G4LivermoreBremsstrahlungModel.cc File Reference

#include "G4LivermoreBremsstrahlungModel.hh"
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
#include "G4Electron.hh"
#include "G4Positron.hh"
#include "G4Gamma.hh"
#include "Randomize.hh"
#include "G4Material.hh"
#include "G4Element.hh"
#include "G4ElementVector.hh"
#include "G4ProductionCutsTable.hh"
#include "G4ParticleChangeForLoss.hh"
#include "G4Generator2BS.hh"
#include "G4Physics2DVector.hh"
#include "G4Exp.hh"
#include "G4Log.hh"
#include "G4ios.hh"
#include <fstream>
#include <iomanip>
#include "G4AutoLock.hh"

Include dependency graph for G4LivermoreBremsstrahlungModel.cc:

Go to the source code of this file.

Variables
static const G4double	emaxlog = 4*G4Log(10.)
static const G4double	alpha = CLHEP::twopi*CLHEP::fine_structure_const
static const G4double	epeaklimit = 300*CLHEP::MeV
static const G4double	elowlimit = 20*CLHEP::keV

Variable Documentation

const G4double alpha = CLHEP::twopi*CLHEP::fine_structure_const

static

Definition at line 78 of file G4LivermoreBremsstrahlungModel.cc.

View newest version in sPHENIX GitHub at line 78 of file G4LivermoreBremsstrahlungModel.cc

Referenced by HadrontherapyRBE::AddAlphaNumerator(), ALICEKF::ALICEKalmanFilter(), G4INCL::Particle::boost(), Acts::Test::Layers::BOOST_AUTO_TEST_CASE(), Acts::Test::BOOST_AUTO_TEST_CASE(), Acts::Test::BOOST_DATA_TEST_CASE(), G4ViewParameters::CatmullRomCubicSplineInterpolation(), G4RadioactiveDecayBase::CollimateDecay(), G4RadioactiveDecay::CollimateDecay(), G4XrayRayleighModel::ComputeCrossSectionPerAtom(), G4LivermoreBremsstrahlungModel::ComputeDXSectionPerAtom(), Acts::ConeBounds::ConeBounds(), PHInitZVertexing::convertHelixCovarianceToEuclideanCovariance(), PHPatternReco::convertHelixCovarianceToEuclideanCovariance(), PHHoughSeeding::convertHelixCovarianceToEuclideanCovariance(), G4INCL::CoulombNonRelativistic::coulombDeviation(), MuCrossSections::CRB_Mephi(), G4Para::CreatePolyhedron(), MuCrossSections::CRK_Mephi(), MuCrossSections::CRN_Mephi(), MuCrossSections::CRP_Mephi(), G4VFieldModel::DescribeYourselfTo(), G4OpBoundaryProcess::DielectricDielectric(), G4ScreenedCoulombClassicalKinematics::DoScreeningComputation(), ECCEStyle(), G4GaussJacobiQ::G4GaussJacobiQ(), G4GaussLaguerreQ::G4GaussLaguerreQ(), PrimaryGeneratorAction1::GeneratePrimaries(), XrayFluoMercuryPrimaryGeneratorAction::GeneratePrimaries(), PrimaryGenerator::GeneratePrimaryVertex(), G4OpBoundaryProcess::GetFacetNormal(), ECCEhpDIRCFastPIDMap::getFastSmearLogLikelihood(), HadrontherapyRBE::GetHitAlphaAndBeta(), DrcPidFast::GetInfo(), PHG4HcalDetector::GetLength(), G4RTRun::GetMixedColour(), G4TheRayTracer::GetMixedColour(), mRICH::getNgamma(), G4Hype::GetPointOnSurface(), G4ParticleHPMadlandNixSpectrum::GIntegral(), QAG4Util::interpolate(), G4ErrorSymMatrix::invertBunchKaufman(), FitNewton::NewtonMinimizerGradHessian::lineSearch(), mRICH::mRICH(), G4GDMLWriteParamvol::Para_dimensionsWrite(), PHG4GDMLWriteParamvol::Para_dimensionsWrite(), G4GDMLReadSolids::ParaRead(), PHG4GDMLWriteSolids::ParaWrite(), G4GDMLWriteSolids::ParaWrite(), PHSimpleKFProp::PropagateTrack(), pyboei(), pyfeyn(), pyhggm(), pymael(), pyprep(), pyptfs(), pyrghm(), pyshow(), pystbh(), pytbhb(), pytbhg(), pytbhq(), Acts::detail::RealQuadraticEquation::RealQuadraticEquation(), G4XrayRayleighModel::SampleSecondaries(), G4DiffuseElasticV2::SampleTableT(), G4NuclNuclDiffuseElastic::SampleTableT(), G4DiffuseElastic::SampleTableT(), PHG4ConeSubsystem::set_color(), PHG4BlockSubsystem::set_color(), PHG4CylinderSubsystem::set_color(), SubtractTowersCS::SetAlpha(), HadrontherapyRBE::SetAlphaNumerator(), G4ModelCmdApplyStringColour< M >::SetNewValue(), RMC01AnalysisManagerMessenger::SetNewValue(), G4ModelCmdApplyColour< M >::SetNewValue(), RMC01AnalysisManager::SetPrimaryPowerLawSpectrumForAdjointSim(), PHG4HcalSubsystem::SetTiltViaNcross(), sPhenixStyle(), G4Para::StreamInfo(), Acts::TrapezoidVolumeBounds::TrapezoidVolumeBounds(), G4Abla::umass(), and FitNewton::NewtonMinimizerGradHessian::zoom().

const G4double elowlimit = 20*CLHEP::keV

static

Definition at line 80 of file G4LivermoreBremsstrahlungModel.cc.

View newest version in sPHENIX GitHub at line 80 of file G4LivermoreBremsstrahlungModel.cc

Referenced by G4LivermoreBremsstrahlungModel::SampleSecondaries().

const G4double emaxlog = 4*G4Log(10.)

static

Definition at line 77 of file G4LivermoreBremsstrahlungModel.cc.

View newest version in sPHENIX GitHub at line 77 of file G4LivermoreBremsstrahlungModel.cc

Referenced by G4LivermoreBremsstrahlungModel::ReadData(), and G4SeltzerBergerModel::ReadData().

const G4double epeaklimit = 300*CLHEP::MeV

static

Definition at line 79 of file G4LivermoreBremsstrahlungModel.cc.

View newest version in sPHENIX GitHub at line 79 of file G4LivermoreBremsstrahlungModel.cc

Referenced by G4LivermoreBremsstrahlungModel::SampleSecondaries().