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 | // $Id: G4InclDataDefs.hh,v 1.5 2008/06/25 17:20:04 kaitanie Exp $ |
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27 | // Translation of INCL4.2/ABLA V3 |
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28 | // Pekka Kaitaniemi, HIP (translation) |
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29 | // Christelle Schmidt, IPNL (fission code) |
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30 | // Alain Boudard, CEA (contact person INCL/ABLA) |
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31 | // Aatos Heikkinen, HIP (project coordination) |
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32 | |
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33 | // All data structures needed by INCL4 are defined here. |
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34 | |
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35 | #ifndef InclDataDefs_hh |
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36 | #define InclDataDefs_hh 1 |
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37 | |
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38 | #define FSIZE 15 |
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39 | /** |
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40 | * Initial values of a hadronic cascade problem. |
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41 | */ |
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42 | class G4Calincl { |
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43 | public: |
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44 | G4Calincl() {}; |
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45 | ~G4Calincl() {}; |
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46 | |
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47 | /** |
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48 | * Here f is an array containing the following initial values: |
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49 | * - f[0] : target mass number |
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50 | * - f[1] : target charge number |
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51 | * - f[2] : bullet energy |
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52 | * - f[3] : minimum proton energy to leave the target (default: 0.0) |
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53 | * - f[4] : nuclear potential (default: 45.0 MeV) |
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54 | * - f[5] : time scale (default: 1.0) |
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55 | * - 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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56 | * - f[7] : minimum neutron energy to leave the target (default: 0.0) |
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57 | * - f[8] : target material identifier (G4Mat) |
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58 | * - f[9] : not used |
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59 | * - f[10] : not used |
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60 | * - f[11] : not used |
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61 | * - f[12] : not used |
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62 | * - f[13] : not used |
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63 | * - f[14] : not used |
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64 | */ |
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65 | G4double f[FSIZE]; |
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66 | |
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67 | /** |
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68 | * Number of events to be processed. |
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69 | */ |
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70 | G4int icoup; |
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71 | }; |
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72 | |
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73 | #define IGRAINESIZE 19 |
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74 | /** |
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75 | * Random seeds used by internal random number generators. |
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76 | * @see G4Incl::standardRandom |
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77 | * @see G4Incl::gaussianRandom |
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78 | */ |
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79 | class G4Hazard{ |
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80 | public: |
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81 | G4Hazard() {}; |
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82 | ~G4Hazard() {}; |
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83 | |
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84 | /** |
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85 | * Random seed |
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86 | */ |
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87 | G4long ial; |
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88 | |
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89 | /** |
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90 | * An array of random seeds. |
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91 | */ |
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92 | G4long igraine[IGRAINESIZE]; |
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93 | }; |
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94 | |
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95 | #define MATSIZE 500 |
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96 | #define MATGEOSIZE 6 |
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97 | /** |
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98 | * Target nuclei to be taken into account in the cascade problem. |
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99 | */ |
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100 | class G4Mat { |
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101 | public: |
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102 | G4Mat() { }; |
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103 | ~G4Mat() { }; |
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104 | |
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105 | /** |
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106 | * Charge numbers. |
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107 | */ |
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108 | G4int zmat[MATSIZE]; |
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109 | |
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110 | /** |
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111 | * Mass number |
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112 | */ |
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113 | G4int amat[MATSIZE]; |
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114 | |
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115 | /** |
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116 | * |
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117 | */ |
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118 | G4double bmax_geo[MATGEOSIZE][MATSIZE]; |
