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Geant4
v4-10.4-release
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Geant4
v4-10.4-release
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함수 | |
| gROOT | SetStyle ("Plain") |
| gStyle | SetOptStat (0) |
변수 | |
| Int_t | ntarg = 5 |
| Int_t | npart = 4 |
| Int_t | nxs = 7 |
| Int_t | ipart = 0 |
| Int_t | itarg = 0 |
| Int_t | ixs = 0 |
| TString | axtit [3] = {"log10(E/MeV)", "Cross section (bn)","log10(p/GeV)"} |
| TString | hed [nxs] = {"Elastic","Elastic","Inelastic","Inelastic","Capture","Fission","ChargeExchange"} |
| TString | fil0 [nxs] = {"elp","el","inlp","inl","cap","fis","cex"} |
| Double_t | x1 [nxs] = {-3,-1,-3,-1,-1,-1,-1} |
| Double_t | x2 [nxs] = {5,6,5,6,6,6,6} |
| Double_t | y1 [nxs] = {0.001,0.001,0.001,0.001,0.00001,0.00001,0.0001} |
| Double_t | y2 [nxs] = {20,10,20,5,1,1,1} |
| TLegend * | leg [nxs] |
| TH1F * | hh [nxs] |
| TString | gtit |
| TString | fin |
| TFile | ff [ntarg] |
| TString | targ [ntarg] = {"H","C","Al","Fe","Pb"} |
| TString | filt [ntarg] = {"h","c","al","fe","pb"} |
| Int_t | col [ntarg] = {2, 3, 4, 5, 6} |
| TString | filp [npart] = {"p_","n_","pi+","pi-"} |
| TString | part [npart] = {"proton","neutron","#pi^{+}","#pi^{-}"} |
| gStyle SetOptStat | ( | 0 | ) |
| gROOT SetStyle | ( | "Plain" | ) |
| Int_t col[ntarg] = {2, 3, 4, 5, 6} |
Style.C 파일의 29 번째 라인에서 정의되었습니다.
다음에 의해서 참조됨 : G4tgbVolume::ConstructG4LogVol(), G4TheMTRayTracer::CreateBitMap(), G4ScoreLogColorMap::DrawColorChartBar(), G4VScoreColorMap::DrawColorChartBar(), CLHEP::RanecuEngine::further_randomize(), G03ColorReader::GetVisAttribute(), CLHEP::HepJamesRandom::HepJamesRandom(), CLHEP::MTwistEngine::MTwistEngine(), CLHEP::RanluxEngine::RanluxEngine(), CCalG4Able::setVisType().
| TFile ff[ntarg] |
Style.C 파일의 26 번째 라인에서 정의되었습니다.
다음에 의해서 참조됨 : G4PenelopeOscillatorManager::BuildOscillatorTable(), G4Abla::DeexcitationAblaxx(), G4ScreenedCoulombClassicalKinematics::DoScreeningComputation(), G4Abla::eflmac(), G4Abla::eflmac_profi(), G4Abla::evapora(), G4JTPolynomialSolver::FindRoots(), ptwXY_groupThreeFunctions(), ptwXY_groupTwoFunctions(), G4PenelopeRayleighModel::ReadDataFile(), G4LivermoreGammaConversionModelRC::SampleSecondaries(), G4ParticleHPVector::SetVerbose().
| TString hed[nxs] = {"Elastic","Elastic","Inelastic","Inelastic","Capture","Fission","ChargeExchange"} |
| Int_t ipart = 0 |
Style.C 파일의 10 번째 라인에서 정의되었습니다.
다음에 의해서 참조됨 : G4CollisionOutput::boostToLabFrame(), G4InuclEvaporation::BreakItUp(), G4HadronCrossSections::CalcScatteringCrossSections(), G4ElementaryParticleCollider::collide(), G4CascadeInterface::copyOutputToHadronicResult(), G4CascadeInterface::copyOutputToReactionProducts(), G4CascadeInterface::coulombBarrierViolation(), G4BigBanger::deExcite(), for(), G4HadronCrossSections::GetParticleCode(), G4NucleiModel::initializeCascad(), PG4gsdk(), PG4gspart(), G4IntraNucleiCascader::releaseSecondary(), G4CollisionOutput::rotateEvent().
| Int_t npart = 4 |
Style.C 파일의 7 번째 라인에서 정의되었습니다.
