9#ifndef NPSMEFTD6GENERAL_H
10#define NPSMEFTD6GENERAL_H
17#include <gsl/gsl_integration.h>
654 virtual bool setFlag(
const std::string
name,
const bool value);
662 virtual bool setFlagStr(
const std::string
name,
const std::string value);
669 return NPSMEFTd6GM.getObj();
708 virtual const double DeltaOalphtoW(
const double dOSMdalpha,
const double mu)
const;
724 virtual const double DeltaOWtoalph(
const double dOSMdMW,
const double mu)
const;
739 virtual const double deltaH3L1(
double C1)
const;
744 virtual const double deltaH3L2(
double C1)
const;
752 virtual const double delta2sH3(
const double C1)
const;
758 virtual const double delta2sBRH3(
const double C1prod,
const double C1Hxx)
const;
772 virtual const double DeltaGF()
const;
783 virtual const double del_A_mu(
const double mu)
const;
791 virtual const double del_Z_mu(
const double mu)
const;
799 virtual const double del_ZA_mu(
const double mu)
const;
808 virtual const double del_e_mu(
const double mu)
const;
816 virtual const double del_sW2_mu(
const double mu)
const;
824 virtual const double delU_gNC(
const double mu)
const;
832 virtual const double delQ_gNC(
const double mu)
const;
840 virtual const double delU_gCC(
const double mu)
const;
849 virtual const double obliqueS()
const;
856 virtual const double obliqueT()
const;
862 virtual const double obliqueU()
const;
869 virtual const double obliqueW()
const;
876 virtual const double obliqueY()
const;
885 virtual const double deltaMz()
const;
891 virtual const double deltaMz2()
const;
897 virtual const double deltaMh()
const;
903 virtual const double deltaMh2()
const;
909 virtual const double deltamt()
const;
915 virtual const double deltamt2()
const;
921 virtual const double deltamb()
const;
927 virtual const double deltamb2()
const;
933 virtual const double deltamc()
const;
939 virtual const double deltamc2()
const;
957 virtual const double deltaGmu()
const;
969 virtual const double deltaaMZ()
const;
981 virtual const double deltaa0()
const;
987 virtual const double deltaa02()
const;
1005 virtual const double deltaMw()
const;
1011 virtual const double deltaMw2()
const;
1019 virtual const double alphaMz()
const;
1035 virtual const double Mw()
const;
1075 virtual const double GammaW()
const;
1130 virtual const double Gamma_Z()
const;
1160 virtual const double RWc()
const;
1256 const double CeeLL_e(
const double mu)
const;
1257 const double CeeLL_mu(
const double mu)
const;
1258 const double CeeLL_tau(
const double mu)
const;
1260 const double CeeLL_up(
const double mu)
const;
1262 const double CeeLL_top(
const double mu)
const;
1264 const double CeeLL_down(
const double mu)
const;
1269 const double CeeLR_e(
const double mu)
const;
1270 const double CeeLR_mu(
const double mu)
const;
1271 const double CeeLR_tau(
const double mu)
const;
1273 const double CeeLR_up(
const double mu)
const;
1275 const double CeeLR_top(
const double mu)
const;
1277 const double CeeLR_down(
const double mu)
const;
1281 const double CeeRL_e(
const double mu)
const;
1282 const double CeeRL_mu(
const double mu)
const;
1283 const double CeeRL_tau(
const double mu)
const;
1285 const double CeeRL_up(
const double mu)
const;
1287 const double CeeRL_top(
const double mu)
const;
1289 const double CeeRL_down(
const double mu)
const;
1293 const double CeeRR_e(
const double mu)
const;
1294 const double CeeRR_mu(
const double mu)
const;
1295 const double CeeRR_tau(
const double mu)
const;
1297 const double CeeRR_up(
const double mu)
const;
1299 const double CeeRR_top(
const double mu)
const;
1301 const double CeeRR_down(
const double mu)
const;
1314 const double tovers2(
const double cosmin,
const double cosmax)
const;
1315 const double uovers2(
const double cosmin,
const double cosmax)
const;
1318 virtual const double delta_Dsigma_f(
const Particle f,
const double pol_e,
const double pol_p,
const double s,
const double cos)
const;
1322 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;
1324 virtual const double delta_sigma_had(
const double pol_e,
const double pol_p,
const double s,
const double cosmin,
const double cosmax)
const;
1330 virtual const double delta_AFB_f(
const Particle f,
const double pol_e,
const double pol_p,
const double s)
const;
1339 virtual const double intDMLL2eus2(
const double s,
const double t0,
const double t1)
const;
1340 virtual const double intDMRR2eus2(
const double s,
const double t0,
const double t1)
const;
1341 virtual const double intDMLR2ets2(
const double s,
const double t0,
const double t1)
const;
1342 virtual const double intDMRL2ets2(
const double s,
const double t0,
const double t1)
const;
1343 virtual const double intDMLR2etildest2(
const double s,
const double t0,
const double t1)
const;
1344 virtual const double intDMRL2etildest2(
const double s,
const double t0,
const double t1)
const;
1347 virtual const double delta_sigma_ee(
const double pol_e,
const double pol_p,
const double s,
const double cosmin,
const double cosmax)
const;
1349 virtual const double delta_sigmaTot_ee(
const double pol_e,
const double pol_p,
const double s)
const;
1351 virtual const double delta_AFB_ee(
const double pol_e,
const double pol_p,
const double s)
const;
1357 virtual const double cQQ1_TWG(
const double mu)
const;
1359 virtual const double cQQ8_TWG(
const double mu)
const;
1361 virtual const double ctt1_TWG(
const double mu)
const;
1363 virtual const double cQt1_TWG(
const double mu)
const;
1365 virtual const double cQt8_TWG(
const double mu)
const;
1367 virtual const double cQq31_TWG(
const double mu)
const;
1369 virtual const double cQq38_TWG(
const double mu)
const;
1371 virtual const double cQq11_TWG(
const double mu)
const;
1373 virtual const double cQq18_TWG(
const double mu)
const;
1375 virtual const double cQu1_TWG(
const double mu)
const;
1377 virtual const double cQu8_TWG(
const double mu)
const;
1379 virtual const double cQd1_TWG(
const double mu)
const;
1381 virtual const double cQd8_TWG(
const double mu)
const;
1383 virtual const double ctq1_TWG(
const double mu)
const;
1385 virtual const double ctq8_TWG(
const double mu)
const;
1387 virtual const double ctu1_TWG(
const double mu)
const;
1389 virtual const double ctu8_TWG(
const double mu)
const;
1391 virtual const double ctd1_TWG(
const double mu)
const;
1393 virtual const double ctd8_TWG(
const double mu)
const;
1395 virtual const double ctH_TWG(
const double mu)
const;
1397 virtual const double cHQm_TWG(
const double mu)
const;
1399 virtual const double cHQp_TWG(
const double mu)
const;
1401 virtual const double cHQ3_TWG(
const double mu)
const;
1403 virtual const double cHt_TWG(
const double mu)
const;
1405 virtual const double cHb_TWG(
const double mu)
const;
1407 virtual const double cHtb_TWG(
const double mu)
const;
1409 virtual const double ctW_TWG(
const double mu)
const;
1411 virtual const double IctW_TWG(
const double mu)
const;
1413 virtual const double ctZ_TWG(
const double mu)
const;
1415 virtual const double IctZ_TWG(
const double mu)
const;
1417 virtual const double ctG_TWG(
const double mu)
const;
1419 virtual const double cbW_TWG(
const double mu)
const;
1421 virtual const double cQlM_TWG(
const double mu)
const;
1423 virtual const double cQlP_TWG(
const double mu)
const;
1425 virtual const double cQl3_TWG(
const double mu)
const;
1427 virtual const double cQe_TWG(
const double mu)
const;
1429 virtual const double ctl_TWG(
const double mu)
const;
1431 virtual const double cte_TWG(
const double mu)
const;
1433 virtual const double ctlS_TWG(
const double mu)
const;
1435 virtual const double ctlT_TWG(
const double mu)
const;
1454 virtual const double delta_Qwemoller(
const double q2,
const double y)
const;
1463 virtual const double delta_alrmoller(
const double q2,
const double y)
const;
1927 virtual const double muggH(
const double sqrt_s)
const;
1935 virtual const double muggHH(
const double sqrt_s)
const;
1942 virtual const double muVBF(
const double sqrt_s)
const;
1959 virtual const double mueeWBF(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
1968 virtual const double mueeHvv(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
1977 virtual const double mueeZBF(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
1986 virtual const double mueeHee(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
2009 virtual const double muWH(
const double sqrt_s)
const;
2023 virtual const double muZH(
const double sqrt_s)
const;
2040 virtual const double mueeZHGen(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
2049 virtual const double mueeZH(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
2058 virtual const double mueeZllH(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
2067 virtual const double mueeZqqH(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
2076 virtual const double mueeZHPol(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
2085 virtual const double mueeZllHPol(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
2094 virtual const double mueeZqqHPol(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
2102 virtual const double aPskPol(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
2110 virtual const double bPskPol(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
2117 virtual const double muVH(
const double sqrt_s)
const;
2138 virtual const double muttH(
const double sqrt_s)
const;
2145 virtual const double mutH(
const double sqrt_s)
const;
2163 virtual const double mutHq(
const double sqrt_s)
const;
2180 virtual const double mueettH(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
2187 virtual const double mummH(
const double sqrt_s)
const;
2202 virtual const double mummZH(
const double sqrt_s)
const;
4135 const double GammaHlljjRatio()
const;
4142 const double deltaGammaHlljjRatio1()
const;
4149 const double deltaGammaHlljjRatio2()
const;
4247 virtual const double Br_H_exo()
const;
4252 virtual const double Br_H_inv()
const;
4409 virtual const double muZHZZ(
const double sqrt_s)
const;
4417 virtual const double muWHZZ(
const double sqrt_s)
const;
4425 virtual const double muVHZZ(
const double sqrt_s)
const;
4507 virtual const double muZHWW(
const double sqrt_s)
const;
4515 virtual const double muWHWW(
const double sqrt_s)
const;
4523 virtual const double muVHWW(
const double sqrt_s)
const;
4699 virtual const double muZHbb(
const double sqrt_s)
const;
4707 virtual const double muWHbb(
const double sqrt_s)
const;
4715 virtual const double muVHbb(
const double sqrt_s)
const;
5224 virtual const double deltaeNP(
const double mu)
const;
5233 virtual const double deltag1ZNP(
const double mu)
const;
5239 virtual const double deltaKZNP(
const double mu)
const;
5245 virtual const double deltag1gaNP(
const double mu)
const;
5257 virtual const double lambdaZNP(
const double mu)
const;
5346 virtual const double dxseeWWdcosBin(
const double sqrt_s,
const double cos1,
const double cos2)
const;
5353 virtual const double xseeWW(
const double sqrt_s)
const;
5363 virtual const double mueeWW(
const double sqrt_s,
const double Pol_em,
const double Pol_ep)
const;
5383 virtual const double mupTVppWZ(
const double sqrt_s,
const double pTV1,
const double pTV2)
const;
6207 virtual const double deltayt_HB(
const double mu)
const;
6220 virtual const double deltayb_HB(
const double mu)
const;
6233 virtual const double deltaytau_HB(
const double mu)
const;
6246 virtual const double deltayc_HB(
const double mu)
const;
6260 virtual const double deltays_HB(
const double mu)
const;
6273 virtual const double deltaymu_HB(
const double mu)
const;
6286 virtual const double deltacZ_HB(
const double mu)
const;
6299 virtual const double cZBox_HB(
const double mu)
const;
6312 virtual const double cZZ_HB(
const double mu)
const;
6325 virtual const double cZga_HB(
const double mu)
const;
6338 virtual const double cgaga_HB(
const double mu)
const;
6351 virtual const double cgg_HB(
const double mu)
const;
6364 virtual const double cggEff_HB(
const double mu)
const;
6377 virtual const double lambz_HB(
const double mu)
const;
6386 virtual const double CEWHL111(
const double mu)
const;
6393 virtual const double CEWHL122(
const double mu)
const;
6400 virtual const double CEWHL133(
const double mu)
const;
6407 virtual const double CEWHL311(
const double mu)
const;
6414 virtual const double CEWHL322(
const double mu)
const;
6421 virtual const double CEWHL333(
const double mu)
const;
6428 virtual const double CEWHQ111(
const double mu)
const;
6435 virtual const double CEWHQ122(
const double mu)
const;
6442 virtual const double CEWHQ133(
const double mu)
const;
6449 virtual const double CEWHQ311(
const double mu)
const;
6456 virtual const double CEWHQ322(
const double mu)
const;
6463 virtual const double CEWHQ333(
const double mu)
const;
6471 virtual const double CEWHQd33(
const double mu)
const;
6478 virtual const double CEWHQu33(
const double mu)
const;
6486 virtual const double CEWHe11(
const double mu)
const;
6493 virtual const double CEWHe22(
const double mu)
const;
6500 virtual const double CEWHe33(
const double mu)
const;
6508 virtual const double CEWHu11(
const double mu)
const;
6515 virtual const double CEWHu22(
const double mu)
const;
6522 virtual const double CEWHu33(
const double mu)
const;
6530 virtual const double CEWHd11(
const double mu)
const;
6537 virtual const double CEWHd22(
const double mu)
const;
6544 virtual const double CEWHd33(
const double mu)
const;
6551 virtual const double CEWll(
const double mu)
const;
6561 virtual const double CEWHQ1uu(
const double mu)
const;
6568 virtual const double CEWHQ1cc(
const double mu)
const;
6575 virtual const double CEWHQ1tt(
const double mu)
const;
6582 virtual const double CEWHQ1dd(
const double mu)
const;
6589 virtual const double CEWHQ1ss(
const double mu)
const;
6596 virtual const double CEWHQ1bb(
const double mu)
const;
6604 virtual const double CEWHQ3uu(
const double mu)
const;
6611 virtual const double CEWHQ3cc(
const double mu)
const;
6618 virtual const double CEWHQ3tt(
const double mu)
const;
6625 virtual const double CEWHQ3dd(
const double mu)
const;
6632 virtual const double CEWHQ3ss(
const double mu)
const;
6639 virtual const double CEWHQ3bb(
const double mu)
const;
6648 virtual const double CEWHuuu(
const double mu)
const;
6655 virtual const double CEWHucc(
const double mu)
const;
6662 virtual const double CEWHutt(
const double mu)
const;
6670 virtual const double CEWHddd(
const double mu)
const;
6677 virtual const double CEWHdss(
const double mu)
const;
6684 virtual const double CEWHdbb(
const double mu)
const;
6693 virtual const double NevLHCppee13(
const int i_bin)
const;
6699 virtual const double NevLHCppmumu13(
const int i_bin)
const;
6705 virtual const double NevLHCpptautau13(
const int i_bin)
const;
6713 virtual const double NevLHCppenu13(
const int i_bin)
const;
6719 virtual const double NevLHCppmunu13(
const int i_bin)
const;
6725 virtual const double NevLHCpptaunu13(
const int i_bin)
const;
6734 virtual const double AuxObs_NP1()
const;
6741 virtual const double AuxObs_NP2()
const;
6748 virtual const double AuxObs_NP3()
const;
6755 virtual const double AuxObs_NP4()
const;
6762 virtual const double AuxObs_NP5()
const;
6769 virtual const double AuxObs_NP6()
const;
6776 virtual const double AuxObs_NP7()
const;
6783 virtual const double AuxObs_NP8()
const;
6790 virtual const double AuxObs_NP9()
const;
6797 virtual const double AuxObs_NP10()
const;
6804 virtual const double AuxObs_NP11()
const;
6811 virtual const double AuxObs_NP12()
const;
6817 virtual const double AuxObs_NP13()
const;
6823 virtual const double AuxObs_NP14()
const;
6829 virtual const double AuxObs_NP15()
const;
6835 virtual const double AuxObs_NP16()
const;
6841 virtual const double AuxObs_NP17()
const;
6847 virtual const double AuxObs_NP18()
