G4INCLKinematicsUtils.hh

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//
// INCL++ intra-nuclear cascade model
// Alain Boudard, CEA-Saclay, France
// Joseph Cugnon, University of Liege, Belgium
// Jean-Christophe David, CEA-Saclay, France
// Pekka Kaitaniemi, CEA-Saclay, France, and Helsinki Institute of Physics, Finland
// Sylvie Leray, CEA-Saclay, France
// Davide Mancusi, CEA-Saclay, France
//
#define INCLXX_IN_GEANT4_MODE 1
 
#include "globals.hh"
 
#ifndef KinematicsUtils_hh
#define KinematicsUtils_hh 1
 
#include "G4INCLThreeVector.hh"
#include "G4INCLParticle.hh"
#include "G4INCLNucleus.hh"
#include "G4INCLParticleSpecies.hh"
 
namespace G4INCL {
 
  namespace KinematicsUtils {
 
    G4double fiveParFit(const G4double a, const G4double b, const G4double c, const G4double d, const G4double e, const G4double x);
    G4double compute_xs(const std::vector<G4double> coefficients, const G4double pLab);
 
    void transformToLocalEnergyFrame(Nucleus const * const n, Particle * const p);
    G4double getLocalEnergy(Nucleus const * const n, Particle * const p);
 
    ThreeVector makeBoostVector(Particle const * const p1, Particle const * const p2);
    G4double totalEnergyInCM(Particle const * const p1, Particle const * const p2);
    G4double squareTotalEnergyInCM(Particle const * const p1, Particle const * const p2);
 
    /** \brief gives the momentum in the CM frame of two particles.
     *
     * The formula is the following:
     * \f[ p_{CM}^2 = \frac{z^2 - m_1^2 m_2^2}{2 z + m_1^2 + m_2^2} \f]
     * where \f$z\f$ is the scalar product of the momentum four-vectors:
     * \f[ z = E_1 E_2 - \vec{p}_1\cdot\vec{p}_2 \f]
     *
     * \param p1 pointer to particle 1
     * \param p2 pointer to particle 2
     * \return the absolute value of the momentum of any of the two particles in
     * the CM frame, in MeV/c.
     */
    G4double momentumInCM(Particle const * const p1, Particle const * const p2);
 
    G4double momentumInCM(const G4double E, const G4double M1, const G4double M2);
 
    /** \brief gives the momentum in the lab frame of two particles.
     *
     * Assumes particle 1 carries all the momentum and particle 2 is at rest.
     *
     * The formula is the following:
     * \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]
     *
     * \param p1 pointer to particle 1
     * \param p2 pointer to particle 2
     * \return the absolute value of the momentum of particle 1 in the lab frame,
     * in MeV/c
     */
    G4double momentumInLab(Particle const * const p1, Particle const * const p2);
    G4double momentumInLab(const G4double s, const G4double m1, const G4double m2);
    G4double sumTotalEnergies(const ParticleList &);
    ThreeVector sumMomenta(const ParticleList &);
    G4double energy(const ThreeVector &p, const G4double m);
    G4double invariantMass(const G4double E, const ThreeVector & p);
    G4double squareInvariantMass(const G4double E, const ThreeVector & p);
    G4double gammaFromKineticEnergy(const ParticleSpecies &p, const G4double EKin);
  }
}
 
#endif