296 lines
11 KiB
Plaintext
296 lines
11 KiB
Plaintext
|
|
*************************************************************
|
|
Geant4 version Name: geant4-08-00-cand-01 (16-December-2005)
|
|
Copyright : Geant4 Collaboration
|
|
Reference : NIM A 506 (2003), 250-303
|
|
WWW : http://cern.ch/geant4
|
|
*************************************************************
|
|
|
|
B01PhysicsList::SetCuts:CutLength : 1 (mm)
|
|
Going to assign importance: 1, to volume: cell_01
|
|
Going to assign importance: 2, to volume: cell_02
|
|
Going to assign importance: 4, to volume: cell_03
|
|
Going to assign importance: 8, to volume: cell_04
|
|
Going to assign importance: 16, to volume: cell_05
|
|
Going to assign importance: 32, to volume: cell_06
|
|
Going to assign importance: 64, to volume: cell_07
|
|
Going to assign importance: 128, to volume: cell_08
|
|
Going to assign importance: 256, to volume: cell_09
|
|
Going to assign importance: 512, to volume: cell_10
|
|
Going to assign importance: 1024, to volume: cell_11
|
|
Going to assign importance: 2048, to volume: cell_12
|
|
Going to assign importance: 4096, to volume: cell_13
|
|
Going to assign importance: 8192, to volume: cell_14
|
|
Going to assign importance: 16384, to volume: cell_15
|
|
Going to assign importance: 32768, to volume: cell_16
|
|
Going to assign importance: 65536, to volume: cell_17
|
|
Going to assign importance: 131072, to volume: cell_18
|
|
=== G4ProcessPlacer::AddProcessAsSecondDoIt: for: neutron
|
|
ProcessName: MScoreProcess
|
|
The initial Vectors:
|
|
GPIL Vector:
|
|
Decay
|
|
LCapture
|
|
LFission
|
|
inelastic
|
|
LElastic
|
|
Transportation
|
|
DoIt Vector:
|
|
Transportation
|
|
LElastic
|
|
inelastic
|
|
LFission
|
|
LCapture
|
|
Decay
|
|
The final Vectors:
|
|
GPIL Vector:
|
|
Decay
|
|
LCapture
|
|
LFission
|
|
inelastic
|
|
LElastic
|
|
MScoreProcess
|
|
Transportation
|
|
DoIt Vector:
|
|
Transportation
|
|
MScoreProcess
|
|
LElastic
|
|
inelastic
|
|
LFission
|
|
LCapture
|
|
Decay
|
|
================================================
|
|
=== G4ProcessPlacer::AddProcessAsSecondDoIt: for: neutron
|
|
ProcessName: MassImportanceProcess
|
|
The initial Vectors:
|
|
GPIL Vector:
|
|
Decay
|
|
LCapture
|
|
LFission
|
|
inelastic
|
|
LElastic
|
|
MScoreProcess
|
|
Transportation
|
|
DoIt Vector:
|
|
Transportation
|
|
MScoreProcess
|
|
LElastic
|
|
inelastic
|
|
LFission
|
|
LCapture
|
|
Decay
|
|
The final Vectors:
|
|
GPIL Vector:
|
|
Decay
|
|
LCapture
|
|
LFission
|
|
inelastic
|
|
LElastic
|
|
MScoreProcess
|
|
MassImportanceProcess
|
|
Transportation
|
|
DoIt Vector:
|
|
Transportation
|
|
MassImportanceProcess
|
|
MScoreProcess
|
|
LElastic
|
|
inelastic
|
|
LFission
|
|
LCapture
|
|
Decay
|
|
================================================
|
|
|
|
conv: Total cross sections has a good parametrisation from 1.5 MeV to 100 GeV for all Z;
|
|
sampling secondary e+e- according to the Bethe-Heitler model
|
|
tables are built for gamma
|
|
Lambda tables from 1.022 MeV to 100 GeV in 100 bins.
|
|
|
|
compt: Total cross sections has a good parametrisation from 10 KeV to (100/Z) GeV
|
|
Sampling according Klein-Nishina model
|
|
tables are built for gamma
|
|
Lambda tables from 100 eV to 100 GeV in 90 bins.
|
|
|
|
phot: Total cross sections from Sandia parametrisation.
|
|
|
|
msc: Model variant of multiple scattering for e-
|
|
Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|
Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
|
|
|
|
eIoni: tables are built for e-
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Delta cross sections from Moller+Bhabha, good description from 1 KeV to 100 GeV.
|
|
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
|
|
|
|
eBrem: tables are built for e-
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Total cross sections from a parametrisation based on the EEDL data library.
|
|
Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV.
|
|
|
|
eIoni: tables are built for e+
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Delta cross sections from Moller+Bhabha, good description from 1 KeV to 100 GeV.
|
|
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
|
|
|
|
eBrem: tables are built for e+
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Total cross sections from a parametrisation based on the EEDL data library.
|
|
Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV.
|
|
|
|
annihil: Heilter model of formula of annihilation into 2 photons
|
|
tables are built for e+
|
|
Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|
|
|
msc: Model variant of multiple scattering for proton
|
|
Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|
Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
|
|
|
|
hIoni: tables are built for proton
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Scaling relation is used to proton dE/dx and range
|
|
Bether-Bloch model for Escaled > 2 MeV, ICRU49 parametrisation for protons below.
