1 | // |
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2 | // ******************************************************************** |
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3 | // * License and Disclaimer * |
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4 | // * * |
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6 | // * the Geant4 Collaboration. It is provided under the terms and * |
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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 | // $Id: G4HEAntiOmegaMinusInelastic.cc,v 1.15 2008/03/17 20:49:17 dennis Exp $ |
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28 | // GEANT4 tag $Name: geant4-09-02 $ |
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29 | // |
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30 | // |
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31 | |
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32 | #include "globals.hh" |
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33 | #include "G4ios.hh" |
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34 | |
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35 | // |
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36 | // G4 Process: Gheisha High Energy Collision model. |
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37 | // This includes the high energy cascading model, the two-body-resonance model |
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38 | // and the low energy two-body model. Not included are the low energy stuff like |
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39 | // nuclear reactions, nuclear fission without any cascading and all processes for |
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40 | // particles at rest. |
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41 | // First work done by J.L.Chuma and F.W.Jones, TRIUMF, June 96. |
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42 | // H. Fesefeldt, RWTH-Aachen, 23-October-1996 |
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43 | // Last modified: 29-July-1998 |
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44 | |
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45 | #include "G4HEAntiOmegaMinusInelastic.hh" |
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46 | |
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47 | G4HadFinalState * G4HEAntiOmegaMinusInelastic:: |
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48 | ApplyYourself( const G4HadProjectile &aTrack, G4Nucleus &targetNucleus ) |
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49 | { |
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50 | G4HEVector * pv = new G4HEVector[MAXPART]; |
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51 | const G4HadProjectile *aParticle = &aTrack; |
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52 | // G4DynamicParticle *originalTarget = targetNucleus.ReturnTargetParticle(); |
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53 | const G4double atomicWeight = targetNucleus.GetN(); |
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54 | const G4double atomicNumber = targetNucleus.GetZ(); |
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55 | G4HEVector incidentParticle(aParticle); |
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56 | |
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57 | G4int incidentCode = incidentParticle.getCode(); |
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58 | G4double incidentMass = incidentParticle.getMass(); |
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59 | G4double incidentTotalEnergy = incidentParticle.getEnergy(); |
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60 | G4double incidentTotalMomentum = incidentParticle.getTotalMomentum(); |
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61 | G4double incidentKineticEnergy = incidentTotalEnergy - incidentMass; |
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62 | |
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63 | if(incidentKineticEnergy < 1.) |
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64 | { |
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65 | G4cout << "GHEAntiOmegaMinusInelastic: incident energy < 1 GeV" << G4endl; |
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66 | } |
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67 | if(verboseLevel > 1) |
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68 | { |
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69 | G4cout << "G4HEAntiOmegaMinusInelastic::ApplyYourself" << G4endl; |
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70 | G4cout << "incident particle " << incidentParticle.getName() |
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71 | << "mass " << incidentMass |
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72 | << "kinetic energy " << incidentKineticEnergy |
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73 | << G4endl; |
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74 | G4cout << "target material with (A,Z) = (" |
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75 | << atomicWeight << "," << atomicNumber << ")" << G4endl; |
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76 | } |
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77 | |
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78 | G4double inelasticity = NuclearInelasticity(incidentKineticEnergy, |
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79 | atomicWeight, atomicNumber); |
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80 | if(verboseLevel > 1) |
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81 | G4cout << "nuclear inelasticity = " << inelasticity << G4endl; |
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82 | |
