F01FieldMessenger.hh

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/// \file field/field01/include/F01FieldMessenger.hh
/// \brief  F01FieldMessenger allows interactive user control of
//     - the strength of the (uniform) magnetic field
//     - the key parameters for the accuracy of integration
//     - the integration method used - a choice between
//          * different embedded Runge-Kutta methods or 'tableaus'
//          * the symplectic Boris method for accelerator setups
//
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#ifndef F01FieldMessenger_h
#define F01FieldMessenger_h 1
 
#include "G4UImessenger.hh"
 
class F01FieldSetup;
class G4UIdirectory;
class G4UIcmdWithAnInteger;
class G4UIcmdWithADouble;
class G4UIcmdWithADoubleAndUnit;
class G4UIcmdWith3VectorAndUnit;
class G4UIcmdWithoutParameter;
 
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class F01FieldMessenger: public G4UImessenger
{
  public:
    F01FieldMessenger(F01FieldSetup* );
    ~F01FieldMessenger() override;
 
    void SetNewValue(G4UIcommand*, G4String) override;
 
  private:
 
    F01FieldSetup*             fEMfieldSetup = nullptr;
 
    G4UIdirectory*             fFieldDir = nullptr;
 
    G4UIcmdWithAnInteger*      fStepperCmd = nullptr;
    G4UIcmdWithADoubleAndUnit* fMagFieldZCmd = nullptr;
    G4UIcmdWith3VectorAndUnit* fMagFieldCmd = nullptr;
    G4UIcmdWithADoubleAndUnit* fMinStepCmd = nullptr;
    G4UIcmdWithADoubleAndUnit* fDeltaOneStepCmd = nullptr;
    G4UIcmdWithADouble*        fEpsMinCmd = nullptr;
    G4UIcmdWithADouble*        fEpsMaxCmd = nullptr;
    G4UIcmdWithoutParameter*   fUpdateCmd = nullptr;
};
 
#endif