i_LNP = (Cud1p_ud_LNP*SUDcL(1,1)*SUDL(0,2) + Cud1_ud_LNP*SDL(1,2)*SUL(0,1)).imag();
    Cud1_1231r_LNP = (Cud1p_ud_LNP*SUDcL(2,1)*SUDL(0,0) + Cud1_ud_LNP*SDL(2,0)*SUL(0,1)).real();
    Cud1_1231i_LNP = (Cud1p_ud_LNP*SUDcL(2,1)*SUDL(0,0) + Cud1_ud_LNP*SDL(2,0)*SUL(0,1)).imag();
    Cud1_1232r_LNP = (Cud1p_ud_LNP*SUDcL(2,1)*SUDL(0,1) + Cud1_ud_LNP*SDL(2,1)*SUL(0,1)).real();
    Cud1_1232i_LNP = (Cud1p_ud_LNP*SUDcL(2,1)*SUDL(0,1) + Cud1_ud_LNP*SDL(2,1)*SUL(0,1)).imag();
    Cud1_1233r_LNP = (Cud1p_ud_LNP*SUDcL(2,1)*SUDL(0,2) + Cud1_u0_LNP*SUL(0,1) + Cud1_ud_LNP*SDL(2,2)*SUL(0,1)).real();
    Cud1_1233i_LNP = (Cud1p_ud_LNP*SUDcL(2,1)*SUDL(0,2) + Cud1_u0_LNP*SUL(0,1) + Cud1_ud_LNP*SDL(2,2)*SUL(0,1)).imag();
    Cud1_1311r_LNP = (Cud1p_ud_LNP*SUDcL(0,2)*SUDL(0,0) + Cud1_u0_LNP*SUL(0,2) + Cud1_ud_LNP*SDL(0,0)*SUL(0,2)).real();
    Cud1_1311i_LNP = (Cud1p_ud_LNP*SUDcL(0,2)*SUDL(0,0) + Cud1_u0_LNP*SUL(0,2) + Cud1_ud_LNP*SDL(0,0)*SUL(0,2)).imag();
    Cud1_1312r_LNP = (Cud1p_ud_LNP*SUDcL(0,2)*SUDL(0,1) + Cud1_ud_LNP*SDL(0,1)*SUL(0,2)).real();
    Cud1_1312i_LNP = (Cud1p_ud_LNP*SUDcL(0,2)*SUDL(0,1) + Cud1_ud_LNP*SDL(0,1)*SUL(0,2)).imag();
    Cud1_1313r_LNP = (Cud1p_ud_LNP*SUDcL(0,2)*SUDL(0,2) + Cud1_ud_LNP*SDL(0,2)*SUL(0,2)).real();
    Cud1_1313i_LNP = (Cud1p_ud_LNP*SUDcL(0,2)*SUDL(0,2) + Cud1_ud_LNP*SDL(0,2)*SUL(0,2)).imag();
    Cud1_1321r_LNP = (Cud1p_ud_LNP*SUDcL(1,2)*SUDL(0,0) + Cud1_ud_LNP*SDL(1,0)*SUL(0,2)).real();
    Cud1_1321i_LNP = (Cud1p_ud_LNP*SUDcL(1,2)*SUDL(0,0) + Cud1_ud_LNP*SDL(1,0)*SUL(0,2)).imag();
    Cud1_1322r_LNP = (Cud1p_ud_LNP*SUDcL(1,2)*SUDL(0,1) + Cud1_u0_LNP*SUL(0,2) + Cud1_ud_LNP*SDL(1,1)*SUL(0,2)).real();
    Cud1_1322i_LNP = (Cud1p_ud_LNP*SUDcL(1,2)*SUDL(0,1) + Cud1_u0_LNP*SUL(0,2) + Cud1_ud_LNP*SDL(1,1)*SUL(0,2)).imag();
    Cud1_1323r_LNP = (Cud1p_ud_LNP*SUDcL(1,2)*SUDL(0,2) + Cud1_ud_LNP*SDL(1,2)*SUL(0,2)).real();
    Cud1_1323i_LNP = (Cud1p_ud_LNP*SUDcL(1,2)*SUDL(0,2) + Cud1_ud_LNP*SDL(1,2)*SUL(0,2)).imag();
    Cud1_1331r_LNP = (Cud1p_ud_LNP*SUDcL(2,2)*SUDL(0,0) + Cud1_ud_LNP*SDL(2,0)*SUL(0,2)).real();
    Cud1_1331i_LNP = (Cud1p_ud_LNP*SUDcL(2,2)*SUDL(0,0) + Cud1_ud_LNP*SDL(2,0)*SUL(0,2)).imag();
    Cud1_1332r_LNP = (Cud1p_ud_LNP*SUDcL(2,2)*SUDL(0,1) + Cud1_ud_LNP*SDL(2,1)*SUL(0,2)).real();
    Cud1_1332i_LNP = (Cud1p_ud_LNP*SUDcL(2,2)*SUDL(0,1) + Cud1_ud_LNP*SDL(2,1)*SUL(0,2)).imag();
    Cud1_1333r_LNP = (Cud1p_ud_LNP*SUDcL(2,2)*SUDL(0,2) + Cud1_u0_LNP*SUL(0,2) + Cud1_ud_LNP*SDL(2,2)*SUL(0,2)).real();
    Cud1_1333i_LNP = (Cud1p_ud_LNP*SUDcL(2,2)*SUDL(0,2) + Cud1_u0_LNP*SUL(0,2) + Cud1_ud_LNP*SDL(2,2)*SUL(0,2)).imag();
    Cud1_2211r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*SDL(0,0) + Cud1p_ud_LNP*SUDcL(0,1)*SUDL(1,0) + Cud1_u0_LNP*SUL(1,1) + Cud1_ud_LNP*SDL(0,0)*SUL(1,1)).real();
    Cud1_2212r_LNP = (Cud1_0d_LNP*SDL(0,1) + Cud1p_ud_LNP*SUDcL(0,1)*SUDL(1,1) + Cud1_ud_LNP*SDL(0,1)*SUL(1,1)).real();
    Cud1_2212i_LNP = (Cud1_0d_LNP*SDL(0,1) + Cud1p_ud_LNP*SUDcL(0,1)*SUDL(1,1) + Cud1_ud_LNP*SDL(0,1)*SUL(1,1)).imag();
    Cud1_2213r_LNP = (Cud1_0d_LNP*SDL(0,2) + Cud1p_ud_LNP*SUDcL(0,1)*SUDL(1,2) + Cud1_ud_LNP*SDL(0,2)*SUL(1,1)).real();
    Cud1_2213i_LNP = (Cud1_0d_LNP*SDL(0,2) + Cud1p_ud_LNP*SUDcL(0,1)*SUDL(1,2) + Cud1_ud_LNP*SDL(0,2)*SUL(1,1)).imag();
    Cud1_2222r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*SDL(1,1) + Cud1p_ud_LNP*SUDcL(1,1)*SUDL(1,1) + Cud1_u0_LNP*SUL(1,1) + Cud1_ud_LNP*SDL(1,1)*SUL(1,1)).real();
    Cud1_2223r_LNP = (Cud1_0d_LNP*SDL(1,2) + Cud1p_ud_LNP*SUDcL(1,1)*SUDL(1,2) + Cud1_ud_LNP*SDL(1,2)*SUL(1,1)).real();
    Cud1_2223i_LNP = (Cud1_0d_LNP*SDL(1,2) + Cud1p_ud_LNP*SUDcL(1,1)*SUDL(1,2) + Cud1_ud_LNP*SDL(1,2)*SUL(1,1)).imag();
    Cud1_2233r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*SDL(2,2) + Cud1p_ud_LNP*SUDcL(2,1)*SUDL(1,2) + Cud1_u0_LNP*SUL(1,1) + Cud1_ud_LNP*SDL(2,2)*SUL(1,1)).real();
    Cud1_2311r_LNP = (Cud1p_ud_LNP*SUDcL(0,2)*SUDL(1,0) + Cud1_u0_LNP*SUL(1,2) + Cud1_ud_LNP*SDL(0,0)*SUL(1,2)).real();
    Cud1_2311i_LNP = (Cud1p_ud_LNP*SUDcL(0,2)*SUDL(1,0) + Cud1_u0_LNP*SUL(1,2) + Cud1_ud_LNP*SDL(0,0)*SUL(1,2)).imag();
    Cud1_2312r_LNP = (Cud1p_ud_LNP*SUDcL(0,2)*SUDL(1,1) + Cud1_ud_LNP*SDL(0,1)*SUL(1,2)).real();
    Cud1_2312i_LNP = (Cud1p_ud_LNP*SUDcL(0,2)*SUDL(1,1) + Cud1_ud_LNP*SDL(0,1)*SUL(1,2)).imag();
    Cud1_2313r_LNP = (Cud1p_ud_LNP*SUDcL(0,2)*SUDL(1,2) + Cud1_ud_LNP*SDL(0,2)*SUL(1,2)).real();
    Cud1_2313i_LNP = (Cud1p_ud_LNP*SUDcL(0,2)*SUDL(1,2) + Cud1_ud_LNP*SDL(0,2)*SUL(1,2)).imag();
    Cud1_2321r_LNP = (Cud1p_ud_LNP*SUDcL(1,2)*SUDL(1,0) + Cud1_ud_LNP*SDL(1,0)*SUL(1,2)).real();
    Cud1_2321i_LNP = (Cud1p_ud_LNP*SUDcL(1,2)*SUDL(1,0) + Cud1_ud_LNP*SDL(1,0)*SUL(1,2)).imag();
    Cud1_2322r_LNP = (Cud1p_ud_LNP*SUDcL(1,2)*SUDL(1,1) + Cud1_u0_LNP*SUL(1,2) + Cud1_ud_LNP*SDL(1,1)*SUL(1,2)).real();
    Cud1_2322i_LNP = (Cud1p_ud_LNP*SUDcL(1,2)*SUDL(1,1) + Cud1_u0_LNP*SUL(1,2) + Cud1_ud_LNP*SDL(1,1)*SUL(1,2)).imag();
    Cud1_2323r_LNP = (Cud1p_ud_LNP*SUDcL(1,2)*SUDL(1,2) + Cud1_ud_LNP*SDL(1,2)*SUL(1,2)).real();
    Cud1_2323i_LNP = (Cud1p_ud_LNP*SUDcL(1,2)*SUDL(1,2) + Cud1_ud_LNP*SDL(1,2)*SUL(1,2)).imag();
    Cud1_2331r_LNP = (Cud1p_ud_LNP*SUDcL(2,2)*SUDL(1,0) + Cud1_ud_LNP*SDL(2,0)*SUL(1,2)).real();
    Cud1_2331i_LNP = (Cud1p_ud_LNP*SUDcL(2,2)*SUDL(1,0) + Cud1_ud_LNP*SDL(2,0)*SUL(1,2)).imag();
    Cud1_2332r_LNP = (Cud1p_ud_LNP*SUDcL(2,2)*SUDL(1,1) + Cud1_ud_LNP*SDL(2,1)*SUL(1,2)).real();
    Cud1_2332i_LNP = (Cud1p_ud_LNP*SUDcL(2,2)*SUDL(1,1) + Cud1_ud_LNP*SDL(2,1)*SUL(1,2)).imag();
    Cud1_2333r_LNP = (Cud1p_ud_LNP*SUDcL(2,2)*SUDL(1,2) + Cud1_u0_LNP*SUL(1,2) + Cud1_ud_LNP*SDL(2,2)*SUL(1,2)).real();
    Cud1_2333i_LNP = (Cud1p_ud_LNP*SUDcL(2,2)*SUDL(1,2) + Cud1_u0_LNP*SUL(1,2) + Cud1_ud_LNP*SDL(2,2)*SUL(1,2)).imag();
    Cud1_3311r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*SDL(0,0) + Cud1p_ud_LNP*SUDcL(0,2)*SUDL(2,0) + Cud1_u0_LNP*SUL(2,2) + Cud1_ud_LNP*SDL(0,0)*SUL(2,2)).real();
    Cud1_3312r_LNP = (Cud1_0d_LNP*SDL(0,1) + Cud1p_ud_LNP*SUDcL(0,2)*SUDL(2,1) + Cud1_ud_LNP*SDL(0,1)*SUL(2,2)).real();
    Cud1_3312i_LNP = (Cud1_0d_LNP*SDL(0,1) + Cud1p_ud_LNP*SUDcL(0,2)*SUDL(2,1) + Cud1_ud_LNP*SDL(0,1)*SUL(2,2)).imag();
    Cud1_3313r_LNP = (Cud1_0d_LNP*SDL(0,2) + Cud1p_ud_LNP*SUDcL(0,2)*SUDL(2,2) + Cud1_ud_LNP*SDL(0,2)*SUL(2,2)).real();
    Cud1_3313i_LNP = (Cud1_0d_LNP*SDL(0,2) + Cud1p_ud_LNP*SUDcL(0,2)*SUDL(2,2) + Cud1_ud_LNP*SDL(0,2)*SUL(2,2)).imag();
    Cud1_3322r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*SDL(1,1) + Cud1p_ud_LNP*SUDcL(1,2)*SUDL(2,1) + Cud1_u0_LNP*SUL(2,2) + Cud1_ud_LNP*SDL(1,1)*SUL(2,2)).real();
    Cud1_3323r_LNP = (Cud1_0d_LNP*SDL(1,2) + Cud1p_ud_LNP*SUDcL(1,2)*SUDL(2,2) + Cud1_ud_LNP*SDL(1,2)*SUL(2,2)).real();
    Cud1_3323i_LNP = (Cud1_0d_LNP*SDL(1,2) + Cud1p_ud_LNP*SUDcL(1,2)*SUDL(2,2) + Cud1_ud_LNP*SDL(1,2)*SUL(2,2)).imag();
    Cud1_3333r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*SDL(2,2) + Cud1p_ud_LNP*SUDcL(2,2)*SUDL(2,2) + Cud1_u0_LNP*SUL(2,2) + Cud1_ud_LNP*SDL(2,2)*SUL(2,2)).real();
 
    Cud8_1111r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*SDL(0,0) + Cud8p_ud_LNP*SUDcL(0,0)*SUDL(0,0) + Cud8_u0_LNP*SUL(0,0) + Cud8_ud_LNP*SDL(0,0)*SUL(0,0)).real();
    Cud8_1112r_LNP = (Cud8_0d_LNP*SDL(0,1) + Cud8p_ud_LNP*SUDcL(0,0)*SUDL(0,1) + Cud8_ud_LNP*SDL(0,1)*SUL(0,0)).real();
    Cud8_1112i_LNP = (Cud8_0d_LNP*SDL(0,1) + Cud8p_ud_LNP*SUDcL(0,0)*SUDL(0,1) + Cud8_ud_LNP*SDL(0,1)*SUL(0,0)).imag();
    Cud8_1113r_LNP = (Cud8_0d_LNP*SDL(0,2) + Cud8p_ud_LNP*SUDcL(0,0)*SUDL(0,2) + Cud8_ud_LNP*SDL(0,2)*SUL(0,0)).real();
    Cud8_1113i_LNP = (Cud8_0d_LNP*SDL(0,2) + Cud8p_ud_LNP*SUDcL(0,0)*SUDL(0,2) + Cud8_ud_LNP*SDL(0,2)*SUL(0,0)).imag();
    Cud8_1122r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*SDL(1,1) + Cud8p_ud_LNP*SUDcL(1,0)*SUDL(0,1) + Cud8_u0_LNP*SUL(0,0) + Cud8_ud_LNP*SDL(1,1)*SUL(0,0)).real();
    Cud8_1123r_LNP = (Cud8_0d_LNP*SDL(1,2) + Cud8p_ud_LNP*SUDcL(1,0)*SUDL(0,2) + Cud8_ud_LNP*SDL(1,2)*SUL(0,0)).real();
    Cud8_1123i_LNP = (Cud8_0d_LNP*SDL(1,2) + Cud8p_ud_LNP*SUDcL(1,0)*SUDL(0,2) + Cud8_ud_LNP*SDL(1,2)*SUL(0,0)).imag();
    Cud8_1133r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*SDL(2,2) + Cud8p_ud_LNP*SUDcL(2,0)*SUDL(0,2) + Cud8_u0_LNP*SUL(0,0) + Cud8_ud_LNP*SDL(2,2)*SUL(0,0)).real();
    Cud8_1211r_LNP = (Cud8p_ud_LNP*SUDcL(0,1)*SUDL(0,0) + Cud8_u0_LNP*SUL(0,1) + Cud8_ud_LNP*SDL(0,0)*SUL(0,1)).real();
    Cud8_1211i_LNP = (Cud8p_ud_LNP*SUDcL(0,1)*SUDL(0,0) + Cud8_u0_LNP*SUL(0,1) + Cud8_ud_LNP*SDL(0,0)*SUL(0,1)).imag();
    Cud8_1212r_LNP = (Cud8p_ud_LNP*SUDcL(0,1)*SUDL(0,1) + Cud8_ud_LNP*SDL(0,1)*SUL(0,1)).real();
    Cud8_1212i_LNP = (Cud8p_ud_LNP*SUDcL(0,1)*SUDL(0,1) + Cud8_ud_LNP*SDL(0,1)*SUL(0,1)).imag();
    Cud8_1213r_LNP = (Cud8p_ud_LNP*SUDcL(0,1)*SUDL(0,2) + Cud8_ud_LNP*SDL(0,2)*SUL(0,1)).real();
    Cud8_1213i_LNP = (Cud8p_ud_LNP*SUDcL(0,1)*SUDL(0,2) + Cud8_ud_LNP*SDL(0,2)*SUL(0,1)).imag();
    Cud8_1221r_LNP = (Cud8p_ud_LNP*SUDcL(1,1)*SUDL(0,0) + Cud8_ud_LNP*SDL(1,0)*SUL(0,1)).real();
    Cud8_1221i_LNP = (Cud8p_ud_LNP*SUDcL(1,1)*SUDL(0,0) + Cud8_ud_LNP*SDL(1,0)*SUL(0,1)).imag();
    Cud8_1222r_LNP = (Cud8p_ud_LNP*SUDcL(1,1)*SUDL(0,1) + Cud8_u0_LNP*SUL(0,1) + Cud8_ud_LNP*SDL(1,1)*SUL(0,1)).real();
    Cud8_1222i_LNP = (Cud8p_ud_LNP*SUDcL(1,1)*SUDL(0,1) + Cud8_u0_LNP*SUL(0,1) + Cud8_ud_LNP*SDL(1,1)*SUL(0,1)).imag();
    Cud8_1223r_LNP = (Cud8p_ud_LNP*SUDcL(1,1)*SUDL(0,2) + Cud8_ud_LNP*SDL(1,2)*SUL(0,1)).real();
    Cud8_1223i_LNP = (Cud8p_ud_LNP*SUDcL(1,1)*SUDL(0,2) + Cud8_ud_LNP*SDL(1,2)*SUL(0,1)).imag();
    Cud8_1231r_LNP = (Cud8p_ud_LNP*SUDcL(2,1)*SUDL(0,0) + Cud8_ud_LNP*SDL(2,0)*SUL(0,1)).real();
    Cud8_1231i_LNP = (Cud8p_ud_LNP*SUDcL(2,1)*SUDL(0,0) + Cud8_ud_LNP*SDL(2,0)*SUL(0,1)).imag();
    Cud8_1232r_LNP = (Cud8p_ud_LNP*SUDcL(2,1)*SUDL(0,1) + Cud8_ud_LNP*SDL(2,1)*SUL(0,1)).real();
    Cud8_1232i_LNP = (Cud8p_ud_LNP*SUDcL(2,1)*SUDL(0,1) + Cud8_ud_LNP*SDL(2,1)*SUL(0,1)).imag();
    Cud8_1233r_LNP = (Cud8p_ud_LNP*SUDcL(2,1)*SUDL(0,2) + Cud8_u0_LNP*SUL(0,1) + Cud8_ud_LNP*SDL(2,2)*SUL(0,1)).real();
    Cud8_1233i_LNP = (Cud8p_ud_LNP*SUDcL(2,1)*SUDL(0,2) + Cud8_u0_LNP*SUL(0,1) + Cud8_ud_LNP*SDL(2,2)*SUL(0,1)).imag();
    Cud8_1311r_LNP = (Cud8p_ud_LNP*SUDcL(0,2)*SUDL(0,0) + Cud8_u0_LNP*SUL(0,2) + Cud8_ud_LNP*SDL(0,0)*SUL(0,2)).real();
    Cud8_1311i_LNP = (Cud8p_ud_LNP*SUDcL(0,2)*SUDL(0,0) + Cud8_u0_LNP*SUL(0,2) + Cud8_ud_LNP*SDL(0,0)*SUL(0,2)).imag();
    Cud8_1312r_LNP = (Cud8p_ud_LNP*SUDcL(0,2)*SUDL(0,1) + Cud8_ud_LNP*SDL(0,1)*SUL(0,2)).real();
    Cud8_1312i_LNP = (Cud8p_ud_LNP*SUDcL(0,2)*SUDL(0,1) + Cud8_ud_LNP*SDL(0,1)*SUL(0,2)).imag();
    Cud8_1313r_LNP = (Cud8p_ud_LNP*SUDcL(0,2)*SUDL(0,2) + Cud8_ud_LNP*SDL(0,2)*SUL(0,2)).real();
    Cud8_1313i_LNP = (Cud8p_ud_LNP*SUDcL(0,2)*SUDL(0,2) + Cud8_ud_LNP*SDL(0,2)*SUL(0,2)).imag();
    Cud8_1321r_LNP = (Cud8p_ud_LNP*SUDcL(1,2)*SUDL(0,0) + Cud8_ud_LNP*SDL(1,0)*SUL(0,2)).real();
    Cud8_1321i_LNP = (Cud8p_ud_LNP*SUDcL(1,2)*SUDL(0,0) + Cud8_ud_LNP*SDL(1,0)*SUL(0,2)).imag();
    Cud8_1322r_LNP = (Cud8p_ud_LNP*SUDcL(1,2)*SUDL(0,1) + Cud8_u0_LNP*SUL(0,2) + Cud8_ud_LNP*SDL(1,1)*SUL(0,2)).real();
    Cud8_1322i_LNP = (Cud8p_ud_LNP*SUDcL(1,2)*SUDL(0,1) + Cud8_u0_LNP*SUL(0,2) + Cud8_ud_LNP*SDL(1,1)*SUL(0,2)).imag();
    Cud8_1323r_LNP = (Cud8p_ud_LNP*SUDcL(1,2)*SUDL(0,2) + Cud8_ud_LNP*SDL(1,2)*SUL(0,2)).real();
    Cud8_1323i_LNP = (Cud8p_ud_LNP*SUDcL(1,2)*SUDL(0,2) + Cud8_ud_LNP*SDL(1,2)*SUL(0,2)).imag();
    Cud8_1331r_LNP = (Cud8p_ud_LNP*SUDcL(2,2)*SUDL(0,0) + Cud8_ud_LNP*SDL(2,0)*SUL(0,2)).real();
    Cud8_1331i_LNP = (Cud8p_ud_LNP*SUDcL(2,2)*SUDL(0,0) + Cud8_ud_LNP*SDL(2,0)*SUL(0,2)).imag();
    Cud8_1332r_LNP = (Cud8p_ud_LNP*SUDcL(2,2)*SUDL(0,1) + Cud8_ud_LNP*SDL(2,1)*SUL(0,2)).real();
    Cud8_1332i_LNP = (Cud8p_ud_LNP*SUDcL(2,2)*SUDL(0,1) + Cud8_ud_LNP*SDL(2,1)*SUL(0,2)).imag();
    Cud8_1333r_LNP = (Cud8p_ud_LNP*SUDcL(2,2)*SUDL(0,2) + Cud8_u0_LNP*SUL(0,2) + Cud8_ud_LNP*SDL(2,2)*SUL(0,2)).real();
    Cud8_1333i_LNP = (Cud8p_ud_LNP*SUDcL(2,2)*SUDL(0,2) + Cud8_u0_LNP*SUL(0,2) + Cud8_ud_LNP*SDL(2,2)*SUL(0,2)).imag();
    Cud8_2211r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*SDL(0,0) + Cud8p_ud_LNP*SUDcL(0,1)*SUDL(1,0) + Cud8_u0_LNP*SUL(1,1) + Cud8_ud_LNP*SDL(0,0)*SUL(1,1)).real();
    Cud8_2212r_LNP = (Cud8_0d_LNP*SDL(0,1) + Cud8p_ud_LNP*SUDcL(0,1)*SUDL(1,1) + Cud8_ud_LNP*SDL(0,1)*SUL(1,1)).real();
    Cud8_2212i_LNP = (Cud8_0d_LNP*SDL(0,1) + Cud8p_ud_LNP*SUDcL(0,1)*SUDL(1,1) + Cud8_ud_LNP*SDL(0,1)*SUL(1,1)).imag();
    Cud8_2213r_LNP = (Cud8_0d_LNP*SDL(0,2) + Cud8p_ud_LNP*SUDcL(0,1)*SUDL(1,2) + Cud8_ud_LNP*SDL(0,2)*SUL(1,1)).real();
    Cud8_2213i_LNP = (Cud8_0d_LNP*SDL(0,2) + Cud8p_ud_LNP*SUDcL(0,1)*SUDL(1,2) + Cud8_ud_LNP*SDL(0,2)*SUL(1,1)).imag();
    Cud8_2222r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*SDL(1,1) + Cud8p_ud_LNP*SUDcL(1,1)*SUDL(1,1) + Cud8_u0_LNP*SUL(1,1) + Cud8_ud_LNP*SDL(1,1)*SUL(1,1)).real();
    Cud8_2223r_LNP = (Cud8_0d_LNP*SDL(1,2) + Cud8p_ud_LNP*SUDcL(1,1)*SUDL(1,2) + Cud8_ud_LNP*SDL(1,2)*SUL(1,1)).real();
    Cud8_2223i_LNP = (Cud8_0d_LNP*SDL(1,2) + Cud8p_ud_LNP*SUDcL(1,1)*SUDL(1,2) + Cud8_ud_LNP*SDL(1,2)*SUL(1,1)).imag();
    Cud8_2233r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*SDL(2,2) + Cud8p_ud_LNP*SUDcL(2,1)*SUDL(1,2) + Cud8_u0_LNP*SUL(1,1) + Cud8_ud_LNP*SDL(2,2)*SUL(1,1)).real();
    Cud8_2311r_LNP = (Cud8p_ud_LNP*SUDcL(0,2)*SUDL(1,0) + Cud8_u0_LNP*SUL(1,2) + Cud8_ud_LNP*SDL(0,0)*SUL(1,2)).real();
    Cud8_2311i_LNP = (Cud8p_ud_LNP*SUDcL(0,2)*SUDL(1,0) + Cud8_u0_LNP*SUL(1,2) + Cud8_ud_LNP*SDL(0,0)*SUL(1,2)).imag();
    Cud8_2312r_LNP = (Cud8p_ud_LNP*SUDcL(0,2)*SUDL(1,1) + Cud8_ud_LNP*SDL(0,1)*SUL(1,2)).real();
    Cud8_2312i_LNP = (Cud8p_ud_LNP*SUDcL(0,2)*SUDL(1,1) + Cud8_ud_LNP*SDL(0,1)*SUL(1,2)).imag();
    Cud8_2313r_LNP = (Cud8p_ud_LNP*SUDcL(0,2)*SUDL(1,2) + Cud8_ud_LNP*SDL(0,2)*SUL(1,2)).real();
    Cud8_2313i_LNP = (Cud8p_ud_LNP*SUDcL(0,2)*SUDL(1,2) + Cud8_ud_LNP*SDL(0,2)*SUL(1,2)).imag();
    Cud8_2321r_LNP = (Cud8p_ud_LNP*SUDcL(1,2)*SUDL(1,0) + Cud8_ud_LNP*SDL(1,0)*SUL(1,2)).real();
    Cud8_2321i_LNP = (Cud8p_ud_LNP*SUDcL(1,2)*SUDL(1,0) + Cud8_ud_LNP*SDL(1,0)*SUL(1,2)).imag();
    Cud8_2322r_LNP = (Cud8p_ud_LNP*SUDcL(1,2)*SUDL(1,1) + Cud8_u0_LNP*SUL(1,2) + Cud8_ud_LNP*SDL(1,1)*SUL(1,2)).real();
    Cud8_2322i_LNP = (Cud8p_ud_LNP*SUDcL(1,2)*SUDL(1,1) + Cud8_u0_LNP*SUL(1,2) + Cud8_ud_LNP*SDL(1,1)*SUL(1,2)).imag();
    Cud8_2323r_LNP = (Cud8p_ud_LNP*SUDcL(1,2)*SUDL(1,2) + Cud8_ud_LNP*SDL(1,2)*SUL(1,2)).real();
    Cud8_2323i_LNP = (Cud8p_ud_LNP*SUDcL(1,2)*SUDL(1,2) + Cud8_ud_LNP*SDL(1,2)*SUL(1,2)).imag();
    Cud8_2331r_LNP = (Cud8p_ud_LNP*SUDcL(2,2)*SUDL(1,0) + Cud8_ud_LNP*SDL(2,0)*SUL(1,2)).real();
    Cud8_2331i_LNP = (Cud8p_ud_LNP*SUDcL(2,2)*SUDL(1,0) + Cud8_ud_LNP*SDL(2,0)*SUL(1,2)).imag();
    Cud8_2332r_LNP = (Cud8p_ud_LNP*SUDcL(2,2)*SUDL(1,1) + Cud8_ud_LNP*SDL(2,1)*SUL(1,2)).real();
    Cud8_2332i_LNP = (Cud8p_ud_LNP*SUDcL(2,2)*SUDL(1,1) + Cud8_ud_LNP*SDL(2,1)*SUL(1,2)).imag();
    Cud8_2333r_LNP = (Cud8p_ud_LNP*SUDcL(2,2)*SUDL(1,2) + Cud8_u0_LNP*SUL(1,2) + Cud8_ud_LNP*SDL(2,2)*SUL(1,2)).real();
    Cud8_2333i_LNP = (Cud8p_ud_LNP*SUDcL(2,2)*SUDL(1,2) + Cud8_u0_LNP*SUL(1,2) + Cud8_ud_LNP*SDL(2,2)*SUL(1,2)).imag();
    Cud8_3311r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*SDL(0,0) + Cud8p_ud_LNP*SUDcL(0,2)*SUDL(2,0) + Cud8_u0_LNP*SUL(2,2) + Cud8_ud_LNP*SDL(0,0)*SUL(2,2)).real();
    Cud8_3312r_LNP = (Cud8_0d_LNP*SDL(0,1) + Cud8p_ud_LNP*SUDcL(0,2)*SUDL(2,1) + Cud8_ud_LNP*SDL(0,1)*SUL(2,2)).real();
    Cud8_3312i_LNP = (Cud8_0d_LNP*SDL(0,1) + Cud8p_ud_LNP*SUDcL(0,2)*SUDL(2,1) + Cud8_ud_LNP*SDL(0,1)*SUL(2,2)).imag();
    Cud8_3313r_LNP = (Cud8_0d_LNP*SDL(0,2) + Cud8p_ud_LNP*SUDcL(0,2)*SUDL(2,2) + Cud8_ud_LNP*SDL(0,2)*SUL(2,2)).real();
    Cud8_3313i_LNP = (Cud8_0d_LNP*SDL(0,2) + Cud8p_ud_LNP*SUDcL(0,2)*SUDL(2,2) + Cud8_ud_LNP*SDL(0,2)*SUL(2,2)).imag();
    Cud8_3322r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*SDL(1,1) + Cud8p_ud_LNP*SUDcL(1,2)*SUDL(2,1) + Cud8_u0_LNP*SUL(2,2) + Cud8_ud_LNP*SDL(1,1)*SUL(2,2)).real();
    Cud8_3323r_LNP = (Cud8_0d_LNP*SDL(1,2) + Cud8p_ud_LNP*SUDcL(1,2)*SUDL(2,2) + Cud8_ud_LNP*SDL(1,2)*SUL(2,2)).real();
    Cud8_3323i_LNP = (Cud8_0d_LNP*SDL(1,2) + Cud8p_ud_LNP*SUDcL(1,2)*SUDL(2,2) + Cud8_ud_LNP*SDL(1,2)*SUL(2,2)).imag();
    Cud8_3333r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*SDL(2,2) + Cud8p_ud_LNP*SUDcL(2,2)*SUDL(2,2) + Cud8_u0_LNP*SUL(2,2) + Cud8_ud_LNP*SDL(2,2)*SUL(2,2)).real();
 
