(Generated on Fri Feb 19 2016 13:25:08 by doxygen 1.8.9.1)
NPEffectiveGIMR.h
Go to the documentation of this file.
1 /*
2  * Copyright (C) 2014 HEPfit Collaboration
3  * All rights reserved.
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 <string.h>
14 #include <stdexcept>
15 
16 
423 class NPEffectiveGIMR : public NPbase {
424 public:
425 
429  static const int NNPEffectiveGIMRVars = 200;
430 
435  static const std::string NPEffectiveGIMRVars[NNPEffectiveGIMRVars];
436 
441  static const int NNPEffectiveGIMRVars_LFU_QFU = 104;
442 
447  static const std::string NPEffectiveGIMRVars_LFU_QFU[NNPEffectiveGIMRVars_LFU_QFU];
448 
454  NPEffectiveGIMR(const bool FlagLeptonUniversal_in = false, const bool FlagQuarkUniversal_in = false);
455 
462  virtual bool PostUpdate();
463 
471  virtual bool CheckParameters(const std::map<std::string, double>& DPars);
472 
479  virtual bool setFlag(const std::string name, const bool value);
480 
481 
483 
494  virtual double DeltaGF() const;
495 
500  virtual double obliqueS() const;
501 
506  virtual double obliqueT() const;
507 
512  virtual double obliqueU() const;
513 
518  virtual double Mw() const;
519 
524  virtual double GammaW() const;
525 
531  virtual double deltaGV_f(const Particle p) const;
532 
538  virtual double deltaGA_f(const Particle p) const;
539 
545  // no generation mixing
546  double deltaGL_f(const Particle p) const;
547 
553  // no generation mixing
554  double deltaGR_f(const Particle p) const;
555 
556 
558 
565  // no generation mixing
566  gslpp::complex deltaGL_Wff(const Particle pbar, const Particle p) const;
573  // no generation mixing
574  gslpp::complex deltaGR_Wff(const Particle pbar, const Particle p) const;
575 
580  double deltaG_hgg() const;
585  double deltaG1_hWW() const;
590  double deltaG2_hWW() const;
595  double deltaG3_hWW() const;
600  double deltaG1_hZZ() const;
605  double deltaG2_hZZ() const;
610  double deltaG3_hZZ() const;
615  double deltaG1_hZA() const;
620  double deltaG2_hZA() const;
625  double deltaG_hAA() const;
626 
632  // no generation mixing
633  gslpp::complex deltaG_hff(const Particle p) const;
634 
641  // no generation mixing
642  gslpp::complex deltaGL_Wffh(const Particle pbar, const Particle p) const;
643 
650  // no generation mixing
651  gslpp::complex deltaGR_Wffh(const Particle pbar, const Particle p) const;
652 
658  // no generation mixing
659  double deltaGL_Zffh(const Particle p) const;
660 
666  // no generation mixing
667  double deltaGR_Zffh(const Particle p) const;
668 
669 
671 
677  gslpp::complex f_triangle(const double tau) const;
685  gslpp::complex AH_f(const double tau) const;
686 
693  virtual double muggH(const double sqrt_s) const;
700  virtual double muVBF(const double sqrt_s) const;
707  virtual double muWH(const double sqrt_s) const;
714  virtual double muZH(const double sqrt_s) const;
722  virtual double mueeZH(const double sqrt_s) const;
729  virtual double muVH(const double sqrt_s) const;
736  virtual double muVBFpVH(const double sqrt_s) const;
743  virtual double muttH(const double sqrt_s) const;
751  virtual double muggHpttH(const double sqrt_s) const;
757  virtual double BrHggRatio() const;
763  virtual double BrHWWRatio() const;
769  virtual double BrHZZRatio() const;
775  virtual double BrHZgaRatio() const;
781  virtual double BrHgagaRatio() const;
787  virtual double BrHtautauRatio() const;
793  virtual double BrHccRatio() const;
799  virtual double BrHbbRatio() const;
805  virtual double computeGammaTotalRatio() const;
812  virtual double deltaGammaTotalRatio1() const;
819  virtual double deltaGammaTotalRatio2() const;
825  double GammaHggRatio() const;
831  double GammaHWWRatio() const;
837  double GammaHZZRatio() const;
