source: trunk/source/processes/hadronic/models/de_excitation/gem_evaporation/src/G4C13GEMProbability.cc @ 1340

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27// $Id: G4C13GEMProbability.cc,v 1.6 2009/09/15 12:54:16 vnivanch Exp $
28// GEANT4 tag $Name: geant4-09-03-ref-09 $
29//
30// Hadronic Process: Nuclear De-excitations
31// by V. Lara (Nov 1999)
32//
33
34
35#include "G4C13GEMProbability.hh"
36
37G4C13GEMProbability::G4C13GEMProbability() :
38  G4GEMProbability(13,6,1.0/2.0) // A,Z,Spin
39{
40
41  ExcitEnergies.push_back(3088.4*keV);
42  ExcitSpins.push_back(1.0/2.0);
43  ExcitLifetimes.push_back(1.04e-15*s);
44
45  ExcitEnergies.push_back(3684.37*keV);
46  ExcitSpins.push_back(3.0/2.0);
47  ExcitLifetimes.push_back(1.04e-15*s);
48
49  ExcitEnergies.push_back( 3853.62*keV);
50  ExcitSpins.push_back(5.0/2.0);
51  ExcitLifetimes.push_back(7.5e-12*s);
52
53  ExcitEnergies.push_back(6864*keV);
54  ExcitSpins.push_back(5.0/2.0);
55  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(6*keV));
56
57  ExcitEnergies.push_back(7492*keV);
58  ExcitSpins.push_back(7.0/2.0);
59  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5*keV));
60
61  ExcitEnergies.push_back(7547*keV);
62  ExcitSpins.push_back(5.0/2.0);
63  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.2*keV));
64
65  ExcitEnergies.push_back(7677*keV);
66  ExcitSpins.push_back(3.0/2.0);
67  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(70*keV));
68
69  ExcitEnergies.push_back(8.2E3*keV);
70  ExcitSpins.push_back(3.0/2.0);
71  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000*keV));
72
73  ExcitEnergies.push_back(8860*keV);
74  ExcitSpins.push_back(1.0/2.0);
75  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(150*keV));
76
77  ExcitEnergies.push_back(9498*keV);
78  ExcitSpins.push_back(3.0/2.0);
79  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5*keV));
80
81  ExcitEnergies.push_back(9897*keV);
82  ExcitSpins.push_back(3.0/2.0);
83  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(26*keV));
84
85  ExcitEnergies.push_back(10753*keV);
86  ExcitSpins.push_back(7.0/2.0);
87  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(55*keV));
88
89  ExcitEnergies.push_back(10818*keV);
90  ExcitSpins.push_back(5.0/2.0);
91  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(24*keV));
92
93  ExcitEnergies.push_back(10996*keV);
94  ExcitSpins.push_back(1.0/2.0);
95  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(37*keV));
96
97  ExcitEnergies.push_back(11080*keV);
98  ExcitSpins.push_back(1.0/2.0);
99  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4*keV));
100
101  ExcitEnergies.push_back(11851*keV);
102  ExcitSpins.push_back(3.0/2.0);
103  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(68*keV));
104
105  ExcitEnergies.push_back(11970*keV);
106  ExcitSpins.push_back(5.0/2.0);
107  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200*keV));
108
109  ExcitEnergies.push_back(12106*keV);
110  ExcitSpins.push_back(9.0/2.0);
111  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(81*keV));
112
113  ExcitEnergies.push_back(12400*keV);
114  ExcitSpins.push_back(7.0/2.0);
115  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(150*keV));
116
117  ExcitEnergies.push_back(13280*keV);
118  ExcitSpins.push_back(3.0/2.0);
119  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(340*keV));
120
121  ExcitEnergies.push_back(13410*keV);
122  ExcitSpins.push_back(9.0/2.0);
123  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(35*keV));
124
125  ExcitEnergies.push_back(13560*keV);
126  ExcitSpins.push_back(5.0/2.0);
127  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500*keV));
128
129  ExcitEnergies.push_back(13760*keV);
130  ExcitSpins.push_back(3.0/2.0);
131  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV));
132
133  ExcitEnergies.push_back(14120*keV);
134  ExcitSpins.push_back(5.0/2.0);
135  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200*keV));
136
137  ExcitEnergies.push_back(14.39E3*keV);
138  ExcitSpins.push_back(5.0/2.0);
139  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(260*keV));
140
141  ExcitEnergies.push_back(14940*keV);
142  ExcitSpins.push_back(3.0/2.0);
143  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(380*keV));
144
145  ExcitEnergies.push_back(15106*keV);
146  ExcitSpins.push_back(3.0/2.0);
147  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5*keV));
148
149  ExcitEnergies.push_back(19500*keV);
150  ExcitSpins.push_back(5.0/2.0);
151  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(450*keV));
152
153  SetExcitationEnergiesPtr(&ExcitEnergies);
154  SetExcitationSpinsPtr(&ExcitSpins);
155  SetExcitationLifetimesPtr(&ExcitLifetimes);
156}
157
158
159G4C13GEMProbability::G4C13GEMProbability(const G4C13GEMProbability &) : G4GEMProbability()
160{
161  throw G4HadronicException(__FILE__, __LINE__, "G4C13GEMProbability::copy_constructor meant to not be accessable");
162}
163
164
165
166
167const G4C13GEMProbability & G4C13GEMProbability::
168operator=(const G4C13GEMProbability &)
169{
170  throw G4HadronicException(__FILE__, __LINE__, "G4C13GEMProbability::operator= meant to not be accessable");
171  return *this;
172}
173
174
175G4bool G4C13GEMProbability::operator==(const G4C13GEMProbability &) const
176{
177  return false;
178}
179
180G4bool G4C13GEMProbability::operator!=(const G4C13GEMProbability &) const
181{
182  return true;
183}
184
185
186
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