G4INCL::KinematicsUtils 네임스페이스 참조

함수
void	transformToLocalEnergyFrame (Nucleus const *const n, Particle *const p)
G4double	getLocalEnergy (Nucleus const *const n, Particle *const p)
ThreeVector	makeBoostVector (Particle const *const p1, Particle const *const p2)
G4double	totalEnergyInCM (Particle const *const p1, Particle const *const p2)
G4double	squareTotalEnergyInCM (Particle const *const p1, Particle const *const p2)
G4double	momentumInCM (Particle const *const p1, Particle const *const p2)
	gives the momentum in the CM frame of two particles. 더 자세히 ...
G4double	momentumInCM (const G4double E, const G4double M1, const G4double M2)
G4double	momentumInLab (Particle const *const p1, Particle const *const p2)
	gives the momentum in the lab frame of two particles. 더 자세히 ...
G4double	momentumInLab (const G4double s, const G4double m1, const G4double m2)
G4double	sumTotalEnergies (const ParticleList &)
ThreeVector	sumMomenta (const ParticleList &)
G4double	energy (const ThreeVector &p, const G4double m)
G4double	invariantMass (const G4double E, const ThreeVector &p)
G4double	squareInvariantMass (const G4double E, const ThreeVector &p)
G4double	gammaFromKineticEnergy (const ParticleSpecies &p, const G4double EKin)

함수 문서화

G4double G4INCL::KinematicsUtils::energy	(	const ThreeVector &	p,
		const G4double	m
	)

G4INCLKinematicsUtils.cc 파일의 158 번째 라인에서 정의되었습니다.

다음을 참조함 : m, G4INCL::ThreeVector::mag2().

G4double G4INCL::KinematicsUtils::gammaFromKineticEnergy	(	const ParticleSpecies &	p,
		const G4double	EKin
	)

G4INCLKinematicsUtils.cc 파일의 170 번째 라인에서 정의되었습니다.

다음을 참조함 : G4INCL::Composite, G4INCL::ParticleTable::getTableMass, G4INCL::ParticleTable::getTableParticleMass, G4INCL::ParticleSpecies::theA, G4INCL::ParticleSpecies::theType, G4INCL::ParticleSpecies::theZ.

G4double G4INCL::KinematicsUtils::getLocalEnergy	(	Nucleus const *const	n,
		Particle *const	p
	)

G4INCLKinematicsUtils.cc 파일의 53 번째 라인에서 정의되었습니다.

다음을 참조함 : G4INCL::Nucleus::getDensity(), G4INCL::NuclearPotential::INuclearPotential::getFermiMomentum(), G4INCL::Particle::getKineticEnergy(), G4INCL::Particle::getMass(), G4INCL::NuclearDensity::getMaximumRadius(), G4INCL::NuclearDensity::getMaxRFromP(), G4INCL::NuclearDensity::getMinPFromR(), G4INCL::Particle::getMomentum(), G4INCL::Particle::getPosition(), G4INCL::Nucleus::getPotential(), G4INCL::Particle::getPotentialEnergy(), G4INCL::Particle::getReflectionMomentum(), G4INCL::NuclearPotential::INuclearPotential::getSeparationEnergy(), G4INCL::Particle::getType(), G4INCL::Nucleus::getUniverseRadius(), INCL_WARN, G4INCL::ThreeVector::mag(), G4INCL::Particle::print().

다음에 의해서 참조됨 : G4INCL::InteractionAvatar::ViolationEMomentumFunctor::scaleParticleMomenta(), G4INCL::InteractionAvatar::ViolationEEnergyFunctor::setParticleEnergy(), transformToLocalEnergyFrame().

G4double G4INCL::KinematicsUtils::invariantMass	(	const G4double	E,
		const ThreeVector &	p
	)

G4INCLKinematicsUtils.cc 파일의 162 번째 라인에서 정의되었습니다.

다음을 참조함 : squareInvariantMass().

다음에 의해서 참조됨 : G4INCL::ClusteringModelIntercomparison::findClusterStartingFrom().

ThreeVector G4INCL::KinematicsUtils::makeBoostVector	(	Particle const *const	p1,
		Particle const *const	p2
	)

G4INCLKinematicsUtils.cc 파일의 89 번째 라인에서 정의되었습니다.

