Geant4 10.7.0
Toolkit for the simulation of the passage of particles through matter
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G4INCLKinematicsUtils.hh
Go to the documentation of this file.
1//
2// ********************************************************************
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24// ********************************************************************
25//
26// INCL++ intra-nuclear cascade model
27// Alain Boudard, CEA-Saclay, France
28// Joseph Cugnon, University of Liege, Belgium
29// Jean-Christophe David, CEA-Saclay, France
30// Pekka Kaitaniemi, CEA-Saclay, France, and Helsinki Institute of Physics, Finland
31// Sylvie Leray, CEA-Saclay, France
32// Davide Mancusi, CEA-Saclay, France
33//
34#define INCLXX_IN_GEANT4_MODE 1
35
36#include "globals.hh"
37
38#ifndef KinematicsUtils_hh
39#define KinematicsUtils_hh 1
40
41#include "G4INCLThreeVector.hh"
42#include "G4INCLParticle.hh"
43#include "G4INCLNucleus.hh"
45
46namespace G4INCL {
47
48 namespace KinematicsUtils {
49
50 void transformToLocalEnergyFrame(Nucleus const * const n, Particle * const p);
51 G4double getLocalEnergy(Nucleus const * const n, Particle * const p);
52
53 ThreeVector makeBoostVector(Particle const * const p1, Particle const * const p2);
54 G4double totalEnergyInCM(Particle const * const p1, Particle const * const p2);
55 G4double squareTotalEnergyInCM(Particle const * const p1, Particle const * const p2);
56
57 /** \brief gives the momentum in the CM frame of two particles.
58 *
59 * The formula is the following:
60 * \f[ p_{CM}^2 = \frac{z^2 - m_1^2 m_2^2}{2 z + m_1^2 + m_2^2} \f]
61 * where \f$z\f$ is the scalar product of the momentum four-vectors:
62 * \f[ z = E_1 E_2 - \vec{p}_1\cdot\vec{p}_2 \f]
63 *
64 * \param p1 pointer to particle 1
65 * \param p2 pointer to particle 2
66 * \return the absolute value of the momentum of any of the two particles in
67 * the CM frame, in MeV/c.
68 */
69 G4double momentumInCM(Particle const * const p1, Particle const * const p2);
70
71 G4double momentumInCM(const G4double E, const G4double M1, const G4double M2);
72
73 /** \brief gives the momentum in the lab frame of two particles.
74 *
75 * Assumes particle 1 carries all the momentum and particle 2 is at rest.
76 *
77 * The formula is the following:
78 * \f[ p_{lab}^2 = \frac{s^2 - 2 s (m_1^2 + m_2^2) + {(m_1^2 - m_2^2)}^2}{4 m_2^2} \f]
79 *
80 * \param p1 pointer to particle 1
81 * \param p2 pointer to particle 2
82 * \return the absolute value of the momentum of particle 1 in the lab frame,
83 * in MeV/c
84 */
85 G4double momentumInLab(Particle const * const p1, Particle const * const p2);
86 G4double momentumInLab(const G4double s, const G4double m1, const G4double m2);
89 G4double energy(const ThreeVector &p, const G4double m);
90 G4double invariantMass(const G4double E, const ThreeVector & p);
93 }
94}
95
96#endif
double G4double
Definition: G4Types.hh:83
G4double squareTotalEnergyInCM(Particle const *const p1, Particle const *const p2)
G4double invariantMass(const G4double E, const ThreeVector &p)
ThreeVector sumMomenta(const ParticleList &)
G4double gammaFromKineticEnergy(const ParticleSpecies &p, const G4double EKin)
G4double squareInvariantMass(const G4double E, const ThreeVector &p)
G4double sumTotalEnergies(const ParticleList &)
G4double energy(const ThreeVector &p, const G4double m)
ThreeVector makeBoostVector(Particle const *const p1, Particle const *const p2)
G4double totalEnergyInCM(Particle const *const p1, Particle const *const p2)
void transformToLocalEnergyFrame(Nucleus const *const n, Particle *const p)
G4double momentumInLab(Particle const *const p1, Particle const *const p2)
gives the momentum in the lab frame of two particles.
G4double momentumInCM(Particle const *const p1, Particle const *const p2)
gives the momentum in the CM frame of two particles.
G4double getLocalEnergy(Nucleus const *const n, Particle *const p)