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| 2 | *************************************************************
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| 3 | Geant4 version Name: global-V09-00-03 (9-May-2008)
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| 4 | Copyright : Geant4 Collaboration
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| 5 | Reference : NIM A 506 (2003), 250-303
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| 6 | WWW : http://cern.ch/geant4
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| 7 | *************************************************************
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| 8 |
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| 9 | PhotInPrimaryGeneratorAction::Constructor: part=gamma, E=100
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| 10 | Visualization Manager instantiating...
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| 11 | Visualization Manager initialising...
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| 12 | Registering graphics systems...
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| 13 |
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| 14 | You have successfully registered the following graphics systems.
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| 15 | Current available graphics systems are:
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| 16 | ASCIITree (ATree)
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| 17 | DAWNFILE (DAWNFILE)
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| 18 | G4HepRep (HepRepXML)
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| 19 | G4HepRepFile (HepRepFile)
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| 20 | RayTracer (RayTracer)
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| 21 | VRML1FILE (VRML1FILE)
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| 22 | VRML2FILE (VRML2FILE)
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| 23 | OpenGLImmediateX (OGLIX)
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| 24 | OpenGLStoredX (OGLSX)
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| 25 |
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| 26 | Registering model factories...
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| 27 |
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| 28 | You have successfully registered the following model factories.
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| 29 | Registered model factories:
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| 30 | generic
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| 31 | drawByCharge
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| 32 | drawByParticleID
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| 33 | drawByOriginVolume
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| 34 | drawByAttribute
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| 35 |
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| 36 | Registered filter factories:
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| 37 | chargeFilter
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| 38 | particleFilter
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| 39 | originVolumeFilter
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| 40 | attributeFilter
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| 41 |
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| 42 | PhotInPrimaryGeneratorAction::SetDetector: is called
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| 43 | /run/verbose 1
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| 44 | ##/tracking/verbose 6
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| 45 | /run/initialize
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| 46 | PhotInPhysicsList::ConstructProcess: is called
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| 47 | PhotInPhysList::ConstructProcess: Part=B+
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| 48 | PhotInPhysList::ConstructProcess: Part=B-
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| 49 | PhotInPhysList::ConstructProcess: Part=B0
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| 50 | PhotInPhysList::ConstructProcess: Part=Bs0
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| 51 | PhotInPhysList::ConstructProcess: Part=D+
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| 52 | PhotInPhysList::ConstructProcess: Part=D-
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| 53 | PhotInPhysList::ConstructProcess: Part=D0
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| 54 | PhotInPhysList::ConstructProcess: Part=Ds+
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| 55 | PhotInPhysList::ConstructProcess: Part=Ds-
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| 56 | PhotInPhysList::ConstructProcess: Part=GenericIon
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| 57 | PhotInPhysList::ConstructProcess: Part=He3
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| 58 | PhotInPhysList::ConstructProcess: Part=J/psi
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| 59 | PhotInPhysList::ConstructProcess: Part=N(1440)+
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| 60 | PhotInPhysList::ConstructProcess: Part=N(1440)0
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| 61 | PhotInPhysList::ConstructProcess: Part=N(1520)+
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| 62 | PhotInPhysList::ConstructProcess: Part=N(1520)0
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| 63 | PhotInPhysList::ConstructProcess: Part=N(1535)+
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| 64 | PhotInPhysList::ConstructProcess: Part=N(1535)0
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| 65 | PhotInPhysList::ConstructProcess: Part=N(1650)+
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| 66 | PhotInPhysList::ConstructProcess: Part=N(1650)0
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| 67 | PhotInPhysList::ConstructProcess: Part=N(1675)+
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| 68 | PhotInPhysList::ConstructProcess: Part=N(1675)0
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| 69 | PhotInPhysList::ConstructProcess: Part=N(1680)+
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| 70 | PhotInPhysList::ConstructProcess: Part=N(1680)0
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| 71 | PhotInPhysList::ConstructProcess: Part=N(1700)+
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| 72 | PhotInPhysList::ConstructProcess: Part=N(1700)0
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| 73 | PhotInPhysList::ConstructProcess: Part=N(1710)+
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| 74 | PhotInPhysList::ConstructProcess: Part=N(1710)0
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| 75 | PhotInPhysList::ConstructProcess: Part=N(1720)+
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| 76 | PhotInPhysList::ConstructProcess: Part=N(1720)0
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| 77 | PhotInPhysList::ConstructProcess: Part=N(1900)+
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| 78 | PhotInPhysList::ConstructProcess: Part=N(1900)0
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| 79 | PhotInPhysList::ConstructProcess: Part=N(1990)+
