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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