Geant4-11
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# ================================================================== # Python module # # This module defines physical units and constants used in HEP, # which are imported from CLHEP library. # # Q, 2005 # ==================================================================
int source.hepunit.alpha_rcl2 = fine_structure_const * classic_electr_radius \ |
Definition at line 291 of file hepunit.py.
Referenced by G4eplusTo2GammaOKVIModel.ComputeCrossSectionPerElectron(), G4eplusTo3GammaOKVIModel.ComputeCrossSectionPerElectron(), and G4Element.ComputeLradTsaiFactor().
Definition at line 155 of file hepunit.py.
Definition at line 277 of file hepunit.py.
Referenced by G4Material.ComputeNuclearInterLength(), G4BraggIonModel.DEDX(), G4BraggModel.DEDX(), G4Abla.DeexcitationAblaxx(), and G4SandiaTable.GetSandiaCofPerAtom().
float source.hepunit.amu_c2 = 931.49432 * MeV |
Definition at line 276 of file hepunit.py.
Referenced by G4NistElementBuilder.AddElement(), G4NucleiProperties.AtomicMass(), G4NistElementBuilder.BuildElement(), G4ecpssrBaseKxsModel.CalculateCrossSection(), G4ecpssrBaseLixsModel.CalculateL1CrossSection(), G4ecpssrBaseLixsModel.CalculateL2CrossSection(), G4ecpssrBaseLixsModel.CalculateL3CrossSection(), G4IonChuFluctuationModel.ChuFluctuationModel(), G4IonCoulombScatteringModel.ComputeCrossSectionPerAtom(), G4hCoulombScatteringModel.ComputeCrossSectionPerAtom(), G4WentzelVIRelModel.ComputeCrossSectionPerAtom(), G4ICRU49NuclearStoppingModel.ComputeDEDXPerVolume(), G4EmCorrections.EffectiveChargeCorrection(), G4NucleiPropertiesTableAME12.GetAtomicMass(), G4NucleiPropertiesTheoreticalTable.GetAtomicMass(), G4EMDissociationSpectrum.GetClosestApproach(), G4EMDissociationCrossSection.GetCrossSectionForProjectile(), G4NistElementBuilder.Initialise(), G4NucleiProperties.MassExcess(), G4ParticleHPContAngularPar.Sample(), and G4IonYangFluctuationModel.YangFluctuationModel().
int source.hepunit.angstrom = 1.e-10*meter |
Definition at line 35 of file hepunit.py.
int source.hepunit.atmosphere = 101325*pascal |
Definition at line 150 of file hepunit.py.
float source.hepunit.Avogadro = 6.0221367e+23/mole |
Definition at line 252 of file hepunit.py.
Referenced by G4Material.AddElementByNumberOfAtoms(), G4Material.ComputeDerivedQuantities(), G4EmDNAChemistry.ConstructMolecule(), G4EmDNAChemistry_option1.ConstructMolecule(), G4EmDNAChemistry_option3.ConstructMolecule(), G4EmDNAChemistry_option2.ConstructMolecule(), G4AtimaEnergyLossModel.dedx_n(), G4DamagedDeoxyribose.Definition(), G4DamagedAdenine.Definition(), G4DamagedGuanine.Definition(), G4DamagedThymine.Definition(), G4DamagedCytosine.Definition(), G4Deoxyribose.Definition(), G4Phosphate.Definition(), G4Adenine.Definition(), G4Guanine.Definition(), G4Thymine.Definition(), G4Cytosine.Definition(), G4ModifiedHistone.Definition(), G4Histone.Definition(), G4Electron_aq.Definition(), G4FakeMolecule.Definition(), G4H2.Definition(), G4H2O.Definition(), G4H2O2.Definition(), G4H3O.Definition(), G4HO2.Definition(), G4Hydrogen.Definition(), G4O2.Definition(), G4O3.Definition(), G4OH.Definition(), G4Oxygen.Definition(), G4DNAScavengerMaterial.Dump(), G4DNAGillespieDirectMethod.FindScavenging(), G4DNAPartiallyDiffusionControlled.GeminateRecombinationProbability(), G4DNAIRT.GetIndependentReactionTime(), G4DNAIRT_geometries.GetIndependentReactionTime(), G4DiffusionControlledReactionModel.GetReactionRadius(), G4DNAPartiallyDiffusionControlled.GetTimeToEncounter(), G4DNATotallyDiffusionControlled.GetTimeToEncounter(), G4DNAScavengerProcess.PostStepGetPhysicalInteractionLength(), G4DNAScavengerMaterial.PrintInfo(), G4DNAGillespieDirectMethod.PropensityFunction(), G4DNAScavengerMaterial.Reset(), G4DNAMolecularReactionData.SetReactionType(), and G4AtimaEnergyLossModel.sezi_p_se().
int source.hepunit.bar = 100000*pascal |
Definition at line 149 of file hepunit.py.
int source.hepunit.barn = 1.e-28*meter2 |
Definition at line 38 of file hepunit.py.
int source.hepunit.becquerel = 1./second |
Definition at line 212 of file hepunit.py.
float source.hepunit.Bohr_radius = electron_Compton_length/fine_structure_const |
Definition at line 289 of file hepunit.py.
Referenced by G4MicroElecInelasticModel_new.BKZ(), G4PenelopeOscillatorManager.BuildOscillatorTable(), G4AntiNuclElastic.CalculateAm(), G4ecpssrBaseKxsModel.CalculateCrossSection(), G4ecpssrBaseLixsModel.CalculateL1CrossSection(), G4ecpssrBaseLixsModel.CalculateL2CrossSection(), G4ecpssrBaseLixsModel.CalculateL3CrossSection(), G4XrayRayleighModel.ComputeCrossSectionPerAtom(), G4DNADingfelderChargeIncreaseModel.CrossSectionPerVolume(), G4DNARuddIonisationModel.DifferentialCrossSection(), G4LowEPComptonModel.SampleSecondaries(), G4LowEPPolarizedComptonModel.SampleSecondaries(), and G4XrayRayleighModel.SampleSecondaries().
Definition at line 256 of file hepunit.py.
Referenced by G4MagHelicalStepper.AdvanceHelix(), G4ErrorSurfaceTrajState.BuildErrorMatrix(), G4hRDEnergyLoss.BuildLabTimeVector(), G4hRDEnergyLoss.BuildProperTimeVector(), G4MaterialPropertiesTable.CalculateGROUPVEL(), G4VLongitudinalStringDecay.CalculateHadronTimePosition(), G4PenelopeRayleighModelMI.CalculateQSquared(), G4OpRayleigh.CalculateRayleighMeanFreePaths(), G4Track.CalculateVelocityForOpticalPhoton(), G4ParticleChange.CheckIt(), G4MicroElecInelasticModel_new.ComputeRelativistVelocity(), G4OpBoundaryProcess.DielectricDichroic(), G4OpBoundaryProcess.DielectricDielectric(), G4OpenGLStoredViewer.DrawDisplayLists(), G4ParticleChange.DumpInfo(), G4QAOLowEnergyLoss.EnergyLoss(), G4KM_NucleonEqRhs.EvaluateRhsGivenB(), G4KM_OpticalEqRhs.EvaluateRhsGivenB(), G4EqEMFieldWithEDM.EvaluateRhsGivenB(), G4EqEMFieldWithSpin.EvaluateRhsGivenB(), G4EqGravityField.EvaluateRhsGivenB(), G4EqMagElectricField.EvaluateRhsGivenB(), G4MonopoleEq.EvaluateRhsGivenB(), G4RepleteEofM.EvaluateRhsGivenB(), G4RKPropagation.FieldTransport(), G4RKPropagation.FreeTransport(), G4ErrorFreeTrajState.G4ErrorFreeTrajState(), G4RayleighAngularGenerator.G4RayleighAngularGenerator(), G4MuonicAtomDecay.GetMeanFreePath(), G4Decay.GetMeanFreePath(), G4RadioactiveDecay.GetMeanFreePath(), G4SynchrotronRadiation.GetMeanFreePath(), G4SynchrotronRadiation.GetRandomEnergySR(), G4RKPropagation.GetSphereIntersectionTimes(), G4MesonAbsorption.GetTimeToAbsorption(), G4Scatterer.GetTimeToInteraction(), field_utils.inverseCurvatureRadius(), G4hRDEnergyLoss.LabTimeIntLog(), G4LundStringFragmentation.Loop_toFragmentString(), G4UCNBoundaryProcess.PostStepDoIt(), G4VXTRenergyLoss.PostStepDoIt(), G4MaxTimeCuts.PostStepGetPhysicalInteractionLength(), G4UserSpecialCuts.PostStepGetPhysicalInteractionLength(), G4Decay.PostStepGetPhysicalInteractionLength(), G4VelocityTable.PrepareVelocityTable(), G4hRDEnergyLoss.ProperTimeIntLog(), G4LivermoreComptonModel.SampleSecondaries(), G4LivermorePolarizedComptonModel.SampleSecondaries(), G4LowEPComptonModel.SampleSecondaries(), G4LowEPPolarizedComptonModel.SampleSecondaries(), G4EqEMFieldWithEDM.SetChargeMomentumMass(), G4EqEMFieldWithSpin.SetChargeMomentumMass(), G4EqMagElectricField.SetChargeMomentumMass(), G4Mag_EqRhs.SetChargeMomentumMass(), G4Mag_SpinEqRhs.SetChargeMomentumMass(), and G4RepleteEofM.SetChargeMomentumMass().
