Molecular flexibility and orientational ordering of nematic liquid crystals

1991 ◽  
Vol 94 (4) ◽  
pp. 2758-2772 ◽  
Author(s):  
Demetri J. Photinos ◽  
Edward T. Samulski ◽  
Hirokazu Toriumi
1989 ◽  
Vol 5 (3) ◽  
pp. 941-952 ◽  
Author(s):  
A. L. Bailey ◽  
G. S. Bates ◽  
E. E. Burnell ◽  
G. L. Hoatson

Author(s):  
Matej Cvetko ◽  
Milan Ambrožič ◽  
Samo Kralj

We study the influence of external electric or magnetic field B on orientational ordering of nematic liquid crystals or of other rod-like objects (e.g. nanotubes immersed in a liquid) in the presence of random anisotropy field type of disorder. The Lebwohl–Lasher lattice type of semi-microscopic approach is used at zero temperature. Therefore, results are valid well below the transition into the isotropic phase. We calculate the correlation function of systems as a function of B, concentration p of impurities imposing random anisotropy field disorder, the disorder strength W and system dimensionality (2D and 3D systems). In order to probe memory effects we calculate correlation length ξ for random and homogeneous initial configurations. We determine the crossover fields B c(p) separating roughly the ordered and disordered regime. Memory effects are apparent only in the latter case, i.e. for B < B c. PACS numbers: 47.51.+a, 47.54.-r, 07.05.Tp, 61.30.-v


1994 ◽  
Vol 4 (2) ◽  
pp. 239-252 ◽  
Author(s):  
A. Hertrich ◽  
A. P. Krekhov ◽  
O. A. Scaldin

1975 ◽  
Vol 36 (1) ◽  
pp. 59-67 ◽  
Author(s):  
V. Vitek ◽  
M. Kléman

1975 ◽  
Vol 36 (C1) ◽  
pp. C1-69-C1-76 ◽  
Author(s):  
L. M. BLINOV ◽  
V. A. KIZEL ◽  
V. G. RUMYANTSEV ◽  
V. V. TITOV

2017 ◽  
Vol 13 (2) ◽  
pp. 4705-4717
Author(s):  
Zhang Qian ◽  
Zhou Xuan ◽  
Zhang Zhidong

Basing on Landau–de Gennes theory, this study investigated the chiral configurations of nematic liquid crystals confined to cylindrical capillaries with homeotropic anchoring on the cylinder walls. When the elastic anisotropy (L2/L1) is large enough, a new structure results from the convergence of two opposite escape directions of the heterochiral twist and escape radial (TER) configurations. The new defect presents when L2/L1≥7 and disappears when L2/L1<7. The new structure possesses a heterochiral hyperbolic defect at the center and two homochiral radial defects on both sides. The two radial defects show different chiralities.


Sign in / Sign up

Export Citation Format

Share Document