Geant4 10.7.0
Toolkit for the simulation of the passage of particles through matter
Loading...
Searching...
No Matches
Public Member Functions | Static Public Member Functions | Static Public Attributes | Protected Member Functions | Protected Attributes | List of all members
G4INCL::Particle Class Reference

#include <G4INCLParticle.hh>

+ Inheritance diagram for G4INCL::Particle:

Public Member Functions

 Particle ()
 
 Particle (ParticleType t, G4double energy, ThreeVector const &momentum, ThreeVector const &position)
 
 Particle (ParticleType t, ThreeVector const &momentum, ThreeVector const &position)
 
virtual ~Particle ()
 
 Particle (const Particle &rhs)
 Copy constructor.
 
Particle & operator= (const Particle &rhs)
 Assignment operator.
 
G4INCL::ParticleType getType () const
 
virtual G4INCL::ParticleSpecies getSpecies () const
 Get the particle species.
 
void setType (ParticleType t)
 
G4bool isNucleon () const
 
ParticipantType getParticipantType () const
 
void setParticipantType (ParticipantType const p)
 
G4bool isParticipant () const
 
G4bool isTargetSpectator () const
 
G4bool isProjectileSpectator () const
 
virtual void makeParticipant ()
 
virtual void makeTargetSpectator ()
 
virtual void makeProjectileSpectator ()
 
G4bool isPion () const
 Is this a pion?
 
G4bool isEta () const
 Is this an eta?
 
G4bool isOmega () const
 Is this an omega?
 
G4bool isEtaPrime () const
 Is this an etaprime?
 
G4bool isPhoton () const
 Is this a photon?
 
G4bool isResonance () const
 Is it a resonance?
 
G4bool isDelta () const
 Is it a Delta?
 
G4bool isSigma () const
 Is this a Sigma?
 
G4bool isKaon () const
 Is this a Kaon?
 
G4bool isAntiKaon () const
 Is this an antiKaon?
 
G4bool isLambda () const
 Is this a Lambda?
 
G4bool isNucleonorLambda () const
 Is this a Nucleon or a Lambda?
 
G4bool isHyperon () const
 Is this an Hyperon?
 
G4bool isMeson () const
 Is this a Meson?
 
G4bool isBaryon () const
 Is this a Baryon?
 
G4bool isStrange () const
 Is this an Strange?
 
G4int getA () const
 Returns the baryon number.
 
G4int getZ () const
 Returns the charge number.
 
G4int getS () const
 Returns the strangeness number.
 
G4double getBeta () const
 
ThreeVector boostVector () const
 
void boost (const ThreeVector &aBoostVector)
 
void lorentzContract (const ThreeVector &aBoostVector, const ThreeVector &refPos)
 Lorentz-contract the particle position around some center.
 
G4double getMass () const
 Get the cached particle mass.
 
G4double getINCLMass () const
 Get the INCL particle mass.
 
virtual G4double getTableMass () const
 Get the tabulated particle mass.
 
G4double getRealMass () const
 Get the real particle mass.
 
void setRealMass ()
 Set the mass of the Particle to its real mass.
 
void setTableMass ()
 Set the mass of the Particle to its table mass.
 
void setINCLMass ()
 Set the mass of the Particle to its table mass.
 
G4double getEmissionQValueCorrection (const G4int AParent, const G4int ZParent) const
 Computes correction on the emission Q-value.
 
G4double getTransferQValueCorrection (const G4int AFrom, const G4int ZFrom, const G4int ATo, const G4int ZTo) const
 Computes correction on the transfer Q-value.
 
G4double getEmissionQValueCorrection (const G4int AParent, const G4int ZParent, const G4int SParent) const
 Computes correction on the emission Q-value for hypernuclei.
 
G4double getTransferQValueCorrection (const G4int AFrom, const G4int ZFrom, const G4int SFrom, const G4int ATo, const G4int ZTo, const G4int STo) const
 Computes correction on the transfer Q-value for hypernuclei.
 
G4double getInvariantMass () const
 Get the the particle invariant mass.
 
G4double getKineticEnergy () const
 Get the particle kinetic energy.
 
G4double getPotentialEnergy () const
 Get the particle potential energy.
 
void setPotentialEnergy (G4double v)
 Set the particle potential energy.
 
G4double getEnergy () const
 
void setMass (G4double mass)
 
void setEnergy (G4double energy)
 
const G4INCL::ThreeVector & getMomentum () const
 
virtual G4INCL::ThreeVector getAngularMomentum () const
 
virtual void setMomentum (const G4INCL::ThreeVector &momentum)
 
const G4INCL::ThreeVector & getPosition () const
 
virtual void setPosition (const G4INCL::ThreeVector &position)
 
G4double getHelicity ()
 
void setHelicity (G4double h)
 
void propagate (G4double step)
 
G4int getNumberOfCollisions () const
 Return the number of collisions undergone by the particle.
 
void setNumberOfCollisions (G4int n)
 Set the number of collisions undergone by the particle.
 
void incrementNumberOfCollisions ()
 Increment the number of collisions undergone by the particle.
 
G4int getNumberOfDecays () const
 Return the number of decays undergone by the particle.
 
void setNumberOfDecays (G4int n)
 Set the number of decays undergone by the particle.
 
void incrementNumberOfDecays ()
 Increment the number of decays undergone by the particle.
 
void setOutOfWell ()
 Mark the particle as out of its potential well.
 
G4bool isOutOfWell () const
 Check if the particle is out of its potential well.
 
void setEmissionTime (G4double t)
 
G4double getEmissionTime ()
 
ThreeVector getTransversePosition () const
 Transverse component of the position w.r.t. the momentum.
 
ThreeVector getLongitudinalPosition () const
 Longitudinal component of the position w.r.t. the momentum.
 
const ThreeVector & adjustMomentumFromEnergy ()
 Rescale the momentum to match the total energy.
 
G4double adjustEnergyFromMomentum ()
 Recompute the energy to match the momentum.
 
G4bool isCluster () const
 
void setFrozenMomentum (const ThreeVector &momentum)
 Set the frozen particle momentum.
 
void setFrozenEnergy (const G4double energy)
 Set the frozen particle momentum.
 
ThreeVector getFrozenMomentum () const
 Get the frozen particle momentum.
 
G4double getFrozenEnergy () const
 Get the frozen particle momentum.
 
ThreeVector getPropagationVelocity () const
 Get the propagation velocity of the particle.
 
void freezePropagation ()
 Freeze particle propagation.
 
void thawPropagation ()
 Unfreeze particle propagation.
 
virtual void rotatePositionAndMomentum (const G4double angle, const ThreeVector &axis)
 Rotate the particle position and momentum.
 
virtual void rotatePosition (const G4double angle, const ThreeVector &axis)
 Rotate the particle position.
 
virtual void rotateMomentum (const G4double angle, const ThreeVector &axis)
 Rotate the particle momentum.
 
std::string print () const
 
std::string dump () const
 
long getID () const
 
ParticleList const * getParticles () const
 
G4double getReflectionMomentum () const
 Return the reflection momentum.
 
void setUncorrelatedMomentum (const G4double p)
 Set the uncorrelated momentum.
 
void rpCorrelate ()
 Make the particle follow a strict r-p correlation.
 
void rpDecorrelate ()
 Make the particle not follow a strict r-p correlation.
 
G4double getCosRPAngle () const
 Get the cosine of the angle between position and momentum.
 
G4double getParticleBias () const
 Get the particle bias.
 
void setParticleBias (G4double ParticleBias)
 Set the particle bias.
 
std::vector< G4int > getBiasCollisionVector () const
 Get the vector list of biased vertices on the particle path.
 
void setBiasCollisionVector (std::vector< G4int > BiasCollisionVector)
 Set the vector list of biased vertices on the particle path.
 
G4int getNumberOfKaon () const
 Number of Kaon inside de nucleus.
 
void setNumberOfKaon (const G4int NK)
 

Static Public Member Functions

static G4double getTotalBias ()
 General bias vector function.
 
static void setINCLBiasVector (std::vector< G4double > NewVector)
 
static void FillINCLBiasVector (G4double newBias)
 
static G4double getBiasFromVector (std::vector< G4int > VectorBias)
 
static std::vector< G4int > MergeVectorBias (Particle const *const p1, Particle const *const p2)
 
static std::vector< G4int > MergeVectorBias (std::vector< G4int > p1, Particle const *const p2)
 

Static Public Attributes

static std::vector< G4double > INCLBiasVector
 Time ordered vector of all bias applied.
 
static G4ThreadLocal G4int nextBiasedCollisionID = 0
 

Protected Member Functions

void swap (Particle &rhs)
 Helper method for the assignment operator.
 

Protected Attributes

G4int theZ
 
G4int theA
 
G4int theS
 
ParticipantType theParticipantType
 
G4INCL::ParticleType theType
 
G4double theEnergy
 
G4double * thePropagationEnergy
 
G4double theFrozenEnergy
 
G4INCL::ThreeVector theMomentum
 
G4INCL::ThreeVector * thePropagationMomentum
 
G4INCL::ThreeVector theFrozenMomentum
 
G4INCL::ThreeVector thePosition
 
G4int nCollisions
 
G4int nDecays
 
G4double thePotentialEnergy
 
long ID
 
G4bool rpCorrelated
 
G4double uncorrelatedMomentum
 
G4double theParticleBias
 
G4int theNKaon
 The number of Kaons inside the nucleus (update during the cascade)
 

Detailed Description

Definition at line 75 of file G4INCLParticle.hh.

Constructor & Destructor Documentation

◆ Particle() [1/4]

G4INCL::Particle::Particle ( )

Definition at line 59 of file G4INCLParticle.cc.

60 : theZ(0), theA(0), theS(0),
61 theParticipantType(TargetSpectator),
62 theType(UnknownParticle),
63 theEnergy(0.0),
64 thePropagationEnergy(&theEnergy),
65 theFrozenEnergy(theEnergy),
66 theMomentum(ThreeVector(0.,0.,0.)),
67 thePropagationMomentum(&theMomentum),
68 theFrozenMomentum(theMomentum),
69 thePosition(ThreeVector(0.,0.,0.)),
70 nCollisions(0),
71 nDecays(0),
72 thePotentialEnergy(0.0),
73 rpCorrelated(false),
74 uncorrelatedMomentum(0.),
75 theParticleBias(1.),
76 theNKaon(0),
77 theHelicity(0.0),
78 emissionTime(0.0),
79 outOfWell(false),
80 theMass(0.)
81 {
82 ID = nextID;
83 nextID++;
84 }
G4INCL::Particle::thePropagationMomentum
G4INCL::ThreeVector * thePropagationMomentum
Definition: G4INCLParticle.hh:1087
G4INCL::Particle::theMomentum
G4INCL::ThreeVector theMomentum
Definition: G4INCLParticle.hh:1086
G4INCL::Particle::thePotentialEnergy
G4double thePotentialEnergy
Definition: G4INCLParticle.hh:1092
G4INCL::Particle::theParticipantType
ParticipantType theParticipantType
Definition: G4INCLParticle.hh:1081
G4INCL::Particle::theType
G4INCL::ParticleType theType
Definition: G4INCLParticle.hh:1082
G4INCL::Particle::theNKaon
G4int theNKaon
The number of Kaons inside the nucleus (update during the cascade)
Definition: G4INCLParticle.hh:1100
G4INCL::Particle::uncorrelatedMomentum
G4double uncorrelatedMomentum
Definition: G4INCLParticle.hh:1096
G4INCL::Particle::thePropagationEnergy
G4double * thePropagationEnergy
Definition: G4INCLParticle.hh:1084
G4INCL::Particle::thePosition
G4INCL::ThreeVector thePosition
Definition: G4INCLParticle.hh:1089
G4INCL::Particle::theFrozenMomentum
G4INCL::ThreeVector theFrozenMomentum
Definition: G4INCLParticle.hh:1088

Referenced by G4INCL::Cluster::Cluster().

◆ Particle() [2/4]

G4INCL::Particle::Particle ( ParticleType  t,
G4double  energy,
ThreeVector const &  momentum,
ThreeVector const &  position 
)

Definition at line 86 of file G4INCLParticle.cc.

88 : theEnergy(energy),
89 thePropagationEnergy(&theEnergy),
90 theFrozenEnergy(theEnergy),
91 theMomentum(momentum),
92 thePropagationMomentum(&theMomentum),
93 theFrozenMomentum(theMomentum),
94 thePosition(position),
95 nCollisions(0), nDecays(0),
96 thePotentialEnergy(0.),
97 rpCorrelated(false),
98 uncorrelatedMomentum(theMomentum.mag()),
99 theParticleBias(1.),
100 theNKaon(0),
101 theHelicity(0.0),
102 emissionTime(0.0), outOfWell(false)
103 {
104 theParticipantType = TargetSpectator;
105 ID = nextID;
106 nextID++;
107 if(theEnergy <= 0.0) {
108 INCL_WARN("Particle with energy " << theEnergy << " created." << '\n');
109 }
110 setType(t);
111 setMass(getInvariantMass());
112 }
INCL_WARN
#define INCL_WARN(x)
Definition: G4INCLLogger.hh:232
G4INCL::Particle::setMass
void setMass(G4double mass)
Definition: G4INCLParticle.hh:778
G4INCL::Particle::getInvariantMass
G4double getInvariantMass() const
Get the the particle invariant mass.
Definition: G4INCLParticle.hh:748
G4INCL::Particle::setType
void setType(ParticleType t)
Definition: G4INCLParticle.hh:187
G4INCL::ThreeVector::mag
G4double mag() const
Definition: G4INCLThreeVector.hh:73

◆ Particle() [3/4]

G4INCL::Particle::Particle ( ParticleType  t,
ThreeVector const &  momentum,
ThreeVector const &  position 
)

Definition at line 114 of file G4INCLParticle.cc.

116 : thePropagationEnergy(&theEnergy),
117 theMomentum(momentum),
118 thePropagationMomentum(&theMomentum),
119 theFrozenMomentum(theMomentum),
120 thePosition(position),
121 nCollisions(0), nDecays(0),
122 thePotentialEnergy(0.),
123 rpCorrelated(false),
124 uncorrelatedMomentum(theMomentum.mag()),
125 theParticleBias(1.),
126 theNKaon(0),
127 theHelicity(0.0),
128 emissionTime(0.0), outOfWell(false)
129 {
130 theParticipantType = TargetSpectator;
131 ID = nextID;
132 nextID++;
133 setType(t);
134 if( isResonance() ) {
135 INCL_ERROR("Cannot create resonance without specifying its momentum four-vector." << '\n');
136 }
137 G4double energy = std::sqrt(theMomentum.mag2() + theMass*theMass);
138 theEnergy = energy;
139 theFrozenEnergy = theEnergy;
140 }
INCL_ERROR
#define INCL_ERROR(x)
Definition: G4INCLLogger.hh:225
G4double
double G4double
Definition: G4Types.hh:83
G4INCL::Particle::isResonance
G4bool isResonance() const
Is it a resonance?
Definition: G4INCLParticle.hh:358
G4INCL::ThreeVector::mag2
G4double mag2() const
Definition: G4INCLThreeVector.hh:78
G4INCL::KinematicsUtils::energy
G4double energy(const ThreeVector &p, const G4double m)
Definition: G4INCLKinematicsUtils.cc:158

◆ ~Particle()

virtual G4INCL::Particle::~Particle ( )
inlinevirtual

Definition at line 80 of file G4INCLParticle.hh.

80{}

◆ Particle() [4/4]

G4INCL::Particle::Particle ( const Particle &  rhs)
inline

Copy constructor.

Does not copy the particle ID.

Definition at line 86 of file G4INCLParticle.hh.

