1 | /*
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2 | ---- Delphes ----
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3 | A Fast Simulator for general purpose LHC detector
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4 | S. Ovyn ~~~~ severine.ovyn@uclouvain.be
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5 |
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6 | Center for Particle Physics and Phenomenology (CP3)
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7 | Universite Catholique de Louvain (UCL)
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8 | Louvain-la-Neuve, Belgium
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9 | */
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10 |
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11 | /// \file SmearUtil.cc
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12 | /// \brief RESOLution class, and some generic definitions
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13 |
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14 |
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15 | #include "interface/SmearUtil.h"
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16 | #include "TRandom.h"
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17 |
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18 | #include <iostream>
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19 | #include <sstream>
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20 | #include <fstream>
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21 | using namespace std;
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22 |
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23 | //------------------------------------------------------------------------------
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24 |
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25 | RESOLution::RESOLution() {
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26 |
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27 | MAX_TRACKER = 2.5; // tracker coverage
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28 | MAX_CALO_CEN = 3.0; // central calorimeter coverage
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29 | MAX_CALO_FWD = 5.0; // forward calorimeter pseudorapidity coverage
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30 | MAX_MU = 2.4; // muon chambers pseudorapidity coverage
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31 | MIN_CALO_VFWD= 5.2; // very forward calorimeter (if any), like CASTOR
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32 | MAX_CALO_VFWD= 6.6; // very forward calorimeter (if any), like CASTOR
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33 | MIN_ZDC = 8.3; // zero-degree calorimeter, coverage
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34 |
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35 | ZDC_S = 140.; // ZDC distance to IP
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36 | RP220_S = 220; // distance of the RP to the IP, in meters
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37 | RP220_X = 0.002;// distance of the RP to the beam, in meters
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38 | FP420_S = 420; // distance of the RP to the IP, in meters
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39 | FP420_X = 0.004;// distance of the RP to the beam, in meters
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40 |
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41 |
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42 | ELG_Scen = 0.028; // S term for central ECAL
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43 | ELG_Ncen = 0.124 ; // N term for central ECAL
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44 | ELG_Ccen = 0.0026 ; // C term for central ECAL
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45 | ELG_Cfwd = 0.107 ; // S term for forward ECAL
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46 | ELG_Sfwd = 2.084 ; // C term for forward ECAL
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47 | ELG_Nfwd = 0.0 ; // N term for central ECAL
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48 |
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49 | HAD_Secal = 0.05 ; // S term for central ECAL // electromagnetic calorimeter
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50 | HAD_Necal = 0.25 ; // N term for central ECAL
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51 | HAD_Cecal = 0.0055 ; // C term for central ECAL
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52 | HAD_Shcal = 0.91 ; // S term for central HCAL // hadronic calorimeter
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53 | HAD_Nhcal = 0. ; // N term for central HCAL
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54 | HAD_Chcal = 0.038 ; // C term for central HCAL
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55 | HAD_Shf = 2.7 ; // S term for central HF // forward calorimeter
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56 | HAD_Nhf = 0. ; // N term for central HF
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57 | HAD_Chf = 0.13 ; // C term for central HF
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58 |
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59 | MU_SmearPt = 0.01 ;
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60 |
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61 | TAU_CONE_ENERGY = 0.15 ; // Delta R = radius of the cone // for "electromagnetic collimation"
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62 | TAU_EM_COLLIMATION = 0.95;
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63 | TAU_CONE_TRACKS= 0.4 ; //Delta R for tracker isolation for tau's
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64 | PT_TRACK_TAU = 2.0 ; // GeV // 6 GeV ????
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65 |
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66 |
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67 | PT_TRACKS_MIN = 0.9 ; // minimal pt needed to reach the calorimeter, in GeV
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68 | PT_QUARKS_MIN = 2.0 ; // minimal pt needed by quarks to reach the tracker, in GeV (??????)
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69 | TRACKING_EFF = 90;
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70 |
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71 |
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72 | TAGGING_B = 40;
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73 | MISTAGGING_C = 10;
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74 | MISTAGGING_L = 1;
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75 |
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76 |
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77 | CONERADIUS = 0.7; // generic jet radius ; not for tau's !!!
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78 | JETALGO = 1; // 1 for Cone algorithm, 2 for MidPoint algorithm, 3 for SIScone algorithm, 4 for kt algorithm
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79 | // Define Cone algorithm.
