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geant4/source/geometry/magneticfield/include/G4RKG3_Stepper.hh
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2016-06-08 15:28:20 +02:00

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C++

// This code implementation is the intellectual property of
// the GEANT4 collaboration.
//
// By copying, distributing or modifying the Program (or any work
// based on the Program) you indicate your acceptance of this statement,
// and all its terms.
//
// $Id: G4RKG3_Stepper.hh,v 1.2.8.1 1999/12/07 20:48:02 gunter Exp $
// GEANT4 tag $Name: geant4-01-00 $
//
//
// J.Apostolakis, V.Grichine 30.01.97
#include "G4MagIntegratorStepper.hh"
#include "G4ThreeVector.hh"
class G4RKG3_Stepper : public G4MagIntegratorStepper
{
public:
G4RKG3_Stepper(G4Mag_EqRhs *EqRhs): G4MagIntegratorStepper(EqRhs,6){};
// integrate over 6 variables only: position & velocity
~G4RKG3_Stepper(){};
// The method it must provide, even if less efficiently
void
Stepper( const G4double yIn[],
const G4double dydx[],
const G4double h,
G4double yOut[],
G4double yErr[] );
// G4double& beta2) const
G4double DistChord() const ;
// Additional "optimised" methods:
// Integrator RK Stepper from G3 with only two field evaluation per
// Step. It is used in propagation initial Step by small substeps
// after solution error and delta geometry considerations.
// B[3] is magnetic field which is passed from substep to substep.
void StepNoErr( const G4double tIn[7],
const G4double dydx[7],
const G4double Step,
G4double tOut[7],
G4double B[3] );
void StepWithEst(const G4double tIn[7],
const G4double dydx[7],
const G4double Step,
G4double tOut[7],
// G4double tError[6],
G4double& alpha2, // to delete ?
G4double& beta2,
const G4double B1[3],
G4double B3[3] );
G4int IntegratorOrder() { return 4; };
protected:
// void Field( const double Point[3],
// double Bfield[3] ) const
// { EqRhs-> GetFieldValue( Point, Bfield ) ; }
private:
G4ThreeVector fyInitial,
fyMidPoint,
fyFinal ;
};