86 :
87 theZ(rhs.theZ),
88 theA(rhs.theA),
89 theS(rhs.theS),
90 theParticipantType(rhs.theParticipantType),
91 theType(rhs.theType),
92 theEnergy(rhs.theEnergy),
93 theFrozenEnergy(rhs.theFrozenEnergy),
94 theMomentum(rhs.theMomentum),
95 theFrozenMomentum(rhs.theFrozenMomentum),
96 thePosition(rhs.thePosition),
97 nCollisions(rhs.nCollisions),
98 nDecays(rhs.nDecays),
99 thePotentialEnergy(rhs.thePotentialEnergy),
100 rpCorrelated(rhs.rpCorrelated),
101 uncorrelatedMomentum(rhs.uncorrelatedMomentum),
102 theParticleBias(rhs.theParticleBias),
103 theNKaon(rhs.theNKaon),
104 theHelicity(rhs.theHelicity),
105 emissionTime(rhs.emissionTime),
106 outOfWell(rhs.outOfWell),
107 theMass(rhs.theMass)
108 {
109 if(rhs.thePropagationEnergy == &(rhs.theFrozenEnergy))
110 thePropagationEnergy = &theFrozenEnergy;
111 else
112 thePropagationEnergy = &theEnergy;
113 if(rhs.thePropagationMomentum == &(rhs.theFrozenMomentum))
114 thePropagationMomentum = &theFrozenMomentum;
115 else
116 thePropagationMomentum = &theMomentum;
117 // ID intentionally not copied
118 ID = nextID++;
119
120 theBiasCollisionVector = rhs.theBiasCollisionVector;
121 }

Member Function Documentation

◆ adjustEnergyFromMomentum()

G4double G4INCL::Particle::adjustEnergyFromMomentum ( )

Recompute the energy to match the momentum.

Definition at line 155 of file G4INCLParticle.cc.

155 {
156 theEnergy = std::sqrt(theMomentum.mag2() + theMass*theMass);
157 return theEnergy;
158 }

Referenced by G4INCL::Nucleus::computeRecoilKinematics(), G4INCL::Nucleus::decayOutgoingPionResonances(), G4INCL::Nucleus::decayOutgoingSigmaZero(), G4INCL::DeltaDecayChannel::fillFinalState(), G4INCL::NKbElasticChannel::fillFinalState(), G4INCL::NKbToLpiChannel::fillFinalState(), G4INCL::NKbToNKbChannel::fillFinalState(), G4INCL::NKbToSpiChannel::fillFinalState(), G4INCL::NKElasticChannel::fillFinalState(), G4INCL::NKToNKChannel::fillFinalState(), G4INCL::NSToNSChannel::fillFinalState(), G4INCL::PionResonanceDecayChannel::fillFinalState(), G4INCL::RecombinationChannel::fillFinalState(), G4INCL::SigmaZeroDecayChannel::fillFinalState(), G4INCL::StrangeAbsorbtionChannel::fillFinalState(), and G4INCL::PhaseSpaceKopylov::generate().

◆ adjustMomentumFromEnergy()

const ThreeVector & G4INCL::Particle::adjustMomentumFromEnergy ( )

Rescale the momentum to match the total energy.

Definition at line 142 of file G4INCLParticle.cc.

142 {
143 const G4double p2 = theMomentum.mag2();
144 G4double newp2 = theEnergy*theEnergy - theMass*theMass;
145 if( newp2<0.0 ) {
146 INCL_ERROR("Particle has E^2 < m^2." << '\n' << print());
147 newp2 = 0.0;
148 theEnergy = theMass;
149 }
150
151 theMomentum *= std::sqrt(newp2/p2);
152 return theMomentum;
153 }
G4INCL::Particle::print
std::string print() const
Definition: G4INCLParticle.hh:953

Referenced by G4INCL::Cluster::Cluster(), G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), G4INCL::CrossSections::interactionDistanceKbarN(), G4INCL::CrossSections::interactionDistanceKN(), G4INCL::CrossSections::interactionDistanceNN(), G4INCL::CrossSections::interactionDistancePiN(), G4INCL::CrossSections::interactionDistanceYN(), G4INCL::StandardPropagationModel::shootParticle(), and G4INCL::KinematicsUtils::transformToLocalEnergyFrame().

◆ boost()

void G4INCL::Particle::boost ( const ThreeVector &  aBoostVector)
inline

Boost the particle using a boost vector.

Example (go to the particle rest frame): particle->boost(particle->boostVector());

Definition at line 422 of file G4INCLParticle.hh.

422 {
423 const G4double beta2 = aBoostVector.mag2();
424 const G4double gamma = 1.0 / std::sqrt(1.0 - beta2);
425 const G4double bp = theMomentum.dot(aBoostVector);
426 const G4double alpha = (gamma*gamma)/(1.0 + gamma);
427
428 theMomentum = theMomentum + aBoostVector * (alpha * bp - gamma * theEnergy);
429 theEnergy = gamma * (theEnergy - bp);
430 }
G4INCL::ThreeVector::dot
G4double dot(const ThreeVector &v) const
Definition: G4INCLThreeVector.hh:97

Referenced by G4INCL::Cluster::boost(), G4INCL::Nucleus::decayOutgoingPionResonances(), G4INCL::Nucleus::decayOutgoingSigmaZero(), G4INCL::PhaseSpaceKopylov::generate(), and G4INCL::InteractionAvatar::preInteraction().

◆ boostVector()

ThreeVector G4INCL::Particle::boostVector ( ) const
inline

Returns a three vector we can give to the boost() -method.

In order to go to the particle rest frame you need to multiply the boost vector by -1.0.

Definition at line 412 of file G4INCLParticle.hh.

412 {
413 return theMomentum / theEnergy;
414 }

Referenced by G4INCL::PhaseSpaceKopylov::generate(), G4INCL::StandardPropagationModel::shootComposite(), and G4INCL::StandardPropagationModel::shootParticle().

◆ dump()

std::string G4INCL::Particle::dump ( ) const
inline

Definition at line 968 of file G4INCLParticle.hh.

968 {
969 std::stringstream ss;
970 ss << "(particle " << ID << " ";
971 ss << ParticleTable::getName(theType);
972 ss << '\n'
973 << thePosition.dump()
974 << '\n'
975 << theMomentum.dump()
976 << '\n'
977 << theEnergy << ")" << '\n';
978 return ss.str();
979 };
G4INCL::ThreeVector::dump
std::string dump() const
Definition: G4INCLThreeVector.hh:206
G4INCL::ParticleTable::getName
std::string getName(const ParticleType t)
Get the native INCL name of the particle.
Definition: G4INCLParticleTable.cc:559

Referenced by G4INCL::BinaryCollisionAvatar::dump(), G4INCL::DecayAvatar::dump(), G4INCL::ParticleEntryAvatar::dump(), and G4INCL::SurfaceAvatar::dump().

◆ FillINCLBiasVector()

void G4INCL::Particle::FillINCLBiasVector ( G4double  newBias)
static

Definition at line 202 of file G4INCLParticle.cc.

202 {
203// assert(G4int(Particle::INCLBiasVector.size())==nextBiasedCollisionID);
204 //assert(G4int(Particle::INCLBiasVector.Size())==nextBiasedCollisionID);
205// assert(std::fabs(newBias - 1.) > 1E-6);
206 Particle::INCLBiasVector.push_back(newBias);
207 //Particle::INCLBiasVector.Push_back(newBias);
208 Particle::nextBiasedCollisionID++;
209 }
G4INCL::Particle::INCLBiasVector
static std::vector< G4double > INCLBiasVector
Time ordered vector of all bias applied.
Definition: G4INCLParticle.hh:1071
G4INCL::Particle::nextBiasedCollisionID
static G4ThreadLocal G4int nextBiasedCollisionID
Definition: G4INCLParticle.hh:1077

Referenced by G4INCL::InteractionAvatar::postInteraction().

◆ freezePropagation()

void G4INCL::Particle::freezePropagation ( )
inline

Freeze particle propagation.

Make the particle use theFrozenMomentum and theFrozenEnergy for propagation. The normal state can be restored by calling the thawPropagation() method.

Definition at line 908 of file G4INCLParticle.hh.

908 {
909 thePropagationMomentum = &theFrozenMomentum;
910 thePropagationEnergy = &theFrozenEnergy;
911 }

◆ getA()

G4int G4INCL::Particle::getA ( ) const
inline

Returns the baryon number.

Definition at line 393 of file G4INCLParticle.hh.

393{ return theA; }

Referenced by G4INCL::Cluster::addParticle(), G4INCL::ClusteringModelIntercomparison::clusterCanEscape(), G4INCL::ClusterDecay::decay(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsideStrangeParticles(), G4INCL::Nucleus::fillEventInfo(), G4INCL::ParticleEntryChannel::fillFinalState(), G4INCL::TransmissionChannel::fillFinalState(), G4INCL::Nucleus::finalizeProjectileRemnant(), G4INCL::PauliStandard::getBlockingProbability(), G4INCL::ClusteringModelIntercomparison::getCluster(), G4INCL::Nucleus::getConservationBalance(), G4INCL::SurfaceAvatar::getTransmissionProbability(), G4INCL::NuclearDensity::getTransmissionRadius(), G4INCL::Nucleus::insertParticle(), G4INCL::ClusterDecay::isStable(), G4INCL::ProjectileRemnant::removeParticle(), G4INCL::StandardPropagationModel::shootComposite(), and G4INCL::StandardPropagationModel::shootParticle().

◆ getAngularMomentum()

virtual G4INCL::ThreeVector G4INCL::Particle::getAngularMomentum ( ) const
inlinevirtual

Get the angular momentum w.r.t. the origin

Reimplemented in G4INCL::Cluster.

Definition at line 800 of file G4INCLParticle.hh.

801 {
802 return thePosition.vector(theMomentum);
803 };
G4INCL::ThreeVector::vector
ThreeVector vector(const ThreeVector &v) const
Definition: G4INCLThreeVector.hh:104

Referenced by G4INCL::Cluster::getAngularMomentum(), and G4INCL::StandardPropagationModel::shootParticle().

◆ getBeta()

G4double G4INCL::Particle::getBeta ( ) const
inline

Definition at line 401 of file G4INCLParticle.hh.

401 {
402 const G4double P = theMomentum.mag();
403 return P/theEnergy;
404 }

◆ getBiasCollisionVector()

std::vector< G4int > G4INCL::Particle::getBiasCollisionVector ( ) const
inline

Get the vector list of biased vertices on the particle path.

Definition at line 1038 of file G4INCLParticle.hh.

1038{ return theBiasCollisionVector; }

Referenced by G4INCL::ClusterDecay::decay(), G4INCL::Nucleus::decayMe(), G4INCL::Nucleus::decayOutgoingClusters(), G4INCL::Nucleus::decayOutgoingPionResonances(), G4INCL::Nucleus::decayOutgoingSigmaZero(), and MergeVectorBias().

◆ getBiasFromVector()

G4double G4INCL::Particle::getBiasFromVector ( std::vector< G4int >  VectorBias)
static

Definition at line 211 of file G4INCLParticle.cc.

211 {
212 if(VectorBias.empty()) return 1.;
213
214 G4double ParticleBias = 1.;
215
216 for(G4int i=0; i<G4int(VectorBias.size()); i++){
217 ParticleBias *= Particle::INCLBiasVector[G4int(VectorBias[i])];
218 }
219
220 return ParticleBias;
221 }
G4int
int G4int
Definition: G4Types.hh:85

Referenced by G4INCL::BinaryCollisionAvatar::getChannel(), G4INCL::ParticleList::getParticleListBias(), and setBiasCollisionVector().

◆ getCosRPAngle()

G4double G4INCL::Particle::getCosRPAngle ( ) const
inline

Get the cosine of the angle between position and momentum.

Definition at line 1014 of file G4INCLParticle.hh.

1014 {
1015 const G4double norm = thePosition.mag2()*thePropagationMomentum->mag2();
1016 if(norm>0.)
1017 return thePosition.dot(*thePropagationMomentum) / std::sqrt(norm);
1018 else
1019 return 1.;
1020 }

◆ getEmissionQValueCorrection() [1/2]

G4double G4INCL::Particle::getEmissionQValueCorrection ( const G4int  AParent,
const G4int  ZParent 
) const
inline

Computes correction on the emission Q-value.

Computes the correction that must be applied to INCL particles in order to obtain the correct Q-value for particle emission from a given nucleus. For absorption, the correction is obviously equal to minus the value returned by this function.

Parameters
AParentthe mass number of the emitting nucleus
ZParentthe charge number of the emitting nucleus
Returns
the correction

Definition at line 602 of file G4INCLParticle.hh.

602 {
603 const G4int SParent = 0;
604 const G4int ADaughter = AParent - theA;
605 const G4int ZDaughter = ZParent - theZ;
606 const G4int SDaughter = 0;
607
608 // Note the minus sign here
609 G4double theQValue;
610 if(isCluster())
611 theQValue = -ParticleTable::getTableQValue(theA, theZ, theS, ADaughter, ZDaughter, SDaughter);
612 else {
613 const G4double massTableParent = ParticleTable::getTableMass(AParent,ZParent,SParent);
614 const G4double massTableDaughter = ParticleTable::getTableMass(ADaughter,ZDaughter,SDaughter);
615 const G4double massTableParticle = getTableMass();
616 theQValue = massTableParent - massTableDaughter - massTableParticle;
617 }
618
619 const G4double massINCLParent = ParticleTable::getINCLMass(AParent,ZParent,SParent);
620 const G4double massINCLDaughter = ParticleTable::getINCLMass(ADaughter,ZDaughter,SDaughter);
621 const G4double massINCLParticle = getINCLMass();
622
623 // The rhs corresponds to the INCL Q-value
624 return theQValue - (massINCLParent-massINCLDaughter-massINCLParticle);
625 }
G4INCL::Particle::isCluster
G4bool isCluster() const
Definition: G4INCLParticle.hh:883
G4INCL::Particle::getINCLMass
G4double getINCLMass() const
Get the INCL particle mass.
Definition: G4INCLParticle.hh:454
G4INCL::Particle::getTableMass
virtual G4double getTableMass() const
Get the tabulated particle mass.
Definition: G4INCLParticle.hh:497
G4INCL::ParticleTable::getTableMass
G4ThreadLocal NuclearMassFn getTableMass
Static pointer to the mass function for nuclei.
Definition: G4INCLParticleTable.cc:1220
G4INCL::ParticleTable::getTableQValue
G4double getTableQValue(const G4int A1, const G4int Z1, const G4int S1, const G4int A2, const G4int Z2, const G4int S2)
Get Q-value (in MeV/c^2)
Definition: G4INCLParticleTable.cc:820
G4INCL::ParticleTable::getINCLMass
G4double getINCLMass(const G4int A, const G4int Z, const G4int S)
Get INCL nuclear mass (in MeV/c^2)
Definition: G4INCLParticleTable.cc:794

Referenced by G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), G4INCL::ParticleEntryChannel::fillFinalState(), G4INCL::TransmissionChannel::fillFinalState(), and G4INCL::SurfaceAvatar::getTransmissionProbability().

◆ getEmissionQValueCorrection() [2/2]

G4double G4INCL::Particle::getEmissionQValueCorrection ( const G4int  AParent,
const G4int  ZParent,
const G4int  SParent 
) const
inline

Computes correction on the emission Q-value for hypernuclei.

Computes the correction that must be applied to INCL particles in order to obtain the correct Q-value for particle emission from a given nucleus. For absorption, the correction is obviously equal to minus the value returned by this function.

Parameters
AParentthe mass number of the emitting nucleus
ZParentthe charge number of the emitting nucleus
SParentthe strangess number of the emitting nucleus
Returns
the correction

Definition at line 678 of file G4INCLParticle.hh.

678 {
679 const G4int ADaughter = AParent - theA;
680 const G4int ZDaughter = ZParent - theZ;
681 const G4int SDaughter = SParent - theS;
682
683 // Note the minus sign here
684 G4double theQValue;
685 if(isCluster())
686 theQValue = -ParticleTable::getTableQValue(theA, theZ, theS, ADaughter, ZDaughter, SDaughter);
687 else {
688 const G4double massTableParent = ParticleTable::getTableMass(AParent,ZParent,SParent);
689 const G4double massTableDaughter = ParticleTable::getTableMass(ADaughter,ZDaughter,SDaughter);
690 const G4double massTableParticle = getTableMass();
691 theQValue = massTableParent - massTableDaughter - massTableParticle;
692 }
693
694 const G4double massINCLParent = ParticleTable::getINCLMass(AParent,ZParent,SParent);
695 const G4double massINCLDaughter = ParticleTable::getINCLMass(ADaughter,ZDaughter,SDaughter);
696 const G4double massINCLParticle = getINCLMass();
697
698 // The rhs corresponds to the INCL Q-value
699 return theQValue - (massINCLParent-massINCLDaughter-massINCLParticle);
700 }

◆ getEmissionTime()

G4double G4INCL::Particle::getEmissionTime ( )
inline

Definition at line 865 of file G4INCLParticle.hh.