    Cqu1_1111r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*SQDL(0,0) + Cqu1_u0_LNP*SQUL(0,0) + Cqu1_0u_LNP*SUL(0,0) + Cqu1_du_LNP*SQDL(0,0)*SUL(0,0) + Cqu1_uu_LNP*SQUL(0,0)*SUL(0,0) + Cqu1_dy_LNP*SQDYucL(0,0)*YuL(0,0) + Cqu1_uy_LNP*SQUYucL(0,0)*YuL(0,0) + Cqu1_y_LNP*YucL(0,0)*YuL(0,0) + Cqu1_yd_LNP*YucL(0,0)*YuSQDL(0,0) + Cqu1_yu_LNP*YucL(0,0)*YuSQUL(0,0)).real();
    Cqu1_1112r_LNP = (Cqu1_0u_LNP*SUL(0,1) + Cqu1_du_LNP*SQDL(0,0)*SUL(0,1) + Cqu1_uu_LNP*SQUL(0,0)*SUL(0,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(0,0) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(0,0) + Cqu1_y_LNP*YucL(0,1)*YuL(0,0) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(0,0) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(0,0)).real();
    Cqu1_1112i_LNP = (Cqu1_0u_LNP*SUL(0,1) + Cqu1_du_LNP*SQDL(0,0)*SUL(0,1) + Cqu1_uu_LNP*SQUL(0,0)*SUL(0,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(0,0) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(0,0) + Cqu1_y_LNP*YucL(0,1)*YuL(0,0) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(0,0) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(0,0)).imag();
    Cqu1_1113r_LNP = (Cqu1_0u_LNP*SUL(0,2) + Cqu1_du_LNP*SQDL(0,0)*SUL(0,2) + Cqu1_uu_LNP*SQUL(0,0)*SUL(0,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(0,0) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(0,0) + Cqu1_y_LNP*YucL(0,2)*YuL(0,0) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(0,0) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(0,0)).real();
    Cqu1_1113i_LNP = (Cqu1_0u_LNP*SUL(0,2) + Cqu1_du_LNP*SQDL(0,0)*SUL(0,2) + Cqu1_uu_LNP*SQUL(0,0)*SUL(0,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(0,0) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(0,0) + Cqu1_y_LNP*YucL(0,2)*YuL(0,0) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(0,0) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(0,0)).imag();
    Cqu1_1122r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*SQDL(0,0) + Cqu1_u0_LNP*SQUL(0,0) + Cqu1_0u_LNP*SUL(1,1) + Cqu1_du_LNP*SQDL(0,0)*SUL(1,1) + Cqu1_uu_LNP*SQUL(0,0)*SUL(1,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(1,0) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(1,0) + Cqu1_y_LNP*YucL(0,1)*YuL(1,0) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(1,0) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(1,0)).real();
    Cqu1_1123r_LNP = (Cqu1_0u_LNP*SUL(1,2) + Cqu1_du_LNP*SQDL(0,0)*SUL(1,2) + Cqu1_uu_LNP*SQUL(0,0)*SUL(1,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(1,0) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(1,0) + Cqu1_y_LNP*YucL(0,2)*YuL(1,0) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(1,0) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(1,0)).real();
    Cqu1_1123i_LNP = (Cqu1_0u_LNP*SUL(1,2) + Cqu1_du_LNP*SQDL(0,0)*SUL(1,2) + Cqu1_uu_LNP*SQUL(0,0)*SUL(1,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(1,0) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(1,0) + Cqu1_y_LNP*YucL(0,2)*YuL(1,0) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(1,0) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(1,0)).imag();
    Cqu1_1133r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*SQDL(0,0) + Cqu1_u0_LNP*SQUL(0,0) + Cqu1_0u_LNP*SUL(2,2) + Cqu1_du_LNP*SQDL(0,0)*SUL(2,2) + Cqu1_uu_LNP*SQUL(0,0)*SUL(2,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(2,0) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(2,0) + Cqu1_y_LNP*YucL(0,2)*YuL(2,0) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(2,0) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(2,0)).real();
    Cqu1_1211r_LNP = (Cqu1_d0_LNP*SQDL(0,1) + Cqu1_u0_LNP*SQUL(0,1) + Cqu1_du_LNP*SQDL(0,1)*SUL(0,0) + Cqu1_uu_LNP*SQUL(0,1)*SUL(0,0) + Cqu1_dy_LNP*SQDYucL(0,0)*YuL(0,1) + Cqu1_uy_LNP*SQUYucL(0,0)*YuL(0,1) + Cqu1_y_LNP*YucL(0,0)*YuL(0,1) + Cqu1_yd_LNP*YucL(0,0)*YuSQDL(0,1) + Cqu1_yu_LNP*YucL(0,0)*YuSQUL(0,1)).real();
    Cqu1_1211i_LNP = (Cqu1_d0_LNP*SQDL(0,1) + Cqu1_u0_LNP*SQUL(0,1) + Cqu1_du_LNP*SQDL(0,1)*SUL(0,0) + Cqu1_uu_LNP*SQUL(0,1)*SUL(0,0) + Cqu1_dy_LNP*SQDYucL(0,0)*YuL(0,1) + Cqu1_uy_LNP*SQUYucL(0,0)*YuL(0,1) + Cqu1_y_LNP*YucL(0,0)*YuL(0,1) + Cqu1_yd_LNP*YucL(0,0)*YuSQDL(0,1) + Cqu1_yu_LNP*YucL(0,0)*YuSQUL(0,1)).imag();
    Cqu1_1212r_LNP = (Cqu1_du_LNP*SQDL(0,1)*SUL(0,1) + Cqu1_uu_LNP*SQUL(0,1)*SUL(0,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(0,1) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(0,1) + Cqu1_y_LNP*YucL(0,1)*YuL(0,1) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(0,1) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(0,1)).real();
    Cqu1_1212i_LNP = (Cqu1_du_LNP*SQDL(0,1)*SUL(0,1) + Cqu1_uu_LNP*SQUL(0,1)*SUL(0,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(0,1) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(0,1) + Cqu1_y_LNP*YucL(0,1)*YuL(0,1) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(0,1) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(0,1)).imag();
    Cqu1_1213r_LNP = (Cqu1_du_LNP*SQDL(0,1)*SUL(0,2) + Cqu1_uu_LNP*SQUL(0,1)*SUL(0,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(0,1) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(0,1) + Cqu1_y_LNP*YucL(0,2)*YuL(0,1) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(0,1) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(0,1)).real();
    Cqu1_1213i_LNP = (Cqu1_du_LNP*SQDL(0,1)*SUL(0,2) + Cqu1_uu_LNP*SQUL(0,1)*SUL(0,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(0,1) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(0,1) + Cqu1_y_LNP*YucL(0,2)*YuL(0,1) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(0,1) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(0,1)).imag();
    Cqu1_1221r_LNP = (Cqu1_du_LNP*SQDL(0,1)*SUL(1,0) + Cqu1_uu_LNP*SQUL(0,1)*SUL(1,0) + Cqu1_dy_LNP*SQDYucL(0,0)*YuL(1,1) + Cqu1_uy_LNP*SQUYucL(0,0)*YuL(1,1) + Cqu1_y_LNP*YucL(0,0)*YuL(1,1) + Cqu1_yd_LNP*YucL(0,0)*YuSQDL(1,1) + Cqu1_yu_LNP*YucL(0,0)*YuSQUL(1,1)).real();
    Cqu1_1221i_LNP = (Cqu1_du_LNP*SQDL(0,1)*SUL(1,0) + Cqu1_uu_LNP*SQUL(0,1)*SUL(1,0) + Cqu1_dy_LNP*SQDYucL(0,0)*YuL(1,1) + Cqu1_uy_LNP*SQUYucL(0,0)*YuL(1,1) + Cqu1_y_LNP*YucL(0,0)*YuL(1,1) + Cqu1_yd_LNP*YucL(0,0)*YuSQDL(1,1) + Cqu1_yu_LNP*YucL(0,0)*YuSQUL(1,1)).imag();
    Cqu1_1222r_LNP = (Cqu1_d0_LNP*SQDL(0,1) + Cqu1_u0_LNP*SQUL(0,1) + Cqu1_du_LNP*SQDL(0,1)*SUL(1,1) + Cqu1_uu_LNP*SQUL(0,1)*SUL(1,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(1,1) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(1,1) + Cqu1_y_LNP*YucL(0,1)*YuL(1,1) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(1,1) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(1,1)).real();
    Cqu1_1222i_LNP = (Cqu1_d0_LNP*SQDL(0,1) + Cqu1_u0_LNP*SQUL(0,1) + Cqu1_du_LNP*SQDL(0,1)*SUL(1,1) + Cqu1_uu_LNP*SQUL(0,1)*SUL(1,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(1,1) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(1,1) + Cqu1_y_LNP*YucL(0,1)*YuL(1,1) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(1,1) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(1,1)).imag();
    Cqu1_1223r_LNP = (Cqu1_du_LNP*SQDL(0,1)*SUL(1,2) + Cqu1_uu_LNP*SQUL(0,1)*SUL(1,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(1,1) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(1,1) + Cqu1_y_LNP*YucL(0,2)*YuL(1,1) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(1,1) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(1,1)).real();
    Cqu1_1223i_LNP = (Cqu1_du_LNP*SQDL(0,1)*SUL(1,2) + Cqu1_uu_LNP*SQUL(0,1)*SUL(1,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(1,1) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(1,1) + Cqu1_y_LNP*YucL(0,2)*YuL(1,1) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(1,1) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(1,1)).imag();
    Cqu1_1231r_LNP = (Cqu1_du_LNP*SQDL(0,1)*SUL(2,0) + Cqu1_uu_LNP*SQUL(0,1)*SUL(2,0) + Cqu1_dy_LNP*SQDYucL(0,0)*YuL(2,1) + Cqu1_uy_LNP*SQUYucL(0,0)*YuL(2,1) + Cqu1_y_LNP*YucL(0,0)*YuL(2,1) + Cqu1_yd_LNP*YucL(0,0)*YuSQDL(2,1) + Cqu1_yu_LNP*YucL(0,0)*YuSQUL(2,1)).real();
    Cqu1_1231i_LNP = (Cqu1_du_LNP*SQDL(0,1)*SUL(2,0) + Cqu1_uu_LNP*SQUL(0,1)*SUL(2,0) + Cqu1_dy_LNP*SQDYucL(0,0)*YuL(2,1) + Cqu1_uy_LNP*SQUYucL(0,0)*YuL(2,1) + Cqu1_y_LNP*YucL(0,0)*YuL(2,1) + Cqu1_yd_LNP*YucL(0,0)*YuSQDL(2,1) + Cqu1_yu_LNP*YucL(0,0)*YuSQUL(2,1)).imag();
    Cqu1_1232r_LNP = (Cqu1_du_LNP*SQDL(0,1)*SUL(2,1) + Cqu1_uu_LNP*SQUL(0,1)*SUL(2,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(2,1) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(2,1) + Cqu1_y_LNP*YucL(0,1)*YuL(2,1) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(2,1) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(2,1)).real();
    Cqu1_1232i_LNP = (Cqu1_du_LNP*SQDL(0,1)*SUL(2,1) + Cqu1_uu_LNP*SQUL(0,1)*SUL(2,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(2,1) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(2,1) + Cqu1_y_LNP*YucL(0,1)*YuL(2,1) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(2,1) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(2,1)).imag();
    Cqu1_1233r_LNP = (Cqu1_d0_LNP*SQDL(0,1) + Cqu1_u0_LNP*SQUL(0,1) + Cqu1_du_LNP*SQDL(0,1)*SUL(2,2) + Cqu1_uu_LNP*SQUL(0,1)*SUL(2,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(2,1) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(2,1) + Cqu1_y_LNP*YucL(0,2)*YuL(2,1) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(2,1) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(2,1)).real();
    Cqu1_1233i_LNP = (Cqu1_d0_LNP*SQDL(0,1) + Cqu1_u0_LNP*SQUL(0,1) + Cqu1_du_LNP*SQDL(0,1)*SUL(2,2) + Cqu1_uu_LNP*SQUL(0,1)*SUL(2,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(2,1) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(2,1) + Cqu1_y_LNP*YucL(0,2)*YuL(2,1) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(2,1) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(2,1)).imag();
    Cqu1_1311r_LNP = (Cqu1_d0_LNP*SQDL(0,2) + Cqu1_u0_LNP*SQUL(0,2) + Cqu1_du_LNP*SQDL(0,2)*SUL(0,0) + Cqu1_uu_LNP*SQUL(0,2)*SUL(0,0) + Cqu1_dy_LNP*SQDYucL(0,0)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(0,0)*YuL(0,2) + Cqu1_y_LNP*YucL(0,0)*YuL(0,2) + Cqu1_yd_LNP*YucL(0,0)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(0,0)*YuSQUL(0,2)).real();
    Cqu1_1311i_LNP = (Cqu1_d0_LNP*SQDL(0,2) + Cqu1_u0_LNP*SQUL(0,2) + Cqu1_du_LNP*SQDL(0,2)*SUL(0,0) + Cqu1_uu_LNP*SQUL(0,2)*SUL(0,0) + Cqu1_dy_LNP*SQDYucL(0,0)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(0,0)*YuL(0,2) + Cqu1_y_LNP*YucL(0,0)*YuL(0,2) + Cqu1_yd_LNP*YucL(0,0)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(0,0)*YuSQUL(0,2)).imag();
    Cqu1_1312r_LNP = (Cqu1_du_LNP*SQDL(0,2)*SUL(0,1) + Cqu1_uu_LNP*SQUL(0,2)*SUL(0,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(0,2) + Cqu1_y_LNP*YucL(0,1)*YuL(0,2) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(0,2)).real();
    Cqu1_1312i_LNP = (Cqu1_du_LNP*SQDL(0,2)*SUL(0,1) + Cqu1_uu_LNP*SQUL(0,2)*SUL(0,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(0,2) + Cqu1_y_LNP*YucL(0,1)*YuL(0,2) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(0,2)).imag();
    Cqu1_1313r_LNP = (Cqu1_du_LNP*SQDL(0,2)*SUL(0,2) + Cqu1_uu_LNP*SQUL(0,2)*SUL(0,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(0,2) + Cqu1_y_LNP*YucL(0,2)*YuL(0,2) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(0,2)).real();
    Cqu1_1313i_LNP = (Cqu1_du_LNP*SQDL(0,2)*SUL(0,2) + Cqu1_uu_LNP*SQUL(0,2)*SUL(0,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(0,2) + Cqu1_y_LNP*YucL(0,2)*YuL(0,2) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(0,2)).imag();
    Cqu1_1321r_LNP = (Cqu1_du_LNP*SQDL(0,2)*SUL(1,0) + Cqu1_uu_LNP*SQUL(0,2)*SUL(1,0) + Cqu1_dy_LNP*SQDYucL(0,0)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(0,0)*YuL(1,2) + Cqu1_y_LNP*YucL(0,0)*YuL(1,2) + Cqu1_yd_LNP*YucL(0,0)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(0,0)*YuSQUL(1,2)).real();
    Cqu1_1321i_LNP = (Cqu1_du_LNP*SQDL(0,2)*SUL(1,0) + Cqu1_uu_LNP*SQUL(0,2)*SUL(1,0) + Cqu1_dy_LNP*SQDYucL(0,0)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(0,0)*YuL(1,2) + Cqu1_y_LNP*YucL(0,0)*YuL(1,2) + Cqu1_yd_LNP*YucL(0,0)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(0,0)*YuSQUL(1,2)).imag();
    Cqu1_1322r_LNP = (Cqu1_d0_LNP*SQDL(0,2) + Cqu1_u0_LNP*SQUL(0,2) + Cqu1_du_LNP*SQDL(0,2)*SUL(1,1) + Cqu1_uu_LNP*SQUL(0,2)*SUL(1,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(1,2) + Cqu1_y_LNP*YucL(0,1)*YuL(1,2) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(1,2)).real();
    Cqu1_1322i_LNP = (Cqu1_d0_LNP*SQDL(0,2) + Cqu1_u0_LNP*SQUL(0,2) + Cqu1_du_LNP*SQDL(0,2)*SUL(1,1) + Cqu1_uu_LNP*SQUL(0,2)*SUL(1,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(1,2) + Cqu1_y_LNP*YucL(0,1)*YuL(1,2) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(1,2)).imag();
    Cqu1_1323r_LNP = (Cqu1_du_LNP*SQDL(0,2)*SUL(1,2) + Cqu1_uu_LNP*SQUL(0,2)*SUL(1,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(1,2) + Cqu1_y_LNP*YucL(0,2)*YuL(1,2) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(1,2)).real();
    Cqu1_1323i_LNP = (Cqu1_du_LNP*SQDL(0,2)*SUL(1,2) + Cqu1_uu_LNP*SQUL(0,2)*SUL(1,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(1,2) + Cqu1_y_LNP*YucL(0,2)*YuL(1,2) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(1,2)).imag();
    Cqu1_1331r_LNP = (Cqu1_du_LNP*SQDL(0,2)*SUL(2,0) + Cqu1_uu_LNP*SQUL(0,2)*SUL(2,0) + Cqu1_dy_LNP*SQDYucL(0,0)*YuL(2,2) + Cqu1_uy_LNP*SQUYucL(0,0)*YuL(2,2) + Cqu1_y_LNP*YucL(0,0)*YuL(2,2) + Cqu1_yd_LNP*YucL(0,0)*YuSQDL(2,2) + Cqu1_yu_LNP*YucL(0,0)*YuSQUL(2,2)).real();
    Cqu1_1331i_LNP = (Cqu1_du_LNP*SQDL(0,2)*SUL(2,0) + Cqu1_uu_LNP*SQUL(0,2)*SUL(2,0) + Cqu1_dy_LNP*SQDYucL(0,0)*YuL(2,2) + Cqu1_uy_LNP*SQUYucL(0,0)*YuL(2,2) + Cqu1_y_LNP*YucL(0,0)*YuL(2,2) + Cqu1_yd_LNP*YucL(0,0)*YuSQDL(2,2) + Cqu1_yu_LNP*YucL(0,0)*YuSQUL(2,2)).imag();
    Cqu1_1332r_LNP = (Cqu1_du_LNP*SQDL(0,2)*SUL(2,1) + Cqu1_uu_LNP*SQUL(0,2)*SUL(2,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(2,2) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(2,2) + Cqu1_y_LNP*YucL(0,1)*YuL(2,2) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(2,2) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(2,2)).real();
    Cqu1_1332i_LNP = (Cqu1_du_LNP*SQDL(0,2)*SUL(2,1) + Cqu1_uu_LNP*SQUL(0,2)*SUL(2,1) + Cqu1_dy_LNP*SQDYucL(0,1)*YuL(2,2) + Cqu1_uy_LNP*SQUYucL(0,1)*YuL(2,2) + Cqu1_y_LNP*YucL(0,1)*YuL(2,2) + Cqu1_yd_LNP*YucL(0,1)*YuSQDL(2,2) + Cqu1_yu_LNP*YucL(0,1)*YuSQUL(2,2)).imag();
    Cqu1_1333r_LNP = (Cqu1_d0_LNP*SQDL(0,2) + Cqu1_u0_LNP*SQUL(0,2) + Cqu1_du_LNP*SQDL(0,2)*SUL(2,2) + Cqu1_uu_LNP*SQUL(0,2)*SUL(2,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(2,2) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(2,2) + Cqu1_y_LNP*YucL(0,2)*YuL(2,2) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(2,2) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(2,2)).real();
    Cqu1_1333i_LNP = (Cqu1_d0_LNP*SQDL(0,2) + Cqu1_u0_LNP*SQUL(0,2) + Cqu1_du_LNP*SQDL(0,2)*SUL(2,2) + Cqu1_uu_LNP*SQUL(0,2)*SUL(2,2) + Cqu1_dy_LNP*SQDYucL(0,2)*YuL(2,2) + Cqu1_uy_LNP*SQUYucL(0,2)*YuL(2,2) + Cqu1_y_LNP*YucL(0,2)*YuL(2,2) + Cqu1_yd_LNP*YucL(0,2)*YuSQDL(2,2) + Cqu1_yu_LNP*YucL(0,2)*YuSQUL(2,2)).imag();
    Cqu1_2211r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*SQDL(1,1) + Cqu1_u0_LNP*SQUL(1,1) + Cqu1_0u_LNP*SUL(0,0) + Cqu1_du_LNP*SQDL(1,1)*SUL(0,0) + Cqu1_uu_LNP*SQUL(1,1)*SUL(0,0) + Cqu1_dy_LNP*SQDYucL(1,0)*YuL(0,1) + Cqu1_uy_LNP*SQUYucL(1,0)*YuL(0,1) + Cqu1_y_LNP*YucL(1,0)*YuL(0,1) + Cqu1_yd_LNP*YucL(1,0)*YuSQDL(0,1) + Cqu1_yu_LNP*YucL(1,0)*YuSQUL(0,1)).real();
    Cqu1_2212r_LNP = (Cqu1_0u_LNP*SUL(0,1) + Cqu1_du_LNP*SQDL(1,1)*SUL(0,1) + Cqu1_uu_LNP*SQUL(1,1)*SUL(0,1) + Cqu1_dy_LNP*SQDYucL(1,1)*YuL(0,1) + Cqu1_uy_LNP*SQUYucL(1,1)*YuL(0,1) + Cqu1_y_LNP*YucL(1,1)*YuL(0,1) + Cqu1_yd_LNP*YucL(1,1)*YuSQDL(0,1) + Cqu1_yu_LNP*YucL(1,1)*YuSQUL(0,1)).real();
    Cqu1_2212i_LNP = (Cqu1_0u_LNP*SUL(0,1) + Cqu1_du_LNP*SQDL(1,1)*SUL(0,1) + Cqu1_uu_LNP*SQUL(1,1)*SUL(0,1) + Cqu1_dy_LNP*SQDYucL(1,1)*YuL(0,1) + Cqu1_uy_LNP*SQUYucL(1,1)*YuL(0,1) + Cqu1_y_LNP*YucL(1,1)*YuL(0,1) + Cqu1_yd_LNP*YucL(1,1)*YuSQDL(0,1) + Cqu1_yu_LNP*YucL(1,1)*YuSQUL(0,1)).imag();
    Cqu1_2213r_LNP = (Cqu1_0u_LNP*SUL(0,2) + Cqu1_du_LNP*SQDL(1,1)*SUL(0,2) + Cqu1_uu_LNP*SQUL(1,1)*SUL(0,2) + Cqu1_dy_LNP*SQDYucL(1,2)*YuL(0,1) + Cqu1_uy_LNP*SQUYucL(1,2)*YuL(0,1) + Cqu1_y_LNP*YucL(1,2)*YuL(0,1) + Cqu1_yd_LNP*YucL(1,2)*YuSQDL(0,1) + Cqu1_yu_LNP*YucL(1,2)*YuSQUL(0,1)).real();
    Cqu1_2213i_LNP = (Cqu1_0u_LNP*SUL(0,2) + Cqu1_du_LNP*SQDL(1,1)*SUL(0,2) + Cqu1_uu_LNP*SQUL(1,1)*SUL(0,2) + Cqu1_dy_LNP*SQDYucL(1,2)*YuL(0,1) + Cqu1_uy_LNP*SQUYucL(1,2)*YuL(0,1) + Cqu1_y_LNP*YucL(1,2)*YuL(0,1) + Cqu1_yd_LNP*YucL(1,2)*YuSQDL(0,1) + Cqu1_yu_LNP*YucL(1,2)*YuSQUL(0,1)).imag();
    Cqu1_2222r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*SQDL(1,1) + Cqu1_u0_LNP*SQUL(1,1) + Cqu1_0u_LNP*SUL(1,1) + Cqu1_du_LNP*SQDL(1,1)*SUL(1,1) + Cqu1_uu_LNP*SQUL(1,1)*SUL(1,1) + Cqu1_dy_LNP*SQDYucL(1,1)*YuL(1,1) + Cqu1_uy_LNP*SQUYucL(1,1)*YuL(1,1) + Cqu1_y_LNP*YucL(1,1)*YuL(1,1) + Cqu1_yd_LNP*YucL(1,1)*YuSQDL(1,1) + Cqu1_yu_LNP*YucL(1,1)*YuSQUL(1,1)).real();
    Cqu1_2223r_LNP = (Cqu1_0u_LNP*SUL(1,2) + Cqu1_du_LNP*SQDL(1,1)*SUL(1,2) + Cqu1_uu_LNP*SQUL(1,1)*SUL(1,2) + Cqu1_dy_LNP*SQDYucL(1,2)*YuL(1,1) + Cqu1_uy_LNP*SQUYucL(1,2)*YuL(1,1) + Cqu1_y_LNP*YucL(1,2)*YuL(1,1) + Cqu1_yd_LNP*YucL(1,2)*YuSQDL(1,1) + Cqu1_yu_LNP*YucL(1,2)*YuSQUL(1,1)).real();
    Cqu1_2223i_LNP = (Cqu1_0u_LNP*SUL(1,2) + Cqu1_du_LNP*SQDL(1,1)*SUL(1,2) + Cqu1_uu_LNP*SQUL(1,1)*SUL(1,2) + Cqu1_dy_LNP*SQDYucL(1,2)*YuL(1,1) + Cqu1_uy_LNP*SQUYucL(1,2)*YuL(1,1) + Cqu1_y_LNP*YucL(1,2)*YuL(1,1) + Cqu1_yd_LNP*YucL(1,2)*YuSQDL(1,1) + Cqu1_yu_LNP*YucL(1,2)*YuSQUL(1,1)).imag();
    Cqu1_2233r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*SQDL(1,1) + Cqu1_u0_LNP*SQUL(1,1) + Cqu1_0u_LNP*SUL(2,2) + Cqu1_du_LNP*SQDL(1,1)*SUL(2,2) + Cqu1_uu_LNP*SQUL(1,1)*SUL(2,2) + Cqu1_dy_LNP*SQDYucL(1,2)*YuL(2,1) + Cqu1_uy_LNP*SQUYucL(1,2)*YuL(2,1) + Cqu1_y_LNP*YucL(1,2)*YuL(2,1) + Cqu1_yd_LNP*YucL(1,2)*YuSQDL(2,1) + Cqu1_yu_LNP*YucL(1,2)*YuSQUL(2,1)).real();
    Cqu1_2311r_LNP = (Cqu1_d0_LNP*SQDL(1,2) + Cqu1_u0_LNP*SQUL(1,2) + Cqu1_du_LNP*SQDL(1,2)*SUL(0,0) + Cqu1_uu_LNP*SQUL(1,2)*SUL(0,0) + Cqu1_dy_LNP*SQDYucL(1,0)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(1,0)*YuL(0,2) + Cqu1_y_LNP*YucL(1,0)*YuL(0,2) + Cqu1_yd_LNP*YucL(1,0)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(1,0)*YuSQUL(0,2)).real();
    Cqu1_2311i_LNP = (Cqu1_d0_LNP*SQDL(1,2) + Cqu1_u0_LNP*SQUL(1,2) + Cqu1_du_LNP*SQDL(1,2)*SUL(0,0) + Cqu1_uu_LNP*SQUL(1,2)*SUL(0,0) + Cqu1_dy_LNP*SQDYucL(1,0)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(1,0)*YuL(0,2) + Cqu1_y_LNP*YucL(1,0)*YuL(0,2) + Cqu1_yd_LNP*YucL(1,0)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(1,0)*YuSQUL(0,2)).imag();
    Cqu1_2312r_LNP = (Cqu1_du_LNP*SQDL(1,2)*SUL(0,1) + Cqu1_uu_LNP*SQUL(1,2)*SUL(0,1) + Cqu1_dy_LNP*SQDYucL(1,1)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(1,1)*YuL(0,2) + Cqu1_y_LNP*YucL(1,1)*YuL(0,2) + Cqu1_yd_LNP*YucL(1,1)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(1,1)*YuSQUL(0,2)).real();
    Cqu1_2312i_LNP = (Cqu1_du_LNP*SQDL(1,2)*SUL(0,1) + Cqu1_uu_LNP*SQUL(1,2)*SUL(0,1) + Cqu1_dy_LNP*SQDYucL(1,1)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(1,1)*YuL(0,2) + Cqu1_y_LNP*YucL(1,1)*YuL(0,2) + Cqu1_yd_LNP*YucL(1,1)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(1,1)*YuSQUL(0,2)).imag();
    Cqu1_2313r_LNP = (Cqu1_du_LNP*SQDL(1,2)*SUL(0,2) + Cqu1_uu_LNP*SQUL(1,2)*SUL(0,2) + Cqu1_dy_LNP*SQDYucL(1,2)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(1,2)*YuL(0,2) + Cqu1_y_LNP*YucL(1,2)*YuL(0,2) + Cqu1_yd_LNP*YucL(1,2)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(1,2)*YuSQUL(0,2)).real();
    Cqu1_2313i_LNP = (Cqu1_du_LNP*SQDL(1,2)*SUL(0,2) + Cqu1_uu_LNP*SQUL(1,2)*SUL(0,2) + Cqu1_dy_LNP*SQDYucL(1,2)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(1,2)*YuL(0,2) + Cqu1_y_LNP*YucL(1,2)*YuL(0,2) + Cqu1_yd_LNP*YucL(1,2)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(1,2)*YuSQUL(0,2)).imag();
    Cqu1_2321r_LNP = (Cqu1_du_LNP*SQDL(1,2)*SUL(1,0) + Cqu1_uu_LNP*SQUL(1,2)*SUL(1,0) + Cqu1_dy_LNP*SQDYucL(1,0)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(1,0)*YuL(1,2) + Cqu1_y_LNP*YucL(1,0)*YuL(1,2) + Cqu1_yd_LNP*YucL(1,0)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(1,0)*YuSQUL(1,2)).real();
    Cqu1_2321i_LNP = (Cqu1_du_LNP*SQDL(1,2)*SUL(1,0) + Cqu1_uu_LNP*SQUL(1,2)*SUL(1,0) + Cqu1_dy_LNP*SQDYucL(1,0)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(1,0)*YuL(1,2) + Cqu1_y_LNP*YucL(1,0)*YuL(1,2) + Cqu1_yd_LNP*YucL(1,0)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(1,0)*YuSQUL(1,2)).imag();
    Cqu1_2322r_LNP = (Cqu1_d0_LNP*SQDL(1,2) + Cqu1_u0_LNP*SQUL(1,2) + Cqu1_du_LNP*SQDL(1,2)*SUL(1,1) + Cqu1_uu_LNP*SQUL(1,2)*SUL(1,1) + Cqu1_dy_LNP*SQDYucL(1,1)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(1,1)*YuL(1,2) + Cqu1_y_LNP*YucL(1,1)*YuL(1,2) + Cqu1_yd_LNP*YucL(1,1)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(1,1)*YuSQUL(1,2)).real();
    Cqu1_2322i_LNP = (Cqu1_d0_LNP*SQDL(1,2) + Cqu1_u0_LNP*SQUL(1,2) + Cqu1_du_LNP*SQDL(1,2)*SUL(1,1) + Cqu1_uu_LNP*SQUL(1,2)*SUL(1,1) + Cqu1_dy_LNP*SQDYucL(1,1)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(1,1)*YuL(1,2) + Cqu1_y_LNP*YucL(1,1)*YuL(1,2) + Cqu1_yd_LNP*YucL(1,1)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(1,1)*YuSQUL(1,2)).imag();
    Cqu1_2323r_LNP = (Cqu1_du_LNP*SQDL(1,2)*SUL(1,2) + Cqu1_uu_LNP*SQUL(1,2)*SUL(1,2) + Cqu1_dy_LNP*SQDYucL(1,2)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(1,2)*YuL(1,2) + Cqu1_y_LNP*YucL(1,2)*YuL(1,2) + Cqu1_yd_LNP*YucL(1,2)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(1,2)*YuSQUL(1,2)).real();
    Cqu1_2323i_LNP = (Cqu1_du_LNP*SQDL(1,2)*SUL(1,2) + Cqu1_uu_LNP*SQUL(1,2)*SUL(1,2) + Cqu1_dy_LNP*SQDYucL(1,2)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(1,2)*YuL(1,2) + Cqu1_y_LNP*YucL(1,2)*YuL(1,2) + Cqu1_yd_LNP*YucL(1,2)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(1,2)*YuSQUL(1,2)).imag();
    Cqu1_2331r_LNP = (Cqu1_du_LNP*SQDL(1,2)*SUL(2,0) + Cqu1_uu_LNP*SQUL(1,2)*SUL(2,0) + Cqu1_dy_LNP*SQDYucL(1,0)*YuL(2,2) + Cqu1_uy_LNP*SQUYucL(1,0)*YuL(2,2) + Cqu1_y_LNP*YucL(1,0)*YuL(2,2) + Cqu1_yd_LNP*YucL(1,0)*YuSQDL(2,2) + Cqu1_yu_LNP*YucL(1,0)*YuSQUL(2,2)).real();
    Cqu1_2331i_LNP = (Cqu1_du_LNP*SQDL(1,2)*SUL(2,0) + Cqu1_uu_LNP*SQUL(1,2)*SUL(2,0) + Cqu1_dy_LNP*SQDYucL(1,0)*YuL(2,2) + Cqu1_uy_LNP*SQUYucL(1,0)*YuL(2,2) + Cqu1_y_LNP*YucL(1,0)*YuL(2,2) + Cqu1_yd_LNP*YucL(1,0)*YuSQDL(2,2) + Cqu1_yu_LNP*YucL(1,0)*YuSQUL(2,2)).imag();
    Cqu1_2332r_LNP = (Cqu1_du_LNP*SQDL(1,2)*SUL(2,1) + Cqu1_uu_LNP*SQUL(1,2)*SUL(2,1) + Cqu1_dy_LNP*SQDYucL(1,1)*YuL(2,2) + Cqu1_uy_LNP*SQUYucL(1,1)*YuL(2,2) + Cqu1_y_LNP*YucL(1,1)*YuL(2,2) + Cqu1_yd_LNP*YucL(1,1)*YuSQDL(2,2) + Cqu1_yu_LNP*YucL(1,1)*YuSQUL(2,2)).real();
    Cqu1_2332i_LNP = (Cqu1_du_LNP*SQDL(1,2)*SUL(2,1) + Cqu1_uu_LNP*SQUL(1,2)*SUL(2,1) + Cqu1_dy_LNP*SQDYucL(1,1)*YuL(2,2) + Cqu1_uy_LNP*SQUYucL(1,1)*YuL(2,2) + Cqu1_y_LNP*YucL(1,1)*YuL(2,2) + Cqu1_yd_LNP*YucL(1,1)*YuSQDL(2,2) + Cqu1_yu_LNP*YucL(1,1)*YuSQUL(2,2)).imag();
    Cqu1_2333r_LNP = (Cqu1_d0_LNP*SQDL(1,2) + Cqu1_u0_LNP*SQUL(1,2) + Cqu1_du_LNP*SQDL(1,2)*SUL(2,2) + Cqu1_uu_LNP*SQUL(1,2)*SUL(2,2) + Cqu1_dy_LNP*SQDYucL(1,2)*YuL(2,2) + Cqu1_uy_LNP*SQUYucL(1,2)*YuL(2,2) + Cqu1_y_LNP*YucL(1,2)*YuL(2,2) + Cqu1_yd_LNP*YucL(1,2)*YuSQDL(2,2) + Cqu1_yu_LNP*YucL(1,2)*YuSQUL(2,2)).real();
    Cqu1_2333i_LNP = (Cqu1_d0_LNP*SQDL(1,2) + Cqu1_u0_LNP*SQUL(1,2) + Cqu1_du_LNP*SQDL(1,2)*SUL(2,2) + Cqu1_uu_LNP*SQUL(1,2)*SUL(2,2) + Cqu1_dy_LNP*SQDYucL(1,2)*YuL(2,2) + Cqu1_uy_LNP*SQUYucL(1,2)*YuL(2,2) + Cqu1_y_LNP*YucL(1,2)*YuL(2,2) + Cqu1_yd_LNP*YucL(1,2)*YuSQDL(2,2) + Cqu1_yu_LNP*YucL(1,2)*YuSQUL(2,2)).imag();
    Cqu1_3311r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*SQDL(2,2) + Cqu1_u0_LNP*SQUL(2,2) + Cqu1_0u_LNP*SUL(0,0) + Cqu1_du_LNP*SQDL(2,2)*SUL(0,0) + Cqu1_uu_LNP*SQUL(2,2)*SUL(0,0) + Cqu1_dy_LNP*SQDYucL(2,0)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(2,0)*YuL(0,2) + Cqu1_y_LNP*YucL(2,0)*YuL(0,2) + Cqu1_yd_LNP*YucL(2,0)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(2,0)*YuSQUL(0,2)).real();
    Cqu1_3312r_LNP = (Cqu1_0u_LNP*SUL(0,1) + Cqu1_du_LNP*SQDL(2,2)*SUL(0,1) + Cqu1_uu_LNP*SQUL(2,2)*SUL(0,1) + Cqu1_dy_LNP*SQDYucL(2,1)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(2,1)*YuL(0,2) + Cqu1_y_LNP*YucL(2,1)*YuL(0,2) + Cqu1_yd_LNP*YucL(2,1)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(2,1)*YuSQUL(0,2)).real();
    Cqu1_3312i_LNP = (Cqu1_0u_LNP*SUL(0,1) + Cqu1_du_LNP*SQDL(2,2)*SUL(0,1) + Cqu1_uu_LNP*SQUL(2,2)*SUL(0,1) + Cqu1_dy_LNP*SQDYucL(2,1)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(2,1)*YuL(0,2) + Cqu1_y_LNP*YucL(2,1)*YuL(0,2) + Cqu1_yd_LNP*YucL(2,1)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(2,1)*YuSQUL(0,2)).imag();
    Cqu1_3313r_LNP = (Cqu1_0u_LNP*SUL(0,2) + Cqu1_du_LNP*SQDL(2,2)*SUL(0,2) + Cqu1_uu_LNP*SQUL(2,2)*SUL(0,2) + Cqu1_dy_LNP*SQDYucL(2,2)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(2,2)*YuL(0,2) + Cqu1_y_LNP*YucL(2,2)*YuL(0,2) + Cqu1_yd_LNP*YucL(2,2)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(2,2)*YuSQUL(0,2)).real();
    Cqu1_3313i_LNP = (Cqu1_0u_LNP*SUL(0,2) + Cqu1_du_LNP*SQDL(2,2)*SUL(0,2) + Cqu1_uu_LNP*SQUL(2,2)*SUL(0,2) + Cqu1_dy_LNP*SQDYucL(2,2)*YuL(0,2) + Cqu1_uy_LNP*SQUYucL(2,2)*YuL(0,2) + Cqu1_y_LNP*YucL(2,2)*YuL(0,2) + Cqu1_yd_LNP*YucL(2,2)*YuSQDL(0,2) + Cqu1_yu_LNP*YucL(2,2)*YuSQUL(0,2)).imag();
    Cqu1_3322r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*SQDL(2,2) + Cqu1_u0_LNP*SQUL(2,2) + Cqu1_0u_LNP*SUL(1,1) + Cqu1_du_LNP*SQDL(2,2)*SUL(1,1) + Cqu1_uu_LNP*SQUL(2,2)*SUL(1,1) + Cqu1_dy_LNP*SQDYucL(2,1)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(2,1)*YuL(1,2) + Cqu1_y_LNP*YucL(2,1)*YuL(1,2) + Cqu1_yd_LNP*YucL(2,1)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(2,1)*YuSQUL(1,2)).real();
    Cqu1_3323r_LNP = (Cqu1_0u_LNP*SUL(1,2) + Cqu1_du_LNP*SQDL(2,2)*SUL(1,2) + Cqu1_uu_LNP*SQUL(2,2)*SUL(1,2) + Cqu1_dy_LNP*SQDYucL(2,2)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(2,2)*YuL(1,2) + Cqu1_y_LNP*YucL(2,2)*YuL(1,2) + Cqu1_yd_LNP*YucL(2,2)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(2,2)*YuSQUL(1,2)).real();
    Cqu1_3323i_LNP = (Cqu1_0u_LNP*SUL(1,2) + Cqu1_du_LNP*SQDL(2,2)*SUL(1,2) + Cqu1_uu_LNP*SQUL(2,2)*SUL(1,2) + Cqu1_dy_LNP*SQDYucL(2,2)*YuL(1,2) + Cqu1_uy_LNP*SQUYucL(2,2)*YuL(1,2) + Cqu1_y_LNP*YucL(2,2)*YuL(1,2) + Cqu1_yd_LNP*YucL(2,2)*YuSQDL(1,2) + Cqu1_yu_LNP*YucL(2,2)*YuSQUL(1,2)).imag();
    Cqu1_3333r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*SQDL(2,2) + Cqu1_u0_LNP*SQUL(2,2) + Cqu1_0u_LNP*SUL(2,2) + Cqu1_du_LNP*SQDL(2,2)*SUL(2,2) + Cqu1_uu_LNP*SQUL(2,2)*SUL(2,2) + Cqu1_dy_LNP*SQDYucL(2,2)*YuL(2,2) + Cqu1_uy_LNP*SQUYucL(2,2)*YuL(2,2) + Cqu1_y_LNP*YucL(2,2)*YuL(2,2) + Cqu1_yd_LNP*YucL(2,2)*YuSQDL(2,2) + Cqu1_yu_LNP*YucL(2,2)*YuSQUL(2,2)).real();
 
