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NPSMEFTd6General.h
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1
2/*
3 * File: NPSMEFTd6General.h
4 * Author: miralles
5 *
6 * Created on 12 September 2022, 14:17
7 */
8
9#ifndef NPSMEFTD6GENERAL_H
10#define NPSMEFTD6GENERAL_H
11
12#include "gslpp.h"
13#include "NPbase.h"
15#include <string.h>
16#include <stdexcept>
17#include <gsl/gsl_integration.h>
18#include <RGESolver.h>
19
593class NPSMEFTd6General : public NPbase {
594public:
595
599 //static const int NNPSMEFTd6GeneralVars = 2708 + 18;
600 static const int NNPSMEFTd6GeneralVars = 2708-208 + 79 ;
601
602
608
613
620 virtual bool PreUpdate();
621
628
635 virtual bool PostUpdate();
636
637 //I think that for this model, with so many parameters, it's better to include only those we're really interested in
638 //Since all the parameters are initialized to zero we can just skip the CheckParameters for this model
646 //virtual bool CheckParameters(const std::map<std::string, double>& DPars);
647
654 virtual bool setFlag(const std::string name, const bool value);
655
662 virtual bool setFlagStr(const std::string name, const std::string value);
663
669 return NPSMEFTd6GM.getObj();
670 }
671
673
678 double getLambda_NP() const {
679 return Lambda_NP;
680 }
681
682
687 double getCG_LNP() const {
688 return CG_LNP;
689 }
690
692 // Functions to facilitate the change of scheme (at tree level)
693
708 virtual const double DeltaOalphtoW(const double dOSMdalpha, const double mu) const;
709
724 virtual const double DeltaOWtoalph(const double dOSMdMW, const double mu) const;
725
727
728 //test function to test speed of code
729 //double test_direct() const;
730
732
733 // Functions used to compute the 1-loop dependence of single Higgs observables
734 // on the Higgs self-coupling
735
739 virtual const double deltaH3L1(double C1) const;
740
744 virtual const double deltaH3L2(double C1) const;
745
747
752 virtual const double delta2sH3(const double C1) const;
753
758 virtual const double delta2sBRH3(const double C1prod, const double C1Hxx) const;
759
761
772 virtual const double DeltaGF() const;
773
775 // Functions to compute quantities involved in indirect corrections, depending on RG scale
776
783 virtual const double del_A_mu(const double mu) const;
784
791 virtual const double del_Z_mu(const double mu) const;
792
799 virtual const double del_ZA_mu(const double mu) const;
800
801
808 virtual const double del_e_mu(const double mu) const;
809
816 virtual const double del_sW2_mu(const double mu) const;
817
824 virtual const double delU_gNC(const double mu) const;
825
832 virtual const double delQ_gNC(const double mu) const;
833
840 virtual const double delU_gCC(const double mu) const;
841
843
849 virtual const double obliqueS() const;
850
856 virtual const double obliqueT() const;
857
862 virtual const double obliqueU() const;
863
869 virtual const double obliqueW() const;
870
876 virtual const double obliqueY() const;
877
878
880
885 virtual const double deltaMz() const;
886
891 virtual const double deltaMz2() const;
892
897 virtual const double deltaMh() const;
898
903 virtual const double deltaMh2() const;
904
909 virtual const double deltamt() const;
910
915 virtual const double deltamt2() const;
916
921 virtual const double deltamb() const;
922
927 virtual const double deltamb2() const;
928
933 virtual const double deltamc() const;
934
939 virtual const double deltamc2() const;
940
945 virtual const double deltamtau() const;
946
951 virtual const double deltamtau2() const;
952
957 virtual const double deltaGmu() const;
958
963 virtual const double deltaGmu2() const;
964
969 virtual const double deltaaMZ() const;
970
975 virtual const double deltaaMZ2() const;
976
981 virtual const double deltaa0() const;
982
987 virtual const double deltaa02() const;
988
993 virtual const double deltaaSMZ() const;
994
999 virtual const double deltaaSMZ2() const;
1000
1005 virtual const double deltaMw() const;
1006
1011 virtual const double deltaMw2() const;
1012
1014
1019 virtual const double alphaMz() const;
1020
1026 virtual const double Dalpha5hMz() const;
1027
1028
1030
1035 virtual const double Mw() const;
1036
1041 virtual const double deltaMwd6() const;
1042
1047 virtual const double deltaMwd62() const;
1048
1055 virtual const double deltaGamma_Wff(const Particle fi, const Particle fj) const;
1056
1063 virtual const double GammaW(const Particle fi, const Particle fj) const;
1064
1069 virtual const double deltaGamma_W() const;
1070
1075 virtual const double GammaW() const;
1076
1081 virtual const double deltaGwd6() const;
1082
1087 virtual const double deltaGwd62() const;
1088
1090
1091
1097 virtual const double deltaGamma_Zf(const Particle f) const;
1098
1111 virtual const double Gamma_Zf(const Particle f) const;
1112
1117 virtual const double deltaGamma_Z() const;
1118
1130 virtual const double Gamma_Z() const;
1131
1136 virtual const double deltaGzd6() const;
1137
1142 virtual const double deltaGzd62() const;
1143
1148 virtual const double BrW(const Particle fi, const Particle fj) const;
1149
1154 virtual const double RWlilj(const Particle li, const Particle lj) const;
1155
1160 virtual const double RWc() const;
1161
1166 virtual const double RZlilj(const Particle li, const Particle lj) const;
1167
1173 virtual const double deltaSigmaHadron() const;
1174
1175
1185 virtual const double sigma0_had() const;
1186
1193 virtual const double deltaA_f(const Particle f) const;
1194
1208 virtual const double A_f(const Particle f) const;
1209
1216 virtual const double deltaAFB(const Particle f) const;
1217
1228 virtual const double AFB(const Particle f) const;
1229
1237 virtual const double deltaR0_f(const Particle f) const;
1238
1250 virtual const double R0_f(const Particle f) const;
1251
1253
1254 // LEP2 definitions for 2 to 2 fermion processes
1255
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;
1259
1260 const double CeeLL_up(const double mu) const;
1261 const double CeeLL_charm(const double mu) const;
1262 const double CeeLL_top(const double mu) const;
1263
1264 const double CeeLL_down(const double mu) const;
1265 const double CeeLL_strange(const double mu) const;
1266 const double CeeLL_bottom(const double mu) const;
1267
1268
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;
1272
1273 const double CeeLR_up(const double mu) const;
1274 const double CeeLR_charm(const double mu) const;
1275 const double CeeLR_top(const double mu) const;
1276
1277 const double CeeLR_down(const double mu) const;
1278 const double CeeLR_strange(const double mu) const;
1279 const double CeeLR_bottom(const double mu) const;
1280
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;
1284
1285 const double CeeRL_up(const double mu) const;
1286 const double CeeRL_charm(const double mu) const;
1287 const double CeeRL_top(const double mu) const;
1288
1289 const double CeeRL_down(const double mu) const;
1290 const double CeeRL_strange(const double mu) const;
1291 const double CeeRL_bottom(const double mu) const;
1292
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;
1296
1297 const double CeeRR_up(const double mu) const;
1298 const double CeeRR_charm(const double mu) const;
1299 const double CeeRR_top(const double mu) const;
1300
1301 const double CeeRR_down(const double mu) const;
1302 const double CeeRR_strange(const double mu) const;
1303 const double CeeRR_bottom(const double mu) const;
1304
1305// Absolute corrections to the helicity amplitudes squared
1306
1307 const double deltaMLR2_f(const Particle f, const double s) const;
1308 const double deltaMRL2_f(const Particle f, const double s) const;
1309
1310 const double deltaMLL2_f(const Particle f, const double s, const double t) const;
1311 const double deltaMRR2_f(const Particle f, const double s, const double t) const;
1312
1313// Some simple functions for cos \theta integrals
1314 const double tovers2(const double cosmin, const double cosmax) const;
1315 const double uovers2(const double cosmin, const double cosmax) const;
1316
1317// Absolute corrections to the differential cross section
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;
1319
1320// Absolute corrections to the differential cross section integrated in [cos \theta_{min},cos \theta_{max}]
1321// Valid for f=/=e
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;
1323
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;
1325
1326// Total cross sections (full acceptance)
1327 virtual const double delta_sigmaTot_f(const Particle f, const double pol_e, const double pol_p, const double s) const;
1328
1329// Forward-Backward asymmetry (full acceptance). Valid for f!=e
1330 virtual const double delta_AFB_f(const Particle f, const double pol_e, const double pol_p, const double s) const;
1331
1332// Expressions for f=e
1333
1334// Corrections to t-channel LR and RL amplitudes
1335 const double deltaMLR2t_e(const double s, const double t) const;
1336 const double deltaMRL2t_e(const double s, const double t) const;
1337
1338// Integrals of the corrections to the squared amplitudes x (t/s)^2, (s/t)^2, (u/s)^2 in [t0, t1]
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;
1345
1346// Absolute corrections to the differential cross section integrated in [cos \theta_{min},cos \theta_{max}]
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;
1348// Absolute corrections to the total cross section
1349 virtual const double delta_sigmaTot_ee(const double pol_e, const double pol_p, const double s) const;
1350// Absolute corrections to the FB asymmetry
1351 virtual const double delta_AFB_ee(const double pol_e, const double pol_p, const double s) const;
1352
