Calorimetric study of activated kinetics of the nematic and smectic phase transitions in an aligned nano-colloidal liquid crystal+aerosil gel

2008 ◽  
Vol 93 (3) ◽  
pp. 899-906 ◽  
Author(s):  
D. Sharma

2005 ◽  
Vol 122 (22) ◽  
pp. 224709 ◽  
Author(s):  
Zdravko Kutnjak ◽  
George Cordoyiannis ◽  
George Nounesis ◽  
Andrija Lebar ◽  
Boštjan Zalar ◽  
...  




Author(s):  
Anna Drzewicz ◽  
Małgorzata Jasiurkowska-Delaporte ◽  
Ewa Juszyńska-Gałązka ◽  
Mirosław Gałązka ◽  
Wojciech Zając ◽  
...  

The impact of high pressure on relaxation dynamics and the crystallization process in the smectic phase with antiferroelectric properties ( phase) of novel liquid crystal was studied.



1980 ◽  
Vol 41 (17) ◽  
pp. 419-422 ◽  
Author(s):  
K.J. Lushington ◽  
G.B. Kasting ◽  
C.W. Garland


1991 ◽  
Vol 27 (3) ◽  
pp. 315-322 ◽  
Author(s):  
K. Engberg ◽  
H. Jonsson ◽  
A. Hult ◽  
U. W. Gedde


2015 ◽  
Vol 88 (6) ◽  
pp. 547-559 ◽  
Author(s):  
P. Kalakonda ◽  
G.S. Iannacchione


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).



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