Higher–Order Bragg Reflection Colors in Polymer–Stabilized Cholesteric Liquid Crystals
The dynamic electro‐optic (EO) response of polymer‐stabilized cholesteric liquid crystals prepared using unpolarized UV light (U–PSCLC), such as reflection bandwidth broadening and either red or blue tuning of the reflection peak, has been previously reported. Herein, recent efforts to use a polariz...
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2021
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oai:doaj.org-article:3ca4ea3e88e2431d99504cb1538ca3fe2021-11-04T09:00:27ZHigher–Order Bragg Reflection Colors in Polymer–Stabilized Cholesteric Liquid Crystals2699-929310.1002/adpr.202100112https://doaj.org/article/3ca4ea3e88e2431d99504cb1538ca3fe2021-11-01T00:00:00Zhttps://doi.org/10.1002/adpr.202100112https://doaj.org/toc/2699-9293The dynamic electro‐optic (EO) response of polymer‐stabilized cholesteric liquid crystals prepared using unpolarized UV light (U–PSCLC), such as reflection bandwidth broadening and either red or blue tuning of the reflection peak, has been previously reported. Herein, recent efforts to use a polarized single argon‐ion laser beam to create PSCLCs (L–PSCLCs) with higher‐order reflections are described. The L–PSCLCs exhibit a primary reflection peak in the near‐infrared (NIR) regime and a second‐order reflection band with a narrow bandwidth in the visible regime that results from a deformed in‐plane CLC helical structure. The initial positions of the reflection bands are adjusted by the chiral dopant concentrations of the CLC mixture, and red, green, and blue reflection colors from the second‐order Bragg reflection are demonstrated. The primary and the second‐order reflection bands can be shifted to longer wavelengths by application of a DC electric field. The reflection efficiency of the higher‐order reflection notch increases with polymer concentration, which affects the degree of in‐plane deformation and fixation of the CLC helix. Modeling is used to further explain the formation of the higher‐order reflection bands of PSCLCs observed experimentally.Kyung Min LeeVictor Yu ReshetnyakMichael E. McConneyEcklin P. CrenshawTimothy J. BunningTimothy J. WhiteNicholas P. GodmanWiley-VCHarticlecholesteric liquid crystalsdeformed cholesteric helixhigher order Bragg reflectionspolymer stabilizationApplied optics. PhotonicsTA1501-1820Optics. LightQC350-467ENAdvanced Photonics Research, Vol 2, Iss 11, Pp n/a-n/a (2021) |
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cholesteric liquid crystals deformed cholesteric helix higher order Bragg reflections polymer stabilization Applied optics. Photonics TA1501-1820 Optics. Light QC350-467 |
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cholesteric liquid crystals deformed cholesteric helix higher order Bragg reflections polymer stabilization Applied optics. Photonics TA1501-1820 Optics. Light QC350-467 Kyung Min Lee Victor Yu Reshetnyak Michael E. McConney Ecklin P. Crenshaw Timothy J. Bunning Timothy J. White Nicholas P. Godman Higher–Order Bragg Reflection Colors in Polymer–Stabilized Cholesteric Liquid Crystals |
description |
The dynamic electro‐optic (EO) response of polymer‐stabilized cholesteric liquid crystals prepared using unpolarized UV light (U–PSCLC), such as reflection bandwidth broadening and either red or blue tuning of the reflection peak, has been previously reported. Herein, recent efforts to use a polarized single argon‐ion laser beam to create PSCLCs (L–PSCLCs) with higher‐order reflections are described. The L–PSCLCs exhibit a primary reflection peak in the near‐infrared (NIR) regime and a second‐order reflection band with a narrow bandwidth in the visible regime that results from a deformed in‐plane CLC helical structure. The initial positions of the reflection bands are adjusted by the chiral dopant concentrations of the CLC mixture, and red, green, and blue reflection colors from the second‐order Bragg reflection are demonstrated. The primary and the second‐order reflection bands can be shifted to longer wavelengths by application of a DC electric field. The reflection efficiency of the higher‐order reflection notch increases with polymer concentration, which affects the degree of in‐plane deformation and fixation of the CLC helix. Modeling is used to further explain the formation of the higher‐order reflection bands of PSCLCs observed experimentally. |
format |
article |
author |
Kyung Min Lee Victor Yu Reshetnyak Michael E. McConney Ecklin P. Crenshaw Timothy J. Bunning Timothy J. White Nicholas P. Godman |
author_facet |
Kyung Min Lee Victor Yu Reshetnyak Michael E. McConney Ecklin P. Crenshaw Timothy J. Bunning Timothy J. White Nicholas P. Godman |
author_sort |
Kyung Min Lee |
title |
Higher–Order Bragg Reflection Colors in Polymer–Stabilized Cholesteric Liquid Crystals |
title_short |
Higher–Order Bragg Reflection Colors in Polymer–Stabilized Cholesteric Liquid Crystals |
title_full |
Higher–Order Bragg Reflection Colors in Polymer–Stabilized Cholesteric Liquid Crystals |
title_fullStr |
Higher–Order Bragg Reflection Colors in Polymer–Stabilized Cholesteric Liquid Crystals |
title_full_unstemmed |
Higher–Order Bragg Reflection Colors in Polymer–Stabilized Cholesteric Liquid Crystals |
title_sort |
higher–order bragg reflection colors in polymer–stabilized cholesteric liquid crystals |
publisher |
Wiley-VCH |
publishDate |
2021 |
url |
https://doaj.org/article/3ca4ea3e88e2431d99504cb1538ca3fe |
work_keys_str_mv |
AT kyungminlee higherorderbraggreflectioncolorsinpolymerstabilizedcholestericliquidcrystals AT victoryureshetnyak higherorderbraggreflectioncolorsinpolymerstabilizedcholestericliquidcrystals AT michaelemcconney higherorderbraggreflectioncolorsinpolymerstabilizedcholestericliquidcrystals AT ecklinpcrenshaw higherorderbraggreflectioncolorsinpolymerstabilizedcholestericliquidcrystals AT timothyjbunning higherorderbraggreflectioncolorsinpolymerstabilizedcholestericliquidcrystals AT timothyjwhite higherorderbraggreflectioncolorsinpolymerstabilizedcholestericliquidcrystals AT nicholaspgodman higherorderbraggreflectioncolorsinpolymerstabilizedcholestericliquidcrystals |
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1718444953189744640 |