2019
DOI: 10.3390/cryst9060314
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Electro-Optical Switching of Dual-Frequency Nematic Liquid Crystals: Regimes of Thin and Thick Cells

Abstract: Conventional display applications of liquid crystals utilize thin layers of mesogenic materials, typically less than 10 µm. However, emerging non-display applications will require thicker, i.e., greater than 100 µm, layers of liquid crystals. Although electro-optical performance of relatively thin liquid crystal cells is well-documented, little is known about the properties of thicker liquid crystal layers. In this paper, the electro-optical response of dual-frequency nematic liquid crystals is studied using a… Show more

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Cited by 21 publications
(12 citation statements)
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“…Unless otherwise specified, we will be using the parameters appropriate for the commercially available MLC‐2048 (Merck Ltd), a dual‐frequency nematic LC, which is well studied in the literature. [ 42–44 ] The Frank elastic constants are K 11 = 12.4 pN and K 33 = 24.7 pN; [ 45 ] we take a pretilt angle of 0.04 rad and an anchoring strength of W = 2 × 10 −4 J m −2 . [ 12 ] We found the wavelength‐dependent refractive indices using the Cauchy coefficients: A e = 1.6950, B e = −0.0015 µm 2 , C e = 0.0035 µm 4 , A o = 1.5200, B o = −0.0212 µm 2 , and C o = 0.0044 µm 4 , with a biasing voltage frequency of 1 kHz.…”
Section: Resultsmentioning
confidence: 99%
“…Unless otherwise specified, we will be using the parameters appropriate for the commercially available MLC‐2048 (Merck Ltd), a dual‐frequency nematic LC, which is well studied in the literature. [ 42–44 ] The Frank elastic constants are K 11 = 12.4 pN and K 33 = 24.7 pN; [ 45 ] we take a pretilt angle of 0.04 rad and an anchoring strength of W = 2 × 10 −4 J m −2 . [ 12 ] We found the wavelength‐dependent refractive indices using the Cauchy coefficients: A e = 1.6950, B e = −0.0015 µm 2 , C e = 0.0035 µm 4 , A o = 1.5200, B o = −0.0212 µm 2 , and C o = 0.0044 µm 4 , with a biasing voltage frequency of 1 kHz.…”
Section: Resultsmentioning
confidence: 99%
“…Different solutions have been proposed to overcome this limitation, although none of them has been successfully implemented in mm-wave. For instance, by using dual frequency LCs, the LC molecules can be actively forced to rotate in both directions depending on the bias frequency, which allows controlling the relaxation times through the applied electric field [19]. Alternatively, polymer network LC (PNLC) mixtures achieve better time response, which is the focus of this work.…”
Section: Introductionmentioning
confidence: 99%
“…When a nematic material with positive dielectric anisotropy is placed in an electric field exceeding a certain threshold, its molecules tend to assume a homeotropic alignment (parallel to the direction of the electric field and perpendicular to the cell surface). If the dielectric anisotropy is negative, the dominant orientation of the molecules is perpendicular to the direction of the electric field [ 9 , 10 , 11 ]. A correlation between the dielectric anisotropy and the molecular structure was described in detail by the theory of Maier and Meier [ 9 , 10 , 12 ].…”
Section: Introductionmentioning
confidence: 99%