865{ return emissionTime; };

◆ getEnergy()

G4double G4INCL::Particle::getEnergy ( ) const
inline

Get the energy of the particle in MeV.

Definition at line 770 of file G4INCLParticle.hh.

771 {
772 return theEnergy;
773 };

Referenced by G4INCL::Cluster::addParticle(), G4INCL::DeltaDecayChannel::computeDecayTime(), G4INCL::PionResonanceDecayChannel::computeDecayTime(), G4INCL::EtaNElasticChannel::fillFinalState(), G4INCL::EtaNToPiNChannel::fillFinalState(), G4INCL::OmegaNElasticChannel::fillFinalState(), G4INCL::OmegaNToPiNChannel::fillFinalState(), G4INCL::ParticleEntryChannel::fillFinalState(), G4INCL::ReflectionChannel::fillFinalState(), G4INCL::TransmissionChannel::fillFinalState(), G4INCL::ClusteringModelIntercomparison::getCluster(), G4INCL::KinematicsUtils::makeBoostVector(), G4INCL::KinematicsUtils::momentumInCM(), G4INCL::InteractionAvatar::preInteraction(), G4INCL::InteractionAvatar::preInteractionBlocking(), G4INCL::ProjectileRemnant::removeParticle(), G4INCL::StandardPropagationModel::shootComposite(), G4INCL::StandardPropagationModel::shootParticle(), G4INCL::KinematicsUtils::squareTotalEnergyInCM(), and G4INCL::KinematicsUtils::transformToLocalEnergyFrame().

◆ getFrozenEnergy()

G4double G4INCL::Particle::getFrozenEnergy ( ) const
inline

Get the frozen particle momentum.

Definition at line 897 of file G4INCLParticle.hh.

897{ return theFrozenEnergy; }

◆ getFrozenMomentum()

ThreeVector G4INCL::Particle::getFrozenMomentum ( ) const
inline

Get the frozen particle momentum.

Definition at line 894 of file G4INCLParticle.hh.

894{ return theFrozenMomentum; }

◆ getHelicity()

G4double G4INCL::Particle::getHelicity ( )
inline

Definition at line 826 of file G4INCLParticle.hh.

826{ return theHelicity; };

◆ getID()

long G4INCL::Particle::getID ( ) const
inline

Definition at line 981 of file G4INCLParticle.hh.

981{ return ID; };

Referenced by G4INCL::ParticleEntryChannel::fillFinalState(), G4INCL::ReflectionChannel::fillFinalState(), G4INCL::PauliStandard::getBlockingProbability(), G4INCL::SurfaceAvatar::getChannel(), G4INCL::ClusteringModelIntercomparison::getCluster(), and G4INCL::ProjectileRemnant::reset().

◆ getINCLMass()

G4double G4INCL::Particle::getINCLMass ( ) const
inline

Get the INCL particle mass.

Definition at line 454 of file G4INCLParticle.hh.

454 {
455 switch(theType) {
456 case Proton:
457 case Neutron:
458 case PiPlus:
459 case PiMinus:
460 case PiZero:
461 case Lambda:
462 case SigmaPlus:
463 case SigmaZero:
464 case SigmaMinus:
465 case KPlus:
466 case KZero:
467 case KZeroBar:
468 case KShort:
469 case KLong:
470 case KMinus:
471 case Eta:
472 case Omega:
473 case EtaPrime:
474 case Photon:
475 return ParticleTable::getINCLMass(theType);
476 break;
477
478 case DeltaPlusPlus:
479 case DeltaPlus:
480 case DeltaZero:
481 case DeltaMinus:
482 return theMass;
483 break;
484
485 case Composite:
486 return ParticleTable::getINCLMass(theA,theZ,theS);
487 break;
488
489 default:
490 INCL_ERROR("Particle::getINCLMass: Unknown particle type." << '\n');
491 return 0.0;
492 break;
493 }
494 }

Referenced by G4INCL::ParticleEntryChannel::fillFinalState(), getEmissionQValueCorrection(), and setINCLMass().

◆ getInvariantMass()

G4double G4INCL::Particle::getInvariantMass ( ) const
inline

Get the the particle invariant mass.

Uses the relativistic invariant

\[ m = \sqrt{E^2 - {\vec p}^2}\]

Definition at line 748 of file G4INCLParticle.hh.

748 {
749 const G4double mass = std::pow(theEnergy, 2) - theMomentum.dot(theMomentum);
750 if(mass < 0.0) {
751 INCL_ERROR("E*E - p*p is negative." << '\n');
752 return 0.0;
753 } else {
754 return std::sqrt(mass);
755 }
756 };

Referenced by G4INCL::Nucleus::finalizeProjectileRemnant(), and Particle().

◆ getKineticEnergy()

G4double G4INCL::Particle::getKineticEnergy ( ) const
inline

Get the particle kinetic energy.

Definition at line 759 of file G4INCLParticle.hh.

759{ return theEnergy - theMass; }

Referenced by G4INCL::NuclearPotential::NuclearPotentialEnergyIsospin::computePotentialEnergy(), G4INCL::NuclearPotential::NuclearPotentialEnergyIsospinSmooth::computePotentialEnergy(), G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), G4INCL::Nucleus::fillEventInfo(), G4INCL::ParticleEntryChannel::fillFinalState(), G4INCL::SurfaceAvatar::getChannel(), G4INCL::Nucleus::getConservationBalance(), G4INCL::KinematicsUtils::getLocalEnergy(), G4INCL::SurfaceAvatar::getTransmissionProbability(), G4INCL::CoulombDistortion::maxImpactParameter(), G4INCL::CDPP::processOneParticle(), and G4INCL::StandardPropagationModel::shootParticle().

◆ getLongitudinalPosition()

ThreeVector G4INCL::Particle::getLongitudinalPosition ( ) const
inline

Longitudinal component of the position w.r.t. the momentum.

Definition at line 873 of file G4INCLParticle.hh.

873 {
874 return *thePropagationMomentum * (thePosition.dot(*thePropagationMomentum)/thePropagationMomentum->mag2());
875 }

Referenced by getTransversePosition().

◆ getMass()

G4double G4INCL::Particle::getMass ( ) const
inline

Get the cached particle mass.

Definition at line 451 of file G4INCLParticle.hh.

451{ return theMass; }

Referenced by G4INCL::DeltaDecayChannel::computeDecayTime(), G4INCL::PionResonanceDecayChannel::computeDecayTime(), G4INCL::SigmaZeroDecayChannel::computeDecayTime(), G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), G4INCL::InteractionAvatar::enforceEnergyConservation(), G4INCL::CrossSectionsMultiPionsAndResonances::etaNToPiN(), G4INCL::DeltaDecayChannel::fillFinalState(), G4INCL::EtaNElasticChannel::fillFinalState(), G4INCL::EtaNToPiNChannel::fillFinalState(), G4INCL::NSToNLChannel::fillFinalState(), G4INCL::NSToNSChannel::fillFinalState(), G4INCL::OmegaNElasticChannel::fillFinalState(), G4INCL::OmegaNToPiNChannel::fillFinalState(), G4INCL::PionResonanceDecayChannel::fillFinalState(), G4INCL::RecombinationChannel::fillFinalState(), G4INCL::SigmaZeroDecayChannel::fillFinalState(), G4INCL::TransmissionChannel::fillFinalState(), G4INCL::Cluster::freezeInternalMotion(), G4INCL::PhaseSpaceKopylov::generate(), G4INCL::NuclearPotential::INuclearPotential::getFermiMomentum(), G4INCL::KinematicsUtils::getLocalEnergy(), G4INCL::SurfaceAvatar::getTransmissionProbability(), G4INCL::CrossSections::interactionDistanceKbarN(), G4INCL::CrossSections::interactionDistanceKN(), G4INCL::CrossSections::interactionDistanceNN(), G4INCL::CrossSections::interactionDistancePiN(), G4INCL::CrossSections::interactionDistanceYN(), G4INCL::Cluster::internalBoostToCM(), G4INCL::KinematicsUtils::momentumInCM(), G4INCL::KinematicsUtils::momentumInLab(), G4INCL::CrossSectionsINCL46::NDeltaToNN(), G4INCL::CrossSectionsMultiPions::NDeltaToNN(), G4INCL::CrossSectionsStrangeness::NNToNLK2pi(), G4INCL::CrossSectionsStrangeness::NNToNLKpi(), G4INCL::CrossSectionsStrangeness::NNToNSK2pi(), G4INCL::CrossSectionsStrangeness::NNToNSKpi(), G4INCL::CrossSectionsMultiPionsAndResonances::omegaNToPiN(), G4INCL::CrossSectionsMultiPionsAndResonances::piMinuspToEtaN(), G4INCL::CrossSectionsMultiPionsAndResonances::piMinuspToOmegaN(), G4INCL::Cluster::print(), G4INCL::ProjectileRemnant::ProjectileRemnant(), and G4INCL::StandardPropagationModel::shootParticle().

◆ getMomentum()

const G4INCL::ThreeVector & G4INCL::Particle::getMomentum ( ) const
inline

Get the momentum vector.

Definition at line 794 of file G4INCLParticle.hh.

795 {
796 return theMomentum;
797 };

Referenced by G4INCL::Cluster::addParticle(), G4INCL::ClusteringModelIntercomparison::clusterCanEscape(), G4INCL::SigmaZeroDecayChannel::computeDecayTime(), G4INCL::Nucleus::computeRecoilKinematics(), G4INCL::Nucleus::decayOutgoingPionResonances(), G4INCL::Nucleus::decayOutgoingSigmaZero(), G4INCL::Nucleus::fillEventInfo(), G4INCL::DeltaProductionChannel::fillFinalState(), G4INCL::ElasticChannel::fillFinalState(), G4INCL::NDeltaEtaProductionChannel::fillFinalState(), G4INCL::NDeltaOmegaProductionChannel::fillFinalState(), G4INCL::NNToNSKpiChannel::fillFinalState(), G4INCL::NpiToLK2piChannel::fillFinalState(), G4INCL::NpiToLKpiChannel::fillFinalState(), G4INCL::NpiToNKKbChannel::fillFinalState(), G4INCL::NpiToSK2piChannel::fillFinalState(), G4INCL::NpiToSKpiChannel::fillFinalState(), G4INCL::ParticleEntryChannel::fillFinalState(), G4INCL::ReflectionChannel::fillFinalState(), G4INCL::StrangeAbsorbtionChannel::fillFinalState(), G4INCL::PauliStandard::getBlockingProbability(), G4INCL::ClusteringModelIntercomparison::getCluster(), G4INCL::Nucleus::getConservationBalance(), G4INCL::KinematicsUtils::getLocalEnergy(), G4INCL::SurfaceAvatar::getTransmissionProbability(), G4INCL::NKbElasticChannel::KaonMomentum(), G4INCL::NKbToLpiChannel::KaonMomentum(), G4INCL::NKbToNKbChannel::KaonMomentum(), G4INCL::NKbToSpiChannel::KaonMomentum(), G4INCL::KinematicsUtils::makeBoostVector(), G4INCL::KinematicsUtils::momentumInCM(), G4INCL::BinaryCollisionAvatar::postInteraction(), G4INCL::InteractionAvatar::preInteraction(), G4INCL::ProjectileRemnant::removeParticle(), G4INCL::ParticleSampler::sampleParticlesIntoList(), G4INCL::StandardPropagationModel::shootComposite(), and G4INCL::StandardPropagationModel::shootParticle().

◆ getNumberOfCollisions()

G4int G4INCL::Particle::getNumberOfCollisions ( ) const
inline

Return the number of collisions undergone by the particle.

Definition at line 834 of file G4INCLParticle.hh.

834{ return nCollisions; }

Referenced by G4INCL::Cluster::addParticle().

◆ getNumberOfDecays()

G4int G4INCL::Particle::getNumberOfDecays ( ) const
inline

Return the number of decays undergone by the particle.

Definition at line 843 of file G4INCLParticle.hh.

843{ return nDecays; }

◆ getNumberOfKaon()

G4int G4INCL::Particle::getNumberOfKaon ( ) const
inline

Number of Kaon inside de nucleus.

Put in the Particle class in order to calculate the "correct" mass of composit particle.

Definition at line 1053 of file G4INCLParticle.hh.

1053{ return theNKaon; };

Referenced by G4INCL::ParticleEntryChannel::fillFinalState(), G4INCL::SurfaceAvatar::getChannel(), and G4INCL::BinaryCollisionAvatar::postInteraction().

◆ getParticipantType()

ParticipantType G4INCL::Particle::getParticipantType ( ) const
inline

Definition at line 310 of file G4INCLParticle.hh.

310 {
311 return theParticipantType;
312 }

Referenced by G4INCL::StandardPropagationModel::generateBinaryCollisionAvatar().

◆ getParticleBias()

G4double G4INCL::Particle::getParticleBias ( ) const
inline

Get the particle bias.

Definition at line 1032 of file G4INCLParticle.hh.

1032{ return theParticleBias; };

◆ getParticles()

ParticleList const * G4INCL::Particle::getParticles ( ) const
inline

Return a NULL pointer

Definition at line 986 of file G4INCLParticle.hh.

986 {
987 INCL_WARN("Particle::getParticles() method was called on a Particle object" << '\n');
988 return 0;
989 }

◆ getPosition()

const G4INCL::ThreeVector & G4INCL::Particle::getPosition ( ) const
inline

Set the position vector.

Definition at line 816 of file G4INCLParticle.hh.

817 {
818 return thePosition;
819 };

Referenced by G4INCL::Cluster::addParticle(), G4INCL::InteractionAvatar::bringParticleInside(), G4INCL::CoulombNone::bringToSurface(), G4INCL::ClusteringModelIntercomparison::clusterCanEscape(), G4INCL::DeltaDecayChannel::fillFinalState(), G4INCL::EtaNToPiPiNChannel::fillFinalState(), G4INCL::NDeltaEtaProductionChannel::fillFinalState(), G4INCL::NDeltaOmegaProductionChannel::fillFinalState(), G4INCL::NDeltaToDeltaSKChannel::fillFinalState(), G4INCL::NDeltaToNLKChannel::fillFinalState(), G4INCL::NDeltaToNNKKbChannel::fillFinalState(), G4INCL::NDeltaToNSKChannel::fillFinalState(), G4INCL::NKbToNKb2piChannel::fillFinalState(), G4INCL::NKToNK2piChannel::fillFinalState(), G4INCL::NNEtaToMultiPionsChannel::fillFinalState(), G4INCL::NNOmegaToMultiPionsChannel::fillFinalState(), G4INCL::NNToMissingStrangenessChannel::fillFinalState(), G4INCL::NNToMultiPionsChannel::fillFinalState(), G4INCL::NNToNLK2piChannel::fillFinalState(), G4INCL::NNToNLKChannel::fillFinalState(), G4INCL::NNToNLKpiChannel::fillFinalState(), G4INCL::NNToNNEtaChannel::fillFinalState(), G4INCL::NNToNNKKbChannel::fillFinalState(), G4INCL::NNToNNOmegaChannel::fillFinalState(), G4INCL::NNToNSK2piChannel::fillFinalState(), G4INCL::NNToNSKChannel::fillFinalState(), G4INCL::NNToNSKpiChannel::fillFinalState(), G4INCL::NpiToMissingStrangenessChannel::fillFinalState(), G4INCL::OmegaNToPiPiNChannel::fillFinalState(), G4INCL::PionResonanceDecayChannel::fillFinalState(), G4INCL::ReflectionChannel::fillFinalState(), G4INCL::SigmaZeroDecayChannel::fillFinalState(), G4INCL::StandardPropagationModel::generateBinaryCollisionAvatar(), G4INCL::PauliStandard::getBlockingProbability(), G4INCL::BinaryCollisionAvatar::getChannel(), G4INCL::ClusteringModelIntercomparison::getCluster(), G4INCL::KinematicsUtils::getLocalEnergy(), G4INCL::StandardPropagationModel::getReflectionTime(), G4INCL::StandardPropagationModel::getTime(), G4INCL::BinaryCollisionAvatar::postInteraction(), and G4INCL::ParticleSampler::sampleParticlesIntoList().