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| 80 | PhotInPhysList::ConstructProcess: Part=N(1990)0
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| 81 | PhotInPhysList::ConstructProcess: Part=N(2090)+
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| 82 | PhotInPhysList::ConstructProcess: Part=N(2090)0
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| 83 | PhotInPhysList::ConstructProcess: Part=N(2190)+
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| 84 | PhotInPhysList::ConstructProcess: Part=N(2190)0
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| 85 | PhotInPhysList::ConstructProcess: Part=N(2220)+
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| 86 | PhotInPhysList::ConstructProcess: Part=N(2220)0
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| 87 | PhotInPhysList::ConstructProcess: Part=N(2250)+
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| 88 | PhotInPhysList::ConstructProcess: Part=N(2250)0
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| 89 | PhotInPhysList::ConstructProcess: Part=a0(1450)+
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| 90 | PhotInPhysList::ConstructProcess: Part=a0(1450)-
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| 91 | PhotInPhysList::ConstructProcess: Part=a0(1450)0
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| 92 | PhotInPhysList::ConstructProcess: Part=a0(980)+
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| 93 | PhotInPhysList::ConstructProcess: Part=a0(980)-
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| 94 | PhotInPhysList::ConstructProcess: Part=a0(980)0
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| 95 | PhotInPhysList::ConstructProcess: Part=a1(1260)+
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| 96 | PhotInPhysList::ConstructProcess: Part=a1(1260)-
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| 97 | PhotInPhysList::ConstructProcess: Part=a1(1260)0
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| 98 | PhotInPhysList::ConstructProcess: Part=a2(1320)+
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| 99 | PhotInPhysList::ConstructProcess: Part=a2(1320)-
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| 100 | PhotInPhysList::ConstructProcess: Part=a2(1320)0
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| 101 | PhotInPhysList::ConstructProcess: Part=alpha
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| 102 | PhotInPhysList::ConstructProcess: Part=anti_B0
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| 103 | PhotInPhysList::ConstructProcess: Part=anti_Bs0
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| 104 | PhotInPhysList::ConstructProcess: Part=anti_D0
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| 105 | PhotInPhysList::ConstructProcess: Part=anti_N(1440)+
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| 106 | PhotInPhysList::ConstructProcess: Part=anti_N(1440)0
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| 107 | PhotInPhysList::ConstructProcess: Part=anti_N(1520)+
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| 108 | PhotInPhysList::ConstructProcess: Part=anti_N(1520)0
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| 109 | PhotInPhysList::ConstructProcess: Part=anti_N(1535)+
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| 110 | PhotInPhysList::ConstructProcess: Part=anti_N(1535)0
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| 111 | PhotInPhysList::ConstructProcess: Part=anti_N(1650)+
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| 112 | PhotInPhysList::ConstructProcess: Part=anti_N(1650)0
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| 113 | PhotInPhysList::ConstructProcess: Part=anti_N(1675)+
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| 114 | PhotInPhysList::ConstructProcess: Part=anti_N(1675)0
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| 115 | PhotInPhysList::ConstructProcess: Part=anti_N(1680)+
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| 116 | PhotInPhysList::ConstructProcess: Part=anti_N(1680)0
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| 117 | PhotInPhysList::ConstructProcess: Part=anti_N(1700)+
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| 118 | PhotInPhysList::ConstructProcess: Part=anti_N(1700)0
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| 119 | PhotInPhysList::ConstructProcess: Part=anti_N(1710)+
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| 120 | PhotInPhysList::ConstructProcess: Part=anti_N(1710)0
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| 121 | PhotInPhysList::ConstructProcess: Part=anti_N(1720)+
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| 122 | PhotInPhysList::ConstructProcess: Part=anti_N(1720)0
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| 123 | PhotInPhysList::ConstructProcess: Part=anti_N(1900)+
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| 124 | PhotInPhysList::ConstructProcess: Part=anti_N(1900)0
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| 125 | PhotInPhysList::ConstructProcess: Part=anti_N(1990)+
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| 126 | PhotInPhysList::ConstructProcess: Part=anti_N(1990)0
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| 127 | PhotInPhysList::ConstructProcess: Part=anti_N(2090)+
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| 128 | PhotInPhysList::ConstructProcess: Part=anti_N(2090)0
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| 129 | PhotInPhysList::ConstructProcess: Part=anti_N(2190)+
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| 130 | PhotInPhysList::ConstructProcess: Part=anti_N(2190)0
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| 131 | PhotInPhysList::ConstructProcess: Part=anti_N(2220)+
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| 132 | PhotInPhysList::ConstructProcess: Part=anti_N(2220)0
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| 133 | PhotInPhysList::ConstructProcess: Part=anti_N(2250)+
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| 134 | PhotInPhysList::ConstructProcess: Part=anti_N(2250)0
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| 135 | PhotInPhysList::ConstructProcess: Part=anti_b_quark
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| 136 | PhotInPhysList::ConstructProcess: Part=anti_c_quark
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| 137 | PhotInPhysList::ConstructProcess: Part=anti_d_quark
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| 138 | PhotInPhysList::ConstructProcess: Part=anti_dd1_diquark
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| 139 | PhotInPhysList::ConstructProcess: Part=anti_delta(1600)+
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| 140 | PhotInPhysList::ConstructProcess: Part=anti_delta(1600)++
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| 141 | PhotInPhysList::ConstructProcess: Part=anti_delta(1600)-
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| 142 | PhotInPhysList::ConstructProcess: Part=anti_delta(1600)0
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| 143 | PhotInPhysList::ConstructProcess: Part=anti_delta(1620)+
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| 144 | PhotInPhysList::ConstructProcess: Part=anti_delta(1620)++
