443 lines
15 KiB
C++
443 lines
15 KiB
C++
//
|
|
// ********************************************************************
|
|
// * DISCLAIMER *
|
|
// * *
|
|
// * The following disclaimer summarizes all the specific disclaimers *
|
|
// * of contributors to this software. The specific disclaimers,which *
|
|
// * govern, are listed with their locations in: *
|
|
// * http://cern.ch/geant4/license *
|
|
// * *
|
|
// * Neither the authors of this software system, nor their employing *
|
|
// * institutes,nor the agencies providing financial support for this *
|
|
// * work make any representation or warranty, express or implied, *
|
|
// * regarding this software system or assume any liability for its *
|
|
// * use. *
|
|
// * *
|
|
// * This code implementation is the intellectual property of the *
|
|
// * GEANT4 collaboration. *
|
|
// * By copying, distributing or modifying the Program (or any work *
|
|
// * based on the Program) you indicate your acceptance of this *
|
|
// * statement, and all its terms. *
|
|
// ********************************************************************
|
|
//
|
|
// neutron_hp -- source file
|
|
// J.P. Wellisch, Nov-1996
|
|
// A prototype of the low energy neutron transport model.
|
|
//
|
|
// there is a lot of unused (and undebugged) code in this file. Kept for the moment just in case. @@
|
|
|
|
#include "G4NeutronHPPhotonDist.hh"
|
|
#include "G4NeutronHPLegendreStore.hh"
|
|
#include "G4Electron.hh"
|
|
#include "G4Poisson.hh"
|
|
|
|
G4bool G4NeutronHPPhotonDist::InitMean(G4std::ifstream & aDataFile)
|
|
{
|
|
G4bool result = true;
|
|
if(aDataFile >> repFlag)
|
|
{
|
|
aDataFile >> targetMass;
|
|
if(repFlag==1)
|
|
{
|
|
// multiplicities
|
|
aDataFile >> nDiscrete;
|
|
disType = new G4int[nDiscrete];
|
|
energy = new G4double[nDiscrete];
|
|
actualMult = new G4int[nDiscrete];
|
|
theYield = new G4NeutronHPVector[nDiscrete];
|
|
for (G4int i=0; i<nDiscrete; i++)
|
|
{
|
|
aDataFile >> disType[i]>>energy[i];
|
|
energy[i]*=eV;
|
|
theYield[i].Init(aDataFile, eV);
|
|
}
|
|
}
|
|
else if(repFlag == 2)
|
|
{
|
|
aDataFile >> theInternalConversionFlag;
|
|
aDataFile >> theBaseEnergy;
|
|
theBaseEnergy*=eV;
|
|
aDataFile >> theInternalConversionFlag;
|
|
aDataFile >> nGammaEnergies;
|
|
theLevelEnergies = new G4double[nGammaEnergies];
|
|
theTransitionProbabilities = new G4double[nGammaEnergies];
|
|
if(theInternalConversionFlag == 2) thePhotonTransitionFraction = new G4double[nGammaEnergies];
|
|
for(G4int ii=0; ii<nGammaEnergies; ii++)
|
|
{
|
|
if(theInternalConversionFlag == 1)
|
|
{
|
|
aDataFile >> theLevelEnergies[ii] >> theTransitionProbabilities[ii];
|
|
theLevelEnergies[ii]*=eV;
|
|
}
|
|
else if(theInternalConversionFlag == 2)
|
|
{
|
|
aDataFile >> theLevelEnergies[ii] >> theTransitionProbabilities[ii] >> thePhotonTransitionFraction[ii];
|
|
theLevelEnergies[ii]*=eV;
|
|
}
|
|
else
|
|
{
|
|
G4Exception("G4NeutronHPPhotonDist: Unknown conversion flag");
|
|
}
|
|
}
|
|
// Note, that this is equivalent to using the 'Gamma' classes.