다음을 참조함 : G4INCL::Particle::getEnergy(), G4INCL::Particle::getMomentum().

다음에 의해서 참조됨 : G4INCL::InteractionAvatar::preInteraction(), squareTotalEnergyInCM().

G4double G4INCL::KinematicsUtils::momentumInCM	(	Particle const *const	p1,
		Particle const *const	p2
	)

gives the momentum in the CM frame of two particles.

The formula is the following:

\[ p_{CM}^2 = \frac{z^2 - m_1^2 m_2^2}{2 z + m_1^2 + m_2^2} \]

where \(z\) is the scalar product of the momentum four-vectors:

\[ z = E_1 E_2 - \vec{p}_1\cdot\vec{p}_2 \]

매개변수

p1	pointer to particle 1
p2	pointer to particle 2

반환값

the absolute value of the momentum of any of the two particles in the CM frame, in MeV/c.

G4INCLKinematicsUtils.cc 파일의 107 번째 라인에서 정의되었습니다.

다음을 참조함 : G4INCL::ThreeVector::dot(), G4INCL::Particle::getEnergy(), G4INCL::Particle::getMass(), G4INCL::Particle::getMomentum(), INCL_ERROR, z.

다음에 의해서 참조됨 : G4INCL::DeltaDecayChannel::computeDecayTime(), G4INCL::PhaseSpaceRauboldLynch::computeMaximumWeightNaive(), G4INCL::Nucleus::computeOneNucleonRecoilKinematics(), G4INCL::PhaseSpaceRauboldLynch::computeWeight(), G4INCL::Nucleus::decayOutgoingDeltas(), G4INCL::Nucleus::decayOutgoingPionResonances(), G4INCL::Nucleus::decayOutgoingSigmaZero(), G4INCL::CrossSectionsMultiPionsAndResonances::etaNToPiN(), G4INCL::NKbToNKbChannel::fillFinalState(), G4INCL::NKbToSpiChannel::fillFinalState(), G4INCL::NYElasticChannel::fillFinalState(), G4INCL::NKElasticChannel::fillFinalState(), G4INCL::NKToNKChannel::fillFinalState(), G4INCL::NpiToLKChannel::fillFinalState(), G4INCL::NpiToSKChannel::fillFinalState(), G4INCL::NKbToLpiChannel::fillFinalState(), G4INCL::DeltaProductionChannel::fillFinalState(), G4INCL::StrangeAbsorbtionChannel::fillFinalState(), G4INCL::DeltaDecayChannel::fillFinalState(), G4INCL::SigmaZeroDecayChannel::fillFinalState(), G4INCL::PionResonanceDecayChannel::fillFinalState(), G4INCL::RecombinationChannel::fillFinalState(), G4INCL::PhaseSpaceKopylov::generate(), G4INCL::NKbElasticChannel::KaonMomentum(), G4INCL::CrossSectionsMultiPionsAndResonances::omegaNToPiN().

G4double G4INCL::KinematicsUtils::momentumInCM	(	const G4double	E,
		const G4double	M1,
		const G4double	M2
	)

G4INCLKinematicsUtils.cc 파일의 119 번째 라인에서 정의되었습니다.

다음을 참조함 : E.

G4double G4INCL::KinematicsUtils::momentumInLab	(	Particle const *const	p1,
		Particle const *const	p2
	)

gives the momentum in the lab frame of two particles.

Assumes particle 1 carries all the momentum and particle 2 is at rest.

The formula is the following:

\[ p_{lab}^2 = \frac{s^2 - 2 s (m_1^2 + m_2^2) + {(m_1^2 - m_2^2)}^2}{4 m_2^2} \]

매개변수

p1	pointer to particle 1
p2	pointer to particle 2

반환값

the absolute value of the momentum of particle 1 in the lab frame, in MeV/c

G4INCLKinematicsUtils.cc 파일의 135 번째 라인에서 정의되었습니다.

다음을 참조함 : G4INCL::Particle::getMass(), m2, squareTotalEnergyInCM().

