Gabriele Cosmo
117 lines
4.1 KiB
C++
117 lines
4.1 KiB
C++
//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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// G4RepleteEofM
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//
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// Class description:
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//
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// This is the right-hand side of equation of motion in a combined
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// field, including: magnetic, electric, gravity, and gradient B field,
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// as well as spin tracking.
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// Author: Peter Gumplinger (TRIUMF), 08.04.2013
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// -------------------------------------------------------------------
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#ifndef G4EOFM_HH
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#define G4EOFM_HH
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#include "G4ChargeState.hh"
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#include "G4EquationOfMotion.hh"
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class G4Field;
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/**
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* @brief G4RepleteEofM is the right-hand side of equation of motion in a
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* combined field, including: magnetic, electric, gravity, and gradient
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* B field, as well as spin tracking.
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*/
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class G4RepleteEofM : public G4EquationOfMotion
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{
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public:
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/**
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* Constructor for G4EquationOfMotion.
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* @param[in] field Pointer to the field.
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* @param[in] nvar The number of integration variables.
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*/
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G4RepleteEofM(G4Field* field, G4int nvar = 8);
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/**
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* Default Destructor.
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*/
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~G4RepleteEofM() override = default;
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/**
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* Sets the charge, momentum and mass of the current particle.
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* Used to set the equation's coefficients.
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* @param[in] particleCharge Magnetic charge and moments in e+ units.
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* @param[in] MomentumXc Particle momentum.
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* @param[in] mass Particle mass.
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*/
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void SetChargeMomentumMass(G4ChargeState particleCharge, // in e+ units
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G4double MomentumXc,
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G4double mass) override;
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/**
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* Calculates the value of the derivative, given the value of the field.
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* @param[in] y Coefficients array.
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* @param[in] Field Field value.
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* @param[out] dydx Derivatives array.
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*/
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void EvaluateRhsGivenB(const G4double y[],
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const G4double Field[],
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G4double dydx[] ) const override;
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/**
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* Setter and getter for the magnetic anomaly.
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*/
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inline void SetAnomaly(G4double a) { anomaly = a; }
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inline G4double GetAnomaly() const { return anomaly; }
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/**
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* Modifiers.
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*/
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inline void SetBField() { fBfield = true; }
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inline void SetEField() { fEfield = true; }
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inline void SetgradB() { fgradB = true; }
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inline void SetSpin() { fSpin = true; }
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private:
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G4int fNvar = 0;
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G4bool fBfield=false, fEfield=false,
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fGfield=false, fgradB=false, fSpin=false;
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G4double charge=0.0, mass=0.0, magMoment=0.0, spin=0.0;
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G4double ElectroMagCof=0.0;
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G4double omegac=0.0, anomaly=0.0;
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G4double beta=0.0, gamma=0.0;
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};
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#endif
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