4.7 Article

Solution to the Fokker-Planck equation for slowly driven Brownian motion: Emergent geometry and a formula for the corresponding thermodynamic metric

期刊

PHYSICAL REVIEW E
卷 105, 期 3, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevE.105.034130

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资金

  1. National Science Foundation Graduate Research Fellowship [DGE 1752814]
  2. U.S. Army Research Laboratory [W911NF-20-1-0151]
  3. U.S. Army Research Office [W911NF-20-1-0151]
  4. Google

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Considerable progress has been made in geometrical approaches to understand and control small out-of-equilibrium systems. However, these methods lack a mathematically rigorous foundation. In this study, a perturbative solution to the Fokker-Planck equation for one-dimensional driven Brownian motion in the overdamped limit is developed using the spectral properties of the corresponding single-particle Schrodinger operator. The perturbation theory provides an exact formula for a Riemannian thermodynamic metric in the space of control parameters, and the optimal dissipation-minimizing driving protocols can be obtained by minimizing the length defined by this metric. The Riemannian geometric structure of the optimal control problem is emergent and persists to all orders of the perturbation expansion.
Considerable progress has recently been made with geometrical approaches to understanding and controlling small out-of-equilibrium systems, but a mathematically rigorous foundation for these methods has been lacking. Towards this end, we develop a perturbative solution to the Fokker-Planck equation for one-dimensional driven Brownian motion in the overdamped limit enabled by the spectral properties of the corresponding single-particle Schrodinger operator. The perturbation theory is in powers of the inverse characteristic timescale of variation of the fastest varying control parameter, measured in units of the system timescale, which is set by the smallest eigenvalue of the corresponding Schrodinger operator. It applies to any Brownian system for which the Schrodinger operator has a confining potential. We use the theory to rigorously derive an exact formula for a Riemannian thermodynamic metric in the space of control parameters of the system. We show that up to second-order terms in the perturbation theory, optimal dissipation-minimizing driving protocols minimize the length defined by this metric. We also show that a previously proposed metric is calculable from our exact formula with corrections that are exponentially suppressed in a characteristic length scale. We illustrate our formula using the two-dimensional example of a harmonic oscillator with time-dependent spring constant in a time-dependent electric field. Lastly, we demonstrate that the Riemannian geometric structure of the optimal control problem is emergent; it derives from the form of the perturbative expansion for the probability density and persists to all orders of the expansion.

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