const;
6853 virtual const double AuxObs_NP19()
const;
6859 virtual const double AuxObs_NP20()
const;
6866 virtual const double AuxObs_NP21()
const;
6873 virtual const double AuxObs_NP22()
const;
6879 virtual const double AuxObs_NP23()
const;
6885 virtual const double AuxObs_NP24()
const;
6891 virtual const double AuxObs_NP25()
const;
6897 virtual const double AuxObs_NP26()
const;
6903 virtual const double AuxObs_NP27()
const;
6909 virtual const double AuxObs_NP28()
const;
6915 virtual const double AuxObs_NP29()
const;
6921 virtual const double AuxObs_NP30()
const;
6925 const double chi2FCChh4Top()
const;
6927 const double chi2FCChhHtt()
const;
6928 const double chi2FCChhZtt()
const;
6929 const double chi2FCChhtt()
const;
6930 const double chi2FCChhtb()
const;
6932 const double chi2FCChhHW()
const;
6933 const double chi2FCChhWW()
const;
6935 const double chi2FCChhee()
const;
6936 const double chi2FCChhmumu()
const;
6937 const double chi2FCChhtata()
const;
6939 const double chi2FCChhenu()
const;
6940 const double chi2FCChhmunu()
const;
6941 const double chi2FCChhtanu()
const;
6943 const double chi2FCChhjj()
const;
6944 const double chi2FCChhbbcc()
const;
6948 const RGESolver& getSMEFTEvol()
const {
6952 gslpp::matrix<gslpp::complex>
getYd()
const {
6956 gslpp::matrix<gslpp::complex>
getYe()
const {
6960 gslpp::matrix<gslpp::complex>
getYu()
const {
6964 inline double getSMEFTCoeffEW(
const std::string
name)
const
6966 return SMEFTEvolEW.GetCoefficient(
name);
6969 inline double getSMEFTCoeffEW(
const std::string
name,
int i,
int j)
const
6971 return SMEFTEvolEW.GetCoefficient(
name, i, j);
6974 inline double getSMEFTCoeffEW(
const std::string
name,
int i,
int j,
int k,
int l)
const
6976 return SMEFTEvolEW.GetCoefficient(
name, i, j, k, l);
6982 inline gslpp::complex getSMEFTCoeffEWMB(
const std::string
name,
int i,
int j, gslpp::matrix<gslpp::complex>
Vi, gslpp::matrix<gslpp::complex> Vj)
const;
6984 inline gslpp::complex getSMEFTCoeffEWMB(
const std::string
name,
int i,
int j,
int k,
int l, gslpp::matrix<gslpp::complex>
Vi, gslpp::matrix<gslpp::complex> Vj, gslpp::matrix<gslpp::complex> Vk, gslpp::matrix<gslpp::complex> Vl)
const;
6986 void printNonVanishingSMEFTCoeffEW()
const;
6988 RGESolver getSMEFTEvolEW()
const
6994 double getSMEFTCoeff(
const std::string
name,
const double mu)
const;
6996 double getSMEFTCoeff(
const std::string
name,
int i,
int j,
const double mu)
const;
6998 double getSMEFTCoeff(
const std::string
name,
int i,
int j,
int k,
int l,
const double mu)
const;
7003 double xlog1(
const double C1Lambda,
const double C2,
const double C3,
const double C4,
const double C5,
const double C6muw)
const;
7005 double xlog2(
const double C1Lambda,
const double C2,
const double C3,
const double C4,
const double C5,
const double C6muw)
const;
7007 double xlog3(
const double C1Lambda,
const double C2,
const double C3,
const double C4,
const double C5,
const double C6muw)
const;
7009 double xlog4(
const double C1Lambda,
const double C2,
const double C3,
const double C4,
const double C5,
const double C6muw)
const;
7011 double xlog5(
const double C1Lambda,
const double C2,
const double C3,
const double C4,
const double C5,
const double C6muw)
const;
7017 inline gslpp::complex getSMEFTCoeffMB(
const std::string
name,
int i,
int j, gslpp::matrix<gslpp::complex>
Vi, gslpp::matrix<gslpp::complex> Vj,
const double mu)
const;
7019 inline gslpp::complex getSMEFTCoeffMB(
const std::string
name,
int i,
int j,
int k,
int l, gslpp::matrix<gslpp::complex>
Vi, gslpp::matrix<gslpp::complex> Vj, gslpp::matrix<gslpp::complex> Vk, gslpp::matrix<gslpp::complex> Vl,
const double mu)
const;
7023 const double getDelta_v()
const
7028 const double getCW_tree()
const
7033 const double getSW_tree()
const
7038 const double getEeMz()
const
7043 const double getGZdL()
const
7048 const double getGZdR()
const
7053 const double getGZlL()
const
7058 const double getGZlR()
const
7063 const double getGZuL()
const
7068 const double getGZuR()
const
7073 const double getGZvL()
const
7078 const double getG1_tree()
const
7083 const double getG2_tree()
const
7088 const double getG3_tree()
const
7093 const double getDelta_Mz2()
const
7098 const double getDelta_ale()
const
7103 const double getDelta_g1()
const
7108 const double getDelta_g2()
const
7113 const double getDelta_xBZ()
const
7118 const double getDelta_xWZ()
const
7123 const double getXBZ_tree()
const
7128 const double getXWZ_tree()
const
7133 const double getMw_tree()
const
7142 const gslpp::matrix<gslpp::complex>& getVdL()
const {
7150 const gslpp::matrix<gslpp::complex>& getVdLd()
const {
7158 const gslpp::matrix<gslpp::complex>& getVdR()
const {
7166 const gslpp::matrix<gslpp::complex>& getVdRd()
const {
7174 const gslpp::matrix<gslpp::complex>& getVeL()
const {
7182 const gslpp::matrix<gslpp::complex>& getVeLd()
const {
7190 const gslpp::matrix<gslpp::complex>& getVeR()
const {
7198 const gslpp::matrix<gslpp::complex>& getVeRd()
const {
7206 const gslpp::matrix<gslpp::complex>& getVuL()
const {
7214 const gslpp::matrix<gslpp::complex>& getVuLd()
const {
7222 const gslpp::matrix<gslpp::complex>& getVuR()
const {
7230 const gslpp::matrix<gslpp::complex>& getVuRd()
const {
7237 const double getLambdaH_tree()
const
7239 return lambdaH_tree;
7245 bool FlagQuadraticWC;
7264 void ChangeToEvolutorsBasisPureSM();
7272 void ChangeToEvolutorsBasisSMEFTtoSM();
7284 void computeQuarkMassesAndCKMFromYukawas();
7290 void setSMEFTEvolWC(RGESolver& RGevol);
7301 std::string SMEFTBasisFlag;
7308 double lambdaH_LEW = 0;
7312 double mtau_LEW = 0;
7319 double s12CKM_LEW = 0.;
7320 double s13CKM_LEW = 0.;
7321 double s23CKM_LEW = 0.;
7322 double dCKM_LEW = 0.;
7323 double Mu_LEW[3] = {0, 0, 0};
7324 double Md_LEW[3] = {0, 0, 0};
7325 double Me_LEW[3] = {0, 0, 0};
7349 double CHG_LNP = 0.;
7350 double CHW_LNP = 0.;
7351 double CHB_LNP = 0.;
7354 double CHWB_LNP = 0.;
7355 double CHD_LNP = 0.;
7356 double CHbox_LNP = 0.;
7358 double CGtilde_LNP = 0.;
7359 double CWtilde_LNP = 0.;
7360 double CHGtilde_LNP = 0.;
7361 double CHWtilde_LNP = 0.;
7362 double CHBtilde_LNP = 0.;
7363 double CHWtildeB_LNP = 0.;
7364 double CHl1_11r_LNP = 0., CHl1_12r_LNP = 0., CHl1_13r_LNP = 0., CHl1_22r_LNP = 0., CHl1_23r_LNP = 0., CHl1_33r_LNP = 0.;
7365 double CHl1_12i_LNP = 0., CHl1_13i_LNP = 0., CHl1_23i_LNP = 0.;
7366 double CHl3_11r_LNP = 0., CHl3_12r_LNP = 0., CHl3_13r_LNP = 0., CHl3_22r_LNP = 0., CHl3_23r_LNP = 0., CHl3_33r_LNP = 0.;
7367 double CHl3_12i_LNP = 0., CHl3_13i_LNP = 0., CHl3_23i_LNP = 0.;
7368 double CHe_11r_LNP = 0., CHe_12r_LNP = 0., CHe_13r_LNP = 0., CHe_22r_LNP = 0., CHe_23r_LNP = 0., CHe_33r_LNP = 0.;
7369 double CHe_12i_LNP = 0., CHe_13i_LNP = 0., CHe_23i_LNP = 0.;
7370 double CHq1_11r_LNP = 0., CHq1_12r_LNP = 0., CHq1_13r_LNP = 0., CHq1_22r_LNP = 0., CHq1_23r_LNP = 0., CHq1_33r_LNP = 0.;
7371 double CHq1_12i_LNP = 0., CHq1_13i_LNP = 0., CHq1_23i_LNP = 0.;
7372 double CHq3_11r_LNP = 0., CHq3_12r_LNP = 0., CHq3_13r_LNP = 0., CHq3_22r_LNP = 0., CHq3_23r_LNP = 0., CHq3_33r_LNP = 0.;
7373 double CHq3_12i_LNP = 0., CHq3_13i_LNP = 0., CHq3_23i_LNP = 0.;
7374 double CHu_11r_LNP = 0., CHu_12r_LNP = 0., CHu_13r_LNP = 0., CHu_22r_LNP = 0., CHu_23r_LNP = 0., CHu_33r_LNP = 0.;
7375 double CHu_12i_LNP = 0., CHu_13i_LNP = 0., CHu_23i_LNP = 0.;
7376 double CHd_11r_LNP = 0., CHd_12r_LNP = 0., CHd_13r_LNP = 0., CHd_22r_LNP = 0., CHd_23r_LNP = 0., CHd_33r_LNP = 0.;
7377 double CHd_12i_LNP = 0., CHd_13i_LNP = 0., CHd_23i_LNP = 0.;
7378 double CHud_11r_LNP = 0., CHud_12r_LNP = 0., CHud_13r_LNP = 0., CHud_21r_LNP = 0., CHud_22r_LNP = 0., CHud_23r_LNP = 0., CHud_31r_LNP = 0., CHud_32r_LNP = 0., CHud_33r_LNP = 0.;
7379 double CHud_11i_LNP = 0., CHud_12i_LNP = 0., CHud_13i_LNP = 0., CHud_21i_LNP = 0., CHud_22i_LNP = 0., CHud_23i_LNP = 0., CHud_31i_LNP = 0., CHud_32i_LNP = 0., CHud_33i_LNP = 0.;
7380 double CeH_11r_LNP = 0., CeH_12r_LNP = 0., CeH_13r_LNP = 0., CeH_21r_LNP = 0., CeH_22r_LNP = 0., CeH_23r_LNP = 0., CeH_31r_LNP = 0., CeH_32r_LNP = 0., CeH_33r_LNP = 0.;
7381 double CeH_11i_LNP = 0., CeH_12i_LNP = 0., CeH_13i_LNP = 0., CeH_21i_LNP = 0., CeH_22i_LNP = 0., CeH_23i_LNP = 0., CeH_31i_LNP = 0., CeH_32i_LNP = 0., CeH_33i_LNP = 0.;
7382 double CuH_11r_LNP = 0., CuH_12r_LNP = 0., CuH_13r_LNP = 0., CuH_21r_LNP = 0., CuH_22r_LNP = 0., CuH_23r_LNP = 0., CuH_31r_LNP = 0., CuH_32r_LNP = 0., CuH_33r_LNP = 0.;
7383 double CuH_11i_LNP = 0., CuH_12i_LNP = 0., CuH_13i_LNP = 0., CuH_21i_LNP = 0., CuH_22i_LNP = 0., CuH_23i_LNP = 0., CuH_31i_LNP = 0., CuH_32i_LNP = 0., CuH_33i_LNP = 0.;
7384 double CdH_11r_LNP = 0., CdH_12r_LNP = 0., CdH_13r_LNP = 0., CdH_21r_LNP = 0., CdH_22r_LNP = 0., CdH_23r_LNP = 0., CdH_31r_LNP = 0., CdH_32r_LNP = 0., CdH_33r_LNP = 0.;
7385 double CdH_11i_LNP = 0., CdH_12i_LNP = 0., CdH_13i_LNP = 0., CdH_21i_LNP = 0., CdH_22i_LNP = 0., CdH_23i_LNP = 0., CdH_31i_LNP = 0., CdH_32i_LNP = 0., CdH_33i_LNP = 0.;
7386 double CuG_11r_LNP = 0., CuG_12r_LNP = 0., CuG_13r_LNP = 0., CuG_21r_LNP = 0., CuG_22r_LNP = 0., CuG_23r_LNP = 0., CuG_31r_LNP = 0., CuG_32r_LNP = 0., CuG_33r_LNP = 0.;
7387 double CuG_11i_LNP = 0., CuG_12i_LNP = 0., CuG_13i_LNP = 0., CuG_21i_LNP = 0., CuG_22i_LNP = 0., CuG_23i_LNP = 0., CuG_31i_LNP = 0., CuG_32i_LNP = 0., CuG_33i_LNP = 0.;
7388 double CuW_11r_LNP = 0., CuW_12r_LNP = 0., CuW_13r_LNP = 0., CuW_21r_LNP = 0., CuW_22r_LNP = 0., CuW_23r_LNP = 0., CuW_31r_LNP = 0., CuW_32r_LNP = 0., CuW_33r_LNP = 0.;
7389 double CuW_11i_LNP = 0., CuW_12i_LNP = 0., CuW_13i_LNP = 0., CuW_21i_LNP = 0., CuW_22i_LNP = 0., CuW_23i_LNP = 0., CuW_31i_LNP = 0., CuW_32i_LNP = 0., CuW_33i_LNP = 0.;
7390 double CuB_11r_LNP = 0., CuB_12r_LNP = 0., CuB_13r_LNP = 0., CuB_21r_LNP = 0., CuB_22r_LNP = 0., CuB_23r_LNP = 0., CuB_31r_LNP = 0., CuB_32r_LNP = 0., CuB_33r_LNP = 0.;
7391 double CuB_11i_LNP = 0., CuB_12i_LNP = 0., CuB_13i_LNP = 0., CuB_21i_LNP = 0., CuB_22i_LNP = 0., CuB_23i_LNP = 0., CuB_31i_LNP = 0., CuB_32i_LNP = 0., CuB_33i_LNP = 0.;
7392 double CdG_11r_LNP = 0., CdG_12r_LNP = 0., CdG_13r_LNP = 0., CdG_21r_LNP = 0., CdG_22r_LNP = 0., CdG_23r_LNP = 0., CdG_31r_LNP = 0., CdG_32r_LNP = 0., CdG_33r_LNP = 0.;
7393 double CdG_11i_LNP = 0., CdG_12i_LNP = 0., CdG_13i_LNP = 0., CdG_21i_LNP = 0., CdG_22i_LNP = 0., CdG_23i_LNP = 0., CdG_31i_LNP = 0., CdG_32i_LNP = 0., CdG_33i_LNP = 0.;
7394 double CdW_11r_LNP = 0., CdW_12r_LNP = 0., CdW_13r_LNP = 0., CdW_21r_LNP = 0., CdW_22r_LNP = 0., CdW_23r_LNP = 0., CdW_31r_LNP = 0., CdW_32r_LNP = 0., CdW_33r_LNP = 0.;
7395 double CdW_11i_LNP = 0., CdW_12i_LNP = 0., CdW_13i_LNP = 0., CdW_21i_LNP = 0., CdW_22i_LNP = 0., CdW_23i_LNP = 0., CdW_31i_LNP = 0., CdW_32i_LNP = 0., CdW_33i_LNP = 0.;
7396 double CdB_11r_LNP = 0., CdB_12r_LNP = 0., CdB_13r_LNP = 0., CdB_21r_LNP = 0., CdB_22r_LNP = 0., CdB_23r_LNP = 0., CdB_31r_LNP = 0., CdB_32r_LNP = 0., CdB_33r_LNP = 0.;
7397 double CdB_11i_LNP = 0., CdB_12i_LNP = 0., CdB_13i_LNP = 0., CdB_21i_LNP = 0., CdB_22i_LNP = 0., CdB_23i_LNP = 0., CdB_31i_LNP = 0., CdB_32i_LNP = 0., CdB_33i_LNP = 0.;
7398 double CeW_11r_LNP = 0., CeW_12r_LNP = 0., CeW_13r_LNP = 0., CeW_21r_LNP = 0., CeW_22r_LNP = 0., CeW_23r_LNP = 0., CeW_31r_LNP = 0., CeW_32r_LNP = 0., CeW_33r_LNP = 0.;
7399 double CeW_11i_LNP = 0., CeW_12i_LNP = 0., CeW_13i_LNP = 0., CeW_21i_LNP = 0., CeW_22i_LNP = 0., CeW_23i_LNP = 0., CeW_31i_LNP = 0., CeW_32i_LNP = 0., CeW_33i_LNP = 0.;
7400 double CeB_11r_LNP = 0., CeB_12r_LNP = 0., CeB_13r_LNP = 0., CeB_21r_LNP = 0., CeB_22r_LNP = 0., CeB_23r_LNP = 0., CeB_31r_LNP = 0., CeB_32r_LNP = 0., CeB_33r_LNP = 0.;
7401 double CeB_11i_LNP = 0., CeB_12i_LNP = 0., CeB_13i_LNP = 0., CeB_21i_LNP = 0., CeB_22i_LNP = 0., CeB_23i_LNP = 0., CeB_31i_LNP = 0., CeB_32i_LNP = 0., CeB_33i_LNP = 0.;
7402 double Cll_1111r_LNP = 0., Cll_1112r_LNP = 0., Cll_1113r_LNP = 0., Cll_1122r_LNP = 0., Cll_1123r_LNP = 0., Cll_1133r_LNP = 0., Cll_1212r_LNP = 0., Cll_1213r_LNP = 0., Cll_1221r_LNP = 0.,
7403 Cll_1222r_LNP = 0., Cll_1223r_LNP = 0., Cll_1231r_LNP = 0., Cll_1232r_LNP = 0., Cll_1233r_LNP = 0., Cll_1313r_LNP = 0., Cll_1322r_LNP = 0., Cll_1323r_LNP = 0., Cll_1331r_LNP = 0.,
7404 Cll_1332r_LNP = 0., Cll_1333r_LNP = 0., Cll_2222r_LNP = 0., Cll_2223r_LNP = 0., Cll_2233r_LNP = 0., Cll_2323r_LNP = 0., Cll_2332r_LNP = 0., Cll_2333r_LNP = 0., Cll_3333r_LNP = 0.;
7405 double Cll_1112i_LNP = 0., Cll_1113i_LNP = 0., Cll_1123i_LNP = 0., Cll_1212i_LNP = 0., Cll_1213i_LNP = 0., Cll_1222i_LNP = 0., Cll_1223i_LNP = 0., Cll_1231i_LNP = 0., Cll_1232i_LNP = 0.,
7406 Cll_1233i_LNP = 0., Cll_1313i_LNP = 0., Cll_1322i_LNP = 0., Cll_1323i_LNP = 0., Cll_1332i_LNP = 0., Cll_1333i_LNP = 0., Cll_2223i_LNP = 0., Cll_2323i_LNP = 0., Cll_2333i_LNP = 0.;
7407 double Clq1_1111r_LNP = 0., Clq1_1112r_LNP = 0., Clq1_1113r_LNP = 0., Clq1_1122r_LNP = 0., Clq1_1123r_LNP = 0., Clq1_1133r_LNP = 0., Clq1_1211r_LNP = 0., Clq1_1212r_LNP = 0., Clq1_1213r_LNP = 0.,
7408 Clq1_1221r_LNP = 0., Clq1_1222r_LNP = 0., Clq1_1223r_LNP = 0., Clq1_1231r_LNP = 0., Clq1_1232r_LNP = 0., Clq1_1233r_LNP = 0., Clq1_1311r_LNP = 0., Clq1_1312r_LNP = 0., Clq1_1313r_LNP = 0.,
7409 Clq1_1321r_LNP = 0., Clq1_1322r_LNP = 0., Clq1_1323r_LNP = 0., Clq1_1331r_LNP = 0., Clq1_1332r_LNP = 0., Clq1_1333r_LNP = 0., Clq1_2211r_LNP = 0., Clq1_2212r_LNP = 0., Clq1_2213r_LNP = 0.,
7410 Clq1_2222r_LNP = 0., Clq1_2223r_LNP = 0., Clq1_2233r_LNP = 0., Clq1_2311r_LNP = 0., Clq1_2312r_LNP = 0., Clq1_2313r_LNP = 0., Clq1_2321r_LNP = 0., Clq1_2322r_LNP = 0., Clq1_2323r_LNP = 0.,
7411 Clq1_2331r_LNP = 0., Clq1_2332r_LNP = 0., Clq1_2333r_LNP = 0., Clq1_3311r_LNP = 0., Clq1_3312r_LNP = 0., Clq1_3313r_LNP = 0., Clq1_3322r_LNP = 0., Clq1_3323r_LNP = 0., Clq1_3333r_LNP = 0.;
7412 double Clq1_1112i_LNP = 0., Clq1_1113i_LNP = 0., Clq1_1123i_LNP = 0., Clq1_1211i_LNP = 0., Clq1_1212i_LNP = 0., Clq1_1213i_LNP = 0., Clq1_1221i_LNP = 0., Clq1_1222i_LNP = 0., Clq1_1223i_LNP = 0.,
7413 Clq1_1231i_LNP = 0., Clq1_1232i_LNP = 0., Clq1_1233i_LNP = 0., Clq1_1311i_LNP = 0., Clq1_1312i_LNP = 0., Clq1_1313i_LNP = 0., Clq1_1321i_LNP = 0., Clq1_1322i_LNP = 0., Clq1_1323i_LNP = 0.,
7414 Clq1_1331i_LNP = 0., Clq1_1332i_LNP = 0., Clq1_1333i_LNP = 0., Clq1_2212i_LNP = 0., Clq1_2213i_LNP = 0., Clq1_2223i_LNP = 0., Clq1_2311i_LNP = 0., Clq1_2312i_LNP = 0., Clq1_2313i_LNP = 0., Clq1_2321i_LNP = 0.,
7415 Clq1_2322i_LNP = 0., Clq1_2323i_LNP = 0., Clq1_2331i_LNP = 0., Clq1_2332i_LNP = 0., Clq1_2333i_LNP = 0., Clq1_3312i_LNP = 0., Clq1_3313i_LNP = 0., Clq1_3323i_LNP = 0.;
7416 double Clq3_1111r_LNP = 0., Clq3_1112r_LNP = 0., Clq3_1113r_LNP = 0., Clq3_1122r_LNP = 0., Clq3_1123r_LNP = 0., Clq3_1133r_LNP = 0., Clq3_1211r_LNP = 0., Clq3_1212r_LNP = 0., Clq3_1213r_LNP = 0.,
7417 Clq3_1221r_LNP = 0., Clq3_1222r_LNP = 0., Clq3_1223r_LNP = 0., Clq3_1231r_LNP = 0., Clq3_1232r_LNP = 0., Clq3_1233r_LNP = 0., Clq3_1311r_LNP = 0., Clq3_1312r_LNP = 0., Clq3_1313r_LNP = 0.,
7418 Clq3_1321r_LNP = 0., Clq3_1322r_LNP = 0., Clq3_1323r_LNP = 0., Clq3_1331r_LNP = 0., Clq3_1332r_LNP = 0., Clq3_1333r_LNP = 0., Clq3_2211r_LNP = 0., Clq3_2212r_LNP = 0., Clq3_2213r_LNP = 0.,
7419 Clq3_2222r_LNP = 0., Clq3_2223r_LNP = 0., Clq3_2233r_LNP = 0., Clq3_2311r_LNP = 0., Clq3_2312r_LNP = 0., Clq3_2313r_LNP = 0., Clq3_2321r_LNP = 0., Clq3_2322r_LNP = 0., Clq3_2323r_LNP = 0.,
7420 Clq3_2331r_LNP = 0., Clq3_2332r_LNP = 0., Clq3_2333r_LNP = 0., Clq3_3311r_LNP = 0., Clq3_3312r_LNP = 0., Clq3_3313r_LNP = 0., Clq3_3322r_LNP = 0., Clq3_3323r_LNP = 0., Clq3_3333r_LNP = 0.;
7421 double Clq3_1112i_LNP = 0., Clq3_1113i_LNP = 0., Clq3_1123i_LNP = 0., Clq3_1211i_LNP = 0., Clq3_1212i_LNP = 0., Clq3_1213i_LNP = 0., Clq3_1221i_LNP = 0., Clq3_1222i_LNP = 0., Clq3_1223i_LNP = 0.,
7422 Clq3_1231i_LNP = 0., Clq3_1232i_LNP = 0., Clq3_1233i_LNP = 0., Clq3_1311i_LNP = 0., Clq3_1312i_LNP = 0., Clq3_1313i_LNP = 0., Clq3_1321i_LNP = 0., Clq3_1322i_LNP = 0., Clq3_1323i_LNP = 0.,