다음에 의해서 참조됨 : G4Pythia6Decayer::ForceParticleDecay(), G4NucleiModel::generateParticleFate(), G4CascadeInterface::retryInelasticNucleus(), G4CollisionOutput::setOnShell().
Style.C 파일의 32 번째 라인에서 정의되었습니다.
다음에 의해서 참조됨 : G4VAtomDeexcitation::AlongStepDeexcitation(), G4NuclearStopping::AlongStepDoIt(), G4eLowEnergyLoss::AlongStepDoIt(), XrayFluoAnalysisManager::analyseStepping(), G4VEmModel::ComputeDEDX(), G4TablesForExtrapolator::ComputeElectronDEDX(), G4TablesForExtrapolator::ComputeMuonDEDX(), G4TablesForExtrapolator::ComputeProtonDEDX(), G4TablesForExtrapolator::ComputeTrasportXS(), G4ThermalNeutrons::ConstructProcess(), G4HadronElasticPhysicsXS::ConstructProcess(), G4VEmModel::CrossSection(), G4ScreenedNuclearRecoil::DepositEnergy(), G4PolyconeSide::DistanceAway(), G4HadronicProcessStore::Dump(), Run::EndOfRun(), G4EmCalculator::FindEmModel(), G4EmCalculator::FindEnergyLossProcess(), G4VHadronPhysics::FindInelasticProcess(), G4EmCalculator::FindLambdaTable(), G4HadronicProcessStore::FindProcess(), XrayTelAnalysis::finish(), G4EmParametersMessenger::G4EmParametersMessenger(), G4UPiNuclearCrossSection::GetElasticCrossSection(), G4UPiNuclearCrossSection::GetInelasticCrossSection(), PhysicsList::GetRange(), G4hPairProduction::InitialiseEnergyLossProcess(), G4alphaIonisation::InitialiseEnergyLossProcess(), G4ePairProduction::InitialiseEnergyLossProcess(), G4hhIonisation::InitialiseEnergyLossProcess(), G4MuPairProduction::InitialiseEnergyLossProcess(), G4ionIonisation::InitialiseEnergyLossProcess(), G4MuIonisation::InitialiseEnergyLossProcess(), G4BohrFluctuations::InitialiseMe(), G4UniversalFluctuation::InitialiseMe(), G4AtimaFluctuations::InitialiseMe(), G4IonFluctuations::InitialiseMe(), G4DecayProducts::IsChecked(), main(), G4DecayProducts::PopProducts(), G4HadronElasticProcess::PostStepDoIt(), G4NeutrinoElectronProcess::PostStepDoIt(), G4VMultipleScattering::PreparePhysicsTable(), G4VEnergyLossProcess::PreparePhysicsTable(), G4HadronicProcessStore::Print(), MCTruthManager::PrintTree(), G4GeneratorPrecompoundInterface::Propagate(), G4GeneratorPrecompoundInterface::PropagateNuclNucl(), DicomDetectorConstruction::ReadPhantomDataFile(), DicomDetectorConstruction::ReadVoxelDensities(), DicomPartialDetectorConstruction::ReadVoxelDensitiesPartial(), G4GammaTransition::SampleTransition(), G4VEmModel::SelectRandomAtom(), G4VMscModel::SetIonisation(), G4EmConfigurator::SetModelForRegion(), G4ScreenedNuclearRecoil::SetNIELPartitionFunction(), G4UniversalFluctuation::SetParticleAndCharge(), G4AtimaFluctuations::SetParticleAndCharge(), G4IonFluctuations::SetParticleAndCharge(), G4EnergyLossForExtrapolator::SetupKinematics(), G4EnergySplitter::SplitEnergyInVolumes().
Style.C 파일의 27 번째 라인에서 정의되었습니다.
다음에 의해서 참조됨 : G4AntiNeutronAnnihilationAtRest::AntiNeutronAnnihilation(), G4QMDReaction::ApplyYourself(), G4ParticleHPInelasticCompFS::CompositeApply().
1.8.5