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83 | incidentKineticEnergy -= inelasticity; |
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84 | |
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85 | G4double excitationEnergyGNP = 0.; |
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86 | G4double excitationEnergyDTA = 0.; |
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87 | |
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88 | G4double excitation = NuclearExcitation(incidentKineticEnergy, |
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89 | atomicWeight, atomicNumber, |
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90 | excitationEnergyGNP, |
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91 | excitationEnergyDTA); |
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92 | if(verboseLevel > 1) |
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93 | G4cout << "nuclear excitation = " << excitation << excitationEnergyGNP |
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94 | << excitationEnergyDTA << G4endl; |
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95 | |
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96 | |
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97 | incidentKineticEnergy -= excitation; |
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98 | incidentTotalEnergy = incidentKineticEnergy + incidentMass; |
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99 | incidentTotalMomentum = std::sqrt( (incidentTotalEnergy-incidentMass) |
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100 | *(incidentTotalEnergy+incidentMass)); |
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101 | |
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102 | |
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103 | G4HEVector targetParticle; |
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104 | if(G4UniformRand() < atomicNumber/atomicWeight) |
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105 | { |
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106 | targetParticle.setDefinition("Proton"); |
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107 | } |
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108 | else |
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109 | { |
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110 | targetParticle.setDefinition("Neutron"); |
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111 | } |
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112 | |
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113 | G4double targetMass = targetParticle.getMass(); |
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114 | G4double centerOfMassEnergy = std::sqrt( incidentMass*incidentMass + targetMass*targetMass |
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115 | + 2.0*targetMass*incidentTotalEnergy); |
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116 | G4double availableEnergy = centerOfMassEnergy - targetMass - incidentMass; |
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117 | |
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118 | // this was the meaning of inElastic in the |
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119 | // original Gheisha stand-alone version. |
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120 | // G4bool inElastic = InElasticCrossSectionInFirstInt |
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121 | // (availableEnergy, incidentCode, incidentTotalMomentum); |
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122 | // by unknown reasons, it has been replaced |
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123 | // to the following code in Geant??? |
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124 | G4bool inElastic = true; |
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125 | // if (G4UniformRand() < elasticCrossSection/totalCrossSection) inElastic = false; |
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126 | |
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127 | vecLength = 0; |
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128 | |
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129 | if(verboseLevel > 1) |
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130 | G4cout << "ApplyYourself: CallFirstIntInCascade for particle " |
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131 | << incidentCode << G4endl; |
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132 | |
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133 | G4bool successful = false; |
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134 | |
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135 | if(inElastic || (!inElastic && atomicWeight < 1.5)) |
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136 | { |
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137 | FirstIntInCasAntiOmegaMinus(inElastic, availableEnergy, pv, vecLength, |
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138 | incidentParticle, targetParticle, atomicWeight); |
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139 | |
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140 | if(verboseLevel > 1) |
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141 | G4cout << "ApplyYourself::StrangeParticlePairProduction" << G4endl; |
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142 | |
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143 | |
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144 | if ((vecLength > 0) && (availableEnergy > 1.)) |
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145 | StrangeParticlePairProduction( availableEnergy, centerOfMassEnergy, |
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146 | pv, vecLength, |
