[1350] | 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 | #ifndef G4INCLINPUT_HH |
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| 27 | #define G4INCLINPUT_HH 1 |
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| 28 | |
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| 29 | #include "G4Nucleus.hh" |
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| 30 | #include "G4HadProjectile.hh" |
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| 31 | #include "G4Proton.hh" |
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| 32 | #include "G4Neutron.hh" |
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| 33 | #include "G4Deuteron.hh" |
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| 34 | #include "G4Triton.hh" |
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| 35 | #include "G4He3.hh" |
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| 36 | #include "G4Alpha.hh" |
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| 37 | #include "G4ParticleTable.hh" |
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| 38 | |
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| 39 | #define FSIZE 15 |
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| 40 | /** |
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| 41 | * Initial values of a hadronic cascade problem. |
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| 42 | */ |
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| 43 | class G4InclInput { |
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| 44 | public: |
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| 45 | G4InclInput() { |
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| 46 | isExtended = false; |
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| 47 | breakupThreshold = 10; |
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| 48 | fTargetA = 0; |
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| 49 | fTargetZ = 0; |
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| 50 | fBulletType = 0; |
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| 51 | fBulletE = 0.0; |
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| 52 | fTimeScale = 1.0; |
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| 53 | fNuclearPotential = 45.0; // Nuclear potential |
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| 54 | icoup = 0; |
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| 55 | |
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| 56 | theExtendedProjectileA = 0; |
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| 57 | theExtendedProjectileZ = 0; |
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| 58 | isExtended = false; |
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| 59 | |
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| 60 | fMinProtonE = 0.0; |
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| 61 | fNuclearPotential = 45.0; |
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| 62 | fTimeScale = 1.0; |
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| 63 | fMinNeutronEnergy = 0.0; |
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| 64 | |
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| 65 | usingInverseKinematics = false; |
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| 66 | }; |
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| 67 | |
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| 68 | G4InclInput(const G4HadProjectile &aTrack, const G4Nucleus &theNucleus, G4bool inverseKinematics); |
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| 69 | |
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| 70 | ~G4InclInput(); |
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| 71 | |
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| 72 | void printInfo(); |
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| 73 | |
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| 74 | static void printProjectileTargetInfo(const G4HadProjectile &aTrack, const G4Nucleus &theNucleus); |
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| 75 | |
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| 76 | static G4bool canUseInverseKinematics(const G4HadProjectile &aTrack, const G4Nucleus &theNucleus); |
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| 77 | |
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| 78 | G4double bulletE() { |
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| 79 | return fBulletE; |
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| 80 | } |
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| 81 | |
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| 82 | G4int getClusterOption() { return 0; }; // No clusters (and in 4.2 there never will be!) |
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| 83 | |
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| 84 | G4int bulletType() { |
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| 85 | return fBulletType; |
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| 86 | }; |
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| 87 | |
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| 88 | void setExtendedProjectileInfo(const G4ParticleDefinition *pd); |
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| 89 | |
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| 90 | G4int getBulletType(const G4ParticleDefinition *pd); |
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| 91 | static G4ParticleDefinition* getParticleDefinition(G4int inclParticleCode); |
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| 92 | |
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| 93 | G4bool isInverseKinematics() { |
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| 94 | return usingInverseKinematics; |
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| 95 | }; |
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| 96 | |
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| 97 | G4int targetA() { return fTargetA; }; |
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| 98 | G4int targetZ() { return fTargetZ; }; |
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| 99 | |
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| 100 | G4int extendedProjectileA() { return theExtendedProjectileA; }; |
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| 101 | G4int extendedProjectileZ() { return theExtendedProjectileZ; }; |
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| 102 | G4bool isExtendedProjectile() { return isExtended; }; |
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| 103 | void isExtendedProjectile(G4bool ext) { isExtended = ext; }; |
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| 104 | |
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| 105 | G4double getPotential() { return fNuclearPotential; }; |
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| 106 | |
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| 107 | G4int getBreakupThreshold() { return breakupThreshold; }; |
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| 108 | G4double getTimeScale() { return fTimeScale; }; |
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| 109 | |
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| 110 | private: |
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| 111 | G4int theExtendedProjectileA; |
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| 112 | G4int theExtendedProjectileZ; |
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| 113 | G4bool isExtended; |
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| 114 | |
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| 115 | G4int breakupThreshold; |
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| 116 | /** |
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| 117 | * Here f is an array containing the following initial values: |
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| 118 | * - f[0] : target mass number |
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| 119 | * - f[1] : target charge number |
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| 120 | */ |
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| 121 | G4int fTargetA, fTargetZ; |
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| 122 | |
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| 123 | /* |
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| 124 | * - f[2] : bullet energy |
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| 125 | */ |
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| 126 | G4double fBulletE; |
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| 127 | |
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| 128 | /* |
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| 129 | * - f[3] : minimum proton energy to leave the target (default: 0.0) |
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| 130 | */ |
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| 131 | G4double fMinProtonE; |
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| 132 | |
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| 133 | /* |
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| 134 | * - f[4] : nuclear potential (default: 45.0 MeV) |
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| 135 | */ |
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| 136 | G4double fNuclearPotential; |
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| 137 | |
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| 138 | /* |
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| 139 | * - f[5] : time scale (default: 1.0) |
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| 140 | */ |
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| 141 | G4double fTimeScale; |
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| 142 | |
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| 143 | /* |
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| 144 | * - f[6] : bullet type (1: proton, 2: neutron, 3: pi+, 4: pi0 5: pi-, 6:H2, 7: H3, 8: He3, 9: He4 |
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| 145 | */ |
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| 146 | G4int fBulletType; |
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| 147 | |
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| 148 | /* |
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| 149 | * - f[7] : minimum neutron energy to leave the target (default: 0.0) |
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| 150 | */ |
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| 151 | G4double fMinNeutronEnergy; |
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| 152 | |
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| 153 | /* |
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| 154 | * - f[8] : target material identifier (G4Mat) |
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| 155 | * - f[9] : not used |
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| 156 | * - f[10] : not used |
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| 157 | * - f[11] : not used |
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| 158 | * - f[12] : not used |
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| 159 | * - f[13] : not used |
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| 160 | * - f[14] : not used |
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| 161 | */ |
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| 162 | // G4double f[FSIZE]; |
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| 163 | |
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| 164 | /** |
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| 165 | * Number of events to be processed. |
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| 166 | */ |
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| 167 | G4int icoup; |
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| 168 | |
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| 169 | G4bool usingInverseKinematics; |
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| 170 | }; |
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| 171 | |
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| 172 | #endif |
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