Stochastic thermodynamics of fractional Brownian motion

This paper is concerned with the stochastic thermodynamics of nonequilibrium 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)...

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Main Authors: S. Mohsen J. Khadem, Rainer Klages, Sabine H. L. Klapp
Format: Article
Language:English
Published: American Physical Society 2022-12-01
Series:Physical Review Research
Online Access:http://doi.org/10.1103/PhysRevResearch.4.043186
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author S. Mohsen J. Khadem
Rainer Klages
Sabine H. L. Klapp
author_facet S. Mohsen J. Khadem
Rainer Klages
Sabine H. L. Klapp
author_sort S. Mohsen J. Khadem
collection DOAJ
description This paper is concerned with the stochastic thermodynamics of nonequilibrium 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 case, the noise is still Gaussian, but the noise correlation function is nonlocal in time, defining a non-Markovian process. We analyze 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 fulfills a generalized FDR. To shed light on the rather abstract quantities resulting from the latter approach, we perform a perturbation expansion in terms of ε=H−1/2, where H is the Hurst parameter of FBM and 1/2 corresponds to the Brownian case. This allows us to calculate analytically, up to linear order in ε, 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.
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spelling doaj.art-044db7e899a94f01b91fbfa534403c6b2024-04-12T17:27:00ZengAmerican Physical SocietyPhysical Review Research2643-15642022-12-014404318610.1103/PhysRevResearch.4.043186Stochastic thermodynamics of fractional Brownian motionS. Mohsen J. KhademRainer KlagesSabine H. L. KlappThis paper is concerned with the stochastic thermodynamics of nonequilibrium 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 case, the noise is still Gaussian, but the noise correlation function is nonlocal in time, defining a non-Markovian process. We analyze 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 fulfills a generalized FDR. To shed light on the rather abstract quantities resulting from the latter approach, we perform a perturbation expansion in terms of ε=H−1/2, where H is the Hurst parameter of FBM and 1/2 corresponds to the Brownian case. This allows us to calculate analytically, up to linear order in ε, 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.http://doi.org/10.1103/PhysRevResearch.4.043186
spellingShingle S. Mohsen J. Khadem
Rainer Klages
Sabine H. L. Klapp
Stochastic thermodynamics of fractional Brownian motion
Physical Review Research
title Stochastic thermodynamics of fractional Brownian motion
title_full Stochastic thermodynamics of fractional Brownian motion
title_fullStr Stochastic thermodynamics of fractional Brownian motion
title_full_unstemmed Stochastic thermodynamics of fractional Brownian motion
title_short Stochastic thermodynamics of fractional Brownian motion
title_sort stochastic thermodynamics of fractional brownian motion
url http://doi.org/10.1103/PhysRevResearch.4.043186
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AT rainerklages stochasticthermodynamicsoffractionalbrownianmotion
AT sabinehlklapp stochasticthermodynamicsoffractionalbrownianmotion