◆ getPotentialEnergy()

G4double G4INCL::Particle::getPotentialEnergy ( ) const
inline

Get the particle potential energy.

Definition at line 762 of file G4INCLParticle.hh.

762{ return thePotentialEnergy; }

Referenced by G4INCL::Cluster::addParticle(), G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), G4INCL::ReflectionChannel::fillFinalState(), G4INCL::TransmissionChannel::fillFinalState(), G4INCL::ClusteringModelIntercomparison::getCluster(), G4INCL::KinematicsUtils::getLocalEnergy(), G4INCL::SurfaceAvatar::getTransmissionProbability(), G4INCL::InteractionAvatar::preInteractionBlocking(), and G4INCL::CDPP::processOneParticle().

◆ getPropagationVelocity()

ThreeVector G4INCL::Particle::getPropagationVelocity ( ) const
inline

Get the propagation velocity of the particle.

Definition at line 900 of file G4INCLParticle.hh.

900{ return (*thePropagationMomentum)/(*thePropagationEnergy); }

Referenced by G4INCL::CoulombNone::bringToSurface(), G4INCL::StandardPropagationModel::getReflectionTime(), and G4INCL::StandardPropagationModel::getTime().

◆ getRealMass()

G4double G4INCL::Particle::getRealMass ( ) const
inline

Get the real particle mass.

Definition at line 540 of file G4INCLParticle.hh.

540 {
541 switch(theType) {
542 case Proton:
543 case Neutron:
544 case PiPlus:
545 case PiMinus:
546 case PiZero:
547 case Lambda:
548 case SigmaPlus:
549 case SigmaZero:
550 case SigmaMinus:
551 case KPlus:
552 case KZero:
553 case KZeroBar:
554 case KShort:
555 case KLong:
556 case KMinus:
557 case Eta:
558 case Omega:
559 case EtaPrime:
560 case Photon:
561 return ParticleTable::getRealMass(theType);
562 break;
563
564 case DeltaPlusPlus:
565 case DeltaPlus:
566 case DeltaZero:
567 case DeltaMinus:
568 return theMass;
569 break;
570
571 case Composite:
572 return ParticleTable::getRealMass(theA,theZ,theS);
573 break;
574
575 default:
576 INCL_ERROR("Particle::getRealMass: Unknown particle type." << '\n');
577 return 0.0;
578 break;
579 }
580 }
G4INCL::ParticleTable::getRealMass
G4double getRealMass(const G4INCL::ParticleType t)
Get particle mass (in MeV/c^2)
Definition: G4INCLParticleTable.cc:710

Referenced by G4INCL::Cluster::getTableMass(), and setRealMass().

◆ getReflectionMomentum()

G4double G4INCL::Particle::getReflectionMomentum ( ) const
inline

Return the reflection momentum.

The reflection momentum is used by calls to getSurfaceRadius to compute the radius of the sphere where the nucleon moves. It is necessary to introduce fuzzy r-p correlations.

Definition at line 997 of file G4INCLParticle.hh.

997 {
998 if(rpCorrelated)
999 return theMomentum.mag();
1000 else
1001 return uncorrelatedMomentum;
1002 }

Referenced by G4INCL::KinematicsUtils::getLocalEnergy(), and G4INCL::Nucleus::getSurfaceRadius().

◆ getS()

G4int G4INCL::Particle::getS ( ) const
inline

Returns the strangeness number.

Definition at line 399 of file G4INCLParticle.hh.

399{ return theS; }

Referenced by G4INCL::Cluster::addParticle(), G4INCL::ClusteringModelIntercomparison::clusterCanEscape(), G4INCL::ClusterDecay::decay(), G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsideStrangeParticles(), G4INCL::Nucleus::fillEventInfo(), G4INCL::ParticleEntryChannel::fillFinalState(), G4INCL::TransmissionChannel::fillFinalState(), G4INCL::Nucleus::finalizeProjectileRemnant(), G4INCL::Nucleus::getConservationBalance(), G4INCL::SurfaceAvatar::getTransmissionProbability(), G4INCL::Nucleus::insertParticle(), G4INCL::ClusterDecay::isStable(), G4INCL::StandardPropagationModel::shootComposite(), and G4INCL::StandardPropagationModel::shootParticle().

◆ getSpecies()

virtual G4INCL::ParticleSpecies G4INCL::Particle::getSpecies ( ) const
inlinevirtual

Get the particle species.

Reimplemented in G4INCL::Cluster.

Definition at line 183 of file G4INCLParticle.hh.

183 {
184 return ParticleSpecies(theType);
185 };

Referenced by G4INCL::CoulombDistortion::maxImpactParameter(), and G4INCL::StandardPropagationModel::shootParticle().

◆ getTableMass()

virtual G4double G4INCL::Particle::getTableMass ( ) const
inlinevirtual

Get the tabulated particle mass.

Reimplemented in G4INCL::Cluster.

Definition at line 497 of file G4INCLParticle.hh.

497 {
498 switch(theType) {
499 case Proton:
500 case Neutron:
501 case PiPlus:
502 case PiMinus:
503 case PiZero:
504 case Lambda:
505 case SigmaPlus:
506 case SigmaZero:
507 case SigmaMinus:
508 case KPlus:
509 case KZero:
510 case KZeroBar:
511 case KShort:
512 case KLong:
513 case KMinus:
514 case Eta:
515 case Omega:
516 case EtaPrime:
517 case Photon:
518 return ParticleTable::getTableParticleMass(theType);
519 break;
520
521 case DeltaPlusPlus:
522 case DeltaPlus:
523 case DeltaZero:
524 case DeltaMinus:
525 return theMass;
526 break;
527
528 case Composite:
529 return ParticleTable::getTableMass(theA,theZ,theS);
530 break;
531
532 default:
533 INCL_ERROR("Particle::getTableMass: Unknown particle type." << '\n');
534 return 0.0;
535 break;
536 }
537 }
G4INCL::ParticleTable::getTableParticleMass
G4ThreadLocal ParticleMassFn getTableParticleMass
Static pointer to the mass function for particles.
Definition: G4INCLParticleTable.cc:1221

Referenced by G4INCL::Nucleus::decayOutgoingPionResonances(), G4INCL::Nucleus::decayOutgoingSigmaZero(), G4INCL::ParticleEntryChannel::fillFinalState(), G4INCL::TransmissionChannel::fillFinalState(), getEmissionQValueCorrection(), getTransferQValueCorrection(), and setTableMass().

◆ getTotalBias()

G4double G4INCL::Particle::getTotalBias ( )
static

General bias vector function.

Definition at line 300 of file G4INCLParticle.cc.

300 {
301 G4double TotalBias = 1.;
302 for(G4int i=0; i<G4int(INCLBiasVector.size());i++) TotalBias *= Particle::INCLBiasVector[i];
303 return TotalBias;
304 }

Referenced by G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), and G4INCL::EventInfo::remnantToParticle().

◆ getTransferQValueCorrection() [1/2]

G4double G4INCL::Particle::getTransferQValueCorrection ( const G4int  AFrom,
const G4int  ZFrom,
const G4int  ATo,
const G4int  ZTo 
) const
inline

Computes correction on the transfer Q-value.

Computes the correction that must be applied to INCL particles in order to obtain the correct Q-value for particle transfer from a given nucleus to another.

Assumes that the receving nucleus is INCL's target nucleus, with the INCL separation energy.

Parameters
AFromthe mass number of the donating nucleus
ZFromthe charge number of the donating nucleus
ATothe mass number of the receiving nucleus
ZTothe charge number of the receiving nucleus
Returns
the correction

Definition at line 642 of file G4INCLParticle.hh.

642 {
643 const G4int SFrom = 0;
644 const G4int STo = 0;
645 const G4int AFromDaughter = AFrom - theA;
646 const G4int ZFromDaughter = ZFrom - theZ;
647 const G4int SFromDaughter = 0;
648 const G4int AToDaughter = ATo + theA;
649 const G4int ZToDaughter = ZTo + theZ;
650 const G4int SToDaughter = 0;
651 const G4double theQValue = ParticleTable::getTableQValue(AToDaughter,ZToDaughter,SToDaughter,AFromDaughter,ZFromDaughter,SFromDaughter,AFrom,ZFrom,SFrom);
652
653 const G4double massINCLTo = ParticleTable::getINCLMass(ATo,ZTo,STo);
654 const G4double massINCLToDaughter = ParticleTable::getINCLMass(AToDaughter,ZToDaughter,SToDaughter);
655 /* Note that here we have to use the table mass in the INCL Q-value. We
656 * cannot use theMass, because at this stage the particle is probably
657 * still off-shell; and we cannot use getINCLMass(), because it leads to
658 * violations of global energy conservation.
659 */
660 const G4double massINCLParticle = getTableMass();
661
662 // The rhs corresponds to the INCL Q-value for particle absorption
663 return theQValue - (massINCLToDaughter-massINCLTo-massINCLParticle);
664 }

◆ getTransferQValueCorrection() [2/2]

G4double G4INCL::Particle::getTransferQValueCorrection ( const G4int  AFrom,
const G4int  ZFrom,
const G4int  SFrom,
const G4int  ATo,
const G4int  ZTo,
const G4int  STo 
) const
inline

Computes correction on the transfer Q-value for hypernuclei.

Computes the correction that must be applied to INCL particles in order to obtain the correct Q-value for particle transfer from a given nucleus to another.

Assumes that the receving nucleus is INCL's target nucleus, with the INCL separation energy.

Parameters
AFromthe mass number of the donating nucleus
ZFromthe charge number of the donating nucleus
SFromthe strangess number of the donating nucleus
ATothe mass number of the receiving nucleus
ZTothe charge number of the receiving nucleus
STothe strangess number of the receiving nucleus
Returns
the correction

Definition at line 719 of file G4INCLParticle.hh.

719 {
720 const G4int AFromDaughter = AFrom - theA;
721 const G4int ZFromDaughter = ZFrom - theZ;
722 const G4int SFromDaughter = SFrom - theS;
723 const G4int AToDaughter = ATo + theA;
724 const G4int ZToDaughter = ZTo + theZ;
725 const G4int SToDaughter = STo + theS;
726 const G4double theQValue = ParticleTable::getTableQValue(AToDaughter,ZToDaughter,SFromDaughter,AFromDaughter,ZFromDaughter,SToDaughter,AFrom,ZFrom,SFrom);
727
728 const G4double massINCLTo = ParticleTable::getINCLMass(ATo,ZTo,STo);
729 const G4double massINCLToDaughter = ParticleTable::getINCLMass(AToDaughter,ZToDaughter,SToDaughter);
730 /* Note that here we have to use the table mass in the INCL Q-value. We
731 * cannot use theMass, because at this stage the particle is probably
732 * still off-shell; and we cannot use getINCLMass(), because it leads to
733 * violations of global energy conservation.
734 */
735 const G4double massINCLParticle = getTableMass();
736
737 // The rhs corresponds to the INCL Q-value for particle absorption
738 return theQValue - (massINCLToDaughter-massINCLTo-massINCLParticle);
739 }

◆ getTransversePosition()

ThreeVector G4INCL::Particle::getTransversePosition ( ) const
inline

Transverse component of the position w.r.t. the momentum.

Definition at line 868 of file G4INCLParticle.hh.

868 {
869 return thePosition - getLongitudinalPosition();
870 }
G4INCL::Particle::getLongitudinalPosition
ThreeVector getLongitudinalPosition() const
Longitudinal component of the position w.r.t. the momentum.
Definition: G4INCLParticle.hh:873

Referenced by G4INCL::StandardPropagationModel::shootComposite(), and G4INCL::StandardPropagationModel::shootParticle().

◆ getType()

G4INCL::ParticleType G4INCL::Particle::getType ( ) const
inline

Get the particle type.

See also
G4INCL::ParticleType

Definition at line 178 of file G4INCLParticle.hh.

178 {
179 return theType;
180 };

Referenced by G4INCL::PionResonanceDecayChannel::computeDecayTime(), G4INCL::NuclearPotential::INuclearPotential::computeKaonPotentialEnergy(), G4INCL::NuclearPotential::INuclearPotential::computePionPotentialEnergy(), G4INCL::NuclearPotential::INuclearPotential::computePionResonancePotentialEnergy(), G4INCL::NuclearPotential::NuclearPotentialConstant::computePotentialEnergy(), G4INCL::NuclearPotential::NuclearPotentialIsospin::computePotentialEnergy(), G4INCL::CrossSectionsINCL46::elasticNNLegacy(), G4INCL::DeltaDecayChannel::fillFinalState(), G4INCL::DeltaProductionChannel::fillFinalState(), G4INCL::ElasticChannel::fillFinalState(), G4INCL::NDeltaEtaProductionChannel::fillFinalState(), G4INCL::NDeltaOmegaProductionChannel::fillFinalState(), G4INCL::NDeltaToDeltaLKChannel::fillFinalState(), G4INCL::NDeltaToDeltaSKChannel::fillFinalState(), G4INCL::NDeltaToNLKChannel::fillFinalState(), G4INCL::NDeltaToNNKKbChannel::fillFinalState(), G4INCL::NDeltaToNSKChannel::fillFinalState(), G4INCL::NKbToL2piChannel::fillFinalState(), G4INCL::NKbToLpiChannel::fillFinalState(), G4INCL::NKbToNKb2piChannel::fillFinalState(), G4INCL::NKbToNKbChannel::fillFinalState(), G4INCL::NKbToNKbpiChannel::fillFinalState(), G4INCL::NKbToS2piChannel::fillFinalState(), G4INCL::NKbToSpiChannel::fillFinalState(), G4INCL::NKToNK2piChannel::fillFinalState(), G4INCL::NKToNKChannel::fillFinalState(), G4INCL::NKToNKpiChannel::fillFinalState(), G4INCL::NNEtaToMultiPionsChannel::fillFinalState(), G4INCL::NNOmegaToMultiPionsChannel::fillFinalState(), G4INCL::NNToMissingStrangenessChannel::fillFinalState(), G4INCL::NNToMultiPionsChannel::fillFinalState(), G4INCL::NNToNLK2piChannel::fillFinalState(), G4INCL::NNToNLKChannel::fillFinalState(), G4INCL::NNToNLKpiChannel::fillFinalState(), G4INCL::NNToNNEtaChannel::fillFinalState(), G4INCL::NNToNNKKbChannel::fillFinalState(), G4INCL::NNToNNOmegaChannel::fillFinalState(), G4INCL::NNToNSK2piChannel::fillFinalState(), G4INCL::NNToNSKChannel::fillFinalState(), G4INCL::NNToNSKpiChannel::fillFinalState(), G4INCL::NpiToMissingStrangenessChannel::fillFinalState(), G4INCL::NSToNLChannel::fillFinalState(), G4INCL::NSToNSChannel::fillFinalState(), G4INCL::PionResonanceDecayChannel::fillFinalState(), G4INCL::RecombinationChannel::fillFinalState(), G4INCL::PauliStandard::getBlockingProbability(), G4INCL::DecayAvatar::getChannel(), G4INCL::NuclearPotential::INuclearPotential::getFermiEnergy(), G4INCL::NuclearPotential::INuclearPotential::getFermiMomentum(), G4INCL::KinematicsUtils::getLocalEnergy(), G4INCL::NuclearPotential::INuclearPotential::getSeparationEnergy(), G4INCL::Nucleus::getSurfaceRadius(), G4INCL::NuclearDensity::getTransmissionRadius(), G4INCL::Nucleus::insertParticle(), G4INCL::ParticleConfig::isPair(), G4INCL::CrossSectionsStrangeness::NDeltaToDeltaLK(), G4INCL::CrossSectionsStrangeness::NDeltaToDeltaSK(), G4INCL::CrossSectionsStrangeness::NDeltaToNLK(), G4INCL::CrossSectionsINCL46::NDeltaToNN(), G4INCL::CrossSectionsMultiPions::NDeltaToNN(), G4INCL::CrossSectionsStrangeness::NDeltaToNNKKb(), G4INCL::CrossSectionsStrangeness::NDeltaToNSK(), G4INCL::CrossSectionsStrangeness::NKbToL2pi(), G4INCL::CrossSectionsStrangeness::NKbToLpi(), G4INCL::CrossSectionsStrangeness::NKbToNKb(), G4INCL::CrossSectionsStrangeness::NKbToNKb2pi(), G4INCL::CrossSectionsStrangeness::NKbToNKbpi(), G4INCL::CrossSectionsStrangeness::NKbToS2pi(), G4INCL::CrossSectionsStrangeness::NKbToSpi(), G4INCL::CrossSectionsStrangeness::NKToNK(), G4INCL::CrossSectionsStrangeness::NKToNK2pi(), G4INCL::CrossSectionsStrangeness::NKToNKpi(), G4INCL::CrossSectionsMultiPions::NNElastic(), G4INCL::CrossSectionsMultiPions::NNOnePi(), G4INCL::CrossSectionsMultiPions::NNOnePiOrDelta(), G4INCL::CrossSectionsMultiPions::NNThreePi(), G4INCL::CrossSectionsStrangeness::NNToMissingStrangeness(), G4INCL::CrossSectionsINCL46::NNToNDelta(), G4INCL::CrossSectionsMultiPions::NNToNDelta(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNDeltaEta(), G4INCL::CrossSectionsMultiPionsAndResonances::NNToNDeltaOmega(), G4INCL::CrossSectionsStrangeness::NNToNLK(), 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::NNToNSK(), G4INCL::CrossSectionsStrangeness::NNToNSK2pi(), G4INCL::CrossSectionsStrangeness::NNToNSKpi(), G4INCL::CrossSectionsMultiPions::NNTot(), G4INCL::CrossSectionsMultiPions::NNTwoPi(), G4INCL::CrossSectionsStrangeness::NpiToLK(), G4INCL::CrossSectionsStrangeness::NpiToLK2pi(), G4INCL::CrossSectionsStrangeness::NpiToLKpi(), G4INCL::CrossSectionsStrangeness::NpiToNKKb(), G4INCL::CrossSectionsStrangeness::NpiToSK(), G4INCL::CrossSectionsStrangeness::NpiToSK2pi(), G4INCL::CrossSectionsStrangeness::NpiToSKpi(), G4INCL::CrossSectionsStrangeness::NSToNL(), G4INCL::CrossSectionsStrangeness::NSToNS(), G4INCL::CrossSectionsStrangeness::p_pimToSzKz(), G4INCL::CrossSectionsINCL46::piNToDelta(), G4INCL::CrossSectionsMultiPions::piNToDelta(), G4INCL::CrossSectionsMultiPionsAndResonances::piNToEtaN(), G4INCL::CrossSectionsMultiPionsAndResonances::piNToOmegaN(), and G4INCL::CrossSectionsMultiPions::piNTot().

