Diffusion in a bistable system: The eigenvalue spectrum of the Fokker-Planck operator and Kramers' reaction rate theory

Yahui Zhan and Bernie D. Shizgal
Phys. Rev. E 99, 042101 – Published 1 April 2019

Abstract

The time-dependent solution of the Fokker-Planck equation with bistable potentials is considered in terms of the eigenfunctions and eigenvalues of the linear Fokker-Planck operator. The Fokker-Planck equation is the high friction limit of the corresponding Kramers' equation. Two different potentials are considered defined with a constant diffusion coefficient, ε, and position-dependent drift coefficients. The smallest nonzero eigenvalue of the Fokker-Planck operator, λ1, provides the long-time rate coefficient for the transformation of the different species in the two stable states. A novel pseudospectral method with nonclassical polynomials is applied to this class of systems. The convergence of the eigenvalues and eigenfunctions of the Fokker-Planck operator versus the number of basis functions is studied and compared with previous results. The results are consistent with Kramers' theory, and a linear relationship between lnλ1 and 1/ε for sufficiently small ε values is verified. A comparison with analytic approximations to λ1 is provided.

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  • Received 10 December 2018

DOI:https://doi.org/10.1103/PhysRevE.99.042101

©2019 American Physical Society

Physics Subject Headings (PhySH)

Statistical Physics & Thermodynamics

Authors & Affiliations

Yahui Zhan

  • Department of Mathematics, University of British Columbia Vancouver, British Columbia, V6T1Z1 Canada

Bernie D. Shizgal

  • Department of Chemistry, University of British Columbia Vancouver, British Columbia, V6T1Z1 Canada

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Issue

Vol. 99, Iss. 4 — April 2019

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