| Geant4 Cross Reference |
1 Environment variable "G4FORCE_RUN_MANAGER_TYPE <<
2 1
3 ###################################### << 2 *************************************************************
4 !!! WARNING - FPE detection is activat << 3 Geant4 version Name: geant4-08-02-patch-01-ref (23-February-2007)
5 ###################################### << 4 Copyright : Geant4 Collaboration
6 << 5 Reference : NIM A 506 (2003), 250-303
7 << 6 WWW : http://cern.ch/geant4
8 ################################ << 7 *************************************************************
9 !!! G4Backtrace is activated !!! << 8
10 ################################ << 9 B01PhysicsList::SetCuts:CutLength : 1 (mm)
11 << 10 Going to assign importance: 1, to volume: cell_01
12 << 11 Going to assign importance: 2, to volume: cell_02
13 ********************************************** << 12 Going to assign importance: 4, to volume: cell_03
14 Geant4 version Name: geant4-11-03-ref-00 ( << 13 Going to assign importance: 8, to volume: cell_04
15 Copyright : Geant4 Coll << 14 Going to assign importance: 16, to volume: cell_05
16 References : NIM A 506 ( << 15 Going to assign importance: 32, to volume: cell_06
17 : IEEE-TNS 53 << 16 Going to assign importance: 64, to volume: cell_07
18 : NIM A 835 ( << 17 Going to assign importance: 128, to volume: cell_08
19 WWW : http://gean << 18 Going to assign importance: 256, to volume: cell_09
20 ********************************************** << 19 Going to assign importance: 512, to volume: cell_10
21 << 20 Going to assign importance: 1024, to volume: cell_11
22 <<< Geant4 Physics List simulation engine: FTF << 21 Going to assign importance: 2048, to volume: cell_12
23 << 22 Going to assign importance: 4096, to volume: cell_13
24 << 23 Going to assign importance: 8192, to volume: cell_14
25 hInelastic FTFP_BERT : threshold between BERT << 24 Going to assign importance: 16384, to volume: cell_15
26 for pions : 3 to 6 GeV << 25 Going to assign importance: 32768, to volume: cell_16
27 for kaons : 3 to 6 GeV << 26 Going to assign importance: 65536, to volume: cell_17
28 for proton : 3 to 6 GeV << 27 Going to assign importance: 131072, to volume: cell_18
29 for neutron : 3 to 6 GeV <<
30 <<
31 ### Adding tracking cuts for neutron TimeCut( <<
32 paraFlag: 0 <<
33 Preparing Importance Sampling <<
34 G4IStore:: Creating new MASS IStore <<
35 G4GeometrySampler:: preparing importance sampl <<
36 G4ImportanceConfigurator:: setting world name <<
37 G4ImportanceConfigurator:: entering importance <<
38 ### G4ImportanceProcess:: Creating <<
39 G4ImportanceProcess:: importance process paraf <<
40 === G4ProcessPlacer::AddProcessAsSecondDoIt: f 28 === G4ProcessPlacer::AddProcessAsSecondDoIt: for: neutron
41 Modifying Process Order for ProcessName: Imp << 29 ProcessName: MScoreProcess
42 The initial AlongStep Vectors: << 30 The initial Vectors:
43 GPIL Vector: 31 GPIL Vector:
>> 32 Decay
>> 33 HadronCapture
>> 34 HadronFission
>> 35 inelastic
>> 36 HadronElastic
44 Transportation 37 Transportation
45 DoIt Vector: 38 DoIt Vector:
46 Transportation 39 Transportation
47 The initial PostStep Vectors: << 40 HadronElastic
>> 41 inelastic
>> 42 HadronFission
>> 43 HadronCapture
>> 44 Decay
>> 45 The final Vectors:
48 GPIL Vector: 46 GPIL Vector:
49 nKiller <<
50 nCapture <<
51 neutronInelastic <<
52 hadElastic <<
53 Decay 47 Decay
>> 48 HadronCapture
>> 49 HadronFission
>> 50 inelastic
>> 51 HadronElastic
>> 52 MScoreProcess
54 Transportation 53 Transportation
55 DoIt Vector: 54 DoIt Vector:
56 Transportation 55 Transportation
>> 56 MScoreProcess
>> 57 HadronElastic
>> 58 inelastic
>> 59 HadronFission
>> 60 HadronCapture
57 Decay 61 Decay
58 hadElastic << 62 ================================================
59 neutronInelastic << 63 === G4ProcessPlacer::AddProcessAsSecondDoIt: for: neutron
60 nCapture << 64 ProcessName: MassImportanceProcess
61 nKiller << 65 The initial Vectors:
62 The final AlongStep Vectors: <<
63 GPIL Vector: 66 GPIL Vector:
64 ImportanceProcess << 67 Decay
>> 68 HadronCapture
>> 69 HadronFission
>> 70 inelastic
>> 71 HadronElastic
>> 72 MScoreProcess
65 Transportation 73 Transportation
66 DoIt Vector: 74 DoIt Vector:
67 Transportation 75 Transportation
68 ImportanceProcess << 76 MScoreProcess
69 The final PostStep Vectors: << 77 HadronElastic
>> 78 inelastic
>> 79 HadronFission
>> 80 HadronCapture
>> 81 Decay
>> 82 The final Vectors:
70 GPIL Vector: 83 GPIL Vector:
71 nKiller <<
72 nCapture <<
73 neutronInelastic <<
74 hadElastic <<
75 Decay 84 Decay
76 ImportanceProcess << 85 HadronCapture
>> 86 HadronFission
>> 87 inelastic
>> 88 HadronElastic
>> 89 MScoreProcess
>> 90 MassImportanceProcess
77 Transportation 91 Transportation
78 DoIt Vector: 92 DoIt Vector:
79 Transportation 93 Transportation
80 ImportanceProcess << 94 MassImportanceProcess
>> 95 MScoreProcess
>> 96 HadronElastic
>> 97 inelastic
>> 98 HadronFission
>> 99 HadronCapture
>> 100 Decay
>> 101 ================================================
>> 102
>> 103 conv: Total cross sections has a good parametrisation from 1.5 MeV to 100 GeV for all Z;
>> 104 sampling secondary e+e- according Bethe-Heitler model
>> 105 tables are built for gamma
>> 106 Lambda tables from 1.022 MeV to 100 GeV in 100 bins.
>> 107
>> 108 compt: Total cross sections has a good parametrisation from 10 KeV to (100/Z) GeV
>> 109 Sampling according Klein-Nishina model
>> 110 tables are built for gamma
>> 111 Lambda tables from 100 eV to 100 GeV in 90 bins.
>> 112
>> 113 phot: Total cross sections from Sandia parametrisation.
>> 114 Sampling according PhotoElectric model
>> 115
>> 116 msc: Model variant of multiple scattering for e-
>> 117 Lambda tables from 100 eV to 100 TeV in 120 bins.