◆ getZ()

G4int G4INCL::Particle::getZ ( ) const
inline

Returns the charge number.

Definition at line 396 of file G4INCLParticle.hh.

396{ return theZ; }

Referenced by G4INCL::Cluster::addParticle(), G4INCL::CoulombNonRelativistic::bringToSurface(), G4INCL::ClusterDecay::decay(), G4INCL::CoulombNonRelativistic::distortOut(), G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), G4INCL::Nucleus::fillEventInfo(), G4INCL::ParticleEntryChannel::fillFinalState(), G4INCL::TransmissionChannel::fillFinalState(), G4INCL::Nucleus::finalizeProjectileRemnant(), G4INCL::PauliStandard::getBlockingProbability(), G4INCL::ClusteringModelIntercomparison::getCluster(), G4INCL::Nucleus::getConservationBalance(), G4INCL::Nucleus::getTransmissionBarrier(), G4INCL::SurfaceAvatar::getTransmissionProbability(), G4INCL::NuclearDensity::getTransmissionRadius(), G4INCL::Nucleus::insertParticle(), G4INCL::ClusterDecay::isStable(), G4INCL::ProjectileRemnant::removeParticle(), G4INCL::StandardPropagationModel::shootComposite(), and G4INCL::StandardPropagationModel::shootParticle().

◆ incrementNumberOfCollisions()

void G4INCL::Particle::incrementNumberOfCollisions ( )
inline

Increment the number of collisions undergone by the particle.

Definition at line 840 of file G4INCLParticle.hh.

840{ nCollisions++; }

◆ incrementNumberOfDecays()

void G4INCL::Particle::incrementNumberOfDecays ( )
inline

Increment the number of decays undergone by the particle.

Definition at line 849 of file G4INCLParticle.hh.

849{ nDecays++; }

◆ isAntiKaon()

G4bool G4INCL::Particle::isAntiKaon ( ) const
inline

Is this an antiKaon?

Definition at line 372 of file G4INCLParticle.hh.

372{ return (theType == KZeroBar || theType == KMinus); }

Referenced by G4INCL::CrossSectionsStrangeness::elastic(), G4INCL::BinaryCollisionAvatar::getChannel(), G4INCL::DecayAvatar::getChannel(), G4INCL::Nucleus::insertParticle(), isMeson(), isStrange(), G4INCL::CrossSectionsStrangeness::NKbelastic(), G4INCL::CrossSectionsStrangeness::NKbToL2pi(), G4INCL::CrossSectionsStrangeness::NKbToLpi(), G4INCL::CrossSectionsStrangeness::NKbToNKb(), G4INCL::CrossSectionsStrangeness::NKbToNKb2pi(), G4INCL::CrossSectionsStrangeness::NKbToNKbpi(), G4INCL::CrossSectionsStrangeness::NKbToS2pi(), G4INCL::CrossSectionsStrangeness::NKbToSpi(), and G4INCL::CrossSectionsStrangeness::total().

◆ isBaryon()

G4bool G4INCL::Particle::isBaryon ( ) const
inline

Is this a Baryon?

Definition at line 387 of file G4INCLParticle.hh.

387{ return (isNucleon() || isResonance() || isHyperon()); }
G4INCL::Particle::isHyperon
G4bool isHyperon() const
Is this an Hyperon?
Definition: G4INCLParticle.hh:381
G4INCL::Particle::isNucleon
G4bool isNucleon() const
Definition: G4INCLParticle.hh:303

Referenced by G4INCL::CDPP::processOneParticle().

◆ isCluster()

G4bool G4INCL::Particle::isCluster ( ) const
inline

Definition at line 883 of file G4INCLParticle.hh.

883 {
884 return (theType == Composite);
885 }

Referenced by getEmissionQValueCorrection(), and G4INCL::SurfaceAvatar::postInteraction().

◆ isDelta()

G4bool G4INCL::Particle::isDelta ( ) const
inline

Is it a Delta?

Definition at line 361 of file G4INCLParticle.hh.

361 {
362 return (theType==DeltaPlusPlus || theType==DeltaPlus ||
363 theType==DeltaZero || theType==DeltaMinus); }

Referenced by G4INCL::CrossSectionsINCL46::elastic(), G4INCL::CrossSectionsMultiPions::elastic(), G4INCL::CrossSectionsMultiPionsAndResonances::elastic(), G4INCL::CrossSectionsStrangeness::elastic(), G4INCL::CrossSectionsTruncatedMultiPions::elastic(), G4INCL::DeltaProductionChannel::fillFinalState(), G4INCL::NDeltaEtaProductionChannel::fillFinalState(), G4INCL::NDeltaOmegaProductionChannel::fillFinalState(), G4INCL::BinaryCollisionAvatar::getChannel(), G4INCL::DecayAvatar::getChannel(), G4INCL::NuclearPotential::INuclearPotential::getFermiMomentum(), isResonance(), G4INCL::CrossSectionsINCL46::NDeltaToNN(), G4INCL::CrossSectionsMultiPions::NDeltaToNN(), G4INCL::CrossSectionsMultiPions::NNTot(), G4INCL::RecombinationChannel::RecombinationChannel(), G4INCL::CrossSectionsINCL46::total(), G4INCL::CrossSectionsMultiPions::total(), G4INCL::CrossSectionsMultiPionsAndResonances::total(), and G4INCL::CrossSectionsStrangeness::total().

◆ isEta()

G4bool G4INCL::Particle::isEta ( ) const
inline

Is this an eta?

Definition at line 346 of file G4INCLParticle.hh.

346{ return (theType == Eta); }

Referenced by G4INCL::CrossSectionsMultiPionsAndResonances::elastic(), G4INCL::CrossSectionsStrangeness::elastic(), G4INCL::CrossSectionsMultiPionsAndResonances::etaNElastic(), G4INCL::CrossSectionsMultiPionsAndResonances::etaNToPiN(), G4INCL::CrossSectionsMultiPionsAndResonances::etaNToPiPiN(), G4INCL::BinaryCollisionAvatar::getChannel(), G4INCL::DecayAvatar::getChannel(), isMeson(), G4INCL::CrossSectionsMultiPionsAndResonances::total(), and G4INCL::CrossSectionsStrangeness::total().

◆ isEtaPrime()

G4bool G4INCL::Particle::isEtaPrime ( ) const
inline

Is this an etaprime?

Definition at line 352 of file G4INCLParticle.hh.

352{ return (theType == EtaPrime); }

Referenced by isMeson(), G4INCL::CrossSectionsMultiPionsAndResonances::total(), and G4INCL::CrossSectionsStrangeness::total().

◆ isHyperon()

G4bool G4INCL::Particle::isHyperon ( ) const
inline

Is this an Hyperon?

Definition at line 381 of file G4INCLParticle.hh.

381{ return (isLambda() || isSigma()); }
G4INCL::Particle::isLambda
G4bool isLambda() const
Is this a Lambda?
Definition: G4INCLParticle.hh:375
G4INCL::Particle::isSigma
G4bool isSigma() const
Is this a Sigma?
Definition: G4INCLParticle.hh:366

Referenced by G4INCL::CrossSectionsStrangeness::elastic(), isBaryon(), isStrange(), and G4INCL::CrossSectionsStrangeness::NYelastic().

◆ isKaon()

G4bool G4INCL::Particle::isKaon ( ) const
inline

Is this a Kaon?

Definition at line 369 of file G4INCLParticle.hh.

369{ return (theType == KPlus || theType == KZero); }

Referenced by G4INCL::CrossSectionsStrangeness::elastic(), G4INCL::ParticleEntryChannel::fillFinalState(), G4INCL::BinaryCollisionAvatar::getChannel(), G4INCL::SurfaceAvatar::getChannel(), G4INCL::Nucleus::insertParticle(), isMeson(), isStrange(), G4INCL::CrossSectionsStrangeness::NKelastic(), G4INCL::CrossSectionsStrangeness::NKToNK(), G4INCL::CrossSectionsStrangeness::NKToNK2pi(), G4INCL::CrossSectionsStrangeness::NKToNKpi(), and G4INCL::CrossSectionsStrangeness::total().

◆ isLambda()

G4bool G4INCL::Particle::isLambda ( ) const
inline

Is this a Lambda?

Definition at line 375 of file G4INCLParticle.hh.

375{ return (theType == Lambda); }

Referenced by G4INCL::NNToMissingStrangenessChannel::fillFinalState(), G4INCL::NpiToMissingStrangenessChannel::fillFinalState(), G4INCL::BinaryCollisionAvatar::getChannel(), G4INCL::Nucleus::getSurfaceRadius(), isHyperon(), isNucleonorLambda(), G4INCL::CrossSectionsStrangeness::NLToNS(), and G4INCL::CrossSectionsStrangeness::total().

◆ isMeson()

G4bool G4INCL::Particle::isMeson ( ) const
inline

Is this a Meson?

Definition at line 384 of file G4INCLParticle.hh.

384{ return (isPion() || isKaon() || isAntiKaon() || isEta() || isEtaPrime() || isOmega()); }
G4INCL::Particle::isEtaPrime
G4bool isEtaPrime() const
Is this an etaprime?
Definition: G4INCLParticle.hh:352
G4INCL::Particle::isOmega
G4bool isOmega() const
Is this an omega?
Definition: G4INCLParticle.hh:349
G4INCL::Particle::isEta
G4bool isEta() const
Is this an eta?
Definition: G4INCLParticle.hh:346
G4INCL::Particle::isPion
G4bool isPion() const
Is this a pion?
Definition: G4INCLParticle.hh:343
G4INCL::Particle::isAntiKaon
G4bool isAntiKaon() const
Is this an antiKaon?
Definition: G4INCLParticle.hh:372
G4INCL::Particle::isKaon
G4bool isKaon() const
Is this a Kaon?
Definition: G4INCLParticle.hh:369

Referenced by G4INCL::StandardPropagationModel::generateBinaryCollisionAvatar(), G4INCL::InteractionAvatar::preInteractionLocalEnergy(), G4INCL::CDPP::processOneParticle(), and G4INCL::StandardPropagationModel::shootParticle().

◆ isNucleon()

G4bool G4INCL::Particle::isNucleon ( ) const
inline

Is this a nucleon?

Definition at line 303 of file G4INCLParticle.hh.

303 {
304 if(theType == G4INCL::Proton || theType == G4INCL::Neutron)
305 return true;
306 else
307 return false;
308 };

Referenced by G4INCL::NuclearPotential::NuclearPotentialEnergyIsospin::computePotentialEnergy(), G4INCL::NuclearPotential::NuclearPotentialEnergyIsospinSmooth::computePotentialEnergy(), G4INCL::CrossSectionsINCL46::elastic(), G4INCL::CrossSectionsMultiPions::elastic(), G4INCL::CrossSectionsMultiPionsAndResonances::elastic(), G4INCL::CrossSectionsStrangeness::elastic(), G4INCL::CrossSectionsTruncatedMultiPions::elastic(), G4INCL::CrossSectionsINCL46::elasticNNLegacy(), G4INCL::EtaNElasticChannel::fillFinalState(), G4INCL::EtaNToPiNChannel::fillFinalState(), G4INCL::EtaNToPiPiNChannel::fillFinalState(), G4INCL::NDeltaToNNKKbChannel::fillFinalState(), G4INCL::NKbElasticChannel::fillFinalState(), G4INCL::NKbToL2piChannel::fillFinalState(), G4INCL::NKbToLpiChannel::fillFinalState(), G4INCL::NKbToNKb2piChannel::fillFinalState(), G4INCL::NKbToNKbChannel::fillFinalState(), G4INCL::NKbToNKbpiChannel::fillFinalState(), G4INCL::NKbToS2piChannel::fillFinalState(), G4INCL::NKbToSpiChannel::fillFinalState(), G4INCL::NKElasticChannel::fillFinalState(), G4INCL::NKToNK2piChannel::fillFinalState(), G4INCL::NKToNKChannel::fillFinalState(), G4INCL::NKToNKpiChannel::fillFinalState(), G4INCL::NLToNSChannel::fillFinalState(), G4INCL::NpiToLK2piChannel::fillFinalState(), G4INCL::NpiToLKChannel::fillFinalState(), G4INCL::NpiToLKpiChannel::fillFinalState(), G4INCL::NpiToNKKbChannel::fillFinalState(), G4INCL::NpiToSK2piChannel::fillFinalState(), G4INCL::NpiToSKChannel::fillFinalState(), G4INCL::NpiToSKpiChannel::fillFinalState(), G4INCL::NSToNLChannel::fillFinalState(), G4INCL::NSToNSChannel::fillFinalState(), G4INCL::NYElasticChannel::fillFinalState(), G4INCL::OmegaNElasticChannel::fillFinalState(), G4INCL::OmegaNToPiNChannel::fillFinalState(), G4INCL::OmegaNToPiPiNChannel::fillFinalState(), G4INCL::PiNElasticChannel::fillFinalState(), G4INCL::PiNToDeltaChannel::fillFinalState(), G4INCL::PiNToEtaChannel::fillFinalState(), G4INCL::PiNToMultiPionsChannel::fillFinalState(), G4INCL::PiNToOmegaChannel::fillFinalState(), G4INCL::StrangeAbsorbtionChannel::fillFinalState(), G4INCL::StandardPropagationModel::generateBinaryCollisionAvatar(), G4INCL::BinaryCollisionAvatar::getChannel(), G4INCL::DecayAvatar::getChannel(), G4INCL::Nucleus::getSurfaceRadius(), G4INCL::Nucleus::insertParticle(), isBaryon(), isNucleonorLambda(), G4INCL::CrossSectionsMultiPions::NNElastic(), G4INCL::CrossSectionsMultiPions::NNTot(), G4INCL::CrossSectionsMultiPions::piMinuspIne(), G4INCL::CrossSectionsMultiPions::piMinuspOnePi(), G4INCL::CrossSectionsMultiPions::piMinuspTwoPi(), G4INCL::CrossSectionsMultiPions::piNIne(), G4INCL::CrossSectionsMultiPions::piNOnePi(), G4INCL::CrossSectionsINCL46::piNToDelta(), G4INCL::CrossSectionsMultiPions::piNToxPiN(), G4INCL::CrossSectionsMultiPions::piNTwoPi(), G4INCL::CrossSectionsMultiPions::piPluspIne(), G4INCL::CrossSectionsMultiPions::piPluspOnePi(), G4INCL::CrossSectionsMultiPions::piPluspTwoPi(), G4INCL::CrossSectionsINCL46::total(), G4INCL::CrossSectionsMultiPions::total(), G4INCL::CrossSectionsMultiPionsAndResonances::total(), and G4INCL::CrossSectionsStrangeness::total().

