On the stochastic thermodynamics of fractional Brownian motion

TL;DR

This paper explores the stochastic thermodynamics of fractional Brownian motion, revealing how non-Markovian noise affects fluctuation relations and proposing a generalized temperature concept to restore thermodynamic consistency.

Contribution

It introduces a formalism for defining a time-nonlocal temperature in non-Markovian Gaussian processes, extending stochastic thermodynamics to fractional Brownian motion.

Findings

Standard thermodynamic notions can be adapted with a time-dependent temperature.

Deviations from fluctuation relations occur when using constant temperature assumptions.

A perturbative approach yields explicit expressions for the generalized temperature and heat exchange.

Abstract

This paper is concerned with the stochastic thermodynamics of non-equilibrium Gaussian processes that can exhibit anomalous diffusion. In the systems considered, the noise correlation function is not necessarily related to friction. Thus, there is no conventional fluctuation-dissipation relation (FDR) of the second kind and no unique way to define a temperature. We start from a Markovian process with time-dependent diffusivity (an example being scaled Brownian motion). It turns out that standard stochastic thermodynamic notions can be applied rather straightforwardly by introducing a time-dependent temperature, yielding the integral fluctuation relation. We then proceed to our focal system, that is, a particle undergoing fractional Brownian motion (FBM). In this system, the noise is Gaussian but the noise correlation function is nonlocal in time, defining a non- Markovian process. We analyse in detail the consequences when using the conventional notions of stochastic thermodynamics with a constant medium temperature. In particular, the heat calculated from dissipation into the medium differs from the log ratio of path probabilities of forward and backward motion, yielding a deviation from the standard integral fluctuation relation for the total entropy production if the latter is defined via system entropy and heat exchange. These apparent inconsistencies can be circumvented by formally defining a time-nonlocal temperature that fulfils a generalized FDR. To shed light on the rather abstract quantities resulting from the latter approach we perform a perturbation expansion. This allows us to calculate analytically, up to linear order, the generalized temperature and the corresponding heat exchange. By this, we provide explicit expressions and a physical interpretation for the leading corrections induced by non-Markovianity.