    Cqu8_1111r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*SQDL(0,0) + Cqu8_u0_LNP*SQUL(0,0) + Cqu8_0u_LNP*SUL(0,0) + Cqu8_du_LNP*SQDL(0,0)*SUL(0,0) + Cqu8_uu_LNP*SQUL(0,0)*SUL(0,0) + Cqu8_dy_LNP*SQDYucL(0,0)*YuL(0,0) + Cqu8_uy_LNP*SQUYucL(0,0)*YuL(0,0) + Cqu8_y_LNP*YucL(0,0)*YuL(0,0) + Cqu8_yd_LNP*YucL(0,0)*YuSQDL(0,0) + Cqu8_yu_LNP*YucL(0,0)*YuSQUL(0,0)).real();
    Cqu8_1112r_LNP = (Cqu8_0u_LNP*SUL(0,1) + Cqu8_du_LNP*SQDL(0,0)*SUL(0,1) + Cqu8_uu_LNP*SQUL(0,0)*SUL(0,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(0,0) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(0,0) + Cqu8_y_LNP*YucL(0,1)*YuL(0,0) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(0,0) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(0,0)).real();
    Cqu8_1112i_LNP = (Cqu8_0u_LNP*SUL(0,1) + Cqu8_du_LNP*SQDL(0,0)*SUL(0,1) + Cqu8_uu_LNP*SQUL(0,0)*SUL(0,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(0,0) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(0,0) + Cqu8_y_LNP*YucL(0,1)*YuL(0,0) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(0,0) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(0,0)).imag();
    Cqu8_1113r_LNP = (Cqu8_0u_LNP*SUL(0,2) + Cqu8_du_LNP*SQDL(0,0)*SUL(0,2) + Cqu8_uu_LNP*SQUL(0,0)*SUL(0,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(0,0) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(0,0) + Cqu8_y_LNP*YucL(0,2)*YuL(0,0) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(0,0) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(0,0)).real();
    Cqu8_1113i_LNP = (Cqu8_0u_LNP*SUL(0,2) + Cqu8_du_LNP*SQDL(0,0)*SUL(0,2) + Cqu8_uu_LNP*SQUL(0,0)*SUL(0,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(0,0) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(0,0) + Cqu8_y_LNP*YucL(0,2)*YuL(0,0) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(0,0) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(0,0)).imag();
    Cqu8_1122r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*SQDL(0,0) + Cqu8_u0_LNP*SQUL(0,0) + Cqu8_0u_LNP*SUL(1,1) + Cqu8_du_LNP*SQDL(0,0)*SUL(1,1) + Cqu8_uu_LNP*SQUL(0,0)*SUL(1,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(1,0) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(1,0) + Cqu8_y_LNP*YucL(0,1)*YuL(1,0) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(1,0) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(1,0)).real();
    Cqu8_1123r_LNP = (Cqu8_0u_LNP*SUL(1,2) + Cqu8_du_LNP*SQDL(0,0)*SUL(1,2) + Cqu8_uu_LNP*SQUL(0,0)*SUL(1,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(1,0) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(1,0) + Cqu8_y_LNP*YucL(0,2)*YuL(1,0) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(1,0) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(1,0)).real();
    Cqu8_1123i_LNP = (Cqu8_0u_LNP*SUL(1,2) + Cqu8_du_LNP*SQDL(0,0)*SUL(1,2) + Cqu8_uu_LNP*SQUL(0,0)*SUL(1,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(1,0) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(1,0) + Cqu8_y_LNP*YucL(0,2)*YuL(1,0) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(1,0) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(1,0)).imag();
    Cqu8_1133r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*SQDL(0,0) + Cqu8_u0_LNP*SQUL(0,0) + Cqu8_0u_LNP*SUL(2,2) + Cqu8_du_LNP*SQDL(0,0)*SUL(2,2) + Cqu8_uu_LNP*SQUL(0,0)*SUL(2,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(2,0) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(2,0) + Cqu8_y_LNP*YucL(0,2)*YuL(2,0) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(2,0) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(2,0)).real();
    Cqu8_1211r_LNP = (Cqu8_d0_LNP*SQDL(0,1) + Cqu8_u0_LNP*SQUL(0,1) + Cqu8_du_LNP*SQDL(0,1)*SUL(0,0) + Cqu8_uu_LNP*SQUL(0,1)*SUL(0,0) + Cqu8_dy_LNP*SQDYucL(0,0)*YuL(0,1) + Cqu8_uy_LNP*SQUYucL(0,0)*YuL(0,1) + Cqu8_y_LNP*YucL(0,0)*YuL(0,1) + Cqu8_yd_LNP*YucL(0,0)*YuSQDL(0,1) + Cqu8_yu_LNP*YucL(0,0)*YuSQUL(0,1)).real();
    Cqu8_1211i_LNP = (Cqu8_d0_LNP*SQDL(0,1) + Cqu8_u0_LNP*SQUL(0,1) + Cqu8_du_LNP*SQDL(0,1)*SUL(0,0) + Cqu8_uu_LNP*SQUL(0,1)*SUL(0,0) + Cqu8_dy_LNP*SQDYucL(0,0)*YuL(0,1) + Cqu8_uy_LNP*SQUYucL(0,0)*YuL(0,1) + Cqu8_y_LNP*YucL(0,0)*YuL(0,1) + Cqu8_yd_LNP*YucL(0,0)*YuSQDL(0,1) + Cqu8_yu_LNP*YucL(0,0)*YuSQUL(0,1)).imag();
    Cqu8_1212r_LNP = (Cqu8_du_LNP*SQDL(0,1)*SUL(0,1) + Cqu8_uu_LNP*SQUL(0,1)*SUL(0,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(0,1) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(0,1) + Cqu8_y_LNP*YucL(0,1)*YuL(0,1) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(0,1) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(0,1)).real();
    Cqu8_1212i_LNP = (Cqu8_du_LNP*SQDL(0,1)*SUL(0,1) + Cqu8_uu_LNP*SQUL(0,1)*SUL(0,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(0,1) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(0,1) + Cqu8_y_LNP*YucL(0,1)*YuL(0,1) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(0,1) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(0,1)).imag();
    Cqu8_1213r_LNP = (Cqu8_du_LNP*SQDL(0,1)*SUL(0,2) + Cqu8_uu_LNP*SQUL(0,1)*SUL(0,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(0,1) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(0,1) + Cqu8_y_LNP*YucL(0,2)*YuL(0,1) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(0,1) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(0,1)).real();
    Cqu8_1213i_LNP = (Cqu8_du_LNP*SQDL(0,1)*SUL(0,2) + Cqu8_uu_LNP*SQUL(0,1)*SUL(0,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(0,1) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(0,1) + Cqu8_y_LNP*YucL(0,2)*YuL(0,1) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(0,1) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(0,1)).imag();
    Cqu8_1221r_LNP = (Cqu8_du_LNP*SQDL(0,1)*SUL(1,0) + Cqu8_uu_LNP*SQUL(0,1)*SUL(1,0) + Cqu8_dy_LNP*SQDYucL(0,0)*YuL(1,1) + Cqu8_uy_LNP*SQUYucL(0,0)*YuL(1,1) + Cqu8_y_LNP*YucL(0,0)*YuL(1,1) + Cqu8_yd_LNP*YucL(0,0)*YuSQDL(1,1) + Cqu8_yu_LNP*YucL(0,0)*YuSQUL(1,1)).real();
    Cqu8_1221i_LNP = (Cqu8_du_LNP*SQDL(0,1)*SUL(1,0) + Cqu8_uu_LNP*SQUL(0,1)*SUL(1,0) + Cqu8_dy_LNP*SQDYucL(0,0)*YuL(1,1) + Cqu8_uy_LNP*SQUYucL(0,0)*YuL(1,1) + Cqu8_y_LNP*YucL(0,0)*YuL(1,1) + Cqu8_yd_LNP*YucL(0,0)*YuSQDL(1,1) + Cqu8_yu_LNP*YucL(0,0)*YuSQUL(1,1)).imag();
    Cqu8_1222r_LNP = (Cqu8_d0_LNP*SQDL(0,1) + Cqu8_u0_LNP*SQUL(0,1) + Cqu8_du_LNP*SQDL(0,1)*SUL(1,1) + Cqu8_uu_LNP*SQUL(0,1)*SUL(1,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(1,1) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(1,1) + Cqu8_y_LNP*YucL(0,1)*YuL(1,1) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(1,1) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(1,1)).real();
    Cqu8_1222i_LNP = (Cqu8_d0_LNP*SQDL(0,1) + Cqu8_u0_LNP*SQUL(0,1) + Cqu8_du_LNP*SQDL(0,1)*SUL(1,1) + Cqu8_uu_LNP*SQUL(0,1)*SUL(1,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(1,1) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(1,1) + Cqu8_y_LNP*YucL(0,1)*YuL(1,1) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(1,1) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(1,1)).imag();
    Cqu8_1223r_LNP = (Cqu8_du_LNP*SQDL(0,1)*SUL(1,2) + Cqu8_uu_LNP*SQUL(0,1)*SUL(1,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(1,1) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(1,1) + Cqu8_y_LNP*YucL(0,2)*YuL(1,1) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(1,1) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(1,1)).real();
    Cqu8_1223i_LNP = (Cqu8_du_LNP*SQDL(0,1)*SUL(1,2) + Cqu8_uu_LNP*SQUL(0,1)*SUL(1,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(1,1) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(1,1) + Cqu8_y_LNP*YucL(0,2)*YuL(1,1) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(1,1) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(1,1)).imag();
    Cqu8_1231r_LNP = (Cqu8_du_LNP*SQDL(0,1)*SUL(2,0) + Cqu8_uu_LNP*SQUL(0,1)*SUL(2,0) + Cqu8_dy_LNP*SQDYucL(0,0)*YuL(2,1) + Cqu8_uy_LNP*SQUYucL(0,0)*YuL(2,1) + Cqu8_y_LNP*YucL(0,0)*YuL(2,1) + Cqu8_yd_LNP*YucL(0,0)*YuSQDL(2,1) + Cqu8_yu_LNP*YucL(0,0)*YuSQUL(2,1)).real();
    Cqu8_1231i_LNP = (Cqu8_du_LNP*SQDL(0,1)*SUL(2,0) + Cqu8_uu_LNP*SQUL(0,1)*SUL(2,0) + Cqu8_dy_LNP*SQDYucL(0,0)*YuL(2,1) + Cqu8_uy_LNP*SQUYucL(0,0)*YuL(2,1) + Cqu8_y_LNP*YucL(0,0)*YuL(2,1) + Cqu8_yd_LNP*YucL(0,0)*YuSQDL(2,1) + Cqu8_yu_LNP*YucL(0,0)*YuSQUL(2,1)).imag();
    Cqu8_1232r_LNP = (Cqu8_du_LNP*SQDL(0,1)*SUL(2,1) + Cqu8_uu_LNP*SQUL(0,1)*SUL(2,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(2,1) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(2,1) + Cqu8_y_LNP*YucL(0,1)*YuL(2,1) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(2,1) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(2,1)).real();
    Cqu8_1232i_LNP = (Cqu8_du_LNP*SQDL(0,1)*SUL(2,1) + Cqu8_uu_LNP*SQUL(0,1)*SUL(2,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(2,1) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(2,1) + Cqu8_y_LNP*YucL(0,1)*YuL(2,1) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(2,1) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(2,1)).imag();
    Cqu8_1233r_LNP = (Cqu8_d0_LNP*SQDL(0,1) + Cqu8_u0_LNP*SQUL(0,1) + Cqu8_du_LNP*SQDL(0,1)*SUL(2,2) + Cqu8_uu_LNP*SQUL(0,1)*SUL(2,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(2,1) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(2,1) + Cqu8_y_LNP*YucL(0,2)*YuL(2,1) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(2,1) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(2,1)).real();
    Cqu8_1233i_LNP = (Cqu8_d0_LNP*SQDL(0,1) + Cqu8_u0_LNP*SQUL(0,1) + Cqu8_du_LNP*SQDL(0,1)*SUL(2,2) + Cqu8_uu_LNP*SQUL(0,1)*SUL(2,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(2,1) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(2,1) + Cqu8_y_LNP*YucL(0,2)*YuL(2,1) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(2,1) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(2,1)).imag();
    Cqu8_1311r_LNP = (Cqu8_d0_LNP*SQDL(0,2) + Cqu8_u0_LNP*SQUL(0,2) + Cqu8_du_LNP*SQDL(0,2)*SUL(0,0) + Cqu8_uu_LNP*SQUL(0,2)*SUL(0,0) + Cqu8_dy_LNP*SQDYucL(0,0)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(0,0)*YuL(0,2) + Cqu8_y_LNP*YucL(0,0)*YuL(0,2) + Cqu8_yd_LNP*YucL(0,0)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(0,0)*YuSQUL(0,2)).real();
    Cqu8_1311i_LNP = (Cqu8_d0_LNP*SQDL(0,2) + Cqu8_u0_LNP*SQUL(0,2) + Cqu8_du_LNP*SQDL(0,2)*SUL(0,0) + Cqu8_uu_LNP*SQUL(0,2)*SUL(0,0) + Cqu8_dy_LNP*SQDYucL(0,0)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(0,0)*YuL(0,2) + Cqu8_y_LNP*YucL(0,0)*YuL(0,2) + Cqu8_yd_LNP*YucL(0,0)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(0,0)*YuSQUL(0,2)).imag();
    Cqu8_1312r_LNP = (Cqu8_du_LNP*SQDL(0,2)*SUL(0,1) + Cqu8_uu_LNP*SQUL(0,2)*SUL(0,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(0,2) + Cqu8_y_LNP*YucL(0,1)*YuL(0,2) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(0,2)).real();
    Cqu8_1312i_LNP = (Cqu8_du_LNP*SQDL(0,2)*SUL(0,1) + Cqu8_uu_LNP*SQUL(0,2)*SUL(0,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(0,2) + Cqu8_y_LNP*YucL(0,1)*YuL(0,2) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(0,2)).imag();
    Cqu8_1313r_LNP = (Cqu8_du_LNP*SQDL(0,2)*SUL(0,2) + Cqu8_uu_LNP*SQUL(0,2)*SUL(0,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(0,2) + Cqu8_y_LNP*YucL(0,2)*YuL(0,2) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(0,2)).real();
    Cqu8_1313i_LNP = (Cqu8_du_LNP*SQDL(0,2)*SUL(0,2) + Cqu8_uu_LNP*SQUL(0,2)*SUL(0,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(0,2) + Cqu8_y_LNP*YucL(0,2)*YuL(0,2) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(0,2)).imag();
    Cqu8_1321r_LNP = (Cqu8_du_LNP*SQDL(0,2)*SUL(1,0) + Cqu8_uu_LNP*SQUL(0,2)*SUL(1,0) + Cqu8_dy_LNP*SQDYucL(0,0)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(0,0)*YuL(1,2) + Cqu8_y_LNP*YucL(0,0)*YuL(1,2) + Cqu8_yd_LNP*YucL(0,0)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(0,0)*YuSQUL(1,2)).real();
    Cqu8_1321i_LNP = (Cqu8_du_LNP*SQDL(0,2)*SUL(1,0) + Cqu8_uu_LNP*SQUL(0,2)*SUL(1,0) + Cqu8_dy_LNP*SQDYucL(0,0)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(0,0)*YuL(1,2) + Cqu8_y_LNP*YucL(0,0)*YuL(1,2) + Cqu8_yd_LNP*YucL(0,0)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(0,0)*YuSQUL(1,2)).imag();
    Cqu8_1322r_LNP = (Cqu8_d0_LNP*SQDL(0,2) + Cqu8_u0_LNP*SQUL(0,2) + Cqu8_du_LNP*SQDL(0,2)*SUL(1,1) + Cqu8_uu_LNP*SQUL(0,2)*SUL(1,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(1,2) + Cqu8_y_LNP*YucL(0,1)*YuL(1,2) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(1,2)).real();
    Cqu8_1322i_LNP = (Cqu8_d0_LNP*SQDL(0,2) + Cqu8_u0_LNP*SQUL(0,2) + Cqu8_du_LNP*SQDL(0,2)*SUL(1,1) + Cqu8_uu_LNP*SQUL(0,2)*SUL(1,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(1,2) + Cqu8_y_LNP*YucL(0,1)*YuL(1,2) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(1,2)).imag();
    Cqu8_1323r_LNP = (Cqu8_du_LNP*SQDL(0,2)*SUL(1,2) + Cqu8_uu_LNP*SQUL(0,2)*SUL(1,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(1,2) + Cqu8_y_LNP*YucL(0,2)*YuL(1,2) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(1,2)).real();
    Cqu8_1323i_LNP = (Cqu8_du_LNP*SQDL(0,2)*SUL(1,2) + Cqu8_uu_LNP*SQUL(0,2)*SUL(1,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(1,2) + Cqu8_y_LNP*YucL(0,2)*YuL(1,2) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(1,2)).imag();
    Cqu8_1331r_LNP = (Cqu8_du_LNP*SQDL(0,2)*SUL(2,0) + Cqu8_uu_LNP*SQUL(0,2)*SUL(2,0) + Cqu8_dy_LNP*SQDYucL(0,0)*YuL(2,2) + Cqu8_uy_LNP*SQUYucL(0,0)*YuL(2,2) + Cqu8_y_LNP*YucL(0,0)*YuL(2,2) + Cqu8_yd_LNP*YucL(0,0)*YuSQDL(2,2) + Cqu8_yu_LNP*YucL(0,0)*YuSQUL(2,2)).real();
    Cqu8_1331i_LNP = (Cqu8_du_LNP*SQDL(0,2)*SUL(2,0) + Cqu8_uu_LNP*SQUL(0,2)*SUL(2,0) + Cqu8_dy_LNP*SQDYucL(0,0)*YuL(2,2) + Cqu8_uy_LNP*SQUYucL(0,0)*YuL(2,2) + Cqu8_y_LNP*YucL(0,0)*YuL(2,2) + Cqu8_yd_LNP*YucL(0,0)*YuSQDL(2,2) + Cqu8_yu_LNP*YucL(0,0)*YuSQUL(2,2)).imag();
    Cqu8_1332r_LNP = (Cqu8_du_LNP*SQDL(0,2)*SUL(2,1) + Cqu8_uu_LNP*SQUL(0,2)*SUL(2,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(2,2) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(2,2) + Cqu8_y_LNP*YucL(0,1)*YuL(2,2) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(2,2) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(2,2)).real();
    Cqu8_1332i_LNP = (Cqu8_du_LNP*SQDL(0,2)*SUL(2,1) + Cqu8_uu_LNP*SQUL(0,2)*SUL(2,1) + Cqu8_dy_LNP*SQDYucL(0,1)*YuL(2,2) + Cqu8_uy_LNP*SQUYucL(0,1)*YuL(2,2) + Cqu8_y_LNP*YucL(0,1)*YuL(2,2) + Cqu8_yd_LNP*YucL(0,1)*YuSQDL(2,2) + Cqu8_yu_LNP*YucL(0,1)*YuSQUL(2,2)).imag();
    Cqu8_1333r_LNP = (Cqu8_d0_LNP*SQDL(0,2) + Cqu8_u0_LNP*SQUL(0,2) + Cqu8_du_LNP*SQDL(0,2)*SUL(2,2) + Cqu8_uu_LNP*SQUL(0,2)*SUL(2,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(2,2) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(2,2) + Cqu8_y_LNP*YucL(0,2)*YuL(2,2) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(2,2) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(2,2)).real();
    Cqu8_1333i_LNP = (Cqu8_d0_LNP*SQDL(0,2) + Cqu8_u0_LNP*SQUL(0,2) + Cqu8_du_LNP*SQDL(0,2)*SUL(2,2) + Cqu8_uu_LNP*SQUL(0,2)*SUL(2,2) + Cqu8_dy_LNP*SQDYucL(0,2)*YuL(2,2) + Cqu8_uy_LNP*SQUYucL(0,2)*YuL(2,2) + Cqu8_y_LNP*YucL(0,2)*YuL(2,2) + Cqu8_yd_LNP*YucL(0,2)*YuSQDL(2,2) + Cqu8_yu_LNP*YucL(0,2)*YuSQUL(2,2)).imag();
    Cqu8_2211r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*SQDL(1,1) + Cqu8_u0_LNP*SQUL(1,1) + Cqu8_0u_LNP*SUL(0,0) + Cqu8_du_LNP*SQDL(1,1)*SUL(0,0) + Cqu8_uu_LNP*SQUL(1,1)*SUL(0,0) + Cqu8_dy_LNP*SQDYucL(1,0)*YuL(0,1) + Cqu8_uy_LNP*SQUYucL(1,0)*YuL(0,1) + Cqu8_y_LNP*YucL(1,0)*YuL(0,1) + Cqu8_yd_LNP*YucL(1,0)*YuSQDL(0,1) + Cqu8_yu_LNP*YucL(1,0)*YuSQUL(0,1)).real();
    Cqu8_2212r_LNP = (Cqu8_0u_LNP*SUL(0,1) + Cqu8_du_LNP*SQDL(1,1)*SUL(0,1) + Cqu8_uu_LNP*SQUL(1,1)*SUL(0,1) + Cqu8_dy_LNP*SQDYucL(1,1)*YuL(0,1) + Cqu8_uy_LNP*SQUYucL(1,1)*YuL(0,1) + Cqu8_y_LNP*YucL(1,1)*YuL(0,1) + Cqu8_yd_LNP*YucL(1,1)*YuSQDL(0,1) + Cqu8_yu_LNP*YucL(1,1)*YuSQUL(0,1)).real();
    Cqu8_2212i_LNP = (Cqu8_0u_LNP*SUL(0,1) + Cqu8_du_LNP*SQDL(1,1)*SUL(0,1) + Cqu8_uu_LNP*SQUL(1,1)*SUL(0,1) + Cqu8_dy_LNP*SQDYucL(1,1)*YuL(0,1) + Cqu8_uy_LNP*SQUYucL(1,1)*YuL(0,1) + Cqu8_y_LNP*YucL(1,1)*YuL(0,1) + Cqu8_yd_LNP*YucL(1,1)*YuSQDL(0,1) + Cqu8_yu_LNP*YucL(1,1)*YuSQUL(0,1)).imag();
    Cqu8_2213r_LNP = (Cqu8_0u_LNP*SUL(0,2) + Cqu8_du_LNP*SQDL(1,1)*SUL(0,2) + Cqu8_uu_LNP*SQUL(1,1)*SUL(0,2) + Cqu8_dy_LNP*SQDYucL(1,2)*YuL(0,1) + Cqu8_uy_LNP*SQUYucL(1,2)*YuL(0,1) + Cqu8_y_LNP*YucL(1,2)*YuL(0,1) + Cqu8_yd_LNP*YucL(1,2)*YuSQDL(0,1) + Cqu8_yu_LNP*YucL(1,2)*YuSQUL(0,1)).real();
    Cqu8_2213i_LNP = (Cqu8_0u_LNP*SUL(0,2) + Cqu8_du_LNP*SQDL(1,1)*SUL(0,2) + Cqu8_uu_LNP*SQUL(1,1)*SUL(0,2) + Cqu8_dy_LNP*SQDYucL(1,2)*YuL(0,1) + Cqu8_uy_LNP*SQUYucL(1,2)*YuL(0,1) + Cqu8_y_LNP*YucL(1,2)*YuL(0,1) + Cqu8_yd_LNP*YucL(1,2)*YuSQDL(0,1) + Cqu8_yu_LNP*YucL(1,2)*YuSQUL(0,1)).imag();
    Cqu8_2222r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*SQDL(1,1) + Cqu8_u0_LNP*SQUL(1,1) + Cqu8_0u_LNP*SUL(1,1) + Cqu8_du_LNP*SQDL(1,1)*SUL(1,1) + Cqu8_uu_LNP*SQUL(1,1)*SUL(1,1) + Cqu8_dy_LNP*SQDYucL(1,1)*YuL(1,1) + Cqu8_uy_LNP*SQUYucL(1,1)*YuL(1,1) + Cqu8_y_LNP*YucL(1,1)*YuL(1,1) + Cqu8_yd_LNP*YucL(1,1)*YuSQDL(1,1) + Cqu8_yu_LNP*YucL(1,1)*YuSQUL(1,1)).real();
    Cqu8_2223r_LNP = (Cqu8_0u_LNP*SUL(1,2) + Cqu8_du_LNP*SQDL(1,1)*SUL(1,2) + Cqu8_uu_LNP*SQUL(1,1)*SUL(1,2) + Cqu8_dy_LNP*SQDYucL(1,2)*YuL(1,1) + Cqu8_uy_LNP*SQUYucL(1,2)*YuL(1,1) + Cqu8_y_LNP*YucL(1,2)*YuL(1,1) + Cqu8_yd_LNP*YucL(1,2)*YuSQDL(1,1) + Cqu8_yu_LNP*YucL(1,2)*YuSQUL(1,1)).real();
    Cqu8_2223i_LNP = (Cqu8_0u_LNP*SUL(1,2) + Cqu8_du_LNP*SQDL(1,1)*SUL(1,2) + Cqu8_uu_LNP*SQUL(1,1)*SUL(1,2) + Cqu8_dy_LNP*SQDYucL(1,2)*YuL(1,1) + Cqu8_uy_LNP*SQUYucL(1,2)*YuL(1,1) + Cqu8_y_LNP*YucL(1,2)*YuL(1,1) + Cqu8_yd_LNP*YucL(1,2)*YuSQDL(1,1) + Cqu8_yu_LNP*YucL(1,2)*YuSQUL(1,1)).imag();
    Cqu8_2233r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*SQDL(1,1) + Cqu8_u0_LNP*SQUL(1,1) + Cqu8_0u_LNP*SUL(2,2) + Cqu8_du_LNP*SQDL(1,1)*SUL(2,2) + Cqu8_uu_LNP*SQUL(1,1)*SUL(2,2) + Cqu8_dy_LNP*SQDYucL(1,2)*YuL(2,1) + Cqu8_uy_LNP*SQUYucL(1,2)*YuL(2,1) + Cqu8_y_LNP*YucL(1,2)*YuL(2,1) + Cqu8_yd_LNP*YucL(1,2)*YuSQDL(2,1) + Cqu8_yu_LNP*YucL(1,2)*YuSQUL(2,1)).real();
    Cqu8_2311r_LNP = (Cqu8_d0_LNP*SQDL(1,2) + Cqu8_u0_LNP*SQUL(1,2) + Cqu8_du_LNP*SQDL(1,2)*SUL(0,0) + Cqu8_uu_LNP*SQUL(1,2)*SUL(0,0) + Cqu8_dy_LNP*SQDYucL(1,0)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(1,0)*YuL(0,2) + Cqu8_y_LNP*YucL(1,0)*YuL(0,2) + Cqu8_yd_LNP*YucL(1,0)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(1,0)*YuSQUL(0,2)).real();
    Cqu8_2311i_LNP = (Cqu8_d0_LNP*SQDL(1,2) + Cqu8_u0_LNP*SQUL(1,2) + Cqu8_du_LNP*SQDL(1,2)*SUL(0,0) + Cqu8_uu_LNP*SQUL(1,2)*SUL(0,0) + Cqu8_dy_LNP*SQDYucL(1,0)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(1,0)*YuL(0,2) + Cqu8_y_LNP*YucL(1,0)*YuL(0,2) + Cqu8_yd_LNP*YucL(1,0)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(1,0)*YuSQUL(0,2)).imag();
    Cqu8_2312r_LNP = (Cqu8_du_LNP*SQDL(1,2)*SUL(0,1) + Cqu8_uu_LNP*SQUL(1,2)*SUL(0,1) + Cqu8_dy_LNP*SQDYucL(1,1)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(1,1)*YuL(0,2) + Cqu8_y_LNP*YucL(1,1)*YuL(0,2) + Cqu8_yd_LNP*YucL(1,1)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(1,1)*YuSQUL(0,2)).real();
    Cqu8_2312i_LNP = (Cqu8_du_LNP*SQDL(1,2)*SUL(0,1) + Cqu8_uu_LNP*SQUL(1,2)*SUL(0,1) + Cqu8_dy_LNP*SQDYucL(1,1)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(1,1)*YuL(0,2) + Cqu8_y_LNP*YucL(1,1)*YuL(0,2) + Cqu8_yd_LNP*YucL(1,1)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(1,1)*YuSQUL(0,2)).imag();
    Cqu8_2313r_LNP = (Cqu8_du_LNP*SQDL(1,2)*SUL(0,2) + Cqu8_uu_LNP*SQUL(1,2)*SUL(0,2) + Cqu8_dy_LNP*SQDYucL(1,2)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(1,2)*YuL(0,2) + Cqu8_y_LNP*YucL(1,2)*YuL(0,2) + Cqu8_yd_LNP*YucL(1,2)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(1,2)*YuSQUL(0,2)).real();
    Cqu8_2313i_LNP = (Cqu8_du_LNP*SQDL(1,2)*SUL(0,2) + Cqu8_uu_LNP*SQUL(1,2)*SUL(0,2) + Cqu8_dy_LNP*SQDYucL(1,2)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(1,2)*YuL(0,2) + Cqu8_y_LNP*YucL(1,2)*YuL(0,2) + Cqu8_yd_LNP*YucL(1,2)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(1,2)*YuSQUL(0,2)).imag();
    Cqu8_2321r_LNP = (Cqu8_du_LNP*SQDL(1,2)*SUL(1,0) + Cqu8_uu_LNP*SQUL(1,2)*SUL(1,0) + Cqu8_dy_LNP*SQDYucL(1,0)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(1,0)*YuL(1,2) + Cqu8_y_LNP*YucL(1,0)*YuL(1,2) + Cqu8_yd_LNP*YucL(1,0)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(1,0)*YuSQUL(1,2)).real();
    Cqu8_2321i_LNP = (Cqu8_du_LNP*SQDL(1,2)*SUL(1,0) + Cqu8_uu_LNP*SQUL(1,2)*SUL(1,0) + Cqu8_dy_LNP*SQDYucL(1,0)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(1,0)*YuL(1,2) + Cqu8_y_LNP*YucL(1,0)*YuL(1,2) + Cqu8_yd_LNP*YucL(1,0)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(1,0)*YuSQUL(1,2)).imag();
    Cqu8_2322r_LNP = (Cqu8_d0_LNP*SQDL(1,2) + Cqu8_u0_LNP*SQUL(1,2) + Cqu8_du_LNP*SQDL(1,2)*SUL(1,1) + Cqu8_uu_LNP*SQUL(1,2)*SUL(1,1) + Cqu8_dy_LNP*SQDYucL(1,1)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(1,1)*YuL(1,2) + Cqu8_y_LNP*YucL(1,1)*YuL(1,2) + Cqu8_yd_LNP*YucL(1,1)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(1,1)*YuSQUL(1,2)).real();
    Cqu8_2322i_LNP = (Cqu8_d0_LNP*SQDL(1,2) + Cqu8_u0_LNP*SQUL(1,2) + Cqu8_du_LNP*SQDL(1,2)*SUL(1,1) + Cqu8_uu_LNP*SQUL(1,2)*SUL(1,1) + Cqu8_dy_LNP*SQDYucL(1,1)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(1,1)*YuL(1,2) + Cqu8_y_LNP*YucL(1,1)*YuL(1,2) + Cqu8_yd_LNP*YucL(1,1)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(1,1)*YuSQUL(1,2)).imag();
    Cqu8_2323r_LNP = (Cqu8_du_LNP*SQDL(1,2)*SUL(1,2) + Cqu8_uu_LNP*SQUL(1,2)*SUL(1,2) + Cqu8_dy_LNP*SQDYucL(1,2)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(1,2)*YuL(1,2) + Cqu8_y_LNP*YucL(1,2)*YuL(1,2) + Cqu8_yd_LNP*YucL(1,2)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(1,2)*YuSQUL(1,2)).real();
    Cqu8_2323i_LNP = (Cqu8_du_LNP*SQDL(1,2)*SUL(1,2) + Cqu8_uu_LNP*SQUL(1,2)*SUL(1,2) + Cqu8_dy_LNP*SQDYucL(1,2)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(1,2)*YuL(1,2) + Cqu8_y_LNP*YucL(1,2)*YuL(1,2) + Cqu8_yd_LNP*YucL(1,2)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(1,2)*YuSQUL(1,2)).imag();
    Cqu8_2331r_LNP = (Cqu8_du_LNP*SQDL(1,2)*SUL(2,0) + Cqu8_uu_LNP*SQUL(1,2)*SUL(2,0) + Cqu8_dy_LNP*SQDYucL(1,0)*YuL(2,2) + Cqu8_uy_LNP*SQUYucL(1,0)*YuL(2,2) + Cqu8_y_LNP*YucL(1,0)*YuL(2,2) + Cqu8_yd_LNP*YucL(1,0)*YuSQDL(2,2) + Cqu8_yu_LNP*YucL(1,0)*YuSQUL(2,2)).real();
    Cqu8_2331i_LNP = (Cqu8_du_LNP*SQDL(1,2)*SUL(2,0) + Cqu8_uu_LNP*SQUL(1,2)*SUL(2,0) + Cqu8_dy_LNP*SQDYucL(1,0)*YuL(2,2) + Cqu8_uy_LNP*SQUYucL(1,0)*YuL(2,2) + Cqu8_y_LNP*YucL(1,0)*YuL(2,2) + Cqu8_yd_LNP*YucL(1,0)*YuSQDL(2,2) + Cqu8_yu_LNP*YucL(1,0)*YuSQUL(2,2)).imag();
    Cqu8_2332r_LNP = (Cqu8_du_LNP*SQDL(1,2)*SUL(2,1) + Cqu8_uu_LNP*SQUL(1,2)*SUL(2,1) + Cqu8_dy_LNP*SQDYucL(1,1)*YuL(2,2) + Cqu8_uy_LNP*SQUYucL(1,1)*YuL(2,2) + Cqu8_y_LNP*YucL(1,1)*YuL(2,2) + Cqu8_yd_LNP*YucL(1,1)*YuSQDL(2,2) + Cqu8_yu_LNP*YucL(1,1)*YuSQUL(2,2)).real();
    Cqu8_2332i_LNP = (Cqu8_du_LNP*SQDL(1,2)*SUL(2,1) + Cqu8_uu_LNP*SQUL(1,2)*SUL(2,1) + Cqu8_dy_LNP*SQDYucL(1,1)*YuL(2,2) + Cqu8_uy_LNP*SQUYucL(1,1)*YuL(2,2) + Cqu8_y_LNP*YucL(1,1)*YuL(2,2) + Cqu8_yd_LNP*YucL(1,1)*YuSQDL(2,2) + Cqu8_yu_LNP*YucL(1,1)*YuSQUL(2,2)).imag();
    Cqu8_2333r_LNP = (Cqu8_d0_LNP*SQDL(1,2) + Cqu8_u0_LNP*SQUL(1,2) + Cqu8_du_LNP*SQDL(1,2)*SUL(2,2) + Cqu8_uu_LNP*SQUL(1,2)*SUL(2,2) + Cqu8_dy_LNP*SQDYucL(1,2)*YuL(2,2) + Cqu8_uy_LNP*SQUYucL(1,2)*YuL(2,2) + Cqu8_y_LNP*YucL(1,2)*YuL(2,2) + Cqu8_yd_LNP*YucL(1,2)*YuSQDL(2,2) + Cqu8_yu_LNP*YucL(1,2)*YuSQUL(2,2)).real();
    Cqu8_2333i_LNP = (Cqu8_d0_LNP*SQDL(1,2) + Cqu8_u0_LNP*SQUL(1,2) + Cqu8_du_LNP*SQDL(1,2)*SUL(2,2) + Cqu8_uu_LNP*SQUL(1,2)*SUL(2,2) + Cqu8_dy_LNP*SQDYucL(1,2)*YuL(2,2) + Cqu8_uy_LNP*SQUYucL(1,2)*YuL(2,2) + Cqu8_y_LNP*YucL(1,2)*YuL(2,2) + Cqu8_yd_LNP*YucL(1,2)*YuSQDL(2,2) + Cqu8_yu_LNP*YucL(1,2)*YuSQUL(2,2)).imag();
    Cqu8_3311r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*SQDL(2,2) + Cqu8_u0_LNP*SQUL(2,2) + Cqu8_0u_LNP*SUL(0,0) + Cqu8_du_LNP*SQDL(2,2)*SUL(0,0) + Cqu8_uu_LNP*SQUL(2,2)*SUL(0,0) + Cqu8_dy_LNP*SQDYucL(2,0)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(2,0)*YuL(0,2) + Cqu8_y_LNP*YucL(2,0)*YuL(0,2) + Cqu8_yd_LNP*YucL(2,0)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(2,0)*YuSQUL(0,2)).real();
    Cqu8_3312r_LNP = (Cqu8_0u_LNP*SUL(0,1) + Cqu8_du_LNP*SQDL(2,2)*SUL(0,1) + Cqu8_uu_LNP*SQUL(2,2)*SUL(0,1) + Cqu8_dy_LNP*SQDYucL(2,1)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(2,1)*YuL(0,2) + Cqu8_y_LNP*YucL(2,1)*YuL(0,2) + Cqu8_yd_LNP*YucL(2,1)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(2,1)*YuSQUL(0,2)).real();
    Cqu8_3312i_LNP = (Cqu8_0u_LNP*SUL(0,1) + Cqu8_du_LNP*SQDL(2,2)*SUL(0,1) + Cqu8_uu_LNP*SQUL(2,2)*SUL(0,1) + Cqu8_dy_LNP*SQDYucL(2,1)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(2,1)*YuL(0,2) + Cqu8_y_LNP*YucL(2,1)*YuL(0,2) + Cqu8_yd_LNP*YucL(2,1)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(2,1)*YuSQUL(0,2)).imag();
    Cqu8_3313r_LNP = (Cqu8_0u_LNP*SUL(0,2) + Cqu8_du_LNP*SQDL(2,2)*SUL(0,2) + Cqu8_uu_LNP*SQUL(2,2)*SUL(0,2) + Cqu8_dy_LNP*SQDYucL(2,2)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(2,2)*YuL(0,2) + Cqu8_y_LNP*YucL(2,2)*YuL(0,2) + Cqu8_yd_LNP*YucL(2,2)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(2,2)*YuSQUL(0,2)).real();
    Cqu8_3313i_LNP = (Cqu8_0u_LNP*SUL(0,2) + Cqu8_du_LNP*SQDL(2,2)*SUL(0,2) + Cqu8_uu_LNP*SQUL(2,2)*SUL(0,2) + Cqu8_dy_LNP*SQDYucL(2,2)*YuL(0,2) + Cqu8_uy_LNP*SQUYucL(2,2)*YuL(0,2) + Cqu8_y_LNP*YucL(2,2)*YuL(0,2) + Cqu8_yd_LNP*YucL(2,2)*YuSQDL(0,2) + Cqu8_yu_LNP*YucL(2,2)*YuSQUL(0,2)).imag();
    Cqu8_3322r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*SQDL(2,2) + Cqu8_u0_LNP*SQUL(2,2) + Cqu8_0u_LNP*SUL(1,1) + Cqu8_du_LNP*SQDL(2,2)*SUL(1,1) + Cqu8_uu_LNP*SQUL(2,2)*SUL(1,1) + Cqu8_dy_LNP*SQDYucL(2,1)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(2,1)*YuL(1,2) + Cqu8_y_LNP*YucL(2,1)*YuL(1,2) + Cqu8_yd_LNP*YucL(2,1)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(2,1)*YuSQUL(1,2)).real();
    Cqu8_3323r_LNP = (Cqu8_0u_LNP*SUL(1,2) + Cqu8_du_LNP*SQDL(2,2)*SUL(1,2) + Cqu8_uu_LNP*SQUL(2,2)*SUL(1,2) + Cqu8_dy_LNP*SQDYucL(2,2)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(2,2)*YuL(1,2) + Cqu8_y_LNP*YucL(2,2)*YuL(1,2) + Cqu8_yd_LNP*YucL(2,2)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(2,2)*YuSQUL(1,2)).real();
    Cqu8_3323i_LNP = (Cqu8_0u_LNP*SUL(1,2) + Cqu8_du_LNP*SQDL(2,2)*SUL(1,2) + Cqu8_uu_LNP*SQUL(2,2)*SUL(1,2) + Cqu8_dy_LNP*SQDYucL(2,2)*YuL(1,2) + Cqu8_uy_LNP*SQUYucL(2,2)*YuL(1,2) + Cqu8_y_LNP*YucL(2,2)*YuL(1,2) + Cqu8_yd_LNP*YucL(2,2)*YuSQDL(1,2) + Cqu8_yu_LNP*YucL(2,2)*YuSQUL(1,2)).imag();
    Cqu8_3333r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*SQDL(2,2) + Cqu8_u0_LNP*SQUL(2,2) + Cqu8_0u_LNP*SUL(2,2) + Cqu8_du_LNP*SQDL(2,2)*SUL(2,2) + Cqu8_uu_LNP*SQUL(2,2)*SUL(2,2) + Cqu8_dy_LNP*SQDYucL(2,2)*YuL(2,2) + Cqu8_uy_LNP*SQUYucL(2,2)*YuL(2,2) + Cqu8_y_LNP*YucL(2,2)*YuL(2,2) + Cqu8_yd_LNP*YucL(2,2)*YuSQDL(2,2) + Cqu8_yu_LNP*YucL(2,2)*YuSQUL(2,2)).real();
 
