lars/geant4
1
0
Fork 0
Code Issues Pull Requests Actions Packages Projects Releases Wiki Activity

Import Geant4 11.1.0.beta source tree

Browse Source
This commit is contained in:
Gabriele Cosmo
2022-07-01 10:44:02 +02:00
parent b3bf75a2a1
commit c07cea1fe0
2172 changed files with 183300 additions and 123938 deletions
Download Patch File Download Diff File Expand all files Collapse all files
examples/extended/biasing/B03/History
+10 -14
View File
@@ -1,20 +1,16 @@
-------------------------------------------------------------------
# Example B03 History
=========================================================
Geant4 - an Object-Oriented Toolkit for Simulation in HEP
=========================================================
See `CONTRIBUTING.rst` for details of **required** info/format for each entry,
which **must** added in reverse chronological order (newest at the top). It must **not**
be used as a substitute for writing good git commit messages!
Category History file
---------------------
This file should be used by G4 developers and category coordinators
to briefly summarize all major modifications introduced in the code
and keep track of all category-tags.
It DOES NOT substitute the CVS log-message one should put at every
committal in the CVS repository !
----------------------------------------------------------
* Reverse chronological order (last date on top), please *
----------------------------------------------------------
## 2021-12-10 Ben Morgan (B03-V11-00-00)
- Change to new Markdown History format
---
# History entries prior to 11.0
March 18th, 2021 Alberto Ribon - B03-V10-07-02
- B03PhysicsList : replaced G4HadronCaptureProcess with
examples/extended/biasing/B03/exampleB03.out
+112 -82
View File
@@ -11,7 +11,7 @@ Environment variable "G4FORCE_RUN_MANAGER_TYPE" enabled with value == Serial. Fo
**************************************************************
Geant4 version Name: geant4-11-00-patch-02 (25-May-2022)
Geant4 version Name: geant4-11-01-beta-01 (30-June-2022)
Copyright : Geant4 Collaboration
References : NIM A 506 (2003), 250-303
: IEEE-TNS 53 (2006), 270-278
@@ -98,6 +98,7 @@ B03PhysicsList::SetCuts:CutLength : 1 (mm)
LPM effect enabled 1
Enable creation and use of sampling tables 0
Apply cuts on all EM processes 0
Use combined TransportationWithMsc Disabled
Use general process 0
Enable linear polarisation for gamma 0
Enable sampling of quantum entanglement 0
@@ -115,7 +116,7 @@ Lowest triplet kinetic energy 1 MeV
Enable sampling of gamma linear polarisation 0
5D gamma conversion model type 0
5D gamma conversion model on isolated ion 0
Livermore data directory livermore
Livermore data directory epics_2017
=======================================================================
====== Ionisation Parameters ========
=======================================================================
@@ -125,8 +126,9 @@ Step function for light ions (0.2, 0.1 mm)
Step function for general ions (0.2, 0.1 mm)
Lowest e+e- kinetic energy 1 keV
Lowest muon/hadron kinetic energy 1 keV
Fluctuations of dE/dx are enabled 1
Use ICRU90 data 0
Fluctuations of dE/dx are enabled 1
Type of fluctuation model 1
Use built-in Birks satuaration 0
Build CSDA range enabled 0
Use cut as a final range enabled 0
@@ -181,10 +183,10 @@ msc: for e- SubType= 10
UrbanMsc : Emin= 0 eV Emax= 100 TeV Nbins=84 100 eV - 100 TeV
StepLim=UseSafety Rfact=0.04 Gfact=2.5 Sfact=0.6 DispFlag:1 Skin=1 Llim=1 mm
eIoni: for e- XStype:1 SubType=2
eIoni: for e- XStype:3 SubType=2
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 1
StepFunction=(0.2, 1 mm), integ: 1, fluct: 1, linLossLim= 0.01
StepFunction=(0.2, 1 mm), integ: 3, fluct: 1, linLossLim= 0.01
