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geant4/examples/extended/biasing/B01/exampleB01.out
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Geant4 version Name: global-V08-00-04 (30-June-2006)
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
Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
hIoni: tables are built for anti_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 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
hIoni: tables are built for pi+
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 > 0.297504 MeV, ICRU49 parametrisation for protons below.
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
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
hIoni: tables are built for pi-
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 > 0.297504 MeV, ICRU49 parametrisation for protons below.
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
Volume name | Importance| Tr.Entering| Population| Collisions| Coll*WGT| NumWGTedE| FluxWGTedE| Av.Tr.WGT|
cell_01_rep:0............ | 1 | 113 | 133 | 113 | 113 | 8.4732787 | 9.1010333 | 1 |
cell_02_rep:0............ | 2 | 72 | 163 | 200 | 100 | 4.323174 | 8.705577 | 1 |
cell_03_rep:0............ | 4 | 85 | 178 | 221 | 55.25 | 5.7181907 | 8.1739911 | 1 |
cell_04_rep:0............ | 8 | 104 | 214 | 250 | 31.25 | 6.2701176 | 8.0477481 | 1 |
cell_05_rep:0............ | 16 | 111 | 235 | 288 | 18 | 6.2358927 | 7.7232756 | 1 |
cell_06_rep:0............ | 32 | 122 | 255 | 283 | 8.84375 | 6.5801742 | 7.7215434 | 1 |
cell_07_rep:0............ | 64 | 130 | 280 | 375 | 5.859375 | 5.651861 | 7.0303223 | 1 |
cell_08_rep:0............ | 128 | 130 | 267 | 335 | 2.6171875 | 5.6877812 | 7.0891822 | 1 |
cell_09_rep:0............ | 256 | 144 | 297 | 475 | 1.8554688 | 4.9052988 | 6.4262423 | 1 |
cell_10_rep:0............ | 512 | 156 | 327 | 464 | 0.90625 | 4.9657552 | 6.5502973 | 1 |
cell_11_rep:0............ | 1024 | 189 | 373 | 541 | 0.52832031 | 0.036775942 | 6.4250402 | 1 |
cell_12_rep:0............ | 2048 | 202 | 443 | 596 | 0.29101562 | 4.9093467 | 6.3738032 | 1 |
cell_13_rep:0............ | 4096 | 226 | 459 | 636 | 0.15527344 | 3.7290047 | 5.8188979 | 1 |
cell_14_rep:0............ | 8192 | 269 | 554 | 935 | 0.11413574 | 4.0605216 | 5.6795257 | 1 |
cell_15_rep:0............ | 16384 | 300 | 614 | 1095 | 0.066833496 | 0.089155765 | 5.1283107 | 1 |
cell_16_rep:0............ | 32768 | 371 | 749 | 1427 | 0.043548584 | 0.042230138 | 4.713344 | 1 |
cell_17_rep:0............ | 65536 | 382 | 779 | 1549 | 0.023635864 | 2.7935776 | 4.1630758 | 1 |
cell_18_rep:0............ | 131072 | 312 | 719 | 1516 | 0.011566162 | 0.14353462 | 4.1215867 | 1 |
rest_rep:0............... | 131072 | 333 | 333 | 0 | 0 | 0 | 0 | 0 |
shieldWorld_rep:0........ | 1 | 15 | 114 | 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
================================================