Phase Transition Dynamics and Stochastic Resonance in Topologically Confined Nematic Liquid Crystals

TL;DR

This study uses numerical simulations to explore how topological defects influence phase transition dynamics and stochastic resonance in confined nematic liquid crystals, revealing size-dependent pathways and boundary effects.

Contribution

It introduces a detailed analysis of defect-mediated phase transition pathways and stochastic resonance behavior in confined nematic liquid crystals using the Lebwohl-Lasher model.

Findings

Small systems have defect structures at corners with no bulk defect formation.

Large systems spontaneously form bulk defects that merge with corner defects.

Boundary anchoring strength significantly affects stochastic resonance and phase transition pathways.

Abstract

Topological defects resulted from boundary constraints in confined liquid crystals have attracted extensive research interests. In this paper, we use numerical simulation to study the phase transition dynamics in the context of stochastic resonance in a bistable liquid crystal device containing defects. This device is made of nematic liquid crystals confined in a shallow square well, and is described by the planar Lebwohl-Lasher model. The stochastic phase transition processes of the system in the presence of a weak oscillating potential is simulated using an over-damped Langevin dynamics. Our simulation results reveal that, depending on system size, the phase transition may follow two distinct pathways: in small systems the pre-existing defect structures at the corners hold until the last stage and there is no newly formed defect point in the bulk during the phase transition, In large systems new defect points appear spontaneously in the bulk and eventually merge with the pre-existing defects at the corners. For both transition pathways stochastic resonance can be observed, but show dramatic difference in their responses to the boundary anchoring strength. In small systems we observe a "sticky-boundary" effect for a certain range of anchoring strength in which the phase transition gets stuck and stochastic resonance becomes de-activated. Our work demonstrates the dynamical interplay among defects, noises, and boundary conditions in confined liquid crystals.