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Classical orbital magnetic moment in a dissipative stochastic system
1Raman Research Institute, Bangalore 560080, India.
Summary
A charged particle in a magnetic field generates an orbital magnetic moment. This moment
Area of Science:
- Physics
- Statistical Mechanics
- Condensed Matter Physics
Background:
- Classical charged particles in magnetic fields exhibit complex dynamics.
- Langevin dynamics describes systems with dissipation and noise.
- The fluctuation-dissipation relation is key to understanding equilibrium states.
Purpose of the Study:
- To analytically investigate the dissipative-stochastic dynamics of a charged particle in a biharmonic potential and magnetic field.
- To examine the orbital magnetic moment generated by the particle under non-equilibrium conditions.
- To explore the influence of deviations from the standard fluctuation-dissipation relation on magnetic properties.
Main Methods:
- Analytical treatment of dissipative-stochastic dynamics.
- Analysis of a charged classical particle in a biharmonic potential and perpendicular magnetic field.
- Introduction of a parameter (η) to modify the fluctuation-dissipation relation.
Main Results:
- A steady state is achieved in the long-time limit.
- The charged particle generates a finite orbital magnetic moment.
- The magnetic moment exhibits a crossover from paramagnetic to diamagnetic behavior as η varies.
- The moment is zero at equilibrium (η=1).
- The magnitude of the orbital magnetic moment is non-monotonic with respect to the applied magnetic field, approaching zero at both small and large field limits.
Conclusions:
- The study demonstrates the generation of a classical orbital magnetic moment in a non-equilibrium steady state.
- The findings offer insights into classical orbital diamagnetism, potentially challenging the classical Bohr-van Leeuwen theorem.
- The results suggest possibilities for experimental realization.
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