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| 145 | PhotInPhysList::ConstructProcess: Part=anti_delta(1620)-
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| 146 | PhotInPhysList::ConstructProcess: Part=anti_delta(1620)0
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| 147 | PhotInPhysList::ConstructProcess: Part=anti_delta(1700)+
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| 148 | PhotInPhysList::ConstructProcess: Part=anti_delta(1700)++
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| 149 | PhotInPhysList::ConstructProcess: Part=anti_delta(1700)-
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| 150 | PhotInPhysList::ConstructProcess: Part=anti_delta(1700)0
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| 151 | PhotInPhysList::ConstructProcess: Part=anti_delta(1900)+
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| 152 | PhotInPhysList::ConstructProcess: Part=anti_delta(1900)++
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| 153 | PhotInPhysList::ConstructProcess: Part=anti_delta(1900)-
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| 154 | PhotInPhysList::ConstructProcess: Part=anti_delta(1900)0
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| 155 | PhotInPhysList::ConstructProcess: Part=anti_delta(1905)+
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| 156 | PhotInPhysList::ConstructProcess: Part=anti_delta(1905)++
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| 157 | PhotInPhysList::ConstructProcess: Part=anti_delta(1905)-
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| 158 | PhotInPhysList::ConstructProcess: Part=anti_delta(1905)0
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| 159 | PhotInPhysList::ConstructProcess: Part=anti_delta(1910)+
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| 160 | PhotInPhysList::ConstructProcess: Part=anti_delta(1910)++
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| 161 | PhotInPhysList::ConstructProcess: Part=anti_delta(1910)-
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| 162 | PhotInPhysList::ConstructProcess: Part=anti_delta(1910)0
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| 163 | PhotInPhysList::ConstructProcess: Part=anti_delta(1920)+
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| 164 | PhotInPhysList::ConstructProcess: Part=anti_delta(1920)++
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| 165 | PhotInPhysList::ConstructProcess: Part=anti_delta(1920)-
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| 166 | PhotInPhysList::ConstructProcess: Part=anti_delta(1920)0
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| 167 | PhotInPhysList::ConstructProcess: Part=anti_delta(1930)+
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| 168 | PhotInPhysList::ConstructProcess: Part=anti_delta(1930)++
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| 169 | PhotInPhysList::ConstructProcess: Part=anti_delta(1930)-
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| 170 | PhotInPhysList::ConstructProcess: Part=anti_delta(1930)0
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| 171 | PhotInPhysList::ConstructProcess: Part=anti_delta(1950)+
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| 172 | PhotInPhysList::ConstructProcess: Part=anti_delta(1950)++
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| 173 | PhotInPhysList::ConstructProcess: Part=anti_delta(1950)-
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| 174 | PhotInPhysList::ConstructProcess: Part=anti_delta(1950)0
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| 175 | PhotInPhysList::ConstructProcess: Part=anti_delta+
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| 176 | PhotInPhysList::ConstructProcess: Part=anti_delta++
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| 177 | PhotInPhysList::ConstructProcess: Part=anti_delta-
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| 178 | PhotInPhysList::ConstructProcess: Part=anti_delta0
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| 179 | PhotInPhysList::ConstructProcess: Part=anti_k(1460)0
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| 180 | PhotInPhysList::ConstructProcess: Part=anti_k0_star(1430)0
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| 181 | PhotInPhysList::ConstructProcess: Part=anti_k1(1270)0
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| 182 | PhotInPhysList::ConstructProcess: Part=anti_k1(1400)0
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| 183 | PhotInPhysList::ConstructProcess: Part=anti_k2(1770)0
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| 184 | PhotInPhysList::ConstructProcess: Part=anti_k2_star(1430)0
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| 185 | PhotInPhysList::ConstructProcess: Part=anti_k2_star(1980)0
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| 186 | PhotInPhysList::ConstructProcess: Part=anti_k3_star(1780)0
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| 187 | PhotInPhysList::ConstructProcess: Part=anti_k_star(1410)0
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| 188 | PhotInPhysList::ConstructProcess: Part=anti_k_star(1680)0
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| 189 | PhotInPhysList::ConstructProcess: Part=anti_k_star0
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| 190 | PhotInPhysList::ConstructProcess: Part=anti_kaon0
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| 191 | PhotInPhysList::ConstructProcess: Part=anti_lambda
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| 192 | PhotInPhysList::ConstructProcess: Part=anti_lambda(1405)
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| 193 | PhotInPhysList::ConstructProcess: Part=anti_lambda(1520)
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| 194 | PhotInPhysList::ConstructProcess: Part=anti_lambda(1600)
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| 195 | PhotInPhysList::ConstructProcess: Part=anti_lambda(1670)
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| 196 | PhotInPhysList::ConstructProcess: Part=anti_lambda(1690)
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| 197 | PhotInPhysList::ConstructProcess: Part=anti_lambda(1800)
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| 198 | PhotInPhysList::ConstructProcess: Part=anti_lambda(1810)
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| 199 | PhotInPhysList::ConstructProcess: Part=anti_lambda(1820)
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| 200 | PhotInPhysList::ConstructProcess: Part=anti_lambda(1830)
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| 201 | PhotInPhysList::ConstructProcess: Part=anti_lambda(1890)
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| 202 | PhotInPhysList::ConstructProcess: Part=anti_lambda(2100)
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| 203 | PhotInPhysList::ConstructProcess: Part=anti_lambda(2110)
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| 204 | PhotInPhysList::ConstructProcess: Part=anti_lambda_c+
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| 205 | PhotInPhysList::ConstructProcess: Part=anti_neutron
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| 206 | PhotInPhysList::ConstructProcess: Part=anti_nu_e
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| 207 | PhotInPhysList::ConstructProcess: Part=anti_nu_mu
