1 | // |
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2 | // ******************************************************************** |
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3 | // * License and Disclaimer * |
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4 | // * * |
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5 | // * The Geant4 software is copyright of the Copyright Holders of * |
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6 | // * the Geant4 Collaboration. It is provided under the terms and * |
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7 | // * conditions of the Geant4 Software License, included in the file * |
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8 | // * LICENSE and available at http://cern.ch/geant4/license . These * |
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9 | // * include a list of copyright holders. * |
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10 | // * * |
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11 | // * Neither the authors of this software system, nor their employing * |
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12 | // * institutes,nor the agencies providing financial support for this * |
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13 | // * work make any representation or warranty, express or implied, * |
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14 | // * regarding this software system or assume any liability for its * |
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15 | // * use. Please see the license in the file LICENSE and URL above * |
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16 | // * for the full disclaimer and the limitation of liability. * |
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17 | // * * |
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18 | // * This code implementation is the result of the scientific and * |
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19 | // * technical work of the GEANT4 collaboration. * |
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20 | // * By using, copying, modifying or distributing the software (or * |
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21 | // * any work based on the software) you agree to acknowledge its * |
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22 | // * use in resulting scientific publications, and indicate your * |
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23 | // * acceptance of all terms of the Geant4 Software license. * |
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24 | // ******************************************************************** |
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25 | // |
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26 | |
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27 | #include "G4CascadeInterface.hh" |
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28 | #include "globals.hh" |
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29 | #include "G4DynamicParticleVector.hh" |
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30 | #include "G4IonTable.hh" |
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31 | #include "G4InuclCollider.hh" |
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32 | // #include "G4IntraNucleiCascader.hh" |
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33 | #include "G4InuclElementaryParticle.hh" |
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34 | #include "G4InuclNuclei.hh" |
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35 | #include "G4InuclParticle.hh" |
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36 | #include "G4CollisionOutput.hh" |
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37 | #include "G4V3DNucleus.hh" |
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38 | #include "G4Track.hh" |
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39 | #include "G4Nucleus.hh" |
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40 | #include "G4NucleiModel.hh" |
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41 | #include "G4LorentzRotation.hh" |
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42 | |
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43 | |
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44 | //#define BERTDEV 1 // A flag to activate a development version of Bertini cascade |
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45 | |
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46 | typedef std::vector<G4InuclElementaryParticle>::iterator particleIterator; |
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47 | typedef std::vector<G4InuclNuclei>::iterator nucleiIterator; |
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48 | |
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49 | G4CascadeInterface::G4CascadeInterface(const G4String& nam) |
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50 | :G4VIntraNuclearTransportModel(nam), verboseLevel(0) |
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51 | { |
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52 | if (verboseLevel > 3) { |
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53 | G4cout << " >>> G4CascadeInterface::G4CascadeInterface" << G4endl; |
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54 | } |
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55 | |
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56 | } |
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57 | |
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58 | |
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59 | G4CascadeInterface::~G4CascadeInterface() |
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60 | {} |
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61 | |
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62 | G4ReactionProductVector* G4CascadeInterface::Propagate(G4KineticTrackVector* , |
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63 | G4V3DNucleus* ) { |
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64 | return 0; |
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65 | } |
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66 | |
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67 | // #define debug_G4CascadeInterface |
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68 | |
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69 | G4HadFinalState* G4CascadeInterface::ApplyYourself(const G4HadProjectile& aTrack, |
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70 | G4Nucleus& theNucleus) { |
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71 | #ifdef debug_G4CascadeInterface |
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72 | static G4int counter(0); |
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73 | counter++; |
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74 | G4cerr << "Reaction number "<< counter << " "<<aTrack.GetDynamicParticle()->GetDefinition()->GetParticleName()<<" "<< aTrack.GetDynamicParticle()->GetKineticEnergy()<<G4endl; |
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75 | #endif |
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76 | |
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77 | theResult.Clear(); |
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78 | |
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79 | if (verboseLevel > 3) { |
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80 | G4cout << " >>> G4CascadeInterface::ApplyYourself" << G4endl; |
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81 | }; |
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82 | |
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83 | G4double eInit = 0.0; |
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84 | G4double eTot = 0.0; |
