[819] | 1 | // |
---|
| 2 | // ******************************************************************** |
---|
| 3 | // * License and Disclaimer * |
---|
| 4 | // * * |
---|
| 5 | // * The Geant4 software is copyright of the Copyright Holders of * |
---|
| 6 | // * the Geant4 Collaboration. It is provided under the terms and * |
---|
| 7 | // * conditions of the Geant4 Software License, included in the file * |
---|
| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These * |
---|
| 9 | // * include a list of copyright holders. * |
---|
| 10 | // * * |
---|
| 11 | // * Neither the authors of this software system, nor their employing * |
---|
| 12 | // * institutes,nor the agencies providing financial support for this * |
---|
| 13 | // * work make any representation or warranty, express or implied, * |
---|
| 14 | // * regarding this software system or assume any liability for its * |
---|
| 15 | // * use. Please see the license in the file LICENSE and URL above * |
---|
| 16 | // * for the full disclaimer and the limitation of liability. * |
---|
| 17 | // * * |
---|
| 18 | // * This code implementation is the result of the scientific and * |
---|
| 19 | // * technical work of the GEANT4 collaboration. * |
---|
| 20 | // * By using, copying, modifying or distributing the software (or * |
---|
| 21 | // * any work based on the software) you agree to acknowledge its * |
---|
| 22 | // * use in resulting scientific publications, and indicate your * |
---|
| 23 | // * acceptance of all terms of the Geant4 Software license. * |
---|
| 24 | // ******************************************************************** |
---|
| 25 | // |
---|
| 26 | // |
---|
| 27 | // $Id: G4O15GEMProbability.cc,v 1.5 2006/06/29 20:23:25 gunter Exp $ |
---|
[1007] | 28 | // GEANT4 tag $Name: geant4-09-02 $ |
---|
[819] | 29 | // |
---|
| 30 | // Hadronic Process: Nuclear De-excitations |
---|
| 31 | // by V. Lara (Nov 1999) |
---|
| 32 | // |
---|
| 33 | |
---|
| 34 | |
---|
| 35 | #include "G4O15GEMProbability.hh" |
---|
| 36 | |
---|
| 37 | G4O15GEMProbability::G4O15GEMProbability() : |
---|
| 38 | G4GEMProbability(15,8,1.0/2.0) // A,Z,Spin |
---|
| 39 | { |
---|
| 40 | |
---|
| 41 | ExcitEnergies.push_back(5183.0*keV); |
---|
| 42 | ExcitSpins.push_back(1.0/2.0); |
---|
| 43 | ExcitLifetimes.push_back(0.07*picosecond); |
---|
| 44 | |
---|
| 45 | ExcitEnergies.push_back(5240.9*keV); |
---|
| 46 | ExcitSpins.push_back(5.0/2.0); |
---|
| 47 | ExcitLifetimes.push_back(2.2*picosecond); |
---|
| 48 | |
---|
| 49 | ExcitEnergies.push_back(6176.3*keV); |
---|
| 50 | ExcitSpins.push_back(3.0/2.0); |
---|
| 51 | ExcitLifetimes.push_back(33.0E-3*picosecond); |
---|
| 52 | |
---|
| 53 | ExcitEnergies.push_back(6793.1*keV); |
---|
| 54 | ExcitSpins.push_back(3.0/2.0); |
---|
| 55 | ExcitLifetimes.push_back(19.0E-3*picosecond); |
---|
| 56 | |
---|
| 57 | ExcitEnergies.push_back(6859.4*keV); |
---|
| 58 | ExcitSpins.push_back(5.0/2.0); |
---|
| 59 | ExcitLifetimes.push_back(0.07*picosecond); |
---|
| 60 | |
---|
| 61 | ExcitEnergies.push_back(7556.8*keV); |
---|
| 62 | ExcitSpins.push_back(1.0/2.0); |
---|
| 63 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.6*keV)); |
---|
| 64 | |
---|
| 65 | ExcitEnergies.push_back(8284.3*keV); |
---|
| 66 | ExcitSpins.push_back(3.0/2.0); |
---|
| 67 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.6*keV)); |
---|
| 68 | |
---|
| 69 | ExcitEnergies.push_back(8743.0*keV); |
---|
| 70 | ExcitSpins.push_back(1.0/2.0); |
---|
| 71 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(32.0*keV)); |
---|
| 72 | |
---|
| 73 | ExcitEnergies.push_back(8922.0*keV); |
---|
| 74 | ExcitSpins.push_back(5.0/2.0); |
---|
| 75 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4.0*keV)); |
---|
| 76 | |
---|
| 77 | ExcitEnergies.push_back(8927.0*keV); |
---|
| 78 | ExcitSpins.push_back(1.0/2.0); |
---|
| 79 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4.0*keV)); |
---|
| 80 | |
---|
| 81 | ExcitEnergies.push_back(8982.4*keV); |
---|
| 82 | ExcitSpins.push_back(1.0/2.0); |