1354 // Top Wilson coefficients in the notation of LHC Top WG arXiv: 1802.07237
1355 // In units of TeV^-2
1356
1357 virtual const double cQQ1_TWG(const double mu) const;
1358
1359 virtual const double cQQ8_TWG(const double mu) const;
1360
1361 virtual const double ctt1_TWG(const double mu) const;
1362
1363 virtual const double cQt1_TWG(const double mu) const;
1364
1365 virtual const double cQt8_TWG(const double mu) const;
1366
1367 virtual const double cQq31_TWG(const double mu) const;
1368
1369 virtual const double cQq38_TWG(const double mu) const;
1370
1371 virtual const double cQq11_TWG(const double mu) const;
1372
1373 virtual const double cQq18_TWG(const double mu) const;
1374
1375 virtual const double cQu1_TWG(const double mu) const;
1376
1377 virtual const double cQu8_TWG(const double mu) const;
1378
1379 virtual const double cQd1_TWG(const double mu) const;
1380
1381 virtual const double cQd8_TWG(const double mu) const;
1382
1383 virtual const double ctq1_TWG(const double mu) const;
1384
1385 virtual const double ctq8_TWG(const double mu) const;
1386
1387 virtual const double ctu1_TWG(const double mu) const;
1388
1389 virtual const double ctu8_TWG(const double mu) const;
1390
1391 virtual const double ctd1_TWG(const double mu) const;
1392
1393 virtual const double ctd8_TWG(const double mu) const;
1394
1395 virtual const double ctH_TWG(const double mu) const;
1396
1397 virtual const double cHQm_TWG(const double mu) const;
1398
1399 virtual const double cHQp_TWG(const double mu) const;
1400
1401 virtual const double cHQ3_TWG(const double mu) const;
1402
1403 virtual const double cHt_TWG(const double mu) const;
1404
1405 virtual const double cHb_TWG(const double mu) const;
1406
1407 virtual const double cHtb_TWG(const double mu) const;
1408
1409 virtual const double ctW_TWG(const double mu) const;
1410
1411 virtual const double IctW_TWG(const double mu) const;
1412
1413 virtual const double ctZ_TWG(const double mu) const;
1414
1415 virtual const double IctZ_TWG(const double mu) const;
1416
1417 virtual const double ctG_TWG(const double mu) const;
1418
1419 virtual const double cbW_TWG(const double mu) const;
1420
1421 virtual const double cQlM_TWG(const double mu) const;
1422
1423 virtual const double cQlP_TWG(const double mu) const;
1424
1425 virtual const double cQl3_TWG(const double mu) const;
1426
1427 virtual const double cQe_TWG(const double mu) const;
1428
1429 virtual const double ctl_TWG(const double mu) const;
1430
1431 virtual const double cte_TWG(const double mu) const;
1432
1433 virtual const double ctlS_TWG(const double mu) const;
1434
1435 virtual const double ctlT_TWG(const double mu) const;
1436
1438 // EW low-energy observables: Muon g-2
1439
1444 virtual const double delta_amuon() const;
1445
1446 // EW low-energy observables: Parity violation
1447
1454 virtual const double delta_Qwemoller(const double q2, const double y) const;
1455
1456
1463 virtual const double delta_alrmoller(const double q2, const double y) const;
1464
1465
1470 virtual const double delta_Qwp() const;
1471
1472
1477 virtual const double delta_Qwn() const;
1478
1479 // EW low-energy observables: neutrino scattering
1480
1485 virtual const double delta_gLnuN2() const;
1486
1491 virtual const double delta_gRnuN2() const;
1492
1498 virtual const double delta_gVnue() const;
1499
1505 virtual const double delta_gAnue() const;
1506
1508 // Lepton decays
1509
1510 // Lepton Flavor universality tests in Tau decays
1511
1517 virtual const double delta_TauLFU_gmuge() const;
1518
1519
1525 virtual const double delta_TauLFU_gtaugmu() const;
1526
1527
1533 virtual const double delta_TauLFU_gtauge() const;
1534
1535
1541 virtual const double delta_TauLFU_gtaugmuPi() const;
1542
1548 virtual const double delta_TauLFU_gtaugmuK() const;
1549
1551 // Modifications of EW/Higgs couplings
1552
1553 // Modifications of Zff couplings
1554
1560 virtual const double deltaGV_f(const Particle p) const;
1561
1567 virtual const double deltaGA_f(const Particle p) const;
1568
1574 // no generation mixing
1575 const double deltaGL_f(const Particle p) const;
1576
1582 // no generation mixing
1583 const double deltaGR_f(const Particle p) const;
1584
1591 // no generation mixing
1592 const double deltaGL_f_mu(const Particle p, const double mu) const;
1593
1600 // no generation mixing
1601 const double deltaGR_f_mu(const Particle p, const double mu) const;
1602
1603 // Modifications of Wff couplings
1604
1611 // no generation mixing
1612 virtual gslpp::complex deltaGL_Wff(const Particle pbar, const Particle p) const;
1619 // no generation mixing
1620 virtual gslpp::complex deltaGR_Wff(const Particle pbar, const Particle p) const;
1621
1629 // no generation mixing
1630 virtual gslpp::complex deltaGL_Wff_mu(const Particle pbar, const Particle p, const double mu) const;
1638 // no generation mixing
1639 virtual gslpp::complex deltaGR_Wff_mu(const Particle pbar, const Particle p, const double mu) const;
1640
1641 // Modifications of Higgs couplings
1642
1647 virtual const double deltaG_hgg() const;
1653 virtual const double deltaG_hggRatio() const;
1658 virtual const double deltaG1_hWW() const;
1663 virtual const double deltaG2_hWW() const;
1668 virtual const double deltaG3_hWW() const;
1673 virtual const double deltaG1_hZZ() const;
1678 virtual const double deltaG2_hZZ() const;
1683 virtual const double deltaG3_hZZ() const;
1688 virtual const double deltaG1_hZA() const;
1694 virtual const double deltaG1_hZARatio() const;
1699 virtual const double deltaG2_hZA() const;
1704 virtual const double deltaG_hAA() const;
1710 virtual const double deltaG_hAARatio() const;
1716 // no generation mixing
1717 virtual gslpp::complex deltaG_hff(const Particle p) const;
1718
1723 virtual const double deltaG_hhhRatio() const;
1724
1725
1727
1733 virtual const double deltaG_hgg_mu(const double mu) const;
1740 virtual const double deltaG_hggRatio_mu(const double mu) const;
1746 virtual const double deltaG1_hWW_mu(const double mu) const;
1752 virtual const double deltaG2_hWW_mu(const double mu) const;
1758 virtual const double deltaG3_hWW_mu(const double mu) const;
1764 virtual const double deltaG1_hZZ_mu(const double mu) const;
1770 virtual const double deltaG2_hZZ_mu(const double mu) const;
1776 virtual const double deltaG3_hZZ_mu(const double mu) const;
1782 virtual const double deltaG1_hZA_mu(const double mu) const;
1789 virtual const double deltaG1_hZARatio_mu(const double mu) const;
1795 virtual const double deltaG2_hZA_mu(const double mu) const;
1801 virtual const double deltaG_hAA_mu(const double mu) const;
1808 virtual const double deltaG_hAARatio_mu(const double mu) const;
1815 // no generation mixing
1816 virtual gslpp::complex deltaG_hff_mu(const Particle p, const double mu) const;
1822 virtual const double deltaG_hhhRatio_mu(const double mu) const;
1823
1825
1832 // no generation mixing
1833 gslpp::complex deltaGL_Wffh(const Particle pbar, const Particle p) const;
1834
1841 // no generation mixing
1842 gslpp::complex deltaGR_Wffh(const Particle pbar, const Particle p) const;
1843
1849 // no generation mixing
1850 const double deltaGL_Zffh(const Particle p) const;
1851
1857 // no generation mixing
1858 const double deltaGR_Zffh(const Particle p) const;
1859
1861
1867 // no generation mixing
1868 gslpp::complex deltaG_hGff(const Particle p) const;
1869
1875 // no generation mixing
1876 gslpp::complex deltaG_hZff(const Particle p) const;
1877
1883 // no generation mixing
1884 gslpp::complex deltaG_hAff(const Particle p) const;
1885
1887
1893 // no generation mixing
1894 gslpp::complex deltaG_Gff(const Particle p) const;
1895
1901 // no generation mixing
1902 gslpp::complex deltaG_Zff(const Particle p) const;
1903
1909 // no generation mixing
1910 gslpp::complex deltaG_Aff(const Particle p) const;
1911
1916 const double deltag3G() const;
1917
1918
1920
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;
1950 virtual const double muVBFgamma(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;
1994 virtual const double muepWBF(const double sqrt_s) const;
2002 virtual const double muepZBF(const double sqrt_s) const;
2009 virtual const double muWH(const double sqrt_s) const;
2016 virtual const double muWHpT250(const double sqrt_s) const;
2023 virtual const double muZH(const double sqrt_s) const;
2030 virtual const double muZHpT250(const double sqrt_s) const;
2031
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;
2124 virtual const double muVHpT250(const double sqrt_s) const;
2131 virtual const double muVBFpVH(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; //AG:added
2152 virtual const double mubbH(const double sqrt_s) const
2153 {
2154 return 1.0;
2155 }; //AG:added
2156
2163 virtual const double mutHq(const double sqrt_s) const;
2171 virtual const double muggHpttH(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;
2195 virtual const double mummHNWA(const double sqrt_s) const;
2202 virtual const double mummZH(const double sqrt_s) const;
2209 virtual const double mummHvv(const double sqrt_s) const;
2216 virtual const double mummHmm(const double sqrt_s) const;
2223 virtual const double mummttH(const double sqrt_s) const;
2224
2225 //AG:added, begin
2226 virtual const double delta_muggH_1(const double sqrt_s) const;
2227 virtual const double delta_muggH_2(const double sqrt_s) const;
2228
2229 virtual const double delta_muVBF_1(const double sqrt_s) const;
2230 virtual const double delta_muVBF_2(const double sqrt_s) const;
2231
2232 virtual const double delta_muWH_1(const double sqrt_s) const;
2233 virtual const double delta_muWH_2(const double sqrt_s) const;
2234