|
|
// G4Exception("G4NeutronHPPhotonDist: Transition probability array not sampled for the moment.");
|
|
}
|
|
else
|
|
{
|
|
G4cout << "Data representation in G4NeutronHPPhotonDist: "<<repFlag<<G4endl;
|
|
G4Exception("G4NeutronHPPhotonDist: This data representation is not implemented.");
|
|
}
|
|
}
|
|
else
|
|
{
|
|
result = false;
|
|
}
|
|
return result;
|
|
}
|
|
|
|
void G4NeutronHPPhotonDist::InitAngular(G4std::ifstream & aDataFile)
|
|
{
|
|
G4int i, ii;
|
|
//angular distributions
|
|
aDataFile >> isoFlag;
|
|
if (isoFlag != 1)
|
|
{
|
|
aDataFile >> tabulationType >> nDiscrete2 >> nIso;
|
|
theShells = new G4double[nDiscrete2];
|
|
theGammas = new G4double[nDiscrete2];
|
|
for (i=0; i< nIso; i++) // isotropic photons
|
|
{
|
|
aDataFile >> theGammas[i] >> theShells[i];
|
|
theGammas[i]*=eV;
|
|
theShells[i]*=eV;
|
|
}
|
|
nNeu = new G4int [nDiscrete2-nIso];
|
|
if(tabulationType==1)theLegendre=new G4NeutronHPLegendreTable *[nDiscrete2-nIso];
|
|
if(tabulationType==2)theAngular =new G4NeutronHPAngularP *[nDiscrete2-nIso];
|
|
for(i=nIso; i< nDiscrete2; i++)
|
|
{
|
|
if(tabulationType==1)
|
|
{
|
|
aDataFile >> theGammas[i] >> theShells[i] >> nNeu[i-nIso];
|
|
theGammas[i]*=eV;
|
|
theShells[i]*=eV;
|
|
theLegendre[i-nIso]=new G4NeutronHPLegendreTable[nNeu[i-nIso]];
|
|
theLegendreManager.Init(aDataFile);
|
|
for (ii=0; ii<nNeu[i-nIso]; ii++)
|
|
{
|
|
theLegendre[i-nIso][ii].Init(aDataFile);
|
|
}
|
|
}
|
|
else if(tabulationType==2)
|
|
{
|
|
aDataFile >> theGammas[i] >> theShells[i] >> nNeu[i-nIso];
|
|
theGammas[i]*=eV;
|
|
theShells[i]*=eV;
|
|
theAngular[i-nIso]=new G4NeutronHPAngularP[nNeu[i-nIso]];
|
|
for (ii=0; ii<nNeu[i-nIso]; ii++)
|
|
{
|
|
theAngular[i-nIso][ii].Init(aDataFile);
|
|
}
|
|
}
|
|
else
|
|
{
|
|
G4cout << "tabulation type: tabulationType"<<G4endl;
|
|
G4Exception("cannot deal with this tabulation type for angular distributions.");
|
|
}
|
|
}
|
|
}
|
|
}
|
|
|
|
|
|
void G4NeutronHPPhotonDist::InitEnergies(G4std::ifstream & aDataFile)
|
|
{
|
|
G4int i, energyDistributionsNeeded = 0;
|
|
for (i=0; i<nDiscrete; i++)
|
|
{
|
|
if( disType[i]==1) energyDistributionsNeeded =1;
|
|
}
|
|
if(!energyDistributionsNeeded) return;
|
|
aDataFile >> nPartials;
|
|
distribution = new G4int[nPartials];
|
|
probs = new G4NeutronHPVector[nPartials];
|
|
partials = new G4NeutronHPPartial * [nPartials];
|
|
G4int nen;
|
|
G4int dummy;
|
|
for (i=0; i<nPartials; i++)
|
|
{
|
|
aDataFile >> dummy;
|
|
probs[i].Init(aDataFile, eV);
|
|
aDataFile >> nen;
|
|
partials[i] = new G4NeutronHPPartial(nen);
|
|