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119 | |
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120 | /** |
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121 | * Number of materials. |
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122 | */ |
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123 | G4int nbmat; |
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124 | }; |
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125 | |
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126 | #define LGNSIZE 9 |
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127 | /** |
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128 | * Properties of light nucleus used as a bullet. |
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129 | */ |
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130 | class G4LightGausNuc { |
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131 | public: |
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132 | G4LightGausNuc() {}; |
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133 | ~G4LightGausNuc() {}; |
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134 | |
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135 | G4double rms1t[LGNSIZE]; |
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136 | G4double pf1t[LGNSIZE]; |
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137 | G4double pfln[LGNSIZE]; |
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138 | G4double tfln[LGNSIZE]; |
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139 | G4double vnuc[LGNSIZE]; |
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140 | }; |
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141 | |
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142 | #define LNSIZE 30 |
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143 | /** |
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144 | * Data of light nuclei. |
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145 | */ |
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146 | class G4LightNuc { |
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147 | public: |
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148 | G4LightNuc() {}; |
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149 | ~G4LightNuc() {}; |
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150 | |
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151 | /** |
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152 | * r |
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153 | */ |
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154 | G4double r[LNSIZE]; |
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155 | |
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156 | /** |
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157 | * a |
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158 | */ |
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159 | G4double a[LNSIZE]; |
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160 | }; |
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161 | |
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162 | #define SAXWROWS 30 |
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163 | #define SAXWCOLS 500 |
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164 | /** |
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165 | * Woods-Saxon density and its first derivative. |
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166 | */ |
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167 | class G4Saxw { |
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168 | public: |
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169 | G4Saxw() {}; |
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170 | ~G4Saxw() {}; |
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171 | |
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172 | /** |
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173 | * x |
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174 | */ |
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175 | G4double x[SAXWROWS][SAXWCOLS]; |
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176 | |
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177 | /** |
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178 | * y |
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179 | */ |
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180 | G4double y[SAXWROWS][SAXWCOLS]; |
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181 | |
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182 | /** |
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183 | * s |
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184 | */ |
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185 | G4double s[SAXWROWS][SAXWCOLS]; |
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186 | |
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187 | /** |
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188 | * imat |
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189 | */ |
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190 | G4int imat; |
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191 | |
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192 | /** |
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193 | * n |
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194 | */ |
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195 | G4int n; |
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196 | |
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197 | /** |
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198 | * k |
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199 | */ |
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200 | G4int k; |
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201 | }; |
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202 | |
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203 | /** |
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204 | * Parameters for INCL4 model. |
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205 | */ |
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206 | class G4Ws { |
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207 | public: |
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208 | G4Ws() {}; |
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209 | ~G4Ws() {}; |
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210 | |
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211 | /** |
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212 | * r0 |
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213 | */ |
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214 | G4double r0; |
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215 | |
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216 | /** |
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217 | * adif |
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218 | */ |
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219 | G4double adif; |
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220 | |
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221 | /** |
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222 | * Maximum radius of the nucleus |
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223 | */ |