Definition at line 257 of file hepunit.py.
Referenced by G4MicroElecInelasticModel_new.BKZ(), G4EmDNAChemistry.ConstructMolecule(), G4EmDNAChemistry_option1.ConstructMolecule(), G4EmDNAChemistry_option3.ConstructMolecule(), G4EmDNAChemistry_option2.ConstructMolecule(), G4MicroElecInelasticModel_new.CrossSectionPerVolume(), G4AdjointhIonisationModel.DefineProjectileProperty(), G4AdjointIonIonisationModel.DefineProjectileProperty(), G4AdjointDeuteron.Definition(), G4AdjointElectron.Definition(), G4AdjointElectronFI.Definition(), G4AdjointHe3.Definition(), G4AdjointPositron.Definition(), G4AdjointProton.Definition(), G4AdjointTriton.Definition(), G4AntiLambda.Definition(), G4AntiNeutron.Definition(), G4AntiOmegaMinus.Definition(), G4AntiProton.Definition(), G4AntiSigmaMinus.Definition(), G4AntiSigmaPlus.Definition(), G4AntiXiMinus.Definition(), G4AntiXiZero.Definition(), G4Lambda.Definition(), G4Neutron.Definition(), G4OmegaMinus.Definition(), G4Proton.Definition(), G4SigmaMinus.Definition(), G4SigmaPlus.Definition(), G4XiMinus.Definition(), G4XiZero.Definition(), G4AntiDeuteron.Definition(), G4AntiDoubleHyperDoubleNeutron.Definition(), G4AntiDoubleHyperH4.Definition(), G4AntiHe3.Definition(), G4AntiHyperAlpha.Definition(), G4AntiHyperH4.Definition(), G4AntiHyperHe5.Definition(), G4AntiHyperTriton.Definition(), G4AntiTriton.Definition(), G4Deuteron.Definition(), G4DoubleHyperDoubleNeutron.Definition(), G4DoubleHyperH4.Definition(), G4He3.Definition(), G4HyperAlpha.Definition(), G4HyperH4.Definition(), G4HyperHe5.Definition(), G4HyperTriton.Definition(), G4Triton.Definition(), G4Electron.Definition(), G4MuonMinus.Definition(), G4MuonPlus.Definition(), G4Positron.Definition(), G4TauMinus.Definition(), G4TauPlus.Definition(), G4DamagedDeoxyribose.Definition(), G4DamagedAdenine.Definition(), G4DamagedGuanine.Definition(), G4DamagedThymine.Definition(), G4DamagedCytosine.Definition(), G4Deoxyribose.Definition(), G4Phosphate.Definition(), G4Adenine.Definition(), G4Guanine.Definition(), G4Thymine.Definition(), G4Cytosine.Definition(), G4ModifiedHistone.Definition(), G4Histone.Definition(), G4Electron_aq.Definition(), G4FakeMolecule.Definition(), G4H2.Definition(), G4H2O.Definition(), G4H2O2.Definition(), G4H3O.Definition(), G4HO2.Definition(), G4Hydrogen.Definition(), G4O2.Definition(), G4O3.Definition(), G4OH.Definition(), G4Oxygen.Definition(), G4ParticleChange.DumpInfo(), G4QAOLowEnergyLoss.EnergyLoss(), G4Molecule.GetDiffusionVelocity(), G4Molecule.GetKineticEnergy(), G4UCNBoundaryProcess.Loss(), G4UCNBoundaryProcess.MRreflectHigh(), G4MicroElecInelasticModel_new.RandomizeEjectedElectronEnergy(), G4MicroElecInelasticModel_new.RandomSelect(), G4LowEPComptonModel.SampleSecondaries(), G4LowEPPolarizedComptonModel.SampleSecondaries(), G4EqEMFieldWithEDM.SetChargeMomentumMass(), G4EqEMFieldWithSpin.SetChargeMomentumMass(), G4Mag_SpinEqRhs.SetChargeMomentumMass(), G4RepleteEofM.SetChargeMomentumMass(), and G4AtimaEnergyLossModel.SetupParameters().
int source.hepunit.candela = 1. |
Definition at line 223 of file hepunit.py.
int source.hepunit.centimeter = 10.*millimeter |
Definition at line 19 of file hepunit.py.
int source.hepunit.centimeter2 = centimeter*centimeter |
Definition at line 20 of file hepunit.py.
int source.hepunit.centimeter3 = centimeter*centimeter*centimeter |
Definition at line 21 of file hepunit.py.
int source.hepunit.classic_electr_radius = elm_coupling/electron_mass_c2 |
Definition at line 287 of file hepunit.py.
Referenced by G4PenelopeBremsstrahlungFS.BuildScaledXSTable(), G4eplusTo2GammaOKVIModel.ComputeCrossSectionPerElectron(), G4PenelopeIonisationXSHandler.ComputeShellCrossSectionsElectron(), G4PenelopeIonisationXSHandler.ComputeShellCrossSectionsPositron(), G4PenelopeRayleighModelMI.CrossSectionPerVolume(), G4PenelopeComptonModel.CrossSectionPerVolume(), G4IonCoulombCrossSection.G4IonCoulombCrossSection(), G4PenelopeAnnihilationModel.G4PenelopeAnnihilationModel(), G4PolarizedIonisationBhabhaXS.Initialize(), G4PolarizedIonisationMollerXS.Initialize(), G4ScreeningMottCrossSection.NuclearCrossSection(), G4PolarizedIonisationModel.SampleSecondaries(), G4PolarizedIonisationBhabhaXS.TotalXSection(), and G4PolarizedIonisationMollerXS.TotalXSection().
int source.hepunit.cm = centimeter |
Definition at line 49 of file hepunit.py.
int source.hepunit.cm2 = centimeter2 |
Definition at line 50 of file hepunit.py.
int source.hepunit.cm3 = centimeter3 |
Definition at line 51 of file hepunit.py.
Definition at line 101 of file hepunit.py.
float source.hepunit.curie = 3.7e+10 * becquerel |
Definition at line 213 of file hepunit.py.
tuple source.hepunit.deg = degree |
Definition at line 76 of file hepunit.py.
tuple source.hepunit.degree = (3.14159265358979323846/180.0)*radian |
Definition at line 68 of file hepunit.py.
float source.hepunit.e_SI = 1.60217733e-19 |
Definition at line 100 of file hepunit.py.
Definition at line 269 of file hepunit.py.
Referenced by G4DNAScreenedRutherfordElasticModel.RutherfordCrossSection(), and G4DNAUeharaScreenedRutherfordElasticModel.RutherfordCrossSection().
int source.hepunit.electron_charge = - eplus |
Definition at line 268 of file hepunit.py.
float source.hepunit.electron_Compton_length = hbarc/electron_mass_c2 |
Definition at line 288 of file hepunit.py.
