G4Log.hh File Reference

#include "G4Types.hh"
#include <limits>
#include <stdint.h>

Go to the source code of this file.

Classes
union	G4LogConsts::ieee754

Namespaces
namespace	G4LogConsts

Functions
G4double	G4LogConsts::get_log_px (const G4double x)
G4double	G4LogConsts::get_log_qx (const G4double x)
uint64_t	G4LogConsts::dp2uint64 (G4double x)
G4double	G4LogConsts::uint642dp (uint64_t ll)
G4float	G4LogConsts::uint322sp (G4int x)
uint32_t	G4LogConsts::sp2uint32 (G4float x)
G4double	G4LogConsts::getMantExponent (const G4double x, G4double &fe)
	Like frexp but vectorising and the exponent is a double.
G4float	G4LogConsts::getMantExponentf (const G4float x, G4float &fe)
	Like frexp but vectorising and the exponent is a float.
G4double	G4Log (G4double x)
G4float	G4LogConsts::get_log_poly (const G4float x)
G4float	G4Logf (G4float x)
void	logv (const uint32_t size, G4double const *__restrict__ iarray, G4double *__restrict__ oarray)
void	G4Logv (const uint32_t size, G4double const *__restrict__ iarray, G4double *__restrict__ oarray)
void	logfv (const uint32_t size, G4float const *__restrict__ iarray, G4float *__restrict__ oarray)
void	G4Logfv (const uint32_t size, G4float const *__restrict__ iarray, G4float *__restrict__ oarray)

Variables
const G4double	G4LogConsts::LOG_UPPER_LIMIT = 1e307
const G4double	G4LogConsts::LOG_LOWER_LIMIT = 0
const G4double	G4LogConsts::SQRTH = 0.70710678118654752440
const G4float	G4LogConsts::MAXNUMF = 3.4028234663852885981170418348451692544e38f
const G4float	G4LogConsts::LOGF_UPPER_LIMIT = MAXNUMF
const G4float	G4LogConsts::LOGF_LOWER_LIMIT = 0
const G4float	G4LogConsts::PX1logf = 7.0376836292E-2f
const G4float	G4LogConsts::PX2logf = -1.1514610310E-1f
const G4float	G4LogConsts::PX3logf = 1.1676998740E-1f
const G4float	G4LogConsts::PX4logf = -1.2420140846E-1f
const G4float	G4LogConsts::PX5logf = 1.4249322787E-1f
const G4float	G4LogConsts::PX6logf = -1.6668057665E-1f
const G4float	G4LogConsts::PX7logf = 2.0000714765E-1f
const G4float	G4LogConsts::PX8logf = -2.4999993993E-1f
const G4float	G4LogConsts::PX9logf = 3.3333331174E-1f
const G4float	G4LogConsts::SQRTHF = 0.707106781186547524f

Function Documentation

G4Log()

G4double G4Log ( G4double  x )

inline

Definition at line 226 of file G4Log.hh.

{
  const G4double original_x = x;
 
  /* separate mantissa from exponent */
  G4double fe;
  x = G4LogConsts::getMantExponent(x, fe);
 
  // blending
  x > G4LogConsts::SQRTH ? fe += 1. : x += x;
  x -= 1.0;
 
  /* rational form */
  G4double px = G4LogConsts::get_log_px(x);
 
  // for the final formula
  const G4double x2 = x * x;
  px *= x;
  px *= x2;
 
  const G4double qx = G4LogConsts::get_log_qx(x);
 
  G4double res = px / qx;
 
  res -= fe * 2.121944400546905827679e-4;
  res -= 0.5 * x2;
 
  res = x + res;
  res += fe * 0.693359375;
 
  if(original_x > G4LogConsts::LOG_UPPER_LIMIT)
    res = std::numeric_limits<G4double>::infinity();
  if(original_x < G4LogConsts::LOG_LOWER_LIMIT)  // THIS IS NAN!
    res = -std::numeric_limits<G4double>::quiet_NaN();
 
