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Non-equilibrium dynamics of disordered systems: understanding the broad continuum of relevant time scales via a strong-disorder RG in configuration space

Cécile Monthus and Thomas Garel

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We show that an appropriate description of the non-equilibrium dynamics of disordered systems is obtained through a strong disorder renormalization procedure in configuration space that we define for any master equation with transitions rates W ( { \cal C} \to { \cal C}^{\prime} ) between configurations. The idea is to eliminate iteratively the configuration with the highest exit rate W_{\rm out} ({ \cal C} )= \sum_{{ \cal C}^{\prime} } W ( { \cal C} \to { \cal C}^{\prime} ) to obtain renormalized transition rates between the remaining configurations. The multiplicative structure of the new generated transition rates suggests that for a very broad class of disordered systems, the distribution of renormalized exit barriers defined as B_{\rm out} ({\cal C} ) \equiv {-}\! \ln W_{\rm out}({\cal C} ) will become broader and broader upon iteration, so that the strong disorder renormalization procedure should become asymptotically exact at large time scales. We have checked numerically this scenario for the non-equilibrium dynamics of a directed polymer in a two-dimensional random medium.


PACS

61.41.+e Polymers, elastomers, and plastics

MSC

82C28 Dynamic renormalization group methods (See also 81T17)

82C44 Dynamics of disordered systems (random Ising systems, etc.)

82D60 Polymers

Subjects

Soft matter, liquids and polymers

Dates

Issue 25 (27 June 2008)

Received 31 March 2008, in final form 1 April 2008

Published 27 May 2008


A Corrigendum for this article has been published in 2008 J. Phys. A: Math. Theor. 41 499801


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