advanced/amsEcal/showers/plotHisto.C 파일 참조

이 파일의 소스 코드 페이지로 가기

함수
hist1	Draw ("HIST")

변수
TFile	f = TFile("run2.root")
TCanvas *	c1 = new TCanvas("c1", " ")
TH1D *	hist1 = (TH1D*)f.Get("1")
TH1D *	hist2 = (TH1D*)f.Get("2")
TH1D *	hist3 = (TH1D*)f.Get("3")
TH1D *	hist4 = (TH1D*)f.Get("4")
TH1D *	hist5 = (TH1D*)f.Get("5")

함수 문서화

hist26 Draw

(

"HIST"

)

다음에 의해서 참조됨 : G4VSceneHandler::AddCompound().

변수 문서화

TCanvas* c1 = new TCanvas("c1", " ")

advanced/amsEcal/showers/plotHisto.C 파일의 7 번째 라인에서 정의되었습니다.

다음에 의해서 참조됨 : G4ExtrudedSolid::AddGeneralPolygonFacets(), G4KineticTrackVector::Boost(), G4KineticTrackVector::BoostBeam(), braggPeak(), G4DNAUeharaScreenedRutherfordElasticModel::BrennerZaiderRandomizeCosTheta(), G4DNAScreenedRutherfordElasticModel::BrennerZaiderRandomizeCosTheta(), G4VLongitudinalStringDecay::CalculateHadronTimePosition(), G4OpRayleigh::CalculateRayleighMeanFreePaths(), G4RKFieldIntegrator::CalculateTotalEnergy(), G4QMDCollision::CalFinalStateOfTheBinaryCollisionJQMD(), G4KleinNishinaCompton::ComputeCrossSectionPerAtom(), G4KleinNishinaModel::ComputeCrossSectionPerAtom(), G4BetheHeitlerModel::ComputeCrossSectionPerAtom(), G4UrbanMscModel::ComputeCrossSectionPerAtom(), G4UrbanAdjointMscModel::ComputeCrossSectionPerAtom(), G4SandiaTable::ComputeMatSandiaMatrixPAI(), G4SandiaTable::ComputeMatTable(), G4JTPolynomialSolver::ComputeNewEstimate(), G4INCL::CoulombNonRelativistic::distortOut(), G4Abla::eflmac(), G4Abla::eflmac_profi(), G4RKFieldIntegrator::Erf(), CLHEP::HepRotation::eulerAngles(), G4INCL::PiNToEtaChannel::fillFinalState(), G4UImanager::ForeachS(), fragmentAngularDistribution(), fragmentAngularDistributionGM(), fragmentAngularDistributionHistogram(), fragmentYieldsPlot(), G4PolyhedraSide::G4PolyhedraSide(), CLHEP::RandGauss::get(), G4VXTRenergyLoss::GetComptonPerAtom(), G4NuclNuclDiffuseElastic::GetCoulombIntegralXsc(), G4DiffuseElastic::GetCoulombIntegralXsc(), G4RKFieldIntegrator::GetExcitationEnergy(), TabulatedField3D::GetFieldValue(), EMField::GetFieldValue(), G4Abla::guet(), G4UImanager::LoopS(), CCalMagneticField::MagneticField(), plot(), 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(), G4UrbanMscModel::SampleCosineTheta(), G4UrbanAdjointMscModel::SampleCosineTheta(), G4BoldyshevTripletModel::SampleSecondaries(), G4SandiaTable::SandiaIntervals(), G4UIcontrolMessenger::SetNewValue(), G4LivermorePolarizedGammaConversionModel::SetPhi(), G4hRDEnergyLoss::SetStepFunction(), G4RDVeLowEnergyLoss::SetStepFunction(), G4BetaDecayCorrections::ShapeFactor(), G4KineticTrackVector::Shift(), G4RKG3_Stepper::StepNoErr(), G4DormandPrinceRK56::Stepper(), G4DormandPrinceRK78::Stepper(), G4CashKarpRKF45::Stepper(), streqci().

TFile f = TFile("run2.root")

advanced/amsEcal/showers/plotHisto.C 파일의 6 번째 라인에서 정의되었습니다.

