Abstract

We consider the stochastic heat equation \[ ∂ t Z = ∂ x 2 Z − Z W ˙ \partial _tZ= \partial _x^2 Z - Z \dot W \] on the real line, where W ˙ \dot W is space-time white noise. h ( t , x ) = − log ⁡ Z ( t , x ) h(t,x)=-\operatorname {log} Z(t,x) is interpreted as a solution of the KPZ equation, and u ( t , x ) = ∂ x h ( t , x ) u(t,x)=\partial _x h(t,x) as a solution of the stochastic Burgers equation. We take Z ( 0 , x ) = exp ⁡ { B ( x ) } Z(0,x)=\exp \{B(x)\} , where B ( x ) B(x) is a two-sided Brownian motion, corresponding to the stationary solution of the stochastic Burgers equation. We show that there exist 0 > c 1 ≤ c 2 > ∞ 0> c_1\le c_2 >\infty such that \[ c 1 t 2 / 3 ≤ Var ⁡ ( log ⁡ Z ( t , x ) ) ≤ c 2 t 2 / 3 . c_1t^{2/3}\le \operatorname {Var}(\operatorname {log} Z(t,x) )\le c_2 t^{2/3}. \] Analogous results are obtained for some moments of the correlation functions of u ( t , x ) u(t,x) . In particular, it is shown there that the bulk diffusivity satisfies \[ c 1 t 1 / 3 ≤ D bulk ( t ) ≤ c 2 t 1 / 3 . c_1t^{1/3}\le D_\textrm {bulk}(t) \le c_2 t^{1/3}. \] The proof uses approximation by weakly asymmetric simple exclusion processes, for which we obtain the microscopic analogies of the results by coupling.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call