7423 Clq3_1331i_LNP = 0., Clq3_1332i_LNP = 0., Clq3_1333i_LNP = 0., Clq3_2212i_LNP = 0., Clq3_2213i_LNP = 0., Clq3_2223i_LNP = 0., Clq3_2311i_LNP = 0., Clq3_2312i_LNP = 0., Clq3_2313i_LNP = 0., Clq3_2321i_LNP = 0.,
7424 Clq3_2322i_LNP = 0., Clq3_2323i_LNP = 0., Clq3_2331i_LNP = 0., Clq3_2332i_LNP = 0., Clq3_2333i_LNP = 0., Clq3_3312i_LNP = 0., Clq3_3313i_LNP = 0., Clq3_3323i_LNP = 0.;
7425 double Cee_1111r_LNP = 0., Cee_1112r_LNP = 0., Cee_1113r_LNP = 0., Cee_1122r_LNP = 0., Cee_1123r_LNP = 0., Cee_1133r_LNP = 0., Cee_1212r_LNP = 0., Cee_1213r_LNP = 0., Cee_1222r_LNP = 0.,
7426 Cee_1223r_LNP = 0., Cee_1232r_LNP = 0., Cee_1233r_LNP = 0., Cee_1313r_LNP = 0., Cee_1323r_LNP = 0., Cee_1333r_LNP = 0., Cee_2222r_LNP = 0., Cee_2223r_LNP = 0., Cee_2233r_LNP = 0.,
7427 Cee_2323r_LNP = 0., Cee_2333r_LNP = 0., Cee_3333r_LNP = 0.;
7428 double Cee_1112i_LNP = 0., Cee_1113i_LNP = 0., Cee_1123i_LNP = 0., Cee_1212i_LNP = 0., Cee_1213i_LNP = 0., Cee_1222i_LNP = 0., Cee_1223i_LNP = 0., Cee_1232i_LNP = 0., Cee_1233i_LNP = 0.,
7429 Cee_1313i_LNP = 0., Cee_1323i_LNP = 0., Cee_1333i_LNP = 0., Cee_2223i_LNP = 0., Cee_2323i_LNP = 0., Cee_2333i_LNP = 0.;
7430 double Ceu_1111r_LNP = 0., Ceu_1112r_LNP = 0., Ceu_1113r_LNP = 0., Ceu_1122r_LNP = 0., Ceu_1123r_LNP = 0., Ceu_1133r_LNP = 0., Ceu_1211r_LNP = 0., Ceu_1212r_LNP = 0., Ceu_1213r_LNP = 0.,
7431 Ceu_1221r_LNP = 0., Ceu_1222r_LNP = 0., Ceu_1223r_LNP = 0., Ceu_1231r_LNP = 0., Ceu_1232r_LNP = 0., Ceu_1233r_LNP = 0., Ceu_1311r_LNP = 0., Ceu_1312r_LNP = 0., Ceu_1313r_LNP = 0.,
7432 Ceu_1321r_LNP = 0., Ceu_1322r_LNP = 0., Ceu_1323r_LNP = 0., Ceu_1331r_LNP = 0., Ceu_1332r_LNP = 0., Ceu_1333r_LNP = 0., Ceu_2211r_LNP = 0., Ceu_2212r_LNP = 0., Ceu_2213r_LNP = 0.,
7433 Ceu_2222r_LNP = 0., Ceu_2223r_LNP = 0., Ceu_2233r_LNP = 0., Ceu_2311r_LNP = 0., Ceu_2312r_LNP = 0., Ceu_2313r_LNP = 0., Ceu_2321r_LNP = 0., Ceu_2322r_LNP = 0., Ceu_2323r_LNP = 0.,
7434 Ceu_2331r_LNP = 0., Ceu_2332r_LNP = 0., Ceu_2333r_LNP = 0., Ceu_3311r_LNP = 0., Ceu_3312r_LNP = 0., Ceu_3313r_LNP = 0., Ceu_3322r_LNP = 0., Ceu_3323r_LNP = 0., Ceu_3333r_LNP = 0.;
7435 double Ceu_1112i_LNP = 0., Ceu_1113i_LNP = 0., Ceu_1123i_LNP = 0., Ceu_1211i_LNP = 0., Ceu_1212i_LNP = 0., Ceu_1213i_LNP = 0., Ceu_1221i_LNP = 0., Ceu_1222i_LNP = 0., Ceu_1223i_LNP = 0.,
7436 Ceu_1231i_LNP = 0., Ceu_1232i_LNP = 0., Ceu_1233i_LNP = 0., Ceu_1311i_LNP = 0., Ceu_1312i_LNP = 0., Ceu_1313i_LNP = 0., Ceu_1321i_LNP = 0., Ceu_1322i_LNP = 0., Ceu_1323i_LNP = 0.,
7437 Ceu_1331i_LNP = 0., Ceu_1332i_LNP = 0., Ceu_1333i_LNP = 0., Ceu_2212i_LNP = 0., Ceu_2213i_LNP = 0., Ceu_2223i_LNP = 0., Ceu_2312i_LNP = 0., Ceu_2313i_LNP = 0., Ceu_2321i_LNP = 0.,
7438 Ceu_2322i_LNP = 0., Ceu_2323i_LNP = 0., Ceu_2331i_LNP = 0., Ceu_2332i_LNP = 0., Ceu_2333i_LNP = 0., Ceu_2311i_LNP = 0., Ceu_3312i_LNP = 0., Ceu_3313i_LNP = 0., Ceu_3323i_LNP = 0.;
7439 double Ced_1111r_LNP = 0., Ced_1112r_LNP = 0., Ced_1113r_LNP = 0., Ced_1122r_LNP = 0., Ced_1123r_LNP = 0., Ced_1133r_LNP = 0., Ced_1211r_LNP = 0., Ced_1212r_LNP = 0., Ced_1213r_LNP = 0.,
7440 Ced_1221r_LNP = 0., Ced_1222r_LNP = 0., Ced_1223r_LNP = 0., Ced_1231r_LNP = 0., Ced_1232r_LNP = 0., Ced_1233r_LNP = 0., Ced_1311r_LNP = 0., Ced_1312r_LNP = 0., Ced_1313r_LNP = 0.,
7441 Ced_1321r_LNP = 0., Ced_1322r_LNP = 0., Ced_1323r_LNP = 0., Ced_1331r_LNP = 0., Ced_1332r_LNP = 0., Ced_1333r_LNP = 0., Ced_2211r_LNP = 0., Ced_2212r_LNP = 0., Ced_2213r_LNP = 0.,
7442 Ced_2222r_LNP = 0., Ced_2223r_LNP = 0., Ced_2233r_LNP = 0., Ced_2311r_LNP = 0., Ced_2312r_LNP = 0., Ced_2313r_LNP = 0., Ced_2321r_LNP = 0., Ced_2322r_LNP = 0., Ced_2323r_LNP = 0.,
7443 Ced_2331r_LNP = 0., Ced_2332r_LNP = 0., Ced_2333r_LNP = 0., Ced_3311r_LNP = 0., Ced_3312r_LNP = 0., Ced_3313r_LNP = 0., Ced_3322r_LNP = 0., Ced_3323r_LNP = 0., Ced_3333r_LNP = 0.;
7444 double Ced_1112i_LNP = 0., Ced_1113i_LNP = 0., Ced_1123i_LNP = 0., Ced_1211i_LNP = 0., Ced_1212i_LNP = 0., Ced_1213i_LNP = 0., Ced_1221i_LNP = 0., Ced_1222i_LNP = 0., Ced_1223i_LNP = 0.,
7445 Ced_1231i_LNP = 0., Ced_1232i_LNP = 0., Ced_1233i_LNP = 0., Ced_1311i_LNP = 0., Ced_1312i_LNP = 0., Ced_1313i_LNP = 0., Ced_1321i_LNP = 0., Ced_1322i_LNP = 0., Ced_1323i_LNP = 0.,
7446 Ced_1331i_LNP = 0., Ced_1332i_LNP = 0., Ced_1333i_LNP = 0., Ced_2212i_LNP = 0., Ced_2213i_LNP = 0., Ced_2223i_LNP = 0., Ced_2312i_LNP = 0., Ced_2313i_LNP = 0., Ced_2321i_LNP = 0.,
7447 Ced_2322i_LNP = 0., Ced_2323i_LNP = 0., Ced_2331i_LNP = 0., Ced_2332i_LNP = 0., Ced_2333i_LNP = 0., Ced_2311i_LNP = 0., Ced_3312i_LNP = 0., Ced_3313i_LNP = 0., Ced_3323i_LNP = 0.;
7448 double Cle_1111r_LNP = 0., Cle_1112r_LNP = 0., Cle_1113r_LNP = 0., Cle_1122r_LNP = 0., Cle_1123r_LNP = 0., Cle_1133r_LNP = 0., Cle_1211r_LNP = 0., Cle_1212r_LNP = 0., Cle_1213r_LNP = 0.,
7449 Cle_1221r_LNP = 0., Cle_1222r_LNP = 0., Cle_1223r_LNP = 0., Cle_1231r_LNP = 0., Cle_1232r_LNP = 0., Cle_1233r_LNP = 0., Cle_1311r_LNP = 0., Cle_1312r_LNP = 0., Cle_1313r_LNP = 0.,
7450 Cle_1321r_LNP = 0., Cle_1322r_LNP = 0., Cle_1323r_LNP = 0., Cle_1331r_LNP = 0., Cle_1332r_LNP = 0., Cle_1333r_LNP = 0., Cle_2211r_LNP = 0., Cle_2212r_LNP = 0., Cle_2213r_LNP = 0.,
7451 Cle_2222r_LNP = 0., Cle_2223r_LNP = 0., Cle_2233r_LNP = 0., Cle_2311r_LNP = 0., Cle_2312r_LNP = 0., Cle_2313r_LNP = 0., Cle_2321r_LNP = 0., Cle_2322r_LNP = 0., Cle_2323r_LNP = 0.,
7452 Cle_2331r_LNP = 0., Cle_2332r_LNP = 0., Cle_2333r_LNP = 0., Cle_3311r_LNP = 0., Cle_3312r_LNP = 0., Cle_3313r_LNP = 0., Cle_3322r_LNP = 0., Cle_3323r_LNP = 0., Cle_3333r_LNP = 0.;
7453 double Cle_1112i_LNP = 0., Cle_1113i_LNP = 0., Cle_1123i_LNP = 0., Cle_1211i_LNP = 0., Cle_1212i_LNP = 0., Cle_1213i_LNP = 0., Cle_1221i_LNP = 0., Cle_1222i_LNP = 0., Cle_1223i_LNP = 0.,
7454 Cle_1231i_LNP = 0., Cle_1232i_LNP = 0., Cle_1233i_LNP = 0., Cle_1311i_LNP = 0., Cle_1312i_LNP = 0., Cle_1313i_LNP = 0., Cle_1321i_LNP = 0., Cle_1322i_LNP = 0., Cle_1323i_LNP = 0.,
7455 Cle_1331i_LNP = 0., Cle_1332i_LNP = 0., Cle_1333i_LNP = 0., Cle_2212i_LNP = 0., Cle_2213i_LNP = 0., Cle_2223i_LNP = 0., Cle_2312i_LNP = 0., Cle_2313i_LNP = 0., Cle_2321i_LNP = 0.,
7456 Cle_2322i_LNP = 0., Cle_2323i_LNP = 0., Cle_2331i_LNP = 0., Cle_2332i_LNP = 0., Cle_2333i_LNP = 0., Cle_2311i_LNP = 0., Cle_3312i_LNP = 0., Cle_3313i_LNP = 0., Cle_3323i_LNP = 0.;
7457 double Clu_1111r_LNP = 0., Clu_1112r_LNP = 0., Clu_1113r_LNP = 0., Clu_1122r_LNP = 0., Clu_1123r_LNP = 0., Clu_1133r_LNP = 0., Clu_1211r_LNP = 0., Clu_1212r_LNP = 0., Clu_1213r_LNP = 0.,
7458 Clu_1221r_LNP = 0., Clu_1222r_LNP = 0., Clu_1223r_LNP = 0., Clu_1231r_LNP = 0., Clu_1232r_LNP = 0., Clu_1233r_LNP = 0., Clu_1311r_LNP = 0., Clu_1312r_LNP = 0., Clu_1313r_LNP = 0.,
7459 Clu_1321r_LNP = 0., Clu_1322r_LNP = 0., Clu_1323r_LNP = 0., Clu_1331r_LNP = 0., Clu_1332r_LNP = 0., Clu_1333r_LNP = 0., Clu_2211r_LNP = 0., Clu_2212r_LNP = 0., Clu_2213r_LNP = 0.,
7460 Clu_2222r_LNP = 0., Clu_2223r_LNP = 0., Clu_2233r_LNP = 0., Clu_2311r_LNP = 0., Clu_2312r_LNP = 0., Clu_2313r_LNP = 0., Clu_2321r_LNP = 0., Clu_2322r_LNP = 0., Clu_2323r_LNP = 0.,
7461 Clu_2331r_LNP = 0., Clu_2332r_LNP = 0., Clu_2333r_LNP = 0., Clu_3311r_LNP = 0., Clu_3312r_LNP = 0., Clu_3313r_LNP = 0., Clu_3322r_LNP = 0., Clu_3323r_LNP = 0., Clu_3333r_LNP = 0.;
7462 double Clu_1112i_LNP = 0., Clu_1113i_LNP = 0., Clu_1123i_LNP = 0., Clu_1211i_LNP = 0., Clu_1212i_LNP = 0., Clu_1213i_LNP = 0., Clu_1221i_LNP = 0., Clu_1222i_LNP = 0., Clu_1223i_LNP = 0.,
7463 Clu_1231i_LNP = 0., Clu_1232i_LNP = 0., Clu_1233i_LNP = 0., Clu_1311i_LNP = 0., Clu_1312i_LNP = 0., Clu_1313i_LNP = 0., Clu_1321i_LNP = 0., Clu_1322i_LNP = 0., Clu_1323i_LNP = 0.,
7464 Clu_1331i_LNP = 0., Clu_1332i_LNP = 0., Clu_1333i_LNP = 0., Clu_2212i_LNP = 0., Clu_2213i_LNP = 0., Clu_2223i_LNP = 0., Clu_2312i_LNP = 0., Clu_2313i_LNP = 0., Clu_2321i_LNP = 0.,
7465 Clu_2322i_LNP = 0., Clu_2323i_LNP = 0., Clu_2331i_LNP = 0., Clu_2332i_LNP = 0., Clu_2333i_LNP = 0., Clu_2311i_LNP = 0., Clu_3312i_LNP = 0., Clu_3313i_LNP = 0., Clu_3323i_LNP = 0.;
7466 double Cld_1111r_LNP = 0., Cld_1112r_LNP = 0., Cld_1113r_LNP = 0., Cld_1122r_LNP = 0., Cld_1123r_LNP = 0., Cld_1133r_LNP = 0., Cld_1211r_LNP = 0., Cld_1212r_LNP = 0., Cld_1213r_LNP = 0.,
7467 Cld_1221r_LNP = 0., Cld_1222r_LNP = 0., Cld_1223r_LNP = 0., Cld_1231r_LNP = 0., Cld_1232r_LNP = 0., Cld_1233r_LNP = 0., Cld_1311r_LNP = 0., Cld_1312r_LNP = 0., Cld_1313r_LNP = 0.,
7468 Cld_1321r_LNP = 0., Cld_1322r_LNP = 0., Cld_1323r_LNP = 0., Cld_1331r_LNP = 0., Cld_1332r_LNP = 0., Cld_1333r_LNP = 0., Cld_2211r_LNP = 0., Cld_2212r_LNP = 0., Cld_2213r_LNP = 0.,
7469 Cld_2222r_LNP = 0., Cld_2223r_LNP = 0., Cld_2233r_LNP = 0., Cld_2311r_LNP = 0., Cld_2312r_LNP = 0., Cld_2313r_LNP = 0., Cld_2321r_LNP = 0., Cld_2322r_LNP = 0., Cld_2323r_LNP = 0.,
7470 Cld_2331r_LNP = 0., Cld_2332r_LNP = 0., Cld_2333r_LNP = 0., Cld_3311r_LNP = 0., Cld_3312r_LNP = 0., Cld_3313r_LNP = 0., Cld_3322r_LNP = 0., Cld_3323r_LNP = 0., Cld_3333r_LNP = 0.;
7471 double Cld_1112i_LNP = 0., Cld_1113i_LNP = 0., Cld_1123i_LNP = 0., Cld_1211i_LNP = 0., Cld_1212i_LNP = 0., Cld_1213i_LNP = 0., Cld_1221i_LNP = 0., Cld_1222i_LNP = 0., Cld_1223i_LNP = 0.,
7472 Cld_1231i_LNP = 0., Cld_1232i_LNP = 0., Cld_1233i_LNP = 0., Cld_1311i_LNP = 0., Cld_1312i_LNP = 0., Cld_1313i_LNP = 0., Cld_1321i_LNP = 0., Cld_1322i_LNP = 0., Cld_1323i_LNP = 0.,
7473 Cld_1331i_LNP = 0., Cld_1332i_LNP = 0., Cld_1333i_LNP = 0., Cld_2212i_LNP = 0., Cld_2213i_LNP = 0., Cld_2223i_LNP = 0., Cld_2312i_LNP = 0., Cld_2313i_LNP = 0., Cld_2321i_LNP = 0.,
7474 Cld_2322i_LNP = 0., Cld_2323i_LNP = 0., Cld_2331i_LNP = 0., Cld_2332i_LNP = 0., Cld_2333i_LNP = 0., Cld_2311i_LNP = 0., Cld_3312i_LNP = 0., Cld_3313i_LNP = 0., Cld_3323i_LNP = 0.;
7475 double Cqe_1111r_LNP = 0., Cqe_1112r_LNP = 0., Cqe_1113r_LNP = 0., Cqe_1122r_LNP = 0., Cqe_1123r_LNP = 0., Cqe_1133r_LNP = 0., Cqe_1211r_LNP = 0., Cqe_1212r_LNP = 0., Cqe_1213r_LNP = 0.,
7476 Cqe_1221r_LNP = 0., Cqe_1222r_LNP = 0., Cqe_1223r_LNP = 0., Cqe_1231r_LNP = 0., Cqe_1232r_LNP = 0., Cqe_1233r_LNP = 0., Cqe_1311r_LNP = 0., Cqe_1312r_LNP = 0., Cqe_1313r_LNP = 0.,
7477 Cqe_1321r_LNP = 0., Cqe_1322r_LNP = 0., Cqe_1323r_LNP = 0., Cqe_1331r_LNP = 0., Cqe_1332r_LNP = 0., Cqe_1333r_LNP = 0., Cqe_2211r_LNP = 0., Cqe_2212r_LNP = 0., Cqe_2213r_LNP = 0.,
7478 Cqe_2222r_LNP = 0., Cqe_2223r_LNP = 0., Cqe_2233r_LNP = 0., Cqe_2311r_LNP = 0., Cqe_2312r_LNP = 0., Cqe_2313r_LNP = 0., Cqe_2321r_LNP = 0., Cqe_2322r_LNP = 0., Cqe_2323r_LNP = 0.,
7479 Cqe_2331r_LNP = 0., Cqe_2332r_LNP = 0., Cqe_2333r_LNP = 0., Cqe_3311r_LNP = 0., Cqe_3312r_LNP = 0., Cqe_3313r_LNP = 0., Cqe_3322r_LNP = 0., Cqe_3323r_LNP = 0., Cqe_3333r_LNP = 0.;
7480 double Cqe_1112i_LNP = 0., Cqe_1113i_LNP = 0., Cqe_1123i_LNP = 0., Cqe_1211i_LNP = 0., Cqe_1212i_LNP = 0., Cqe_1213i_LNP = 0., Cqe_1221i_LNP = 0., Cqe_1222i_LNP = 0., Cqe_1223i_LNP = 0.,
7481 Cqe_1231i_LNP = 0., Cqe_1232i_LNP = 0., Cqe_1233i_LNP = 0., Cqe_1311i_LNP = 0., Cqe_1312i_LNP = 0., Cqe_1313i_LNP = 0., Cqe_1321i_LNP = 0., Cqe_1322i_LNP = 0., Cqe_1323i_LNP = 0.,
7482 Cqe_1331i_LNP = 0., Cqe_1332i_LNP = 0., Cqe_1333i_LNP = 0., Cqe_2212i_LNP = 0., Cqe_2213i_LNP = 0., Cqe_2223i_LNP = 0., Cqe_2312i_LNP = 0., Cqe_2313i_LNP = 0., Cqe_2321i_LNP = 0.,
7483 Cqe_2322i_LNP = 0., Cqe_2323i_LNP = 0., Cqe_2331i_LNP = 0., Cqe_2332i_LNP = 0., Cqe_2333i_LNP = 0., Cqe_2311i_LNP = 0., Cqe_3312i_LNP = 0., Cqe_3313i_LNP = 0., Cqe_3323i_LNP = 0.;
7484 double Cledq_1111r_LNP = 0., Cledq_1112r_LNP = 0., Cledq_1113r_LNP = 0., Cledq_1121r_LNP = 0., Cledq_1122r_LNP = 0., Cledq_1123r_LNP = 0., Cledq_1131r_LNP = 0., Cledq_1132r_LNP = 0., Cledq_1133r_LNP = 0.,
7485 Cledq_1211r_LNP = 0., Cledq_1212r_LNP = 0., Cledq_1213r_LNP = 0., Cledq_1221r_LNP = 0., Cledq_1222r_LNP = 0., Cledq_1223r_LNP = 0., Cledq_1231r_LNP = 0., Cledq_1232r_LNP = 0., Cledq_1233r_LNP = 0.,
7486 Cledq_1311r_LNP = 0., Cledq_1312r_LNP = 0., Cledq_1313r_LNP = 0., Cledq_1321r_LNP = 0., Cledq_1322r_LNP = 0., Cledq_1323r_LNP = 0., Cledq_1331r_LNP = 0., Cledq_1332r_LNP = 0., Cledq_1333r_LNP = 0.,
7487 Cledq_2111r_LNP = 0., Cledq_2112r_LNP = 0., Cledq_2113r_LNP = 0., Cledq_2121r_LNP = 0., Cledq_2122r_LNP = 0., Cledq_2123r_LNP = 0., Cledq_2131r_LNP = 0., Cledq_2132r_LNP = 0., Cledq_2133r_LNP = 0.,
7488 Cledq_2211r_LNP = 0., Cledq_2212r_LNP = 0., Cledq_2213r_LNP = 0., Cledq_2221r_LNP = 0., Cledq_2222r_LNP = 0., Cledq_2223r_LNP = 0., Cledq_2231r_LNP = 0., Cledq_2232r_LNP = 0., Cledq_2233r_LNP = 0.,
7489 Cledq_2311r_LNP = 0., Cledq_2312r_LNP = 0., Cledq_2313r_LNP = 0., Cledq_2321r_LNP = 0., Cledq_2322r_LNP = 0., Cledq_2323r_LNP = 0., Cledq_2331r_LNP = 0., Cledq_2332r_LNP = 0., Cledq_2333r_LNP = 0.,
7490 Cledq_3111r_LNP = 0., Cledq_3112r_LNP = 0., Cledq_3113r_LNP = 0., Cledq_3121r_LNP = 0., Cledq_3122r_LNP = 0., Cledq_3123r_LNP = 0., Cledq_3131r_LNP = 0., Cledq_3132r_LNP = 0., Cledq_3133r_LNP = 0.,
7491 Cledq_3211r_LNP = 0., Cledq_3212r_LNP = 0., Cledq_3213r_LNP = 0., Cledq_3221r_LNP = 0., Cledq_3222r_LNP = 0., Cledq_3223r_LNP = 0., Cledq_3231r_LNP = 0., Cledq_3232r_LNP = 0., Cledq_3233r_LNP = 0.,
7492 Cledq_3311r_LNP = 0., Cledq_3312r_LNP = 0., Cledq_3313r_LNP = 0., Cledq_3321r_LNP = 0., Cledq_3322r_LNP = 0., Cledq_3323r_LNP = 0., Cledq_3331r_LNP = 0., Cledq_3332r_LNP = 0., Cledq_3333r_LNP = 0.;
7493 double Cledq_1111i_LNP = 0., Cledq_1112i_LNP = 0., Cledq_1113i_LNP = 0., Cledq_1121i_LNP = 0., Cledq_1122i_LNP = 0., Cledq_1123i_LNP = 0., Cledq_1131i_LNP = 0., Cledq_1132i_LNP = 0., Cledq_1133i_LNP = 0.,
7494 Cledq_1211i_LNP = 0., Cledq_1212i_LNP = 0., Cledq_1213i_LNP = 0., Cledq_1221i_LNP = 0., Cledq_1222i_LNP = 0., Cledq_1223i_LNP = 0., Cledq_1231i_LNP = 0., Cledq_1232i_LNP = 0., Cledq_1233i_LNP = 0.,
7495 Cledq_1311i_LNP = 0., Cledq_1312i_LNP = 0., Cledq_1313i_LNP = 0., Cledq_1321i_LNP = 0., Cledq_1322i_LNP = 0., Cledq_1323i_LNP = 0., Cledq_1331i_LNP = 0., Cledq_1332i_LNP = 0., Cledq_1333i_LNP = 0.,
7496 Cledq_2111i_LNP = 0., Cledq_2112i_LNP = 0., Cledq_2113i_LNP = 0., Cledq_2121i_LNP = 0., Cledq_2122i_LNP = 0., Cledq_2123i_LNP = 0., Cledq_2131i_LNP = 0., Cledq_2132i_LNP = 0., Cledq_2133i_LNP = 0.,
7497 Cledq_2211i_LNP = 0., Cledq_2212i_LNP = 0., Cledq_2213i_LNP = 0., Cledq_2221i_LNP = 0., Cledq_2222i_LNP = 0., Cledq_2223i_LNP = 0., Cledq_2231i_LNP = 0., Cledq_2232i_LNP = 0., Cledq_2233i_LNP = 0.,
7498 Cledq_2311i_LNP = 0., Cledq_2312i_LNP = 0., Cledq_2313i_LNP = 0., Cledq_2321i_LNP = 0., Cledq_2322i_LNP = 0., Cledq_2323i_LNP = 0., Cledq_2331i_LNP = 0., Cledq_2332i_LNP = 0., Cledq_2333i_LNP = 0.,
7499 Cledq_3111i_LNP = 0., Cledq_3112i_LNP = 0., Cledq_3113i_LNP = 0., Cledq_3121i_LNP = 0., Cledq_3122i_LNP = 0., Cledq_3123i_LNP = 0., Cledq_3131i_LNP = 0., Cledq_3132i_LNP = 0., Cledq_3133i_LNP = 0.,
7500 Cledq_3211i_LNP = 0., Cledq_3212i_LNP = 0., Cledq_3213i_LNP = 0., Cledq_3221i_LNP = 0., Cledq_3222i_LNP = 0., Cledq_3223i_LNP = 0., Cledq_3231i_LNP = 0., Cledq_3232i_LNP = 0., Cledq_3233i_LNP = 0.,
7501 Cledq_3311i_LNP = 0., Cledq_3312i_LNP = 0., Cledq_3313i_LNP = 0., Cledq_3321i_LNP = 0., Cledq_3322i_LNP = 0., Cledq_3323i_LNP = 0., Cledq_3331i_LNP = 0., Cledq_3332i_LNP = 0., Cledq_3333i_LNP = 0.;
7502 double Cqq1_1111r_LNP = 0., Cqq1_1112r_LNP = 0., Cqq1_1113r_LNP = 0., Cqq1_1122r_LNP = 0., Cqq1_1123r_LNP = 0., Cqq1_1133r_LNP = 0., Cqq1_1212r_LNP = 0., Cqq1_1213r_LNP = 0., Cqq1_1221r_LNP = 0.,
7503 Cqq1_1222r_LNP = 0., Cqq1_1223r_LNP = 0., Cqq1_1231r_LNP = 0., Cqq1_1232r_LNP = 0., Cqq1_1233r_LNP = 0., Cqq1_1313r_LNP = 0., Cqq1_1322r_LNP = 0., Cqq1_1323r_LNP = 0., Cqq1_1331r_LNP = 0.,
7504 Cqq1_1332r_LNP = 0., Cqq1_1333r_LNP = 0., Cqq1_2222r_LNP = 0., Cqq1_2223r_LNP = 0., Cqq1_2233r_LNP = 0., Cqq1_2323r_LNP = 0., Cqq1_2332r_LNP = 0., Cqq1_2333r_LNP = 0., Cqq1_3333r_LNP = 0.;
7505 double Cqq1_1112i_LNP = 0., Cqq1_1113i_LNP = 0., Cqq1_1123i_LNP = 0., Cqq1_1212i_LNP = 0., Cqq1_1213i_LNP = 0., Cqq1_1222i_LNP = 0., Cqq1_1223i_LNP = 0., Cqq1_1231i_LNP = 0., Cqq1_1232i_LNP = 0.,
