Abstract

We study the motion of a Brownian particle subjected to Lorentz force due to an external magnetic field. Each spatial degree of freedom of the particle is coupled to a different thermostat. We show that the magnetic field results in correlation between different velocity components in the stationary state. Integrating the velocity autocorrelation matrix, we obtain the diffusion matrix that enters the Fokker–Planck equation for the probability density. The eigenvectors of the diffusion matrix do not align with the temperature axes. As a consequence the Brownian particle performs spatially correlated diffusion. We further show that in the presence of an isotropic confining potential, an unusual, flux-free steady state emerges which is characterized by a non-Boltzmann density distribution, which can be rotated by reversing the magnetic field. The nontrivial steady state properties of our system result from the Lorentz force induced coupling of the spatial degrees of freedom which cease to exist in equilibrium corresponding to a single-temperature system.

Highlights

  • The trajectory of a charged particle is curved by the Lorentz force due to an external magnetic field

  • We have recently shown that by driving the system into a nonequilibrium stationary state one preserves the unusual features of the dynamics under Lorentz force

  • We study the motion of a Brownian particle subjected to Lorentz force with each spatial degree of freedom coupled to a different thermostat

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Summary

Introduction

The trajectory of a charged particle is curved by the Lorentz force due to an external magnetic field. The unusual properties of the stationary regime have their origin in the fact that the Lorentz force mixes different velocity components of the particle which results in coupling of the spatial degrees of freedom [11]. If one considers that each spatial degree of freedom is coupled to a different thermostat, an interesting steady state may be envisaged in the presence of Lorentz force. We study the motion of a Brownian particle subjected to Lorentz force with each spatial degree of freedom coupled to a different thermostat.

Velocity distribution
Diffusion Equation
Nonequilibrium steady state
Uniform magnetic field
Spatially inhomogeneous magnetic field
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