===== EM models for the G4Region DefaultRegionForTheWorld ======
MollerBhabha : Emin= 0 eV Emax= 100 TeV
@@ -201,10 +203,10 @@ msc: for e+ SubType= 10
UrbanMsc : Emin= 0 eV Emax= 100 TeV Nbins=84 100 eV - 100 TeV
StepLim=UseSafety Rfact=0.04 Gfact=2.5 Sfact=0.6 DispFlag:1 Skin=1 Llim=1 mm
eIoni: for e+ XStype:1 SubType=2
eIoni: for e+ XStype:3 SubType=2
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 1
StepFunction=(0.2, 1 mm), integ: 1, fluct: 1, linLossLim= 0.01
StepFunction=(0.2, 1 mm), integ: 3, fluct: 1, linLossLim= 0.01
===== EM models for the G4Region DefaultRegionForTheWorld ======
MollerBhabha : Emin= 0 eV Emax= 100 TeV
@@ -225,10 +227,10 @@ msc: for proton SubType= 10
UrbanMsc : Emin= 0 eV Emax= 100 TeV Nbins=84 100 eV - 100 TeV
StepLim=Minimal Rfact=0.2 Gfact=2.5 Sfact=0.6 DispFlag:0 Skin=1 Llim=1 mm
hIoni: for proton XStype:1 SubType=2
hIoni: for proton XStype:3 SubType=2
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 1
StepFunction=(0.2, 0.1 mm), integ: 1, fluct: 1, linLossLim= 0.01
StepFunction=(0.2, 0.1 mm), integ: 3, fluct: 1, linLossLim= 0.01
===== EM models for the G4Region DefaultRegionForTheWorld ======
Bragg : Emin= 0 eV Emax= 2 MeV
BetheBloch : Emin= 2 MeV Emax= 100 TeV
@@ -238,10 +240,10 @@ msc: for GenericIon SubType= 10
UrbanMsc : Emin= 0 eV Emax= 100 TeV
StepLim=Minimal Rfact=0.2 Gfact=2.5 Sfact=0.6 DispFlag:0 Skin=1 Llim=1 mm
hIoni: for GenericIon XStype:1 SubType=2
hIoni: for GenericIon XStype:3 SubType=2
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 1
StepFunction=(0.2, 0.1 mm), integ: 1, fluct: 1, linLossLim= 0.01
StepFunction=(0.2, 0.1 mm), integ: 3, fluct: 1, linLossLim= 0.01
===== EM models for the G4Region DefaultRegionForTheWorld ======
Bragg : Emin= 0 eV Emax= 2 MeV
BetheBloch : Emin= 2 MeV Emax= 100 TeV
@@ -251,10 +253,10 @@ msc: for alpha SubType= 10
UrbanMsc : Emin= 0 eV Emax= 100 TeV
StepLim=Minimal Rfact=0.2 Gfact=2.5 Sfact=0.6 DispFlag:0 Skin=1 Llim=1 mm
hIoni: for alpha XStype:1 SubType=2
hIoni: for alpha XStype:3 SubType=2
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 1
StepFunction=(0.2, 0.1 mm), integ: 1, fluct: 1, linLossLim= 0.01
StepFunction=(0.2, 0.1 mm), integ: 3, fluct: 1, linLossLim= 0.01
===== EM models for the G4Region DefaultRegionForTheWorld ======
Bragg : Emin= 0 eV Emax=7.9452 MeV
BetheBloch : Emin=7.9452 MeV Emax= 100 TeV
@@ -264,10 +266,10 @@ msc: for anti_proton SubType= 10
UrbanMsc : Emin= 0 eV Emax= 100 TeV Nbins=84 100 eV - 100 TeV
StepLim=Minimal Rfact=0.2 Gfact=2.5 Sfact=0.6 DispFlag:0 Skin=1 Llim=1 mm
hIoni: for anti_proton XStype:1 SubType=2
hIoni: for anti_proton XStype:3 SubType=2
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 1
StepFunction=(0.2, 0.1 mm), integ: 1, fluct: 1, linLossLim= 0.01
StepFunction=(0.2, 0.1 mm), integ: 3, fluct: 1, linLossLim= 0.01
===== EM models for the G4Region DefaultRegionForTheWorld ======
ICRU73QO : Emin= 0 eV Emax= 2 MeV
BetheBloch : Emin= 2 MeV Emax= 100 TeV
@@ -277,10 +279,10 @@ msc: for kaon+ SubType= 10
UrbanMsc : Emin= 0 eV Emax= 100 TeV Nbins=84 100 eV - 100 TeV
StepLim=Minimal Rfact=0.2 Gfact=2.5 Sfact=0.6 DispFlag:0 Skin=1 Llim=1 mm
hIoni: for kaon+ XStype:1 SubType=2
hIoni: for kaon+ XStype:3 SubType=2
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 1
StepFunction=(0.2, 0.1 mm), integ: 1, fluct: 1, linLossLim= 0.01
StepFunction=(0.2, 0.1 mm), integ: 3, fluct: 1, linLossLim= 0.01
===== EM models for the G4Region DefaultRegionForTheWorld ======
Bragg : Emin= 0 eV Emax=1.05231 MeV
BetheBloch : Emin=1.05231 MeV Emax= 100 TeV
@@ -290,10 +292,10 @@ msc: for kaon- SubType= 10
UrbanMsc : Emin= 0 eV Emax= 100 TeV Nbins=84 100 eV - 100 TeV
StepLim=Minimal Rfact=0.2 Gfact=2.5 Sfact=0.6 DispFlag:0 Skin=1 Llim=1 mm