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80 | C_SEEDTHRESHOLD = 1.0;
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81 | C_ADJACENCYCUT = 2;
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82 | C_MAXITERATIONS = 100;
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83 | C_IRATCH = 1;
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84 | C_OVERLAPTHRESHOLD = 0.75;
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85 |
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86 | //Define MidPoint algorithm.
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87 | M_SEEDTHRESHOLD = 1.0;
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88 | M_CONEAREAFRACTION = 0.25;
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89 | M_MAXPAIRSIZE = 2;
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90 | M_MAXITERATIONS = 100;
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91 | M_OVERLAPTHRESHOLD = 0.75;
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92 |
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93 | }
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94 |
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95 | //------------------------------------------------------------------------------
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96 | void RESOLution::ReadDataCard(const string datacard) {
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97 |
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98 | string temp_string;
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99 | istringstream curstring;
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100 |
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101 | ifstream fichier_a_lire(datacard.c_str());
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102 | if(!fichier_a_lire.good()) {
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103 | cout << datacard << "Datadard " << datacard << " not found, use default values" << endl;
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104 | return;
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105 | }
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106 |
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107 | while (getline(fichier_a_lire,temp_string)) {
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108 | curstring.clear(); // needed when using several times istringstream::str(string)
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109 | curstring.str(temp_string);
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110 | string varname;
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111 | float value;
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112 |
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113 | if(strstr(temp_string.c_str(),"#")) { }
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114 | else if(strstr(temp_string.c_str(),"MAX_TRACKER")){curstring >> varname >> value; MAX_TRACKER = value;}
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115 | else if(strstr(temp_string.c_str(),"MAX_CALO_CEN")){curstring >> varname >> value; MAX_CALO_CEN = value;}
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116 | else if(strstr(temp_string.c_str(),"MAX_CALO_FWD")){curstring >> varname >> value; MAX_CALO_FWD = value;}
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117 | else if(strstr(temp_string.c_str(),"MAX_MU")){curstring >> varname >> value; MAX_MU = value;}
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118 | else if(strstr(temp_string.c_str(),"ELG_Scen")){curstring >> varname >> value; ELG_Scen = value;}
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119 | else if(strstr(temp_string.c_str(),"ELG_Ncen")){curstring >> varname >> value; ELG_Ncen = value;}
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120 | else if(strstr(temp_string.c_str(),"ELG_Ccen")){curstring >> varname >> value; ELG_Ccen = value;}
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121 | else if(strstr(temp_string.c_str(),"ELG_Sfwd")){curstring >> varname >> value; ELG_Sfwd = value;}
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122 | else if(strstr(temp_string.c_str(),"ELG_Cfwd")){curstring >> varname >> value; ELG_Cfwd = value;}
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123 | else if(strstr(temp_string.c_str(),"ELG_Nfwd")){curstring >> varname >> value; ELG_Nfwd = value;}
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124 | else if(strstr(temp_string.c_str(),"HAD_Secal")){curstring >> varname >> value; HAD_Secal = value;}
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125 | else if(strstr(temp_string.c_str(),"HAD_Necal")){curstring >> varname >> value; HAD_Necal = value;}
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126 | else if(strstr(temp_string.c_str(),"HAD_Cecal")){curstring >> varname >> value; HAD_Cecal = value;}
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127 | else if(strstr(temp_string.c_str(),"HAD_Shcal")){curstring >> varname >> value; HAD_Shcal = value;}
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128 | else if(strstr(temp_string.c_str(),"HAD_Nhcal")){curstring >> varname >> value; HAD_Nhcal = value;}
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129 | else if(strstr(temp_string.c_str(),"HAD_Chcal")){curstring >> varname >> value; HAD_Chcal = value;}
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130 | else if(strstr(temp_string.c_str(),"HAD_Shf")){curstring >> varname >> value; HAD_Shf = value;}
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131 | else if(strstr(temp_string.c_str(),"HAD_Nhf")){curstring >> varname >> value; HAD_Nhf = value;}
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132 | else if(strstr(temp_string.c_str(),"HAD_Chf")){curstring >> varname >> value; HAD_Chf = value;}
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133 | else if(strstr(temp_string.c_str(),"MU_SmearPt")){curstring >> varname >> value; MU_SmearPt = value;}
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134 | else if(strstr(temp_string.c_str(),"TAU_CONE_ENERGY")){curstring >> varname >> value; TAU_CONE_ENERGY = value;}
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135 | else if(strstr(temp_string.c_str(),"TAU_CONE_TRACKS")){curstring >> varname >> value; TAU_CONE_TRACKS = value;}