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224 | G4double rmaxws; |
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225 | |
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226 | /** |
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227 | * drws |
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228 | */ |
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229 | G4double drws; |
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230 | |
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231 | /** |
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232 | * Shape of the surface of the nucleus: |
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233 | * - -1: Woods-Saxon density with impact parameter dependence |
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234 | * - 0: Woods-Saxon density without impact parameter dependence |
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235 | * - 1: Sharp surface (hard sphere) |
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236 | */ |
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237 | G4double nosurf; |
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238 | |
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239 | /** |
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240 | * Parameter related to the maximum radius of the nucleus. |
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241 | * |
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242 | * rmaxws = r0 + xfoisa*A |
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243 | */ |
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244 | G4double xfoisa; |
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245 | |
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246 | /** |
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247 | * Pauli blocking used in the simulation: |
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248 | * - 0: statistic Pauli blocking |
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249 | * - 1: strict Pauli blocking |
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250 | * - 2: no Pauli blocking |
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251 | */ |
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252 | G4double npaulstr; |
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253 | |
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254 | /** |
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255 | * Maximum impact parameter |
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256 | */ |
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257 | G4double bmax; |
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258 | }; |
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259 | |
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260 | #define DTONSIZE 13 |
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261 | /** |
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262 | * Random seeds used by internal random number generators. |
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263 | * @see G4Incl::standardRandom |
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264 | * @see G4Incl::gaussianRandom |
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265 | */ |
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266 | class G4Dton { |
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267 | public: |
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268 | G4Dton() {}; |
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269 | ~G4Dton() {}; |
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270 | |
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271 | G4double c[DTONSIZE]; |
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272 | G4double d[DTONSIZE]; |
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273 | G4double fn; |
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274 | }; |
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275 | |
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276 | #define SPL2SIZE 100 |
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277 | /** |
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278 | * Random seeds used by internal random number generators. |
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279 | * @see G4Incl::standardRandom |
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280 | * @see G4Incl::gaussianRandom |
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281 | */ |
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282 | class G4Spl2 { |
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283 | public: |
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284 | G4Spl2() {}; |
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285 | ~G4Spl2() {}; |
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286 | |
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287 | G4double x[SPL2SIZE]; |
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288 | G4double y[SPL2SIZE]; |
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289 | G4double a[SPL2SIZE]; |
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290 | G4double b[SPL2SIZE]; |
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291 | G4double c[SPL2SIZE]; |
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292 | G4int n; |
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293 | }; |
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294 | |
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295 | // incl4.2.cc: |
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296 | |
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297 | //#define BL1SIZE 300 |
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298 | #define BL1SIZE 3000 |
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299 | /** |
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300 | * Random seeds used by internal random number generators. |
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301 | * @see G4Incl::standardRandom |
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302 | * @see G4Incl::gaussianRandom |
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303 | */ |
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304 | class G4Bl1 { |
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305 | public: |
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306 | G4Bl1() {}; |
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307 | ~G4Bl1() {}; |
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308 | |
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309 | G4double p1[BL1SIZE],p2[BL1SIZE],p3[BL1SIZE]; |
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310 | G4double eps[BL1SIZE]; |
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311 | G4int ind1[BL1SIZE],ind2[BL1SIZE]; |
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312 | G4double ta; |
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313 | }; |
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314 | |
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315 | #define BL2CROISSIZE 19900 |
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316 | #define BL2INDSIZE 19900 |
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317 | /** |
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318 | * |
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319 | */ |
