434 lines
15 KiB
C++
434 lines
15 KiB
C++
//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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// -------------------------------------------------------------------
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//
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// Geant4 Class file
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//
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// File name: G4PolarizedComptonModel
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//
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// Author: Andreas Schaelicke
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#include "G4PolarizedComptonModel.hh"
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#include "G4Exp.hh"
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#include "G4Log.hh"
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#include "G4ParticleChangeForGamma.hh"
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#include "G4PhysicalConstants.hh"
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#include "G4PolarizationManager.hh"
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#include "G4PolarizationHelper.hh"
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#include "G4PolarizedComptonXS.hh"
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#include "G4StokesVector.hh"
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#include "G4SystemOfUnits.hh"
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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G4PolarizedComptonModel::G4PolarizedComptonModel(const G4ParticleDefinition*,
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const G4String& nam)
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: G4KleinNishinaCompton(nullptr, nam)
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, fVerboseLevel(0)
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{
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fCrossSectionCalculator = new G4PolarizedComptonXS();
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fBeamPolarization = G4StokesVector::ZERO;
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fTargetPolarization = G4StokesVector::ZERO;
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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G4PolarizedComptonModel::~G4PolarizedComptonModel()
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{
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delete fCrossSectionCalculator;
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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G4double G4PolarizedComptonModel::ComputeAsymmetryPerAtom(G4double gammaEnergy,
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G4double /*Z*/)
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{
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G4double asymmetry = 0.0;
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G4double k0 = gammaEnergy / electron_mass_c2;
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G4double k1 = 1. + 2. * k0;
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asymmetry = -k0;
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asymmetry *=
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(k0 + 1.) * sqr(k1) * G4Log(k1) - 2. * k0 * (5. * sqr(k0) + 4. * k0 + 1.);
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asymmetry /= ((k0 - 2.) * k0 - 2.) * sqr(k1) * G4Log(k1) +
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2. * k0 * (k0 * (k0 + 1.) * (k0 + 8.) + 2.);
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if(asymmetry > 1.)
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{
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G4ExceptionDescription ed;
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ed << "ERROR in G4PolarizedComptonModel::ComputeAsymmetryPerAtom.\n"
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<< " asymmetry = " << asymmetry << "\n";
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G4Exception("G4PolarizedComptonModel::ComputeAsymmetryPerAtom", "pol035",
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JustWarning, ed);
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}
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return asymmetry;
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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G4double G4PolarizedComptonModel::ComputeCrossSectionPerAtom(
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const G4ParticleDefinition* pd, G4double kinEnergy, G4double Z, G4double A,
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G4double cut, G4double emax)
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{
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G4double xs = G4KleinNishinaCompton::ComputeCrossSectionPerAtom(
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pd, kinEnergy, Z, A, cut, emax);
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G4double polzz = fBeamPolarization.p3() * fTargetPolarization.z();
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if(polzz > 0.0)
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{
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G4double asym = ComputeAsymmetryPerAtom(kinEnergy, Z);
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xs *= (1. + polzz * asym);
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}
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return xs;
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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void G4PolarizedComptonModel::SampleSecondaries(
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std::vector<G4DynamicParticle*>* fvect, const G4MaterialCutsCouple*,
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const G4DynamicParticle* aDynamicGamma, G4double, G4double)
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{
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// do nothing below the threshold
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if(aDynamicGamma->GetKineticEnergy() <= LowEnergyLimit())
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{
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return;
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}
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const G4Track* aTrack = fParticleChange->GetCurrentTrack();
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G4VPhysicalVolume* aPVolume = aTrack->GetVolume();
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G4LogicalVolume* aLVolume = aPVolume->GetLogicalVolume();
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if(fVerboseLevel >= 1)
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{
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G4cout << "G4PolarizedComptonModel::SampleSecondaries in "
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<< aLVolume->GetName() << G4endl;
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}
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G4PolarizationManager* polarizationManager =
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G4PolarizationManager::GetInstance();
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// obtain polarization of the beam
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fBeamPolarization = G4StokesVector(aDynamicGamma->GetPolarization());
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fBeamPolarization.SetPhoton();
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// obtain polarization of the media
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G4bool targetIsPolarized = polarizationManager->IsPolarized(aLVolume);
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fTargetPolarization = polarizationManager->GetVolumePolarization(aLVolume);
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// if beam is linear polarized or target is transversely polarized
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// determine the angle to x-axis
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// (assumes same PRF as in the polarization definition)
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G4ThreeVector gamDirection0 = aDynamicGamma->GetMomentumDirection();
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// transfer fTargetPolarization
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// into the gamma frame (problem electron is at rest)
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if(targetIsPolarized)
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{
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fTargetPolarization.rotateUz(gamDirection0);
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}
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// The scattered gamma energy is sampled according to
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// Klein - Nishina formula.
