MagneticField.hpp

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 * [1] Meineke, et al., J. Comp. Chem. 26, 252-271 (2005).
 * [2] Fennell & Gezelter, J. Chem. Phys. 124, 234104 (2006).
 * [3] Sun, Lin & Gezelter, J. Chem. Phys. 128, 234107 (2008).
 * [4] Vardeman, Stocker & Gezelter, J. Chem. Theory Comput. 7, 834 (2011).
 * [5] Kuang & Gezelter, Mol. Phys., 110, 691-701 (2012).
 * [6] Lamichhane, Gezelter & Newman, J. Chem. Phys. 141, 134109 (2014).
 * [7] Lamichhane, Newman & Gezelter, J. Chem. Phys. 141, 134110 (2014).
 * [8] Bhattarai, Newman & Gezelter, Phys. Rev. B 99, 094106 (2019).
 */
 
/*! \file perturbations/MagneticField.hpp
    \brief Uniform Magnetic Field perturbation
*/
 
#ifndef PERTURBATIONS_MAGNETICFIELD_HPP
#define PERTURBATIONS_MAGNETICFIELD_HPP
 
#include "brains/ForceModifier.hpp"
#include "brains/SimInfo.hpp"
 
namespace OpenMD {
 
  //! Applies a uniform (vector) magnetic field to the system
  /*! The field is applied as an external perturbation.  The user specifies
 
  \code{.unparsed}
    magneticField = (a, b, c);
  \endcode
 
    in the .omd file where the values of a, b, and c are in units of Tesla
 
    When a charge moves in a magnetic field, there is no work done, so
    there is no change in potential.
 
    The field itself is
 
    \f$ \mathbf{B} = \left( \begin{array}{c} a \\ b \\ c \end{array}
    \right) \f$
 
   The external magnetic field applies a force on moving charged
   atoms, \f$ \mathbf{F} = C \mathbf{v} \times \mathbf{B} \f$ and a
   torque on moving (and rotating) dipoles, \f$ \mathbf{\tau} =
   \mathbf{D} \times ( \mathbf{v} \times \mathbf{B} ) +
   (\mathbf{\omega} \times \mathbf{D} ) \times \mathbf{B} \f$
 
  */
  class MagneticField : public ForceModifier {
  public:
    MagneticField(SimInfo* info);
 
  private:
    void modifyForces() override;
    void initialize();
 
    bool initialized;
    bool doMagneticField;
 
    Globals* simParams;
    Vector3d MF;
  };
}  // namespace OpenMD
 
#endif