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geant4/examples/extended/biasing/B01/exampleB01.out
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Geant4 version Name: global-V09-00-02 (14-December-2007)
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
preparing importance sampling
creating istore
creating importance configurator
entering configure
importance configurator push_back
pushed
vsampler configurator loop
looping 1
sampler configurator
entering importance configure, paraflag 0
creating importance process, paraflag is: 0
importance process paraflag is: 0
=== G4ProcessPlacer::AddProcessAsSecondDoIt: for: neutron
Modifying Process Order for ProcessName: ImportanceProcess
The initial AlongStep Vectors:
GPIL Vector:
Transportation
DoIt Vector:
Transportation
The initial PostStep Vectors:
GPIL Vector:
Decay
HadronCapture
HadronFission
inelastic
HadronElastic
Transportation
DoIt Vector:
Transportation
HadronElastic
inelastic
HadronFission
HadronCapture
Decay
The final AlongStep Vectors:
GPIL Vector:
ImportanceProcess
Transportation
DoIt Vector:
Transportation
ImportanceProcess
The final PostStep Vectors:
GPIL Vector:
Decay
HadronCapture
HadronFission
inelastic
HadronElastic
ImportanceProcess
Transportation
DoIt Vector:
Transportation
ImportanceProcess
HadronElastic
inelastic
HadronFission
HadronCapture
Decay
================================================
configure preconf
conv: Total cross sections has a good parametrisation from 1.5 MeV to 100 GeV for all Z;
sampling secondary e+e- according 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.
Sampling according PhotoElectric model
msc: Model variant of multiple scattering for e-
Lambda tables from 100 eV to 100 TeV in 120 bins.
LateralDisplacementFlag= 1 Skin= 0
Boundary/stepping algorithm is active with RangeFactor= 0.02 Step limit type 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 and sampling from MollerBhabha model
Good description from 1 KeV to 100 GeV.
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 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 and sampling from StandBrem model (based on the EEDL data library)
Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV. LPM flag 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 and sampling from MollerBhabha model
Good description from 1 KeV to 100 GeV.
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 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 and sampling from StandBrem model (based on the EEDL data library)
Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV. LPM flag 1
annihil: Sampling according eplus2gg model
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.
LateralDisplacementFlag= 1 Skin= 0
Boundary/stepping algorithm is active with RangeFactor= 0.02 Step limit type 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 from proton dE/dx and range.
Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV
Parametrisation from Bragg for protons below.
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1
msc: Model variant of multiple scattering for GenericIon
LateralDisplacementFlag= 0 Skin= 0
Boundary/stepping algorithm is active with RangeFactor= 0.2 Step limit type 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 from proton dE/dx and range.
Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV
Parametrisation from Bragg for protons below.
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1
msc: Model variant of multiple scattering for mu+
Lambda tables from 100 eV to 100 TeV in 120 bins.
LateralDisplacementFlag= 1 Skin= 0
Boundary/stepping algorithm is active with RangeFactor= 0.02 Step limit type 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, fluct: 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, fluct: 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 from proton dE/dx and range.
Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV
Parametrisation from Bragg for protons below.
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1
msc: Model variant of multiple scattering for pi-
Lambda tables from 100 eV to 100 TeV in 120 bins.
LateralDisplacementFlag= 1 Skin= 0
Boundary/stepping algorithm is active with RangeFactor= 0.02 Step limit type 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 from proton dE/dx and range.
Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV
Parametrisation from Bragg for protons below.