다음에 의해서 참조됨 : G4MTcoutDestination::AddMasterOutput(), G4GMocrenFileSceneHandler::AddPrimitive(), G4ForwardXrayTR::AngleDensity(), G4OpenInventorXtExaminerViewer::animateSensorCB(), G4OpenInventorXtExaminerViewer::animateSensorRotationCB(), G4AntiNeutronAnnihilationAtRest::AntiNeutronAnnihilation(), G4ErrorMatrix::apply(), G4ErrorSymMatrix::apply(), G4NeutronRadCapture::ApplyYourself(), CB_G4UserEventAction::BeginOfEventAction(), CB_G4UserRunAction::BeginOfRunAction(), braggPeak(), G4FermiBreakUpVI::BreakFragment(), G4PenelopeRayleighModel::BuildFormFactorTable(), G4StatMFMicroPartition::CalcPartitionProbability(), Call< g, f, A >::call(), checkBeam(), ChromosomeParameterisation::ChromosomeParameterisation(), pyG4UserStackingAction::CB_G4UserStackingAction::ClassifyNewTrack(), cm_energy(), G4RToEConvForPositron::ComputeLoss(), G4RToEConvForElectron::ComputeLoss(), c2_factory< float_type >::const_plugin_function(), G4ChipsKaonMinusInelasticXS::CrossSectionFormula(), G4ChipsPionMinusInelasticXS::CrossSectionFormula(), G4ChipsKaonPlusInelasticXS::CrossSectionFormula(), G4ChipsPionPlusInelasticXS::CrossSectionFormula(), csz__huft_build(), G4MagneticFieldModel::DescribeYourselfTo(), G4AdjointIonIonisationModel::DiffCrossSectionPerAtomPrimToSecond(), G4AdjointhIonisationModel::DiffCrossSectionPerAtomPrimToSecond(), G4AtimaFluctuations::Dispersion(), G4TriangularFacet::Distance(), G4FermiFragmentsPoolVI::Dump(), G4BraggModel::ElectronicStoppingPower(), CB_G4UserEventAction::EndOfEventAction(), HistoManager::EndOfRun(), CB_G4UserRunAction::EndOfRunAction(), G4PolynomialPDF::Evaluate(), G4AntiNeutronAnnihilationAtRest::ExNu(), G4ASTARStopping::FindData(), G4PSTARStopping::FindData(), fragmentAngularDistribution(), fragmentAngularDistributionGM(), fragmentAngularDistributionHistogram(), fragmentEnergy(), fragmentEnergyDistributionDifferentAngles(), fragmentYieldsPlot(), G4eIonisationSpectrum::Function(), G4RDeIonisationSpectrum::Function(), G4eBremsstrahlungSpectrum::Function(), G4RDeBremsstrahlungSpectrum::Function(), G4AdjointBremsstrahlungModel::G4AdjointBremsstrahlungModel(), G4AnyMethod::G4AnyMethod(), G4ElasticHadrNucleusHE::G4ElasticHadrNucleusHE(), G4Expf(), G4LevelReader::G4LevelReader(), G4Logf(), G4PhotonEvaporation::G4PhotonEvaporation(), G4Pow::G4Pow(), GammaFit(), CLHEP::RandBinomial::genBinomial(), G4eeToHadronsModel::GenerateCMPhoton(), GammaRayTelPrimaryGeneratorAction::GeneratePrimaries(), G4TripathiLightCrossSection::GetElementCrossSection(), G4ElectroNuclearCrossSection::GetEquivalentPhotonEnergy(), G4PolynomialPDF::GetX(), G4FermiFragmentsPoolVI::Initialise(), G4PhotonEvaporation::InitialiseGRData(), G4PolarizedMollerCrossSection::Initialize(), G4TessellatedSolid::InsideNoVoxels(), G4INCL::IFunction1D::inverseCDFTable(), HepPolyhedron::InvertFacets(), G4INCL::InvFInterpolationTable::InvFInterpolationTable(), G4EmCorrections::KShellCorrection(), G4LevelReader::LevelManager(), G4EmCorrections::LShellCorrection(), G4NuclearLevelData::MaxLevelEnergy(), pyG4UserStackingAction::CB_G4UserStackingAction::NewStage(), G4TessellatedSolid::Normal(), G4LevelReader::NormalizedICCProbability(), c2_const_ptr< G4double >::operator=(), c2_ptr< G4double >::operator=(), c2_factory< float_type >::plugin_function(), CB_G4UserTrackingAction::PostUserTrackingAction(), pyG4UserStackingAction::CB_G4UserStackingAction::PrepareNewEvent(), CB_G4UserTrackingAction::PreUserTrackingAction(), G4INCL::IFunction1D::primitive(), G4OpenInventorXtExaminerViewer::processSoEvent(), ptwXY_createFromFunctionBisect(), ptwXY_f_integrate(), ptwXY_groupOneFunction(), ptwXY_groupThreeFunctions(), ptwXY_groupTwoFunctions(), ptwXY_unitbaseInterpolate(), readExfor(), G4IonFluctuations::RelativisticFactor(), G4SampleResonance::SampleMass(), G4VScatteringCollision::SampleResonanceMass(), G4LivermoreGammaConversionModelRC::SampleSecondaries(), G4eBremsstrahlungRelModel::SampleSecondaries(), G4eBremParametrizedModel::SampleSecondaries(), G4ICRU73QOModel::SampleSecondaries(), G4BraggModel::SampleSecondaries(), G4BraggIonModel::SampleSecondaries(), G4MuBetheBlochModel::SampleSecondaries(), G4AtimaEnergyLossModel::SampleSecondaries(), G4LindhardSorensenIonModel::SampleSecondaries(), G4BetheBlochModel::SampleSecondaries(), c2_const_ptr< G4double >::set_function(), G4INCL::Config::setAutosaveFrequency(), G4hhElastic::SetCofF2(), G4hhElastic::SetCofF3(), G4VEmProcess::SetCrossSectionBiasingFactor(), G4VEnergyLossProcess::SetCrossSectionBiasingFactor(), HistoManager::SetDefaultBeamPositionFlag(), G4MTcoutDestination::SetDefaultOutput(), G4INCL::Config::setFermiMomentumType(), G4VPrimitiveScorer::SetFilter(), G4GHEKinematicsVector::setFlag(), RE01PrimaryGeneratorAction::SetHEPEvtGenerator(), ExN04PrimaryGeneratorAction::SetHEPEvtGenerator(), G4ReactionProduct::SetMayBeKilled(), G4ReactionProduct::SetNewlyAdded(), G4VEmModel::SetParticleChange(), G4BetaPlusDecay::SetUpBetaSpectrumSampler(), G4BetaMinusDecay::SetUpBetaSpectrumSampler(), G4EmCorrections::ShellCorrection(), G4BraggModel::StoppingPower(), G4OpenInventorXtExaminerViewer::superimpositionEvent(), G4OpenInventorXtExaminerViewer::updateSpeedIndicator(), CB_G4UserSteppingAction::UserSteppingAction(), w_ZBase::VMethod(), CB_XBase::VMethodA(), CB_XBase::VMethodB(), G4eeCrossSections::Width2p(), G4eeCrossSections::WidthPg(), cheprep::BHepRepWriter::writeReal(), xDataXML_importFile2().

