Structure and Phase Transitions in Partially Confined Smectic Liquid Crystals

1996 ◽  
Vol 464 ◽  
Author(s):  
L. J. Martinez-Miranda ◽  
Yushan Shi ◽  
Satyendra Kumar

ABSTRACTWe present the results of an X-ray scattering study on partially confined smectic-A (layered) LC films. This partial confinement is achieved by placing the LC material inside the open grooves of a glass grating. Samples prepared in this manner are confined in the direction perpendicular to the gratings. Samples in which the LC is contained entirely inside the grooves develop an induced molecular tilt, which results in a compression of the smectic layers. The molecular tilt varies as the amount of the LC material increases, eventually forming a thin overlayer film above the gratings. As the thickness varies, a second region develops in the films. The layer spacing in this region is close to the bulk layer spacing. This structural evolution is coupled to a variation in the nematic-to-smectic-A phase transition temperature of the samples from the bulk. In addition, the nature of the phase transition is driven first order. The effects of partial confinement on a sm-C* LC film is discussed briefly.

2010 ◽  
Vol 46 (9) ◽  
pp. 1866-1877 ◽  
Author(s):  
Zhiyong Jiang ◽  
Yujing Tang ◽  
Jens Rieger ◽  
Hans-Friedrich Enderle ◽  
Dieter Lilge ◽  
...  

1990 ◽  
Vol 59 (6) ◽  
pp. 2036-2053 ◽  
Author(s):  
Jean-Paul Pouget ◽  
Seiichi Kagoshima ◽  
Tsuyoshi Tamegai ◽  
Yoshio Nogami ◽  
Koichi Kubo ◽  
...  

1990 ◽  
Vol 2 (51) ◽  
pp. 10549-10558 ◽  
Author(s):  
F Brunet ◽  
D F McMorrow ◽  
A Gibaud ◽  
C Patterson

2001 ◽  
Vol 16 (6) ◽  
pp. 1814-1821 ◽  
Author(s):  
H. C. Kang ◽  
S. H. Seo ◽  
D. Y. Noh

We present an x-ray scattering study on the evolution of the growth mode, the surface morphology, and the lattice strain of AlN/sapphire(0001) films during sputter growth. Aligned epitaxial planar layers with strain relaxed to about 2% are nucleated during initial stage growth. As the film thickness increases to an effective “critical” thickness of approximately 250 Å, the growth gradually crosses over to the less aligned island growth. As the growth crossover occurs, the growth front becomes substantially rougher and the residual strain begins to relax. The cogrowth of the planar layer and the islands results in a nonuniform strain distribution.


1988 ◽  
Vol 105 (2) ◽  
pp. K107-K110 ◽  
Author(s):  
B. Pura ◽  
J. Przedmojski ◽  
K. Wentowska ◽  
R. D??browski ◽  
K. Czupryński

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