>> 118 Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
>> 119
>> 120 eIoni: tables are built for e-
>> 121 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 122 Lambda tables from threshold to 100 TeV in 120 bins.
>> 123 Delta cross sections and sampling from MollerBhabha model
>> 124 Good description from 1 KeV to 100 GeV.
>> 125 Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
>> 126
>> 127 eBrem: tables are built for e-
>> 128 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 129 Lambda tables from threshold to 100 TeV in 120 bins.
>> 130 Total cross sections and sampling from StandBrem model (based on the EEDL data library)
>> 131 Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV.
>> 132
>> 133 eIoni: tables are built for e+
>> 134 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 135 Lambda tables from threshold to 100 TeV in 120 bins.
>> 136 Delta cross sections and sampling from MollerBhabha model
>> 137 Good description from 1 KeV to 100 GeV.
>> 138 Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
>> 139
>> 140 eBrem: tables are built for e+
>> 141 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 142 Lambda tables from threshold to 100 TeV in 120 bins.
>> 143 Total cross sections and sampling from StandBrem model (based on the EEDL data library)
>> 144 Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV.
>> 145
>> 146 annihil: Sampling according eplus2gg model
>> 147 tables are built for e+
>> 148 Lambda tables from 100 eV to 100 TeV in 120 bins.
>> 149
>> 150 msc: Model variant of multiple scattering for proton
>> 151 Lambda tables from 100 eV to 100 TeV in 120 bins.
>> 152 Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
>> 153
>> 154 hIoni: tables are built for proton
>> 155 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 156 Lambda tables from threshold to 100 TeV in 120 bins.
>> 157 Scaling relation is used from proton dE/dx and range.
>> 158 Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV
>> 159 Parametrisation from Bragg for protons below.
>> 160 Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
>> 161
>> 162 msc: Model variant of multiple scattering for GenericIon
>> 163 Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
>> 164
>> 165 hIoni: tables are built for anti_proton
>> 166 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 167 Lambda tables from threshold to 100 TeV in 120 bins.
>> 168 Scaling relation is used from proton dE/dx and range.
>> 169 Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV
>> 170 Parametrisation from Bragg for protons below.
>> 171 Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
>> 172
>> 173 msc: Model variant of multiple scattering for mu+
>> 174 Lambda tables from 100 eV to 100 TeV in 120 bins.
>> 175 Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
>> 176
>> 177 muIoni: tables are built for mu+
>> 178 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 179 Lambda tables from threshold to 100 TeV in 120 bins.
>> 180 Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below,
>> 181 radiative corrections for E > 1 GeV
>> 182 Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
>> 183
>> 184 muBrems: tables are built for mu+
>> 185 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 186 Lambda tables from threshold to 100 TeV in 120 bins.
>> 187 Parametrised model
>> 188
>> 189 muPairProd: tables are built for mu+
>> 190 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 191 Lambda tables from threshold to 100 TeV in 120 bins.
>> 192 Parametrised model
>> 193
>> 194 muIoni: tables are built for mu-
>> 195 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 196 Lambda tables from threshold to 100 TeV in 120 bins.
>> 197 Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below,
>> 198 radiative corrections for E > 1 GeV
>> 199 Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
>> 200
>> 201 muBrems: tables are built for mu-
>> 202 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 203 Lambda tables from threshold to 100 TeV in 120 bins.
>> 204 Parametrised model
>> 205
>> 206 muPairProd: tables are built for mu-
>> 207 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 208 Lambda tables from threshold to 100 TeV in 120 bins.
>> 209 Parametrised model
>> 210
>> 211 hIoni: tables are built for pi+
>> 212 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 213 Lambda tables from threshold to 100 TeV in 120 bins.
>> 214 Scaling relation is used from proton dE/dx and range.
>> 215 Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV
>> 216 Parametrisation from Bragg for protons below.
>> 217 Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
>> 218
>> 219 msc: Model variant of multiple scattering for pi-
>> 220 Lambda tables from 100 eV to 100 TeV in 120 bins.
>> 221 Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
>> 222
>> 223 hIoni: tables are built for pi-
>> 224 dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
>> 225 Lambda tables from threshold to 100 TeV in 120 bins.
>> 226 Scaling relation is used from proton dE/dx and range.
>> 227 Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV
>> 228 Parametrisation from Bragg for protons below.
>> 229 Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
>> 230 Volume name | Importance| Tr.Entering| Population| Collisions| Coll*WGT| NumWGTedE| FluxWGTedE| Av.Tr.WGT|
>> 231 cell_01_rep:0............ | 1 | 115 | 132 | 129 | 129 | 4.9419 | 9.2192509 | 1 |
>> 232 cell_02_rep:0............ | 2 | 73 | 152 | 153 | 76.5 | 6.6608595 | 9.0352099 | 1 |
>> 233 cell_03_rep:0............ | 4 | 91 | 201 | 186 | 46.5 | 7.7197107 | 8.7377469 | 1 |
>> 234 cell_04_rep:0............ | 8 | 92 | 212 | 251 | 31.375 | 7.0717677 | 8.0004664 | 1 |
>> 235 cell_05_rep:0............ | 16 | 117 | 229 | 237 | 14.8125 | 7.1619879 | 8.050541 | 1 |
>> 236 cell_06_rep:0............ | 32 | 133 | 301 | 355 | 11.09375 | 6.7661673 | 7.8071533 | 1 |
>> 237 cell_07_rep:0............ | 64 | 146 | 304 | 380 | 5.9375 | 6.1055566 | 7.3480228 | 1 |
>> 238 cell_08_rep:0............ | 128 | 177 | 376 | 439 | 3.4296875 | 5.9739486 | 7.0847309 | 1 |
>> 239 cell_09_rep:0............ | 256 | 196 | 418 | 553 | 2.1601562 | 4.7073021 | 6.9428614 | 1 |
>> 240 cell_10_rep:0............ | 512 | 199 | 436 | 556 | 1.0859375 | 5.735939 | 7.0925789 | 1 |
>> 241 cell_11_rep:0............ | 1024 | 237 | 485 | 619 | 0.60449219 | 5.4202268 | 6.8240104 | 1 |
>> 242 cell_12_rep:0............ | 2048 | 274 | 556 | 764 | 0.37304688 | 0.41403405 | 6.4856097 | 1 |
>> 243 cell_13_rep:0............ | 4096 | 271 | 592 | 809 | 0.19750977 | 5.0683218 | 6.2675874 | 1 |
>> 244 cell_14_rep:0............ | 8192 | 296 | 639 | 952 | 0.11621094 | 4.5960937 | 5.7266154 | 1 |
>> 245 cell_15_rep:0............ | 16384 | 322 | 634 | 977 | 0.059631348 | 4.4000889 | 5.5248549 | 1 |
>> 246 cell_16_rep:0............ | 32768 | 355 | 724 | 1194 | 0.036437988 | 0.029596617 | 5.1972504 | 1 |
>> 247 cell_17_rep:0............ | 65536 | 376 | 788 | 1285 | 0.019607544 | 3.9244532 | 5.0901448 | 1 |
>> 248 cell_18_rep:0............ | 131072 | 325 | 790 | 1329 | 0.010139465 | 3.8972239 | 5.0709833 | 1 |
>> 249 rest_rep:0............... | 131072 | 366 | 366 | 0 | 0 | 0 | 0 | 0 |
>> 250 shieldWorld_rep:0........ | 1 | 11 | 109 | 0 | 0 | 10 | 10 | 1 |
>> 251 === G4ProcessPlacer::RemoveProcess: for: neutron
>> 252 ProcessName: MassImportanceProcess, will be removed!
