Abstract

We study a relationship between optimal transport theory and stochastic thermodynamics for the Fokker-Planck equation. We show that the lower bound on the entropy production is the action measured by the path length of the $L^2$-Wasserstein distance. Because the $L^2$-Wasserstein distance is a geometric measure of optimal transport theory, our result implies a geometric interpretation of the entropy production. Based on this interpretation, we obtain a thermodynamic trade-off relation between transition time and the entropy production. This thermodynamic trade-off relation is regarded as a thermodynamic speed limit which gives a tighter bound of the entropy production. We also discuss stochastic thermodynamics for the subsystem and derive a lower bound on the partial entropy production as a generalization of the second law of information thermodynamics. Our formalism also provides a geometric picture of the optimal protocol to minimize the entropy production. We illustrate these results by the optimal stochastic heat engine and show a geometrical bound of the efficiency.

Highlights

  • Geometry is a helpful tool to consider the difference between two quantities, and the geometric concept for probability distributions is widely used in statistical physics

  • We discuss a geometrical feature of stochastic thermodynamics for the Fokker-Planck equation based on the L2-Wasserstein distance

  • Based on L2-Wasserstein distance, we can introduce a differential geometry of stochastic thermodynamics for the Fokker-Planck equation, closely related to the entropy production

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Summary

INTRODUCTION

Geometry is a helpful tool to consider the difference between two quantities, and the geometric concept for probability distributions is widely used in statistical physics. Several thermodynamic trade-off relations about the efficiency of the stochastic heat engine has been derived based on the optimal transport theory [51,52]. The entropy production can be proportional to the action with some assumptions where the force is given by the potential This result provides a geometric interpretation of the entropy production for the Fokker-Planck equation. We numerically illustrate a tightness of a generalized thermodynamic speed limit and the optimal heat engine based on the Wasserstein distance. We discuss an information-thermodynamic interpretation and derive a new lower bound on the partial entropy production in Sec. IV B.

Stochastic thermodynamics for Fokker-Planck equation
Optimal transport theory and L2-Wasserstein distance
Relation between Wasserstein distance and entropy production rate
Geometric lower bounds on entropy production and thermodynamic speed limits
Stochastic thermodynamics for subsystem
Information thermodynamics
Stochastic heat engine and geometrical bounds on efficiency
Adiabatic process
Analytical calculation of geometric optimal protocol
Numerical illustration of thermodynamic speed limits
Numerical calculation of optimal stochastic heat engine in finite time
DISCUSSION

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