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| 208 | PhotInPhysList::ConstructProcess: Part=anti_nu_tau
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| 209 | PhotInPhysList::ConstructProcess: Part=anti_omega-
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| 210 | PhotInPhysList::ConstructProcess: Part=anti_omega_c0
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| 211 | PhotInPhysList::ConstructProcess: Part=anti_proton
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| 212 | PhotInPhysList::ConstructProcess: Part=anti_s_quark
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| 213 | PhotInPhysList::ConstructProcess: Part=anti_sd0_diquark
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| 214 | PhotInPhysList::ConstructProcess: Part=anti_sd1_diquark
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| 215 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1385)+
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| 216 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1385)-
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| 217 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1385)0
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| 218 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1660)+
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| 219 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1660)-
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| 220 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1660)0
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| 221 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1670)+
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| 222 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1670)-
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| 223 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1670)0
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| 224 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1750)+
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| 225 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1750)-
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| 226 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1750)0
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| 227 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1775)+
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| 228 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1775)-
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| 229 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1775)0
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| 230 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1915)+
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| 231 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1915)-
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| 232 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1915)0
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| 233 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1940)+
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| 234 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1940)-
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| 235 | PhotInPhysList::ConstructProcess: Part=anti_sigma(1940)0
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| 236 | PhotInPhysList::ConstructProcess: Part=anti_sigma(2030)+
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| 237 | PhotInPhysList::ConstructProcess: Part=anti_sigma(2030)-
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| 238 | PhotInPhysList::ConstructProcess: Part=anti_sigma(2030)0
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| 239 | PhotInPhysList::ConstructProcess: Part=anti_sigma+
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| 240 | PhotInPhysList::ConstructProcess: Part=anti_sigma-
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| 241 | PhotInPhysList::ConstructProcess: Part=anti_sigma0
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| 242 | PhotInPhysList::ConstructProcess: Part=anti_sigma_c+
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| 243 | PhotInPhysList::ConstructProcess: Part=anti_sigma_c++
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| 244 | PhotInPhysList::ConstructProcess: Part=anti_sigma_c0
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| 245 | PhotInPhysList::ConstructProcess: Part=anti_ss1_diquark
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| 246 | PhotInPhysList::ConstructProcess: Part=anti_su0_diquark
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| 247 | PhotInPhysList::ConstructProcess: Part=anti_su1_diquark
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| 248 | PhotInPhysList::ConstructProcess: Part=anti_t_quark
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| 249 | PhotInPhysList::ConstructProcess: Part=anti_u_quark
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| 250 | PhotInPhysList::ConstructProcess: Part=anti_ud0_diquark
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| 251 | PhotInPhysList::ConstructProcess: Part=anti_ud1_diquark
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| 252 | PhotInPhysList::ConstructProcess: Part=anti_uu1_diquark
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| 253 | PhotInPhysList::ConstructProcess: Part=anti_xi(1530)-
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| 254 | PhotInPhysList::ConstructProcess: Part=anti_xi(1530)0
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| 255 | PhotInPhysList::ConstructProcess: Part=anti_xi(1690)-
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| 256 | PhotInPhysList::ConstructProcess: Part=anti_xi(1690)0
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| 257 | PhotInPhysList::ConstructProcess: Part=anti_xi(1820)-
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| 258 | PhotInPhysList::ConstructProcess: Part=anti_xi(1820)0
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| 259 | PhotInPhysList::ConstructProcess: Part=anti_xi(1950)-
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| 260 | PhotInPhysList::ConstructProcess: Part=anti_xi(1950)0
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| 261 | PhotInPhysList::ConstructProcess: Part=anti_xi(2030)-
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| 262 | PhotInPhysList::ConstructProcess: Part=anti_xi(2030)0
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| 263 | PhotInPhysList::ConstructProcess: Part=anti_xi-
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| 264 | PhotInPhysList::ConstructProcess: Part=anti_xi0
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| 265 | PhotInPhysList::ConstructProcess: Part=anti_xi_c+
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| 266 | PhotInPhysList::ConstructProcess: Part=anti_xi_c0
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| 267 | PhotInPhysList::ConstructProcess: Part=b1(1235)+
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| 268 | PhotInPhysList::ConstructProcess: Part=b1(1235)-
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| 269 | PhotInPhysList::ConstructProcess: Part=b1(1235)0
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| 270 | PhotInPhysList::ConstructProcess: Part=b_quark
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| 271 | PhotInPhysList::ConstructProcess: Part=c_quark
