Geant4 11.1.1
Toolkit for the simulation of the passage of particles through matter
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G4O15GEMProbability.cc
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1//
2// ********************************************************************
3// * License and Disclaimer *
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6// * the Geant4 Collaboration. It is provided under the terms and *
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9// * include a list of copyright holders. *
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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 *
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18// * This code implementation is the result of the scientific and *
19// * technical work of the GEANT4 collaboration. *
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25//
26//
27// Hadronic Process: Nuclear De-excitations
28// by V. Lara (Nov 1999)
29//
30
31#include "G4O15GEMProbability.hh"
32#include "G4SystemOfUnits.hh"
33
34G4O15GEMProbability::G4O15GEMProbability() :
35 G4GEMProbability(15,8,1.0/2.0) // A,Z,Spin
36{
37
38 ExcitEnergies.push_back(5183.0*keV);
39 ExcitSpins.push_back(1.0/2.0);
40 ExcitLifetimes.push_back(0.07*picosecond);
41
42 ExcitEnergies.push_back(5240.9*keV);
43 ExcitSpins.push_back(5.0/2.0);
44 ExcitLifetimes.push_back(2.2*picosecond);
45
46 ExcitEnergies.push_back(6176.3*keV);
47 ExcitSpins.push_back(3.0/2.0);
48 ExcitLifetimes.push_back(33.0E-3*picosecond);
49
50 ExcitEnergies.push_back(6793.1*keV);
51 ExcitSpins.push_back(3.0/2.0);
52 ExcitLifetimes.push_back(19.0E-3*picosecond);
53
54 ExcitEnergies.push_back(6859.4*keV);
55 ExcitSpins.push_back(5.0/2.0);
56 ExcitLifetimes.push_back(0.07*picosecond);
57
58 ExcitEnergies.push_back(7556.8*keV);
59 ExcitSpins.push_back(1.0/2.0);
60 ExcitLifetimes.push_back(fPlanck/(1.6*keV));
61
62 ExcitEnergies.push_back(8284.3*keV);
63 ExcitSpins.push_back(3.0/2.0);
64 ExcitLifetimes.push_back(fPlanck/(3.6*keV));
65
66 ExcitEnergies.push_back(8743.0*keV);
67 ExcitSpins.push_back(1.0/2.0);
68 ExcitLifetimes.push_back(fPlanck/(32.0*keV));
69
70 ExcitEnergies.push_back(8922.0*keV);
71 ExcitSpins.push_back(5.0/2.0);
72 ExcitLifetimes.push_back(fPlanck/(4.0*keV));
73
74 ExcitEnergies.push_back(8927.0*keV);
75 ExcitSpins.push_back(1.0/2.0);
76 ExcitLifetimes.push_back(fPlanck/(4.0*keV));
77
78 ExcitEnergies.push_back(8982.4*keV);
79 ExcitSpins.push_back(1.0/2.0);
80 ExcitLifetimes.push_back(fPlanck/(3.9*keV));
81
82 ExcitEnergies.push_back(9487.0*keV);
83 ExcitSpins.push_back(5.0/2.0);
84 ExcitLifetimes.push_back(fPlanck/(10.1*keV));
85
86 ExcitEnergies.push_back(9527.0*keV);
87 ExcitSpins.push_back(1.0/2.0);
88 ExcitLifetimes.push_back(fPlanck/(280.0*keV));
89
90 ExcitEnergies.push_back(9610.0*keV);
91 ExcitSpins.push_back(3.0/2.0);
92 ExcitLifetimes.push_back(fPlanck/(8.8*keV));
93
94 ExcitEnergies.push_back(9662.0*keV);
95 ExcitSpins.push_back(7.0/2.0);
96 ExcitLifetimes.push_back(fPlanck/(2.0*keV));
97
98 ExcitEnergies.push_back(9720.0*keV);
99 ExcitSpins.push_back(1.0/2.0);
100 ExcitLifetimes.push_back(fPlanck/(1185.0*keV));
101
102 ExcitEnergies.push_back(10291.0*keV);
103 ExcitSpins.push_back(5.0/2.0);
104 ExcitLifetimes.push_back(fPlanck/(3.0*keV));
105
106 ExcitEnergies.push_back(10296.0*keV);
107 ExcitSpins.push_back(5.0/2.0);
108 ExcitLifetimes.push_back(fPlanck/(11.0*keV));
109
110 ExcitEnergies.push_back(10478.0*keV);
111 ExcitSpins.push_back(3.0/2.0);
112 ExcitLifetimes.push_back(fPlanck/(25.0*keV));
113
114 ExcitEnergies.push_back(10506.0*keV);
115 ExcitSpins.push_back(3.0/2.0);
116 ExcitLifetimes.push_back(fPlanck/(140.0*keV));
117
118 ExcitEnergies.push_back(10917.0*keV);
119 ExcitSpins.push_back(7.0/2.0);
120 ExcitLifetimes.push_back(fPlanck/(90.0*keV));
121