다음에 의해서 참조됨 : G4INCL::CrossSectionsINCL46::elasticNNLegacy(), G4INCL::CrossSectionsMultiPionsAndResonances::etaNElastic(), G4INCL::CrossSectionsMultiPionsAndResonances::etaNToPiN(), G4INCL::CrossSectionsMultiPionsAndResonances::etaNToPiPiN(), G4INCL::NNToMissingStrangenessChannel::fillFinalState(), G4INCL::NpiToMissingStrangenessChannel::fillFinalState(), G4INCL::EtaNElasticChannel::fillFinalState(), G4INCL::EtaNToPiNChannel::fillFinalState(), G4INCL::DeltaProductionChannel::fillFinalState(), G4INCL::ElasticChannel::fillFinalState(), G4INCL::NKbToSpiChannel::KaonMomentum(), G4INCL::NpiToLKChannel::KaonMomentum(), G4INCL::NKbToNKbChannel::KaonMomentum(), G4INCL::NpiToSKChannel::KaonMomentum(), G4INCL::NKbToLpiChannel::KaonMomentum(), G4INCL::NKbElasticChannel::KaonMomentum(), G4INCL::CrossSectionsINCL46::NDeltaToNN(), G4INCL::CrossSectionsStrangeness::NKbelastic(), G4INCL::CrossSectionsStrangeness::NKbToNKb(), G4INCL::CrossSectionsStrangeness::NKbToNKb2pi(), G4INCL::CrossSectionsStrangeness::NKbToNKbpi(), G4INCL::CrossSectionsStrangeness::NKbToS2pi(), G4INCL::CrossSectionsStrangeness::NKbToSpi(), G4INCL::CrossSectionsStrangeness::NKelastic(), G4INCL::CrossSectionsStrangeness::NKToNK(), G4INCL::CrossSectionsStrangeness::NKToNK2pi(), G4INCL::CrossSectionsStrangeness::NKToNKpi(), G4INCL::CrossSectionsStrangeness::NLToNS(), G4INCL::CrossSectionsMultiPions::NNElastic(), G4INCL::CrossSectionsMultiPions::NNElasticFixed(), G4INCL::CrossSectionsMultiPions::NNOnePiOrDelta(), G4INCL::CrossSectionsMultiPions::NNThreePi(), G4INCL::CrossSectionsStrangeness::NNToMissingStrangeness(), G4INCL::CrossSectionsINCL46::NNToNDelta(), G4INCL::CrossSectionsStrangeness::NNToNLK(), G4INCL::CrossSectionsStrangeness::NNToNSK(), G4INCL::CrossSectionsMultiPions::NNTotFixed(), G4INCL::CrossSectionsMultiPions::NNTwoPi(), G4INCL::CrossSectionsStrangeness::NpiToLK2pi(), G4INCL::CrossSectionsStrangeness::NpiToLKpi(), G4INCL::CrossSectionsStrangeness::NpiToMissingStrangeness(), G4INCL::CrossSectionsStrangeness::NpiToNKKb(), G4INCL::CrossSectionsStrangeness::NpiToSK2pi(), G4INCL::CrossSectionsStrangeness::NpiToSKpi(), G4INCL::CrossSectionsStrangeness::NSToNL(), G4INCL::CrossSectionsStrangeness::NSToNS(), G4INCL::CrossSectionsStrangeness::NYelastic(), G4INCL::CrossSectionsMultiPionsAndResonances::omegaNElastic(), G4INCL::CrossSectionsMultiPionsAndResonances::omegaNInelastic(), G4INCL::CrossSectionsMultiPionsAndResonances::omegaNToPiN(), G4INCL::CrossSectionsStrangeness::p_kmToL_pp_pm(), G4INCL::CrossSectionsStrangeness::p_kmToL_pz(), G4INCL::CrossSectionsStrangeness::p_pimToLK0(), G4INCL::CrossSectionsStrangeness::p_pimToSmKp(), G4INCL::CrossSectionsStrangeness::p_pimToSzKz(), G4INCL::CrossSectionsStrangeness::p_pipToSpKp(), G4INCL::CrossSectionsStrangeness::p_pizToSzKp(), G4INCL::CrossSectionsMultiPions::piMinuspIne(), G4INCL::CrossSectionsMultiPions::piMinuspOnePi(), G4INCL::CrossSectionsMultiPionsAndResonances::piMinuspToEtaN(), G4INCL::CrossSectionsMultiPionsAndResonances::piMinuspToOmegaN(), G4INCL::CrossSectionsMultiPions::piMinuspTwoPi(), G4INCL::CrossSectionsMultiPions::piNIne(), G4INCL::CrossSectionsMultiPions::piNOnePi(), G4INCL::CrossSectionsMultiPions::piNToxPiN(), G4INCL::CrossSectionsMultiPions::piNTwoPi(), G4INCL::CrossSectionsMultiPions::piPluspIne(), G4INCL::CrossSectionsMultiPions::piPluspOnePi(), G4INCL::CrossSectionsMultiPions::piPluspTwoPi().

