Relaxation dynamics of an elastic string in random media

TL;DR

This study numerically analyzes the relaxation of an elastic string in random media, revealing a logarithmic growth of correlation length driven by thermal activation over energy barriers, with a transient power-law regime influenced by disorder structure.

Contribution

It demonstrates that the energy barrier exponent matches the fluctuation exponent and characterizes the crossover from power-law to logarithmic growth in relaxation dynamics.

Findings

Correlation length grows as $(\, ext{ln}\, t)^{1/ ilde ext{chi}}$

Energy barrier exponent $ ilde{ ext{chi}}$ equals fluctuation exponent $ ext{chi}=1/3$

Transient power-law growth with nonuniversal exponent $z$

Abstract

We investigate numerically the relaxation dynamics of an elastic string in two-dimensional random media by thermal fluctuations starting from a flat configuration. Measuring spatial fluctuations of its mean position, we find that the correlation length grows in time asymptotically as $\xi \sim (\ln t)^{1/\tilde\chi}$. This implies that the relaxation dynamics is driven by thermal activations over random energy barriers which scale as $E_B(\ell) \sim \ell^{\tilde\chi}$ with a length scale $\ell$. Numerical data strongly suggest that the energy barrier exponent $\tilde{\chi}$ is identical to the energy fluctuation exponent $\chi=1/3$. We also find that there exists a long transient regime, where the correlation length follows a power-law dynamics as $\xi \sim t^{1/z}$ with a nonuniversal dynamic exponent $z$. The origin of the transient scaling behavior is discussed in the context of the relaxation dynamics on finite ramified clusters of disorder.