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G4INCLKinematicsUtils.hh
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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 #define INCLXX_IN_GEANT4_MODE 1
34 
35 #include "globals.hh"
36 
37 #ifndef KinematicsUtils_hh
38 #define KinematicsUtils_hh 1
39 
40 #include "G4INCLThreeVector.hh"
41 #include "G4INCLParticle.hh"
42 #include "G4INCLNucleus.hh"
43 #include "G4INCLParticleSpecies.hh"
44 
45 namespace G4INCL {
46 
47  namespace KinematicsUtils {
48 
49  void transformToLocalEnergyFrame(Nucleus const * const n, Particle * const p);
50  G4double getLocalEnergy(Nucleus const * const n, Particle * const p);
51 
52  ThreeVector makeBoostVector(Particle const * const p1, Particle const * const p2);
53  G4double totalEnergyInCM(Particle const * const p1, Particle const * const p2);
54  G4double squareTotalEnergyInCM(Particle const * const p1, Particle const * const p2);
55 
56  /** \brief gives the momentum in the CM frame of two particles.
57  *
58  * The formula is the following:
59  * \f[ p_{CM}^2 = \frac{z^2 - m_1^2 m_2^2}{2 z + m_1^2 + m_2^2} \f]
60  * where \f$z\f$ is the scalar product of the momentum four-vectors:
61  * \f[ z = E_1 E_2 - \vec{p}_1\cdot\vec{p}_2 \f]
62  *
63  * \param p1 pointer to particle 1
64  * \param p2 pointer to particle 2
65  * \return the absolute value of the momentum of any of the two particles in
66  * the CM frame, in MeV/c.
67  */
68  G4double momentumInCM(Particle const * const p1, Particle const * const p2);
69 
70  G4double momentumInCM(const G4double E, const G4double M1, const G4double M2);
71 
72  /** \brief gives the momentum in the lab frame of two particles.
73  *
74  * Assumes particle 1 carries all the momentum and particle 2 is at rest.
75  *
76  * The formula is the following:
77  * \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]
78  *
79  * \param p1 pointer to particle 1
80  * \param p2 pointer to particle 2
81  * \return the absolute value of the momentum of particle 1 in the lab frame,
82  * in MeV/c
83  */
84  G4double momentumInLab(Particle const * const p1, Particle const * const p2);
85  G4double momentumInLab(const G4double s, const G4double m1, const G4double m2);
88  G4double energy(const ThreeVector &p, const G4double m);
89  G4double invariantMass(const G4double E, const ThreeVector & p);
92  }
93 }
94 
95 #endif
void transformToLocalEnergyFrame(Nucleus const *const n, Particle *const p)
const XML_Char * s
G4double squareTotalEnergyInCM(Particle const *const p1, Particle const *const p2)
ThreeVector sumMomenta(const ParticleList &)
const char * p
Definition: xmltok.h:285
G4double momentumInCM(Particle const *const p1, Particle const *const p2)
gives the momentum in the CM frame of two particles.
ThreeVector makeBoostVector(Particle const *const p1, Particle const *const p2)
G4double gammaFromKineticEnergy(const ParticleSpecies &p, const G4double EKin)
const G4int n
G4double invariantMass(const G4double E, const ThreeVector &p)
G4double energy(const ThreeVector &p, const G4double m)
G4double squareInvariantMass(const G4double E, const ThreeVector &p)
G4double momentumInLab(Particle const *const p1, Particle const *const p2)
gives the momentum in the lab frame of two particles.
double G4double
Definition: G4Types.hh:76
G4double totalEnergyInCM(Particle const *const p1, Particle const *const p2)
G4double sumTotalEnergies(const ParticleList &)
G4double getLocalEnergy(Nucleus const *const n, Particle *const p)