>> 253 The initial Vectors:
>> 254 GPIL Vector:
>> 255 Decay
>> 256 HadronCapture
>> 257 HadronFission
>> 258 inelastic
>> 259 HadronElastic
>> 260 MScoreProcess
>> 261 MassImportanceProcess
>> 262 Transportation
>> 263 DoIt Vector:
>> 264 Transportation
>> 265 MassImportanceProcess
>> 266 MScoreProcess
>> 267 HadronElastic
>> 268 inelastic
>> 269 HadronFission
>> 270 HadronCapture
>> 271 Decay
>> 272 The final Vectors:
>> 273 GPIL Vector:
>> 274 Decay
>> 275 HadronCapture
>> 276 HadronFission
>> 277 inelastic
>> 278 HadronElastic
>> 279 MScoreProcess
>> 280 Transportation
>> 281 DoIt Vector:
>> 282 Transportation
>> 283 MScoreProcess
>> 284 HadronElastic
>> 285 inelastic
>> 286 HadronFission
>> 287 HadronCapture
>> 288 Decay
>> 289 ================================================
>> 290 === G4ProcessPlacer::RemoveProcess: for: neutron
>> 291 ProcessName: MScoreProcess, will be removed!
>> 292 The initial Vectors:
>> 293 GPIL Vector:
>> 294 Decay
>> 295 HadronCapture
>> 296 HadronFission
>> 297 inelastic
>> 298 HadronElastic
>> 299 MScoreProcess
>> 300 Transportation
>> 301 DoIt Vector:
>> 302 Transportation
>> 303 MScoreProcess
>> 304 HadronElastic
>> 305 inelastic
>> 306 HadronFission
>> 307 HadronCapture
>> 308 Decay
>> 309 The final Vectors:
>> 310 GPIL Vector:
>> 311 Decay
>> 312 HadronCapture
>> 313 HadronFission
>> 314 inelastic
>> 315 HadronElastic
>> 316 Transportation
>> 317 DoIt Vector:
>> 318 Transportation
>> 319 HadronElastic
>> 320 inelastic
>> 321 HadronFission
>> 322 HadronCapture
81 Decay 323 Decay
82 hadElastic <<
83 neutronInelastic <<
84 nCapture <<
85 nKiller <<
86 ============================================== 324 ================================================
87 B01DetectorConstruction:: Creating Importance <<
88 Going to assign importance: 1, to volume: cell <<
89 Going to assign importance: 2, to volume: cell <<
90 Going to assign importance: 4, to volume: cell <<
91 Going to assign importance: 8, to volume: cell <<
92 Going to assign importance: 16, to volume: cel <<
93 Going to assign importance: 32, to volume: cel <<
94 Going to assign importance: 64, to volume: cel <<
95 Going to assign importance: 128, to volume: ce <<
96 Going to assign importance: 256, to volume: ce <<
97 Going to assign importance: 512, to volume: ce <<
98 Going to assign importance: 1024, to volume: c <<
99 Going to assign importance: 2048, to volume: c <<
100 Going to assign importance: 4096, to volume: c <<
101 Going to assign importance: 8192, to volume: c <<
102 Going to assign importance: 16384, to volume: <<
103 Going to assign importance: 32768, to volume: <<
104 Going to assign importance: 65536, to volume: <<
105 Going to assign importance: 131072, to volume: <<
106 ============================================== <<
107 ====== Electromagnetic Physics <<
108 ============================================== <<
109 LPM effect enabled <<
110 Enable creation and use of sampling tables <<
111 Apply cuts on all EM processes <<
112 Use combined TransportationWithMsc <<
113 Use general process <<
114 Enable linear polarisation for gamma <<
115 Enable photoeffect sampling below K-shell <<
116 Enable sampling of quantum entanglement <<
117 X-section factor for integral approach <<
118 Min kinetic energy for tables <<
119 Max kinetic energy for tables <<
120 Number of bins per decade of a table <<
121 Verbose level <<
122 Verbose level for worker thread <<
123 Bremsstrahlung energy threshold above which <<
124 primary e+- is added to the list of secondar <<
125 Bremsstrahlung energy threshold above which pr <<
126 muon/hadron is added to the list of secondar <<
127 Positron annihilation at rest model <<
128 Enable 3 gamma annihilation on fly <<
129 Lowest triplet kinetic energy <<
130 Enable sampling of gamma linear polarisation <<
131 5D gamma conversion model type <<
132 5D gamma conversion model on isolated ion <<
133 Use Ricardo-Gerardo pair production model <<
134 Livermore data directory <<
135 ============================================== <<
136 ====== Ionisation Parameters <<
137 ============================================== <<
138 Step function for e+- <<
139 Step function for muons/hadrons <<
140 Step function for light ions <<
141 Step function for general ions <<
142 Lowest e+e- kinetic energy <<
143 Lowest muon/hadron kinetic energy <<
144 Use ICRU90 data <<
145 Fluctuations of dE/dx are enabled <<
146 Type of fluctuation model for leptons and hadr <<
147 Use built-in Birks satuaration <<
148 Build CSDA range enabled <<
149 Use cut as a final range enabled <<
150 Enable angular generator interface <<
151 Max kinetic energy for CSDA tables <<
152 Max kinetic energy for NIEL computation <<
153 Linear loss limit <<
154 Read data from file for e+e- pair production b <<
155 ============================================== <<
156 ====== Multiple Scattering Par <<
157 ============================================== <<
158 Type of msc step limit algorithm for e+- <<
159 Type of msc step limit algorithm for muons/had <<
160 Msc lateral displacement for e+- enabled <<
161 Msc lateral displacement for muons and hadrons <<
162 Urban msc model lateral displacement alg96 <<
163 Range factor for msc step limit for e+- <<
