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Updated: Jun 10, 2025

Orientational Transition in a Liquid Crystal Triggered by the Thermodynamic Growth of Interfacial Wetting Sheets
Published on: May 15, 2017
Edge-on anchored discotic liquid crystals in spherical shells: A computational study of the phases and defects
Daniel Salgado-Blanco1, Enrique Díaz-Herrera2, José A Martínez-González3
1Investigadores por México <a href="https://ror.org/059ex5q34">CONAHCYT</a> - Centro Nacional de Supercómputo, <a href="https://ror.org/03sbzv212">Instituto Potosino de Investigación Científica y Tecnológica</a>, Camino a la Presa San José 2055, 78216, San Luis Potosí, México and Grupo de Ciencia e Ingeniería Computacionales, Centro Nacional de Supercómputo. <a href="https://ror.org/03sbzv212">IPICYT</a>, Camino a la Presa San José 2055, Col. Lomas 4a Sección, San Luis Potosí, S. L. P. 78216, México.
Abstract:
The self-assembly of liquid crystal droplets and shells represents a captivating frontier in soft matter physics, promising precision engineering of functional materials. In this study, we delve into the phase behavior and investigate defect formation patterns in spherical shell-confined discotic liquid crystals (DLCs) through NpT Monte Carlo simulations. These shells are created by confining DLCs between two spherical surfaces, promoting the same anchoring. In this study, we focus on the case when both surfaces promote edge-on (planar) anchoring. Our study confirms a general result which states that, when a liquid crystal is under strong confinement, the nature of the isotropic-nematic transition changes from first order into continuous. Furthermore, as expected, topological defects at the spherical surface arise due to the topological constraints on the director field. Notably, our investigation reveals a unique topological defect configuration, characterized by the formation of four disclination lines that bridge the inner and external surfaces. Additionally, we observe a mixed ±1/2 wedge-twist disclination line that forms an arch that terminates at the outer surface. This arch decreases its length with decreasing temperature to eventually disappear.
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