Dynamics of Order Reconstruction in a Nanoconfined Nematic Liquid Crystal with a Topological Defect

At the wall in a hybrid nematic cell with strong anchoring, the nematic director is parallel to one wall and perpendicular to the other. Within the Landau-de Gennes theory, we have investigated the dynamics of s = ±1/2 wedge disclinations in such a cell, using the two-dimensional finite-difference i...

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Main Authors: Xuan Zhou, Zhidong Zhang
Format: Article
Language:English
Published: MDPI AG 2013-12-01
Series:International Journal of Molecular Sciences
Subjects:
Online Access:http://www.mdpi.com/1422-0067/14/12/24135
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spelling doaj-e67bc0ed1fb74f8086cbb1de818ff65d2020-11-24T22:01:01ZengMDPI AGInternational Journal of Molecular Sciences1422-00672013-12-011412241352415310.3390/ijms141224135ijms141224135Dynamics of Order Reconstruction in a Nanoconfined Nematic Liquid Crystal with a Topological DefectXuan Zhou0Zhidong Zhang1Department of physics, Hebei University of Technology, Tianjin 300401, ChinaDepartment of physics, Hebei University of Technology, Tianjin 300401, ChinaAt the wall in a hybrid nematic cell with strong anchoring, the nematic director is parallel to one wall and perpendicular to the other. Within the Landau-de Gennes theory, we have investigated the dynamics of s = ±1/2 wedge disclinations in such a cell, using the two-dimensional finite-difference iterative method. Our results show that with the cell gap decreasing, the core of the defect explodes, and the biaxiality propagates inside the cell. At a critical value of dc* ≈ 9ξ (where ξ is the characteristic length for order-parameter changes), the exchange solution is stable, while the defect core solution becomes metastable. Comparing to the case with no initial disclination, the value at which the exchange solution becomes stable increases relatively. At a critical separation of dc ≈ 6ξ, the system undergoes a structural transition, and the defect core merges into a biaxial layer with large biaxiality. For weak anchoring boundary conditions, a similar structural transition takes place at a relative lower critical value. Because of the weakened frustration, the asymmetric boundary conditions repel the defect to the weak anchoring boundary and have a relatively lower critical value of da, where the shape of the defect deforms. Further, the response time between two very close cell gaps is about tens of microseconds, and the response becomes slower as the defect explodes.http://www.mdpi.com/1422-0067/14/12/24135biaxial transitiontopological defecteigenvalue exchangeresponse time
collection DOAJ
language English
format Article
sources DOAJ
author Xuan Zhou
Zhidong Zhang
spellingShingle Xuan Zhou
Zhidong Zhang
Dynamics of Order Reconstruction in a Nanoconfined Nematic Liquid Crystal with a Topological Defect
International Journal of Molecular Sciences
biaxial transition
topological defect
eigenvalue exchange
response time
author_facet Xuan Zhou
Zhidong Zhang
author_sort Xuan Zhou
title Dynamics of Order Reconstruction in a Nanoconfined Nematic Liquid Crystal with a Topological Defect
title_short Dynamics of Order Reconstruction in a Nanoconfined Nematic Liquid Crystal with a Topological Defect
title_full Dynamics of Order Reconstruction in a Nanoconfined Nematic Liquid Crystal with a Topological Defect
title_fullStr Dynamics of Order Reconstruction in a Nanoconfined Nematic Liquid Crystal with a Topological Defect
title_full_unstemmed Dynamics of Order Reconstruction in a Nanoconfined Nematic Liquid Crystal with a Topological Defect
title_sort dynamics of order reconstruction in a nanoconfined nematic liquid crystal with a topological defect
publisher MDPI AG
series International Journal of Molecular Sciences
issn 1422-0067
publishDate 2013-12-01
description At the wall in a hybrid nematic cell with strong anchoring, the nematic director is parallel to one wall and perpendicular to the other. Within the Landau-de Gennes theory, we have investigated the dynamics of s = ±1/2 wedge disclinations in such a cell, using the two-dimensional finite-difference iterative method. Our results show that with the cell gap decreasing, the core of the defect explodes, and the biaxiality propagates inside the cell. At a critical value of dc* ≈ 9ξ (where ξ is the characteristic length for order-parameter changes), the exchange solution is stable, while the defect core solution becomes metastable. Comparing to the case with no initial disclination, the value at which the exchange solution becomes stable increases relatively. At a critical separation of dc ≈ 6ξ, the system undergoes a structural transition, and the defect core merges into a biaxial layer with large biaxiality. For weak anchoring boundary conditions, a similar structural transition takes place at a relative lower critical value. Because of the weakened frustration, the asymmetric boundary conditions repel the defect to the weak anchoring boundary and have a relatively lower critical value of da, where the shape of the defect deforms. Further, the response time between two very close cell gaps is about tens of microseconds, and the response becomes slower as the defect explodes.
topic biaxial transition
topological defect
eigenvalue exchange
response time
url http://www.mdpi.com/1422-0067/14/12/24135
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AT zhidongzhang dynamicsoforderreconstructioninananoconfinednematicliquidcrystalwithatopologicaldefect
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