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G4F20GEMProbability.cc
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26 // $Id: G4F20GEMProbability.cc 74869 2013-10-23 09:26:17Z gcosmo $
27 //
28 // Hadronic Process: Nuclear De-excitations
29 // by V. Lara (Nov 1999)
30 //
31 
32 #include "G4F20GEMProbability.hh"
33 #include "G4PhysicalConstants.hh"
34 #include "G4SystemOfUnits.hh"
35 #include "G4Log.hh"
36 
37 G4F20GEMProbability::G4F20GEMProbability() :
38  G4GEMProbability(20,9,2.0) // A,Z,Spin
39 {
40 
41  ExcitEnergies.push_back(655.95*keV);
42  ExcitSpins.push_back(3.0);
43  ExcitLifetimes.push_back(0.28*picosecond);
44 
45  ExcitEnergies.push_back(822.9*keV);
46  ExcitSpins.push_back(4.0);
47  ExcitLifetimes.push_back(55*picosecond);
48 
49  ExcitEnergies.push_back(983.8*keV);
50  ExcitSpins.push_back(3.0);
51  ExcitLifetimes.push_back(1.1*picosecond);
52 
53  ExcitEnergies.push_back(1056.93*keV);
54  ExcitSpins.push_back(1.0);
55  ExcitLifetimes.push_back(31.0e-3*picosecond);
56 
57  ExcitEnergies.push_back(1309.22*keV);
58  ExcitSpins.push_back(2.0);
59  ExcitLifetimes.push_back(0.62*picosecond);
60 
61  ExcitEnergies.push_back(1843.4*keV);
62  ExcitSpins.push_back(2.0);
63  ExcitLifetimes.push_back(21.0e-3*picosecond);
64 
65  ExcitEnergies.push_back(2043.9*keV);
66  ExcitSpins.push_back(2.0);
67  ExcitLifetimes.push_back(26.0e-3*picosecond);
68 
69  ExcitEnergies.push_back(2194.6*keV);
70  ExcitSpins.push_back(2.0);
71  ExcitLifetimes.push_back(8.0e-3*picosecond);
72 
73  ExcitEnergies.push_back(2966.2*keV);
74  ExcitSpins.push_back(3.0);
75  ExcitLifetimes.push_back(42.0e-3*picosecond);
76 
77  ExcitEnergies.push_back(3488.4*keV);
78  ExcitSpins.push_back(1.0);
79  ExcitLifetimes.push_back(30.0e-3*picosecond);
80 
81  ExcitEnergies.push_back(3525.9*keV);
82  ExcitSpins.push_back(0.0);
83  ExcitLifetimes.push_back(21.0e-3*picosecond);
84 
85  ExcitEnergies.push_back(3587.1*keV);
86  ExcitSpins.push_back(3.0);
87  ExcitLifetimes.push_back(21.0e-3*picosecond);
88 
89  ExcitEnergies.push_back(6627.0*keV);
90  ExcitSpins.push_back(2.0);
91  ExcitLifetimes.push_back(hbar_Planck*G4Log(2.0)/(0.29*keV));
92 
93  ExcitEnergies.push_back(6648.0*keV);
94  ExcitSpins.push_back(1.0);
95  ExcitLifetimes.push_back(fPlanck/(1.62*keV));
96 
97  ExcitEnergies.push_back(6685.0*keV);
98  ExcitSpins.push_back(0.0);
99  ExcitLifetimes.push_back(fPlanck/(3.80*keV));
100 
101  ExcitEnergies.push_back(6692.0*keV);
102  ExcitSpins.push_back(1.0);
103  ExcitLifetimes.push_back(fPlanck/(5.23*keV));
104 
105  ExcitEnergies.push_back(6696.0*keV);
106  ExcitSpins.push_back(2.0);
107  ExcitLifetimes.push_back(fPlanck/(1.05*keV));
108 
109  ExcitEnergies.push_back(6699.0*keV);
110  ExcitSpins.push_back(1.0);
111  ExcitLifetimes.push_back(fPlanck/(2.85*keV));
112 
113  ExcitEnergies.push_back(6709.0*keV);
114  ExcitSpins.push_back(0.0);
115  ExcitLifetimes.push_back(fPlanck/(1.14*keV));
116 
117  ExcitEnergies.push_back(6717.0*keV);
118  ExcitSpins.push_back(0.0);
119  ExcitLifetimes.push_back(fPlanck/(0.95*keV));
120 
121  ExcitEnergies.push_back(6791.0*keV);