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320 | class G4Bl2 { |
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321 | public: |
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322 | G4Bl2() {}; |
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323 | ~G4Bl2() {}; |
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324 | |
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325 | /** |
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326 | * |
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327 | */ |
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328 | G4double crois[BL2CROISSIZE]; |
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329 | |
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330 | /** |
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331 | * |
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332 | */ |
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333 | G4int k; |
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334 | |
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335 | /** |
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336 | * |
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337 | */ |
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338 | G4int ind[BL2INDSIZE]; |
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339 | |
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340 | /** |
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341 | * |
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342 | */ |
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343 | G4int jnd[BL2INDSIZE]; |
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344 | }; |
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345 | |
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346 | //#define BL3SIZE 300 |
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347 | #define BL3SIZE 3000 |
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348 | /** |
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349 | * |
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350 | */ |
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351 | class G4Bl3 { |
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352 | public: |
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353 | G4Bl3() {}; |
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354 | ~G4Bl3() {}; |
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355 | |
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356 | /** |
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357 | * r1 and r2 |
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358 | */ |
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359 | G4double r1,r2; |
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360 | |
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361 | /** |
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362 | * Nucleon positions |
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363 | */ |
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364 | G4double x1[BL3SIZE], x2[BL3SIZE],x3[BL3SIZE]; |
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365 | |
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366 | /** |
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367 | * Mass numbers |
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368 | */ |
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369 | G4int ia1,ia2; |
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370 | |
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371 | /** |
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372 | * rab2 |
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373 | */ |
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374 | G4double rab2; |
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375 | }; |
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376 | |
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377 | /** |
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378 | * G4Bl4 |
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379 | */ |
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380 | class G4Bl4 { |
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381 | public: |
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382 | G4Bl4() {}; |
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383 | ~G4Bl4() {}; |
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384 | |
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385 | /** |
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386 | * tmax5 |
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387 | */ |
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388 | G4double tmax5; |
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389 | }; |
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390 | |
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391 | //#define BL5SIZE 300 |
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392 | #define BL5SIZE 3000 |
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393 | /** |
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394 | * G4Bl5 |
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395 | */ |
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396 | class G4Bl5 { |
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397 | public: |
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398 | G4Bl5() {}; |
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399 | ~G4Bl5() {}; |
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400 | |
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401 | /** |
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402 | * tlg |
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403 | */ |
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404 | G4double tlg[BL5SIZE]; |
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405 | |
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406 | /** |
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407 | * nesc |
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408 | */ |
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409 | G4int nesc[BL5SIZE]; |
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410 | }; |
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411 | |
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412 | /** |
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413 | * G4Bl6 |
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414 | */ |
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415 | class G4Bl6 { |
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416 | public: |
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417 | G4Bl6() {}; |
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418 | ~G4Bl6() {}; |
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419 | |
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420 | /** |
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421 | * xx10 |
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422 | */ |
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423 | G4double xx10; |
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424 | |
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425 | /** |
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426 | * isa |
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427 | */ |