164 Range factor for msc step limit for muons/hadr <<
165 Geometry factor for msc step limitation of e+- <<
166 Safety factor for msc step limit for e+- <<
167 Skin parameter for msc step limitation of e+- <<
168 Lambda limit for msc step limit for e+- <<
169 Use Mott correction for e- scattering <<
170 Factor used for dynamic computation of angular <<
171 limit between single and multiple scattering <<
172 Fixed angular limit between single <<
173 and multiple scattering <<
174 Upper energy limit for e+- multiple scattering <<
175 Type of electron single scattering model <<
176 Type of nuclear form-factor <<
177 Screening factor <<
178 ============================================== <<
179 <<
180 phot: for gamma SubType=12 BuildTable=0 <<
181 LambdaPrime table from 200 keV to 100 Te <<
182 ===== EM models for the G4Region Defaul <<
183 LivermorePhElectric : Emin= 0 eV Emax= 1 <<
184 <<
185 compt: for gamma SubType=13 BuildTable=1 <<
186 Lambda table from 100 eV to 1 MeV, 7 bi <<
187 LambdaPrime table from 1 MeV to 100 TeV <<
188 ===== EM models for the G4Region Defaul <<
189 Klein-Nishina : Emin= 0 eV Emax= 1 <<
190 <<
191 conv: for gamma SubType=14 BuildTable=1 <<
192 Lambda table from 1.022 MeV to 100 TeV, <<
193 ===== EM models for the G4Region Defaul <<
194 BetheHeitlerLPM : Emin= 0 eV Emax= 1 <<
195 <<
196 Rayl: for gamma SubType=11 BuildTable=1 <<
197 Lambda table from 100 eV to 150 keV, 7 <<
198 LambdaPrime table from 150 keV to 100 Te <<
199 ===== EM models for the G4Region Defaul <<
200 LivermoreRayleigh : Emin= 0 eV Emax= 1 <<
201 <<
202 msc: for e- SubType= 10 <<
203 ===== EM models for the G4Region Defaul <<
204 UrbanMsc : Emin= 0 eV Emax= 1 <<
205 StepLim=UseSafety Rfact=0.04 Gfact=2 <<
206 WentzelVIUni : Emin= 100 MeV Emax= 1 <<
207 StepLim=UseSafety Rfact=0.04 Gfact=2 <<
208 <<
209 eIoni: for e- XStype:3 SubType=2 <<
210 dE/dx and range tables from 100 eV to 1 <<
211 Lambda tables from threshold to 100 TeV, <<
212 StepFunction=(0.2, 1 mm), integ: 3, fluc <<
213 ===== EM models for the G4Region Defaul <<
214 MollerBhabha : Emin= 0 eV Emax= 1 <<
215 <<
216 eBrem: for e- XStype:4 SubType=3 <<
217 dE/dx and range tables from 100 eV to 1 <<
218 Lambda tables from threshold to 100 TeV, <<
219 LPM flag: 1 for E > 1 GeV, VertexHighEn <<
220 ===== EM models for the G4Region Defaul <<
221 eBremSB : Emin= 0 eV Emax= <<
222 eBremLPM : Emin= 1 GeV Emax= 1 <<
223 <<
224 CoulombScat: for e- XStype:1 SubType=1 BuildT <<
225 Lambda table from 100 MeV to 100 TeV, 7 <<
226 ThetaMin(p) < Theta(degree) < 180, pLimi <<
227 ===== EM models for the G4Region Defaul <<
228 eCoulombScattering : Emin= 100 MeV Emax= 1 <<
229 <<
230 msc: for e+ SubType= 10 <<
231 ===== EM models for the G4Region Defaul <<
232 UrbanMsc : Emin= 0 eV Emax= 1 <<
233 StepLim=UseSafety Rfact=0.04 Gfact=2 <<
234 WentzelVIUni : Emin= 100 MeV Emax= 1 <<
235 StepLim=UseSafety Rfact=0.04 Gfact=2 <<
236 <<
237 eIoni: for e+ XStype:3 SubType=2 <<
238 dE/dx and range tables from 100 eV to 1 <<
239 Lambda tables from threshold to 100 TeV, <<
240 StepFunction=(0.2, 1 mm), integ: 3, fluc <<
241 ===== EM models for the G4Region Defaul <<
242 MollerBhabha : Emin= 0 eV Emax= 1 <<
243 <<
244 eBrem: for e+ XStype:4 SubType=3 <<
245 dE/dx and range tables from 100 eV to 1 <<
246 Lambda tables from threshold to 100 TeV, <<
247 LPM flag: 1 for E > 1 GeV, VertexHighEn <<
248 ===== EM models for the G4Region Defaul <<
249 eBremSB : Emin= 0 eV Emax= <<
250 eBremLPM : Emin= 1 GeV Emax= 1 <<
251 <<
252 annihil: for e+ XStype:2 SubType=5 AtRestMode <<
253 ===== EM models for the G4Region Defaul <<
254 eplus2gg : Emin= 0 eV Emax= 1 <<
255 <<
256 CoulombScat: for e+ XStype:1 SubType=1 BuildT <<
257 Lambda table from 100 MeV to 100 TeV, 7 <<
258 ThetaMin(p) < Theta(degree) < 180, pLimi <<
259 ===== EM models for the G4Region Defaul <<
260 eCoulombScattering : Emin= 100 MeV Emax= 1 <<
261 <<
262 msc: for proton SubType= 10 <<
263 ===== EM models for the G4Region Defaul <<
264 WentzelVIUni : Emin= 0 eV Emax= 1 <<
265 StepLim=Minimal Rfact=0.2 Gfact=2.5 <<
266 <<
267 hIoni: for proton XStype:3 SubType=2 <<
268 dE/dx and range tables from 100 eV to 1 <<
269 Lambda tables from threshold to 100 TeV, <<
270 StepFunction=(0.2, 0.1 mm), integ: 3, fl <<
271 ===== EM models for the G4Region Defaul <<
272 Bragg : Emin= 0 eV Emax= <<
273 BetheBloch : Emin= 2 MeV Emax= 1 <<
274 <<
275 hBrems: for proton XStype:1 SubType=3 <<
276 dE/dx and range tables from 100 eV to 1 <<
277 Lambda tables from threshold to 100 TeV, <<
278 ===== EM models for the G4Region Defaul <<
279 hBrem : Emin= 0 eV Emax= 1 <<
280 <<
281 hPairProd: for proton XStype:1 SubType=4 <<
282 dE/dx and range tables from 100 eV to 1 <<
283 Lambda tables from threshold to 100 TeV, <<
284 Sampling table 17x1001 from 7.50618 GeV <<
285 ===== EM models for the G4Region Defaul <<
286 hPairProd : Emin= 0 eV Emax= 1 <<
287 <<
288 CoulombScat: for proton XStype:1 SubType=1 Bu <<
289 Lambda table from threshold to 100 TeV, <<
290 ThetaMin(p) < Theta(degree) < 180, pLimi <<
291 ===== EM models for the G4Region Defaul <<
292 eCoulombScattering : Emin= 0 eV Emax= 1 <<
293 <<
294 msc: for GenericIon SubType= 10 <<
295 ===== EM models for the G4Region Defaul <<