    Cqd1_1111r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*SDL(0,0) + Cqd1_d0_LNP*SQDL(0,0) + Cqd1_dd_LNP*SDL(0,0)*SQDL(0,0) + Cqd1_u0_LNP*SQUL(0,0) + Cqd1_ud_LNP*SDL(0,0)*SQUL(0,0) + Cqd1_yd_LNP*SQDYdcL(0,0)*YdcL(0,0) + Cqd1_dy_LNP*SQDYdcL(0,0)*YdL(0,0) + Cqd1_uy_LNP*SQUYdcL(0,0)*YdL(0,0) + Cqd1_y_LNP*YdcL(0,0)*YdL(0,0) + Cqd1_yu_LNP*YdcL(0,0)*YdSQUL(0,0)).real();
    Cqd1_1112r_LNP = (Cqd1_0d_LNP*SDL(0,1) + Cqd1_dd_LNP*SDL(0,1)*SQDL(0,0) + Cqd1_ud_LNP*SDL(0,1)*SQUL(0,0) + Cqd1_yd_LNP*SQDYdcL(0,0)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(0,0) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(0,0) + Cqd1_y_LNP*YdcL(0,1)*YdL(0,0) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(0,0)).real();
    Cqd1_1112i_LNP = (Cqd1_0d_LNP*SDL(0,1) + Cqd1_dd_LNP*SDL(0,1)*SQDL(0,0) + Cqd1_ud_LNP*SDL(0,1)*SQUL(0,0) + Cqd1_yd_LNP*SQDYdcL(0,0)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(0,0) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(0,0) + Cqd1_y_LNP*YdcL(0,1)*YdL(0,0) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(0,0)).imag();
    Cqd1_1113r_LNP = (Cqd1_0d_LNP*SDL(0,2) + Cqd1_dd_LNP*SDL(0,2)*SQDL(0,0) + Cqd1_ud_LNP*SDL(0,2)*SQUL(0,0) + Cqd1_yd_LNP*SQDYdcL(0,0)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(0,0) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(0,0) + Cqd1_y_LNP*YdcL(0,2)*YdL(0,0) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(0,0)).real();
    Cqd1_1113i_LNP = (Cqd1_0d_LNP*SDL(0,2) + Cqd1_dd_LNP*SDL(0,2)*SQDL(0,0) + Cqd1_ud_LNP*SDL(0,2)*SQUL(0,0) + Cqd1_yd_LNP*SQDYdcL(0,0)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(0,0) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(0,0) + Cqd1_y_LNP*YdcL(0,2)*YdL(0,0) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(0,0)).imag();
    Cqd1_1122r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*SDL(1,1) + Cqd1_d0_LNP*SQDL(0,0) + Cqd1_dd_LNP*SDL(1,1)*SQDL(0,0) + Cqd1_u0_LNP*SQUL(0,0) + Cqd1_ud_LNP*SDL(1,1)*SQUL(0,0) + Cqd1_yd_LNP*SQDYdcL(1,0)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(1,0) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(1,0) + Cqd1_y_LNP*YdcL(0,1)*YdL(1,0) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(1,0)).real();
    Cqd1_1123r_LNP = (Cqd1_0d_LNP*SDL(1,2) + Cqd1_dd_LNP*SDL(1,2)*SQDL(0,0) + Cqd1_ud_LNP*SDL(1,2)*SQUL(0,0) + Cqd1_yd_LNP*SQDYdcL(1,0)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(1,0) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(1,0) + Cqd1_y_LNP*YdcL(0,2)*YdL(1,0) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(1,0)).real();
    Cqd1_1123i_LNP = (Cqd1_0d_LNP*SDL(1,2) + Cqd1_dd_LNP*SDL(1,2)*SQDL(0,0) + Cqd1_ud_LNP*SDL(1,2)*SQUL(0,0) + Cqd1_yd_LNP*SQDYdcL(1,0)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(1,0) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(1,0) + Cqd1_y_LNP*YdcL(0,2)*YdL(1,0) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(1,0)).imag();
    Cqd1_1133r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*SDL(2,2) + Cqd1_d0_LNP*SQDL(0,0) + Cqd1_dd_LNP*SDL(2,2)*SQDL(0,0) + Cqd1_u0_LNP*SQUL(0,0) + Cqd1_ud_LNP*SDL(2,2)*SQUL(0,0) + Cqd1_yd_LNP*SQDYdcL(2,0)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(2,0) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(2,0) + Cqd1_y_LNP*YdcL(0,2)*YdL(2,0) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(2,0)).real();
    Cqd1_1211r_LNP = (Cqd1_d0_LNP*SQDL(0,1) + Cqd1_dd_LNP*SDL(0,0)*SQDL(0,1) + Cqd1_u0_LNP*SQUL(0,1) + Cqd1_ud_LNP*SDL(0,0)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(0,1)*YdcL(0,0) + Cqd1_dy_LNP*SQDYdcL(0,0)*YdL(0,1) + Cqd1_uy_LNP*SQUYdcL(0,0)*YdL(0,1) + Cqd1_y_LNP*YdcL(0,0)*YdL(0,1) + Cqd1_yu_LNP*YdcL(0,0)*YdSQUL(0,1)).real();
    Cqd1_1211i_LNP = (Cqd1_d0_LNP*SQDL(0,1) + Cqd1_dd_LNP*SDL(0,0)*SQDL(0,1) + Cqd1_u0_LNP*SQUL(0,1) + Cqd1_ud_LNP*SDL(0,0)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(0,1)*YdcL(0,0) + Cqd1_dy_LNP*SQDYdcL(0,0)*YdL(0,1) + Cqd1_uy_LNP*SQUYdcL(0,0)*YdL(0,1) + Cqd1_y_LNP*YdcL(0,0)*YdL(0,1) + Cqd1_yu_LNP*YdcL(0,0)*YdSQUL(0,1)).imag();
    Cqd1_1212r_LNP = (Cqd1_dd_LNP*SDL(0,1)*SQDL(0,1) + Cqd1_ud_LNP*SDL(0,1)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(0,1)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(0,1) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(0,1) + Cqd1_y_LNP*YdcL(0,1)*YdL(0,1) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(0,1)).real();
    Cqd1_1212i_LNP = (Cqd1_dd_LNP*SDL(0,1)*SQDL(0,1) + Cqd1_ud_LNP*SDL(0,1)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(0,1)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(0,1) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(0,1) + Cqd1_y_LNP*YdcL(0,1)*YdL(0,1) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(0,1)).imag();
    Cqd1_1213r_LNP = (Cqd1_dd_LNP*SDL(0,2)*SQDL(0,1) + Cqd1_ud_LNP*SDL(0,2)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(0,1)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(0,1) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(0,1) + Cqd1_y_LNP*YdcL(0,2)*YdL(0,1) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(0,1)).real();
    Cqd1_1213i_LNP = (Cqd1_dd_LNP*SDL(0,2)*SQDL(0,1) + Cqd1_ud_LNP*SDL(0,2)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(0,1)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(0,1) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(0,1) + Cqd1_y_LNP*YdcL(0,2)*YdL(0,1) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(0,1)).imag();
    Cqd1_1221r_LNP = (Cqd1_dd_LNP*SDL(1,0)*SQDL(0,1) + Cqd1_ud_LNP*SDL(1,0)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(1,1)*YdcL(0,0) + Cqd1_dy_LNP*SQDYdcL(0,0)*YdL(1,1) + Cqd1_uy_LNP*SQUYdcL(0,0)*YdL(1,1) + Cqd1_y_LNP*YdcL(0,0)*YdL(1,1) + Cqd1_yu_LNP*YdcL(0,0)*YdSQUL(1,1)).real();
    Cqd1_1221i_LNP = (Cqd1_dd_LNP*SDL(1,0)*SQDL(0,1) + Cqd1_ud_LNP*SDL(1,0)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(1,1)*YdcL(0,0) + Cqd1_dy_LNP*SQDYdcL(0,0)*YdL(1,1) + Cqd1_uy_LNP*SQUYdcL(0,0)*YdL(1,1) + Cqd1_y_LNP*YdcL(0,0)*YdL(1,1) + Cqd1_yu_LNP*YdcL(0,0)*YdSQUL(1,1)).imag();
    Cqd1_1222r_LNP = (Cqd1_d0_LNP*SQDL(0,1) + Cqd1_dd_LNP*SDL(1,1)*SQDL(0,1) + Cqd1_u0_LNP*SQUL(0,1) + Cqd1_ud_LNP*SDL(1,1)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(1,1)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(1,1) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(1,1) + Cqd1_y_LNP*YdcL(0,1)*YdL(1,1) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(1,1)).real();
    Cqd1_1222i_LNP = (Cqd1_d0_LNP*SQDL(0,1) + Cqd1_dd_LNP*SDL(1,1)*SQDL(0,1) + Cqd1_u0_LNP*SQUL(0,1) + Cqd1_ud_LNP*SDL(1,1)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(1,1)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(1,1) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(1,1) + Cqd1_y_LNP*YdcL(0,1)*YdL(1,1) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(1,1)).imag();
    Cqd1_1223r_LNP = (Cqd1_dd_LNP*SDL(1,2)*SQDL(0,1) + Cqd1_ud_LNP*SDL(1,2)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(1,1)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(1,1) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(1,1) + Cqd1_y_LNP*YdcL(0,2)*YdL(1,1) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(1,1)).real();
    Cqd1_1223i_LNP = (Cqd1_dd_LNP*SDL(1,2)*SQDL(0,1) + Cqd1_ud_LNP*SDL(1,2)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(1,1)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(1,1) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(1,1) + Cqd1_y_LNP*YdcL(0,2)*YdL(1,1) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(1,1)).imag();
    Cqd1_1231r_LNP = (Cqd1_dd_LNP*SDL(2,0)*SQDL(0,1) + Cqd1_ud_LNP*SDL(2,0)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(2,1)*YdcL(0,0) + Cqd1_dy_LNP*SQDYdcL(0,0)*YdL(2,1) + Cqd1_uy_LNP*SQUYdcL(0,0)*YdL(2,1) + Cqd1_y_LNP*YdcL(0,0)*YdL(2,1) + Cqd1_yu_LNP*YdcL(0,0)*YdSQUL(2,1)).real();
    Cqd1_1231i_LNP = (Cqd1_dd_LNP*SDL(2,0)*SQDL(0,1) + Cqd1_ud_LNP*SDL(2,0)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(2,1)*YdcL(0,0) + Cqd1_dy_LNP*SQDYdcL(0,0)*YdL(2,1) + Cqd1_uy_LNP*SQUYdcL(0,0)*YdL(2,1) + Cqd1_y_LNP*YdcL(0,0)*YdL(2,1) + Cqd1_yu_LNP*YdcL(0,0)*YdSQUL(2,1)).imag();
    Cqd1_1232r_LNP = (Cqd1_dd_LNP*SDL(2,1)*SQDL(0,1) + Cqd1_ud_LNP*SDL(2,1)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(2,1)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(2,1) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(2,1) + Cqd1_y_LNP*YdcL(0,1)*YdL(2,1) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(2,1)).real();
    Cqd1_1232i_LNP = (Cqd1_dd_LNP*SDL(2,1)*SQDL(0,1) + Cqd1_ud_LNP*SDL(2,1)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(2,1)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(2,1) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(2,1) + Cqd1_y_LNP*YdcL(0,1)*YdL(2,1) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(2,1)).imag();
    Cqd1_1233r_LNP = (Cqd1_d0_LNP*SQDL(0,1) + Cqd1_dd_LNP*SDL(2,2)*SQDL(0,1) + Cqd1_u0_LNP*SQUL(0,1) + Cqd1_ud_LNP*SDL(2,2)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(2,1)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(2,1) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(2,1) + Cqd1_y_LNP*YdcL(0,2)*YdL(2,1) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(2,1)).real();
    Cqd1_1233i_LNP = (Cqd1_d0_LNP*SQDL(0,1) + Cqd1_dd_LNP*SDL(2,2)*SQDL(0,1) + Cqd1_u0_LNP*SQUL(0,1) + Cqd1_ud_LNP*SDL(2,2)*SQUL(0,1) + Cqd1_yd_LNP*SQDYdcL(2,1)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(2,1) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(2,1) + Cqd1_y_LNP*YdcL(0,2)*YdL(2,1) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(2,1)).imag();
    Cqd1_1311r_LNP = (Cqd1_d0_LNP*SQDL(0,2) + Cqd1_dd_LNP*SDL(0,0)*SQDL(0,2) + Cqd1_u0_LNP*SQUL(0,2) + Cqd1_ud_LNP*SDL(0,0)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(0,0) + Cqd1_dy_LNP*SQDYdcL(0,0)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(0,0)*YdL(0,2) + Cqd1_y_LNP*YdcL(0,0)*YdL(0,2) + Cqd1_yu_LNP*YdcL(0,0)*YdSQUL(0,2)).real();
    Cqd1_1311i_LNP = (Cqd1_d0_LNP*SQDL(0,2) + Cqd1_dd_LNP*SDL(0,0)*SQDL(0,2) + Cqd1_u0_LNP*SQUL(0,2) + Cqd1_ud_LNP*SDL(0,0)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(0,0) + Cqd1_dy_LNP*SQDYdcL(0,0)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(0,0)*YdL(0,2) + Cqd1_y_LNP*YdcL(0,0)*YdL(0,2) + Cqd1_yu_LNP*YdcL(0,0)*YdSQUL(0,2)).imag();
    Cqd1_1312r_LNP = (Cqd1_dd_LNP*SDL(0,1)*SQDL(0,2) + Cqd1_ud_LNP*SDL(0,1)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(0,2) + Cqd1_y_LNP*YdcL(0,1)*YdL(0,2) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(0,2)).real();
    Cqd1_1312i_LNP = (Cqd1_dd_LNP*SDL(0,1)*SQDL(0,2) + Cqd1_ud_LNP*SDL(0,1)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(0,2) + Cqd1_y_LNP*YdcL(0,1)*YdL(0,2) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(0,2)).imag();
    Cqd1_1313r_LNP = (Cqd1_dd_LNP*SDL(0,2)*SQDL(0,2) + Cqd1_ud_LNP*SDL(0,2)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(0,2) + Cqd1_y_LNP*YdcL(0,2)*YdL(0,2) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(0,2)).real();
    Cqd1_1313i_LNP = (Cqd1_dd_LNP*SDL(0,2)*SQDL(0,2) + Cqd1_ud_LNP*SDL(0,2)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(0,2) + Cqd1_y_LNP*YdcL(0,2)*YdL(0,2) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(0,2)).imag();
    Cqd1_1321r_LNP = (Cqd1_dd_LNP*SDL(1,0)*SQDL(0,2) + Cqd1_ud_LNP*SDL(1,0)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(0,0) + Cqd1_dy_LNP*SQDYdcL(0,0)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(0,0)*YdL(1,2) + Cqd1_y_LNP*YdcL(0,0)*YdL(1,2) + Cqd1_yu_LNP*YdcL(0,0)*YdSQUL(1,2)).real();
    Cqd1_1321i_LNP = (Cqd1_dd_LNP*SDL(1,0)*SQDL(0,2) + Cqd1_ud_LNP*SDL(1,0)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(0,0) + Cqd1_dy_LNP*SQDYdcL(0,0)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(0,0)*YdL(1,2) + Cqd1_y_LNP*YdcL(0,0)*YdL(1,2) + Cqd1_yu_LNP*YdcL(0,0)*YdSQUL(1,2)).imag();
    Cqd1_1322r_LNP = (Cqd1_d0_LNP*SQDL(0,2) + Cqd1_dd_LNP*SDL(1,1)*SQDL(0,2) + Cqd1_u0_LNP*SQUL(0,2) + Cqd1_ud_LNP*SDL(1,1)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(1,2) + Cqd1_y_LNP*YdcL(0,1)*YdL(1,2) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(1,2)).real();
    Cqd1_1322i_LNP = (Cqd1_d0_LNP*SQDL(0,2) + Cqd1_dd_LNP*SDL(1,1)*SQDL(0,2) + Cqd1_u0_LNP*SQUL(0,2) + Cqd1_ud_LNP*SDL(1,1)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(1,2) + Cqd1_y_LNP*YdcL(0,1)*YdL(1,2) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(1,2)).imag();
    Cqd1_1323r_LNP = (Cqd1_dd_LNP*SDL(1,2)*SQDL(0,2) + Cqd1_ud_LNP*SDL(1,2)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(1,2) + Cqd1_y_LNP*YdcL(0,2)*YdL(1,2) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(1,2)).real();
    Cqd1_1323i_LNP = (Cqd1_dd_LNP*SDL(1,2)*SQDL(0,2) + Cqd1_ud_LNP*SDL(1,2)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(1,2) + Cqd1_y_LNP*YdcL(0,2)*YdL(1,2) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(1,2)).imag();
    Cqd1_1331r_LNP = (Cqd1_dd_LNP*SDL(2,0)*SQDL(0,2) + Cqd1_ud_LNP*SDL(2,0)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(2,2)*YdcL(0,0) + Cqd1_dy_LNP*SQDYdcL(0,0)*YdL(2,2) + Cqd1_uy_LNP*SQUYdcL(0,0)*YdL(2,2) + Cqd1_y_LNP*YdcL(0,0)*YdL(2,2) + Cqd1_yu_LNP*YdcL(0,0)*YdSQUL(2,2)).real();
    Cqd1_1331i_LNP = (Cqd1_dd_LNP*SDL(2,0)*SQDL(0,2) + Cqd1_ud_LNP*SDL(2,0)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(2,2)*YdcL(0,0) + Cqd1_dy_LNP*SQDYdcL(0,0)*YdL(2,2) + Cqd1_uy_LNP*SQUYdcL(0,0)*YdL(2,2) + Cqd1_y_LNP*YdcL(0,0)*YdL(2,2) + Cqd1_yu_LNP*YdcL(0,0)*YdSQUL(2,2)).imag();
    Cqd1_1332r_LNP = (Cqd1_dd_LNP*SDL(2,1)*SQDL(0,2) + Cqd1_ud_LNP*SDL(2,1)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(2,2)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(2,2) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(2,2) + Cqd1_y_LNP*YdcL(0,1)*YdL(2,2) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(2,2)).real();
    Cqd1_1332i_LNP = (Cqd1_dd_LNP*SDL(2,1)*SQDL(0,2) + Cqd1_ud_LNP*SDL(2,1)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(2,2)*YdcL(0,1) + Cqd1_dy_LNP*SQDYdcL(0,1)*YdL(2,2) + Cqd1_uy_LNP*SQUYdcL(0,1)*YdL(2,2) + Cqd1_y_LNP*YdcL(0,1)*YdL(2,2) + Cqd1_yu_LNP*YdcL(0,1)*YdSQUL(2,2)).imag();
    Cqd1_1333r_LNP = (Cqd1_d0_LNP*SQDL(0,2) + Cqd1_dd_LNP*SDL(2,2)*SQDL(0,2) + Cqd1_u0_LNP*SQUL(0,2) + Cqd1_ud_LNP*SDL(2,2)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(2,2)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(2,2) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(2,2) + Cqd1_y_LNP*YdcL(0,2)*YdL(2,2) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(2,2)).real();
    Cqd1_1333i_LNP = (Cqd1_d0_LNP*SQDL(0,2) + Cqd1_dd_LNP*SDL(2,2)*SQDL(0,2) + Cqd1_u0_LNP*SQUL(0,2) + Cqd1_ud_LNP*SDL(2,2)*SQUL(0,2) + Cqd1_yd_LNP*SQDYdcL(2,2)*YdcL(0,2) + Cqd1_dy_LNP*SQDYdcL(0,2)*YdL(2,2) + Cqd1_uy_LNP*SQUYdcL(0,2)*YdL(2,2) + Cqd1_y_LNP*YdcL(0,2)*YdL(2,2) + Cqd1_yu_LNP*YdcL(0,2)*YdSQUL(2,2)).imag();
    Cqd1_2211r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*SDL(0,0) + Cqd1_d0_LNP*SQDL(1,1) + Cqd1_dd_LNP*SDL(0,0)*SQDL(1,1) + Cqd1_u0_LNP*SQUL(1,1) + Cqd1_ud_LNP*SDL(0,0)*SQUL(1,1) + Cqd1_yd_LNP*SQDYdcL(0,1)*YdcL(1,0) + Cqd1_dy_LNP*SQDYdcL(1,0)*YdL(0,1) + Cqd1_uy_LNP*SQUYdcL(1,0)*YdL(0,1) + Cqd1_y_LNP*YdcL(1,0)*YdL(0,1) + Cqd1_yu_LNP*YdcL(1,0)*YdSQUL(0,1)).real();
    Cqd1_2212r_LNP = (Cqd1_0d_LNP*SDL(0,1) + Cqd1_dd_LNP*SDL(0,1)*SQDL(1,1) + Cqd1_ud_LNP*SDL(0,1)*SQUL(1,1) + Cqd1_yd_LNP*SQDYdcL(0,1)*YdcL(1,1) + Cqd1_dy_LNP*SQDYdcL(1,1)*YdL(0,1) + Cqd1_uy_LNP*SQUYdcL(1,1)*YdL(0,1) + Cqd1_y_LNP*YdcL(1,1)*YdL(0,1) + Cqd1_yu_LNP*YdcL(1,1)*YdSQUL(0,1)).real();
    Cqd1_2212i_LNP = (Cqd1_0d_LNP*SDL(0,1) + Cqd1_dd_LNP*SDL(0,1)*SQDL(1,1) + Cqd1_ud_LNP*SDL(0,1)*SQUL(1,1) + Cqd1_yd_LNP*SQDYdcL(0,1)*YdcL(1,1) + Cqd1_dy_LNP*SQDYdcL(1,1)*YdL(0,1) + Cqd1_uy_LNP*SQUYdcL(1,1)*YdL(0,1) + Cqd1_y_LNP*YdcL(1,1)*YdL(0,1) + Cqd1_yu_LNP*YdcL(1,1)*YdSQUL(0,1)).imag();
    Cqd1_2213r_LNP = (Cqd1_0d_LNP*SDL(0,2) + Cqd1_dd_LNP*SDL(0,2)*SQDL(1,1) + Cqd1_ud_LNP*SDL(0,2)*SQUL(1,1) + Cqd1_yd_LNP*SQDYdcL(0,1)*YdcL(1,2) + Cqd1_dy_LNP*SQDYdcL(1,2)*YdL(0,1) + Cqd1_uy_LNP*SQUYdcL(1,2)*YdL(0,1) + Cqd1_y_LNP*YdcL(1,2)*YdL(0,1) + Cqd1_yu_LNP*YdcL(1,2)*YdSQUL(0,1)).real();
    Cqd1_2213i_LNP = (Cqd1_0d_LNP*SDL(0,2) + Cqd1_dd_LNP*SDL(0,2)*SQDL(1,1) + Cqd1_ud_LNP*SDL(0,2)*SQUL(1,1) + Cqd1_yd_LNP*SQDYdcL(0,1)*YdcL(1,2) + Cqd1_dy_LNP*SQDYdcL(1,2)*YdL(0,1) + Cqd1_uy_LNP*SQUYdcL(1,2)*YdL(0,1) + Cqd1_y_LNP*YdcL(1,2)*YdL(0,1) + Cqd1_yu_LNP*YdcL(1,2)*YdSQUL(0,1)).imag();
    Cqd1_2222r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*SDL(1,1) + Cqd1_d0_LNP*SQDL(1,1) + Cqd1_dd_LNP*SDL(1,1)*SQDL(1,1) + Cqd1_u0_LNP*SQUL(1,1) + Cqd1_ud_LNP*SDL(1,1)*SQUL(1,1) + Cqd1_yd_LNP*SQDYdcL(1,1)*YdcL(1,1) + Cqd1_dy_LNP*SQDYdcL(1,1)*YdL(1,1) + Cqd1_uy_LNP*SQUYdcL(1,1)*YdL(1,1) + Cqd1_y_LNP*YdcL(1,1)*YdL(1,1) + Cqd1_yu_LNP*YdcL(1,1)*YdSQUL(1,1)).real();
    Cqd1_2223r_LNP = (Cqd1_0d_LNP*SDL(1,2) + Cqd1_dd_LNP*SDL(1,2)*SQDL(1,1) + Cqd1_ud_LNP*SDL(1,2)*SQUL(1,1) + Cqd1_yd_LNP*SQDYdcL(1,1)*YdcL(1,2) + Cqd1_dy_LNP*SQDYdcL(1,2)*YdL(1,1) + Cqd1_uy_LNP*SQUYdcL(1,2)*YdL(1,1) + Cqd1_y_LNP*YdcL(1,2)*YdL(1,1) + Cqd1_yu_LNP*YdcL(1,2)*YdSQUL(1,1)).real();
    Cqd1_2223i_LNP = (Cqd1_0d_LNP*SDL(1,2) + Cqd1_dd_LNP*SDL(1,2)*SQDL(1,1) + Cqd1_ud_LNP*SDL(1,2)*SQUL(1,1) + Cqd1_yd_LNP*SQDYdcL(1,1)*YdcL(1,2) + Cqd1_dy_LNP*SQDYdcL(1,2)*YdL(1,1) + Cqd1_uy_LNP*SQUYdcL(1,2)*YdL(1,1) + Cqd1_y_LNP*YdcL(1,2)*YdL(1,1) + Cqd1_yu_LNP*YdcL(1,2)*YdSQUL(1,1)).imag();
    Cqd1_2233r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*SDL(2,2) + Cqd1_d0_LNP*SQDL(1,1) + Cqd1_dd_LNP*SDL(2,2)*SQDL(1,1) + Cqd1_u0_LNP*SQUL(1,1) + Cqd1_ud_LNP*SDL(2,2)*SQUL(1,1) + Cqd1_yd_LNP*SQDYdcL(2,1)*YdcL(1,2) + Cqd1_dy_LNP*SQDYdcL(1,2)*YdL(2,1) + Cqd1_uy_LNP*SQUYdcL(1,2)*YdL(2,1) + Cqd1_y_LNP*YdcL(1,2)*YdL(2,1) + Cqd1_yu_LNP*YdcL(1,2)*YdSQUL(2,1)).real();
    Cqd1_2311r_LNP = (Cqd1_d0_LNP*SQDL(1,2) + Cqd1_dd_LNP*SDL(0,0)*SQDL(1,2) + Cqd1_u0_LNP*SQUL(1,2) + Cqd1_ud_LNP*SDL(0,0)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(1,0) + Cqd1_dy_LNP*SQDYdcL(1,0)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(1,0)*YdL(0,2) + Cqd1_y_LNP*YdcL(1,0)*YdL(0,2) + Cqd1_yu_LNP*YdcL(1,0)*YdSQUL(0,2)).real();
    Cqd1_2311i_LNP = (Cqd1_d0_LNP*SQDL(1,2) + Cqd1_dd_LNP*SDL(0,0)*SQDL(1,2) + Cqd1_u0_LNP*SQUL(1,2) + Cqd1_ud_LNP*SDL(0,0)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(1,0) + Cqd1_dy_LNP*SQDYdcL(1,0)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(1,0)*YdL(0,2) + Cqd1_y_LNP*YdcL(1,0)*YdL(0,2) + Cqd1_yu_LNP*YdcL(1,0)*YdSQUL(0,2)).imag();
    Cqd1_2312r_LNP = (Cqd1_dd_LNP*SDL(0,1)*SQDL(1,2) + Cqd1_ud_LNP*SDL(0,1)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(1,1) + Cqd1_dy_LNP*SQDYdcL(1,1)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(1,1)*YdL(0,2) + Cqd1_y_LNP*YdcL(1,1)*YdL(0,2) + Cqd1_yu_LNP*YdcL(1,1)*YdSQUL(0,2)).real();
    Cqd1_2312i_LNP = (Cqd1_dd_LNP*SDL(0,1)*SQDL(1,2) + Cqd1_ud_LNP*SDL(0,1)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(1,1) + Cqd1_dy_LNP*SQDYdcL(1,1)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(1,1)*YdL(0,2) + Cqd1_y_LNP*YdcL(1,1)*YdL(0,2) + Cqd1_yu_LNP*YdcL(1,1)*YdSQUL(0,2)).imag();
    Cqd1_2313r_LNP = (Cqd1_dd_LNP*SDL(0,2)*SQDL(1,2) + Cqd1_ud_LNP*SDL(0,2)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(1,2) + Cqd1_dy_LNP*SQDYdcL(1,2)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(1,2)*YdL(0,2) + Cqd1_y_LNP*YdcL(1,2)*YdL(0,2) + Cqd1_yu_LNP*YdcL(1,2)*YdSQUL(0,2)).real();
    Cqd1_2313i_LNP = (Cqd1_dd_LNP*SDL(0,2)*SQDL(1,2) + Cqd1_ud_LNP*SDL(0,2)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(1,2) + Cqd1_dy_LNP*SQDYdcL(1,2)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(1,2)*YdL(0,2) + Cqd1_y_LNP*YdcL(1,2)*YdL(0,2) + Cqd1_yu_LNP*YdcL(1,2)*YdSQUL(0,2)).imag();
    Cqd1_2321r_LNP = (Cqd1_dd_LNP*SDL(1,0)*SQDL(1,2) + Cqd1_ud_LNP*SDL(1,0)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(1,0) + Cqd1_dy_LNP*SQDYdcL(1,0)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(1,0)*YdL(1,2) + Cqd1_y_LNP*YdcL(1,0)*YdL(1,2) + Cqd1_yu_LNP*YdcL(1,0)*YdSQUL(1,2)).real();
    Cqd1_2321i_LNP = (Cqd1_dd_LNP*SDL(1,0)*SQDL(1,2) + Cqd1_ud_LNP*SDL(1,0)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(1,0) + Cqd1_dy_LNP*SQDYdcL(1,0)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(1,0)*YdL(1,2) + Cqd1_y_LNP*YdcL(1,0)*YdL(1,2) + Cqd1_yu_LNP*YdcL(1,0)*YdSQUL(1,2)).imag();
    Cqd1_2322r_LNP = (Cqd1_d0_LNP*SQDL(1,2) + Cqd1_dd_LNP*SDL(1,1)*SQDL(1,2) + Cqd1_u0_LNP*SQUL(1,2) + Cqd1_ud_LNP*SDL(1,1)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(1,1) + Cqd1_dy_LNP*SQDYdcL(1,1)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(1,1)*YdL(1,2) + Cqd1_y_LNP*YdcL(1,1)*YdL(1,2) + Cqd1_yu_LNP*YdcL(1,1)*YdSQUL(1,2)).real();
    Cqd1_2322i_LNP = (Cqd1_d0_LNP*SQDL(1,2) + Cqd1_dd_LNP*SDL(1,1)*SQDL(1,2) + Cqd1_u0_LNP*SQUL(1,2) + Cqd1_ud_LNP*SDL(1,1)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(1,1) + Cqd1_dy_LNP*SQDYdcL(1,1)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(1,1)*YdL(1,2) + Cqd1_y_LNP*YdcL(1,1)*YdL(1,2) + Cqd1_yu_LNP*YdcL(1,1)*YdSQUL(1,2)).imag();
    Cqd1_2323r_LNP = (Cqd1_dd_LNP*SDL(1,2)*SQDL(1,2) + Cqd1_ud_LNP*SDL(1,2)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(1,2) + Cqd1_dy_LNP*SQDYdcL(1,2)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(1,2)*YdL(1,2) + Cqd1_y_LNP*YdcL(1,2)*YdL(1,2) + Cqd1_yu_LNP*YdcL(1,2)*YdSQUL(1,2)).real();
    Cqd1_2323i_LNP = (Cqd1_dd_LNP*SDL(1,2)*SQDL(1,2) + Cqd1_ud_LNP*SDL(1,2)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(1,2) + Cqd1_dy_LNP*SQDYdcL(1,2)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(1,2)*YdL(1,2) + Cqd1_y_LNP*YdcL(1,2)*YdL(1,2) + Cqd1_yu_LNP*YdcL(1,2)*YdSQUL(1,2)).imag();
    Cqd1_2331r_LNP = (Cqd1_dd_LNP*SDL(2,0)*SQDL(1,2) + Cqd1_ud_LNP*SDL(2,0)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(2,2)*YdcL(1,0) + Cqd1_dy_LNP*SQDYdcL(1,0)*YdL(2,2) + Cqd1_uy_LNP*SQUYdcL(1,0)*YdL(2,2) + Cqd1_y_LNP*YdcL(1,0)*YdL(2,2) + Cqd1_yu_LNP*YdcL(1,0)*YdSQUL(2,2)).real();
    Cqd1_2331i_LNP = (Cqd1_dd_LNP*SDL(2,0)*SQDL(1,2) + Cqd1_ud_LNP*SDL(2,0)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(2,2)*YdcL(1,0) + Cqd1_dy_LNP*SQDYdcL(1,0)*YdL(2,2) + Cqd1_uy_LNP*SQUYdcL(1,0)*YdL(2,2) + Cqd1_y_LNP*YdcL(1,0)*YdL(2,2) + Cqd1_yu_LNP*YdcL(1,0)*YdSQUL(2,2)).imag();
    Cqd1_2332r_LNP = (Cqd1_dd_LNP*SDL(2,1)*SQDL(1,2) + Cqd1_ud_LNP*SDL(2,1)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(2,2)*YdcL(1,1) + Cqd1_dy_LNP*SQDYdcL(1,1)*YdL(2,2) + Cqd1_uy_LNP*SQUYdcL(1,1)*YdL(2,2) + Cqd1_y_LNP*YdcL(1,1)*YdL(2,2) + Cqd1_yu_LNP*YdcL(1,1)*YdSQUL(2,2)).real();
    Cqd1_2332i_LNP = (Cqd1_dd_LNP*SDL(2,1)*SQDL(1,2) + Cqd1_ud_LNP*SDL(2,1)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(2,2)*YdcL(1,1) + Cqd1_dy_LNP*SQDYdcL(1,1)*YdL(2,2) + Cqd1_uy_LNP*SQUYdcL(1,1)*YdL(2,2) + Cqd1_y_LNP*YdcL(1,1)*YdL(2,2) + Cqd1_yu_LNP*YdcL(1,1)*YdSQUL(2,2)).imag();
    Cqd1_2333r_LNP = (Cqd1_d0_LNP*SQDL(1,2) + Cqd1_dd_LNP*SDL(2,2)*SQDL(1,2) + Cqd1_u0_LNP*SQUL(1,2) + Cqd1_ud_LNP*SDL(2,2)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(2,2)*YdcL(1,2) + Cqd1_dy_LNP*SQDYdcL(1,2)*YdL(2,2) + Cqd1_uy_LNP*SQUYdcL(1,2)*YdL(2,2) + Cqd1_y_LNP*YdcL(1,2)*YdL(2,2) + Cqd1_yu_LNP*YdcL(1,2)*YdSQUL(2,2)).real();
    Cqd1_2333i_LNP = (Cqd1_d0_LNP*SQDL(1,2) + Cqd1_dd_LNP*SDL(2,2)*SQDL(1,2) + Cqd1_u0_LNP*SQUL(1,2) + Cqd1_ud_LNP*SDL(2,2)*SQUL(1,2) + Cqd1_yd_LNP*SQDYdcL(2,2)*YdcL(1,2) + Cqd1_dy_LNP*SQDYdcL(1,2)*YdL(2,2) + Cqd1_uy_LNP*SQUYdcL(1,2)*YdL(2,2) + Cqd1_y_LNP*YdcL(1,2)*YdL(2,2) + Cqd1_yu_LNP*YdcL(1,2)*YdSQUL(2,2)).imag();
    Cqd1_3311r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*SDL(0,0) + Cqd1_d0_LNP*SQDL(2,2) + Cqd1_dd_LNP*SDL(0,0)*SQDL(2,2) + Cqd1_u0_LNP*SQUL(2,2) + Cqd1_ud_LNP*SDL(0,0)*SQUL(2,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(2,0) + Cqd1_dy_LNP*SQDYdcL(2,0)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(2,0)*YdL(0,2) + Cqd1_y_LNP*YdcL(2,0)*YdL(0,2) + Cqd1_yu_LNP*YdcL(2,0)*YdSQUL(0,2)).real();
    Cqd1_3312r_LNP = (Cqd1_0d_LNP*SDL(0,1) + Cqd1_dd_LNP*SDL(0,1)*SQDL(2,2) + Cqd1_ud_LNP*SDL(0,1)*SQUL(2,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(2,1) + Cqd1_dy_LNP*SQDYdcL(2,1)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(2,1)*YdL(0,2) + Cqd1_y_LNP*YdcL(2,1)*YdL(0,2) + Cqd1_yu_LNP*YdcL(2,1)*YdSQUL(0,2)).real();
    Cqd1_3312i_LNP = (Cqd1_0d_LNP*SDL(0,1) + Cqd1_dd_LNP*SDL(0,1)*SQDL(2,2) + Cqd1_ud_LNP*SDL(0,1)*SQUL(2,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(2,1) + Cqd1_dy_LNP*SQDYdcL(2,1)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(2,1)*YdL(0,2) + Cqd1_y_LNP*YdcL(2,1)*YdL(0,2) + Cqd1_yu_LNP*YdcL(2,1)*YdSQUL(0,2)).imag();
    Cqd1_3313r_LNP = (Cqd1_0d_LNP*SDL(0,2) + Cqd1_dd_LNP*SDL(0,2)*SQDL(2,2) + Cqd1_ud_LNP*SDL(0,2)*SQUL(2,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(2,2) + Cqd1_dy_LNP*SQDYdcL(2,2)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(2,2)*YdL(0,2) + Cqd1_y_LNP*YdcL(2,2)*YdL(0,2) + Cqd1_yu_LNP*YdcL(2,2)*YdSQUL(0,2)).real();
    Cqd1_3313i_LNP = (Cqd1_0d_LNP*SDL(0,2) + Cqd1_dd_LNP*SDL(0,2)*SQDL(2,2) + Cqd1_ud_LNP*SDL(0,2)*SQUL(2,2) + Cqd1_yd_LNP*SQDYdcL(0,2)*YdcL(2,2) + Cqd1_dy_LNP*SQDYdcL(2,2)*YdL(0,2) + Cqd1_uy_LNP*SQUYdcL(2,2)*YdL(0,2) + Cqd1_y_LNP*YdcL(2,2)*YdL(0,2) + Cqd1_yu_LNP*YdcL(2,2)*YdSQUL(0,2)).imag();
    Cqd1_3322r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*SDL(1,1) + Cqd1_d0_LNP*SQDL(2,2) + Cqd1_dd_LNP*SDL(1,1)*SQDL(2,2) + Cqd1_u0_LNP*SQUL(2,2) + Cqd1_ud_LNP*SDL(1,1)*SQUL(2,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(2,1) + Cqd1_dy_LNP*SQDYdcL(2,1)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(2,1)*YdL(1,2) + Cqd1_y_LNP*YdcL(2,1)*YdL(1,2) + Cqd1_yu_LNP*YdcL(2,1)*YdSQUL(1,2)).real();
    Cqd1_3323r_LNP = (Cqd1_0d_LNP*SDL(1,2) + Cqd1_dd_LNP*SDL(1,2)*SQDL(2,2) + Cqd1_ud_LNP*SDL(1,2)*SQUL(2,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(2,2) + Cqd1_dy_LNP*SQDYdcL(2,2)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(2,2)*YdL(1,2) + Cqd1_y_LNP*YdcL(2,2)*YdL(1,2) + Cqd1_yu_LNP*YdcL(2,2)*YdSQUL(1,2)).real();
    Cqd1_3323i_LNP = (Cqd1_0d_LNP*SDL(1,2) + Cqd1_dd_LNP*SDL(1,2)*SQDL(2,2) + Cqd1_ud_LNP*SDL(1,2)*SQUL(2,2) + Cqd1_yd_LNP*SQDYdcL(1,2)*YdcL(2,2) + Cqd1_dy_LNP*SQDYdcL(2,2)*YdL(1,2) + Cqd1_uy_LNP*SQUYdcL(2,2)*YdL(1,2) + Cqd1_y_LNP*YdcL(2,2)*YdL(1,2) + Cqd1_yu_LNP*YdcL(2,2)*YdSQUL(1,2)).imag();
    Cqd1_3333r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*SDL(2,2) + Cqd1_d0_LNP*SQDL(2,2) + Cqd1_dd_LNP*SDL(2,2)*SQDL(2,2) + Cqd1_u0_LNP*SQUL(2,2) + Cqd1_ud_LNP*SDL(2,2)*SQUL(2,2) + Cqd1_yd_LNP*SQDYdcL(2,2)*YdcL(2,2) + Cqd1_dy_LNP*SQDYdcL(2,2)*YdL(2,2) + Cqd1_uy_LNP*SQUYdcL(2,2)*YdL(2,2) + Cqd1_y_LNP*YdcL(2,2)*YdL(2,2) + Cqd1_yu_LNP*YdcL(2,2)*YdSQUL(2,2)).real();
 