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85 | G4double sumBaryon = 0.0; |
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86 | G4double sumEnergy = 0.0; |
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87 | |
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88 | // Make conversion between native Geant4 and Bertini cascade classes. |
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89 | // NOTE: Geant4 units are MeV = 1 and GeV = 1000. Cascade code by default use GeV = 1. |
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90 | |
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91 | enum particleType { nuclei = 0, proton = 1, neutron = 2, pionPlus = 3, |
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92 | pionMinus = 5, pionZero = 7, photon = 10, |
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93 | kaonPlus = 11, kaonMinus = 13, kaonZero = 15, |
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94 | kaonZeroBar = 17, lambda = 21, sigmaPlus = 23, |
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95 | sigmaZero = 25, sigmaMinus = 27, xiZero = 29, xiMinus = 31 }; |
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96 | |
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97 | G4int bulletType = 0; |
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98 | |
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99 | // Coding particles |
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100 | if (aTrack.GetDefinition() == G4Proton::Proton() ) bulletType = proton; |
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101 | if (aTrack.GetDefinition() == G4Neutron::Neutron() ) bulletType = neutron; |
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102 | if (aTrack.GetDefinition() == G4PionPlus::PionPlus() ) bulletType = pionPlus; |
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103 | if (aTrack.GetDefinition() == G4PionMinus::PionMinus() ) bulletType = pionMinus; |
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104 | if (aTrack.GetDefinition() == G4PionZero::PionZero() ) bulletType = pionZero; |
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105 | if (aTrack.GetDefinition() == G4Gamma::Gamma() ) bulletType = photon; |
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106 | if (aTrack.GetDefinition() == G4KaonPlus::KaonPlus() ) bulletType = kaonPlus; |
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107 | if (aTrack.GetDefinition() == G4KaonMinus::KaonMinus() ) bulletType = kaonMinus; |
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108 | if (aTrack.GetDefinition() == G4Lambda::Lambda() ) bulletType = lambda; |
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109 | if (aTrack.GetDefinition() == G4SigmaPlus::SigmaPlus() ) bulletType = sigmaPlus; |
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110 | if (aTrack.GetDefinition() == G4SigmaZero::SigmaZero() ) bulletType = sigmaZero; |
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111 | if (aTrack.GetDefinition() == G4SigmaMinus::SigmaMinus() ) bulletType = sigmaMinus; |
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112 | if (aTrack.GetDefinition() == G4XiZero::XiZero() ) bulletType = xiZero; |
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113 | if (aTrack.GetDefinition() == G4XiMinus::XiMinus() ) bulletType = xiMinus; |
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114 | |
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115 | if (aTrack.GetDefinition() == G4KaonZeroLong::KaonZeroLong() || |
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116 | aTrack.GetDefinition() == G4KaonZeroShort::KaonZeroShort() ) { |
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117 | if (G4UniformRand() > 0.5) { |
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118 | bulletType = kaonZero; |
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119 | } else { |
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120 | bulletType = kaonZeroBar; |
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121 | } |
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122 | } |
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123 | |
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124 | // Code momentum and energy. |
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125 | G4double px,py,pz; |
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126 | px=aTrack.Get4Momentum().px() / GeV; |
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127 | py=aTrack.Get4Momentum().py() / GeV; |
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128 | pz=aTrack.Get4Momentum().pz() / GeV; |
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129 | |
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130 | G4LorentzVector projectileMomentum = aTrack.Get4Momentum(); |
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131 | G4LorentzRotation toZ; |
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132 | toZ.rotateZ(-projectileMomentum.phi()); |
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133 | toZ.rotateY(-projectileMomentum.theta()); |
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134 | G4LorentzRotation toLabFrame = toZ.inverse(); |
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135 | |
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136 | G4CascadeMomentum momentumBullet; |
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137 | momentumBullet[0] =0.; |
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138 | momentumBullet[1] =0; |
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139 | momentumBullet[2] =0; |
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140 | momentumBullet[3] =std::sqrt(px*px+py*py+pz*pz); |
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141 | |
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142 | G4InuclElementaryParticle * bullet = new G4InuclElementaryParticle(momentumBullet, bulletType); |
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143 | |
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144 | sumEnergy = bullet->getKineticEnergy(); // In GeV |
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145 | |
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146 | if (bulletType == proton || bulletType == neutron || bulletType == lambda || |
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147 | bulletType == sigmaPlus || bulletType == sigmaZero || bulletType == sigmaMinus || |
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148 | bulletType == xiZero || bulletType == xiMinus) { |
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149 | |
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150 | sumBaryon += 1; |
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151 | } |
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152 | |
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153 | // Set target |
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154 | G4InuclNuclei* target = 0; |
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155 | G4InuclParticle* targetH = 0; |
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156 | // and outcoming particles |
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157 | G4DynamicParticle* cascadeParticle = 0; |
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158 | |
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159 | G4CascadeMomentum targetMomentum; |
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160 | |
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161 | G4double theNucleusA = theNucleus.GetN(); |
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162 | |
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163 | if ( !(G4int(theNucleusA) == 1) ) { |
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164 | target = new G4InuclNuclei(targetMomentum, |
