Geant4.10
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Variables | |
tuple | input_file_1 = TFile('test35a.root','READ') |
tuple | input_file_2 = TFile('test35b.root','READ') |
tuple | c1 = TCanvas('c1', 'test35', 200, 10, 700, 500) |
int | n = 41 |
tuple | bin = array( 'f' ) |
tuple | h_1 = TH1F('unbiased','Source Spectrum',40,bin) |
tuple | h_2 = TH1F('biased','Source Spectrum',40,bin) |
tuple | t1 = gROOT.FindObject('MyTuple') |
tuple plottest35.bin = array( 'f' ) |
Definition at line 22 of file plottest35.py.
Referenced by Histo.AddPhantomGamma(), Histo.AddPhantomStep(), G4CrossSectionHandler.BuildCrossSectionsForMaterials(), G4RDCrossSectionHandler.BuildCrossSectionsForMaterials(), G4RDBremsstrahlungCrossSectionHandler.BuildCrossSectionsForMaterials(), G4RDeIonisationCrossSectionHandler.BuildCrossSectionsForMaterials(), G4BremsstrahlungCrossSectionHandler.BuildCrossSectionsForMaterials(), G4eIonisationCrossSectionHandler.BuildCrossSectionsForMaterials(), G4VEnergyLossProcess.BuildDEDXTable(), G4VEnergyLossProcess.BuildLambdaTable(), G4RDVCrossSectionHandler.BuildMeanFreePathForMaterials(), G4VCrossSectionHandler.BuildMeanFreePathForMaterials(), G4PenelopeIonisationXSHandler.BuildXSTable(), G4RDLinLogLogInterpolation.Calculate(), G4RDLinLogInterpolation.Calculate(), G4LinLogLogInterpolation.Calculate(), G4LinInterpolator.Calculate(), G4LinLogInterpolation.Calculate(), G4LogLogInterpolator.Calculate(), G4RDLinInterpolation.Calculate(), G4RDLogLogInterpolation.Calculate(), G4RDSemiLogInterpolation.Calculate(), G4LinInterpolation.Calculate(), G4LogLogInterpolation.Calculate(), G4SemiLogInterpolation.Calculate(), RunAction.ComputeFluenceError(), Run.ComputeStatistics(), G4NeutronHPFastLegendre.Evaluate(), Em10RunAction.FillEn(), XrayFluoDataSet.FindValue(), G4hhIonisation.InitialiseEnergyLossProcess(), G4mplIonisation.InitialiseEnergyLossProcess(), G4NeutronHPFastLegendre.Integrate(), RunAction.PrintFluence(), G4DataSet.RandomSelect(), G4RDEMDataSet.RandomSelect(), G4EMDataSet.RandomSelect(), G4RadioactiveDecay.SetDecayBias(), and G4RadioactiveDecay.SetSourceTimeProfile().
tuple plottest35.c1 = TCanvas('c1', 'test35', 200, 10, 700, 500) |
Definition at line 14 of file plottest35.py.
