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liuyihui 1 year ago
commit d6ebd65d0c
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      .README.txt
  2. 212
      .clang-format
  3. 1
      .gitignore
  4. 24
      .vscode/c_cpp_properties.json
  5. 5
      .vscode/settings.json
  6. 69
      CMakeLists.txt
  7. 12
      G4.code-workspace
  8. 21
      GNUmakefile
  9. 118
      History
  10. 172
      README
  11. 67
      exampleB1.cc
  12. 16
      exampleB1.in
  13. 917
      exampleB1.out
  14. 21
      include/ActionInitialization.hh
  15. 29
      include/DetectorConstruction.hh
  16. 31
      include/EventAction.hh
  17. 38
      include/PrimaryGeneratorAction.hh
  18. 35
      include/RunAction.hh
  19. 31
      include/SteppingAction.hh
  20. 16
      init_vis.mac
  21. 30
      run1.mac
  22. 27
      run2.mac
  23. 32
      src/ActionInitialization.cc
  24. 135
      src/DetectorConstruction.cc
  25. 20
      src/EventAction.cc
  26. 67
      src/PrimaryGeneratorAction.cc
  27. 107
      src/RunAction.cc
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      src/SteppingAction.cc
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      vis.mac

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///\file "B1/.README.txt"
///\brief Example B1 README page
/*! \page ExampleB1 Example %B1
This example demonstrates a very simple application where an energy
deposit is accounted in user actions and their associated objects
and a dose in a selected volume is calculated.
\section B1_s1 GEOMETRY DEFINITION
The geometry is constructed in the B1::DetectorConstruction class.
The setup consists of a an envelope of box shape containing two
volumes: a spherical cone and a trapezoid.
In this example we use some common materials materials for medical
applications. The envelope is made of water and the two inner volumes
are made from tissue and bone materials.
The materials are created with the help of the G4NistManager class,
which allows to build a material from the NIST database using their
names. Available materials and their compositions can be found in
<a href="http://geant4.web.cern.ch/geant4/UserDocumentation/UsersGuides
/ForApplicationDeveloper/html/apas10.html">
the Geant4 User's Guide for Application Developers, Appendix 10:
Geant4 Materials Database
</a>.
\section B1_s2 PHYSICS LIST
The particle's type and the physic processes which will be available
in this example are set in the QBBC physics list. This physics list
requires data files for electromagnetic and hadronic processes.
See more on installation of the datasets in
<a href="http://geant4.web.cern.ch/geant4/UserDocumentation/UsersGuides
/InstallationGuide/html/ch03s03.html">
Geant4 Installation Guide, Chapter 3.3: Note On Geant4 Datasets </a>.
The following datasets: G4LEDATA, G4LEVELGAMMADATA, G4NEUTRONXSDATA,
G4SAIDXSDATA and G4ENSDFSTATEDATA are mandatory for this example.
In addition the build-in interactive command:
\verbatim
/process/(in)activate processName
\endverbatim
allows to activate/inactivate the processes one by one.
\section B1_s3 ACTION INITALIZATION
A newly introduced class, B1::ActionInitialization, instantiates and registers
to Geant4 kernel all user action classes.
While in sequential mode the action classes are instatiated just once,
via invoking the method:
B1::ActionInitialization::Build()
in multi-threading mode the same method is invoked for each thread worker
and so all user action classes are defined thread-local.
A run action class is instantiated both thread-local
and global that's why its instance is created also in the method
B1::ActionInitialization::BuildForMaster()
which is invoked only in multi-threading mode.
\section B1_s4 PRIMARY GENERATOR
The primary generator is defined in the B1::PrimaryGeneratorAction class.
The default kinematics is a 6 MeV gamma, randomly distributed in front
of the envelope across 80% of the transverse (X,Y) envelope size.
This default setting can be changed via the Geant4 built-in commands
of the G4ParticleGun class.
\section B1_s5 DETECTOR RESPONSE
This example demonstrates a simple scoring implemented directly
in the user action classes. Alternative ways of scoring via Geant4 classes
can be found in the other examples.
The energy deposited is collected step by step for a selected volume
in B1::SteppingAction and accumulated event by event in B1::EventAction.
At end of event, the value acummulated in B1::EventAction is added in B1::RunAction
and summed over the whole run (see B1::EventAction::EndOfevent()).
Total dose deposited is computed at B1::RunAction::EndOfRunAction(),
and printed together with informations about the primary particle.
In multi-threading mode the energy accumulated in G4Accumulable objects per
workers is merged to the master in B1::RunAction::EndOfRunAction() and the final
result is printed on the screen.
G4Accumulable<G4double> type instead of G4double type is used for the B1::RunAction
data members in order to facilitate merging of the values accumulated on workers
to the master. Currently the accumulables have to be registered to G4AccumulablesManager
and G4AccumulablesManager::Merge() has to be called from the users code. This is planned
to be further simplified with a closer integration of G4Accumulable classes in
the Geant4 kernel next year.
An example of creating and computing new units (e.g., dose) is also shown
in the class constructor.
<hr>
The following paragraphs are common to all basic examples
\section B1_A VISUALISATION
The visualization manager is set via the G4VisExecutive class
in the main() function in exampleB1.cc.
The initialisation of the drawing is done via a set of /vis/ commands
in the macro vis.mac. This macro is automatically read from
the main function when the example is used in interactive running mode.
By default, vis.mac opens an OpenGL viewer (/vis/open OGL).
The user can change the initial viewer by commenting out this line
and instead uncommenting one of the other /vis/open statements, such as
HepRepFile or DAWNFILE (which produce files that can be viewed with the
HepRApp and DAWN viewers, respectively). Note that one can always
open new viewers at any time from the command line. For example, if
you already have a view in, say, an OpenGL window with a name
"viewer-0", then
\verbatim
/vis/open DAWNFILE
\endverbatim
then to get the same view
\verbatim
/vis/viewer/copyView viewer-0
\endverbatim
or to get the same view *plus* scene-modifications
\verbatim
/vis/viewer/set/all viewer-0
\endverbatim
then to see the result
\verbatim
/vis/viewer/flush
\endverbatim
The DAWNFILE, HepRepFile drivers are always available
(since they require no external libraries), but the OGL driver requires
that the Geant4 libraries have been built with the OpenGL option.
