Strong-coupling behaviour in discrete Kardar-Parisi-Zhang equations
T. J. Newman, A. J. Bray

TL;DR
This paper introduces a new discretization scheme for the KPZ equation that accurately captures strong-coupling behavior, avoids finite-time singularities, and enhances understanding of universality classes in discrete KPZ models.
Contribution
A systematic discretization scheme for the KPZ equation that preserves strong-coupling properties and improves analysis of universality classes.
Findings
The scheme contains no finite-time singularities.
It better captures the strong-coupling physics.
It clarifies the diversity of universality classes.
Abstract
We present a systematic discretization scheme for the Kardar-Parisi-Zhang (KPZ) equation, which correctly captures the strong-coupling properties of the continuum model. In particular we show that the scheme contains no finite-time singularities in contrast to conventional schemes. The implications of these results to i) previous numerical integration of the KPZ equation, and ii) the non-trivial diversity of universality classes for discrete models of `KPZ-type' are examined. The new scheme makes the strong-coupling physics of the KPZ equation more transparent than the original continuum version and allows the possibility of building new continuum models which may be easier to analyse in the strong-coupling regime.
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