source: trunk/source/processes/hadronic/models/de_excitation/gem_evaporation/src/G4B11GEMProbability.cc @ 1340

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27// $Id: G4B11GEMProbability.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 "G4B11GEMProbability.hh"
36
37G4B11GEMProbability::G4B11GEMProbability() :
38  G4GEMProbability(11,5,3.0/2.0) // A,Z,Spin
39{
40    ExcitEnergies.push_back(2124.693*keV);
41    ExcitSpins.push_back(1.0/2.0);
42    ExcitLifetimes.push_back(3.8e-15*s);
43
44    ExcitEnergies.push_back(4444.89*keV);
45    ExcitSpins.push_back(5.0/2.0);
46    ExcitLifetimes.push_back(0.82e-15*s);
47
48    ExcitEnergies.push_back(5020.31*keV);
49    ExcitSpins.push_back(3.0/2.0);
50    ExcitLifetimes.push_back(0.236e-15*s);
51
52    ExcitEnergies.push_back(6742.9*keV);
53    ExcitSpins.push_back(7.0/2.0);
54    ExcitLifetimes.push_back(15.0e-15*s);
55
56    ExcitEnergies.push_back(6791.8*keV);
57    ExcitSpins.push_back(1.0/2.0);
58    ExcitLifetimes.push_back(1.18e-15*s);
59
60    ExcitEnergies.push_back(7285.51*keV);
61    ExcitSpins.push_back(5.0/2.0);
62    ExcitLifetimes.push_back(0.4e-15*s);
63
64    ExcitEnergies.push_back(7977.84*keV);
65    ExcitSpins.push_back(3.0/2.0);
66    ExcitLifetimes.push_back(0.4e-15*s);
67
68    ExcitEnergies.push_back(8560.3*keV);
69    ExcitSpins.push_back(5.0/2.0);
70    ExcitLifetimes.push_back(0.49e-15*s);
71
72    ExcitEnergies.push_back(8920.2*keV);
73    ExcitSpins.push_back(5.0/2.0);
74    ExcitLifetimes.push_back(4.4e-15*s);
75
76    ExcitEnergies.push_back(9185.0*keV);
77    ExcitSpins.push_back(7.0/2.0);
78    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.9*eV));
79
80    ExcitEnergies.push_back(9274.4*keV);
81    ExcitSpins.push_back(5.0/2.0);
82    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4.0*keV));
83
84    ExcitEnergies.push_back(9876.0*keV);
85    ExcitSpins.push_back(3.0/2.0);
86    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(110.0*keV));
87
88    ExcitEnergies.push_back(10260.0*keV);
89    ExcitSpins.push_back(3.0/2.0);
90    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(165.0*keV));
91
92    ExcitEnergies.push_back(10330.0*keV);
93    ExcitSpins.push_back(5.0/2.0);
94    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(110.0*keV));
95
96    ExcitEnergies.push_back(10597.0*keV);
97    ExcitSpins.push_back(7.0/2.0);
98    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV));
99
100    ExcitEnergies.push_back(10960.0*keV);
101    ExcitSpins.push_back(5.0/2.0);
102    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4500.0*keV));
103
104    ExcitEnergies.push_back(11265.0*keV);
105    ExcitSpins.push_back(9.0/2.0);
106    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(110.0*keV));
107
108    ExcitEnergies.push_back(11444.0*keV);
109    ExcitSpins.push_back(0.0);
110    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(103.0*keV));
111
112    ExcitEnergies.push_back(11886.0*keV);
113    ExcitSpins.push_back(5.0/2.0);
114    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200.0*keV));
115
116    ExcitEnergies.push_back(12.0e3*keV);
117    ExcitSpins.push_back(7.0/2.0);
118    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV));
119
120    ExcitEnergies.push_back(12557.0*keV);
121    ExcitSpins.push_back(1.0/2.0);
122    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(210.0*keV));
123
124    ExcitEnergies.push_back(12916.0*keV);
125    ExcitSpins.push_back(1.0/2.0);
126    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(155.0*keV));
127
128    ExcitEnergies.push_back(13137.0*keV);
129    ExcitSpins.push_back(9.0/2.0);
130    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(426.0*keV));
131
132    ExcitEnergies.push_back(13.16e3*keV);
133    ExcitSpins.push_back(7.0/2.0);
134    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(430.0*keV));
135
136    ExcitEnergies.push_back(14.04e3*keV);
137    ExcitSpins.push_back(11.0/2.0);
138    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500.0*keV));
139
140    ExcitEnergies.push_back(14.34e3*keV);
141    ExcitSpins.push_back(5.0/2.0);
142    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(254.0*keV));
143
144    ExcitEnergies.push_back(14565.0*keV);
145    ExcitSpins.push_back(0.0);
146    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30.0*keV));
147
148    ExcitEnergies.push_back(15.32e3*keV);
149    ExcitSpins.push_back(5.0/2.0);
150    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(635.0*keV));
151
152    ExcitEnergies.push_back(16437.0*keV);
153    ExcitSpins.push_back(5.0/2.0);
154    ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30.0*keV));
155
156    SetExcitationEnergiesPtr(&ExcitEnergies);
157    SetExcitationSpinsPtr(&ExcitSpins);
158    SetExcitationLifetimesPtr(&ExcitLifetimes);
159}
160
161
162G4B11GEMProbability::G4B11GEMProbability(const G4B11GEMProbability &): G4GEMProbability()
163{
164  throw G4HadronicException(__FILE__, __LINE__, "G4B11GEMProbability::copy_constructor meant to not be accessable");}
165
166
167
168
169const G4B11GEMProbability & G4B11GEMProbability::
170operator=(const G4B11GEMProbability &)
171{
172  throw G4HadronicException(__FILE__, __LINE__, "G4B11GEMProbability::operator= meant to not be accessable");
173  return *this;
174}
175
176
177G4bool G4B11GEMProbability::operator==(const G4B11GEMProbability &) const
178{
179  return false;
180}
181
182G4bool G4B11GEMProbability::operator!=(const G4B11GEMProbability &) const
183{
184  return true;
185}
186
187
188
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