2235 virtual const double delta_muZH_1(const double sqrt_s) const;
2236 virtual const double delta_muZH_2(const double sqrt_s) const;
2237
2238 virtual const double delta_muVH_1(const double sqrt_s) const;
2239 virtual const double delta_muVH_2(const double sqrt_s) const;
2240
2241 virtual const double delta_muttH_1(const double sqrt_s) const;
2242 virtual const double delta_muttH_2(const double sqrt_s) const;
2243
2244 virtual const double delta_mutH_1(const double sqrt_s) const;
2245 virtual const double delta_mutH_2(const double sqrt_s) const;
2246
2247 virtual const double delta_mubbH_1(const double sqrt_s) const
2248 {
2249 return 0.0;
2250 }
2251 virtual const double delta_mubbH_2(const double sqrt_s) const
2252 {
2253 return 0.0;
2254 }
2255 //AG:end
2256
2258
2263 virtual const double computeGammaTotalRatio() const;
2270 virtual const double deltaGammaTotalRatio1() const;
2277 virtual const double deltaGammaTotalRatio1noError() const;
2284 virtual const double deltaGammaTotalRatio2() const;
2285
2291 const double GammaHggRatio() const;
2298 const double deltaGammaHggRatio1() const;
2305 const double deltaGammaHggRatio2() const;
2311 virtual const double BrHggRatio() const;
2312
2318 const double GammaHWWRatio() const;
2325 const double deltaGammaHWWRatio1() const;
2332 const double deltaGammaHWWRatio2() const;
2338 virtual const double BrHWWRatio() const;
2339
2346 const double GammaHWlvRatio() const;
2353 const double deltaGammaHWlvRatio1() const;
2360 const double deltaGammaHWlvRatio2() const;
2366 virtual const double BrHWlvRatio() const;
2367
2373 const double GammaHWW2l2vRatio() const;
2380 const double deltaGammaHWW2l2vRatio1() const;
2387 const double deltaGammaHWW2l2vRatio2() const;
2393 virtual const double BrHWW2l2vRatio() const;
2394
2400 const double GammaHWjjRatio() const;
2407 const double deltaGammaHWjjRatio1() const;
2414 const double deltaGammaHWjjRatio2() const;
2420 virtual const double BrHWjjRatio() const;
2421
2427 const double GammaHWW4jRatio() const;
2434 const double deltaGammaHWW4jRatio1() const;
2441 const double deltaGammaHWW4jRatio2() const;
2447 virtual const double BrHWW4jRatio() const;
2448
2454 const double GammaHWffRatio() const;
2461 const double deltaGammaHWffRatio1() const;
2468 const double deltaGammaHWffRatio2() const;
2474 virtual const double BrHWffRatio() const;
2475
2481 const double GammaHWW4fRatio() const;
2488 const double deltaGammaHWW4fRatio1() const;
2495 const double deltaGammaHWW4fRatio2() const;
2501 virtual const double BrHWW4fRatio() const;
2502
2508 const double GammaHZZRatio() const;
2515 const double deltaGammaHZZRatio1() const;
2522 const double deltaGammaHZZRatio2() const;
2528 virtual const double BrHZZRatio() const;
2529
2535 const double GammaHZllRatio() const;
2542 const double deltaGammaHZllRatio1() const;
2549 const double deltaGammaHZllRatio2() const;
2555 virtual const double BrHZllRatio() const;
2556
2562 const double GammaHZeeRatio() const;
2569 const double deltaGammaHZeeRatio1() const;
2576 const double deltaGammaHZeeRatio2() const;
2577
2583 const double GammaHZmumuRatio() const;
2590 const double deltaGammaHZmumuRatio1() const;
2597 const double deltaGammaHZmumuRatio2() const;
2598
2604 const double GammaHZZ4lRatio() const;
2611 const double deltaGammaHZZ4lRatio1() const;
2618 const double deltaGammaHZZ4lRatio2() const;
2624 virtual const double BrHZZ4lRatio() const;
2625
2631 const double GammaHZZ4eRatio() const;
2638 const double deltaGammaHZZ4eRatio1() const;
2645 const double deltaGammaHZZ4eRatio2() const;
2651 virtual const double BrHZZ4eRatio() const;
2652
2658 const double GammaHZZ2e2muRatio() const;
2665 const double deltaGammaHZZ2e2muRatio1() const;
2672 const double deltaGammaHZZ2e2muRatio2() const;
2678 virtual const double BrHZZ2e2muRatio() const;
2679
2685 const double GammaHZZ4muRatio() const;
2692 const double deltaGammaHZZ4muRatio1() const;
2699 const double deltaGammaHZZ4muRatio2() const;
2705 virtual const double BrHZZ4muRatio() const;
2706
2712 const double GammaHZvvRatio() const;
2719 const double deltaGammaHZvvRatio1() const;
2726 const double deltaGammaHZvvRatio2() const;
2732 virtual const double BrHZvvRatio() const;
2733
2739 const double GammaHZZ4vRatio() const;
2746 const double deltaGammaHZZ4vRatio1() const;
2753 const double deltaGammaHZZ4vRatio2() const;
2759 virtual const double BrHZZ4vRatio() const;
2760
2766 const double GammaHZuuRatio() const;
2773 const double deltaGammaHZuuRatio1() const;
2780 const double deltaGammaHZuuRatio2() const;
2786 virtual const double BrHZuuRatio() const;
2787
2793 const double GammaHZZ4uRatio() const {
2794 return 1.0;
2795 };
2796
2803 const double deltaGammaHZZ4uRatio1() const {
2804 return 0.0;
2805 };
2806
2813 const double deltaGammaHZZ4uRatio2() const {
2814 return 0.0;
2815 };
2821 virtual const double BrHZZ4uRatio() const;
2822
2828 const double GammaHZddRatio() const;
2835 const double deltaGammaHZddRatio1() const;
2842 const double deltaGammaHZddRatio2() const;
2848 virtual const double BrHZddRatio() const;
2849
2855 const double GammaHZZ4dRatio() const {
2856 return 1.0;
2857 };
2858
2865 const double deltaGammaHZZ4dRatio1() const {
2866 return 0.0;
2867 };
2868
2875 const double deltaGammaHZZ4dRatio2() const {
2876 return 0.0;
2877 };
2883 virtual const double BrHZZ4dRatio() const;
2884
2890 const double GammaHZffRatio() const;
2897 const double deltaGammaHZffRatio1() const;
2904 const double deltaGammaHZffRatio2() const;
2910 virtual const double BrHZffRatio() const;
2911
2917 const double GammaHZZ4fRatio() const;
2924 const double deltaGammaHZZ4fRatio1() const;
2931 const double deltaGammaHZZ4fRatio2() const;
2937 virtual const double BrHZZ4fRatio() const;
2938
2944 virtual const double BrHVVRatio() const;
2945
2951 const double GammaHZgaRatio() const;
2958 const double deltaGammaHZgaRatio1() const;
2965 const double deltaGammaHZgaRatio2() const;
2971 virtual const double BrHZgaRatio() const;
2977 virtual const double BrHZgallRatio() const;
2983 virtual const double BrHZgaeeRatio() const;
2989 virtual const double BrHZgamumuRatio() const;
2990
2996 const double GammaHgagaRatio() const;
3003 const double deltaGammaHgagaRatio1() const;
3010 const double deltaGammaHgagaRatio2() const;
3016 virtual const double BrHgagaRatio() const;
3017
3023 const double deltaGammaHffRatio1(const double mf, const double CifH) const; //AG:added
3030 const double deltaGammaHffRatio2(const double mf, const double CifH) const; //AG:added
3031
3037 const double GammaHmumuRatio() const;
3044 const double deltaGammaHmumuRatio1() const;
3051 const double deltaGammaHmumuRatio2() const;
3057 virtual const double BrHmumuRatio() const;
3058
3064 const double GammaHtautauRatio() const;
3071 const double deltaGammaHtautauRatio1() const;
3078 const double deltaGammaHtautauRatio2() const;
3084 virtual const double BrHtautauRatio() const;
3085
3091 const double GammaHccRatio() const;
3098 const double deltaGammaHccRatio1() const;
3105 const double deltaGammaHccRatio2() const;
3111 virtual const double BrHccRatio() const;
3117 const double GammaHssRatio() const;
3124 const double deltaGammaHssRatio1() const;
3131 const double deltaGammaHssRatio2() const;
3137 virtual const double BrHssRatio() const;
3143 const double GammaHbbRatio() const;
3150 const double deltaGammaHbbRatio1() const;
3157 const double deltaGammaHbbRatio2() const;
3163 virtual const double BrHbbRatio() const;
3164
3165 // General 4 fermion final states
3166
3172 const double GammaH2L2LRatio() const;
3179 const double deltaGammaH2L2LRatio1() const;
3186 const double deltaGammaH2L2LRatio2() const;
3192 virtual const double BrH2L2LRatio() const;
3193
3199 const double GammaH2e2muRatio() const;
3206 const double deltaGammaH2e2muRatio1() const;
3213 const double deltaGammaH2e2muRatio2() const;
3219 virtual const double BrH2e2muRatio() const;
3220
3226 const double GammaH2v2vRatio() const;
3233 const double deltaGammaH2v2vRatio1() const;
3240 const double deltaGammaH2v2vRatio2() const;
3246 virtual const double BrH2v2vRatio() const;
3247
3253 const double GammaH2L2vRatio() const;
3260 const double deltaGammaH2L2vRatio1() const;
3267 const double deltaGammaH2L2vRatio2() const;
3273 virtual const double BrH2L2vRatio() const;
3274
3275
3281 const double GammaH2L2v2Ratio() const;
3288 const double deltaGammaH2L2v2Ratio1() const;
3295 const double deltaGammaH2L2v2Ratio2() const;
3301 virtual const double BrH2L2v2Ratio() const;
3302
3303
3309 const double GammaH2e2vRatio() const;
3316 const double deltaGammaH2e2vRatio1() const;
3323 const double deltaGammaH2e2vRatio2() const;
3329 virtual const double BrH2e2vRatio() const;
3330
3331
3337 const double GammaH2mu2vRatio() const;
3344 const double deltaGammaH2mu2vRatio1() const;
3351 const double deltaGammaH2mu2vRatio2() const;
3357 virtual const double BrH2mu2vRatio() const;
3358
3359
3365 const double GammaH2u2uRatio() const;
3372 const double deltaGammaH2u2uRatio1() const;
3379 const double deltaGammaH2u2uRatio2() const;
3385 virtual const double BrH2u2uRatio() const;
3386
3392 const double GammaH2d2dRatio() const;
3399 const double deltaGammaH2d2dRatio1() const;
3406 const double deltaGammaH2d2dRatio2() const;
3412 virtual const double BrH2d2dRatio() const;
3413
3419 const double GammaH2u2dRatio() const;
3426 const double deltaGammaH2u2dRatio1() const;
3433 const double deltaGammaH2u2dRatio2() const;
3439 virtual const double BrH2u2dRatio() const;
3440
3446 const double GammaH2L2uRatio() const;
3453 const double deltaGammaH2L2uRatio1() const;
3460 const double deltaGammaH2L2uRatio2() const;
3466 virtual const double BrH2L2uRatio() const;
3467
