Geant4 9.6.0
Toolkit for the simulation of the passage of particles through matter
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G4C12GEMProbability.cc
Go to the documentation of this file.
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25//
26// $Id$
27//
28// Hadronic Process: Nuclear De-excitations
29// by V. Lara (Nov 1999)
30//
31
32#include "G4C12GEMProbability.hh"
33#include "G4SystemOfUnits.hh"
34
35G4C12GEMProbability::G4C12GEMProbability() :
36 G4GEMProbability(12,6,0.0) // A,Z,Spin
37{
38
39 ExcitEnergies.push_back(4438.91*keV);
40 ExcitSpins.push_back(2.0);
41 ExcitLifetimes.push_back(fPlanck/(10.8e-3*eV));
42
43 ExcitEnergies.push_back(7654.2*keV);
44 ExcitSpins.push_back(0.0);
45 ExcitLifetimes.push_back(fPlanck/(8.5*keV));
46
47 ExcitEnergies.push_back(9641*keV);
48 ExcitSpins.push_back(3.0);
49 ExcitLifetimes.push_back(fPlanck/(34*keV));
50
51 ExcitEnergies.push_back(1.03E+4*keV);
52 ExcitSpins.push_back(0.0);
53 ExcitLifetimes.push_back(fPlanck/(3.0e3*keV));
54
55 ExcitEnergies.push_back(10844*keV);
56 ExcitSpins.push_back(1.0);
57 ExcitLifetimes.push_back(fPlanck/(315*keV));
58
59 ExcitEnergies.push_back(1.116E+4*keV);
60 ExcitSpins.push_back(2.0);
61 ExcitLifetimes.push_back(fPlanck/(430*keV));
62
63 ExcitEnergies.push_back(1.1828E+4*keV);
64 ExcitSpins.push_back(2.0);
65 ExcitLifetimes.push_back(fPlanck/(260*keV));
66
67 ExcitEnergies.push_back(12710*keV);
68 ExcitSpins.push_back(1.0);
69 ExcitLifetimes.push_back(fPlanck/(18.1*eV));
70
71 ExcitEnergies.push_back(13352*keV);
72 ExcitSpins.push_back(2.0);
73 ExcitLifetimes.push_back(fPlanck/(375*keV));
74
75 ExcitEnergies.push_back(14083*keV);
76 ExcitSpins.push_back(4.0);
77 ExcitLifetimes.push_back(fPlanck/(258*keV));
78
79 ExcitEnergies.push_back(15110*keV);
80 ExcitSpins.push_back(1.0);
81 ExcitLifetimes.push_back(fPlanck/(42*eV));
82
83 ExcitEnergies.push_back(16106.7*keV);
84 ExcitSpins.push_back(2.0);
85 ExcitLifetimes.push_back(fPlanck/(5.2*keV));
86
87 ExcitEnergies.push_back(16.57E+3*keV);
88 ExcitSpins.push_back(2.0);
89 ExcitLifetimes.push_back(fPlanck/(300*keV));
90
91 ExcitEnergies.push_back(17.23E+3*keV);
92 ExcitSpins.push_back(1.0);
93 ExcitLifetimes.push_back(fPlanck/(1150*keV));
94
95 ExcitEnergies.push_back(17.76E+3*keV);
96 ExcitSpins.push_back(0.0);
97 ExcitLifetimes.push_back(fPlanck/(80*keV));
98
99 ExcitEnergies.push_back(18.13E+3*keV);
100 ExcitSpins.push_back(1.0);
101 ExcitLifetimes.push_back(fPlanck/(600*keV));
102
103 ExcitEnergies.push_back(18.27E+3*keV);
104 ExcitSpins.push_back(4.0);
105 ExcitLifetimes.push_back(fPlanck/(300*keV));
106
107 ExcitEnergies.push_back(18.38E+3*keV);
108 ExcitSpins.push_back(3.0);
109 ExcitLifetimes.push_back(fPlanck/(220*keV));
110
111 ExcitEnergies.push_back(18.39E+3*keV);
112 ExcitSpins.push_back(2.0);
113 ExcitLifetimes.push_back(fPlanck/(43*keV));
114
115 ExcitEnergies.push_back(18.6E+3*keV);
116 ExcitSpins.push_back(3.0);
117 ExcitLifetimes.push_back(fPlanck/(300*keV));
118
119 ExcitEnergies.push_back(18.80E+3*keV);
