Definition at line 227 of file G4Log.hh.
References fe, G4LogConsts::get_log_px(), G4LogConsts::get_log_qx(), G4LogConsts::getMantExponent(), G4LogConsts::LOG_LOWER_LIMIT, G4LogConsts::LOG_UPPER_LIMIT, G4LogConsts::SQRTH, and test::x.
Referenced by G4EnergyLossForExtrapolator::AverageScatteringAngle(), G4VEnergyLossProcess::BuildLambdaTable(), G4PairProductionRelModel::CalcLPMFunctions(), G4KleinNishinaModel::ComputeCrossSectionPerAtom(), G4KleinNishinaCompton::ComputeCrossSectionPerAtom(), G4BetheHeitlerModel::ComputeCrossSectionPerAtom(), G4UrbanMscModel::ComputeCrossSectionPerAtom(), G4eeToTwoGammaModel::ComputeCrossSectionPerElectron(), G4MollerBhabhaModel::ComputeCrossSectionPerElectron(), G4BraggIonModel::ComputeCrossSectionPerElectron(), G4ICRU73QOModel::ComputeCrossSectionPerElectron(), G4BraggModel::ComputeCrossSectionPerElectron(), G4MuBetheBlochModel::ComputeCrossSectionPerElectron(), G4BetheBlochModel::ComputeCrossSectionPerElectron(), G4MollerBhabhaModel::ComputeDEDXPerVolume(), G4BraggModel::ComputeDEDXPerVolume(), G4BraggIonModel::ComputeDEDXPerVolume(), G4ICRU73QOModel::ComputeDEDXPerVolume(), G4MuBetheBlochModel::ComputeDEDXPerVolume(), G4BetheBlochModel::ComputeDEDXPerVolume(), G4hBremsstrahlungModel::ComputeDMicroscopicCrossSection(), G4hPairProductionModel::ComputeDMicroscopicCrossSection(), G4MuBremsstrahlungModel::ComputeDMicroscopicCrossSection(), G4MuPairProductionModel::ComputeDMicroscopicCrossSection(), G4LivermoreBremsstrahlungModel::ComputeDXSectionPerAtom(), G4SeltzerBergerModel::ComputeDXSectionPerAtom(), G4GoudsmitSaundersonMscModel::ComputeGeomPathLength(), G4UrbanMscModel::ComputeGeomPathLength(), G4MuBremsstrahlungModel::ComputeMicroscopicCrossSection(), G4MuPairProductionModel::ComputeMicroscopicCrossSection(), G4UrbanMscModel::ComputeTheta0(), G4WentzelOKandVIxSection::ComputeTransportCrossSectionPerAtom(), G4WentzelVIRelXSection::ComputeTransportCrossSectionPerAtom(), G4UrbanMscModel::ComputeTruePathLengthLimit(), G4WentzelVIModel::ComputeTrueStepLength(), G4WentzelVIRelModel::ComputeTrueStepLength(), G4GoudsmitSaundersonMscModel::ComputeTrueStepLength(), G4UrbanMscModel::ComputeTrueStepLength(), G4MuPairProductionModel::ComputMuPairLoss(), G4EquilibriumEvaporator::deExcite(), G4ionEffectiveCharge::EffectiveCharge(), G4NucleiModel::fillZoneRadii(), G4InuclSpecialFunctions::G4cbrt(), G4F20GEMProbability::G4F20GEMProbability(), G4O17GEMProbability::G4O17GEMProbability(), G4PhysicsLnVector::G4PhysicsLnVector(), G4PhysicsLogVector::G4PhysicsLogVector(), G4NucleiModel::generateInteractionLength(), G4PreCompoundProton::GetOpt2(), G4mplIonisationWithDeltaModel::Initialise(), G4mplIonisationModel::Initialise(), G4MuPairProductionModel::Initialise(), G4VEmModel::InitialiseElementSelectors(), G4NucleiModel::initializeCascad(), G4SynchrotronRadiation::InvSynFracInt(), G4Pow::logX(), G4DipBustGenerator::PolarAngle(), G4VEmProcess::PostStepGetPhysicalInteractionLength(), G4VEnergyLossProcess::PostStepGetPhysicalInteractionLength(), G4InuclSpecialFunctions::randomGauss(), G4PhysicsLnVector::Retrieve(), G4PhysicsLogVector::Retrieve(), G4DipBustGenerator::SampleDirection(), G4DeltaAngle::SampleDirection(), G4RayleighAngularGenerator::SampleDirection(), G4ModifiedTsai::SampleDirection(), G4UniversalFluctuation::SampleFluctuations(), G4WentzelVIRelModel::SampleScattering(), G4WentzelVIModel::SampleScattering(), G4GoudsmitSaundersonMscModel::SampleScattering(), G4LivermoreGammaConversionModel::SampleSecondaries(), G4LivermoreComptonModel::SampleSecondaries(), G4LivermoreBremsstrahlungModel::SampleSecondaries(), G4SeltzerBergerModel::SampleSecondaries(), G4KleinNishinaModel::SampleSecondaries(), G4KleinNishinaCompton::SampleSecondaries(), G4BetheHeitlerModel::SampleSecondaries(), G4PairProductionRelModel::SampleSecondaries(), G4eBremsstrahlungRelModel::SampleSecondaries(), G4eBremParametrizedModel::SampleSecondaries(), G4eeToTwoGammaModel::SampleSecondaries(), G4MuPairProductionModel::SampleSecondaries(), G4MuBremsstrahlungModel::SampleSecondaries(), G4MuBetheBlochModel::SampleSecondaries(), G4GoudsmitSaundersonTable::SampleTheta(), G4PhysicsLnVector::ScaleVector(), G4PhysicsLogVector::ScaleVector(), G4DiscreteGammaTransition::SelectGamma(), G4IonisParamMat::SetMeanExcitationEnergy(), G4EnergyLossForExtrapolator::TrueStepLength(), and G4NucleiModel::zoneIntegralWoodsSaxon().
251 res -= fe * 2.121944400546905827679e-4;
255 res += fe * 0.693359375;
258 res = std::numeric_limits<G4double>::infinity();
260 res = - std::numeric_limits<G4double>::quiet_NaN();
G4double get_log_qx(const G4double x)
G4double getMantExponent(const G4double x, G4double &fe)
Like frexp but vectorising and the exponent is a double.
G4double get_log_px(const G4double x)
const G4double LOG_LOWER_LIMIT
const G4double LOG_UPPER_LIMIT