3473 const double GammaH2L2dRatio() const;
3480 const double deltaGammaH2L2dRatio1() const;
3487 const double deltaGammaH2L2dRatio2() const;
3493 virtual const double BrH2L2dRatio() const;
3494
3500 const double GammaH2v2uRatio() const;
3507 const double deltaGammaH2v2uRatio1() const;
3514 const double deltaGammaH2v2uRatio2() const;
3520 virtual const double BrH2v2uRatio() const;
3521
3527 const double GammaH2v2dRatio() const;
3534 const double deltaGammaH2v2dRatio1() const;
3541 const double deltaGammaH2v2dRatio2() const;
3547 virtual const double BrH2v2dRatio() const;
3548
3554 const double GammaH4LRatio() const;
3561 const double deltaGammaH4LRatio1() const;
3568 const double deltaGammaH4LRatio2() const;
3574 virtual const double BrH4LRatio() const;
3575
3576
3582 const double GammaH4L2Ratio() const;
3589 const double deltaGammaH4L2Ratio1() const;
3596 const double deltaGammaH4L2Ratio2() const;
3602 virtual const double BrH4L2Ratio() const;
3603
3604
3610 const double GammaH4eRatio() const;
3617 const double deltaGammaH4eRatio1() const;
3624 const double deltaGammaH4eRatio2() const;
3630 virtual const double BrH4eRatio() const;
3631
3632
3638 const double GammaH4muRatio() const;
3645 const double deltaGammaH4muRatio1() const;
3652 const double deltaGammaH4muRatio2() const;
3658 virtual const double BrH4muRatio() const;
3659
3660
3666 const double GammaH4vRatio() const;
3673 const double deltaGammaH4vRatio1() const;
3680 const double deltaGammaH4vRatio2() const;
3686 virtual const double BrH4vRatio() const;
3687
3693 const double GammaH4uRatio() const;
3700 const double deltaGammaH4uRatio1() const;
3707 const double deltaGammaH4uRatio2() const;
3713 virtual const double BrH4uRatio() const;
3714
3720 const double GammaH4dRatio() const;
3727 const double deltaGammaH4dRatio1() const;
3734 const double deltaGammaH4dRatio2() const;
3740 virtual const double BrH4dRatio() const;
3741
3747 const double GammaHLvvLRatio() const;
3754 const double deltaGammaHLvvLRatio1() const;
3761 const double deltaGammaHLvvLRatio2() const;
3767 virtual const double BrHLvvLRatio() const;
3768
3774 const double GammaHevmuvRatio() const;
3781 const double deltaGammaHevmuvRatio1() const;
3788 const double deltaGammaHevmuvRatio2() const;
3794 virtual const double BrHevmuvRatio() const;
3795
3796
3802 const double GammaHudduRatio() const;
3809 const double deltaGammaHudduRatio1() const;
3816 const double deltaGammaHudduRatio2() const;
3822 virtual const double BrHudduRatio() const;
3823
3829 const double GammaHLvudRatio() const;
3836 const double deltaGammaHLvudRatio1() const;
3843 const double deltaGammaHLvudRatio2() const;
3849 virtual const double BrHLvudRatio() const;
3850
3856 const double GammaH2udRatio() const;
3863 const double deltaGammaH2udRatio1() const;
3870 const double deltaGammaH2udRatio2() const;
3876 virtual const double BrH2udRatio() const;
3877
3883 const double GammaH2LvRatio() const;
3890 const double deltaGammaH2LvRatio1() const;
3897 const double deltaGammaH2LvRatio2() const;
3903 virtual const double BrH2LvRatio() const;
3904
3910 const double GammaH2Lv2Ratio() const;
3917 const double deltaGammaH2Lv2Ratio1() const;
3924 const double deltaGammaH2Lv2Ratio2() const;
3930 virtual const double BrH2Lv2Ratio() const;
3931
3932
3938 const double GammaH2evRatio() const;
3945 const double deltaGammaH2evRatio1() const;
3952 const double deltaGammaH2evRatio2() const;
3958 virtual const double BrH2evRatio() const;
3959
3960
3966 const double GammaH2muvRatio() const;
3973 const double deltaGammaH2muvRatio1() const;
3980 const double deltaGammaH2muvRatio2() const;
3986 virtual const double BrH2muvRatio() const;
3987
3988
3994 const double GammaH4fRatio() const;
4001 const double deltaGammaH4fRatio1() const;
4008 const double deltaGammaH4fRatio2() const;
4014 virtual const double BrH4fRatio() const;
4015
4016
4022 const double GammaH4fNCRatio() const;
4029 const double deltaGammaH4fNCRatio1() const;
4036 const double deltaGammaH4fNCRatio2() const;
4042 virtual const double BrH4fNCRatio() const;
4043
4049 const double GammaH4fCCRatio() const;
4056 const double deltaGammaH4fCCRatio1() const;
4063 const double deltaGammaH4fCCRatio2() const;
4069 virtual const double BrH4fCCRatio() const;
4070
4071
4072 // DECAYS INVOLVING ONLY ELECTRONS, MUONS OR NEUTRINOS IN THE FINAL STATES
4073
4079 const double GammaH4lRatio() const;
4086 const double deltaGammaH4lRatio1() const;
4093 const double deltaGammaH4lRatio2() const;
4099 virtual const double BrH4lRatio() const;
4100
4106 const double GammaH2l2vRatio() const;
4113 const double deltaGammaH2l2vRatio1() const;
4120 const double deltaGammaH2l2vRatio2() const;
4126 virtual const double BrH2l2vRatio() const;
4127
4129
4135 const double GammaHlljjRatio() const;
4142 const double deltaGammaHlljjRatio1() const;
4149 const double deltaGammaHlljjRatio2() const;
4155 virtual const double BrHlljjRatio() const;
4156
4157
4163 const double GammaHlvjjRatio() const;
4170 const double deltaGammaHlvjjRatio1() const;
4177 const double deltaGammaHlvjjRatio2() const;
4183 virtual const double BrHlvjjRatio() const;
4184
4185
4191 const double GammaHlv_lvorjjRatio() const;
4198 const double deltaGammaHlv_lvorjjRatio1() const;
4205 const double deltaGammaHlv_lvorjjRatio2() const;
4211 virtual const double BrHlv_lvorjjRatio() const;
4212
4213
4219 const double GammaHll_vvorjjRatio() const;
4226 const double deltaGammaHll_vvorjjRatio1() const;
4233 const double deltaGammaHll_vvorjjRatio2() const;
4239 virtual const double BrHll_vvorjjRatio() const;
4240
4242
4247 virtual const double Br_H_exo() const;
4252 virtual const double Br_H_inv() const;
4258 virtual const double Br_H_inv_NP() const;
4264 virtual const double BrHvisRatio() const;
4270 virtual const double BrHtoinvRatio() const;
4271
4273
4280 virtual const double muttHZbbboost(const double sqrt_s) const;
4281
4288 virtual const double muttHgagaZeeboost(const double sqrt_s) const;
4289
4297 virtual const double muggHgaga(const double sqrt_s) const;
4305 virtual const double muVBFHgaga(const double sqrt_s) const;
4313 virtual const double muZHgaga(const double sqrt_s) const;
4321 virtual const double muWHgaga(const double sqrt_s) const;
4329 virtual const double muVHgaga(const double sqrt_s) const;
4337 virtual const double muttHgaga(const double sqrt_s) const;
4345 virtual const double muggHZga(const double sqrt_s) const;
4353 virtual const double muVBFHZga(const double sqrt_s) const;
4361 virtual const double muZHZga(const double sqrt_s) const;
4369 virtual const double muWHZga(const double sqrt_s) const;
4377 virtual const double muVHZga(const double sqrt_s) const;
4385 virtual const double muttHZga(const double sqrt_s) const;
4393 virtual const double muggHZZ(const double sqrt_s) const;
4401 virtual const double muVBFHZZ(const double sqrt_s) 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;
4433 virtual const double muttHZZ(const double sqrt_s) const;
4434
4442 virtual const double muggHZZ4l(const double sqrt_s) const;
4450 virtual const double muVBFHZZ4l(const double sqrt_s) const;
4458 virtual const double muZHZZ4l(const double sqrt_s) const;
4466 virtual const double muWHZZ4l(const double sqrt_s) const;
4474 virtual const double muVHZZ4l(const double sqrt_s) const;
4482 virtual const double muttHZZ4l(const double sqrt_s) const;
4483
4491 virtual const double muggHWW(const double sqrt_s) const;
4499 virtual const double muVBFHWW(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;
4531 virtual const double muttHWW(const double sqrt_s) const;
4539 virtual const double muggHWW2l2v(const double sqrt_s) const;
4547 virtual const double muVBFHWW2l2v(const double sqrt_s) const;
4555 virtual const double muZHWW2l2v(const double sqrt_s) const;
4563 virtual const double muWHWW2l2v(const double sqrt_s) const;
4571 virtual const double muVHWW2l2v(const double sqrt_s) const;
4579 virtual const double muttHWW2l2v(const double sqrt_s) const;
4587 virtual const double muggHmumu(const double sqrt_s) const;
4595 virtual const double muVBFHmumu(const double sqrt_s) const;
4603 virtual const double muZHmumu(const double sqrt_s) const;
4611 virtual const double muWHmumu(const double sqrt_s) const;
4619 virtual const double muVHmumu(const double sqrt_s) const;
4627 virtual const double muttHmumu(const double sqrt_s) const;
4635 virtual const double muggHtautau(const double sqrt_s) const;
4643 virtual const double muVBFHtautau(const double sqrt_s) const;
4651 virtual const double muZHtautau(const double sqrt_s) const;
4659 virtual const double muWHtautau(const double sqrt_s) const;
4667 virtual const double muVHtautau(const double sqrt_s) const;
4675 virtual const double muttHtautau(const double sqrt_s) const;
4683 virtual const double muggHbb(const double sqrt_s) const;
4691 virtual const double muVBFHbb(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;
4723 virtual const double muttHbb(const double sqrt_s) const;
4724
4726 //-----------------------------------------------------------------------------------------
4727 //-- Special Hadron collider signal strengths with separate full TH unc U(prod x decay) ---
4728 //-----------------------------------------------------------------------------------------
4730
4738 virtual const double muTHUggHgaga(const double sqrt_s) const;
4746 virtual const double muTHUVBFHgaga(const double sqrt_s) const;
4754 virtual const double muTHUZHgaga(const double sqrt_s) const;
4762 virtual const double muTHUWHgaga(const double sqrt_s) const;
4770 virtual const double muTHUVHgaga(const double sqrt_s) const;
4778 virtual const double muTHUttHgaga(const double sqrt_s) const;
