TY - JOUR
T1 - Memorizable Electro-Birefringence Effect Exhibited by Transparent Liquid Crystal/Polymer Composite Materials
AU - Yamaguchi, Masaki
AU - Okumura, Yasushi
AU - Nishikawa, Hiroya
AU - Matsukizono, Hiroyuki
AU - Kikuchi, Hirotsugu
N1 - Publisher Copyright:
© 2024 The Authors. Advanced Electronic Materials published by Wiley-VCH GmbH.
PY - 2024/9
Y1 - 2024/9
N2 - Polymer-dispersed liquid crystals (PDLCs) with nano-phase-separated structures, in which nanometer-sized liquid crystal (LC) domains are dispersed within a polymer matrix (nano-PDLCs), are transparent solid materials whose optical properties can be modulated by applying an electric field (E-field). Because the proportion of LC that can respond to an electric field is small, the specific surface area of the phase-separated interface of nano-PDLCs is larger than that of conventional PDLCs, resulting in higher drive voltages than those of conventional PDLCs. To lower the driving voltage of nano-PDLCs, highly polar LCs (C3DIO) are used with a large dielectric anisotropy (>10000), and prepared nano-PDLCs using DIO mixtures obtained by mixing them with related compounds as the host LC. Nano-PDLCs employing DIO mixtures exhibit higher E-field responsivity than those using conventional LC. In addition, the electro-optical Kerr coefficient at visible wavelength is significantly high, reaching 10−8 m V−2. Furthermore, nano-PDLCs using the DIO mixture exhibit a memory effect in which the induced birefringence remains even after the removal of the in-plane E-field. Memorized birefringence can be erased by heating or applying an E-field perpendicular to the substrate surface. Nano-PDLCs using a DIO mixture can be rewritable electro-birefringence-responsive materials that can memorize arbitrary birefringence values.
AB - Polymer-dispersed liquid crystals (PDLCs) with nano-phase-separated structures, in which nanometer-sized liquid crystal (LC) domains are dispersed within a polymer matrix (nano-PDLCs), are transparent solid materials whose optical properties can be modulated by applying an electric field (E-field). Because the proportion of LC that can respond to an electric field is small, the specific surface area of the phase-separated interface of nano-PDLCs is larger than that of conventional PDLCs, resulting in higher drive voltages than those of conventional PDLCs. To lower the driving voltage of nano-PDLCs, highly polar LCs (C3DIO) are used with a large dielectric anisotropy (>10000), and prepared nano-PDLCs using DIO mixtures obtained by mixing them with related compounds as the host LC. Nano-PDLCs employing DIO mixtures exhibit higher E-field responsivity than those using conventional LC. In addition, the electro-optical Kerr coefficient at visible wavelength is significantly high, reaching 10−8 m V−2. Furthermore, nano-PDLCs using the DIO mixture exhibit a memory effect in which the induced birefringence remains even after the removal of the in-plane E-field. Memorized birefringence can be erased by heating or applying an E-field perpendicular to the substrate surface. Nano-PDLCs using a DIO mixture can be rewritable electro-birefringence-responsive materials that can memorize arbitrary birefringence values.
KW - electro-birefringence effect
KW - ferroelectric nematic liquid crystal
KW - memory effect
KW - polymer dispersed liquid crystal
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U2 - 10.1002/aelm.202400055
DO - 10.1002/aelm.202400055
M3 - Article
AN - SCOPUS:85192574525
SN - 2199-160X
VL - 10
JO - Advanced Electronic Materials
JF - Advanced Electronic Materials
IS - 9
M1 - 2400055
ER -