◆ isNucleonorLambda()

G4bool G4INCL::Particle::isNucleonorLambda ( ) const
inline

Is this a Nucleon or a Lambda?

Definition at line 378 of file G4INCLParticle.hh.

378{ return (isNucleon() || isLambda()); }

Referenced by G4INCL::ParticleEntryChannel::fillFinalState(), and G4INCL::SurfaceAvatar::getChannel().

◆ isOmega()

G4bool G4INCL::Particle::isOmega ( ) const
inline

Is this an omega?

Definition at line 349 of file G4INCLParticle.hh.

349{ return (theType == Omega); }

Referenced by G4INCL::CrossSectionsMultiPionsAndResonances::elastic(), G4INCL::BinaryCollisionAvatar::getChannel(), G4INCL::DecayAvatar::getChannel(), isMeson(), G4INCL::CrossSectionsMultiPionsAndResonances::omegaNElastic(), G4INCL::CrossSectionsMultiPionsAndResonances::omegaNInelastic(), G4INCL::CrossSectionsMultiPionsAndResonances::omegaNToPiN(), G4INCL::CrossSectionsMultiPionsAndResonances::total(), and G4INCL::CrossSectionsStrangeness::total().

◆ isOutOfWell()

G4bool G4INCL::Particle::isOutOfWell ( ) const
inline

Check if the particle is out of its potential well.

Definition at line 862 of file G4INCLParticle.hh.

862{ return outOfWell; }

Referenced by G4INCL::NuclearPotential::INuclearPotential::computeKaonPotentialEnergy(), G4INCL::NuclearPotential::INuclearPotential::computePionPotentialEnergy(), and G4INCL::NuclearPotential::INuclearPotential::computePionResonancePotentialEnergy().

◆ isParticipant()

G4bool G4INCL::Particle::isParticipant ( ) const
inline

Definition at line 318 of file G4INCLParticle.hh.

318 {
319 return (theParticipantType==Participant);
320 }

Referenced by G4INCL::StandardPropagationModel::generateBinaryCollisionAvatar().

◆ isPhoton()

G4bool G4INCL::Particle::isPhoton ( ) const
inline

Is this a photon?

Definition at line 355 of file G4INCLParticle.hh.

355{ return (theType == Photon); }

◆ isPion()

G4bool G4INCL::Particle::isPion ( ) const
inline

Is this a pion?

Definition at line 343 of file G4INCLParticle.hh.

343{ return (theType == PiPlus || theType == PiZero || theType == PiMinus); }

Referenced by G4INCL::CrossSectionsMultiPions::elastic(), G4INCL::CrossSectionsMultiPionsAndResonances::elastic(), G4INCL::CrossSectionsStrangeness::elastic(), G4INCL::CrossSectionsTruncatedMultiPions::elastic(), G4INCL::NpiToMissingStrangenessChannel::fillFinalState(), G4INCL::StandardPropagationModel::generateBinaryCollisionAvatar(), G4INCL::Nucleus::insertParticle(), isMeson(), G4INCL::CrossSectionsStrangeness::NpiToLK(), G4INCL::CrossSectionsStrangeness::NpiToLK2pi(), G4INCL::CrossSectionsStrangeness::NpiToLKpi(), G4INCL::CrossSectionsStrangeness::NpiToMissingStrangeness(), G4INCL::CrossSectionsStrangeness::NpiToNKKb(), G4INCL::CrossSectionsStrangeness::NpiToSK(), G4INCL::CrossSectionsStrangeness::NpiToSK2pi(), G4INCL::CrossSectionsStrangeness::NpiToSKpi(), G4INCL::CrossSectionsMultiPionsAndResonances::piMinuspToEtaN(), G4INCL::CrossSectionsMultiPionsAndResonances::piMinuspToOmegaN(), G4INCL::CrossSectionsINCL46::piNToDelta(), G4INCL::CrossSectionsMultiPions::piNToDelta(), G4INCL::CrossSectionsMultiPions::piNTot(), G4INCL::CrossSectionsINCL46::total(), G4INCL::CrossSectionsMultiPions::total(), G4INCL::CrossSectionsMultiPionsAndResonances::total(), and G4INCL::CrossSectionsStrangeness::total().

◆ isProjectileSpectator()

G4bool G4INCL::Particle::isProjectileSpectator ( ) const
inline

Definition at line 326 of file G4INCLParticle.hh.

326 {
327 return (theParticipantType==ProjectileSpectator);
328 }

Referenced by G4INCL::SurfaceAvatar::getChannel().

◆ isResonance()

G4bool G4INCL::Particle::isResonance ( ) const
inline

Is it a resonance?

Definition at line 358 of file G4INCLParticle.hh.

358{ return isDelta(); }
G4INCL::Particle::isDelta
G4bool isDelta() const
Is it a Delta?
Definition: G4INCLParticle.hh:361

Referenced by G4INCL::NDeltaToDeltaLKChannel::fillFinalState(), G4INCL::NDeltaToDeltaSKChannel::fillFinalState(), G4INCL::NDeltaToNSKChannel::fillFinalState(), G4INCL::StandardPropagationModel::generateBinaryCollisionAvatar(), G4INCL::SurfaceAvatar::getChannel(), G4INCL::Nucleus::getSurfaceRadius(), isBaryon(), Particle(), G4INCL::CDPP::processOneParticle(), and setType().

◆ isSigma()

G4bool G4INCL::Particle::isSigma ( ) const
inline

Is this a Sigma?

Definition at line 366 of file G4INCLParticle.hh.

366{ return (theType == SigmaPlus || theType == SigmaZero || theType == SigmaMinus); }

Referenced by G4INCL::BinaryCollisionAvatar::getChannel(), G4INCL::DecayAvatar::getChannel(), isHyperon(), G4INCL::CrossSectionsStrangeness::NSToNL(), G4INCL::CrossSectionsStrangeness::NSToNS(), and G4INCL::CrossSectionsStrangeness::total().

◆ isStrange()

G4bool G4INCL::Particle::isStrange ( ) const
inline

Is this an Strange?

Definition at line 390 of file G4INCLParticle.hh.

390{ return (isKaon() || isAntiKaon() || isHyperon()); }

◆ isTargetSpectator()

G4bool G4INCL::Particle::isTargetSpectator ( ) const
inline

Definition at line 322 of file G4INCLParticle.hh.

322 {
323 return (theParticipantType==TargetSpectator);
324 }

Referenced by G4INCL::SurfaceAvatar::getChannel(), G4INCL::Nucleus::insertParticle(), G4INCL::SurfaceAvatar::postInteraction(), and G4INCL::BinaryCollisionAvatar::preInteraction().

◆ lorentzContract()

void G4INCL::Particle::lorentzContract ( const ThreeVector &  aBoostVector,
const ThreeVector &  refPos 
)
inline

Lorentz-contract the particle position around some center.

Apply Lorentz contraction to the position component along the direction of the boost vector.

Parameters
aBoostVectorthe boost vector (velocity) [c]
refPosthe reference position

Definition at line 440 of file G4INCLParticle.hh.

440 {
441 const G4double beta2 = aBoostVector.mag2();
442 const G4double gamma = 1.0 / std::sqrt(1.0 - beta2);
443 const ThreeVector theRelativePosition = thePosition - refPos;
444 const ThreeVector transversePosition = theRelativePosition - aBoostVector * (theRelativePosition.dot(aBoostVector) / aBoostVector.mag2());
445 const ThreeVector longitudinalPosition = theRelativePosition - transversePosition;
446
447 thePosition = refPos + transversePosition + longitudinalPosition / gamma;
448 }

◆ makeParticipant()

virtual void G4INCL::Particle::makeParticipant ( )
inlinevirtual

Reimplemented in G4INCL::Cluster.

Definition at line 330 of file G4INCLParticle.hh.

330 {
331 theParticipantType = Participant;
332 }

Referenced by G4INCL::Store::loadParticles(), and G4INCL::Cluster::makeParticipant().

◆ makeProjectileSpectator()

virtual void G4INCL::Particle::makeProjectileSpectator ( )
inlinevirtual

Reimplemented in G4INCL::Cluster.

Definition at line 338 of file G4INCLParticle.hh.

338 {
339 theParticipantType = ProjectileSpectator;
340 }

Referenced by G4INCL::Cluster::makeProjectileSpectator(), and G4INCL::StandardPropagationModel::shootParticle().

◆ makeTargetSpectator()

virtual void G4INCL::Particle::makeTargetSpectator ( )
inlinevirtual

Reimplemented in G4INCL::Cluster.

Definition at line 334 of file G4INCLParticle.hh.

334 {
335 theParticipantType = TargetSpectator;
336 }

Referenced by G4INCL::Cluster::makeTargetSpectator().

◆ MergeVectorBias() [1/2]

std::vector< G4int > G4INCL::Particle::MergeVectorBias ( Particle const *const  p1,
Particle const *const  p2 
)
static

Definition at line 223 of file G4INCLParticle.cc.

223 {
224 std::vector<G4int> MergedVectorBias;
225 std::vector<G4int> VectorBias1 = p1->getBiasCollisionVector();
226 std::vector<G4int> VectorBias2 = p2->getBiasCollisionVector();
227 G4int i = 0;
228 G4int j = 0;
229 if(VectorBias1.size()==0 && VectorBias2.size()==0) return MergedVectorBias;
230 else if(VectorBias1.size()==0) return VectorBias2;
231 else if(VectorBias2.size()==0) return VectorBias1;
232
233 while(i < G4int(VectorBias1.size()) || j < G4int(VectorBias2.size())){
234 if(VectorBias1[i]==VectorBias2[j]){
235 MergedVectorBias.push_back(VectorBias1[i]);
236 i++;
237 j++;
238 if(i == G4int(VectorBias1.size())){
239 for(;j<G4int(VectorBias2.size());j++) MergedVectorBias.push_back(VectorBias2[j]);
240 }
241 else if(j == G4int(VectorBias2.size())){
242 for(;i<G4int(VectorBias1.size());i++) MergedVectorBias.push_back(VectorBias1[i]);
243 }
244 } else if(VectorBias1[i]<VectorBias2[j]){
245 MergedVectorBias.push_back(VectorBias1[i]);
246 i++;
247 if(i == G4int(VectorBias1.size())){
248 for(;j<G4int(VectorBias2.size());j++) MergedVectorBias.push_back(VectorBias2[j]);
249 }
250 }
251 else {
252 MergedVectorBias.push_back(VectorBias2[j]);
253 j++;
254 if(j == G4int(VectorBias2.size())){
255 for(;i<G4int(VectorBias1.size());i++) MergedVectorBias.push_back(VectorBias1[i]);
256 }
257 }
258 }
259 return MergedVectorBias;
260 }

Referenced by G4INCL::BinaryCollisionAvatar::getChannel(), G4INCL::ParticleList::getParticleListBias(), and G4INCL::ParticleList::getParticleListBiasVector().

◆ MergeVectorBias() [2/2]

std::vector< G4int > G4INCL::Particle::MergeVectorBias ( std::vector< G4int >  p1,
Particle const *const  p2 
)
static

Definition at line 262 of file G4INCLParticle.cc.

262 {
263 std::vector<G4int> MergedVectorBias;
264 std::vector<G4int> VectorBias = p2->getBiasCollisionVector();
265 G4int i = 0;
266 G4int j = 0;
267 if(p1.size()==0 && VectorBias.size()==0) return MergedVectorBias;
268 else if(p1.size()==0) return VectorBias;
269 else if(VectorBias.size()==0) return p1;
270
271 while(i < G4int(p1.size()) || j < G4int(VectorBias.size())){
272 if(p1[i]==VectorBias[j]){
273 MergedVectorBias.push_back(p1[i]);
274 i++;
275 j++;
276 if(i == G4int(p1.size())){
277 for(;j<G4int(VectorBias.size());j++) MergedVectorBias.push_back(VectorBias[j]);
278 }
279 else if(j == G4int(VectorBias.size())){
280 for(;i<G4int(p1.size());i++) MergedVectorBias.push_back(p1[i]);
281 }
282 } else if(p1[i]<VectorBias[j]){
283 MergedVectorBias.push_back(p1[i]);
284 i++;
285 if(i == G4int(p1.size())){
286 for(;j<G4int(VectorBias.size());j++) MergedVectorBias.push_back(VectorBias[j]);
287 }
288 }
289 else {
290 MergedVectorBias.push_back(VectorBias[j]);
291 j++;
292 if(j == G4int(VectorBias.size())){
293 for(;i<G4int(p1.size());i++) MergedVectorBias.push_back(p1[i]);
294 }
295 }
296 }
297 return MergedVectorBias;
298 }

◆ operator=()

Particle & G4INCL::Particle::operator= ( const Particle &  rhs)
inline

Assignment operator.

Does not copy the particle ID.

Definition at line 168 of file G4INCLParticle.hh.

168 {
169 Particle temporaryParticle(rhs);
170 swap(temporaryParticle);
171 return *this;
172 }
G4INCL::Particle::swap
void swap(Particle &rhs)
Helper method for the assignment operator.
Definition: G4INCLParticle.hh:125

Referenced by G4INCL::Cluster::operator=().

◆ print()

std::string G4INCL::Particle::print ( ) const
inline

Definition at line 953 of file G4INCLParticle.hh.

953 {
954 std::stringstream ss;
955 ss << "Particle (ID = " << ID << ") type = ";
956 ss << ParticleTable::getName(theType);
957 ss << '\n'
958 << " energy = " << theEnergy << '\n'
959 << " momentum = "
960 << theMomentum.print()
961 << '\n'
962 << " position = "
963 << thePosition.print()
964 << '\n';
965 return ss.str();
966 };
G4INCL::ThreeVector::print
std::string print() const
Definition: G4INCLThreeVector.hh:200

Referenced by adjustMomentumFromEnergy(), G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), G4INCL::ParticleEntryChannel::fillFinalState(), G4INCL::BinaryCollisionAvatar::getChannel(), G4INCL::KinematicsUtils::getLocalEnergy(), G4INCL::StandardPropagationModel::getReflectionTime(), G4INCL::CrossSectionsMultiPions::piNTot(), and G4INCL::ProjectileRemnant::removeParticle().

◆ propagate()

void G4INCL::Particle::propagate ( G4double  step)
inline

Definition at line 829 of file G4INCLParticle.hh.

829 {
830 thePosition += ((*thePropagationMomentum)*(step/(*thePropagationEnergy)));
831 };

Referenced by G4INCL::StandardPropagationModel::generateBinaryCollisionAvatar().

◆ rotateMomentum()

virtual void G4INCL::Particle::rotateMomentum ( const G4double  angle,
const ThreeVector &  axis 
)
inlinevirtual

Rotate the particle momentum.

Parameters
anglethe rotation angle
axisa unit vector representing the rotation axis

Reimplemented in G4INCL::Cluster.

Definition at line 948 of file G4INCLParticle.hh.

948 {
949 theMomentum.rotate(angle, axis);
950 theFrozenMomentum.rotate(angle, axis);
951 }
G4INCL::ThreeVector::rotate
void rotate(const G4double angle, const ThreeVector &axis)
Rotate the vector by a given angle around a given axis.
Definition: G4INCLThreeVector.hh:179

Referenced by G4INCL::Cluster::rotateMomentum(), and rotatePositionAndMomentum().

◆ rotatePosition()

virtual void G4INCL::Particle::rotatePosition ( const G4double  angle,
const ThreeVector &  axis 
)
inlinevirtual

Rotate the particle position.