    Cqd8_1111r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*SDL(0,0) + Cqd8_d0_LNP*SQDL(0,0) + Cqd8_dd_LNP*SDL(0,0)*SQDL(0,0) + Cqd8_u0_LNP*SQUL(0,0) + Cqd8_ud_LNP*SDL(0,0)*SQUL(0,0) + Cqd8_yd_LNP*SQDYdcL(0,0)*YdcL(0,0) + Cqd8_dy_LNP*SQDYdcL(0,0)*YdL(0,0) + Cqd8_uy_LNP*SQUYdcL(0,0)*YdL(0,0) + Cqd8_y_LNP*YdcL(0,0)*YdL(0,0) + Cqd8_yu_LNP*YdcL(0,0)*YdSQUL(0,0)).real();
    Cqd8_1112r_LNP = (Cqd8_0d_LNP*SDL(0,1) + Cqd8_dd_LNP*SDL(0,1)*SQDL(0,0) + Cqd8_ud_LNP*SDL(0,1)*SQUL(0,0) + Cqd8_yd_LNP*SQDYdcL(0,0)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(0,0) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(0,0) + Cqd8_y_LNP*YdcL(0,1)*YdL(0,0) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(0,0)).real();
    Cqd8_1112i_LNP = (Cqd8_0d_LNP*SDL(0,1) + Cqd8_dd_LNP*SDL(0,1)*SQDL(0,0) + Cqd8_ud_LNP*SDL(0,1)*SQUL(0,0) + Cqd8_yd_LNP*SQDYdcL(0,0)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(0,0) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(0,0) + Cqd8_y_LNP*YdcL(0,1)*YdL(0,0) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(0,0)).imag();
    Cqd8_1113r_LNP = (Cqd8_0d_LNP*SDL(0,2) + Cqd8_dd_LNP*SDL(0,2)*SQDL(0,0) + Cqd8_ud_LNP*SDL(0,2)*SQUL(0,0) + Cqd8_yd_LNP*SQDYdcL(0,0)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(0,0) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(0,0) + Cqd8_y_LNP*YdcL(0,2)*YdL(0,0) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(0,0)).real();
    Cqd8_1113i_LNP = (Cqd8_0d_LNP*SDL(0,2) + Cqd8_dd_LNP*SDL(0,2)*SQDL(0,0) + Cqd8_ud_LNP*SDL(0,2)*SQUL(0,0) + Cqd8_yd_LNP*SQDYdcL(0,0)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(0,0) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(0,0) + Cqd8_y_LNP*YdcL(0,2)*YdL(0,0) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(0,0)).imag();
    Cqd8_1122r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*SDL(1,1) + Cqd8_d0_LNP*SQDL(0,0) + Cqd8_dd_LNP*SDL(1,1)*SQDL(0,0) + Cqd8_u0_LNP*SQUL(0,0) + Cqd8_ud_LNP*SDL(1,1)*SQUL(0,0) + Cqd8_yd_LNP*SQDYdcL(1,0)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(1,0) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(1,0) + Cqd8_y_LNP*YdcL(0,1)*YdL(1,0) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(1,0)).real();
    Cqd8_1123r_LNP = (Cqd8_0d_LNP*SDL(1,2) + Cqd8_dd_LNP*SDL(1,2)*SQDL(0,0) + Cqd8_ud_LNP*SDL(1,2)*SQUL(0,0) + Cqd8_yd_LNP*SQDYdcL(1,0)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(1,0) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(1,0) + Cqd8_y_LNP*YdcL(0,2)*YdL(1,0) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(1,0)).real();
    Cqd8_1123i_LNP = (Cqd8_0d_LNP*SDL(1,2) + Cqd8_dd_LNP*SDL(1,2)*SQDL(0,0) + Cqd8_ud_LNP*SDL(1,2)*SQUL(0,0) + Cqd8_yd_LNP*SQDYdcL(1,0)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(1,0) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(1,0) + Cqd8_y_LNP*YdcL(0,2)*YdL(1,0) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(1,0)).imag();
    Cqd8_1133r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*SDL(2,2) + Cqd8_d0_LNP*SQDL(0,0) + Cqd8_dd_LNP*SDL(2,2)*SQDL(0,0) + Cqd8_u0_LNP*SQUL(0,0) + Cqd8_ud_LNP*SDL(2,2)*SQUL(0,0) + Cqd8_yd_LNP*SQDYdcL(2,0)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(2,0) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(2,0) + Cqd8_y_LNP*YdcL(0,2)*YdL(2,0) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(2,0)).real();
    Cqd8_1211r_LNP = (Cqd8_d0_LNP*SQDL(0,1) + Cqd8_dd_LNP*SDL(0,0)*SQDL(0,1) + Cqd8_u0_LNP*SQUL(0,1) + Cqd8_ud_LNP*SDL(0,0)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(0,1)*YdcL(0,0) + Cqd8_dy_LNP*SQDYdcL(0,0)*YdL(0,1) + Cqd8_uy_LNP*SQUYdcL(0,0)*YdL(0,1) + Cqd8_y_LNP*YdcL(0,0)*YdL(0,1) + Cqd8_yu_LNP*YdcL(0,0)*YdSQUL(0,1)).real();
    Cqd8_1211i_LNP = (Cqd8_d0_LNP*SQDL(0,1) + Cqd8_dd_LNP*SDL(0,0)*SQDL(0,1) + Cqd8_u0_LNP*SQUL(0,1) + Cqd8_ud_LNP*SDL(0,0)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(0,1)*YdcL(0,0) + Cqd8_dy_LNP*SQDYdcL(0,0)*YdL(0,1) + Cqd8_uy_LNP*SQUYdcL(0,0)*YdL(0,1) + Cqd8_y_LNP*YdcL(0,0)*YdL(0,1) + Cqd8_yu_LNP*YdcL(0,0)*YdSQUL(0,1)).imag();
    Cqd8_1212r_LNP = (Cqd8_dd_LNP*SDL(0,1)*SQDL(0,1) + Cqd8_ud_LNP*SDL(0,1)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(0,1)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(0,1) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(0,1) + Cqd8_y_LNP*YdcL(0,1)*YdL(0,1) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(0,1)).real();
    Cqd8_1212i_LNP = (Cqd8_dd_LNP*SDL(0,1)*SQDL(0,1) + Cqd8_ud_LNP*SDL(0,1)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(0,1)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(0,1) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(0,1) + Cqd8_y_LNP*YdcL(0,1)*YdL(0,1) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(0,1)).imag();
    Cqd8_1213r_LNP = (Cqd8_dd_LNP*SDL(0,2)*SQDL(0,1) + Cqd8_ud_LNP*SDL(0,2)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(0,1)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(0,1) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(0,1) + Cqd8_y_LNP*YdcL(0,2)*YdL(0,1) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(0,1)).real();
    Cqd8_1213i_LNP = (Cqd8_dd_LNP*SDL(0,2)*SQDL(0,1) + Cqd8_ud_LNP*SDL(0,2)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(0,1)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(0,1) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(0,1) + Cqd8_y_LNP*YdcL(0,2)*YdL(0,1) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(0,1)).imag();
    Cqd8_1221r_LNP = (Cqd8_dd_LNP*SDL(1,0)*SQDL(0,1) + Cqd8_ud_LNP*SDL(1,0)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(1,1)*YdcL(0,0) + Cqd8_dy_LNP*SQDYdcL(0,0)*YdL(1,1) + Cqd8_uy_LNP*SQUYdcL(0,0)*YdL(1,1) + Cqd8_y_LNP*YdcL(0,0)*YdL(1,1) + Cqd8_yu_LNP*YdcL(0,0)*YdSQUL(1,1)).real();
    Cqd8_1221i_LNP = (Cqd8_dd_LNP*SDL(1,0)*SQDL(0,1) + Cqd8_ud_LNP*SDL(1,0)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(1,1)*YdcL(0,0) + Cqd8_dy_LNP*SQDYdcL(0,0)*YdL(1,1) + Cqd8_uy_LNP*SQUYdcL(0,0)*YdL(1,1) + Cqd8_y_LNP*YdcL(0,0)*YdL(1,1) + Cqd8_yu_LNP*YdcL(0,0)*YdSQUL(1,1)).imag();
    Cqd8_1222r_LNP = (Cqd8_d0_LNP*SQDL(0,1) + Cqd8_dd_LNP*SDL(1,1)*SQDL(0,1) + Cqd8_u0_LNP*SQUL(0,1) + Cqd8_ud_LNP*SDL(1,1)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(1,1)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(1,1) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(1,1) + Cqd8_y_LNP*YdcL(0,1)*YdL(1,1) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(1,1)).real();
    Cqd8_1222i_LNP = (Cqd8_d0_LNP*SQDL(0,1) + Cqd8_dd_LNP*SDL(1,1)*SQDL(0,1) + Cqd8_u0_LNP*SQUL(0,1) + Cqd8_ud_LNP*SDL(1,1)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(1,1)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(1,1) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(1,1) + Cqd8_y_LNP*YdcL(0,1)*YdL(1,1) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(1,1)).imag();
    Cqd8_1223r_LNP = (Cqd8_dd_LNP*SDL(1,2)*SQDL(0,1) + Cqd8_ud_LNP*SDL(1,2)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(1,1)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(1,1) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(1,1) + Cqd8_y_LNP*YdcL(0,2)*YdL(1,1) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(1,1)).real();
    Cqd8_1223i_LNP = (Cqd8_dd_LNP*SDL(1,2)*SQDL(0,1) + Cqd8_ud_LNP*SDL(1,2)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(1,1)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(1,1) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(1,1) + Cqd8_y_LNP*YdcL(0,2)*YdL(1,1) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(1,1)).imag();
    Cqd8_1231r_LNP = (Cqd8_dd_LNP*SDL(2,0)*SQDL(0,1) + Cqd8_ud_LNP*SDL(2,0)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(2,1)*YdcL(0,0) + Cqd8_dy_LNP*SQDYdcL(0,0)*YdL(2,1) + Cqd8_uy_LNP*SQUYdcL(0,0)*YdL(2,1) + Cqd8_y_LNP*YdcL(0,0)*YdL(2,1) + Cqd8_yu_LNP*YdcL(0,0)*YdSQUL(2,1)).real();
    Cqd8_1231i_LNP = (Cqd8_dd_LNP*SDL(2,0)*SQDL(0,1) + Cqd8_ud_LNP*SDL(2,0)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(2,1)*YdcL(0,0) + Cqd8_dy_LNP*SQDYdcL(0,0)*YdL(2,1) + Cqd8_uy_LNP*SQUYdcL(0,0)*YdL(2,1) + Cqd8_y_LNP*YdcL(0,0)*YdL(2,1) + Cqd8_yu_LNP*YdcL(0,0)*YdSQUL(2,1)).imag();
    Cqd8_1232r_LNP = (Cqd8_dd_LNP*SDL(2,1)*SQDL(0,1) + Cqd8_ud_LNP*SDL(2,1)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(2,1)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(2,1) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(2,1) + Cqd8_y_LNP*YdcL(0,1)*YdL(2,1) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(2,1)).real();
    Cqd8_1232i_LNP = (Cqd8_dd_LNP*SDL(2,1)*SQDL(0,1) + Cqd8_ud_LNP*SDL(2,1)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(2,1)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(2,1) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(2,1) + Cqd8_y_LNP*YdcL(0,1)*YdL(2,1) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(2,1)).imag();
    Cqd8_1233r_LNP = (Cqd8_d0_LNP*SQDL(0,1) + Cqd8_dd_LNP*SDL(2,2)*SQDL(0,1) + Cqd8_u0_LNP*SQUL(0,1) + Cqd8_ud_LNP*SDL(2,2)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(2,1)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(2,1) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(2,1) + Cqd8_y_LNP*YdcL(0,2)*YdL(2,1) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(2,1)).real();
    Cqd8_1233i_LNP = (Cqd8_d0_LNP*SQDL(0,1) + Cqd8_dd_LNP*SDL(2,2)*SQDL(0,1) + Cqd8_u0_LNP*SQUL(0,1) + Cqd8_ud_LNP*SDL(2,2)*SQUL(0,1) + Cqd8_yd_LNP*SQDYdcL(2,1)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(2,1) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(2,1) + Cqd8_y_LNP*YdcL(0,2)*YdL(2,1) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(2,1)).imag();
    Cqd8_1311r_LNP = (Cqd8_d0_LNP*SQDL(0,2) + Cqd8_dd_LNP*SDL(0,0)*SQDL(0,2) + Cqd8_u0_LNP*SQUL(0,2) + Cqd8_ud_LNP*SDL(0,0)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(0,0) + Cqd8_dy_LNP*SQDYdcL(0,0)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(0,0)*YdL(0,2) + Cqd8_y_LNP*YdcL(0,0)*YdL(0,2) + Cqd8_yu_LNP*YdcL(0,0)*YdSQUL(0,2)).real();
    Cqd8_1311i_LNP = (Cqd8_d0_LNP*SQDL(0,2) + Cqd8_dd_LNP*SDL(0,0)*SQDL(0,2) + Cqd8_u0_LNP*SQUL(0,2) + Cqd8_ud_LNP*SDL(0,0)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(0,0) + Cqd8_dy_LNP*SQDYdcL(0,0)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(0,0)*YdL(0,2) + Cqd8_y_LNP*YdcL(0,0)*YdL(0,2) + Cqd8_yu_LNP*YdcL(0,0)*YdSQUL(0,2)).imag();
    Cqd8_1312r_LNP = (Cqd8_dd_LNP*SDL(0,1)*SQDL(0,2) + Cqd8_ud_LNP*SDL(0,1)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(0,2) + Cqd8_y_LNP*YdcL(0,1)*YdL(0,2) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(0,2)).real();
    Cqd8_1312i_LNP = (Cqd8_dd_LNP*SDL(0,1)*SQDL(0,2) + Cqd8_ud_LNP*SDL(0,1)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(0,2) + Cqd8_y_LNP*YdcL(0,1)*YdL(0,2) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(0,2)).imag();
    Cqd8_1313r_LNP = (Cqd8_dd_LNP*SDL(0,2)*SQDL(0,2) + Cqd8_ud_LNP*SDL(0,2)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(0,2) + Cqd8_y_LNP*YdcL(0,2)*YdL(0,2) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(0,2)).real();
    Cqd8_1313i_LNP = (Cqd8_dd_LNP*SDL(0,2)*SQDL(0,2) + Cqd8_ud_LNP*SDL(0,2)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(0,2) + Cqd8_y_LNP*YdcL(0,2)*YdL(0,2) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(0,2)).imag();
    Cqd8_1321r_LNP = (Cqd8_dd_LNP*SDL(1,0)*SQDL(0,2) + Cqd8_ud_LNP*SDL(1,0)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(0,0) + Cqd8_dy_LNP*SQDYdcL(0,0)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(0,0)*YdL(1,2) + Cqd8_y_LNP*YdcL(0,0)*YdL(1,2) + Cqd8_yu_LNP*YdcL(0,0)*YdSQUL(1,2)).real();
    Cqd8_1321i_LNP = (Cqd8_dd_LNP*SDL(1,0)*SQDL(0,2) + Cqd8_ud_LNP*SDL(1,0)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(0,0) + Cqd8_dy_LNP*SQDYdcL(0,0)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(0,0)*YdL(1,2) + Cqd8_y_LNP*YdcL(0,0)*YdL(1,2) + Cqd8_yu_LNP*YdcL(0,0)*YdSQUL(1,2)).imag();
    Cqd8_1322r_LNP = (Cqd8_d0_LNP*SQDL(0,2) + Cqd8_dd_LNP*SDL(1,1)*SQDL(0,2) + Cqd8_u0_LNP*SQUL(0,2) + Cqd8_ud_LNP*SDL(1,1)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(1,2) + Cqd8_y_LNP*YdcL(0,1)*YdL(1,2) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(1,2)).real();
    Cqd8_1322i_LNP = (Cqd8_d0_LNP*SQDL(0,2) + Cqd8_dd_LNP*SDL(1,1)*SQDL(0,2) + Cqd8_u0_LNP*SQUL(0,2) + Cqd8_ud_LNP*SDL(1,1)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(1,2) + Cqd8_y_LNP*YdcL(0,1)*YdL(1,2) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(1,2)).imag();
    Cqd8_1323r_LNP = (Cqd8_dd_LNP*SDL(1,2)*SQDL(0,2) + Cqd8_ud_LNP*SDL(1,2)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(1,2) + Cqd8_y_LNP*YdcL(0,2)*YdL(1,2) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(1,2)).real();
    Cqd8_1323i_LNP = (Cqd8_dd_LNP*SDL(1,2)*SQDL(0,2) + Cqd8_ud_LNP*SDL(1,2)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(1,2) + Cqd8_y_LNP*YdcL(0,2)*YdL(1,2) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(1,2)).imag();
    Cqd8_1331r_LNP = (Cqd8_dd_LNP*SDL(2,0)*SQDL(0,2) + Cqd8_ud_LNP*SDL(2,0)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(2,2)*YdcL(0,0) + Cqd8_dy_LNP*SQDYdcL(0,0)*YdL(2,2) + Cqd8_uy_LNP*SQUYdcL(0,0)*YdL(2,2) + Cqd8_y_LNP*YdcL(0,0)*YdL(2,2) + Cqd8_yu_LNP*YdcL(0,0)*YdSQUL(2,2)).real();
    Cqd8_1331i_LNP = (Cqd8_dd_LNP*SDL(2,0)*SQDL(0,2) + Cqd8_ud_LNP*SDL(2,0)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(2,2)*YdcL(0,0) + Cqd8_dy_LNP*SQDYdcL(0,0)*YdL(2,2) + Cqd8_uy_LNP*SQUYdcL(0,0)*YdL(2,2) + Cqd8_y_LNP*YdcL(0,0)*YdL(2,2) + Cqd8_yu_LNP*YdcL(0,0)*YdSQUL(2,2)).imag();
    Cqd8_1332r_LNP = (Cqd8_dd_LNP*SDL(2,1)*SQDL(0,2) + Cqd8_ud_LNP*SDL(2,1)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(2,2)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(2,2) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(2,2) + Cqd8_y_LNP*YdcL(0,1)*YdL(2,2) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(2,2)).real();
    Cqd8_1332i_LNP = (Cqd8_dd_LNP*SDL(2,1)*SQDL(0,2) + Cqd8_ud_LNP*SDL(2,1)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(2,2)*YdcL(0,1) + Cqd8_dy_LNP*SQDYdcL(0,1)*YdL(2,2) + Cqd8_uy_LNP*SQUYdcL(0,1)*YdL(2,2) + Cqd8_y_LNP*YdcL(0,1)*YdL(2,2) + Cqd8_yu_LNP*YdcL(0,1)*YdSQUL(2,2)).imag();
    Cqd8_1333r_LNP = (Cqd8_d0_LNP*SQDL(0,2) + Cqd8_dd_LNP*SDL(2,2)*SQDL(0,2) + Cqd8_u0_LNP*SQUL(0,2) + Cqd8_ud_LNP*SDL(2,2)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(2,2)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(2,2) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(2,2) + Cqd8_y_LNP*YdcL(0,2)*YdL(2,2) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(2,2)).real();
    Cqd8_1333i_LNP = (Cqd8_d0_LNP*SQDL(0,2) + Cqd8_dd_LNP*SDL(2,2)*SQDL(0,2) + Cqd8_u0_LNP*SQUL(0,2) + Cqd8_ud_LNP*SDL(2,2)*SQUL(0,2) + Cqd8_yd_LNP*SQDYdcL(2,2)*YdcL(0,2) + Cqd8_dy_LNP*SQDYdcL(0,2)*YdL(2,2) + Cqd8_uy_LNP*SQUYdcL(0,2)*YdL(2,2) + Cqd8_y_LNP*YdcL(0,2)*YdL(2,2) + Cqd8_yu_LNP*YdcL(0,2)*YdSQUL(2,2)).imag();
    Cqd8_2211r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*SDL(0,0) + Cqd8_d0_LNP*SQDL(1,1) + Cqd8_dd_LNP*SDL(0,0)*SQDL(1,1) + Cqd8_u0_LNP*SQUL(1,1) + Cqd8_ud_LNP*SDL(0,0)*SQUL(1,1) + Cqd8_yd_LNP*SQDYdcL(0,1)*YdcL(1,0) + Cqd8_dy_LNP*SQDYdcL(1,0)*YdL(0,1) + Cqd8_uy_LNP*SQUYdcL(1,0)*YdL(0,1) + Cqd8_y_LNP*YdcL(1,0)*YdL(0,1) + Cqd8_yu_LNP*YdcL(1,0)*YdSQUL(0,1)).real();
    Cqd8_2212r_LNP = (Cqd8_0d_LNP*SDL(0,1) + Cqd8_dd_LNP*SDL(0,1)*SQDL(1,1) + Cqd8_ud_LNP*SDL(0,1)*SQUL(1,1) + Cqd8_yd_LNP*SQDYdcL(0,1)*YdcL(1,1) + Cqd8_dy_LNP*SQDYdcL(1,1)*YdL(0,1) + Cqd8_uy_LNP*SQUYdcL(1,1)*YdL(0,1) + Cqd8_y_LNP*YdcL(1,1)*YdL(0,1) + Cqd8_yu_LNP*YdcL(1,1)*YdSQUL(0,1)).real();
    Cqd8_2212i_LNP = (Cqd8_0d_LNP*SDL(0,1) + Cqd8_dd_LNP*SDL(0,1)*SQDL(1,1) + Cqd8_ud_LNP*SDL(0,1)*SQUL(1,1) + Cqd8_yd_LNP*SQDYdcL(0,1)*YdcL(1,1) + Cqd8_dy_LNP*SQDYdcL(1,1)*YdL(0,1) + Cqd8_uy_LNP*SQUYdcL(1,1)*YdL(0,1) + Cqd8_y_LNP*YdcL(1,1)*YdL(0,1) + Cqd8_yu_LNP*YdcL(1,1)*YdSQUL(0,1)).imag();
    Cqd8_2213r_LNP = (Cqd8_0d_LNP*SDL(0,2) + Cqd8_dd_LNP*SDL(0,2)*SQDL(1,1) + Cqd8_ud_LNP*SDL(0,2)*SQUL(1,1) + Cqd8_yd_LNP*SQDYdcL(0,1)*YdcL(1,2) + Cqd8_dy_LNP*SQDYdcL(1,2)*YdL(0,1) + Cqd8_uy_LNP*SQUYdcL(1,2)*YdL(0,1) + Cqd8_y_LNP*YdcL(1,2)*YdL(0,1) + Cqd8_yu_LNP*YdcL(1,2)*YdSQUL(0,1)).real();
    Cqd8_2213i_LNP = (Cqd8_0d_LNP*SDL(0,2) + Cqd8_dd_LNP*SDL(0,2)*SQDL(1,1) + Cqd8_ud_LNP*SDL(0,2)*SQUL(1,1) + Cqd8_yd_LNP*SQDYdcL(0,1)*YdcL(1,2) + Cqd8_dy_LNP*SQDYdcL(1,2)*YdL(0,1) + Cqd8_uy_LNP*SQUYdcL(1,2)*YdL(0,1) + Cqd8_y_LNP*YdcL(1,2)*YdL(0,1) + Cqd8_yu_LNP*YdcL(1,2)*YdSQUL(0,1)).imag();
    Cqd8_2222r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*SDL(1,1) + Cqd8_d0_LNP*SQDL(1,1) + Cqd8_dd_LNP*SDL(1,1)*SQDL(1,1) + Cqd8_u0_LNP*SQUL(1,1) + Cqd8_ud_LNP*SDL(1,1)*SQUL(1,1) + Cqd8_yd_LNP*SQDYdcL(1,1)*YdcL(1,1) + Cqd8_dy_LNP*SQDYdcL(1,1)*YdL(1,1) + Cqd8_uy_LNP*SQUYdcL(1,1)*YdL(1,1) + Cqd8_y_LNP*YdcL(1,1)*YdL(1,1) + Cqd8_yu_LNP*YdcL(1,1)*YdSQUL(1,1)).real();
    Cqd8_2223r_LNP = (Cqd8_0d_LNP*SDL(1,2) + Cqd8_dd_LNP*SDL(1,2)*SQDL(1,1) + Cqd8_ud_LNP*SDL(1,2)*SQUL(1,1) + Cqd8_yd_LNP*SQDYdcL(1,1)*YdcL(1,2) + Cqd8_dy_LNP*SQDYdcL(1,2)*YdL(1,1) + Cqd8_uy_LNP*SQUYdcL(1,2)*YdL(1,1) + Cqd8_y_LNP*YdcL(1,2)*YdL(1,1) + Cqd8_yu_LNP*YdcL(1,2)*YdSQUL(1,1)).real();
    Cqd8_2223i_LNP = (Cqd8_0d_LNP*SDL(1,2) + Cqd8_dd_LNP*SDL(1,2)*SQDL(1,1) + Cqd8_ud_LNP*SDL(1,2)*SQUL(1,1) + Cqd8_yd_LNP*SQDYdcL(1,1)*YdcL(1,2) + Cqd8_dy_LNP*SQDYdcL(1,2)*YdL(1,1) + Cqd8_uy_LNP*SQUYdcL(1,2)*YdL(1,1) + Cqd8_y_LNP*YdcL(1,2)*YdL(1,1) + Cqd8_yu_LNP*YdcL(1,2)*YdSQUL(1,1)).imag();
    Cqd8_2233r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*SDL(2,2) + Cqd8_d0_LNP*SQDL(1,1) + Cqd8_dd_LNP*SDL(2,2)*SQDL(1,1) + Cqd8_u0_LNP*SQUL(1,1) + Cqd8_ud_LNP*SDL(2,2)*SQUL(1,1) + Cqd8_yd_LNP*SQDYdcL(2,1)*YdcL(1,2) + Cqd8_dy_LNP*SQDYdcL(1,2)*YdL(2,1) + Cqd8_uy_LNP*SQUYdcL(1,2)*YdL(2,1) + Cqd8_y_LNP*YdcL(1,2)*YdL(2,1) + Cqd8_yu_LNP*YdcL(1,2)*YdSQUL(2,1)).real();
    Cqd8_2311r_LNP = (Cqd8_d0_LNP*SQDL(1,2) + Cqd8_dd_LNP*SDL(0,0)*SQDL(1,2) + Cqd8_u0_LNP*SQUL(1,2) + Cqd8_ud_LNP*SDL(0,0)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(1,0) + Cqd8_dy_LNP*SQDYdcL(1,0)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(1,0)*YdL(0,2) + Cqd8_y_LNP*YdcL(1,0)*YdL(0,2) + Cqd8_yu_LNP*YdcL(1,0)*YdSQUL(0,2)).real();
    Cqd8_2311i_LNP = (Cqd8_d0_LNP*SQDL(1,2) + Cqd8_dd_LNP*SDL(0,0)*SQDL(1,2) + Cqd8_u0_LNP*SQUL(1,2) + Cqd8_ud_LNP*SDL(0,0)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(1,0) + Cqd8_dy_LNP*SQDYdcL(1,0)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(1,0)*YdL(0,2) + Cqd8_y_LNP*YdcL(1,0)*YdL(0,2) + Cqd8_yu_LNP*YdcL(1,0)*YdSQUL(0,2)).imag();
    Cqd8_2312r_LNP = (Cqd8_dd_LNP*SDL(0,1)*SQDL(1,2) + Cqd8_ud_LNP*SDL(0,1)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(1,1) + Cqd8_dy_LNP*SQDYdcL(1,1)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(1,1)*YdL(0,2) + Cqd8_y_LNP*YdcL(1,1)*YdL(0,2) + Cqd8_yu_LNP*YdcL(1,1)*YdSQUL(0,2)).real();
    Cqd8_2312i_LNP = (Cqd8_dd_LNP*SDL(0,1)*SQDL(1,2) + Cqd8_ud_LNP*SDL(0,1)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(1,1) + Cqd8_dy_LNP*SQDYdcL(1,1)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(1,1)*YdL(0,2) + Cqd8_y_LNP*YdcL(1,1)*YdL(0,2) + Cqd8_yu_LNP*YdcL(1,1)*YdSQUL(0,2)).imag();
    Cqd8_2313r_LNP = (Cqd8_dd_LNP*SDL(0,2)*SQDL(1,2) + Cqd8_ud_LNP*SDL(0,2)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(1,2) + Cqd8_dy_LNP*SQDYdcL(1,2)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(1,2)*YdL(0,2) + Cqd8_y_LNP*YdcL(1,2)*YdL(0,2) + Cqd8_yu_LNP*YdcL(1,2)*YdSQUL(0,2)).real();
    Cqd8_2313i_LNP = (Cqd8_dd_LNP*SDL(0,2)*SQDL(1,2) + Cqd8_ud_LNP*SDL(0,2)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(1,2) + Cqd8_dy_LNP*SQDYdcL(1,2)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(1,2)*YdL(0,2) + Cqd8_y_LNP*YdcL(1,2)*YdL(0,2) + Cqd8_yu_LNP*YdcL(1,2)*YdSQUL(0,2)).imag();
    Cqd8_2321r_LNP = (Cqd8_dd_LNP*SDL(1,0)*SQDL(1,2) + Cqd8_ud_LNP*SDL(1,0)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(1,0) + Cqd8_dy_LNP*SQDYdcL(1,0)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(1,0)*YdL(1,2) + Cqd8_y_LNP*YdcL(1,0)*YdL(1,2) + Cqd8_yu_LNP*YdcL(1,0)*YdSQUL(1,2)).real();
    Cqd8_2321i_LNP = (Cqd8_dd_LNP*SDL(1,0)*SQDL(1,2) + Cqd8_ud_LNP*SDL(1,0)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(1,0) + Cqd8_dy_LNP*SQDYdcL(1,0)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(1,0)*YdL(1,2) + Cqd8_y_LNP*YdcL(1,0)*YdL(1,2) + Cqd8_yu_LNP*YdcL(1,0)*YdSQUL(1,2)).imag();
    Cqd8_2322r_LNP = (Cqd8_d0_LNP*SQDL(1,2) + Cqd8_dd_LNP*SDL(1,1)*SQDL(1,2) + Cqd8_u0_LNP*SQUL(1,2) + Cqd8_ud_LNP*SDL(1,1)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(1,1) + Cqd8_dy_LNP*SQDYdcL(1,1)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(1,1)*YdL(1,2) + Cqd8_y_LNP*YdcL(1,1)*YdL(1,2) + Cqd8_yu_LNP*YdcL(1,1)*YdSQUL(1,2)).real();
    Cqd8_2322i_LNP = (Cqd8_d0_LNP*SQDL(1,2) + Cqd8_dd_LNP*SDL(1,1)*SQDL(1,2) + Cqd8_u0_LNP*SQUL(1,2) + Cqd8_ud_LNP*SDL(1,1)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(1,1) + Cqd8_dy_LNP*SQDYdcL(1,1)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(1,1)*YdL(1,2) + Cqd8_y_LNP*YdcL(1,1)*YdL(1,2) + Cqd8_yu_LNP*YdcL(1,1)*YdSQUL(1,2)).imag();
    Cqd8_2323r_LNP = (Cqd8_dd_LNP*SDL(1,2)*SQDL(1,2) + Cqd8_ud_LNP*SDL(1,2)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(1,2) + Cqd8_dy_LNP*SQDYdcL(1,2)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(1,2)*YdL(1,2) + Cqd8_y_LNP*YdcL(1,2)*YdL(1,2) + Cqd8_yu_LNP*YdcL(1,2)*YdSQUL(1,2)).real();
    Cqd8_2323i_LNP = (Cqd8_dd_LNP*SDL(1,2)*SQDL(1,2) + Cqd8_ud_LNP*SDL(1,2)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(1,2) + Cqd8_dy_LNP*SQDYdcL(1,2)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(1,2)*YdL(1,2) + Cqd8_y_LNP*YdcL(1,2)*YdL(1,2) + Cqd8_yu_LNP*YdcL(1,2)*YdSQUL(1,2)).imag();
    Cqd8_2331r_LNP = (Cqd8_dd_LNP*SDL(2,0)*SQDL(1,2) + Cqd8_ud_LNP*SDL(2,0)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(2,2)*YdcL(1,0) + Cqd8_dy_LNP*SQDYdcL(1,0)*YdL(2,2) + Cqd8_uy_LNP*SQUYdcL(1,0)*YdL(2,2) + Cqd8_y_LNP*YdcL(1,0)*YdL(2,2) + Cqd8_yu_LNP*YdcL(1,0)*YdSQUL(2,2)).real();
    Cqd8_2331i_LNP = (Cqd8_dd_LNP*SDL(2,0)*SQDL(1,2) + Cqd8_ud_LNP*SDL(2,0)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(2,2)*YdcL(1,0) + Cqd8_dy_LNP*SQDYdcL(1,0)*YdL(2,2) + Cqd8_uy_LNP*SQUYdcL(1,0)*YdL(2,2) + Cqd8_y_LNP*YdcL(1,0)*YdL(2,2) + Cqd8_yu_LNP*YdcL(1,0)*YdSQUL(2,2)).imag();
    Cqd8_2332r_LNP = (Cqd8_dd_LNP*SDL(2,1)*SQDL(1,2) + Cqd8_ud_LNP*SDL(2,1)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(2,2)*YdcL(1,1) + Cqd8_dy_LNP*SQDYdcL(1,1)*YdL(2,2) + Cqd8_uy_LNP*SQUYdcL(1,1)*YdL(2,2) + Cqd8_y_LNP*YdcL(1,1)*YdL(2,2) + Cqd8_yu_LNP*YdcL(1,1)*YdSQUL(2,2)).real();
    Cqd8_2332i_LNP = (Cqd8_dd_LNP*SDL(2,1)*SQDL(1,2) + Cqd8_ud_LNP*SDL(2,1)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(2,2)*YdcL(1,1) + Cqd8_dy_LNP*SQDYdcL(1,1)*YdL(2,2) + Cqd8_uy_LNP*SQUYdcL(1,1)*YdL(2,2) + Cqd8_y_LNP*YdcL(1,1)*YdL(2,2) + Cqd8_yu_LNP*YdcL(1,1)*YdSQUL(2,2)).imag();
    Cqd8_2333r_LNP = (Cqd8_d0_LNP*SQDL(1,2) + Cqd8_dd_LNP*SDL(2,2)*SQDL(1,2) + Cqd8_u0_LNP*SQUL(1,2) + Cqd8_ud_LNP*SDL(2,2)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(2,2)*YdcL(1,2) + Cqd8_dy_LNP*SQDYdcL(1,2)*YdL(2,2) + Cqd8_uy_LNP*SQUYdcL(1,2)*YdL(2,2) + Cqd8_y_LNP*YdcL(1,2)*YdL(2,2) + Cqd8_yu_LNP*YdcL(1,2)*YdSQUL(2,2)).real();
    Cqd8_2333i_LNP = (Cqd8_d0_LNP*SQDL(1,2) + Cqd8_dd_LNP*SDL(2,2)*SQDL(1,2) + Cqd8_u0_LNP*SQUL(1,2) + Cqd8_ud_LNP*SDL(2,2)*SQUL(1,2) + Cqd8_yd_LNP*SQDYdcL(2,2)*YdcL(1,2) + Cqd8_dy_LNP*SQDYdcL(1,2)*YdL(2,2) + Cqd8_uy_LNP*SQUYdcL(1,2)*YdL(2,2) + Cqd8_y_LNP*YdcL(1,2)*YdL(2,2) + Cqd8_yu_LNP*YdcL(1,2)*YdSQUL(2,2)).imag();
    Cqd8_3311r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*SDL(0,0) + Cqd8_d0_LNP*SQDL(2,2) + Cqd8_dd_LNP*SDL(0,0)*SQDL(2,2) + Cqd8_u0_LNP*SQUL(2,2) + Cqd8_ud_LNP*SDL(0,0)*SQUL(2,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(2,0) + Cqd8_dy_LNP*SQDYdcL(2,0)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(2,0)*YdL(0,2) + Cqd8_y_LNP*YdcL(2,0)*YdL(0,2) + Cqd8_yu_LNP*YdcL(2,0)*YdSQUL(0,2)).real();
    Cqd8_3312r_LNP = (Cqd8_0d_LNP*SDL(0,1) + Cqd8_dd_LNP*SDL(0,1)*SQDL(2,2) + Cqd8_ud_LNP*SDL(0,1)*SQUL(2,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(2,1) + Cqd8_dy_LNP*SQDYdcL(2,1)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(2,1)*YdL(0,2) + Cqd8_y_LNP*YdcL(2,1)*YdL(0,2) + Cqd8_yu_LNP*YdcL(2,1)*YdSQUL(0,2)).real();
    Cqd8_3312i_LNP = (Cqd8_0d_LNP*SDL(0,1) + Cqd8_dd_LNP*SDL(0,1)*SQDL(2,2) + Cqd8_ud_LNP*SDL(0,1)*SQUL(2,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(2,1) + Cqd8_dy_LNP*SQDYdcL(2,1)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(2,1)*YdL(0,2) + Cqd8_y_LNP*YdcL(2,1)*YdL(0,2) + Cqd8_yu_LNP*YdcL(2,1)*YdSQUL(0,2)).imag();
    Cqd8_3313r_LNP = (Cqd8_0d_LNP*SDL(0,2) + Cqd8_dd_LNP*SDL(0,2)*SQDL(2,2) + Cqd8_ud_LNP*SDL(0,2)*SQUL(2,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(2,2) + Cqd8_dy_LNP*SQDYdcL(2,2)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(2,2)*YdL(0,2) + Cqd8_y_LNP*YdcL(2,2)*YdL(0,2) + Cqd8_yu_LNP*YdcL(2,2)*YdSQUL(0,2)).real();
    Cqd8_3313i_LNP = (Cqd8_0d_LNP*SDL(0,2) + Cqd8_dd_LNP*SDL(0,2)*SQDL(2,2) + Cqd8_ud_LNP*SDL(0,2)*SQUL(2,2) + Cqd8_yd_LNP*SQDYdcL(0,2)*YdcL(2,2) + Cqd8_dy_LNP*SQDYdcL(2,2)*YdL(0,2) + Cqd8_uy_LNP*SQUYdcL(2,2)*YdL(0,2) + Cqd8_y_LNP*YdcL(2,2)*YdL(0,2) + Cqd8_yu_LNP*YdcL(2,2)*YdSQUL(0,2)).imag();
    Cqd8_3322r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*SDL(1,1) + Cqd8_d0_LNP*SQDL(2,2) + Cqd8_dd_LNP*SDL(1,1)*SQDL(2,2) + Cqd8_u0_LNP*SQUL(2,2) + Cqd8_ud_LNP*SDL(1,1)*SQUL(2,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(2,1) + Cqd8_dy_LNP*SQDYdcL(2,1)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(2,1)*YdL(1,2) + Cqd8_y_LNP*YdcL(2,1)*YdL(1,2) + Cqd8_yu_LNP*YdcL(2,1)*YdSQUL(1,2)).real();
    Cqd8_3323r_LNP = (Cqd8_0d_LNP*SDL(1,2) + Cqd8_dd_LNP*SDL(1,2)*SQDL(2,2) + Cqd8_ud_LNP*SDL(1,2)*SQUL(2,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(2,2) + Cqd8_dy_LNP*SQDYdcL(2,2)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(2,2)*YdL(1,2) + Cqd8_y_LNP*YdcL(2,2)*YdL(1,2) + Cqd8_yu_LNP*YdcL(2,2)*YdSQUL(1,2)).real();
    Cqd8_3323i_LNP = (Cqd8_0d_LNP*SDL(1,2) + Cqd8_dd_LNP*SDL(1,2)*SQDL(2,2) + Cqd8_ud_LNP*SDL(1,2)*SQUL(2,2) + Cqd8_yd_LNP*SQDYdcL(1,2)*YdcL(2,2) + Cqd8_dy_LNP*SQDYdcL(2,2)*YdL(1,2) + Cqd8_uy_LNP*SQUYdcL(2,2)*YdL(1,2) + Cqd8_y_LNP*YdcL(2,2)*YdL(1,2) + Cqd8_yu_LNP*YdcL(2,2)*YdSQUL(1,2)).imag();
    Cqd8_3333r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*SDL(2,2) + Cqd8_d0_LNP*SQDL(2,2) + Cqd8_dd_LNP*SDL(2,2)*SQDL(2,2) + Cqd8_u0_LNP*SQUL(2,2) + Cqd8_ud_LNP*SDL(2,2)*SQUL(2,2) + Cqd8_yd_LNP*SQDYdcL(2,2)*YdcL(2,2) + Cqd8_dy_LNP*SQDYdcL(2,2)*YdL(2,2) + Cqd8_uy_LNP*SQUYdcL(2,2)*YdL(2,2) + Cqd8_y_LNP*YdcL(2,2)*YdL(2,2) + Cqd8_yu_LNP*YdcL(2,2)*YdSQUL(2,2)).real();
 