partials[i]->InitInterpolation(aDataFile);
|
|
partials[i]->Init(aDataFile);
|
|
}
|
|
}
|
|
|
|
void G4NeutronHPPhotonDist::InitPartials(G4std::ifstream & aDataFile)
|
|
{
|
|
aDataFile >> nDiscrete >> targetMass;
|
|
if(nDiscrete != 1)
|
|
{
|
|
theTotalXsec.Init(aDataFile, eV);
|
|
}
|
|
G4int i;
|
|
theGammas = new G4double[nDiscrete];
|
|
theShells = new G4double[nDiscrete];
|
|
isPrimary = new G4int[nDiscrete];
|
|
disType = new G4int[nDiscrete];
|
|
thePartialXsec = new G4NeutronHPVector[nDiscrete];
|
|
for(i=0; i<nDiscrete; i++)
|
|
{
|
|
aDataFile>>theGammas[i]>>theShells[i]>>isPrimary[i]>>disType[i];
|
|
theGammas[i]*=eV;
|
|
theShells[i]*=eV;
|
|
thePartialXsec[i].Init(aDataFile, eV);
|
|
}
|
|
}
|
|
|
|
G4ReactionProductVector * G4NeutronHPPhotonDist::GetPhotons(G4double anEnergy)
|
|
{
|
|
// the partial cross-section case is not in this yet. @@@@
|
|
G4int i, ii, iii;
|
|
G4int nSecondaries = 0;
|
|
G4ReactionProductVector * thePhotons = new G4ReactionProductVector;
|
|
if(repFlag==1)
|
|
{
|
|
G4double current=0;
|
|
for(i=0; i<nDiscrete; i++)
|
|
{
|
|
current = theYield[i].GetY(anEnergy);
|
|
actualMult[i] = G4Poisson(current); // max cut-off still missing @@@
|
|
if(nDiscrete==1&¤t<1.0001)
|
|
{
|
|
actualMult[i] = static_cast<G4int>(current);
|
|
if(current<1)
|
|
{
|
|
actualMult[i] = 0;
|
|
if(G4UniformRand()<current) actualMult[i] = 1;
|
|
}
|
|
}
|
|
nSecondaries += actualMult[i];
|
|
}
|
|
for(i=0;i<nSecondaries;i++)
|
|
{
|
|
G4ReactionProduct * theOne = new G4ReactionProduct;
|
|
theOne->SetDefinition(G4Gamma::Gamma());
|
|
thePhotons->push_back(theOne);
|
|
}
|
|
G4int count=0;
|
|
for(i=0; i<nDiscrete; i++)
|
|
{
|
|
for(ii=0; ii< actualMult[i]; ii++)
|
|
{
|
|
if(disType[i]==1) // continuum
|
|
{
|
|
G4double sum=0, run=0;
|
|
for(iii=0; iii<nPartials; iii++) sum+=probs[iii].GetY(anEnergy);
|
|
G4double random = G4UniformRand();
|
|
G4int theP = 0;
|
|
for(iii=0; iii<nPartials; iii++)
|
|
{
|
|
run+=probs[iii].GetY(anEnergy);
|
|
theP = iii;
|
|
if(random<run/sum) break;
|
|
}
|
|
if(theP==nPartials) theP=nPartials-1; // das sortiert J aus.
|
|
sum=0;
|
|
G4NeutronHPVector * temp;
|
|
temp = partials[theP]->GetY(anEnergy); //@@@ look at, seems fishy
|
|
G4double eGamm = temp->Sample();
|
|
thePhotons->operator[](count)->SetKineticEnergy(eGamm);
|
|
delete temp;
|
|
}
|
|
else // discrete
|
|
{
|
|
thePhotons->operator[](count)->SetKineticEnergy(energy[i]);
|
|
}
|
|
count++;
|
|
if(count > nSecondaries) G4Exception("G4NeutronHPPhotonDist::GetPhotons inconsistancy");
|
|
}
|
|
}
|
|
// now do the angular distributions...
