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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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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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: QGSC_CHIPS.icc,v 1.2 2009/04/17 15:29:19 mkossov Exp $ |
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27 | // GEANT4 tag $Name: geant4-09-03-cand-03 $ |
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28 | // |
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29 | //--------------------------------------------------------------------------- |
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30 | // |
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31 | // ClassName: QGSC_CHIPS |
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32 | // |
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33 | // Author: 2009 M.Kosov (Development of the QGSC_QGSC physics list) |
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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 tis file the aim is to get rid of LHEP, use the |
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39 | // QGSC model with the Energy Flow interface for CHIPS from E=0 for all |
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40 | // hadrons and gradually substitute QGSC by the native CHIPS (G4QCollision) |
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41 | // process starting from low energies (first nucleons, then mesons, after that |
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42 | // hyperons and antibaryons). The present "QGSC" model at low energies is |
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43 | // jus a temporary (far from ideal) interface to the CHIPS model. The nuclear |
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44 | // fragmentation CHIPS algorithm is the same in both models, but the first |
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45 | // interaction is temporary taken from the QGSC algorithm, which is not expected |
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46 | // to work at low energies, but temporary can be used as an interface to CHIPS. |
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47 | //------------------------------------------------------------------------------- |
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48 | |
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49 | #include "globals.hh" |
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50 | #include "G4ParticleDefinition.hh" |
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51 | #include "G4ParticleWithCuts.hh" |
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52 | #include "G4ProcessManager.hh" |
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53 | #include "G4ProcessVector.hh" |
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54 | #include "G4ParticleTypes.hh" |
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55 | #include "G4ParticleTable.hh" |
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56 | |
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57 | #include "G4Material.hh" |
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58 | #include "G4MaterialTable.hh" |
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59 | #include "G4ios.hh" |
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60 | #include <iomanip> |
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61 | |
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62 | #include "G4DecayPhysics.hh" |
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63 | #include "G4EmStandardPhysics.hh" |
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64 | #include "G4EmExtraPhysics.hh" |
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65 | #include "G4IonPhysics.hh" |
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66 | #include "G4QStoppingPhysics.hh" |
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67 | #include "G4HadronQElasticPhysics.hh" |
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68 | #include "G4NeutronTrackingCut.hh" |
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69 | |
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70 | #include "G4DataQuestionaire.hh" |
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71 | #include "HadronPhysicsQGSC_CHIPS.hh" |
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72 | |
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73 | template<class T> TQGSC_CHIPS<T>::TQGSC_CHIPS(G4int ver): T() |
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74 | { |
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75 | G4DataQuestionaire it(photon); |
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76 | G4cout << "<<< Geant4 Physics List simulation engine: QGSC_CHIPS 1.0"<<G4endl; |
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77 | G4cout <<G4endl<<G4endl; |
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78 | // default cut value (1.0 mm) |
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79 | this->defaultCutValue = 0.7*mm; |
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80 | this->SetVerboseLevel(ver); |
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81 | |
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82 | // EM Physics |
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83 | this->RegisterPhysics( new G4EmStandardPhysics(ver)); |
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84 | |
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85 | // Synchroton Radiation & GN Physics |
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86 | this->RegisterPhysics( new G4EmExtraPhysics("extra EM")); |
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87 | |
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88 | // Decays |
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89 | this->RegisterPhysics( new G4DecayPhysics("decay",ver) ); |
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90 | |
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91 | // Hadron Elastic scattering, "CHIPS" version |
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92 | this-> RegisterPhysics( new G4HadronQElasticPhysics("elastic",ver)); |
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93 | |
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94 | // Hadron Physics, "CHIPS" version |
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95 | G4bool quasiElastic; |
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96 | this->RegisterPhysics( new HadronPhysicsQGSC_CHIPS("hadron", quasiElastic=true)); |
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97 | |
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98 | // Stopping Physics, "CHIPS" version |
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99 | this->RegisterPhysics( new G4QStoppingPhysics("stopping", ver, false) ); |
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100 | |
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101 | // Ion Physics |
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102 | this->RegisterPhysics( new G4IonPhysics("ion") ); |
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103 | |
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104 | // Neutron tracking cut |
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105 | this->RegisterPhysics( new G4NeutronTrackingCut("Neutron tracking cut", ver) ); |
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106 | |
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107 | } |
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108 | |
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109 | template<class T> TQGSC_CHIPS<T>::~TQGSC_CHIPS() {} |
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110 | |
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111 | template<class T> void TQGSC_CHIPS<T>::SetCuts() |
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112 | { |
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113 | if (this->verboseLevel >1) G4cout << "QGSC_CHIPS::SetCuts:"; |
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114 | // " G4VUserPhysicsList::SetCutsWithDefault" method sets |
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115 | // the default cut value for all particle types |
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116 | |
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117 | this->SetCutsWithDefault(); |
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118 | |
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119 | // if (this->verboseLevel >0) |
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120 | // G4VUserPhysicsList::DumpCutValuesTable(); |
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121 | } |
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122 | |
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