Referenced by G4mplIonisationModel.Initialise(), and G4mplIonisationWithDeltaModel.Initialise().
float source.hepunit.electron_mass_c2 = 0.51099906 * MeV |
Definition at line 273 of file hepunit.py.
Referenced by G4NistElementBuilder.AddElement(), G4AdjointComptonModel.AdjointCrossSection(), G4NeutrinoElectronNcModel.ApplyYourself(), G4NeutronElectronElModel.ApplyYourself(), G4NeutrinoElectronCcModel.ApplyYourself(), G4EmCaptureCascade.ApplyYourself(), G4MuonMinusBoundDecay.ApplyYourself(), G4eIonisationSpectrum.AverageEnergy(), G4EmCorrections.Bethe(), G4hBetheBlochModel.BetheBlochFormula(), G4MicroElecInelasticModel_new.BKZ(), G4PenelopeIonisationXSHandler.BuildDeltaTable(), G4PenelopeBremsstrahlungFS.BuildScaledXSTable(), G4PenelopeBremsstrahlungModel.BuildXSTable(), G4ecpssrBaseKxsModel.CalculateCrossSection(), G4Generator2BN.Calculatedsdkdt(), G4ecpssrBaseLixsModel.CalculateL1CrossSection(), G4OrlicLiXsModel.CalculateL2CrossSection(), G4ecpssrBaseLixsModel.CalculateL2CrossSection(), G4OrlicLiXsModel.CalculateL3CrossSection(), G4ecpssrBaseLixsModel.CalculateL3CrossSection(), G4PenelopeRayleighModelMI.CalculateQSquared(), G4ecpssrBaseLixsModel.CalculateVelocity(), G4PolarizedAnnihilationModel.ComputeAsymmetriesPerElectron(), G4PolarizedComptonModel.ComputeAsymmetryPerAtom(), G4eeToHadronsModel.ComputeCMCrossSectionPerElectron(), G4KleinNishinaCompton.ComputeCrossSectionPerAtom(), G4KleinNishinaModel.ComputeCrossSectionPerAtom(), G4PairProductionRelModel.ComputeCrossSectionPerAtom(), G4UrbanAdjointMscModel.ComputeCrossSectionPerAtom(), G4GammaConversionToMuons.ComputeCrossSectionPerAtom(), G4PolarizedIonisationModel.ComputeCrossSectionPerElectron(), G4MuBetheBlochModel.ComputeCrossSectionPerElectron(), G4MollerBhabhaModel.ComputeCrossSectionPerElectron(), G4PenelopeAnnihilationModel.ComputeCrossSectionPerElectron(), G4eeToTwoGammaModel.ComputeCrossSectionPerElectron(), G4eplusTo2GammaOKVIModel.ComputeCrossSectionPerElectron(), G4eplusTo3GammaOKVIModel.ComputeCrossSectionPerElectron(), G4mplIonisationModel.ComputeDEDXAhlen(), G4mplIonisationWithDeltaModel.ComputeDEDXAhlen(), G4MuBetheBlochModel.ComputeDEDXPerVolume(), G4MollerBhabhaModel.ComputeDEDXPerVolume(), G4MuBremsstrahlungModel.ComputeDMicroscopicCrossSection(), G4hBremsstrahlungModel.ComputeDMicroscopicCrossSection(), G4MuPairProductionModel.ComputeDMicroscopicCrossSection(), G4TablesForExtrapolator.ComputeElectronDEDX(), G4eplusTo3GammaOKVIModel.ComputeF(), G4eplusTo3GammaOKVIModel.ComputeFS(), G4WentzelOKandVIxSection.ComputeMaxElectronScattering(), G4eBremParametrizedModel.ComputeParametrizedDXSectionPerAtom(), G4PenelopeIonisationXSHandler.ComputeShellCrossSectionsElectron(), G4PenelopeIonisationXSHandler.ComputeShellCrossSectionsPositron(), G4Generator2BN.ConstructMajorantSurface(), G4GoudsmitSaundersonMscModel.CrossSectionPerVolume(), G4DNADingfelderChargeIncreaseModel.CrossSectionPerVolume(), G4AdjointhIonisationModel.DefineProjectileProperty(), G4AdjointIonIonisationModel.DefineProjectileProperty(), G4AdjointElectron.Definition(), G4AdjointElectronFI.Definition(), G4AdjointPositron.Definition(), G4Electron.Definition(), G4Positron.Definition(), G4hImpactIonisation.DeltaRaysEnergy(), G4AdjointeIonisationModel.DiffCrossSectionMoller(), G4AdjointComptonModel.DiffCrossSectionPerAtomPrimToScatPrim(), G4AdjointhIonisationModel.DiffCrossSectionPerAtomPrimToSecond(), G4AdjointIonIonisationModel.DiffCrossSectionPerAtomPrimToSecond(), G4PenelopeComptonModel.DifferentialCrossSection(), G4DNARuddIonisationModel.DifferentialCrossSection(), G4InitXscPAI.DifPAIxSection(), G4PAIxSection.DifPAIxSection(), G4PAIySection.DifPAIySection(), G4hImpactIonisation.ElectronicLossFluctuation(), G4QAOLowEnergyLoss.EnergyLoss(), G4NeutrinoNucleusModel.FinalBarion(), G4ANuElNucleusCcModel.G4ANuElNucleusCcModel(), G4BoldyshevTripletModel.G4BoldyshevTripletModel(), G4DNAGenericIonsManager.G4DNAGenericIonsManager(), G4GoudsmitSaundersonMscModel.G4GoudsmitSaundersonMscModel(), G4IonCoulombCrossSection.G4IonCoulombCrossSection(), G4IonisParamElm.G4IonisParamElm(), G4LivermoreNuclearGammaConversionModel.G4LivermoreNuclearGammaConversionModel(), G4LivermorePolarizedGammaConversionModel.G4LivermorePolarizedGammaConversionModel(), G4mplIonisationWithDeltaModel.G4mplIonisationWithDeltaModel(), G4NeutrinoElectronCcXsc.G4NeutrinoElectronCcXsc(), G4NeutrinoElectronNcXsc.G4NeutrinoElectronNcXsc(), G4NeutronElectronElModel.G4NeutronElectronElModel(), G4NeutronElectronElXsc.G4NeutronElectronElXsc(), G4NuElNucleusCcModel.G4NuElNucleusCcModel(), G4PenelopeGammaConversionModel.G4PenelopeGammaConversionModel(), G4PolarizedGammaConversion.G4PolarizedGammaConversion(), G4eeToHadronsModel.GenerateCMPhoton(), G4HyperNucleiProperties.GetAtomicMass(), G4VXTRenergyLoss.GetComptonPerAtom(), G4NeutrinoElectronCcXsc.GetElementCrossSection(), G4NeutrinoElectronNcXsc.GetElementCrossSection(), G4NucleiPropertiesTableAME12.GetNuclearMass(), G4NucleiPropertiesTheoreticalTable.GetNuclearMass(), G4PenelopeRayleighModel.GetPMaxTable(), G4PenelopeRayleighModelMI.GetPMaxTable(), G4PenelopeBremsstrahlungModel.GetPositronXSCorrection(), G4AdjointComptonModel.GetSecondAdjEnergyMaxForScatProjToProj(), G4AdjointComptonModel.GetSecondAdjEnergyMinForProdToProj(), G4GoudsmitSaundersonMscModel.GetTransportMeanFreePath(), G4GoudsmitSaundersonMscModel.GetTransportMeanFreePathOnly(), G4NistElementBuilder.Initialise(), G4BoldyshevTripletModel.Initialise(), G4eBremsstrahlungRelModel.InitialiseElementData(), G4hhIonisation.InitialiseEnergyLossProcess(), G4hIonisation.InitialiseEnergyLossProcess(), G4PolarizedGammaConversion.InitialiseProcess(), G4PolarizedBremsstrahlungXS.Initialize(), G4NeutrinoElectronNcModel.IsApplicable(), G4NeutrinoElectronCcModel.IsApplicable(), G4NeutrinoElectronCcXsc.IsElementApplicable(), G4NeutrinoElectronNcXsc.IsElementApplicable(), G4PenelopeComptonModel.KleinNishinaCrossSection(), G4