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dc.contributor.authorChang, Chia-Mingen_US
dc.contributor.authorLin, Yi-Hsinen_US
dc.contributor.authorReshetnyak, Victoren_US
dc.contributor.authorPark, Chui Hoen_US
dc.contributor.authorManda, Rameshen_US
dc.contributor.authorLee, Seung Heeen_US
dc.date.accessioned2019-04-03T06:43:41Z-
dc.date.available2019-04-03T06:43:41Z-
dc.date.issued2017-08-21en_US
dc.identifier.issn1094-4087en_US
dc.identifier.urihttp://dx.doi.org/10.1364/OE.25.019807en_US
dc.identifier.urihttp://hdl.handle.net/11536/146033-
dc.description.abstractPolymer-dispersed liquid crystals (PDLCs) modulate the amplitude and optical phase of light. The optical phase modulation of PDLC can be dissected into two parts: Kerr phase and orientational phase according to the electro-optical (EO) response. We investigated the origins of the Kerr and orientational phases in PDLCs and their connection with the two-step EO response. The Kerr phase is attributed to LC orientation in the center of LC droplets. The orientational phase results from orientation of LC molecules near LC-polymer interfaces. Both phases can be adjusted by varying the droplet size. The two-step EO response in small droplets (<333 nm) is related to the Kerr and orientational phases, and possibly to rotation of point defects. A modified PDLC model considering the Kerr and orientational phases is proposed. Our findings suggest the possibility of versatile photonic devices using pure optical phase modulation. (C) 2017 Optical Society of Americaen_US
dc.language.isoen_USen_US
dc.titleOrigins of Kerr phase and orientational phase in polymer-dispersed liquid crystalsen_US
dc.typeArticleen_US
dc.identifier.doi10.1364/OE.25.019807en_US
dc.identifier.journalOPTICS EXPRESSen_US
dc.citation.volume25en_US
dc.citation.issue17en_US
dc.citation.spage19807en_US
dc.citation.epage19821en_US
dc.contributor.department光電工程學系zh_TW
dc.contributor.departmentDepartment of Photonicsen_US
dc.identifier.wosnumberWOS:000409338000016en_US
dc.citation.woscount7en_US
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