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147 | incidentParticle, targetParticle); |
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148 | HighEnergyCascading( successful, pv, vecLength, |
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149 | excitationEnergyGNP, excitationEnergyDTA, |
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150 | incidentParticle, targetParticle, |
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151 | atomicWeight, atomicNumber); |
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152 | if (!successful) |
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153 | HighEnergyClusterProduction( successful, pv, vecLength, |
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154 | excitationEnergyGNP, excitationEnergyDTA, |
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155 | incidentParticle, targetParticle, |
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156 | atomicWeight, atomicNumber); |
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157 | if (!successful) |
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158 | MediumEnergyCascading( successful, pv, vecLength, |
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159 | excitationEnergyGNP, excitationEnergyDTA, |
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160 | incidentParticle, targetParticle, |
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161 | atomicWeight, atomicNumber); |
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162 | |
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163 | if (!successful) |
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164 | MediumEnergyClusterProduction( successful, pv, vecLength, |
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165 | excitationEnergyGNP, excitationEnergyDTA, |
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166 | incidentParticle, targetParticle, |
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167 | atomicWeight, atomicNumber); |
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168 | if (!successful) |
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169 | QuasiElasticScattering( successful, pv, vecLength, |
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170 | excitationEnergyGNP, excitationEnergyDTA, |
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171 | incidentParticle, targetParticle, |
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172 | atomicWeight, atomicNumber); |
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173 | } |
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174 | if (!successful) |
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175 | { |
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176 | ElasticScattering( successful, pv, vecLength, |
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177 | incidentParticle, |
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178 | atomicWeight, atomicNumber); |
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179 | } |
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180 | |
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181 | if (!successful) |
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182 | { |
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183 | G4cout << "GHEInelasticInteraction::ApplyYourself fails to produce final state particles" << G4endl; |
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184 | } |
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185 | FillParticleChange(pv, vecLength); |
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186 | delete [] pv; |
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187 | theParticleChange.SetStatusChange(stopAndKill); |
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188 | return & theParticleChange; |
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189 | } |
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190 | |
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191 | void |
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192 | G4HEAntiOmegaMinusInelastic::FirstIntInCasAntiOmegaMinus( G4bool &inElastic, |
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193 | const G4double availableEnergy, |
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194 | G4HEVector pv[], |
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195 | G4int &vecLen, |
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196 | G4HEVector incidentParticle, |
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197 | G4HEVector targetParticle, |
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198 | const G4double atomicWeight ) |
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199 | |
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200 | // AntiOmega undergoes interaction with nucleon within a nucleus. |
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201 | // As in Geant3, we think that this routine has absolutely no influence |
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202 | // on the whole performance of the program. Take AntiLambda instaed. |
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203 | |
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204 | { |
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205 | static const G4double expxu = std::log(MAXFLOAT); // upper bound for arg. of exp |
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206 | static const G4double expxl = -expxu; // lower bound for arg. of exp |
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207 | |
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208 | static const G4double protb = 0.7; |
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209 | static const G4double neutb = 0.7; |
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210 | static const G4double c = 1.25; |