BraggIonModel.MaxSecondaryEnergy(), G4BraggModel.MaxSecondaryEnergy(), G4ICRU73QOModel.MaxSecondaryEnergy(), G4PAIModel.MaxSecondaryEnergy(), G4PAIPhotModel.MaxSecondaryEnergy(), G4mplIonisationWithDeltaModel.MaxSecondaryEnergy(), G4MuBetheBlochModel.MaxSecondaryEnergy(), G4AtimaEnergyLossModel.MaxSecondaryEnergy(), G4IonParametrisedLossModel.MaxSecondaryEnergy(), G4hImpactIonisation.MicroscopicCrossSection(), G4PixeCrossSectionHandler.MicroscopicCrossSection(), G4mplIonisation.MinPrimaryEnergy(), G4hIonisation.MinPrimaryEnergy(), G4hhIonisation.MinPrimaryEnergy(), G4eeToHadronsMultiModel.ModelDescription(), G4InitXscPAI.Normalisation(), G4PAIxSection.NormShift(), G4PAIySection.NormShift(), G4ScreeningMottCrossSection.NuclearCrossSection(), G4NucleiProperties.NuclearMass(), G4InitXscPAI.PAIdNdxPlasmon(), G4PAIxSection.PAIdNdxPlasmon(), G4PAIySection.PAIdNdxPlasmon(), G4PAIxSection.PAIdNdxResonance(), G4VEmProcess.PostStepDoIt(), G4GammaConversionToMuons.PostStepDoIt(), G4hImpactIonisation.PostStepDoIt(), G4PenelopeBremsstrahlungAngular.PrepareTables(), G4eIonisationSpectrum.Probability(), G4DNARuddIonisationExtendedModel.ProposedSampledEnergy(), G4DNACPA100IonisationModel.RandomizeEjectedElectronDirection(), G4DNAPTBIonisationModel.RandomizeEjectedElectronDirection(), G4MicroElecInelasticModel_new.RandomizeEjectedElectronEnergy(), G4DNABornIonisationModel1.RandomizeEjectedElectronEnergy(), G4DNABornIonisationModel2.RandomizeEjectedElectronEnergy(), G4MicroElecInelasticModel.RandomizeEjectedElectronEnergy(), G4DNAPTBIonisationModel.RandomizeEjectedElectronEnergy(), G4DNARuddIonisationModel.RandomizeEjectedElectronEnergy(), G4AdjointComptonModel.RapidSampleSecondaries(), G4DNARuddIonisationExtendedModel.RejectionFunction(), G4DNAScreenedRutherfordElasticModel.RutherfordCrossSection(), G4DNAUeharaScreenedRutherfordElasticModel.RutherfordCrossSection(), G4NeutrinoElectronCcModel.SampleCosCMS(), G4SauterGavrilaAngularDistribution.SampleDirection(), G4PhotoElectricAngularGeneratorSauterGavrila.SampleDirection(), G4PhotoElectricAngularGeneratorPolarized.SampleDirection(), G4DeltaAngle.SampleDirection(), G4DeltaAngleFreeScat.SampleDirection(), G4Generator2BS.SampleDirection(), G4PenelopeBremsstrahlungAngular.SampleDirection(), G4DNABornAngle.SampleDirectionForShell(), G4DNARuddAngle.SampleDirectionForShell(), G4PenelopePhotoElectricModel.SampleElectronDirection(), G4NeutrinoElectronNcModel.SampleElectronTkin(), G4eIonisationSpectrum.SampleEnergy(), G4PenelopeIonisationModel.SampleFinalStateElectron(), G4PenelopeIonisationModel.SampleFinalStatePositron(), G4GoudsmitSaundersonMscModel.SampleMSC(), G4AdjointBremsstrahlungModel.SampleSecondaries(), G4AdjointComptonModel.SampleSecondaries(), G4AdjointPhotoElectricModel.SampleSecondaries(), G4LivermoreBremsstrahlungModel.SampleSecondaries(), G4eBremParametrizedModel.SampleSecondaries(), G4DNABornIonisationModel1.SampleSecondaries(), G4DNABornIonisationModel2.SampleSecondaries(), G4DNACPA100ExcitationModel.SampleSecondaries(), G4DNACPA100IonisationModel.SampleSecondaries(), G4DNADingfelderChargeDecreaseModel.SampleSecondaries(), G4DNADingfelderChargeIncreaseModel.SampleSecondaries(), G4DNAEmfietzoglouIonisationModel.SampleSecondaries(), G4BoldyshevTripletModel.SampleSecondaries(), G4PolarizedAnnihilationModel.SampleSecondaries(), G4mplIonisationWithDeltaModel.SampleSecondaries(), G4LivermoreComptonModel.SampleSecondaries(), G4LivermoreIonisationModel.SampleSecondaries(), G4LivermoreNuclearGammaConversionModel.SampleSecondaries(), G4LivermorePolarizedComptonModel.SampleSecondaries(), G4LivermorePolarizedGammaConversionModel.SampleSecondaries(), G4LowEPComptonModel.SampleSecondaries(), G4LowEPPolarizedComptonModel.SampleSecondaries(), G4MicroElecInelasticModel.SampleSecondaries(), G4MicroElecInelasticModel_new.SampleSecondaries(), G4PenelopeAnnihilationModel.SampleSecondaries(), G4PenelopeComptonModel.SampleSecondaries(), G4PenelopeGammaConversionModel.SampleSecondaries(), G4PenelopeRayleighModel.SampleSecondaries(), G4PenelopeRayleighModelMI.SampleSecondaries(), G4MuBetheBlochModel.SampleSecondaries(), G4PolarizedComptonModel.SampleSecondaries(), G4PolarizedIonisationModel.SampleSecondaries(), G4AtimaEnergyLossModel.SampleSecondaries(), G4BetheBlochModel.SampleSecondaries(), G4BraggIonModel.SampleSecondaries(), G4BraggModel.SampleSecondaries(), G4eeToTwoGammaModel.SampleSecondaries(), G4ICRU73QOModel.SampleSecondaries(), G4KleinNishinaCompton.SampleSecondaries(), G4KleinNishinaModel.SampleSecondaries(), G4LindhardSorensenIonModel.SampleSecondaries(), G4MollerBhabhaModel.SampleSecondaries(), G4eplusTo2GammaOKVIModel.SampleSecondaries(), G4eplusTo3GammaOKVIModel.SampleSecondaries(), G4eeToHadronsModel.SampleSecondaries(), G4DNAPTBIonisationModel.SampleSecondaries(), G4DNAScreenedRutherfordElasticModel.ScreeningFactor(), G4DNAUeharaScreenedRutherfordElasticModel.ScreeningFactor(), G4CollisionOutput.setOnShell(), G4AtimaEnergyLossModel.SetupParameters(), G4BetheBlochModel.SetupParameters(), G4MicroElecInelasticModel_new.TransferedEnergy(), and G4MicroElecInelasticModel.TransferedEnergy().
int source.hepunit.electronvolt = 1.e-6*megaelectronvolt |
Definition at line 107 of file hepunit.py.
Definition at line 285 of file hepunit.py.
Referenced by G4WilsonAbrasionModel.ApplyYourself(), G4MicroElecInelasticModel_new.BKZ(), G4StatMFMicroCanonical.CalcFreeInternalEnergy(), G4StatMFMicroPartition.CalcPartitionProbability(), G4StatMFMacroCanonical.CalculateTemperature(), G4StatMFMacroTemperature.FragsExcitEnergy(), G4EMDissociationSpectrum.GetClosestApproach(), G4StatMFMicroPartition.GetCoulombEnergy(), G4StatMFMicroPartition.GetPartitionEnergy(), G4StatMFMacroCanonical.Initialize(), G4StatMFMicroCanonical.Initialize(), and G4StatMFChannel.SolveEqOfMotion().
int source.hepunit.eplus = 1. |
Definition at line 99 of file hepunit.py.
Definition at line 282 of file hepunit.py.
