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This commit is contained in:
Gabriele Cosmo
2017-06-30 10:49:55 +02:00
parent 3a5407696b
commit 1a1316fea4
2180 changed files with 237880 additions and 59109 deletions
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examples/advanced/hadrontherapy/src/HadrontherapyPhysicsList.cc
+42 -148
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@@ -28,11 +28,11 @@
//
//
// ****** SUGGESTED PHYSICS FOR ACCURATE SIMULATIONS *********
// ****** IN MEDICAL PHYSICS APPLI CATIONS *********
//
// At moment, if accurate simulations are necessary, we suggest the use of the
// Physics Lists 'HADRONTHERAPY_1';
// 'HADRONTHERAPY_1' and 'HADRONTHERAPY_2' are both suggested;
// It can be activated inside any macro file using the command:
// /Physics/addPhysics HADRONTHERAPY_1
// /Physics/addPhysics HADRONTHERAPY_1 (HADRONTHERAPY_2)
#include "G4SystemOfUnits.hh"
#include "G4RunManager.hh"
@@ -43,16 +43,10 @@
#include "HadrontherapyStepMax.hh"
#include "G4PhysListFactory.hh"
#include "G4VPhysicsConstructor.hh"
// Local physic directly implemented in the Hadronthrapy directory
// Physic dedicated to the ion-ion inelastic processes
//
#include "LocalIonIonInelasticPhysic.hh"
#include "G4HadronPhysicsQGSP_BIC_HP.hh"
#include "G4HadronPhysicsQGSP_BIC.hh"
#include "G4EmStandardPhysics_option3.hh"
#include "G4EmStandardPhysics_option4.hh"
#include "G4EmStandardPhysics.hh"
#include "G4EmExtraPhysics.hh"
#include "G4StoppingPhysics.hh"
#include "G4DecayPhysics.hh"
@@ -81,41 +75,13 @@ HadrontherapyPhysicsList::HadrontherapyPhysicsList() : G4VModularPhysicsList()
cutForElectron = defaultCutValue;
cutForPositron = defaultCutValue;
pMessenger = new HadrontherapyPhysicsListMessenger(this);
pMessenger = new HadrontherapyPhysicsListMessenger(this);
SetVerboseLevel(1);
// ****** Definition of defaults for the physics processes *****
// ****** in case no physics is called by the macro file *****
//
// The default physics corresponds to the actual QGSP_BIC_HP list
// but with the following differences:
// --> G4EmStandardPhysics_option4 for the electromagnetic processes
// is used n place of the less accurate G4EmStandardPhysics
// --> The G4RadioactiveDecayPhysics is add
// --> G4HadronPhysicsQGSP_BIC is used in place of G4HadronPhysicsQGSP_BIC_HP
// --> G4HadronElasticPhysics is used in place of G4HadronElasticPhysics_HP
decay_List = new G4DecayPhysics();
// Elecromagnetic physics
//
emPhysicsList = new G4EmStandardPhysics_option4();
emName = G4String("emstandard_opt4");
// Hadronic physics
//
hadronPhys.push_back( new G4DecayPhysics());
hadronPhys.push_back( new G4RadioactiveDecayPhysics());
hadronPhys.push_back( new G4IonBinaryCascadePhysics());
hadronPhys.push_back( new G4EmExtraPhysics());
hadronPhys.push_back( new G4HadronElasticPhysics());
hadronPhys.push_back( new G4StoppingPhysics());
hadronPhys.push_back( new G4HadronPhysicsQGSP_BIC());
// Decay physics
//
decay_List = new G4DecayPhysics();
radioactiveDecay_List = new G4RadioactiveDecayPhysics();
}
/////////////////////////////////////////////////////////////////////////////
@@ -123,8 +89,8 @@ HadrontherapyPhysicsList::~HadrontherapyPhysicsList()
{
delete pMessenger;
delete emPhysicsList;
delete decay_List;
delete radioactiveDecay_List;
delete decay_List;
//delete radioactiveDecay_List;
hadronPhys.clear();
for(size_t i=0; i<hadronPhys.size(); i++)