|
|
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
|
|
|
|
msc: Model variant of multiple scattering for GenericIon
|
|
|
|
msc: Model variant of multiple scattering for mu+
|
|
Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|
Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
|
|
|
|
muIoni: tables are built for mu+
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below,
|
|
radiative corrections for E > 1 GeV
|
|
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
|
|
|
|
muBrems: tables are built for mu+
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Parametrised model
|
|
|
|
muPairProd: tables are built for mu+
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Parametrised model
|
|
|
|
muIoni: tables are built for mu-
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below,
|
|
radiative corrections for E > 1 GeV
|
|
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
|
|
|
|
muBrems: tables are built for mu-
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Parametrised model
|
|
|
|
muPairProd: tables are built for mu-
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Parametrised model
|
|
|
|
msc: Model variant of multiple scattering for pi-
|
|
Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|
Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
|
|
Volume name | Importance| Tr.Entering| Population| Collisions| Coll*WGT| NumWGTedE| FluxWGTedE| Av.Tr.WGT|
|
|
cell_01_rep:0............ | 1 | 111 | 134 | 131 | 131 | 7.7860235 | 9.1470607 | 1 |
|
|
cell_02_rep:0............ | 2 | 89 | 173 | 191 | 95.5 | 6.5725833 | 8.4009087 | 1 |
|
|
cell_03_rep:0............ | 4 | 94 | 198 | 195 | 48.75 | 8.1266652 | 8.7051742 | 1 |
|
|
cell_04_rep:0............ | 8 | 121 | 249 | 258 | 32.25 | 6.2161377 | 8.2818871 | 1 |
|
|
cell_05_rep:0............ | 16 | 158 | 327 | 404 | 25.25 | 5.7902782 | 7.8825536 | 1 |
|
|
cell_06_rep:0............ | 32 | 172 | 381 | 422 | 13.1875 | 5.7466488 | 7.8354734 | 1 |
|
|
cell_07_rep:0............ | 64 | 192 | 394 | 578 | 9.03125 | 0.27715221 | 6.8450076 | 1 |
|
|
cell_08_rep:0............ | 128 | 216 | 445 | 649 | 5.0703125 | 5.0240389 | 6.7365735 | 1 |
|
|
cell_09_rep:0............ | 256 | 246 | 521 | 825 | 3.2226562 | 4.6137525 | 6.3768025 | 1 |
|
|
cell_10_rep:0............ | 512 | 244 | 548 | 781 | 1.5253906 | 5.1560281 | 6.6650097 | 1 |
|
|
cell_11_rep:0............ | 1024 | 277 | 555 | 770 | 0.75195312 | 0.63315862 | 6.4423602 | 1 |
|
|
cell_12_rep:0............ | 2048 | 319 | 653 | 952 | 0.46484375 | 4.6419804 | 6.6177668 | 1 |
|
|
cell_13_rep:0............ | 4096 | 326 | 688 | 1044 | 0.25488281 | 3.8347969 | 6.3132198 | 1 |
|
|
cell_14_rep:0............ | 8192 | 315 | 654 | 998 | 0.12182617 | 0.23732449 | 6.1765661 | 1 |
|
|
cell_15_rep:0............ | 16384 | 307 | 623 | 1032 | 0.062988281 | 3.2698756 | 5.8998212 | 1 |
|
|
cell_16_rep:0............ | 32768 | 313 | 644 | 1035 | 0.031585693 | 0.13643685 | 5.8093517 | 1 |
|
|
cell_17_rep:0............ | 65536 | 345 | 722 | 1123 | 0.01713562 | 0.08543507 | 5.8104435 | 1 |
|
|
cell_18_rep:0............ | 131072 | 304 | 723 | 1168 |0.0089111328 | 0.82062282 | 5.6784205 | 1 |
|
|
rest_rep:0............... | 131072 | 346 | 346 | 0 | 0 | 0 | 0 | 0 |
|
|
shieldWorld_rep:0........ | 1 | 4 | 104 | 0 | 0 | 10 | 10 | 1 |
|
|
=== G4ProcessPlacer::RemoveProcess: for: neutron
|
|
ProcessName: MassImportanceProcess, will be removed!
|
|
The initial Vectors:
|
|
GPIL Vector:
|
|
Decay
|
|
LCapture
|
|
LFission
|
|
inelastic
|
|
LElastic
|
|
MScoreProcess
|
|
MassImportanceProcess
|
|
Transportation
|
|
DoIt Vector:
|
|
Transportation
|
|
MassImportanceProcess
|
|
MScoreProcess
|
|
LElastic
|
|
inelastic
|
|
LFission
|
|
LCapture
|
|
Decay
|
|
The final Vectors:
|
|
GPIL Vector:
|
|
Decay
|
|
LCapture
|
|
LFission
|
|
inelastic
|
|
LElastic
|
|
MScoreProcess
|
|
Transportation
|
|
DoIt Vector:
|
|
Transportation
|
|
MScoreProcess
|
|
LElastic
|
|
inelastic
|
|
LFission
|
|
LCapture
|
|
Decay
|
|
================================================
|
|
=== G4ProcessPlacer::RemoveProcess: for: neutron
|
|
ProcessName: MScoreProcess, will be removed!
|
|
The initial Vectors:
|
|
GPIL Vector:
|
|
Decay
|
|
LCapture
|
|
LFission
|
|
inelastic
|
|
LElastic
|
|
MScoreProcess
|
|
Transportation
|
|
DoIt Vector:
|
|
Transportation
|
|
MScoreProcess
|
|
LElastic
|
|
inelastic
|
|
LFission
|
|
LCapture
|
|
Decay
|
|
The final Vectors:
|
|
GPIL Vector:
|
|
Decay
|
|
LCapture
|
|
LFission
|
|
inelastic
|
|
LElastic
|
|
Transportation
|
|
DoIt Vector:
|
|
Transportation
|
|
LElastic
|
|
inelastic
|
|
LFission
|
|
LCapture
|
|
Decay
|
|
================================================
|