hIoni: for kaon- XStype:1 SubType=2
hIoni: for kaon- XStype:3 SubType=2
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 1
StepFunction=(0.2, 0.1 mm), integ: 1, fluct: 1, linLossLim= 0.01
StepFunction=(0.2, 0.1 mm), integ: 3, fluct: 1, linLossLim= 0.01
===== EM models for the G4Region DefaultRegionForTheWorld ======
ICRU73QO : Emin= 0 eV Emax=1.05231 MeV
BetheBloch : Emin=1.05231 MeV Emax= 100 TeV
@@ -303,14 +305,13 @@ msc: for mu+ SubType= 10
UrbanMsc : Emin= 0 eV Emax= 100 TeV Nbins=84 100 eV - 100 TeV
StepLim=Minimal Rfact=0.2 Gfact=2.5 Sfact=0.6 DispFlag:0 Skin=1 Llim=1 mm
muIoni: for mu+ XStype:1 SubType=2
muIoni: for mu+ XStype:3 SubType=2
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 1
StepFunction=(0.2, 0.1 mm), integ: 1, fluct: 1, linLossLim= 0.01
StepFunction=(0.2, 0.1 mm), integ: 3, fluct: 1, linLossLim= 0.01
===== EM models for the G4Region DefaultRegionForTheWorld ======
Bragg : Emin= 0 eV Emax= 200 keV
BetheBloch : Emin= 200 keV Emax= 1 GeV
MuBetheBloch : Emin= 1 GeV Emax= 100 TeV
MuBetheBloch : Emin= 200 keV Emax= 100 TeV
muBrems: for mu+ XStype:1 SubType=3
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
@@ -321,7 +322,7 @@ muBrems: for mu+ XStype:1 SubType=3
muPairProd: for mu+ XStype:1 SubType=4
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 0
Sampling table 21x1001 from 1 GeV to 100 TeV
Sampling table 21x1001 from 0.85 GeV to 100 TeV
===== EM models for the G4Region DefaultRegionForTheWorld ======
muPairProd : Emin= 0 eV Emax= 100 TeV ModifiedMephi
@@ -330,14 +331,13 @@ msc: for mu- SubType= 10
UrbanMsc : Emin= 0 eV Emax= 100 TeV Nbins=84 100 eV - 100 TeV
StepLim=Minimal Rfact=0.2 Gfact=2.5 Sfact=0.6 DispFlag:0 Skin=1 Llim=1 mm
muIoni: for mu- XStype:1 SubType=2
muIoni: for mu- XStype:3 SubType=2
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 1
StepFunction=(0.2, 0.1 mm), integ: 1, fluct: 1, linLossLim= 0.01
StepFunction=(0.2, 0.1 mm), integ: 3, fluct: 1, linLossLim= 0.01
===== EM models for the G4Region DefaultRegionForTheWorld ======
ICRU73QO : Emin= 0 eV Emax= 200 keV
BetheBloch : Emin= 200 keV Emax= 1 GeV
MuBetheBloch : Emin= 1 GeV Emax= 100 TeV
MuBetheBloch : Emin= 200 keV Emax= 100 TeV
muBrems: for mu- XStype:1 SubType=3
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
@@ -348,7 +348,7 @@ muBrems: for mu- XStype:1 SubType=3
muPairProd: for mu- XStype:1 SubType=4
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 0
Sampling table 21x1001 from 1 GeV to 100 TeV
Sampling table 21x1001 from 0.85 GeV to 100 TeV
===== EM models for the G4Region DefaultRegionForTheWorld ======
muPairProd : Emin= 0 eV Emax= 100 TeV ModifiedMephi
@@ -357,10 +357,10 @@ msc: for pi+ SubType= 10
UrbanMsc : Emin= 0 eV Emax= 100 TeV Nbins=84 100 eV - 100 TeV
StepLim=Minimal Rfact=0.2 Gfact=2.5 Sfact=0.6 DispFlag:0 Skin=1 Llim=1 mm
hIoni: for pi+ XStype:1 SubType=2
hIoni: for pi+ XStype:3 SubType=2
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 1
StepFunction=(0.2, 0.1 mm), integ: 1, fluct: 1, linLossLim= 0.01
StepFunction=(0.2, 0.1 mm), integ: 3, fluct: 1, linLossLim= 0.01
===== EM models for the G4Region DefaultRegionForTheWorld ======
Bragg : Emin= 0 eV Emax=297.505 keV
BetheBloch : Emin=297.505 keV Emax= 100 TeV
@@ -370,10 +370,10 @@ msc: for pi- SubType= 10
UrbanMsc : Emin= 0 eV Emax= 100 TeV Nbins=84 100 eV - 100 TeV
StepLim=Minimal Rfact=0.2 Gfact=2.5 Sfact=0.6 DispFlag:0 Skin=1 Llim=1 mm
hIoni: for pi- XStype:1 SubType=2
hIoni: for pi- XStype:3 SubType=2
dE/dx and range tables from 100 eV to 100 TeV in 84 bins
Lambda tables from threshold to 100 TeV, 7 bins/decade, spline: 1
StepFunction=(0.2, 0.1 mm), integ: 1, fluct: 1, linLossLim= 0.01
