Numéro
J. Phys. I France
Volume 3, Numéro 6, June 1993
Page(s) 1329 - 1357
DOI https://doi.org/10.1051/jp1:1993183
DOI: 10.1051/jp1:1993183
J. Phys. I France 3 (1993) 1329-1357

Dynamics of manifolds in random media: the selfconsistent Hartree approximation

Harald Kinzelbach and Heinz Horner

Institut für Theoretische Physik, Philosophenweg 19, D-6900 Heidelberg, Germany


(Received 22 December 1992, accepted 12 February 1993)

Abstract
We discuss a dynamical description of fluctuating manifolds in random media, using an approximation which becomes exact in the `spherical limit' $N \rightarrow \infty$, N being the dimension of the transversal fluctuations. The system behaviour is studied in detail for the case of quenched disorder with short range correlations. In the static limit, we recover solutions known from a replica calculation with one step replica symmetry breaking. In the dynamical formulation it turns out that this replica symmetry breaking is related to broken ergodicity for temperatures below a critical point. While the static behaviour in the low temperature phase superficially seems to be not very different from that of the high temperature phase, the dynamic treatment shows that the manifolds get dynamically localized below the critical temperature. The value we find for this `freezing temperature' is higher than the corresponding result from replica theory. Introducing an additional external quadratic potential, we find that the character of the phase transition changes with increasing coupling strength $\mu$. There is a tricritical point $\mu^*$, for $\mu < \mu^*$ the phase transition is of first order, for $\mu > \mu^*$ it becomes a second order one. We give the phase diagram for this generalized model and discuss the dynamical behaviour in the different regimes.

PACS
05.40 - 61.40

© Les Editions de Physique 1993

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