843  double GammaHZgaRatio() const;
849  double GammaHgagaRatio() const;
855  double GammaHtautauRatio() const;
861  double GammaHccRatio() const;
867  double GammaHbbRatio() const;
874  double deltaGammaHggRatio1() const;
881  double deltaGammaHWWRatio1() const;
888  double deltaGammaHZZRatio1() const;
895  double deltaGammaHZgaRatio1() const;
902  double deltaGammaHgagaRatio1() const;
909  double deltaGammaHtautauRatio1() const;
916  double deltaGammaHccRatio1() const;
923  double deltaGammaHbbRatio1() const;
930  double deltaGammaHggRatio2() const;
937  double deltaGammaHWWRatio2() const;
944  double deltaGammaHZZRatio2() const;
951  double deltaGammaHZgaRatio2() const;
958  double deltaGammaHgagaRatio2() const;
965  double deltaGammaHtautauRatio2() const;
972  double deltaGammaHccRatio2() const;
979  double deltaGammaHbbRatio2() const;
980 
982 protected:
983 
988  virtual void setParameter(const std::string name, const double& value);
989 
990  double CHG;
991  double CHW;
992  double CHB;
993  double CHWB;
994  double CHD;
995  double CHbox;
996  double CH;
997  double CHL1_11;
998  double CHL1_12r;
999  double CHL1_13r;
1000  double CHL1_22;
1001  double CHL1_23r;
1002  double CHL1_33;
1003  double CHL1_12i;
1004  double CHL1_13i;
1005  double CHL1_23i;
1006  double CHL3_11;
1007  double CHL3_12r;
1008  double CHL3_13r;
1009  double CHL3_22;
1010  double CHL3_23r;
1011  double CHL3_33;
1012  double CHL3_12i;
1013  double CHL3_13i;
1014  double CHL3_23i;
1015  double CHe_11;
1016  double CHe_12r;
1017  double CHe_13r;
1018  double CHe_22;
1019  double CHe_23r;
1020  double CHe_33;
1021  double CHe_12i;
1022  double CHe_13i;
1023  double CHe_23i;
1024  double CHQ1_11;
1025  double CHQ1_12r;
1026  double CHQ1_13r;
1027  double CHQ1_22;
1028  double CHQ1_23r;
1029  double CHQ1_33;
1030  double CHQ1_12i;
1031  double CHQ1_13i;
1032  double CHQ1_23i;
1033  double CHQ3_11;
1034  double CHQ3_12r;
1035  double CHQ3_13r;
1036  double CHQ3_22;
1037  double CHQ3_23r;
1038  double CHQ3_33;
1039  double CHQ3_12i;
1040  double CHQ3_13i;
1041  double CHQ3_23i;
1042  double CHu_11;
1043  double CHu_12r;
1044  double CHu_13r;
1045  double CHu_22;
1046  double CHu_23r;
1047  double CHu_33;
1048  double CHu_12i;
1049  double CHu_13i;
1050  double CHu_23i;
1051  double CHd_11;
1052  double CHd_12r;
1053  double CHd_13r;
1054  double CHd_22;
1055  double CHd_23r;
1056  double CHd_33;
1057  double CHd_12i;
1058  double CHd_13i;
1059  double CHd_23i;
1060  double CHud_11r;
1061  double CHud_12r;
1062  double CHud_13r;
1063  double CHud_22r;
1064  double CHud_23r;
1065  double CHud_33r;
1066  double CHud_11i;
1067  double CHud_12i;
1068  double CHud_13i;
1069  double CHud_22i;
1070  double CHud_23i;
1071  double CHud_33i;
1072  double CeH_11r;
1073  double CeH_12r;
1074  double CeH_13r;
1075  double CeH_22r;
1076  double CeH_23r;
1077  double CeH_33r;
1078  double CeH_11i;
1079  double CeH_12i;
1080  double CeH_13i;
1081  double CeH_22i;
1082  double CeH_23i;
1083  double CeH_33i;
1084  double CuH_11r;
1085  double CuH_12r;
1086  double CuH_13r;
1087  double CuH_22r;
1088  double CuH_23r;
1089  double CuH_33r;
1090  double CuH_11i;
1091  double CuH_12i;
1092  double CuH_13i;
1093  double CuH_22i;
1094  double CuH_23i;
1095  double CuH_33i;
1096  double CdH_11r;
1097  double CdH_12r;
1098  double CdH_13r;
1099  double CdH_22r;
1100  double CdH_23r;
1101  double CdH_33r;
1102  double CdH_11i;
1103  double CdH_12i;
1104  double CdH_13i;
1105  double CdH_22i;
1106  double CdH_23i;
1107  double CdH_33i;
1108  double CLL_1221;
1109  double CLL_2112;
1110  double Lambda_NP;
1111 // The error in the parameters multiplying the dimension-6 operator coefficients in the production cross sections.