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165 | theNucleusA, |
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166 | theNucleus.GetZ()); |
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167 | target->setEnergy(); |
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168 | |
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169 | const G4CascadeMomentum& bmom = bullet->getMomentum(); |
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170 | eInit = std::sqrt(bmom[0] * bmom[0]); |
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171 | const G4CascadeMomentum& tmom = target->getMomentum(); |
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172 | eInit += std::sqrt(tmom[0] * tmom[0]); |
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173 | |
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174 | sumBaryon += theNucleusA; |
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175 | |
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176 | if (verboseLevel > 2) { |
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177 | G4cout << "Bullet: " << G4endl; |
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178 | bullet->printParticle(); |
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179 | } |
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180 | if (verboseLevel > 2) { |
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181 | G4cout << "Target: " << G4endl; |
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182 | target->printParticle(); |
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183 | } |
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184 | } |
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185 | |
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186 | G4CollisionOutput output; |
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187 | |
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188 | // Colliders initialisation |
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189 | // G4ElementaryParticleCollider* colep = new G4ElementaryParticleCollider; |
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190 | // G4IntraNucleiCascader* inc = new G4IntraNucleiCascader; // the actual cascade |
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191 | // inc->setInteractionCase(1); // Interaction type is particle with nuclei. |
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192 | inc.setInteractionCase(1); // Interaction type is particle with nuclei. |
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193 | |
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194 | // G4NonEquilibriumEvaporator* noneq = new G4NonEquilibriumEvaporator; |
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195 | // G4EquilibriumEvaporator* eqil = new G4EquilibriumEvaporator; |
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196 | // G4Fissioner* fiss = new G4Fissioner; |
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197 | // G4BigBanger* bigb = new G4BigBanger; |
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198 | G4InuclCollider* collider = new G4InuclCollider(&colep, &inc, &noneq, &eqil, &fiss, &bigb); |
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199 | |
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200 | G4int maxTries = 100; // maximum tries for inelastic collision to avoid infinite loop |
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201 | G4int nTries = 0; // try counter |
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202 | |
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203 | #ifdef BERTDEV |
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204 | G4int coulombOK =0; // flag for correct Coulomb barrier |
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205 | #endif |
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206 | if (G4int(theNucleusA) == 1) { // special treatment for target H(1,1) (proton) |
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207 | |
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208 | targetH = new G4InuclElementaryParticle(targetMomentum, 1); |
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209 | |
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210 | G4float cutElastic[32]; |
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211 | |
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212 | cutElastic[proton ] = 1.0; // GeV |
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213 | cutElastic[neutron ] = 1.0; |
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214 | cutElastic[pionPlus ] = 0.6; |
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215 | cutElastic[pionMinus] = 0.2; |
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216 | cutElastic[pionZero ] = 0.2; |
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217 | cutElastic[kaonPlus ] = 0.5; |
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218 | cutElastic[kaonMinus] = 0.5; |
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219 | cutElastic[kaonMinus] = 0.5; |
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220 | cutElastic[kaonZero] = 0.5; |
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221 | cutElastic[kaonZeroBar] = 0.5; |
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222 | cutElastic[lambda] = 1.0; |
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223 | cutElastic[sigmaPlus] = 1.0; |
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224 | cutElastic[sigmaZero] = 1.0; |
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225 | cutElastic[sigmaMinus] = 1.0; |
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226 | cutElastic[xiZero] = 1.0; |
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227 | cutElastic[xiMinus] = 1.0; |
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228 | |
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229 | if (momentumBullet[3] > cutElastic[bulletType]) { // inelastic collision possible |
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230 | |
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231 | do { // we try to create inelastic interaction |
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232 | output = collider->collide(bullet, targetH); |
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233 | nTries++; |
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234 | } while( |
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235 | (nTries < maxTries) && |
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236 | (output.getOutgoingParticles().size() == 2 && // elastic: bullet + p = H(1,1) coming out |
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237 | (output.getOutgoingParticles().begin()->type() == bulletType || |
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238 | output.getOutgoingParticles().begin()->type() == proton) |
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239 | ) |
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240 | ); |
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241 | } else { // only elastic collision is energetically possible |
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242 | output = collider->collide(bullet, targetH); |
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243 | } |
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244 | |
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245 | sumBaryon += 1; |
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246 | |
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247 | const G4CascadeMomentum& bmom = bullet->getMomentum(); |
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248 | eInit = std::sqrt(bmom[0] * bmom[0]); |
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249 | const G4CascadeMomentum& tmom = targetH->getMomentum(); |
