Brownian motion of a charged particle in electromagnetic fluctuations at finite temperature

TL;DR

This paper investigates the motion of a charged particle in electromagnetic fluctuations at finite temperature, deriving the Langevin equation and analyzing the unique saturation behavior of velocity dispersion in a supraohmic environment.

Contribution

It derives the Langevin equation for a charged particle in a supraohmic environment using the Feynman-Vernon influence functional and establishes the fluctuation-dissipation theorem from first principles.

Findings

Velocity dispersion initially grows then saturates due to force correlation changes.

Supraohmic environment leads to a different saturation mechanism than ohmic environments.

Backreaction effects are negligible when the charge's motion is minimal.

Abstract

The fluctuation-dissipation theorem is a central theorem in nonequilibrium statistical mechanics by which the evolution of velocity fluctuations of the Brownian particle under a fluctuating environment is intimately related to its dissipative behavior. This can be illuminated in particular by an example of Brownian motion in an ohmic environment where the dissipative effect can be accounted for by the first-order time derivative of the position. Here we explore the dynamics of the Brownian particle coupled to a supraohmic environment by considering the motion of a charged particle interacting with the electromagnetic fluctuations at finite temperature. We also derive particle's equation of motion, the Langevin equation, by minimizing the corresponding stochastic effective action, which is obtained with the method of Feynman-Vernon influence functional. The fluctuation-dissipation theorem is established from first principles. The backreaction on the charge is known in terms of electromagnetic self-force given by a third-order time derivative of the position, leading to the supraohmic dynamics. This self-force can be argued to be insignificant throughout the evolution when the charge barely moves. The stochastic force arising from the supraohmic environment is found to have both positive and negative correlations, and it drives the charge into a fluctuating motion. Although positive force correlations give rise to the growth of the velocity dispersion initially, its growth slows down when correlation turns negative, and finally halts, thus leading to the saturation of the velocity dispersion. The saturation mechanism in a suparohmic environment is found to be distinctly different from that in an ohmic environment. The comparison is discussed.