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This commit is contained in:
Gabriele Cosmo
2021-06-25 16:12:29 +02:00
parent c968e26a39
commit 6399a014b6
4200 changed files with 207479 additions and 237366 deletions
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source/processes/electromagnetic/standard/src/G4PAIySection.cc
+13 -13
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@@ -146,7 +146,7 @@ void G4PAIySection::Initialize( const G4Material* material,
fA3 = G4DataVector(fIntervalNumber+2,0.0);
fA4 = G4DataVector(fIntervalNumber+2,0.0);
for( i = 1; i <= fIntervalNumber; i++ )
for( i = 1; i <= fIntervalNumber; ++i )
{
if ( sandia->GetSandiaMatTablePAI(i-1,0) < 1.*eV )
{
@@ -182,7 +182,7 @@ void G4PAIySection::Initialize( const G4Material* material,
}
if( fVerbose > 0 )
{
for( i = 1; i <= fIntervalNumber; i++ )
for( i = 1; i <= fIntervalNumber; ++i )
{
G4cout<<i<<"\t"<<fEnergyInterval[i]/keV<<"\t"<<fA1[i]<<"\t"<<fA2[i]<<"\t"
<<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl;
@@ -191,7 +191,7 @@ void G4PAIySection::Initialize( const G4Material* material,
if( fVerbose > 0 ) {
G4cout<<"Now checking, if two borders are too close together"<<G4endl;
}
for( i = 1; i < fIntervalNumber; i++ )
for( i = 1; i < fIntervalNumber; ++i )
{
if( fEnergyInterval[i+1]-fEnergyInterval[i] >
1.5*fDelta*(fEnergyInterval[i+1]+fEnergyInterval[i]) ) continue;
@@ -210,7 +210,7 @@ void G4PAIySection::Initialize( const G4Material* material,
}
if( fVerbose > 0 )
{
for( i = 1; i <= fIntervalNumber; i++ )
for( i = 1; i <= fIntervalNumber; ++i )
{
G4cout<<i<<"\t"<<fEnergyInterval[i]/keV<<"\t"<<fA1[i]<<"\t"<<fA2[i]<<"\t"
<<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl;
@@ -228,7 +228,7 @@ void G4PAIySection::Initialize( const G4Material* material,
// Preparation of integral PAI cross section for input betaGammaSq
for( i = 1; i <= fSplineNumber; i++ )
for( i = 1; i <= fSplineNumber; ++i )
{
fDifPAIySection[i] = DifPAIySection(i,betaGammaSq);
@@ -254,13 +254,13 @@ void G4PAIySection::ComputeLowEnergyCof(const G4Material* material)
G4double* thisMaterialZ = new G4double[numberOfElements];
G4double* thisMaterialCof = new G4double[numberOfElements];
for( i = 0; i < numberOfElements; i++ )
for( i = 0; i < numberOfElements; ++i )
{
thisMaterialZ[i] = material->GetElement(i)->GetZ();
sumZ += thisMaterialZ[i];
thisMaterialCof[i] = p0+p1*thisMaterialZ[i]+p2*thisMaterialZ[i]*thisMaterialZ[i];
}
for( i = 0; i < numberOfElements; i++ )
for( i = 0; i < numberOfElements; ++i )
{
sumCof += thisMaterialCof[i]*thisMaterialZ[i]/sumZ;
}
@@ -290,7 +290,7 @@ void G4PAIySection::InitPAI()
IntegralCerenkov();
IntegralPlasmon();
for( i = 0; i<= fSplineNumber; i++)
for( i = 0; i<= fSplineNumber; ++i)
{
fPAItable[i][fRefGammaNumber] = fIntegralPAIySection[i];
@@ -304,7 +304,7 @@ void G4PAIySection::InitPAI()
betaGammaSq = fLorentzFactor[j]*fLorentzFactor[j] - 1;
for(i = 1; i <= fSplineNumber; i++)
for(i = 1; i <= fSplineNumber; ++i)
{
fDifPAIySection[i] = DifPAIySection(i,betaGammaSq);
fdNdxCerenkov[i] = PAIdNdxCerenkov(i,betaGammaSq);
@@ -314,7 +314,7 @@ void G4PAIySection::InitPAI()
IntegralCerenkov();
IntegralPlasmon();
for(i = 0; i <= fSplineNumber; i++)
for(i = 0; i <= fSplineNumber; ++i)
{
fPAItable[i][j] = fIntegralPAIySection[i];
}
@@ -346,7 +346,7 @@ void G4PAIySection::NormShift(G4double betaGammaSq)
j = 1;
for(i=2;i<=fSplineNumber;i++)
for(i=2;i<=fSplineNumber;++i)
{
if(fSplineEnergy[i]<fEnergyInterval[j+1])
{
@@ -409,7 +409,7 @@ void G4PAIySection::SplainPAI(G4double betaGammaSq)
if(fSplineEnergy[i+1] > fEnergyInterval[k+1])
{
k++; // Here next energy point is in next energy interval
i++;
++i;
continue;
}
// Shifting of arrayes for inserting the geometrical
@@ -539,7 +539,7 @@ G4double G4PAIySection::RePartDielectricConst(G4double enb)
x0 = enb;
result = 0;
for(G4int i=1;i<=fIntervalNumber-1;i++)
for(G4int i=1;i<=fIntervalNumber-1;++i)
{
x1 = fEnergyInterval[i];
x2 = fEnergyInterval[i+1];