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428 | G4double isa; |
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429 | }; |
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430 | |
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431 | /** |
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432 | * G4Bl8 |
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433 | */ |
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434 | class G4Bl8 { |
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435 | public: |
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436 | G4Bl8() {}; |
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437 | ~G4Bl8() {}; |
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438 | |
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439 | /** |
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440 | * rathr |
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441 | */ |
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442 | G4double rathr; |
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443 | |
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444 | /** |
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445 | * ramass |
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446 | */ |
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447 | G4double ramass; |
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448 | }; |
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449 | |
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450 | //#define BL9SIZE 300 |
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451 | #define BL9SIZE 3000 |
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452 | /** |
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453 | * G4Bl9 |
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454 | */ |
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455 | class G4Bl9 { |
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456 | public: |
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457 | G4Bl9() { |
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458 | l1 = 0; |
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459 | l2 = 0; |
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460 | }; |
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461 | ~G4Bl9() {}; |
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462 | |
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463 | /** |
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464 | * hel |
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465 | */ |
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466 | G4double hel[BL9SIZE]; |
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467 | |
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468 | /** |
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469 | * l1 and l2 |
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470 | */ |
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471 | G4int l1,l2; |
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472 | }; |
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473 | |
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474 | /** |
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475 | * G4Bl10 |
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476 | */ |
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477 | class G4Bl10 { |
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478 | public: |
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479 | G4Bl10() {}; |
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480 | ~G4Bl10() {}; |
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481 | |
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482 | /** |
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483 | * ri4, rs4, r2i, r2s, pdummy, pf |
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484 | */ |
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485 | G4double ri4,rs4,r2i,r2s,pdummy,pf; |
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486 | }; |
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487 | |
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488 | /** |
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489 | * G4Kind |
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490 | */ |
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491 | class G4Kind { |
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492 | public: |
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493 | G4Kind() {}; |
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494 | ~G4Kind() {}; |
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495 | |
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496 | /** |
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497 | * kindf7 |
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498 | */ |
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499 | G4int kindf7; |
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500 | }; |
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501 | |
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502 | #define VARSIZE 3 |
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503 | #define VAEPSSIZE 250 |
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504 | #define VAAVM 1000 |
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505 | /** |
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506 | * Extra information on collisions between nucleons. |
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507 | */ |
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508 | class G4VarAvat { |
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509 | public: |
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510 | G4VarAvat() {}; |
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511 | ~G4VarAvat() {}; |
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512 | |
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513 | /** |
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514 | * |
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515 | */ |
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516 | G4int kveux; |
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517 | |
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518 | /** |
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519 | * |
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520 | */ |
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521 | G4double bavat; |
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522 | |
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523 | /** |
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524 | * |
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525 | */ |
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526 | G4int nopartavat,ncolavat; |
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527 | |
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528 | /** |
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529 | * |
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530 | */ |
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531 | G4double r1_in[VARSIZE],r1_first_avat[VARSIZE]; |
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532 | |
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533 | /** |
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534 | * |