4786 virtual const double muTHUggHZga(const double sqrt_s) const;
4794 virtual const double muTHUVBFHZga(const double sqrt_s) const;
4802 virtual const double muTHUZHZga(const double sqrt_s) const;
4810 virtual const double muTHUWHZga(const double sqrt_s) const;
4818 virtual const double muTHUVHZga(const double sqrt_s) const;
4826 virtual const double muTHUttHZga(const double sqrt_s) const;
4834 virtual const double muTHUggHZZ(const double sqrt_s) const;
4842 virtual const double muTHUVBFHZZ(const double sqrt_s) const;
4850 virtual const double muTHUZHZZ(const double sqrt_s) const;
4858 virtual const double muTHUWHZZ(const double sqrt_s) const;
4866 virtual const double muTHUVHZZ(const double sqrt_s) const;
4874 virtual const double muTHUttHZZ(const double sqrt_s) const;
4875
4883 virtual const double muTHUggHZZ4l(const double sqrt_s) const;
4891 virtual const double muTHUVBFHZZ4l(const double sqrt_s) const;
4899 virtual const double muTHUZHZZ4l(const double sqrt_s) const;
4907 virtual const double muTHUWHZZ4l(const double sqrt_s) const;
4915 virtual const double muTHUVHZZ4l(const double sqrt_s) const;
4923 virtual const double muTHUttHZZ4l(const double sqrt_s) const;
4924
4932 virtual const double muTHUggHWW(const double sqrt_s) const;
4940 virtual const double muTHUVBFHWW(const double sqrt_s) const;
4948 virtual const double muTHUZHWW(const double sqrt_s) const;
4956 virtual const double muTHUWHWW(const double sqrt_s) const;
4964 virtual const double muTHUVHWW(const double sqrt_s) const;
4972 virtual const double muTHUttHWW(const double sqrt_s) const;
4980 virtual const double muTHUggHWW2l2v(const double sqrt_s) const;
4988 virtual const double muTHUVBFHWW2l2v(const double sqrt_s) const;
4996 virtual const double muTHUZHWW2l2v(const double sqrt_s) const;
5004 virtual const double muTHUWHWW2l2v(const double sqrt_s) const;
5012 virtual const double muTHUVHWW2l2v(const double sqrt_s) const;
5020 virtual const double muTHUttHWW2l2v(const double sqrt_s) const;
5028 virtual const double muTHUggHmumu(const double sqrt_s) const;
5036 virtual const double muTHUVBFHmumu(const double sqrt_s) const;
5044 virtual const double muTHUZHmumu(const double sqrt_s) const;
5052 virtual const double muTHUWHmumu(const double sqrt_s) const;
5060 virtual const double muTHUVHmumu(const double sqrt_s) const;
5068 virtual const double muTHUttHmumu(const double sqrt_s) const;
5076 virtual const double muTHUggHtautau(const double sqrt_s) const;
5084 virtual const double muTHUVBFHtautau(const double sqrt_s) const;
5092 virtual const double muTHUZHtautau(const double sqrt_s) const;
5100 virtual const double muTHUWHtautau(const double sqrt_s) const;
5108 virtual const double muTHUVHtautau(const double sqrt_s) const;
5116 virtual const double muTHUttHtautau(const double sqrt_s) const;
5124 virtual const double muTHUggHbb(const double sqrt_s) const;
5132 virtual const double muTHUVBFHbb(const double sqrt_s) const;
5140 virtual const double muTHUZHbb(const double sqrt_s) const;
5148 virtual const double muTHUWHbb(const double sqrt_s) const;
5156 virtual const double muTHUVHbb(const double sqrt_s) const;
5164 virtual const double muTHUttHbb(const double sqrt_s) const;
5165
5174 virtual const double muTHUVBFBRinv(const double sqrt_s) const;
5182 virtual const double muTHUVBFHinv(const double sqrt_s) const;
5191 virtual const double muTHUVHBRinv(const double sqrt_s) const;
5199 virtual const double muTHUVHinv(const double sqrt_s) const;
5200
5208 virtual const double muTHUggHZZ4mu(const double sqrt_s) const;
5216 virtual const double muTHUggHZgamumu(const double sqrt_s) const;
5217
5219
5224 virtual const double deltaeNP(const double mu) const;
5225
5227
5228
5233 virtual const double deltag1ZNP(const double mu) const;
5234
5239 virtual const double deltaKZNP(const double mu) const;
5240
5245 virtual const double deltag1gaNP(const double mu) const;
5246
5251 virtual const double deltaKgammaNP(const double mu) const;
5252
5257 virtual const double lambdaZNP(const double mu) const;
5258
5260
5266 virtual const double deltag1ZNPEff() const;
5267
5273 virtual const double deltaKgammaNPEff() const;
5274
5276
5286 virtual const double deltaxseeWW4fLEP2(const double sqrt_s, const int fstate) const;
5287
5297 virtual const double xseeWW4fLEP2(const double sqrt_s, const int fstate) const;
5298
5305 virtual const double deltaxseeWWtotLEP2(const double sqrt_s) const;
5306
5307
5314 virtual const double xseeWWtotLEP2(const double sqrt_s) const;
5315
5323 virtual const double deltadxsdcoseeWWlvjjLEP2(const double sqrt_s, const int bin) const;
5324
5332 virtual const double dxsdcoseeWWlvjjLEP2(const double sqrt_s, const int bin) const;
5333
5339 virtual const double dxseeWWdcos(const double sqrt_s, const double cos) const;
5340
5346 virtual const double dxseeWWdcosBin(const double sqrt_s, const double cos1, const double cos2) const;
5347
5353 virtual const double xseeWW(const double sqrt_s) const;
5354
5363 virtual const double mueeWW(const double sqrt_s, const double Pol_em, const double Pol_ep) const;
5364
5366
5367 //----- High Energy diboson observables at hadron colliders
5368
5374 virtual const double ppZHprobe(const double sqrt_s) const;
5375
5383 virtual const double mupTVppWZ(const double sqrt_s, const double pTV1, const double pTV2) const;
5384
5385
5387
5388 //----- Simplified Template Cross Sections Bins
5389
5390 //----- Stage 0
5391
5396 virtual const double STXS0_qqH(const double sqrt_s) const;
5397
5398
5399 //----- Stage 1
5400
5405 virtual const double STXS_ggH_VBFtopo_j3v(const double sqrt_s) const;
5406
5407
5412 virtual const double STXS_ggH_VBFtopo_j3(const double sqrt_s) const;
5413
5418 virtual const double STXS_ggH0j(const double sqrt_s) const;
5419
5424 virtual const double STXS_ggH1j_pTH_0_60(const double sqrt_s) const;
5425
5430 virtual const double STXS_ggH1j_pTH_60_120(const double sqrt_s) const;
5431
5436 virtual const double STXS_ggH1j_pTH_120_200(const double sqrt_s) const;
5437
5442 virtual const double STXS_ggH1j_pTH_200(const double sqrt_s) const;
5443
5448 virtual const double STXS_ggH2j_pTH_0_200(const double sqrt_s) const;
5449
5454 virtual const double STXS_ggH2j_pTH_0_60(const double sqrt_s) const;
5455
5456
5461 virtual const double STXS_ggH2j_pTH_60_120(const double sqrt_s) const;
5462
5463
5468 virtual const double STXS_ggH2j_pTH_120_200(const double sqrt_s) const;
5469
5470
5475 virtual const double STXS_ggH2j_pTH_200(const double sqrt_s) const;
5476
5481 virtual const double STXS_qqHqq_VBFtopo_Rest(const double sqrt_s) const;
5482
5483
5488 virtual const double STXS_qqHqq_VBFtopo_j3v(const double sqrt_s) const;
5489
5490
5495 virtual const double STXS_qqHqq_VBFtopo_j3(const double sqrt_s) const;
5496
5501 virtual const double STXS_qqHqq_nonVHtopo(const double sqrt_s) const;
5502
5507 virtual const double STXS_qqHqq_VHtopo(const double sqrt_s) const;
5508
5513 virtual const double STXS_qqHqq_Rest(const double sqrt_s) const;
5514
5519 virtual const double STXS_qqHqq_pTj_200(const double sqrt_s) const;
5520
5525 virtual const double STXS_qqHlv_pTV_0_250(const double sqrt_s) const;
5526
5527
5532 virtual const double STXS_qqHlv_pTV_0_150(const double sqrt_s) const;
5533
5534
5539 virtual const double STXS_qqHlv_pTV_150_250_0j(const double sqrt_s) const;
5540
5541
5546 virtual const double STXS_qqHlv_pTV_150_250_1j(const double sqrt_s) const;
5547
5548
5553 virtual const double STXS_qqHlv_pTV_250(const double sqrt_s) const;
5554
5559 virtual const double STXS_qqHll_pTV_0_150(const double sqrt_s) const;
5560
5565 virtual const double STXS_qqHll_pTV_150_250(const double sqrt_s) const;
5566
5567
5572 virtual const double STXS_qqHll_pTV_150_250_0j(const double sqrt_s) const;
5573
5574
5579 virtual const double STXS_qqHll_pTV_150_250_1j(const double sqrt_s) const;
5580
5585 virtual const double STXS_qqHll_pTV_250(const double sqrt_s) const;
5586
5587
5592 virtual const double STXS_ttHtH(const double sqrt_s) const;
5593
5598 virtual const double STXS_WHqqHqq_VBFtopo_j3v(const double sqrt_s) const;
5599
5604 virtual const double STXS_WHqqHqq_VBFtopo_j3(const double sqrt_s) const;
5605
5610 virtual const double STXS_WHqqHqq_VH2j(const double sqrt_s) const;
5611
5616 virtual const double STXS_WHqqHqq_Rest(const double sqrt_s) const;
5617
5622 virtual const double STXS_WHqqHqq_pTj1_200(const double sqrt_s) const;
5623
5628 virtual const double STXS_ZHqqHqq_VBFtopo_j3v(const double sqrt_s) const;
5629
5634 virtual const double STXS_ZHqqHqq_VBFtopo_j3(const double sqrt_s) const;
5635
5640 virtual const double STXS_ZHqqHqq_VH2j(const double sqrt_s) const;
5641
5646 virtual const double STXS_ZHqqHqq_Rest(const double sqrt_s) const;
5647
5652 virtual const double STXS_ZHqqHqq_pTj1_200(const double sqrt_s) const;
5653
5654
5655 //----- Stage 1.2
5656 // From ATLAS-CONF-2020-053
5657 // Expressions valid in the {G_F, M_Z, M_W} scheme
5658
5662 virtual const double STXS12_BrH4lRatio() const;
5663
5667 virtual const double STXS12_BrHevmuvRatio() const;
5668
5672 virtual const double STXS12_BrHgagaRatio() const;
5673
5677 virtual const double STXS12_BrHbbRatio() const;
5678
5683 virtual const double STXS12_ggH_pTH200_300_Nj01(const double sqrt_s) const;
5684
5689 virtual const double STXS12_ggH_pTH300_450_Nj01(const double sqrt_s) const;
5690
5695 virtual const double STXS12_ggH_pTH450_650_Nj01(const double sqrt_s) const;
5696
5701 virtual const double STXS12_ggH_pTH650_Inf_Nj01(const double sqrt_s) const;
5702
5707 virtual const double STXS12_ggH_pTH0_10_Nj0(const double sqrt_s) const;
5708
5709
5714 virtual const double STXS12_ggH_pTH10_200_Nj0(const double sqrt_s) const;
5715
