lars/geant4
1
0
Fork 0
Code Issues Pull Requests Actions Packages Projects Releases Wiki Activity

Import Geant4 10.3.0.beta source tree

Browse Source
This commit is contained in:
Gabriele Cosmo
2016-06-30 14:12:05 +02:00
parent a654a7ab1f
commit 4ec577e5c4
2021 changed files with 100995 additions and 78277 deletions
Download Patch File Download Diff File Expand all files Collapse all files
source/processes/electromagnetic/standard/src/G4eeToTwoGammaModel.cc
+4 -4
View File
@@ -23,7 +23,7 @@
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
// $Id: G4eeToTwoGammaModel.cc 91726 2015-08-03 15:41:36Z gcosmo $
// $Id: G4eeToTwoGammaModel.cc 96934 2016-05-18 09:10:41Z gcosmo $
//
// -------------------------------------------------------------------
//
@@ -91,7 +91,7 @@ G4eeToTwoGammaModel::G4eeToTwoGammaModel(const G4ParticleDefinition*,
isInitialised(false)
{
theGamma = G4Gamma::Gamma();
fParticleChange = 0;
fParticleChange = nullptr;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
@@ -177,7 +177,7 @@ void G4eeToTwoGammaModel::SampleSecondaries(vector<G4DynamicParticle*>* vdp,
if(PositKinEnergy == 0.0) {
G4double cost = 2.*rndmEngine->flat()-1.;
G4double sint = sqrt((1. - cost)*(1. + cost));
G4double phi = twopi * G4UniformRand();
G4double phi = twopi * rndmEngine->flat();
G4ThreeVector dir(sint*cos(phi), sint*sin(phi), cost);
phi = twopi * rndmEngine->flat();
G4ThreeVector pol(cos(phi), sin(phi), 0.0);
@@ -239,7 +239,7 @@ void G4eeToTwoGammaModel::SampleSecondaries(vector<G4DynamicParticle*>* vdp,
G4ThreeVector Phot1Direction(sint*cos(phi), sint*sin(phi), cost);
Phot1Direction.rotateUz(PositDirection);
aGamma1 = new G4DynamicParticle (theGamma,Phot1Direction, Phot1Energy);
phi = twopi * G4UniformRand();
phi = twopi * rndmEngine->flat();
G4ThreeVector pol1(cos(phi), sin(phi), 0.0);
pol1.rotateUz(Phot1Direction);
aGamma1->SetPolarization(pol1.x(),pol1.y(),pol1.z());