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535 | */ |
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536 | G4double epsd[VAEPSSIZE],eps2[VAEPSSIZE],eps4[VAEPSSIZE],eps6[VAEPSSIZE],epsf[VAEPSSIZE]; |
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537 | |
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538 | /** |
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539 | * |
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540 | */ |
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541 | G4int nb_avat; |
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542 | |
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543 | /** |
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544 | * |
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545 | */ |
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546 | G4double timeavat[VAAVM],l1avat[VAAVM],l2avat[VAAVM],jpartl1[VAAVM],jpartl2[VAAVM]; |
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547 | |
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548 | /** |
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549 | * |
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550 | */ |
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551 | G4double del1avat[VAAVM],del2avat[VAAVM],energyavat[VAAVM]; |
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552 | |
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553 | /** |
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554 | * |
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555 | */ |
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556 | G4double bloc_paul[VAAVM],bloc_cdpp[VAAVM],go_out[VAAVM]; |
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557 | }; |
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558 | |
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559 | #define VARNTPSIZE 255 |
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560 | class G4VarNtp { |
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561 | public: |
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562 | G4VarNtp() {}; |
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563 | ~G4VarNtp() {}; |
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564 | |
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565 | /** |
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566 | * Clear and initialize all variables and arrays. |
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567 | */ |
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568 | void clear() { |
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569 | particleIndex = 0; |
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570 | projType = 0; |
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571 | projEnergy = 0.0; |
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572 | targetA = 0; |
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573 | targetZ = 0; |
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574 | massini = 0; |
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575 | mzini = 0; |
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576 | exini = 0; |
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577 | pcorem = 0; |
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578 | mcorem = 0; |
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579 | pxrem = 0; |
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580 | pyrem = 0; |
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581 | pzrem = 0; |
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582 | mulncasc = 0; |
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583 | mulnevap = 0; |
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584 | mulntot = 0; |
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585 | bimpact = 0.0; |
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586 | jremn = 0; |
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587 | kfis = 0; |
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588 | estfis = 0; |
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589 | izfis = 0; |
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590 | iafis = 0; |
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591 | ntrack = 0; |
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592 | for(G4int i = 0; i < VARNTPSIZE; i++) { |
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593 | itypcasc[i] = 0; |
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594 | avv[i] = 0; |
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595 | zvv[i] = 0; |
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596 | enerj[i] = 0.0; |
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597 | plab[i] = 0.0; |
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598 | tetlab[i] = 0.0; |
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599 | philab[i] = 0.0; |
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600 | full[i] = false; |
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601 | } |
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602 | } |
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603 | |
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604 | void addParticle(G4double A, G4double Z, G4double E, G4double P, G4double theta, G4double phi) { |
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605 | if(full[particleIndex]) { |
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606 | G4cout <<"G4VarNtp: Error. Index i = " << particleIndex << " is already occupied by particle:" << G4endl; |
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607 | G4cout <<"A = " << avv[particleIndex] << " Z = " << zvv[particleIndex] << G4endl; |
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608 | G4cout <<"Tried to replace it with:" << G4endl; |
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609 | G4cout <<"A = " << Z << " Z = " << Z << G4endl; |
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610 | } else { |
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611 | avv[particleIndex] = (int) A; |
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612 | zvv[particleIndex] = (int) Z; |
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613 | enerj[particleIndex] = E; |
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614 | plab[particleIndex] = P; |
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615 | tetlab[particleIndex] = theta; |
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616 | philab[particleIndex] = phi; |
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617 | full[particleIndex] = true; |
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618 | ntrack = particleIndex + 1; |
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619 | particleIndex++; |
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620 | } |
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621 | } |
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622 | |
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623 | /** |
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624 | * Baryon number conservation check. |
---|
625 | */ |
---|
626 | G4int getTotalBaryonNumber() { |
---|
627 | G4int baryonNumber = 0; |
---|
628 | for(G4int i = 0; i < ntrack; i++) { |
---|
629 | if(avv[i] > 0) { |
---|
630 | baryonNumber += avv[i]; |
---|
631 | } |
---|
632 | } |