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136 | else if(strstr(temp_string.c_str(),"PT_TRACK_TAU")){curstring >> varname >> value; PT_TRACK_TAU = value;}
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137 | else if(strstr(temp_string.c_str(),"PT_TRACKS_MIN")){curstring >> varname >> value; PT_TRACKS_MIN = value;}
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138 | else if(strstr(temp_string.c_str(),"TAGGING_B")){curstring >> varname >> value; TAGGING_B = (int)value;}
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139 | else if(strstr(temp_string.c_str(),"MISTAGGING_C")){curstring >> varname >> value; MISTAGGING_C = (int)value;}
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140 | else if(strstr(temp_string.c_str(),"MISTAGGING_L")){curstring >> varname >> value; MISTAGGING_L = (int)value;}
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141 | else if(strstr(temp_string.c_str(),"CONERADIUS")){curstring >> varname >> value; CONERADIUS = value;}
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142 | else if(strstr(temp_string.c_str(),"JETALGO")){curstring >> varname >> value; JETALGO = (int)value;}
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143 | else if(strstr(temp_string.c_str(),"TRACKING_EFF")){curstring >> varname >> value; TRACKING_EFF = (int)value;}
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144 | }
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145 |
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146 | // Define Cone algorithm.
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147 | C_SEEDTHRESHOLD = 1.0;
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148 | C_ADJACENCYCUT = 2;
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149 | C_MAXITERATIONS = 100;
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150 | C_IRATCH = 1;
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151 | C_OVERLAPTHRESHOLD = 0.75;
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152 |
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153 | //Define MidPoint algorithm.
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154 | M_SEEDTHRESHOLD = 1.0;
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155 | M_CONEAREAFRACTION = 0.25;
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156 | M_MAXPAIRSIZE = 2;
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157 | M_MAXITERATIONS = 100;
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158 | M_OVERLAPTHRESHOLD = 0.75;
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159 |
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160 | }
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161 |
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162 |
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163 | // **********Provides the smeared TLorentzVector for the electrons********
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164 | // Smears the electron energy, and changes the 4-momentum accordingly
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165 | // different smearing if the electron is central (eta < 2.5) or forward
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166 | void RESOLution::SmearElectron(TLorentzVector &electron) {
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167 | // the 'electron' variable will be changed by the function
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168 | float energy = electron.E(); // before smearing
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169 | float energyS = 0.0; // after smearing // \sigma/E = C + N/E + S/\sqrt{E}
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170 |
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171 | if(fabs(electron.Eta()) < MAX_TRACKER) { // if the electron is inside the tracker
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172 | energyS = gRandom->Gaus(energy, sqrt(
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173 | pow(ELG_Ncen,2) +
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174 | pow(ELG_Ccen*energy,2) +
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175 | pow(ELG_Scen*sqrt(energy),2) ));
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176 | } else { // outside the tracker
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177 | energyS = gRandom->Gaus(energy, sqrt(
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178 | pow(ELG_Nfwd,2) +
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179 | pow(ELG_Cfwd*energy,2) +
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180 | pow(ELG_Sfwd*sqrt(energy),2) ) );
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181 | }
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182 | electron.SetPtEtaPhiE(energyS/cosh(electron.Eta()), electron.Eta(), electron.Phi(), energyS);
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183 |
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184 | if(electron.E() < 0)electron.SetPxPyPzE(0,0,0,0); // no negative values after smearing !
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185 | }
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186 |
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187 |
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188 | // **********Provides the smeared TLorentzVector for the muons********
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189 | // Smears the muon pT and changes the 4-momentum accordingly
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190 | void RESOLution::SmearMu(TLorentzVector &muon) {
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191 | // the 'muon' variable will be changed by the function
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192 | float pt = muon.Pt(); // before smearing
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193 | float ptS = gRandom->Gaus(pt, MU_SmearPt*pt ); // after smearing // \sigma/E = C + N/E + S/\sqrt{E}
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194 |
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195 | muon.SetPtEtaPhiE(ptS, muon.Eta(), muon.Phi(), ptS*cosh(muon.Eta()));
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196 |
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197 | if(muon.E() < 0)muon.SetPxPyPzE(0,0,0,0); // no negative values after smearing !