Referenced by G4DNAMolecularReactionData.ComputeEffectiveRadius(), G4DNAScreenedRutherfordElasticModel.RutherfordCrossSection(), and G4DNAUeharaScreenedRutherfordElasticModel.RutherfordCrossSection().
int source.hepunit.eV = electronvolt |
Definition at line 117 of file hepunit.py.
Definition at line 175 of file hepunit.py.
int source.hepunit.fermi = 1.e-15*meter |
Definition at line 36 of file hepunit.py.
int source.hepunit.fine_structure_const = elm_coupling/hbarc |
Definition at line 286 of file hepunit.py.
Referenced by G4PenelopeOscillatorManager.BuildOscillatorTable(), G4PenelopeBremsstrahlungFS.BuildScaledXSTable(), G4ecpssrBaseKxsModel.CalculateCrossSection(), G4AntiNuclElastic.CalculateZommerfeld(), G4eeToHadronsModel.ComputeCMCrossSectionPerElectron(), G4Element.ComputeCoulombFactor(), G4GammaConversionToMuons.ComputeCrossSectionPerAtom(), G4KokoulinMuonNuclearXS.ComputeDDMicroscopicCrossSection(), G4HadronNucleonXsc.CoulombBarrier(), G4InitXscPAI.DifPAIxSection(), G4PAIxSection.DifPAIxSection(), G4PAIySection.DifPAIySection(), G4PhotoElectricAngularGeneratorPolarized.DSigmaKshellGavrila1959(), G4PhotoElectricAngularGeneratorPolarized.DSigmaL1shellGavrila(), G4QAOLowEnergyLoss.EnergyLoss(), G4MuonRadiativeDecayChannelWithSpin.fron(), G4BetaDecayCorrections.G4BetaDecayCorrections(), G4mplIonisationWithDeltaModel.G4mplIonisationWithDeltaModel(), G4NeutronElectronElXsc.G4NeutronElectronElXsc(), G4PAIySection.G4PAIySection(), G4eeToHadronsModel.GenerateCMPhoton(), G4EMDissociationSpectrum.GetGeneralE1Spectrum(), G4EMDissociationSpectrum.GetGeneralE2Spectrum(), G4SynchrotronRadiation.GetMeanFreePath(), G4MuonicAtomHelper.GetMuonDecayRate(), G4MuonMinusBoundDecay.GetMuonDecayRate(), G4eeCrossSections.Initialise(), G4mplIonisationModel.Initialise(), G4mplIonisationWithDeltaModel.Initialise(), G4PenelopeGammaConversionModel.InitializeScreeningFunctions(), G4EmCorrections.MottCorrection(), G4InitXscPAI.Normalisation(), G4PAIxSection.NormShift(), G4PAIySection.NormShift(), G4PAIxSection.PAIdNdxCerenkov(), G4PAIySection.PAIdNdxCerenkov(), G4InitXscPAI.PAIdNdxCherenkov(), G4PAIxSection.PAIdNdxMM(), G4InitXscPAI.PAIdNdxPlasmon(), G4PAIxSection.PAIdNdxPlasmon(), G4PAIySection.PAIdNdxPlasmon(), G4PAIxSection.PAIdNdxResonance(), G4LivermoreBremsstrahlungModel.SampleSecondaries(), G4LivermoreComptonModel.SampleSecondaries(), G4LivermorePolarizedComptonModel.SampleSecondaries(), G4PenelopeGammaConversionModel.SampleSecondaries(), and G4MonopoleEq.SetChargeMomentumMass().
int source.hepunit.g = gram |
Definition at line 132 of file hepunit.py.
int source.hepunit.gauss = 1.e-4*tesla |
Definition at line 191 of file hepunit.py.
int source.hepunit.GeV = gigaelectronvolt |
Definition at line 119 of file hepunit.py.
int source.hepunit.gigaelectronvolt = 1.e+3*megaelectronvolt |
Definition at line 109 of file hepunit.py.
int source.hepunit.gram = 1.e-3*kilogram |
Definition at line 127 of file hepunit.py.
Definition at line 218 of file hepunit.py.
Definition at line 262 of file hepunit.py.
Referenced by G4PenelopeRayleighModelMI.CalculateQSquared(), G4OpRayleigh.CalculateRayleighMeanFreePaths(), G4OpBoundaryProcess.DielectricDichroic(), G4OpBoundaryProcess.DielectricDielectric(), G4RayleighAngularGenerator.G4RayleighAngularGenerator(), G4PhononDownconversion.GetMeanFreePath(), G4PhononScattering.GetMeanFreePath(), G4LivermoreComptonModel.SampleSecondaries(), G4LivermorePolarizedComptonModel.SampleSecondaries(), G4LowEPComptonModel.SampleSecondaries(), and G4LowEPPolarizedComptonModel.SampleSecondaries().
float source.hepunit.halfpi = pi/2. |
Definition at line 248 of file hepunit.py.
Definition at line 263 of file hepunit.py.
Referenced by G4INCLXXInterface.ApplyYourself(), G4MicroElecInelasticModel_new.BKZ(), G4AblaInterface.DeExcite(), G4AdjointhIonisationModel.DefineProjectileProperty(), G4AdjointIonIonisationModel.DefineProjectileProperty(), G4AdjointDeuteron.Definition(), G4AdjointElectron.Definition(), G4AdjointElectronFI.Definition(), G4AdjointHe3.Definition(), G4AdjointPositron.Definition(), G4AdjointProton.Definition(), G4AdjointTriton.Definition(), G4AntiLambda.Definition(), G4AntiNeutron.Definition(), G4AntiOmegaMinus.Definition(), G4AntiProton.Definition(), G4AntiSigmaMinus.Definition(), G4AntiSigmaPlus.Definition(), G4AntiSigmaZero.Definition(), G4AntiXiMinus.Definition(), G4AntiXiZero.Definition(), G4Lambda.Definition(), G4Neutron.Definition(), G4OmegaMinus.Definition(), G4Proton.Definition(), G4SigmaMinus.Definition(), G4SigmaPlus.Definition(), G4SigmaZero.Definition(), G4XiMinus.Definition(), G4XiZero.Definition(), G4AntiDeuteron.Definition(), G4AntiDoubleHyperDoubleNeutron.Definition(), G4AntiDoubleHyperH4.Definition(), G4AntiHe3.Definition(), G4AntiHyperAlpha.Definition(), G4AntiHyperH4.Definition(), G4AntiHyperHe5.Definition(), G4AntiHyperTriton.Definition(), G4AntiTriton.Definition(), G4Deuteron.Definition(), G4DoubleHyperDoubleNeutron.Definition(), G4DoubleHyperH4.Definition(), G4He3.Definition(), G4HyperAlpha.Definition(), G4HyperH4.Definition(), G4HyperHe5.Definition(), G4HyperTriton.Definition(), G4Triton.Definition(), G4PionZero.Definition(), G4Electron.Definition(), G4MuonMinus.Definition(), G4MuonPlus.Definition(), G4Positron.Definition(), G4TauMinus.Definition(), G4TauPlus.Definition(), G4ParticleChange.DumpInfo(), G4F20GEMProbability.G4F20GEMProbability(), G4O17GEMProbability.G4O17GEMProbability(), G4SynchrotronRadiation.GetRandomEnergySR(), G4UCNBoundaryProcess.Loss(), G4LowEPComptonModel.SampleSecondaries(), G4LowEPPolarizedComptonModel.SampleSecondaries(), G4EqEMFieldWithEDM.SetChargeMomentumMass(), G4EqEMFieldWithSpin.SetChargeMomentumMass(), G4Mag_SpinEqRhs.SetChargeMomentumMass(), G4RepleteEofM.SetChargeMomentumMass(), G4AtimaEnergyLossModel.SetupParameters(), and G4EvaporationProbability.TotalProbability().
float source.hepunit.hbarc = hbar_Planck * c_light |
Definition at line 264 of file hepunit.py.