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| 272 | PhotInPhysList::ConstructProcess: Part=chargedgeantino
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| 273 | PhotInPhysList::ConstructProcess: Part=d_quark
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| 274 | PhotInPhysList::ConstructProcess: Part=dd1_diquark
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| 275 | PhotInPhysList::ConstructProcess: Part=delta(1600)+
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| 276 | PhotInPhysList::ConstructProcess: Part=delta(1600)++
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| 277 | PhotInPhysList::ConstructProcess: Part=delta(1600)-
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| 278 | PhotInPhysList::ConstructProcess: Part=delta(1600)0
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| 279 | PhotInPhysList::ConstructProcess: Part=delta(1620)+
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| 280 | PhotInPhysList::ConstructProcess: Part=delta(1620)++
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| 281 | PhotInPhysList::ConstructProcess: Part=delta(1620)-
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| 282 | PhotInPhysList::ConstructProcess: Part=delta(1620)0
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| 283 | PhotInPhysList::ConstructProcess: Part=delta(1700)+
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| 284 | PhotInPhysList::ConstructProcess: Part=delta(1700)++
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| 285 | PhotInPhysList::ConstructProcess: Part=delta(1700)-
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| 286 | PhotInPhysList::ConstructProcess: Part=delta(1700)0
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| 287 | PhotInPhysList::ConstructProcess: Part=delta(1900)+
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| 288 | PhotInPhysList::ConstructProcess: Part=delta(1900)++
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| 289 | PhotInPhysList::ConstructProcess: Part=delta(1900)-
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| 290 | PhotInPhysList::ConstructProcess: Part=delta(1900)0
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| 291 | PhotInPhysList::ConstructProcess: Part=delta(1905)+
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| 292 | PhotInPhysList::ConstructProcess: Part=delta(1905)++
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| 293 | PhotInPhysList::ConstructProcess: Part=delta(1905)-
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| 294 | PhotInPhysList::ConstructProcess: Part=delta(1905)0
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| 295 | PhotInPhysList::ConstructProcess: Part=delta(1910)+
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| 296 | PhotInPhysList::ConstructProcess: Part=delta(1910)++
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| 297 | PhotInPhysList::ConstructProcess: Part=delta(1910)-
|
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| 298 | PhotInPhysList::ConstructProcess: Part=delta(1910)0
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| 299 | PhotInPhysList::ConstructProcess: Part=delta(1920)+
|
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| 300 | PhotInPhysList::ConstructProcess: Part=delta(1920)++
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| 301 | PhotInPhysList::ConstructProcess: Part=delta(1920)-
|
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| 302 | PhotInPhysList::ConstructProcess: Part=delta(1920)0
|
|---|
| 303 | PhotInPhysList::ConstructProcess: Part=delta(1930)+
|
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| 304 | PhotInPhysList::ConstructProcess: Part=delta(1930)++
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| 305 | PhotInPhysList::ConstructProcess: Part=delta(1930)-
|
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| 306 | PhotInPhysList::ConstructProcess: Part=delta(1930)0
|
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| 307 | PhotInPhysList::ConstructProcess: Part=delta(1950)+
|
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| 308 | PhotInPhysList::ConstructProcess: Part=delta(1950)++
|
|---|
| 309 | PhotInPhysList::ConstructProcess: Part=delta(1950)-
|
|---|
| 310 | PhotInPhysList::ConstructProcess: Part=delta(1950)0
|
|---|
| 311 | PhotInPhysList::ConstructProcess: Part=delta+
|
|---|
| 312 | PhotInPhysList::ConstructProcess: Part=delta++
|
|---|
| 313 | PhotInPhysList::ConstructProcess: Part=delta-
|
|---|
| 314 | PhotInPhysList::ConstructProcess: Part=delta0
|
|---|
| 315 | PhotInPhysList::ConstructProcess: Part=deuteron
|
|---|
| 316 | PhotInPhysList::ConstructProcess: Part=e+
|
|---|
| 317 | PhotInPhysList::ConstructProcess: Part=e-
|
|---|
| 318 | PhotInPhysList::ConstructProcess: Part=eta
|
|---|
| 319 | PhotInPhysList::ConstructProcess: Part=eta(1295)
|
|---|
| 320 | PhotInPhysList::ConstructProcess: Part=eta(1405)
|
|---|
| 321 | PhotInPhysList::ConstructProcess: Part=eta(1475)
|
|---|
| 322 | PhotInPhysList::ConstructProcess: Part=eta2(1645)
|
|---|
| 323 | PhotInPhysList::ConstructProcess: Part=eta2(1870)
|
|---|
| 324 | PhotInPhysList::ConstructProcess: Part=eta_prime
|
|---|
| 325 | PhotInPhysList::ConstructProcess: Part=f0(1370)
|
|---|
| 326 | PhotInPhysList::ConstructProcess: Part=f0(1500)
|
|---|
| 327 | PhotInPhysList::ConstructProcess: Part=f0(1710)
|
|---|
| 328 | PhotInPhysList::ConstructProcess: Part=f0(600)
|
|---|
| 329 | PhotInPhysList::ConstructProcess: Part=f0(980)
|
|---|
| 330 | PhotInPhysList::ConstructProcess: Part=f1(1285)
|
|---|
| 331 | PhotInPhysList::ConstructProcess: Part=f1(1420)
|
|---|
| 332 | PhotInPhysList::ConstructProcess: Part=f2(1270)
|
|---|
| 333 | PhotInPhysList::ConstructProcess: Part=f2(1810)
|
|---|
| 334 | PhotInPhysList::ConstructProcess: Part=f2(2010)
|
|---|
| 335 | PhotInPhysList::ConstructProcess: Part=f2_prime(1525)
|
|---|
| 336 | PhotInPhysList::ConstructProcess: Part=gamma
|
|---|
| 337 | PhotInPhysList::ConstructProcess: Part=geantino
|
|---|
| 338 | PhotInPhysList::ConstructProcess: Part=gluon
|
|---|
| 339 | PhotInPhysList::ConstructProcess: Part=h1(1170)
|
|---|
| 340 | PhotInPhysList::ConstructProcess: Part=h1(1380)
|
|---|
| 341 | PhotInPhysList::ConstructProcess: Part=k(1460)+
|
|---|
| 342 | PhotInPhysList::ConstructProcess: Part=k(1460)-
|
|---|
| 343 | PhotInPhysList::ConstructProcess: Part=k(1460)0
|
|---|
| 344 | PhotInPhysList::ConstructProcess: Part=k0_star(1430)+
|
|---|
| 345 | PhotInPhysList::ConstructProcess: Part=k0_star(1430)-
|
|---|
| 346 | PhotInPhysList::ConstructProcess: Part=k0_star(1430)0
|
|---|
| 347 | PhotInPhysList::ConstructProcess: Part=k1(1270)+
|
|---|
| 348 | PhotInPhysList::ConstructProcess: Part=k1(1270)-
|
|---|
| 349 | PhotInPhysList::ConstructProcess: Part=k1(1270)0
|
|---|
| 350 | PhotInPhysList::ConstructProcess: Part=k1(1400)+
|
|---|
| 351 | PhotInPhysList::ConstructProcess: Part=k1(1400)-
|
|---|
| 352 | PhotInPhysList::ConstructProcess: Part=k1(1400)0
|
|---|
| 353 | PhotInPhysList::ConstructProcess: Part=k2(1770)+
|
|---|
| 354 | PhotInPhysList::ConstructProcess: Part=k2(1770)-
|
|---|
| 355 | PhotInPhysList::ConstructProcess: Part=k2(1770)0
|
|---|
| 356 | PhotInPhysList::ConstructProcess: Part=k2_star(1430)+
|
|---|
| 357 | PhotInPhysList::ConstructProcess: Part=k2_star(1430)-