  return res;
}

Referenced by G4PenelopeCrossSection::AddCrossSectionPoint(), G4PenelopeCrossSection::AddShellCrossSectionPoint(), G4Nucleus::AnnihilationEvaporationEffects(), G4LFission::ApplyYourself(), G4MuonMinusBoundDecay::ApplyYourself(), G4ParticleHPFissionFS::ApplyYourself(), G4EnergyLossForExtrapolator::AverageScatteringAngle(), G4EmCorrections::BarkasCorrection(), G4EmCorrections::Bethe(), G4VEnergyLossProcess::BuildLambdaTable(), G4GammaGeneralProcess::BuildPhysicsTable(), G4PenelopeBremsstrahlungFS::BuildScaledXSTable(), G4StatMFMacroBiNucleon::CalcEntropy(), G4StatMFMacroMultiNucleon::CalcEntropy(), G4StatMFMacroNucleon::CalcEntropy(), G4StatMFMacroTetraNucleon::CalcEntropy(), G4StatMFMacroTriNucleon::CalcEntropy(), G4StatMFMicroPartition::CalcPartitionProbability(), G4PreCompoundTransitions::CalculateProbability(), G4QMDCollision::CalFinalStateOfTheBinaryCollisionJQMD(), G4QuasiElRatios::ChExElCoef(), G4Reggeons::Chi_pomeron(), G4Reggeons::Chi_reggeon(), G4Nucleus::Cinema(), G4PolarizedComptonModel::ComputeAsymmetryPerAtom(), G4KleinNishinaCompton::ComputeCrossSectionPerAtom(), G4KleinNishinaModel::ComputeCrossSectionPerAtom(), G4PenelopeGammaConversionModel::ComputeCrossSectionPerAtom(), G4PenelopePhotoElectricModel::ComputeCrossSectionPerAtom(), G4PenelopeRayleighModel::ComputeCrossSectionPerAtom(), G4PenelopeRayleighModelMI::ComputeCrossSectionPerAtom(), G4BetheHeitlerModel::ComputeCrossSectionPerAtom(), G4UrbanAdjointMscModel::ComputeCrossSectionPerAtom(), G4UrbanMscModel::ComputeCrossSectionPerAtom(), G4GammaConversionToMuons::ComputeCrossSectionPerAtom(), G4MuBetheBlochModel::ComputeCrossSectionPerElectron(), G4AtimaEnergyLossModel::ComputeCrossSectionPerElectron(), G4BetheBlochModel::ComputeCrossSectionPerElectron(), G4BraggIonModel::ComputeCrossSectionPerElectron(), G4BraggModel::ComputeCrossSectionPerElectron(), G4LindhardSorensenIonModel::ComputeCrossSectionPerElectron(), G4MollerBhabhaModel::ComputeCrossSectionPerElectron(), G4ICRU73QOModel::ComputeCrossSectionPerElectron(), G4eeToTwoGammaModel::ComputeCrossSectionPerElectron(), G4eplusTo2GammaOKVIModel::ComputeCrossSectionPerElectron(), G4eplusTo3GammaOKVIModel::ComputeCrossSectionPerElectron(), G4ComponentGGHadronNucleusXsc::ComputeCrossSections(), G4eDPWAElasticDCS::ComputeCSPerAtom(), G4KokoulinMuonNuclearXS::ComputeDDMicroscopicCrossSection(), G4MuBetheBlochModel::ComputeDEDXPerVolume(), G4BetheBlochModel::ComputeDEDXPerVolume(), G4BraggIonModel::ComputeDEDXPerVolume(), G4BraggModel::ComputeDEDXPerVolume(), G4LindhardSorensenIonModel::ComputeDEDXPerVolume(), G4MollerBhabhaModel::ComputeDEDXPerVolume(), G4ICRU73QOModel::ComputeDEDXPerVolume(), G4MuBremsstrahlungModel::ComputeDMicroscopicCrossSection(), G4hBremsstrahlungModel::ComputeDMicroscopicCrossSection(), G4MuPairProductionModel::ComputeDMicroscopicCrossSection(), G4LivermoreBremsstrahlungModel::ComputeDXSectionPerAtom(), G4SeltzerBergerModel::ComputeDXSectionPerAtom(), G4eplusTo3GammaOKVIModel::ComputeF(), G4eplusTo3GammaOKVIModel::ComputeF0(), G4UrbanAdjointMscModel::ComputeGeomPathLength(), G4UrbanMscModel::ComputeGeomPathLength(), G4MuBremsstrahlungModel::ComputeMicroscopicCrossSection(), G4MuPairProductionModel::ComputeMicroscopicCrossSection(), G4PairProductionRelModel::ComputeParametrizedXSectionPerAtom(), G4PairProductionRelModel::ComputePhi12(), G4eDPWAElasticDCS::ComputeScatteringPowerCorrection(), G4GoudsmitSaundersonTable::ComputeScatteringPowerCorrection(), G4UrbanAdjointMscModel::ComputeTheta0(), G4UrbanMscModel::ComputeTheta0(), G4WentzelOKandVIxSection::ComputeTransportCrossSectionPerAtom(), G4GoudsmitSaundersonMscModel::ComputeTruePathLengthLimit(), G4UrbanAdjointMscModel::ComputeTruePathLengthLimit(), G4UrbanMscModel::ComputeTruePathLengthLimit(), G4GoudsmitSaundersonMscModel::ComputeTrueStepLength(), G4UrbanAdjointMscModel::ComputeTrueStepLength(), G4UrbanMscModel::ComputeTrueStepLength(), G4WentzelVIModel::ComputeTrueStepLength(), G4MuPairProductionModel::ComputMuPairLoss(), G4NuclNuclDiffuseElastic::CoulombAmplitude(), G4DiffractiveExcitation::CreateStrings(), G4AngularDistribution::Cross(), G4XPDGElastic::CrossSection(), G4XpimNTotal::CrossSection(), G4XpipNTotal::CrossSection(), G4LowEXsection::CrossSection(), G4GoudsmitSaundersonMscModel::CrossSectionPerVolume(), G4VEmProcess::CrossSectionPerVolume(), G4EmCorrections::DensityCorrection(), G4AtimaFluctuations::Dispersion(), G4ionEffectiveCharge::EffectiveCharge(), G4LegendrePolynomial::EvalAssocLegendrePoly(), G4Nucleus::EvaporationEffects(), G4QuasiElRatios::FetchElTot(), G4NucleiModel::fillZoneRadii(), G4JTPolynomialSolver::FindRoots(), G4InuclSpecialFunctions::G4cbrt(), G4ElasticHadrNucleusHE::G4ElasticHadrNucleusHE(), G4F20GEMProbability::G4F20GEMProbability(), G4GSMottCorrection::G4GSMottCorrection(), G4GSPWACorrections::G4GSPWACorrections(), G4NeutronCaptureXS::G4NeutronCaptureXS(), G4O17GEMProbability::G4O17GEMProbability(), G4PenelopeRayleighModel::G4PenelopeRayleighModel(), G4PenelopeRayleighModelMI::G4PenelopeRayleighModelMI(), G4PhysicsLogVector::G4PhysicsLogVector(), G4FPYSamplingOps::G4SampleWatt(), G4VEmProcess::G4VEmProcess(), G4VEnergyLossProcess::G4VEnergyLossProcess(), G4XNNElasticLowE::G4XNNElasticLowE(), G4XnpElasticLowE::G4XnpElasticLowE(), G4XnpTotalLowE::G4XnpTotalLowE(), G4NuclNuclDiffuseElastic::GammaLogB2n(), G4eeToHadronsModel::GenerateCMPhoton(), G4NucleiModel::generateInteractionLength(), G4RPGReaction::GenerateNBodyEvent(), G4RPGReaction::GenerateNBodyEventT(), G4ComponentAntiNuclNuclearXS::GetAntiHadronNucleonElCrSc(), G4ComponentAntiNuclNuclearXS::GetAntiHadronNucleonTotCrSc(), G4hhElastic::GetAqq(), G4hhElastic::GetAQQ(), G4ParticleHPInterpolator::GetBinIntegral(), G4QuasiElRatios::GetChExFactor(), G4LindhardSorensenData::GetDeltaL(), G4PenelopeIonisationXSHandler::GetDensityCorrection(), G4IonisParamMat::GetDensityCorrection(), G4PhotoNuclearCrossSection::GetElementCrossSection(), G4ElectroNuclearCrossSection::GetElementCrossSection(), G4ElectroNuclearCrossSection::GetEquivalentPhotonEnergy(), G4ElectroNuclearCrossSection::GetEquivalentPhotonQ2(), G4ChipsAntiBaryonElasticXS::GetExchangeT(), G4ChipsHyperonElasticXS::GetExchangeT(), G4ChipsPionMinusElasticXS::GetExchangeT(), G4ChipsPionPlusElasticXS::GetExchangeT(), G4RKFieldIntegrator::GetExcitationEnergy(), G4GoudsmitSaundersonTable::GetGSAngularDtr(), G4NuclNuclDiffuseElastic::GetHadronNucleonXscNS(), G4PenelopeCrossSection::GetHardCrossSection(), G4ComponentAntiNuclNuclearXS::GetInelasticElementCrossSection(), G4IonProtonCrossSection::GetIsoCrossSection(), G4PhotoNuclearCrossSection::GetIsoCrossSection(), G4ParticleHPKallbachMannSyst::GetKallbachZero(), G4VEmProcess::GetLambda(), G4PenelopeBremsstrahlungFS::GetMomentumIntegral(), G4RPGInelastic::GetNormalizationConstant(), G4PenelopeCrossSection::GetNormalizedShellCrossSection(), 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G4AntiNuclElastic::SampleInvariantT(), G4HadronElastic::SampleInvariantT(), G4EvaporationProbability::SampleKineticEnergy(), G4GoudsmitSaundersonMscModel::SampleMSC(), G4NeutrinoNucleusModel::SampleQkr(), G4VLongitudinalStringDecay::SampleQuarkPt(), G4KineticTrack::SampleResidualLifetime(), G4WentzelVIModel::SampleScattering(), G4LivermoreBremsstrahlungModel::SampleSecondaries(), G4eBremParametrizedModel::SampleSecondaries(), G4eBremsstrahlungRelModel::SampleSecondaries(), G4BoldyshevTripletModel::SampleSecondaries(), G4LivermoreComptonModel::SampleSecondaries(), G4LivermoreComptonModifiedModel::SampleSecondaries(), G4LivermoreGammaConversionModelRC::SampleSecondaries(), G4LivermoreNuclearGammaConversionModel::SampleSecondaries(), G4LivermorePolarizedComptonModel::SampleSecondaries(), G4PenelopeComptonModel::SampleSecondaries(), G4HeatedKleinNishinaCompton::SampleSecondaries(), G4MuBetheBlochModel::SampleSecondaries(), G4MuBremsstrahlungModel::SampleSecondaries(), 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G4Logf()