From Release 9.6 the vis.mac macro in example B1 has additional commands
that demonstrate additional functionality of the vis system, such as
displaying text, axes, scales, date, logo and shows how to change
viewpoint and style. Consider copying these to other examples or
your application. To see even more commands use help or
ls or browse the available UI commands in the Application
Developers Guide, Section 7.1.
For more information on visualization, including information on how to
install and run DAWN, OpenGL and HepRApp, see the visualization tutorials,
for example,\n
- <a href="http://geant4.slac.stanford.edu/Presentations/vis/G4OpenGLTutorial/G4OpenGLTutorial.html">
OpenGL Tutorial </a>
- <a href="http://geant4.slac.stanford.edu/Presentations/vis/G4DAWNTutorial/G4DAWNTutorial.html">
DAWN Tutorial </a>
- <a href="http://geant4.slac.stanford.edu/Presentations/vis/G4HepRAppTutorial/G4HepRAppTutorial.html">
HepRApp Tutorial </a>
The tracks are automatically drawn at the end of each event, accumulated
for all events and erased at the beginning of the next run.
\section B1_B USER INTERFACES
The user command interface is set via the G4UIExecutive class
in the main() function in exampleB1.cc
The selection of the user command interface is then done automatically
according to the Geant4 configuration or it can be done explicitly via
the third argument of the G4UIExecutive constructor (see exampleB4a.cc).
\section B1_C HOW TO RUN
- Execute exampleB1 in the 'interactive mode' with visualization
\verbatim
% exampleB1
and type in the commands from run1.mac line by line:
Idle> /control/verbose 2
Idle> /tracking/verbose 1
Idle> /run/beamOn 10
Idle> ...
Idle> exit
\endverbatim
or
\verbatim
Idle> /control/execute run1.mac
....
Idle> exit
\endverbatim
- Execute exampleB1 in the 'batch' mode from macro files
(without visualization)
\verbatim
% exampleB1 run2.mac
% exampleB1 exampleB1.in > exampleB1.out
\endverbatim
*/

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@ -0,0 +1 @@
build/

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{
"configurations": [
{
"name": "Win32",
"includePath": [
"${default}",
"${workspaceFolder}/include",
"D:/Geant4/dist/include/Geant4"
],
"defines": [
"_DEBUG",
"UNICODE",
"_UNICODE"
],
"windowsSdkVersion": "10.0.19041.0",
"compilerPath": "D:/Microsoft/VisualStudio/2022/Community/VC/Tools/MSVC/14.31.31103/bin/Hostx64/x64/cl.exe",
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}
}

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#----------------------------------------------------------------------------
# Setup the project
cmake_minimum_required(VERSION 3.16...3.21)
project(B1)
#----------------------------------------------------------------------------
# Find Geant4 package, activating all available UI and Vis drivers by default
# You can set WITH_GEANT4_UIVIS to OFF via the command line or ccmake/cmake-gui
# to build a batch mode only executable
#
option(WITH_GEANT4_UIVIS "Build example with Geant4 UI and Vis drivers" ON)
if(WITH_GEANT4_UIVIS)
find_package(Geant4 REQUIRED ui_all vis_all)
else()
find_package(Geant4 REQUIRED)
endif()
#----------------------------------------------------------------------------
# Setup Geant4 include directories and compile definitions
# Setup include directory for this project
#
include(${Geant4_USE_FILE})
include_directories(${PROJECT_SOURCE_DIR}/include)
#----------------------------------------------------------------------------
# Locate sources and headers for this project
# NB: headers are included so they will show up in IDEs
#
file(GLOB sources ${PROJECT_SOURCE_DIR}/src/*.cc)
file(GLOB headers ${PROJECT_SOURCE_DIR}/include/*.hh)
#----------------------------------------------------------------------------
# Add the executable, and link it to the Geant4 libraries
#
add_executable(exampleB1 exampleB1.cc ${sources} ${headers})
target_link_libraries(exampleB1 ${Geant4_LIBRARIES})
#----------------------------------------------------------------------------
# Copy all scripts to the build directory, i.e. the directory in which we
# build B1. This is so that we can run the executable directly because it
# relies on these scripts being in the current working directory.
#
set(EXAMPLEB1_SCRIPTS
exampleB1.in
exampleB1.out
init_vis.mac
run1.mac
run2.mac
vis.mac
)
foreach(_script ${EXAMPLEB1_SCRIPTS})
configure_file(
${PROJECT_SOURCE_DIR}/${_script}
${PROJECT_BINARY_DIR}/${_script}
COPYONLY
)
endforeach()
#----------------------------------------------------------------------------
# For internal Geant4 use - but has no effect if you build this
# example standalone
#
add_custom_target(B1 DEPENDS exampleB1)
#----------------------------------------------------------------------------
# Install the executable to 'bin' directory under CMAKE_INSTALL_PREFIX
#
install(TARGETS exampleB1 DESTINATION bin)

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{
"folders": [
{
"path": "."
}
],
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"files.associations": {
"*.icc": "cpp"
}
}
}

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# --------------------------------------------------------------
# GNUmakefile for examples module. Gabriele Cosmo, 06/04/98.
# --------------------------------------------------------------
name := exampleB1
G4TARGET := $(name)
G4EXLIB := true
ifndef G4INSTALL
G4INSTALL = ../../..
endif
.PHONY: all
all: lib bin
include $(G4INSTALL)/config/binmake.gmk
visclean:
rm -f g4*.prim g4*.eps g4*.wrl
rm -f .DAWN_*

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-------------------------------------------------------------------
=========================================================
Geant4 - an Object-Oriented Toolkit for Simulation in HEP
=========================================================
Example B1 History file
-----------------------
This file should be used by the G4 example coordinator to briefly
summarize all major modifications introduced in the code and keep
track of all tags.