1112  double eVBF2_HZZ1;
1113  double eVBF2_HZZ2;
1114  double eVBF2_HZZ3;
1115  double eVBF2_HZA1;
1116  double eVBF2_HZA2;
1117  double eVBF2_HAA;
1118  double eVBF2_HWW1;
1119  double eVBF2_HWW2;
1120  double eVBF2_HWW3;
1121  double eVBF2_Hgg;
1122  double eVBF2_HZuL;
1123  double eVBF2_HZuR;
1124  double eVBF2_HZdL;
1125  double eVBF2_HZdR;
1126  double eVBF2_HWud;
1127  double eVBF2_ZuL;
1128  double eVBF2_ZuR;
1129  double eVBF2_ZdL;
1130  double eVBF2_ZdR;
1131  double eVBF2_Wud;
1132  double eVBF78_HZZ1;
1133  double eVBF78_HZZ2;
1134  double eVBF78_HZZ3;
1135  double eVBF78_HZA1;
1136  double eVBF78_HZA2;
1137  double eVBF78_HAA;
1138  double eVBF78_HWW1;
1139  double eVBF78_HWW2;
1140  double eVBF78_HWW3;
1141  double eVBF78_Hgg;
1142  double eVBF78_HZuL;
1143  double eVBF78_HZuR;
1144  double eVBF78_HZdL;
1145  double eVBF78_HZdR;
1146  double eVBF78_HWud;
1147  double eVBF78_ZuL;
1148  double eVBF78_ZuR;
1149  double eVBF78_ZdL;
1150  double eVBF78_ZdR;
1151  double eVBF78_Wud;
1152 
1153  double eWH2_HWW1;
1154  double eWH2_HWW2;
1155  double eWH2_HWW3;
1156  double eWH2_HWud;
1157  double eWH2_Wud;
1158  double eWH78_HWW1;
1159  double eWH78_HWW2;
1160  double eWH78_HWW3;
1161  double eWH78_HWud;
1162  double eWH78_Wud;
1163 
1164  double eZH2_HZZ1;
1165  double eZH2_HZZ2;
1166  double eZH2_HZZ3;
1167  double eZH2_HZA1;
1168  double eZH2_HZA2;
1169  double eZH2_HZuL;
1170  double eZH2_HZuR;
1171  double eZH2_HZdL;
1172  double eZH2_HZdR;
1173  double eZH2_ZuL;
1174  double eZH2_ZuR;
1175  double eZH2_ZdL;
1176  double eZH2_ZdR;
1177  double eZH78_HZZ1;
1178  double eZH78_HZZ2;
1179  double eZH78_HZZ3;
1180  double eZH78_HZA1;
1181  double eZH78_HZA2;
1182  double eZH78_HZuL;
1183  double eZH78_HZuR;
1184  double eZH78_HZdL;
1185  double eZH78_HZdR;
1186  double eZH78_ZuL;
1187  double eZH78_ZuR;
1188  double eZH78_ZdL;
1189  double eZH78_ZdR;
1190 
1191  double ettH2_Htt;
1192  double ettH2_Hgg;
1193  double ettH78_Htt;
1194  double ettH78_Hgg;
1195 
1196  double MwInput;
1197 
1198  double LambdaNP2;
1199  double v2_over_LambdaNP2;
1200  double cW_tree;
1201  double sW_tree;
1202  double cW2_tree;
1203  double sW2_tree;
1204  double delta_ZZ;
1205  double delta_AA;
1206  double delta_AZ;
1207  double delta_h;
1208 
1214  double CHF1_diag(const Particle F) const;
1215 
1221  double CHF3_diag(const Particle F) const;
1222 
1228  double CHf_diag(const Particle f) const;
1229 
1235  gslpp::complex CHud_diag(const Particle u) const;
1236 
1242  gslpp::complex CfH_diag(const Particle f) const;
1243 
1244 
1246 private:
1247 
1248  bool FlagMwInput;
1249  bool FlagQuadraticTerms;
1250 
1255  const bool FlagLeptonUniversal;
1256 
1261  const bool FlagQuarkUniversal;
1262 
1263 };
1264 
1265 #endif /* NPEFFECTIVEGIMR_H */
1266 
NPEffectiveGIMR::eVBF2_HWW1
double eVBF2_HWW1
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1118
NPEffectiveGIMR::eVBF2_HZdR
double eVBF2_HZdR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1125
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:2206
NPEffectiveGIMR::CeH_23r
double CeH_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1076
NPEffectiveGIMR::eVBF78_ZuR
double eVBF78_ZuR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1148
NPEffectiveGIMR::obliqueU
virtual double obliqueU() const
The oblique parameter .
