Liquid crystal chiroptical polarization rotators for the near-UV region: theory, materials, and device applications

Author(s):  
D. Saulnier ◽  
B. Taylor ◽  
K. L. Marshall ◽  
T. J. Kessler ◽  
S. D. Jacobs
1991 ◽  
Author(s):  
Neil Collings ◽  
Wei Xue ◽  
Giancarlo Pedrini

2015 ◽  
Vol 15 (10) ◽  
pp. 7711-7716 ◽  
Author(s):  
Dong Hun Lee ◽  
Myung-Hyun Lee

We propose a gapped surface plasmon polariton waveguide (G-SPPW) device based on a liquid crystal (LC) at a wavelength of 1.55 μm. The G-SPPW device is composed of an input 2.0-μm-wide and 5.0-μm-long insulator-metal-insulator waveguide (IMI-W), an 8-μm-long gap, and an output 2.0-μm-wide and 25.0-μm-long IMI-W. The LC is used for the gap and the 5.15-μm-thick upper and lower dielectric layers. The input surface plasmon polaritons (SPPs) propagate and jump over the gap in the G-SPPW with a coupling loss of less than ∼0.68 dB. The propagation and coupling losses of the 38-μm-long G-SPPW device are varied in the range of ∼0.5268 dB to ∼2.6716 dB and ∼0.1446 dB to ∼0.6784 dB, respectively, with LC tilt angles (1, 2) = 0° ∼ 90° at a fixed 90° twist angle. The normalized transmission of the G-SPPW device is also varied in the range from −3.351 dB to −0.6714 dB with 1, 2 = 0° ∼ 90° at a fixed 90° twist angle. The output SPP characteristics of the G-SPPW device can be properly controlled by the orientation of the LC molecules. The proposed G-SPPW device shows potential for new active plasmonic device applications.


2017 ◽  
Author(s):  
Kenneth L. Marshall ◽  
Debra J. Saulnier ◽  
Tanya Z. Kosc ◽  
Oleg Didovets ◽  
Shaw-Horng Chen

2011 ◽  
Vol 19 (8) ◽  
pp. 7553 ◽  
Author(s):  
Yuan-Di Chen ◽  
Ko-Ting Cheng ◽  
Cheng-Kai Liu ◽  
Andy Ying-Guey Fuh

2008 ◽  
Vol 10 (5) ◽  
pp. 055301 ◽  
Author(s):  
V Tkachenko ◽  
A A Dyomin ◽  
G V Tkachenko ◽  
G Abbate ◽  
I A Sukhoivanov

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