    Cquqd1_1111r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(0,0) + Cquqd1_00_LNP*YdcL(0,0)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(0,0)).real();
    Cquqd1_1111i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(0,0) + Cquqd1_00_LNP*YdcL(0,0)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(0,0)).imag();
    Cquqd1_1112r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(0,0) + Cquqd1_00_LNP*YdcL(0,1)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(0,1)).real();
    Cquqd1_1112i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(0,0) + Cquqd1_00_LNP*YdcL(0,1)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(0,1)).imag();
    Cquqd1_1113r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(0,0) + Cquqd1_00_LNP*YdcL(0,2)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(0,2)).real();
    Cquqd1_1113i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(0,0) + Cquqd1_00_LNP*YdcL(0,2)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(0,2)).imag();
    Cquqd1_1121r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(0,0) + Cquqd1_00_LNP*YdcL(1,0)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(0,0)).real();
    Cquqd1_1121i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(0,0) + Cquqd1_00_LNP*YdcL(1,0)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(0,0)).imag();
    Cquqd1_1122r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(0,0) + Cquqd1_00_LNP*YdcL(1,1)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(0,1)).real();
    Cquqd1_1122i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(0,0) + Cquqd1_00_LNP*YdcL(1,1)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(0,1)).imag();
    Cquqd1_1123r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(0,0) + Cquqd1_00_LNP*YdcL(1,2)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(0,2)).real();
    Cquqd1_1123i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(0,0) + Cquqd1_00_LNP*YdcL(1,2)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(0,2)).imag();
    Cquqd1_1131r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(0,0) + Cquqd1_00_LNP*YdcL(2,0)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(0,0)).real();
    Cquqd1_1131i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(0,0) + Cquqd1_00_LNP*YdcL(2,0)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(0,0)).imag();
    Cquqd1_1132r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(0,0) + Cquqd1_00_LNP*YdcL(2,1)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(0,1)).real();
    Cquqd1_1132i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(0,0) + Cquqd1_00_LNP*YdcL(2,1)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(0,1)).imag();
    Cquqd1_1133r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(0,0) + Cquqd1_00_LNP*YdcL(2,2)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(0,2)).real();
    Cquqd1_1133i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,0)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(0,0)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(0,0) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(0,0) + Cquqd1_00_LNP*YdcL(2,2)*YucL(0,0) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(0,2)).imag();
    Cquqd1_1211r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(0,1) + Cquqd1_00_LNP*YdcL(0,0)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(0,0)).real();
    Cquqd1_1211i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(0,1) + Cquqd1_00_LNP*YdcL(0,0)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(0,0)).imag();
    Cquqd1_1212r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(0,1) + Cquqd1_00_LNP*YdcL(0,1)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(0,1)).real();
    Cquqd1_1212i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(0,1) + Cquqd1_00_LNP*YdcL(0,1)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(0,1)).imag();
    Cquqd1_1213r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(0,1) + Cquqd1_00_LNP*YdcL(0,2)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(0,2)).real();
    Cquqd1_1213i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(0,1) + Cquqd1_00_LNP*YdcL(0,2)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(0,2)).imag();
    Cquqd1_1221r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(0,1) + Cquqd1_00_LNP*YdcL(1,0)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(0,0)).real();
    Cquqd1_1221i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(0,1) + Cquqd1_00_LNP*YdcL(1,0)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(0,0)).imag();
    Cquqd1_1222r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(0,1) + Cquqd1_00_LNP*YdcL(1,1)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(0,1)).real();
    Cquqd1_1222i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(0,1) + Cquqd1_00_LNP*YdcL(1,1)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(0,1)).imag();
    Cquqd1_1223r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(0,1) + Cquqd1_00_LNP*YdcL(1,2)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(0,2)).real();
    Cquqd1_1223i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(0,1) + Cquqd1_00_LNP*YdcL(1,2)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(0,2)).imag();
    Cquqd1_1231r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(0,1) + Cquqd1_00_LNP*YdcL(2,0)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(0,0)).real();
    Cquqd1_1231i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(0,1) + Cquqd1_00_LNP*YdcL(2,0)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(0,0)).imag();
    Cquqd1_1232r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(0,1) + Cquqd1_00_LNP*YdcL(2,1)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(0,1)).real();
    Cquqd1_1232i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(0,1) + Cquqd1_00_LNP*YdcL(2,1)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(0,1)).imag();
    Cquqd1_1233r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(0,1) + Cquqd1_00_LNP*YdcL(2,2)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(0,2)).real();
    Cquqd1_1233i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,1)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(0,1)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(0,1) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(0,1) + Cquqd1_00_LNP*YdcL(2,2)*YucL(0,1) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(0,2)).imag();
    Cquqd1_1311r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(0,2) + Cquqd1_00_LNP*YdcL(0,0)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(0,0)).real();
    Cquqd1_1311i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(0,2) + Cquqd1_00_LNP*YdcL(0,0)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(0,0)).imag();
    Cquqd1_1312r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(0,2) + Cquqd1_00_LNP*YdcL(0,1)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(0,1)).real();
    Cquqd1_1312i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(0,2) + Cquqd1_00_LNP*YdcL(0,1)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(0,1)).imag();
    Cquqd1_1313r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(0,2) + Cquqd1_00_LNP*YdcL(0,2)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(0,2)).real();
    Cquqd1_1313i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(0,2) + Cquqd1_00_LNP*YdcL(0,2)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(0,2)).imag();
    Cquqd1_1321r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(0,2) + Cquqd1_00_LNP*YdcL(1,0)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(0,0)).real();
    Cquqd1_1321i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(0,2) + Cquqd1_00_LNP*YdcL(1,0)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(0,0)).imag();
    Cquqd1_1322r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(0,2) + Cquqd1_00_LNP*YdcL(1,1)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(0,1)).real();
    Cquqd1_1322i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(0,2) + Cquqd1_00_LNP*YdcL(1,1)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(0,1)).imag();
    Cquqd1_1323r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(0,2) + Cquqd1_00_LNP*YdcL(1,2)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(0,2)).real();
    Cquqd1_1323i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(0,2) + Cquqd1_00_LNP*YdcL(1,2)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(0,2)).imag();
    Cquqd1_1331r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(0,2) + Cquqd1_00_LNP*YdcL(2,0)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(0,0)).real();
    Cquqd1_1331i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(0,2) + Cquqd1_00_LNP*YdcL(2,0)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,0)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(0,0)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(0,0) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(0,0) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(0,0)).imag();
    Cquqd1_1332r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(0,2) + Cquqd1_00_LNP*YdcL(2,1)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(0,1)).real();
    Cquqd1_1332i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(0,2) + Cquqd1_00_LNP*YdcL(2,1)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,1)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(0,1)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(0,1) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(0,1) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(0,1)).imag();
    Cquqd1_1333r_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(0,2) + Cquqd1_00_LNP*YdcL(2,2)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(0,2)).real();
    Cquqd1_1333i_LNP = (Cquqd1_d0_LNP*SQDYucL(0,2)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(0,2)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(0,2) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(0,2) + Cquqd1_00_LNP*YdcL(2,2)*YucL(0,2) + Cquqd1p_d0_LNP*SQDYucL(0,2)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(0,2)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(0,2) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(0,2) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(0,2)).imag();
    Cquqd1_2111r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(1,0) + Cquqd1_00_LNP*YdcL(0,0)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(1,0)).real();
    Cquqd1_2111i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(1,0) + Cquqd1_00_LNP*YdcL(0,0)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(1,0)).imag();
    Cquqd1_2112r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(1,0) + Cquqd1_00_LNP*YdcL(0,1)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(1,1)).real();
    Cquqd1_2112i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(1,0) + Cquqd1_00_LNP*YdcL(0,1)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(1,1)).imag();
    Cquqd1_2113r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(1,0) + Cquqd1_00_LNP*YdcL(0,2)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(1,2)).real();
    Cquqd1_2113i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(1,0) + Cquqd1_00_LNP*YdcL(0,2)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(1,2)).imag();
    Cquqd1_2121r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(1,0) + Cquqd1_00_LNP*YdcL(1,0)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(1,0)).real();
    Cquqd1_2121i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(1,0) + Cquqd1_00_LNP*YdcL(1,0)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(1,0)).imag();
    Cquqd1_2122r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(1,0) + Cquqd1_00_LNP*YdcL(1,1)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(1,1)).real();
    Cquqd1_2122i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(1,0) + Cquqd1_00_LNP*YdcL(1,1)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(1,1)).imag();
    Cquqd1_2123r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(1,0) + Cquqd1_00_LNP*YdcL(1,2)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(1,2)).real();
    Cquqd1_2123i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(1,0) + Cquqd1_00_LNP*YdcL(1,2)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(1,2)).imag();
    Cquqd1_2131r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(1,0) + Cquqd1_00_LNP*YdcL(2,0)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(1,0)).real();
    Cquqd1_2131i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(1,0) + Cquqd1_00_LNP*YdcL(2,0)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(1,0)).imag();
    Cquqd1_2132r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(1,0) + Cquqd1_00_LNP*YdcL(2,1)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(1,1)).real();
    Cquqd1_2132i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(1,0) + Cquqd1_00_LNP*YdcL(2,1)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(1,1)).imag();
    Cquqd1_2133r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(1,0) + Cquqd1_00_LNP*YdcL(2,2)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(1,2)).real();
    Cquqd1_2133i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,0)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(1,0)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(1,0) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(1,0) + Cquqd1_00_LNP*YdcL(2,2)*YucL(1,0) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(1,2)).imag();
    Cquqd1_2211r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(1,1) + Cquqd1_00_LNP*YdcL(0,0)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(1,0)).real();
    Cquqd1_2211i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(1,1) + Cquqd1_00_LNP*YdcL(0,0)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(1,0)).imag();
    Cquqd1_2212r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(1,1) + Cquqd1_00_LNP*YdcL(0,1)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(1,1)).real();
    Cquqd1_2212i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(1,1) + Cquqd1_00_LNP*YdcL(0,1)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(1,1)).imag();
    Cquqd1_2213r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(1,1) + Cquqd1_00_LNP*YdcL(0,2)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(1,2)).real();
    Cquqd1_2213i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(1,1) + Cquqd1_00_LNP*YdcL(0,2)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(1,2)).imag();
    Cquqd1_2221r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(1,1) + Cquqd1_00_LNP*YdcL(1,0)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(1,0)).real();
    Cquqd1_2221i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(1,1) + Cquqd1_00_LNP*YdcL(1,0)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(1,0)).imag();
    Cquqd1_2222r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(1,1) + Cquqd1_00_LNP*YdcL(1,1)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(1,1)).real();
    Cquqd1_2222i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(1,1) + Cquqd1_00_LNP*YdcL(1,1)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(1,1)).imag();
    Cquqd1_2223r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(1,1) + Cquqd1_00_LNP*YdcL(1,2)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(1,2)).real();
    Cquqd1_2223i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(1,1) + Cquqd1_00_LNP*YdcL(1,2)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(1,2)).imag();
    Cquqd1_2231r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(1,1) + Cquqd1_00_LNP*YdcL(2,0)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(1,0)).real();
    Cquqd1_2231i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(1,1) + Cquqd1_00_LNP*YdcL(2,0)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(1,0)).imag();
    Cquqd1_2232r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(1,1) + Cquqd1_00_LNP*YdcL(2,1)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(1,1)).real();
    Cquqd1_2232i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(1,1) + Cquqd1_00_LNP*YdcL(2,1)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(1,1)).imag();
    Cquqd1_2233r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(1,1) + Cquqd1_00_LNP*YdcL(2,2)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(1,2)).real();
    Cquqd1_2233i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,1)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(1,1)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(1,1) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(1,1) + Cquqd1_00_LNP*YdcL(2,2)*YucL(1,1) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(1,2)).imag();
    Cquqd1_2311r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(1,2) + Cquqd1_00_LNP*YdcL(0,0)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(1,0)).real();
    Cquqd1_2311i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(1,2) + Cquqd1_00_LNP*YdcL(0,0)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(1,0)).imag();
    Cquqd1_2312r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(1,2) + Cquqd1_00_LNP*YdcL(0,1)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(1,1)).real();
    Cquqd1_2312i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(1,2) + Cquqd1_00_LNP*YdcL(0,1)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(1,1)).imag();
    Cquqd1_2313r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(1,2) + Cquqd1_00_LNP*YdcL(0,2)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(1,2)).real();
    Cquqd1_2313i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(1,2) + Cquqd1_00_LNP*YdcL(0,2)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(1,2)).imag();
    Cquqd1_2321r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(1,2) + Cquqd1_00_LNP*YdcL(1,0)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(1,0)).real();
    Cquqd1_2321i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(1,2) + Cquqd1_00_LNP*YdcL(1,0)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(1,0)).imag();
    Cquqd1_2322r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(1,2) + Cquqd1_00_LNP*YdcL(1,1)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(1,1)).real();
    Cquqd1_2322i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(1,2) + Cquqd1_00_LNP*YdcL(1,1)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(1,1)).imag();
    Cquqd1_2323r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(1,2) + Cquqd1_00_LNP*YdcL(1,2)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(1,2)).real();
    Cquqd1_2323i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(1,2) + Cquqd1_00_LNP*YdcL(1,2)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(1,2)).imag();
    Cquqd1_2331r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(1,2) + Cquqd1_00_LNP*YdcL(2,0)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(1,0)).real();
    Cquqd1_2331i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(1,2) + Cquqd1_00_LNP*YdcL(2,0)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,0)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(1,0)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(1,0) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(1,0) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(1,0)).imag();
    Cquqd1_2332r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(1,2) + Cquqd1_00_LNP*YdcL(2,1)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(1,1)).real();
    Cquqd1_2332i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(1,2) + Cquqd1_00_LNP*YdcL(2,1)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,1)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(1,1)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(1,1) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(1,1) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(1,1)).imag();
    Cquqd1_2333r_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(1,2) + Cquqd1_00_LNP*YdcL(2,2)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(1,2)).real();
    Cquqd1_2333i_LNP = (Cquqd1_d0_LNP*SQDYucL(1,2)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(1,2)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(1,2) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(1,2) + Cquqd1_00_LNP*YdcL(2,2)*YucL(1,2) + Cquqd1p_d0_LNP*SQDYucL(1,2)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(1,2)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(1,2) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(1,2) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(1,2)).imag();
    Cquqd1_3111r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(2,0) + Cquqd1_00_LNP*YdcL(0,0)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(2,0)).real();
    Cquqd1_3111i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(2,0) + Cquqd1_00_LNP*YdcL(0,0)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(2,0)).imag();
    Cquqd1_3112r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(2,0) + Cquqd1_00_LNP*YdcL(0,1)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(2,1)).real();
    Cquqd1_3112i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(2,0) + Cquqd1_00_LNP*YdcL(0,1)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(2,1)).imag();
    Cquqd1_3113r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(2,0) + Cquqd1_00_LNP*YdcL(0,2)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(2,2)).real();
    Cquqd1_3113i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(2,0) + Cquqd1_00_LNP*YdcL(0,2)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(0,0) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(0,0) + Cquqd1p_0d_LNP*SQDYdcL(0,0)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(0,0)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(0,0)*YucL(2,2)).imag();
    Cquqd1_3121r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(2,0) + Cquqd1_00_LNP*YdcL(1,0)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(2,0)).real();
    Cquqd1_3121i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(2,0) + Cquqd1_00_LNP*YdcL(1,0)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(2,0)).imag();
    Cquqd1_3122r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(2,0) + Cquqd1_00_LNP*YdcL(1,1)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(2,1)).real();
    Cquqd1_3122i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(2,0) + Cquqd1_00_LNP*YdcL(1,1)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(2,1)).imag();
    Cquqd1_3123r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(2,0) + Cquqd1_00_LNP*YdcL(1,2)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(2,2)).real();
    Cquqd1_3123i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(2,0) + Cquqd1_00_LNP*YdcL(1,2)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(1,0) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(1,0) + Cquqd1p_0d_LNP*SQDYdcL(1,0)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(1,0)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(1,0)*YucL(2,2)).imag();
    Cquqd1_3131r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(2,0) + Cquqd1_00_LNP*YdcL(2,0)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(2,0)).real();
    Cquqd1_3131i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(2,0) + Cquqd1_00_LNP*YdcL(2,0)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(2,0)).imag();
    Cquqd1_3132r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(2,0) + Cquqd1_00_LNP*YdcL(2,1)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(2,1)).real();
    Cquqd1_3132i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(2,0) + Cquqd1_00_LNP*YdcL(2,1)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(2,1)).imag();
    Cquqd1_3133r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(2,0) + Cquqd1_00_LNP*YdcL(2,2)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(2,2)).real();
    Cquqd1_3133i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,0)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(2,0)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(2,0) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(2,0) + Cquqd1_00_LNP*YdcL(2,2)*YucL(2,0) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(2,0) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(2,0) + Cquqd1p_0d_LNP*SQDYdcL(2,0)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(2,0)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(2,0)*YucL(2,2)).imag();
    Cquqd1_3211r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(2,1) + Cquqd1_00_LNP*YdcL(0,0)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(2,0)).real();
    Cquqd1_3211i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(2,1) + Cquqd1_00_LNP*YdcL(0,0)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(2,0)).imag();
    Cquqd1_3212r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(2,1) + Cquqd1_00_LNP*YdcL(0,1)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(2,1)).real();
    Cquqd1_3212i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(2,1) + Cquqd1_00_LNP*YdcL(0,1)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(2,1)).imag();
    Cquqd1_3213r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(2,1) + Cquqd1_00_LNP*YdcL(0,2)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(2,2)).real();
    Cquqd1_3213i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(2,1) + Cquqd1_00_LNP*YdcL(0,2)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(0,1) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(0,1) + Cquqd1p_0d_LNP*SQDYdcL(0,1)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(0,1)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(0,1)*YucL(2,2)).imag();
    Cquqd1_3221r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(2,1) + Cquqd1_00_LNP*YdcL(1,0)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(2,0)).real();
    Cquqd1_3221i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(2,1) + Cquqd1_00_LNP*YdcL(1,0)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(2,0)).imag();
    Cquqd1_3222r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(2,1) + Cquqd1_00_LNP*YdcL(1,1)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(2,1)).real();
    Cquqd1_3222i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(2,1) + Cquqd1_00_LNP*YdcL(1,1)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(2,1)).imag();
    Cquqd1_3223r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(2,1) + Cquqd1_00_LNP*YdcL(1,2)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(2,2)).real();
    Cquqd1_3223i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(2,1) + Cquqd1_00_LNP*YdcL(1,2)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(1,1) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(1,1) + Cquqd1p_0d_LNP*SQDYdcL(1,1)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(1,1)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(1,1)*YucL(2,2)).imag();
    Cquqd1_3231r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(2,1) + Cquqd1_00_LNP*YdcL(2,0)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(2,0)).real();
    Cquqd1_3231i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(2,1) + Cquqd1_00_LNP*YdcL(2,0)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(2,0)).imag();
    Cquqd1_3232r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(2,1) + Cquqd1_00_LNP*YdcL(2,1)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(2,1)).real();
    Cquqd1_3232i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(2,1) + Cquqd1_00_LNP*YdcL(2,1)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(2,1)).imag();
    Cquqd1_3233r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(2,1) + Cquqd1_00_LNP*YdcL(2,2)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(2,2)).real();
    Cquqd1_3233i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,1)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(2,1)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(2,1) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(2,1) + Cquqd1_00_LNP*YdcL(2,2)*YucL(2,1) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(2,1) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(2,1) + Cquqd1p_0d_LNP*SQDYdcL(2,1)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(2,1)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(2,1)*YucL(2,2)).imag();
    Cquqd1_3311r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(2,2) + Cquqd1_00_LNP*YdcL(0,0)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(2,0)).real();
    Cquqd1_3311i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(0,0) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(0,0) + Cquqd1_0d_LNP*SQDYdcL(0,0)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(0,0)*YucL(2,2) + Cquqd1_00_LNP*YdcL(0,0)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(2,0)).imag();
    Cquqd1_3312r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(2,2) + Cquqd1_00_LNP*YdcL(0,1)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(2,1)).real();
    Cquqd1_3312i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(0,1) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(0,1) + Cquqd1_0d_LNP*SQDYdcL(0,1)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(0,1)*YucL(2,2) + Cquqd1_00_LNP*YdcL(0,1)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(2,1)).imag();
    Cquqd1_3313r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(2,2) + Cquqd1_00_LNP*YdcL(0,2)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(2,2)).real();
    Cquqd1_3313i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(0,2) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(0,2) + Cquqd1_0d_LNP*SQDYdcL(0,2)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(0,2)*YucL(2,2) + Cquqd1_00_LNP*YdcL(0,2)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(0,2) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(0,2) + Cquqd1p_0d_LNP*SQDYdcL(0,2)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(0,2)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(0,2)*YucL(2,2)).imag();
    Cquqd1_3321r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(2,2) + Cquqd1_00_LNP*YdcL(1,0)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(2,0)).real();
    Cquqd1_3321i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(1,0) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(1,0) + Cquqd1_0d_LNP*SQDYdcL(1,0)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(1,0)*YucL(2,2) + Cquqd1_00_LNP*YdcL(1,0)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(2,0)).imag();
    Cquqd1_3322r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(2,2) + Cquqd1_00_LNP*YdcL(1,1)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(2,1)).real();
    Cquqd1_3322i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(1,1) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(1,1) + Cquqd1_0d_LNP*SQDYdcL(1,1)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(1,1)*YucL(2,2) + Cquqd1_00_LNP*YdcL(1,1)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(2,1)).imag();
    Cquqd1_3323r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(2,2) + Cquqd1_00_LNP*YdcL(1,2)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(2,2)).real();
    Cquqd1_3323i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(1,2) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(1,2) + Cquqd1_0d_LNP*SQDYdcL(1,2)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(1,2)*YucL(2,2) + Cquqd1_00_LNP*YdcL(1,2)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(1,2) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(1,2) + Cquqd1p_0d_LNP*SQDYdcL(1,2)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(1,2)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(1,2)*YucL(2,2)).imag();
    Cquqd1_3331r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(2,2) + Cquqd1_00_LNP*YdcL(2,0)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(2,0)).real();
    Cquqd1_3331i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(2,0) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(2,0) + Cquqd1_0d_LNP*SQDYdcL(2,0)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(2,0)*YucL(2,2) + Cquqd1_00_LNP*YdcL(2,0)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,0)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(2,0)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(2,0) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(2,0) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(2,0)).imag();
    Cquqd1_3332r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(2,2) + Cquqd1_00_LNP*YdcL(2,1)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(2,1)).real();
    Cquqd1_3332i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(2,1) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(2,1) + Cquqd1_0d_LNP*SQDYdcL(2,1)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(2,1)*YucL(2,2) + Cquqd1_00_LNP*YdcL(2,1)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,1)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(2,1)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(2,1) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(2,1) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(2,1)).imag();
    Cquqd1_3333r_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(2,2) + Cquqd1_00_LNP*YdcL(2,2)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(2,2)).real();
    Cquqd1_3333i_LNP = (Cquqd1_d0_LNP*SQDYucL(2,2)*YdcL(2,2) + Cquqd1_u0_LNP*SQUYucL(2,2)*YdcL(2,2) + Cquqd1_0d_LNP*SQDYdcL(2,2)*YucL(2,2) + Cquqd1_0u_LNP*SQUYdcL(2,2)*YucL(2,2) + Cquqd1_00_LNP*YdcL(2,2)*YucL(2,2) + Cquqd1p_d0_LNP*SQDYucL(2,2)*YdcL(2,2) + Cquqd1p_u0_LNP*SQUYucL(2,2)*YdcL(2,2) + Cquqd1p_0d_LNP*SQDYdcL(2,2)*YucL(2,2) + Cquqd1p_0u_LNP*SQUYdcL(2,2)*YucL(2,2) + Cquqd1p_00_LNP*YdcL(2,2)*YucL(2,2)).imag();
 
