Abstract

We study a continuous quasi-two-dimensional order-disorder phase transition that occurs in a simple model of a material that is inhomogeneously strained due to the presence of dislocation lines. Performing Monte Carlo simulations of different system sizes and using finite size scaling, we measure critical exponents describing the transition of β=0.18±0.02, γ=1.0±0.1, and α=0.10±0.02. Comparable exponents have been reported in a variety of physical systems. These systems undergo a range of different types of phase transitions, including structural transitions, exciton percolation, and magnetic ordering. In particular, similar exponents have been found to describe the development of magnetic order at the onset of the pseudogap transition in high-temperature superconductors. Their common universal critical exponents suggest that the essential physics of the transition in all of these physical systems is the same as in our simple model. We argue that the nature of the transition in our model is related to surface transitions although our model has no free surface.

Highlights

  • Real solids are commonly in a strained state

  • In order to study the critical behavior of this process, we consider a mesoscopic spin model in which the coupling between spins reflects the strain field induced by the dislocation walls

  • The critical exponents found are comparable with exponents that have been measured experimentally in a variety of materials, and for different types of transitions [1, 2, 7,8,9,10,11,12,13,14]

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Summary

Introduction

Real solids are commonly in a strained state. This can be due to a variety of reasons, ranging from forces applied upon them to the presence of structural defects, to ongoing phase transformations. Each layer orders at a different critical temperature. In order to study the critical behavior of this process, we consider a mesoscopic spin model in which the coupling between spins reflects the strain field induced by the dislocation walls.

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