Definition: NPEffectiveGIMR.cpp:1050
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:873
NPEffectiveGIMR::CHu_33
double CHu_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1047
NPEffectiveGIMR::deltaG3_hZZ
double deltaG3_hZZ() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1194
NPEffectiveGIMR::CuH_33i
double CuH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1095
NPEffectiveGIMR::CHe_12i
double CHe_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1021
NPEffectiveGIMR::eVBF2_HZZ1
double eVBF2_HZZ1
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1112
NPEffectiveGIMR::eWH2_HWW3
double eWH2_HWW3
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1155
NPEffectiveGIMR::CHe_23r
double CHe_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1019
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:1918
NPEffectiveGIMR::CHL3_22
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1009
NPEffectiveGIMR::CHD
double CHD
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:994
NPEffectiveGIMR::deltaG1_hWW
double deltaG1_hWW() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1161
NPEffectiveGIMR::CdH_33r
double CdH_33r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1101
NPEffectiveGIMR::eVBF78_HZZ1
double eVBF78_HZZ1
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1132
NPEffectiveGIMR::CHL1_13i
double CHL1_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1004
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:1517
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:2027
NPEffectiveGIMR::CHu_13i
double CHu_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1049
NPEffectiveGIMR::CHQ3_12i
double CHQ3_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1039
NPEffectiveGIMR::eVBF2_HZZ3
double eVBF2_HZZ3
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1114
NPEffectiveGIMR::eVBF78_HWW1
double eVBF78_HWW1
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1138
NPEffectiveGIMR::CdH_23i
double CdH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1106
NPbase
The auxiliary base model class for other model classes.
Definition: NPbase.h:66
NPEffectiveGIMR::Mw
virtual double Mw() const
The mass of the boson, .
Definition: NPEffectiveGIMR.cpp:1055
NPEffectiveGIMR::MwInput
double MwInput
The input value for the -boson mass if FlagMwInput is true.
Definition: NPEffectiveGIMR.h:1196
NPEffectiveGIMR::CeH_13i
double CeH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1080
NPEffectiveGIMR::CHQ1_33
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1029
NPEffectiveGIMR::deltaGA_f
virtual double deltaGA_f(const Particle p) const
New physics contribution to the neutral-current axial-vector coupling .
Definition: NPEffectiveGIMR.cpp:1087
NPEffectiveGIMR::CLL_1221
double CLL_1221
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1108
NPEffectiveGIMR::eVBF2_HAA
double eVBF2_HAA
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1117
NPEffectiveGIMR::eVBF2_HZuR
double eVBF2_HZuR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1123
NPEffectiveGIMR::CHud_22r
double CHud_22r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1063
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:2200
NPEffectiveGIMR::CHL3_11
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1006
Particle
A class for particles.
Definition: Particle.h:26
NPEffectiveGIMR::CHQ1_13r
double CHQ1_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1026
NPEffectiveGIMR::BrHtautauRatio
virtual double BrHtautauRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:1846
NPEffectiveGIMR::eVBF2_HWW3
double eVBF2_HWW3
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1120
NPEffectiveGIMR::LambdaNP2
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPEffectiveGIMR.h:1198
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:1162
NPEffectiveGIMR::CHQ1_11
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1024
NPEffectiveGIMR::CuH_22i
double CuH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1093
NPEffectiveGIMR::CHQ3_13i
double CHQ3_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1040
NPEffectiveGIMR::CH
double CH
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:996
NPEffectiveGIMR::GammaHgagaRatio
double GammaHgagaRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2086
NPEffectiveGIMR::CHQ3_23i
double CHQ3_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1041
NPEffectiveGIMR::CuH_11i
double CuH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1090
NPEffectiveGIMR::eVBF2_HZZ2
double eVBF2_HZZ2
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1113
NPEffectiveGIMR::CHd_13i
double CHd_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1058
NPEffectiveGIMR::CeH_11r
double CeH_11r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1072
NPEffectiveGIMR::CHL1_23i
double CHL1_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1005
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:1182
NPEffectiveGIMR::setFlag
virtual bool setFlag(const std::string name, const bool value)
A method to set a flag of NPEffectiveGIMR.