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250 | eInit += std::sqrt(tmom[0] * tmom[0]); |
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251 | |
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252 | if (verboseLevel > 2) { |
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253 | G4cout << "Target: " << G4endl; |
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254 | targetH->printParticle(); |
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255 | } |
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256 | |
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257 | } else { // treat all other targets excepet H(1,1) |
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258 | |
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259 | do // we try to create inelastic interaction |
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260 | { |
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261 | #ifdef BERTDEV |
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262 | coulombOK=0; // by default coulomb analysis is OK |
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263 | #endif |
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264 | output = collider->collide(bullet, target ); |
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265 | nTries++; |
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266 | |
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267 | #ifdef BERTDEV |
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268 | G4double coulumbBarrier = 8.7 * MeV; |
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269 | std::vector<G4InuclElementaryParticle> p= output.getOutgoingParticles(); |
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270 | if(!p.empty()) { |
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271 | for( particleIterator ipart = p.begin(); ipart != p.end(); ipart++) { |
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272 | if (ipart->type() == proton) { |
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273 | G4double e = ipart->getKineticEnergy()*GeV; |
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274 | if (e < coulumbBarrier) coulombOK= 1; // If event with coulomb barrier violation detected -> retry |
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275 | // G4cout << "///AH "<< e << "" << coulumbBarrier <<G4endl; |
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276 | } |
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277 | } |
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278 | } |
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279 | } while( |
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280 | (nTries < maxTries) && // conditions for next try |
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281 | (coulombOK==1) && |
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282 | ((output.getOutgoingParticles().size() + output.getNucleiFragments().size()) > 2.5) && |
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283 | (output.getOutgoingParticles().size()!=0) |
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284 | ); |
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285 | #else |
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286 | |
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287 | } while( |
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288 | (nTries < maxTries) && |
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289 | (output.getOutgoingParticles().size() + output.getNucleiFragments().size() < 2.5) && |
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290 | (output.getOutgoingParticles().size()!=0) && |
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291 | (output.getOutgoingParticles().begin()->type()==bullet->type()) |
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292 | ); |
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293 | #endif |
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294 | } |
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295 | |
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296 | if (verboseLevel > 1) |
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297 | { |
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298 | G4cout << " Cascade output: " << G4endl; |
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299 | output.printCollisionOutput(); |
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300 | } |
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301 | |
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302 | // Convert cascade data to use hadronics interface |
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303 | std::vector<G4InuclNuclei> nucleiFragments = output.getNucleiFragments(); |
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304 | std::vector<G4InuclElementaryParticle> particles = output.getOutgoingParticles(); |
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305 | |
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306 | theResult.SetStatusChange(stopAndKill); |
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307 | |
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308 | if (!particles.empty()) { |
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309 | particleIterator ipart; |
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310 | G4int outgoingParticle; |
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311 | |
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312 | for (ipart = particles.begin(); ipart != particles.end(); ipart++) { |
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313 | outgoingParticle = ipart->type(); |
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314 | const G4CascadeMomentum& mom = ipart->getMomentum(); |
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315 | eTot += std::sqrt(mom[0] * mom[0]); |
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316 | |
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317 | G4double ekin = ipart->getKineticEnergy() * GeV; |
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318 | G4ThreeVector aMom(mom[1], mom[2], mom[3]); |
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319 | aMom = aMom.unit(); |
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320 | |
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321 | if (ipart->baryon() ) { |
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322 | sumBaryon -= 1; |
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323 | } |
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324 | |
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325 | sumEnergy -= ekin / GeV; |
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326 | |
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327 | switch(outgoingParticle) { |
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328 | |
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329 | case proton: |
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330 | #ifdef debug_G4CascadeInterface |
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331 | G4cerr << "proton " << counter << " " << aMom << " " << ekin << G4endl; |
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332 | #endif |
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333 | cascadeParticle = |
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334 | new G4DynamicParticle(G4Proton::ProtonDefinition(), aMom, ekin); |
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335 | break; |
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336 | |
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337 | case neutron: |
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338 | |
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339 | #ifdef debug_G4CascadeInterface |