|
|
if( isoFlag == 1)
|
|
{
|
|
for (i=0; i< nSecondaries; i++)
|
|
{
|
|
G4double costheta = 2.*G4UniformRand()-1;
|
|
G4double theta = acos(costheta);
|
|
G4double phi = twopi*G4UniformRand();
|
|
G4double sinth = sin(theta);
|
|
G4double en = thePhotons->operator[](i)->GetTotalEnergy();
|
|
G4ThreeVector temp(en*sinth*cos(phi), en*sinth*sin(phi), en*cos(theta) );
|
|
thePhotons->operator[](i)->SetMomentum( temp ) ;
|
|
// G4cout << "Isotropic distribution in PhotonDist"<<temp<<G4endl;
|
|
}
|
|
}
|
|
else
|
|
{
|
|
for(i=0; i<nSecondaries; i++)
|
|
{
|
|
G4double currentEnergy = thePhotons->operator[](i)->GetTotalEnergy();
|
|
for(ii=0; ii<nDiscrete2; ii++)
|
|
{
|
|
if (abs(currentEnergy-theGammas[ii])<0.1*keV) break;
|
|
}
|
|
if(ii==nDiscrete2) ii--; // fix for what seems an (file12 vs file 14) inconsistancy found in the ENDF 7N14 data. @@
|
|
if(ii<nIso)
|
|
{
|
|
// isotropic distribution
|
|
G4double theta = pi*G4UniformRand();
|
|
G4double phi = twopi*G4UniformRand();
|
|
G4double sinth = sin(theta);
|
|
G4double en = thePhotons->operator[](i)->GetTotalEnergy();
|
|
G4ThreeVector tempVector(en*sinth*cos(phi), en*sinth*sin(phi), en*cos(theta) );
|
|
thePhotons->operator[](i)->SetMomentum( tempVector ) ;
|
|
}
|
|
else if(tabulationType==1)
|
|
{
|
|
// legendre polynomials
|
|
G4int it(0);
|
|
for (iii=0; iii<nNeu[ii-nIso]; iii++) // find the neutron energy
|
|
{
|
|
it = iii;
|
|
if(theLegendre[ii-nIso][iii].GetEnergy()>anEnergy)
|
|
break;
|
|
}
|
|
G4NeutronHPLegendreStore aStore(2);
|
|
aStore.SetCoeff(1, &(theLegendre[ii-nIso][it]));
|
|
aStore.SetCoeff(0, &(theLegendre[ii-nIso][it-1]));
|
|
G4double cosTh = aStore.SampleMax(anEnergy);
|
|
G4double theta = acos(cosTh);
|
|
G4double phi = twopi*G4UniformRand();
|
|
G4double sinth = sin(theta);
|
|
G4double en = thePhotons->operator[](i)->GetTotalEnergy();
|
|
G4ThreeVector tempVector(en*sinth*cos(phi), en*sinth*sin(phi), en*cos(theta) );
|
|
thePhotons->operator[](i)->SetMomentum( tempVector ) ;
|
|
}
|
|
else
|
|
{
|
|
// tabulation of probabilities.
|
|
G4int it(0);
|
|
for (iii=0; iii<nNeu[ii-nIso]; iii++) // find the neutron energy
|
|
{
|
|
it = iii;
|
|
if(theAngular[ii-nIso][iii].GetEnergy()>anEnergy)
|
|
break;
|
|
}
|
|
G4double costh = theAngular[ii-nIso][it].GetCosTh(); // no interpolation yet @@
|
|
G4double theta = acos(costh);
|
|
G4double phi = twopi*G4UniformRand();
|
|
G4double sinth = sin(theta);
|
|
G4double en = thePhotons->operator[](i)->GetTotalEnergy();
|
|
G4ThreeVector tmpVector(en*sinth*cos(phi), en*sinth*sin(phi), en*costh );
|
|
thePhotons->operator[](i)->SetMomentum( tmpVector ) ;
|
|
}
|
|
}
|
|
}
|
|
}
|
|
else if(repFlag == 2)
|
|
{
|
|
G4double * running = new G4double[nGammaEnergies];
|
|
running[0]=theTransitionProbabilities[0];
|
|
G4int i;
|
|
for(i=1; i<nGammaEnergies; i++)
|
|
{
|
|
running[i]=running[i-1]+theTransitionProbabilities[i];
|
|
}
|
|
G4double random = G4UniformRand();
|
|
G4int it=0;
|
|
for(i=0; i<nGammaEnergies; i++)