296 UrbanMsc : Emin= 0 eV Emax= 1 <<
297 StepLim=Minimal Rfact=0.2 Gfact=2.5 <<
298 <<
299 ionIoni: for GenericIon XStype:3 SubType=2 <<
300 dE/dx and range tables from 100 eV to 1 <<
301 Lambda tables from threshold to 100 TeV, <<
302 StepFunction=(0.2, 0.1 mm), integ: 3, fl <<
303 ===== EM models for the G4Region Defaul <<
304 Bragg : Emin= 0 eV Emax= <<
305 BetheBloch : Emin= 2 MeV Emax= 1 <<
306 <<
307 msc: for alpha SubType= 10 <<
308 ===== EM models for the G4Region Defaul <<
309 UrbanMsc : Emin= 0 eV Emax= 1 <<
310 StepLim=Minimal Rfact=0.2 Gfact=2.5 <<
311 <<
312 ionIoni: for alpha XStype:3 SubType=2 <<
313 dE/dx and range tables from 100 eV to 1 <<
314 Lambda tables from threshold to 100 TeV, <<
315 StepFunction=(0.2, 0.1 mm), integ: 3, fl <<
316 ===== EM models for the G4Region Defaul <<
317 BraggIon : Emin= 0 eV Emax=7.9 <<
318 BetheBloch : Emin=7.9452 MeV Emax= <<
319 <<
320 msc: for anti_proton SubType= 10 <<
321 ===== EM models for the G4Region Defaul <<
322 WentzelVIUni : Emin= 0 eV Emax= 1 <<
323 StepLim=Minimal Rfact=0.2 Gfact=2.5 <<
324 <<
325 hIoni: for anti_proton XStype:3 SubType=2 <<
326 dE/dx and range tables from 100 eV to 1 <<
327 Lambda tables from threshold to 100 TeV, <<
328 StepFunction=(0.2, 0.1 mm), integ: 3, fl <<
329 ===== EM models for the G4Region Defaul <<
330 ICRU73QO : Emin= 0 eV Emax= <<
331 BetheBloch : Emin= 2 MeV Emax= 1 <<
332 <<
333 hBrems: for anti_proton XStype:1 SubType=3 <<
334 dE/dx and range tables from 100 eV to 1 <<
335 Lambda tables from threshold to 100 TeV, <<
336 ===== EM models for the G4Region Defaul <<
337 hBrem : Emin= 0 eV Emax= 1 <<
338 <<
339 hPairProd: for anti_proton XStype:1 SubType <<
340 dE/dx and range tables from 100 eV to 1 <<
341 Lambda tables from threshold to 100 TeV, <<
342 Sampling table 17x1001 from 7.50618 GeV <<
343 ===== EM models for the G4Region Defaul <<
344 hPairProd : Emin= 0 eV Emax= 1 <<
345 <<
346 CoulombScat: for anti_proton XStype:1 SubType <<
347 Lambda table from threshold to 100 TeV, <<
348 ThetaMin(p) < Theta(degree) < 180, pLimi <<
349 ===== EM models for the G4Region Defaul <<
350 eCoulombScattering : Emin= 0 eV Emax= 1 <<
351 <<
352 msc: for kaon+ SubType= 10 <<
353 ===== EM models for the G4Region Defaul <<
354 WentzelVIUni : Emin= 0 eV Emax= 1 <<
355 StepLim=Minimal Rfact=0.2 Gfact=2.5 <<
356 <<
357 hIoni: for kaon+ XStype:3 SubType=2 <<
358 dE/dx and range tables from 100 eV to 1 <<
359 Lambda tables from threshold to 100 TeV, <<
360 StepFunction=(0.2, 0.1 mm), integ: 3, fl <<
361 ===== EM models for the G4Region Defaul <<
362 Bragg : Emin= 0 eV Emax=1.0 <<
363 BetheBloch : Emin=1.05231 MeV Emax= <<
364 <<
365 hBrems: for kaon+ XStype:1 SubType=3 <<
366 dE/dx and range tables from 100 eV to 1 <<
367 Lambda tables from threshold to 100 TeV, <<
368 ===== EM models for the G4Region Defaul <<
369 hBrem : Emin= 0 eV Emax= 1 <<
370 <<
371 hPairProd: for kaon+ XStype:1 SubType=4 <<
372 dE/dx and range tables from 100 eV to 1 <<
373 Lambda tables from threshold to 100 TeV, <<
374 Sampling table 18x1001 from 3.94942 GeV <<
375 ===== EM models for the G4Region Defaul <<
376 hPairProd : Emin= 0 eV Emax= 1 <<
377 <<
378 CoulombScat: for kaon+ XStype:1 SubType=1 Bui <<
379 Lambda table from threshold to 100 TeV, <<
380 ThetaMin(p) < Theta(degree) < 180, pLimi <<
381 ===== EM models for the G4Region Defaul <<
382 eCoulombScattering : Emin= 0 eV Emax= 1 <<
383 <<
384 msc: for kaon- SubType= 10 <<
385 ===== EM models for the G4Region Defaul <<
386 WentzelVIUni : Emin= 0 eV Emax= 1 <<
387 StepLim=Minimal Rfact=0.2 Gfact=2.5 <<
388 <<
389 hIoni: for kaon- XStype:3 SubType=2 <<
390 dE/dx and range tables from 100 eV to 1 <<
391 Lambda tables from threshold to 100 TeV, <<
392 StepFunction=(0.2, 0.1 mm), integ: 3, fl <<
393 ===== EM models for the G4Region Defaul <<
394 ICRU73QO : Emin= 0 eV Emax=1.0 <<
395 BetheBloch : Emin=1.05231 MeV Emax= <<
396 <<
397 hBrems: for kaon- XStype:1 SubType=3 <<
398 dE/dx and range tables from 100 eV to 1 <<
399 Lambda tables from threshold to 100 TeV, <<
400 ===== EM models for the G4Region Defaul <<
401 hBrem : Emin= 0 eV Emax= 1 <<
402 <<
403 hPairProd: for kaon- XStype:1 SubType=4 <<
404 dE/dx and range tables from 100 eV to 1 <<
405 Lambda tables from threshold to 100 TeV, <<
406 Sampling table 18x1001 from 3.94942 GeV <<
407 ===== EM models for the G4Region Defaul <<
408 hPairProd : Emin= 0 eV Emax= 1 <<
409 <<
410 CoulombScat: for kaon- XStype:1 SubType=1 Bui <<
411 Used Lambda table of kaon+ <<
412 ThetaMin(p) < Theta(degree) < 180, pLimi <<
413 ===== EM models for the G4Region Defaul <<
414 eCoulombScattering : Emin= 0 eV Emax= 1 <<
415 <<
416 msc: for mu+ SubType= 10 <<
417 ===== EM models for the G4Region Defaul <<
418 WentzelVIUni : Emin= 0 eV Emax= 1 <<
419 StepLim=Minimal Rfact=0.2 Gfact=2.5 <<
420 <<
421 muIoni: for mu+ XStype:3 SubType=2 <<
422 dE/dx and range tables from 100 eV to 1 <<
423 Lambda tables from threshold to 100 TeV, <<
424 StepFunction=(0.2, 0.1 mm), integ: 3, fl <<
425 ===== EM models for the G4Region Defaul <<
426 Bragg : Emin= 0 eV Emax= 2 <<
427 MuBetheBloch : Emin= 200 keV Emax= 1 <<
428 <<
429 muBrems: for mu+ XStype:1 SubType=3 <<
430 dE/dx and range tables from 100 eV to 1 <<