----------------------------------------------------------
* Reverse chronological order (last date on top), please *
----------------------------------------------------------
13-07-21 I. Hrivnacova (exampleB1-V10-07-03)
- Use B1 in multiple inclusion protection ifdefs
- Fixes in Doxygen documentation
12-07-21 I. Hrivnacova (exampleB1-V10-07-02)
- Introduced namespace instead of a class names prefix
- Declare overriding functions 'override' (and removed 'virtual' keyword)
31-05-21 I. Hrivnacova (exampleB1-V10-07-01)
- Use nullptr instead of 0
- Clean trailing whitespaces from all files
30-05-21 M.Maire (exampleB1-V10-07-00)
- exampleB1.cc: use G4SteppingVerboseWithUnits
02/11/20 B.Morgan (exampleB1-V10-06-01)
- Support same CMake version range as core Geant4
30/06/20 G. Cosmo (exampleB1-V10-06-00)
- Migrated to use G4RunManagerFactory, therefore implicitly enabling
tasking by default in MT builds.
21/11/19 G. Cosmo (exampleB1-V10-05-00)
- Use default MixMax random engine.
26/09/16 I. Hrivnacova (exampleB1-V10-02-01)
- Updated for renaming G4Parameter in G4Accumulable
20/09/16 J. Allison (exampleB1-V10-02-00)
- vis.mac: Added this to make "Envelope" transparent blue:
# "Envelope" is transparent blue to represent water
/vis/geometry/set/colour Envelope 0 0 0 1 .3
02/11/15 I. Hrivnacova (exampleB1-V10-01-03)
- B1Run class replaced with a code based on G4Parameter
04/05/15 I. Hrivnacova (exampleB1-V10-01-02)
- Coding guidelines: removed empty lines
23/04/15 mma (exampleB1-V10-01-01)
- RunAction : come back to previous formula
21/04/15 mma (exampleB1-V10-01-00)
- RunAction : correct calculation of rmsEdep
29/11/14 I. Hrivnacova
- Use G4endl instead of \n in G4cout;
this makes each new line in the output on threads preceded with
G4WTN >
06/11/14 I. Hrivnacova
- Removed G4UI_USE/G4VIS_USE tests and init.mac macro (not needed)
- Moved G4UIExecutive at the beginning of main() in all examples
- Perform run initialization in macros instead of main()
28/10/13 I. Hrivnacova (exampleB1-V09-06-06)
- Removed SetNumberOfThreads(4) from main (use Geant4 default)
26/10/13 mma (exampleB1-V09-06-05)
- Use /run/printProgress. Cleanup in EventAction
08/10/13 I. Hrivnacova (exampleB1-V09-06-04)
- Removed B1EventInformation for keeping maximum simplicity
- Improved documentation (added paragraph on Run::Merge())
- Code clean-up
09/06/13 I. Hrivnacova (exampleB1-V09-06-03)
- clarify local names in user actions
05/06/13 mma (exampleB1-V09-06-02)
- add section about ACTION INITALIZATION to README and .README
- update section DETECTOR RESPONSE
05/05/13 I. Hrivnacova (exampleB1-V09-06-01)
- Migration for MT (by Makoto):
Added B1ActionInitialization, B1EventInformation and B1Run classes
and updated actions classes accordingly.
README files still need to be updated.
15/01/13 I. Hrivnacova (exampleB1-V09-06-00)
- Tag for a test only (g4svn update with svn 1.7.x)
13/11/12 I. Hrivnacova (exampleB1-V09-05-03)
- Use QBBC physics list instead of QGSP_BIC_EMY, which becomes
obsolete
02/11/12 J. Allison (exampleB1-V09-05-01 and 02)
- README: Improved.
02/11/12 J. Allison (exampleB1-V09-05-00)
- vis.mac: Improved view and added text, scale, logo etc. to scene.
14/11/11 I. Hrivnacova
- The first tagged version of the new B1 example
(tagged in basic)
31/10/11 I. Hrivnacova
- change volume names
- scoring in 1 volume only, with new scheme
05/09/11 M. Maire, P. Gueye
- Created.

172
README

@ -0,0 +1,172 @@
-------------------------------------------------------------------
=========================================================
Geant4 - an Object-Oriented Toolkit for Simulation in HEP
=========================================================
Example B1
-----------
This example demonstrates a very simple application where an energy
deposit is accounted in user actions and their associated objects
and a dose in a selected volume is calculated.
1- GEOMETRY DEFINITION
The geometry is constructed in the B1::DetectorConstruction class.
The setup consists of a an envelope of box shape containing two
volumes: a spherical cone and a trapezoid.
In this example we use some common materials materials for medical
applications. The envelope is made of water and the two inner volumes
are made from tissue and bone materials.
The materials are created with the help of the G4NistManager class,
which allows to build a material from the NIST database using their
names. All available materials can be found in the Geant4 User's Guide
for Application Developers, Appendix 10: Geant4 Materials Database.
2- PHYSICS LIST
The particle's type and the physic processes which will be available
in this example are set in the QBBC physics list. This physics list
requires data files for electromagnetic and hadronic processes.
See more on installation of the datasets in Geant4 Installation Guide,
Chapter 3.3: Note On Geant4 Datasets:
http://geant4.web.cern.ch/geant4/UserDocumentation/UsersGuides
/InstallationGuide/html/ch03s03.html
The following datasets: G4LEDATA, G4LEVELGAMMADATA, G4NEUTRONXSDATA,
G4SAIDXSDATA and G4ENSDFSTATEDATA are mandatory for this example.
In addition the build-in interactive command:
/process/(in)activate processName
allows to activate/inactivate the processes one by one.
3- ACTION INITALIZATION
A newly introduced class, B1::ActionInitialization, instantiates and registers
to Geant4 kernel all user action classes.