G4double G4INCL::KinematicsUtils::momentumInLab	(	const G4double	s,
		const G4double	m1,
		const G4double	m2
	)

G4INCLKinematicsUtils.cc 파일의 124 번째 라인에서 정의되었습니다.

다음을 참조함 : INCL_ERROR, m2.

G4double G4INCL::KinematicsUtils::squareInvariantMass	(	const G4double	E,
		const ThreeVector &	p
	)

G4INCLKinematicsUtils.cc 파일의 166 번째 라인에서 정의되었습니다.

다음을 참조함 : G4INCL::ThreeVector::mag2().

다음에 의해서 참조됨 : invariantMass().

G4double G4INCL::KinematicsUtils::squareTotalEnergyInCM	(	Particle const *const	p1,
		Particle const *const	p2
	)

G4INCLKinematicsUtils.cc 파일의 98 번째 라인에서 정의되었습니다.

다음을 참조함 : G4INCL::Particle::getEnergy(), INCL_ERROR, G4INCL::ThreeVector::mag2(), makeBoostVector().

다음에 의해서 참조됨 : G4INCL::CrossSectionsINCL46::elasticNNLegacy(), G4INCL::ElasticChannel::fillFinalState(), G4INCL::StandardPropagationModel::generateBinaryCollisionAvatar(), G4INCL::BinaryCollisionAvatar::getChannel(), momentumInLab(), G4INCL::CrossSectionsStrangeness::NDeltaToDeltaLK(), G4INCL::CrossSectionsStrangeness::NDeltaToDeltaSK(), G4INCL::CrossSectionsStrangeness::NDeltaToNLK(), G4INCL::CrossSectionsINCL46::NDeltaToNN(), G4INCL::CrossSectionsMultiPions::NDeltaToNN(), G4INCL::CrossSectionsStrangeness::NDeltaToNSK(), G4INCL::CrossSectionsMultiPions::NNElastic(), G4INCL::CrossSectionsMultiPions::NNFourPi(), G4INCL::CrossSectionsMultiPions::NNTot(), totalEnergyInCM().

ThreeVector G4INCL::KinematicsUtils::sumMomenta

(

const ParticleList &

pl

)

G4INCLKinematicsUtils.cc 파일의 150 번째 라인에서 정의되었습니다.

다음을 참조함 : e.

G4double G4INCL::KinematicsUtils::sumTotalEnergies

(

const ParticleList &

pl

)

G4INCLKinematicsUtils.cc 파일의 142 번째 라인에서 정의되었습니다.

다음을 참조함 : E, e.

G4double G4INCL::KinematicsUtils::totalEnergyInCM	(	Particle const *const	p1,
		Particle const *const	p2
	)

G4INCLKinematicsUtils.cc 파일의 94 번째 라인에서 정의되었습니다.

다음을 참조함 : squareTotalEnergyInCM().

