Monte Carlo simulation of a disclination core in nematic solutions of rodlike molecules
- 10 May 1993
- journal article
- research article
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 70 (19) , 2916-2919
- https://doi.org/10.1103/physrevlett.70.2916
Abstract
The core structure of a disclination line defect in a nematic liquid crystal is simulated by a Monte Carlo technique in which molecules are represented as hard spherocylinders, with aspect ratios ranging from 5 to 15. For small aspect ratios (5 and 8), we confirm the mean-field Landau theory that the core is biaxial with negative order parameter at the center. The order parameter coherence length is small, of the order of the molecular diameter. For large aspect ratios, we discover a new microscopically ‘‘escaped’’ structure for -1/2 wedge disclinations, in which the molecules point predominantly along the disclination line. Free energy calculations demonstrate that the ‘‘escaped’’ structure is of lower energy than the unescaped ‘‘flat’’ structure, which is metastable. We expect the ‘‘escaped’’ structure to retard disclination mobility.Keywords
This publication has 13 references indexed in Scilit:
- Phase diagram for a system of hard spherocylindersPhysical Review A, 1991
- Structure of hard-core models for liquid crystalsThe Journal of Physical Chemistry, 1988
- Defect Core Structure in Nematic Liquid CrystalsPhysical Review Letters, 1987
- Freeze-Fracture Imaging of Ordered Phases of Tobacco Mosaic Virus in WaterMolecular Crystals and Liquid Crystals, 1986
- Lattice of disclinations: The structure of the blue phases of cholesteric liquid crystalsPhysical Review A, 1983
- Some magnetohydrodynamic effects in liquid crystalsArchive for Rational Mechanics and Analysis, 1966
- I. Liquid crystals. On the theory of liquid crystalsDiscussions of the Faraday Society, 1958
- THE EFFECTS OF SHAPE ON THE INTERACTION OF COLLOIDAL PARTICLESAnnals of the New York Academy of Sciences, 1949
- The theory of liquid crystalsTransactions of the Faraday Society, 1933
- The effect of a magnetic field on the nematic stateTransactions of the Faraday Society, 1933