While in sequential mode the action classes are instatiated just once,
via invoking the method:
B1::ActionInitialization::Build()
in multi-threading mode the same method is invoked for each thread worker
and so all user action classes are defined thread-local.
A run action class is instantiated both thread-local
and global that's why its instance is created also in the method
B1::ActionInitialization::BuildForMaster()
which is invoked only in multi-threading mode.
4- PRIMARY GENERATOR
The primary generator is defined in the B1::PrimaryGeneratorAction class.
The default kinematics is a 6 MeV gamma, randomly distributed in front
of the envelope across 80% of the transverse (X,Y) envelope size.
This default setting can be changed via the Geant4 built-in commands
of the G4ParticleGun class.
5- DETECTOR RESPONSE
This example demonstrates a simple scoring implemented directly
in the user action classes. Alternative ways of scoring via Geant4 classes
can be found in the other examples.
The energy deposited is collected step by step for a selected volume
in B1::SteppingAction and accumulated event by event in B1::EventAction.
At end of event, the value acummulated in B1::EventAction is added in B1::RunAction
and summed over the whole run (see B1::EventAction::EndOfevent()).
Total dose deposited is computed at B1::RunAction::EndOfRunAction(),
and printed together with informations about the primary particle.
In multi-threading mode the energy accumulated in G4Accumulable objects per
workers is merged to the master in B1::RunAction::EndOfRunAction() and the final
result is printed on the screen.
G4Parameter<G4double> type instead of G4double type is used for the B1::RunAction
data members in order to facilitate merging of the values accumulated on workers
to the master. Currently the accumulables have to be registered to G4AccumulablesManager
and G4AccumulablesManager::Merge() has to be called from the users code. This is planned
to be further simplified with a closer integration of G4Accumulable classes in
the Geant4 kernel next year.
An example of creating and computing new units (e.g., dose) is also shown
in the class constructor.
The following paragraphs are common to all basic examples
A- VISUALISATION
The visualization manager is set via the G4VisExecutive class
in the main() function in exampleB1.cc.
The initialisation of the drawing is done via a set of /vis/ commands
in the macro vis.mac. This macro is automatically read from
the main function when the example is used in interactive running mode.
By default, vis.mac opens an OpenGL viewer (/vis/open OGL).
The user can change the initial viewer by commenting out this line
and instead uncommenting one of the other /vis/open statements, such as
HepRepFile or DAWNFILE (which produce files that can be viewed with the
HepRApp and DAWN viewers, respectively). Note that one can always
open new viewers at any time from the command line. For example, if
you already have a view in, say, an OpenGL window with a name
"viewer-0", then
/vis/open DAWNFILE
then to get the same view
/vis/viewer/copyView viewer-0
or to get the same view *plus* scene-modifications
/vis/viewer/set/all viewer-0
then to see the result
/vis/viewer/flush
The DAWNFILE, HepRepFile drivers are always available
(since they require no external libraries), but the OGL driver requires
that the Geant4 libraries have been built with the OpenGL option.
From Release 9.6 the vis.mac macro in example B1 has additional commands
that demonstrate additional functionality of the vis system, such as
displaying text, axes, scales, date, logo and shows how to change
viewpoint and style. Consider copying these to other examples or
your application. To see even more commands use help or
ls or browse the available UI commands in the Application
Developers Guide, Section 7.1.
For more information on visualization, including information on how to
install and run DAWN, OpenGL and HepRApp, see the visualization tutorials,
for example,
http://geant4.slac.stanford.edu/Presentations/vis/G4[VIS]Tutorial/G4[VIS]Tutorial.html
(where [VIS] can be replaced by DAWN, OpenGL and HepRApp)
The tracks are automatically drawn at the end of each event, accumulated
for all events and erased at the beginning of the next run.
B- USER INTERFACES
The user command interface is set via the G4UIExecutive class
in the main() function in exampleB1.cc
The selection of the user command interface is then done automatically
according to the Geant4 configuration or it can be done explicitly via
the third argument of the G4UIExecutive constructor (see exampleB4a.cc).
C- HOW TO RUN
- Execute exampleB1 in the 'interactive mode' with visualization:
% ./exampleB1
and type in the commands from run1.mac line by line:
Idle> /control/verbose 2
Idle> /tracking/verbose 1
Idle> /run/beamOn 10
Idle> ...
Idle> exit
or
Idle> /control/execute run1.mac
....
Idle> exit
- Execute exampleB1 in the 'batch' mode from macro files
(without visualization)
% ./exampleB1 run2.mac
% ./exampleB1 exampleB1.in > exampleB1.out

@ -0,0 +1,67 @@
#include "ActionInitialization.hh" // 用户初始化
#include "DetectorConstruction.hh" // 探测器构建文件
#include "G4RunManagerFactory.hh" // 管理类
#include "G4SteppingVerbose.hh" // step信息管理 verbose越大,输出越丰富
#include "G4UIExecutive.hh" // UI操作
#include "G4UImanager.hh" // UI管理
#include "G4VisExecutive.hh" // 可视化
#include "QBBC.hh" // 物理过程
#include "Randomize.hh" // 随机数
using namespace B1;
int main(int argc, char** argv) {
// argc 为 1 时,说明参数只有可执行文件本身,运行在GUI模式下
// 如果 argc 不为 1,则运行在 batch mode,例如 example.exe run1.mac
G4UIExecutive* ui = nullptr;
if (argc == 1) {
ui = new G4UIExecutive(argc, argv);
}
// 调整 step 的输出信息
G4int precision = 4;
G4SteppingVerbose::UseBestUnit(precision);
// 构建运行管理器
auto* runManager = G4RunManagerFactory::CreateRunManager(G4RunManagerType::Default);
// 进行强制类的初始化
//
// 探测器构建
runManager->SetUserInitialization(new DetectorConstruction());
// 物理过程列表
G4VModularPhysicsList* physicsList = new QBBC;
physicsList->SetVerboseLevel(1);
runManager->SetUserInitialization(physicsList);
// 用户初始化
runManager->SetUserInitialization(new ActionInitialization());
// 可视化初始化
// G4VisExecutive 可以输入 verbose 参数,用于控制输出的详细程度
// https://www.hep.ph.ic.ac.uk/~yoshiu/COMET/comet_g4HTMLdoc/_vis_.html
G4VisManager* visManager = new G4VisExecutive;
visManager->Initialize();
// 用户界面管理器的指针
G4UImanager* UImanager = G4UImanager::GetUIpointer();
// 根据模式,选择开始进行模拟,或打开GUI
//
if (!ui) {
// batch mode
G4String command = "/control/execute ";
G4String fileName = argv[1];
UImanager->ApplyCommand(command + fileName);
} else {
// interactive mode
UImanager->ApplyCommand("/control/execute init_vis.mac");
ui->SessionStart();
delete ui;
}
// 释放指针
delete visManager;
delete runManager;
}

@ -0,0 +1,16 @@
# Macro file for example B1 test
/run/initialize
# gamma 6 MeV
/gun/particle gamma
/gun/energy 6 MeV
#
/run/printProgress 100
/run/beamOn 1000
#
# proton 210 MeV
/gun/particle proton
/gun/energy 210 MeV
#
/run/beamOn 1000

@ -0,0 +1,917 @@
Environment variable "G4FORCE_RUN_MANAGER_TYPE" enabled with value == Serial. Forcing G4RunManager type...
