108 lines
3.9 KiB
C++
108 lines
3.9 KiB
C++
//
|
|
// ********************************************************************
|
|
// * License and Disclaimer *
|
|
// * *
|
|
// * The Geant4 software is copyright of the Copyright Holders of *
|
|
// * the Geant4 Collaboration. It is provided under the terms and *
|
|
// * conditions of the Geant4 Software License, included in the file *
|
|
// * LICENSE and available at http://cern.ch/geant4/license . These *
|
|
// * include a list of copyright holders. *
|
|
// * *
|
|
// * Neither the authors of this software system, nor their employing *
|
|
// * institutes,nor the agencies providing financial support for this *
|
|
// * work make any representation or warranty, express or implied, *
|
|
// * regarding this software system or assume any liability for its *
|
|
// * use. Please see the license in the file LICENSE and URL above *
|
|
// * for the full disclaimer and the limitation of liability. *
|
|
// * *
|
|
// * This code implementation is the result of the scientific and *
|
|
// * technical work of the GEANT4 collaboration. *
|
|
// * By using, copying, modifying or distributing the software (or *
|
|
// * any work based on the software) you agree to acknowledge its *
|
|
// * use in resulting scientific publications, and indicate your *
|
|
// * acceptance of all terms of the Geant4 Software license. *
|
|
// ********************************************************************
|
|
//
|
|
// G4EqEMFieldWithSpin
|
|
//
|
|
// Class description:
|
|
//
|
|
// This is the right-hand side of equation of motion in a combined
|
|
// electric and magnetic field.
|
|
|
|
// Authors: Chris Gong & Peter Gumplinger (TRIUMF), 30.08.2007
|
|
// -------------------------------------------------------------------
|
|
#ifndef G4EQEMFIELDWITHSPIN_HH
|
|
#define G4EQEMFIELDWITHSPIN_HH
|
|
|
|
#include "G4ChargeState.hh"
|
|
#include "G4EquationOfMotion.hh"
|
|
|
|
class G4ElectroMagneticField;
|
|
|
|
/**
|
|
* @brief G4EqEMFieldWithSpin implements the right-hand side of equation
|
|
* of motion in a combined electric and magnetic field.
|
|
*/
|
|
|
|
class G4EqEMFieldWithSpin : public G4EquationOfMotion
|
|
{
|
|
public:
|
|
|
|
/**
|
|
* Constructor for G4EqEMFieldWithSpin.
|
|
* @param[in] emField Pointer to the electromagnetic field.
|
|
*/
|
|
G4EqEMFieldWithSpin(G4ElectroMagneticField* emField );
|
|
|
|
/**
|
|
* Default Destructor.
|
|
*/
|
|
~G4EqEMFieldWithSpin() override = default;
|
|
|
|
/**
|
|
* Sets the charge, momentum and mass of the current particle.
|
|
* Used to set the equation's coefficients.
|
|
* @param[in] particleCharge Magnetic charge and moments in e+ units.
|
|
* @param[in] MomentumXc Particle momentum.
|
|
* @param[in] mass Particle mass.
|
|
*/
|
|
void SetChargeMomentumMass(G4ChargeState particleCharge, // in e+ units
|
|
G4double MomentumXc,
|
|
G4double mass) override;
|
|
|
|
/**
|
|
* Calculates the value of the derivative, given the value of the
|
|
* electromagnetic field.
|
|
* @param[in] y Coefficients array.
|
|
* @param[in] Field Field value.
|
|
* @param[out] dydx Derivatives array.
|
|
*/
|
|
void EvaluateRhsGivenB(const G4double y[],
|
|
const G4double Field[],
|
|
G4double dydx[] ) const override;
|
|
|
|
/**
|
|
* Setter and getter for magnetic anomaly.
|
|
*/
|
|
inline void SetAnomaly(G4double a) { anomaly = a; }
|
|
inline G4double GetAnomaly() const { return anomaly; }
|
|
|
|
/**
|
|
* Returns the equation type-ID, "kEqEMfieldWithSpin".
|
|
*/
|
|
inline G4EquationType GetEquationType() const override { return kEqEMfieldWithSpin; }
|
|
|
|
private:
|
|
|
|
G4double charge{0.}, mass{0.}, magMoment{0.}, spin{0.};
|
|
|
|
G4double fElectroMagCof{0.};
|
|
G4double fMassCof{0.};
|
|
|
|
G4double omegac{0.}, anomaly{0.0011659208};
|
|
G4double beta{0.}, gamma{0.};
|
|
};
|
|
|
|
#endif
|