Abstract

We numerically study the geometry of a driven elastic string at its sample-dependent depinning threshold in random-periodic media. We find that the anisotropic finite-size scaling of the average square width $\overline{w^2}$ and of its associated probability distribution are both controlled by the ratio $k=M/L^{\zeta_{dep}}$, where $\zeta_{dep}$ is the random-manifold depinning roughness exponent, $L$ is the longitudinal size of the string and $M$ the transverse periodicity of the random medium. The rescaled average square width $\overline{w^2}/L^{2\zeta_{dep}}$ displays a non-trivial single minimum for a finite value of $k$. We show that the initial decrease for small $k$ reflects the crossover at $k \sim 1$ from the random-periodic to the random-manifold roughness. The increase for very large $k$ implies that the increasingly rare critical configurations, accompanying the crossover to Gumbel critical-force statistics, display anomalous roughness properties: a transverse-periodicity scaling in spite that $\overline{w^2} \ll M$, and subleading corrections to the standard random-manifold longitudinal-size scaling. Our results are relevant to understanding the dimensional crossover from interface to particle depinning. Received: 20 October 2010, Accepted: 1 December 2010; Edited by: A. Vindigni; Reviewed by: A. A. Fedorenko, CNRS-Lab. de Physique, ENS de Lyon, France; DOI: 10.4279/PIP.020008

Highlights

  • The study of the static and dynamic properties of d-dimensional elastic interfaces in d+1-dimensional random media is of interest in a wide range of physical systems

  • In the absence of an external drive, the ground state of the system is disordered but well characterized by a self-affine rough geometry with a diverging typical width w ∼ Lζeq, where L is the linear size of the elastic object and ζeq is the equilibrium roughness exponent

  • This result is a numerical confirmation of the two-loop functional renormalization group result of Ref. [16] which shows that the ζ = 0 fixed point, leading to a universal logarithmic growth of displacements at equilibrium is unstable

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Summary

Introduction

The study of the static and dynamic properties of d-dimensional elastic interfaces in d+1-dimensional random media is of interest in a wide range of physical systems. Some concrete experimental examples are magnetic [1,2,3,4] or ferroelectric [5,6] domain walls, contact lines of liquids [7], fluid invasion in porous media [8, 9], and fractures [10, 11] In all these systems, the basic physics is controlled by the competition between quenched disorder (induced by the presence of impurities in the host materials) which promotes the wandering of the elastic object, against the elastic forces which tend to make the elastic object flat.

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