############################################
!!! WARNING - FPE detection is activated !!!
############################################
################################
!!! G4Backtrace is activated !!!
################################
**************************************************************
Geant4 version Name: geant4-11-00-patch-01 (8-March-2022)
Copyright : Geant4 Collaboration
References : NIM A 506 (2003), 250-303
: IEEE-TNS 53 (2006), 270-278
: NIM A 835 (2016), 186-225
WWW : http://geant4.org/
**************************************************************
<<< Reference Physics List QBBC
Visualization Manager instantiating with verbosity "warnings (3)"...
Visualization Manager initialising...
Registering graphics systems...
You have successfully registered the following graphics systems.
Registered graphics systems are:
ASCIITree (ATree)
DAWNFILE (DAWNFILE)
G4HepRepFile (HepRepFile)
RayTracer (RayTracer)
VRML2FILE (VRML2FILE)
gMocrenFile (gMocrenFile)
OpenGLImmediateQt (OGLIQt, OGLI)
OpenGLStoredQt (OGLSQt, OGL, OGLS)
OpenGLImmediateXm (OGLIXm, OGLIQt_FALLBACK)
OpenGLStoredXm (OGLSXm, OGLSQt_FALLBACK)
OpenGLImmediateX (OGLIX, OGLIQt_FALLBACK, OGLIXm_FALLBACK)
OpenGLStoredX (OGLSX, OGLSQt_FALLBACK, OGLSXm_FALLBACK)
RayTracerX (RayTracerX)
Registering model factories...
You have successfully registered the following model factories.
Registered model factories:
generic
drawByAttribute
drawByCharge
drawByOriginVolume
drawByParticleID
drawByEncounteredVolume
Registered models:
None
Registered filter factories:
attributeFilter
chargeFilter
originVolumeFilter
particleFilter
encounteredVolumeFilter
Registered filters:
None
You have successfully registered the following user vis actions.
Run Duration User Vis Actions: none
End of Event User Vis Actions: none
End of Run User Vis Actions: none
Some /vis commands (optionally) take a string to specify colour.
"/vis/list" to see available colours.
Checking overlaps for volume Envelope:0 (G4Box) ... OK!
Checking overlaps for volume Shape1:0 (G4Cons) ... OK!
Checking overlaps for volume Shape2:0 (G4Trd) ... OK!
### HadronInelasticQBBC Construct Process:
Emin(FTFP)= 3 GeV Emax(FTFP)= 100000 GeV
Emin(BERT)= 1 GeV Emax(BERT)= 6 GeV Emax(BERTpions)= 12 GeV
Emin(BIC) = 0 GeV Emax(BIC)= 1.5 GeV.
### Adding tracking cuts for neutron TimeCut(ns)= 10000 KinEnergyCut(MeV)= 0
=======================================================================
====== Electromagnetic Physics Parameters ========
=======================================================================
LPM effect enabled 1
Enable creation and use of sampling tables 0
Apply cuts on all EM processes 0
Use general process 0
Enable linear polarisation for gamma 0
Enable sampling of quantum entanglement 0
X-section factor for integral approach 0.8
Min kinetic energy for tables 100 eV
Max kinetic energy for tables 100 TeV
Number of bins per decade of a table 7
Verbose level 1
Verbose level for worker thread 0
Bremsstrahlung energy threshold above which
primary e+- is added to the list of secondary 100 TeV
Bremsstrahlung energy threshold above which primary
muon/hadron is added to the list of secondary 100 TeV
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
=======================================================================
====== Ionisation Parameters ========
=======================================================================
Step function for e+- (0.2, 1 mm)
Step function for muons/hadrons (0.2, 0.1 mm)
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
Use built-in Birks satuaration 0
Build CSDA range enabled 0
Use cut as a final range enabled 0
Enable angular generator interface 0
Max kinetic energy for CSDA tables 1 GeV
Max kinetic energy for NIEL computation 0 eV
Linear loss limit 0.01
Read data from file for e+e- pair production by mu 0
=======================================================================
====== Multiple Scattering Parameters ========
=======================================================================
Type of msc step limit algorithm for e+- 1
Type of msc step limit algorithm for muons/hadrons 0
Msc lateral displacement for e+- enabled 1
Msc lateral displacement for muons and hadrons 0
Urban msc model lateral displacement alg96 1
Range factor for msc step limit for e+- 0.04
Range factor for msc step limit for muons/hadrons 0.2
Geometry factor for msc step limitation of e+- 2.5
Safety factor for msc step limit for e+- 0.6
Skin parameter for msc step limitation of e+- 1
Lambda limit for msc step limit for e+- 1 mm
Use Mott correction for e- scattering 0
Factor used for dynamic computation of angular
limit between single and multiple scattering 1
Fixed angular limit between single
and multiple scattering 3.1416 rad
Upper energy limit for e+- multiple scattering 100 MeV
Type of electron single scattering model 0
Type of nuclear form-factor 1
Screening factor 1
=======================================================================