---|
633 | return baryonNumber; |
---|
634 | } |
---|
635 | |
---|
636 | /** |
---|
637 | * Return total energy. |
---|
638 | */ |
---|
639 | G4double getTotalEnergy() { |
---|
640 | G4double energy = 0.0; |
---|
641 | for(G4int i = 0; i < ntrack; i++) { |
---|
642 | energy += std::sqrt(std::pow(plab[i], 2) + std::pow(getMass(i), 2)); // E^2 = p^2 + m^2 |
---|
643 | } |
---|
644 | |
---|
645 | return energy; |
---|
646 | } |
---|
647 | |
---|
648 | /** |
---|
649 | * Return total three momentum. |
---|
650 | */ |
---|
651 | G4double getTotalThreeMomentum() { |
---|
652 | G4double momentum = 0; |
---|
653 | for(G4int i = 0; i < ntrack; i++) { |
---|
654 | momentum += plab[i]; |
---|
655 | } |
---|
656 | return momentum; |
---|
657 | } |
---|
658 | |
---|
659 | G4double getMomentumSum() { |
---|
660 | G4double momentum = 0; |
---|
661 | for(G4int i = 0; i < ntrack; i++) { |
---|
662 | momentum += plab[i]; |
---|
663 | } |
---|
664 | return momentum; |
---|
665 | } |
---|
666 | |
---|
667 | G4double getMass(G4int particle) { |
---|
668 | const G4double protonMass = 938.272; |
---|
669 | const G4double neutronMass = 939.565; |
---|
670 | const G4double pionMass = 139.57; |
---|
671 | |
---|
672 | G4double mass = 0.0; |
---|
673 | if(avv[particle] == 1 && zvv[particle] == 1) mass = protonMass; |
---|
674 | if(avv[particle] == 1 && zvv[particle] == 0) mass = neutronMass; |
---|
675 | if(avv[particle] == -1) mass = pionMass; |
---|
676 | if(avv[particle] > 1) |
---|
677 | mass = avv[particle] * protonMass + zvv[particle] * neutronMass; |
---|
678 | return mass; |
---|
679 | } |
---|
680 | |
---|
681 | /** |
---|
682 | * Dump debugging output. |
---|
683 | */ |
---|
684 | void dump() { |
---|
685 | G4int nProton = 0, nNeutron = 0; |
---|
686 | G4int nPiPlus = 0, nPiZero = 0, nPiMinus = 0; |
---|
687 | G4int nH2 = 0, nHe3 = 0, nAlpha = 0; |
---|
688 | G4int nFragments = 0; |
---|
689 | G4int nParticles = 0; |
---|
690 | G4cout <<"Particles produced in the event (" << ntrack << "):" << G4endl; |
---|
691 | G4cout <<"A \t Z \t Ekin \t Ptot \t Theta \t Phi" << G4endl; |
---|
692 | for(G4int i = 0; i < ntrack; i++) { |
---|
693 | nParticles++; |
---|
694 | if(avv[i] == 1 && zvv[i] == 1) nProton++; // Count multiplicities |
---|
695 | if(avv[i] == 1 && zvv[i] == 0) nNeutron++; |
---|
696 | if(avv[i] == -1 && zvv[i] == 1) nPiPlus++; |
---|
697 | if(avv[i] == -1 && zvv[i] == 0) nPiZero++; |
---|
698 | if(avv[i] == -1 && zvv[i] == -1) nPiMinus++; |
---|
699 | if(avv[i] == 2 && zvv[i] == 1) nH2++; |
---|
700 | if(avv[i] == 3 && zvv[i] == 2) nHe3++; |
---|
701 | if(avv[i] == 4 && zvv[i] == 2) nAlpha++; |
---|
702 | if( zvv[i] > 2) nFragments++; |
---|
703 | |
---|
704 | G4cout << i << " \t " << avv[i] << " \t " << zvv[i] << " \t " << enerj[i] << " \t " |
---|
705 | << plab[i] << " \t " << tetlab[i] << " \t " << philab[i] << G4endl; |
---|
706 | } |
---|
707 | |
---|
708 | G4cout <<"Summary of event: " << G4endl; |
---|
709 | G4cout <<"Projectile type: " << projType <<" Energy: " << projEnergy << G4endl; |
---|
710 | G4cout <<"Target A = " << targetA << " Z = " << targetZ << G4endl; |
---|
711 | G4cout <<"Remnant from cascade: " << G4endl; |
---|
712 | G4cout <<"A = " << massini << " Z = " << mzini << " excitation E = " << exini << G4endl; |
---|
713 | G4cout <<"Particle multiplicities:" << G4endl; |
---|
714 | G4cout <<"Protons: " << nProton << " Neutrons: " << nNeutron << G4endl; |
---|
715 | G4cout <<"pi+: " << nPiPlus << " pi0: " << nPiZero << " pi-: " << nPiMinus << G4endl; |
---|
716 | G4cout <<"H2: " << nH2 << " He3: " << nHe3 << " Alpha: " << nAlpha << G4endl; |
---|
717 | G4cout <<"Nucleus fragments = " << nFragments << G4endl; |
---|
718 | G4cout <<"Conservation laws:" << G4endl; |
---|
719 | G4cout <<"Baryon number = " << getTotalBaryonNumber() << G4endl; |
---|
720 | G4cout <<"Number of particles = " << nParticles << G4endl; |
---|
721 | } |
---|
722 | |
---|
723 | /** |
---|
724 | * Projectile type. |
---|
725 | */ |
---|
726 | G4int projType; |
---|
727 | |
---|
728 | /** |
---|
729 | * Projectile energy. |
---|
730 | */ |
---|
731 | G4double projEnergy; |
---|
732 | |
---|
733 | /** |
---|
734 | * Target mass number. |
---|
735 | */ |
---|
736 | G4int targetA; |
---|
737 | |
---|
738 | /** |
---|
739 | * Target charge number. |
---|
740 | */ |
---|
741 | G4int targetZ; |
---|
742 | |
---|
743 | /** |
---|
744 | * A of the remnant. |
---|
745 | */ |
---|
746 | G4double massini; |
---|
747 | |
---|
748 | /** |
---|
749 | * Z of the remnant. |
---|
750 | */ |
---|
751 | G4double mzini; |
---|
752 | |
---|
753 | /** |
---|
754 | * Excitation energy. |
---|
755 | */ |
---|
756 | G4double exini; |
---|
757 | |
---|
758 | G4double pcorem, mcorem, pxrem, pyrem, pzrem; |
---|
759 | |
---|
760 | /** |
---|
761 | * Cascade n multip. |
---|
762 | */ |
---|
763 | G4int mulncasc; |
---|
764 | |
---|
765 | /** |
---|
766 | * Evaporation n multip. |
---|
767 | */ |
---|
768 | G4int mulnevap; |
---|
769 | |
---|
770 | /** |
---|
771 | * Total n multip. |
---|
772 | */ |
---|
773 | G4int mulntot; |
---|
774 | |
---|
775 | /** |
---|
776 | * Impact parameter. |
---|
777 | */ |
---|
778 | G4double bimpact; |
---|
779 | |
---|
780 | /** |
---|
781 | * Remnant Intrinsic Spin. |
---|
782 | */ |
---|
783 | G4int jremn; |
---|
784 | |
---|
785 | /** |
---|
786 | * Fission 1/0=Y/N. |
---|
787 | */ |
---|
788 | G4int kfis; |
---|
789 | |
---|
790 | /** |
---|
791 | * Excit energy at fis. |
---|
792 | */ |
---|
793 | G4double estfis; |
---|
794 | |
---|
795 | /** |
---|
796 | * Z of fiss nucleus. |
---|
797 | */ |
---|
798 | G4int izfis; |
---|
799 | |
---|
800 | /** |
---|
801 | * A of fiss nucleus. |
---|
802 | */ |
---|
803 | G4int iafis; |
---|
804 | |
---|
805 | /** |
---|
806 | * Number of particles. |
---|
807 | */ |
---|
808 | G4int ntrack; |
---|
809 | |
---|
810 | /** |
---|
811 | * The state of the index: |
---|
812 | * true = reserved |
---|
813 | * false = free |
---|
814 | */ |
---|
815 | G4bool full[VARNTPSIZE]; |
---|
816 | |
---|
817 | /** |
---|
818 | * emitted in cascade (0) or evaporation (1). |
---|
819 | */ |
---|
820 | G4int itypcasc[VARNTPSIZE]; |
---|
821 | |
---|
822 | |
---|
823 | /** |
---|
824 | * A (-1 for pions). |
---|
825 | */ |
---|
826 | G4int avv[VARNTPSIZE]; |
---|
827 | |
---|
828 | /** |
---|
829 | * Z |
---|
830 | */ |
---|
831 | G4int zvv[VARNTPSIZE]; |
---|
832 | |
---|
833 | /** |
---|
834 | * Kinetic energy. |
---|
835 | */ |
---|
836 | G4double enerj[VARNTPSIZE]; |
---|
837 | |
---|
838 | /** |
---|
839 | * Momentum. |
---|
840 | */ |
---|
841 | G4double plab[VARNTPSIZE]; |
---|
842 | |
---|
843 | /** |
---|
844 | * Theta angle. |
---|
845 | */ |
---|
846 | G4double tetlab[VARNTPSIZE]; |
---|
847 | |
---|
848 | /** |
---|
849 | * Phi angle. |
---|
850 | */ |
---|
851 | G4double philab[VARNTPSIZE]; |
---|
852 | |
---|
853 | private: |
---|
854 | G4int particleIndex; |
---|
855 | }; |
---|
856 | |
---|
857 | /** |
---|
858 | * Pauli blocking. |
---|
859 | */ |
---|
860 | class G4Paul { |
---|
861 | public: |
---|
862 | G4Paul() {}; |
---|
863 | ~G4Paul() {}; |
---|
864 | |
---|
865 | /** |
---|
866 | * |
---|
867 | */ |
---|
868 | G4double ct0,ct1,ct2,ct3,ct4,ct5,ct6,pr,pr2,xrr,xrr2; |
---|
869 | |
---|
870 | /** |
---|
871 | * |
---|
872 | */ |
---|
873 | G4double cp0,cp1,cp2,cp3,cp4,cp5,cp6; |
---|
874 | }; |
---|
875 | |
---|
876 | |
---|
877 | #endif |
---|