Continuum limit of random matrix products in statistical mechanics of disordered systems

TL;DR

This paper studies a diffusion limit of random matrix products in disordered systems, deriving explicit formulas for Lyapunov exponents and connecting the continuum approximation to known singular behaviors in disordered Ising models.

Contribution

It introduces a diffusion model as a continuum limit of matrix products, providing explicit Lyapunov exponent formulas and linking them to physical singularities in disordered systems.

Findings

Explicit Lyapunov exponent formula in terms of Bessel functions

Continuum limit captures Derrida-Hilhorst singularity

Mathematical analysis of free energy in McCoy-Wu model

Abstract

We consider a particular weak disorder limit ("continuum limit") of matrix products that arise in the analysis of disordered statistical mechanics systems, with a particular focus on random transfer matrices. The limit system is a diffusion model for which the leading Lyapunov exponent can be expressed explicitly in terms of modified Bessel functions, a formula that appears in the physical literature on these disordered systems. We provide an analysis of the diffusion system as well as of the link with the matrix products. We then apply the results to the framework considered by Derrida and Hilhorst [J. Phys. A (1983)], which deals in particular with the strong interaction limit for disordered Ising model in one dimension and that identifies a singular behavior of the Lyapunov exponent (of the transfer matrix), and to the two dimensional Ising model with columnar disorder (McCoy-Wu model). We show that the continuum limit sharply captures the Derrida and Hilhorst singularity. Moreover we revisit the analysis by McCoy and Wu [Phys. Rev. 1968] and remark that it can be interpreted in terms of the continuum limit approximation. We provide a mathematical analysis of the continuum approximation of the free energy of the McCoy-Wu model, clarifying the prediction (by McCoy and Wu) that, in this approximation, the free energy of the two dimensional Ising model with columnar disorder is $C^\infty$ but not analytic at the critical temperature.