phot: for gamma SubType=12 BuildTable=0
LambdaPrime table from 200 keV to 100 TeV in 61 bins
===== EM models for the G4Region DefaultRegionForTheWorld ======
LivermorePhElectric : Emin= 0 eV Emax= 100 TeV SauterGavrila Fluo
compt: for gamma SubType=13 BuildTable=1
Lambda table from 100 eV to 1 MeV, 7 bins/decade, spline: 1
LambdaPrime table from 1 MeV to 100 TeV in 56 bins
===== EM models for the G4Region DefaultRegionForTheWorld ======
Klein-Nishina : Emin= 0 eV Emax= 100 TeV
conv: for gamma SubType=14 BuildTable=1
Lambda table from 1.022 MeV to 100 TeV, 18 bins/decade, spline: 1
===== EM models for the G4Region DefaultRegionForTheWorld ======
BetheHeitlerLPM : Emin= 0 eV Emax= 100 TeV ModifiedTsai
Rayl: for gamma SubType=11 BuildTable=1
Lambda table from 100 eV to 100 keV, 7 bins/decade, spline: 0
LambdaPrime table from 100 keV to 100 TeV in 63 bins
===== EM models for the G4Region DefaultRegionForTheWorld ======
LivermoreRayleigh : Emin= 0 eV Emax= 100 TeV CullenGenerator
msc: for e- SubType= 10
===== EM models for the G4Region DefaultRegionForTheWorld ======
UrbanMsc : Emin= 0 eV Emax= 100 MeV Nbins=42 100 eV - 100 MeV
StepLim=UseSafety Rfact=0.04 Gfact=2.5 Sfact=0.6 DispFlag:1 Skin=1 Llim=1 mm
WentzelVIUni : Emin= 100 MeV Emax= 100 TeV Nbins=42 100 MeV - 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
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
MollerBhabha : Emin= 0 eV Emax= 100 TeV
eBrem: for e- XStype:4 SubType=3
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
LPM flag: 1 for E > 1 GeV, VertexHighEnergyTh(GeV)= 100000
===== EM models for the G4Region DefaultRegionForTheWorld ======
eBremSB : Emin= 0 eV Emax= 1 GeV ModifiedTsai
eBremLPM : Emin= 1 GeV Emax= 100 TeV ModifiedTsai
CoulombScat: for e- XStype:1 SubType=1 BuildTable=1
Lambda table from 100 MeV to 100 TeV, 7 bins/decade, spline: 0
ThetaMin(p) < Theta(degree) < 180 pLimit(GeV^1)= 0.139531
===== EM models for the G4Region DefaultRegionForTheWorld ======
eCoulombScattering : Emin= 100 MeV Emax= 100 TeV
msc: for e+ SubType= 10
===== EM models for the G4Region DefaultRegionForTheWorld ======
UrbanMsc : Emin= 0 eV Emax= 100 MeV Nbins=42 100 eV - 100 MeV
StepLim=UseSafety Rfact=0.04 Gfact=2.5 Sfact=0.6 DispFlag:1 Skin=1 Llim=1 mm
WentzelVIUni : Emin= 100 MeV Emax= 100 TeV Nbins=42 100 MeV - 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
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
MollerBhabha : Emin= 0 eV Emax= 100 TeV
eBrem: for e+ XStype:4 SubType=3
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
LPM flag: 1 for E > 1 GeV, VertexHighEnergyTh(GeV)= 100000
===== EM models for the G4Region DefaultRegionForTheWorld ======
eBremSB : Emin= 0 eV Emax= 1 GeV ModifiedTsai
eBremLPM : Emin= 1 GeV Emax= 100 TeV ModifiedTsai
annihil: for e+ XStype:2 SubType=5 BuildTable=0
===== EM models for the G4Region DefaultRegionForTheWorld ======
eplus2gg : Emin= 0 eV Emax= 100 TeV
CoulombScat: for e+ XStype:1 SubType=1 BuildTable=1
Lambda table from 100 MeV to 100 TeV, 7 bins/decade, spline: 0
ThetaMin(p) < Theta(degree) < 180 pLimit(GeV^1)= 0.139531
===== EM models for the G4Region DefaultRegionForTheWorld ======
eCoulombScattering : Emin= 100 MeV Emax= 100 TeV
msc: for proton SubType= 10
===== EM models for the G4Region DefaultRegionForTheWorld ======
WentzelVIUni : 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
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
Bragg : Emin= 0 eV Emax= 2 MeV
BetheBloch : Emin= 2 MeV Emax= 100 TeV
hBrems: for proton XStype:1 SubType=3
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
hBrem : Emin= 0 eV Emax= 100 TeV ModifiedMephi
hPairProd: for proton 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 17x1001 from 7.50618 GeV to 100 TeV
===== EM models for the G4Region DefaultRegionForTheWorld ======
hPairProd : Emin= 0 eV Emax= 100 TeV ModifiedMephi
CoulombScat: for proton XStype:1 SubType=1 BuildTable=1
Lambda table from threshold to 100 TeV, 7 bins/decade, spline: 0
ThetaMin(p) < Theta(degree) < 180 pLimit(GeV^1)= 0.139531
===== EM models for the G4Region DefaultRegionForTheWorld ======
eCoulombScattering : Emin= 0 eV Emax= 100 TeV
msc: for GenericIon SubType= 10
===== EM models for the G4Region DefaultRegionForTheWorld ======
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
ionIoni: for GenericIon XStype:1 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= 0.02
Stopping Power data for 17 ion/material pairs
===== EM models for the G4Region DefaultRegionForTheWorld ======
BraggIon : Emin= 0 eV Emax= 2 MeV
BetheBloch : Emin= 2 MeV Emax= 100 TeV
msc: for alpha SubType= 10
===== EM models for the G4Region DefaultRegionForTheWorld ======
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
ionIoni: for alpha XStype:1 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= 0.02
===== EM models for the G4Region DefaultRegionForTheWorld ======
BraggIon : Emin= 0 eV Emax=7.9452 MeV