Parameters
anglethe rotation angle
axisa unit vector representing the rotation axis

Reimplemented in G4INCL::Cluster.

Definition at line 939 of file G4INCLParticle.hh.

939 {
940 thePosition.rotate(angle, axis);
941 }

Referenced by G4INCL::Cluster::rotatePosition(), and rotatePositionAndMomentum().

◆ rotatePositionAndMomentum()

virtual void G4INCL::Particle::rotatePositionAndMomentum ( const G4double  angle,
const ThreeVector &  axis 
)
inlinevirtual

Rotate the particle position and momentum.

Parameters
anglethe rotation angle
axisa unit vector representing the rotation axis

Definition at line 929 of file G4INCLParticle.hh.

929 {
930 rotatePosition(angle, axis);
931 rotateMomentum(angle, axis);
932 }
G4INCL::Particle::rotateMomentum
virtual void rotateMomentum(const G4double angle, const ThreeVector &axis)
Rotate the particle momentum.
Definition: G4INCLParticle.hh:948
G4INCL::Particle::rotatePosition
virtual void rotatePosition(const G4double angle, const ThreeVector &axis)
Rotate the particle position.
Definition: G4INCLParticle.hh:939

◆ rpCorrelate()

void G4INCL::Particle::rpCorrelate ( )
inline

Make the particle follow a strict r-p correlation.

Definition at line 1008 of file G4INCLParticle.hh.

1008{ rpCorrelated = true; }

Referenced by G4INCL::InteractionAvatar::bringParticleInside(), G4INCL::ParticleEntryAvatar::postInteraction(), and G4INCL::SurfaceAvatar::postInteraction().

◆ rpDecorrelate()

void G4INCL::Particle::rpDecorrelate ( )
inline

Make the particle not follow a strict r-p correlation.

Definition at line 1011 of file G4INCLParticle.hh.

1011{ rpCorrelated = false; }

◆ setBiasCollisionVector()

void G4INCL::Particle::setBiasCollisionVector ( std::vector< G4int >  BiasCollisionVector)
inline

Set the vector list of biased vertices on the particle path.

Definition at line 1041 of file G4INCLParticle.hh.

1041 {
1042 this->theBiasCollisionVector = BiasCollisionVector;
1043 this->setParticleBias(Particle::getBiasFromVector(BiasCollisionVector));
1044 }
G4INCL::Particle::setParticleBias
void setParticleBias(G4double ParticleBias)
Set the particle bias.
Definition: G4INCLParticle.hh:1035
G4INCL::Particle::getBiasFromVector
static G4double getBiasFromVector(std::vector< G4int > VectorBias)
Definition: G4INCLParticle.cc:211

Referenced by G4INCL::Nucleus::decayOutgoingPionResonances(), G4INCL::Nucleus::decayOutgoingSigmaZero(), and G4INCL::SurfaceAvatar::postInteraction().

◆ setEmissionTime()

void G4INCL::Particle::setEmissionTime ( G4double  t)
inline

Definition at line 864 of file G4INCLParticle.hh.

864{ emissionTime = t; }

Referenced by G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), and G4INCL::Nucleus::finalizeProjectileRemnant().

◆ setEnergy()

void G4INCL::Particle::setEnergy ( G4double  energy)
inline

Set the energy of the particle in MeV.

Definition at line 786 of file G4INCLParticle.hh.

787 {
788 this->theEnergy = energy;
789 };

Referenced by G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), G4INCL::DeltaProductionChannel::fillFinalState(), G4INCL::EtaNElasticChannel::fillFinalState(), G4INCL::EtaNToPiNChannel::fillFinalState(), G4INCL::NSToNLChannel::fillFinalState(), G4INCL::NSToNSChannel::fillFinalState(), G4INCL::OmegaNElasticChannel::fillFinalState(), G4INCL::OmegaNToPiNChannel::fillFinalState(), G4INCL::CrossSections::interactionDistanceKbarN(), G4INCL::CrossSections::interactionDistanceKN(), G4INCL::CrossSections::interactionDistanceNN(), G4INCL::CrossSections::interactionDistancePiN(), G4INCL::CrossSections::interactionDistanceYN(), G4INCL::StandardPropagationModel::shootParticle(), G4INCL::KinematicsUtils::transformToLocalEnergyFrame(), and G4INCL::Nucleus::useFusionKinematics().

◆ setFrozenEnergy()

void G4INCL::Particle::setFrozenEnergy ( const G4double  energy)
inline

Set the frozen particle momentum.

Definition at line 891 of file G4INCLParticle.hh.

891{ theFrozenEnergy = energy; }

◆ setFrozenMomentum()

void G4INCL::Particle::setFrozenMomentum ( const ThreeVector &  momentum)
inline

Set the frozen particle momentum.

Definition at line 888 of file G4INCLParticle.hh.

888{ theFrozenMomentum = momentum; }

◆ setHelicity()

void G4INCL::Particle::setHelicity ( G4double  h)
inline

Definition at line 827 of file G4INCLParticle.hh.

827{ theHelicity = h; };

Referenced by G4INCL::DeltaDecayChannel::fillFinalState(), G4INCL::DeltaProductionChannel::fillFinalState(), G4INCL::NDeltaEtaProductionChannel::fillFinalState(), and G4INCL::NDeltaOmegaProductionChannel::fillFinalState().

◆ setINCLBiasVector()

void G4INCL::Particle::setINCLBiasVector ( std::vector< G4double >  NewVector)
static

Definition at line 306 of file G4INCLParticle.cc.

306 {
307 Particle::INCLBiasVector = NewVector;
308 }

◆ setINCLMass()

void G4INCL::Particle::setINCLMass ( )
inline

Set the mass of the Particle to its table mass.

Definition at line 589 of file G4INCLParticle.hh.

589{ setMass(getINCLMass()); }

Referenced by G4INCL::Cluster::Cluster(), setType(), and G4INCL::StandardPropagationModel::shootParticle().

◆ setMass()

void G4INCL::Particle::setMass ( G4double  mass)
inline

Set the mass of the particle in MeV/c^2.

Definition at line 778 of file G4INCLParticle.hh.

779 {
780 this->theMass = mass;
781 }

Referenced by G4INCL::Nucleus::computeRecoilKinematics(), G4INCL::DeltaProductionChannel::fillFinalState(), G4INCL::NDeltaEtaProductionChannel::fillFinalState(), G4INCL::NDeltaOmegaProductionChannel::fillFinalState(), G4INCL::NDeltaToDeltaLKChannel::fillFinalState(), G4INCL::NDeltaToDeltaSKChannel::fillFinalState(), G4INCL::Nucleus::finalizeProjectileRemnant(), G4INCL::PhaseSpaceKopylov::generate(), Particle(), setINCLMass(), setRealMass(), setTableMass(), and G4INCL::Nucleus::useFusionKinematics().

◆ setMomentum()

virtual void G4INCL::Particle::setMomentum ( const G4INCL::ThreeVector &  momentum)
inlinevirtual

Set the momentum vector.

Definition at line 808 of file G4INCLParticle.hh.

809 {
810 this->theMomentum = momentum;
811 };

Referenced by G4INCL::Nucleus::decayOutgoingPionResonances(), G4INCL::Nucleus::decayOutgoingSigmaZero(), G4INCL::DeltaDecayChannel::fillFinalState(), G4INCL::DeltaProductionChannel::fillFinalState(), G4INCL::ElasticChannel::fillFinalState(), G4INCL::EtaNElasticChannel::fillFinalState(), G4INCL::EtaNToPiNChannel::fillFinalState(), G4INCL::NKbElasticChannel::fillFinalState(), G4INCL::NKbToLpiChannel::fillFinalState(), G4INCL::NKbToNKbChannel::fillFinalState(), G4INCL::NKbToSpiChannel::fillFinalState(), G4INCL::NKElasticChannel::fillFinalState(), G4INCL::NKToNKChannel::fillFinalState(), G4INCL::NSToNLChannel::fillFinalState(), G4INCL::NSToNSChannel::fillFinalState(), G4INCL::OmegaNElasticChannel::fillFinalState(), G4INCL::OmegaNToPiNChannel::fillFinalState(), G4INCL::PionResonanceDecayChannel::fillFinalState(), G4INCL::RecombinationChannel::fillFinalState(), G4INCL::ReflectionChannel::fillFinalState(), G4INCL::SigmaZeroDecayChannel::fillFinalState(), G4INCL::StrangeAbsorbtionChannel::fillFinalState(), G4INCL::PhaseSpaceKopylov::generate(), and G4INCL::Nucleus::useFusionKinematics().

◆ setNumberOfCollisions()

void G4INCL::Particle::setNumberOfCollisions ( G4int  n)
inline

Set the number of collisions undergone by the particle.

Definition at line 837 of file G4INCLParticle.hh.

837{ nCollisions = n; }

◆ setNumberOfDecays()

void G4INCL::Particle::setNumberOfDecays ( G4int  n)
inline

Set the number of decays undergone by the particle.

Definition at line 846 of file G4INCLParticle.hh.

846{ nDecays = n; }

◆ setNumberOfKaon()

void G4INCL::Particle::setNumberOfKaon ( const G4int  NK)
inline

Definition at line 1054 of file G4INCLParticle.hh.

1054{ theNKaon = NK; }

Referenced by G4INCL::ParticleEntryChannel::fillFinalState(), G4INCL::SurfaceAvatar::getChannel(), and G4INCL::BinaryCollisionAvatar::postInteraction().

◆ setOutOfWell()

void G4INCL::Particle::setOutOfWell ( )
inline

Mark the particle as out of its potential well.

This flag is used to control pions created outside their potential well in delta decay. The pion potential checks it and returns zero if it is true (necessary in order to correctly enforce energy conservation). The Nucleus::applyFinalState() method uses it to determine whether new avatars should be generated for the particle.

Definition at line 859 of file G4INCLParticle.hh.

859{ outOfWell = true; }

◆ setParticipantType()

void G4INCL::Particle::setParticipantType ( ParticipantType const  p)
inline

Definition at line 314 of file G4INCLParticle.hh.

314 {
315 theParticipantType = p;
316 }

◆ setParticleBias()

void G4INCL::Particle::setParticleBias ( G4double  ParticleBias)
inline

Set the particle bias.

Definition at line 1035 of file G4INCLParticle.hh.

1035{ this->theParticleBias = ParticleBias; }

Referenced by setBiasCollisionVector().

◆ setPosition()

virtual void G4INCL::Particle::setPosition ( const G4INCL::ThreeVector &  position)
inlinevirtual

Reimplemented in G4INCL::Cluster.

Definition at line 821 of file G4INCLParticle.hh.

822 {
823 this->thePosition = position;
824 };
position
#define position
Definition: xmlparse.cc:622

Referenced by G4INCL::InteractionAvatar::bringParticleInside(), G4INCL::CoulombNone::bringToSurface(), G4INCL::ReflectionChannel::fillFinalState(), G4INCL::ClusteringModelIntercomparison::getCluster(), G4INCL::ParticleSampler::sampleParticlesIntoList(), G4INCL::Cluster::setPosition(), and G4INCL::StandardPropagationModel::shootParticle().

◆ setPotentialEnergy()

void G4INCL::Particle::setPotentialEnergy ( G4double  v)
inline

Set the particle potential energy.

Definition at line 765 of file G4INCLParticle.hh.

765{ thePotentialEnergy = v; }

Referenced by G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), G4INCL::Store::loadParticles(), and G4INCL::Nucleus::updatePotentialEnergy().

◆ setRealMass()

void G4INCL::Particle::setRealMass ( )
inline

Set the mass of the Particle to its real mass.

Definition at line 583 of file G4INCLParticle.hh.

583{ setMass(getRealMass()); }
G4INCL::Particle::getRealMass
G4double getRealMass() const
Get the real particle mass.
Definition: G4INCLParticle.hh:540

Referenced by G4INCL::ClusterDecay::decay().

◆ setTableMass()

void G4INCL::Particle::setTableMass ( )
inline

Set the mass of the Particle to its table mass.

Definition at line 586 of file G4INCLParticle.hh.

586{ setMass(getTableMass()); }

Referenced by G4INCL::Nucleus::decayOutgoingPionResonances(), G4INCL::Nucleus::decayOutgoingSigmaZero(), G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), G4INCL::ProjectileRemnant::ProjectileRemnant(), and G4INCL::ProjectileRemnant::reset().

◆ setType()

void G4INCL::Particle::setType ( ParticleType  t)
inline

Definition at line 187 of file G4INCLParticle.hh.

187 {
188 theType = t;
189 switch(theType)
190 {
191 case DeltaPlusPlus:
192 theA = 1;
193 theZ = 2;
194 theS = 0;
195 break;
196 case Proton:
197 case DeltaPlus:
198 theA = 1;
199 theZ = 1;
200 theS = 0;
201 break;
202 case Neutron:
203 case DeltaZero:
204 theA = 1;
205 theZ = 0;
206 theS = 0;
207 break;
208 case DeltaMinus:
209 theA = 1;
210 theZ = -1;
211 theS = 0;
212 break;
213 case PiPlus:
214 theA = 0;
215 theZ = 1;
216 theS = 0;
217 break;
218 case PiZero:
219 case Eta:
220 case Omega:
221 case EtaPrime:
222 case Photon:
223 theA = 0;
224 theZ = 0;
225 theS = 0;
226 break;
227 case PiMinus:
228 theA = 0;
229 theZ = -1;
230 theS = 0;
231 break;
232 case Lambda:
233 theA = 1;
234 theZ = 0;
235 theS = -1;
236 break;
237 case SigmaPlus:
238 theA = 1;
239 theZ = 1;
240 theS = -1;
241 break;
242 case SigmaZero:
243 theA = 1;
244 theZ = 0;
245 theS = -1;
246 break;
247 case SigmaMinus:
248 theA = 1;
249 theZ = -1;
250 theS = -1;
251 break;
252 case KPlus:
253 theA = 0;
254 theZ = 1;
255 theS = 1;
256 break;
257 case KZero:
258 theA = 0;
259 theZ = 0;
260 theS = 1;
261 break;
262 case KZeroBar:
263 theA = 0;
264 theZ = 0;
265 theS = -1;
266 break;
267 case KShort:
268 theA = 0;
269 theZ = 0;
270// theS should not be defined
271 break;
272 case KLong:
273 theA = 0;
274 theZ = 0;
275// theS should not be defined
276 break;
277 case KMinus:
278 theA = 0;
279 theZ = -1;
280 theS = -1;
281 break;
282 case Composite:
283 // INCL_ERROR("Trying to set particle type to Composite! Construct a Cluster object instead" << '\n');
284 theA = 0;
285 theZ = 0;
286 theS = 0;
287 break;
288 case UnknownParticle:
289 theA = 0;
290 theZ = 0;
291 theS = 0;
292 INCL_ERROR("Trying to set particle type to Unknown!" << '\n');
293 break;
294 }
295
296 if( !isResonance() && t!=Composite )
297 setINCLMass();
298 }
G4INCL::Particle::setINCLMass
void setINCLMass()
Set the mass of the Particle to its table mass.
Definition: G4INCLParticle.hh:589

Referenced by G4INCL::Cluster::Cluster(), G4INCL::ClusterDecay::decay(), G4INCL::DeltaDecayChannel::fillFinalState(), G4INCL::DeltaProductionChannel::fillFinalState(), G4INCL::ElasticChannel::fillFinalState(), G4INCL::EtaNToPiNChannel::fillFinalState(), G4INCL::EtaNToPiPiNChannel::fillFinalState(), G4INCL::NDeltaEtaProductionChannel::fillFinalState(), G4INCL::NDeltaOmegaProductionChannel::fillFinalState(), G4INCL::NDeltaToDeltaLKChannel::fillFinalState(), G4INCL::NDeltaToDeltaSKChannel::fillFinalState(), G4INCL::NDeltaToNLKChannel::fillFinalState(), G4INCL::NDeltaToNNKKbChannel::fillFinalState(), G4INCL::NDeltaToNSKChannel::fillFinalState(), G4INCL::NeutralKaonDecayChannel::fillFinalState(), G4INCL::NKbToL2piChannel::fillFinalState(), G4INCL::NKbToLpiChannel::fillFinalState(), G4INCL::NKbToNKb2piChannel::fillFinalState(), G4INCL::NKbToNKbChannel::fillFinalState(), G4INCL::NKbToNKbpiChannel::fillFinalState(), G4INCL::NKbToS2piChannel::fillFinalState(), G4INCL::NKbToSpiChannel::fillFinalState(), G4INCL::NKToNK2piChannel::fillFinalState(), G4INCL::NKToNKChannel::fillFinalState(), G4INCL::NKToNKpiChannel::fillFinalState(), G4INCL::NNEtaToMultiPionsChannel::fillFinalState(), G4INCL::NNOmegaToMultiPionsChannel::fillFinalState(), G4INCL::NNToMissingStrangenessChannel::fillFinalState(), G4INCL::NNToMultiPionsChannel::fillFinalState(), G4INCL::NNToNLK2piChannel::fillFinalState(), G4INCL::NNToNLKChannel::fillFinalState(), G4INCL::NNToNLKpiChannel::fillFinalState(), G4INCL::NNToNNEtaChannel::fillFinalState(), G4INCL::NNToNNKKbChannel::fillFinalState(), G4INCL::NNToNNOmegaChannel::fillFinalState(), G4INCL::NNToNSK2piChannel::fillFinalState(), G4INCL::NNToNSKChannel::fillFinalState(), G4INCL::NNToNSKpiChannel::fillFinalState(), G4INCL::NpiToMissingStrangenessChannel::fillFinalState(), G4INCL::NSToNLChannel::fillFinalState(), G4INCL::NSToNSChannel::fillFinalState(), G4INCL::OmegaNToPiNChannel::fillFinalState(), G4INCL::OmegaNToPiPiNChannel::fillFinalState(), G4INCL::PiNToMultiPionsChannel::fillFinalState(), G4INCL::PionResonanceDecayChannel::fillFinalState(), G4INCL::RecombinationChannel::fillFinalState(), G4INCL::SigmaZeroDecayChannel::fillFinalState(), G4INCL::StrangeAbsorbtionChannel::fillFinalState(), and Particle().

