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
Summary
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.
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