Geant4-11
G4O17GEMProbability.cc
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26//
27// Hadronic Process: Nuclear De-excitations
28// by V. Lara (Nov 1999)
29//
30
31#include "G4O17GEMProbability.hh"
32#include "G4PhysicalConstants.hh"
33#include "G4SystemOfUnits.hh"
34#include "G4Log.hh"
35
36G4O17GEMProbability::G4O17GEMProbability() :
37 G4GEMProbability(17,9,5.0/2.0) // A,Z,Spin
38{
39
40 ExcitEnergies.push_back(870.81*keV);
41 ExcitSpins.push_back(1.0/2.0);
42 ExcitLifetimes.push_back(179.2*picosecond);
43
44 ExcitEnergies.push_back(3055.2*keV);
45 ExcitSpins.push_back(1.0/2.0);
46 ExcitLifetimes.push_back(83.0E-3*picosecond);
47
48 ExcitEnergies.push_back(3841.0*keV);
49 ExcitSpins.push_back(5.0/2.0);
50 ExcitLifetimes.push_back(17.0E-3*picosecond);
51
52 ExcitEnergies.push_back(4553.0*keV);
53 ExcitSpins.push_back(3.0/2.0);
54 ExcitLifetimes.push_back(fPlanck/(40.0*keV));
55
56 ExcitEnergies.push_back(5086.0*keV);
57 ExcitSpins.push_back(3.0/2.0);
58 ExcitLifetimes.push_back(fPlanck/(95.0*keV));
59
60 ExcitEnergies.push_back(5380.0*keV);
61 ExcitSpins.push_back(3.0/2.0);
62 ExcitLifetimes.push_back(fPlanck/(28.0*keV));
63
64 ExcitEnergies.push_back(5698.0*keV);
65 ExcitSpins.push_back(7.0/2.0);
66 ExcitLifetimes.push_back(fPlanck/(3.4*keV));
67
68 ExcitEnergies.push_back(5870.0*keV);
69 ExcitSpins.push_back(3.0/2.0);
70 ExcitLifetimes.push_back(fPlanck/(6.6*keV));
71
72 ExcitEnergies.push_back(5940.0*keV);
73 ExcitSpins.push_back(1.0/2.0);
74 ExcitLifetimes.push_back(fPlanck/(32.0*keV));
75
76 ExcitEnergies.push_back(6357.0*keV);
77 ExcitSpins.push_back(1.0/2.0);
78 ExcitLifetimes.push_back(fPlanck/(124.0*keV));
79
80 ExcitEnergies.push_back(7168.7*keV);
81 ExcitSpins.push_back(5.0/2.0);
82 ExcitLifetimes.push_back(fPlanck/(1.5*keV));
83
84 ExcitEnergies.push_back(7202.0*keV);
85 ExcitSpins.push_back(3.0/2.0);
86 ExcitLifetimes.push_back(fPlanck/(280.0*keV));
87
88 ExcitEnergies.push_back(7383.1*keV);
89 ExcitSpins.push_back(5.0/2.0);
90 ExcitLifetimes.push_back(fPlanck/(0.6*keV));
91
92 ExcitEnergies.push_back(7386.0*keV);
93 ExcitSpins.push_back(5.0/2.0);
94 ExcitLifetimes.push_back(fPlanck/(0.9*keV));
95
96 ExcitEnergies.push_back(7560.0*keV);
97 ExcitSpins.push_back(3.0/2.0);
98 ExcitLifetimes.push_back(fPlanck/(500.0*keV));
99
100 ExcitEnergies.push_back(7577.0*keV);
101 ExcitSpins.push_back(7.0/2.0);
102 ExcitLifetimes.push_back(fPlanck/(1.0*keV));
103
104 ExcitEnergies.push_back(7690.0*keV);
105 ExcitSpins.push_back(7.0/2.0);
106 ExcitLifetimes.push_back(fPlanck/(18.0*keV));
107
108 ExcitEnergies.push_back(7956.0*keV);
109 ExcitSpins.push_back(1.0/2.0);
110 ExcitLifetimes.push_back(fPlanck/(90.0*keV));
111
112 ExcitEnergies.push_back(7990.0*keV);
113 ExcitSpins.push_back(1.0/2.0);
114 ExcitLifetimes.push_back(fPlanck/(270.0*keV));
115
116 ExcitEnergies.push_back(8070.0*keV);
117 ExcitSpins.push_back(3.0/2.0);
118 ExcitLifetimes.push_back(fPlanck/(85.0*keV));
119
120 ExcitEnergies.push_back(8180.0*keV);
121 ExcitSpins.push_back(1.0/2.0);
122 ExcitLifetimes.push_back(fPlanck/(69.0*keV));
123
124 ExcitEnergies.push_back(8200.0*keV);
125 ExcitSpins.push_back(3.0/2.0);
126 ExcitLifetimes.push_back(fPlanck/(60.0*keV));
127
128 ExcitEnergies.push_back(8352.0*keV);
129 ExcitSpins.push_back(1.0/2.0);
130 ExcitLifetimes.push_back(fPlanck/(9.0*keV));
131
132 ExcitEnergies.push_back(8410.0*keV);
133 ExcitSpins.push_back(5.0/2.0);
134 ExcitLifetimes.push_back(fPlanck/(4.0*keV));
135
136 ExcitEnergies.push_back(8474.0*keV);
137 ExcitSpins.push_back(7.0/2.0);
138 ExcitLifetimes.push_back(fPlanck/(7.0*keV));
139
