// 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 1.5 2000/11/01 15:15:51 gcosmo Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
//
// class G4RKG3_Stepper
//
// Class description:
//
// Integrator Runga-Kutta Stepper from Geant3.

// History:
// - Created. J.Apostolakis, V.Grichine - 30.01.97

#ifndef G4RKG3_Stepper_hh
#define G4RKG3_Stepper_hh

#include "G4MagIntegratorStepper.hh"
#include "G4ThreeVector.hh"

class G4RKG3_Stepper : public G4MagIntegratorStepper
{
  public:  // with description

    G4RKG3_Stepper(G4Mag_EqRhs *EqRhs)
      : G4MagIntegratorStepper(EqRhs,6){;}
      // Integrate over 6 variables only:  position & velocity.

    ~G4RKG3_Stepper(){;}

    void Stepper( const G4double yIn[],
	          const G4double dydx[],
	                G4double h,
		        G4double yOut[],
		        G4double yErr[]  );
      // The method which must be provided, even if less efficient.

    G4double  DistChord() const ;
 
    void StepNoErr( const G4double tIn[7],
		    const G4double dydx[7],
		          G4double Step,
			  G4double tOut[7],
			  G4double B[3] );
      // 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 StepWithEst( const G4double  tIn[7],
		      const G4double dydx[7],
		            G4double Step,
			    G4double tOut[7],
			    G4double& alpha2,    // to delete ?
			    G4double& beta2,
		      const G4double B1[3],
			    G4double B2[3] );
      // Integrator for RK from G3 with evaluation of error in solution and delta
      // geometry based on naive similarity with the case of uniform magnetic field.
      // B1[3] is input  and is the first magnetic field values
      // B2[3] is output and is the final magnetic field values.

  public:  // without description

    G4int IntegratorOrder() const { return 4; }
  
  protected:
    //	void Field( const G4double Point[3],
    //			  G4double Bfield[3] )  const
    //	  { EqRhs-> GetFieldValue( Point, Bfield ) ; }

  private:

    G4ThreeVector fyInitial,
	          fyMidPoint,
		  fyFinal ;
};

#endif