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340 | G4cerr << "neutron "<< counter<<" "<<aMom<<" "<< ekin<<G4endl; |
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341 | #endif |
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342 | cascadeParticle = |
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343 | new G4DynamicParticle(G4Neutron::NeutronDefinition(), aMom, ekin); |
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344 | break; |
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345 | |
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346 | case pionPlus: |
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347 | cascadeParticle = |
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348 | new G4DynamicParticle(G4PionPlus::PionPlusDefinition(), aMom, ekin); |
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349 | |
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350 | #ifdef debug_G4CascadeInterface |
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351 | G4cerr << "pionPlus "<< counter<<" "<<aMom<<" "<< ekin<<G4endl; |
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352 | #endif |
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353 | break; |
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354 | |
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355 | case pionMinus: |
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356 | cascadeParticle = |
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357 | new G4DynamicParticle(G4PionMinus::PionMinusDefinition(), aMom, ekin); |
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358 | |
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359 | #ifdef debug_G4CascadeInterface |
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360 | G4cerr << "pionMinus "<< counter<<" "<<aMom<<" "<< ekin<<G4endl; |
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361 | #endif |
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362 | break; |
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363 | |
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364 | case pionZero: |
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365 | cascadeParticle = |
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366 | new G4DynamicParticle(G4PionZero::PionZeroDefinition(), aMom, ekin); |
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367 | |
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368 | #ifdef debug_G4CascadeInterface |
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369 | G4cerr << "pionZero "<< counter<<" "<<aMom<<" "<< ekin<<G4endl; |
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370 | #endif |
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371 | break; |
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372 | |
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373 | case photon: |
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374 | cascadeParticle = |
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375 | new G4DynamicParticle(G4Gamma::Gamma(), aMom, ekin); |
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376 | |
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377 | #ifdef debug_G4CascadeInterface |
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378 | G4cerr << "photon "<< counter<<" "<<aMom<<" "<< ekin<<G4endl; |
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379 | #endif |
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380 | break; |
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381 | |
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382 | |
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383 | case kaonPlus: |
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384 | cascadeParticle = |
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385 | new G4DynamicParticle(G4KaonPlus::KaonPlusDefinition(), aMom, ekin); |
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386 | break; |
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387 | |
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388 | case kaonMinus: |
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389 | cascadeParticle = |
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390 | new G4DynamicParticle(G4KaonMinus::KaonMinusDefinition(), aMom, ekin); |
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391 | break; |
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392 | |
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393 | case kaonZero: |
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394 | if (G4UniformRand() > 0.5) { |
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395 | cascadeParticle = new G4DynamicParticle( |
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396 | G4KaonZeroLong::KaonZeroLongDefinition(), |
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397 | aMom, ekin); |
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398 | } else { |
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399 | cascadeParticle = new G4DynamicParticle( |
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400 | G4KaonZeroShort::KaonZeroShortDefinition(), |
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401 | aMom, ekin); |
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402 | } |
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403 | break; |
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404 | |
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405 | case kaonZeroBar: |
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406 | if (G4UniformRand() > 0.5) { |
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407 | cascadeParticle = new G4DynamicParticle( |
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408 | G4KaonZeroLong::KaonZeroLongDefinition(), |
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409 | aMom, ekin); |
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410 | } else { |
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411 | cascadeParticle = new G4DynamicParticle( |
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412 | G4KaonZeroShort::KaonZeroShortDefinition(), |
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413 | aMom, ekin); |
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414 | } |
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415 | break; |
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416 | |
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417 | case lambda: |
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418 | cascadeParticle = |
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419 | new G4DynamicParticle(G4Lambda::LambdaDefinition(), aMom, ekin); |
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420 | break; |
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421 | |
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422 | case sigmaPlus: |
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423 | cascadeParticle = |
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424 | new G4DynamicParticle(G4SigmaPlus::SigmaPlusDefinition(), aMom, ekin); |
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425 | break; |
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426 | |
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427 | case sigmaZero: |
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428 | cascadeParticle = |
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429 | new G4DynamicParticle(G4SigmaZero::SigmaZeroDefinition(), aMom, ekin); |
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430 | break; |
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431 | |
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432 | case sigmaMinus: |
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433 | cascadeParticle = |