BetheBloch : Emin=7.9452 MeV Emax= 100 TeV
msc: for anti_proton SubType= 10
===== EM models for the G4Region DefaultRegionForTheWorld ======
WentzelVIUni : 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
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
ICRU73QO : Emin= 0 eV Emax= 2 MeV
BetheBloch : Emin= 2 MeV Emax= 100 TeV
hBrems: for anti_proton XStype:1 SubType=3
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
hBrem : Emin= 0 eV Emax= 100 TeV ModifiedMephi
hPairProd: for anti_proton 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 17x1001 from 7.50618 GeV to 100 TeV
===== EM models for the G4Region DefaultRegionForTheWorld ======
hPairProd : Emin= 0 eV Emax= 100 TeV ModifiedMephi
CoulombScat: for anti_proton XStype:1 SubType=1 BuildTable=1
Lambda table from threshold to 100 TeV, 7 bins/decade, spline: 0
ThetaMin(p) < Theta(degree) < 180 pLimit(GeV^1)= 0.139531
===== EM models for the G4Region DefaultRegionForTheWorld ======
eCoulombScattering : Emin= 0 eV Emax= 100 TeV
msc: for kaon+ SubType= 10
===== EM models for the G4Region DefaultRegionForTheWorld ======
WentzelVIUni : 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
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
Bragg : Emin= 0 eV Emax=1.05231 MeV
BetheBloch : Emin=1.05231 MeV Emax= 100 TeV
hBrems: for kaon+ XStype:1 SubType=3
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
hBrem : Emin= 0 eV Emax= 100 TeV ModifiedMephi
hPairProd: for kaon+ 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 18x1001 from 3.94942 GeV to 100 TeV
===== EM models for the G4Region DefaultRegionForTheWorld ======
hPairProd : Emin= 0 eV Emax= 100 TeV ModifiedMephi
CoulombScat: for kaon+ XStype:1 SubType=1 BuildTable=1
Lambda table from threshold to 100 TeV, 7 bins/decade, spline: 0
ThetaMin(p) < Theta(degree) < 180 pLimit(GeV^1)= 0.139531
===== EM models for the G4Region DefaultRegionForTheWorld ======
eCoulombScattering : Emin= 0 eV Emax= 100 TeV
msc: for kaon- SubType= 10
===== EM models for the G4Region DefaultRegionForTheWorld ======
WentzelVIUni : 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
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
ICRU73QO : Emin= 0 eV Emax=1.05231 MeV
BetheBloch : Emin=1.05231 MeV Emax= 100 TeV
hBrems: for kaon- XStype:1 SubType=3
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
hBrem : Emin= 0 eV Emax= 100 TeV ModifiedMephi
hPairProd: for kaon- 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 18x1001 from 3.94942 GeV to 100 TeV
===== EM models for the G4Region DefaultRegionForTheWorld ======
hPairProd : Emin= 0 eV Emax= 100 TeV ModifiedMephi
CoulombScat: for kaon- XStype:1 SubType=1 BuildTable=1
Used Lambda table of kaon+
ThetaMin(p) < Theta(degree) < 180 pLimit(GeV^1)= 0.139531
===== EM models for the G4Region DefaultRegionForTheWorld ======
eCoulombScattering : Emin= 0 eV Emax= 100 TeV
msc: for mu+ SubType= 10
===== EM models for the G4Region DefaultRegionForTheWorld ======
WentzelVIUni : 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
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
===== 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
muBrems: for mu+ XStype:1 SubType=3
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
MuBrem : Emin= 0 eV Emax= 100 TeV ModifiedMephi
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
muPairProd : Emin= 0 eV Emax= 100 TeV ModifiedMephi
CoulombScat: for mu+ XStype:1 SubType=1 BuildTable=1
Lambda table from threshold to 100 TeV, 7 bins/decade, spline: 0
ThetaMin(p) < Theta(degree) < 180 pLimit(GeV^1)= 0.139531
===== EM models for the G4Region DefaultRegionForTheWorld ======
eCoulombScattering : Emin= 0 eV Emax= 100 TeV
msc: for mu- SubType= 10
===== EM models for the G4Region DefaultRegionForTheWorld ======
WentzelVIUni : 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
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
===== 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
muBrems: for mu- XStype:1 SubType=3
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
MuBrem : Emin= 0 eV Emax= 100 TeV ModifiedMephi
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
muPairProd : Emin= 0 eV Emax= 100 TeV ModifiedMephi
CoulombScat: for mu- XStype:1 SubType=1 BuildTable=1
Used Lambda table of mu+
ThetaMin(p) < Theta(degree) < 180 pLimit(GeV^1)= 0.139531
===== EM models for the G4Region DefaultRegionForTheWorld ======
eCoulombScattering : Emin= 0 eV Emax= 100 TeV
msc: for pi+ SubType= 10
===== EM models for the G4Region DefaultRegionForTheWorld ======
WentzelVIUni : 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
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
Bragg : Emin= 0 eV Emax=297.505 keV
BetheBloch : Emin=297.505 keV Emax= 100 TeV
hBrems: for pi+ XStype:1 SubType=3
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
hBrem : Emin= 0 eV Emax= 100 TeV ModifiedMephi
hPairProd: for pi+ 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 20x1001 from 1.11656 GeV to 100 TeV