431 Lambda tables from threshold to 100 TeV, <<
432 ===== EM models for the G4Region Defaul <<
433 MuBrem : Emin= 0 eV Emax= 1 <<
434 <<
435 muPairProd: for mu+ XStype:1 SubType=4 <<
436 dE/dx and range tables from 100 eV to 1 <<
437 Lambda tables from threshold to 100 TeV, <<
438 Sampling table 21x1001 from 0.85 GeV to <<
439 ===== EM models for the G4Region Defaul <<
440 muPairProd : Emin= 0 eV Emax= 1 <<
441 <<
442 CoulombScat: for mu+ XStype:1 SubType=1 Build <<
443 Lambda table from threshold to 100 TeV, <<
444 ThetaMin(p) < Theta(degree) < 180, pLimi <<
445 ===== EM models for the G4Region Defaul <<
446 eCoulombScattering : Emin= 0 eV Emax= 1 <<
447 <<
448 msc: for mu- SubType= 10 <<
449 ===== EM models for the G4Region Defaul <<
450 WentzelVIUni : Emin= 0 eV Emax= 1 <<
451 StepLim=Minimal Rfact=0.2 Gfact=2.5 <<
452 <<
453 muIoni: for mu- XStype:3 SubType=2 <<
454 dE/dx and range tables from 100 eV to 1 <<
455 Lambda tables from threshold to 100 TeV, <<
456 StepFunction=(0.2, 0.1 mm), integ: 3, fl <<
457 ===== EM models for the G4Region Defaul <<
458 ICRU73QO : Emin= 0 eV Emax= 2 <<
459 MuBetheBloch : Emin= 200 keV Emax= 1 <<
460 <<
461 muBrems: for mu- XStype:1 SubType=3 <<
462 dE/dx and range tables from 100 eV to 1 <<
463 Lambda tables from threshold to 100 TeV, <<
464 ===== EM models for the G4Region Defaul <<
465 MuBrem : Emin= 0 eV Emax= 1 <<
466 <<
467 muPairProd: for mu- XStype:1 SubType=4 <<
468 dE/dx and range tables from 100 eV to 1 <<
469 Lambda tables from threshold to 100 TeV, <<
470 Sampling table 21x1001 from 0.85 GeV to <<
471 ===== EM models for the G4Region Defaul <<
472 muPairProd : Emin= 0 eV Emax= 1 <<
473 <<
474 CoulombScat: for mu- XStype:1 SubType=1 Build <<
475 Used Lambda table of mu+ <<
476 ThetaMin(p) < Theta(degree) < 180, pLimi <<
477 ===== EM models for the G4Region Defaul <<
478 eCoulombScattering : Emin= 0 eV Emax= 1 <<
479 <<
480 msc: for pi+ SubType= 10 <<
481 ===== EM models for the G4Region Defaul <<
482 WentzelVIUni : Emin= 0 eV Emax= 1 <<
483 StepLim=Minimal Rfact=0.2 Gfact=2.5 <<
484 <<
485 hIoni: for pi+ XStype:3 SubType=2 <<
486 dE/dx and range tables from 100 eV to 1 <<
487 Lambda tables from threshold to 100 TeV, <<
488 StepFunction=(0.2, 0.1 mm), integ: 3, fl <<
489 ===== EM models for the G4Region Defaul <<
490 Bragg : Emin= 0 eV Emax=297 <<
491 BetheBloch : Emin=297.505 keV Emax= <<
492 <<
493 hBrems: for pi+ XStype:1 SubType=3 <<
494 dE/dx and range tables from 100 eV to 1 <<
495 Lambda tables from threshold to 100 TeV, <<
496 ===== EM models for the G4Region Defaul <<
497 hBrem : Emin= 0 eV Emax= 1 <<
498 <<
499 hPairProd: for pi+ XStype:1 SubType=4 <<
500 dE/dx and range tables from 100 eV to 1 <<
501 Lambda tables from threshold to 100 TeV, <<
502 Sampling table 20x1001 from 1.11656 GeV <<
503 ===== EM models for the G4Region Defaul <<
504 hPairProd : Emin= 0 eV Emax= 1 <<
505 <<
506 CoulombScat: for pi+ XStype:1 SubType=1 Build <<
507 Lambda table from threshold to 100 TeV, <<
508 ThetaMin(p) < Theta(degree) < 180, pLimi <<
509 ===== EM models for the G4Region Defaul <<
510 eCoulombScattering : Emin= 0 eV Emax= 1 <<
511 <<
512 msc: for pi- SubType= 10 <<
513 ===== EM models for the G4Region Defaul <<
514 WentzelVIUni : Emin= 0 eV Emax= 1 <<
515 StepLim=Minimal Rfact=0.2 Gfact=2.5 <<
516 <<
517 hIoni: for pi- XStype:3 SubType=2 <<
518 dE/dx and range tables from 100 eV to 1 <<
519 Lambda tables from threshold to 100 TeV, <<
520 StepFunction=(0.2, 0.1 mm), integ: 3, fl <<
521 ===== EM models for the G4Region Defaul <<
522 ICRU73QO : Emin= 0 eV Emax=297 <<
523 BetheBloch : Emin=297.505 keV Emax= <<
524 <<
525 hBrems: for pi- XStype:1 SubType=3 <<
526 dE/dx and range tables from 100 eV to 1 <<
527 Lambda tables from threshold to 100 TeV, <<
528 ===== EM models for the G4Region Defaul <<
529 hBrem : Emin= 0 eV Emax= 1 <<
530 <<
531 hPairProd: for pi- XStype:1 SubType=4 <<
532 dE/dx and range tables from 100 eV to 1 <<
533 Lambda tables from threshold to 100 TeV, <<
534 Sampling table 20x1001 from 1.11656 GeV <<
535 ===== EM models for the G4Region Defaul <<
536 hPairProd : Emin= 0 eV Emax= 1 <<
537 <<
538 CoulombScat: for pi- XStype:1 SubType=1 Build <<
539 Used Lambda table of pi+ <<
540 ThetaMin(p) < Theta(degree) < 180, pLimi <<
541 ===== EM models for the G4Region Defaul <<
542 eCoulombScattering : Emin= 0 eV Emax= 1 <<
543 <<
544 ============================================== <<
545 HADRONIC PROCESSES SUMMARY ( <<
546 ---------------------------------------------- <<
547 Hadronic Processes <<
548 Process: hadElastic <<
549 Model: hElasticCHIPS: 0 eV <<
550 Cr_sctns: G4NeutronElasticXS: 0 eV <<
551 Process: neutronInelastic <<
552 Model: FTFP: 3 Ge <<
553 Model: BertiniCascade: 0 eV <<
554 Cr_sctns: G4NeutronInelasticXS: 0 eV <<
555 Process: nCapture <<
556 Model: nRadCapture: 0 eV <<
557 Cr_sctns: G4NeutronCaptureXS: 0 eV <<
558 Process: nKiller <<
559 ---------------------------------------------- <<
560 Hadronic Processes <<
561 Process: hadElastic <<
562 Model: hElasticLHEP: 0 eV <<
563 Cr_sctns: Glauber-Gribov: 0 eV <<
564 Process: B-Inelastic <<
565 Model: FTFP: 0 eV <<
566 Cr_sctns: Glauber-Gribov: 0 eV <<
567 ---------------------------------------------- <<
