[2] | 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;
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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 | if(fabs(hadron.Eta()) < MAX_CALO_CEN) {
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| 215 | energyS = gRandom->Gaus(energy_hcal, sqrt(
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| 216 | pow(HAD_Nhcal,2) +
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| 217 | pow(HAD_Chcal*energy_hcal,2) +
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| 218 | pow(HAD_Shcal*sqrt(energy_hcal),2) ))
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| 219 | +
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| 220 | gRandom->Gaus(energy_ecal, sqrt(
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| 221 | pow(HAD_Necal,2) +
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| 222 | pow(HAD_Cecal*energy_ecal,2) +
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| 223 | pow(HAD_Secal*sqrt(energy_ecal),2) ) );
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| 224 | } else {
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| 225 | energyS = gRandom->Gaus(energy,
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| 226 | pow(HAD_Nhf,2) +
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| 227 | pow(HAD_Chf*energy,2) +
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| 228 | pow(HAD_Shf*sqrt(energy),2) );
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| 229 | }
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| 230 | hadron.SetPtEtaPhiE(energyS/cosh(hadron.Eta()),hadron.Eta(), hadron.Phi(), energyS);
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| 231 |
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| 232 | if(hadron.E() < 0)hadron.SetPxPyPzE(0,0,0,0);
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| 233 | }
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| 234 |
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| 235 | // **********Provides the energy in the cone of radius TAU_CONE_ENERGY for the tau identification********
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| 236 | // to be taken into account, a calo tower should
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| 237 | // 1) have a transverse energy \f$ E_T = \sqrt{E_X^2 + E_Y^2} \f$ above a given threshold
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| 238 | // 2) be inside a cone with a radius R and the axis defined by (eta,phi)
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| 239 | double RESOLution::EnergySmallCone(const vector<PhysicsTower> &towers, const float eta, const float phi) {
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| 240 | double Energie=0;
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| 241 | for(unsigned int i=0; i < towers.size(); i++) {
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| 242 | if(towers[i].fourVector.pt() < M_SEEDTHRESHOLD) continue;
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| 243 | if((DeltaR(phi,eta,towers[i].fourVector.phi(),towers[i].fourVector.eta()) < TAU_CONE_ENERGY)) {
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| 244 | Energie += towers[i].fourVector.E;
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| 245 | }
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| 246 | }
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| 247 | return Energie;
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| 248 | }
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| 249 |
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| 250 |
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| 251 | // **********Provides the number of tracks in the cone of radius TAU_CONE_TRACKS for the tau identification********
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| 252 | // to be taken into account, a track should
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| 253 | // 1) avec a transverse momentum \$f p_T \$ above a given threshold
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| 254 | // 2) be inside a cone with a radius R and the axis defined by (eta,phi)
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| 255 | // IMPORTANT REMARK !!!!!
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| 256 | // previously, the argument 'phi' was before the argument 'eta'
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| 257 | // this has been changed for consistency with the other functions
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| 258 | // double check your running code that uses NumTracks !
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| 259 | unsigned int RESOLution::NumTracks(const vector<TLorentzVector> &tracks, const float pt_track, const float eta, const float phi) {
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| 260 | unsigned int numtrack=0;
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| 261 | for(unsigned int i=0; i < tracks.size(); i++) {
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| 262 | if((tracks[i].Pt() < pt_track )||
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| 263 | (DeltaR(phi,eta,tracks[i].Phi(),tracks[i].Eta()) > TAU_CONE_TRACKS)
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| 264 | )continue;
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| 265 | numtrack++;
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| 266 | }
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| 267 | return numtrack;
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| 268 | }
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| 269 |
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| 270 |
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| 271 | //*** 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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| 272 | //used by Btaggedjet
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| 273 | ///// Attention : bug removed => CONERADIUS/2 -> CONERADIUS !!
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| 274 | int RESOLution::Bjets(const TSimpleArray<TRootGenParticle> &subarray, const float eta, const float phi) {
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| 275 | float emax=0;
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| 276 | int Ppid=0;
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| 277 | if(subarray.GetEntries()>0) {
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| 278 | 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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| 279 | float genDeltaR = DeltaR(subarray[i]->Phi,subarray[i]->Eta,phi,eta);
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| 280 | if(genDeltaR < CONERADIUS && subarray[i]->E > emax) {
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| 281 | emax=subarray[i]->E;
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| 282 | Ppid=abs(subarray[i]->PID);
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| 283 | }
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| 284 | }
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| 285 | }
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| 286 | return Ppid;
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| 287 | }
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| 288 |
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| 289 |
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| 290 | //******************** Simulates the b-tagging efficiency for real bjet, or the misendentification for other jets****************
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| 291 | bool RESOLution::Btaggedjet(const TLorentzVector &JET, const TSimpleArray<TRootGenParticle> &subarray) {
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| 292 | 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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| 293 | 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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| 294 | 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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| 295 | return false;
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| 296 | }
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| 297 |
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| 298 | //**************************** Returns the delta Phi ****************************
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| 299 | float DeltaPhi(const float phi1, const float phi2) {
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| 300 | float deltaphi=phi1-phi2; // in here, -PI < phi < PI
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| 301 | if(fabs(deltaphi) > PI) deltaphi=2.*PI-fabs(deltaphi);// put deltaphi between 0 and PI
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| 302 | else deltaphi=fabs(deltaphi);
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| 303 |
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| 304 | return deltaphi;
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| 305 | }
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| 306 |
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| 307 | //**************************** Returns the delta R****************************
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| 308 | float DeltaR(const float phi1, const float eta1, const float phi2, const float eta2) {
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| 309 | return sqrt(pow(DeltaPhi(phi1,phi2),2) + pow(eta1-eta2,2));
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| 310 | }
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| 311 |
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| 312 | int sign(const int myint) {
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| 313 | if (myint >0) return 1;
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| 314 | else if (myint <0) return -1;
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| 315 | else return 0;
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| 316 | }
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| 317 |
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| 318 | int sign(const float myfloat) {
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| 319 | if (myfloat >0) return 1;
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| 320 | else if (myfloat <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 |
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| 325 | float Charge(const long int pid) {
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| 326 | // source: RPP chap 34 Monte Carlo Particle Numbering Scheme
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| 327 | /* switch (abs(pid)) {
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| 328 | case 1: case 3: case 5: case 7: return (float) sign(pid)*(-1/3); break; // d, s, b, b'
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| 329 | case 2: case 4: case 6: case 8: return (float) sign(pid)*2/3; break; // u, c, t, t'
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| 330 |
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| 331 | case 11: case 13: case 15: return (float) sign(pid)*(-1); break; // e, mu, tau
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| 332 | case 12: case 14: case 16: return (float) 0; break; // nu_e, nu_mu, nu_tau
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| 333 |
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| 334 | case 9: case 21: case 22: case 23: case 25:
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| 335 | case 32: case 33: case 35: case 36: return (float) 0; break; // neutral gauge/higgs bosons
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| 336 | case 24: case 34: case 37: return (float) sign(pid); break; // charged gauge/higgs bosons
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| 337 | }
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| 338 | */
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| 339 | return 0;
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| 340 | }
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