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198 | }
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199 |
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200 |
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201 | // **********Provides the smeared TLorentzVector for the hadrons********
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202 | // Smears the hadron 4-momentum
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203 | void RESOLution::SmearHadron(TLorentzVector &hadron, const float frac)
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204 | // the 'hadron' variable will be changed by the function
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205 | // the 'frac' variable describes the long-living particles. Should be 0.7 for K0S and Lambda, 1. otherwise
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206 | {
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207 | float energy = hadron.E(); // before smearing
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208 | float energyS = 0.0; // after smearing // \sigma/E = C + N/E + S/\sqrt{E}
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209 | float energy_ecal = (1.0 - frac)*energy; // electromagnetic calorimeter
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210 | float energy_hcal = frac*energy; // hadronic calorimeter
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211 | // frac takes into account the decay of long-living particles, that decay in the calorimeters
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212 | // some of the particles decay mostly in the ecal, some mostly in the hcal
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213 |
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214 | float energyS1,energyS2;
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215 | if(fabs(hadron.Eta()) < MAX_CALO_CEN) {
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216 | energyS1 = gRandom->Gaus(energy_hcal, sqrt(
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217 | pow(HAD_Nhcal,2) +
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218 | pow(HAD_Chcal*energy_hcal,2) +
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219 | pow(HAD_Shcal*sqrt(energy_hcal),2) )) ;
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220 |
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221 |
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222 | energyS2 = gRandom->Gaus(energy_ecal, sqrt(
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223 | pow(HAD_Necal,2) +
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224 | pow(HAD_Cecal*energy_ecal,2) +
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225 | pow(HAD_Secal*sqrt(energy_ecal),2) ) );
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226 |
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227 | energyS = ((energyS1>0)?energyS1:0) + ((energyS2>0)?energyS2:0);
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228 | } else {
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229 | energyS = gRandom->Gaus(energy, sqrt(
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230 | pow(HAD_Nhf,2) +
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231 | pow(HAD_Chf*energy,2) +
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232 | pow(HAD_Shf*sqrt(energy),2) ));
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233 | }
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234 |
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235 |
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236 | hadron.SetPtEtaPhiE(energyS/cosh(hadron.Eta()),hadron.Eta(), hadron.Phi(), energyS);
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237 |
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238 | if(hadron.E() < 0)hadron.SetPxPyPzE(0,0,0,0);
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239 | }
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240 |
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241 | // **********Provides the energy in the cone of radius TAU_CONE_ENERGY for the tau identification********
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242 | // to be taken into account, a calo tower should
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243 | // 1) have a transverse energy \f$ E_T = \sqrt{E_X^2 + E_Y^2} \f$ above a given threshold
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244 | // 2) be inside a cone with a radius R and the axis defined by (eta,phi)
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245 | double RESOLution::EnergySmallCone(const vector<PhysicsTower> &towers, const float eta, const float phi) {
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246 | double Energie=0;
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247 | for(unsigned int i=0; i < towers.size(); i++) {
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248 | if(towers[i].fourVector.pt() < M_SEEDTHRESHOLD) continue;
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249 | if((DeltaR(phi,eta,towers[i].fourVector.phi(),towers[i].fourVector.eta()) < TAU_CONE_ENERGY)) {
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250 | Energie += towers[i].fourVector.E;
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251 | }
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252 | }
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253 | return Energie;
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254 | }
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255 |
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256 |
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257 | // **********Provides the number of tracks in the cone of radius TAU_CONE_TRACKS for the tau identification********
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258 | // to be taken into account, a track should
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259 | // 1) avec a transverse momentum \$f p_T \$ above a given threshold
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260 | // 2) be inside a cone with a radius R and the axis defined by (eta,phi)
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261 | // IMPORTANT REMARK !!!!!
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262 | // previously, the argument 'phi' was before the argument 'eta'
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263 | // this has been changed for consistency with the other functions
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264 | // double check your running code that uses NumTracks !
