research

Exact results for the Kardar--Parisi--Zhang equation with spatially correlated noise

Abstract

We investigate the Kardar--Parisi--Zhang (KPZ) equation in dd spatial dimensions with Gaussian spatially long--range correlated noise --- characterized by its second moment R(xβƒ—βˆ’xβƒ—β€²)∝∣xβƒ—βˆ’xβƒ—β€²βˆ£2Οβˆ’dR(\vec{x}-\vec{x}') \propto |\vec{x}-\vec{x}'|^{2\rho-d} --- by means of dynamic field theory and the renormalization group. Using a stochastic Cole--Hopf transformation we derive {\em exact} exponents and scaling functions for the roughening transition and the smooth phase above the lower critical dimension dc=2(1+ρ)d_c = 2 (1+\rho). Below the lower critical dimension, there is a line Οβˆ—(d)\rho_*(d) marking the stability boundary between the short-range and long-range noise fixed points. For ρβ‰₯Οβˆ—(d)\rho \geq \rho_*(d), the general structure of the renormalization-group equations fixes the values of the dynamic and roughness exponents exactly, whereas above Οβˆ—(d)\rho_*(d), one has to rely on some perturbational techniques. We discuss the location of this stability boundary Οβˆ—(d)\rho_* (d) in light of the exact results derived in this paper, and from results known in the literature. In particular, we conjecture that there might be two qualitatively different strong-coupling phases above and below the lower critical dimension, respectively.Comment: 21 pages, 15 figure

    Similar works

    Full text

    thumbnail-image

    Available Versions

    Last time updated on 11/12/2019