===== EM models for the G4Region DefaultRegionForTheWorld ======
hPairProd : Emin= 0 eV Emax= 100 TeV ModifiedMephi
CoulombScat: for pi+ XStype:1 SubType=1 BuildTable=1
Lambda table from threshold to 100 TeV, 7 bins/decade, spline: 0
ThetaMin(p) < Theta(degree) < 180 pLimit(GeV^1)= 0.139531
===== EM models for the G4Region DefaultRegionForTheWorld ======
eCoulombScattering : Emin= 0 eV Emax= 100 TeV
msc: for pi- SubType= 10
===== EM models for the G4Region DefaultRegionForTheWorld ======
WentzelVIUni : 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
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
ICRU73QO : Emin= 0 eV Emax=297.505 keV
BetheBloch : Emin=297.505 keV Emax= 100 TeV
hBrems: for pi- XStype:1 SubType=3
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
===== EM models for the G4Region DefaultRegionForTheWorld ======
hBrem : Emin= 0 eV Emax= 100 TeV ModifiedMephi
hPairProd: for pi- 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 20x1001 from 1.11656 GeV to 100 TeV
===== EM models for the G4Region DefaultRegionForTheWorld ======
hPairProd : Emin= 0 eV Emax= 100 TeV ModifiedMephi
CoulombScat: for pi- XStype:1 SubType=1 BuildTable=1
Used Lambda table of pi+
ThetaMin(p) < Theta(degree) < 180 pLimit(GeV^1)= 0.139531
===== EM models for the G4Region DefaultRegionForTheWorld ======
eCoulombScattering : Emin= 0 eV Emax= 100 TeV
====================================================================
HADRONIC PROCESSES SUMMARY (verbose level 1)
---------------------------------------------------
Hadronic Processes for neutron
Process: hadElastic
Model: hElasticCHIPS: 0 eV ---> 100 TeV
Cr_sctns: G4NeutronElasticXS: 0 eV ---> 100 TeV
Process: neutronInelastic
Model: FTFP: 3 GeV ---> 100 TeV
Model: BertiniCascade: 1 GeV ---> 6 GeV
Model: Binary Cascade: 0 eV ---> 1.5 GeV
Cr_sctns: G4NeutronInelasticXS: 0 eV ---> 100 TeV
Process: nCapture
Model: nRadCapture: 0 eV ---> 100 TeV
Cr_sctns: G4NeutronCaptureXS: 0 eV ---> 100 TeV
Process: nKiller
---------------------------------------------------
Hadronic Processes for B-
Process: hadElastic
Model: hElasticLHEP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Process: B-Inelastic
Model: FTFP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
---------------------------------------------------
Hadronic Processes for D-
Process: hadElastic
Model: hElasticLHEP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
Process: D-Inelastic
Model: FTFP: 0 eV ---> 100 TeV
Cr_sctns: Glauber-Gribov: 0 eV ---> 100 TeV
---------------------------------------------------
Hadronic Processes for GenericIon
Process: ionInelastic
Model: Binary Light Ion Cascade: 0 eV /n ---> 6 GeV/n
Model: FTFP: 3 GeV/n ---> 100 TeV/n
Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV ---> 25.6 PeV
Process: ionElastic
Model: NNDiffuseElastic: 0 eV /n ---> 100 TeV/n
Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV ---> 25.6 PeV
---------------------------------------------------
Hadronic Processes for He3
Process: hadElastic
Model: hElasticLHEP: 0 eV /n ---> 100 TeV/n
Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV ---> 25.6 PeV
Process: He3Inelastic
Model: Binary Light Ion Cascade: 0 eV /n ---> 6 GeV/n
Model: FTFP: 3 GeV/n ---> 100 TeV/n
Cr_sctns: G4ParticleInelasticXS: 0 eV ---> 25.6 PeV
---------------------------------------------------
Hadronic Processes for alpha
Process: hadElastic
Model: hElasticLHEP: 0 eV /n ---> 100 TeV/n
Cr_sctns: Glauber-Gribov Nucl-nucl: 0 eV ---> 25.6 PeV
Process: alphaInelastic
Model: Binary Light Ion Cascade: 0 eV /n ---> 6 GeV/n
Model: FTFP: 3 GeV/n ---> 100 TeV/n
Cr_sctns: G4ParticleInelasticXS: 0 eV ---> 25.6 PeV
---------------------------------------------------
Hadronic Processes for anti_He3
Process: hadElastic
Model: hElasticLHEP: 0 eV /n ---> 100.1 MeV/n
Model: AntiAElastic: 100 MeV/n ---> 100 TeV/n
Cr_sctns: AntiAGlauber: 0 eV ---> 25.6 PeV
Process: anti_He3Inelastic
Model: FTFP: 0 eV /n ---> 100 TeV/n
Cr_sctns: AntiAGlauber: 0 eV ---> 25.6 PeV
Process: hFritiofCaptureAtRest
---------------------------------------------------
Hadronic Processes for anti_alpha
Process: hadElastic
Model: hElasticLHEP: 0 eV /n ---> 100.1 MeV/n
Model: AntiAElastic: 100 MeV/n ---> 100 TeV/n
Cr_sctns: AntiAGlauber: 0 eV ---> 25.6 PeV
Process: anti_alphaInelastic
Model: FTFP: 0 eV /n ---> 100 TeV/n
Cr_sctns: AntiAGlauber: 0 eV ---> 25.6 PeV
Process: hFritiofCaptureAtRest
---------------------------------------------------
Hadronic Processes for anti_deuteron
Process: hadElastic
Model: hElasticLHEP: 0 eV /n ---> 100.1 MeV/n
Model: AntiAElastic: 100 MeV/n ---> 100 TeV/n
Cr_sctns: AntiAGlauber: 0 eV ---> 25.6 PeV
Process: anti_deuteronInelastic
Model: FTFP: 0 eV /n ---> 100 TeV/n
Cr_sctns: AntiAGlauber: 0 eV ---> 25.6 PeV
Process: hFritiofCaptureAtRest
---------------------------------------------------
Hadronic Processes for anti_lambda