7506 Cqq1_1233i_LNP = 0., Cqq1_1313i_LNP = 0., Cqq1_1322i_LNP = 0., Cqq1_1323i_LNP = 0., Cqq1_1332i_LNP = 0., Cqq1_1333i_LNP = 0., Cqq1_2223i_LNP = 0., Cqq1_2323i_LNP = 0., Cqq1_2333i_LNP = 0.;
7507 double Cqq3_1111r_LNP = 0., Cqq3_1112r_LNP = 0., Cqq3_1113r_LNP = 0., Cqq3_1122r_LNP = 0., Cqq3_1123r_LNP = 0., Cqq3_1133r_LNP = 0., Cqq3_1212r_LNP = 0., Cqq3_1213r_LNP = 0., Cqq3_1221r_LNP = 0.,
7508 Cqq3_1222r_LNP = 0., Cqq3_1223r_LNP = 0., Cqq3_1231r_LNP = 0., Cqq3_1232r_LNP = 0., Cqq3_1233r_LNP = 0., Cqq3_1313r_LNP = 0., Cqq3_1322r_LNP = 0., Cqq3_1323r_LNP = 0., Cqq3_1331r_LNP = 0.,
7509 Cqq3_1332r_LNP = 0., Cqq3_1333r_LNP = 0., Cqq3_2222r_LNP = 0., Cqq3_2223r_LNP = 0., Cqq3_2233r_LNP = 0., Cqq3_2323r_LNP = 0., Cqq3_2332r_LNP = 0., Cqq3_2333r_LNP = 0., Cqq3_3333r_LNP = 0.;
7510 double Cqq3_1112i_LNP = 0., Cqq3_1113i_LNP = 0., Cqq3_1123i_LNP = 0., Cqq3_1212i_LNP = 0., Cqq3_1213i_LNP = 0., Cqq3_1222i_LNP = 0., Cqq3_1223i_LNP = 0., Cqq3_1231i_LNP = 0., Cqq3_1232i_LNP = 0.,
7511 Cqq3_1233i_LNP = 0., Cqq3_1313i_LNP = 0., Cqq3_1322i_LNP = 0., Cqq3_1323i_LNP = 0., Cqq3_1332i_LNP = 0., Cqq3_1333i_LNP = 0., Cqq3_2223i_LNP = 0., Cqq3_2323i_LNP = 0., Cqq3_2333i_LNP = 0.;
7512 double Cuu_1111r_LNP = 0., Cuu_1112r_LNP = 0., Cuu_1113r_LNP = 0., Cuu_1122r_LNP = 0., Cuu_1123r_LNP = 0., Cuu_1133r_LNP = 0., Cuu_1212r_LNP = 0., Cuu_1213r_LNP = 0., Cuu_1221r_LNP = 0.,
7513 Cuu_1222r_LNP = 0., Cuu_1223r_LNP = 0., Cuu_1231r_LNP = 0., Cuu_1232r_LNP = 0., Cuu_1233r_LNP = 0., Cuu_1313r_LNP = 0., Cuu_1322r_LNP = 0., Cuu_1323r_LNP = 0., Cuu_1331r_LNP = 0.,
7514 Cuu_1332r_LNP = 0., Cuu_1333r_LNP = 0., Cuu_2222r_LNP = 0., Cuu_2223r_LNP = 0., Cuu_2233r_LNP = 0., Cuu_2323r_LNP = 0., Cuu_2332r_LNP = 0., Cuu_2333r_LNP = 0., Cuu_3333r_LNP = 0.;
7515 double Cuu_1112i_LNP = 0., Cuu_1113i_LNP = 0., Cuu_1123i_LNP = 0., Cuu_1212i_LNP = 0., Cuu_1213i_LNP = 0., Cuu_1222i_LNP = 0., Cuu_1223i_LNP = 0., Cuu_1231i_LNP = 0., Cuu_1232i_LNP = 0.,
7516 Cuu_1233i_LNP = 0., Cuu_1313i_LNP = 0., Cuu_1322i_LNP = 0., Cuu_1323i_LNP = 0., Cuu_1332i_LNP = 0., Cuu_1333i_LNP = 0., Cuu_2223i_LNP = 0., Cuu_2323i_LNP = 0., Cuu_2333i_LNP = 0.;
7517 double Cdd_1111r_LNP = 0., Cdd_1112r_LNP = 0., Cdd_1113r_LNP = 0., Cdd_1122r_LNP = 0., Cdd_1123r_LNP = 0., Cdd_1133r_LNP = 0., Cdd_1212r_LNP = 0., Cdd_1213r_LNP = 0., Cdd_1221r_LNP = 0.,
7518 Cdd_1222r_LNP = 0., Cdd_1223r_LNP = 0., Cdd_1231r_LNP = 0., Cdd_1232r_LNP = 0., Cdd_1233r_LNP = 0., Cdd_1313r_LNP = 0., Cdd_1322r_LNP = 0., Cdd_1323r_LNP = 0., Cdd_1331r_LNP = 0.,
7519 Cdd_1332r_LNP = 0., Cdd_1333r_LNP = 0., Cdd_2222r_LNP = 0., Cdd_2223r_LNP = 0., Cdd_2233r_LNP = 0., Cdd_2323r_LNP = 0., Cdd_2332r_LNP = 0., Cdd_2333r_LNP = 0., Cdd_3333r_LNP = 0.;
7520 double Cdd_1112i_LNP = 0., Cdd_1113i_LNP = 0., Cdd_1123i_LNP = 0., Cdd_1212i_LNP = 0., Cdd_1213i_LNP = 0., Cdd_1222i_LNP = 0., Cdd_1223i_LNP = 0., Cdd_1231i_LNP = 0., Cdd_1232i_LNP = 0.,
7521 Cdd_1233i_LNP = 0., Cdd_1313i_LNP = 0., Cdd_1322i_LNP = 0., Cdd_1323i_LNP = 0., Cdd_1332i_LNP = 0., Cdd_1333i_LNP = 0., Cdd_2223i_LNP = 0., Cdd_2323i_LNP = 0., Cdd_2333i_LNP = 0.;
7522 double Cud1_1111r_LNP = 0., Cud1_1112r_LNP = 0., Cud1_1113r_LNP = 0., Cud1_1122r_LNP = 0., Cud1_1123r_LNP = 0., Cud1_1133r_LNP = 0., Cud1_1211r_LNP = 0., Cud1_1212r_LNP = 0., Cud1_1213r_LNP = 0.,
7523 Cud1_1221r_LNP = 0., Cud1_1222r_LNP = 0., Cud1_1223r_LNP = 0., Cud1_1231r_LNP = 0., Cud1_1232r_LNP = 0., Cud1_1233r_LNP = 0., Cud1_1311r_LNP = 0., Cud1_1312r_LNP = 0., Cud1_1313r_LNP = 0.,
7524 Cud1_1321r_LNP = 0., Cud1_1322r_LNP = 0., Cud1_1323r_LNP = 0., Cud1_1331r_LNP = 0., Cud1_1332r_LNP = 0., Cud1_1333r_LNP = 0., Cud1_2211r_LNP = 0., Cud1_2212r_LNP = 0., Cud1_2213r_LNP = 0.,
7525 Cud1_2222r_LNP = 0., Cud1_2223r_LNP = 0., Cud1_2233r_LNP = 0., Cud1_2311r_LNP = 0., Cud1_2312r_LNP = 0., Cud1_2313r_LNP = 0., Cud1_2321r_LNP = 0., Cud1_2322r_LNP = 0., Cud1_2323r_LNP = 0.,
7526 Cud1_2331r_LNP = 0., Cud1_2332r_LNP = 0., Cud1_2333r_LNP = 0., Cud1_3311r_LNP = 0., Cud1_3312r_LNP = 0., Cud1_3313r_LNP = 0., Cud1_3322r_LNP = 0., Cud1_3323r_LNP = 0., Cud1_3333r_LNP = 0.;
7527 double Cud1_1112i_LNP = 0., Cud1_1113i_LNP = 0., Cud1_1123i_LNP = 0., Cud1_1211i_LNP = 0., Cud1_1212i_LNP = 0., Cud1_1213i_LNP = 0., Cud1_1221i_LNP = 0., Cud1_1222i_LNP = 0., Cud1_1223i_LNP = 0.,
7528 Cud1_1231i_LNP = 0., Cud1_1232i_LNP = 0., Cud1_1233i_LNP = 0., Cud1_1311i_LNP = 0., Cud1_1312i_LNP = 0., Cud1_1313i_LNP = 0., Cud1_1321i_LNP = 0., Cud1_1322i_LNP = 0., Cud1_1323i_LNP = 0.,
7529 Cud1_1331i_LNP = 0., Cud1_1332i_LNP = 0., Cud1_1333i_LNP = 0., Cud1_2212i_LNP = 0., Cud1_2213i_LNP = 0., Cud1_2223i_LNP = 0., Cud1_2312i_LNP = 0., Cud1_2313i_LNP = 0., Cud1_2321i_LNP = 0.,
7530 Cud1_2322i_LNP = 0., Cud1_2323i_LNP = 0., Cud1_2331i_LNP = 0., Cud1_2332i_LNP = 0., Cud1_2333i_LNP = 0., Cud1_2311i_LNP = 0., Cud1_3312i_LNP = 0., Cud1_3313i_LNP = 0., Cud1_3323i_LNP = 0.;
7531 double Cud8_1111r_LNP = 0., Cud8_1112r_LNP = 0., Cud8_1113r_LNP = 0., Cud8_1122r_LNP = 0., Cud8_1123r_LNP = 0., Cud8_1133r_LNP = 0., Cud8_1211r_LNP = 0., Cud8_1212r_LNP = 0., Cud8_1213r_LNP = 0.,
7532 Cud8_1221r_LNP = 0., Cud8_1222r_LNP = 0., Cud8_1223r_LNP = 0., Cud8_1231r_LNP = 0., Cud8_1232r_LNP = 0., Cud8_1233r_LNP = 0., Cud8_1311r_LNP = 0., Cud8_1312r_LNP = 0., Cud8_1313r_LNP = 0.,
7533 Cud8_1321r_LNP = 0., Cud8_1322r_LNP = 0., Cud8_1323r_LNP = 0., Cud8_1331r_LNP = 0., Cud8_1332r_LNP = 0., Cud8_1333r_LNP = 0., Cud8_2211r_LNP = 0., Cud8_2212r_LNP = 0., Cud8_2213r_LNP = 0.,
7534 Cud8_2222r_LNP = 0., Cud8_2223r_LNP = 0., Cud8_2233r_LNP = 0., Cud8_2311r_LNP = 0., Cud8_2312r_LNP = 0., Cud8_2313r_LNP = 0., Cud8_2321r_LNP = 0., Cud8_2322r_LNP = 0., Cud8_2323r_LNP = 0.,
7535 Cud8_2331r_LNP = 0., Cud8_2332r_LNP = 0., Cud8_2333r_LNP = 0., Cud8_3311r_LNP = 0., Cud8_3312r_LNP = 0., Cud8_3313r_LNP = 0., Cud8_3322r_LNP = 0., Cud8_3323r_LNP = 0., Cud8_3333r_LNP = 0.;
7536 double Cud8_1112i_LNP = 0., Cud8_1113i_LNP = 0., Cud8_1123i_LNP = 0., Cud8_1211i_LNP = 0., Cud8_1212i_LNP = 0., Cud8_1213i_LNP = 0., Cud8_1221i_LNP = 0., Cud8_1222i_LNP = 0., Cud8_1223i_LNP = 0.,
7537 Cud8_1231i_LNP = 0., Cud8_1232i_LNP = 0., Cud8_1233i_LNP = 0., Cud8_1311i_LNP = 0., Cud8_1312i_LNP = 0., Cud8_1313i_LNP = 0., Cud8_1321i_LNP = 0., Cud8_1322i_LNP = 0., Cud8_1323i_LNP = 0.,
7538 Cud8_1331i_LNP = 0., Cud8_1332i_LNP = 0., Cud8_1333i_LNP = 0., Cud8_2212i_LNP = 0., Cud8_2213i_LNP = 0., Cud8_2223i_LNP = 0., Cud8_2312i_LNP = 0., Cud8_2313i_LNP = 0., Cud8_2321i_LNP = 0.,
7539 Cud8_2322i_LNP = 0., Cud8_2323i_LNP = 0., Cud8_2331i_LNP = 0., Cud8_2332i_LNP = 0., Cud8_2333i_LNP = 0., Cud8_2311i_LNP = 0., Cud8_3312i_LNP = 0., Cud8_3313i_LNP = 0., Cud8_3323i_LNP = 0.;
7540 double Cqu1_1111r_LNP = 0., Cqu1_1112r_LNP = 0., Cqu1_1113r_LNP = 0., Cqu1_1122r_LNP = 0., Cqu1_1123r_LNP = 0., Cqu1_1133r_LNP = 0., Cqu1_1211r_LNP = 0., Cqu1_1212r_LNP = 0., Cqu1_1213r_LNP = 0.,
7541 Cqu1_1221r_LNP = 0., Cqu1_1222r_LNP = 0., Cqu1_1223r_LNP = 0., Cqu1_1231r_LNP = 0., Cqu1_1232r_LNP = 0., Cqu1_1233r_LNP = 0., Cqu1_1311r_LNP = 0., Cqu1_1312r_LNP = 0., Cqu1_1313r_LNP = 0.,
7542 Cqu1_1321r_LNP = 0., Cqu1_1322r_LNP = 0., Cqu1_1323r_LNP = 0., Cqu1_1331r_LNP = 0., Cqu1_1332r_LNP = 0., Cqu1_1333r_LNP = 0., Cqu1_2211r_LNP = 0., Cqu1_2212r_LNP = 0., Cqu1_2213r_LNP = 0.,
7543 Cqu1_2222r_LNP = 0., Cqu1_2223r_LNP = 0., Cqu1_2233r_LNP = 0., Cqu1_2311r_LNP = 0., Cqu1_2312r_LNP = 0., Cqu1_2313r_LNP = 0., Cqu1_2321r_LNP = 0., Cqu1_2322r_LNP = 0., Cqu1_2323r_LNP = 0.,
7544 Cqu1_2331r_LNP = 0., Cqu1_2332r_LNP = 0., Cqu1_2333r_LNP = 0., Cqu1_3311r_LNP = 0., Cqu1_3312r_LNP = 0., Cqu1_3313r_LNP = 0., Cqu1_3322r_LNP = 0., Cqu1_3323r_LNP = 0., Cqu1_3333r_LNP = 0.;
7545 double Cqu1_1112i_LNP = 0., Cqu1_1113i_LNP = 0., Cqu1_1123i_LNP = 0., Cqu1_1211i_LNP = 0., Cqu1_1212i_LNP = 0., Cqu1_1213i_LNP = 0., Cqu1_1221i_LNP = 0., Cqu1_1222i_LNP = 0., Cqu1_1223i_LNP = 0.,
7546 Cqu1_1231i_LNP = 0., Cqu1_1232i_LNP = 0., Cqu1_1233i_LNP = 0., Cqu1_1311i_LNP = 0., Cqu1_1312i_LNP = 0., Cqu1_1313i_LNP = 0., Cqu1_1321i_LNP = 0., Cqu1_1322i_LNP = 0., Cqu1_1323i_LNP = 0.,
7547 Cqu1_1331i_LNP = 0., Cqu1_1332i_LNP = 0., Cqu1_1333i_LNP = 0., Cqu1_2212i_LNP = 0., Cqu1_2213i_LNP = 0., Cqu1_2223i_LNP = 0., Cqu1_2312i_LNP = 0., Cqu1_2313i_LNP = 0., Cqu1_2321i_LNP = 0.,
7548 Cqu1_2322i_LNP = 0., Cqu1_2323i_LNP = 0., Cqu1_2331i_LNP = 0., Cqu1_2332i_LNP = 0., Cqu1_2333i_LNP = 0., Cqu1_2311i_LNP = 0., Cqu1_3312i_LNP = 0., Cqu1_3313i_LNP = 0., Cqu1_3323i_LNP = 0.;
7549 double Cqu8_1111r_LNP = 0., Cqu8_1112r_LNP = 0., Cqu8_1113r_LNP = 0., Cqu8_1122r_LNP = 0., Cqu8_1123r_LNP = 0., Cqu8_1133r_LNP = 0., Cqu8_1211r_LNP = 0., Cqu8_1212r_LNP = 0., Cqu8_1213r_LNP = 0.,
7550 Cqu8_1221r_LNP = 0., Cqu8_1222r_LNP = 0., Cqu8_1223r_LNP = 0., Cqu8_1231r_LNP = 0., Cqu8_1232r_LNP = 0., Cqu8_1233r_LNP = 0., Cqu8_1311r_LNP = 0., Cqu8_1312r_LNP = 0., Cqu8_1313r_LNP = 0.,
7551 Cqu8_1321r_LNP = 0., Cqu8_1322r_LNP = 0., Cqu8_1323r_LNP = 0., Cqu8_1331r_LNP = 0., Cqu8_1332r_LNP = 0., Cqu8_1333r_LNP = 0., Cqu8_2211r_LNP = 0., Cqu8_2212r_LNP = 0., Cqu8_2213r_LNP = 0.,
7552 Cqu8_2222r_LNP = 0., Cqu8_2223r_LNP = 0., Cqu8_2233r_LNP = 0., Cqu8_2311r_LNP = 0., Cqu8_2312r_LNP = 0., Cqu8_2313r_LNP = 0., Cqu8_2321r_LNP = 0., Cqu8_2322r_LNP = 0., Cqu8_2323r_LNP = 0.,
7553 Cqu8_2331r_LNP = 0., Cqu8_2332r_LNP = 0., Cqu8_2333r_LNP = 0., Cqu8_3311r_LNP = 0., Cqu8_3312r_LNP = 0., Cqu8_3313r_LNP = 0., Cqu8_3322r_LNP = 0., Cqu8_3323r_LNP = 0., Cqu8_3333r_LNP = 0.;
7554 double Cqu8_1112i_LNP = 0., Cqu8_1113i_LNP = 0., Cqu8_1123i_LNP = 0., Cqu8_1211i_LNP = 0., Cqu8_1212i_LNP = 0., Cqu8_1213i_LNP = 0., Cqu8_1221i_LNP = 0., Cqu8_1222i_LNP = 0., Cqu8_1223i_LNP = 0.,
7555 Cqu8_1231i_LNP = 0., Cqu8_1232i_LNP = 0., Cqu8_1233i_LNP = 0., Cqu8_1311i_LNP = 0., Cqu8_1312i_LNP = 0., Cqu8_1313i_LNP = 0., Cqu8_1321i_LNP = 0., Cqu8_1322i_LNP = 0., Cqu8_1323i_LNP = 0.,
7556 Cqu8_1331i_LNP = 0., Cqu8_1332i_LNP = 0., Cqu8_1333i_LNP = 0., Cqu8_2212i_LNP = 0., Cqu8_2213i_LNP = 0., Cqu8_2223i_LNP = 0., Cqu8_2312i_LNP = 0., Cqu8_2313i_LNP = 0., Cqu8_2321i_LNP = 0.,
7557 Cqu8_2322i_LNP = 0., Cqu8_2323i_LNP = 0., Cqu8_2331i_LNP = 0., Cqu8_2332i_LNP = 0., Cqu8_2333i_LNP = 0., Cqu8_2311i_LNP = 0., Cqu8_3312i_LNP = 0., Cqu8_3313i_LNP = 0., Cqu8_3323i_LNP = 0.;
7558 double Cqd1_1111r_LNP = 0., Cqd1_1112r_LNP = 0., Cqd1_1113r_LNP = 0., Cqd1_1122r_LNP = 0., Cqd1_1123r_LNP = 0., Cqd1_1133r_LNP = 0., Cqd1_1211r_LNP = 0., Cqd1_1212r_LNP = 0., Cqd1_1213r_LNP = 0.,
7559 Cqd1_1221r_LNP = 0., Cqd1_1222r_LNP = 0., Cqd1_1223r_LNP = 0., Cqd1_1231r_LNP = 0., Cqd1_1232r_LNP = 0., Cqd1_1233r_LNP = 0., Cqd1_1311r_LNP = 0., Cqd1_1312r_LNP = 0., Cqd1_1313r_LNP = 0.,
7560 Cqd1_1321r_LNP = 0., Cqd1_1322r_LNP = 0., Cqd1_1323r_LNP = 0., Cqd1_1331r_LNP = 0., Cqd1_1332r_LNP = 0., Cqd1_1333r_LNP = 0., Cqd1_2211r_LNP = 0., Cqd1_2212r_LNP = 0., Cqd1_2213r_LNP = 0.,
7561 Cqd1_2222r_LNP = 0., Cqd1_2223r_LNP = 0., Cqd1_2233r_LNP = 0., Cqd1_2311r_LNP = 0., Cqd1_2312r_LNP = 0., Cqd1_2313r_LNP = 0., Cqd1_2321r_LNP = 0., Cqd1_2322r_LNP = 0., Cqd1_2323r_LNP = 0.,
7562 Cqd1_2331r_LNP = 0., Cqd1_2332r_LNP = 0., Cqd1_2333r_LNP = 0., Cqd1_3311r_LNP = 0., Cqd1_3312r_LNP = 0., Cqd1_3313r_LNP = 0., Cqd1_3322r_LNP = 0., Cqd1_3323r_LNP = 0., Cqd1_3333r_LNP = 0.;
7563 double Cqd1_1112i_LNP = 0., Cqd1_1113i_LNP = 0., Cqd1_1123i_LNP = 0., Cqd1_1211i_LNP = 0., Cqd1_1212i_LNP = 0., Cqd1_1213i_LNP = 0., Cqd1_1221i_LNP = 0., Cqd1_1222i_LNP = 0., Cqd1_1223i_LNP = 0.,
7564 Cqd1_1231i_LNP = 0., Cqd1_1232i_LNP = 0., Cqd1_1233i_LNP = 0., Cqd1_1311i_LNP = 0., Cqd1_1312i_LNP = 0., Cqd1_1313i_LNP = 0., Cqd1_1321i_LNP = 0., Cqd1_1322i_LNP = 0., Cqd1_1323i_LNP = 0.,
7565 Cqd1_1331i_LNP = 0., Cqd1_1332i_LNP = 0., Cqd1_1333i_LNP = 0., Cqd1_2212i_LNP = 0., Cqd1_2213i_LNP = 0., Cqd1_2223i_LNP = 0., Cqd1_2312i_LNP = 0., Cqd1_2313i_LNP = 0., Cqd1_2321i_LNP = 0.,
7566 Cqd1_2322i_LNP = 0., Cqd1_2323i_LNP = 0., Cqd1_2331i_LNP = 0., Cqd1_2332i_LNP = 0., Cqd1_2333i_LNP = 0., Cqd1_2311i_LNP = 0., Cqd1_3312i_LNP = 0., Cqd1_3313i_LNP = 0., Cqd1_3323i_LNP = 0.;
7567 double Cqd8_1111r_LNP = 0., Cqd8_1112r_LNP = 0., Cqd8_1113r_LNP = 0., Cqd8_1122r_LNP = 0., Cqd8_1123r_LNP = 0., Cqd8_1133r_LNP = 0., Cqd8_1211r_LNP = 0., Cqd8_1212r_LNP = 0., Cqd8_1213r_LNP = 0.,
7568 Cqd8_1221r_LNP = 0., Cqd8_1222r_LNP = 0., Cqd8_1223r_LNP = 0., Cqd8_1231r_LNP = 0., Cqd8_1232r_LNP = 0., Cqd8_1233r_LNP = 0., Cqd8_1311r_LNP = 0., Cqd8_1312r_LNP = 0., Cqd8_1313r_LNP = 0.,
7569 Cqd8_1321r_LNP = 0., Cqd8_1322r_LNP = 0., Cqd8_1323r_LNP = 0., Cqd8_1331r_LNP = 0., Cqd8_1332r_LNP = 0., Cqd8_1333r_LNP = 0., Cqd8_2211r_LNP = 0., Cqd8_2212r_LNP = 0., Cqd8_2213r_LNP = 0.,
7570 Cqd8_2222r_LNP = 0., Cqd8_2223r_LNP = 0., Cqd8_2233r_LNP = 0., Cqd8_2311r_LNP = 0., Cqd8_2312r_LNP = 0., Cqd8_2313r_LNP = 0., Cqd8_2321r_LNP = 0., Cqd8_2322r_LNP = 0., Cqd8_2323r_LNP = 0.,
7571 Cqd8_2331r_LNP = 0., Cqd8_2332r_LNP = 0., Cqd8_2333r_LNP = 0., Cqd8_3311r_LNP = 0., Cqd8_3312r_LNP = 0., Cqd8_3313r_LNP = 0., Cqd8_3322r_LNP = 0., Cqd8_3323r_LNP = 0., Cqd8_3333r_LNP = 0.;
7572 double Cqd8_1112i_LNP = 0., Cqd8_1113i_LNP = 0., Cqd8_1123i_LNP = 0., Cqd8_1211i_LNP = 0., Cqd8_1212i_LNP = 0., Cqd8_1213i_LNP = 0., Cqd8_1221i_LNP = 0., Cqd8_1222i_LNP = 0., Cqd8_1223i_LNP = 0.,
7573 Cqd8_1231i_LNP = 0., Cqd8_1232i_LNP = 0., Cqd8_1233i_LNP = 0., Cqd8_1311i_LNP = 0., Cqd8_1312i_LNP = 0., Cqd8_1313i_LNP = 0., Cqd8_1321i_LNP = 0., Cqd8_1322i_LNP = 0., Cqd8_1323i_LNP = 0.,
7574 Cqd8_1331i_LNP = 0., Cqd8_1332i_LNP = 0., Cqd8_1333i_LNP = 0., Cqd8_2212i_LNP = 0., Cqd8_2213i_LNP = 0., Cqd8_2223i_LNP = 0., Cqd8_2312i_LNP = 0., Cqd8_2313i_LNP = 0., Cqd8_2321i_LNP = 0.,
7575 Cqd8_2322i_LNP = 0., Cqd8_2323i_LNP = 0., Cqd8_2331i_LNP = 0., Cqd8_2332i_LNP = 0., Cqd8_2333i_LNP = 0., Cqd8_2311i_LNP = 0., Cqd8_3312i_LNP = 0., Cqd8_3313i_LNP = 0., Cqd8_3323i_LNP = 0.;
7576 double Cquqd1_1111r_LNP = 0., Cquqd1_1112r_LNP = 0., Cquqd1_1113r_LNP = 0., Cquqd1_1121r_LNP = 0., Cquqd1_1122r_LNP = 0., Cquqd1_1123r_LNP = 0., Cquqd1_1131r_LNP = 0., Cquqd1_1132r_LNP = 0., Cquqd1_1133r_LNP = 0.,
7577 Cquqd1_1211r_LNP = 0., Cquqd1_1212r_LNP = 0., Cquqd1_1213r_LNP = 0., Cquqd1_1221r_LNP = 0., Cquqd1_1222r_LNP = 0., Cquqd1_1223r_LNP = 0., Cquqd1_1231r_LNP = 0., Cquqd1_1232r_LNP = 0., Cquqd1_1233r_LNP = 0.,
7578 Cquqd1_1311r_LNP = 0., Cquqd1_1312r_LNP = 0., Cquqd1_1313r_LNP = 0., Cquqd1_1321r_LNP = 0., Cquqd1_1322r_LNP = 0., Cquqd1_1323r_LNP = 0., Cquqd1_1331r_LNP = 0., Cquqd1_1332r_LNP = 0., Cquqd1_1333r_LNP = 0.,
7579 Cquqd1_2111r_LNP = 0., Cquqd1_2112r_LNP = 0., Cquqd1_2113r_LNP = 0., Cquqd1_2121r_LNP = 0., Cquqd1_2122r_LNP = 0., Cquqd1_2123r_LNP = 0., Cquqd1_2131r_LNP = 0., Cquqd1_2132r_LNP = 0., Cquqd1_2133r_LNP = 0.,
7580 Cquqd1_2211r_LNP = 0., Cquqd1_2212r_LNP = 0., Cquqd1_2213r_LNP = 0., Cquqd1_2221r_LNP = 0., Cquqd1_2222r_LNP = 0., Cquqd1_2223r_LNP = 0., Cquqd1_2231r_LNP = 0., Cquqd1_2232r_LNP = 0., Cquqd1_2233r_LNP = 0.,
7581 Cquqd1_2311r_LNP = 0., Cquqd1_2312r_LNP = 0., Cquqd1_2313r_LNP = 0., Cquqd1_2321r_LNP = 0., Cquqd1_2322r_LNP = 0., Cquqd1_2323r_LNP = 0., Cquqd1_2331r_LNP = 0., Cquqd1_2332r_LNP = 0., Cquqd1_2333r_LNP = 0.,
7582 Cquqd1_3111r_LNP = 0., Cquqd1_3112r_LNP = 0., Cquqd1_3113r_LNP = 0., Cquqd1_3121r_LNP = 0., Cquqd1_3122r_LNP = 0., Cquqd1_3123r_LNP = 0., Cquqd1_3131r_LNP = 0., Cquqd1_3132r_LNP = 0., Cquqd1_3133r_LNP = 0.,
7583 Cquqd1_3211r_LNP = 0., Cquqd1_3212r_LNP = 0., Cquqd1_3213r_LNP = 0., Cquqd1_3221r_LNP = 0., Cquqd1_3222r_LNP = 0., Cquqd1_3223r_LNP = 0., Cquqd1_3231r_LNP = 0., Cquqd1_3232r_LNP = 0., Cquqd1_3233r_LNP = 0.,
7584 Cquqd1_3311r_LNP = 0., Cquqd1_3312r_LNP = 0., Cquqd1_3313r_LNP = 0., Cquqd1_3321r_LNP = 0., Cquqd1_3322r_LNP = 0., Cquqd1_3323r_LNP = 0., Cquqd1_3331r_LNP = 0., Cquqd1_3332r_LNP = 0., Cquqd1_3333r_LNP = 0.;
