The Smectic Layer Reorientation Induced by an Electric Field in a Short Pitch Ferroelectric Liquid Crystal

2004 ◽  
Vol 311 (1) ◽  
pp. 77-82 ◽  
Author(s):  
Chang-Jae Yu ◽  
Wan-Soo Kim ◽  
Sin-Doo Lee
1989 ◽  
Vol 28 (Part 2, No. 1) ◽  
pp. L119-L120 ◽  
Author(s):  
Masahiro Johno ◽  
A. D. L. Chandani ◽  
Yukio Ouchi ◽  
Hideo Takezoe ◽  
Atsuo Fukuda ◽  
...  

2002 ◽  
Vol 80 (14) ◽  
pp. 2439-2441 ◽  
Author(s):  
Keizo Nakayama ◽  
Junji Ohtsubo ◽  
Masanori Ozaki ◽  
Katsumi Yoshino

2018 ◽  
Vol 149 (23) ◽  
pp. 234901 ◽  
Author(s):  
Susanna K. Ahola ◽  
Petri Ingman ◽  
Reino Laatikainen ◽  
Jari Sinkkonen ◽  
Jukka Jokisaari

2002 ◽  
Vol 41 (Part 1, No. 5A) ◽  
pp. 2989-2992 ◽  
Author(s):  
Takeshi Murashige ◽  
Hideo Fujikake ◽  
Seiichiro Ikehata ◽  
Fumio Sato

Doklady BGUIR ◽  
2019 ◽  
pp. 21-27
Author(s):  
E. P. Pozhidaev ◽  
T. P. Tkachenko ◽  
A. V. Kuznetsov ◽  
I. N. Kompanets

In a known display cell with the nematic liquid crystal (NLC) and interdigital electrodes on one of the glass substrates, the “In-Plane Switching” (IPS) mode is implemented, in which the NLC main optical axis reorients in a plane parallel to substrates, providing the most correct color reproduction at different angles view, up to 178 ° horizontally and vertically. Unfortunately, the creation of interdigital metal electrodes complicates and increases the technological process cost and causes a decrease in image contrast. At the same time, experimental results and calculations based on classical electro-optics of crystals indicate that electrooptical switching in the IPS mode is a natural and intrinsic feature of a conventional (with continuous electrodes) display cell with a planar-oriented layer of the ferroelectric liquid crystal (FLC), in which the effect of the deformed (by the electric field) helix FLC nanostructure is realized (DHF effect). In such a cell, the reorientation of the main optical axis under the influence of a weak electric field also occurs in the substrate plane if the FLC has a small pitch (about 100 nm or less) and a large tilt angle of molecules in the layer (about 38 ° or more). The dependences of the FLC cell light transmittance measured in this work, confirmed the achievement of the IPS electro-optical mode in the DHF FLC cell; moreover, the light modulation frequency was 1 kHz. Thus, while maintaining all the advantages of the IPS mode known in NLC, its implementation in FLC allows additionally obtaining technological advantages and multiple increase in modulation frequency.


Author(s):  
Anna V. Ryzhkova ◽  
Pratibha Ramarao ◽  
Maryam Nikkhou ◽  
Igor Muševič

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