Referenced by G4VXTRenergyLoss.AngleXTRdEdx(), G4DiffuseElastic.BuildAngleTable(), G4DiffuseElasticV2.BuildAngleTable(), G4GEMProbability.CalcProbability(), G4AntiNuclElastic.CalculateAm(), G4PenelopeRayleighModelMI.CalculateQSquared(), G4XrayRayleighModel.ComputeCrossSectionPerAtom(), G4HadronNucleonXsc.CoulombBarrier(), G4InitXscPAI.DifPAIxSection(), G4PAIxSection.DifPAIxSection(), G4PAIySection.DifPAIySection(), G4KM_NucleonEqRhs.G4KM_NucleonEqRhs(), G4mplIonisationWithDeltaModel.G4mplIonisationWithDeltaModel(), G4NeutrinoElectronCcXsc.G4NeutrinoElectronCcXsc(), G4NeutrinoElectronNcXsc.G4NeutrinoElectronNcXsc(), G4NeutronElectronElXsc.G4NeutronElectronElXsc(), G4Nucleus.G4Nucleus(), G4WilsonAbrasionModel.GetAbradedNucleons(), G4VXTRenergyLoss.GetAngleVector(), G4AntiNuclElastic.GetcosTeta1(), G4EMDissociationCrossSection.GetCrossSectionForProjectile(), G4DiffuseElastic.GetDiffElasticProb(), G4DiffuseElastic.GetDiffElasticSumProb(), G4DiffuseElastic.GetDiffuseElasticSumXsc(), G4NuclNuclDiffuseElastic.GetDiffuseElasticSumXsc(), G4DiffuseElastic.GetDiffuseElasticXsc(), G4NuclNuclDiffuseElastic.GetDiffuseElasticXsc(), G4AntiProtonField.GetField(), G4KaonMinusField.GetField(), G4KaonPlusField.GetField(), G4KaonZeroField.GetField(), G4PionMinusField.GetField(), G4PionPlusField.GetField(), G4PionZeroField.GetField(), G4SigmaMinusField.GetField(), G4SigmaPlusField.GetField(), G4SigmaZeroField.GetField(), G4VXTRenergyLoss.GetGasFormationZone(), G4EMDissociationSpectrum.GetGeneralE1Spectrum(), G4EMDissociationSpectrum.GetGeneralE2Spectrum(), G4StrawTubeXTRadiator.GetMediumFormationZone(), G4VXTRenergyLoss.GetPlateFormationZone(), G4StrawTubeXTRadiator.GetStackFactor(), G4InitXscPAI.ImPartDielectricConst(), G4PAIxSection.ImPartDielectricConst(), G4PAIySection.ImPartDielectricConst(), G4DiffuseElastic.IntegralElasticProb(), G4NuclNuclDiffuseElastic.IntegralElasticProb(), G4GeneratorPrecompoundInterface.MakeCoalescence(), G4InitXscPAI.Normalisation(), G4PAIxSection.NormShift(), G4PAIySection.NormShift(), G4VXTRenergyLoss.OneInterfaceXTRdEdx(), G4PAIxSection.PAIdNdxCerenkov(), G4PAIySection.PAIdNdxCerenkov(), G4InitXscPAI.PAIdNdxCherenkov(), G4PAIxSection.PAIdNdxMM(), G4InitXscPAI.PAIdNdxPlasmon(), G4PAIxSection.PAIdNdxPlasmon(), G4PAIySection.PAIdNdxPlasmon(), G4PAIxSection.PAIdNdxResonance(), G4InitXscPAI.RePartDielectricConst(), G4PAIxSection.RePartDielectricConst(), G4PAIySection.RePartDielectricConst(), G4GEMChannel.SampleKineticEnergy(), G4XrayRayleighModel.SampleSecondaries(), G4DiffuseElastic.SampleThetaCMS(), G4NuclNuclDiffuseElastic.SampleThetaCMS(), G4KM_OpticalEqRhs.SetFactor(), G4GaussXTRadiator.SpectralXTRdEdx(), G4RegularXTRadiator.SpectralXTRdEdx(), G4TransparentRegXTRadiator.SpectralXTRdEdx(), G4XTRRegularRadModel.SpectralXTRdEdx(), G4XTRTransparentRegRadModel.SpectralXTRdEdx(), G4DiffuseElastic.TestAngleTable(), and G4NuclNuclDiffuseElastic.TestAngleTable().
Definition at line 265 of file hepunit.py.
Referenced by G4Reggeons.Chi_pomeron(), G4Reggeons.Chi_reggeon(), G4UCNMaterialPropertiesTable.ConditionsValid(), G4XAnnihilationChannel.CrossSection(), G4QAOLowEnergyLoss.EnergyLoss(), G4UCNMicroRoughnessHelper.IntIminus(), G4UCNMicroRoughnessHelper.IntIplus(), G4UCNMicroRoughnessHelper.ProbIminus(), G4UCNMicroRoughnessHelper.ProbIplus(), and G4UCNMaterialPropertiesTable.TransConditionsValid().
Definition at line 197 of file hepunit.py.
int source.hepunit.hertz = 1./second |
Definition at line 87 of file hepunit.py.
int source.hepunit.joule = electronvolt/e_SI |
Definition at line 113 of file hepunit.py.
Definition at line 298 of file hepunit.py.
Referenced by G4LENDElastic.ApplyYourself(), G4LENDModel.ApplyYourself(), G4OpRayleigh.CalculateRayleighMeanFreePaths(), G4DNAMolecularReactionData.ComputeEffectiveRadius(), G4ParticleHPCaptureData.GetCrossSection(), G4ParticleHPElasticData.GetCrossSection(), G4ParticleHPFissionData.GetCrossSection(), G4Molecule.GetDiffusionVelocity(), and G4Nucleus.GetThermalPz().
int source.hepunit.kelvin = 1. |
Definition at line 202 of file hepunit.py.
int source.hepunit.keV = kiloelectronvolt |
Definition at line 118 of file hepunit.py.
int source.hepunit.kg = kilogram |
Definition at line 131 of file hepunit.py.
Definition at line 303 of file hepunit.py.
Referenced by G4Material.G4Material().
int source.hepunit.kiloelectronvolt = 1.e-3*megaelectronvolt |
Definition at line 108 of file hepunit.py.
int source.hepunit.kilogauss = 1.e-1*tesla |
Definition at line 192 of file hepunit.py.
Definition at line 126 of file hepunit.py.
int source.hepunit.kilohertz = 1.e+3*hertz |
Definition at line 88 of file hepunit.py.
int source.hepunit.kilometer = 1000.*meter |
Definition at line 27 of file hepunit.py.
Definition at line 28 of file hepunit.py.
Definition at line 29 of file hepunit.py.
int source.hepunit.kilovolt = 1.e-3*megavolt |
Definition at line 164 of file hepunit.py.
int source.hepunit.km = kilometer |
Definition at line 57 of file hepunit.py.
int source.hepunit.km2 = kilometer2 |
Definition at line 58 of file hepunit.py.
int source.hepunit.km3 = kilometer3 |
Definition at line 59 of file hepunit.py.
Definition at line 228 of file hepunit.py.
Definition at line 233 of file hepunit.py.
int source.hepunit.m = meter |
Definition at line 53 of file hepunit.py.
int source.hepunit.m2 = meter2 |
Definition at line 54 of file hepunit.py.
int source.hepunit.m3 = meter3 |
Definition at line 55 of file hepunit.py.
int source.hepunit.megaelectronvolt = 1. |
Definition at line 106 of file hepunit.py.
int source.hepunit.megahertz = 1.e+6*hertz |
Definition at line 89 of file hepunit.py.
int source.hepunit.megavolt = megaelectronvolt/eplus |
Definition at line 163 of file hepunit.py.
int source.hepunit.meter = 1000.*millimeter |
Definition at line 23 of file hepunit.py.
Definition at line 24 of file hepunit.py.
Definition at line 25 of file hepunit.py.
int source.hepunit.MeV = megaelectronvolt |
Definition at line 116 of file hepunit.py.
int source.hepunit.mg = milligram |
Definition at line 133 of file hepunit.py.
int source.hepunit.microampere = 1.e-6*ampere |
Definition at line 157 of file hepunit.py.
int source.hepunit.microbarn = 1.e-6 *barn |
Definition at line 40 of file hepunit.py.
int source.hepunit.microfarad = 1.e-6*farad |
Definition at line 177 of file hepunit.py.
int source.hepunit.micrometer = 1.e-6 *meter |
Definition at line 33 of file hepunit.py.
int source.hepunit.microsecond = 1.e-6 *second |
Definition at line 84 of file hepunit.py.
int source.hepunit.milliampere = 1.e-3*ampere |
Definition at line 156 of file hepunit.py.
int source.hepunit.millibarn = 1.e-3 *barn |
Definition at line 39 of file hepunit.py.
int source.hepunit.millifarad = 1.e-3*farad |
Definition at line 176 of file hepunit.py.
int source.hepunit.milligram = 1.e-3*gram |
Definition at line 128 of file hepunit.py.
int source.hepunit.millimeter = 1. |
Definition at line 15 of file hepunit.py.
int source.hepunit.millimeter2 = millimeter*millimeter |
Definition at line 16 of file hepunit.py.
int source.hepunit.millimeter3 = millimeter*millimeter*millimeter |
Definition at line 17 of file hepunit.py.
int source.hepunit.milliradian = 1.e-3*radian |
Definition at line 67 of file hepunit.py.
int source.hepunit.millisecond = 1.e-3 *second |
Definition at line 83 of file hepunit.py.
int source.hepunit.mm = millimeter |
Definition at line 45 of file hepunit.py.
int source.hepunit.mm2 = millimeter2 |
Definition at line 46 of file hepunit.py.
int source.hepunit.mm3 = millimeter3 |
Definition at line 47 of file hepunit.py.
int source.hepunit.mole = 1. |
Definition at line 207 of file hepunit.py.
int source.hepunit.mrad = milliradian |
Definition at line 74 of file hepunit.py.
int source.hepunit.ms = millisecond |
Definition at line 94 of file hepunit.py.
Definition at line 281 of file hepunit.py.
int source.hepunit.nanoampere = 1.e-9*ampere |
Definition at line 158 of file hepunit.py.
int source.hepunit.nanobarn = 1.e-9 *barn |
Definition at line 41 of file hepunit.py.
int source.hepunit.nanofarad = 1.e-9*farad |
Definition at line 178 of file hepunit.py.
int source.hepunit.nanometer = 1.e-9 *meter |
Definition at line 34 of file hepunit.py.
int source.hepunit.nanosecond = 1. |
Definition at line 81 of file hepunit.py.
float source.hepunit.neutron_mass_c2 = 939.56563 * MeV |
Definition at line 275 of file hepunit.py.
Referenced by G4MuMinusCapturePrecompound.ApplyYourself(), G4UCNMaterialPropertiesTable.ConditionsValid(), G4AntiNeutron.Definition(), G4Neutron.Definition(), G4FermiFragmentsPoolVI.Dump(), G4GEMProbability.Dump(), G4NeutronElectronElModel.G4NeutronElectronElModel(), G4NeutronElectronElXsc.G4NeutronElectronElXsc(), G4AntiProtonField.GetField(), G4KaonMinusField.GetField(), G4KaonPlusField.GetField(), G4KaonZeroField.GetField(), G4NeutronField.GetField(), G4PionMinusField.GetField(), G4PionPlusField.GetField(), G4PionZeroField.GetField(), G4SigmaMinusField.GetField(), G4SigmaPlusField.GetField(), G4SigmaZeroField.GetField(), G4UCNMicroRoughnessHelper.IntIminus(), G4UCNMicroRoughnessHelper.IntIplus(), G4UCNBoundaryProcess.Loss(), G4UCNBoundaryProcess.MRreflectHigh(), G4UCNBoundaryProcess.PostStepDoIt(), G4UCNMicroRoughnessHelper.ProbIminus(), G4UCNMicroRoughnessHelper.ProbIplus(), G4KM_OpticalEqRhs.SetFactor(), and G4UCNMaterialPropertiesTable.TransConditionsValid().
Definition at line 143 of file hepunit.py.
int source.hepunit.ns = nanosecond |
Definition at line 92 of file hepunit.py.
Definition at line 170 of file hepunit.py.
float source.hepunit.parsec = 3.0856775807e+16*meter |
Definition at line 31 of file hepunit.py.
Definition at line 148 of file hepunit.py.
float source.hepunit.pc = parsec |
Definition at line 61 of file hepunit.py.
float source.hepunit.perCent = 0.01 |
Definition at line 238 of file hepunit.py.
float source.hepunit.perMillion = 0.000001 |
Definition at line 240 of file hepunit.py.
float source.hepunit.perThousand = 0.001 |
Definition at line 239 of file hepunit.py.
int source.hepunit.petaelectronvolt = 1.e+9*megaelectronvolt |
Definition at line 111 of file hepunit.py.
int source.hepunit.PeV = petaelectronvolt |
Definition at line 121 of file hepunit.py.
float source.hepunit.pi = 3.14159265358979323846 |
Definition at line 246 of file hepunit.py.
Definition at line 249 of file hepunit.py.
int source.hepunit.picobarn = 1.e-12*barn |
Definition at line 42 of file hepunit.py.
int source.hepunit.picofarad = 1.e-12*farad |
Definition at line 179 of file hepunit.py.
int source.hepunit.picosecond = 1.e-12*second |
Definition at line 85 of file hepunit.py.
float source.hepunit.proton_mass_c2 = 938.27231 * MeV |
Definition at line 274 of file hepunit.py.
Referenced by G4NuclearStopping.AlongStepDoIt(), G4hImpactIonisation.AlongStepDoIt(), G4VMultipleScattering.AlongStepGetPhysicalInteractionLength(), G4hImpactIonisation.AntiProtonParametrisedDEDX(), G4ANuElNucleusCcModel.ApplyYourself(), G4ANuElNucleusNcModel.ApplyYourself(), G4ANuMuNucleusCcModel.ApplyYourself(), G4ANuMuNucleusNcModel.ApplyYourself(), G4MuonVDNuclearModel.ApplyYourself(), G4NuElNucleusCcModel.ApplyYourself(), G4NuElNucleusNcModel.ApplyYourself(), G4NuMuNucleusCcModel.ApplyYourself(), G4NuMuNucleusNcModel.ApplyYourself(), G4LEHadronProtonElastic.ApplyYourself(), G4LEnp.ApplyYourself(), G4LEpp.ApplyYourself(), G4hImpactIonisation.BarkasTerm(), G4hImpactIonisation.BlochTerm(), G4VXTRenergyLoss.BuildAngleForEnergyBank(), G4VXTRenergyLoss.BuildAngleTable(), G4hRDEnergyLoss.BuildDEDXTable(), G4VXTRenergyLoss.BuildEnergyTable(), G4VXTRenergyLoss.BuildGlobalAngleTable(), G4hImpactIonisation.BuildLossTable(), G4hImpactIonisation.BuildPhysicsTable(), G4ForwardXrayTR.BuildXrayTRtables(), G4MuonVDNuclearModel.CalculateEMVertex(), G4hParametrisedLossModel.ChemicalFactor(), G4BraggModel.ChemicalFactor(), G4IonCoulombScatteringModel.ComputeCrossSectionPerAtom(), G4hCoulombScatteringModel.ComputeCrossSectionPerAtom(), G4KokoulinMuonNuclearXS.ComputeDDMicroscopicCrossSection(), G4hImpactIonisation.ComputeDEDX(), G4ICRU49NuclearStoppingModel.ComputeDEDXPerVolume(), G4KokoulinMuonNuclearXS.ComputeMicroscopicCrossSection(), G4DNADingfelderChargeIncreaseModel.CrossSectionPerVolume(), G4MicroElecInelasticModel.CrossSectionPerVolume(), G4MicroElecInelasticModel_new.CrossSectionPerVolume(), G4ICRU73QOModel.DEDXPerElement(), G4AdjointCSManager.DefineCurrentParticle(), G4AdjointhIonisationModel.DefineProjectileProperty(), G4AdjointIonIonisationModel.DefineProjectileProperty(), G4AdjointDeuteron.Definition(), G4AdjointHe3.Definition(), G4AdjointProton.Definition(), G4AdjointTriton.Definition(), G4AntiLambda.Definition(), G4AntiNeutron.Definition(), G4AntiOmegaMinus.Definition(), G4AntiProton.Definition(), G4AntiSigmaMinus.Definition(), G4AntiSigmaPlus.Definition(), G4AntiXiMinus.Definition(), G4AntiXiZero.Definition(), G4Lambda.Definition(), G4Neutron.Definition(), G4OmegaMinus.Definition(), G4Proton.Definition(), G4SigmaMinus.Definition(), G4SigmaPlus.Definition(), G4XiMinus.Definition(), G4XiZero.Definition(), G4AntiDeuteron.Definition(), G4AntiDoubleHyperDoubleNeutron.Definition(), G4AntiDoubleHyperH4.Definition(), G4AntiHe3.Definition(), G4AntiHyperAlpha.Definition(), G4AntiHyperH4.Definition(), G4AntiHyperHe5.Definition(), G4AntiHyperTriton.Definition(), G4AntiTriton.Definition(), G4Deuteron.Definition(), G4DoubleHyperDoubleNeutron.Definition(), G4DoubleHyperH4.Definition(), G4He3.Definition(), G4HyperAlpha.Definition(), G4HyperH4.Definition(), G4HyperHe5.Definition(), G4HyperTriton.Definition(), G4Triton.Definition(), G4DNARuddIonisationModel.DifferentialCrossSection(), G4FermiFragmentsPoolVI.Dump(), G4hImpactIonisation.ElectronicLossFluctuation(), G4QAOLowEnergyLoss.EnergyLoss(), G4IonisParamElm.G4IonisParamElm(), G4UrbanAdjointMscModel.G4UrbanAdjointMscModel(), G4hImpactIonisation.GetConstraints(), G4AntiProtonField.GetField(), G4KaonMinusField.GetField(), G4KaonPlusField.GetField(), G4KaonZeroField.GetField(), G4PionMinusField.GetField(), G4PionPlusField.GetField(), G4PionZeroField.GetField(), G4ProtonField.GetField(), G4SigmaMinusField.GetField(), G4SigmaPlusField.GetField(), G4SigmaZeroField.GetField(), G4MuNeutrinoNucleusTotXsc.GetIsoCrossSection(), G4ElNeutrinoNucleusTotXsc.GetIsoCrossSection(), G4VXTRenergyLoss.GetMeanFreePath(), G4VXTRenergyLoss.GetNumberOfPhotons(), G4UAtomicDeexcitation.GetShellIonisationCrossSectionPerAtom(), G4NistElementBuilder.Initialise(), G4PAIPhotData.Initialise(), G4PAIModelData.Initialise(), G4MicroElecInelasticModel.Initialise(), G4MicroElecInelasticModel_new.Initialise(), G4EmSaturation.InitialiseBirksCoefficient(), G4hhIonisation.InitialiseEnergyLossProcess(), G4hIonisation.InitialiseEnergyLossProcess(), G4hNuclearStoppingModel.InitializeMe(), G4hIonEffChargeSquare.IonEffChargeSquare(), G4EmCorrections.IonHighOrderCorrections(), G4MuonVDNuclearModel.MakeSamplingTable(), G4ForwardXrayTR.PostStepDoIt(), G4VXTRenergyLoss.PostStepDoIt(), G4hImpactIonisation.ProtonParametrisedDEDX(), G4DNAPTBIonisationModel.RandomizeEjectedElectronDirection(), G4MicroElecInelasticModel_new.RandomizeEjectedElectronEnergy(), G4DNABornIonisationModel1.RandomizeEjectedElectronEnergy(), G4DNABornIonisationModel2.RandomizeEjectedElectronEnergy(), G4MicroElecInelasticModel.RandomizeEjectedElectronEnergy(), G4DNAPTBIonisationModel.RandomizeEjectedElectronEnergy(), G4DNARuddIonisationModel.RandomizeEjectedElectronEnergy(), G4MicroElecInelasticModel_new.RandomSelect(), G4DNADingfelderChargeDecreaseModel.SampleSecondaries(), G4DNADingfelderChargeIncreaseModel.SampleSecondaries(), G4MicroElecInelasticModel.SampleSecondaries(), G4MicroElecInelasticModel_new.SampleSecondaries(), G4ContinuousGainOfEnergy.SetDirectParticle(), G4KM_OpticalEqRhs.SetFactor(), G4VEmProcess.StartTracking(), G4hParametrisedLossModel.TheValue(), G4MicroElecInelasticModel_new.TransferedEnergy(), and G4MicroElecInelasticModel.TransferedEnergy().
int source.hepunit.rad = radian |
Definition at line 73 of file hepunit.py.
int source.hepunit.radian = 1. |
Definition at line 66 of file hepunit.py.
int source.hepunit.s = second |
Definition at line 93 of file hepunit.py.
int source.hepunit.second = 1.e+9 *nanosecond |
Definition at line 82 of file hepunit.py.
int source.hepunit.sr = steradian |
Definition at line 75 of file hepunit.py.
int source.hepunit.steradian = 1. |
Definition at line 70 of file hepunit.py.
int source.hepunit.STP_Pressure = 1.*atmosphere |
Definition at line 302 of file hepunit.py.
Referenced by G4NistMaterialBuilder.BuildMaterial(), G4IonisParamMat.ComputeDensityEffectParameters(), G4GDMLReadMaterials.MaterialRead(), G4GDMLWriteMaterials.MaterialWrite(), and G4GDMLReadMaterials.PRead().
float source.hepunit.STP_Temperature = 273.15*kelvin |
Definition at line 301 of file hepunit.py.
Referenced by MyMaterials.Construct(), Construct(), QMaterials.Construct(), ExN03DetectorConstruction.DefineMaterials(), and G4GDMLWriteMaterials.MaterialWrite().
int source.hepunit.teraelectronvolt = 1.e+6*megaelectronvolt |
Definition at line 110 of file hepunit.py.
Definition at line 189 of file hepunit.py.
int source.hepunit.TeV = teraelectronvolt |
Definition at line 120 of file hepunit.py.
int source.hepunit.twopi = 2.*pi |
Definition at line 247 of file hepunit.py.
int source.hepunit.twopi_mc2_rcl2 = twopi * electron_mass_c2 \ |
Definition at line 293 of file hepunit.py.
Referenced by G4AdjointComptonModel.AdjointCrossSection(), G4AdjointhIonisationModel.AdjointCrossSection(), G4hImpactIonisation.BarkasTerm(), G4hBetheBlochModel.BetheBlochFormula(), G4hImpactIonisation.BlochTerm(), G4IonParametrisedLossModel.ComputeCrossSectionPerAtom(), G4MuBetheBlochModel.ComputeCrossSectionPerElectron(), G4AtimaEnergyLossModel.ComputeCrossSectionPerElectron(), G4MollerBhabhaModel.ComputeCrossSectionPerElectron(), G4MollerBhabhaModel.ComputeDEDXPerVolume(), G4EmCorrections.ComputeIonCorrections(), G4hImpactIonisation.DeltaRaysEnergy(), G4AdjointeIonisationModel.DiffCrossSectionMoller(), G4mplIonisationModel.Dispersion(), G4mplIonisationWithDeltaModel.Dispersion(), G4PAIModel.Dispersion(), G4PAIPhotModel.Dispersion(), G4hImpactIonisation.ElectronicLossFluctuation(), G4IonisParamElm.G4IonisParamElm(), G4EmCorrections.HighOrderCorrections(), G4EmCorrections.IonBarkasCorrection(), G4hImpactIonisation.MicroscopicCrossSection(), G4PixeCrossSectionHandler.MicroscopicCrossSection(), G4AdjointComptonModel.RapidSampleSecondaries(), and G4AdjointhIonisationModel.RapidSampleSecondaries().
Definition at line 306 of file hepunit.py.
Referenced by MyMaterials.Construct(), Construct(), QMaterials.Construct(), G4EzWorld.CreateWorld(), ExN03DetectorConstruction.DefineMaterials(), G4gsmate(), G4Material.G4Material(), and G4NistMaterialBuilder.HepAndNuclearMaterials().
int source.hepunit.volt = 1.e-6*megavolt |
Definition at line 165 of file hepunit.py.
Definition at line 138 of file hepunit.py.
Definition at line 184 of file hepunit.py.