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NPEffectiveGIMR.h
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1 /*
2  * Copyright (C) 2014 HEPfit Collaboration
3  *
4  *
5  * For the licensing terms see doc/COPYING.
6  */
7 
8 #ifndef NPEFFECTIVEGIMR_H
9 #define NPEFFECTIVEGIMR_H
10 
11 #include "gslpp.h"
12 #include "NPbase.h"
13 #include "LEP2GIMR.h"
14 #include <string.h>
15 #include <stdexcept>
16 
17 
610 class NPEffectiveGIMR : public NPbase {
611 public:
612 
616  static const int NNPEffectiveGIMRVars = 331;
617 
622  static const std::string NPEffectiveGIMRVars[NNPEffectiveGIMRVars];
623 
628  static const int NNPEffectiveGIMRVars_LFU_QFU = 121;
629 
634  static const std::string NPEffectiveGIMRVars_LFU_QFU[NNPEffectiveGIMRVars_LFU_QFU];
635 
641  NPEffectiveGIMR(const bool FlagLeptonUniversal_in = false, const bool FlagQuarkUniversal_in = false);
642 
649  virtual bool PostUpdate();
650 
658  virtual bool CheckParameters(const std::map<std::string, double>& DPars);
659 
666  virtual bool setFlag(const std::string name, const bool value);
667 
668 
670 
681  virtual double DeltaGF() const;
682 
687  virtual double obliqueS() const;
688 
693  virtual double obliqueT() const;
694 
699  virtual double obliqueU() const;
700 
701  virtual double deltaMz2() const;
702 
707  virtual double Mw() const;
708 
713  virtual double GammaW() const;
714 
720  virtual double deltaGV_f(const Particle p) const;
721 
727  virtual double deltaGA_f(const Particle p) const;
728 
734  // no generation mixing
735  double deltaGL_f(const Particle p) const;
736 
742  // no generation mixing
743  double deltaGR_f(const Particle p) const;
744 
745 
747 
748  double CLL_mu() const;
749  double CLL_tau() const;
750  double CLL_up() const;
751  double CLL_down() const;
752  double CLL_charm() const;
753  double CLL_strange() const;
754  double CLL_bottom() const;
755 
756  double CLR_mu() const;
757  double CLR_tau() const;
758  double CLR_up() const;
759  double CLR_down() const;
760  double CLR_charm() const;
761  double CLR_strange() const;
762  double CLR_bottom() const;
763 
764  double CRL_mu() const;
765  double CRL_tau() const;
766  double CRL_up() const;
767  double CRL_down() const;
768  double CRL_charm() const;
769  double CRL_strange() const;
770  double CRL_bottom() const;
771 
772  double CRR_mu() const;
773  double CRR_tau() const;
774  double CRR_up() const;
775  double CRR_down() const;
776  double CRR_charm() const;
777  double CRR_strange() const;
778  double CRR_bottom() const;
779 
781 
783 
790  // no generation mixing
791  virtual gslpp::complex deltaGL_Wff(const Particle pbar, const Particle p) const;
798  // no generation mixing
799  virtual gslpp::complex deltaGR_Wff(const Particle pbar, const Particle p) const;
800 
805  virtual double deltaG_hgg() const;
810  virtual double deltaG1_hWW() const;
815  virtual double deltaG2_hWW() const;
820  virtual double deltaG3_hWW() const;
825  virtual double deltaG1_hZZ() const;
830  virtual double deltaG2_hZZ() const;
835  virtual double deltaG3_hZZ() const;
840  virtual double deltaG1_hZA() const;
845  virtual double deltaG2_hZA() const;
850  virtual double deltaG_hAA() const;
851 
857  // no generation mixing
858  virtual gslpp::complex deltaG_hff(const Particle p) const;
859 
866  // no generation mixing
867  gslpp::complex deltaGL_Wffh(const Particle pbar, const Particle p) const;
868 
875  // no generation mixing
876  gslpp::complex deltaGR_Wffh(const Particle pbar, const Particle p) const;
877 
883  // no generation mixing
884  double deltaGL_Zffh(const Particle p) const;
885 
891  // no generation mixing
892  double deltaGR_Zffh(const Particle p) const;
893 
899  // no generation mixing
900  gslpp::complex deltaG_hGff(const Particle p) const;
901 
907  // no generation mixing
908  gslpp::complex deltaG_hZff(const Particle p) const;
909 
915  // no generation mixing
916  gslpp::complex deltaG_hAff(const Particle p) const;
917 
923  // no generation mixing
924  gslpp::complex deltaG_Gff(const Particle p) const;
925 
931  // no generation mixing
932  gslpp::complex deltaG_Zff(const Particle p) const;
933 
939  // no generation mixing
940  gslpp::complex deltaG_Aff(const Particle p) const;
941 
946  double deltag3G() const;
947 
948 
950 
956  gslpp::complex f_triangle(const double tau) const;
964  gslpp::complex AH_f(const double tau) const;
965 
972  virtual double muggH(const double sqrt_s) const;
979  virtual double muVBF(const double sqrt_s) const;
987  virtual double mueeWBF(const double sqrt_s) const;
994  virtual double muWH(const double sqrt_s) const;
1001  virtual double muZH(const double sqrt_s) const;
1009  virtual double mueeZH(const double sqrt_s) const;
1016  virtual double muVH(const double sqrt_s) const;
1023  virtual double muVBFpVH(const double sqrt_s) const;
1030  virtual double muttH(const double sqrt_s) const;
1038  virtual double muggHpttH(const double sqrt_s) const;
1046  virtual double mueettH(const double sqrt_s) const;
1052  virtual double BrHggRatio() const;
1058  virtual double BrHWWRatio() const;
1064  virtual double BrHZZRatio() const;
1070  virtual double BrHZgaRatio() const;
1076  virtual double BrHgagaRatio() const;
1082  virtual double BrHmumuRatio() const;
1088  virtual double BrHtautauRatio() const;
1094  virtual double BrHccRatio() const;
1100  virtual double BrHbbRatio() const;
1106  virtual double computeGammaTotalRatio() const;
1113  virtual double deltaGammaTotalRatio1() const;
1120  virtual double deltaGammaTotalRatio2() const;
1126  double GammaHggRatio() const;
1132  double GammaHWWRatio() const;
1138  double GammaHZZRatio() const;
1144  double GammaHZgaRatio() const;
1150  double GammaHgagaRatio() const;
1156  double GammaHmumuRatio() const;
1162  double GammaHtautauRatio() const;
1168  double GammaHccRatio() const;
1174  double GammaHbbRatio() const;
1181  double deltaGammaHggRatio1() const;
1188  double deltaGammaHWWRatio1() const;
1195  double deltaGammaHZZRatio1() const;
1202  double deltaGammaHZgaRatio1() const;
1209  double deltaGammaHgagaRatio1() const;
1216  double deltaGammaHmumuRatio1() const;
1223  double deltaGammaHtautauRatio1() const;
1230  double deltaGammaHccRatio1() const;
1237  double deltaGammaHbbRatio1() const;
1244  double deltaGammaHggRatio2() const;
1251  double deltaGammaHWWRatio2() const;
1258  double deltaGammaHZZRatio2() const;
1265  double deltaGammaHZgaRatio2() const;
1272  double deltaGammaHgagaRatio2() const;
1279  double deltaGammaHmumuRatio2() const;
1286  double deltaGammaHtautauRatio2() const;
1293  double deltaGammaHccRatio2() const;
1300  double deltaGammaHbbRatio2() const;
1301 
1302 
1303  virtual double LEP2sigmaMu(const double s) const;
1304  virtual double LEP2sigmaTau(const double s) const;
1305  virtual double LEP2sigmaHadron(const double s) const;
1306  virtual double LEP2AFBmu(const double s) const;
1307  virtual double LEP2AFBtau(const double s) const;
1308  virtual double LEP2AFBbottom(const double s) const;
1309  virtual double LEP2AFBcharm(const double s) const;
1310  virtual double LEP2Rbottom(const double s) const;
1311  virtual double LEP2Rcharm(const double s) const;
1312 
1314 protected:
1315 
1320  virtual void setParameter(const std::string name, const double& value);
1321 
1322  double CG;
1323  double CW;
1324  double CHG;
1325  double CHW;
1326  double CHB;
1327  double CHWB;
1328  double CHD;
1329  double CHbox;
1330  double CH;
1331  double CHL1_11;
1332  double CHL1_12r;
1333  double CHL1_13r;
1334  double CHL1_22;
1335  double CHL1_23r;
1336  double CHL1_33;
1337  double CHL1_12i;
1338  double CHL1_13i;
1339  double CHL1_23i;
1340  double CHL3_11;
1341  double CHL3_12r;
1342  double CHL3_13r;
1343  double CHL3_22;
1344  double CHL3_23r;
1345  double CHL3_33;
1346  double CHL3_12i;
1347  double CHL3_13i;
