Abstract

Physical scenarios that require a relativistic treatment are ubiquitous in nature, ranging from cosmological objects to charge carriers in Dirac materials. Interestingly all of these situations have in common that the systems typically operate very far from thermal equilibrium. Therefore, if and how the framework of stochastic thermodynamics applies at relativistic energies is a salient question. In the present work we generalize the notions of stochastic heat and work for the relativistic Langevin equation and derive the fluctuation theorems without and with feedback. For processes with feedback we consider the ramifications of the lack of simultaneity of events in the inertial frames of observer and Brownian particles, and we argue that the framework of absolute irreversibility is instrumental to avoid acausal considerations. The analysis is concluded with a few remarks on potential experimental applications in graphene.

Highlights

  • The Universe is full of objects that defy the common anthropocentric understanding of nature

  • For processes with feedback we consider the ramifications of the lack of simultaneity of events in the inertial frames of observer and Brownian particles, and we argue that the framework of absolute irreversibility is instrumental to avoid acausal considerations

  • In the present analysis we have comprehensively shown how the framework of stochastic thermodynamics applies to Brownian motion at relativistic energies

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Summary

June 2020

Department of Physics, University of Maryland, Baltimore County, Baltimore, MD 21250, United States of America 1 Author to whom any correspondence should be addressed. Keywords: stochastic thermodynamics, relativistic Brownian motion, fluctuation theorems, relativistic Maxwell’s demon

Introduction
Stochastic energetics of the relativistic Ornstein–Uhlenbeck process
Stochastic thermodynamics and fluctuation theorems
Relativistic fluctuation–dissipation theorem and detailed balance
Fluctuation theorem for the irreversible entropy production
Maxwell’s demon at relativistic energies
Concluding remarks
Full Text
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