ON THE ELECTROCLINIC EFFECT IN SMECTIC A* POLYMERS AND LOW MOLAR MASS ANALOGUES

1993 ◽  
pp. 301-317 ◽  
Author(s):  
L. Komitov ◽  
S. T. Lagerwall ◽  
B. Stebler ◽  
E. Chiellini ◽  
G. Galli ◽  
...  
Keyword(s):  
1989 ◽  
Vol 5 (2) ◽  
pp. 463-478 ◽  
Author(s):  
F. Hardouin ◽  
G. Sigaud ◽  
P. Keller ◽  
H. Richard ◽  
Nguyen Huu Tinh ◽  
...  
Keyword(s):  

2004 ◽  
Vol 43 (26) ◽  
pp. 3429-3432 ◽  
Author(s):  
Channabasaveshwar V. Yelamaggad ◽  
Subbarao Krishna Prasad ◽  
Geetha G. Nair ◽  
Indudhara Swamy Shashikala ◽  
Doddamane S. Shankar Rao ◽  
...  
Keyword(s):  

2004 ◽  
Vol 116 (26) ◽  
pp. 3511-3514 ◽  
Author(s):  
Channabasaveshwar V. Yelamaggad ◽  
Subbarao Krishna Prasad ◽  
Geetha G. Nair ◽  
Indudhara Swamy Shashikala ◽  
Doddamane S. Shankar Rao ◽  
...  
Keyword(s):  

The impact of liquid crystals over the past 20 years in the area of electro-optical displays is generally acknowledged as stemming from a combination of chemistry (molecular engineering) and physics (development of practical display modes). Starting with the early experiments on dynamic scattering, a review is given of the developments in this field arising from the chemist’s ability to respond to the requirements set first for reliable materials for twisted nematic displays, later for supertwist devices and electrically addressed smectic A displays, and most recently for ferroelectric displays and the electroclinic effect. Although the driving force for such research has been the demand for materials for ever faster switching devices able to portray more complex data, the benefits of this quest for new liquid-crystal materials on basic understanding of the properties of liquid crystals and their relation to molecular structure should not be forgotten, and this aspect is firmly emphasized.


Author(s):  
K.J. Ihn ◽  
R. Pindak ◽  
J. A. N. Zasadzinski

A new liquid crystal (called the smectic-A* phase) that combines cholesteric twist and smectic layering was a surprise as smectic phases preclude twist distortions. However, the twist grain boundary (TGB) model of Renn and Lubensky predicted a defect-mediated smectic phase that incorporates cholesteric twist by a lattice of screw dislocations. The TGB model for the liquid crystal analog of the Abrikosov phase of superconductors consists of regularly spaced grain boundaries of screw dislocations, parallel to each other within the grain boundary, but rotated by a fixed angle with respect to adjacent grain boundaries. The dislocations divide the layers into blocks which rotate by a discrete amount, Δθ, given by the ratio of the layer spacing, d, to the distance between grain boundaries, lb; Δθ ≈ d/lb (Fig. 1).


1978 ◽  
Vol 3 ◽  
pp. 357-357
Author(s):  
J. Als-Nielsen ◽  
R. J. Birgeneau ◽  
M. Kaplan ◽  
J. D. Litster ◽  
C. R. Safinya
Keyword(s):  
X Ray ◽  

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