    Cquqd8_1111r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(0,0) + Cquqd8_00_LNP*YdcL(0,0)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(0,0)).real();
    Cquqd8_1111i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(0,0) + Cquqd8_00_LNP*YdcL(0,0)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(0,0)).imag();
    Cquqd8_1112r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(0,0) + Cquqd8_00_LNP*YdcL(0,1)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(0,1)).real();
    Cquqd8_1112i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(0,0) + Cquqd8_00_LNP*YdcL(0,1)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(0,1)).imag();
    Cquqd8_1113r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(0,0) + Cquqd8_00_LNP*YdcL(0,2)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(0,2)).real();
    Cquqd8_1113i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(0,0) + Cquqd8_00_LNP*YdcL(0,2)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(0,2)).imag();
    Cquqd8_1121r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(0,0) + Cquqd8_00_LNP*YdcL(1,0)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(0,0)).real();
    Cquqd8_1121i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(0,0) + Cquqd8_00_LNP*YdcL(1,0)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(0,0)).imag();
    Cquqd8_1122r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(0,0) + Cquqd8_00_LNP*YdcL(1,1)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(0,1)).real();
    Cquqd8_1122i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(0,0) + Cquqd8_00_LNP*YdcL(1,1)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(0,1)).imag();
    Cquqd8_1123r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(0,0) + Cquqd8_00_LNP*YdcL(1,2)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(0,2)).real();
    Cquqd8_1123i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(0,0) + Cquqd8_00_LNP*YdcL(1,2)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(0,2)).imag();
    Cquqd8_1131r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(0,0) + Cquqd8_00_LNP*YdcL(2,0)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(0,0)).real();
    Cquqd8_1131i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(0,0) + Cquqd8_00_LNP*YdcL(2,0)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(0,0)).imag();
    Cquqd8_1132r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(0,0) + Cquqd8_00_LNP*YdcL(2,1)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(0,1)).real();
    Cquqd8_1132i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(0,0) + Cquqd8_00_LNP*YdcL(2,1)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(0,1)).imag();
    Cquqd8_1133r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(0,0) + Cquqd8_00_LNP*YdcL(2,2)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(0,2)).real();
    Cquqd8_1133i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,0)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(0,0)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(0,0) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(0,0) + Cquqd8_00_LNP*YdcL(2,2)*YucL(0,0) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(0,2)).imag();
    Cquqd8_1211r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(0,1) + Cquqd8_00_LNP*YdcL(0,0)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(0,0)).real();
    Cquqd8_1211i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(0,1) + Cquqd8_00_LNP*YdcL(0,0)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(0,0)).imag();
    Cquqd8_1212r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(0,1) + Cquqd8_00_LNP*YdcL(0,1)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(0,1)).real();
    Cquqd8_1212i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(0,1) + Cquqd8_00_LNP*YdcL(0,1)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(0,1)).imag();
    Cquqd8_1213r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(0,1) + Cquqd8_00_LNP*YdcL(0,2)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(0,2)).real();
    Cquqd8_1213i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(0,1) + Cquqd8_00_LNP*YdcL(0,2)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(0,2)).imag();
    Cquqd8_1221r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(0,1) + Cquqd8_00_LNP*YdcL(1,0)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(0,0)).real();
    Cquqd8_1221i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(0,1) + Cquqd8_00_LNP*YdcL(1,0)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(0,0)).imag();
    Cquqd8_1222r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(0,1) + Cquqd8_00_LNP*YdcL(1,1)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(0,1)).real();
    Cquqd8_1222i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(0,1) + Cquqd8_00_LNP*YdcL(1,1)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(0,1)).imag();
    Cquqd8_1223r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(0,1) + Cquqd8_00_LNP*YdcL(1,2)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(0,2)).real();
    Cquqd8_1223i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(0,1) + Cquqd8_00_LNP*YdcL(1,2)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(0,2)).imag();
    Cquqd8_1231r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(0,1) + Cquqd8_00_LNP*YdcL(2,0)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(0,0)).real();
    Cquqd8_1231i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(0,1) + Cquqd8_00_LNP*YdcL(2,0)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(0,0)).imag();
    Cquqd8_1232r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(0,1) + Cquqd8_00_LNP*YdcL(2,1)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(0,1)).real();
    Cquqd8_1232i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(0,1) + Cquqd8_00_LNP*YdcL(2,1)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(0,1)).imag();
    Cquqd8_1233r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(0,1) + Cquqd8_00_LNP*YdcL(2,2)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(0,2)).real();
    Cquqd8_1233i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,1)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(0,1)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(0,1) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(0,1) + Cquqd8_00_LNP*YdcL(2,2)*YucL(0,1) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(0,2)).imag();
    Cquqd8_1311r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(0,2) + Cquqd8_00_LNP*YdcL(0,0)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(0,0)).real();
    Cquqd8_1311i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(0,2) + Cquqd8_00_LNP*YdcL(0,0)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(0,0)).imag();
    Cquqd8_1312r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(0,2) + Cquqd8_00_LNP*YdcL(0,1)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(0,1)).real();
    Cquqd8_1312i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(0,2) + Cquqd8_00_LNP*YdcL(0,1)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(0,1)).imag();
    Cquqd8_1313r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(0,2) + Cquqd8_00_LNP*YdcL(0,2)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(0,2)).real();
    Cquqd8_1313i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(0,2) + Cquqd8_00_LNP*YdcL(0,2)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(0,2)).imag();
    Cquqd8_1321r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(0,2) + Cquqd8_00_LNP*YdcL(1,0)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(0,0)).real();
    Cquqd8_1321i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(0,2) + Cquqd8_00_LNP*YdcL(1,0)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(0,0)).imag();
    Cquqd8_1322r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(0,2) + Cquqd8_00_LNP*YdcL(1,1)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(0,1)).real();
    Cquqd8_1322i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(0,2) + Cquqd8_00_LNP*YdcL(1,1)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(0,1)).imag();
    Cquqd8_1323r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(0,2) + Cquqd8_00_LNP*YdcL(1,2)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(0,2)).real();
    Cquqd8_1323i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(0,2) + Cquqd8_00_LNP*YdcL(1,2)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(0,2)).imag();
    Cquqd8_1331r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(0,2) + Cquqd8_00_LNP*YdcL(2,0)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(0,0)).real();
    Cquqd8_1331i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(0,2) + Cquqd8_00_LNP*YdcL(2,0)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,0)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(0,0)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(0,0) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(0,0) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(0,0)).imag();
    Cquqd8_1332r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(0,2) + Cquqd8_00_LNP*YdcL(2,1)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(0,1)).real();
    Cquqd8_1332i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(0,2) + Cquqd8_00_LNP*YdcL(2,1)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,1)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(0,1)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(0,1) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(0,1) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(0,1)).imag();
    Cquqd8_1333r_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(0,2) + Cquqd8_00_LNP*YdcL(2,2)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(0,2)).real();
    Cquqd8_1333i_LNP = (Cquqd8_d0_LNP*SQDYucL(0,2)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(0,2)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(0,2) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(0,2) + Cquqd8_00_LNP*YdcL(2,2)*YucL(0,2) + Cquqd8p_d0_LNP*SQDYucL(0,2)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(0,2)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(0,2) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(0,2) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(0,2)).imag();
    Cquqd8_2111r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(1,0) + Cquqd8_00_LNP*YdcL(0,0)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(1,0)).real();
    Cquqd8_2111i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(1,0) + Cquqd8_00_LNP*YdcL(0,0)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(1,0)).imag();
    Cquqd8_2112r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(1,0) + Cquqd8_00_LNP*YdcL(0,1)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(1,1)).real();
    Cquqd8_2112i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(1,0) + Cquqd8_00_LNP*YdcL(0,1)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(1,1)).imag();
    Cquqd8_2113r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(1,0) + Cquqd8_00_LNP*YdcL(0,2)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(1,2)).real();
    Cquqd8_2113i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(1,0) + Cquqd8_00_LNP*YdcL(0,2)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(1,2)).imag();
    Cquqd8_2121r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(1,0) + Cquqd8_00_LNP*YdcL(1,0)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(1,0)).real();
    Cquqd8_2121i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(1,0) + Cquqd8_00_LNP*YdcL(1,0)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(1,0)).imag();
    Cquqd8_2122r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(1,0) + Cquqd8_00_LNP*YdcL(1,1)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(1,1)).real();
    Cquqd8_2122i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(1,0) + Cquqd8_00_LNP*YdcL(1,1)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(1,1)).imag();
    Cquqd8_2123r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(1,0) + Cquqd8_00_LNP*YdcL(1,2)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(1,2)).real();
    Cquqd8_2123i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(1,0) + Cquqd8_00_LNP*YdcL(1,2)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(1,2)).imag();
    Cquqd8_2131r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(1,0) + Cquqd8_00_LNP*YdcL(2,0)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(1,0)).real();
    Cquqd8_2131i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(1,0) + Cquqd8_00_LNP*YdcL(2,0)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(1,0)).imag();
    Cquqd8_2132r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(1,0) + Cquqd8_00_LNP*YdcL(2,1)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(1,1)).real();
    Cquqd8_2132i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(1,0) + Cquqd8_00_LNP*YdcL(2,1)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(1,1)).imag();
    Cquqd8_2133r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(1,0) + Cquqd8_00_LNP*YdcL(2,2)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(1,2)).real();
    Cquqd8_2133i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,0)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(1,0)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(1,0) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(1,0) + Cquqd8_00_LNP*YdcL(2,2)*YucL(1,0) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(1,2)).imag();
    Cquqd8_2211r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(1,1) + Cquqd8_00_LNP*YdcL(0,0)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(1,0)).real();
    Cquqd8_2211i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(1,1) + Cquqd8_00_LNP*YdcL(0,0)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(1,0)).imag();
    Cquqd8_2212r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(1,1) + Cquqd8_00_LNP*YdcL(0,1)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(1,1)).real();
    Cquqd8_2212i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(1,1) + Cquqd8_00_LNP*YdcL(0,1)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(1,1)).imag();
    Cquqd8_2213r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(1,1) + Cquqd8_00_LNP*YdcL(0,2)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(1,2)).real();
    Cquqd8_2213i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(1,1) + Cquqd8_00_LNP*YdcL(0,2)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(1,2)).imag();
    Cquqd8_2221r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(1,1) + Cquqd8_00_LNP*YdcL(1,0)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(1,0)).real();
    Cquqd8_2221i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(1,1) + Cquqd8_00_LNP*YdcL(1,0)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(1,0)).imag();
    Cquqd8_2222r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(1,1) + Cquqd8_00_LNP*YdcL(1,1)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(1,1)).real();
    Cquqd8_2222i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(1,1) + Cquqd8_00_LNP*YdcL(1,1)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(1,1)).imag();
    Cquqd8_2223r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(1,1) + Cquqd8_00_LNP*YdcL(1,2)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(1,2)).real();
    Cquqd8_2223i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(1,1) + Cquqd8_00_LNP*YdcL(1,2)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(1,2)).imag();
    Cquqd8_2231r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(1,1) + Cquqd8_00_LNP*YdcL(2,0)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(1,0)).real();
    Cquqd8_2231i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(1,1) + Cquqd8_00_LNP*YdcL(2,0)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(1,0)).imag();
    Cquqd8_2232r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(1,1) + Cquqd8_00_LNP*YdcL(2,1)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(1,1)).real();
    Cquqd8_2232i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(1,1) + Cquqd8_00_LNP*YdcL(2,1)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(1,1)).imag();
    Cquqd8_2233r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(1,1) + Cquqd8_00_LNP*YdcL(2,2)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(1,2)).real();
    Cquqd8_2233i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,1)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(1,1)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(1,1) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(1,1) + Cquqd8_00_LNP*YdcL(2,2)*YucL(1,1) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(1,2)).imag();
    Cquqd8_2311r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(1,2) + Cquqd8_00_LNP*YdcL(0,0)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(1,0)).real();
    Cquqd8_2311i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(1,2) + Cquqd8_00_LNP*YdcL(0,0)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(1,0)).imag();
    Cquqd8_2312r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(1,2) + Cquqd8_00_LNP*YdcL(0,1)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(1,1)).real();
    Cquqd8_2312i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(1,2) + Cquqd8_00_LNP*YdcL(0,1)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(1,1)).imag();
    Cquqd8_2313r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(1,2) + Cquqd8_00_LNP*YdcL(0,2)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(1,2)).real();
    Cquqd8_2313i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(1,2) + Cquqd8_00_LNP*YdcL(0,2)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(1,2)).imag();
    Cquqd8_2321r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(1,2) + Cquqd8_00_LNP*YdcL(1,0)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(1,0)).real();
    Cquqd8_2321i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(1,2) + Cquqd8_00_LNP*YdcL(1,0)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(1,0)).imag();
    Cquqd8_2322r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(1,2) + Cquqd8_00_LNP*YdcL(1,1)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(1,1)).real();
    Cquqd8_2322i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(1,2) + Cquqd8_00_LNP*YdcL(1,1)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(1,1)).imag();
    Cquqd8_2323r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(1,2) + Cquqd8_00_LNP*YdcL(1,2)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(1,2)).real();
    Cquqd8_2323i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(1,2) + Cquqd8_00_LNP*YdcL(1,2)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(1,2)).imag();
    Cquqd8_2331r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(1,2) + Cquqd8_00_LNP*YdcL(2,0)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(1,0)).real();
    Cquqd8_2331i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(1,2) + Cquqd8_00_LNP*YdcL(2,0)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,0)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(1,0)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(1,0) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(1,0) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(1,0)).imag();
    Cquqd8_2332r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(1,2) + Cquqd8_00_LNP*YdcL(2,1)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(1,1)).real();
    Cquqd8_2332i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(1,2) + Cquqd8_00_LNP*YdcL(2,1)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,1)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(1,1)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(1,1) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(1,1) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(1,1)).imag();
    Cquqd8_2333r_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(1,2) + Cquqd8_00_LNP*YdcL(2,2)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(1,2)).real();
    Cquqd8_2333i_LNP = (Cquqd8_d0_LNP*SQDYucL(1,2)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(1,2)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(1,2) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(1,2) + Cquqd8_00_LNP*YdcL(2,2)*YucL(1,2) + Cquqd8p_d0_LNP*SQDYucL(1,2)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(1,2)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(1,2) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(1,2) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(1,2)).imag();
    Cquqd8_3111r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(2,0) + Cquqd8_00_LNP*YdcL(0,0)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(2,0)).real();
    Cquqd8_3111i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(2,0) + Cquqd8_00_LNP*YdcL(0,0)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(2,0)).imag();
    Cquqd8_3112r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(2,0) + Cquqd8_00_LNP*YdcL(0,1)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(2,1)).real();
    Cquqd8_3112i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(2,0) + Cquqd8_00_LNP*YdcL(0,1)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(2,1)).imag();
    Cquqd8_3113r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(2,0) + Cquqd8_00_LNP*YdcL(0,2)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(2,2)).real();
    Cquqd8_3113i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(2,0) + Cquqd8_00_LNP*YdcL(0,2)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(0,0) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(0,0) + Cquqd8p_0d_LNP*SQDYdcL(0,0)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(0,0)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(0,0)*YucL(2,2)).imag();
    Cquqd8_3121r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(2,0) + Cquqd8_00_LNP*YdcL(1,0)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(2,0)).real();
    Cquqd8_3121i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(2,0) + Cquqd8_00_LNP*YdcL(1,0)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(2,0)).imag();
    Cquqd8_3122r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(2,0) + Cquqd8_00_LNP*YdcL(1,1)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(2,1)).real();
    Cquqd8_3122i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(2,0) + Cquqd8_00_LNP*YdcL(1,1)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(2,1)).imag();
    Cquqd8_3123r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(2,0) + Cquqd8_00_LNP*YdcL(1,2)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(2,2)).real();
    Cquqd8_3123i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(2,0) + Cquqd8_00_LNP*YdcL(1,2)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(1,0) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(1,0) + Cquqd8p_0d_LNP*SQDYdcL(1,0)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(1,0)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(1,0)*YucL(2,2)).imag();
    Cquqd8_3131r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(2,0) + Cquqd8_00_LNP*YdcL(2,0)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(2,0)).real();
    Cquqd8_3131i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(2,0) + Cquqd8_00_LNP*YdcL(2,0)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(2,0)).imag();
    Cquqd8_3132r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(2,0) + Cquqd8_00_LNP*YdcL(2,1)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(2,1)).real();
    Cquqd8_3132i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(2,0) + Cquqd8_00_LNP*YdcL(2,1)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(2,1)).imag();
    Cquqd8_3133r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(2,0) + Cquqd8_00_LNP*YdcL(2,2)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(2,2)).real();
    Cquqd8_3133i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,0)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(2,0)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(2,0) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(2,0) + Cquqd8_00_LNP*YdcL(2,2)*YucL(2,0) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(2,0) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(2,0) + Cquqd8p_0d_LNP*SQDYdcL(2,0)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(2,0)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(2,0)*YucL(2,2)).imag();
    Cquqd8_3211r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(2,1) + Cquqd8_00_LNP*YdcL(0,0)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(2,0)).real();
    Cquqd8_3211i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(2,1) + Cquqd8_00_LNP*YdcL(0,0)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(2,0)).imag();
    Cquqd8_3212r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(2,1) + Cquqd8_00_LNP*YdcL(0,1)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(2,1)).real();
    Cquqd8_3212i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(2,1) + Cquqd8_00_LNP*YdcL(0,1)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(2,1)).imag();
    Cquqd8_3213r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(2,1) + Cquqd8_00_LNP*YdcL(0,2)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(2,2)).real();
    Cquqd8_3213i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(2,1) + Cquqd8_00_LNP*YdcL(0,2)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(0,1) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(0,1) + Cquqd8p_0d_LNP*SQDYdcL(0,1)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(0,1)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(0,1)*YucL(2,2)).imag();
    Cquqd8_3221r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(2,1) + Cquqd8_00_LNP*YdcL(1,0)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(2,0)).real();
    Cquqd8_3221i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(2,1) + Cquqd8_00_LNP*YdcL(1,0)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(2,0)).imag();
    Cquqd8_3222r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(2,1) + Cquqd8_00_LNP*YdcL(1,1)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(2,1)).real();
    Cquqd8_3222i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(2,1) + Cquqd8_00_LNP*YdcL(1,1)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(2,1)).imag();
    Cquqd8_3223r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(2,1) + Cquqd8_00_LNP*YdcL(1,2)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(2,2)).real();
    Cquqd8_3223i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(2,1) + Cquqd8_00_LNP*YdcL(1,2)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(1,1) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(1,1) + Cquqd8p_0d_LNP*SQDYdcL(1,1)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(1,1)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(1,1)*YucL(2,2)).imag();
    Cquqd8_3231r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(2,1) + Cquqd8_00_LNP*YdcL(2,0)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(2,0)).real();
    Cquqd8_3231i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(2,1) + Cquqd8_00_LNP*YdcL(2,0)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(2,0)).imag();
    Cquqd8_3232r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(2,1) + Cquqd8_00_LNP*YdcL(2,1)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(2,1)).real();
    Cquqd8_3232i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(2,1) + Cquqd8_00_LNP*YdcL(2,1)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(2,1)).imag();
    Cquqd8_3233r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(2,1) + Cquqd8_00_LNP*YdcL(2,2)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(2,2)).real();
    Cquqd8_3233i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,1)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(2,1)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(2,1) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(2,1) + Cquqd8_00_LNP*YdcL(2,2)*YucL(2,1) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(2,1) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(2,1) + Cquqd8p_0d_LNP*SQDYdcL(2,1)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(2,1)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(2,1)*YucL(2,2)).imag();
    Cquqd8_3311r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(2,2) + Cquqd8_00_LNP*YdcL(0,0)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(2,0)).real();
    Cquqd8_3311i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(0,0) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(0,0) + Cquqd8_0d_LNP*SQDYdcL(0,0)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(0,0)*YucL(2,2) + Cquqd8_00_LNP*YdcL(0,0)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(2,0)).imag();
    Cquqd8_3312r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(2,2) + Cquqd8_00_LNP*YdcL(0,1)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(2,1)).real();
    Cquqd8_3312i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(0,1) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(0,1) + Cquqd8_0d_LNP*SQDYdcL(0,1)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(0,1)*YucL(2,2) + Cquqd8_00_LNP*YdcL(0,1)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(2,1)).imag();
    Cquqd8_3313r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(2,2) + Cquqd8_00_LNP*YdcL(0,2)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(2,2)).real();
    Cquqd8_3313i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(0,2) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(0,2) + Cquqd8_0d_LNP*SQDYdcL(0,2)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(0,2)*YucL(2,2) + Cquqd8_00_LNP*YdcL(0,2)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(0,2) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(0,2) + Cquqd8p_0d_LNP*SQDYdcL(0,2)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(0,2)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(0,2)*YucL(2,2)).imag();
    Cquqd8_3321r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(2,2) + Cquqd8_00_LNP*YdcL(1,0)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(2,0)).real();
    Cquqd8_3321i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(1,0) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(1,0) + Cquqd8_0d_LNP*SQDYdcL(1,0)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(1,0)*YucL(2,2) + Cquqd8_00_LNP*YdcL(1,0)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(2,0)).imag();
    Cquqd8_3322r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(2,2) + Cquqd8_00_LNP*YdcL(1,1)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(2,1)).real();
    Cquqd8_3322i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(1,1) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(1,1) + Cquqd8_0d_LNP*SQDYdcL(1,1)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(1,1)*YucL(2,2) + Cquqd8_00_LNP*YdcL(1,1)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(2,1)).imag();
    Cquqd8_3323r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(2,2) + Cquqd8_00_LNP*YdcL(1,2)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(2,2)).real();
    Cquqd8_3323i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(1,2) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(1,2) + Cquqd8_0d_LNP*SQDYdcL(1,2)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(1,2)*YucL(2,2) + Cquqd8_00_LNP*YdcL(1,2)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(1,2) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(1,2) + Cquqd8p_0d_LNP*SQDYdcL(1,2)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(1,2)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(1,2)*YucL(2,2)).imag();
    Cquqd8_3331r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(2,2) + Cquqd8_00_LNP*YdcL(2,0)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(2,0)).real();
    Cquqd8_3331i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(2,0) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(2,0) + Cquqd8_0d_LNP*SQDYdcL(2,0)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(2,0)*YucL(2,2) + Cquqd8_00_LNP*YdcL(2,0)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,0)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(2,0)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(2,0) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(2,0) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(2,0)).imag();
    Cquqd8_3332r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(2,2) + Cquqd8_00_LNP*YdcL(2,1)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(2,1)).real();
    Cquqd8_3332i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(2,1) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(2,1) + Cquqd8_0d_LNP*SQDYdcL(2,1)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(2,1)*YucL(2,2) + Cquqd8_00_LNP*YdcL(2,1)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,1)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(2,1)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(2,1) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(2,1) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(2,1)).imag();
    Cquqd8_3333r_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(2,2) + Cquqd8_00_LNP*YdcL(2,2)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(2,2)).real();
    Cquqd8_3333i_LNP = (Cquqd8_d0_LNP*SQDYucL(2,2)*YdcL(2,2) + Cquqd8_u0_LNP*SQUYucL(2,2)*YdcL(2,2) + Cquqd8_0d_LNP*SQDYdcL(2,2)*YucL(2,2) + Cquqd8_0u_LNP*SQUYdcL(2,2)*YucL(2,2) + Cquqd8_00_LNP*YdcL(2,2)*YucL(2,2) + Cquqd8p_d0_LNP*SQDYucL(2,2)*YdcL(2,2) + Cquqd8p_u0_LNP*SQUYucL(2,2)*YdcL(2,2) + Cquqd8p_0d_LNP*SQDYdcL(2,2)*YucL(2,2) + Cquqd8p_0u_LNP*SQUYdcL(2,2)*YucL(2,2) + Cquqd8p_00_LNP*YdcL(2,2)*YucL(2,2)).imag();
 
}

◆ setParameter()

void NPSMEFTd6MFV::setParameter	(	const std::string	name,
		const double &	value
	)

protectedvirtual

Reimplemented from StandardModel.

Definition at line 223 of file NPSMEFTd6MFV.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) {
        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("Cll_aabb_LNP") == 0) {
        Cll_aabb_LNP = value;
    } else if (name.compare("Cll_abba_LNP") == 0) {
        Cll_abba_LNP = value;
    } else if (name.compare("Cee_LNP") == 0) {
        Cee_LNP = value;
    } else if (name.compare("Cle_LNP") == 0) {
        Cle_LNP = value;
    } else if (name.compare("CuH_0_LNP") == 0) {
        CuH_0_LNP = value;
    } else if (name.compare("CuH_u_LNP") == 0) {
        CuH_u_LNP = value;
    } else if (name.compare("CuH_d_LNP") == 0) {
        CuH_d_LNP = value;
    } else if (name.compare("CuG_0_LNP") == 0) {
        CuG_0_LNP = value;
    } else if (name.compare("CuG_u_LNP") == 0) {
        CuG_u_LNP = value;
    } else if (name.compare("CuG_d_LNP") == 0) {
        CuG_d_LNP = value;
    } else if (name.compare("CuW_0_LNP") == 0) {
        CuW_0_LNP = value;
    } else if (name.compare("CuW_u_LNP") == 0) {
        CuW_u_LNP = value;
    } else if (name.compare("CuW_d_LNP") == 0) {
        CuW_d_LNP = value;
    } else if (name.compare("CuB_0_LNP") == 0) {
        CuB_0_LNP = value;
    } else if (name.compare("CuB_u_LNP") == 0) {
        CuB_u_LNP = value;
    } else if (name.compare("CuB_d_LNP") == 0) {
        CuB_d_LNP = value;
    } else if (name.compare("CdH_0_LNP") == 0) {
        CdH_0_LNP = value;
    } else if (name.compare("CdH_u_LNP") == 0) {
        CdH_u_LNP = value;
    } else if (name.compare("CdH_d_LNP") == 0) {
        CdH_d_LNP = value;
    } else if (name.compare("CdG_0_LNP") == 0) {
        CdG_0_LNP = value;
    } else if (name.compare("CdG_u_LNP") == 0) {
        CdG_u_LNP = value;
    } else if (name.compare("CdG_d_LNP") == 0) {
        CdG_d_LNP = value;
    } else if (name.compare("CdW_0_LNP") == 0) {
        CdW_0_LNP = value;
    } else if (name.compare("CdW_u_LNP") == 0) {
        CdW_u_LNP = value;
    } else if (name.compare("CdW_d_LNP") == 0) {
        CdW_d_LNP = value;
    } else if (name.compare("CdB_0_LNP") == 0) {
        CdB_0_LNP = value;
    } else if (name.compare("CdB_u_LNP") == 0) {
        CdB_u_LNP = value;
    } else if (name.compare("CdB_d_LNP") == 0) {
        CdB_d_LNP = value;
    } else if (name.compare("CHq1_0_LNP") == 0) {
        CHq1_0_LNP = value;
    } else if (name.compare("CHq1_u_LNP") == 0) {
        CHq1_u_LNP = value;
    } else if (name.compare("CHq1_d_LNP") == 0) {
        CHq1_d_LNP = value;
    } else if (name.compare("CHq3_0_LNP") == 0) {
        CHq3_0_LNP = value;
    } else if (name.compare("CHq3_u_LNP") == 0) {
        CHq3_u_LNP = value;
    } else if (name.compare("CHq3_d_LNP") == 0) {
        CHq3_d_LNP = value;
    } else if (name.compare("CHu_0_LNP") == 0) {
        CHu_0_LNP = value;
    } else if (name.compare("CHu_u_LNP") == 0) {
        CHu_u_LNP = value;
    } else if (name.compare("CHd_0_LNP") == 0) {
        CHd_0_LNP = value;
    } else if (name.compare("CHd_d_LNP") == 0) {
        CHd_d_LNP = value;
    } else if (name.compare("CHud_ud_LNP") == 0) {
        CHud_ud_LNP = value;
    } else if (name.compare("Clq1_0_LNP") == 0) {
        Clq1_0_LNP = value;
    } else if (name.compare("Clq1_u_LNP") == 0) {
        Clq1_u_LNP = value;
    } else if (name.compare("Clq1_d_LNP") == 0) {
        Clq1_d_LNP = value;
    } else if (name.compare("Clq3_0_LNP") == 0) {
        Clq3_0_LNP = value;
    } else if (name.compare("Clq3_u_LNP") == 0) {
        Clq3_u_LNP = value;
    } else if (name.compare("Clq3_d_LNP") == 0) {
        Clq3_d_LNP = value;
    } else if (name.compare("Cqe_0_LNP") == 0) {
        Cqe_0_LNP = value;
    } else if (name.compare("Cqe_u_LNP") == 0) {
        Cqe_u_LNP = value;
    } else if (name.compare("Cqe_d_LNP") == 0) {
        Cqe_d_LNP = value;
    } else if (name.compare("Clu_0_LNP") == 0) {
        Clu_0_LNP = value;
    } else if (name.compare("Clu_u_LNP") == 0) {
        Clu_u_LNP = value;
    } else if (name.compare("Ceu_0_LNP") == 0) {
        Ceu_0_LNP = value;
    } else if (name.compare("Ceu_u_LNP") == 0) {
        Ceu_u_LNP = value;
    } else if (name.compare("Cld_0_LNP") == 0) {
        Cld_0_LNP = value;
    } else if (name.compare("Cld_d_LNP") == 0) {
        Cld_d_LNP = value;
    } else if (name.compare("Ced_0_LNP") == 0) {
        Ced_0_LNP = value;
    } else if (name.compare("Ced_d_LNP") == 0) {
        Ced_d_LNP = value;
    } else if (name.compare("Cqq1_00_LNP") == 0) {
        Cqq1_00_LNP = value;
    } else if (name.compare("Cqq1_u0_LNP") == 0) {
        Cqq1_u0_LNP = value;
    } else if (name.compare("Cqq1_d0_LNP") == 0) {
        Cqq1_d0_LNP = value;
    } else if (name.compare("Cqq1_uu_LNP") == 0) {
        Cqq1_uu_LNP = value;
    } else if (name.compare("Cqq1_dd_LNP") == 0) {
        Cqq1_dd_LNP = value;
    } else if (name.compare("Cqq1_ud_LNP") == 0) {
        Cqq1_ud_LNP = value;
    } else if (name.compare("Cqq1p_00_LNP") == 0) {
        Cqq1p_00_LNP = value;
    } else if (name.compare("Cqq1p_u0_LNP") == 0) {
        Cqq1p_u0_LNP = value;
    } else if (name.compare("Cqq1p_d0_LNP") == 0) {
        Cqq1p_d0_LNP = value;
    } else if (name.compare("Cqq1p_uu_LNP") == 0) {
        Cqq1p_uu_LNP = value;
    } else if (name.compare("Cqq1p_dd_LNP") == 0) {
        Cqq1p_dd_LNP = value;
    } else if (name.compare("Cqq1p_ud_LNP") == 0) {
        Cqq1p_ud_LNP = value;
    } else if (name.compare("Cqq3_00_LNP") == 0) {
        Cqq3_00_LNP = value;
    } else if (name.compare("Cqq3_u0_LNP") == 0) {
        Cqq3_u0_LNP = value;
    } else if (name.compare("Cqq3_d0_LNP") == 0) {
        Cqq3_d0_LNP = value;
    } else if (name.compare("Cqq3_uu_LNP") == 0) {
        Cqq3_uu_LNP = value;
    } else if (name.compare("Cqq3_dd_LNP") == 0) {
        Cqq3_dd_LNP = value;
    } else if (name.compare("Cqq3_ud_LNP") == 0) {
        Cqq3_ud_LNP = value;
    } else if (name.compare("Cqq3p_00_LNP") == 0) {
        Cqq3p_00_LNP = value;
    } else if (name.compare("Cqq3p_u0_LNP") == 0) {
        Cqq3p_u0_LNP = value;
    } else if (name.compare("Cqq3p_d0_LNP") == 0) {
        Cqq3p_d0_LNP = value;
    } else if (name.compare("Cqq3p_uu_LNP") == 0) {
        Cqq3p_uu_LNP = value;
    } else if (name.compare("Cqq3p_dd_LNP") == 0) {
        Cqq3p_dd_LNP = value;
    } else if (name.compare("Cqq3p_ud_LNP") == 0) {
        Cqq3p_ud_LNP = value;
    } else if (name.compare("Cuu_00_LNP") == 0) {
        Cuu_00_LNP = value;
    } else if (name.compare("Cuu_u0_LNP") == 0) {
        Cuu_u0_LNP = value;
    } else if (name.compare("Cuu_uu_LNP") == 0) {
        Cuu_uu_LNP = value;
    } else if (name.compare("Cuup_00_LNP") == 0) {
        Cuup_00_LNP = value;
    } else if (name.compare("Cuup_u0_LNP") == 0) {
        Cuup_u0_LNP = value;
    } else if (name.compare("Cuup_uu_LNP") == 0) {
        Cuup_uu_LNP = value;
    } else if (name.compare("Cdd_00_LNP") == 0) {
        Cdd_00_LNP = value;
    } else if (name.compare("Cdd_d0_LNP") == 0) {
        Cdd_d0_LNP = value;
    } else if (name.compare("Cdd_dd_LNP") == 0) {
        Cdd_dd_LNP = value;
    } else if (name.compare("Cddp_00_LNP") == 0) {
        Cddp_00_LNP = value;
    } else if (name.compare("Cddp_d0_LNP") == 0) {
        Cddp_d0_LNP = value;
    } else if (name.compare("Cddp_dd_LNP") == 0) {
        Cddp_dd_LNP = value;
    } else if (name.compare("Cud1_00_LNP") == 0) {
        Cud1_00_LNP = value;
    } else if (name.compare("Cud1_u0_LNP") == 0) {
        Cud1_u0_LNP = value;
    } else if (name.compare("Cud1_0d_LNP") == 0) {
        Cud1_0d_LNP = value;
    } else if (name.compare("Cud1_ud_LNP") == 0) {
        Cud1_ud_LNP = value;
    } else if (name.compare("Cud1p_ud_LNP") == 0) {
        Cud1p_ud_LNP = value;
    } else if (name.compare("Cud8_00_LNP") == 0) {
        Cud8_00_LNP = value;
    } else if (name.compare("Cud8_u0_LNP") == 0) {
        Cud8_u0_LNP = value;
    } else if (name.compare("Cud8_0d_LNP") == 0) {
        Cud8_0d_LNP = value;
    } else if (name.compare("Cud8_ud_LNP") == 0) {
        Cud8_ud_LNP = value;
    } else if (name.compare("Cud8p_ud_LNP") == 0) {
        Cud8p_ud_LNP = value;
    } else if (name.compare("Cqu1_00_LNP") == 0) {
        Cqu1_00_LNP = value;
    } else if (name.compare("Cqu1_u0_LNP") == 0) {
        Cqu1_u0_LNP = value;
    } else if (name.compare("Cqu1_d0_LNP") == 0) {
        Cqu1_d0_LNP = value;
    } else if (name.compare("Cqu1_0u_LNP") == 0) {
        Cqu1_0u_LNP = value;
    } else if (name.compare("Cqu1_uu_LNP") == 0) {
        Cqu1_uu_LNP = value;
    } else if (name.compare("Cqu1_du_LNP") == 0) {
        Cqu1_du_LNP = value;
    } else if (name.compare("Cqu1_y_LNP") == 0) {
        Cqu1_y_LNP = value;
    } else if (name.compare("Cqu1_uy_LNP") == 0) {
        Cqu1_uy_LNP = value;
    } else if (name.compare("Cqu1_dy_LNP") == 0) {
        Cqu1_dy_LNP = value;
    } else if (name.compare("Cqu1_yu_LNP") == 0) {
        Cqu1_yu_LNP = value;
    } else if (name.compare("Cqu1_yd_LNP") == 0) {
        Cqu1_yd_LNP = value;
    } else if (name.compare("Cqu8_00_LNP") == 0) {
        Cqu8_00_LNP = value;
    } else if (name.compare("Cqu8_u0_LNP") == 0) {
        Cqu8_u0_LNP = value;
    } else if (name.compare("Cqu8_d0_LNP") == 0) {
        Cqu8_d0_LNP = value;
    } else if (name.compare("Cqu8_0u_LNP") == 0) {
        Cqu8_0u_LNP = value;
    } else if (name.compare("Cqu8_uu_LNP") == 0) {
        Cqu8_uu_LNP = value;
    } else if (name.compare("Cqu8_du_LNP") == 0) {
        Cqu8_du_LNP = value;
    } else if (name.compare("Cqu8_y_LNP") == 0) {
        Cqu8_y_LNP = value;
    } else if (name.compare("Cqu8_uy_LNP") == 0) {
        Cqu8_uy_LNP = value;
    } else if (name.compare("Cqu8_dy_LNP") == 0) {
        Cqu8_dy_LNP = value;
    } else if (name.compare("Cqu8_yu_LNP") == 0) {
        Cqu8_yu_LNP = value;
    } else if (name.compare("Cqu8_yd_LNP") == 0) {
        Cqu8_yd_LNP = value;
    } else if (name.compare("Cqd1_00_LNP") == 0) {
        Cqd1_00_LNP = value;
    } else if (name.compare("Cqd1_u0_LNP") == 0) {
        Cqd1_u0_LNP = value;
    } else if (name.compare("Cqd1_d0_LNP") == 0) {
        Cqd1_d0_LNP = value;
    } else if (name.compare("Cqd1_0d_LNP") == 0) {
        Cqd1_0d_LNP = value;
    } else if (name.compare("Cqd1_ud_LNP") == 0) {
        Cqd1_ud_LNP = value;
    } else if (name.compare("Cqd1_dd_LNP") == 0) {
        Cqd1_dd_LNP = value;
    } else if (name.compare("Cqd1_y_LNP") == 0) {
        Cqd1_y_LNP = value;
    } else if (name.compare("Cqd1_uy_LNP") == 0) {
        Cqd1_uy_LNP = value;
    } else if (name.compare("Cqd1_dy_LNP") == 0) {
        Cqd1_dy_LNP = value;
    } else if (name.compare("Cqd1_yu_LNP") == 0) {
        Cqd1_yu_LNP = value;
    } else if (name.compare("Cqd1_yd_LNP") == 0) {
        Cqd1_yd_LNP = value;
    } else if (name.compare("Cqd8_00_LNP") == 0) {
        Cqd8_00_LNP = value;
    } else if (name.compare("Cqd8_u0_LNP") == 0) {
        Cqd8_u0_LNP = value;
    } else if (name.compare("Cqd8_d0_LNP") == 0) {
        Cqd8_d0_LNP = value;
    } else if (name.compare("Cqd8_0d_LNP") == 0) {
        Cqd8_0d_LNP = value;
    } else if (name.compare("Cqd8_ud_LNP") == 0) {
        Cqd8_ud_LNP = value;
    } else if (name.compare("Cqd8_dd_LNP") == 0) {
        Cqd8_dd_LNP = value;
    } else if (name.compare("Cqd8_y_LNP") == 0) {
        Cqd8_y_LNP = value;
    } else if (name.compare("Cqd8_uy_LNP") == 0) {
        Cqd8_uy_LNP = value;
    } else if (name.compare("Cqd8_dy_LNP") == 0) {
        Cqd8_dy_LNP = value;
    } else if (name.compare("Cqd8_yu_LNP") == 0) {
        Cqd8_yu_LNP = value;
    } else if (name.compare("Cqd8_yd_LNP") == 0) {
        Cqd8_yd_LNP = value;
    } else if (name.compare("Cquqd1_00_LNP") == 0) {
        Cquqd1_00_LNP = value;
    } else if (name.compare("Cquqd1_u0_LNP") == 0) {
        Cquqd1_u0_LNP = value;
    } else if (name.compare("Cquqd1_d0_LNP") == 0) {
        Cquqd1_d0_LNP = value;
    } else if (name.compare("Cquqd1_0u_LNP") == 0) {
        Cquqd1_0u_LNP = value;
    } else if (name.compare("Cquqd1_0d_LNP") == 0) {
        Cquqd1_0d_LNP = value;
    } else if (name.compare("Cquqd1p_00_LNP") == 0) {
        Cquqd1p_00_LNP = value;
    } else if (name.compare("Cquqd1p_u0_LNP") == 0) {
        Cquqd1p_u0_LNP = value;
    } else if (name.compare("Cquqd1p_d0_LNP") == 0) {
        Cquqd1p_d0_LNP = value;
    } else if (name.compare("Cquqd1p_0u_LNP") == 0) {
        Cquqd1p_0u_LNP = value;
    } else if (name.compare("Cquqd1p_0d_LNP") == 0) {
        Cquqd1p_0d_LNP = value;
    } else if (name.compare("Cquqd8_00_LNP") == 0) {
        Cquqd8_00_LNP = value;
    } else if (name.compare("Cquqd8_u0_LNP") == 0) {
        Cquqd8_u0_LNP = value;
    } else if (name.compare("Cquqd8_d0_LNP") == 0) {
        Cquqd8_d0_LNP = value;
    } else if (name.compare("Cquqd8_0u_LNP") == 0) {
        Cquqd8_0u_LNP = value;
    } else if (name.compare("Cquqd8_0d_LNP") == 0) {
        Cquqd8_0d_LNP = value;
    } else if (name.compare("Cquqd8p_00_LNP") == 0) {
        Cquqd8p_00_LNP = value;
    } else if (name.compare("Cquqd8p_u0_LNP") == 0) {
        Cquqd8p_u0_LNP = value;
    } else if (name.compare("Cquqd8p_d0_LNP") == 0) {
        Cquqd8p_d0_LNP = value;
    } else if (name.compare("Cquqd8p_0u_LNP") == 0) {
        Cquqd8p_0u_LNP = value;
    } else if (name.compare("Cquqd8p_0d_LNP") == 0) {
        Cquqd8p_0d_LNP = value;
    }  else if (name.compare("Lambda_NP") == 0) {
        Lambda_NP = value;
    } else {
        NPSMEFTd6General::setParameter(name, value);
    }
}

Member Data Documentation

◆ CdB_0_LNP

double NPSMEFTd6MFV::CdB_0_LNP = 0.

protected

Definition at line 77 of file NPSMEFTd6MFV.h.

◆ CdB_d_LNP

double NPSMEFTd6MFV::CdB_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{Hq}^{(1)})_{ij}$.

Definition at line 77 of file NPSMEFTd6MFV.h.

◆ CdB_u_LNP

double NPSMEFTd6MFV::CdB_u_LNP = 0.

protected

Definition at line 77 of file NPSMEFTd6MFV.h.

◆ Cdd_00_LNP

double NPSMEFTd6MFV::Cdd_00_LNP = 0.

protected

Definition at line 125 of file NPSMEFTd6MFV.h.

◆ Cdd_d0_LNP

double NPSMEFTd6MFV::Cdd_d0_LNP = 0.

protected

Definition at line 125 of file NPSMEFTd6MFV.h.

◆ Cdd_dd_LNP

double NPSMEFTd6MFV::Cdd_dd_LNP = 0.

protected

Definition at line 125 of file NPSMEFTd6MFV.h.

