Geant4 Cross Reference |
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 // Hadronic Process: Nuclear De-excitations 28 // by V. Lara (Nov 1999) 29 // 30 31 #include "G4C11GEMProbability.hh" 32 #include "G4SystemOfUnits.hh" 33 34 G4C11GEMProbability::G4C11GEMProbability() : 35 G4GEMProbability(11,6,3.0/2.0) // A,Z,Spin 36 { 37 38 ExcitEnergies.push_back(2000.0*keV); 39 ExcitSpins.push_back(1.0/2.0); 40 ExcitLifetimes.push_back(24.0e-15*s); 41 42 ExcitEnergies.push_back(4318.8*keV); 43 ExcitSpins.push_back(5.0/2.0); 44 ExcitLifetimes.push_back(8.3e-15*s); 45 46 ExcitEnergies.push_back(4804.2*keV); 47 ExcitSpins.push_back(3.0/2.0); 48 ExcitLifetimes.push_back(7.6e-15*s); 49 50 ExcitEnergies.push_back(6339.2*keV); 51 ExcitSpins.push_back(1.0/2.0); 52 ExcitLifetimes.push_back(77.0e-15*s); 53 54 ExcitEnergies.push_back(6478.2*keV); 55 ExcitSpins.push_back(7.0/2.0); 56 ExcitLifetimes.push_back(6.0e-15*s); 57 58 ExcitEnergies.push_back(6904.8*keV); 59 ExcitSpins.push_back(5.0/2.0); 60 ExcitLifetimes.push_back(48.0e-15*s); 61 62 ExcitEnergies.push_back(7499.7*keV); 63 ExcitSpins.push_back(3.0/2.0); 64 ExcitLifetimes.push_back(63.0e-15*s); 65 66 ExcitEnergies.push_back(8104.5*keV); 67 ExcitSpins.push_back(3.0/2.0); 68 ExcitLifetimes.push_back(fPlanck/(11*eV)); 69 70 ExcitEnergies.push_back(8420*keV); 71 ExcitSpins.push_back(5.0/2.0); 72 ExcitLifetimes.push_back(fPlanck/(15.2*eV)); 73 74 ExcitEnergies.push_back(8699*keV); 75 ExcitSpins.push_back(7.0/2.0); 76 ExcitLifetimes.push_back(fPlanck/(9*keV)); 77 78 ExcitEnergies.push_back(8701*keV); 79 ExcitSpins.push_back(5.0/2.0); 80 ExcitLifetimes.push_back(fPlanck/(15*keV)); 81 82 ExcitEnergies.push_back(9.20E+3*keV); 83 ExcitSpins.push_back(5.0/2.0); 84 ExcitLifetimes.push_back(fPlanck/(500*keV)); 85 86 ExcitEnergies.push_back(9.645E+3*keV); 87 ExcitSpins.push_back(3.0/2.0); 88 ExcitLifetimes.push_back(fPlanck/(210*keV)); 89 90 ExcitEnergies.push_back(9.78E+3*keV); 91 ExcitSpins.push_back(5.0/2.0); 92 ExcitLifetimes.push_back(fPlanck/(240*keV)); 93 94 ExcitEnergies.push_back(9.97E+3*keV); 95 ExcitSpins.push_back(7.0/2.0); 96 ExcitLifetimes.push_back(fPlanck/(120*keV)); 97 98 ExcitEnergies.push_back(10083*keV); 99 ExcitSpins.push_back(7.0/2.0); 100 ExcitLifetimes.push_back(fPlanck/(230*keV)); 101 102 ExcitEnergies.push_back(10679*keV); 103 ExcitSpins.push_back(9.0/2.0); 104 ExcitLifetimes.push_back(fPlanck/(200*keV)); 105 106 ExcitEnergies.push_back(12.51E+3*keV); 107 ExcitSpins.push_back(1.0/2.0); 108 ExcitLifetimes.push_back(fPlanck/(490*keV)); 109 110 ExcitEnergies.push_back(12.65E+3*keV); 111 ExcitSpins.push_back(7.0/2.0); 112 ExcitLifetimes.push_back(fPlanck/(360*keV)); 113 } 114 115 G4C11GEMProbability::~G4C11GEMProbability() 116 {} 117