Dynamic tuning of the director field in liquid crystal shells using block copolymers

When an orientationally ordered system, like a nematic liquid crystal (LC), is confined on a self-closing spherical shell, topological constraints arise with intriguing consequences that depend critically on how the LC is aligned in the shell. We demonstrate reversible dynamic tuning of the alignmen...

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Main Authors: JungHyun Noh, Yiwei Wang, Hsin-Ling Liang, Venkata Subba Rao Jampani, Apala Majumdar, Jan P. F. Lagerwall
Format: Article
Language:English
Published: American Physical Society 2020-07-01
Series:Physical Review Research
Online Access:http://doi.org/10.1103/PhysRevResearch.2.033160
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author JungHyun Noh
Yiwei Wang
Hsin-Ling Liang
Venkata Subba Rao Jampani
Apala Majumdar
Jan P. F. Lagerwall
author_facet JungHyun Noh
Yiwei Wang
Hsin-Ling Liang
Venkata Subba Rao Jampani
Apala Majumdar
Jan P. F. Lagerwall
author_sort JungHyun Noh
collection DOAJ
description When an orientationally ordered system, like a nematic liquid crystal (LC), is confined on a self-closing spherical shell, topological constraints arise with intriguing consequences that depend critically on how the LC is aligned in the shell. We demonstrate reversible dynamic tuning of the alignment, and thereby the topology, of nematic LC shells stabilized by the nonionic amphiphilic block copolymer Pluronic F127. Deep in the nematic phase, the director (the average molecule orientation) is tangential to the interface, but upon approaching the temperature T_{NI} of the nematic-isotropic transition, the director realigns to normal. We link this to a delicate interplay between an interfacial tension that is nearly independent of director orientation, and the configuration-dependent elastic deformation energy of an LC confined in a shell. The process is primarily triggered by the heating-induced reduction of the nematic order parameter, hence realignment temperatures differ by several tens of degrees between LCs with high and low T_{NI}, respectively. The temperature of realignment is always lower on the positive-curved shell outside than at the negative-curved inside, yielding a complex topological reconfiguration on heating. Complementing experimental investigations with mathematical modeling and computer simulations, we identify and investigate three different trajectories, distinguished by their configurations of topological defects in the initial tangential-aligned shell. Our results uncover a new aspect of the complex response of LCs to curved confinement, demonstrating that the order of the LC itself can influence the alignment and thereby the topology of the system. They also reveal the potential of amphiphilic block copolymer stabilizers for enabling continuous tunability of LC shell configuration, opening doors for in-depth studies of topological dynamics as well as novel applications in, e.g., sensing and programed soft actuators.
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spelling doaj.art-cad4f9f75dde4b7d8537bba618e91d402024-04-12T16:57:57ZengAmerican Physical SocietyPhysical Review Research2643-15642020-07-012303316010.1103/PhysRevResearch.2.033160Dynamic tuning of the director field in liquid crystal shells using block copolymersJungHyun NohYiwei WangHsin-Ling LiangVenkata Subba Rao JampaniApala MajumdarJan P. F. LagerwallWhen an orientationally ordered system, like a nematic liquid crystal (LC), is confined on a self-closing spherical shell, topological constraints arise with intriguing consequences that depend critically on how the LC is aligned in the shell. We demonstrate reversible dynamic tuning of the alignment, and thereby the topology, of nematic LC shells stabilized by the nonionic amphiphilic block copolymer Pluronic F127. Deep in the nematic phase, the director (the average molecule orientation) is tangential to the interface, but upon approaching the temperature T_{NI} of the nematic-isotropic transition, the director realigns to normal. We link this to a delicate interplay between an interfacial tension that is nearly independent of director orientation, and the configuration-dependent elastic deformation energy of an LC confined in a shell. The process is primarily triggered by the heating-induced reduction of the nematic order parameter, hence realignment temperatures differ by several tens of degrees between LCs with high and low T_{NI}, respectively. The temperature of realignment is always lower on the positive-curved shell outside than at the negative-curved inside, yielding a complex topological reconfiguration on heating. Complementing experimental investigations with mathematical modeling and computer simulations, we identify and investigate three different trajectories, distinguished by their configurations of topological defects in the initial tangential-aligned shell. Our results uncover a new aspect of the complex response of LCs to curved confinement, demonstrating that the order of the LC itself can influence the alignment and thereby the topology of the system. They also reveal the potential of amphiphilic block copolymer stabilizers for enabling continuous tunability of LC shell configuration, opening doors for in-depth studies of topological dynamics as well as novel applications in, e.g., sensing and programed soft actuators.http://doi.org/10.1103/PhysRevResearch.2.033160
spellingShingle JungHyun Noh
Yiwei Wang
Hsin-Ling Liang
Venkata Subba Rao Jampani
Apala Majumdar
Jan P. F. Lagerwall
Dynamic tuning of the director field in liquid crystal shells using block copolymers
Physical Review Research
title Dynamic tuning of the director field in liquid crystal shells using block copolymers
title_full Dynamic tuning of the director field in liquid crystal shells using block copolymers
title_fullStr Dynamic tuning of the director field in liquid crystal shells using block copolymers
title_full_unstemmed Dynamic tuning of the director field in liquid crystal shells using block copolymers
title_short Dynamic tuning of the director field in liquid crystal shells using block copolymers
title_sort dynamic tuning of the director field in liquid crystal shells using block copolymers
url http://doi.org/10.1103/PhysRevResearch.2.033160
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