Definition: NPEffectiveGIMR.cpp:911
NPEffectiveGIMR::CeH_22i
double CeH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1081
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:947
NPEffectiveGIMR::deltaG_hgg
double deltaG_hgg() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1156
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:2177
NPEffectiveGIMR::ettH2_Hgg
double ettH2_Hgg
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPEffectiveGIMR.h:1192
NPEffectiveGIMR::deltaG1_hZA
double deltaG1_hZA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1201
NPEffectiveGIMR::CHu_23r
double CHu_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1046
NPEffectiveGIMR::eWH2_HWud
double eWH2_HWud
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1156
NPEffectiveGIMR::CHud_33r
double CHud_33r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1065
NPEffectiveGIMR::ettH2_Htt
double ettH2_Htt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPEffectiveGIMR.h:1191
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:929
NPEffectiveGIMR::eVBF2_HZdL
double eVBF2_HZdL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1124
NPEffectiveGIMR::eVBF2_HZA2
double eVBF2_HZA2
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1116
NPEffectiveGIMR::CHG
double CHG
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:990
NPEffectiveGIMR::CHd_33
double CHd_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1056
NPEffectiveGIMR::GammaHccRatio
double GammaHccRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2156
NPEffectiveGIMR::delta_AA
double delta_AA
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPEffectiveGIMR.h:1205
NPEffectiveGIMR::CHL3_33
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1011
NPEffectiveGIMR::delta_AZ
double delta_AZ
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPEffectiveGIMR.h:1206
NPEffectiveGIMR::eWH2_Wud
double eWH2_Wud
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1157
NPEffectiveGIMR::CHe_13r
double CHe_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1017
NPEffectiveGIMR::deltaG_hff
gslpp::complex deltaG_hff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1216
NPEffectiveGIMR::NNPEffectiveGIMRVars
static const int NNPEffectiveGIMRVars
The number of the model parameters in NPEffectiveGIMR.
Definition: NPEffectiveGIMR.h:429
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:1180
NPEffectiveGIMR::CHu_12r
double CHu_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1043
NPEffectiveGIMR::GammaHtautauRatio
double GammaHtautauRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2126
NPEffectiveGIMR::eVBF78_HWud
double eVBF78_HWud
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1146
NPEffectiveGIMR::CeH_23i
double CeH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1082
NPbase.h
NPEffectiveGIMR::CHL1_23r
double CHL1_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1001
NPEffectiveGIMR::obliqueS
virtual double obliqueS() const
The oblique parameter .
Definition: NPEffectiveGIMR.cpp:1040
NPEffectiveGIMR::obliqueT
virtual double obliqueT() const
The oblique parameter .
Definition: NPEffectiveGIMR.cpp:1045
NPEffectiveGIMR::CeH_11i
double CeH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1078
NPEffectiveGIMR::CeH_22r
double CeH_22r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1075
NPEffectiveGIMR::eZH2_ZdR
double eZH2_ZdR
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1176
NPEffectiveGIMR::deltaGL_Wff
gslpp::complex deltaGL_Wff(const Particle pbar, const Particle p) const
New physics contribution to the charged current coupling .
Definition: NPEffectiveGIMR.cpp:1130
NPEffectiveGIMR::CuH_13r
double CuH_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1086
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:1160
NPEffectiveGIMR::eZH2_ZuR
double eZH2_ZuR
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1174
NPEffectiveGIMR::CHu_22
double CHu_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1045
NPEffectiveGIMR::eVBF2_HZuL
double eVBF2_HZuL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1122
NPEffectiveGIMR::eWH2_HWW2
double eWH2_HWW2
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1154
NPEffectiveGIMR::eVBF78_Hgg
double eVBF78_Hgg
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1141
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:1966
NPEffectiveGIMR::CHud_23r
double CHud_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1064
NPEffectiveGIMR::cW2_tree
double cW2_tree
The sqaure of the tree level values for the cosine of the weak angle.
Definition: NPEffectiveGIMR.h:1202
NPEffectiveGIMR::CHud_33i
double CHud_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1071
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:1184
NPEffectiveGIMR::GammaW
virtual double GammaW() const
The total width of the boson, .
Definition: NPEffectiveGIMR.cpp:1066
NPEffectiveGIMR::DeltaGF
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPEffectiveGIMR.cpp:1035
NPEffectiveGIMR::CHe_12r
double CHe_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1016
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:1189
NPEffectiveGIMR::eVBF78_ZdR
double eVBF78_ZdR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1150
NPEffectiveGIMR::CHe_33
double CHe_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1020
Model::name
std::string name
The name of the model.
Definition: Model.h:203
NPEffectiveGIMR::CdH_22r
double CdH_22r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1099
NPEffectiveGIMR::eVBF78_HZZ3
double eVBF78_HZZ3
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1134
NPEffectiveGIMR::FlagQuarkUniversal
const bool FlagQuarkUniversal
An internal boolean flag that is true if assuming quark flavour universality.
