Abstract

We characterize the crossover regime to the KPZ equation for a class of one-dimensional weakly asymmetric exclusion processes. The crossover depends on the strength asymmetry an2−γan^{2-γ} (a,γ>0a,γ>0) and it occurs at γ=1/2γ=1/2. We show that the density field is a solution of an Ornstein-Uhlenbeck equation if γ∈(1/2,1]γ\in(1/2,1], while for γ=1/2γ=1/2 it is an energy solution of the KPZ equation. The corresponding crossover for the current of particles is readily obtained.

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