|
|---|
| 358 | PhotInPhysList::ConstructProcess: Part=k2_star(1430)0
|
|---|
| 359 | PhotInPhysList::ConstructProcess: Part=k2_star(1980)+
|
|---|
| 360 | PhotInPhysList::ConstructProcess: Part=k2_star(1980)-
|
|---|
| 361 | PhotInPhysList::ConstructProcess: Part=k2_star(1980)0
|
|---|
| 362 | PhotInPhysList::ConstructProcess: Part=k3_star(1780)+
|
|---|
| 363 | PhotInPhysList::ConstructProcess: Part=k3_star(1780)-
|
|---|
| 364 | PhotInPhysList::ConstructProcess: Part=k3_star(1780)0
|
|---|
| 365 | PhotInPhysList::ConstructProcess: Part=k_star(1410)+
|
|---|
| 366 | PhotInPhysList::ConstructProcess: Part=k_star(1410)-
|
|---|
| 367 | PhotInPhysList::ConstructProcess: Part=k_star(1410)0
|
|---|
| 368 | PhotInPhysList::ConstructProcess: Part=k_star(1680)+
|
|---|
| 369 | PhotInPhysList::ConstructProcess: Part=k_star(1680)-
|
|---|
| 370 | PhotInPhysList::ConstructProcess: Part=k_star(1680)0
|
|---|
| 371 | PhotInPhysList::ConstructProcess: Part=k_star+
|
|---|
| 372 | PhotInPhysList::ConstructProcess: Part=k_star-
|
|---|
| 373 | PhotInPhysList::ConstructProcess: Part=k_star0
|
|---|
| 374 | PhotInPhysList::ConstructProcess: Part=kaon+
|
|---|
| 375 | PhotInPhysList::ConstructProcess: Part=kaon-
|
|---|
| 376 | PhotInPhysList::ConstructProcess: Part=kaon0
|
|---|
| 377 | PhotInPhysList::ConstructProcess: Part=kaon0L
|
|---|
| 378 | PhotInPhysList::ConstructProcess: Part=kaon0S
|
|---|
| 379 | PhotInPhysList::ConstructProcess: Part=lambda
|
|---|
| 380 | PhotInPhysList::ConstructProcess: Part=lambda(1405)
|
|---|
| 381 | PhotInPhysList::ConstructProcess: Part=lambda(1520)
|
|---|
| 382 | PhotInPhysList::ConstructProcess: Part=lambda(1600)
|
|---|
| 383 | PhotInPhysList::ConstructProcess: Part=lambda(1670)
|
|---|
| 384 | PhotInPhysList::ConstructProcess: Part=lambda(1690)
|
|---|
| 385 | PhotInPhysList::ConstructProcess: Part=lambda(1800)
|
|---|
| 386 | PhotInPhysList::ConstructProcess: Part=lambda(1810)
|
|---|
| 387 | PhotInPhysList::ConstructProcess: Part=lambda(1820)
|
|---|
| 388 | PhotInPhysList::ConstructProcess: Part=lambda(1830)
|
|---|
| 389 | PhotInPhysList::ConstructProcess: Part=lambda(1890)
|
|---|
| 390 | PhotInPhysList::ConstructProcess: Part=lambda(2100)
|
|---|
| 391 | PhotInPhysList::ConstructProcess: Part=lambda(2110)
|
|---|
| 392 | PhotInPhysList::ConstructProcess: Part=lambda_c+
|
|---|
| 393 | PhotInPhysList::ConstructProcess: Part=mu+
|
|---|
| 394 | PhotInPhysList::ConstructProcess: Part=mu-
|
|---|
| 395 | PhotInPhysList::ConstructProcess: Part=neutron
|
|---|
| 396 | PhotInPhysList::ConstructProcess: Part=nu_e
|
|---|
| 397 | PhotInPhysList::ConstructProcess: Part=nu_mu
|
|---|
| 398 | PhotInPhysList::ConstructProcess: Part=nu_tau
|
|---|
| 399 | PhotInPhysList::ConstructProcess: Part=omega
|
|---|
| 400 | PhotInPhysList::ConstructProcess: Part=omega(1420)
|
|---|
| 401 | PhotInPhysList::ConstructProcess: Part=omega(1650)
|
|---|
| 402 | PhotInPhysList::ConstructProcess: Part=omega-
|
|---|
| 403 | PhotInPhysList::ConstructProcess: Part=omega3(1670)
|
|---|
| 404 | PhotInPhysList::ConstructProcess: Part=omega_c0
|
|---|
| 405 | PhotInPhysList::ConstructProcess: Part=opticalphoton
|
|---|
| 406 | PhotInPhysList::ConstructProcess: Part=phi
|
|---|
| 407 | PhotInPhysList::ConstructProcess: Part=phi(1680)
|
|---|
| 408 | PhotInPhysList::ConstructProcess: Part=phi3(1850)
|
|---|
| 409 | PhotInPhysList::ConstructProcess: Part=pi(1300)+
|
|---|
| 410 | PhotInPhysList::ConstructProcess: Part=pi(1300)-
|
|---|
| 411 | PhotInPhysList::ConstructProcess: Part=pi(1300)0
|
|---|
| 412 | PhotInPhysList::ConstructProcess: Part=pi+
|
|---|
| 413 | PhotInPhysList::ConstructProcess: Part=pi-
|
|---|
| 414 | PhotInPhysList::ConstructProcess: Part=pi0
|
|---|
| 415 | PhotInPhysList::ConstructProcess: Part=pi2(1670)+
|
|---|
| 416 | PhotInPhysList::ConstructProcess: Part=pi2(1670)-
|
|---|
| 417 | PhotInPhysList::ConstructProcess: Part=pi2(1670)0
|
|---|
| 418 | PhotInPhysList::ConstructProcess: Part=proton
|
|---|
| 419 | PhotInPhysList::ConstructProcess: Part=rho(1450)+
|
|---|
| 420 | PhotInPhysList::ConstructProcess: Part=rho(1450)-
|
|---|
| 421 | PhotInPhysList::ConstructProcess: Part=rho(1450)0
|
|---|
| 422 | PhotInPhysList::ConstructProcess: Part=rho(1700)+
|
|---|
| 423 | PhotInPhysList::ConstructProcess: Part=rho(1700)-
|
|---|
| 424 | PhotInPhysList::ConstructProcess: Part=rho(1700)0
|
|---|
| 425 | PhotInPhysList::ConstructProcess: Part=rho+
|
|---|
| 426 | PhotInPhysList::ConstructProcess: Part=rho-
|
|---|
| 427 | PhotInPhysList::ConstructProcess: Part=rho0
|
|---|
| 428 | PhotInPhysList::ConstructProcess: Part=rho3(1690)+
|
|---|
| 429 | PhotInPhysList::ConstructProcess: Part=rho3(1690)-
|
|---|
| 430 | PhotInPhysList::ConstructProcess: Part=rho3(1690)0
|
|---|
| 431 | PhotInPhysList::ConstructProcess: Part=s_quark
|
|---|
| 432 | PhotInPhysList::ConstructProcess: Part=sd0_diquark
|
|---|
| 433 | PhotInPhysList::ConstructProcess: Part=sd1_diquark
|
|---|
| 434 | PhotInPhysList::ConstructProcess: Part=sigma(1385)+
|
|---|
| 435 | PhotInPhysList::ConstructProcess: Part=sigma(1385)-
|
|---|
| 436 | PhotInPhysList::ConstructProcess: Part=sigma(1385)0
|
|---|
| 437 | PhotInPhysList::ConstructProcess: Part=sigma(1660)+
|
|---|
| 438 | PhotInPhysList::ConstructProcess: Part=sigma(1660)-
|
|---|
| 439 | PhotInPhysList::ConstructProcess: Part=sigma(1660)0
|
|---|
| 440 | PhotInPhysList::ConstructProcess: Part=sigma(1670)+
|
|---|
| 441 | PhotInPhysList::ConstructProcess: Part=sigma(1670)-
|
|---|
| 442 | PhotInPhysList::ConstructProcess: Part=sigma(1670)0
|
|---|
| 443 | PhotInPhysList::ConstructProcess: Part=sigma(1750)+
|
|---|
| 444 | PhotInPhysList::ConstructProcess: Part=sigma(1750)-
|
|---|
| 445 | PhotInPhysList::ConstructProcess: Part=sigma(1750)0
|
|---|
| 446 | PhotInPhysList::ConstructProcess: Part=sigma(1775)+
|
|---|
| 447 | PhotInPhysList::ConstructProcess: Part=sigma(1775)-
|
|---|
| 448 | PhotInPhysList::ConstructProcess: Part=sigma(1775)0
|
|---|
| 449 | PhotInPhysList::ConstructProcess: Part=sigma(1915)+
|
|---|
| 450 | PhotInPhysList::ConstructProcess: Part=sigma(1915)-
|
|---|
| 451 | PhotInPhysList::ConstructProcess: Part=sigma(1915)0
|
|---|
| 452 | PhotInPhysList::ConstructProcess: Part=sigma(1940)+
|
|---|
| 453 | PhotInPhysList::ConstructProcess: Part=sigma(1940)-
|
|---|
| 454 | PhotInPhysList::ConstructProcess: Part=sigma(1940)0
|
|---|
| 455 | PhotInPhysList::ConstructProcess: Part=sigma(2030)+
|
|---|
| 456 | PhotInPhysList::ConstructProcess: Part=sigma(2030)-
|
|---|
| 457 | PhotInPhysList::ConstructProcess: Part=sigma(2030)0
|
|---|
| 458 | PhotInPhysList::ConstructProcess: Part=sigma+
|
|---|
| 459 | PhotInPhysList::ConstructProcess: Part=sigma-
|
|---|
| 460 | PhotInPhysList::ConstructProcess: Part=sigma0
|
|---|
| 461 | PhotInPhysList::ConstructProcess: Part=sigma_c+
|
|---|
| 462 | PhotInPhysList::ConstructProcess: Part=sigma_c++
|
|---|
| 463 | PhotInPhysList::ConstructProcess: Part=sigma_c0
|
|---|
| 464 | PhotInPhysList::ConstructProcess: Part=ss1_diquark
|
|---|
| 465 | PhotInPhysList::ConstructProcess: Part=su0_diquark
|
|---|
| 466 | PhotInPhysList::ConstructProcess: Part=su1_diquark
|
|---|
| 467 | PhotInPhysList::ConstructProcess: Part=t_quark
|
|---|
| 468 | PhotInPhysList::ConstructProcess: Part=tau+
|
|---|
| 469 | PhotInPhysList::ConstructProcess: Part=tau-