568 Hadronic Processes <<
569 Process: hadElastic <<
570 Model: hElasticLHEP: 0 eV <<
571 Cr_sctns: Glauber-Gribov: 0 eV <<
572 Process: D-Inelastic <<
573 Model: FTFP: 0 eV <<
574 Cr_sctns: Glauber-Gribov: 0 eV <<
575 ---------------------------------------------- <<
576 Hadronic Processes <<
577 Process: ionInelastic <<
578 Model: Binary Light Ion Cascade: 0 eV <<
579 Model: FTFP: 3 Ge <<
580 Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV <<
581 ---------------------------------------------- <<
582 Hadronic Processes <<
583 Process: hadElastic <<
584 Model: hElasticLHEP: 0 eV <<
585 Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV <<
586 Process: He3Inelastic <<
587 Model: Binary Light Ion Cascade: 0 eV <<
588 Model: FTFP: 3 Ge <<
589 Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV <<
590 ---------------------------------------------- <<
591 Hadronic Processes <<
592 Process: hadElastic <<
593 Model: hElasticLHEP: 0 eV <<
594 Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV <<
595 Process: alphaInelastic <<
596 Model: Binary Light Ion Cascade: 0 eV <<
597 Model: FTFP: 3 Ge <<
598 Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV <<
599 ---------------------------------------------- <<
600 Hadronic Processes <<
601 Process: hadElastic <<
602 Model: hElasticLHEP: 0 eV <<
603 Model: AntiAElastic: 100 <<
604 Cr_sctns: AntiAGlauber: 0 eV <<
605 Process: anti_He3Inelastic <<
606 Model: FTFP: 0 eV <<
607 Cr_sctns: AntiAGlauber: 0 eV <<
608 Process: hFritiofCaptureAtRest <<
609 ---------------------------------------------- <<
610 Hadronic Processes <<
611 Process: hadElastic <<
612 Model: hElasticLHEP: 0 eV <<
613 Model: AntiAElastic: 100 <<
614 Cr_sctns: AntiAGlauber: 0 eV <<
615 Process: anti_alphaInelastic <<
616 Model: FTFP: 0 eV <<
617 Cr_sctns: AntiAGlauber: 0 eV <<
618 Process: hFritiofCaptureAtRest <<
619 ---------------------------------------------- <<
620 Hadronic Processes <<
621 Process: hadElastic <<
622 Model: hElasticLHEP: 0 eV <<
623 Model: AntiAElastic: 100 <<
624 Cr_sctns: AntiAGlauber: 0 eV <<
625 Process: anti_deuteronInelastic <<
626 Model: FTFP: 0 eV <<
627 Cr_sctns: AntiAGlauber: 0 eV <<
628 Process: hFritiofCaptureAtRest <<
629 ---------------------------------------------- <<
630 Hadronic Processes <<
631 Process: hFritiofCaptureAtRest <<
632 ---------------------------------------------- <<
633 Hadronic Processes <<
634 Process: hadElastic <<
635 Model: hElasticLHEP: 0 eV <<
636 Cr_sctns: Glauber-Gribov: 0 eV <<
637 Process: anti_lambdaInelastic <<
638 Model: FTFP: 0 eV <<
639 Cr_sctns: Glauber-Gribov: 0 eV <<
640 Process: hFritiofCaptureAtRest <<
641 ---------------------------------------------- <<
642 Hadronic Processes <<
643 Process: hadElastic <<
644 Model: hElasticLHEP: 0 eV <<
645 Model: AntiAElastic: 100 <<
646 Cr_sctns: AntiAGlauber: 0 eV <<
647 Process: anti_neutronInelastic <<
648 Model: FTFP: 0 eV <<
649 Cr_sctns: AntiAGlauber: 0 eV <<
650 Process: hFritiofCaptureAtRest <<
651 ---------------------------------------------- <<
652 Hadronic Processes <<
653 Process: hadElastic <<
654 Model: hElasticLHEP: 0 eV <<
655 Model: AntiAElastic: 100 <<
656 Cr_sctns: AntiAGlauber: 0 eV <<
657 Process: anti_protonInelastic <<
658 Model: FTFP: 0 eV <<
659 Cr_sctns: AntiAGlauber: 0 eV <<
660 Process: hFritiofCaptureAtRest <<
661 ---------------------------------------------- <<
662 Hadronic Processes <<
663 Process: hadElastic <<
664 Model: hElasticLHEP: 0 eV <<
665 Model: AntiAElastic: 100 <<
666 Cr_sctns: AntiAGlauber: 0 eV <<
667 Process: anti_tritonInelastic <<
668 Model: FTFP: 0 eV <<
669 Cr_sctns: AntiAGlauber: 0 eV <<
670 Process: hFritiofCaptureAtRest <<
671 ---------------------------------------------- <<
672 Hadronic Processes <<
673 Process: hadElastic <<
674 Model: hElasticLHEP: 0 eV <<
675 Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV <<
676 Process: dInelastic <<
677 Model: Binary Light Ion Cascade: 0 eV <<
678 Model: FTFP: 3 Ge <<
679 Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV <<
680 ---------------------------------------------- <<
681 Hadronic Processes <<
682 Process: positronNuclear <<
683 Model: G4ElectroVDNuclearModel: 0 eV <<
684 Cr_sctns: ElectroNuclearXS: 0 eV <<
685 ---------------------------------------------- <<
686 Hadronic Processes <<
687 Process: electronNuclear <<
688 Model: G4ElectroVDNuclearModel: 0 eV <<
689 Cr_sctns: ElectroNuclearXS: 0 eV <<
690 ---------------------------------------------- <<
691 Hadronic Processes <<
692 Process: photonNuclear <<
693 Model: GammaNPreco: 0 eV <<
694 Model: BertiniCascade: 199 <<
695 Model: TheoFSGenerator: 3 Ge <<
696 Cr_sctns: GammaNuclearXS: 0 eV <<
697 ---------------------------------------------- <<
698 Hadronic Processes <<
699 Process: hadElastic <<
700 Model: hElasticLHEP: 0 eV <<
701 Cr_sctns: Glauber-Gribov: 0 eV <<
702 Process: kaon+Inelastic <<
703 Model: FTFP: 3 Ge <<
704 Model: BertiniCascade: 0 eV <<
705 Cr_sctns: Glauber-Gribov: 0 eV <<
706 ---------------------------------------------- <<
707 Hadronic Processes <<
708 Process: hadElastic <<
709 Model: hElasticLHEP: 0 eV <<
710 Cr_sctns: Glauber-Gribov: 0 eV <<
711 Process: kaon-Inelastic <<