StepFunction=(0.2, 0.1 mm), integ: 3, fluct: 1, linLossLim= 0.01
===== EM models for the G4Region DefaultRegionForTheWorld ======
ICRU73QO : Emin= 0 eV Emax=297.505 keV
BetheBloch : Emin=297.505 keV Emax= 100 TeV
@@ -386,192 +386,222 @@ hIoni: for pi- XStype:1 SubType=2
Process: hadElastic
Model: hElasticLHEP: 0 eV /n ---> 100 TeV/n
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: Binary Light Ion Cascade: 0 eV /n ---> 110 MeV/n
Model: QMDModel: 100 MeV/n ---> 10 GeV/n
Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV ---> 25.6 PeV
---------------------------------------------------
Hadronic Processes for anti_lambda
Process: hadElastic
Model: hElasticLHEP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: ANTI-FTFP: 0 eV ---> 20 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
---------------------------------------------------
Hadronic Processes for anti_neutron
Process: hadElastic
Model: hElasticLHEP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: ANTI-FTFP: 0 eV ---> 20 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
---------------------------------------------------
Hadronic Processes for anti_proton
Process: hadElastic
Model: hElasticLHEP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: ANTI-FTFP: 0 eV ---> 20 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
---------------------------------------------------
Hadronic Processes for deuteron
Process: hadElastic
Model: hElasticLHEP: 0 eV /n ---> 100 TeV/n
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: Binary Light Ion Cascade: 0 eV /n ---> 110 MeV/n
Model: QMDModel: 100 MeV/n ---> 10 GeV/n
Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV ---> 25.6 PeV
---------------------------------------------------
Hadronic Processes for kaon+
Process: hadElastic
Model: hElasticLHEP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: BertiniCascade: 0 eV ---> 22 MeV
Model: TheoFSGenerator: 19 GeV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
---------------------------------------------------
Hadronic Processes for kaon-
Process: hadElastic
Model: hElasticLHEP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: BertiniCascade: 0 eV ---> 22 MeV
Model: TheoFSGenerator: 19 GeV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
---------------------------------------------------
Hadronic Processes for lambda
Process: hadElastic
Model: hElasticLHEP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: BertiniCascade: 0 eV ---> 22 MeV
Model: TheoFSGenerator: 19 GeV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
---------------------------------------------------
Hadronic Processes for neutron
Process: hadElastic
Model: hElasticLHEP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: BertiniCascade: 0 eV ---> 22 MeV
Model: TheoFSGenerator: 19 GeV ---> 100 TeV
Cr_sctns: G4NeutronInelasticXS: 0 eV ---> 100 TeV
Process: nFission
Model: G4LFission: 0 eV ---> 2.88022e+295 J
Cr_sctns: ZeroXS: 0 eV ---> 100 TeV
Process: nCapture
Model: nRadCapture: 0 eV ---> 100 TeV
Cr_sctns: G4NeutronCaptureXS: 0 eV ---> 100 TeV
---------------------------------------------------
Hadronic Processes for pi+
Process: hadElastic
Model: hElasticLHEP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: BertiniCascade: 0 eV ---> 22 MeV
Model: TheoFSGenerator: 19 GeV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
---------------------------------------------------
Hadronic Processes for pi-
Process: hadElastic
Model: hElasticLHEP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: BertiniCascade: 0 eV ---> 22 MeV
Model: TheoFSGenerator: 19 GeV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
---------------------------------------------------