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// The random number techniques of Butcher & Messel are used
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// (Nuc Phys 20(1960),15).
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// Note : Effects due to binding of atomic electrons are neglected.
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G4double gamEnergy0 = aDynamicGamma->GetKineticEnergy();
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G4double E0_m = gamEnergy0 / electron_mass_c2;
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// sample the energy rate of the scattered gamma
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G4double epsilon, sint2;
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G4double onecost = 0.0;
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G4double Phi = 0.0;
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G4double greject = 1.0;
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G4double cosTeta = 1.0;
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G4double sinTeta = 0.0;
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G4double eps0 = 1. / (1. + 2. * E0_m);
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G4double epsilon0sq = eps0 * eps0;
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G4double alpha1 = -G4Log(eps0);
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G4double alpha2 = alpha1 + 0.5 * (1. - epsilon0sq);
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G4double polarization = fBeamPolarization.p3() * fTargetPolarization.p3();
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CLHEP::HepRandomEngine* rndmEngineMod = G4Random::getTheEngine();
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G4int nloop = 0;
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G4bool end = false;
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G4double rndm[3];
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do
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{
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do
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{
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++nloop;
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// false interaction if too many iterations
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if(nloop > fLoopLim)
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{
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PrintWarning(aDynamicGamma, nloop, greject, onecost, Phi,
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"too many iterations");
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return;
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}
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// 3 random numbers to sample scattering
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rndmEngineMod->flatArray(3, rndm);
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if(alpha1 > alpha2 * rndm[0])
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{
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epsilon = G4Exp(-alpha1 * rndm[1]);
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}
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else
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{
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epsilon = std::sqrt(epsilon0sq + (1. - epsilon0sq) * rndm[1]);
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}
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onecost = (1. - epsilon) / (epsilon * E0_m);
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sint2 = onecost * (2. - onecost);
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G4double gdiced = 2. * (1. / epsilon + epsilon);
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G4double gdist = 1. / epsilon + epsilon - sint2 -
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polarization * (1. / epsilon - epsilon) * (1. - onecost);
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greject = gdist / gdiced;
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if(greject > 1.0)
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{
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PrintWarning(aDynamicGamma, nloop, greject, onecost, Phi,
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"theta majoranta wrong");
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}
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// Loop checking, 03-Aug-2015, Vladimir Ivanchenko
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} while(greject < rndm[2]);
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// assuming phi loop successful
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end = true;
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// scattered gamma angles. ( Z - axis along the parent gamma)
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cosTeta = 1. - onecost;
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sinTeta = std::sqrt(sint2);
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do
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{
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++nloop;
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// 2 random numbers to sample scattering
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rndmEngineMod->flatArray(2, rndm);
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// false interaction if too many iterations
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Phi = twopi * rndm[0];
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if(nloop > fLoopLim)
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{
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PrintWarning(aDynamicGamma, nloop, greject, onecost, Phi,
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"too many iterations");
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return;
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}
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G4double gdiced = 1. / epsilon + epsilon - sint2 +
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std::abs(fBeamPolarization.p3()) *
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(std::abs((1. / epsilon - epsilon) * cosTeta *
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fTargetPolarization.p3()) +
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(1. - epsilon) * sinTeta *
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(std::sqrt(sqr(fTargetPolarization.p1()) +
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sqr(fTargetPolarization.p2())))) +
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sint2 * (std::sqrt(sqr(fBeamPolarization.p1()) +
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sqr(fBeamPolarization.p2())));
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G4double gdist =
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1. / epsilon + epsilon - sint2 +
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fBeamPolarization.p3() *
