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Localised polymer networks in chiral nematic liquid crystals for high speed photonic switching
Author(s) -
Chloe C. Tartan,
Patrick S. Salter,
Martin J. Booth,
Stephen Morris,
Steve J. Elston
Publication year - 2016
Publication title -
journal of applied physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.699
H-Index - 319
eISSN - 1089-7550
pISSN - 0021-8979
DOI - 10.1063/1.4948701
Subject(s) - liquid crystal , materials science , photonics , electric field , optoelectronics , optics , laser , polymer , biaxial nematic , phase (matter) , optical switch , helix (gastropod) , switching time , photonic crystal , physics , quantum mechanics , composite material , ecology , snail , biology
Self-assembled periodic structures based upon chiralliquid crystalline materials have significant potential in the field of photonics ranging from fast-switching optoelectronic devices to low-threshold lasers. The flexoelectro-optic effect, which is observed in chiralnematic liquid crystals (LCs) when an electric field is applied perpendicular to the helical axis, has significant potential as it exhibits analogue switching in 10–100 μs. However, the major technological barrier that prohibits the commercial realisation of this electro-opticeffect is the requirement of a uniform, in-plane alignment of the helix axis between glass substrates. Here, it is shown that periodic polymer structures engineered in the nematic phase of a chiral nematic LC device using direct laser writing can result in the spontaneous formation of the necessary uniform lying helix (ULH) state. Specifically, two-photon polymerization is used in conjunction with a spatial light modulator so as to correct for aberrations introduced by the bounding glass substrates enabling the polymer structures to be fabricated directly into the device. The ULH state appears to be stable in the absence of an externally applied electric field, and the optimum contrast between the bright and dark states is obtained using polymer structures that have periodicities of the order of the device thickness

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