Definition: NPEffectiveGIMR.h:1261
NPEffectiveGIMR::eVBF2_Hgg
double eVBF2_Hgg
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1121
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:1161
NPEffectiveGIMR::deltaG1_hZZ
double deltaG1_hZZ() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1184
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:1673
NPEffectiveGIMR::GammaHggRatio
double GammaHggRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:1942
NPEffectiveGIMR::eVBF78_HZuL
double eVBF78_HZuL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1142
NPEffectiveGIMR::eVBF78_HZdL
double eVBF78_HZdL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1144
NPEffectiveGIMR::CHd_11
double CHd_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1051
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:1627
NPEffectiveGIMR::CHu_11
double CHu_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1042
NPEffectiveGIMR::deltaG2_hZZ
double deltaG2_hZZ() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1189
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:1265
NPEffectiveGIMR::CHQ3_13r
double CHQ3_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1035
NPEffectiveGIMR::v2_over_LambdaNP2
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPEffectiveGIMR.h:1199
NPEffectiveGIMR::CHud_13r
double CHud_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1062
NPEffectiveGIMR::eVBF2_HWud
double eVBF2_HWud
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1126
NPEffectiveGIMR::eZH2_HZZ1
double eZH2_HZZ1
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1164
NPEffectiveGIMR::CHud_12i
double CHud_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1067
NPEffectiveGIMR::CuH_13i
double CuH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1092
NPEffectiveGIMR::CHL3_23i
double CHL3_23i
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1014
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:1181
NPEffectiveGIMR::computeGammaTotalRatio
virtual double computeGammaTotalRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:1906
NPEffectiveGIMR::CHQ1_23r
double CHQ1_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1028
NPEffectiveGIMR::CHQ1_12r
double CHQ1_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1025
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:441
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:2172
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:1187
NPEffectiveGIMR::CHL3_13r
double CHL3_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1008
NPEffectiveGIMR::GammaHZgaRatio
double GammaHZgaRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2046
NPEffectiveGIMR::CHQ1_23i
double CHQ1_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1032
NPEffectiveGIMR::deltaGR_Wff
gslpp::complex deltaGR_Wff(const Particle pbar, const Particle p) const
New physics contribution to the charged current coupling .
Definition: NPEffectiveGIMR.cpp:1147
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:1458
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:1248
NPEffectiveGIMR::eVBF78_HAA
double eVBF78_HAA
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1137
NPEffectiveGIMR::GammaHWWRatio
double GammaHWWRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:1977
NPEffectiveGIMR::CHu_12i
double CHu_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1048
NPEffectiveGIMR::FlagLeptonUniversal
const bool FlagLeptonUniversal
An internal boolean flag that is true if assuming lepton flavour universality.
Definition: NPEffectiveGIMR.h:1255
NPEffectiveGIMR::CHL1_22
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1000
NPEffectiveGIMR::eZH2_ZdL
double eZH2_ZdL
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1175
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:1230
NPEffectiveGIMR::eVBF78_Wud
double eVBF78_Wud
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1151
NPEffectiveGIMR::eVBF2_ZdL
double eVBF2_ZdL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1129
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:1186
NPEffectiveGIMR::CHL1_33
double CHL1_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1002
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:1688
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:1958
NPEffectiveGIMR::CHQ3_23r
double CHQ3_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1037
NPEffectiveGIMR::eVBF78_HZuR
double eVBF78_HZuR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1143
NPEffectiveGIMR::CHQ3_12r
double CHQ3_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1034
NPEffectiveGIMR::NPEffectiveGIMRVars
static const std::string NPEffectiveGIMRVars[NNPEffectiveGIMRVars]
A string array containing the labels of the model parameters in NPEffectiveGIMR.
Definition: NPEffectiveGIMR.h:435
NPEffectiveGIMR::eVBF2_ZuR
double eVBF2_ZuR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1128
NPEffectiveGIMR::CeH_33r
double CeH_33r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1077
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:2062
NPEffectiveGIMR::CHud_11r
double CHud_11r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1060
NPEffectiveGIMR::CuH_12i
double CuH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1091
NPEffectiveGIMR::eZH2_HZdL
double eZH2_HZdL
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1171
NPEffectiveGIMR::CuH_12r
double CuH_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1085
NPEffectiveGIMR::CuH_11r
double CuH_11r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1084
NPEffectiveGIMR::CHd_12r
double CHd_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1052
NPEffectiveGIMR::CdH_11r
double CdH_11r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1096
NPEffectiveGIMR::CHW
double CHW
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:991
NPEffectiveGIMR::CuH_33r
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1089
NPEffectiveGIMR::CHd_22
double CHd_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1054
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:2113
NPEffectiveGIMR::eVBF78_HZdR
double eVBF78_HZdR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1145
NPEffectiveGIMR::CHB
double CHB
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:992
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:1660
NPEffectiveGIMR::eVBF78_HZA2
double eVBF78_HZA2
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1136
NPEffectiveGIMR::CHud_13i
double CHud_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1068
NPEffectiveGIMR::eVBF78_HZA1
double eVBF78_HZA1
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1135
NPEffectiveGIMR::CdH_22i
double CdH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1105
NPEffectiveGIMR::CHQ3_22
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1036
NPEffectiveGIMR::CHe_22
double CHe_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1018
NPEffectiveGIMR::CHL3_12i
double CHL3_12i
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1012
NPEffectiveGIMR::CHL3_23r
double CHL3_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1010
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:1188
NPEffectiveGIMR::CHud_12r
double CHud_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1061
NPEffectiveGIMR::eVBF78_ZuL
double eVBF78_ZuL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1147
NPEffectiveGIMR::eVBF78_HZZ2
double eVBF78_HZZ2
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1133
NPEffectiveGIMR::CHu_23i
double CHu_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1050
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:335
NPEffectiveGIMR::deltaGR_f
double deltaGR_f(const Particle p) const
New physics contribution to the neutral-current right-handed coupling .