|
|
{
|
|
it = i;
|
|
if(random < running[i]/running[nGammaEnergies-1]) break;
|
|
}
|
|
delete [] running;
|
|
G4double totalEnergy = theBaseEnergy - theLevelEnergies[it];
|
|
G4ReactionProduct * theOne = new G4ReactionProduct;
|
|
theOne->SetDefinition(G4Gamma::Gamma());
|
|
random = G4UniformRand();
|
|
if(theInternalConversionFlag==2 && random>thePhotonTransitionFraction[it])
|
|
{
|
|
theOne->SetDefinition(G4Electron::Electron());
|
|
}
|
|
theOne->SetTotalEnergy(totalEnergy);
|
|
if( isoFlag == 1)
|
|
{
|
|
G4double costheta = 2.*G4UniformRand()-1;
|
|
G4double theta = acos(costheta);
|
|
G4double phi = twopi*G4UniformRand();
|
|
G4double sinth = sin(theta);
|
|
G4double en = theOne->GetTotalEnergy();
|
|
G4ThreeVector temp(en*sinth*cos(phi), en*sinth*sin(phi), en*cos(theta) );
|
|
theOne->SetMomentum( temp ) ;
|
|
}
|
|
else
|
|
{
|
|
G4double currentEnergy = theOne->GetTotalEnergy();
|
|
for(ii=0; ii<nDiscrete2; ii++)
|
|
{
|
|
if (abs(currentEnergy-theGammas[ii])<0.1*keV) break;
|
|
}
|
|
if(ii==nDiscrete2) ii--; // fix for what seems an (file12 vs file 14) inconsistancy found in the ENDF 7N14 data. @@
|
|
if(ii<nIso)
|
|
{
|
|
// isotropic distribution
|
|
G4double theta = pi*G4UniformRand();
|
|
G4double phi = twopi*G4UniformRand();
|
|
G4double sinth = sin(theta);
|
|
G4double en = theOne->GetTotalEnergy();
|
|
G4ThreeVector tempVector(en*sinth*cos(phi), en*sinth*sin(phi), en*cos(theta) );
|
|
theOne->SetMomentum( tempVector ) ;
|
|
}
|
|
else if(tabulationType==1)
|
|
{
|
|
// legendre polynomials
|
|
G4int it(0);
|
|
for (iii=0; iii<nNeu[ii-nIso]; iii++) // find the neutron energy
|
|
{
|
|
it = iii;
|
|
if(theLegendre[ii-nIso][iii].GetEnergy()>anEnergy)
|
|
break;
|
|
}
|
|
G4NeutronHPLegendreStore aStore(2);
|
|
aStore.SetCoeff(1, &(theLegendre[ii-nIso][it]));
|
|
aStore.SetCoeff(0, &(theLegendre[ii-nIso][it-1]));
|
|
G4double cosTh = aStore.SampleMax(anEnergy);
|
|
G4double theta = acos(cosTh);
|
|
G4double phi = twopi*G4UniformRand();
|
|
G4double sinth = sin(theta);
|
|
G4double en = theOne->GetTotalEnergy();
|
|
G4ThreeVector tempVector(en*sinth*cos(phi), en*sinth*sin(phi), en*cos(theta) );
|
|
theOne->SetMomentum( tempVector ) ;
|
|
}
|
|
else
|
|
{
|
|
// tabulation of probabilities.
|
|
G4int it(0);
|
|
for (iii=0; iii<nNeu[ii-nIso]; iii++) // find the neutron energy
|
|
{
|
|
it = iii;
|
|
if(theAngular[ii-nIso][iii].GetEnergy()>anEnergy)
|
|
break;
|
|
}
|
|
G4double costh = theAngular[ii-nIso][it].GetCosTh(); // no interpolation yet @@
|
|
G4double theta = acos(costh);
|
|
G4double phi = twopi*G4UniformRand();
|
|
G4double sinth = sin(theta);
|
|
G4double en = theOne->GetTotalEnergy();
|
|
G4ThreeVector tmpVector(en*sinth*cos(phi), en*sinth*sin(phi), en*costh );
|
|
theOne->SetMomentum( tmpVector ) ;
|
|
}
|
|
}
|
|
thePhotons->push_back(theOne);
|
|
}
|
|
else
|
|
{
|
|
delete thePhotons;
|
|
thePhotons = NULL; // no gamma data available; some work needed @@@@@@@
|
|
}
|
|
return thePhotons;
|
|
}
|
|
|