7585 double Cquqd1_1111i_LNP = 0., Cquqd1_1112i_LNP = 0., Cquqd1_1113i_LNP = 0., Cquqd1_1121i_LNP = 0., Cquqd1_1122i_LNP = 0., Cquqd1_1123i_LNP = 0., Cquqd1_1131i_LNP = 0., Cquqd1_1132i_LNP = 0., Cquqd1_1133i_LNP = 0.,
7586 Cquqd1_1211i_LNP = 0., Cquqd1_1212i_LNP = 0., Cquqd1_1213i_LNP = 0., Cquqd1_1221i_LNP = 0., Cquqd1_1222i_LNP = 0., Cquqd1_1223i_LNP = 0., Cquqd1_1231i_LNP = 0., Cquqd1_1232i_LNP = 0., Cquqd1_1233i_LNP = 0.,
7587 Cquqd1_1311i_LNP = 0., Cquqd1_1312i_LNP = 0., Cquqd1_1313i_LNP = 0., Cquqd1_1321i_LNP = 0., Cquqd1_1322i_LNP = 0., Cquqd1_1323i_LNP = 0., Cquqd1_1331i_LNP = 0., Cquqd1_1332i_LNP = 0., Cquqd1_1333i_LNP = 0.,
7588 Cquqd1_2111i_LNP = 0., Cquqd1_2112i_LNP = 0., Cquqd1_2113i_LNP = 0., Cquqd1_2121i_LNP = 0., Cquqd1_2122i_LNP = 0., Cquqd1_2123i_LNP = 0., Cquqd1_2131i_LNP = 0., Cquqd1_2132i_LNP = 0., Cquqd1_2133i_LNP = 0.,
7589 Cquqd1_2211i_LNP = 0., Cquqd1_2212i_LNP = 0., Cquqd1_2213i_LNP = 0., Cquqd1_2221i_LNP = 0., Cquqd1_2222i_LNP = 0., Cquqd1_2223i_LNP = 0., Cquqd1_2231i_LNP = 0., Cquqd1_2232i_LNP = 0., Cquqd1_2233i_LNP = 0.,
7590 Cquqd1_2311i_LNP = 0., Cquqd1_2312i_LNP = 0., Cquqd1_2313i_LNP = 0., Cquqd1_2321i_LNP = 0., Cquqd1_2322i_LNP = 0., Cquqd1_2323i_LNP = 0., Cquqd1_2331i_LNP = 0., Cquqd1_2332i_LNP = 0., Cquqd1_2333i_LNP = 0.,
7591 Cquqd1_3111i_LNP = 0., Cquqd1_3112i_LNP = 0., Cquqd1_3113i_LNP = 0., Cquqd1_3121i_LNP = 0., Cquqd1_3122i_LNP = 0., Cquqd1_3123i_LNP = 0., Cquqd1_3131i_LNP = 0., Cquqd1_3132i_LNP = 0., Cquqd1_3133i_LNP = 0.,
7592 Cquqd1_3211i_LNP = 0., Cquqd1_3212i_LNP = 0., Cquqd1_3213i_LNP = 0., Cquqd1_3221i_LNP = 0., Cquqd1_3222i_LNP = 0., Cquqd1_3223i_LNP = 0., Cquqd1_3231i_LNP = 0., Cquqd1_3232i_LNP = 0., Cquqd1_3233i_LNP = 0.,
7593 Cquqd1_3311i_LNP = 0., Cquqd1_3312i_LNP = 0., Cquqd1_3313i_LNP = 0., Cquqd1_3321i_LNP = 0., Cquqd1_3322i_LNP = 0., Cquqd1_3323i_LNP = 0., Cquqd1_3331i_LNP = 0., Cquqd1_3332i_LNP = 0., Cquqd1_3333i_LNP = 0.;
7594 double Cquqd8_1111r_LNP = 0., Cquqd8_1112r_LNP = 0., Cquqd8_1113r_LNP = 0., Cquqd8_1121r_LNP = 0., Cquqd8_1122r_LNP = 0., Cquqd8_1123r_LNP = 0., Cquqd8_1131r_LNP = 0., Cquqd8_1132r_LNP = 0., Cquqd8_1133r_LNP = 0.,
7595 Cquqd8_1211r_LNP = 0., Cquqd8_1212r_LNP = 0., Cquqd8_1213r_LNP = 0., Cquqd8_1221r_LNP = 0., Cquqd8_1222r_LNP = 0., Cquqd8_1223r_LNP = 0., Cquqd8_1231r_LNP = 0., Cquqd8_1232r_LNP = 0., Cquqd8_1233r_LNP = 0.,
7596 Cquqd8_1311r_LNP = 0., Cquqd8_1312r_LNP = 0., Cquqd8_1313r_LNP = 0., Cquqd8_1321r_LNP = 0., Cquqd8_1322r_LNP = 0., Cquqd8_1323r_LNP = 0., Cquqd8_1331r_LNP = 0., Cquqd8_1332r_LNP = 0., Cquqd8_1333r_LNP = 0.,
7597 Cquqd8_2111r_LNP = 0., Cquqd8_2112r_LNP = 0., Cquqd8_2113r_LNP = 0., Cquqd8_2121r_LNP = 0., Cquqd8_2122r_LNP = 0., Cquqd8_2123r_LNP = 0., Cquqd8_2131r_LNP = 0., Cquqd8_2132r_LNP = 0., Cquqd8_2133r_LNP = 0.,
7598 Cquqd8_2211r_LNP = 0., Cquqd8_2212r_LNP = 0., Cquqd8_2213r_LNP = 0., Cquqd8_2221r_LNP = 0., Cquqd8_2222r_LNP = 0., Cquqd8_2223r_LNP = 0., Cquqd8_2231r_LNP = 0., Cquqd8_2232r_LNP = 0., Cquqd8_2233r_LNP = 0.,
7599 Cquqd8_2311r_LNP = 0., Cquqd8_2312r_LNP = 0., Cquqd8_2313r_LNP = 0., Cquqd8_2321r_LNP = 0., Cquqd8_2322r_LNP = 0., Cquqd8_2323r_LNP = 0., Cquqd8_2331r_LNP = 0., Cquqd8_2332r_LNP = 0., Cquqd8_2333r_LNP = 0.,
7600 Cquqd8_3111r_LNP = 0., Cquqd8_3112r_LNP = 0., Cquqd8_3113r_LNP = 0., Cquqd8_3121r_LNP = 0., Cquqd8_3122r_LNP = 0., Cquqd8_3123r_LNP = 0., Cquqd8_3131r_LNP = 0., Cquqd8_3132r_LNP = 0., Cquqd8_3133r_LNP = 0.,
7601 Cquqd8_3211r_LNP = 0., Cquqd8_3212r_LNP = 0., Cquqd8_3213r_LNP = 0., Cquqd8_3221r_LNP = 0., Cquqd8_3222r_LNP = 0., Cquqd8_3223r_LNP = 0., Cquqd8_3231r_LNP = 0., Cquqd8_3232r_LNP = 0., Cquqd8_3233r_LNP = 0.,
7602 Cquqd8_3311r_LNP = 0., Cquqd8_3312r_LNP = 0., Cquqd8_3313r_LNP = 0., Cquqd8_3321r_LNP = 0., Cquqd8_3322r_LNP = 0., Cquqd8_3323r_LNP = 0., Cquqd8_3331r_LNP = 0., Cquqd8_3332r_LNP = 0., Cquqd8_3333r_LNP = 0.;
7603 double Cquqd8_1111i_LNP = 0., Cquqd8_1112i_LNP = 0., Cquqd8_1113i_LNP = 0., Cquqd8_1121i_LNP = 0., Cquqd8_1122i_LNP = 0., Cquqd8_1123i_LNP = 0., Cquqd8_1131i_LNP = 0., Cquqd8_1132i_LNP = 0., Cquqd8_1133i_LNP = 0.,
7604 Cquqd8_1211i_LNP = 0., Cquqd8_1212i_LNP = 0., Cquqd8_1213i_LNP = 0., Cquqd8_1221i_LNP = 0., Cquqd8_1222i_LNP = 0., Cquqd8_1223i_LNP = 0., Cquqd8_1231i_LNP = 0., Cquqd8_1232i_LNP = 0., Cquqd8_1233i_LNP = 0.,
7605 Cquqd8_1311i_LNP = 0., Cquqd8_1312i_LNP = 0., Cquqd8_1313i_LNP = 0., Cquqd8_1321i_LNP = 0., Cquqd8_1322i_LNP = 0., Cquqd8_1323i_LNP = 0., Cquqd8_1331i_LNP = 0., Cquqd8_1332i_LNP = 0., Cquqd8_1333i_LNP = 0.,
7606 Cquqd8_2111i_LNP = 0., Cquqd8_2112i_LNP = 0., Cquqd8_2113i_LNP = 0., Cquqd8_2121i_LNP = 0., Cquqd8_2122i_LNP = 0., Cquqd8_2123i_LNP = 0., Cquqd8_2131i_LNP = 0., Cquqd8_2132i_LNP = 0., Cquqd8_2133i_LNP = 0.,
7607 Cquqd8_2211i_LNP = 0., Cquqd8_2212i_LNP = 0., Cquqd8_2213i_LNP = 0., Cquqd8_2221i_LNP = 0., Cquqd8_2222i_LNP = 0., Cquqd8_2223i_LNP = 0., Cquqd8_2231i_LNP = 0., Cquqd8_2232i_LNP = 0., Cquqd8_2233i_LNP = 0.,
7608 Cquqd8_2311i_LNP = 0., Cquqd8_2312i_LNP = 0., Cquqd8_2313i_LNP = 0., Cquqd8_2321i_LNP = 0., Cquqd8_2322i_LNP = 0., Cquqd8_2323i_LNP = 0., Cquqd8_2331i_LNP = 0., Cquqd8_2332i_LNP = 0., Cquqd8_2333i_LNP = 0.,
7609 Cquqd8_3111i_LNP = 0., Cquqd8_3112i_LNP = 0., Cquqd8_3113i_LNP = 0., Cquqd8_3121i_LNP = 0., Cquqd8_3122i_LNP = 0., Cquqd8_3123i_LNP = 0., Cquqd8_3131i_LNP = 0., Cquqd8_3132i_LNP = 0., Cquqd8_3133i_LNP = 0.,
7610 Cquqd8_3211i_LNP = 0., Cquqd8_3212i_LNP = 0., Cquqd8_3213i_LNP = 0., Cquqd8_3221i_LNP = 0., Cquqd8_3222i_LNP = 0., Cquqd8_3223i_LNP = 0., Cquqd8_3231i_LNP = 0., Cquqd8_3232i_LNP = 0., Cquqd8_3233i_LNP = 0.,
7611 Cquqd8_3311i_LNP = 0., Cquqd8_3312i_LNP = 0., Cquqd8_3313i_LNP = 0., Cquqd8_3321i_LNP = 0., Cquqd8_3322i_LNP = 0., Cquqd8_3323i_LNP = 0., Cquqd8_3331i_LNP = 0., Cquqd8_3332i_LNP = 0., Cquqd8_3333i_LNP = 0.;
7612 double Clequ1_1111r_LNP = 0., Clequ1_1112r_LNP = 0., Clequ1_1113r_LNP = 0., Clequ1_1121r_LNP = 0., Clequ1_1122r_LNP = 0., Clequ1_1123r_LNP = 0., Clequ1_1131r_LNP = 0., Clequ1_1132r_LNP = 0., Clequ1_1133r_LNP = 0.,
7613 Clequ1_1211r_LNP = 0., Clequ1_1212r_LNP = 0., Clequ1_1213r_LNP = 0., Clequ1_1221r_LNP = 0., Clequ1_1222r_LNP = 0., Clequ1_1223r_LNP = 0., Clequ1_1231r_LNP = 0., Clequ1_1232r_LNP = 0., Clequ1_1233r_LNP = 0.,
7614 Clequ1_1311r_LNP = 0., Clequ1_1312r_LNP = 0., Clequ1_1313r_LNP = 0., Clequ1_1321r_LNP = 0., Clequ1_1322r_LNP = 0., Clequ1_1323r_LNP = 0., Clequ1_1331r_LNP = 0., Clequ1_1332r_LNP = 0., Clequ1_1333r_LNP = 0.,
7615 Clequ1_2111r_LNP = 0., Clequ1_2112r_LNP = 0., Clequ1_2113r_LNP = 0., Clequ1_2121r_LNP = 0., Clequ1_2122r_LNP = 0., Clequ1_2123r_LNP = 0., Clequ1_2131r_LNP = 0., Clequ1_2132r_LNP = 0., Clequ1_2133r_LNP = 0.,
7616 Clequ1_2211r_LNP = 0., Clequ1_2212r_LNP = 0., Clequ1_2213r_LNP = 0., Clequ1_2221r_LNP = 0., Clequ1_2222r_LNP = 0., Clequ1_2223r_LNP = 0., Clequ1_2231r_LNP = 0., Clequ1_2232r_LNP = 0., Clequ1_2233r_LNP = 0.,
7617 Clequ1_2311r_LNP = 0., Clequ1_2312r_LNP = 0., Clequ1_2313r_LNP = 0., Clequ1_2321r_LNP = 0., Clequ1_2322r_LNP = 0., Clequ1_2323r_LNP = 0., Clequ1_2331r_LNP = 0., Clequ1_2332r_LNP = 0., Clequ1_2333r_LNP = 0.,
7618 Clequ1_3111r_LNP = 0., Clequ1_3112r_LNP = 0., Clequ1_3113r_LNP = 0., Clequ1_3121r_LNP = 0., Clequ1_3122r_LNP = 0., Clequ1_3123r_LNP = 0., Clequ1_3131r_LNP = 0., Clequ1_3132r_LNP = 0., Clequ1_3133r_LNP = 0.,
7619 Clequ1_3211r_LNP = 0., Clequ1_3212r_LNP = 0., Clequ1_3213r_LNP = 0., Clequ1_3221r_LNP = 0., Clequ1_3222r_LNP = 0., Clequ1_3223r_LNP = 0., Clequ1_3231r_LNP = 0., Clequ1_3232r_LNP = 0., Clequ1_3233r_LNP = 0.,
7620 Clequ1_3311r_LNP = 0., Clequ1_3312r_LNP = 0., Clequ1_3313r_LNP = 0., Clequ1_3321r_LNP = 0., Clequ1_3322r_LNP = 0., Clequ1_3323r_LNP = 0., Clequ1_3331r_LNP = 0., Clequ1_3332r_LNP = 0., Clequ1_3333r_LNP = 0.;
7621 double Clequ1_1111i_LNP = 0., Clequ1_1112i_LNP = 0., Clequ1_1113i_LNP = 0., Clequ1_1121i_LNP = 0., Clequ1_1122i_LNP = 0., Clequ1_1123i_LNP = 0., Clequ1_1131i_LNP = 0., Clequ1_1132i_LNP = 0., Clequ1_1133i_LNP = 0.,
7622 Clequ1_1211i_LNP = 0., Clequ1_1212i_LNP = 0., Clequ1_1213i_LNP = 0., Clequ1_1221i_LNP = 0., Clequ1_1222i_LNP = 0., Clequ1_1223i_LNP = 0., Clequ1_1231i_LNP = 0., Clequ1_1232i_LNP = 0., Clequ1_1233i_LNP = 0.,
7623 Clequ1_1311i_LNP = 0., Clequ1_1312i_LNP = 0., Clequ1_1313i_LNP = 0., Clequ1_1321i_LNP = 0., Clequ1_1322i_LNP = 0., Clequ1_1323i_LNP = 0., Clequ1_1331i_LNP = 0., Clequ1_1332i_LNP = 0., Clequ1_1333i_LNP = 0.,
7624 Clequ1_2111i_LNP = 0., Clequ1_2112i_LNP = 0., Clequ1_2113i_LNP = 0., Clequ1_2121i_LNP = 0., Clequ1_2122i_LNP = 0., Clequ1_2123i_LNP = 0., Clequ1_2131i_LNP = 0., Clequ1_2132i_LNP = 0., Clequ1_2133i_LNP = 0.,
7625 Clequ1_2211i_LNP = 0., Clequ1_2212i_LNP = 0., Clequ1_2213i_LNP = 0., Clequ1_2221i_LNP = 0., Clequ1_2222i_LNP = 0., Clequ1_2223i_LNP = 0., Clequ1_2231i_LNP = 0., Clequ1_2232i_LNP = 0., Clequ1_2233i_LNP = 0.,
7626 Clequ1_2311i_LNP = 0., Clequ1_2312i_LNP = 0., Clequ1_2313i_LNP = 0., Clequ1_2321i_LNP = 0., Clequ1_2322i_LNP = 0., Clequ1_2323i_LNP = 0., Clequ1_2331i_LNP = 0., Clequ1_2332i_LNP = 0., Clequ1_2333i_LNP = 0.,
7627 Clequ1_3111i_LNP = 0., Clequ1_3112i_LNP = 0., Clequ1_3113i_LNP = 0., Clequ1_3121i_LNP = 0., Clequ1_3122i_LNP = 0., Clequ1_3123i_LNP = 0., Clequ1_3131i_LNP = 0., Clequ1_3132i_LNP = 0., Clequ1_3133i_LNP = 0.,
7628 Clequ1_3211i_LNP = 0., Clequ1_3212i_LNP = 0., Clequ1_3213i_LNP = 0., Clequ1_3221i_LNP = 0., Clequ1_3222i_LNP = 0., Clequ1_3223i_LNP = 0., Clequ1_3231i_LNP = 0., Clequ1_3232i_LNP = 0., Clequ1_3233i_LNP = 0.,
7629 Clequ1_3311i_LNP = 0., Clequ1_3312i_LNP = 0., Clequ1_3313i_LNP = 0., Clequ1_3321i_LNP = 0., Clequ1_3322i_LNP = 0., Clequ1_3323i_LNP = 0., Clequ1_3331i_LNP = 0., Clequ1_3332i_LNP = 0., Clequ1_3333i_LNP = 0.;
7630 double Clequ3_1111r_LNP = 0., Clequ3_1112r_LNP = 0., Clequ3_1113r_LNP = 0., Clequ3_1121r_LNP = 0., Clequ3_1122r_LNP = 0., Clequ3_1123r_LNP = 0., Clequ3_1131r_LNP = 0., Clequ3_1132r_LNP = 0., Clequ3_1133r_LNP = 0.,
7631 Clequ3_1211r_LNP = 0., Clequ3_1212r_LNP = 0., Clequ3_1213r_LNP = 0., Clequ3_1221r_LNP = 0., Clequ3_1222r_LNP = 0., Clequ3_1223r_LNP = 0., Clequ3_1231r_LNP = 0., Clequ3_1232r_LNP = 0., Clequ3_1233r_LNP = 0.,
7632 Clequ3_1311r_LNP = 0., Clequ3_1312r_LNP = 0., Clequ3_1313r_LNP = 0., Clequ3_1321r_LNP = 0., Clequ3_1322r_LNP = 0., Clequ3_1323r_LNP = 0., Clequ3_1331r_LNP = 0., Clequ3_1332r_LNP = 0., Clequ3_1333r_LNP = 0.,
7633 Clequ3_2111r_LNP = 0., Clequ3_2112r_LNP = 0., Clequ3_2113r_LNP = 0., Clequ3_2121r_LNP = 0., Clequ3_2122r_LNP = 0., Clequ3_2123r_LNP = 0., Clequ3_2131r_LNP = 0., Clequ3_2132r_LNP = 0., Clequ3_2133r_LNP = 0.,
7634 Clequ3_2211r_LNP = 0., Clequ3_2212r_LNP = 0., Clequ3_2213r_LNP = 0., Clequ3_2221r_LNP = 0., Clequ3_2222r_LNP = 0., Clequ3_2223r_LNP = 0., Clequ3_2231r_LNP = 0., Clequ3_2232r_LNP = 0., Clequ3_2233r_LNP = 0.,
7635 Clequ3_2311r_LNP = 0., Clequ3_2312r_LNP = 0., Clequ3_2313r_LNP = 0., Clequ3_2321r_LNP = 0., Clequ3_2322r_LNP = 0., Clequ3_2323r_LNP = 0., Clequ3_2331r_LNP = 0., Clequ3_2332r_LNP = 0., Clequ3_2333r_LNP = 0.,
7636 Clequ3_3111r_LNP = 0., Clequ3_3112r_LNP = 0., Clequ3_3113r_LNP = 0., Clequ3_3121r_LNP = 0., Clequ3_3122r_LNP = 0., Clequ3_3123r_LNP = 0., Clequ3_3131r_LNP = 0., Clequ3_3132r_LNP = 0., Clequ3_3133r_LNP = 0.,
7637 Clequ3_3211r_LNP = 0., Clequ3_3212r_LNP = 0., Clequ3_3213r_LNP = 0., Clequ3_3221r_LNP = 0., Clequ3_3222r_LNP = 0., Clequ3_3223r_LNP = 0., Clequ3_3231r_LNP = 0., Clequ3_3232r_LNP = 0., Clequ3_3233r_LNP = 0.,
7638 Clequ3_3311r_LNP = 0., Clequ3_3312r_LNP = 0., Clequ3_3313r_LNP = 0., Clequ3_3321r_LNP = 0., Clequ3_3322r_LNP = 0., Clequ3_3323r_LNP = 0., Clequ3_3331r_LNP = 0., Clequ3_3332r_LNP = 0., Clequ3_3333r_LNP = 0.;
7639 double Clequ3_1111i_LNP = 0., Clequ3_1112i_LNP = 0., Clequ3_1113i_LNP = 0., Clequ3_1121i_LNP = 0., Clequ3_1122i_LNP = 0., Clequ3_1123i_LNP = 0., Clequ3_1131i_LNP = 0., Clequ3_1132i_LNP = 0., Clequ3_1133i_LNP = 0.,
7640 Clequ3_1211i_LNP = 0., Clequ3_1212i_LNP = 0., Clequ3_1213i_LNP = 0., Clequ3_1221i_LNP = 0., Clequ3_1222i_LNP = 0., Clequ3_1223i_LNP = 0., Clequ3_1231i_LNP = 0., Clequ3_1232i_LNP = 0., Clequ3_1233i_LNP = 0.,
7641 Clequ3_1311i_LNP = 0., Clequ3_1312i_LNP = 0., Clequ3_1313i_LNP = 0., Clequ3_1321i_LNP = 0., Clequ3_1322i_LNP = 0., Clequ3_1323i_LNP = 0., Clequ3_1331i_LNP = 0., Clequ3_1332i_LNP = 0., Clequ3_1333i_LNP = 0.,
7642 Clequ3_2111i_LNP = 0., Clequ3_2112i_LNP = 0., Clequ3_2113i_LNP = 0., Clequ3_2121i_LNP = 0., Clequ3_2122i_LNP = 0., Clequ3_2123i_LNP = 0., Clequ3_2131i_LNP = 0., Clequ3_2132i_LNP = 0., Clequ3_2133i_LNP = 0.,
7643 Clequ3_2211i_LNP = 0., Clequ3_2212i_LNP = 0., Clequ3_2213i_LNP = 0., Clequ3_2221i_LNP = 0., Clequ3_2222i_LNP = 0., Clequ3_2223i_LNP = 0., Clequ3_2231i_LNP = 0., Clequ3_2232i_LNP = 0., Clequ3_2233i_LNP = 0.,
7644 Clequ3_2311i_LNP = 0., Clequ3_2312i_LNP = 0., Clequ3_2313i_LNP = 0., Clequ3_2321i_LNP = 0., Clequ3_2322i_LNP = 0., Clequ3_2323i_LNP = 0., Clequ3_2331i_LNP = 0., Clequ3_2332i_LNP = 0., Clequ3_2333i_LNP = 0.,
7645 Clequ3_3111i_LNP = 0., Clequ3_3112i_LNP = 0., Clequ3_3113i_LNP = 0., Clequ3_3121i_LNP = 0., Clequ3_3122i_LNP = 0., Clequ3_3123i_LNP = 0., Clequ3_3131i_LNP = 0., Clequ3_3132i_LNP = 0., Clequ3_3133i_LNP = 0.,
7646 Clequ3_3211i_LNP = 0., Clequ3_3212i_LNP = 0., Clequ3_3213i_LNP = 0., Clequ3_3221i_LNP = 0., Clequ3_3222i_LNP = 0., Clequ3_3223i_LNP = 0., Clequ3_3231i_LNP = 0., Clequ3_3232i_LNP = 0., Clequ3_3233i_LNP = 0.,
7647 Clequ3_3311i_LNP = 0., Clequ3_3312i_LNP = 0., Clequ3_3313i_LNP = 0., Clequ3_3321i_LNP = 0., Clequ3_3322i_LNP = 0., Clequ3_3323i_LNP = 0., Clequ3_3331i_LNP = 0., Clequ3_3332i_LNP = 0., Clequ3_3333i_LNP = 0.;
7651 double eggFint = 0.;
7652 double eggFpar = 0.;
7653 double ettHint = 0.;
7654 double ettHpar = 0.;
7655 double eVBFint = 0.;
7656 double eVBFpar = 0.;
7661 double eeeWBFint = 0.;
7662 double eeeWBFpar = 0.;
7663 double eeeZHint = 0.;
7664 double eeeZHpar = 0.;
7665 double eeettHint = 0.;
7666 double eeettHpar = 0.;
7667 double eepWBFint = 0.;
7668 double eepWBFpar = 0.;
7669 double eepZBFint = 0.;
7670 double eepZBFpar = 0.;
7671 double eHggint = 0.;
7672 double eHggpar = 0.;
7673 double eHWWint = 0.;
7674 double eHWWpar = 0.;
7675 double eHZZint = 0.;
7676 double eHZZpar = 0.;
7677 double eHZgaint = 0.;
7678 double eHZgapar = 0.;
7679 double eHgagaint = 0.;
7680 double eHgagapar = 0.;
7681 double eHmumuint = 0.;
7682 double eHmumupar = 0.;
7683 double eHtautauint = 0.;
7684 double eHtautaupar = 0.;
7685 double eHccint = 0.;
7686 double eHccpar = 0.;
7687 double eHssint = 0.;
7688 double eHsspar = 0.;
7689 double eHbbint = 0.;
7690 double eHbbpar = 0.;
7693 double eeeWWint = 0., edeeWWdcint = 0.;
7695 double eggFHgaga = 0., eggFHZga = 0., eggFHZZ = 0., eggFHWW = 0., eggFHtautau = 0., eggFHbb = 0., eggFHmumu = 0.;
7696 double eVBFHgaga = 0., eVBFHZga = 0., eVBFHZZ = 0., eVBFHWW = 0., eVBFHtautau = 0., eVBFHbb = 0., eVBFHmumu = 0.;
7697 double eWHgaga = 0., eWHZga = 0., eWHZZ = 0., eWHWW = 0., eWHtautau = 0., eWHbb = 0., eWHmumu = 0.;
7698 double eZHgaga = 0., eZHZga = 0., eZHZZ = 0., eZHWW = 0., eZHtautau = 0., eZHbb = 0., eZHmumu = 0.;
7699 double ettHgaga = 0., ettHZga = 0., ettHZZ = 0., ettHWW = 0., ettHtautau = 0., ettHbb = 0., ettHmumu = 0.;
7700 double eVBFHinv = 0., eVHinv = 0.;
7702 double eHwidth = 0.;
7715 double v2_over_LambdaNP2;
7730 double lambdaH_tree;
7750 double dZH, dZH1, dZH2;
7760 double cAsch, cWsch;
7763 double Yuku,Yukc,Yukt;
7768 double aiG, ai3G, ai2G;
7769 double aiT, aiH, aiWW, aiB, aiHW, aiHB;
7771 double aiHQ, aipHQ, aiHL, aipHL, aiHu, aiHd, aiHe;
7775 double dGammaHTotR1, dGammaHTotR2, GammaHTotR;
7791 double CHq1EWuu = 0., CHq1EWcc = 0., CHq1EWtt = 0.;
7792 double CHq3EWuu = 0., CHq3EWcc = 0., CHq3EWtt = 0.;
7793 double CHuEWuu = 0., CHuEWcc = 0., CHuEWtt = 0.;
7795 double CHq1EWdd = 0., CHq1EWss = 0., CHq1EWbb = 0.;
7796 double CHq3EWdd = 0., CHq3EWss = 0., CHq3EWbb = 0.;
7797 double CHdEWdd = 0., CHdEWss = 0., CHdEWbb = 0.;
7799 gslpp::complex CHq3EWud = gslpp::complex(0., 0.,
false), CHq3EWcs = gslpp::complex(0., 0.,
false), CHq3EWtb = gslpp::complex(0., 0.,
false);
8008 double CHF1_diag(
const Particle F)
const;
8015 double CHF3_diag(
const Particle F)
const;
8022 gslpp::complex CHF3CC_diag(
const Particle F)
const;
8029 double CHf_diag(
const Particle f)
const;
8036 gslpp::complex CHud_diag(
const Particle u)
const;
8043 gslpp::complex CfH_diag(
const Particle f)
const;
8050 gslpp::complex CfG_diag(
const Particle f)
const;
8057 gslpp::complex CfW_diag(
const Particle f)
const;
8064 gslpp::complex CfB_diag(
const Particle f)
const;
8076 gslpp::complex CfH_diag_mu(
const Particle f,
const double mu)
const;
8081 RGESolver SMEFTEvolEW;
8083 RGESolver SMEFTEvolMH, SMEFTEvol240, SMEFTEvol365, SMEFTEvol550, SMEFTEvol1000, SMEFTEvol1500, SMEFTEvol3000, SMEFTEvol5000;
8085 RGESolver SMEFTEvolUV;
8089 double tmu2 = 0., tmu3 = 0., tmu4 = 0., tmu5 = 0., tmuw = 0.;
8093 gslpp::matrix<gslpp::complex> VuL, VuLd, VuR, VuRd, VdL, VdLd, VdR, VdRd, VeL, VeLd, VeR, VeRd, MUQ, MDQ;
8096 bool FlagQuadraticTerms;
8099 bool FlagLoopH3d6Quad;
8101 bool FlagmultiScaleRGE;
8104 bool FlagCorrsInSMRunning;
8106 gsl_integration_cquad_workspace * w_WW;
8107 double ZeroAle(
double *dAle5h,
double *params);
8108 bool isSMInitialConditionComputed;
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
An observable class for the combinations of coefficients of the Warsaw basis constrained by EWPO.
std::string name
The name of the model.
A model class for new physics in the form of the dimension-six effective Lagrangian.
virtual const double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
virtual const double deltamt2() const
The relative correction to the mass of the quark squared, , with respect to ref. point used in the S...
virtual const double STXS12_ttH_pTH300_Inf(const double sqrt_s) const
The STXS bin , .
const double deltaGammaH4eRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double muTHUggHZgamumu(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
const double deltaGammaH4fNCRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double alphaMz() const
The electromagnetic coupling at the -mass scale.
virtual const double BrHudduRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double delta_sigmaTot_ee(const double pol_e, const double pol_p, const double s) const
virtual const double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
virtual gslpp::complex deltaGL_Wff(const Particle pbar, const Particle p) const
New physics contribution to the charged current coupling .
virtual const double deltadxsdcoseeWWlvjjLEP2(const double sqrt_s, const int bin) const
The new physics contribution to the differential cross section in pb for , with for the 4 bins defi...
const double deltaGammaH2l2vRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double cHt_TWG(const double mu) const
virtual const double muVBFHZZ4l(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double deltaG_hAA() const
The new physics contribution to the coupling of the effective interaction .
const double GammaHLvvLRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double muttHZbbboost(const double sqrt_s) const
The ratio in the channel in the current model and in the Standard Model.
virtual const double muTHUWHWW2l2v(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
const double deltaGammaHbbRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaHll_vvorjjRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double deltaG_hggRatio_mu(const double mu) const
The full new physics contribution to the coupling of the effective interaction , including new local ...
const double deltaGammaHWlvRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double STXS12_qqHqq_mjj60_120_Nj2(const double sqrt_s) const
The STXS bin , .
const double deltaMRL2t_e(const double s, const double t) const
const double GammaH2evRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double del_A_mu(const double mu) const
Correction to photon WF.
virtual const double delQ_gNC(const double mu) const
Separate, charge-proportional, indirect correction to EW neutral currents.
virtual const double BrH4eRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double STXS_ggH_VBFtopo_j3v(const double sqrt_s) const
The STXS bin .
virtual const double muVBFHZZ(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double muTHUWHmumu(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
virtual const double muTHUttHgaga(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into 2 photons in the curre...
virtual const double deltaA_f(const Particle f) const
The new physics contribution to the left-right asymmetry in at the -pole, .
const double deltaGammaHZmumuRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
virtual const double STXS_qqHqq_VHtopo(const double sqrt_s) const
The STXS bin .
virtual const double STXS12_ggH_pTH10_Inf_Nj0(const double sqrt_s) const
The STXS bin , .
virtual const double BrH2v2uRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double GammaHssRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double cQq18_TWG(const double mu) const
virtual const double STXS_ggH1j_pTH_60_120(const double sqrt_s) const
The STXS bin .
virtual const double muWHpT250(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
const double tovers2(const double cosmin, const double cosmax) const
const double CeeLR_charm(const double mu) const
virtual const double cQe_TWG(const double mu) const
virtual const double ctW_TWG(const double mu) const
virtual const double STXS12_qqHqq_mjj0_60_Nj2(const double sqrt_s) const
The STXS bin , .
const double deltaGammaH4fRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double STXS_ggH2j_pTH_200(const double sqrt_s) const
The STXS bin .
virtual const double deltaG_hhhRatio_mu(const double mu) const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
const double deltaGammaH2d2dRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaHWjjRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double CeeLR_mu(const double mu) const
virtual const double delU_gNC(const double mu) const
Universal indirect correction to EW neutral currents.
const double CeeLR_tau(const double mu) const
virtual const double CEWHe11(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
NPSMEFTd6General()
Constructor.
virtual const double cQlP_TWG(const double mu) const
virtual const double cHb_TWG(const double mu) const
virtual bool PostUpdate()
The post-update method for NPSMEFTd6General.
virtual const double STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double muttHbb(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
virtual const double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
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 in...
virtual const double STXS12_ggH_mjj0_350_pTH120_200_Nj2(const double sqrt_s) const
The STXS bin , .
const double deltaGammaH4fNCRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double STXS_ZHqqHqq_VBFtopo_j3(const double sqrt_s) const
The STXS bin .
virtual const double delta_muttH_1(const double sqrt_s) const
The SMEFT linear correction to the ratio between the t-tbar-Higgs associated production cross-sectio...
const double deltaGammaHWW4fRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
virtual const double STXS12_ggH_pTH450_650(const double sqrt_s) const
The STXS bin , .
virtual const double mummH(const double sqrt_s) const
The ratio between the production cross-section in the current model and in the Standard Model.
virtual const double STXS12_qqHqq_Nj1(const double sqrt_s) const
The STXS bin , .
virtual const double BrHvisRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double BrHZgaeeRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double delta_TauLFU_gtaugmu() const
The computation of the correction to the LFU ratio .
virtual const double mueeWBF(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the production cross-section in the current model and in the Standard Model.
const double deltag3G() const
The new physics contribution to the coupling of the effective interaction .
gslpp::complex deltaG_Aff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
virtual const double muZHgaga(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into 2 photons in the curren...
virtual const double deltaMz2() const
The relative correction to the mass of the boson squared, , with respect to ref. point used in the S...
const double GammaHZffRatio() const
The ratio of the , with any fermion, in the current model and in the Standard Model.
virtual const double bPskPol(const double sqrt_s, const double Pol_em, const double Pol_ep) const
the angular parameter from (arXiv:1708.09079 [hep-ph]).
virtual const double intDMLR2ets2(const double s, const double t0, const double t1) const
virtual const double BrH4muRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double deltaGammaHffRatio1(const double mf, const double CifH) const
The ratio of the in the current model and in the Standard Model.
const double deltaGammaHmumuRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
virtual const double delta_muVBF_1(const double sqrt_s) const
The SMEFT linear correction to the ratio between the vector-boson fusion Higgs production cross-sect...
virtual const double STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double muWHZga(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
virtual const double delta_mutH_1(const double sqrt_s) const
The SMEFT linear correction to the ratio between the t-Higgs associated production cross-section in ...
virtual const double BrHmumuRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double cHtb_TWG(const double mu) const
virtual const double muWHtautau(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
virtual const double STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double deltaGammaTotalRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double delta_muVBF_2(const double sqrt_s) const
The SMEFT quadratic correction to the ratio between the vector-boson fusion Higgs production cross-s...
virtual const double BrHWWRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double CeeLL_e(const double mu) const
virtual const double muttHgaga(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into 2 photons in the curre...
virtual const double BrH4uRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double obliqueU() const
The oblique parameter .
const double deltaGammaHLvvLRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double delta_muggH_1(const double sqrt_s) const
The SMEFT linear correction to the ratio between the gluon-gluon fusion Higgs production cross-secti...
virtual const double delta_muVH_1(const double sqrt_s) const
The SMEFT linear correction to the ratio between the Z-Higgs and W-Higgs associated production cross...
const double GammaHWffRatio() const
The ratio of the , with any fermion, in the current model and in the Standard Model.
virtual const double deltaGmu2() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
const double deltaGR_f(const Particle p) const
New physics contribution to the neutral-current right-handed coupling .
virtual const double Gamma_Zf(const Particle f) const
The decay width of the boson into a given fermion pair, .
virtual const double deltaSigmaHadron() const
The new physics contribution to the cross section for the process at the pole, .
const double deltaGammaHffRatio2(const double mf, const double CifH) const
The new physics contribution to the ratio of the in the current model and in the Standard Model at ...
virtual const double muggHpttH(const double sqrt_s) const
The ratio between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section...
virtual const double BrH2udRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double muttHZZ(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
const double deltaGammaHlvjjRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double delta_muZH_2(const double sqrt_s) const
The SMEFT quadratic correction to the ratio between the Z-Higgs associated production cross-section ...
gslpp::complex deltaGL_Wffh(const Particle pbar, const Particle p) const
The new physics contribution to the coupling of the effective interaction .
virtual const double STXS12_qqHlv_pTV0_75(const double sqrt_s) const
The STXS bin , .
virtual const double muTHUVHBRinv(const double sqrt_s) const
The ratio between the VH production cross-section in the current model and in the Standard Model,...
const double deltaGammaH4fCCRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaH2v2vRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
gslpp::complex deltaG_hGff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
virtual const double muTHUZHZZ4l(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
virtual const double deltays_HB(const double mu) const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
const double GammaH2u2dRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double muZHtautau(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
virtual const double muTHUWHZZ4l(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
virtual const double STXS12_ggH_mjj0_350_pTH0_60_Nj2(const double sqrt_s) const
The STXS bin , .
const double CeeRR_charm(const double mu) const
const double GammaHggRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double mueeZHPol(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the associated production cross-section in the current model and in the Standard ...
virtual const double STXS_ttHtH(const double sqrt_s) const
The STXS bin .
virtual const double BrHevmuvRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double cZZ_HB(const double mu) const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
const double deltaGammaH4lRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double ctt1_TWG(const double mu) const
virtual const double DeltaOWtoalph(const double dOSMdMW, const double mu) const
Difference in prediction in scheme and W mass scheme, computed from observable in W mass scheme....
virtual const double BrHlv_lvorjjRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double deltaGamma_W() const
The new physics contribution to the total decay width of the boson, .
const double GammaH2L2v2Ratio() const
The ratio of the ( ) in the current model and in the Standard Model.
const double deltaGammaHZgaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double BrH4dRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double deltaGammaHZZ4muRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaHggRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaHZZ4uRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double delta_muWH_2(const double sqrt_s) const
The SMEFT quadratic correction to the ratio between the W-Higgs associated production cross-section ...
virtual const double BrHZgamumuRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double CeeLL_charm(const double mu) const
const double CeeRL_tau(const double mu) const
virtual const double deltag1ZNP(const double mu) const
The new physics contribution to the anomalous triple gauge coupling .
virtual const double BrH2v2vRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double BrH4vRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double BrHll_vvorjjRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double muttHWW2l2v(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
virtual const double BrHZuuRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double muttHZZ4l(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
virtual const double STXS_qqHlv_pTV_0_250(const double sqrt_s) const
The STXS bin .