Hadronic Processes for proton
Process: hadElastic
Model: hElasticLHEP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: BertiniCascade: 0 eV ---> 22 MeV
Model: TheoFSGenerator: 19 GeV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
---------------------------------------------------
Hadronic Processes for sigma-
Process: hadElastic
Model: hElasticLHEP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: BertiniCascade: 0 eV ---> 22 MeV
Model: TheoFSGenerator: 19 GeV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
---------------------------------------------------
Hadronic Processes for triton
Process: hadElastic
Model: hElasticLHEP: 0 eV /n ---> 100 TeV/n
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 25.6 PeV
Process: inelastic
Model: Binary Light Ion Cascade: 0 eV /n ---> 110 MeV/n
Model: QMDModel: 100 MeV/n ---> 10 GeV/n
Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV ---> 25.6 PeV
================================================================
=======================================================================
====== Pre-compound/De-excitation Physics Parameters ========
=======================================================================
Type of pre-compound inverse x-section 3
Pre-compound model active 1
Pre-compound excitation low energy (MeV) 0.1
Pre-compound excitation high energy (MeV) 30
Pre-compound excitation low energy 100 keV
Pre-compound excitation high energy 30 MeV
Type of de-excitation inverse x-section 3
Type of de-excitation factory Evaporation+GEM
Number of de-excitation channels 68
Min excitation energy (keV) 0.01
Min energy per nucleon for multifragmentation (MeV) 2e+05
Limit excitation energy for Fermi BreakUp (MeV) 20
Min excitation energy 10 eV
Min energy per nucleon for multifragmentation 200 GeV
Limit excitation energy for Fermi BreakUp 20 MeV
Level density (1/MeV) 0.075
Use simple level density model 1
Use discrete excitation energy of the residual 0
Time limit for long lived isomeres (ns) 1
Use discrete excitation energy of the residual 1
Time limit for long lived isomeres 1 ns
Isomer production flag 1
Internal e- conversion flag 1
Store e- internal conversion data 0
@@ -583,18 +613,18 @@ Max 2J for sampling of angular correlations 10
=======================================================================
Type of pre-compound inverse x-section 3
Pre-compound model active 1
Pre-compound excitation low energy (MeV) 0.1
Pre-compound excitation high energy (MeV) 30
Pre-compound excitation low energy 100 keV
Pre-compound excitation high energy 30 MeV
Type of de-excitation inverse x-section 3
Type of de-excitation factory Evaporation+GEM
Number of de-excitation channels 68
Min excitation energy (keV) 0.01
Min energy per nucleon for multifragmentation (MeV) 2e+05
Limit excitation energy for Fermi BreakUp (MeV) 20
Min excitation energy 10 eV
Min energy per nucleon for multifragmentation 200 GeV
Limit excitation energy for Fermi BreakUp 20 MeV
Level density (1/MeV) 0.075
Use simple level density model 1
Use discrete excitation energy of the residual 0
Time limit for long lived isomeres (ns) 1
Use discrete excitation energy of the residual 1
Time limit for long lived isomeres 1 ns
Isomer production flag 1
Internal e- conversion flag 1
Store e- internal conversion data 0
@@ -616,7 +646,7 @@ Max 2J for sampling of angular correlations 10
*** G4Exception : GeomBias1001
issued by : G4ImportanceAlgorithm::Warning()
Calculate() - ipre_over_ipost ! in [0.25, 4].
ipre_over_ipost = 4096.
ipre_over_ipost = 16384.
*** This is just a warning message. ***
-------- WWWW -------- G4Exception-END --------- WWWW -------
@@ -636,24 +666,24 @@ ipre_over_ipost = 4096.
