Geant4 9.6.0
Toolkit for the simulation of the passage of particles through matter
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G4INCLKinematicsUtils.hh
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1//
2// ********************************************************************
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24// ********************************************************************
25//
26// INCL++ intra-nuclear cascade model
27// Pekka Kaitaniemi, CEA and Helsinki Institute of Physics
28// Davide Mancusi, CEA
29// Alain Boudard, CEA
30// Sylvie Leray, CEA
31// Joseph Cugnon, University of Liege
32//
33// INCL++ revision: v5.1.8
34//
35#define INCLXX_IN_GEANT4_MODE 1
36
37#include "globals.hh"
38
39#ifndef KinematicsUtils_hh
40#define KinematicsUtils_hh 1
41
42#include "G4INCLThreeVector.hh"
43#include "G4INCLParticle.hh"
44#include "G4INCLNucleus.hh"
46
47namespace G4INCL {
48
50 public:
51 static void transformToLocalEnergyFrame(Nucleus const * const n, Particle * const p);
52 static G4double getLocalEnergy(Nucleus const * const n, Particle * const p);
53
54 static ThreeVector makeBoostVector(Particle const * const p1, Particle const * const p2);
55 static G4double totalEnergyInCM(Particle const * const p1, Particle const * const p2);
56 static G4double squareTotalEnergyInCM(Particle const * const p1, Particle const * const p2);
57
58 /** \brief gives the momentum in the CM frame of two particles.
59 *
60 * The formula is the following:
61 * \f[ p_{CM}^2 = \frac{z^2 - m_1^2 m_2^2}{2 z + m_1^2 + m_2^2} \f]
62 * where \f$z\f$ is the scalar product of the momentum four-vectors:
63 * \f[ z = E_1 E_2 - \vec{p}_1\cdot\vec{p}_2 \f]
64 *
65 * \param p1 pointer to particle 1
66 * \param p2 pointer to particle 2
67 * \return the absolute value of the momentum of any of the two particles in
68 * the CM frame, in MeV/c.
69 */
70 static G4double momentumInCM(Particle const * const p1, Particle const * const p2);
71
72 static G4double momentumInCM(const G4double E, const G4double M1, const G4double M2);
73
74 /** \brief gives the momentum in the lab frame of two particles.
75 *
76 * Assumes particle 1 carries all the momentum and particle 2 is at rest.
77 *
78 * The formula is the following:
79 * \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]
80 *
81 * \param p1 pointer to particle 1
82 * \param p2 pointer to particle 2
83 * \return the absolute value of the momentum of particle 1 in the lab frame,
84 * in MeV/c
85 */
86 static G4double momentumInLab(Particle const * const p1, Particle const * const p2);
87 static G4double momentumInLab(const G4double s, const G4double m1, const G4double m2);
89 static ThreeVector sumMomenta(const ParticleList &);
90 static G4double energy(const ThreeVector &p, const G4double m);
91 static G4double invariantMass(const G4double E, const ThreeVector & p);
92 static G4double gammaFromKineticEnergy(const ParticleSpecies &p, const G4double EKin);
93 };
94}
95
96#endif
double G4double
Definition: G4Types.hh:64
static G4double squareTotalEnergyInCM(Particle const *const p1, Particle const *const p2)
static G4double invariantMass(const G4double E, const ThreeVector &p)
static ThreeVector sumMomenta(const ParticleList &)
static G4double gammaFromKineticEnergy(const ParticleSpecies &p, const G4double EKin)
static G4double sumTotalEnergies(const ParticleList &)
static G4double energy(const ThreeVector &p, const G4double m)
static ThreeVector makeBoostVector(Particle const *const p1, Particle const *const p2)
static G4double totalEnergyInCM(Particle const *const p1, Particle const *const p2)
static void transformToLocalEnergyFrame(Nucleus const *const n, Particle *const p)
static G4double momentumInLab(Particle const *const p1, Particle const *const p2)
gives the momentum in the lab frame of two particles.
static G4double momentumInCM(Particle const *const p1, Particle const *const p2)
gives the momentum in the CM frame of two particles.
static G4double getLocalEnergy(Nucleus const *const n, Particle *const p)
std::list< G4INCL::Particle * > ParticleList