5720 virtual const double STXS12_ggH_pTH10_Inf_Nj0(const double sqrt_s) const;
5721
5726 virtual const double STXS12_ggH_pTH0_60_Nj1(const double sqrt_s) const;
5727
5728
5733 virtual const double STXS12_ggH_mjj0_350_pTH0_60_Nj1(const double sqrt_s) const;
5734
5739 virtual const double STXS12_ggH_pTH60_120_Nj1(const double sqrt_s) const;
5740
5745 virtual const double STXS12_ggH_pTH120_200_Nj1(const double sqrt_s) const;
5746
5751 virtual const double STXS12_ggH_mjj0_350_pTH0_60_Nj2(const double sqrt_s) const;
5752
5757 virtual const double STXS12_ggH_mjj0_350_pTH60_120_Nj2(const double sqrt_s) const;
5758
5763 virtual const double STXS12_ggH_mjj0_350_pTH120_200_Nj2(const double sqrt_s) const;
5764
5769 virtual const double STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2(const double sqrt_s) const;
5770
5775 virtual const double STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2(const double sqrt_s) const;
5776
5781 virtual const double STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2(const double sqrt_s) const;
5782
5787 virtual const double STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2(const double sqrt_s) const;
5788
5793 virtual const double STXS12_ggH_mjj350_700_pTH0_200_Nj2(const double sqrt_s) const; //AG:added
5794
5799 virtual const double STXS12_ggH_mjj700_Inf_pTH0_200_Nj2(const double sqrt_s) const; //AG:added
5800
5801
5806 virtual const double STXS12_ggH_pTH200_300(const double sqrt_s) const;
5807
5808
5813 virtual const double STXS12_ggH_pTH300_450(const double sqrt_s) const;
5814
5815
5820 virtual const double STXS12_ggH_pTH450_Inf(const double sqrt_s) const;
5821
5822
5827 virtual const double STXS12_ggH_pTH450_650(const double sqrt_s) const;
5828
5829
5834 virtual const double STXS12_ggH_pTH650_Inf(const double sqrt_s) const;
5835
5836
5841 virtual const double STXS12_ggHll_pTV0_75(const double sqrt_s) const;
5842
5847 virtual const double STXS12_ggHll_pTV75_150(const double sqrt_s) const;
5848
5853 virtual const double STXS12_ggHll_pTV150_250_Nj0(const double sqrt_s) const;
5854
5859 virtual const double STXS12_ggHll_pTV150_250_Nj1(const double sqrt_s) const;
5860
5865 virtual const double STXS12_ggHll_pTV250_Inf(const double sqrt_s) const;
5866
5867
5868
5873 virtual const double STXS12_qqHqq_VH_veto_Nj01(const double sqrt_s) const;
5874
5875
5876
5877
5882 virtual const double STXS12_qqHqq_Nj0(const double sqrt_s) const;
5883
5888 virtual const double STXS12_qqHqq_Nj1(const double sqrt_s) const;
5889
5894 virtual const double STXS12_qqHqq_mjj0_60_Nj2(const double sqrt_s) const;
5895
5900 virtual const double STXS12_qqHqq_mjj60_120_Nj2(const double sqrt_s) const;
5901
5906 virtual const double STXS12_qqHqq_mjj120_350_Nj2(const double sqrt_s) const;
5907
5912 virtual const double STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2(const double sqrt_s) const;
5913
5914
5915
5920 virtual const double STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2(const double sqrt_s) const;
5921
5926 virtual const double STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2(const double sqrt_s) const;
5927
5932 virtual const double STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2(const double sqrt_s) const;
5933
5938 virtual const double STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2(const double sqrt_s) const;
5939
5944 virtual const double STXS12_qqHqq_mjj350_700_pTH0_200_Nj2(const double sqrt_s) const; //AG:added
5945
5950 virtual const double STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2(const double sqrt_s) const; //AG:added
5951
5956 virtual const double STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2(const double sqrt_s) const; //AG:added
5957
5962 virtual const double STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2(const double sqrt_s) const; //AG:added
5963
5968 virtual const double STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2(const double sqrt_s) const; //AG:added
5969
5974 virtual const double STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2(const double sqrt_s) const; //AG:added
5975
5980 virtual const double STXS12_qqHlv_pTV0_75(const double sqrt_s) const;
5981
5986 virtual const double STXS12_qqHlv_pTV75_150(const double sqrt_s) const;
5987
5992 virtual const double STXS12_qqHlv_pTV150_250_Nj0(const double sqrt_s) const;
5993
5998 virtual const double STXS12_qqHlv_pTV150_250_Nj1(const double sqrt_s) const;
5999
6004 virtual const double STXS12_qqHlv_pTV250_Inf(const double sqrt_s) const;
6005
6010 virtual const double STXS12_qqHlv_pTV0_150(const double sqrt_s) const; //AG:added
6011
6016 virtual const double STXS12_qqHlv_pTV250_400(const double sqrt_s) const; //AG:added
6017
6022 virtual const double STXS12_qqHlv_pTV400_Inf(const double sqrt_s) const; //AG:added
6023
6028 virtual const double STXS12_qqHll_pTV0_75(const double sqrt_s) const;
6029
6034 virtual const double STXS12_qqHll_pTV75_150(const double sqrt_s) const;
6035
6040 virtual const double STXS12_qqHll_pTV150_250_Nj0(const double sqrt_s) const;
6041
6046 virtual const double STXS12_qqHll_pTV150_250_Nj1(const double sqrt_s) const;
6047
6052 virtual const double STXS12_qqHll_pTV250_Inf(const double sqrt_s) const;
6053
6058 virtual const double STXS12_qqHll_pTV0_150(const double sqrt_s) const; //AG:added
6059
6064 virtual const double STXS12_qqHll_pTV250_400(const double sqrt_s) const; //AG:added
6065
6070 virtual const double STXS12_qqHll_pTV400_Inf(const double sqrt_s) const; //AG:added
6071
6076 virtual const double STXS12_ttH_pTH0_60(const double sqrt_s) const;
6077
6082 virtual const double STXS12_ttH_pTH60_120(const double sqrt_s) const;
6083
6088 virtual const double STXS12_ttH_pTH120_200(const double sqrt_s) const;
6089
6094 virtual const double STXS12_ttH_pTH200_300(const double sqrt_s) const;
6095
6100 virtual const double STXS12_ttH_pTH300_Inf(const double sqrt_s) const;
6101
6106 virtual const double STXS12_ttH_pTH300_450(const double sqrt_s) const; //AG:added
6107
6112 virtual const double STXS12_ttH_pTH450_Inf(const double sqrt_s) const; //AG:added
6113
6118 virtual const double STXS12_tH(const double sqrt_s) const;
6119
6121
6126 virtual const double kappamueff() const;
6127
6132 virtual const double kappataueff() const;
6133
6138 virtual const double kappaceff() const;
6139
6144 virtual const double kappaseff() const;
6145
6150 virtual const double kappabeff() const;
6151
6156 virtual const double kappaGeff() const;
6157
6162 virtual const double kappaZeff() const;
6163
6168 virtual const double kappaWeff() const;
6169
6174 virtual const double kappaZ4feff() const;
6175
6180 virtual const double kappaW4feff() const;
6181
6186 virtual const double kappaAeff() const;
6187
6192 virtual const double kappaZAeff() const;
6193
6195
6207 virtual const double deltayt_HB(const double mu) const;
6208
6220 virtual const double deltayb_HB(const double mu) const;
6221
6233 virtual const double deltaytau_HB(const double mu) const;
6234
6246 virtual const double deltayc_HB(const double mu) const;
6247
6248
6260 virtual const double deltays_HB(const double mu) const;
6261
6273 virtual const double deltaymu_HB(const double mu) const;
6274
6286 virtual const double deltacZ_HB(const double mu) const;
6287
6299 virtual const double cZBox_HB(const double mu) const;
6300
6312 virtual const double cZZ_HB(const double mu) const;
6313
6325 virtual const double cZga_HB(const double mu) const;
6326
6338 virtual const double cgaga_HB(const double mu) const;
6339
6351 virtual const double cgg_HB(const double mu) const;
6352
6364 virtual const double cggEff_HB(const double mu) const;
6365
6377 virtual const double lambz_HB(const double mu) const;
6378
6380
6386 virtual const double CEWHL111(const double mu) const;
6387
6393 virtual const double CEWHL122(const double mu) const;
6394
6400 virtual const double CEWHL133(const double mu) const;
6401
6407 virtual const double CEWHL311(const double mu) const;
6408
6414 virtual const double CEWHL322(const double mu) const;
6415
6421 virtual const double CEWHL333(const double mu) const;
6422
6428 virtual const double CEWHQ111(const double mu) const;
6429
6435 virtual const double CEWHQ122(const double mu) const;
6436
6442 virtual const double CEWHQ133(const double mu) const;
6443
6449 virtual const double CEWHQ311(const double mu) const;
6450
6456 virtual const double CEWHQ322(const double mu) const;
6457
6463 virtual const double CEWHQ333(const double mu) const;
6464
6465
6471 virtual const double CEWHQd33(const double mu) const;
6472
6478 virtual const double CEWHQu33(const double mu) const;
6479
6480
6486 virtual const double CEWHe11(const double mu) const;
6487
6493 virtual const double CEWHe22(const double mu) const;
6494
6500 virtual const double CEWHe33(const double mu) const;
6501
6502
6508 virtual const double CEWHu11(const double mu) const;
6509
6515 virtual const double CEWHu22(const double mu) const;
6516
6522 virtual const double CEWHu33(const double mu) const;
6523
6524
6530 virtual const double CEWHd11(const double mu) const;
6531
6537 virtual const double CEWHd22(const double mu) const;
6538
6544 virtual const double CEWHd33(const double mu) const;
6545
6551 virtual const double CEWll(const double mu) const;
6552
6553
6554 //----- The same, in the quark mass basis ----------
6555
6561 virtual const double CEWHQ1uu(const double mu) const;
6562
6568 virtual const double CEWHQ1cc(const double mu) const;
6569
6575 virtual const double CEWHQ1tt(const double mu) const;
6576
6582 virtual const double CEWHQ1dd(const double mu) const;
6583
6589 virtual const double CEWHQ1ss(const double mu) const;
6590
6596 virtual const double CEWHQ1bb(const double mu) const;
