Novel liquid-crystal phase-transition behavior at the chiral nematic–smectic-A–smectic-Cpoint

1989 ◽  
Vol 62 (18) ◽  
pp. 2136-2139 ◽  
Author(s):  
D. S. Parmar ◽  
N. A. Clark ◽  
D. M. Walba ◽  
M. D. Wand
Soft Matter ◽  
2019 ◽  
Author(s):  
Ahram Suh ◽  
Min-Jun Gim ◽  
Daniel Beller ◽  
Dong Ki Yoon

We study transformations of self-organised defect arrays at the nematic–smectic A liquid crystal phase transition, and show that these defect configurations are correlated, or “remembered”, across the phase transition.


1998 ◽  
Vol 5 (4-6) ◽  
pp. 835-838 ◽  
Author(s):  
E.L. Duarte ◽  
A.J. Palangana ◽  
R. Itri ◽  
A.R. Sampaio ◽  
A.A. Barbosa

2002 ◽  
Vol 12 (9) ◽  
pp. 377-380
Author(s):  
K. B. Cooper ◽  
M. P. Lilly ◽  
J. P. Eisenstein ◽  
L. N. Pfeiffer ◽  
K. W. West

Transport measurements of high-mohility two-dimensional electron systems at low temperatures have revealed a large resistance anisotropy around half-filling of excited Landau levels. These results have been attributed to electronic stripe-phase formation with spontaneously broken orientational symmetry. Mechanisms which are known to break the orientational symmetry include poorly-understood crystal structure effects and an in-plane magnetic field, $B_{||}$. Here we report that a large $B_{||}$ also causes the transport anisotropy to persist up to much higher temperatures. In this regime, we find that the anisotropic resistance scales sublinearly with $B_{||}/T$. These observations support the proposal that the transition from anisotropic to isotropic transport reflects a liquid crystal phase transition where local stripe order persists even in the isotropic regime.


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