Geant4-11
G4F20GEMProbability.cc
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26//
27// Hadronic Process: Nuclear De-excitations
28// by V. Lara (Nov 1999)
29//
30
31#include "G4F20GEMProbability.hh"
32#include "G4PhysicalConstants.hh"
33#include "G4SystemOfUnits.hh"
34#include "G4Log.hh"
35
36G4F20GEMProbability::G4F20GEMProbability() :
37 G4GEMProbability(20,9,2.0) // A,Z,Spin
38{
39
40 ExcitEnergies.push_back(655.95*keV);
41 ExcitSpins.push_back(3.0);
42 ExcitLifetimes.push_back(0.28*picosecond);
43
44 ExcitEnergies.push_back(822.9*keV);
45 ExcitSpins.push_back(4.0);
46 ExcitLifetimes.push_back(55*picosecond);
47
48 ExcitEnergies.push_back(983.8*keV);
49 ExcitSpins.push_back(3.0);
50 ExcitLifetimes.push_back(1.1*picosecond);
51
52 ExcitEnergies.push_back(1056.93*keV);
53 ExcitSpins.push_back(1.0);
54 ExcitLifetimes.push_back(31.0e-3*picosecond);
55
56 ExcitEnergies.push_back(1309.22*keV);
57 ExcitSpins.push_back(2.0);
58 ExcitLifetimes.push_back(0.62*picosecond);
59
60 ExcitEnergies.push_back(1843.4*keV);
61 ExcitSpins.push_back(2.0);
62 ExcitLifetimes.push_back(21.0e-3*picosecond);
63
64 ExcitEnergies.push_back(2043.9*keV);
65 ExcitSpins.push_back(2.0);
66 ExcitLifetimes.push_back(26.0e-3*picosecond);
67
68 ExcitEnergies.push_back(2194.6*keV);
69 ExcitSpins.push_back(2.0);
70 ExcitLifetimes.push_back(8.0e-3*picosecond);
71
72 ExcitEnergies.push_back(2966.2*keV);
73 ExcitSpins.push_back(3.0);
74 ExcitLifetimes.push_back(42.0e-3*picosecond);
75
76 ExcitEnergies.push_back(3488.4*keV);
77 ExcitSpins.push_back(1.0);
78 ExcitLifetimes.push_back(30.0e-3*picosecond);
79
80 ExcitEnergies.push_back(3525.9*keV);
81 ExcitSpins.push_back(0.0);
82 ExcitLifetimes.push_back(21.0e-3*picosecond);
83
84 ExcitEnergies.push_back(3587.1*keV);
85 ExcitSpins.push_back(3.0);
86 ExcitLifetimes.push_back(21.0e-3*picosecond);
87
88 ExcitEnergies.push_back(6627.0*keV);
89 ExcitSpins.push_back(2.0);
90 ExcitLifetimes.push_back(hbar_Planck*G4Log(2.0)/(0.29*keV));
91
92 ExcitEnergies.push_back(6648.0*keV);
93 ExcitSpins.push_back(1.0);
94 ExcitLifetimes.push_back(fPlanck/(1.62*keV));
95
96 ExcitEnergies.push_back(6685.0*keV);
97 ExcitSpins.push_back(0.0);
98 ExcitLifetimes.push_back(fPlanck/(3.80*keV));
99
100 ExcitEnergies.push_back(6692.0*keV);
101 ExcitSpins.push_back(1.0);
102 ExcitLifetimes.push_back(fPlanck/(5.23*keV));
103
104 ExcitEnergies.push_back(6696.0*keV);
105 ExcitSpins.push_back(2.0);
106 ExcitLifetimes.push_back(fPlanck/(1.05*keV));
107
108 ExcitEnergies.push_back(6699.0*keV);
109 ExcitSpins.push_back(1.0);
110 ExcitLifetimes.push_back(fPlanck/(2.85*keV));
111
112 ExcitEnergies.push_back(6709.0*keV);
113 ExcitSpins.push_back(0.0);
114 ExcitLifetimes.push_back(fPlanck/(1.14*keV));
