Consider the dynamics of a tracer particle subject to a constant driving force E in a one-dimensional lattice gas of hard-core particles whose transition rates are symmetric. We show that the mean displacement of the driven tracer XT(E,t) grows in time t as XT(E,t)={}{α}t, rather than the linear time dependence found for noninteracting (ghost) bath particles. The prefactor {α} is determined implicitly, as the solution of a transcendental equation, for an arbitrary magnitude of the driving force and an arbitrary concentration of the lattice-gas particles. In limiting cases the prefactor is obtained explicitly. Analytical predictions are seen to be in good agreement with the results of numerical simulations. {} 1996 The American Physical Society.
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Burlatsky et al. (1996) studied this question.
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