Referenced by G4KineticTrackVector.Boost(), G4KineticTrackVector.BoostBeam(), G4VLongitudinalStringDecay.CalculateHadronTimePosition(), G4QMDCollision.CalFinalStateOfTheBinaryCollisionJQMD(), G4HeatedKleinNishinaCompton.ComputeCrossSectionPerAtom(), G4KleinNishinaCompton.ComputeCrossSectionPerAtom(), G4KleinNishinaModel.ComputeCrossSectionPerAtom(), G4UrbanMscModel.ComputeCrossSectionPerAtom(), G4INCL::CoulombNonRelativistic.distortOut(), G4Abla.eflmac(), CLHEP::HepRotation.eulerAngles(), G4UImanager.ForeachS(), G4DPMJET2_5CrossSectionParamSet.G4DPMJET2_5CrossSectionParamSet(), G4PolyhedraSide.G4PolyhedraSide(), CLHEP::RandGauss.get(), G4VXTRenergyLoss.GetComptonPerAtom(), G4NuclNuclDiffuseElastic.GetCoulombIntegralXsc(), G4DiffuseElastic.GetCoulombIntegralXsc(), TabulatedField3D.GetFieldValue(), EMField.GetFieldValue(), G4Abla.guet(), G4UImanager.LoopS(), CCalMagneticField.MagneticField(), G4InitXscPAI.RePartDielectricConst(), G4PAIySection.RePartDielectricConst(), G4PAIxSection.RePartDielectricConst(), CLHEP::RandGauss.restoreDistState(), CLHEP::RandFlat.restoreDistState(), CLHEP::HepLorentzRotation.rotateX(), CLHEP::HepRotation.rotateX(), CLHEP::HepLorentzRotation.rotateY(), CLHEP::HepRotation.rotateY(), CLHEP::HepLorentzRotation.rotateZ(), CLHEP::HepRotation.rotateZ(), G4InitXscPAI.RutherfordIntegral(), G4PAIySection.RutherfordIntegral(), G4PAIxSection.RutherfordIntegral(), G4BoldyshevTripletModel.SampleSecondaries(), G4SandiaTable.SandiaIntervals(), G4hRDEnergyLoss.SetStepFunction(), G4RDVeLowEnergyLoss.SetStepFunction(), G4BetaDecayCorrections.ShapeFactor(), G4KineticTrackVector.Shift(), G4RKG3_Stepper.StepNoErr(), G4CashKarpRKF45.Stepper(), and UPolyhedraSide.UPolyhedraSide().
tuple plottest35.h_1 = TH1F('unbiased','Source Spectrum',40,bin) |
Definition at line 27 of file plottest35.py.
tuple plottest35.h_2 = TH1F('biased','Source Spectrum',40,bin) |
Definition at line 28 of file plottest35.py.
tuple plottest35.input_file_1 = TFile('test35a.root','READ') |
Definition at line 8 of file plottest35.py.
tuple plottest35.input_file_2 = TFile('test35b.root','READ') |
Definition at line 9 of file plottest35.py.
int plottest35.n = 41 |
Definition at line 21 of file plottest35.py.
tuple plottest35.t1 = gROOT.FindObject('MyTuple') |
Definition at line 33 of file plottest35.py.
Referenced by G4AdjointhIonisationModel.AdjointCrossSection(), G4Abla.breakItUp(), G4QMDCollision.CalFinalStateOfTheBinaryCollisionJQMD(), G4RToEConvForElectron.ComputeLoss(), G4RToEConvForPositron.ComputeLoss(), G4CollisionNN.CrossSection(), G4DNABornIonisationModel.DifferentialCrossSection(), G4MicroElecInelasticModel.DifferentialCrossSection(), G4MuElecInelasticModel.DifferentialCrossSection(), UTubs.DistanceToIn(), G4CutTubs.DistanceToIn(), UCons.DistanceToIn(), G4OTubs.DistanceToIn(), USphere.DistanceToIn(), G4Tubs.DistanceToIn(), G4Cons.DistanceToIn(), G4Sphere.DistanceToIn(), UTet.DistanceToOut(), G4CutTubs.DistanceToOut(), UTubs.DistanceToOut(), G4OTubs.DistanceToOut(), G4Tet.DistanceToOut(), UCons.DistanceToOut(), USphere.DistanceToOut(), G4Tubs.DistanceToOut(), G4Cons.DistanceToOut(), G4Sphere.DistanceToOut(), CLHEP::HepLorentzVector.findBoostToCM(), G4DataQuestionaire.G4DataQuestionaire(), G4INCL::DeltaDecayChannel.getFinalState(), G4MuonMinusBoundDecay.GetMuonCaptureRate(), G4NucleiModel.initializeCascad(), G4ErrorMatrix.invert(), G4ErrorSymMatrix.invert(), G4INCL::ParticleConfig.isPair(), G4UImanager.LoopS(), G4DNASancheExcitationModel.PartialCrossSection(), G4AdjointhIonisationModel.RapidSampleSecondaries(), and UTet.SafetyFromInside().