122  ExcitSpins.push_back(0.0);
123  ExcitLifetimes.push_back(fPlanck/(1.9*keV));
124 
125  ExcitEnergies.push_back(6835.0*keV);
126  ExcitSpins.push_back(1.0);
127  ExcitLifetimes.push_back(fPlanck/(1.7*keV));
128 
129  ExcitEnergies.push_back(6837.0*keV);
130  ExcitSpins.push_back(1.0);
131  ExcitLifetimes.push_back(fPlanck/(0.4*keV));
132 
133  ExcitEnergies.push_back(6856.0*keV);
134  ExcitSpins.push_back(1.0);
135  ExcitLifetimes.push_back(fPlanck/(1.3*keV));
136 
137  ExcitEnergies.push_back(6858.0*keV);
138  ExcitSpins.push_back(1.0);
139  ExcitLifetimes.push_back(fPlanck/(19.0*keV));
140 
141  ExcitEnergies.push_back(7005.0*keV);
142  ExcitSpins.push_back(0.0);
143  ExcitLifetimes.push_back(fPlanck/(24.0*keV));
144 
145  ExcitEnergies.push_back(7076.0*keV);
146  ExcitSpins.push_back(1.0);
147  ExcitLifetimes.push_back(fPlanck/(24.0*keV));
148 
149  ExcitEnergies.push_back(7171.0*keV);
150  ExcitSpins.push_back(2.0);
151  ExcitLifetimes.push_back(fPlanck/(14.0*keV));
152 
153  ExcitEnergies.push_back(7311.0*keV);
154  ExcitSpins.push_back(1.0);
155  ExcitLifetimes.push_back(fPlanck/(33.0*keV));
156 
157  ExcitEnergies.push_back(7355.0*keV);
158  ExcitSpins.push_back(1.0);
159  ExcitLifetimes.push_back(fPlanck/(19.0*keV));
160 
161  ExcitEnergies.push_back(7410.0*keV);
162  ExcitSpins.push_back(2.0);
163  ExcitLifetimes.push_back(fPlanck/(10.0*keV));
164 
165  ExcitEnergies.push_back(7489.0*keV);
166  ExcitSpins.push_back(2.0);
167  ExcitLifetimes.push_back(fPlanck/(57.0*keV));
168 
169  ExcitEnergies.push_back(7503.0*keV);
170  ExcitSpins.push_back(0.0);
171  ExcitLifetimes.push_back(fPlanck/(85.0*keV));
172 
173  ExcitEnergies.push_back(7670.0*keV);
174  ExcitSpins.push_back(2.0);
175  ExcitLifetimes.push_back(fPlanck/(60.0*keV));
176 
177  ExcitEnergies.push_back(7800.0*keV);
178  ExcitSpins.push_back(1.0);
179  ExcitLifetimes.push_back(fPlanck/(100.0*keV));
180 
181  ExcitEnergies.push_back(8150.0*keV);
182  ExcitSpins.push_back(1.0);
183  ExcitLifetimes.push_back(fPlanck/(190.0*keV));
184 
185  ExcitEnergies.push_back(10228.0*keV);
186  ExcitSpins.push_back(0.0);
187  ExcitLifetimes.push_back(fPlanck/(200.0*keV));
188 
189  ExcitEnergies.push_back(10641.0*keV);
190  ExcitSpins.push_back(1.0);
191  ExcitLifetimes.push_back(fPlanck/(60.0*keV));
192 
193  ExcitEnergies.push_back(10807.0*keV);
194  ExcitSpins.push_back(0.0);
195  ExcitLifetimes.push_back(fPlanck/(330.0*keV));
196 
197 }
198 
199 G4F20GEMProbability::~G4F20GEMProbability()
200 {}
201 
G4GEMProbability::ExcitLifetimes
std::vector< G4double > ExcitLifetimes
Definition: G4GEMProbability.hh:132
G4GEMProbability::ExcitSpins
std::vector< G4double > ExcitSpins
Definition: G4GEMProbability.hh:129
G4F20GEMProbability.hh
G4Log.hh
G4GEMProbability::ExcitEnergies
std::vector< G4double > ExcitEnergies
Definition: G4GEMProbability.hh:126
G4PhysicalConstants.hh
G4Log
G4double G4Log(G4double x)
Definition: G4Log.hh:227
python.hepunit.picosecond
int picosecond
Definition: hepunit.py:86
G4SystemOfUnits.hh
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