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434 | new G4DynamicParticle(G4SigmaMinus::SigmaMinusDefinition(), aMom, ekin); |
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435 | break; |
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436 | |
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437 | case xiZero: |
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438 | cascadeParticle = |
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439 | new G4DynamicParticle(G4XiZero::XiZeroDefinition(), aMom, ekin); |
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440 | break; |
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441 | |
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442 | case xiMinus: |
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443 | cascadeParticle = |
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444 | new G4DynamicParticle(G4XiMinus::XiMinusDefinition(), aMom, ekin); |
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445 | break; |
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446 | |
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447 | default: |
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448 | G4cout << " ERROR: G4CascadeInterface::Propagate undefined particle type" |
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449 | << G4endl; |
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450 | } |
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451 | |
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452 | cascadeParticle->Set4Momentum(cascadeParticle->Get4Momentum()*=toLabFrame); |
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453 | theResult.AddSecondary(cascadeParticle); |
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454 | } |
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455 | } |
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456 | |
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457 | // get nuclei fragments |
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458 | G4DynamicParticle * aFragment = 0; |
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459 | G4ParticleDefinition * aIonDef = 0; |
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460 | G4ParticleTable *theTableOfParticles = G4ParticleTable::GetParticleTable(); |
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461 | |
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462 | if (!nucleiFragments.empty()) { |
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463 | nucleiIterator ifrag; |
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464 | |
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465 | for (ifrag = nucleiFragments.begin(); ifrag != nucleiFragments.end(); ifrag++) |
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466 | { |
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467 | G4double eKin = ifrag->getKineticEnergy() * GeV; |
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468 | const G4CascadeMomentum& mom = ifrag->getMomentum(); |
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469 | eTot += std::sqrt(mom[0] * mom[0]); |
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470 | |
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471 | G4ThreeVector aMom(mom[1], mom[2], mom[3]); |
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472 | aMom = aMom.unit(); |
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473 | |
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474 | // hpw @@@ ==> Should be zero: G4double fragmentExitation = ifrag->getExitationEnergyInGeV(); |
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475 | |
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476 | if (verboseLevel > 2) { |
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477 | G4cout << " Nuclei fragment: " << G4endl; |
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478 | ifrag->printParticle(); |
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479 | } |
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480 | |
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481 | G4int A = G4int(ifrag->getA()); |
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482 | G4int Z = G4int(ifrag->getZ()); |
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483 | aIonDef = theTableOfParticles->FindIon(Z, A, 0, Z); |
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484 | |
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485 | aFragment = new G4DynamicParticle(aIonDef, aMom, eKin); |
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486 | |
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487 | sumBaryon -= A; |
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488 | sumEnergy -= eKin / GeV; |
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489 | |
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490 | aFragment->Set4Momentum(aFragment->Get4Momentum()*=toLabFrame); |
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491 | theResult.AddSecondary(aFragment); |
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492 | } |
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493 | } |
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494 | |
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495 | if (verboseLevel > 2) { |
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496 | if (sumBaryon != 0) { |
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497 | G4cout << "ERROR: no baryon number conservation, sum of baryons = " |
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498 | << sumBaryon << G4endl; |
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499 | } |
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500 | |
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501 | if (sumEnergy > 0.01 ) { |
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502 | G4cout << "Kinetic energy conservation violated by " |
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503 | << sumEnergy << " GeV" << G4endl; |
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504 | } |
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505 | |
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506 | G4cout << "Total energy conservation at level ~" |
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507 | << (eInit - eTot) * GeV << " MeV" << G4endl; |
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508 | |
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509 | if (sumEnergy < -5.0e-5 ) { // 0.05 MeV |
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510 | G4cout << "FATAL ERROR: energy created " |
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511 | << sumEnergy * GeV << " MeV" << G4endl; |
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512 | } |
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513 | } |
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514 | |
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515 | delete bullet; |
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516 | // delete inc; |
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517 | delete collider; |
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518 | |
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519 | if(target != 0) delete target; |
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520 | if(targetH != 0) delete targetH; |
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521 | // if(cascadeParticle != 0) delete cascadeParticle; |
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522 | // if(aFragment != 0) delete aFragment; |
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523 | |
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524 | return &theResult; |
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525 | } |
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