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1
++ ConcreteSD/Collisions id 0
++ ConcreteSD/CollWeight id 1
++ ConcreteSD/Population id 2
++ ConcreteSD/TrackEnter id 3
++ ConcreteSD/SL id 4
++ ConcreteSD/SLW id 5
++ ConcreteSD/SLWE id 6
++ ConcreteSD/SLW_V id 7
++ ConcreteSD/SLWE_V id 8
### Run 0 start.
###### EndOfRunAction
=============================================================
Number of event processed : 100
=============================================================
Volume | Tr.Entering | Population | Collisions | Coll*WGT | NumWGTedE | FluxWGTedE | Av.Tr.WGT | SL | SLW | SLW_v | SLWE | SLWE_v |
cell_00 | 15 | 115 | 0 | 0 | 6.1693238 | 7.188295 | 1 | 2532.137 | 2532.137 | 78.12431 | 18201.747 | 481.97417 |
cell_01 | 110 | 136 | 144 | 144 | 7.5216138 | 8.7754593 | 1 | 11872.863 | 11872.863 | 334.63119 | 104189.82 | 2516.9666 |
cell_02 | 74 | 196 | 217 | 108.5 | 8.1052514 | 8.7570374 | 0.5 | 17778.519 | 8889.2597 | 233.54288 | 77843.579 | 1892.9237 |
cell_03 | 91 | 210 | 207 | 51.75 | 7.5922639 | 8.5918388 | 0.25 | 19594.449 | 4898.6122 | 135.58275 | 42088.086 | 1029.38 |
cell_04 | 117 | 279 | 378 | 47.25 | 6.2266601 | 7.7116445 | 0.125 | 30673.893 | 3834.2366 | 121.13123 | 29568.269 | 754.243 |
cell_05 | 133 | 318 | 437 | 27.3125 | 5.7489132 | 7.5024664 | 0.0625 | 32642.28 | 2040.1425 | 68.533945 | 15306.101 | 393.9957 |
cell_06 | 151 | 333 | 480 | 15 | 5.1433918 | 7.0956906 | 0.03125 | 36018.114 | 1125.5661 | 40.777795 | 7986.6686 | 209.73618 |
cell_07 | 177 | 412 | 636 | 9.9375 | 0.066616337 | 6.705372 | 0.015625 | 46841.617 | 731.90027 | 1965.7765 | 4907.6636 | 130.95283 |
cell_08 | 197 | 449 | 704 | 5.5 | 3.6435456 | 6.1452679 | 0.0078125 | 50071.975 | 391.18731 | 18.16726 | 2403.9508 | 66.19324 |
cell_09 | 224 | 510 | 876 | 3.421875 | 3.8825485 | 5.8797423 | 0.00390625 | 55829.968 | 218.08581 | 9.3342389 | 1282.2884 | 36.240635 |
cell_10 | 246 | 533 | 881 | 1.7207031 | 3.8256521 | 5.9375623 | 0.001953125 | 57222.209 | 111.76213 | 4.8739454 | 663.59459 | 18.646019 |
cell_11 | 255 | 569 | 955 | 0.93261719 | 3.750962 | 5.6920465 | 0.0009765625 | 61230.795 | 59.795698 | 2.6064336 | 340.35989 | 9.7766332 |
cell_12 | 301 | 647 | 1113 | 0.54345703 | 0.40008235 | 5.086439 | 0.00048828125 | 70839.28 | 34.589492 | 13.215827 | 175.93734 | 5.2874193 |
cell_13 | 353 | 789 | 1557 | 0.38012695 | 3.1708067 | 4.7100104 | 0.00024414062 | 92751.696 | 22.644457 | 1.0519334 | 106.65563 | 3.3354775 |
cell_14 | 387 | 823 | 1653 | 0.20178223 | 2.997233 | 4.4191157 | 0.00012207031 | 99295.668 | 12.121053 | 0.5754521 | 53.564337 | 1.724764 |
cell_15 | 421 | 920 | 1933 | 0.11798096 | 0.16704108 | 4.1903824 | 6.1035156e-05 | 109936.62 | 6.7099985 | 5.5391092 | 28.11746 | 0.92525875 |
cell_16 | 466 | 1001 | 1987 | 0.060638428 | 2.7742618 | 4.1818373 | 3.0517578e-05 | 115154.22 | 3.5142278 | 0.17524981 | 14.695929 | 0.48618886 |
cell_17 | 527 | 1160 | 2312 | 0.03527832 | 0.12747609 | 4.0136176 | 1.5258789e-05 | 131119.17 | 2.0007197 | 2.118756 | 8.0301238 | 0.27009073 |
cell_18 | 538 | 1264 | 2527 | 0.01927948 | 2.4519093 | 3.9615137 | 7.6293945e-06 | 143738.51 | 1.0966378 | 0.060193964 | 4.3443456 | 0.14759014 |
cell_19 | 596 | 596 | 0 | 0 | 2.7600991 | 4.1615587 | 7.6293945e-06 | 85856.912 | 0.65503626 | 0.032889241 | 2.7259719 | 0.090777566 |
=============================================
=== G4ProcessPlacer::RemoveProcess: for: neutron
ProcessName: ImportanceProcess, will be removed!
The initial AlongStep Vectors:
GPIL Vector:
ImportanceProcess
Transportation
DoIt Vector:
Transportation
ImportanceProcess
The initial PostStep Vectors:
GPIL Vector:
Decay
HadronCapture
HadronFission
inelastic
HadronElastic
ImportanceProcess
Transportation
DoIt Vector:
Transportation
ImportanceProcess
HadronElastic
inelastic
HadronFission
HadronCapture
Decay
The final AlongStep Vectors:
GPIL Vector:
Transportation
DoIt Vector:
Transportation
The final PostStep Vectors:
GPIL Vector:
Decay
HadronCapture
HadronFission
inelastic
HadronElastic
Transportation
DoIt Vector:
Transportation
HadronElastic
inelastic
HadronFission
HadronCapture
Decay
================================================