G4PenelopeBremsstrahlungAngular Class Reference

#include <G4PenelopeBremsstrahlungAngular.hh>

Inheritance diagram for G4PenelopeBremsstrahlungAngular:

Public Member Functions
	G4PenelopeBremsstrahlungAngular ()
	~G4PenelopeBremsstrahlungAngular ()
G4double	PolarAngle (const G4double initial_energy, const G4double final_energy, const G4int Z)
G4ThreeVector &	SampleDirection (const G4DynamicParticle *dp, G4double out_energy, G4int Z, const G4Material *mat=0)
	Samples the direction of the outgoing photon (in global coordinates). More...
void	SetVerbosityLevel (G4int vl)
	Set/Get Verbosity level. More...
G4int	GetVerbosityLevel ()
void	Initialize ()
void	PrepareTables (const G4Material *material, G4bool isMaster)
	Reserved for Master Model. More...
Public Member Functions inherited from G4VEmAngularDistribution
	G4VEmAngularDistribution (const G4String &name)
virtual	~G4VEmAngularDistribution ()
virtual G4ThreeVector &	SampleDirectionForShell (const G4DynamicParticle *dp, G4double finalTotalEnergy, G4int Z, G4int shellID, const G4Material *)
const G4String &	GetName () const

Additional Inherited Members
Protected Attributes inherited from G4VEmAngularDistribution
G4ThreeVector	fLocalDirection

Detailed Description

Definition at line 56 of file G4PenelopeBremsstrahlungAngular.hh.

Constructor & Destructor Documentation

G4PenelopeBremsstrahlungAngular::G4PenelopeBremsstrahlungAngular

(

)

Definition at line 60 of file G4PenelopeBremsstrahlungAngular.cc.

                                                                 : 
  G4VEmAngularDistribution("Penelope"), theEffectiveZSq(0),
  theLorentzTables1(0),theLorentzTables2(0)
  
{
  dataRead = false;
  verbosityLevel = 0;
}

G4PenelopeBremsstrahlungAngular::~G4PenelopeBremsstrahlungAngular

(

)

Definition at line 71 of file G4PenelopeBremsstrahlungAngular.cc.

{
  ClearTables();
}

Member Function Documentation

G4int G4PenelopeBremsstrahlungAngular::GetVerbosityLevel ( )

inline

Definition at line 78 of file G4PenelopeBremsstrahlungAngular.hh.

{return verbosityLevel;};

void G4PenelopeBremsstrahlungAngular::Initialize

(

)

Reserved for Master Model The Initialize() method forces the cleaning of tables

Definition at line 78 of file G4PenelopeBremsstrahlungAngular.cc.

Referenced by G4PenelopeBremsstrahlungModel::Initialise(), and G4PenelopeBremsstrahlungModel::InitialiseLocal().

{
  ClearTables();
}

G4double G4PenelopeBremsstrahlungAngular::PolarAngle	(	const G4double	initial_energy,
		const G4double	final_energy,
		const G4int	Z
	)

Old interface, backwards compatibility. Will not work in this case it will produce a G4Exception().

Definition at line 468 of file G4PenelopeBremsstrahlungAngular.cc.

References FatalException, G4cout, G4endl, and G4Exception().

{
  G4cout << "WARNING: G4PenelopeBremsstrahlungAngular() does NOT support PolarAngle()" << G4endl;
  G4cout << "Please use the alternative interface SampleDirection()" << G4endl;
  G4Exception("G4PenelopeBremsstrahlungAngular::PolarAngle()",
          "em0005",FatalException,"Unsupported interface");  
  return 0;
}

void G4PenelopeBremsstrahlungAngular::PrepareTables	(	const G4Material *	material,
		G4bool	isMaster
	)

Reserved for Master Model.

Definition at line 174 of file G4PenelopeBremsstrahlungAngular.cc.

References python.hepunit::electron_mass_c2, FatalException, G4endl, G4Exception(), python.hepunit::MeV, G4PhysicsTable::push_back(), G4PhysicsFreeVector::PutValue(), G4PhysicsVector::SetSpline(), and G4PhysicsVector::Value().

Referenced by G4PenelopeBremsstrahlungModel::Initialise(), and G4PenelopeBremsstrahlungModel::InitialiseLocal().