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((1. / epsilon - epsilon) * cosTeta * fTargetPolarization.p3() +
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(1. - epsilon) * sinTeta *
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(std::cos(Phi) * fTargetPolarization.p1() +
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std::sin(Phi) * fTargetPolarization.p2())) -
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sint2 * (std::cos(2. * Phi) * fBeamPolarization.p1() +
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std::sin(2. * Phi) * fBeamPolarization.p2());
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greject = gdist / gdiced;
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if(greject > 1.0)
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{
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PrintWarning(aDynamicGamma, nloop, greject, onecost, Phi,
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"phi majoranta wrong");
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}
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if(greject < 1.e-3)
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{
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PrintWarning(aDynamicGamma, nloop, greject, onecost, Phi,
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"phi loop ineffective");
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// restart theta loop
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end = false;
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break;
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}
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// Loop checking, 03-Aug-2015, Vladimir Ivanchenko
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} while(greject < rndm[1]);
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} while(!end);
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G4double dirx = sinTeta * std::cos(Phi);
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G4double diry = sinTeta * std::sin(Phi);
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G4double dirz = cosTeta;
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// update G4VParticleChange for the scattered gamma
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G4ThreeVector gamDirection1(dirx, diry, dirz);
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gamDirection1.rotateUz(gamDirection0);
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G4double gamEnergy1 = epsilon * gamEnergy0;
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G4double edep = 0.0;
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if(gamEnergy1 > lowestSecondaryEnergy)
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{
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fParticleChange->ProposeMomentumDirection(gamDirection1);
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fParticleChange->SetProposedKineticEnergy(gamEnergy1);
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}
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else
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{
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fParticleChange->ProposeTrackStatus(fStopAndKill);
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fParticleChange->SetProposedKineticEnergy(0.0);
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edep = gamEnergy1;
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}
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// calculate Stokes vector of final state photon and electron
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G4ThreeVector nInteractionFrame =
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G4PolarizationHelper::GetFrame(gamDirection1, gamDirection0);
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// transfer fBeamPolarization and fTargetPolarization
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// into the interaction frame (note electron is in gamma frame)
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if(fVerboseLevel >= 1)
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{
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G4cout << "========================================" << G4endl;
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G4cout << " nInteractionFrame = " << nInteractionFrame << G4endl;
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G4cout << " GammaDirection0 = " << gamDirection0 << G4endl;
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G4cout << " gammaPolarization = " << fBeamPolarization << G4endl;
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G4cout << " electronPolarization = " << fTargetPolarization << G4endl;
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}
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fBeamPolarization.InvRotateAz(nInteractionFrame, gamDirection0);
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fTargetPolarization.InvRotateAz(nInteractionFrame, gamDirection0);
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if(fVerboseLevel >= 1)
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{
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G4cout << "----------------------------------------" << G4endl;
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G4cout << " gammaPolarization = " << fBeamPolarization << G4endl;
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G4cout << " electronPolarization = " << fTargetPolarization << G4endl;
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G4cout << "----------------------------------------" << G4endl;
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}
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// initialize the polarization transfer matrix
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fCrossSectionCalculator->Initialize(epsilon, E0_m, 0., fBeamPolarization,
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fTargetPolarization, 2);
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if(gamEnergy1 > lowestSecondaryEnergy)
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{
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// in interaction frame
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// calculate polarization transfer to the photon (in interaction plane)
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fFinalGammaPolarization = fCrossSectionCalculator->GetPol2();
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if(fVerboseLevel >= 1)
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{
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G4cout << " gammaPolarization1 = " << fFinalGammaPolarization << G4endl;
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}
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fFinalGammaPolarization.SetPhoton();
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// translate polarization into particle reference frame
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fFinalGammaPolarization.RotateAz(nInteractionFrame, gamDirection1);