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211 | |
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212 | static const G4int numMul = 1200; |
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213 | static const G4int numMulAn = 400; |
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214 | static const G4int numSec = 60; |
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215 | |
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216 | // G4int neutronCode = Neutron.getCode(); |
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217 | G4int protonCode = Proton.getCode(); |
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218 | |
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219 | G4int targetCode = targetParticle.getCode(); |
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220 | // G4double incidentMass = incidentParticle.getMass(); |
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221 | // G4double incidentEnergy = incidentParticle.getEnergy(); |
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222 | G4double incidentTotalMomentum = incidentParticle.getTotalMomentum(); |
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223 | |
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224 | static G4bool first = true; |
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225 | static G4double protmul[numMul], protnorm[numSec]; // proton constants |
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226 | static G4double protmulAn[numMulAn],protnormAn[numSec]; |
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227 | static G4double neutmul[numMul], neutnorm[numSec]; // neutron constants |
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228 | static G4double neutmulAn[numMulAn],neutnormAn[numSec]; |
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229 | |
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230 | // misc. local variables |
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231 | // np = number of pi+, nm = number of pi-, nz = number of pi0 |
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232 | |
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233 | G4int i, counter, nt, np, nm, nz; |
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234 | |
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235 | if( first ) |
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236 | { // compute normalization constants, this will only be done once |
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237 | first = false; |
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238 | for( i=0; i<numMul ; i++ ) protmul[i] = 0.0; |
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239 | for( i=0; i<numSec ; i++ ) protnorm[i] = 0.0; |
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240 | counter = -1; |
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241 | for( np=0; np<(numSec/3); np++ ) |
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242 | { |
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243 | for( nm=std::max(0,np-2); nm<=(np+1); nm++ ) |
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244 | { |
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245 | for( nz=0; nz<numSec/3; nz++ ) |
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246 | { |
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247 | if( ++counter < numMul ) |
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248 | { |
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249 | nt = np+nm+nz; |
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250 | if( (nt>0) && (nt<=numSec) ) |
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251 | { |
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252 | protmul[counter] = pmltpc(np,nm,nz,nt,protb,c); |
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253 | protnorm[nt-1] += protmul[counter]; |
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254 | } |
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255 | } |
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256 | } |
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257 | } |
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258 | } |
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259 | for( i=0; i<numMul; i++ )neutmul[i] = 0.0; |
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260 | for( i=0; i<numSec; i++ )neutnorm[i] = 0.0; |
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261 | counter = -1; |
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262 | for( np=0; np<numSec/3; np++ ) |
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263 | { |
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264 | for( nm=std::max(0,np-1); nm<=(np+2); nm++ ) |
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265 | { |
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266 | for( nz=0; nz<numSec/3; nz++ ) |
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267 | { |
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268 | if( ++counter < numMul ) |
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269 | { |
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270 | nt = np+nm+nz; |
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271 | if( (nt>0) && (nt<=numSec) ) |
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272 | { |
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273 | neutmul[counter] = pmltpc(np,nm,nz,nt,neutb,c); |
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274 | neutnorm[nt-1] += neutmul[counter]; |
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275 | } |
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276 | } |
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277 | } |
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278 | } |
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279 | } |
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280 | for( i=0; i<numSec; i++ ) |
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281 | { |
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282 | if( protnorm[i] > 0.0 )protnorm[i] = 1.0/protnorm[i]; |
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283 | if( neutnorm[i] > 0.0 )neutnorm[i] = 1.0/neutnorm[i]; |
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284 | } |
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285 | // annihilation |
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286 | for( i=0; i<numMulAn ; i++ ) protmulAn[i] = 0.0; |
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287 | for( i=0; i<numSec ; i++ ) protnormAn[i] = 0.0; |
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288 | counter = -1; |
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289 | for( np=1; np<(numSec/3); np++ ) |
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290 | { |
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291 | nm = std::max(0,np-1); |
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292 | for( nz=0; nz<numSec/3; nz++ ) |
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293 | { |
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294 | if( ++counter < numMulAn ) |
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295 | { |
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296 | nt = np+nm+nz; |
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297 | if( (nt>1) && (nt<=numSec) ) |
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298 | { |
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299 | protmulAn[counter] = pmltpc(np,nm,nz,nt,protb,c); |
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300 | protnormAn[nt-1] += protmulAn[counter]; |
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301 | } |
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302 | } |
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303 | } |
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304 | } |
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305 | for( i=0; i<numMulAn; i++ ) neutmulAn[i] = 0.0; |
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306 | for( i=0; i<numSec; i++ ) neutnormAn[i] = 0.0; |
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307 | counter = -1; |
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308 | for( np=0; np<numSec/3; np++ ) |
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309 | { |
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310 | nm = np; |
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311 | for( nz=0; nz<numSec/3; nz++ ) |
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312 | { |
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313 | if( ++counter < numMulAn ) |
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314 | { |
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315 | nt = np+nm+nz; |
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316 | if( (nt>1) && (nt<=numSec) ) |
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317 | { |
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318 | neutmulAn[counter] = pmltpc(np,nm,nz,nt,neutb,c); |
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319 | neutnormAn[nt-1] += neutmulAn[counter]; |
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320 | } |
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321 | } |
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322 | } |
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323 | } |
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324 | for( i=0; i<numSec; i++ ) |
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325 | { |
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326 | if( protnormAn[i] > 0.0 )protnormAn[i] = 1.0/protnormAn[i]; |
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327 | if( neutnormAn[i] > 0.0 )neutnormAn[i] = 1.0/neutnormAn[i]; |
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328 | } |
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329 | } // end of initialization |
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330 | |
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331 | |
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332 | // initialize the first two places |
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333 | // the same as beam and target |
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334 | pv[0] = incidentParticle; |
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335 | pv[1] = targetParticle; |
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336 | vecLen = 2; |
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337 | |
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338 | if( !inElastic ) |
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339 | { // some two-body reactions |
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340 | G4double cech[] = {0.50, 0.45, 0.40, 0.35, 0.30, 0.25, 0.06, 0.04, 0.005, 0.}; |
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341 | |
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342 | G4int iplab = std::min(9, G4int( incidentTotalMomentum*2.5 )); |
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343 | if( G4UniformRand() < cech[iplab]/std::pow(atomicWeight,0.42) ) |
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344 | { |
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345 | G4double ran = G4UniformRand(); |
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346 | |
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347 | if ( targetCode == protonCode) |
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348 | { |
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349 | if(ran < 0.2) |
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350 | { |
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351 | pv[0] = AntiSigmaZero; |
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352 | } |
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353 | else if (ran < 0.4) |
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354 | { |
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355 | pv[0] = AntiSigmaMinus; |
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356 | pv[1] = Neutron; |
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357 | } |
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358 | else if (ran < 0.6) |
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359 | { |
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360 | pv[0] = Proton; |
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361 | pv[1] = AntiLambda; |
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362 | } |
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363 | else if (ran < 0.8) |
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364 | { |
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365 | pv[0] = Proton; |
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366 | pv[1] = AntiSigmaZero; |
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367 | } |
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368 | else |
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369 | { |
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370 | pv[0] = Neutron; |
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371 | pv[1] = AntiSigmaMinus; |
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372 | } |
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373 | } |
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374 | else |
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375 | { |
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376 | if (ran < 0.2) |
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377 | { |
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378 | pv[0] = AntiSigmaZero; |
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379 | } |
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380 | else if (ran < 0.4) |
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381 | { |
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382 | pv[0] = AntiSigmaPlus; |
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383 | pv[1] = Proton; |
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384 | } |
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385 | else if (ran < 0.6) |
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386 | { |
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387 | pv[0] = Neutron; |
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388 | pv[1] = AntiLambda; |
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389 | } |
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390 | else if (ran < 0.8) |
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391 | { |
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392 | pv[0] = Neutron; |
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393 | pv[1] = AntiSigmaZero; |
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394 | } |
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395 | else |
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396 | { |
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397 | pv[0] = Proton; |
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398 | pv[1] = AntiSigmaPlus; |
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399 | } |
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400 | } |
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401 | } |
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402 | return; |
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403 | } |
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404 | else if (availableEnergy <= PionPlus.getMass()) |
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405 | return; |
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406 | |
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407 | // inelastic scattering |
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408 | |
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409 | np = 0; nm = 0; nz = 0; |
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410 | G4double anhl[] = {1.00, 1.00, 1.00, 1.00, 1.00, 1.00, 1.00, 1.00, 0.97, 0.88, |
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411 | 0.85, 0.81, 0.75, 0.64, 0.64, 0.55, 0.55, 0.45, 0.47, 0.40, |
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412 | 0.39, 0.36, 0.33, 0.10, 0.01}; |
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413 | G4int iplab = G4int( incidentTotalMomentum*10.); |
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414 | if ( iplab > 9) iplab = 10 + G4int( (incidentTotalMomentum -1.)*5. ); |
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415 | if ( iplab > 14) iplab = 15 + G4int( incidentTotalMomentum -2. ); |
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416 | if ( iplab > 22) iplab = 23 + G4int( (incidentTotalMomentum -10.)/10.); |
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417 | iplab = std::min(24, iplab); |
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418 | |
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419 | if ( G4UniformRand() > anhl[iplab] ) |
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420 | { // non- annihilation channels |
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421 | |
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422 | // number of total particles vs. centre of mass Energy - 2*proton mass |
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423 | |
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424 | G4double aleab = std::log(availableEnergy); |
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425 | G4double n = 3.62567+aleab*(0.665843+aleab*(0.336514 |
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426 | + aleab*(0.117712+0.0136912*aleab))) - 2.0; |
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427 | |
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428 | // normalization constant for kno-distribution. |
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429 | // calculate first the sum of all constants, check for numerical problems. |
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430 | G4double test, dum, anpn = 0.0; |
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431 | |
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432 | for (nt=1; nt<=numSec; nt++) { |
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433 | test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) ); |
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434 | dum = pi*nt/(2.0*n*n); |
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435 | if (std::fabs(dum) < 1.0) { |
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436 | if( test >= 1.0e-10 )anpn += dum*test; |
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437 | } else { |
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438 | anpn += dum*test; |
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439 | } |
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440 | } |
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441 | |
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442 | G4double ran = G4UniformRand(); |
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443 | G4double excs = 0.0; |
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444 | if( targetCode == protonCode ) |
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445 | { |
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446 | counter = -1; |
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447 | for (np=0; np<numSec/3; np++) { |
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448 | for (nm=std::max(0,np-2); nm<=(np+1); nm++) { |
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449 | for (nz=0; nz<numSec/3; nz++) { |
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450 | if (++counter < numMul) { |
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451 | nt = np+nm+nz; |
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452 | if ( (nt>0) && (nt<=numSec) ) { |
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453 | test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) ); |
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454 | dum = (pi/anpn)*nt*protmul[counter]*protnorm[nt-1]/(2.0*n*n); |
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455 | if (std::fabs(dum) < 1.0) { |
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456 | if( test >= 1.0e-10 )excs += dum*test; |
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457 | } else { |
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458 | excs += dum*test; |
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459 | } |
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460 | |
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461 | if (ran < excs) goto outOfLoop; //-----------------------> |
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462 | } |
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463 | } |
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464 | } |
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465 | } |
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466 | } |
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467 | |
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468 | // 3 previous loops continued to the end |
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469 | inElastic = false; // quasi-elastic scattering |
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470 | return; |
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471 | } |
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472 | else |
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473 | { // target must be a neutron |
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474 | counter = -1; |
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475 | for (np=0; np<numSec/3; np++) { |
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476 | for (nm=std::max(0,np-1); nm<=(np+2); nm++) { |
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477 | for (nz=0; nz<numSec/3; nz++) { |
---|
478 | if (++counter < numMul) { |
---|
479 | nt = np+nm+nz; |
---|
480 | if ( (nt>0) && (nt<=numSec) ) { |
---|
481 | test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) ); |
---|
482 | dum = (pi/anpn)*nt*neutmul[counter]*neutnorm[nt-1]/(2.0*n*n); |
---|
483 | if (std::fabs(dum) < 1.0) { |
---|
484 | if( test >= 1.0e-10 )excs += dum*test; |
---|
485 | } else { |
---|
486 | excs += dum*test; |
---|
487 | } |
---|
488 | |
---|
489 | if (ran < excs) goto outOfLoop; // -----------> |
---|
490 | } |
---|
491 | } |
---|
492 | } |
---|
493 | } |
---|
494 | } |
---|
495 | // 3 previous loops continued to the end |
---|
496 | inElastic = false; // quasi-elastic scattering. |
---|
497 | return; |
---|
498 | } |
---|
499 | |
---|
500 | outOfLoop: // <----------------------------------- |
---|
501 | |
---|
502 | ran = G4UniformRand(); |
---|
503 | |
---|
504 | if( targetCode == protonCode) |
---|
505 | { |
---|
506 | if( np == nm) |
---|
507 | { |
---|
508 | if (ran < 0.40) |
---|
509 | { |
---|
510 | } |
---|
511 | else if (ran < 0.8) |
---|
512 | { |
---|
513 | pv[0] = AntiSigmaZero; |
---|
514 | } |
---|
515 | else |
---|
516 | { |
---|
517 | pv[0] = AntiSigmaMinus; |
---|
518 | pv[1] = Neutron; |
---|
519 | } |
---|
520 | } |
---|
521 | else if (np == (nm+1)) |
---|
522 | { |
---|
523 | if( ran < 0.25) |
---|
524 | { |
---|
525 | pv[1] = Neutron; |
---|
526 | } |
---|
527 | else if (ran < 0.5) |
---|
528 | { |
---|
529 | pv[0] = AntiSigmaZero; |
---|
530 | pv[1] = Neutron; |
---|
531 | } |
---|
532 | else |
---|
533 | { |
---|
534 | pv[0] = AntiSigmaPlus; |
---|
535 | } |
---|
536 | } |
---|
537 | else if (np == (nm-1)) |
---|
538 | { |
---|
539 | pv[0] = AntiSigmaMinus; |
---|
540 | } |
---|
541 | else |
---|
542 | { |
---|
543 | pv[0] = AntiSigmaPlus; |
---|
544 | pv[1] = Neutron; |
---|
545 | } |
---|
546 | } |
---|
547 | else |
---|
548 | { |
---|
549 | if( np == nm) |
---|
550 | { |
---|
551 | if (ran < 0.4) |
---|
552 | { |
---|
553 | } |
---|
554 | else if(ran < 0.8) |
---|
555 | { |
---|
556 | pv[0] = AntiSigmaZero; |
---|
557 | } |
---|
558 | else |
---|
559 | { |
---|
560 | pv[0] = AntiSigmaPlus; |
---|
561 | pv[1] = Proton; |
---|
562 | } |
---|
563 | } |
---|
564 | else if ( np == (nm-1)) |
---|
565 | { |
---|
566 | if (ran < 0.5) |
---|
567 | { |
---|
568 | pv[0] = AntiSigmaMinus; |
---|
569 | } |
---|
570 | else if (ran < 0.75) |
---|
571 | { |
---|
572 | pv[1] = Proton; |
---|
573 | } |
---|
574 | else |
---|
575 | { |
---|
576 | pv[0] = AntiSigmaZero; |
---|
577 | pv[1] = Proton; |
---|
578 | } |
---|
579 | } |
---|
580 | else if (np == (nm+1)) |
---|
581 | { |
---|
582 | pv[0] = AntiSigmaPlus; |
---|
583 | } |
---|
584 | else |
---|
585 | { |
---|
586 | pv[0] = AntiSigmaMinus; |
---|
587 | pv[1] = Proton; |
---|
588 | } |
---|
589 | } |
---|
590 | |
---|
591 | } |
---|
592 | else // annihilation |
---|
593 | { |
---|
594 | if ( availableEnergy > 2. * PionPlus.getMass() ) |
---|
595 | { |
---|
596 | |
---|
597 | G4double aleab = std::log(availableEnergy); |
---|
598 | G4double n = 3.62567+aleab*(0.665843+aleab*(0.336514 |
---|
599 | + aleab*(0.117712+0.0136912*aleab))) - 2.0; |
---|
600 | |
---|
601 | // normalization constant for kno-distribution. |
---|
602 | // calculate first the sum of all constants, check for numerical problems. |
---|
603 | G4double test, dum, anpn = 0.0; |
---|
604 | |
---|
605 | for (nt=2; nt<=numSec; nt++) { |
---|
606 | test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) ); |
---|
607 | dum = pi*nt/(2.0*n*n); |
---|
608 | if (std::fabs(dum) < 1.0) { |
---|
609 | if( test >= 1.0e-10 )anpn += dum*test; |
---|
610 | } else { |
---|
611 | anpn += dum*test; |
---|
612 | } |
---|
613 | } |
---|
614 | |
---|
615 | G4double ran = G4UniformRand(); |
---|
616 | G4double excs = 0.0; |
---|
617 | if( targetCode == protonCode ) |
---|
618 | { |
---|
619 | counter = -1; |
---|
620 | for( np=1; np<numSec/3; np++ ) |
---|
621 | { |
---|
622 | nm = np-1; |
---|
623 | for( nz=0; nz<numSec/3; nz++ ) |
---|
624 | { |
---|
625 | if( ++counter < numMulAn ) |
---|
626 | { |
---|
627 | nt = np+nm+nz; |
---|
628 | if ( (nt>1) && (nt<=numSec) ) { |
---|
629 | test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) ); |
---|
630 | dum = (pi/anpn)*nt*protmulAn[counter]*protnormAn[nt-1]/(2.0*n*n); |
---|
631 | if (std::fabs(dum) < 1.0) { |
---|
632 | if( test >= 1.0e-10 )excs += dum*test; |
---|
633 | } else { |
---|
634 | excs += dum*test; |
---|
635 | } |
---|
636 | |
---|
637 | if (ran < excs) goto outOfLoopAn; //-----------------------> |
---|
638 | } |
---|
639 | } |
---|
640 | } |
---|
641 | } |
---|
642 | // 3 previous loops continued to the end |
---|
643 | inElastic = false; // quasi-elastic scattering |
---|
644 | return; |
---|
645 | } |
---|
646 | else |
---|
647 | { // target must be a neutron |
---|
648 | counter = -1; |
---|
649 | for( np=0; np<numSec/3; np++ ) |
---|
650 | { |
---|
651 | nm = np; |
---|
652 | for( nz=0; nz<numSec/3; nz++ ) |
---|
653 | { |
---|
654 | if( ++counter < numMulAn ) |
---|
655 | { |
---|
656 | nt = np+nm+nz; |
---|
657 | if ( (nt>1) && (nt<=numSec) ) { |
---|
658 | test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) ); |
---|
659 | dum = (pi/anpn)*nt*neutmulAn[counter]*neutnormAn[nt-1]/(2.0*n*n); |
---|
660 | if (std::fabs(dum) < 1.0) { |
---|
661 | if( test >= 1.0e-10 )excs += dum*test; |
---|
662 | } else { |
---|
663 | excs += dum*test; |
---|
664 | } |
---|
665 | |
---|
666 | if (ran < excs) goto outOfLoopAn; // --------------------------> |
---|
667 | } |
---|
668 | } |
---|
669 | } |
---|
670 | } |
---|
671 | inElastic = false; // quasi-elastic scattering. |
---|
672 | return; |
---|
673 | } |
---|
674 | outOfLoopAn: // <------------------------------------------------------------------ |
---|
675 | vecLen = 0; |
---|
676 | } |
---|
677 | } |
---|
678 | |
---|
679 | nt = np + nm + nz; |
---|
680 | while ( nt > 0) |
---|
681 | { |
---|
682 | G4double ran = G4UniformRand(); |
---|
683 | if ( ran < (G4double)np/nt) |
---|
684 | { |
---|
685 | if( np > 0 ) |
---|
686 | { pv[vecLen++] = PionPlus; |
---|
687 | np--; |
---|
688 | } |
---|
689 | } |
---|
690 | else if ( ran < (G4double)(np+nm)/nt) |
---|
691 | { |
---|
692 | if( nm > 0 ) |
---|
693 | { |
---|
694 | pv[vecLen++] = PionMinus; |
---|
695 | nm--; |
---|
696 | } |
---|
697 | } |
---|
698 | else |
---|
699 | { |
---|
700 | if( nz > 0 ) |
---|
701 | { |
---|
702 | pv[vecLen++] = PionZero; |
---|
703 | nz--; |
---|
704 | } |
---|
705 | } |
---|
706 | nt = np + nm + nz; |
---|
707 | } |
---|
708 | if (verboseLevel > 1) |
---|
709 | { |
---|
710 | G4cout << "Particles produced: " ; |
---|
711 | G4cout << pv[0].getName() << " " ; |
---|
712 | G4cout << pv[1].getName() << " " ; |
---|
713 | for (i=2; i < vecLen; i++) |
---|
714 | { |
---|
715 | G4cout << pv[i].getName() << " " ; |
---|
716 | } |
---|
717 | G4cout << G4endl; |
---|
718 | } |
---|
719 | return; |
---|
720 | } |
---|
721 | |
---|
722 | |
---|
723 | |
---|
724 | |
---|
725 | |
---|
726 | |
---|
727 | |
---|
728 | |
---|
729 | |
---|
730 | |
---|