{
  //Unused at the moment: the G4PenelopeBremsstrahlungAngular is thread-local, so each worker 
  //builds its own version of the tables.
  /*
    if (!isMaster)    
    //Should not be here!
    G4Exception("G4PenelopeBremsstrahlungAngular::PrepareTables()",
    "em0100",FatalException,"Worker thread in this method");  
  */

  //Check if data file has already been read
  if (!dataRead)
    {
      ReadDataFile();
      if (!dataRead)    
    G4Exception("G4PenelopeBremsstrahlungAngular::PrepareInterpolationTables()",
            "em2001",FatalException,"Unable to build interpolation table");
    }
  
  if (!theLorentzTables1)
      theLorentzTables1 = new std::map<G4double,G4PhysicsTable*>;
  if (!theLorentzTables2)
    theLorentzTables2 = new std::map<G4double,G4PhysicsTable*>;

  G4double Zmat = CalculateEffectiveZ(material);

  const G4int reducedEnergyGrid=21;
  //Support arrays. 
  G4double betas[NumberofEPoints]; //betas for interpolation
  //tables for interpolation
  G4double Q1[NumberofEPoints][NumberofKPoints];
  G4double Q2[NumberofEPoints][NumberofKPoints];
  //expanded tables for interpolation
  G4double Q1E[NumberofEPoints][reducedEnergyGrid];
  G4double Q2E[NumberofEPoints][reducedEnergyGrid]; 
  G4double pZ[NumberofZPoints] = {2.0,8.0,13.0,47.0,79.0,92.0};

  G4int i=0,j=0,k=0; // i=index for Z, j=index for E, k=index for K 
  //Interpolation in Z
  for (i=0;i<NumberofEPoints;i++)
    {
      for (j=0;j<NumberofKPoints;j++)
    {
      G4PhysicsFreeVector* QQ1vector = new G4PhysicsFreeVector(NumberofZPoints);
      G4PhysicsFreeVector* QQ2vector = new G4PhysicsFreeVector(NumberofZPoints);

      //fill vectors
      for (k=0;k<NumberofZPoints;k++)
        {
          QQ1vector->PutValue(k,pZ[k],std::log(QQ1[k][i][j]));
          QQ2vector->PutValue(k,pZ[k],QQ2[k][i][j]);
        }

      QQ1vector->SetSpline(true);
      QQ2vector->SetSpline(true);
      
      Q1[i][j]= std::exp(QQ1vector->Value(Zmat));     
      Q2[i][j]=QQ2vector->Value(Zmat);
      delete QQ1vector;
      delete QQ2vector;
    }
    }
  G4double pE[NumberofEPoints] = {1.0e-03*MeV,5.0e-03*MeV,1.0e-02*MeV,5.0e-02*MeV,
                  1.0e-01*MeV,5.0e-01*MeV};
  G4double pK[NumberofKPoints] = {0.0,0.6,0.8,0.95};
  G4double ppK[reducedEnergyGrid]; 

  for(i=0;i<reducedEnergyGrid;i++)
    ppK[i]=((G4double) i) * 0.05;
  

  for(i=0;i<NumberofEPoints;i++)
    betas[i]=std::sqrt(pE[i]*(pE[i]+2*electron_mass_c2))/(pE[i]+electron_mass_c2);
  

  for (i=0;i<NumberofEPoints;i++)
    {
      for (j=0;j<NumberofKPoints;j++)
    Q1[i][j]=Q1[i][j]/Zmat;
    }

  //Expanded table of distribution parameters
  for (i=0;i<NumberofEPoints;i++)
    {
      G4PhysicsFreeVector* Q1vector = new G4PhysicsFreeVector(NumberofKPoints);    
      G4PhysicsFreeVector* Q2vector = new G4PhysicsFreeVector(NumberofKPoints);

      for (j=0;j<NumberofKPoints;j++)
    {
      Q1vector->PutValue(j,pK[j],std::log(Q1[i][j])); //logarithmic 
      Q2vector->PutValue(j,pK[j],Q2[i][j]);
    }

