1 | // |
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2 | // ******************************************************************** |
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3 | // * License and Disclaimer * |
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10 | // * * |
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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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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 | // $Id: HadronPhysicsQGSC_CHIPS.cc,v 1.6 2009/04/17 15:29:19 mkossov Exp $ |
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27 | // GEANT4 tag $Name: geant4-09-03 $ |
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28 | // |
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29 | //--------------------------------------------------------------------------- |
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30 | // |
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31 | // ClassName: HadronPhysicsQGSC_CHIPS |
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32 | // |
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33 | // Author: 2009 M. Kosov |
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34 | // |
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35 | // Modified: |
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36 | // |
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37 | //---------------------------------------------------------------------------- |
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38 | // Short description: In fact this is the definition of the Hadronic Inelastic |
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39 | // physics. The definition of the Hadronic Elastic physics one can find in the |
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40 | // G4HadronQElasticPhysics, which is stable (the same for all physics lists). |
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41 | // The only "unstable" part of the physics is the Hadronic Inelastic physics, |
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42 | // which is usually composed of the wixing of the High Energy Inelastic Model |
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43 | // (HEIM) and the Low Energy Inelastic Model (LEIM), which are applied only for |
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44 | // some hadrons (mostly nucleons and pi-mesons), above the LHEP model, which |
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45 | // usually covers all particles (but for Sigma_0 ?) and sometimes covers the |
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46 | // "hole" between the LEIM and HIME at intermediate energies. The name of the |
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47 | // Physics list is usually have a form HEIM_LEIM and the inelastic interactions |
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48 | // are defined in the HadronicPhysicsHEIM_LEIM class. So in this particular |
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49 | // physics list the low energy model is CHIPS (G4QCollision process) and the |
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50 | // high energy model is QGSC (QGS with the Energy Flow interface to CHIPS), |
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51 | // which are in terms of the energy boundary are mixed not on the model level, |
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52 | // but on the process level (G4DiscProcessMixer class). The LHEP is completely |
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53 | // excluded from this physics list, because the MiscLHEP is substituted by the |
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54 | // MiscQGSC class (QGS with the Energy Flow interface to CHIPS), covering all |
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55 | // particles, which are not N, pi, or K, defined by the separate builders. |
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56 | //--------------------------------------------------------------------------- |
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57 | |
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58 | #include "HadronPhysicsQGSC_CHIPS.hh" |
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59 | |
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60 | #include "globals.hh" |
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61 | #include "G4ios.hh" |
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62 | #include <iomanip> |
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63 | #include "G4ParticleDefinition.hh" |
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64 | #include "G4ParticleTable.hh" |
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65 | |
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66 | #include "G4MesonConstructor.hh" |
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67 | #include "G4BaryonConstructor.hh" |
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68 | #include "G4ShortLivedConstructor.hh" |
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69 | |
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70 | HadronPhysicsQGSC_CHIPS::HadronPhysicsQGSC_CHIPS(const G4String& name, G4bool quasiElastic) |
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71 | : G4VPhysicsConstructor(name), QuasiElastic(quasiElastic) |
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72 | {} |
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73 | |
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74 | void HadronPhysicsQGSC_CHIPS::CreateModels() |
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75 | { |
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76 | theNeut = new G4QNeutronBuilder; |
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77 | theNeut->RegisterMe(theQGSCNeut=new G4QGSC_CHIPSNeutronBuilder(QuasiElastic)); |
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78 | //theQGSCNeut = new G4QGSC_CHIPSNeutronBuilder(QuasiElastic)); |
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79 | |
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80 | theQGSCNeut->SetMinEnergy(0.0*GeV); |
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81 | |
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82 | theProt = new G4QProtonBuilder; |
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83 | theProt->RegisterMe(theQGSCProt = new G4QGSC_CHIPSProtonBuilder(QuasiElastic)); |
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84 | //theQGSCProt = new G4QGSC_CHIPSProtonBuilder(QuasiElastic); |
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85 | |
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86 | theQGSCProt->SetMinEnergy(0.0*GeV); |
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87 | |
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88 | thePiK = new G4PiKBuilder; |
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89 | thePiK->RegisterMe(theQGSCPiK=new G4QGSC_CHIPSPiKBuilder(QuasiElastic)); |
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90 | |
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91 | theQGSCPiK->SetMinEnergy(0.0*GeV); |
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92 | |
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93 | theMiscQGSC=new G4MiscQGSCBuilder(0); // No verbose (@@ to be developed) |
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94 | } |
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95 | |
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96 | HadronPhysicsQGSC_CHIPS::~HadronPhysicsQGSC_CHIPS() |
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97 | { |
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98 | delete theQGSCNeut; |
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99 | delete theNeut; |
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100 | |
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101 | delete theQGSCProt; |
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102 | delete theProt; |
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103 | |
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104 | delete theQGSCPiK; |
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105 | delete thePiK; |
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106 | |
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107 | delete theMiscQGSC; |
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108 | } |
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109 | |
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110 | void HadronPhysicsQGSC_CHIPS::ConstructParticle() |
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111 | { |
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112 | G4MesonConstructor pMesonConstructor; |
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113 | pMesonConstructor.ConstructParticle(); |
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114 | |
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115 | G4BaryonConstructor pBaryonConstructor; |
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116 | pBaryonConstructor.ConstructParticle(); |
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117 | |
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118 | G4ShortLivedConstructor pShortLivedConstructor; |
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119 | pShortLivedConstructor.ConstructParticle(); |
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120 | } |
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121 | |
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122 | #include "G4ProcessManager.hh" |
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123 | void HadronPhysicsQGSC_CHIPS::ConstructProcess() |
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124 | { |
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125 | CreateModels(); |
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126 | theNeut->Build(); |
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127 | theProt->Build(); |
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128 | thePiK->Build(); |
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129 | theMiscQGSC->Build(); |
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130 | } |
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131 | |
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