◆ setUncorrelatedMomentum()

void G4INCL::Particle::setUncorrelatedMomentum ( const G4double  p)
inline

Set the uncorrelated momentum.

Definition at line 1005 of file G4INCLParticle.hh.

1005{ uncorrelatedMomentum = p; }

◆ swap()

void G4INCL::Particle::swap ( Particle &  rhs)
inlineprotected

Helper method for the assignment operator.

Definition at line 125 of file G4INCLParticle.hh.

125 {
126 std::swap(theZ, rhs.theZ);
127 std::swap(theA, rhs.theA);
128 std::swap(theS, rhs.theS);
129 std::swap(theParticipantType, rhs.theParticipantType);
130 std::swap(theType, rhs.theType);
131 if(rhs.thePropagationEnergy == &(rhs.theFrozenEnergy))
132 thePropagationEnergy = &theFrozenEnergy;
133 else
134 thePropagationEnergy = &theEnergy;
135 std::swap(theEnergy, rhs.theEnergy);
136 std::swap(theFrozenEnergy, rhs.theFrozenEnergy);
137 if(rhs.thePropagationMomentum == &(rhs.theFrozenMomentum))
138 thePropagationMomentum = &theFrozenMomentum;
139 else
140 thePropagationMomentum = &theMomentum;
141 std::swap(theMomentum, rhs.theMomentum);
142 std::swap(theFrozenMomentum, rhs.theFrozenMomentum);
143 std::swap(thePosition, rhs.thePosition);
144 std::swap(nCollisions, rhs.nCollisions);
145 std::swap(nDecays, rhs.nDecays);
146 std::swap(thePotentialEnergy, rhs.thePotentialEnergy);
147 // ID intentionally not swapped
148
149 std::swap(theHelicity, rhs.theHelicity);
150 std::swap(emissionTime, rhs.emissionTime);
151 std::swap(outOfWell, rhs.outOfWell);
152
153 std::swap(theMass, rhs.theMass);
154 std::swap(rpCorrelated, rhs.rpCorrelated);
155 std::swap(uncorrelatedMomentum, rhs.uncorrelatedMomentum);
156
157 std::swap(theParticleBias, rhs.theParticleBias);
158 std::swap(theBiasCollisionVector, rhs.theBiasCollisionVector);
159
160 }

Referenced by operator=(), and G4INCL::Cluster::swap().

◆ thawPropagation()

void G4INCL::Particle::thawPropagation ( )
inline

Unfreeze particle propagation.

Make the particle use theMomentum and theEnergy for propagation. Call this method to restore the normal propagation if the freezePropagation() method has been called.

Definition at line 919 of file G4INCLParticle.hh.

919 {
920 thePropagationMomentum = &theMomentum;
921 thePropagationEnergy = &theEnergy;
922 }

Referenced by G4INCL::ReflectionChannel::fillFinalState().

Member Data Documentation

◆ ID

long G4INCL::Particle::ID
protected

Definition at line 1093 of file G4INCLParticle.hh.

Referenced by dump(), getID(), Particle(), G4INCL::Cluster::print(), and print().

◆ INCLBiasVector

std::vector< G4double > G4INCL::Particle::INCLBiasVector
static

Time ordered vector of all bias applied.

/!\ Caution /!\ methods Assotiated to G4VectorCache<T> are: Push_back(…), operator[], Begin(), End(), Clear(), Size() and Pop_back()

Definition at line 1071 of file G4INCLParticle.hh.

Referenced by FillINCLBiasVector(), getBiasFromVector(), getTotalBias(), G4INCL::INCL::processEvent(), and setINCLBiasVector().

◆ nCollisions

G4int G4INCL::Particle::nCollisions
protected

Definition at line 1090 of file G4INCLParticle.hh.

Referenced by G4INCL::Cluster::addParticle(), getNumberOfCollisions(), incrementNumberOfCollisions(), G4INCL::ProjectileRemnant::reset(), setNumberOfCollisions(), swap(), and G4INCL::Cluster::updateClusterParameters().

◆ nDecays

G4int G4INCL::Particle::nDecays
protected

Definition at line 1091 of file G4INCLParticle.hh.

Referenced by getNumberOfDecays(), incrementNumberOfDecays(), setNumberOfDecays(), and swap().

◆ nextBiasedCollisionID

G4ThreadLocal G4int G4INCL::Particle::nextBiasedCollisionID = 0
static

Definition at line 1077 of file G4INCLParticle.hh.

Referenced by FillINCLBiasVector(), G4INCL::InteractionAvatar::postInteraction(), and G4INCL::INCL::processEvent().

◆ rpCorrelated

G4bool G4INCL::Particle::rpCorrelated
protected

Definition at line 1095 of file G4INCLParticle.hh.

Referenced by getReflectionMomentum(), rpCorrelate(), rpDecorrelate(), and swap().

◆ theA

G4int G4INCL::Particle::theA
protected

Definition at line 1080 of file G4INCLParticle.hh.

Referenced by G4INCL::ProjectileRemnant::addAllDynamicalSpectators(), G4INCL::ProjectileRemnant::addMostDynamicalSpectators(), G4INCL::Cluster::addParticle(), G4INCL::Nucleus::applyFinalState(), G4INCL::Cluster::Cluster(), G4INCL::Nucleus::computeRecoilKinematics(), G4INCL::Nucleus::decayInsideDeltas(), G4INCL::Nucleus::decayInsideStrangeParticles(), G4INCL::Nucleus::decayMe(), G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), getA(), getEmissionQValueCorrection(), getINCLMass(), getRealMass(), G4INCL::Cluster::getSpecies(), getTableMass(), getTransferQValueCorrection(), G4INCL::Cluster::initializeParticles(), G4INCL::Nucleus::insertParticle(), G4INCL::Cluster::internalBoostToCM(), G4INCL::Nucleus::Nucleus(), G4INCL::Cluster::print(), G4INCL::ProjectileRemnant::removeParticle(), G4INCL::ProjectileRemnant::reset(), G4INCL::Cluster::setA(), setType(), swap(), and G4INCL::Cluster::updateClusterParameters().

◆ theEnergy

G4double G4INCL::Particle::theEnergy
protected

Definition at line 1083 of file G4INCLParticle.hh.

Referenced by G4INCL::ProjectileRemnant::addAllDynamicalSpectators(), G4INCL::ProjectileRemnant::addMostDynamicalSpectators(), G4INCL::Cluster::addParticle(), adjustEnergyFromMomentum(), adjustMomentumFromEnergy(), boost(), boostVector(), dump(), getBeta(), getEnergy(), getInvariantMass(), getKineticEnergy(), G4INCL::Cluster::internalBoostToCM(), Particle(), G4INCL::Cluster::print(), print(), G4INCL::ProjectileRemnant::removeParticle(), G4INCL::ProjectileRemnant::reset(), setEnergy(), swap(), thawPropagation(), G4INCL::Cluster::updateClusterParameters(), and G4INCL::Nucleus::useFusionKinematics().

◆ theFrozenEnergy

G4double G4INCL::Particle::theFrozenEnergy
protected

Definition at line 1085 of file G4INCLParticle.hh.

Referenced by freezePropagation(), getFrozenEnergy(), Particle(), setFrozenEnergy(), and swap().

◆ theFrozenMomentum

G4INCL::ThreeVector G4INCL::Particle::theFrozenMomentum
protected

Definition at line 1088 of file G4INCLParticle.hh.

Referenced by freezePropagation(), getFrozenMomentum(), Particle(), rotateMomentum(), setFrozenMomentum(), and swap().

◆ theMomentum

G4INCL::ThreeVector G4INCL::Particle::theMomentum
protected

Definition at line 1086 of file G4INCLParticle.hh.

Referenced by G4INCL::ProjectileRemnant::addAllDynamicalSpectators(), G4INCL::ProjectileRemnant::addMostDynamicalSpectators(), G4INCL::Cluster::addParticle(), adjustEnergyFromMomentum(), adjustMomentumFromEnergy(), boost(), boostVector(), G4INCL::Nucleus::computeRecoilKinematics(), dump(), G4INCL::Cluster::freezeInternalMotion(), getAngularMomentum(), getBeta(), getInvariantMass(), getMomentum(), getReflectionMomentum(), G4INCL::Cluster::internalBoostToCM(), Particle(), G4INCL::Cluster::print(), print(), G4INCL::ProjectileRemnant::removeParticle(), G4INCL::ProjectileRemnant::reset(), rotateMomentum(), setMomentum(), swap(), thawPropagation(), G4INCL::Cluster::updateClusterParameters(), and G4INCL::Nucleus::useFusionKinematics().

◆ theNKaon

G4int G4INCL::Particle::theNKaon
protected

The number of Kaons inside the nucleus (update during the cascade)

Definition at line 1100 of file G4INCLParticle.hh.

Referenced by G4INCL::Nucleus::emitInsideKaon(), getNumberOfKaon(), and setNumberOfKaon().

◆ theParticipantType

ParticipantType G4INCL::Particle::theParticipantType
protected

Definition at line 1081 of file G4INCLParticle.hh.

Referenced by getParticipantType(), isParticipant(), isProjectileSpectator(), isTargetSpectator(), makeParticipant(), makeProjectileSpectator(), makeTargetSpectator(), Particle(), setParticipantType(), and swap().

◆ theParticleBias

G4double G4INCL::Particle::theParticleBias
protected

Definition at line 1098 of file G4INCLParticle.hh.

Referenced by getParticleBias(), setParticleBias(), and swap().

◆ thePosition

G4INCL::ThreeVector G4INCL::Particle::thePosition
protected

Definition at line 1089 of file G4INCLParticle.hh.

Referenced by G4INCL::Cluster::addParticle(), G4INCL::Cluster::boost(), G4INCL::Cluster::Cluster(), G4INCL::Nucleus::computeRecoilKinematics(), dump(), getAngularMomentum(), getCosRPAngle(), getLongitudinalPosition(), getPosition(), getTransversePosition(), G4INCL::Cluster::initializeParticles(), G4INCL::Nucleus::initializeParticles(), G4INCL::Cluster::internalBoostToCM(), lorentzContract(), G4INCL::Cluster::print(), print(), propagate(), G4INCL::ProjectileRemnant::reset(), rotatePosition(), setPosition(), G4INCL::Cluster::setPosition(), swap(), and G4INCL::Cluster::updateClusterParameters().

◆ thePotentialEnergy

G4double G4INCL::Particle::thePotentialEnergy
protected

Definition at line 1092 of file G4INCLParticle.hh.

Referenced by G4INCL::Cluster::addParticle(), getPotentialEnergy(), G4INCL::ProjectileRemnant::reset(), setPotentialEnergy(), swap(), and G4INCL::Cluster::updateClusterParameters().

◆ thePropagationEnergy

G4double* G4INCL::Particle::thePropagationEnergy
protected

Definition at line 1084 of file G4INCLParticle.hh.

Referenced by freezePropagation(), Particle(), swap(), and thawPropagation().

◆ thePropagationMomentum

G4INCL::ThreeVector* G4INCL::Particle::thePropagationMomentum
protected

Definition at line 1087 of file G4INCLParticle.hh.

Referenced by freezePropagation(), getCosRPAngle(), getLongitudinalPosition(), getPropagationVelocity(), Particle(), swap(), and thawPropagation().

◆ theS

G4int G4INCL::Particle::theS
protected

Definition at line 1080 of file G4INCLParticle.hh.

Referenced by G4INCL::ProjectileRemnant::addAllDynamicalSpectators(), G4INCL::ProjectileRemnant::addMostDynamicalSpectators(), G4INCL::Cluster::addParticle(), G4INCL::Nucleus::applyFinalState(), G4INCL::Cluster::Cluster(), G4INCL::Nucleus::computeRecoilKinematics(), G4INCL::Nucleus::decayMe(), G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), getEmissionQValueCorrection(), getINCLMass(), getRealMass(), getS(), G4INCL::Cluster::getSpecies(), getTableMass(), getTransferQValueCorrection(), G4INCL::Nucleus::insertParticle(), G4INCL::Nucleus::Nucleus(), G4INCL::Cluster::print(), G4INCL::Cluster::setS(), setType(), swap(), and G4INCL::Cluster::updateClusterParameters().

◆ theType

G4INCL::ParticleType G4INCL::Particle::theType
protected

Definition at line 1082 of file G4INCLParticle.hh.

Referenced by dump(), getINCLMass(), getRealMass(), getSpecies(), getTableMass(), getType(), isAntiKaon(), isCluster(), isDelta(), isEta(), isEtaPrime(), isKaon(), isLambda(), isNucleon(), isOmega(), isPhoton(), isPion(), isSigma(), G4INCL::Cluster::print(), print(), setType(), and swap().

◆ theZ

G4int G4INCL::Particle::theZ
protected

Definition at line 1080 of file G4INCLParticle.hh.

Referenced by G4INCL::ProjectileRemnant::addAllDynamicalSpectators(), G4INCL::ProjectileRemnant::addMostDynamicalSpectators(), G4INCL::Cluster::addParticle(), G4INCL::Nucleus::applyFinalState(), G4INCL::Cluster::Cluster(), G4INCL::Nucleus::computeRecoilKinematics(), G4INCL::Nucleus::decayInsideDeltas(), G4INCL::Nucleus::decayInsideStrangeParticles(), G4INCL::Nucleus::decayMe(), G4INCL::Nucleus::emitInsideKaon(), G4INCL::Nucleus::emitInsideLambda(), G4INCL::Nucleus::emitInsidePions(), G4INCL::Nucleus::emitInsideStrangeParticles(), getEmissionQValueCorrection(), getINCLMass(), getRealMass(), G4INCL::Cluster::getSpecies(), getTableMass(), getTransferQValueCorrection(), G4INCL::Nucleus::getTransmissionBarrier(), getZ(), G4INCL::Cluster::initializeParticles(), G4INCL::Nucleus::insertParticle(), G4INCL::Nucleus::Nucleus(), G4INCL::Cluster::print(), G4INCL::ProjectileRemnant::removeParticle(), G4INCL::ProjectileRemnant::reset(), setType(), G4INCL::Cluster::setZ(), swap(), and G4INCL::Cluster::updateClusterParameters().

◆ uncorrelatedMomentum

G4double G4INCL::Particle::uncorrelatedMomentum
protected

Definition at line 1096 of file G4INCLParticle.hh.

Referenced by getReflectionMomentum(), setUncorrelatedMomentum(), and swap().

The documentation for this class was generated from the following files: