Behavior of the Cholesteric Liquid-Crystal Fabry-Perot Cavity in the Bragg Reflection Band

2000 ◽  
Vol 84 (6) ◽  
pp. 1168-1171 ◽  
Author(s):  
Zhizhong Zhuang ◽  
Young Jin Kim ◽  
J. S. Patel
1999 ◽  
Vol 24 (1) ◽  
pp. 55 ◽  
Author(s):  
Jay E. Stockley ◽  
Gary D. Sharp ◽  
Kristina M. Johnson

2018 ◽  
Vol 6 (45) ◽  
pp. 12377-12385 ◽  
Author(s):  
Amid Ranjkesh ◽  
Tae-Hoon Yoon

A dual thermal and electrical polymer-stabilized cholesteric liquid crystal has been fabricated by using ultraviolet light absorbers. The Bragg reflection can be autonomously controlled by temperature and manually by an electric field.


Sensors ◽  
2020 ◽  
Vol 20 (16) ◽  
pp. 4643
Author(s):  
Soyeon Ahn ◽  
Myeong Ock Ko ◽  
Jong-Hyun Kim ◽  
Zhongping Chen ◽  
Min Yong Jeon

We report the results of an experimental study of the characterization of second-order reflection bands from a cholesteric liquid crystal (CLC) cell that depends on the applied electric field, using a wide bandwidth wavelength-swept laser. The second-order reflection bands around 1300 nm and 1500 nm were observed using an optical spectrum analyzer when an electric field was applied to a horizontally oriented electrode cell with a pitch of 1.77 μm. A second-order reflection spectrum began to appear when the intensity of the electric field was 1.03 Vrms/μm with the angle of incidence to the CLC cell fixed at 36°. The reflectance increased as the intensity of the electric field increased at an angle of incidence of 20°, whereas at an incident angle of 36°, when an electric field of a predetermined value or more was applied to the CLC cell, it was confirmed that deformation was completely formed in the liquid crystal and the reflectance was saturated to a constant level. As the intensity of the electric field increased further, the reflection band shifted to a longer wavelength and discontinuous wavelength shift due to the pitch jump was observed rather than a continuous wavelength increase. In addition, the reflection band changed when the angle of incidence on the CLC cell was changed. As the angle of incidence gradually increased, the center wavelength of the reflection band moved towards shorter wavelengths. In the future, we intend to develop a device for optical wavelength filters based on side-polished optical fibers. This is expected to have a potential application as a wavelength notch filter or a bandpass filter.


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