=============================================================
=============================================================
Volume | Tr.Entering | Population | Collisions | Coll*WGT | NumWGTedE | FluxWGTedE | Av.Tr.WGT | SL | SLW | SLW_v | SLWE | SLWE_v |
cell_00 | 42 | 137 | 0 | 0 | 0.00187798 | 2.58678 | 1 | 7435.72 | 7435.72 | 381201 | 19234.6 | 715.888 |
cell_01 | 143 | 169 | 326 | 326 | 0.00186836 | 4.71158 | 1 | 22601.2 | 22601.2 | 1.53793e+06 | 106487 | 2873.41 |
cell_02 | 180 | 299 | 884 | 442 | 0.000662167 | 3.01184 | 0.5 | 51114 | 25557 | 3.52414e+06 | 76973.5 | 2333.57 |
cell_03 | 300 | 452 | 1512 | 378 | 0.00122066 | 2.32281 | 0.25 | 83802.9 | 20950.7 | 1.27676e+06 | 48664.6 | 1558.49 |
cell_04 | 450 | 662 | 2359 | 294.875 | 0.000633263 | 1.75479 | 0.125 | 126114 | 15764.2 | 1.48076e+06 | 27662.9 | 937.708 |
cell_05 | 689 | 951 | 3835 | 239.688 | 0.000340383 | 1.31797 | 0.0625 | 192676 | 12042.3 | 1.71179e+06 | 15871.4 | 582.663 |
cell_06 | 985 | 1313 | 5763 | 180.094 | 0.000212153 | 0.971561 | 0.03125 | 276370 | 8636.57 | 1.57994e+06 | 8390.95 | 335.19 |
cell_07 | 1311 | 1750 | 7696 | 120.25 | 0.000159737 | 0.835298 | 0.015625 | 360035 | 5625.55 | 1.22257e+06 | 4699.01 | 195.29 |
cell_08 | 1569 | 2119 | 9819 | 76.7109 | 0.000144459 | 0.71372 | 0.0078125 | 457691 | 3575.71 | 770507 | 2552.06 | 111.307 |
cell_09 | 1913 | 2562 | 11987 | 46.8242 | 0.000109508 | 0.629828 | 0.00390625 | 536383 | 2095.25 | 533853 | 1319.65 | 58.4611 |
cell_10 | 2184 | 3018 | 14272 | 27.875 | 0.000104244 | 0.606641 | 0.00195312 | 632911 | 1236.15 | 322686 | 749.902 | 33.6382 |
cell_11 | 2477 | 3344 | 15561 | 15.1963 | 8.59806e-05 | 0.537942 | 0.000976562 | 683344 | 667.328 | 191946 | 358.984 | 16.5037 |
cell_12 | 2758 | 3757 | 18079 | 8.82764 | 7.70425e-05 | 0.461918 | 0.000488281 | 792784 | 387.102 | 112547 | 178.809 | 8.67088 |
cell_13 | 2937 | 4002 | 18859 | 4.60425 | 6.62855e-05 | 0.419788 | 0.000244141 | 824639 | 201.328 | 63615.7 | 84.5151 | 4.2168 |
cell_14 | 3097 | 4332 | 20204 | 2.46631 | 6.40584e-05 | 0.421251 | 0.00012207 | 870071 | 106.21 | 34811.1 | 44.741 | 2.22994 |
cell_15 | 3259 | 4573 | 21270 | 1.29822 | 6.33226e-05 | 0.416255 | 6.10352e-05 | 918808 | 56.0796 | 18431.5 | 23.3434 | 1.16713 |
cell_16 | 3403 | 4776 | 22598 | 0.689636 | 6.27419e-05 | 0.386088 | 3.05176e-05 | 964268 | 29.4271 | 9348.31 | 11.3615 | 0.586531 |
cell_17 | 3329 | 4835 | 21968 | 0.335205 | 5.95469e-05 | 0.361499 | 1.52588e-05 | 944928 | 14.4184 | 4563.87 | 5.21226 | 0.271764 |
cell_18 | 2349 | 4334 | 18483 | 0.141014 | 6.39378e-05 | 0.399177 | 7.62939e-06 | 804435 | 6.13735 | 1966.82 | 2.44989 | 0.125754 |