---|
| 83 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.9*keV)); |
---|
| 84 | |
---|
| 85 | ExcitEnergies.push_back(9487.0*keV); |
---|
| 86 | ExcitSpins.push_back(5.0/2.0); |
---|
| 87 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(10.1*keV)); |
---|
| 88 | |
---|
| 89 | ExcitEnergies.push_back(9527.0*keV); |
---|
| 90 | ExcitSpins.push_back(1.0/2.0); |
---|
| 91 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(280.0*keV)); |
---|
| 92 | |
---|
| 93 | ExcitEnergies.push_back(9610.0*keV); |
---|
| 94 | ExcitSpins.push_back(3.0/2.0); |
---|
| 95 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(8.8*keV)); |
---|
| 96 | |
---|
| 97 | ExcitEnergies.push_back(9662.0*keV); |
---|
| 98 | ExcitSpins.push_back(7.0/2.0); |
---|
| 99 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.0*keV)); |
---|
| 100 | |
---|
| 101 | ExcitEnergies.push_back(9720.0*keV); |
---|
| 102 | ExcitSpins.push_back(1.0/2.0); |
---|
| 103 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1185.0*keV)); |
---|
| 104 | |
---|
| 105 | ExcitEnergies.push_back(10291.0*keV); |
---|
| 106 | ExcitSpins.push_back(5.0/2.0); |
---|
| 107 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.0*keV)); |
---|
| 108 | |
---|
| 109 | ExcitEnergies.push_back(10296.0*keV); |
---|
| 110 | ExcitSpins.push_back(5.0/2.0); |
---|
| 111 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(11.0*keV)); |
---|
| 112 | |
---|
| 113 | ExcitEnergies.push_back(10478.0*keV); |
---|
| 114 | ExcitSpins.push_back(3.0/2.0); |
---|
| 115 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(25.0*keV)); |
---|
| 116 | |
---|
| 117 | ExcitEnergies.push_back(10506.0*keV); |
---|
| 118 | ExcitSpins.push_back(3.0/2.0); |
---|
| 119 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(140.0*keV)); |
---|
| 120 | |
---|
| 121 | ExcitEnergies.push_back(10917.0*keV); |
---|
| 122 | ExcitSpins.push_back(7.0/2.0); |
---|
| 123 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(90.0*keV)); |
---|
| 124 | |
---|
| 125 | ExcitEnergies.push_back(10938.0*keV); |
---|
| 126 | ExcitSpins.push_back(1.0/2.0); |
---|
| 127 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(99.0*keV)); |
---|
| 128 | |
---|
| 129 | ExcitEnergies.push_back(11025.0*keV); |
---|
| 130 | ExcitSpins.push_back(1.0/2.0); |
---|
| 131 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(25.0*keV)); |
---|
| 132 | |
---|
| 133 | ExcitEnergies.push_back(11218.0*keV); |
---|
| 134 | ExcitSpins.push_back(3.0/2.0); |
---|
| 135 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40.0*keV)); |
---|
| 136 | |
---|
| 137 | ExcitEnergies.push_back(11569.0*keV); |
---|
| 138 | ExcitSpins.push_back(5.0/2.0); |
---|
| 139 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20.0*keV)); |
---|
| 140 | |
---|
| 141 | ExcitEnergies.push_back(11616.0*keV); |
---|
| 142 | ExcitSpins.push_back(3.0/2.0); |
---|
| 143 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(80.0*keV)); |
---|
| 144 | |
---|
| 145 | ExcitEnergies.push_back(11748.0*keV); |
---|
| 146 | ExcitSpins.push_back(5.0/2.0); |
---|
| 147 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(99.0*keV)); |
---|
| 148 | |
---|
| 149 | ExcitEnergies.push_back(11846.0*keV); |
---|
| 150 | ExcitSpins.push_back(5.0/2.0); |
---|
| 151 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(65.0*keV)); |
---|
| 152 | |
---|
| 153 | ExcitEnergies.push_back(11980.0*keV); |
---|
| 154 | ExcitSpins.push_back(5.0/2.0); |
---|
| 155 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20.0*keV)); |
---|
| 156 | |
---|
| 157 | ExcitEnergies.push_back(12129.0*keV); |
---|
| 158 | ExcitSpins.push_back(5.0/2.0); |
---|
| 159 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200.0*keV)); |
---|
| 160 | |
---|
| 161 | ExcitEnergies.push_back(12471.0*keV); |
---|
| 162 | ExcitSpins.push_back(5.0/2.0); |
---|
| 163 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(77.0*keV)); |
---|
| 164 | |
---|
| 165 | ExcitEnergies.push_back(12835.0*keV); |
---|
| 166 | ExcitSpins.push_back(1.0/2.0); |
---|