{
@@ -136,6 +102,7 @@ HadrontherapyPhysicsList::~HadrontherapyPhysicsList()
void HadrontherapyPhysicsList::ConstructParticle()
{
decay_List -> ConstructParticle();
}
/////////////////////////////////////////////////////////////////////////////
@@ -145,10 +112,11 @@ void HadrontherapyPhysicsList::ConstructProcess()
//
AddTransportation();
// Electromagnetic physics
//
decay_List -> ConstructProcess();
emPhysicsList -> ConstructProcess();
em_config.AddModels();
//em_config.AddModels();
// Hadronic physics
//
@@ -188,34 +156,11 @@ void HadrontherapyPhysicsList::AddPhysicsList(const G4String& name)
G4RunManager::GetRunManager() -> PhysicsHasBeenModified();
G4cout << "THE FOLLOWING ELECTROMAGNETIC PHYSICS LIST HAS BEEN ACTIVATED: G4EmStandardPhysics_option4" << G4endl;
// The following 'local_ion_ion_inelastic' is an example of implemenation of
// inelastic hadronic models to be used when
// mucleus-nulceus (ion-ion) interactions have to be
// taken into account;
// It must be used, of course, in connection with other lists: electromagnetic
// plus hadronic elastic plus nucleon-nulcleon hadronic inelastic
//
// An example of coplete physics list using the 'local_ion_ion_inelastic' physics
// is the one named HADRONTHERAPY_2, and defined below.
//
} else if (name == "standard_opt3") {
emName = name;
delete emPhysicsList;
hadronPhys.clear();
emPhysicsList = new G4EmStandardPhysics_option3();
G4RunManager::GetRunManager() -> PhysicsHasBeenModified();
G4cout << "THE FOLLOWING ELECTROMAGNETIC PHYSICS LIST HAS BEEN ACTIVATED: G4EmStandardPhysics_option3" << G4endl;
} else if (name == "local_ion_ion_inelastic") {
hadronPhys.push_back(new LocalIonIonInelasticPhysic());
locIonIonInelasticIsRegistered = true;
////////////////////////////////////////
// ELECTROMAGNETIC + HADRONIC MODELS
////////////////////////////////////////
} else if (name == "HADRONTHERAPY_1") {
// The HADRONTHERAPY_1 physics list corresponds to the actual QGSP_BIC_HP list
// but with the following differences:
// --> G4EmStandardPhysics_option4 for the electromagnetic processes
// is used in place of the less accurate G4EmStandardPhysics
// --> The G4RadioactiveDecayPhysics is added
} else if (name == "HADRONTHERAPY_1") {
AddPhysicsList("standard_opt4");
hadronPhys.push_back( new G4DecayPhysics());
@@ -225,45 +170,25 @@ void HadrontherapyPhysicsList::AddPhysicsList(const G4String& name)
hadronPhys.push_back( new G4HadronElasticPhysicsHP());
hadronPhys.push_back( new G4StoppingPhysics());
hadronPhys.push_back( new G4HadronPhysicsQGSP_BIC_HP());
hadronPhys.push_back( new G4NeutronTrackingCut());
G4cout << "HADRONTHERAPY_1 PHYSICS LIST has been activated" << G4endl;
}
} else if (name == "HADRONTHERAPY_2") {
// The HADRONTHERAPY_2 physics list corresponds to the actual QGSP_BIC_HP list
// but with the following differences:
// --> G4EmStandardPhysics_option4 for the electromagnetic processes
// is used in place of the less accurate G4EmStandardPhysics
// --> The G4RadioactiveDecayPhysics is added
// --> The 'local_ion_ion_inelastic' physics is used in place of the
// G4IonBinaryCascadePhysics(): it used the QMD model to treat
// the ion-ion inelastic interactions
else if (name == "HADRONTHERAPY_2") {
// HP models are switched off
AddPhysicsList("standard_opt4");
AddPhysicsList("local_ion_ion_inelastic");
hadronPhys.push_back( new G4DecayPhysics());