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265 | unsigned int RESOLution::NumTracks(const vector<TLorentzVector> &tracks, const float pt_track, const float eta, const float phi) {
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266 | unsigned int numtrack=0;
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267 | for(unsigned int i=0; i < tracks.size(); i++) {
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268 | if((tracks[i].Pt() < pt_track )||
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269 | (DeltaR(phi,eta,tracks[i].Phi(),tracks[i].Eta()) > TAU_CONE_TRACKS)
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270 | )continue;
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271 | numtrack++;
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272 | }
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273 | return numtrack;
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274 | }
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275 |
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276 |
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277 | //*** Returns the PID of the particle with the highest energy, in a cone with a radius CONERADIUS and an axis (eta,phi) *********
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278 | //used by Btaggedjet
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279 | ///// Attention : bug removed => CONERADIUS/2 -> CONERADIUS !!
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280 | int RESOLution::Bjets(const TSimpleArray<TRootGenParticle> &subarray, const float eta, const float phi) {
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281 | float emax=0;
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282 | int Ppid=0;
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283 | if(subarray.GetEntries()>0) {
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284 | for(int i=0; i < subarray.GetEntries();i++) { // should have pt>PT_JETMIN and a small cone radius (r<CONE_JET)
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285 | float genDeltaR = DeltaR(subarray[i]->Phi,subarray[i]->Eta,phi,eta);
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286 | if(genDeltaR < CONERADIUS && subarray[i]->E > emax) {
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287 | emax=subarray[i]->E;
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288 | Ppid=abs(subarray[i]->PID);
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289 | }
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290 | }
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291 | }
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292 | return Ppid;
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293 | }
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294 |
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295 |
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296 | //******************** Simulates the b-tagging efficiency for real bjet, or the misendentification for other jets****************
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297 | bool RESOLution::Btaggedjet(const TLorentzVector &JET, const TSimpleArray<TRootGenParticle> &subarray) {
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298 | if( rand()%100 < (TAGGING_B+1) && Bjets(subarray,JET.Eta(),JET.Phi())==pB ) return true; // b-tag of b-jets is 40%
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299 | else if( rand()%100 < (MISTAGGING_C+1) && Bjets(subarray,JET.Eta(),JET.Phi())==pC ) return true; // b-tag of c-jets is 10%
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300 | else if( rand()%100 < (MISTAGGING_L+1) && Bjets(subarray,JET.Eta(),JET.Phi())!=0) return true; // b-tag of light jets is 1%
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301 | return false;
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302 | }
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303 |
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304 | //**************************** Returns the delta Phi ****************************
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305 | float DeltaPhi(const float phi1, const float phi2) {
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306 | float deltaphi=phi1-phi2; // in here, -PI < phi < PI
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307 | if(fabs(deltaphi) > PI) deltaphi=2.*PI-fabs(deltaphi);// put deltaphi between 0 and PI
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308 | else deltaphi=fabs(deltaphi);
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309 |
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310 | return deltaphi;
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311 | }
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312 |
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313 | //**************************** Returns the delta R****************************
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314 | float DeltaR(const float phi1, const float eta1, const float phi2, const float eta2) {
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315 | return sqrt(pow(DeltaPhi(phi1,phi2),2) + pow(eta1-eta2,2));
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316 | }
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317 |
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318 | int sign(const int myint) {
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319 | if (myint >0) return 1;
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320 | else if (myint <0) return -1;
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321 | else return 0;
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322 | }
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323 |
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324 | int sign(const float myfloat) {
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325 | if (myfloat >0) return 1;
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326 | else if (myfloat <0) return -1;
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327 | else return 0;
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328 | }
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329 |
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330 |
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331 | float Charge(const long int pid) {
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332 | // source: RPP chap 34 Monte Carlo Particle Numbering Scheme
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333 | /* switch (abs(pid)) {
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334 | case 1: case 3: case 5: case 7: return (float) sign(pid)*(-1/3); break; // d, s, b, b'
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335 | case 2: case 4: case 6: case 8: return (float) sign(pid)*2/3; break; // u, c, t, t'
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336 |
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337 | case 11: case 13: case 15: return (float) sign(pid)*(-1); break; // e, mu, tau
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338 | case 12: case 14: case 16: return (float) 0; break; // nu_e, nu_mu, nu_tau
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339 |
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340 | case 9: case 21: case 22: case 23: case 25:
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341 | case 32: case 33: case 35: case 36: return (float) 0; break; // neutral gauge/higgs bosons
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342 | case 24: case 34: case 37: return (float) sign(pid); break; // charged gauge/higgs bosons
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343 | }
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344 | */
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345 | return 0;
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346 | }
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