      for (j=0;j<reducedEnergyGrid;j++)
    {
      Q1E[i][j]=Q1vector->Value(ppK[j]);
      Q2E[i][j]=Q2vector->Value(ppK[j]);
    }
      delete Q1vector;
      delete Q2vector;
    } 
  //
  //TABLES to be stored
  //
  G4PhysicsTable* theTable1 = new G4PhysicsTable();
  G4PhysicsTable* theTable2 = new G4PhysicsTable();
  // the table will contain reducedEnergyGrid G4PhysicsFreeVectors with different
  // values of k, 
  // Each of the G4PhysicsFreeVectors has a profile of
  // y vs. E
  //
  //reserve space of the vectors.
  for (j=0;j<reducedEnergyGrid;j++)   
    {
      G4PhysicsFreeVector* thevec = new G4PhysicsFreeVector(NumberofEPoints);
      theTable1->push_back(thevec);
      G4PhysicsFreeVector* thevec2 = new G4PhysicsFreeVector(NumberofEPoints);
      theTable2->push_back(thevec2);
    }  

  for (j=0;j<reducedEnergyGrid;j++)
    {
      G4PhysicsFreeVector* thevec = (G4PhysicsFreeVector*) (*theTable1)[j];
      G4PhysicsFreeVector* thevec2 = (G4PhysicsFreeVector*) (*theTable2)[j];
      for (i=0;i<NumberofEPoints;i++)
    {
      thevec->PutValue(i,betas[i],Q1E[i][j]);
      thevec2->PutValue(i,betas[i],Q2E[i][j]);
    }
      thevec->SetSpline(true);
      thevec2->SetSpline(true);
    }

  if (theLorentzTables1 && theLorentzTables2)
    {
      theLorentzTables1->insert(std::make_pair(Zmat,theTable1));
      theLorentzTables2->insert(std::make_pair(Zmat,theTable2));
    }
  else
    {
      G4ExceptionDescription ed;
      ed << "Unable to create tables of Lorentz coefficients for " << G4endl;
      ed << "<Z>= "  << Zmat << " in G4PenelopeBremsstrahlungAngular" << G4endl;
      delete theTable1;
      delete theTable2;
      G4Exception("G4PenelopeBremsstrahlungAngular::PrepareInterpolationTables()",
          "em2005",FatalException,ed);  
    }
  
  return;
}

G4ThreeVector & G4PenelopeBremsstrahlungAngular::SampleDirection ( const G4DynamicParticle *  dp, G4double  out_energy, G4int  Z, const G4Material *  mat = 0  )

virtual

Samples the direction of the outgoing photon (in global coordinates).

Implements G4VEmAngularDistribution.

Definition at line 329 of file G4PenelopeBremsstrahlungAngular.cc.

References python.hepunit::electron_mass_c2, FatalException, G4VEmAngularDistribution::fLocalDirection, G4cout, G4endl, G4Exception(), G4UniformRand, G4DynamicParticle::GetKineticEnergy(), G4DynamicParticle::GetMomentumDirection(), G4Material::GetName(), python.hepunit::keV, G4INCL::Math::max(), G4INCL::Math::min(), CLHEP::Hep3Vector::rotateUz(), CLHEP::Hep3Vector::set(), python.hepunit::twopi, and G4PhysicsVector::Value().

Referenced by G4PenelopeBremsstrahlungModel::SampleSecondaries().

{
  if (!material)
    {
      G4Exception("G4PenelopeBremsstrahlungAngular::SampleDirection()",
          "em2040",FatalException,"The pointer to G4Material* is NULL");
      return fLocalDirection;
    }
  
  //Retrieve the effective Z
  G4double Zmat = 0;

  if (!theEffectiveZSq)
    {
      G4Exception("G4PenelopeBremsstrahlungAngular::SampleDirection()",
          "em2040",FatalException,"EffectiveZ table not available");
      return fLocalDirection;
    }

  //found in the table: return it 
  if (theEffectiveZSq->count(material))
    Zmat = theEffectiveZSq->find(material)->second; 
  else
    {
      G4Exception("G4PenelopeBremsstrahlungAngular::SampleDirection()",
          "em2040",FatalException,"Material not found in the effectiveZ table");
      return fLocalDirection;
    }

  if (verbosityLevel > 0)
    {
      G4cout << "Effective <Z> for material : " << material->GetName() << 
    " = " << Zmat << G4endl;
    }

  G4double ePrimary = dp->GetKineticEnergy();