G4float G4Logf ( G4float  x )

inline

Definition at line 307 of file G4Log.hh.

{
  const G4float original_x = x;
 
  G4float fe;
  x = G4LogConsts::getMantExponentf(x, fe);
 
  x > G4LogConsts::SQRTHF ? fe += 1.f : x += x;
  x -= 1.0f;
 
  const G4float x2 = x * x;
 
  G4float res = G4LogConsts::get_log_poly(x);
  res *= x2 * x;
 
  res += -2.12194440e-4f * fe;
  res += -0.5f * x2;
 
  res = x + res;
 
  res += 0.693359375f * fe;
 
  if(original_x > G4LogConsts::LOGF_UPPER_LIMIT)
    res = std::numeric_limits<G4float>::infinity();
  if(original_x < G4LogConsts::LOGF_LOWER_LIMIT)
    res = -std::numeric_limits<G4float>::quiet_NaN();
 
  return res;
}

G4Logfv()

void G4Logfv	(	const uint32_t	size,
		G4float const *__restrict__	iarray,
		G4float *__restrict__	oarray
	)

G4Logv()

void G4Logv	(	const uint32_t	size,
		G4double const *__restrict__	iarray,
		G4double *__restrict__	oarray
	)

logfv()

void logfv	(	const uint32_t	size,
		G4float const *__restrict__	iarray,
		G4float *__restrict__	oarray
	)

logv()

void logv	(	const uint32_t	size,
		G4double const *__restrict__	iarray,
		G4double *__restrict__	oarray
	)