Definition: NPEffectiveGIMR.cpp:1111
NPEffectiveGIMR::CdH_13i
double CdH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1104
NPEffectiveGIMR::CHbox
double CHbox
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:995
NPEffectiveGIMR::CeH_13r
double CeH_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1074
NPEffectiveGIMR::CHd_12i
double CHd_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1057
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:1183
NPEffectiveGIMR::CdH_33i
double CdH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1107
NPEffectiveGIMR::BrHccRatio
virtual double BrHccRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:1866
NPEffectiveGIMR::BrHZZRatio
virtual double BrHZZRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:1786
NPEffectiveGIMR::CHd_23i
double CHd_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1059
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:991
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:1158
NPEffectiveGIMR::eVBF2_ZuL
double eVBF2_ZuL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1127
NPEffectiveGIMR::eVBF78_HWW3
double eVBF78_HWW3
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1140
NPEffectiveGIMR::GammaHZZRatio
double GammaHZZRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2011
NPEffectiveGIMR::CHud_22i
double CHud_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1069
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:965
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:447
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:1732
NPEffectiveGIMR
A model class for new physics in the form of the dimension-six effective Lagrangian.
Definition: NPEffectiveGIMR.h:423
NPEffectiveGIMR::CHL3_13i
double CHL3_13i
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1013
NPEffectiveGIMR::CHQ1_22
double CHQ1_22
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1027
NPEffectiveGIMR::BrHZgaRatio
virtual double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:1806
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:2074
NPEffectiveGIMR::GammaHbbRatio
double GammaHbbRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:2185
NPEffectiveGIMR::CdH_23r
double CdH_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1100
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:2002
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:1178
NPEffectiveGIMR::BrHgagaRatio
virtual double BrHgagaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:1826
NPEffectiveGIMR::CdH_12i
double CdH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1103
NPEffectiveGIMR::CdH_12r
double CdH_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1097
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:1993
NPEffectiveGIMR::CHWB
double CHWB
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:993
NPEffectiveGIMR::eZH2_HZuR
double eZH2_HZuR
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1170
NPEffectiveGIMR::deltaGV_f
virtual double deltaGV_f(const Particle p) const
New physics contribution to the neutral-current vector coupling .
Definition: NPEffectiveGIMR.cpp:1082
NPEffectiveGIMR::NPEffectiveGIMR
NPEffectiveGIMR(const bool FlagLeptonUniversal_in=false, const bool FlagQuarkUniversal_in=false)
Constructor.
