The zero-temperature random-field Ising model on a bi-layered Bethe lattice

TL;DR

This paper analytically solves the zero-temperature random-field Ising model on a bi-layered Bethe lattice, revealing how inter-layer interactions influence infinite avalanches and phase transitions in magnetization.

Contribution

It introduces an analytical solution for the model on a bi-layered Bethe lattice and explores how inter-layer interaction strengths affect infinite avalanches and phase transitions.

Findings

Infinite avalanches occur for small disorder values.

Reducing inter-layer bond strength can induce a phase transition.

Monte-Carlo simulations support analytical results.

Abstract

The zero-temperature random-field Ising model is solved analytically for magnetisation vs external field for a bi-layered Bethe lattice. The mechanisms of infinite avalanches which are observed for small values of disorder are established. The effects of variable inter-layer interaction strengths on infinite avalanches are investigated. The spin-field correlation length is calculated and its critical behaviour is discussed. Direct Monte-Carlo simulations of spin-flip dynamics are shown to support the analytical findings. We find, paradoxically, that a reduction of the inter-layer bond strength can cause a phase transition from a regime with continuous magnetisation reversal to a regime where magnetisation exhibits a discontinuity associated with an infinite avalanche. This effect is understood in terms of the proposed mechanisms for the infinite avalanche.