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Geant4/processes/hadronic/models/inclxx/incl_physics/include/G4INCLCoulombDistortion.hh

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 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 /** \file G4INCLCoulombDistortion.hh
 39  * \brief Static class for selecting Coulomb distortion.
 40  *
 41  * \date 14 February 2011
 42  * \author Davide Mancusi
 43  */
 44 
 45 #ifndef G4INCLCOULOMBDISTORTION_HH_
 46 #define G4INCLCOULOMBDISTORTION_HH_
 47 
 48 #include "G4INCLParticle.hh"
 49 #include "G4INCLNucleus.hh"
 50 #include "G4INCLICoulomb.hh"
 51 #include "G4INCLConfig.hh"
 52 
 53 namespace G4INCL {
 54 
 55   /**
 56    * Coulomb distortion
 57    */
 58   namespace CoulombDistortion {
 59     /** \brief Modify the momentum of an incoming particle and position it on
 60      *         the surface of the nucleus.
 61      *
 62      * This method places Particle p on the surface of Nucleus n and modifies
 63      * the direction of its momentum to be tangent to the Coulomb trajectory in
 64      * that point.
 65      *
 66      * The input particle has to be prepared with its asymptotic momentum. Its
 67      * position is used only for the purpose of computing the asymptotic impact
 68      * parameter; in other words, this method only uses the components of the
 69      * position that are perpendicular to the momentum. The remaining component
 70      * is not used, and can be set to any value.
 71      *
 72      * This method returns a ParticleEntry avatar for the projectile.
 73      *
 74      * \param p incoming particle
 75      * \param n distorting nucleus
 76      * \return the ParticleEntryAvatar for the projectile particle
 77      **/
 78     ParticleEntryAvatar *bringToSurface(Particle *p, Nucleus * const n);
 79 
 80     /** \brief Modify the momentum of an incoming cluster and position it on
 81      *         the surface of the target.
 82      *
 83      * Same as the Particle-based bringToSurface method, but for incoming heavy
 84      * ions.
 85      *
 86      * This method returns a list of ParticleEntry avatars for the participant
 87      * nucleons
 88      *
 89      * \param c incoming heavy ion
 90      * \param n distorting nucleus
 91      * \return a list of ParticleEntryAvatars
 92      **/
 93     IAvatarList bringToSurface(Cluster * const c, Nucleus * const n);
 94 
 95     /** \brief Modify the momentum of an outgoing particle. */
 96     void distortOut(ParticleList const &pL, Nucleus const * const n);
 97 
 98     /** \brief Return the maximum impact parameter for Coulomb-distorted
 99      *         trajectories. **/
100     G4double maxImpactParameter(ParticleSpecies const &p, const G4double kinE, Nucleus const * const n);
101 
102     /** \brief Return the maximum impact parameter for Coulomb-distorted
103      *         trajectories. **/
104     G4double maxImpactParameter(Particle const * const p, Nucleus const * const n);
105 
106     /** \brief Set the Coulomb-distortion algorithm. */
107     void setCoulomb(ICoulomb * const coulomb);
108 
109     /** \brief Delete the Coulomb-distortion object. */
110     void deleteCoulomb();
111 
112     /// \brief Initialize the Coulomb-distortion algorithm
113     void initialize(Config const * const theConfig);
114 
115   }
116 }
117 
118 #endif /* G4INCLCOULOMBDISTORTION_HH_ */
119