TH1D* hist1 = (TH1D*)f.Get("1")

advanced/amsEcal/showers/plotHisto.C 파일의 9 번째 라인에서 정의되었습니다.

다음에 의해서 참조됨 : fragmentAngularDistributionHistogram(), fragmentEnergyDistributionDifferentAngles().

TH1D* hist2 = (TH1D*)f.Get("2")

advanced/amsEcal/showers/plotHisto.C 파일의 12 번째 라인에서 정의되었습니다.

다음에 의해서 참조됨 : fragmentEnergyDistributionDifferentAngles().

TH1D* hist3 = (TH1D*)f.Get("3")

advanced/amsEcal/showers/plotHisto.C 파일의 15 번째 라인에서 정의되었습니다.

다음에 의해서 참조됨 : fragmentEnergyDistributionDifferentAngles().

TH1D* hist4 = (TH1D*)f.Get("4")

advanced/amsEcal/showers/plotHisto.C 파일의 18 번째 라인에서 정의되었습니다.

다음에 의해서 참조됨 : fragmentEnergyDistributionDifferentAngles().

TH1D* hist5 = (TH1D*)f.Get("5")

advanced/amsEcal/showers/plotHisto.C 파일의 21 번째 라인에서 정의되었습니다.

다음에 의해서 참조됨 : fragmentEnergyDistributionDifferentAngles().