1348  double CHL3_23i;
1349  double CHe_11;
1350  double CHe_12r;
1351  double CHe_13r;
1352  double CHe_22;
1353  double CHe_23r;
1354  double CHe_33;
1355  double CHe_12i;
1356  double CHe_13i;
1357  double CHe_23i;
1358  double CHQ1_11;
1359  double CHQ1_12r;
1360  double CHQ1_13r;
1361  double CHQ1_22;
1362  double CHQ1_23r;
1363  double CHQ1_33;
1364  double CHQ1_12i;
1365  double CHQ1_13i;
1366  double CHQ1_23i;
1367  double CHQ3_11;
1368  double CHQ3_12r;
1369  double CHQ3_13r;
1370  double CHQ3_22;
1371  double CHQ3_23r;
1372  double CHQ3_33;
1373  double CHQ3_12i;
1374  double CHQ3_13i;
1375  double CHQ3_23i;
1376  double CHu_11;
1377  double CHu_12r;
1378  double CHu_13r;
1379  double CHu_22;
1380  double CHu_23r;
1381  double CHu_33;
1382  double CHu_12i;
1383  double CHu_13i;
1384  double CHu_23i;
1385  double CHd_11;
1386  double CHd_12r;
1387  double CHd_13r;
1388  double CHd_22;
1389  double CHd_23r;
1390  double CHd_33;
1391  double CHd_12i;
1392  double CHd_13i;
1393  double CHd_23i;
1394  double CHud_11r;
1395  double CHud_12r;
1396  double CHud_13r;
1397  double CHud_22r;
1398  double CHud_23r;
1399  double CHud_33r;
1400  double CHud_11i;
1401  double CHud_12i;
1402  double CHud_13i;
1403  double CHud_22i;
1404  double CHud_23i;
1405  double CHud_33i;
1406  double CeH_11r;
1407  double CeH_12r;
1408  double CeH_13r;
1409  double CeH_22r;
1410  double CeH_23r;
1411  double CeH_33r;
1412  double CeH_11i;
1413  double CeH_12i;
1414  double CeH_13i;
1415  double CeH_22i;
1416  double CeH_23i;
1417  double CeH_33i;
1418  double CuH_11r;
1419  double CuH_12r;
1420  double CuH_13r;
1421  double CuH_22r;
1422  double CuH_23r;
1423  double CuH_33r;
1424  double CuH_11i;
1425  double CuH_12i;
1426  double CuH_13i;
1427  double CuH_22i;
1428  double CuH_23i;
1429  double CuH_33i;
1430  double CdH_11r;
1431  double CdH_12r;
1432  double CdH_13r;
1433  double CdH_22r;
1434  double CdH_23r;
1435  double CdH_33r;
1436  double CdH_11i;
1437  double CdH_12i;
1438  double CdH_13i;
1439  double CdH_22i;
1440  double CdH_23i;
1441  double CdH_33i;
1442  double CuG_11r;
1443  double CuG_12r;
1444  double CuG_13r;
1445  double CuG_22r;
1446  double CuG_23r;
1447  double CuG_33r;
1448  double CuG_11i;
1449  double CuG_12i;
1450  double CuG_13i;
1451  double CuG_22i;
1452  double CuG_23i;
1453  double CuG_33i;
1454  double CuW_11r;
1455  double CuW_12r;
1456  double CuW_13r;
1457  double CuW_22r;
1458  double CuW_23r;
1459  double CuW_33r;
1460  double CuW_11i;
1461  double CuW_12i;
1462  double CuW_13i;
1463  double CuW_22i;
1464  double CuW_23i;
1465  double CuW_33i;
1466  double CuB_11r;
1467  double CuB_12r;
1468  double CuB_13r;
1469  double CuB_22r;
1470  double CuB_23r;
1471  double CuB_33r;
1472  double CuB_11i;
1473  double CuB_12i;
1474  double CuB_13i;
1475  double CuB_22i;
1476  double CuB_23i;
1477  double CuB_33i;
1478  double CLL_1111;
1479  double CLL_1221, CLL_2112, CLL_1122, CLL_2211;
1480  double CLL_1331, CLL_3113, CLL_1133, CLL_3311;
1481  double CLQ1_1111;
1482  double CLQ1_1122, CLQ1_2211, CLQ1_1221, CLQ1_2112;
1483  double CLQ1_1133, CLQ1_3311, CLQ1_1331, CLQ1_3113;
1484  double CLQ1_1123, CLQ1_2223, CLQ1_3323;
1485  double CLQ1_1132, CLQ1_2232, CLQ1_3332;
1486  double CLQ3_1111;
1487  double CLQ3_1122, CLQ3_2211, CLQ3_1221, CLQ3_2112;
1488  double CLQ3_1133, CLQ3_3311, CLQ3_1331, CLQ3_3113;
1489  double CLQ3_1123, CLQ3_2223, CLQ3_3323;
1490  double CLQ3_1132, CLQ3_2232, CLQ3_3332;
1491  double Cee_1111;
1492  double Cee_1122, Cee_2211;
1493  double Cee_1133, Cee_3311;
1494  double Ceu_1111;
1495  double Ceu_1122, Ceu_2211;
1496  double Ceu_1133, Ceu_3311;
1497  double Ced_1111;
1498  double Ced_1122, Ced_2211;
1499  double Ced_1133, Ced_3311;
1500  double Ced_1123, Ced_2223, Ced_3323;
1501  double Ced_1132, Ced_2232, Ced_3332;
1502  double CLe_1111;
1503  double CLe_1122, CLe_2211;
1504  double CLe_1133, CLe_3311;
1505  double CLu_1111;
1506  double CLu_1122, CLu_2211;
1507  double CLu_1133, CLu_3311;
1508  double CLd_1111;
1509  double CLd_1122, CLd_2211;
1510  double CLd_1133, CLd_3311;
1511  double CLd_1123, CLd_2223, CLd_3323;
1512  double CLd_1132, CLd_2232, CLd_3332;
1513  double CQe_1111;
1514  double CQe_1122, CQe_2211;
1515  double CQe_1133, CQe_3311;
1516  double CQe_2311, CQe_2322, CQe_2333;
1517  double CQe_3211, CQe_3222, CQe_3233;
1518  double Lambda_NP;
1519 // The error in the parameters multiplying the dimension-6 operator coefficients in the production cross sections.
1520  double eVBF2_HZZ1;
1521  double eVBF2_HZZ2;
1522  double eVBF2_HZZ3;
1523  double eVBF2_HZA1;
1524  double eVBF2_HZA2;
1525  double eVBF2_HAA;
1526  double eVBF2_HWW1;
1527  double eVBF2_HWW2;
1528  double eVBF2_HWW3;
1529  double eVBF2_Hgg;
1530  double eVBF2_HZuL;
1531  double eVBF2_HZuR;
1532  double eVBF2_HZdL;
1533  double eVBF2_HZdR;
1534  double eVBF2_HWud;
1535  double eVBF2_ZuL;
1536  double eVBF2_ZuR;
1537  double eVBF2_ZdL;
1538  double eVBF2_ZdR;
1539  double eVBF2_Wud;
1540  double eVBF78_HZZ1;
1541  double eVBF78_HZZ2;
1542  double eVBF78_HZZ3;
1543  double eVBF78_HZA1;
1544  double eVBF78_HZA2;
1545  double eVBF78_HAA;
1546  double eVBF78_HWW1;
1547  double eVBF78_HWW2;
1548  double eVBF78_HWW3;
1549  double eVBF78_Hgg;
1550  double eVBF78_HZuL;
1551  double eVBF78_HZuR;
1552  double eVBF78_HZdL;
1553  double eVBF78_HZdR;
1554  double eVBF78_HWud;
1555  double eVBF78_ZuL;
1556  double eVBF78_ZuR;
1557  double eVBF78_ZdL;
1558  double eVBF78_ZdR;
1559  double eVBF78_Wud;
1560 
1561  double eWH2_HWW1;
1562  double eWH2_HWW2;
1563  double eWH2_HWW3;
1564  double eWH2_HWud;
1565  double eWH2_Wud;
1566  double eWH78_HWW1;
1567  double eWH78_HWW2;
1568  double eWH78_HWW3;
1569  double eWH78_HWud;
1570  double eWH78_Wud;
1571 
1572  double eZH2_HZZ1;
1573  double eZH2_HZZ2;
1574  double eZH2_HZZ3;
1575  double eZH2_HZA1;
1576  double eZH2_HZA2;
1577  double eZH2_HZuL;
1578  double eZH2_HZuR;
1579  double eZH2_HZdL;
1580  double eZH2_HZdR;
1581  double eZH2_ZuL;
1582  double eZH2_ZuR;
1583  double eZH2_ZdL;
1584  double eZH2_ZdR;
1585  double eZH78_HZZ1;
1586  double eZH78_HZZ2;
1587  double eZH78_HZZ3;
1588  double eZH78_HZA1;
1589  double eZH78_HZA2;
1590  double eZH78_HZuL;
1591  double eZH78_HZuR;
1592  double eZH78_HZdL;
1593  double eZH78_HZdR;
1594  double eZH78_ZuL;
1595  double eZH78_ZuR;
1596  double eZH78_ZdL;
1597  double eZH78_ZdR;
1598 
1599  double ettH2_Htt;
1600  double ettH2_Hgg;
1601  double ettH78_Htt;
1602  double ettH78_Hgg;
1603 
1604  double MwInput;
1605 
1606  double LambdaNP2;
1607  double v2_over_LambdaNP2;
1608  double cW_tree;
1609  double sW_tree;
1610  double cW2_tree;
1611  double sW2_tree;
1612  double delta_ZZ;
1613  double delta_AA;
1614  double delta_AZ;
1615  double delta_h;
1616 
1622  double CHF1_diag(const Particle F) const;
1623 
1629  double CHF3_diag(const Particle F) const;
1630 
1636  double CHf_diag(const Particle f) const;
1637 
1643  gslpp::complex CHud_diag(const Particle u) const;
1644 
1650  gslpp::complex CfH_diag(const Particle f) const;
1651 
1657  gslpp::complex CfG_diag(const Particle f) const;
1658 
1664  gslpp::complex CfW_diag(const Particle f) const;
1665 
1671  gslpp::complex CfB_diag(const Particle f) const;
1672 
1673  const LEP2GIMR myLEP2GIMR;
1674 
1676 private:
1677 
1678  bool FlagMwInput;
1679  bool FlagQuadraticTerms;
1680 
1685  const bool FlagLeptonUniversal;
1686 
1691  const bool FlagQuarkUniversal;
1692 
1693 };
1694 
1695 #endif /* NPEFFECTIVEGIMR_H */
1696 
NPEffectiveGIMR::CuG_11i
double CuG_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1448
NPEffectiveGIMR::eWH2_HWW1
double eWH2_HWW1
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1561
NPEffectiveGIMR::AH_f
gslpp::complex AH_f(const double tau) const
Fermionic loop function entering in the calculation of the effective and couplings.
Definition: NPEffectiveGIMR.cpp:1985
NPEffectiveGIMR::CeH_11r
double CeH_11r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1406
NPEffectiveGIMR::deltaGammaHbbRatio2
double deltaGammaHbbRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3347
NPEffectiveGIMR::CuB_23i
double CuB_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1476
NPEffectiveGIMR::CHL1_13i
double CHL1_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1338
NPEffectiveGIMR::deltaGammaHccRatio1
double deltaGammaHccRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3313
NPEffectiveGIMR::eZH78_HZuL
double eZH78_HZuL
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1590
NPEffectiveGIMR::GammaHZZRatio
double GammaHZZRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:3122
NPEffectiveGIMR::delta_ZZ
double delta_ZZ
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPEffectiveGIMR.h:1612
NPEffectiveGIMR::CuB_23r
double CuB_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1470
NPEffectiveGIMR::deltaMz2
virtual double deltaMz2() const
Definition: NPEffectiveGIMR.cpp:1709
NPEffectiveGIMR::muVBFpVH
virtual 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 ...
Definition: NPEffectiveGIMR.cpp:2685
NPEffectiveGIMR::CLe_1111
double CLe_1111
Definition: NPEffectiveGIMR.h:1502
NPEffectiveGIMR::MwInput
double MwInput
The input value for the -boson mass if FlagMwInput is true.
Definition: NPEffectiveGIMR.h:1604
NPEffectiveGIMR::LEP2AFBbottom
virtual double LEP2AFBbottom(const double s) const
Definition: NPEffectiveGIMR.cpp:3637
NPEffectiveGIMR::CHf_diag
double CHf_diag(const Particle f) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f.
Definition: NPEffectiveGIMR.cpp:1541
NPEffectiveGIMR::deltaG_hff
virtual gslpp::complex deltaG_hff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1875
NPEffectiveGIMR::CHQ1_12i
double CHQ1_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1364
NPEffectiveGIMR::CLQ3_1111
double CLQ3_1111
Definition: NPEffectiveGIMR.h:1486
NPEffectiveGIMR::CLd_2211
double CLd_2211
Definition: NPEffectiveGIMR.h:1509
NPEffectiveGIMR::eZH2_HZZ3
double eZH2_HZZ3
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1574
NPEffectiveGIMR::CHL1_12i
double CHL1_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1337
NPEffectiveGIMR::CuW_23i
double CuW_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1464
NPEffectiveGIMR::eVBF2_HZdL
double eVBF2_HZdL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1532
NPEffectiveGIMR::CHud_22r
double CHud_22r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1397
NPEffectiveGIMR::CeH_12i
double CeH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1413
NPEffectiveGIMR::eVBF2_HAA
double eVBF2_HAA
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1525
NPEffectiveGIMR::CLe_3311
double CLe_3311
Definition: NPEffectiveGIMR.h:1504
NPEffectiveGIMR::LEP2Rcharm
virtual double LEP2Rcharm(const double s) const
Definition: NPEffectiveGIMR.cpp:3656
NPEffectiveGIMR::Ced_1111
double Ced_1111
Definition: NPEffectiveGIMR.h:1497
NPEffectiveGIMR::CHQ1_13r
double CHQ1_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1360
NPEffectiveGIMR::eVBF2_HZA2
double eVBF2_HZA2
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1524
NPEffectiveGIMR::eWH78_Wud
double eWH78_Wud
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1570
NPEffectiveGIMR::sW_tree
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPEffectiveGIMR.h:1609
NPEffectiveGIMR::CRL_bottom
double CRL_bottom() const
Definition: NPEffectiveGIMR.cpp:3457
NPEffectiveGIMR::deltaGammaHZgaRatio2
double deltaGammaHZgaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3185
NPEffectiveGIMR::eVBF2_HZdR
double eVBF2_HZdR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1533
NPEffectiveGIMR::CHQ3_13i
double CHQ3_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1374
NPEffectiveGIMR::deltaG_Gff
gslpp::complex deltaG_Gff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1942
Particle
A class for particles.
Definition: Particle.h:26
NPEffectiveGIMR::deltaGammaHggRatio1
double deltaGammaHggRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3069
NPEffectiveGIMR::eVBF78_ZuR
double eVBF78_ZuR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1556
NPEffectiveGIMR::eZH2_HZA2
double eZH2_HZA2
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1576
NPEffectiveGIMR::CuB_13r
double CuB_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1468
NPEffectiveGIMR::delta_AZ
double delta_AZ
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPEffectiveGIMR.h:1614
NPEffectiveGIMR::CLQ1_1123
double CLQ1_1123
Definition: NPEffectiveGIMR.h:1484
NPEffectiveGIMR::deltaG_hZff
gslpp::complex deltaG_hZff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1928
NPEffectiveGIMR::eVBF2_HZZ1
double eVBF2_HZZ1
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1520
NPEffectiveGIMR::eVBF2_Wud
double eVBF2_Wud
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1539
NPEffectiveGIMR::CuH_11i
double CuH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1424
NPEffectiveGIMR::CheckParameters
virtual bool CheckParameters(const std::map< std::string, double > &DPars)
A method to check if all the mandatory parameters for NPEffectiveGIMR have been provided in model ini...
Definition: NPEffectiveGIMR.cpp:1444
NPEffectiveGIMR::deltaGammaHZZRatio2
double deltaGammaHZZRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3147
NPEffectiveGIMR::CuH_22r
double CuH_22r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1421
NPEffectiveGIMR::eVBF78_HWud
double eVBF78_HWud
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1554
NPEffectiveGIMR::CLQ3_1221
double CLQ3_1221
Definition: NPEffectiveGIMR.h:1487
NPEffectiveGIMR::CHL1_23r
double CHL1_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1335
NPEffectiveGIMR::deltaGV_f
virtual double deltaGV_f(const Particle p) const
New physics contribution to the neutral-current vector coupling .
Definition: NPEffectiveGIMR.cpp:1741
NPEffectiveGIMR::setFlag
virtual bool setFlag(const std::string name, const bool value)
A method to set a flag of NPEffectiveGIMR.
Definition: NPEffectiveGIMR.cpp:1486
NPEffectiveGIMR::deltaGammaHmumuRatio2
double deltaGammaHmumuRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3259
NPEffectiveGIMR::CHL1_11
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1331
NPEffectiveGIMR::eWH78_HWW3
double eWH78_HWW3
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1568
NPEffectiveGIMR::deltaGammaHWWRatio2
double deltaGammaHWWRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3113
NPEffectiveGIMR::CLL_1111
double CLL_1111
Definition: NPEffectiveGIMR.h:1478
NPEffectiveGIMR::CW
double CW
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1323
NPEffectiveGIMR::CLQ1_2112
double CLQ1_2112
Definition: NPEffectiveGIMR.h:1482
NPEffectiveGIMR::CHu_23r
double CHu_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1380
NPEffectiveGIMR::eWH2_HWud
double eWH2_HWud
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1564
NPEffectiveGIMR::eWH2_HWW2
double eWH2_HWW2
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1562
NPEffectiveGIMR::GammaHtautauRatio
double GammaHtautauRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:3267
NPEffectiveGIMR::GammaHmumuRatio
double GammaHmumuRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:3237
NPEffectiveGIMR::CRL_up
double CRL_up() const
Definition: NPEffectiveGIMR.cpp:3437
NPEffectiveGIMR::CHQ3_12i
double CHQ3_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1373
NPEffectiveGIMR::CHu_13i
double CHu_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1383
NPEffectiveGIMR::CLL_1331
double CLL_1331
Definition: NPEffectiveGIMR.h:1480
NPEffectiveGIMR::eVBF2_HZZ3
double eVBF2_HZZ3
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1522
NPEffectiveGIMR::CdH_23i
double CdH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1440
NPEffectiveGIMR::GammaHbbRatio
double GammaHbbRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:3326
NPEffectiveGIMR::CLQ1_2223
double CLQ1_2223
Definition: NPEffectiveGIMR.h:1484
NPEffectiveGIMR::CfW_diag
gslpp::complex CfW_diag(const Particle f) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f.
Definition: NPEffectiveGIMR.cpp:1634
NPEffectiveGIMR::CLu_1133
double CLu_1133
Definition: NPEffectiveGIMR.h:1507
LEP2GIMR.h
NPEffectiveGIMR::BrHgagaRatio
virtual double BrHgagaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2914
NPbase.h
NPEffectiveGIMR::CQe_1122
double CQe_1122
Definition: NPEffectiveGIMR.h:1514
NPEffectiveGIMR::CLL_1221
double CLL_1221
Definition: NPEffectiveGIMR.h:1479
NPEffectiveGIMR::CHud_33i
double CHud_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1405
NPEffectiveGIMR::Ced_3332
double Ced_3332
Definition: NPEffectiveGIMR.h:1501
NPEffectiveGIMR::CHe_33
double CHe_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1354
NPEffectiveGIMR::CuW_12i
double CuW_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1461
NPEffectiveGIMR::deltaGammaHgagaRatio1
double deltaGammaHgagaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3213
NPEffectiveGIMR::eVBF2_HWW1
double eVBF2_HWW1
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1526
NPEffectiveGIMR::CLd_3311
double CLd_3311
Definition: NPEffectiveGIMR.h:1510
NPEffectiveGIMR::eWH2_Wud
double eWH2_Wud
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1565
NPEffectiveGIMR::CLQ1_3113
double CLQ1_3113
Definition: NPEffectiveGIMR.h:1483
NPEffectiveGIMR::CLL_1122
double CLL_1122
Definition: NPEffectiveGIMR.h:1479
NPEffectiveGIMR::CHD
double CHD
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1328
NPEffectiveGIMR::eWH2_HWW3
double eWH2_HWW3
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1563
NPEffectiveGIMR::CRR_up
double CRR_up() const
Definition: NPEffectiveGIMR.cpp:3473
NPEffectiveGIMR::CLQ3_2112
double CLQ3_2112
Definition: NPEffectiveGIMR.h:1487
NPEffectiveGIMR::CHu_12r
double CHu_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1377
NPEffectiveGIMR::CeH_23i
double CeH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1416
NPEffectiveGIMR::eVBF2_HWW3
double eVBF2_HWW3
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1528
NPEffectiveGIMR::eWH78_HWud
double eWH78_HWud
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1569
NPEffectiveGIMR::LambdaNP2
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPEffectiveGIMR.h:1606
NPEffectiveGIMR::eZH2_ZdR
double eZH2_ZdR
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1584
NPEffectiveGIMR::CHL3_22
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1343
NPEffectiveGIMR::Cee_2211
double Cee_2211
Definition: NPEffectiveGIMR.h:1492
NPEffectiveGIMR::LEP2AFBtau
virtual double LEP2AFBtau(const double s) const
Definition: NPEffectiveGIMR.cpp:3601
NPEffectiveGIMR::CLQ3_1122
double CLQ3_1122
Definition: NPEffectiveGIMR.h:1487
NPEffectiveGIMR::muWH
virtual 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...
Definition: NPEffectiveGIMR.cpp:2350
NPEffectiveGIMR::CRL_mu
double CRL_mu() const
Definition: NPEffectiveGIMR.cpp:3427
NPEffectiveGIMR::CLd_1123
double CLd_1123
Definition: NPEffectiveGIMR.h:1511
LEP2GIMR
A class for NP analyses of LEP-II observables with the dimension 6 operators in the GIMR basis.
Definition: LEP2GIMR.h:26
gslpp.h
NPEffectiveGIMR::CHu_11
double CHu_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1376
NPEffectiveGIMR::deltaGR_Wffh
gslpp::complex deltaGR_Wffh(const Particle pbar, const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1898
NPEffectiveGIMR::CQe_3311
double CQe_3311
Definition: NPEffectiveGIMR.h:1515
NPEffectiveGIMR::CeH_11i
double CeH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1412
NPEffectiveGIMR::CLQ1_1122
double CLQ1_1122
Definition: NPEffectiveGIMR.h:1482
NPEffectiveGIMR::eVBF2_HZZ2
double eVBF2_HZZ2
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1521
NPEffectiveGIMR::Mw
virtual double Mw() const
The mass of the boson, .
Definition: NPEffectiveGIMR.cpp:1714
NPEffectiveGIMR::v2_over_LambdaNP2
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPEffectiveGIMR.h:1607
NPEffectiveGIMR::deltaGammaTotalRatio1
virtual double deltaGammaTotalRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3027
NPEffectiveGIMR::CfG_diag
gslpp::complex CfG_diag(const Particle f) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f.
Definition: NPEffectiveGIMR.cpp:1608
NPEffectiveGIMR::eZH2_ZuR
double eZH2_ZuR
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1582
NPEffectiveGIMR::eVBF78_Hgg
double eVBF78_Hgg
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1549
NPEffectiveGIMR::CuW_33i
double CuW_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1465
NPEffectiveGIMR::CRR_bottom
double CRR_bottom() const
Definition: NPEffectiveGIMR.cpp:3493
NPEffectiveGIMR::BrHtautauRatio
virtual double BrHtautauRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2954
NPEffectiveGIMR::CHud_13r
double CHud_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1396
NPEffectiveGIMR::CeH_22i
double CeH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1415
NPEffectiveGIMR::CHL1_23i
double CHL1_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1339
NPEffectiveGIMR::eVBF78_HWW1
double eVBF78_HWW1
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1546
NPEffectiveGIMR::deltaG_Zff
gslpp::complex deltaG_Zff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1949
NPEffectiveGIMR::CuW_11i
double CuW_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1460
NPEffectiveGIMR::Ceu_1122
double Ceu_1122
Definition: NPEffectiveGIMR.h:1495
NPEffectiveGIMR::BrHccRatio
virtual double BrHccRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2974
gslpp::complex
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
NPEffectiveGIMR::CHL3_23i
double CHL3_23i
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1348
NPEffectiveGIMR::muttH
virtual 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...
Definition: NPEffectiveGIMR.cpp:2700
NPEffectiveGIMR::CHud_12i
double CHud_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1401
NPEffectiveGIMR::eZH78_HZdL
double eZH78_HZdL
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1592
NPEffectiveGIMR::CHQ1_33
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1363
NPEffectiveGIMR::ettH2_Htt
double ettH2_Htt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPEffectiveGIMR.h:1599
NPEffectiveGIMR::CHud_33r
double CHud_33r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1399
NPEffectiveGIMR::eVBF2_HZuR
double eVBF2_HZuR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1531
NPEffectiveGIMR::LEP2sigmaMu
virtual double LEP2sigmaMu(const double s) const
Definition: NPEffectiveGIMR.cpp:3500
NPEffectiveGIMR::CHd_33
double CHd_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1390
NPEffectiveGIMR::CQe_1111
double CQe_1111
Definition: NPEffectiveGIMR.h:1513
NPEffectiveGIMR::CLQ3_3311
double CLQ3_3311
Definition: NPEffectiveGIMR.h:1488
NPEffectiveGIMR::CLQ3_2211
double CLQ3_2211
Definition: NPEffectiveGIMR.h:1487
NPEffectiveGIMR::CHQ1_23r
double CHQ1_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1362
NPEffectiveGIMR::CuH_22i
double CuH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1427
NPEffectiveGIMR::CLL_bottom
double CLL_bottom() const
Definition: NPEffectiveGIMR.cpp:3387
NPEffectiveGIMR::CHL3_11
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1340
NPEffectiveGIMR::CHQ3_23i
double CHQ3_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1375
NPEffectiveGIMR::deltaGammaHtautauRatio1
double deltaGammaHtautauRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3283
NPEffectiveGIMR::Cee_1122
double Cee_1122
Definition: NPEffectiveGIMR.h:1492
NPEffectiveGIMR::delta_AA
double delta_AA
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPEffectiveGIMR.h:1613
NPEffectiveGIMR::Ceu_1133
double Ceu_1133
Definition: NPEffectiveGIMR.h:1496
NPEffectiveGIMR::CLQ1_1133
double CLQ1_1133
Definition: NPEffectiveGIMR.h:1483
NPEffectiveGIMR::Ced_3323
double Ced_3323
Definition: NPEffectiveGIMR.h:1500
NPEffectiveGIMR::Ceu_1111
double Ceu_1111
Definition: NPEffectiveGIMR.h:1494
NPEffectiveGIMR::CQe_1133
double CQe_1133
Definition: NPEffectiveGIMR.h:1515
NPEffectiveGIMR::CfB_diag
gslpp::complex CfB_diag(const Particle f) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f.
Definition: NPEffectiveGIMR.cpp:1660
NPEffectiveGIMR::Ceu_2211
double Ceu_2211
Definition: NPEffectiveGIMR.h:1495
NPEffectiveGIMR::CHd_13i
double CHd_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1392
NPEffectiveGIMR::mueettH
virtual double mueettH(const double sqrt_s) const
The ratio between the production cross-section in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2769
NPEffectiveGIMR::muggH
virtual double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
Definition: NPEffectiveGIMR.cpp:1990
NPEffectiveGIMR::deltaG_hgg
virtual double deltaG_hgg() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1815
NPEffectiveGIMR::CLR_mu
double CLR_mu() const
Definition: NPEffectiveGIMR.cpp:3392
NPEffectiveGIMR::CuW_13r
double CuW_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1456
NPEffectiveGIMR::deltaGammaHWWRatio1
double deltaGammaHWWRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3104
NPEffectiveGIMR::NNPEffectiveGIMRVars
static const int NNPEffectiveGIMRVars
The number of the model parameters in NPEffectiveGIMR.
Definition: NPEffectiveGIMR.h:616
NPEffectiveGIMR::CuB_12r
double CuB_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1467
NPEffectiveGIMR
A model class for new physics in the form of the dimension-six effective Lagrangian.
Definition: NPEffectiveGIMR.h:610
NPEffectiveGIMR::ettH2_Hgg
double ettH2_Hgg
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPEffectiveGIMR.h:1600
NPEffectiveGIMR::CuG_13r
double CuG_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1444
NPEffectiveGIMR::CeH_22r
double CeH_22r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1409
NPEffectiveGIMR::CLQ3_2232
double CLQ3_2232
Definition: NPEffectiveGIMR.h:1490
NPEffectiveGIMR::CfH_diag
gslpp::complex CfH_diag(const Particle f) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f.
Definition: NPEffectiveGIMR.cpp:1582
NPEffectiveGIMR::CuH_13r
double CuH_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1420
NPEffectiveGIMR::deltaGA_f
virtual double deltaGA_f(const Particle p) const
New physics contribution to the neutral-current axial-vector coupling .
Definition: NPEffectiveGIMR.cpp:1746
NPEffectiveGIMR::CLQ1_2232
double CLQ1_2232
Definition: NPEffectiveGIMR.h:1485
NPEffectiveGIMR::CLL_charm
double CLL_charm() const
Definition: NPEffectiveGIMR.cpp:3377
NPEffectiveGIMR::CuG_11r
double CuG_11r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1442
NPEffectiveGIMR::deltaGR_Zffh
double deltaGR_Zffh(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1915
NPEffectiveGIMR::CuW_22i
double CuW_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1463
NPEffectiveGIMR::LEP2AFBcharm
virtual double LEP2AFBcharm(const double s) const
Definition: NPEffectiveGIMR.cpp:3619
NPEffectiveGIMR::eVBF2_ZuR
double eVBF2_ZuR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1536
NPEffectiveGIMR::cW2_tree
double cW2_tree
The sqaure of the tree level values for the cosine of the weak angle.
Definition: NPEffectiveGIMR.h:1610
NPEffectiveGIMR::CHG
double CHG
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1324
NPEffectiveGIMR::muZH
virtual 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...
Definition: NPEffectiveGIMR.cpp:2425
NPEffectiveGIMR::NNPEffectiveGIMRVars_LFU_QFU
static const int NNPEffectiveGIMRVars_LFU_QFU
The number of the model parameters in NPEffectiveGIMR with lepton and quark flavour universalities.
Definition: NPEffectiveGIMR.h:628
NPEffectiveGIMR::CLQ1_3323
double CLQ1_3323
Definition: NPEffectiveGIMR.h:1484
NPEffectiveGIMR::CHud_23r
double CHud_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1398
NPEffectiveGIMR::deltaGL_f
double deltaGL_f(const Particle p) const
New physics contribution to the neutral-current left-handed coupling .
Definition: NPEffectiveGIMR.cpp:1751
NPEffectiveGIMR::BrHZZRatio
virtual double BrHZZRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2874
NPEffectiveGIMR::CRR_charm
double CRR_charm() const
Definition: NPEffectiveGIMR.cpp:3483
NPEffectiveGIMR::CLQ1_1221
double CLQ1_1221
Definition: NPEffectiveGIMR.h:1482
NPEffectiveGIMR::BrHmumuRatio
virtual double BrHmumuRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2934
NPEffectiveGIMR::CLL_3311
double CLL_3311
Definition: NPEffectiveGIMR.h:1480
NPEffectiveGIMR::CRR_strange
double CRR_strange() const
Definition: NPEffectiveGIMR.cpp:3488
NPEffectiveGIMR::CuG_23i
double CuG_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1452
NPEffectiveGIMR::Ced_1132
double Ced_1132
Definition: NPEffectiveGIMR.h:1501
NPEffectiveGIMR::CHL3_33
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1345
NPEffectiveGIMR::CHe_12r
double CHe_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1350
NPEffectiveGIMR::CuH_12i
double CuH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1425
NPEffectiveGIMR::CQe_2311
double CQe_2311
Definition: NPEffectiveGIMR.h:1516
NPEffectiveGIMR::CHe_13r
double CHe_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1351
NPEffectiveGIMR::eZH78_HZA1
double eZH78_HZA1
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1588
NPEffectiveGIMR::CuG_22r
double CuG_22r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1445
NPEffectiveGIMR::CLR_tau
double CLR_tau() const
Definition: NPEffectiveGIMR.cpp:3397
NPEffectiveGIMR::CG
double CG
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1322
NPEffectiveGIMR::CLL_down
double CLL_down() const
Definition: NPEffectiveGIMR.cpp:3372
NPEffectiveGIMR::eVBF78_Wud
double eVBF78_Wud
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1559
NPEffectiveGIMR::deltaGammaHgagaRatio2
double deltaGammaHgagaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3224
NPEffectiveGIMR::eVBF78_HZZ3
double eVBF78_HZZ3
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1542
NPEffectiveGIMR::CLR_charm
double CLR_charm() const
Definition: NPEffectiveGIMR.cpp:3412
NPEffectiveGIMR::CHd_22
double CHd_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1388
NPEffectiveGIMR::deltaGammaHccRatio2
double deltaGammaHccRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3318
NPbase
The auxiliary base model class for other model classes.
Definition: NPbase.h:66
NPEffectiveGIMR::eZH78_ZuL
double eZH78_ZuL
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1594
NPEffectiveGIMR::deltaG1_hWW
virtual double deltaG1_hWW() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1820
NPEffectiveGIMR::deltag3G
double deltag3G() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1963
NPEffectiveGIMR::CHu_22
double CHu_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1379
NPEffectiveGIMR::obliqueT
virtual double obliqueT() const
The oblique parameter .
Definition: NPEffectiveGIMR.cpp:1699
NPEffectiveGIMR::eVBF78_HZdL
double eVBF78_HZdL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1552
NPEffectiveGIMR::eVBF78_HZuR
double eVBF78_HZuR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1551
NPEffectiveGIMR::CHud_13i
double CHud_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1402
NPEffectiveGIMR::NPEffectiveGIMRVars
static const std::string NPEffectiveGIMRVars[NNPEffectiveGIMRVars]
A string array containing the labels of the model parameters in NPEffectiveGIMR.
Definition: NPEffectiveGIMR.h:622
NPEffectiveGIMR::CuG_33r
double CuG_33r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1447
NPEffectiveGIMR::computeGammaTotalRatio
virtual double computeGammaTotalRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:3014
NPEffectiveGIMR::CHL3_23r
double CHL3_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1344
NPEffectiveGIMR::CuB_22r
double CuB_22r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1469
NPEffectiveGIMR::CLu_3311
double CLu_3311
Definition: NPEffectiveGIMR.h:1507
NPEffectiveGIMR::eZH2_HZZ1
double eZH2_HZZ1
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1572
NPEffectiveGIMR::eVBF2_HZuL
double eVBF2_HZuL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1530
NPEffectiveGIMR::CHbox
double CHbox
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1329
NPEffectiveGIMR::CLe_1122
double CLe_1122
Definition: NPEffectiveGIMR.h:1503
NPEffectiveGIMR::eZH78_HZA2
double eZH78_HZA2
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1589
NPEffectiveGIMR::eVBF2_HWud
double eVBF2_HWud
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1534
NPEffectiveGIMR::eZH78_ZdR
double eZH78_ZdR
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1597
NPEffectiveGIMR::CuH_13i
double CuH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1426
NPEffectiveGIMR::CdH_11r
double CdH_11r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1430
NPEffectiveGIMR::CHF1_diag
double CHF1_diag(const Particle F) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle F.
Definition: NPEffectiveGIMR.cpp:1505
NPEffectiveGIMR::CLd_2232
double CLd_2232
Definition: NPEffectiveGIMR.h:1512
NPEffectiveGIMR::eVBF78_ZdR
double eVBF78_ZdR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1558
NPEffectiveGIMR::CHud_diag
gslpp::complex CHud_diag(const Particle u) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f.
Definition: NPEffectiveGIMR.cpp:1567
NPEffectiveGIMR::CLQ3_2223
double CLQ3_2223
Definition: NPEffectiveGIMR.h:1489
NPEffectiveGIMR::CLQ1_2211
double CLQ1_2211
Definition: NPEffectiveGIMR.h:1482
NPEffectiveGIMR::CdH_33i
double CdH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1441
NPEffectiveGIMR::CLQ3_1133
double CLQ3_1133
Definition: NPEffectiveGIMR.h:1488
NPEffectiveGIMR::eVBF78_HWW3
double eVBF78_HWW3
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1548
NPEffectiveGIMR::CdH_22r
double CdH_22r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1433
NPEffectiveGIMR::FlagQuarkUniversal
const bool FlagQuarkUniversal
An internal boolean flag that is true if assuming quark flavour universality.
Definition: NPEffectiveGIMR.h:1691
NPEffectiveGIMR::deltaG_hAff
gslpp::complex deltaG_hAff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1935
NPEffectiveGIMR::CLL_3113
double CLL_3113
Definition: NPEffectiveGIMR.h:1480
NPEffectiveGIMR::CuW_33r
double CuW_33r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1459
NPEffectiveGIMR::CLQ3_1123
double CLQ3_1123
Definition: NPEffectiveGIMR.h:1489
NPEffectiveGIMR::CHud_22i
double CHud_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1403
NPEffectiveGIMR::deltaG2_hWW
virtual double deltaG2_hWW() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1825
NPEffectiveGIMR::muggHpttH
virtual double muggHpttH(const double sqrt_s) const
The ratio between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section...
Definition: NPEffectiveGIMR.cpp:2755
NPEffectiveGIMR::GammaW
virtual double GammaW() const
The total width of the boson, .
Definition: NPEffectiveGIMR.cpp:1725
NPEffectiveGIMR::CHQ1_22
double CHQ1_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1361
NPEffectiveGIMR::eZH78_ZuR
double eZH78_ZuR
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1595
NPEffectiveGIMR::eVBF2_Hgg
double eVBF2_Hgg
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1529
NPEffectiveGIMR::Cee_3311
double Cee_3311
Definition: NPEffectiveGIMR.h:1493
NPEffectiveGIMR::CHB
double CHB
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1326
NPEffectiveGIMR::eVBF78_HZuL
double eVBF78_HZuL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1550
NPEffectiveGIMR::NPEffectiveGIMRVars_LFU_QFU
static const std::string NPEffectiveGIMRVars_LFU_QFU[NNPEffectiveGIMRVars_LFU_QFU]
A string array containing the labels of the model parameters in NPEffectiveGIMR with lepton and quark...
Definition: NPEffectiveGIMR.h:634
NPEffectiveGIMR::DeltaGF
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPEffectiveGIMR.cpp:1689
NPEffectiveGIMR::eVBF78_HZA1
double eVBF78_HZA1
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1543
NPEffectiveGIMR::CLe_1133
double CLe_1133
Definition: NPEffectiveGIMR.h:1504
NPEffectiveGIMR::CHL3_13r
double CHL3_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1342
NPEffectiveGIMR::CLR_strange
double CLR_strange() const
Definition: NPEffectiveGIMR.cpp:3417
NPEffectiveGIMR::deltaG1_hZA
virtual double deltaG1_hZA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1860
NPEffectiveGIMR::CHd_11
double CHd_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1385
NPEffectiveGIMR::eZH78_ZdL
double eZH78_ZdL
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1596
NPEffectiveGIMR::CLR_down
double CLR_down() const
Definition: NPEffectiveGIMR.cpp:3407
NPEffectiveGIMR::CdH_12r
double CdH_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1431
NPEffectiveGIMR::CHQ3_13r
double CHQ3_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1369
NPEffectiveGIMR::CLL_1133
double CLL_1133
Definition: NPEffectiveGIMR.h:1480
NPEffectiveGIMR::CHL1_22
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1334
NPEffectiveGIMR::Ced_2211
double Ced_2211
Definition: NPEffectiveGIMR.h:1498
NPEffectiveGIMR::CuW_12r
double CuW_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1455
NPEffectiveGIMR::eZH2_ZdL
double eZH2_ZdL
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1583
NPEffectiveGIMR::CHWB
double CHWB
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1327
NPEffectiveGIMR::CdH_13i
double CdH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1438
NPEffectiveGIMR::CRL_down
double CRL_down() const
Definition: NPEffectiveGIMR.cpp:3442
NPEffectiveGIMR::eVBF78_ZuL
double eVBF78_ZuL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1555
NPEffectiveGIMR::CHL1_12r
double CHL1_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1332
NPEffectiveGIMR::eZH2_HZuR
double eZH2_HZuR
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1578
NPEffectiveGIMR::CLQ1_3311
double CLQ1_3311
Definition: NPEffectiveGIMR.h:1483
NPEffectiveGIMR::LEP2Rbottom
virtual double LEP2Rbottom(const double s) const
Definition: NPEffectiveGIMR.cpp:3709
NPEffectiveGIMR::muVH
virtual 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...
Definition: NPEffectiveGIMR.cpp:2672
NPEffectiveGIMR::setParameter
virtual void setParameter(const std::string name, const double &value)
A method to set the value of a parameter of the model.
Definition: NPEffectiveGIMR.cpp:558
NPEffectiveGIMR::CHL1_33
double CHL1_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1336
NPEffectiveGIMR::eZH78_HZuR
double eZH78_HZuR
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1591
NPEffectiveGIMR::GammaHggRatio
double GammaHggRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:3053
NPEffectiveGIMR::Ced_2223
double Ced_2223
Definition: NPEffectiveGIMR.h:1500
NPEffectiveGIMR::muVBF
virtual double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
Definition: NPEffectiveGIMR.cpp:2026
NPEffectiveGIMR::eWH78_HWW1
double eWH78_HWW1
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1566
NPEffectiveGIMR::CHQ3_12r
double CHQ3_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1368
NPEffectiveGIMR::CeH_33r
double CeH_33r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1411
NPEffectiveGIMR::f_triangle
gslpp::complex f_triangle(const double tau) const
Loop function entering in the calculation of the effective and couplings.
Definition: NPEffectiveGIMR.cpp:1973
NPEffectiveGIMR::eVBF2_ZuL
double eVBF2_ZuL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1535
NPEffectiveGIMR::deltaG_hGff
gslpp::complex deltaG_hGff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1921
NPEffectiveGIMR::Cee_1133
double Cee_1133
Definition: NPEffectiveGIMR.h:1493
NPEffectiveGIMR::CuH_11r
double CuH_11r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1418
NPEffectiveGIMR::CHud_11r
double CHud_11r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1394
NPEffectiveGIMR::CLQ1_1132
double CLQ1_1132
Definition: NPEffectiveGIMR.h:1485
NPEffectiveGIMR::CRR_tau
double CRR_tau() const
Definition: NPEffectiveGIMR.cpp:3467
NPEffectiveGIMR::CHQ1_12r
double CHQ1_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1359
NPEffectiveGIMR::CuH_33r
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1423
NPEffectiveGIMR::CdH_23r
double CdH_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1434
NPEffectiveGIMR::eZH2_HZdL
double eZH2_HZdL
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1579
NPEffectiveGIMR::FlagMwInput
bool FlagMwInput
A boolean flag that is true if the W mass is taken as an input parameter. (Warning: The W width is no...
Definition: NPEffectiveGIMR.h:1678
NPEffectiveGIMR::CHQ3_33
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1372
NPEffectiveGIMR::CHW
double CHW
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1325
NPEffectiveGIMR::GammaHWWRatio
double GammaHWWRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:3088
NPEffectiveGIMR::eVBF78_HAA
double eVBF78_HAA
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1545
NPEffectiveGIMR::deltaGammaTotalRatio2
virtual double deltaGammaTotalRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3040
NPEffectiveGIMR::CHQ1_23i
double CHQ1_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1366
NPEffectiveGIMR::CdH_11i
double CdH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1436
NPEffectiveGIMR::CHu_12i
double CHu_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1382
NPEffectiveGIMR::CLL_tau
double CLL_tau() const
Definition: NPEffectiveGIMR.cpp:3362
NPEffectiveGIMR::CdH_12i
double CdH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1437
NPEffectiveGIMR::Ced_3311
double Ced_3311
Definition: NPEffectiveGIMR.h:1499
NPEffectiveGIMR::FlagLeptonUniversal
const bool FlagLeptonUniversal
An internal boolean flag that is true if assuming lepton flavour universality.
Definition: NPEffectiveGIMR.h:1685
NPEffectiveGIMR::eVBF78_HZdR
double eVBF78_HZdR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1553
NPEffectiveGIMR::CRL_tau
double CRL_tau() const
Definition: NPEffectiveGIMR.cpp:3432
NPEffectiveGIMR::LEP2sigmaTau
virtual double LEP2sigmaTau(const double s) const
Definition: NPEffectiveGIMR.cpp:3516
NPEffectiveGIMR::CLL_2112
double CLL_2112
Definition: NPEffectiveGIMR.h:1479
NPEffectiveGIMR::mueeWBF
virtual double mueeWBF(const double sqrt_s) const
The ratio between the production cross-section in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2219
NPEffectiveGIMR::CRR_down
double CRR_down() const
Definition: NPEffectiveGIMR.cpp:3478
NPEffectiveGIMR::eVBF78_HZA2
double eVBF78_HZA2
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1544
NPEffectiveGIMR::eZH2_HZuL
double eZH2_HZuL
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1577
NPEffectiveGIMR::CLQ1_1111
double CLQ1_1111
Definition: NPEffectiveGIMR.h:1481
NPEffectiveGIMR::eVBF2_ZdL
double eVBF2_ZdL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1537
NPEffectiveGIMR::CuG_22i
double CuG_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1451
NPEffectiveGIMR::eVBF78_HWW2
double eVBF78_HWW2
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1547
NPEffectiveGIMR::CuG_12i
double CuG_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1449
NPEffectiveGIMR::CHQ3_23r
double CHQ3_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1371
NPEffectiveGIMR::Ced_1133
double Ced_1133
Definition: NPEffectiveGIMR.h:1499
NPEffectiveGIMR::CHe_22
double CHe_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1352
NPEffectiveGIMR::CHL3_12i
double CHL3_12i
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1346
NPEffectiveGIMR::eVBF2_HWW2
double eVBF2_HWW2
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1527
NPEffectiveGIMR::CuW_22r
double CuW_22r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1457
NPEffectiveGIMR::deltaGR_Wff
virtual gslpp::complex deltaGR_Wff(const Particle pbar, const Particle p) const
New physics contribution to the charged current coupling .
Definition: NPEffectiveGIMR.cpp:1806
NPEffectiveGIMR::CLL_strange
double CLL_strange() const
Definition: NPEffectiveGIMR.cpp:3382
NPEffectiveGIMR::CHQ3_22
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1370
NPEffectiveGIMR::CdH_22i
double CdH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1439
NPEffectiveGIMR::eVBF78_ZdL
double eVBF78_ZdL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1557
NPEffectiveGIMR::LEP2sigmaHadron
virtual double LEP2sigmaHadron(const double s) const
Definition: NPEffectiveGIMR.cpp:3532
NPEffectiveGIMR::CHud_12r
double CHud_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1395
NPEffectiveGIMR::deltaGammaHmumuRatio1
double deltaGammaHmumuRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3253
NPEffectiveGIMR::CHQ1_13i
double CHQ1_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1365
NPEffectiveGIMR::CQe_3211
double CQe_3211
Definition: NPEffectiveGIMR.h:1517
NPEffectiveGIMR::CHu_23i
double CHu_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1384
NPEffectiveGIMR::obliqueU
virtual double obliqueU() const
The oblique parameter .
Definition: NPEffectiveGIMR.cpp:1704
NPEffectiveGIMR::CLQ3_3332
double CLQ3_3332
Definition: NPEffectiveGIMR.h:1490
NPEffectiveGIMR::BrHZgaRatio
virtual double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2894
NPEffectiveGIMR::deltaG3_hWW
virtual double deltaG3_hWW() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1830
NPEffectiveGIMR::PostUpdate
virtual bool PostUpdate()
The post-update method for NPEffectiveGIMR.
Definition: NPEffectiveGIMR.cpp:535
NPEffectiveGIMR::CuH_12r
double CuH_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1419
NPEffectiveGIMR::CHd_12i
double CHd_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1391
NPEffectiveGIMR::CHL3_12r
double CHL3_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1341
NPEffectiveGIMR::CHd_23r
double CHd_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1389
NPEffectiveGIMR::CHd_12r
double CHd_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1386
NPEffectiveGIMR::Ced_1123
double Ced_1123
Definition: NPEffectiveGIMR.h:1500
NPEffectiveGIMR::deltaGammaHZgaRatio1
double deltaGammaHZgaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3173
NPEffectiveGIMR::GammaHccRatio
double GammaHccRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:3297
NPEffectiveGIMR::deltaG_Aff
gslpp::complex deltaG_Aff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1956
NPEffectiveGIMR::deltaG_hAA
virtual double deltaG_hAA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1870
NPEffectiveGIMR::deltaGL_Wff
virtual gslpp::complex deltaGL_Wff(const Particle pbar, const Particle p) const
New physics contribution to the charged current coupling .
Definition: NPEffectiveGIMR.cpp:1789
NPEffectiveGIMR::CLQ1_3332
double CLQ1_3332
Definition: NPEffectiveGIMR.h:1485
NPEffectiveGIMR::CuW_23r
double CuW_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1458
NPEffectiveGIMR::CQe_3233
double CQe_3233
Definition: NPEffectiveGIMR.h:1517
NPEffectiveGIMR::CuH_23r
double CuH_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1422
NPEffectiveGIMR::CLd_1122
double CLd_1122
Definition: NPEffectiveGIMR.h:1509
NPEffectiveGIMR::ettH78_Hgg
double ettH78_Hgg
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPEffectiveGIMR.h:1602
NPEffectiveGIMR::deltaGammaHggRatio2
double deltaGammaHggRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3077
NPEffectiveGIMR::CuB_22i
double CuB_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1475
NPEffectiveGIMR::CLL_2211
double CLL_2211
Definition: NPEffectiveGIMR.h:1479
NPEffectiveGIMR::FlagQuadraticTerms
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on.
Definition: NPEffectiveGIMR.h:1679
NPEffectiveGIMR::CuG_33i
double CuG_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1453
NPEffectiveGIMR::Ceu_3311
double Ceu_3311
Definition: NPEffectiveGIMR.h:1496
NPEffectiveGIMR::eZH78_HZZ2
double eZH78_HZZ2
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1586
NPEffectiveGIMR::CLQ3_3113
double CLQ3_3113
Definition: NPEffectiveGIMR.h:1488
NPEffectiveGIMR::deltaG2_hZA
virtual double deltaG2_hZA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1865
NPEffectiveGIMR::myLEP2GIMR
const LEP2GIMR myLEP2GIMR
Definition: NPEffectiveGIMR.h:1673
NPEffectiveGIMR::CLQ3_1331
double CLQ3_1331
Definition: NPEffectiveGIMR.h:1488
NPEffectiveGIMR::CQe_2322
double CQe_2322
Definition: NPEffectiveGIMR.h:1516
NPEffectiveGIMR::deltaGL_Wffh
gslpp::complex deltaGL_Wffh(const Particle pbar, const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1889
NPEffectiveGIMR::GammaHgagaRatio
double GammaHgagaRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:3197
NPEffectiveGIMR::CLd_3323
double CLd_3323
Definition: NPEffectiveGIMR.h:1511
NPEffectiveGIMR::CHe_13i
double CHe_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1356
NPEffectiveGIMR::eVBF78_HZZ2
double eVBF78_HZZ2
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1541
NPEffectiveGIMR::CLR_bottom
double CLR_bottom() const
Definition: NPEffectiveGIMR.cpp:3422
NPEffectiveGIMR::BrHggRatio
virtual double BrHggRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2834
NPEffectiveGIMR::CLd_1133
double CLd_1133
Definition: NPEffectiveGIMR.h:1510
NPEffectiveGIMR::eZH2_ZuL
double eZH2_ZuL
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1581
NPEffectiveGIMR::CeH_13r
double CeH_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1408
NPEffectiveGIMR::BrHWWRatio
virtual double BrHWWRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2854
NPEffectiveGIMR::CuB_33i
double CuB_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1477
NPEffectiveGIMR::CLu_1122
double CLu_1122
Definition: NPEffectiveGIMR.h:1506
NPEffectiveGIMR::Lambda_NP
double Lambda_NP
The new physics scale [GeV].
Definition: NPEffectiveGIMR.h:1518
Model::name
std::string name
The name of the model.
Definition: Model.h:275
NPEffectiveGIMR::CLQ3_1132
double CLQ3_1132
Definition: NPEffectiveGIMR.h:1490
NPEffectiveGIMR::CRL_strange
double CRL_strange() const
Definition: NPEffectiveGIMR.cpp:3452
NPEffectiveGIMR::CHd_23i
double CHd_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1393
NPEffectiveGIMR::CHd_13r
double CHd_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1387
NPEffectiveGIMR::CuB_11r
double CuB_11r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1466
NPEffectiveGIMR::CuH_23i
double CuH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1428
NPEffectiveGIMR::obliqueS
virtual double obliqueS() const
The oblique parameter .
Definition: NPEffectiveGIMR.cpp:1694
NPEffectiveGIMR::CQe_2211
double CQe_2211
Definition: NPEffectiveGIMR.h:1514
NPEffectiveGIMR::CQe_2333
double CQe_2333
Definition: NPEffectiveGIMR.h:1516
NPEffectiveGIMR::deltaGL_Zffh
double deltaGL_Zffh(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1907
NPEffectiveGIMR::CLd_2223
double CLd_2223
Definition: NPEffectiveGIMR.h:1511
NPEffectiveGIMR::Cee_1111
double Cee_1111
Definition: NPEffectiveGIMR.h:1491
NPEffectiveGIMR::mueeZH
virtual double mueeZH(const double sqrt_s) const
The ratio between the associated production cross-section in the current model and in the Standard ...
Definition: NPEffectiveGIMR.cpp:2567
NPEffectiveGIMR::deltaG3_hZZ
virtual double deltaG3_hZZ() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1853
NPEffectiveGIMR::eVBF2_HZA1
double eVBF2_HZA1
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1523
NPEffectiveGIMR::CuB_12i
double CuB_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1473
NPEffectiveGIMR::CuG_12r
double CuG_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1443
NPEffectiveGIMR::CHe_11
double CHe_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1349
NPEffectiveGIMR::CHL3_13i
double CHL3_13i
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1347
NPEffectiveGIMR::CRL_charm
double CRL_charm() const
Definition: NPEffectiveGIMR.cpp:3447
NPEffectiveGIMR::eVBF2_ZdR
double eVBF2_ZdR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1538
NPEffectiveGIMR::eZH78_HZdR
double eZH78_HZdR
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1593
NPEffectiveGIMR::CuH_33i
double CuH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1429
NPEffectiveGIMR::eZH2_HZZ2
double eZH2_HZZ2
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1573
NPEffectiveGIMR::sW2_tree
double sW2_tree
The sqaure of the tree level values for the sine of the weak angle.
Definition: NPEffectiveGIMR.h:1611
NPEffectiveGIMR::eZH78_HZZ1
double eZH78_HZZ1
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1585
NPEffectiveGIMR::CeH_12r
double CeH_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1407
NPEffectiveGIMR::deltaGammaHZZRatio1
double deltaGammaHZZRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3138
NPEffectiveGIMR::CQe_3222
double CQe_3222
Definition: NPEffectiveGIMR.h:1517
NPEffectiveGIMR::CHe_23r
double CHe_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1353
NPEffectiveGIMR::eZH2_HZdR
double eZH2_HZdR
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1580
NPEffectiveGIMR::CeH_33i
double CeH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1417
NPEffectiveGIMR::CLQ3_3323
double CLQ3_3323
Definition: NPEffectiveGIMR.h:1489
NPEffectiveGIMR::CdH_33r
double CdH_33r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1435
NPEffectiveGIMR::Ced_2232
double Ced_2232
Definition: NPEffectiveGIMR.h:1501
NPEffectiveGIMR::CHu_13r
double CHu_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1378
NPEffectiveGIMR::CuB_33r
double CuB_33r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1471
NPEffectiveGIMR::NPEffectiveGIMR
NPEffectiveGIMR(const bool FlagLeptonUniversal_in=false, const bool FlagQuarkUniversal_in=false)
Constructor.
Definition: NPEffectiveGIMR.cpp:106
NPEffectiveGIMR::eWH78_HWW2
double eWH78_HWW2
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1567
NPEffectiveGIMR::CuG_23r
double CuG_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1446
NPEffectiveGIMR::CHQ3_11
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1367
NPEffectiveGIMR::CLL_mu
double CLL_mu() const
Definition: NPEffectiveGIMR.cpp:3357
NPEffectiveGIMR::CLd_3332
double CLd_3332
Definition: NPEffectiveGIMR.h:1512
NPEffectiveGIMR::CLe_2211
double CLe_2211
Definition: NPEffectiveGIMR.h:1503
NPEffectiveGIMR::Ced_1122
double Ced_1122
Definition: NPEffectiveGIMR.h:1498
NPEffectiveGIMR::deltaGammaHtautauRatio2
double deltaGammaHtautauRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3289
NPEffectiveGIMR::CHud_23i
double CHud_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1404
NPEffectiveGIMR::CuG_13i
double CuG_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1450
NPEffectiveGIMR::cW_tree
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPEffectiveGIMR.h:1608
NPEffectiveGIMR::CHud_11i
double CHud_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1400
NPEffectiveGIMR::CeH_13i
double CeH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1414
NPEffectiveGIMR::CuB_13i
double CuB_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1474
NPEffectiveGIMR::CRR_mu
double CRR_mu() const
Definition: NPEffectiveGIMR.cpp:3462
NPEffectiveGIMR::CLu_1111
double CLu_1111
Definition: NPEffectiveGIMR.h:1505
NPEffectiveGIMR::CuW_11r
double CuW_11r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1454
NPEffectiveGIMR::deltaGammaHbbRatio1
double deltaGammaHbbRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPEffectiveGIMR.cpp:3341
NPEffectiveGIMR::CLu_2211
double CLu_2211
Definition: NPEffectiveGIMR.h:1506
NPEffectiveGIMR::CHL1_13r
double CHL1_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1333
NPEffectiveGIMR::CLQ1_1331
double CLQ1_1331
Definition: NPEffectiveGIMR.h:1483
NPEffectiveGIMR::deltaG1_hZZ
virtual double deltaG1_hZZ() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1843
NPEffectiveGIMR::deltaG2_hZZ
virtual double deltaG2_hZZ() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1848
NPEffectiveGIMR::CLL_up
double CLL_up() const
Definition: NPEffectiveGIMR.cpp:3367
NPEffectiveGIMR::deltaGR_f
double deltaGR_f(const Particle p) const
New physics contribution to the neutral-current right-handed coupling .
Definition: NPEffectiveGIMR.cpp:1770
NPEffectiveGIMR::CLR_up
double CLR_up() const
Definition: NPEffectiveGIMR.cpp:3402
NPEffectiveGIMR::CeH_23r
double CeH_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1410
NPEffectiveGIMR::CLd_1111
double CLd_1111
Definition: NPEffectiveGIMR.h:1508
NPEffectiveGIMR::LEP2AFBmu
virtual double LEP2AFBmu(const double s) const
Definition: NPEffectiveGIMR.cpp:3582
NPEffectiveGIMR::CHu_33
double CHu_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1381
NPEffectiveGIMR::CLd_1132
double CLd_1132
Definition: NPEffectiveGIMR.h:1512
NPEffectiveGIMR::BrHbbRatio
virtual double BrHbbRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2994
NPEffectiveGIMR::eZH78_HZZ3
double eZH78_HZZ3
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at the LHC (7...
Definition: NPEffectiveGIMR.h:1587
NPEffectiveGIMR::ettH78_Htt
double ettH78_Htt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPEffectiveGIMR.h:1601
NPEffectiveGIMR::CdH_13r
double CdH_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1432
NPEffectiveGIMR::CuW_13i
double CuW_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1462
NPEffectiveGIMR::CHF3_diag
double CHF3_diag(const Particle F) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle F.
Definition: NPEffectiveGIMR.cpp:1523
NPEffectiveGIMR::CHQ1_11
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1358
NPEffectiveGIMR::CHe_12i
double CHe_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1355
NPEffectiveGIMR::CHe_23i
double CHe_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1357
NPEffectiveGIMR::CH
double CH
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1330
NPEffectiveGIMR::delta_h
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPEffectiveGIMR.h:1615
NPEffectiveGIMR::eZH2_HZA1
double eZH2_HZA1
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1575
NPEffectiveGIMR::CuB_11i
double CuB_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1472
NPEffectiveGIMR::eVBF78_HZZ1
double eVBF78_HZZ1
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1540
NPEffectiveGIMR::GammaHZgaRatio
double GammaHZgaRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:3157