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// G4TExplicitEuler
//
// Class description:
//
// Templated version of G4ExplicitEuler.
// Adapted from G4G4TExplicitEuler class.
//
// Information from G4Explicit Euler:
// ----------------------------------
// Explicit Euler stepper for magnetic field: x_1 = x_0 + h * dx_0.
// The simplistic approach to solving linear differential equations.
// Take the current derivative and add it to the current position.

// Author: Josh Xie (CERN, Google Summer of Code 2014), June 2014
// Supervisors:  Sandro Wenzel, John Apostolakis (CERN)
// --------------------------------------------------------------------
#ifndef G4TExplicitEuler_HH
#define G4TExplicitEuler_HH

#include "G4TMagErrorStepper.hh"
#include "G4ThreeVector.hh"

/**
 * @brief G4TExplicitEuler is a templated version of G4ExplicitEuler stepper.
 */

template <class T_Equation, int N>
class G4TExplicitEuler
  : public G4TMagErrorStepper<G4TExplicitEuler<T_Equation, N>, T_Equation, N>
{
  public:

    static constexpr double IntegratorCorrection = 1.;

    G4TExplicitEuler(T_Equation* EqRhs, G4int numberOfVariables = N)
      : G4TMagErrorStepper<G4TExplicitEuler<T_Equation, N>, T_Equation, N>
                           (EqRhs, numberOfVariables), fEquation_Rhs(EqRhs)
    {
      if( numberOfVariables != N )
      {
        G4ExceptionDescription msg;
        msg << "Equation has an incompatible number of variables." ;
        msg << "   template N = " << N << " equation-Nvar= "
            << numberOfVariables;
        G4Exception("G4TExplicitEuler: constructor", "GeomField0003",
                    FatalErrorInArgument, msg );
      }
    }
   
    ~G4TExplicitEuler() = default;

    inline void DumbStepper(const G4double yIn[],
                            const G4double dydx[],
                            G4double h, G4double yOut[]) // override final
    {
      // Initialise time to t0, needed when it is not updated by the integration.
      // yOut[7] = yIn[7];   //  Better to set it to NaN;  // TODO

      for(G4int i = 0; i < N; ++i)
      {
        yOut[i] = yIn[i] + h * dydx[i];  // 1st and only Step
      }

      return;
    }

    G4int IntegratorOrder() const { return 1; }

  private:

    T_Equation* fEquation_Rhs;
};

#endif