virtual const double BrH2evRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double CeeLL_mu(const double mu) const
virtual const double mupTVppWZ(const double sqrt_s, const double pTV1, const double pTV2) const
The number of events in in a given bin, normalized to the SM prediction. From arXiv: 1712....
virtual const double delta_mubbH_1(const double sqrt_s) const
The SMEFT linear correction to the ratio between the bbH production cross-section in the current mod...
virtual const double delta_muZH_1(const double sqrt_s) const
The SMEFT linear correction to the ratio between the Z-Higgs associated production cross-section in ...
virtual const double STXS12_ggH_pTH200_300_Nj01(const double sqrt_s) const
The STXS bin , .
virtual const double BrH2d2dRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double CeeLR_strange(const double mu) const
virtual const double CEWHQ333(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
virtual const double delta_gLnuN2() const
The computation of the correction to the effective neutrino nucleon LH coupling: delta_gLnuN2.
const double deltaGammaH4LRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double deltaMwd62() const
The relative NP corrections to the mass of the boson squared, .
virtual const double muggHZga(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
virtual const double deltaG2_hZA_mu(const double mu) const
The new physics contribution to the coupling of the effective interaction .
const double GammaHevmuvRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double BrHZZRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double Mw() const
The mass of the boson, .
virtual const double ctd8_TWG(const double mu) const
virtual const double ctq1_TWG(const double mu) const
virtual const double CEWHQd33(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
virtual const double CEWHQ311(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
const double deltaGammaHevmuvRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaH2e2vRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double STXS_ggH1j_pTH_0_60(const double sqrt_s) const
The STXS bin .
const double GammaHZZ4muRatio() const
The ratio of the in the current model and in the Standard Model.
static const int NNPSMEFTd6GeneralVars
The number of the model parameters in NPSMEFTd6General (including the 18 parameters needed for the SM...
virtual const double muTHUZHtautau(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
const double deltaGammaH2L2LRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double mummHvv(const double sqrt_s) const
The ratio between the production cross-section in the current model and in the Standard Model.
virtual const double BrHZffRatio() const
The ratio of the Br , with any fermion, in the current model and in the Standard Model.
const double CeeRL_mu(const double mu) const
virtual const double STXS_qqHlv_pTV_150_250_1j(const double sqrt_s) const
The STXS bin .
virtual const double BrHWW4fRatio() const
The ratio of the Br , with any fermion, in the current model and in the Standard Model.
virtual const double delta_Qwp() const
The computation of the proton weak charge: Qwp.
const double deltaGammaH2v2vRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double STXS12_BrH4lRatio() const
The STXS BR , .
virtual const double muZHZZ4l(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
virtual const double CEWHQu33(const double mu) const
Combination of coefficients of the Warsaw basis not constrained by EWPO (at LO) .
virtual const double cQq31_TWG(const double mu) const
virtual const double deltaG_hggRatio() const
The full new physics contribution to the coupling of the effective interaction , including new local ...
const double GammaHZZ2e2muRatio() const
The ratio of the in the current model and in the Standard Model.
const double deltaGammaH4dRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double delta_sigma_had(const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const
const double deltaGammaH2u2dRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaH2evRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double muTHUttHZZ4l(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
const double deltaGammaHWW4jRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaMLL2_f(const Particle f, const double s, const double t) const
virtual const double deltaKgammaNPEff() const
The new physics contribution to the effective anomalous triple gauge coupling from arXiv: 1708....
const double deltaGammaHZvvRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaH2d2dRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double delta_TauLFU_gtaugmuPi() const
The computation of the correction to the LFU ratio .
virtual const double STXS_WHqqHqq_VH2j(const double sqrt_s) const
The STXS bin .
virtual const double STXS12_ggH_mjj0_350_pTH0_60_Nj1(const double sqrt_s) const
The STXS bin , .
virtual const double muTHUttHZZ(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
virtual const double RZlilj(const Particle li, const Particle lj) const
The lepton universality ratio .
virtual const double deltaG2_hZZ_mu(const double mu) const
The new physics contribution to the coupling of the effective interaction .
virtual const double cQd1_TWG(const double mu) const
virtual const double muggHmumu(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
virtual const double muWHmumu(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
virtual const double deltamtau2() const
The relative correction to the mass of the lepton squared, , with respect to ref....
virtual const double STXS_ZHqqHqq_Rest(const double sqrt_s) const
The STXS bin .
virtual const double muTHUVBFHgaga(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into 2 photons in the...
virtual const double deltacZ_HB(const double mu) const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual const double delta_sigma_ee(const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const
const double GammaHZZ4dRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double cHQp_TWG(const double mu) const
virtual const double STXS12_qqHlv_pTV150_250_Nj0(const double sqrt_s) const
The STXS bin , .
virtual const double STXS_WHqqHqq_Rest(const double sqrt_s) const
The STXS bin .
virtual const double BrHZZ4fRatio() const
The ratio of the Br , with any fermion, in the current model and in the Standard Model.
virtual const double CEWHu33(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
virtual const double mueeHvv(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the associated production cross-section in the current model and in the Standard ...
const double deltaGammaH2L2dRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double STXS_ZHqqHqq_VH2j(const double sqrt_s) const
The STXS bin .
virtual const double muTHUVHZZ4l(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
const double deltaGR_Zffh(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
virtual const double STXS12_ggHll_pTV250_Inf(const double sqrt_s) const
The STXS bin , .
const double deltaGammaH2Lv2Ratio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
const double GammaH2v2vRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double STXS12_qqHqq_mjj120_350_Nj2(const double sqrt_s) const
The STXS bin , .
gslpp::complex deltaG_Zff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
virtual const double dxsdcoseeWWlvjjLEP2(const double sqrt_s, const int bin) const
The differential cross section in pb for , with for the 4 bins defined in arXiv: 1606....
const double deltaGammaHZZ2e2muRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double mueeZH(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the associated production cross-section in the current model and in the Standard ...
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
const double deltaGammaHgagaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double muTHUVHinv(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into invisible states in the...
const double GammaHZZ4lRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double STXS_ZHqqHqq_VBFtopo_j3v(const double sqrt_s) const
The STXS bin .
virtual const double deltaG_hAA_mu(const double mu) const
The new physics contribution to the coupling of the effective interaction .
virtual const double deltaMw2() const
The relative correction to the mass of the boson squared, , with respect to ref. point used in the S...
const double deltaGammaH4vRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double GammaH4eRatio() const
The ratio of the in the current model and in the Standard Model.
const double CeeLR_up(const double mu) const
const double GammaH2u2uRatio() const
The ratio of the in the current model and in the Standard Model.
const double GammaHWW4fRatio() const
The ratio of the , with any fermion, in the current model and in the Standard Model.
virtual const double muVHmumu(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
virtual const double BrH2u2dRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double muTHUWHWW(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
virtual const double mummttH(const double sqrt_s) const
The ratio between the production cross-section in the current model and in the Standard Model.
virtual const double intDMLL2eus2(const double s, const double t0, const double t1) const
virtual const double BrHssRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double muZHZga(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
virtual const double BrH2L2vRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
const double deltaGammaHZZ4dRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double muTHUVHWW(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
virtual const double muTHUttHWW2l2v(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
const double deltaGammaH2v2dRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaHWlvRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double CEWHL111(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
const double deltaGammaHZllRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
const double GammaHbbRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double sigma0_had() const
The cross section for the process at the pole, .
virtual const double deltaG1_hWW_mu(const double mu) const
The new physics contribution to the coupling of the effective interaction .
virtual const double STXS12_qqHlv_pTV400_Inf(const double sqrt_s) const
The STXS bin , .
virtual const double delta_muttH_2(const double sqrt_s) const
The SMEFT quadratic correction to the ratio between the t-tbar-Higgs associated production cross-sec...
const double GammaHlvjjRatio() const
The ratio of the ( \Gamma(H\to l l j j) \Gamma(H\to l l j j)_{\mathrm{SM}} \Gamma(H\to l l j j) l=e,...
virtual const double muTHUWHZZ(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
virtual const double muVHgaga(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into 2 photons in the curren...
const double deltaGammaHWffRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
const double GammaHZllRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double cQlM_TWG(const double mu) const
virtual const double BrH4LRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
const double deltaGammaH2l2vRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
const double GammaH2mu2vRatio() const
The ratio of the in the current model and in the Standard Model.
const double GammaHZZ4eRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double STXS12_ggH_pTH450_Inf(const double sqrt_s) const
The STXS bin , .
virtual const double muTHUZHbb(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
virtual const double Gamma_Z() const
The total decay width of the boson, .
virtual const double cQd8_TWG(const double mu) const
virtual const double STXS12_ggH_pTH60_120_Nj1(const double sqrt_s) const
The STXS bin , .
virtual const double BrH2muvRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double deltaGammaHZeeRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaH2udRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2(const double sqrt_s) const
The STXS bin , .
const double deltaGammaH2muvRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double deltaaSMZ2() const
The relative correction to the strong coupling constant at the Z pole, , with respect to ref....
virtual const double STXS12_qqHll_pTV400_Inf(const double sqrt_s) const
The STXS bin , .
const double GammaH2e2muRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double deltaeNP(const double mu) const
The new physics relative contribution to the EW coupling constant .
virtual const double mueeWW(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the production cross-section in the current model and in the Standard Model.
const double GammaH4fNCRatio() const
The ratio of the via NC in the current model and in the Standard Model.
const double GammaHZZ4vRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double BrHWjjRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double STXS12_qqHlv_pTV0_150(const double sqrt_s) const
The STXS bin , .
virtual const double deltaGamma_Zf(const Particle f) const
The new physics contribution to the decay width of the boson into a given fermion pair,...
virtual const double STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2(const double sqrt_s) const
The STXS bin , .
const double deltaGammaH2v2uRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaH4vRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double GammaHZuuRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
const double deltaGammaH2L2uRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double BrHVVRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double STXS_ggH2j_pTH_120_200(const double sqrt_s) const
The STXS bin .
const double deltaGammaH4dRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double muTHUVBFHZZ(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double kappaW4feff() const
The effective coupling .
virtual const double STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double STXS12_ggH_mjj350_700_pTH0_200_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double GammaW() const
The total width of the boson, .
virtual const double cgg_HB(const double mu) const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
const double deltaGammaHZZ4vRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double BrH2v2dRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double deltaGammaHWW2l2vRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double delta_TauLFU_gtauge() const
The computation of the correction to the LFU ratio .
virtual NPSMEFTd6GeneralMatching & getMatching() const
A method to get the Matching object for this model.
virtual const double CEWHd11(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
const double GammaH4dRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double deltaGwd62() const
The relative NP corrections to the width of the boson squared, .
virtual const double muTHUWHbb(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
virtual const double muVBFHtautau(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double STXS12_qqHll_pTV75_150(const double sqrt_s) const
The STXS bin , .
const double deltaGammaH2u2uRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double GammaHll_vvorjjRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
const double deltaGammaHZZ4lRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double STXS_qqHqq_VBFtopo_Rest(const double sqrt_s) const
The STXS bin .
const double deltaGammaHbbRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double deltamtau() const
The relative correction to the mass of the lepton, , with respect to ref. point used in the SM calcu...
const double deltaGammaHWjjRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaH4LRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double deltaGammaTotalRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double deltaa02() const
The relative correction to the electromagnetic constant at zero momentum, , with respect to ref....
virtual const double cQQ1_TWG(const double mu) const
virtual const double BrHgagaRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double STXS12_ggH_pTH200_300(const double sqrt_s) const
The STXS bin , .
virtual const double kappataueff() const
The effective coupling .
virtual const double deltaGzd62() const
The relative NP corrections to the width of the boson squared, .
virtual const double STXS12_ggHll_pTV75_150(const double sqrt_s) const
The STXS bin , .
const double deltaGammaHZZ4eRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double STXS12_qqHlv_pTV250_Inf(const double sqrt_s) const
The STXS bin , .
const double GammaH2e2vRatio() const
The ratio of the in the current model and in the Standard Model.
const double deltaGammaH2mu2vRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double GammaHZgaRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double muttHWW(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
virtual const double BrH2L2uRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double RWc() const
The ratio .
virtual const double deltaG3_hZZ() const
The new physics contribution to the coupling of the effective interaction .
virtual const double muggHZZ(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
const double GammaH2LvRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
const double deltaGammaH4uRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double xseeWW(const double sqrt_s) const
Total cross section in pb, with .
virtual const double muTHUggHZZ(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
virtual const double deltaGA_f(const Particle p) const
New physics contribution to the neutral-current axial-vector coupling .
virtual const double BrHZZ4eRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double muTHUVHmumu(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
virtual const double BrHccRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double CeeLR_top(const double mu) const
virtual const double Br_H_exo() const
The branching ratio of the of the Higgs into exotic particles.
virtual const double deltaG_hAARatio_mu(const double mu) const
The full new physics contribution to the coupling of the effective interaction , including new local ...
virtual const double STXS12_qqHqq_VH_veto_Nj01(const double sqrt_s) const
The STXS bin , VH-veto Ref. 2402.05742.
virtual const double mueeZHGen(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the associated production cross-section in the current model and in the Standard ...
const double deltaGammaH4muRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double deltaG1_hZARatio_mu(const double mu) const
The full new physics contribution to the coupling of the effective interaction , including new local ...
virtual const double STXS12_qqHlv_pTV75_150(const double sqrt_s) const
The STXS bin , .
const double CeeRR_strange(const double mu) const
virtual const double muVHbb(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
virtual const double BrH2l2vRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual gslpp::complex deltaG_hff_mu(const Particle p, const double mu) const
The new physics contribution to the coupling of the effective interaction .
virtual const double muWHZZ(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
const double CeeLR_e(const double mu) const
virtual const double cZga_HB(const double mu) const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual const double deltaGamma_Z() const
The new physics contribution to the total decay width of the boson, .
const double deltaGammaHLvudRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double STXS12_qqHlv_pTV150_250_Nj1(const double sqrt_s) const
The STXS bin , .
virtual const double muVHpT250(const double sqrt_s) const
The ratio between the WH+ZH associated production cross-section in the current model and in the Stan...
virtual const double deltag1gaNP(const double mu) const
The new physics contribution to the anomalous triple gauge coupling .
const double GammaHWW4jRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double ctlS_TWG(const double mu) const
virtual const double kappaseff() const
The effective coupling .
const double deltaGammaHWW2l2vRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double STXS_qqHll_pTV_150_250(const double sqrt_s) const
The STXS bin .
virtual const double BrHtoinvRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double mueeZqqHPol(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the associated production cross-section in the current model and in the Standard ...
virtual const double Br_H_inv_NP() const
The branching ratio of the of the Higgs into invisible particles (only invisible new particles).
virtual const double STXS_ggH0j(const double sqrt_s) const
The STXS bin .
const double deltaGammaHWW4jRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double uovers2(const double cosmin, const double cosmax) const
virtual const double muTHUVBFHZZ4l(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double cQl3_TWG(const double mu) const
const double CeeRR_e(const double mu) const
virtual const double CEWHL311(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
const double deltaGammaHlvjjRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
const double deltaGammaH2L2vRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double deltaG3_hWW_mu(const double mu) const
The new physics contribution to the coupling of the effective interaction .
const double deltaGammaH4eRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double CeeRR_down(const double mu) const
virtual const double BrHtautauRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double muTHUWHgaga(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into 2 photons in the curren...
const double GammaH4muRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double muttHtautau(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
virtual const double delta_TauLFU_gmuge() const
The computation of the correction to the LFU ratio .
virtual const double deltaG3_hZZ_mu(const double mu) const
The new physics contribution to the coupling of the effective interaction .
const double GammaHLvudRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
const double deltaGammaH2muvRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double BrH4fNCRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double STXS12_qqHqq_Nj0(const double sqrt_s) const
The STXS bin , .
const double deltaGammaHWffRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
virtual const double delta_gRnuN2() const
The computation of the correction to the effective neutrino nucleon RH coupling: delta_gRnuN2.
virtual bool setFlagStr(const std::string name, const std::string value)
A method to set a flag of NPSMEFTd6General.
virtual const double dxseeWWdcos(const double sqrt_s, const double cos) const
The differential distribution for , with , as a function of the polar angle.
const double deltaGammaH2mu2vRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
const double deltaGammaH2u2uRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double ctG_TWG(const double mu) const
virtual const double deltaGV_f(const Particle p) const
New physics contribution to the neutral-current vector coupling .
virtual const double BrH2L2v2Ratio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double muTHUZHWW2l2v(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
virtual const double BrHZZ4uRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double cgaga_HB(const double mu) const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual const double STXS12_ttH_pTH300_450(const double sqrt_s) const
The STXS bin , .
const double CeeRL_charm(const double mu) const
virtual const double CEWHQ122(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
const double GammaH2L2uRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double cZBox_HB(const double mu) const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual const double STXS12_ggH_mjj700_Inf_pTH0_200_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double BrHLvudRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double cte_TWG(const double mu) const
const double GammaH2Lv2Ratio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double BrHlvjjRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double deltaymu_HB(const double mu) const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual const double BrHLvvLRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
const double CeeRR_mu(const double mu) const
const double GammaH2v2dRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double BrHbbRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double deltaa0() const
The relative correction to the electromagnetic constant at zero momentum, , with respect to ref....
virtual const double deltaG2_hZA() const
The new physics contribution to the coupling of the effective interaction .
virtual const double delta_sigmaTot_f(const Particle f, const double pol_e, const double pol_p, const double s) const
gslpp::complex deltaG_hZff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
virtual const double STXS_WHqqHqq_pTj1_200(const double sqrt_s) const
The STXS bin .
virtual const double muTHUVBFHmumu(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double muTHUttHmumu(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
virtual gslpp::complex deltaG_hff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
virtual const double IctZ_TWG(const double mu) const
virtual const double muttHZga(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
const double deltaGammaH2L2vRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double muTHUggHtautau(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
virtual const double STXS12_ggH_mjj0_350_pTH60_120_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double cQt8_TWG(const double mu) const
virtual const double STXS12_BrHgagaRatio() const
The STXS BR .
virtual const double CEWHQ133(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
virtual const double muTHUVHgaga(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into 2 photons in the curren...
virtual const double STXS_ggH1j_pTH_120_200(const double sqrt_s) const
The STXS bin .
virtual const double delta_muggH_2(const double sqrt_s) const
The SMEFT quadratic correction to the ratio between the gluon-gluon fusion Higgs production cross-se...
virtual const double muggHWW2l2v(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
virtual const double delta_Qwn() const
The computation of the neutron weak charge: Qwn.
virtual const double cQq38_TWG(const double mu) const
virtual const double cQu1_TWG(const double mu) const
virtual const double CEWHL333(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
virtual const double muWHZZ4l(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
virtual const double STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double deltaytau_HB(const double mu) const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual const double deltaH3L1(double C1) const
The coefficient of the 1-loop linear term in the Higgs selfcoupling.
virtual const double muTHUttHZga(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
virtual const double STXS12_ggH_pTH120_200_Nj1(const double sqrt_s) const
The STXS bin , .
virtual const double deltaG1_hZZ_mu(const double mu) const
The new physics contribution to the coupling of the effective interaction .
virtual const double deltamb() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
virtual const double STXS_ggH_VBFtopo_j3(const double sqrt_s) const
The STXS bin .
virtual const double CEWHu11(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
const double deltaMRR2_f(const Particle f, const double s, const double t) const
virtual const double IctW_TWG(const double mu) const
virtual const double delta_muVH_2(const double sqrt_s) const
The SMEFT quadratic correction to the ratio between the Z-Higgs and W-Higgs associated production cr...
virtual const double delta_muWH_1(const double sqrt_s) const
The SMEFT linear correction to the ratio between the W-Higgs associated production cross-section in ...
virtual const double STXS12_qqHqq_mjj350_700_pTH0_200_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double muVHtautau(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
virtual const double muTHUggHmumu(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
virtual const double deltaGammaTotalRatio1noError() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double STXS_ggH1j_pTH_200(const double sqrt_s) const
The STXS bin .
virtual const double kappaAeff() const
The effective coupling .
const double GammaHudduRatio() const
The ratio of the in the current model and in the Standard Model.
const double deltaGammaHZeeRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double cHQm_TWG(const double mu) const
gslpp::complex deltaGR_Wffh(const Particle pbar, const Particle p) const
The new physics contribution to the coupling of the effective interaction .
virtual const double CEWHL133(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
virtual const double cHQ3_TWG(const double mu) const
static const std::string NPSMEFTd6GeneralVars[NNPSMEFTd6GeneralVars]
A string array containing the labels of the model parameters in NPSMEFTd6General.
virtual const double BrW(const Particle fi, const Particle fj) const
The branching ratio of the boson decaying into a SM fermion pair, .
const double GammaHmumuRatio() const
The ratio of the in the current model and in the Standard Model.
const double deltaGammaHZZ4fRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
const double GammaHZvvRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double STXS12_BrHevmuvRatio() const
The STXS BR .
virtual const double mubbH(const double sqrt_s) const
The ratio between the bbH production cross-section in the current model and in the Standard Model.
virtual const double muTHUVBFHWW(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double ppZHprobe(const double sqrt_s) const
The direction constrained by in the boosted regime, . From arXiv:1807.01796 and the contribution to ...
virtual const double mueeZqqH(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the associated production cross-section in the current model and in the Standard ...
const double GammaH4LRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
const double GammaHZZ4uRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double STXS12_qqHll_pTV150_250_Nj1(const double sqrt_s) const
The STXS bin , .
virtual gslpp::complex deltaGL_Wff_mu(const Particle pbar, const Particle p, const double mu) const
New physics contribution to the charged current coupling .
virtual const double BrHZvvRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double muggHWW(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
const double deltaGammaH2L2uRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double muggHgaga(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2...
virtual const double aPskPol(const double sqrt_s, const double Pol_em, const double Pol_ep) const
the angular parameter from (arXiv:1708.09079 [hep-ph]).
const double deltaGammaH2L2LRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double muTHUggHZga(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
virtual const double muttHmumu(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
virtual const double BrHZZ4muRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double BrHZddRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double STXS12_qqHll_pTV0_75(const double sqrt_s) const
The STXS bin , .
virtual const double STXS12_ggHll_pTV0_75(const double sqrt_s) const
The STXS bin , .
const double deltaGammaHudduRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaHlv_lvorjjRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double muepZBF(const double sqrt_s) const
The ratio between the production cross-section in the current model and in the Standard Model.
virtual const double deltaG_hgg_mu(const double mu) const
The new physics contribution to the coupling of the effective interaction .
const double deltaGammaH2L2v2Ratio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double BrH2e2muRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double BrH4L2Ratio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double delta_AFB_f(const Particle f, const double pol_e, const double pol_p, const double s) const
virtual const double kappamueff() const
The effective coupling .
const double GammaH2d2dRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double CEWHd22(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
virtual const double deltaMh2() const
The relative correction to the mass of the boson squared, , with respect to ref. point used in the S...
const double CeeLR_down(const double mu) const
const double deltaMLR2_f(const Particle f, const double s) const
virtual const double delta2sBRH3(const double C1prod, const double C1Hxx) const
Quadratic contribution from the Higgs self-couplings modifications to the signal strength for in the...
virtual const double kappaZAeff() const
The effective coupling .
const double CeeRL_down(const double mu) const
gslpp::complex deltaG_Gff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
virtual const double muTHUZHgaga(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into 2 photons in the curren...