712 Model: FTFP: 3 Ge <<
713 Model: BertiniCascade: 0 eV <<
714 Cr_sctns: Glauber-Gribov: 0 eV <<
715 Process: hBertiniCaptureAtRest <<
716 ---------------------------------------------- <<
717 Hadronic Processes <<
718 Process: hadElastic <<
719 Model: hElasticLHEP: 0 eV <<
720 Cr_sctns: Glauber-Gribov: 0 eV <<
721 Process: lambdaInelastic <<
722 Model: FTFP: 3 Ge <<
723 Model: BertiniCascade: 0 eV <<
724 Cr_sctns: Glauber-Gribov: 0 eV <<
725 ---------------------------------------------- <<
726 Hadronic Processes <<
727 Process: muonNuclear <<
728 Model: G4MuonVDNuclearModel: 0 eV <<
729 Cr_sctns: KokoulinMuonNuclearXS: 0 eV <<
730 ---------------------------------------------- <<
731 Hadronic Processes <<
732 Process: muonNuclear <<
733 Model: G4MuonVDNuclearModel: 0 eV <<
734 Cr_sctns: KokoulinMuonNuclearXS: 0 eV <<
735 Process: muMinusCaptureAtRest <<
736 ---------------------------------------------- <<
737 Hadronic Processes <<
738 Process: hadElastic <<
739 Model: hElasticGlauber: 0 eV <<
740 Cr_sctns: BarashenkovGlauberGribov: 0 eV <<
741 Process: pi+Inelastic <<
742 Model: FTFP: 3 Ge <<
743 Model: BertiniCascade: 0 eV <<
744 Cr_sctns: BarashenkovGlauberGribov: 0 eV <<
745 ---------------------------------------------- <<
746 Hadronic Processes <<
747 Process: hadElastic <<
748 Model: hElasticGlauber: 0 eV <<
749 Cr_sctns: BarashenkovGlauberGribov: 0 eV <<
750 Process: pi-Inelastic <<
751 Model: FTFP: 3 Ge <<
752 Model: BertiniCascade: 0 eV <<
753 Cr_sctns: BarashenkovGlauberGribov: 0 eV <<
754 Process: hBertiniCaptureAtRest <<
755 ---------------------------------------------- <<
756 Hadronic Processes <<
757 Process: hadElastic <<
758 Model: hElasticCHIPS: 0 eV <<
759 Cr_sctns: BarashenkovGlauberGribov: 0 eV <<
760 Process: protonInelastic <<
761 Model: FTFP: 3 Ge <<
762 Model: BertiniCascade: 0 eV <<
763 Cr_sctns: BarashenkovGlauberGribov: 0 eV <<
764 ---------------------------------------------- <<
765 Hadronic Processes <<
766 Process: hadElastic <<
767 Model: hElasticLHEP: 0 eV <<
768 Cr_sctns: Glauber-Gribov: 0 eV <<
769 Process: sigma-Inelastic <<
770 Model: FTFP: 3 Ge <<
771 Model: BertiniCascade: 0 eV <<
772 Cr_sctns: Glauber-Gribov: 0 eV <<
773 Process: hBertiniCaptureAtRest <<
774 ---------------------------------------------- <<
775 Hadronic Processes <<
776 Process: hadElastic <<
777 Model: hElasticLHEP: 0 eV <<
778 Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV <<
779 Process: tInelastic <<
780 Model: Binary Light Ion Cascade: 0 eV <<
781 Model: FTFP: 3 Ge <<
782 Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV <<
783 ============================================== <<
784 ====== Geant4 Native Pre-compound Model <<
785 ============================================== <<
786 Type of pre-compound inverse x-section <<
787 Pre-compound model active <<
788 Pre-compound excitation low energy <<
789 Pre-compound excitation high energy <<
790 Angular generator for pre-compound model <<
791 Use NeverGoBack option for pre-compound model <<
792 Use SoftCutOff option for pre-compound model <<
793 Use CEM transitions for pre-compound model <<
794 Use GNASH transitions for pre-compound model <<
795 Use HETC submodel for pre-compound model <<
796 ============================================== <<
797 ====== Nuclear De-excitation Module Para <<
798 ============================================== <<
799 Type of de-excitation inverse x-section <<
800 Type of de-excitation factory <<
801 Number of de-excitation channels <<
802 Min excitation energy <<
803 Min energy per nucleon for multifragmentation <<
804 Limit excitation energy for Fermi BreakUp <<
805 Level density (1/MeV) <<
806 Use simple level density model <<
807 Use discrete excitation energy of the residual <<
808 Time limit for long lived isomeres <<
809 Isomer production flag <<
810 Internal e- conversion flag <<
811 Store e- internal conversion data <<
812 Correlated gamma emission flag <<
813 Max 2J for sampling of angular correlations <<
814 ============================================== <<
815 ++ ConcreteSD/Collisions id 0 <<
816 ++ ConcreteSD/CollWeight id 1 <<
817 ++ ConcreteSD/Population id 2 <<
818 ++ ConcreteSD/TrackEnter id 3 <<
819 ++ ConcreteSD/SL id 4 <<
820 ++ ConcreteSD/SLW id 5 <<
821 ++ ConcreteSD/SLWE id 6 <<
822 ++ ConcreteSD/SLW_V id 7 <<
823 ++ ConcreteSD/SLWE_V id 8 <<
824 ### Run 0 start. <<
825 ###### EndOfRunAction <<
826 <<
827 --------------------End of Global Run--------- <<
828 Number of event processed : 100 <<
829 ============================================== <<
830 ============================================== <<
831 Volume | Tr.Entering | Population <<
832 cell_00 | 32 | 127 <<
833 cell_01 | 139 | 179 <<
834 cell_02 | 174 | 270 <<
835 cell_03 | 229 | 334 <<
836 cell_04 | 254 | 381 <<
837 cell_05 | 291 | 420 <<
838 cell_06 | 327 | 472 <<
839 cell_07 | 296 | 437 <<
840 cell_08 | 262 | 372 <<
841 cell_09 | 260 | 356 <<
842 cell_10 | 229 | 331 <<
843 cell_11 | 186 | 270 <<
844 cell_12 | 154 | 220 <<
845 cell_13 | 123 | 185 <<
846 cell_14 | 109 | 157 <<
847 cell_15 | 79 | 112 <<
848 cell_16 | 68 | 99 <<
849 cell_17 | 53 | 82 <<
850 cell_18 | 32 | 57 <<
851 cell_19 | 25 | 25 <<
852 ============================================= <<