120 ExcitSpins.push_back(2.0);
121 ExcitLifetimes.push_back(fPlanck/(100*keV));
122
123 ExcitEnergies.push_back(19.2E+3*keV);
124 ExcitSpins.push_back(1.0);
125 ExcitLifetimes.push_back(fPlanck/(1100*keV));
126
127 ExcitEnergies.push_back(19.39E+3*keV);
128 ExcitSpins.push_back(2.0);
129 ExcitLifetimes.push_back(fPlanck/(800*keV));
130
131 ExcitEnergies.push_back(19.55E+3*keV);
132 ExcitSpins.push_back(4.0);
133 ExcitLifetimes.push_back(fPlanck/(490*keV));
134
135 ExcitEnergies.push_back(19.69E+3*keV);
136 ExcitSpins.push_back(1.0);
137 ExcitLifetimes.push_back(fPlanck/(230*keV));
138
139 ExcitEnergies.push_back(20.0E+3*keV);
140 ExcitSpins.push_back(2.0);
141 ExcitLifetimes.push_back(fPlanck/(100*keV));
142
143 ExcitEnergies.push_back(20.27E+3*keV);
144 ExcitSpins.push_back(1.0);
145 ExcitLifetimes.push_back(fPlanck/(140*keV));
146
147 ExcitEnergies.push_back(20.5E+3*keV);
148 ExcitSpins.push_back(3.0);
149 ExcitLifetimes.push_back(fPlanck/(180*keV));
150
151 ExcitEnergies.push_back(20.62E+3*keV);
152 ExcitSpins.push_back(3.0);
153 ExcitLifetimes.push_back(fPlanck/(200*keV));
154
155 ExcitEnergies.push_back(21.60E+3*keV);
156 ExcitSpins.push_back(2.0);
157 ExcitLifetimes.push_back(fPlanck/(1200*keV));
158
159 ExcitEnergies.push_back(22.0E+3*keV);
160 ExcitSpins.push_back(1.0);
161 ExcitLifetimes.push_back(fPlanck/(800*keV));
162
163 ExcitEnergies.push_back(22.40E+3*keV);
164 ExcitSpins.push_back(1.0);
165 ExcitLifetimes.push_back(fPlanck/(275*keV));
166
167 ExcitEnergies.push_back(22.65E+3*keV);
168 ExcitSpins.push_back(1.0);
169 ExcitLifetimes.push_back(fPlanck/(3200*keV));
170
171 ExcitEnergies.push_back(23.04E+3 *keV);
172 ExcitSpins.push_back(2.0);
173 ExcitLifetimes.push_back(fPlanck/(60*keV));
174
175 ExcitEnergies.push_back(23.52E+3*keV);
176 ExcitSpins.push_back(1.0);
177 ExcitLifetimes.push_back(fPlanck/(230*keV));
178
179 ExcitEnergies.push_back(23.92E+3*keV);
180 ExcitSpins.push_back(1.0);
181 ExcitLifetimes.push_back(fPlanck/(400*keV));
182
183 ExcitEnergies.push_back(25.30E+3*keV);
184 ExcitSpins.push_back(1.0);
185 ExcitLifetimes.push_back(fPlanck/(510*keV));
186
187 ExcitEnergies.push_back(25.4E+3*keV);
188 ExcitSpins.push_back(1.0);
189 ExcitLifetimes.push_back(fPlanck/(2000*keV));
190
191 ExcitEnergies.push_back(27.0E+3*keV);
192 ExcitSpins.push_back(1.0);
193 ExcitLifetimes.push_back(fPlanck/(1400*keV));
194
195 ExcitEnergies.push_back(27595.0*keV);
196 ExcitSpins.push_back(0.0);
197 ExcitLifetimes.push_back(fPlanck/(30*keV));
198
199 ExcitEnergies.push_back(28.2E+3*keV);
200 ExcitSpins.push_back(1.0);
201 ExcitLifetimes.push_back(fPlanck/(1600*keV));
202}
203
204G4C12GEMProbability::~G4C12GEMProbability()
205{}
G4GEMProbability::ExcitSpins
std::vector< G4double > ExcitSpins
Definition: G4GEMProbability.hh:129
G4GEMProbability::ExcitEnergies
std::vector< G4double > ExcitEnergies
Definition: G4GEMProbability.hh:126
G4GEMProbability::ExcitLifetimes
std::vector< G4double > ExcitLifetimes
Definition: G4GEMProbability.hh:132