|
|---|
| 470 | PhotInPhysList::ConstructProcess: Part=triton
|
|---|
| 471 | PhotInPhysList::ConstructProcess: Part=u_quark
|
|---|
| 472 | PhotInPhysList::ConstructProcess: Part=ud0_diquark
|
|---|
| 473 | PhotInPhysList::ConstructProcess: Part=ud1_diquark
|
|---|
| 474 | PhotInPhysList::ConstructProcess: Part=uu1_diquark
|
|---|
| 475 | PhotInPhysList::ConstructProcess: Part=xi(1530)-
|
|---|
| 476 | PhotInPhysList::ConstructProcess: Part=xi(1530)0
|
|---|
| 477 | PhotInPhysList::ConstructProcess: Part=xi(1690)-
|
|---|
| 478 | PhotInPhysList::ConstructProcess: Part=xi(1690)0
|
|---|
| 479 | PhotInPhysList::ConstructProcess: Part=xi(1820)-
|
|---|
| 480 | PhotInPhysList::ConstructProcess: Part=xi(1820)0
|
|---|
| 481 | PhotInPhysList::ConstructProcess: Part=xi(1950)-
|
|---|
| 482 | PhotInPhysList::ConstructProcess: Part=xi(1950)0
|
|---|
| 483 | PhotInPhysList::ConstructProcess: Part=xi(2030)-
|
|---|
| 484 | PhotInPhysList::ConstructProcess: Part=xi(2030)0
|
|---|
| 485 | PhotInPhysList::ConstructProcess: Part=xi-
|
|---|
| 486 | PhotInPhysList::ConstructProcess: Part=xi0
|
|---|
| 487 | PhotInPhysList::ConstructProcess: Part=xi_c+
|
|---|
| 488 | PhotInPhysList::ConstructProcess: Part=xi_c0
|
|---|
| 489 | PhotInPhysicsList::SetCuts: default cut length : 1 mm
|
|---|
| 490 | /run/dumpRegion
|
|---|
| 491 |
|
|---|
| 492 | Region <DefaultRegionForTheWorld> -- appears in <World> world volume
|
|---|
| 493 | Root logical volume(s) : World
|
|---|
| 494 | Pointers : G4VUserRegionInformation[0], G4UserLimits[0], G4FastSimulationManager[0], G4UserSteppingAction[0]
|
|---|
| 495 | Materials : Vac
|
|---|
| 496 | Production cuts : gamma 1 mm e- 1 mm e+ 1 mm
|
|---|
| 497 |
|
|---|
| 498 | Region <Region0> -- appears in <World> world volume
|
|---|
| 499 | Root logical volume(s) : Sect-0
|
|---|
| 500 | Pointers : G4VUserRegionInformation[0], G4UserLimits[0], G4FastSimulationManager[0], G4UserSteppingAction[0]
|
|---|
| 501 | Materials : Aluminium Scintillator
|
|---|
| 502 | Production cuts : gamma 1 mm e- 1 mm e+ 1 mm
|
|---|
| 503 |
|
|---|
| 504 | Region <Region1> -- appears in <World> world volume
|
|---|
| 505 | Root logical volume(s) : Sect-1
|
|---|
| 506 | Pointers : G4VUserRegionInformation[0], G4UserLimits[0], G4FastSimulationManager[0], G4UserSteppingAction[0]
|
|---|
| 507 | Materials : Aluminium Scintillator
|
|---|
| 508 | Production cuts : gamma 1 cm e- 1 cm e+ 1 cm
|
|---|
| 509 |
|
|---|
| 510 | Region <Region2> -- appears in <World> world volume
|
|---|
| 511 | Root logical volume(s) : Sect-2
|
|---|
| 512 | Pointers : G4VUserRegionInformation[0], G4UserLimits[0], G4FastSimulationManager[0], G4UserSteppingAction[0]
|
|---|
| 513 | Materials : Aluminium Scintillator
|
|---|
| 514 | Production cuts : gamma 10 cm e- 10 cm e+ 10 cm
|
|---|
| 515 | /PhotIn/projParticle pi+
|
|---|
| 516 | PhotInPrimaryGeneratorAction::SetProjectileName:Before Name=pi+, oldName=gamma
|
|---|
| 517 | PhotInPrimaryGeneratorAction::SetProjectileName: After Name=pi+
|
|---|
| 518 | /PhotIn/projEnergy 100.
|
|---|
| 519 | PhotInPrimaryGeneratorAction::SetProjectileEnergy: before E=100
|
|---|
| 520 | PhotInPrimaryGeneratorAction::SetProjectileEnergy: before E=100
|
|---|
| 521 | /run/beamOn 1
|
|---|
| 522 |
|
|---|
| 523 | conv: Total cross sections has a good parametrisation from 1.5 MeV to 100 GeV for all Z;
|
|---|
| 524 | sampling secondary e+e- according Bethe-Heitler model
|
|---|
| 525 | tables are built for gamma
|
|---|
| 526 | Lambda tables from 1.022 MeV to 100 GeV in 100 bins.
|
|---|
| 527 |
|
|---|
| 528 | compt: Total cross sections has a good parametrisation from 10 KeV to (100/Z) GeV
|
|---|
| 529 | Sampling according Klein-Nishina model
|
|---|
| 530 | tables are built for gamma
|
|---|
| 531 | Lambda tables from 100 eV to 100 GeV in 90 bins.
|
|---|
| 532 |
|
|---|
| 533 | phot: Total cross sections from Sandia parametrisation.
|
|---|
| 534 | Sampling according PhotoElectric model
|
|---|
| 535 |
|
|---|
| 536 | msc: Model variant of multiple scattering for e-
|
|---|
| 537 | Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 538 | LateralDisplacementFlag= 1 Skin= 0
|
|---|
| 539 | Boundary/stepping algorithm is active with RangeFactor= 0.02 Step limit type 1
|
|---|
| 540 |
|
|---|
| 541 | eIoni: tables are built for e-
|
|---|
| 542 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 543 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 544 | Delta cross sections and sampling from MollerBhabha model
|
|---|
| 545 | Good description from 1 KeV to 100 GeV.
|
|---|
| 546 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1
|
|---|
| 547 |
|
|---|
| 548 | eBrem: tables are built for e-
|
|---|
| 549 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 550 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 551 | Total cross sections and sampling from StandBrem model (based on the EEDL data library)
|
|---|
| 552 | Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV. LPM flag 1
|
|---|
| 553 |
|
|---|
| 554 | eIoni: tables are built for e+
|
|---|
| 555 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 556 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 557 | Delta cross sections and sampling from MollerBhabha model
|
|---|
| 558 | Good description from 1 KeV to 100 GeV.
|
|---|
| 559 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1
|
|---|
| 560 |
|
|---|
| 561 | eBrem: tables are built for e+
|
|---|
| 562 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 563 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 564 | Total cross sections and sampling from StandBrem model (based on the EEDL data library)
|
|---|
| 565 | Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV. LPM flag 1
|
|---|
| 566 |
|
|---|
| 567 | annihil: Sampling according eplus2gg model
|
|---|
| 568 | tables are built for e+
|
|---|
| 569 | Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 570 |
|
|---|
| 571 | annihil: Sampling according eplus2gg model
|
|---|
| 572 | tables are built for e+
|
|---|
| 573 | Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 574 |
|
|---|
| 575 | msc: Model variant of multiple scattering for proton
|
|---|
| 576 | Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 577 | LateralDisplacementFlag= 1 Skin= 0
|
|---|
| 578 | Boundary/stepping algorithm is active with RangeFactor= 0.02 Step limit type 1
|
|---|
| 579 |
|
|---|
| 580 | hIoni: tables are built for proton
|
|---|
| 581 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 582 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 583 | Scaling relation is used from proton dE/dx and range.
|
|---|
| 584 | Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV
|
|---|
| 585 | Parametrisation from Bragg for protons below. NuclearStopping= 1
|
|---|
| 586 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1
|
|---|
| 587 |
|
|---|
| 588 | msc: Model variant of multiple scattering for GenericIon
|
|---|
| 589 | LateralDisplacementFlag= 0 Skin= 0
|
|---|
| 590 | Boundary/stepping algorithm is active with RangeFactor= 0.2 Step limit type 1
|
|---|
| 591 |
|
|---|
| 592 | hIoni: tables are built for anti_proton
|
|---|
| 593 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 594 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 595 | Scaling relation is used from proton dE/dx and range.