cell_19 | 1971 | 1971 | 0 | 0 | 9.72052e-05 | 0.58562 | 7.62939e-06 | 311518 | 2.37669 | 679.726 | 1.39184 | 0.0660729 |
cell_00 | 56 | 152 | 0 | 0 | 0.000766839 | 0.921708 | 1 | 9721.32 | 9721.32 | 608478 | 8960.22 | 466.605 |
cell_01 | 173 | 208 | 547 | 547 | 0.00484826 | 3.14426 | 1 | 31991.4 | 31991.4 | 624732 | 100589 | 3028.86 |
cell_02 | 203 | 317 | 1035 | 517.5 | 0.0012227 | 2.27579 | 0.5 | 59356.7 | 29678.4 | 1.82216e+06 | 67541.7 | 2227.96 |
cell_03 | 269 | 397 | 1533 | 383.25 | 0.000422849 | 1.52657 | 0.25 | 79601.5 | 19900.4 | 2.55338e+06 | 30379.3 | 1079.7 |
cell_04 | 344 | 486 | 1938 | 242.25 | 0.000262606 | 1.33691 | 0.125 | 94870.3 | 11858.8 | 2.16811e+06 | 15854.1 | 569.359 |
cell_05 | 461 | 672 | 2860 | 178.75 | 0.000242149 | 1.05964 | 0.0625 | 137935 | 8620.96 | 1.4589e+06 | 9135.12 | 353.272 |
cell_06 | 646 | 860 | 3868 | 120.875 | 0.000189489 | 0.84777 | 0.03125 | 188515 | 5891.11 | 1.10092e+06 | 4994.3 | 208.613 |
cell_07 | 829 | 1156 | 5386 | 84.1562 | 0.000123391 | 0.722229 | 0.015625 | 249949 | 3905.46 | 975923 | 2820.64 | 120.42 |
cell_08 | 1011 | 1402 | 6547 | 51.1484 | 0.000118855 | 0.676321 | 0.0078125 | 287631 | 2247.12 | 551115 | 1519.77 | 65.5026 |
cell_09 | 1185 | 1606 | 7377 | 28.8164 | 9.36548e-05 | 0.554573 | 0.00390625 | 322678 | 1260.46 | 333828 | 699.017 | 31.2646 |
cell_10 | 1310 | 1826 | 8380 | 16.3672 | 9.57533e-05 | 0.548476 | 0.00195312 | 367771 | 718.303 | 187793 | 393.972 | 17.9818 |
cell_11 | 1445 | 1988 | 9104 | 8.89062 | 0.000101425 | 0.54072 | 0.000976562 | 406881 | 397.345 | 98212 | 214.853 | 9.96117 |
cell_12 | 1627 | 2243 | 10552 | 5.15234 | 8.72255e-05 | 0.503437 | 0.000488281 | 472548 | 230.737 | 63328.8 | 116.161 | 5.52389 |
cell_13 | 1873 | 2544 | 11757 | 2.87036 | 8.14767e-05 | 0.471355 | 0.000244141 | 518180 | 126.509 | 35277.9 | 59.6305 | 2.87433 |
cell_14 | 2193 | 2998 | 13526 | 1.65112 | 7.61515e-05 | 0.453906 | 0.00012207 | 607180 | 74.1187 | 22186.7 | 33.6429 | 1.68955 |
cell_15 | 2387 | 3315 | 15362 | 0.937622 | 6.70198e-05 | 0.433793 | 6.10352e-05 | 670488 | 40.9233 | 13201.5 | 17.7523 | 0.884762 |
cell_16 | 2436 | 3443 | 16053 | 0.489899 | 6.45592e-05 | 0.42613 | 3.05176e-05 | 689631 | 21.0459 | 6833.21 | 8.96827 | 0.441147 |
cell_17 | 2352 | 3443 | 15435 | 0.235519 | 7.18192e-05 | 0.418871 | 1.52588e-05 | 682960 | 10.4211 | 3071.43 | 4.36512 | 0.220588 |
cell_18 | 1722 | 3191 | 13271 | 0.10125 | 8.22242e-05 | 0.48822 | 7.62939e-06 | 580127 | 4.42602 | 1297.99 | 2.16087 | 0.106726 |
cell_19 | 1492 | 1492 | 0 | 0 | 0.000133795 | 0.668888 | 7.62939e-06 | 237851 | 1.81466 | 419.959 | 1.2138 | 0.0561883 |
=============================================