virtual const double muVHWW2l2v(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
virtual const double STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double BrHWW4jRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double deltaGammaH2e2vRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaHWW4fRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
virtual const double muWHbb(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
const double GammaHtautauRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double deltayt_HB(const double mu) const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual const double Br_H_inv() const
The branching ratio of the of the Higgs into invisible particles.
virtual const double delta_gVnue() const
The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gV...
const double deltaGammaH4L2Ratio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double cQQ8_TWG(const double mu) const
virtual const double BrHZgallRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double cbW_TWG(const double mu) const
virtual const double STXS12_tH(const double sqrt_s) const
The STXS bin .
virtual const double deltamc2() const
The relative correction to the mass of the quark squared, , with respect to ref. point used in the S...
virtual const double BrHWffRatio() const
The ratio of the Br , with any fermion, in the current model and in the Standard Model.
virtual const double muVHZZ4l(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
virtual const double intDMRL2ets2(const double s, const double t0, const double t1) const
const double deltaGammaHZZ4vRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double cQu8_TWG(const double mu) const
virtual const double kappaZ4feff() const
The effective coupling .
virtual const double STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2(const double sqrt_s) const
The STXS bin , .
const double deltaGL_f_mu(const Particle p, const double mu) const
New physics contribution to the neutral-current left-handed coupling .
const double deltaGammaHgagaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double deltaG1_hZA() const
The new physics contribution to the coupling of the effective interaction .
virtual const double muVBFHWW2l2v(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double BrHZllRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
const double deltaGammaHZZ2e2muRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double ctu1_TWG(const double mu) const
virtual const double muTHUttHtautau(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
virtual const double STXS_ggH2j_pTH_0_200(const double sqrt_s) const
The STXS bin .
const double deltaGammaHZgaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double mueeZllHPol(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the associated production cross-section in the current model and in the Standard ...
virtual const double muVBFHmumu(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double muVBFgamma(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in association with a hard ...
virtual const double STXS12_ggHll_pTV150_250_Nj1(const double sqrt_s) const
The STXS bin , .
virtual const double lambz_HB(const double mu) const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual const double muWHWW(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
virtual const double muTHUggHZZ4mu(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
const double deltaGammaHmumuRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double STXS_qqHqq_VBFtopo_j3(const double sqrt_s) const
The STXS bin .
const double deltaGammaHZZ4uRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double muZHmumu(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
virtual const double delta2sH3(const double C1) const
Quadratic contribution from the Higgs self-couplings modifications to the signal strength for an obse...
virtual const double BrH2L2dRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double muTHUVBFBRinv(const double sqrt_s) const
The ratio between the VBF production cross-section in the current model and in the Standard Model,...
virtual const double STXS12_ggH_pTH10_200_Nj0(const double sqrt_s) const
The STXS bin , .
const double CeeLR_bottom(const double mu) const
virtual const double STXS_qqHlv_pTV_250(const double sqrt_s) const
The STXS bin .
const double GammaH4fRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double STXS12_qqHll_pTV250_400(const double sqrt_s) const
The STXS bin , .
virtual const double STXS_qqHlv_pTV_0_150(const double sqrt_s) const
The STXS bin .
virtual const double cQq11_TWG(const double mu) const
virtual const double DeltaGF() const
New physics contribution to the Fermi constant.
virtual const double muZHpT250(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
const double deltaGammaH2u2dRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double STXS12_BrHbbRatio() const
The STXS BR .
virtual const double BrHWW2l2vRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double deltaG1_hZZ() const
The new physics contribution to the coupling of the effective interaction .
virtual const double muTHUVHtautau(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
virtual const double deltaMw() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
virtual const double kappaceff() const
The effective coupling .
virtual const double deltamb2() const
The relative correction to the mass of the quark squared, , with respect to ref. point used in the S...
virtual gslpp::complex deltaGR_Wff_mu(const Particle pbar, const Particle p, const double mu) const
New physics contribution to the charged current coupling .
const double CeeLL_down(const double mu) const
virtual const double RWlilj(const Particle li, const Particle lj) const
The lepton universality ratio .
const double deltaGammaHZZ4eRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaH4muRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double Dalpha5hMz() const
The 5-quark contribution to the running of the em constant to the pole. .
virtual const double muTHUggHgaga(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2...
virtual const double STXS_qqHqq_VBFtopo_j3v(const double sqrt_s) const
The STXS bin .
const double GammaH2muvRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double DeltaOalphtoW(const double dOSMdalpha, const double mu) const
Difference in prediction in scheme and W mass scheme, computed from observable in scheme....
const double GammaH2l2vRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double deltaxseeWWtotLEP2(const double sqrt_s) const
The new physics contribution to the total cross section in pb for , summing over all final states for...
virtual const double muggHZZ4l(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
const double deltaGammaH4uRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double xseeWW4fLEP2(const double sqrt_s, const int fstate) const
The cross section in pb for , with the different fermion final states for C.O.M. energies in 188-208...
const double deltaGammaHlv_lvorjjRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double muZHZZ(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
virtual const double kappaGeff() const
The effective coupling .
virtual const double kappaZeff() const
The effective coupling .
virtual const double STXS_qqHll_pTV_150_250_0j(const double sqrt_s) const
The STXS bin .
const double deltaGammaHZZ4fRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
virtual const double STXS12_ggHll_pTV150_250_Nj0(const double sqrt_s) const
The STXS bin , .
virtual const double muTHUttHbb(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
virtual const double STXS12_ggH_pTH0_10_Nj0(const double sqrt_s) const
The STXS bin , .
virtual const double deltaGamma_Wff(const Particle fi, const Particle fj) const
The new physics contribution to the decay width of the boson into a given fermion pair,...
virtual const double muZHbb(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
const double GammaH2v2uRatio() const
The ratio of the in the current model and in the Standard Model.
const double CeeRR_top(const double mu) const
virtual const double xseeWWtotLEP2(const double sqrt_s) const
The total cross section in pb for , summing over all final states for C.O.M. energies in 188-208 GeV....
virtual const double delta_mutH_2(const double sqrt_s) const
The SMEFT quadratic correction to the ratio between the t-Higgs associated production cross-section ...
virtual const double deltaG2_hWW() const
The new physics contribution to the coupling of the effective interaction .
virtual const double muTHUVHZZ(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
virtual const double STXS_ggH2j_pTH_60_120(const double sqrt_s) const
The STXS bin .
const double GammaHWlvRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double obliqueW() const
The oblique parameter . (Simplified implementation. Contribution only from .)
const double deltaGammaH2v2dRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double STXS_ggH2j_pTH_0_60(const double sqrt_s) const
The STXS bin .
void GenerateSMInitialConditions()
Generates the initial condition for the Standard Model parameters.
const double deltaMRL2_f(const Particle f, const double s) const
virtual const double muTHUVHZga(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
const double deltaGammaH4fRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double muZHWW2l2v(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
const double deltaGammaHccRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double STXS_qqHll_pTV_150_250_1j(const double sqrt_s) const
The STXS bin .
virtual const double muTHUggHbb(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
virtual const double deltaG1_hZARatio() const
The full new physics contribution to the coupling of the effective interaction , including new local ...
virtual const double deltaH3L2(double C1) const
The coefficient of the 1-loop quadratic term in the Higgs selfcoupling.
virtual const double del_sW2_mu(const double mu) const
Correction to (sin squared of) weak mixing angle.
virtual const double ctu8_TWG(const double mu) const
virtual const double deltamt() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
virtual const double STXS12_ttH_pTH200_300(const double sqrt_s) const
The STXS bin , .
const double CeeRL_top(const double mu) const
const double deltaGammaHssRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaHZffRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
const double deltaGammaHevmuvRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double muTHUggHWW(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
const double deltaGR_f_mu(const Particle p, const double mu) const
New physics contribution to the neutral-current right-handed coupling .
virtual const double A_f(const Particle f) const
The left-right asymmetry in at the -pole, .
virtual const double intDMLR2etildest2(const double s, const double t0, const double t1) const
virtual const double STXS12_ttH_pTH0_60(const double sqrt_s) const
The STXS bin , .
virtual const double deltaG3_hWW() const
The new physics contribution to the coupling of the effective interaction .
virtual const double deltaR0_f(const Particle f) const
The new physics contribution to the ratio , and , for charged leptons, quarks and neutrinos,...
virtual const double muggHtautau(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
const double GammaHZmumuRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double del_Z_mu(const double mu) const
Correction to Z WF.
const double deltaGammaHZZ4dRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double deltaAFB(const Particle f) const
The new physics contribution to the forward-backward asymmetry in at the -pole, .
virtual const double obliqueS() const
The oblique parameter . (Simplified implementation. Contribution only from .)
virtual const double BrHZZ4vRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double deltaMLR2t_e(const double s, const double t) const
virtual const double muggHbb(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
virtual const double delta_TauLFU_gtaugmuK() const
The computation of the correction to the LFU ratio .
virtual const double STXS12_ggH_pTH300_450_Nj01(const double sqrt_s) const
The STXS bin , .
const double deltaGammaHLvvLRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double muVBFHZga(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double muVHWW(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
virtual const double mueeZBF(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the production cross-section in the current model and in the Standard Model.
const double deltaGammaH2L2v2Ratio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double deltaGwd6() const
The relative NP corrections to the width of the boson, .
virtual const double intDMRL2etildest2(const double s, const double t0, const double t1) const
virtual const double ctZ_TWG(const double mu) const
virtual const double CEWHQ111(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
const double GammaHgagaRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double kappabeff() const
The effective coupling .
virtual const double muTHUVBFHWW2l2v(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
const double GammaHccRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double delta_Qwemoller(const double q2, const double y) const
The computation of the electron's weak charge.
virtual const double R0_f(const Particle f) const
The ratio , and , for charged leptons, quarks and neutrinos, respectively.
const double deltaGammaHZllRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double BrH2mu2vRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double deltaGammaHZuuRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double deltaaSMZ() const
The relative correction to the strong coupling constant at the Z pole, , with respect to ref....
virtual const double STXS12_ggH_pTH300_450(const double sqrt_s) const
The STXS bin , .
virtual const double intDMRR2eus2(const double s, const double t0, const double t1) const
virtual const double deltaG_hAARatio() const
The full new physics contribution to the coupling of the effective interaction , including new local ...
virtual bool PreUpdate()
The pre-update method for NPSMEFTd6General.
virtual const double mummHmm(const double sqrt_s) const
The ratio between the production cross-section in the current model and in the Standard Model.
virtual const double STXS12_qqHll_pTV0_150(const double sqrt_s) const
The STXS bin , .
virtual const double deltag1ZNPEff() const
The new physics contribution to the effective anomalous triple gauge coupling from arXiv: 1708....
virtual const double muepWBF(const double sqrt_s) const
The ratio between the production cross-section in the current model and in the Standard Model.
const double deltaGammaHudduRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double ctH_TWG(const double mu) const
virtual const double STXS12_ttH_pTH450_Inf(const double sqrt_s) const
The STXS bin , .
virtual const double cQt1_TWG(const double mu) const
virtual const double BrHZZ4lRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double ctl_TWG(const double mu) const
const double deltaGammaH2LvRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double lambdaZNP(const double mu) const
The new physics contribution to the anomalous triple gauge coupling .
virtual const double muTHUVHWW2l2v(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
virtual const double delU_gCC(const double mu) const
Universal indirect correction to EW charged currents.
virtual const double mummHNWA(const double sqrt_s) const
The ratio between the production cross-section in the current model and in the Standard Model,...
const double GammaH4fCCRatio() const
The ratio of the via CC in the current model and in the Standard Model.
const double deltaGammaHZZ4muRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double CEWHL122(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
const double CeeRL_up(const double mu) const
virtual const double mueettH(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the production cross-section in the current model and in the Standard Model.
const double deltaGammaH4fCCRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double muTHUVBFHinv(const double sqrt_s) const
The ratio between the VBF production cross-section with subsequent decay into invisible states in th...
virtual const double STXS_qqHll_pTV_250(const double sqrt_s) const
The STXS bin .
const double CeeRR_tau(const double mu) const
virtual const double muTHUVBFHtautau(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
const double deltaGammaHZddRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double BrH2LvRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
const double deltaGammaHZffRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
virtual const double cggEff_HB(const double mu) const
The effective Higgs-basis coupling . (Similar to cgg_HB but including modifications of SM loops....
const double CeeLL_strange(const double mu) const
virtual const double muTHUggHZZ4l(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
virtual const double AFB(const Particle f) const
The forward-backward asymmetry in at the -pole, .
const double deltaGammaH2evRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double muTHUttHWW(const double sqrt_s) const
The ratio between the ttH production cross-section with subsequent decay into in the current model ...
virtual const double BrHggRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double GammaHWW2l2vRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double BrH4lRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double STXS_qqHqq_nonVHtopo(const double sqrt_s) const
The STXS bin .
virtual const double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
const double deltaGammaH2L2dRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double BrHWlvRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double CEWHL322(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
virtual const double muVBFHgaga(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into 2 photons in the...
virtual const double muTHUZHZga(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
virtual const double CEWHe22(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
const double CeeRL_bottom(const double mu) const
virtual const double deltaKZNP(const double mu) const
The new physics contribution to the anomalous triple gauge coupling .
virtual const double deltayc_HB(const double mu) const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
virtual const double mummZH(const double sqrt_s) const
The ratio between the production cross-section in the current model and in the Standard Model.
virtual const double muTHUVHbb(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
virtual const double STXS_qqHqq_Rest(const double sqrt_s) const
The STXS bin .
const double CeeLL_bottom(const double mu) const
virtual const double muVHZga(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
virtual const double muWHWW2l2v(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
virtual const double muTHUVBFHbb(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double CEWHQ322(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
virtual gslpp::complex deltaGR_Wff(const Particle pbar, const Particle p) const
New physics contribution to the charged current coupling .
virtual const double STXS_qqHlv_pTV_150_250_0j(const double sqrt_s) const
The STXS bin .
const double deltaGammaH2e2muRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double muVBFHWW(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double muZHWW(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
virtual const double delta_alrmoller(const double q2, const double y) const
The computation of the parity violating asymmetry in Moller scattering.
const double CeeRR_up(const double mu) const
virtual const double delta_mubbH_2(const double sqrt_s) const
The SMEFT quadratic correction to the ratio between the bbH production cross-section in the current ...
gslpp::complex deltaG_hAff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
const double GammaHZddRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double muTHUZHZZ(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
const double CeeLL_top(const double mu) const
virtual const double mutHq(const double sqrt_s) const
The ratio between the t-q-Higgs associated production cross-section in the current model and in the ...
const double deltaGammaHZvvRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double muTHUZHmumu(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
virtual const double deltaxseeWW4fLEP2(const double sqrt_s, const int fstate) const
The new physics contribution to the cross section in pb for , with the different fermion final state...
virtual const double deltamc() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
const double GammaH4lRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double deltaG1_hWW() const
The new physics contribution to the coupling of the effective interaction .
const double deltaGammaHZZ4lRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double BrH4fRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double deltaGzd6() const
The relative NP corrections to the width of the boson, .
virtual const double deltaG2_hWW_mu(const double mu) const
The new physics contribution to the coupling of the effective interaction .
virtual const double STXS12_ggH_pTH650_Inf_Nj01(const double sqrt_s) const
The STXS bin , .
virtual const double BrH2L2LRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
virtual const double deltaKgammaNP(const double mu) const
The new physics contribution to the anomalous triple gauge coupling .
virtual const double obliqueY() const
The oblique parameter . (Simplified implementation. Contribution only from .)
virtual const double STXS12_qqHll_pTV150_250_Nj0(const double sqrt_s) const
The STXS bin , .
const double CeeLL_up(const double mu) const
virtual const double BrH2u2uRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double deltaG1_hZA_mu(const double mu) const
The new physics contribution to the coupling of the effective interaction .
virtual const double muttHgagaZeeboost(const double sqrt_s) const
The ratio in the , channel channel in the current model and in the Standard Model.
const double deltaGammaH2Lv2Ratio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
const double GammaHlv_lvorjjRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
double getCG_LNP() const
Return CG_LNP.
const double deltaGammaHll_vvorjjRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double obliqueT() const
The oblique parameter . (Simplified implementation. Contribution only from .)
virtual const double STXS12_ttH_pTH60_120(const double sqrt_s) const
The STXS bin , .
virtual const double STXS12_qqHll_pTV250_Inf(const double sqrt_s) const
The STXS bin , .
virtual const double muVH(const double sqrt_s) const
The ratio between the WH+ZH associated production cross-section in the current model and in the Stan...
virtual const double computeGammaTotalRatio() const
The ratio of the in the current model and in the Standard Model.
const double deltaGammaHtautauRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double mueeHee(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the associated production cross-section in the current model and in the Standard ...
virtual const double kappaWeff() const
The effective coupling .
virtual const double STXS_qqHqq_pTj_200(const double sqrt_s) const
The STXS bin .
virtual const double STXS0_qqH(const double sqrt_s) const
The STXS0 bin .
virtual const double CEWHe33(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
virtual const double mutH(const double sqrt_s) const
The ratio between the t-Higgs associated production cross-section in the current model and in the St...
virtual const double delta_gAnue() const
The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gA...
const double deltaGammaHtautauRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double GammaH4vRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double muWHgaga(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into 2 photons in the curren...
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 STXS12_ttH_pTH120_200(const double sqrt_s) const
The STXS bin , .
const double deltaGammaHZuuRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
const double deltaGammaHWWRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
double getLambda_NP() const
Return Lambda_NP.
virtual const double STXS_ZHqqHqq_pTj1_200(const double sqrt_s) const
The STXS bin .
virtual const double muttH(const double sqrt_s) const
The ratio between the t-tbar-Higgs associated production cross-section in the current model and in t...
virtual const double deltaG_hgg() const
The new physics contribution to the coupling of the effective interaction .
virtual const double BrHZZ2e2muRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double deltaGammaHWWRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGL_Zffh(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
const double deltaGammaHZddRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double muVHZZ(const double sqrt_s) const
The ratio between the VH production cross-section with subsequent decay into in the current model a...
const double deltaGammaHggRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double deltaGammaHZmumuRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double CeeRL_e(const double mu) const
const double deltaGammaH4lRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double muTHUWHtautau(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
virtual const double CEWHu22(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
const double GammaH2L2vRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref....
const double deltaGammaHssRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double GammaH2L2LRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
virtual const double deltaaMZ2() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref....
const double GammaH4uRatio() const
The ratio of the in the current model and in the Standard Model.
const double deltaGammaH2udRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double GammaH2udRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double muTHUVBFHZga(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double delta_AFB_ee(const double pol_e, const double pol_p, const double s) const
virtual const double mueeZllH(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the associated production cross-section in the current model and in the Standard ...
virtual const double STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2(const double sqrt_s) const
The STXS bin , .
virtual const double CEWHd33(const double mu) const
Combination of coefficients of the Warsaw basis constrained by EWPO .
const double deltaGammaH2v2uRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double muTHUZHWW(const double sqrt_s) const
The ratio between the ZH production cross-section with subsequent decay into in the current model a...
virtual const double BrH4fCCRatio() const
The ratio of the Br in the current model and in the Standard Model.
const double GammaHZeeRatio() const
The ratio of the in the current model and in the Standard Model.
const double CeeRL_strange(const double mu) const
virtual const double STXS12_ggH_pTH0_60_Nj1(const double sqrt_s) const
The STXS bin , .
virtual const double muTHUWHZga(const double sqrt_s) const
The ratio between the WH production cross-section with subsequent decay into in the current model a...
const double deltaGammaH4L2Ratio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double delta_amuon() const
The computation of the anomalous magnetic moment of the muon .
virtual const double STXS12_qqHlv_pTV250_400(const double sqrt_s) const
The STXS bin , .
virtual const double STXS12_ggH_pTH450_650_Nj01(const double sqrt_s) const
The STXS bin , .
virtual const double muVBFHbb(const double sqrt_s) const
The ratio between the VBF Higgs production cross-section with subsequent decay into in the current ...
virtual const double muggHH(const double sqrt_s) const
The ratio between the gluon-gluon fusion di-Higgs production cross-section in the current model and ...
virtual const double muVBFpVH(const double sqrt_s) const
The ratio between the sum of VBF and WH+ZH associated production cross-section in the current model ...
virtual const double BrHZZ4dRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
const double deltaGammaH2LvRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
virtual const double BrH2e2vRatio() const
The ratio of the Br in the current model and in the Standard Model.
virtual const double ctlT_TWG(const double mu) const
virtual const double muTHUggHWW2l2v(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section with subsequent decay into ...
const double GammaH4L2Ratio() const
The ratio of the ( ) in the current model and in the Standard Model.
const double deltaGammaHZZRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double STXS12_ggH_pTH650_Inf(const double sqrt_s) const
The STXS bin , .
const double deltaGammaH2e2muRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double BrH2Lv2Ratio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
const double deltaGammaHZZRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
const double CeeLL_tau(const double mu) const
virtual const double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
virtual const double del_e_mu(const double mu) const
Correction to electric charge.
const double GammaHZZ4fRatio() const
The ratio of the , with any fermion, in the current model and in the Standard Model.
const double deltaGL_f(const Particle p) const
New physics contribution to the neutral-current left-handed coupling .
const double CeeRR_bottom(const double mu) const
virtual const double del_ZA_mu(const double mu) const
Correction to Z-A mixing.
const double GammaH2L2dRatio() const
The ratio of the ( ) in the current model and in the Standard Model.
const double GammaHZZRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double STXS_qqHll_pTV_0_150(const double sqrt_s) const
The STXS bin .
const double GammaHWWRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double ctq8_TWG(const double mu) const
virtual const double ctd1_TWG(const double mu) const
virtual const double STXS_WHqqHqq_VBFtopo_j3(const double sqrt_s) const
The STXS bin .
virtual const double STXS_WHqqHqq_VBFtopo_j3v(const double sqrt_s) const
The STXS bin .
virtual const double deltayb_HB(const double mu) const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
const double GammaHWjjRatio() const
The ratio of the in the current model and in the Standard Model.
virtual const double dxseeWWdcosBin(const double sqrt_s, const double cos1, const double cos2) const
The integral of differential distribution for , with in a given bin of the polar angle.
const double deltaGammaHccRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
virtual const double deltaG2_hZZ() const
The new physics contribution to the coupling of the effective interaction .
const double deltaGammaHLvudRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
A class for the matching in the NPSMEFTd6_General model at the scale .
The auxiliary base model class for other model classes.
virtual const double BrHlljjRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
const gslpp::matrix< gslpp::complex > & getYe() const
A get method to retrieve the Yukawa matrix of the charged leptons, .
const gslpp::matrix< gslpp::complex > & getYu() const
A get method to retrieve the Yukawa matrix of the up-type quarks, .
const gslpp::matrix< gslpp::complex > & getYd() const
A get method to retrieve the Yukawa matrix of the down-type quarks, .
gslpp::matrix< gslpp::complex > Yu
The Yukawa matrix of the up-type quarks.
bool FlagMWinput
A boolean for the model flag MWinput.
gslpp::matrix< gslpp::complex > Yd
The Yukawa matrix of the down-type quarks.
const double Mw_tree() const
The tree-level mass of the boson, .
gslpp::matrix< gslpp::complex > Ye
The Yukawa matrix of the charged leptons.
virtual void setParameter(const std::string name, const double &value)
A method to set the value of a parameter of StandardModel.
StdVectorFiller< int > Vi