|
|---|
| 596 | Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV
|
|---|
| 597 | Parametrisation from Bragg for protons below. NuclearStopping= 1
|
|---|
| 598 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1
|
|---|
| 599 |
|
|---|
| 600 | msc: Model variant of multiple scattering for mu+
|
|---|
| 601 | Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 602 | LateralDisplacementFlag= 1 Skin= 0
|
|---|
| 603 | Boundary/stepping algorithm is active with RangeFactor= 0.02 Step limit type 1
|
|---|
| 604 |
|
|---|
| 605 | muIoni: tables are built for mu+
|
|---|
| 606 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 607 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 608 | Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below,
|
|---|
| 609 | radiative corrections for E > 1 GeV
|
|---|
| 610 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1
|
|---|
| 611 |
|
|---|
| 612 | muBrems: tables are built for mu+
|
|---|
| 613 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 614 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 615 | Parametrised model
|
|---|
| 616 |
|
|---|
| 617 | muPairProd: tables are built for mu+
|
|---|
| 618 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 619 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 620 | Parametrised model
|
|---|
| 621 |
|
|---|
| 622 | muIoni: tables are built for mu-
|
|---|
| 623 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 624 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 625 | Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below,
|
|---|
| 626 | radiative corrections for E > 1 GeV
|
|---|
| 627 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1
|
|---|
| 628 |
|
|---|
| 629 | muBrems: tables are built for mu-
|
|---|
| 630 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 631 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 632 | Parametrised model
|
|---|
| 633 |
|
|---|
| 634 | muPairProd: tables are built for mu-
|
|---|
| 635 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 636 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 637 | Parametrised model
|
|---|
| 638 |
|
|---|
| 639 | hIoni: tables are built for pi+
|
|---|
| 640 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 641 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 642 | Scaling relation is used from proton dE/dx and range.
|
|---|
| 643 | Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV
|
|---|
| 644 | Parametrisation from Bragg for protons below. NuclearStopping= 1
|
|---|
| 645 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1
|
|---|
| 646 |
|
|---|
| 647 | msc: Model variant of multiple scattering for pi-
|
|---|
| 648 | Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 649 | LateralDisplacementFlag= 1 Skin= 0
|
|---|
| 650 | Boundary/stepping algorithm is active with RangeFactor= 0.02 Step limit type 1
|
|---|
| 651 |
|
|---|
| 652 | hIoni: tables are built for pi-
|
|---|
| 653 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|---|
| 654 | Lambda tables from threshold to 100 TeV in 120 bins.
|
|---|
| 655 | Scaling relation is used from proton dE/dx and range.
|
|---|
| 656 | Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV
|
|---|
| 657 | Parametrisation from Bragg for protons below. NuclearStopping= 1
|
|---|
| 658 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1
|
|---|
| 659 |
|
|---|
| 660 | ========= Table of registered couples ==============================
|
|---|
| 661 |
|
|---|
| 662 | Index : 0 used in the geometry : Yes recalculation needed : No
|
|---|
| 663 | Material : Vac
|
|---|
| 664 | Range cuts : gamma 1 mm e- 1 mm e+ 1 mm
|
|---|
| 665 | Energy thresholds : gamma 990 eV e- 990 eV e+ 990 eV
|
|---|
| 666 | Region(s) which use this couple :
|
|---|
| 667 | DefaultRegionForTheWorld
|
|---|
| 668 |
|
|---|
| 669 | Index : 1 used in the geometry : Yes recalculation needed : No
|
|---|
| 670 | Material : Aluminium
|
|---|
| 671 | Range cuts : gamma 1 mm e- 1 mm e+ 1 mm
|
|---|
| 672 | Energy thresholds : gamma 6.88731 keV e- 596.68 keV e+ 568.011 keV
|
|---|
| 673 | Region(s) which use this couple :
|
|---|
| 674 | Region0
|
|---|
| 675 |
|
|---|
| 676 | Index : 2 used in the geometry : Yes recalculation needed : No
|
|---|
| 677 | Material : Scintillator
|
|---|
| 678 | Range cuts : gamma 1 mm e- 1 mm e+ 1 mm
|
|---|
| 679 | Energy thresholds : gamma 2.36895 keV e- 355.791 keV e+ 347.138 keV
|
|---|
| 680 | Region(s) which use this couple :
|
|---|
| 681 | Region0
|
|---|
| 682 |
|
|---|
| 683 | Index : 3 used in the geometry : Yes recalculation needed : No
|
|---|
| 684 | Material : Aluminium
|
|---|
| 685 | Range cuts : gamma 1 cm e- 1 cm e+ 1 cm
|
|---|
| 686 | Energy thresholds : gamma 20.4949 keV e- 4.54874 MeV e+ 4.2772 MeV
|
|---|
| 687 | Region(s) which use this couple :
|
|---|
| 688 | Region1
|
|---|
| 689 |
|
|---|
| 690 | Index : 4 used in the geometry : Yes recalculation needed : No
|
|---|
| 691 | Material : Scintillator
|
|---|
| 692 | Range cuts : gamma 1 cm e- 1 cm e+ 1 cm
|
|---|
| 693 | Energy thresholds : gamma 5.69883 keV e- 2.20017 MeV e+ 2.06883 MeV
|
|---|
| 694 | Region(s) which use this couple :
|
|---|
| 695 | Region1
|
|---|
| 696 |
|
|---|
| 697 | Index : 5 used in the geometry : Yes recalculation needed : No
|
|---|
| 698 | Material : Aluminium
|
|---|
| 699 | Range cuts : gamma 10 cm e- 10 cm e+ 10 cm
|
|---|
| 700 | Energy thresholds : gamma 79.141 keV e- 56.7407 MeV e+ 54.0144 MeV
|
|---|
| 701 | Region(s) which use this couple :
|
|---|
| 702 | Region2
|
|---|
| 703 |
|
|---|
| 704 | Index : 6 used in the geometry : Yes recalculation needed : No
|
|---|
| 705 | Material : Scintillator
|
|---|
| 706 | Range cuts : gamma 10 cm e- 10 cm e+ 10 cm
|
|---|
| 707 | Energy thresholds : gamma 18.8645 keV e- 23.386 MeV e+ 22.2624 MeV
|
|---|
| 708 | Region(s) which use this couple :
|
|---|
| 709 | Region2
|
|---|
| 710 |
|
|---|
| 711 | ====================================================================
|
|---|
| 712 |
|
|---|
| 713 | Start Run processing.
|
|---|
| 714 | PhotInPrimaryGeneratorAction::GeneratePrimaries: pi+,E=100
|
|---|
| 715 | PhotInPrimaryGeneratorAction::GeneratePrimaries: part&E're redefined
|
|---|
