| 1 | // |
|---|
| 2 | // ******************************************************************** |
|---|
| 3 | // * License and Disclaimer * |
|---|
| 4 | // * * |
|---|
| 5 | // * The Geant4 software is copyright of the Copyright Holders of * |
|---|
| 6 | // * the Geant4 Collaboration. It is provided under the terms and * |
|---|
| 7 | // * conditions of the Geant4 Software License, included in the file * |
|---|
| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These * |
|---|
| 9 | // * include a list of copyright holders. * |
|---|
| 10 | // * * |
|---|
| 11 | // * Neither the authors of this software system, nor their employing * |
|---|
| 12 | // * institutes,nor the agencies providing financial support for this * |
|---|
| 13 | // * work make any representation or warranty, express or implied, * |
|---|
| 14 | // * regarding this software system or assume any liability for its * |
|---|
| 15 | // * use. Please see the license in the file LICENSE and URL above * |
|---|
| 16 | // * for the full disclaimer and the limitation of liability. * |
|---|
| 17 | // * * |
|---|
| 18 | // * This code implementation is the result of the scientific and * |
|---|
| 19 | // * technical work of the GEANT4 collaboration. * |
|---|
| 20 | // * By using, copying, modifying or distributing the software (or * |
|---|
| 21 | // * any work based on the software) you agree to acknowledge its * |
|---|
| 22 | // * use in resulting scientific publications, and indicate your * |
|---|
| 23 | // * acceptance of all terms of the Geant4 Software license. * |
|---|
| 24 | // ******************************************************************** |
|---|
| 25 | // |
|---|
| 26 | #ifndef G4FieldPropagation_h |
|---|
| 27 | #define G4FieldPropagation_h 1 |
|---|
| 28 | |
|---|
| 29 | #include "G4KineticTrackVector.hh" |
|---|
| 30 | |
|---|
| 31 | class G4FieldPropagation |
|---|
| 32 | { |
|---|
| 33 | public: |
|---|
| 34 | G4FieldPropagation() {} |
|---|
| 35 | G4FieldPropagation(const G4FieldPropagation &) {} |
|---|
| 36 | |
|---|
| 37 | virtual ~G4FieldPropagation() {} |
|---|
| 38 | |
|---|
| 39 | // Operators |
|---|
| 40 | const G4FieldPropagation & operator=(const G4FieldPropagation &right); |
|---|
| 41 | |
|---|
| 42 | int operator==(const G4FieldPropagation &right) const; |
|---|
| 43 | int operator!=(const G4FieldPropagation &right) const; |
|---|
| 44 | |
|---|
| 45 | // Methods |
|---|
| 46 | |
|---|
| 47 | // only theActive are propagated, nothing else |
|---|
| 48 | // only theSpectators define the field, nothing else |
|---|
| 49 | virtual void Transport(G4KineticTrackVector &theActive, const G4KineticTrackVector &theSpectators, G4double theTimeStep) = 0; |
|---|
| 50 | |
|---|
| 51 | virtual G4double GetExcitationEnergy(G4int nHit, const G4KineticTrackVector &theParticles) = 0; |
|---|
| 52 | |
|---|
| 53 | // methods for calculating potentials for different types of particles |
|---|
| 54 | virtual void Init(G4int z, G4int a) = 0; // prepare potentials' functions |
|---|
| 55 | |
|---|
| 56 | // aPosition is relative to the nucleus center |
|---|
| 57 | virtual G4double GetNeutronPotential(G4double radius) = 0; |
|---|
| 58 | virtual G4double GetNeutronPotential(G4ThreeVector &aPosition) = 0; |
|---|
| 59 | |
|---|
| 60 | virtual G4double GetProtonPotential(G4double radius) = 0; |
|---|
| 61 | virtual G4double GetProtonPotential(G4ThreeVector &aPosition) = 0; |
|---|
| 62 | |
|---|
| 63 | virtual G4double GetAntiprotonPotential(G4double radius) = 0; |
|---|
| 64 | virtual G4double GetAntiprotonPotential(G4ThreeVector &aPosition) = 0; |
|---|
| 65 | |
|---|
| 66 | virtual G4double GetKaonPotential(G4double radius) = 0; |
|---|
| 67 | virtual G4double GetKaonPotential(G4ThreeVector &aPosition) = 0; |
|---|
| 68 | |
|---|
| 69 | virtual G4double GetPionPotential(G4double radius) = 0; |
|---|
| 70 | virtual G4double GetPionPotential(G4ThreeVector &aPosition) = 0; |
|---|
| 71 | }; |
|---|
| 72 | |
|---|
| 73 | #endif // G4FieldPropagation_h |
|---|
| 74 | |
|---|
| 75 | |
|---|