Definition: NPEffectiveGIMR.cpp:76
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:2102
NPEffectiveGIMR::CLL_2112
double CLL_2112
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1109
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:1277
NPEffectiveGIMR::CHud_23i
double CHud_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1070
NPEffectiveGIMR::deltaG2_hZA
double deltaG2_hZA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1206
NPEffectiveGIMR::CHL1_12r
double CHL1_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:998
NPEffectiveGIMR::deltaG2_hWW
double deltaG2_hWW() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1166
NPEffectiveGIMR::eVBF2_HWW2
double eVBF2_HWW2
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1119
NPEffectiveGIMR::CuH_23i
double CuH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1094
NPEffectiveGIMR::ettH78_Htt
double ettH78_Htt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPEffectiveGIMR.h:1193
NPEffectiveGIMR::eVBF2_ZdR
double eVBF2_ZdR
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1130
NPEffectiveGIMR::CHQ1_13i
double CHQ1_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1031
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:1179
NPEffectiveGIMR::deltaG_hAA
double deltaG_hAA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1211
NPEffectiveGIMR::CdH_13r
double CdH_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1098
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:2036
NPEffectiveGIMR::CHe_23i
double CHe_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1023
NPEffectiveGIMR::CHL3_12r
double CHL3_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1007
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:2148
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:1185
NPEffectiveGIMR::CdH_11i
double CdH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1102
NPEffectiveGIMR::CeH_33i
double CeH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1083
NPEffectiveGIMR::CHQ3_33
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1038
NPEffectiveGIMR::deltaGR_Zffh
double deltaGR_Zffh(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1256
NPEffectiveGIMR::BrHggRatio
virtual double BrHggRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:1746
NPEffectiveGIMR::delta_ZZ
double delta_ZZ
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPEffectiveGIMR.h:1204
NPEffectiveGIMR::eWH2_HWW1
double eWH2_HWW1
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1153
NPEffectiveGIMR::deltaGL_Zffh
double deltaGL_Zffh(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1248
NPEffectiveGIMR::BrHWWRatio
virtual double BrHWWRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:1766
NPEffectiveGIMR::CHu_13r
double CHu_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1044
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:1159
NPEffectiveGIMR::eVBF78_HWW2
double eVBF78_HWW2
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1139
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:1930
NPEffectiveGIMR::deltaG3_hWW
double deltaG3_hWW() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPEffectiveGIMR.cpp:1171
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:1282
NPEffectiveGIMR::cW_tree
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPEffectiveGIMR.h:1200
NPEffectiveGIMR::CHud_11i
double CHud_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1066
NPEffectiveGIMR::CHQ3_11
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1033
NPEffectiveGIMR::eZH2_HZuL
double eZH2_HZuL
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1169
NPEffectiveGIMR::eVBF78_ZdL
double eVBF78_ZdL
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at the LHC (...
Definition: NPEffectiveGIMR.h:1149
NPEffectiveGIMR::CHL1_13r
double CHL1_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:999
gslpp::complex
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
NPEffectiveGIMR::PostUpdate
virtual bool PostUpdate()
The post-update method for NPEffectiveGIMR.
Definition: NPEffectiveGIMR.cpp:312
NPEffectiveGIMR::Lambda_NP
double Lambda_NP
The new physics scale [GeV].
Definition: NPEffectiveGIMR.h:1110
NPEffectiveGIMR::CeH_12i
double CeH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1079
NPEffectiveGIMR::CHd_23r
double CHd_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1055
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:1239
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:1006
NPEffectiveGIMR::sW_tree
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPEffectiveGIMR.h:1201
NPEffectiveGIMR::delta_h
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPEffectiveGIMR.h:1207
NPEffectiveGIMR::CHd_13r
double CHd_13r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1053
NPEffectiveGIMR::BrHbbRatio
virtual double BrHbbRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPEffectiveGIMR.cpp:1886
NPEffectiveGIMR::eZH2_HZA1
double eZH2_HZA1
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1167
NPEffectiveGIMR::eZH2_HZA2
double eZH2_HZA2
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1168
NPEffectiveGIMR::deltaGL_f
double deltaGL_f(const Particle p) const
New physics contribution to the neutral-current left-handed coupling .
Definition: NPEffectiveGIMR.cpp:1092
NPEffectiveGIMR::eVBF2_Wud
double eVBF2_Wud
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1131
NPEffectiveGIMR::CuH_22r
double CuH_22r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1087
NPEffectiveGIMR::CuH_23r
double CuH_23r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1088
NPEffectiveGIMR::eVBF2_HZA1
double eVBF2_HZA1
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPEffectiveGIMR.h:1115
NPEffectiveGIMR::eZH2_HZZ2
double eZH2_HZZ2
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1165
NPEffectiveGIMR::CHe_11
double CHe_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:1015
NPEffectiveGIMR::CeH_12r
double CeH_12r
The dimension-6 operator coefficient (real part).
Definition: NPEffectiveGIMR.h:1073
NPEffectiveGIMR::eZH2_HZdR
double eZH2_HZdR
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1172
NPEffectiveGIMR::ettH78_Hgg
double ettH78_Hgg
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPEffectiveGIMR.h:1194
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:1249
NPEffectiveGIMR::sW2_tree
double sW2_tree
The sqaure of the tree level values for the sine of the weak angle.
Definition: NPEffectiveGIMR.h:1203
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:1177
NPEffectiveGIMR::CHQ1_12i
double CHQ1_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1030
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:2142
NPEffectiveGIMR::CHe_13i
double CHe_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1022
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:1312
NPEffectiveGIMR::CHL1_11
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPEffectiveGIMR.h:997
NPEffectiveGIMR::eZH2_HZZ3
double eZH2_HZZ3
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1166
NPEffectiveGIMR::CHL1_12i
double CHL1_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPEffectiveGIMR.h:1003
NPEffectiveGIMR::eZH2_ZuL
double eZH2_ZuL
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPEffectiveGIMR.h:1173