The browser you are using is not supported by this website. All versions of Internet Explorer are no longer supported, either by us or Microsoft (read more here: https://www.microsoft.com/en-us/microsoft-365/windows/end-of-ie-support).

Please use a modern browser to fully experience our website, such as the newest versions of Edge, Chrome, Firefox or Safari etc.

Photo of Tobias Ambjörnsson

Tobias Ambjörnsson

Senior lecturer

Photo of Tobias Ambjörnsson

Diffusion of finite-sized hard-core interacting particles in a one-dimensional box: Tagged particle dynamics

Author

  • L. Lizana
  • Tobias Ambjörnsson

Summary, in English

We solve a nonequilibrium statistical-mechanics problem exactly, namely, the single-file dynamics of N hard-core interacting particles (the particles cannot pass each other) of size Delta diffusing in a one-dimensional system of finite length L with reflecting boundaries at the ends. We obtain an exact expression for the conditional probability density function rho T(yT,t vertical bar yT,0) that a tagged particle T (T=1,...,N) is at position yT at time t given that it at time t=0 was at position yT,0. Using a Bethe ansatz we obtain the N-particle probability density function and, by integrating out the coordinates (and averaging over initial positions) of all particles but particle T, we arrive at an exact expression for rho T(yT,t vertical bar yT,0) in terms of Jacobi polynomials or hypergeometric functions. Going beyond previous studies, we consider the asymptotic limit of large N, maintaining L finite, using a nonstandard asymptotic technique. We derive an exact expression for rho T(yT,t vertical bar yT,0) for a tagged particle located roughly in the middle of the system, from which we find that there are three time regimes of interest for finite-sized systems: (A) for times much smaller than the collision time t <tau(coll)=1/(rho D-2), where rho=N/L is the particle concentration and D is the diffusion constant for each particle, the tagged particle undergoes a normal diffusion; (B) for times much larger than the collision time t tau(coll) but times smaller than the equilibrium time t <tau(eq)=L-2/D, we find a single-file regime where rho T(yT,t vertical bar yT,0) is a Gaussian with a mean-square displacement scaling as t(1/2); and (C) for times longer than the equilibrium time t tau(eq), rho T(yT,t vertical bar yT,0) approaches a polynomial-type equilibrium probability density function. Notably, only regimes (A) and (B) are found in the previously considered infinite systems.

Department/s

  • Computational Biology and Biological Physics - Has been reorganised

Publishing year

2009

Language

English

Publication/Series

Physical Review E (Statistical, Nonlinear, and Soft Matter Physics)

Volume

80

Issue

5

Document type

Journal article

Publisher

American Physical Society

Topic

  • Biophysics
  • Other Physics Topics

Keywords

  • statistical
  • probability
  • polynomials
  • diffusion
  • mechanics
  • many-body problems

Status

Published

ISBN/ISSN/Other

  • ISSN: 1539-3755