Geant4 11.2.2
Toolkit for the simulation of the passage of particles through matter
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G4C12GEMProbability.cc
Go to the documentation of this file.
1//
2// ********************************************************************
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6// * the Geant4 Collaboration. It is provided under the terms and *
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14// * regarding this software system or assume any liability for its *
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25//
26//
27// Hadronic Process: Nuclear De-excitations
28// by V. Lara (Nov 1999)
29//
30
31#include "G4C12GEMProbability.hh"
32#include "G4SystemOfUnits.hh"
33
34G4C12GEMProbability::G4C12GEMProbability() :
35 G4GEMProbability(12,6,0.0) // A,Z,Spin
36{
37
38 ExcitEnergies.push_back(4438.91*keV);
39 ExcitSpins.push_back(2.0);
40 ExcitLifetimes.push_back(fPlanck/(10.8e-3*eV));
41
42 ExcitEnergies.push_back(7654.2*keV);
43 ExcitSpins.push_back(0.0);
44 ExcitLifetimes.push_back(fPlanck/(8.5*keV));
45
46 ExcitEnergies.push_back(9641*keV);
47 ExcitSpins.push_back(3.0);
48 ExcitLifetimes.push_back(fPlanck/(34*keV));
49
50 ExcitEnergies.push_back(1.03E+4*keV);
51 ExcitSpins.push_back(0.0);
52 ExcitLifetimes.push_back(fPlanck/(3.0e3*keV));
53
54 ExcitEnergies.push_back(10844*keV);
55 ExcitSpins.push_back(1.0);
56 ExcitLifetimes.push_back(fPlanck/(315*keV));
57
58 ExcitEnergies.push_back(1.116E+4*keV);
59 ExcitSpins.push_back(2.0);
60 ExcitLifetimes.push_back(fPlanck/(430*keV));
61
62 ExcitEnergies.push_back(1.1828E+4*keV);
63 ExcitSpins.push_back(2.0);
64 ExcitLifetimes.push_back(fPlanck/(260*keV));
65
66 ExcitEnergies.push_back(12710*keV);
67 ExcitSpins.push_back(1.0);
68 ExcitLifetimes.push_back(fPlanck/(18.1*eV));
69
70 ExcitEnergies.push_back(13352*keV);
71 ExcitSpins.push_back(2.0);
72 ExcitLifetimes.push_back(fPlanck/(375*keV));
73
74 ExcitEnergies.push_back(14083*keV);
75 ExcitSpins.push_back(4.0);
76 ExcitLifetimes.push_back(fPlanck/(258*keV));
77
78 ExcitEnergies.push_back(15110*keV);
79 ExcitSpins.push_back(1.0);
80 ExcitLifetimes.push_back(fPlanck/(42*eV));
81
82 ExcitEnergies.push_back(16105.8*keV);
83 ExcitSpins.push_back(2.0);
84 ExcitLifetimes.push_back(fPlanck/(5.2*keV));
85
86 ExcitEnergies.push_back(16.57E+3*keV);
87 ExcitSpins.push_back(2.0);
88 ExcitLifetimes.push_back(fPlanck/(300*keV));
89
90 ExcitEnergies.push_back(17.23E+3*keV);
91 ExcitSpins.push_back(1.0);
92 ExcitLifetimes.push_back(fPlanck/(1150*keV));
93
94 ExcitEnergies.push_back(17.76E+3*keV);
95 ExcitSpins.push_back(0.0);
96 ExcitLifetimes.push_back(fPlanck/(80*keV));
97
98 ExcitEnergies.push_back(18.13E+3*keV);
99 ExcitSpins.push_back(1.0);
100 ExcitLifetimes.push_back(fPlanck/(600*keV));
101
102 ExcitEnergies.push_back(18.27E+3*keV);
103 ExcitSpins.push_back(4.0);
104 ExcitLifetimes.push_back(fPlanck/(300*keV));
105
106 ExcitEnergies.push_back(18.38E+3*keV);
107 ExcitSpins.push_back(3.0);
108 ExcitLifetimes.push_back(fPlanck/(220*keV));
109
110 ExcitEnergies.push_back(18.39E+3*keV);
111 ExcitSpins.push_back(2.0);