140 ExcitEnergies.push_back(8508.0*keV);
141 ExcitSpins.push_back(5.0/2.0);
142 ExcitLifetimes.push_back(hbar_Planck*G4Log(2.0)/(5.0*keV));
143
144 ExcitEnergies.push_back(8700.0*keV);
145 ExcitSpins.push_back(3.0/2.0);
146 ExcitLifetimes.push_back(fPlanck/(50.0*keV));
147
148 ExcitEnergies.push_back(8898.0*keV);
149 ExcitSpins.push_back(3.0/2.0);
150 ExcitLifetimes.push_back(fPlanck/(101.0*keV));
151
152 ExcitEnergies.push_back(8972.0*keV);
153 ExcitSpins.push_back(7.0/2.0);
154 ExcitLifetimes.push_back(fPlanck/(21.0*keV));
155
156 ExcitEnergies.push_back(9148.0*keV);
157 ExcitSpins.push_back(1.0/2.0);
158 ExcitLifetimes.push_back(fPlanck/(4.0*keV));
159
160 ExcitEnergies.push_back(9187.0*keV);
161 ExcitSpins.push_back(7.0/2.0);
162 ExcitLifetimes.push_back(fPlanck/(3.0*keV));
163
164 ExcitEnergies.push_back(9201.0*keV);
165 ExcitSpins.push_back(5.0/2.0);
166 ExcitLifetimes.push_back(fPlanck/(5.5*keV));
167
168 ExcitEnergies.push_back(9422.0*keV);
169 ExcitSpins.push_back(3.0/2.0);
170 ExcitLifetimes.push_back(fPlanck/(120.0*keV));
171
172 ExcitEnergies.push_back(9493.0*keV);
173 ExcitSpins.push_back(5.0/2.0);
174 ExcitLifetimes.push_back(hbar_Planck*G4Log(2.0)/(15.0*keV));
175
176 ExcitEnergies.push_back(9720.0*keV);
177 ExcitSpins.push_back(7.0/2.0);
178 ExcitLifetimes.push_back(fPlanck/(16.0*keV));
179
180 ExcitEnergies.push_back(9775.0*keV);
181 ExcitSpins.push_back(3.0/2.0);
182 ExcitLifetimes.push_back(fPlanck/(25.0*keV));
183
184 ExcitEnergies.push_back(9977.0*keV);
185 ExcitSpins.push_back(5.0/2.0);
186 ExcitLifetimes.push_back(fPlanck/(80.0*keV));
187
188 ExcitEnergies.push_back(10178.0*keV);
189 ExcitSpins.push_back(7.0/2.0);
190 ExcitLifetimes.push_back(fPlanck/(40.0*keV));
191
192 ExcitEnergies.push_back(10337.0*keV);
193 ExcitSpins.push_back(5.0/2.0);
194 ExcitLifetimes.push_back(fPlanck/(150.0*keV));
195
196 ExcitEnergies.push_back(10490.0*keV);
197 ExcitSpins.push_back(5.0/2.0);
198 ExcitLifetimes.push_back(fPlanck/(75.0*keV));
199
200 ExcitEnergies.push_back(10773.0*keV);
201 ExcitSpins.push_back(1.0/2.0);
202 ExcitLifetimes.push_back(fPlanck/(80.0*keV));
203
204 ExcitEnergies.push_back(10910.0*keV);
205 ExcitSpins.push_back(5.0/2.0);
206 ExcitLifetimes.push_back(fPlanck/(57.0*keV));
207
208 ExcitEnergies.push_back(11076.0*keV);
209 ExcitSpins.push_back(1.0/2.0);
210 ExcitLifetimes.push_back(fPlanck/(5.0*keV));
211
212 ExcitEnergies.push_back(12946.0*keV);
213 ExcitSpins.push_back(1.0/2.0);
214 ExcitLifetimes.push_back(fPlanck/(6.0*keV));
215
216 ExcitEnergies.push_back(14980.0*keV);
217 ExcitSpins.push_back(5.0/2.0);
218 ExcitLifetimes.push_back(fPlanck/(150.0*keV));
219
220 ExcitEnergies.push_back(21.7E3*keV);
221 ExcitSpins.push_back(5.0/2.0);
222 ExcitLifetimes.push_back(fPlanck/(750.0*keV));
223
224 ExcitEnergies.push_back(22.1E3*keV);
225 ExcitSpins.push_back(7.0/2.0);
226 ExcitLifetimes.push_back(fPlanck/(750.0*keV));
227
228 ExcitEnergies.push_back(22.5E3*keV);
229 ExcitSpins.push_back(3.0/2.0);
230 ExcitLifetimes.push_back(fPlanck/(1000.0*keV));
231
232 ExcitEnergies.push_back(23.0E3*keV);
233 ExcitSpins.push_back(1.0/2.0);
234 ExcitLifetimes.push_back(fPlanck/(400.0*keV));
235}
236
237G4O17GEMProbability::~G4O17GEMProbability()
238{}
G4Log
G4double G4Log(G4double x)
Definition: G4Log.hh:226
keV
static constexpr double keV
Definition: G4SIunits.hh:202
picosecond
static constexpr double picosecond
Definition: G4SIunits.hh:141
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
source.hepunit.hbar_Planck
float hbar_Planck
Definition: hepunit.py:263
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