6597
6598
6604 virtual const double CEWHQ3uu(const double mu) const;
6605
6611 virtual const double CEWHQ3cc(const double mu) const;
6612
6618 virtual const double CEWHQ3tt(const double mu) const;
6619
6625 virtual const double CEWHQ3dd(const double mu) const;
6626
6632 virtual const double CEWHQ3ss(const double mu) const;
6633
6639 virtual const double CEWHQ3bb(const double mu) const;
6640
6641
6642
6648 virtual const double CEWHuuu(const double mu) const;
6649
6655 virtual const double CEWHucc(const double mu) const;
6656
6662 virtual const double CEWHutt(const double mu) const;
6663
6664
6670 virtual const double CEWHddd(const double mu) const;
6671
6677 virtual const double CEWHdss(const double mu) const;
6678
6684 virtual const double CEWHdbb(const double mu) const;
6685
6686
6688
6693 virtual const double NevLHCppee13(const int i_bin) const;
6694
6699 virtual const double NevLHCppmumu13(const int i_bin) const;
6700
6705 virtual const double NevLHCpptautau13(const int i_bin) const;
6706
6708
6713 virtual const double NevLHCppenu13(const int i_bin) const;
6714
6719 virtual const double NevLHCppmunu13(const int i_bin) const;
6720
6725 virtual const double NevLHCpptaunu13(const int i_bin) const;
6726
6728
6734 virtual const double AuxObs_NP1() const;
6735
6741 virtual const double AuxObs_NP2() const;
6742
6748 virtual const double AuxObs_NP3() const;
6749
6755 virtual const double AuxObs_NP4() const;
6756
6762 virtual const double AuxObs_NP5() const;
6763
6769 virtual const double AuxObs_NP6() const;
6770
6776 virtual const double AuxObs_NP7() const;
6777
6783 virtual const double AuxObs_NP8() const;
6784
6790 virtual const double AuxObs_NP9() const;
6791
6797 virtual const double AuxObs_NP10() const;
6798
6804 virtual const double AuxObs_NP11() const;
6805
6811 virtual const double AuxObs_NP12() const;
6812
6817 virtual const double AuxObs_NP13() const;
6818
6823 virtual const double AuxObs_NP14() const;
6824
6829 virtual const double AuxObs_NP15() const;
6830
6835 virtual const double AuxObs_NP16() const;
6836
6841 virtual const double AuxObs_NP17() const;
6842
6847 virtual const double AuxObs_NP18() const;
6848
6853 virtual const double AuxObs_NP19() const;
6854
6859 virtual const double AuxObs_NP20() const;
6860
6866 virtual const double AuxObs_NP21() const;
6867
6873 virtual const double AuxObs_NP22() const;
6874
6879 virtual const double AuxObs_NP23() const;
6880
6885 virtual const double AuxObs_NP24() const;
6886
6891 virtual const double AuxObs_NP25() const;
6892
6897 virtual const double AuxObs_NP26() const;
6898
6903 virtual const double AuxObs_NP27() const;
6904
6909 virtual const double AuxObs_NP28() const;
6910
6915 virtual const double AuxObs_NP29() const;
6916
6921 virtual const double AuxObs_NP30() const;
6922
6923 // FCC-hh 84 TeV likelihoods (chi2FCChhXX)
6924
6925 const double chi2FCChh4Top() const;
6926
6927 const double chi2FCChhHtt() const;
6928 const double chi2FCChhZtt() const;
6929 const double chi2FCChhtt() const;
6930 const double chi2FCChhtb() const;
6931
6932 const double chi2FCChhHW() const;
6933 const double chi2FCChhWW() const;
6934
6935 const double chi2FCChhee() const;
6936 const double chi2FCChhmumu() const;
6937 const double chi2FCChhtata() const;
6938
6939 const double chi2FCChhenu() const;
6940 const double chi2FCChhmunu() const;
6941 const double chi2FCChhtanu() const;
6942
6943 const double chi2FCChhjj() const;
6944 const double chi2FCChhbbcc() const;
6945
6947
6948 const RGESolver& getSMEFTEvol() const {
6949 return SMEFTEvolEW;
6950 }
6951
6952 gslpp::matrix<gslpp::complex> getYd() const {
6953 return Yd;
6954 }
6955
6956 gslpp::matrix<gslpp::complex> getYe() const {
6957 return Ye;
6958 }
6959
6960 gslpp::matrix<gslpp::complex> getYu() const {
6961 return Yu;
6962 }
6963
6964 inline double getSMEFTCoeffEW(const std::string name) const
6965 {
6966 return SMEFTEvolEW.GetCoefficient(name);
6967 }
6968
6969 inline double getSMEFTCoeffEW(const std::string name, int i, int j) const
6970 {
6971 return SMEFTEvolEW.GetCoefficient(name, i, j);
6972 }
6973
6974 inline double getSMEFTCoeffEW(const std::string name, int i, int j, int k, int l) const
6975 {
6976 return SMEFTEvolEW.GetCoefficient(name, i, j, k, l);
6977 }
6978
6979 // Coefficients of fermionic operators in the mass basis
6980
6981 // Coefficients are assumed to be complex, "name" is the name without R or I at the end. That is added here
6982 inline gslpp::complex getSMEFTCoeffEWMB(const std::string name, int i, int j, gslpp::matrix<gslpp::complex> Vi, gslpp::matrix<gslpp::complex> Vj) const;
6983
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;
6985
6986 void printNonVanishingSMEFTCoeffEW() const;
6987
6988 RGESolver getSMEFTEvolEW() const
6989 {
6990 return SMEFTEvolEW;
6991 }
6992
6993 // Functions to select the operators at different scales
6994 double getSMEFTCoeff(const std::string name, const double mu) const;
6995
6996 double getSMEFTCoeff(const std::string name, int i, int j, const double mu) const;
6997
6998 double getSMEFTCoeff(const std::string name, int i, int j, int k, int l, const double mu) const;
6999
7000 // Functions used by the above to compute the approximation by a polynomial up to log^5 to the RG evolution
7001
7002 // Coeff of term proportional to log(mu/Lambda)
7003 double xlog1(const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const;
7004 // Coeff of term proportional to log^2(mu/Lambda)
7005 double xlog2(const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const;
7006 // Coeff of term proportional to log^3(mu/Lambda)
7007 double xlog3(const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const;
7008 // Coeff of term proportional to log^4(mu/Lambda)
7009 double xlog4(const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const;
7010 // Coeff of term proportional to log^5(mu/Lambda)
7011 double xlog5(const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const;
7012
7013
7014 // Coefficients of fermionic operators in the mass basis
7015
7016 // Coefficients are assumed to be complex, "name" is the name without R or I at the end. That is added here
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;
7018
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;
7020
7022
7023 const double getDelta_v() const
7024 {
7025 return delta_v;
7026 }
7027
7028 const double getCW_tree() const
7029 {
7030 return cW_tree;
7031 }
7032
7033 const double getSW_tree() const
7034 {
7035 return sW_tree;
7036 }
7037
7038 const double getEeMz() const
7039 {
7040 return eeMz;
7041 }
7042
7043 const double getGZdL() const
7044 {
7045 return gZdL;
7046 }
7047
7048 const double getGZdR() const
7049 {
7050 return gZdR;
7051 }
7052
7053 const double getGZlL() const
7054 {
7055 return gZlL;
7056 }
7057
7058 const double getGZlR() const
7059 {
7060 return gZlR;
7061 }
7062
7063 const double getGZuL() const
7064 {
7065 return gZuL;
7066 }
7067
7068 const double getGZuR() const
7069 {
7070 return gZuR;
7071 }
7072
7073 const double getGZvL() const
7074 {
7075 return gZvL;
7076 }
7077
7078 const double getG1_tree() const
7079 {
7080 return g1_tree;
7081 }
7082
7083 const double getG2_tree() const
7084 {
7085 return g2_tree;
7086 }
7087
7088 const double getG3_tree() const
7089 {
7090 return g3_tree;
7091 }
7092
7093 const double getDelta_Mz2() const
7094 {
7095 return delta_Mz2;
7096 }
7097
7098 const double getDelta_ale() const
7099 {
7100 return delta_ale;
7101 }
7102
7103 const double getDelta_g1() const
7104 {
7105 return delta_g1;
7106 }
7107
7108 const double getDelta_g2() const
7109 {
7110 return delta_g2;
7111 }
7112
7113 const double getDelta_xBZ() const
7114 {
7115 return delta_xBZ;
7116 }
7117
7118 const double getDelta_xWZ() const
7119 {
7120 return delta_xWZ;
7121 }
7122
7123 const double getXBZ_tree() const
7124 {
7125 return xBZ_tree;
7126 }
7127
7128 const double getXWZ_tree() const
7129 {
7130 return xWZ_tree;
7131 }
7132
7133 const double getMw_tree() const
7134 {
7135 return Mw_tree;
7136 }
7137
7142 const gslpp::matrix<gslpp::complex>& getVdL() const {
7143 return VdL;
7144 }
7145
7150 const gslpp::matrix<gslpp::complex>& getVdLd() const {
7151 return VdLd;
7152 }
7153
7158 const gslpp::matrix<gslpp::complex>& getVdR() const {
7159 return VdR;
7160 }
7161
7166 const gslpp::matrix<gslpp::complex>& getVdRd() const {
7167 return VdRd;
7168 }
7169
7174 const gslpp::matrix<gslpp::complex>& getVeL() const {
7175 return VeL;
7176 }
7177
7182 const gslpp::matrix<gslpp::complex>& getVeLd() const {
7183 return VeLd;
7184 }
7185
7190 const gslpp::matrix<gslpp::complex>& getVeR() const {
7191 return VeR;
7192 }
7193
7198 const gslpp::matrix<gslpp::complex>& getVeRd() const {
7199 return VeRd;
7200 }
7201
7206 const gslpp::matrix<gslpp::complex>& getVuL() const {
7207 return VuL;
7208 }
7209
7214 const gslpp::matrix<gslpp::complex>& getVuLd() const {
7215 return VuLd;
7216 }
7217
7222 const gslpp::matrix<gslpp::complex>& getVuR() const {
7223 return VuR;
7224 }
7225
7230 const gslpp::matrix<gslpp::complex>& getVuRd() const {
7231 return VuRd;
7232 }
7233
7237 const double getLambdaH_tree() const
7238 {
7239 return lambdaH_tree;
7240 }
7241 bool FlagNewTerms;
7242 bool FlagMomProp;
7243 bool FlagMomVert;
7244 bool FlagHiggsExch;
7245 bool FlagQuadraticWC;
7246
7248protected:
7249
7250 //Old definition we won't use it
7251 //virtual void ComputeQuarkMassFromMCParameters(quark q);
7252
7257 virtual void setParameter(const std::string name, const double& value);
7258
7259
7264 void ChangeToEvolutorsBasisPureSM();
7265
7266
7272 void ChangeToEvolutorsBasisSMEFTtoSM();
7273
7274
7278 //virtual void computeYukawas(); TO BE FIXED ASAP!!!!!