112 ExcitLifetimes.push_back(fPlanck/(43*keV));
113
114 ExcitEnergies.push_back(18.6E+3*keV);
115 ExcitSpins.push_back(3.0);
116 ExcitLifetimes.push_back(fPlanck/(300*keV));
117
118 ExcitEnergies.push_back(18.80E+3*keV);
119 ExcitSpins.push_back(2.0);
120 ExcitLifetimes.push_back(fPlanck/(100*keV));
121
122 ExcitEnergies.push_back(19.2E+3*keV);
123 ExcitSpins.push_back(1.0);
124 ExcitLifetimes.push_back(fPlanck/(1100*keV));
125
126 ExcitEnergies.push_back(19.39E+3*keV);
127 ExcitSpins.push_back(2.0);
128 ExcitLifetimes.push_back(fPlanck/(800*keV));
129
130 ExcitEnergies.push_back(19.55E+3*keV);
131 ExcitSpins.push_back(4.0);
132 ExcitLifetimes.push_back(fPlanck/(490*keV));
133
134 ExcitEnergies.push_back(19.69E+3*keV);
135 ExcitSpins.push_back(1.0);
136 ExcitLifetimes.push_back(fPlanck/(230*keV));
137
138 ExcitEnergies.push_back(20.0E+3*keV);
139 ExcitSpins.push_back(2.0);
140 ExcitLifetimes.push_back(fPlanck/(100*keV));
141
142 ExcitEnergies.push_back(20.27E+3*keV);
143 ExcitSpins.push_back(1.0);
144 ExcitLifetimes.push_back(fPlanck/(140*keV));
145
146 ExcitEnergies.push_back(20.5E+3*keV);
147 ExcitSpins.push_back(3.0);
148 ExcitLifetimes.push_back(fPlanck/(180*keV));
149
150 ExcitEnergies.push_back(20.62E+3*keV);
151 ExcitSpins.push_back(3.0);
152 ExcitLifetimes.push_back(fPlanck/(200*keV));
153
154 ExcitEnergies.push_back(21.60E+3*keV);
155 ExcitSpins.push_back(2.0);
156 ExcitLifetimes.push_back(fPlanck/(1200*keV));
157
158 ExcitEnergies.push_back(22.0E+3*keV);
159 ExcitSpins.push_back(1.0);
160 ExcitLifetimes.push_back(fPlanck/(800*keV));
161
162 ExcitEnergies.push_back(22.40E+3*keV);
163 ExcitSpins.push_back(1.0);
164 ExcitLifetimes.push_back(fPlanck/(275*keV));
165
166 ExcitEnergies.push_back(22.65E+3*keV);
167 ExcitSpins.push_back(1.0);
168 ExcitLifetimes.push_back(fPlanck/(3200*keV));
169
170 ExcitEnergies.push_back(23.04E+3 *keV);
171 ExcitSpins.push_back(2.0);
172 ExcitLifetimes.push_back(fPlanck/(60*keV));
173
174 ExcitEnergies.push_back(23.52E+3*keV);
175 ExcitSpins.push_back(1.0);
176 ExcitLifetimes.push_back(fPlanck/(230*keV));
177
178 ExcitEnergies.push_back(23.92E+3*keV);
179 ExcitSpins.push_back(1.0);
180 ExcitLifetimes.push_back(fPlanck/(400*keV));
181
182 ExcitEnergies.push_back(25.30E+3*keV);
183 ExcitSpins.push_back(1.0);
184 ExcitLifetimes.push_back(fPlanck/(510*keV));
185
186 ExcitEnergies.push_back(25.4E+3*keV);
187 ExcitSpins.push_back(1.0);
188 ExcitLifetimes.push_back(fPlanck/(2000*keV));
189
190 ExcitEnergies.push_back(27.0E+3*keV);
191 ExcitSpins.push_back(1.0);
192 ExcitLifetimes.push_back(fPlanck/(1400*keV));
193
194 ExcitEnergies.push_back(27595.0*keV);
195 ExcitSpins.push_back(0.0);
196 ExcitLifetimes.push_back(fPlanck/(30*keV));
197
198 ExcitEnergies.push_back(28.2E+3*keV);
199 ExcitSpins.push_back(1.0);
200 ExcitLifetimes.push_back(fPlanck/(1600*keV));
201}
202
G4GEMProbability::ExcitSpins
std::vector< G4double > ExcitSpins
Definition G4GEMProbability.hh:124
G4GEMProbability::ExcitEnergies
std::vector< G4double > ExcitEnergies
Definition G4GEMProbability.hh:121
G4GEMProbability::ExcitLifetimes
std::vector< G4double > ExcitLifetimes
Definition G4GEMProbability.hh:127