◆ Cddp_00_LNP

double NPSMEFTd6MFV::Cddp_00_LNP = 0.

protected

Definition at line 125 of file NPSMEFTd6MFV.h.

◆ Cddp_d0_LNP

double NPSMEFTd6MFV::Cddp_d0_LNP = 0.

protected

Definition at line 125 of file NPSMEFTd6MFV.h.

◆ Cddp_dd_LNP

double NPSMEFTd6MFV::Cddp_dd_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ud}^{(1)})_{ijkm}$.

Definition at line 125 of file NPSMEFTd6MFV.h.

◆ CdG_0_LNP

double NPSMEFTd6MFV::CdG_0_LNP = 0.

protected

Definition at line 71 of file NPSMEFTd6MFV.h.

◆ CdG_d_LNP

double NPSMEFTd6MFV::CdG_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{dW})_{ij}$.

Definition at line 71 of file NPSMEFTd6MFV.h.

◆ CdG_u_LNP

double NPSMEFTd6MFV::CdG_u_LNP = 0.

protected

Definition at line 71 of file NPSMEFTd6MFV.h.

◆ CdH_0_LNP

double NPSMEFTd6MFV::CdH_0_LNP = 0.

protected

Definition at line 68 of file NPSMEFTd6MFV.h.

◆ CdH_d_LNP

double NPSMEFTd6MFV::CdH_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{dG})_{ij}$.

Definition at line 68 of file NPSMEFTd6MFV.h.

◆ CdH_u_LNP

double NPSMEFTd6MFV::CdH_u_LNP = 0.

protected

Definition at line 68 of file NPSMEFTd6MFV.h.

◆ CdW_0_LNP

double NPSMEFTd6MFV::CdW_0_LNP = 0.

protected

Definition at line 74 of file NPSMEFTd6MFV.h.

◆ CdW_d_LNP

double NPSMEFTd6MFV::CdW_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{dB})_{ij}$.

Definition at line 74 of file NPSMEFTd6MFV.h.

◆ CdW_u_LNP

double NPSMEFTd6MFV::CdW_u_LNP = 0.

protected

Definition at line 74 of file NPSMEFTd6MFV.h.

◆ Ced_0_LNP

double NPSMEFTd6MFV::Ced_0_LNP = 0.

protected

Definition at line 113 of file NPSMEFTd6MFV.h.

◆ Ced_d_LNP

double NPSMEFTd6MFV::Ced_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qq}^{(1)})_{ijkm}$.

Definition at line 113 of file NPSMEFTd6MFV.h.

◆ Cee_LNP

double NPSMEFTd6MFV::Cee_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{le})_{ijkm}$.

Definition at line 50 of file NPSMEFTd6MFV.h.

◆ Ceu_0_LNP

double NPSMEFTd6MFV::Ceu_0_LNP = 0.

protected

Definition at line 107 of file NPSMEFTd6MFV.h.

◆ Ceu_u_LNP

double NPSMEFTd6MFV::Ceu_u_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ld})_{ijkm}$.

Definition at line 107 of file NPSMEFTd6MFV.h.

◆ CHd_0_LNP

double NPSMEFTd6MFV::CHd_0_LNP = 0.

protected

Definition at line 89 of file NPSMEFTd6MFV.h.

◆ CHd_d_LNP

double NPSMEFTd6MFV::CHd_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{Hud})_{ij}$.

Definition at line 89 of file NPSMEFTd6MFV.h.

◆ CHe_LNP

double NPSMEFTd6MFV::CHe_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ll})_{ijkm}$.

Definition at line 41 of file NPSMEFTd6MFV.h.

◆ CHl1_LNP

double NPSMEFTd6MFV::CHl1_LNP = 0.

protected

< Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{Hl}^{(1)})_{ij}$.

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{Hl}^{(3)})_{ij}$.

Definition at line 35 of file NPSMEFTd6MFV.h.

◆ CHl3_LNP

double NPSMEFTd6MFV::CHl3_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{He})_{ij}$.

Definition at line 38 of file NPSMEFTd6MFV.h.

◆ CHq1_0_LNP

double NPSMEFTd6MFV::CHq1_0_LNP = 0.

protected

Definition at line 80 of file NPSMEFTd6MFV.h.

◆ CHq1_d_LNP

double NPSMEFTd6MFV::CHq1_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{Hq}^{(3)})_{ij}$.

Definition at line 80 of file NPSMEFTd6MFV.h.

◆ CHq1_u_LNP

double NPSMEFTd6MFV::CHq1_u_LNP = 0.

protected

Definition at line 80 of file NPSMEFTd6MFV.h.

◆ CHq3_0_LNP

double NPSMEFTd6MFV::CHq3_0_LNP = 0.

protected

Definition at line 83 of file NPSMEFTd6MFV.h.

◆ CHq3_d_LNP

double NPSMEFTd6MFV::CHq3_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{Hu})_{ij}$.

Definition at line 83 of file NPSMEFTd6MFV.h.

◆ CHq3_u_LNP

double NPSMEFTd6MFV::CHq3_u_LNP = 0.

protected

Definition at line 83 of file NPSMEFTd6MFV.h.

◆ CHu_0_LNP

double NPSMEFTd6MFV::CHu_0_LNP = 0.

protected

Definition at line 86 of file NPSMEFTd6MFV.h.

◆ CHu_u_LNP

double NPSMEFTd6MFV::CHu_u_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{Hd})_{ij}$.

Definition at line 86 of file NPSMEFTd6MFV.h.

◆ CHud_ud_LNP

double NPSMEFTd6MFV::CHud_ud_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{lq}^{(1)})_{ijkm}$.

Definition at line 92 of file NPSMEFTd6MFV.h.

◆ Cld_0_LNP

double NPSMEFTd6MFV::Cld_0_LNP = 0.

protected

Definition at line 110 of file NPSMEFTd6MFV.h.

◆ Cld_d_LNP

double NPSMEFTd6MFV::Cld_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ed})_{ijkm}$.

Definition at line 110 of file NPSMEFTd6MFV.h.

◆ Cle_LNP

double NPSMEFTd6MFV::Cle_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{uH})_{ij}$.

Definition at line 53 of file NPSMEFTd6MFV.h.

◆ Cll_aabb_LNP

double NPSMEFTd6MFV::Cll_aabb_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ll})_{ijkm}$.

Definition at line 44 of file NPSMEFTd6MFV.h.

◆ Cll_abba_LNP

double NPSMEFTd6MFV::Cll_abba_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ee})_{ijkm}$.

Definition at line 47 of file NPSMEFTd6MFV.h.

◆ Clq1_0_LNP

double NPSMEFTd6MFV::Clq1_0_LNP = 0.

protected

Definition at line 95 of file NPSMEFTd6MFV.h.

◆ Clq1_d_LNP

double NPSMEFTd6MFV::Clq1_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{lq}^{(3)})_{ijkm}$.

Definition at line 95 of file NPSMEFTd6MFV.h.

◆ Clq1_u_LNP

double NPSMEFTd6MFV::Clq1_u_LNP = 0.

protected

Definition at line 95 of file NPSMEFTd6MFV.h.

◆ Clq3_0_LNP

double NPSMEFTd6MFV::Clq3_0_LNP = 0.

protected

Definition at line 98 of file NPSMEFTd6MFV.h.

◆ Clq3_d_LNP

double NPSMEFTd6MFV::Clq3_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qe})_{ijkm}$.

Definition at line 98 of file NPSMEFTd6MFV.h.

◆ Clq3_u_LNP

double NPSMEFTd6MFV::Clq3_u_LNP = 0.

protected

Definition at line 98 of file NPSMEFTd6MFV.h.

◆ Clu_0_LNP

double NPSMEFTd6MFV::Clu_0_LNP = 0.

protected

Definition at line 104 of file NPSMEFTd6MFV.h.

◆ Clu_u_LNP

double NPSMEFTd6MFV::Clu_u_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{eu})_{ijkm}$.

Definition at line 104 of file NPSMEFTd6MFV.h.

◆ Cqd1_00_LNP

double NPSMEFTd6MFV::Cqd1_00_LNP = 0.

protected

Definition at line 140 of file NPSMEFTd6MFV.h.

◆ Cqd1_0d_LNP

double NPSMEFTd6MFV::Cqd1_0d_LNP = 0.

protected

Definition at line 140 of file NPSMEFTd6MFV.h.

◆ Cqd1_d0_LNP

double NPSMEFTd6MFV::Cqd1_d0_LNP = 0.

protected

Definition at line 140 of file NPSMEFTd6MFV.h.

◆ Cqd1_dd_LNP

double NPSMEFTd6MFV::Cqd1_dd_LNP = 0.

protected

Definition at line 140 of file NPSMEFTd6MFV.h.

◆ Cqd1_dy_LNP

double NPSMEFTd6MFV::Cqd1_dy_LNP = 0.

protected

Definition at line 140 of file NPSMEFTd6MFV.h.

◆ Cqd1_u0_LNP

double NPSMEFTd6MFV::Cqd1_u0_LNP = 0.

protected

Definition at line 140 of file NPSMEFTd6MFV.h.

◆ Cqd1_ud_LNP

double NPSMEFTd6MFV::Cqd1_ud_LNP = 0.

protected

Definition at line 140 of file NPSMEFTd6MFV.h.

◆ Cqd1_uy_LNP

double NPSMEFTd6MFV::Cqd1_uy_LNP = 0.

protected

Definition at line 140 of file NPSMEFTd6MFV.h.

◆ Cqd1_y_LNP

double NPSMEFTd6MFV::Cqd1_y_LNP = 0.

protected

Definition at line 140 of file NPSMEFTd6MFV.h.

◆ Cqd1_yd_LNP

double NPSMEFTd6MFV::Cqd1_yd_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qd}^{(8)})_{ijkm}$.

Definition at line 140 of file NPSMEFTd6MFV.h.

◆ Cqd1_yu_LNP

double NPSMEFTd6MFV::Cqd1_yu_LNP = 0.

protected

Definition at line 140 of file NPSMEFTd6MFV.h.

◆ Cqd8_00_LNP

double NPSMEFTd6MFV::Cqd8_00_LNP = 0.

protected

Definition at line 143 of file NPSMEFTd6MFV.h.

◆ Cqd8_0d_LNP

double NPSMEFTd6MFV::Cqd8_0d_LNP = 0.

protected

Definition at line 143 of file NPSMEFTd6MFV.h.

◆ Cqd8_d0_LNP

double NPSMEFTd6MFV::Cqd8_d0_LNP = 0.

protected

Definition at line 143 of file NPSMEFTd6MFV.h.

◆ Cqd8_dd_LNP

double NPSMEFTd6MFV::Cqd8_dd_LNP = 0.

protected

Definition at line 143 of file NPSMEFTd6MFV.h.

◆ Cqd8_dy_LNP

double NPSMEFTd6MFV::Cqd8_dy_LNP = 0.

protected

Definition at line 143 of file NPSMEFTd6MFV.h.

◆ Cqd8_u0_LNP

double NPSMEFTd6MFV::Cqd8_u0_LNP = 0.

protected

Definition at line 143 of file NPSMEFTd6MFV.h.

◆ Cqd8_ud_LNP

double NPSMEFTd6MFV::Cqd8_ud_LNP = 0.

protected

Definition at line 143 of file NPSMEFTd6MFV.h.

◆ Cqd8_uy_LNP

double NPSMEFTd6MFV::Cqd8_uy_LNP = 0.

protected

Definition at line 143 of file NPSMEFTd6MFV.h.

◆ Cqd8_y_LNP

double NPSMEFTd6MFV::Cqd8_y_LNP = 0.

protected

Definition at line 143 of file NPSMEFTd6MFV.h.

◆ Cqd8_yd_LNP

double NPSMEFTd6MFV::Cqd8_yd_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{quqd}^{(1)})_{ijkm}$.

Definition at line 143 of file NPSMEFTd6MFV.h.

◆ Cqd8_yu_LNP

double NPSMEFTd6MFV::Cqd8_yu_LNP = 0.

protected

Definition at line 143 of file NPSMEFTd6MFV.h.

◆ Cqe_0_LNP

double NPSMEFTd6MFV::Cqe_0_LNP = 0.

protected

Definition at line 101 of file NPSMEFTd6MFV.h.

◆ Cqe_d_LNP

double NPSMEFTd6MFV::Cqe_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{lu})_{ijkm}$.

Definition at line 101 of file NPSMEFTd6MFV.h.

◆ Cqe_u_LNP

double NPSMEFTd6MFV::Cqe_u_LNP = 0.

protected

Definition at line 101 of file NPSMEFTd6MFV.h.

◆ Cqq1_00_LNP

double NPSMEFTd6MFV::Cqq1_00_LNP = 0.

protected

Definition at line 116 of file NPSMEFTd6MFV.h.

◆ Cqq1_d0_LNP

double NPSMEFTd6MFV::Cqq1_d0_LNP = 0.

protected

Definition at line 116 of file NPSMEFTd6MFV.h.

◆ Cqq1_dd_LNP

double NPSMEFTd6MFV::Cqq1_dd_LNP = 0.

protected

Definition at line 116 of file NPSMEFTd6MFV.h.

◆ Cqq1_u0_LNP

double NPSMEFTd6MFV::Cqq1_u0_LNP = 0.

protected

Definition at line 116 of file NPSMEFTd6MFV.h.

◆ Cqq1_ud_LNP

double NPSMEFTd6MFV::Cqq1_ud_LNP = 0.

protected

Definition at line 116 of file NPSMEFTd6MFV.h.

◆ Cqq1_uu_LNP

double NPSMEFTd6MFV::Cqq1_uu_LNP = 0.

protected

Definition at line 116 of file NPSMEFTd6MFV.h.

◆ Cqq1p_00_LNP

double NPSMEFTd6MFV::Cqq1p_00_LNP = 0.

protected

Definition at line 116 of file NPSMEFTd6MFV.h.

◆ Cqq1p_d0_LNP

double NPSMEFTd6MFV::Cqq1p_d0_LNP = 0.

protected

Definition at line 116 of file NPSMEFTd6MFV.h.

◆ Cqq1p_dd_LNP

double NPSMEFTd6MFV::Cqq1p_dd_LNP = 0.

protected

Definition at line 116 of file NPSMEFTd6MFV.h.

◆ Cqq1p_u0_LNP

double NPSMEFTd6MFV::Cqq1p_u0_LNP = 0.

protected

Definition at line 116 of file NPSMEFTd6MFV.h.

◆ Cqq1p_ud_LNP

double NPSMEFTd6MFV::Cqq1p_ud_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qq}^{(3)})_{ijkm}$.

Definition at line 116 of file NPSMEFTd6MFV.h.

◆ Cqq1p_uu_LNP

double NPSMEFTd6MFV::Cqq1p_uu_LNP = 0.

protected

Definition at line 116 of file NPSMEFTd6MFV.h.

◆ Cqq3_00_LNP

double NPSMEFTd6MFV::Cqq3_00_LNP = 0.

protected

Definition at line 119 of file NPSMEFTd6MFV.h.

◆ Cqq3_d0_LNP

double NPSMEFTd6MFV::Cqq3_d0_LNP = 0.

protected

Definition at line 119 of file NPSMEFTd6MFV.h.

◆ Cqq3_dd_LNP

double NPSMEFTd6MFV::Cqq3_dd_LNP = 0.

protected

Definition at line 119 of file NPSMEFTd6MFV.h.

◆ Cqq3_u0_LNP

double NPSMEFTd6MFV::Cqq3_u0_LNP = 0.

protected

Definition at line 119 of file NPSMEFTd6MFV.h.

◆ Cqq3_ud_LNP

double NPSMEFTd6MFV::Cqq3_ud_LNP = 0.

protected

Definition at line 119 of file NPSMEFTd6MFV.h.

◆ Cqq3_uu_LNP

double NPSMEFTd6MFV::Cqq3_uu_LNP = 0.

protected

Definition at line 119 of file NPSMEFTd6MFV.h.

◆ Cqq3p_00_LNP

double NPSMEFTd6MFV::Cqq3p_00_LNP = 0.

protected

Definition at line 119 of file NPSMEFTd6MFV.h.

◆ Cqq3p_d0_LNP

double NPSMEFTd6MFV::Cqq3p_d0_LNP = 0.

protected

Definition at line 119 of file NPSMEFTd6MFV.h.

◆ Cqq3p_dd_LNP

double NPSMEFTd6MFV::Cqq3p_dd_LNP = 0.

protected

Definition at line 119 of file NPSMEFTd6MFV.h.

◆ Cqq3p_u0_LNP

double NPSMEFTd6MFV::Cqq3p_u0_LNP = 0.

protected

Definition at line 119 of file NPSMEFTd6MFV.h.

◆ Cqq3p_ud_LNP

double NPSMEFTd6MFV::Cqq3p_ud_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{uu})_{ijkm}$.

Definition at line 119 of file NPSMEFTd6MFV.h.

◆ Cqq3p_uu_LNP

double NPSMEFTd6MFV::Cqq3p_uu_LNP = 0.

protected

Definition at line 119 of file NPSMEFTd6MFV.h.

◆ Cqu1_00_LNP

double NPSMEFTd6MFV::Cqu1_00_LNP = 0.

protected

Definition at line 134 of file NPSMEFTd6MFV.h.

◆ Cqu1_0u_LNP

double NPSMEFTd6MFV::Cqu1_0u_LNP = 0.

protected

Definition at line 134 of file NPSMEFTd6MFV.h.

◆ Cqu1_d0_LNP

double NPSMEFTd6MFV::Cqu1_d0_LNP = 0.

protected

Definition at line 134 of file NPSMEFTd6MFV.h.

◆ Cqu1_du_LNP

double NPSMEFTd6MFV::Cqu1_du_LNP = 0.

protected

Definition at line 134 of file NPSMEFTd6MFV.h.

◆ Cqu1_dy_LNP

double NPSMEFTd6MFV::Cqu1_dy_LNP = 0.

protected

Definition at line 134 of file NPSMEFTd6MFV.h.

◆ Cqu1_u0_LNP

double NPSMEFTd6MFV::Cqu1_u0_LNP = 0.

protected

Definition at line 134 of file NPSMEFTd6MFV.h.

◆ Cqu1_uu_LNP

double NPSMEFTd6MFV::Cqu1_uu_LNP = 0.

protected

Definition at line 134 of file NPSMEFTd6MFV.h.

◆ Cqu1_uy_LNP

double NPSMEFTd6MFV::Cqu1_uy_LNP = 0.

protected

Definition at line 134 of file NPSMEFTd6MFV.h.

◆ Cqu1_y_LNP

double NPSMEFTd6MFV::Cqu1_y_LNP = 0.

protected

Definition at line 134 of file NPSMEFTd6MFV.h.

◆ Cqu1_yd_LNP

double NPSMEFTd6MFV::Cqu1_yd_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qu}^{(8)})_{ijkm}$.

Definition at line 134 of file NPSMEFTd6MFV.h.

◆ Cqu1_yu_LNP

double NPSMEFTd6MFV::Cqu1_yu_LNP = 0.

protected

Definition at line 134 of file NPSMEFTd6MFV.h.

◆ Cqu8_00_LNP

double NPSMEFTd6MFV::Cqu8_00_LNP = 0.

protected

Definition at line 137 of file NPSMEFTd6MFV.h.

◆ Cqu8_0u_LNP

double NPSMEFTd6MFV::Cqu8_0u_LNP = 0.

protected

Definition at line 137 of file NPSMEFTd6MFV.h.

◆ Cqu8_d0_LNP

double NPSMEFTd6MFV::Cqu8_d0_LNP = 0.

protected

Definition at line 137 of file NPSMEFTd6MFV.h.

◆ Cqu8_du_LNP

double NPSMEFTd6MFV::Cqu8_du_LNP = 0.

protected

Definition at line 137 of file NPSMEFTd6MFV.h.

◆ Cqu8_dy_LNP

double NPSMEFTd6MFV::Cqu8_dy_LNP = 0.

protected

Definition at line 137 of file NPSMEFTd6MFV.h.

◆ Cqu8_u0_LNP

double NPSMEFTd6MFV::Cqu8_u0_LNP = 0.

protected

Definition at line 137 of file NPSMEFTd6MFV.h.

◆ Cqu8_uu_LNP

double NPSMEFTd6MFV::Cqu8_uu_LNP = 0.

protected

Definition at line 137 of file NPSMEFTd6MFV.h.

◆ Cqu8_uy_LNP

double NPSMEFTd6MFV::Cqu8_uy_LNP = 0.

protected

Definition at line 137 of file NPSMEFTd6MFV.h.

◆ Cqu8_y_LNP

double NPSMEFTd6MFV::Cqu8_y_LNP = 0.

protected

Definition at line 137 of file NPSMEFTd6MFV.h.

◆ Cqu8_yd_LNP

double NPSMEFTd6MFV::Cqu8_yd_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qd}^{(1)})_{ijkm}$.

Definition at line 137 of file NPSMEFTd6MFV.h.

◆ Cqu8_yu_LNP

double NPSMEFTd6MFV::Cqu8_yu_LNP = 0.

protected

Definition at line 137 of file NPSMEFTd6MFV.h.

◆ Cquqd1_00_LNP

double NPSMEFTd6MFV::Cquqd1_00_LNP = 0.

protected

Definition at line 146 of file NPSMEFTd6MFV.h.

◆ Cquqd1_0d_LNP

double NPSMEFTd6MFV::Cquqd1_0d_LNP = 0.

protected

Definition at line 146 of file NPSMEFTd6MFV.h.

◆ Cquqd1_0u_LNP

double NPSMEFTd6MFV::Cquqd1_0u_LNP = 0.

protected

Definition at line 146 of file NPSMEFTd6MFV.h.

◆ Cquqd1_d0_LNP

double NPSMEFTd6MFV::Cquqd1_d0_LNP = 0.

protected

Definition at line 146 of file NPSMEFTd6MFV.h.

◆ Cquqd1_u0_LNP

double NPSMEFTd6MFV::Cquqd1_u0_LNP = 0.

protected

Definition at line 146 of file NPSMEFTd6MFV.h.

◆ Cquqd1p_00_LNP

double NPSMEFTd6MFV::Cquqd1p_00_LNP = 0.

protected

Definition at line 146 of file NPSMEFTd6MFV.h.

◆ Cquqd1p_0d_LNP

double NPSMEFTd6MFV::Cquqd1p_0d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{quqd}^{(8)})_{ijkm}$.

Definition at line 146 of file NPSMEFTd6MFV.h.

◆ Cquqd1p_0u_LNP

double NPSMEFTd6MFV::Cquqd1p_0u_LNP = 0.

protected

Definition at line 146 of file NPSMEFTd6MFV.h.

◆ Cquqd1p_d0_LNP

double NPSMEFTd6MFV::Cquqd1p_d0_LNP = 0.

protected

Definition at line 146 of file NPSMEFTd6MFV.h.

◆ Cquqd1p_u0_LNP

double NPSMEFTd6MFV::Cquqd1p_u0_LNP = 0.

protected

Definition at line 146 of file NPSMEFTd6MFV.h.

◆ Cquqd8_00_LNP

double NPSMEFTd6MFV::Cquqd8_00_LNP = 0.

protected

Definition at line 149 of file NPSMEFTd6MFV.h.

◆ Cquqd8_0d_LNP

double NPSMEFTd6MFV::Cquqd8_0d_LNP = 0.

protected

Definition at line 149 of file NPSMEFTd6MFV.h.

◆ Cquqd8_0u_LNP

double NPSMEFTd6MFV::Cquqd8_0u_LNP = 0.

protected

Definition at line 149 of file NPSMEFTd6MFV.h.

◆ Cquqd8_d0_LNP

double NPSMEFTd6MFV::Cquqd8_d0_LNP = 0.

protected

Definition at line 149 of file NPSMEFTd6MFV.h.

◆ Cquqd8_u0_LNP

double NPSMEFTd6MFV::Cquqd8_u0_LNP = 0.

protected

Definition at line 149 of file NPSMEFTd6MFV.h.

◆ Cquqd8p_00_LNP

double NPSMEFTd6MFV::Cquqd8p_00_LNP = 0.

protected

Definition at line 149 of file NPSMEFTd6MFV.h.

◆ Cquqd8p_0d_LNP

double NPSMEFTd6MFV::Cquqd8p_0d_LNP = 0.

protected

Definition at line 149 of file NPSMEFTd6MFV.h.

◆ Cquqd8p_0u_LNP

double NPSMEFTd6MFV::Cquqd8p_0u_LNP = 0.

protected

Definition at line 149 of file NPSMEFTd6MFV.h.

◆ Cquqd8p_d0_LNP

double NPSMEFTd6MFV::Cquqd8p_d0_LNP = 0.

protected

Definition at line 149 of file NPSMEFTd6MFV.h.

◆ Cquqd8p_u0_LNP

double NPSMEFTd6MFV::Cquqd8p_u0_LNP = 0.

protected

Definition at line 149 of file NPSMEFTd6MFV.h.

◆ CuB_0_LNP

double NPSMEFTd6MFV::CuB_0_LNP = 0.

protected

Definition at line 65 of file NPSMEFTd6MFV.h.

◆ CuB_d_LNP

double NPSMEFTd6MFV::CuB_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{dH})_{ij}$.

Definition at line 65 of file NPSMEFTd6MFV.h.

◆ CuB_u_LNP

double NPSMEFTd6MFV::CuB_u_LNP = 0.

protected

Definition at line 65 of file NPSMEFTd6MFV.h.

◆ Cud1_00_LNP

double NPSMEFTd6MFV::Cud1_00_LNP = 0.

protected

Definition at line 128 of file NPSMEFTd6MFV.h.

◆ Cud1_0d_LNP

double NPSMEFTd6MFV::Cud1_0d_LNP = 0.

protected

Definition at line 128 of file NPSMEFTd6MFV.h.

◆ Cud1_u0_LNP

double NPSMEFTd6MFV::Cud1_u0_LNP = 0.

protected

Definition at line 128 of file NPSMEFTd6MFV.h.

◆ Cud1_ud_LNP

double NPSMEFTd6MFV::Cud1_ud_LNP = 0.

protected

Definition at line 128 of file NPSMEFTd6MFV.h.

◆ Cud1p_ud_LNP

double NPSMEFTd6MFV::Cud1p_ud_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{ud}^{(8)})_{ijkm}$.

Definition at line 128 of file NPSMEFTd6MFV.h.

◆ Cud8_00_LNP

double NPSMEFTd6MFV::Cud8_00_LNP = 0.

protected

Definition at line 131 of file NPSMEFTd6MFV.h.

◆ Cud8_0d_LNP

double NPSMEFTd6MFV::Cud8_0d_LNP = 0.

protected

Definition at line 131 of file NPSMEFTd6MFV.h.

◆ Cud8_u0_LNP

double NPSMEFTd6MFV::Cud8_u0_LNP = 0.

protected

Definition at line 131 of file NPSMEFTd6MFV.h.

◆ Cud8_ud_LNP

double NPSMEFTd6MFV::Cud8_ud_LNP = 0.

protected

Definition at line 131 of file NPSMEFTd6MFV.h.

◆ Cud8p_ud_LNP

double NPSMEFTd6MFV::Cud8p_ud_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{qu}^{(1)})_{ijkm}$.

Definition at line 131 of file NPSMEFTd6MFV.h.

◆ CuG_0_LNP

double NPSMEFTd6MFV::CuG_0_LNP = 0.

protected

Definition at line 59 of file NPSMEFTd6MFV.h.

◆ CuG_d_LNP

double NPSMEFTd6MFV::CuG_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{uW})_{ij}$.

Definition at line 59 of file NPSMEFTd6MFV.h.

◆ CuG_u_LNP

double NPSMEFTd6MFV::CuG_u_LNP = 0.

protected

Definition at line 59 of file NPSMEFTd6MFV.h.

◆ CuH_0_LNP

double NPSMEFTd6MFV::CuH_0_LNP = 0.

protected

Definition at line 56 of file NPSMEFTd6MFV.h.

◆ CuH_d_LNP

double NPSMEFTd6MFV::CuH_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{uG})_{ij}$.

Definition at line 56 of file NPSMEFTd6MFV.h.

◆ CuH_u_LNP

double NPSMEFTd6MFV::CuH_u_LNP = 0.

protected

Definition at line 56 of file NPSMEFTd6MFV.h.

◆ Cuu_00_LNP

double NPSMEFTd6MFV::Cuu_00_LNP = 0.

protected

Definition at line 122 of file NPSMEFTd6MFV.h.

◆ Cuu_u0_LNP

double NPSMEFTd6MFV::Cuu_u0_LNP = 0.

protected

Definition at line 122 of file NPSMEFTd6MFV.h.

◆ Cuu_uu_LNP

double NPSMEFTd6MFV::Cuu_uu_LNP = 0.

protected

Definition at line 122 of file NPSMEFTd6MFV.h.

◆ Cuup_00_LNP

double NPSMEFTd6MFV::Cuup_00_LNP = 0.

protected

Definition at line 122 of file NPSMEFTd6MFV.h.

◆ Cuup_u0_LNP

double NPSMEFTd6MFV::Cuup_u0_LNP = 0.

protected

Definition at line 122 of file NPSMEFTd6MFV.h.

◆ Cuup_uu_LNP

double NPSMEFTd6MFV::Cuup_uu_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{dd})_{ijkm}$.

Definition at line 122 of file NPSMEFTd6MFV.h.

◆ CuW_0_LNP

double NPSMEFTd6MFV::CuW_0_LNP = 0.

protected

Definition at line 62 of file NPSMEFTd6MFV.h.

◆ CuW_d_LNP

double NPSMEFTd6MFV::CuW_d_LNP = 0.

protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient $(C_{uB})_{ij}$.

Definition at line 62 of file NPSMEFTd6MFV.h.

◆ CuW_u_LNP

double NPSMEFTd6MFV::CuW_u_LNP = 0.

protected

Definition at line 62 of file NPSMEFTd6MFV.h.

◆ NNPSMEFTd6MFVVars

const int NPSMEFTd6MFV::NNPSMEFTd6MFVVars = 178+1

static

Definition at line 17 of file NPSMEFTd6MFV.h.

◆ NPSMEFTd6MFVVars

std::string NPSMEFTd6MFV::NPSMEFTd6MFVVars

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","Cll_aabb_LNP","Cll_abba_LNP","Cee_LNP","Cle_LNP",
    "CuH_0_LNP","CuH_u_LNP","CuH_d_LNP","CuG_0_LNP","CuG_u_LNP","CuG_d_LNP","CuW_0_LNP","CuW_u_LNP",
    "CuW_d_LNP","CuB_0_LNP","CuB_u_LNP","CuB_d_LNP","CdH_0_LNP","CdH_u_LNP","CdH_d_LNP","CdG_0_LNP",
    "CdG_u_LNP","CdG_d_LNP","CdW_0_LNP","CdW_u_LNP","CdW_d_LNP","CdB_0_LNP","CdB_u_LNP","CdB_d_LNP",
    "CHq1_0_LNP","CHq1_u_LNP","CHq1_d_LNP","CHq3_0_LNP","CHq3_u_LNP","CHq3_d_LNP","CHu_0_LNP","CHu_u_LNP",
    "CHd_0_LNP","CHd_d_LNP","CHud_ud_LNP","Clq1_0_LNP","Clq1_u_LNP","Clq1_d_LNP","Clq3_0_LNP","Clq3_u_LNP",
    "Clq3_d_LNP","Cqe_0_LNP","Cqe_u_LNP","Cqe_d_LNP","Clu_0_LNP","Clu_u_LNP","Ceu_0_LNP","Ceu_u_LNP",
    "Cld_0_LNP","Cld_d_LNP","Ced_0_LNP","Ced_d_LNP","Cqq1_00_LNP","Cqq1_u0_LNP","Cqq1_d0_LNP","Cqq1_uu_LNP",
    "Cqq1_dd_LNP","Cqq1_ud_LNP","Cqq1p_00_LNP","Cqq1p_u0_LNP","Cqq1p_d0_LNP","Cqq1p_uu_LNP","Cqq1p_dd_LNP","Cqq1p_ud_LNP",
    "Cqq3_00_LNP","Cqq3_u0_LNP","Cqq3_d0_LNP","Cqq3_uu_LNP","Cqq3_dd_LNP","Cqq3_ud_LNP","Cqq3p_00_LNP","Cqq3p_u0_LNP",
    "Cqq3p_d0_LNP","Cqq3p_uu_LNP","Cqq3p_dd_LNP","Cqq3p_ud_LNP","Cuu_00_LNP","Cuu_u0_LNP","Cuu_uu_LNP","Cuup_00_LNP",
    "Cuup_u0_LNP","Cuup_uu_LNP","Cdd_00_LNP","Cdd_d0_LNP","Cdd_dd_LNP","Cddp_00_LNP","Cddp_d0_LNP","Cddp_dd_LNP",
    "Cud1_00_LNP","Cud1_u0_LNP","Cud1_0d_LNP","Cud1_ud_LNP","Cud1p_ud_LNP","Cud8_00_LNP","Cud8_u0_LNP","Cud8_0d_LNP",
    "Cud8_ud_LNP","Cud8p_ud_LNP","Cqu1_00_LNP","Cqu1_u0_LNP","Cqu1_d0_LNP","Cqu1_0u_LNP","Cqu1_uu_LNP","Cqu1_du_LNP",
    "Cqu1_y_LNP","Cqu1_uy_LNP","Cqu1_dy_LNP","Cqu1_yu_LNP","Cqu1_yd_LNP","Cqu8_00_LNP","Cqu8_u0_LNP","Cqu8_d0_LNP",
    "Cqu8_0u_LNP","Cqu8_uu_LNP","Cqu8_du_LNP","Cqu8_y_LNP","Cqu8_uy_LNP","Cqu8_dy_LNP","Cqu8_yu_LNP","Cqu8_yd_LNP",
    "Cqd1_00_LNP","Cqd1_u0_LNP","Cqd1_d0_LNP","Cqd1_0d_LNP","Cqd1_ud_LNP","Cqd1_dd_LNP","Cqd1_y_LNP","Cqd1_uy_LNP",
    "Cqd1_dy_LNP","Cqd1_yu_LNP","Cqd1_yd_LNP","Cqd8_00_LNP","Cqd8_u0_LNP","Cqd8_d0_LNP","Cqd8_0d_LNP","Cqd8_ud_LNP",
    "Cqd8_dd_LNP","Cqd8_y_LNP","Cqd8_uy_LNP","Cqd8_dy_LNP","Cqd8_yu_LNP","Cqd8_yd_LNP","Cquqd1_00_LNP","Cquqd1_u0_LNP",
    "Cquqd1_d0_LNP","Cquqd1_0u_LNP","Cquqd1_0d_LNP","Cquqd1p_00_LNP","Cquqd1p_u0_LNP","Cquqd1p_d0_LNP","Cquqd1p_0u_LNP","Cquqd1p_0d_LNP",
    "Cquqd8_00_LNP","Cquqd8_u0_LNP","Cquqd8_d0_LNP","Cquqd8_0u_LNP","Cquqd8_0d_LNP","Cquqd8p_00_LNP","Cquqd8p_u0_LNP","Cquqd8p_d0_LNP",
    "Cquqd8p_0u_LNP","Cquqd8p_0d_LNP",
    "Lambda_NP"
}

Definition at line 19 of file NPSMEFTd6MFV.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

◆ NPSMEFTd6MFV()

Member Function Documentation

◆ PostUpdate()

◆ setNPSMEFTd6GeneralParameters()

◆ setParameter()

Member Data Documentation

◆ CdB_0_LNP

◆ CdB_d_LNP

◆ CdB_u_LNP

◆ Cdd_00_LNP

◆ Cdd_d0_LNP

◆ Cdd_dd_LNP

◆ Cddp_00_LNP

◆ Cddp_d0_LNP

◆ Cddp_dd_LNP

◆ CdG_0_LNP

◆ CdG_d_LNP

◆ CdG_u_LNP

◆ CdH_0_LNP

◆ CdH_d_LNP

◆ CdH_u_LNP

◆ CdW_0_LNP

◆ CdW_d_LNP

◆ CdW_u_LNP

◆ Ced_0_LNP

◆ Ced_d_LNP

◆ Cee_LNP

◆ Ceu_0_LNP

◆ Ceu_u_LNP

◆ CHd_0_LNP

◆ CHd_d_LNP

◆ CHe_LNP

◆ CHl1_LNP

◆ CHl3_LNP

◆ CHq1_0_LNP

◆ CHq1_d_LNP

◆ CHq1_u_LNP

◆ CHq3_0_LNP

◆ CHq3_d_LNP

◆ CHq3_u_LNP

◆ CHu_0_LNP

◆ CHu_u_LNP

◆ CHud_ud_LNP

◆ Cld_0_LNP

◆ Cld_d_LNP

◆ Cle_LNP

◆ Cll_aabb_LNP

◆ Cll_abba_LNP

◆ Clq1_0_LNP

◆ Clq1_d_LNP

◆ Clq1_u_LNP

◆ Clq3_0_LNP

◆ Clq3_d_LNP

◆ Clq3_u_LNP

◆ Clu_0_LNP

◆ Clu_u_LNP

◆ Cqd1_00_LNP

◆ Cqd1_0d_LNP

◆ Cqd1_d0_LNP

◆ Cqd1_dd_LNP

◆ Cqd1_dy_LNP

◆ Cqd1_u0_LNP

◆ Cqd1_ud_LNP

◆ Cqd1_uy_LNP

◆ Cqd1_y_LNP

◆ Cqd1_yd_LNP

◆ Cqd1_yu_LNP

◆ Cqd8_00_LNP

◆ Cqd8_0d_LNP

◆ Cqd8_d0_LNP

◆ Cqd8_dd_LNP

◆ Cqd8_dy_LNP

◆ Cqd8_u0_LNP