7279
7280
7284 void computeQuarkMassesAndCKMFromYukawas();
7285
7286
7290 void setSMEFTEvolWC(RGESolver& RGevol);
7291
7292
7296// void getWCFromEvolutor();
7297
7299
7300// Flag and integer to specify flavor basis "UP" (1, default), "DOWN" (2)
7301 std::string SMEFTBasisFlag;
7302 int flavBas = 1;
7303
7304 //For the SM parameters used in the evolutor we start at the EW scale
7305 double g1_LEW = 0;
7306 double g2_LEW = 0;
7307 double g3_LEW = 0;
7308 double lambdaH_LEW = 0;
7309 double mH2_LEW = 0;
7310 double me_LEW = 0;
7311 double mmu_LEW = 0;
7312 double mtau_LEW = 0;
7313 double mu_LEW = 0;
7314 double mc_LEW = 0;
7315 double mt_LEW = 0;
7316 double md_LEW = 0;
7317 double ms_LEW = 0;
7318 double mb_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};
7326
7327
7328 //We won't need the SM at the NP scale anymore
7329 //double g1_LNP = 0;
7330 //double g2_LNP = 0;
7331 //double g3_LNP = 0;
7332 //double lambdaH_LNP = 0;
7333 //double muH_LNP = 0;
7334 //double Ye_LNP = 0;
7335 //double Ymu_LNP = 0;
7336 //double Ytau_LNP = 0;
7337 //double Yu_LNP = 0;
7338 //double Yc_LNP = 0;
7339 //double Yt_LNP = 0;
7340 //double Yd_LNP = 0;
7341 //double Ys_LNP = 0;
7342 //double Yb_LNP = 0;
7343 //double s12CKM_LNP = 0.;
7344 //double s13CKM_LNP = 0.;
7345 //double s23CKM_LNP = 0.;
7346 //double dCKM_LNP = 0.;
7347 double CG_LNP = 0.;
7348 double CW_LNP = 0.;
7349 double CHG_LNP = 0.;
7350 double CHW_LNP = 0.;
7351 double CHB_LNP = 0.;
7352 double CDB_LNP = 0;
7353 double CDW_LNP = 0;
7354 double CHWB_LNP = 0.;
7355 double CHD_LNP = 0.;
7356 double CHbox_LNP = 0.;
7357 double CH_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.;
7648
7649 double Lambda_NP;
7650 // The intrinsic and parametric theory relative errors in the Higgs observables.
7651 double eggFint = 0.;
7652 double eggFpar = 0.;
7653 double ettHint = 0.;
7654 double ettHpar = 0.;
7655 double eVBFint = 0.;
7656 double eVBFpar = 0.;
7657 double eWHint = 0.;
7658 double eWHpar = 0.;
7659 double eZHint = 0.;
7660 double eZHpar = 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.;
7691
7692 // Intrinsic errors in \f$ee \to WW\f$ observables: error in total and differential cross section
7693 double eeeWWint = 0., edeeWWdcint = 0.;
7694
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.;
7701
7702 double eHwidth = 0.;
7703
7704 double BrHinv = 0.;
7705 double BrHexo = 0.;
7706
7707 // ----------------------------------------------------------------------------
7708 // Internal parameters
7709 // ----------------------------------------------------------------------------
7710
7711 double LambdaNP2;
7712 double LambdaNPm2;
7713
7714 double v2;
7715 double v2_over_LambdaNP2;
7716 double aleMz;
7717 double eeMz;
7718 double eeMz2;
7719 double cW_tree;
7720 double sW_tree;
7721 double cW2_tree;
7722 double sW2_tree;
7723
7724 double g1_tree;
7725 double g2_tree;
7726 double g3_tree;
7727
7728 double Mw_tree;
7729
7730 double lambdaH_tree;
7731
7732 double gZvL;
7733 double gZlL, gZlR;
7734 double gZuL, gZuR;
7735 double gZdL, gZdR;
7736
7737 double UevL;
7738 double VudL;
7739
7740 double delta_ZZ;
7741 double delta_AA;
7742 double delta_AZ;
7743
7744 double delta_Z;
7745 double delta_A;
7746 double delta_ZA;
7747
7748 double delta_h;
7749
7750 double dZH, dZH1, dZH2;
7751
7752 double cHSM;
7753
7754 double cLHd6;
7755
7756 double cLH3d62;
7757
7758 double cNLOd6;
7759
7760 double cAsch, cWsch;
7761
7762// double Yuke,Yukmu,Yuktau;///< SM lepton Yukawas
7763 double Yuku,Yukc,Yukt;
7764// double Yukd,Yuks,Yukb;///< SM d-quark Yukawas
7765
7766
7767 // STXS ci: denote them as ai to separate from the normal conventions
7768 double aiG, ai3G, ai2G;
7769 double aiT, aiH, aiWW, aiB, aiHW, aiHB;
7770 double aiA;
7771 double aiHQ, aipHQ, aiHL, aipHL, aiHu, aiHd, aiHe;
7772 double aiu, aiuG;
7773
7774 // Cache variables
7775 double dGammaHTotR1, dGammaHTotR2, GammaHTotR;
7776
7777 double delta_GF;
7778
7779 double delta_MZ;
7780 double delta_MW;
7781 double delta_v;
7782 double delta_e;
7783 double delta_sW2;
7784 double delta_UgNC;
7785 double delta_QgNC;
7786 double delta_UgCC;
7787
7788 double delta_em;
7789
7790 // Operators entering in the EWPO (mass basis)
7791 double CHq1EWuu = 0., CHq1EWcc = 0., CHq1EWtt = 0.;
7792 double CHq3EWuu = 0., CHq3EWcc = 0., CHq3EWtt = 0.;
7793 double CHuEWuu = 0., CHuEWcc = 0., CHuEWtt = 0.;
7794
7795 double CHq1EWdd = 0., CHq1EWss = 0., CHq1EWbb = 0.;
7796 double CHq3EWdd = 0., CHq3EWss = 0., CHq3EWbb = 0.;
7797 double CHdEWdd = 0., CHdEWss = 0., CHdEWbb = 0.;
7798
7799 gslpp::complex CHq3EWud = gslpp::complex(0., 0., false), CHq3EWcs = gslpp::complex(0., 0., false), CHq3EWtb = gslpp::complex(0., 0., false);
7800
7801 double C1Htotal;
7802
7803 //AG:begin
7813 double delta_GF_2;
7814
7825 double delta_ale;
7826
7835 double delta_ale_2;
7836
7844 double delta_Mz2;
7845
7858 double delta_Mz2_2;
7859
7872 double delta_g1;
7873
7891 double delta_g1_2;
7892
7902 double delta_g2;
7903
7920 double delta_g2_2;
7921
7930 double xWZ_tree;
7931
7940 double xBZ_tree;
7941
7952 double delta_xWZ;
7953
7964 double delta_xBZ;
7965
7982 double delta_xWZ_2;
7983
8000 double delta_xBZ_2;
8001 //AG:end
8002
8008 double CHF1_diag(const Particle F) const;
8009
8015 double CHF3_diag(const Particle F) const;
8016
8022 gslpp::complex CHF3CC_diag(const Particle F) const;
8023
8029 double CHf_diag(const Particle f) const;
8030
8036 gslpp::complex CHud_diag(const Particle u) const;
8037
8043 gslpp::complex CfH_diag(const Particle f) const;
8044
8050 gslpp::complex CfG_diag(const Particle f) const;
8051
8057 gslpp::complex CfW_diag(const Particle f) const;
8058
8064 gslpp::complex CfB_diag(const Particle f) const;
8065
8067 // Scale-dependent versions of some of the above
8069
8076 gslpp::complex CfH_diag_mu(const Particle f, const double mu) const;
8077
8078
8080
8081 RGESolver SMEFTEvolEW;
8082
8083 RGESolver SMEFTEvolMH, SMEFTEvol240, SMEFTEvol365, SMEFTEvol550, SMEFTEvol1000, SMEFTEvol1500, SMEFTEvol3000, SMEFTEvol5000;
8084
8085 RGESolver SMEFTEvolUV; // Reference at UV (Lambda_NP). Used to be able to access values of the coefficients via the RGEsolver methods. It is not evolved.
8086
8087 // Log of the RGE scales associated to the non-trivial evolutors (for SMEFTEvolEW the scale is muw), from top to bottom.
8088 // Initialize here to 0. Set in PostUpdate
8089 double tmu2 = 0., tmu3 = 0., tmu4 = 0., tmu5 = 0., tmuw = 0.;
8090
8091private:
8092
8093 gslpp::matrix<gslpp::complex> VuL, VuLd, VuR, VuRd, VdL, VdLd, VdR, VdRd, VeL, VeLd, VeR, VeRd, MUQ, MDQ;
8094
8095 bool FlagMWinput;
8096 bool FlagQuadraticTerms;
8097 bool FlagHiggsSM;
8098 bool FlagLoopHd6;
8099 bool FlagLoopH3d6Quad;
8100 bool FlagRGEci;
8101 bool FlagmultiScaleRGE;
8102 bool FlagfiniteNLO;
8103 bool FlagmatchLEFT;
8104 bool FlagCorrsInSMRunning;
8105
8106 gsl_integration_cquad_workspace * w_WW;
8107 double ZeroAle(double *dAle5h, double *params); //This was define as a const but we're changing the value of dAle5h so it shouldn't be a const function
8108 bool isSMInitialConditionComputed;
8109
8110};
8111
8112#endif /* NPSMEFTD6GENERAL_H */
8113
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.
Definition: Model.h:285
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.
Definition: NPbase.h:66
virtual const double BrHlljjRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPbase.h:2608
A class for particles.
Definition: Particle.h:26
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.
Test Observable.
Test Observable.
StdVectorFiller< int > Vi
const double sqrt_s[12]