hadronPhys.push_back( new G4RadioactiveDecayPhysics());
hadronPhys.push_back( new G4IonBinaryCascadePhysics());
hadronPhys.push_back( new G4EmExtraPhysics());
hadronPhys.push_back( new G4HadronElasticPhysicsHP());
hadronPhys.push_back( new G4HadronElasticPhysics());
hadronPhys.push_back( new G4StoppingPhysics());
hadronPhys.push_back( new G4HadronPhysicsQGSP_BIC_HP());
hadronPhys.push_back( new G4HadronPhysicsQGSP_BIC());
hadronPhys.push_back( new G4NeutronTrackingCut());
G4cout << "HADRONTHERAPY_2 PHYSICS LIST has been acivated" << G4endl;
}
else if (name == "QGSP_BIC_EMY") {
AddPhysicsList("standard_opt3");
//emPhysicsList = new G4EmLivermorePhysics();
hadronPhys.push_back( new G4HadronPhysicsQGSP_BIC());
hadronPhys.push_back( new G4EmExtraPhysics());
hadronPhys.push_back( new G4HadronElasticPhysics());
hadronPhys.push_back( new G4StoppingPhysics());
hadronPhys.push_back( new G4IonBinaryCascadePhysics());
hadronPhys.push_back( new G4NeutronTrackingCut());
hadronPhys.push_back( new G4DecayPhysics());
}
else {
G4cout << "HADRONTHERAPY_2 PHYSICS LIST has been activated" << G4endl; }
else {
G4cout << "PhysicsList::AddPhysicsList: <" << name << ">"
<< " is not defined"
<< G4endl;
@@ -274,52 +199,21 @@ void HadrontherapyPhysicsList::AddPhysicsList(const G4String& name)
/////////////////////////////////////////////////////////////////////////////
void HadrontherapyPhysicsList::AddStepMax()
{
// Step limitation seen as a process
// This process must exist in all threads.
//
HadrontherapyStepMax* stepMaxProcess = new HadrontherapyStepMax();
G4AutoDelete::Register( stepMaxProcess );
auto particleIterator=GetParticleIterator();
particleIterator->reset();
while ((*particleIterator)()){
G4ParticleDefinition* particle = particleIterator->value();
G4ProcessManager* pmanager = particle->GetProcessManager();
if (stepMaxProcess->IsApplicable(*particle) && pmanager)
{
pmanager ->AddDiscreteProcess(stepMaxProcess);
}
}
}
/////////////////////////////////////////////////////////////////////////////
void HadrontherapyPhysicsList::SetCuts()
{
if (verboseLevel >0){
G4cout << "PhysicsList::SetCuts:";
G4cout << "CutLength : " << G4BestUnit(defaultCutValue,"Length") << G4endl;
}
// Step limitation seen as a process
// This process must exist in all threads.
//
HadrontherapyStepMax* stepMaxProcess = new HadrontherapyStepMax();
G4AutoDelete::Register( stepMaxProcess );
// Production thresholds for detector regions
// The G4Regions, for which you want define a given cut via de macro command
// '/run/setCutForRegion <G4Region name> <cut value>'
// must be defined here
//
SetCutValue(cutForGamma, "gamma");
SetCutValue(cutForElectron, "e-");
SetCutValue(cutForPositron, "e+");
// At moment, only 'DetectorLog' is defined as G4Region
//
G4String regName[] = {"DetectorLog"};
G4double fuc = 1.;
for(G4int i=0;i<1;i++)
{
G4Region* reg = G4RegionStore::GetInstance()->GetRegion(regName[i]);
G4ProductionCuts* cuts = new G4ProductionCuts;
cuts->SetProductionCut(defaultCutValue*fuc);
reg->SetProductionCuts(cuts);
fuc *= 10.;
auto particleIterator = GetParticleIterator();
particleIterator->reset();
while ((*particleIterator)()){
G4ParticleDefinition* particle = particleIterator->value();
G4ProcessManager* pmanager = particle->GetProcessManager();
if (stepMaxProcess->IsApplicable(*particle) && pmanager)
{
pmanager ->AddDiscreteProcess(stepMaxProcess);
}
}
}