115
116 ExcitEnergies.push_back(6717.0*keV);
117 ExcitSpins.push_back(0.0);
118 ExcitLifetimes.push_back(fPlanck/(0.95*keV));
119
120 ExcitEnergies.push_back(6791.0*keV);
121 ExcitSpins.push_back(0.0);
122 ExcitLifetimes.push_back(fPlanck/(1.9*keV));
123
124 ExcitEnergies.push_back(6835.0*keV);
125 ExcitSpins.push_back(1.0);
126 ExcitLifetimes.push_back(fPlanck/(1.7*keV));
127
128 ExcitEnergies.push_back(6837.0*keV);
129 ExcitSpins.push_back(1.0);
130 ExcitLifetimes.push_back(fPlanck/(0.4*keV));
131
132 ExcitEnergies.push_back(6856.0*keV);
133 ExcitSpins.push_back(1.0);
134 ExcitLifetimes.push_back(fPlanck/(1.3*keV));
135
136 ExcitEnergies.push_back(6858.0*keV);
137 ExcitSpins.push_back(1.0);
138 ExcitLifetimes.push_back(fPlanck/(19.0*keV));
139
140 ExcitEnergies.push_back(7005.0*keV);
141 ExcitSpins.push_back(0.0);
142 ExcitLifetimes.push_back(fPlanck/(24.0*keV));
143
144 ExcitEnergies.push_back(7076.0*keV);
145 ExcitSpins.push_back(1.0);
146 ExcitLifetimes.push_back(fPlanck/(24.0*keV));
147
148 ExcitEnergies.push_back(7171.0*keV);
149 ExcitSpins.push_back(2.0);
150 ExcitLifetimes.push_back(fPlanck/(14.0*keV));
151
152 ExcitEnergies.push_back(7311.0*keV);
153 ExcitSpins.push_back(1.0);
154 ExcitLifetimes.push_back(fPlanck/(33.0*keV));
155
156 ExcitEnergies.push_back(7355.0*keV);
157 ExcitSpins.push_back(1.0);
158 ExcitLifetimes.push_back(fPlanck/(19.0*keV));
159
160 ExcitEnergies.push_back(7410.0*keV);
161 ExcitSpins.push_back(2.0);
162 ExcitLifetimes.push_back(fPlanck/(10.0*keV));
163
164 ExcitEnergies.push_back(7489.0*keV);
165 ExcitSpins.push_back(2.0);
166 ExcitLifetimes.push_back(fPlanck/(57.0*keV));
167
168 ExcitEnergies.push_back(7503.0*keV);
169 ExcitSpins.push_back(0.0);
170 ExcitLifetimes.push_back(fPlanck/(85.0*keV));
171
172 ExcitEnergies.push_back(7670.0*keV);
173 ExcitSpins.push_back(2.0);
174 ExcitLifetimes.push_back(fPlanck/(60.0*keV));
175
176 ExcitEnergies.push_back(7800.0*keV);
177 ExcitSpins.push_back(1.0);
178 ExcitLifetimes.push_back(fPlanck/(100.0*keV));
179
180 ExcitEnergies.push_back(8150.0*keV);
181 ExcitSpins.push_back(1.0);
182 ExcitLifetimes.push_back(fPlanck/(190.0*keV));
183
184 ExcitEnergies.push_back(10228.0*keV);
185 ExcitSpins.push_back(0.0);
186 ExcitLifetimes.push_back(fPlanck/(200.0*keV));
187
188 ExcitEnergies.push_back(10641.0*keV);
189 ExcitSpins.push_back(1.0);
190 ExcitLifetimes.push_back(fPlanck/(60.0*keV));
191
192 ExcitEnergies.push_back(10807.0*keV);
193 ExcitSpins.push_back(0.0);
194 ExcitLifetimes.push_back(fPlanck/(330.0*keV));
195
196}
197
198G4F20GEMProbability::~G4F20GEMProbability()
199{}
200
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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