  G4double beta = std::sqrt(ePrimary*(ePrimary+2*electron_mass_c2))/
    (ePrimary+electron_mass_c2);
  G4double cdt = 0;
  G4double sinTheta = 0;
  G4double phi = 0;

  //Use a pure dipole distribution for energy above 500 keV
  if (ePrimary > 500*keV)
    {
      cdt = 2.0*G4UniformRand() - 1.0;
      if (G4UniformRand() > 0.75)
    {
      if (cdt<0)
        cdt = -1.0*std::pow(-cdt,1./3.);
      else
        cdt = std::pow(cdt,1./3.);
    }
      cdt = (cdt+beta)/(1.0+beta*cdt);
      //Get primary kinematics
      sinTheta = std::sqrt(1. - cdt*cdt);
      phi  = twopi * G4UniformRand(); 
      fLocalDirection.set(sinTheta* std::cos(phi),
              sinTheta* std::sin(phi),
              cdt);
      //rotate
      fLocalDirection.rotateUz(dp->GetMomentumDirection());
      //return
      return fLocalDirection;
    }
  
  if (!(theLorentzTables1->count(Zmat)) || !(theLorentzTables2->count(Zmat)))
    {
      G4ExceptionDescription ed;
      ed << "Unable to retrieve Lorentz tables for Z= " << Zmat << G4endl;
      G4Exception("G4PenelopeBremsstrahlungAngular::SampleDirection()",
          "em2006",FatalException,ed);
    }
    
  //retrieve actual tables
  const G4PhysicsTable* theTable1 = theLorentzTables1->find(Zmat)->second;
  const G4PhysicsTable* theTable2 = theLorentzTables2->find(Zmat)->second;
      
  G4double RK=20.0*eGamma/ePrimary;
  G4int ik=std::min((G4int) RK,19);
  
  G4double P10=0,P11=0,P1=0;
  G4double P20=0,P21=0,P2=0;

  //First coefficient
  const G4PhysicsFreeVector* v1 = (G4PhysicsFreeVector*) (*theTable1)[ik];
  const G4PhysicsFreeVector* v2 = (G4PhysicsFreeVector*) (*theTable1)[ik+1];
  P10 = v1->Value(beta);
  P11 = v2->Value(beta);
  P1=P10+(RK-(G4double) ik)*(P11-P10);
  
  //Second coefficient
  const G4PhysicsFreeVector* v3 = (G4PhysicsFreeVector*) (*theTable2)[ik];
  const G4PhysicsFreeVector* v4 = (G4PhysicsFreeVector*) (*theTable2)[ik+1];
  P20=v3->Value(beta); 
  P21=v4->Value(beta);
  P2=P20+(RK-(G4double) ik)*(P21-P20);
  
  //Sampling from the Lorenz-trasformed dipole distributions
  P1=std::min(std::exp(P1)/beta,1.0);
  G4double betap = std::min(std::max(beta*(1.0+P2/beta),0.0),0.9999);
  
  G4double testf=0;
  
  if (G4UniformRand() < P1)
    {
      do{
    cdt = 2.0*G4UniformRand()-1.0;
    testf=2.0*G4UniformRand()-(1.0+cdt*cdt);
      }while(testf>0);
    }
  else
    {
      do{
    cdt = 2.0*G4UniformRand()-1.0;
    testf=G4UniformRand()-(1.0-cdt*cdt);
      }while(testf>0);
    }
  cdt = (cdt+betap)/(1.0+betap*cdt);

  //Get primary kinematics
  sinTheta = std::sqrt(1. - cdt*cdt);
  phi  = twopi * G4UniformRand(); 
  fLocalDirection.set(sinTheta* std::cos(phi),
              sinTheta* std::sin(phi),
              cdt);
  //rotate
  fLocalDirection.rotateUz(dp->GetMomentumDirection());
  //return
  return fLocalDirection;
  
}

void G4PenelopeBremsstrahlungAngular::SetVerbosityLevel ( G4int  vl )

inline

Set/Get Verbosity level.

Definition at line 77 of file G4PenelopeBremsstrahlungAngular.hh.

{verbosityLevel = vl;};

---

The documentation for this class was generated from the following files:

• G4PenelopeBremsstrahlungAngular.hh
• G4PenelopeBremsstrahlungAngular.cc