다음에 의해서 참조됨 : G4INCL::CrossSectionsMultiPionsAndResonances::etaNToPiN(), G4INCL::EtaNToPiPiNChannel::fillFinalState(), G4INCL::NNToNSKChannel::fillFinalState(), G4INCL::NNToNSKpiChannel::fillFinalState(), G4INCL::PiNToEtaChannel::fillFinalState(), G4INCL::NpiToLK2piChannel::fillFinalState(), G4INCL::NpiToLKpiChannel::fillFinalState(), G4INCL::NpiToMissingStrangenessChannel::fillFinalState(), G4INCL::NpiToNKKbChannel::fillFinalState(), G4INCL::NpiToSK2piChannel::fillFinalState(), G4INCL::NpiToSKpiChannel::fillFinalState(), G4INCL::NSToNLChannel::fillFinalState(), G4INCL::NSToNSChannel::fillFinalState(), G4INCL::OmegaNToPiPiNChannel::fillFinalState(), G4INCL::PiNToMultiPionsChannel::fillFinalState(), G4INCL::NDeltaToDeltaLKChannel::fillFinalState(), G4INCL::NNToNSK2piChannel::fillFinalState(), G4INCL::NDeltaToDeltaSKChannel::fillFinalState(), G4INCL::NDeltaToNLKChannel::fillFinalState(), G4INCL::NDeltaToNNKKbChannel::fillFinalState(), G4INCL::NNToNLKpiChannel::fillFinalState(), G4INCL::NDeltaToNSKChannel::fillFinalState(), G4INCL::NKbToL2piChannel::fillFinalState(), G4INCL::NKbToNKb2piChannel::fillFinalState(), G4INCL::NNToMissingStrangenessChannel::fillFinalState(), G4INCL::NKbToNKbpiChannel::fillFinalState(), G4INCL::NKbToS2piChannel::fillFinalState(), G4INCL::NKToNK2piChannel::fillFinalState(), G4INCL::NKToNKpiChannel::fillFinalState(), G4INCL::NLToNSChannel::fillFinalState(), G4INCL::NNEtaToMultiPionsChannel::fillFinalState(), G4INCL::NNOmegaToMultiPionsChannel::fillFinalState(), G4INCL::NNToMultiPionsChannel::fillFinalState(), G4INCL::NNToNLK2piChannel::fillFinalState(), G4INCL::NNToNLKChannel::fillFinalState(), G4INCL::NNToNNEtaChannel::fillFinalState(), G4INCL::NNToNNKKbChannel::fillFinalState(), G4INCL::NNToNNOmegaChannel::fillFinalState(), G4INCL::DeltaProductionChannel::fillFinalState(), G4INCL::NDeltaEtaProductionChannel::fillFinalState(), G4INCL::StrangeAbsorbtionChannel::fillFinalState(), G4INCL::NDeltaOmegaProductionChannel::fillFinalState(), G4INCL::RecombinationChannel::fillFinalState(), G4INCL::CrossSectionsStrangeness::NDeltaToNNKKb(), G4INCL::CrossSectionsMultiPions::NNOnePi(), G4INCL::CrossSectionsMultiPions::NNOnePiOrDelta(), G4INCL::CrossSectionsMultiPions::NNThreePi(), G4INCL::CrossSectionsINCL46::NNToNDelta(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNDeltaEta(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNDeltaOmega(), G4INCL::CrossSectionsStrangeness::NNToNLK2pi(), G4INCL::CrossSectionsStrangeness::NNToNLKpi(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNEta(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNEtaExclu(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNEtaFourPi(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNEtaOnePi(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNEtaOnePiOrDelta(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNEtaThreePi(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNEtaTwoPi(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNEtaxPi(), G4INCL::CrossSectionsStrangeness::NNToNNKKb(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNOmega(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNOmegaExclu(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNOmegaFourPi(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNOmegaOnePi(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNOmegaOnePiOrDelta(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNOmegaThreePi(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNOmegaTwoPi(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNNOmegaxPi(), G4INCL::CrossSectionsStrangeness::NNToNSK2pi(), G4INCL::CrossSectionsStrangeness::NNToNSKpi(), G4INCL::CrossSectionsMultiPions::NNTwoPi(), G4INCL::CrossSectionsMultiPionsAndResonances::omegaNToPiN(), G4INCL::CrossSectionsMultiPionsAndResonances::piMinuspToEtaN(), G4INCL::CrossSectionsMultiPionsAndResonances::piMinuspToOmegaN(), G4INCL::CrossSectionsINCL46::piNToDelta(), G4INCL::CrossSectionsMultiPions::piNToDelta(), G4INCL::CrossSectionsMultiPions::piNTot().

void G4INCL::KinematicsUtils::transformToLocalEnergyFrame	(	Nucleus const *const	n,
		Particle *const	p
	)

G4INCLKinematicsUtils.cc 파일의 45 번째 라인에서 정의되었습니다.

다음을 참조함 : G4INCL::Particle::adjustMomentumFromEnergy(), G4INCL::Particle::getEnergy(), getLocalEnergy(), G4INCL::Particle::setEnergy().

다음에 의해서 참조됨 : G4INCL::StandardPropagationModel::generateBinaryCollisionAvatar(), G4INCL::InteractionAvatar::preInteractionLocalEnergy().