122 ExcitEnergies.push_back(10938.0*keV);
123 ExcitSpins.push_back(1.0/2.0);
124 ExcitLifetimes.push_back(fPlanck/(99.0*keV));
125
126 ExcitEnergies.push_back(11025.0*keV);
127 ExcitSpins.push_back(1.0/2.0);
128 ExcitLifetimes.push_back(fPlanck/(25.0*keV));
129
130 ExcitEnergies.push_back(11218.0*keV);
131 ExcitSpins.push_back(3.0/2.0);
132 ExcitLifetimes.push_back(fPlanck/(40.0*keV));
133
134 ExcitEnergies.push_back(11569.0*keV);
135 ExcitSpins.push_back(5.0/2.0);
136 ExcitLifetimes.push_back(fPlanck/(20.0*keV));
137
138 ExcitEnergies.push_back(11616.0*keV);
139 ExcitSpins.push_back(3.0/2.0);
140 ExcitLifetimes.push_back(fPlanck/(80.0*keV));
141
142 ExcitEnergies.push_back(11748.0*keV);
143 ExcitSpins.push_back(5.0/2.0);
144 ExcitLifetimes.push_back(fPlanck/(99.0*keV));
145
146 ExcitEnergies.push_back(11846.0*keV);
147 ExcitSpins.push_back(5.0/2.0);
148 ExcitLifetimes.push_back(fPlanck/(65.0*keV));
149
150 ExcitEnergies.push_back(11980.0*keV);
151 ExcitSpins.push_back(5.0/2.0);
152 ExcitLifetimes.push_back(fPlanck/(20.0*keV));
153
154 ExcitEnergies.push_back(12129.0*keV);
155 ExcitSpins.push_back(5.0/2.0);
156 ExcitLifetimes.push_back(fPlanck/(200.0*keV));
157
158 ExcitEnergies.push_back(12471.0*keV);
159 ExcitSpins.push_back(5.0/2.0);
160 ExcitLifetimes.push_back(fPlanck/(77.0*keV));
161
162 ExcitEnergies.push_back(12835.0*keV);
163 ExcitSpins.push_back(1.0/2.0);
164 ExcitLifetimes.push_back(fPlanck/(16.0*keV));
165
166 ExcitEnergies.push_back(13450.0*keV);
167 ExcitSpins.push_back(1.0/2.0);
168 ExcitLifetimes.push_back(fPlanck/(1000.0*keV));
169
170 ExcitEnergies.push_back(14030.0*keV);
171 ExcitSpins.push_back(1.0/2.0);
172 ExcitLifetimes.push_back(fPlanck/(160.0*keV));
173
174 ExcitEnergies.push_back(14270.0*keV);
175 ExcitSpins.push_back(1.0/2.0);
176 ExcitLifetimes.push_back(fPlanck/(340.0*keV));
177
178 ExcitEnergies.push_back(14465.0*keV);
179 ExcitSpins.push_back(3.0/2.0);
180 ExcitLifetimes.push_back(fPlanck/(100.0*keV));
181
182 ExcitEnergies.push_back(15100.0*keV);
183 ExcitSpins.push_back(1.0/2.0);
184 ExcitLifetimes.push_back(fPlanck/(1000.0*keV));
185
186 ExcitEnergies.push_back(15900.0*keV);
187 ExcitSpins.push_back(1.0/2.0);
188 ExcitLifetimes.push_back(fPlanck/(350.0*keV));
189
190 ExcitEnergies.push_back(16430.0*keV);
191 ExcitSpins.push_back(1.0/2.0);
192 ExcitLifetimes.push_back(fPlanck/(560.0*keV));
193
194 ExcitEnergies.push_back(16900.0*keV);
195 ExcitSpins.push_back(1.0/2.0);
196 ExcitLifetimes.push_back(fPlanck/(1000.0*keV));
197
198 ExcitEnergies.push_back(17510.0*keV);
199 ExcitSpins.push_back(1.0/2.0);
200 ExcitLifetimes.push_back(fPlanck/(600.0*keV));
201
202 ExcitEnergies.push_back(17990.0*keV);
203 ExcitSpins.push_back(1.0/2.0);
204 ExcitLifetimes.push_back(fPlanck/(200.0*keV));
205
206 ExcitEnergies.push_back(18400.0*keV);
207 ExcitSpins.push_back(1.0/2.0);
208 ExcitLifetimes.push_back(fPlanck/(1000.0*keV));
209
210 ExcitEnergies.push_back(20500.0*keV);
211 ExcitSpins.push_back(1.0/2.0);
212 ExcitLifetimes.push_back(fPlanck/(2000.0*keV));
213
214 ExcitEnergies.push_back(22000.0*keV);
215 ExcitSpins.push_back(1.0/2.0);
216 ExcitLifetimes.push_back(fPlanck/(2000.0*keV));
217
218 ExcitEnergies.push_back(26000.0*keV);
219 ExcitSpins.push_back(13.0/2.0);
220 ExcitLifetimes.push_back(fPlanck/(600.0*keV));
221
222 ExcitEnergies.push_back(28000.0*keV);
223 ExcitSpins.push_back(9.0/2.0);
224 ExcitLifetimes.push_back(fPlanck/(2500.0*keV));
225}
226
227G4O15GEMProbability::~G4O15GEMProbability()
228{}
G4GEMProbability::ExcitSpins
std::vector< G4double > ExcitSpins
Definition: G4GEMProbability.hh:117
G4GEMProbability::ExcitEnergies
std::vector< G4double > ExcitEnergies
Definition: G4GEMProbability.hh:114
G4GEMProbability::ExcitLifetimes
std::vector< G4double > ExcitLifetimes
Definition: G4GEMProbability.hh:120