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if(fFinalGammaPolarization.mag() > 1. + 1.e-8)
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{
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G4ExceptionDescription ed;
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ed << "ERROR in Polarizaed Compton Scattering !\n";
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ed << "Polarization of final photon more than 100%.\n";
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ed << fFinalGammaPolarization
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<< " mag = " << fFinalGammaPolarization.mag() << "\n";
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G4Exception("G4PolarizedComptonModel::SampleSecondaries", "pol033",
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FatalException, ed);
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}
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// store polarization vector
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fParticleChange->ProposePolarization(fFinalGammaPolarization);
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if(fVerboseLevel >= 1)
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{
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G4cout << " gammaPolarization1 = " << fFinalGammaPolarization << G4endl;
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G4cout << " GammaDirection1 = " << gamDirection1 << G4endl;
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}
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}
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// kinematic of the scattered electron
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G4double eKinEnergy = gamEnergy0 - gamEnergy1;
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if(eKinEnergy > lowestSecondaryEnergy)
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{
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G4ThreeVector eDirection =
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gamEnergy0 * gamDirection0 - gamEnergy1 * gamDirection1;
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eDirection = eDirection.unit();
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finalElectronPolarization = fCrossSectionCalculator->GetPol3();
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if(fVerboseLevel >= 1)
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{
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G4cout << " electronPolarization1 = " << finalElectronPolarization
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<< G4endl;
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}
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// transfer into particle reference frame
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finalElectronPolarization.RotateAz(nInteractionFrame, eDirection);
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if(fVerboseLevel >= 1)
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{
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G4cout << " electronPolarization1 = " << finalElectronPolarization
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<< G4endl << " ElecDirection = " << eDirection << G4endl;
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}
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// create G4DynamicParticle object for the electron.
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G4DynamicParticle* aElectron =
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new G4DynamicParticle(theElectron, eDirection, eKinEnergy);
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// store polarization vector
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if(finalElectronPolarization.mag() > 1. + 1.e-8)
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{
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G4ExceptionDescription ed;
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ed << "ERROR in Polarized Compton Scattering !\n";
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ed << "Polarization of final electron more than 100%.\n";
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ed << finalElectronPolarization
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<< " mag = " << finalElectronPolarization.mag() << G4endl;
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G4Exception("G4PolarizedComptonModel::SampleSecondaries", "pol034",
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FatalException, ed);
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}
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aElectron->SetPolarization(finalElectronPolarization.p1(),
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finalElectronPolarization.p2(),
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finalElectronPolarization.p3());
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fvect->push_back(aElectron);
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}
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else
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{
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edep += eKinEnergy;
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}
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// energy balance
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if(edep > 0.0)
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{
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fParticleChange->ProposeLocalEnergyDeposit(edep);
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}
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}
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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void G4PolarizedComptonModel::PrintWarning(const G4DynamicParticle* dp,
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G4int nloop, G4double grej,
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G4double onecos, G4double phi,
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const G4String sss) const
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{
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G4ExceptionDescription ed;
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ed << "Problem of scattering sampling: " << sss << "\n"
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<< "Niter= " << nloop << " grej= " << grej
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<< " cos(theta)= " << 1.0 - onecos << " phi= " << phi << "\n"
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<< "Gamma E(MeV)= " << dp->GetKineticEnergy() / MeV
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<< " dir= " << dp->GetMomentumDirection()
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<< " pol= " << dp->GetPolarization();
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G4Exception("G4PolarizedComptonModel::SampleSecondaries", "em0044",
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JustWarning, ed, "");
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}
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