| 167 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(16.0*keV)); |
---|
| 168 | |
---|
| 169 | ExcitEnergies.push_back(13450.0*keV); |
---|
| 170 | ExcitSpins.push_back(1.0/2.0); |
---|
| 171 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV)); |
---|
| 172 | |
---|
| 173 | ExcitEnergies.push_back(14030.0*keV); |
---|
| 174 | ExcitSpins.push_back(1.0/2.0); |
---|
| 175 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(160.0*keV)); |
---|
| 176 | |
---|
| 177 | ExcitEnergies.push_back(14270.0*keV); |
---|
| 178 | ExcitSpins.push_back(1.0/2.0); |
---|
| 179 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(340.0*keV)); |
---|
| 180 | |
---|
| 181 | ExcitEnergies.push_back(14465.0*keV); |
---|
| 182 | ExcitSpins.push_back(3.0/2.0); |
---|
| 183 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV)); |
---|
| 184 | |
---|
| 185 | ExcitEnergies.push_back(15100.0*keV); |
---|
| 186 | ExcitSpins.push_back(1.0/2.0); |
---|
| 187 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV)); |
---|
| 188 | |
---|
| 189 | ExcitEnergies.push_back(15900.0*keV); |
---|
| 190 | ExcitSpins.push_back(1.0/2.0); |
---|
| 191 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(350.0*keV)); |
---|
| 192 | |
---|
| 193 | ExcitEnergies.push_back(16430.0*keV); |
---|
| 194 | ExcitSpins.push_back(1.0/2.0); |
---|
| 195 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(560.0*keV)); |
---|
| 196 | |
---|
| 197 | ExcitEnergies.push_back(16900.0*keV); |
---|
| 198 | ExcitSpins.push_back(1.0/2.0); |
---|
| 199 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV)); |
---|
| 200 | |
---|
| 201 | ExcitEnergies.push_back(17510.0*keV); |
---|
| 202 | ExcitSpins.push_back(1.0/2.0); |
---|
| 203 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600.0*keV)); |
---|
| 204 | |
---|
| 205 | ExcitEnergies.push_back(17990.0*keV); |
---|
| 206 | ExcitSpins.push_back(1.0/2.0); |
---|
| 207 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200.0*keV)); |
---|
| 208 | |
---|
| 209 | ExcitEnergies.push_back(18400.0*keV); |
---|
| 210 | ExcitSpins.push_back(1.0/2.0); |
---|
| 211 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV)); |
---|
| 212 | |
---|
| 213 | ExcitEnergies.push_back(20500.0*keV); |
---|
| 214 | ExcitSpins.push_back(1.0/2.0); |
---|
| 215 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2000.0*keV)); |
---|
| 216 | |
---|
| 217 | ExcitEnergies.push_back(22000.0*keV); |
---|
| 218 | ExcitSpins.push_back(1.0/2.0); |
---|
| 219 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2000.0*keV)); |
---|
| 220 | |
---|
| 221 | ExcitEnergies.push_back(26000.0*keV); |
---|
| 222 | ExcitSpins.push_back(13.0/2.0); |
---|
| 223 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600.0*keV)); |
---|
| 224 | |
---|
| 225 | ExcitEnergies.push_back(28000.0*keV); |
---|
| 226 | ExcitSpins.push_back(9.0/2.0); |
---|
| 227 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2500.0*keV)); |
---|
| 228 | |
---|
| 229 | |
---|
| 230 | } |
---|
| 231 | |
---|
| 232 | |
---|
| 233 | G4O15GEMProbability::G4O15GEMProbability(const G4O15GEMProbability &) : G4GEMProbability() |
---|
| 234 | { |
---|
| 235 | throw G4HadronicException(__FILE__, __LINE__, "G4O15GEMProbability::copy_constructor meant to not be accessable"); |
---|
| 236 | } |
---|
| 237 | |
---|
| 238 | |
---|
| 239 | |
---|
| 240 | |
---|
| 241 | const G4O15GEMProbability & G4O15GEMProbability:: |
---|
| 242 | operator=(const G4O15GEMProbability &) |
---|
| 243 | { |
---|
| 244 | throw G4HadronicException(__FILE__, __LINE__, "G4O15GEMProbability::operator= meant to not be accessable"); |
---|
| 245 | return *this; |
---|
| 246 | } |
---|
| 247 | |
---|
| 248 | |
---|
| 249 | G4bool G4O15GEMProbability::operator==(const G4O15GEMProbability &) const |
---|
| 250 | { |
---|
| 251 | return false; |
---|
| 252 | } |
---|
| 253 | |
---|
| 254 | G4bool G4O15GEMProbability::operator!=(const G4O15GEMProbability &) const |
---|
| 255 | { |
---|
| 256 | return true; |
---|
| 257 | } |
---|
| 258 | |
---|
| 259 | |
---|
| 260 | |
---|