Homeotropic reverse-mode polymer-liquid crystal device
We have proposed a new type of reverse-mode polymer-liquid crystal device: homeotropic reverse-mode polymer-liquid crystal (HRPLC). This device consists of a liquid crystal with a dielectric constant having negative anisotropy and a pair of glass plates covered with a homeotropic alignment layer. Th...
Gespeichert in:
Veröffentlicht in: | Journal of applied physics 1997-02, Vol.81 (4), p.1962-1965 |
---|---|
Hauptverfasser: | , , , |
Format: | Artikel |
Sprache: | eng |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 1965 |
---|---|
container_issue | 4 |
container_start_page | 1962 |
container_title | Journal of applied physics |
container_volume | 81 |
creator | Murai, Hideya Gotoh, Tomohisa Nakata, Taisaku Hasegawa, Etsuo |
description | We have proposed a new type of reverse-mode polymer-liquid crystal device: homeotropic reverse-mode polymer-liquid crystal (HRPLC). This device consists of a liquid crystal with a dielectric constant having negative anisotropy and a pair of glass plates covered with a homeotropic alignment layer. The HRPLC’s operation is the reverse of the usual; i.e., it is clear when no voltage is applied and opaque under applied voltage. We have confirmed that the HRPLC operates well in reverse mode and have studied the dependence of its properties on liquid crystal material, curing process, and cell thickness. Experimental results indicate the HRPLC has a 30:1 contrast ratio over an operating voltage range of 0–11 V. In special fabrication conditions, the transmittance–voltage curve of the HRPLC drops to a minimum at a certain voltage level and begins to increase at that point. We have proposed a model to explain this result. |
doi_str_mv | 10.1063/1.364052 |
format | Article |
fullrecord | <record><control><sourceid>crossref</sourceid><recordid>TN_cdi_crossref_primary_10_1063_1_364052</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>10_1063_1_364052</sourcerecordid><originalsourceid>FETCH-LOGICAL-c291t-7c315d63c696dd2b847dd69621e909378f94fa43545c565c18ceb9bfb7b6084a3</originalsourceid><addsrcrecordid>eNotj01LxDAUAIMoWFfBn9Cjl6zv5TtHWdRdWPCi59Imr1BpSU3qQv-9ynqaOQ0MY_cIWwQjH3ErjQItLliF4Dy3WsMlqwAEcuetv2Y3pXwCIDrpK2b2aaK05DQPoc50olyITylSPadxnSjzcfj6HmId8lqWdqwjnYZAt-yqb8dCd__csI-X5_fdnh_fXg-7pyMPwuPCbZCoo5HBeBOj6JyyMf66QPLgpXW9V32rpFY6aKMDukCd7_rOdgacauWGPZy7IadSMvXNnIepzWuD0Pz9Nticf-UPfC9HNw</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Homeotropic reverse-mode polymer-liquid crystal device</title><source>AIP Digital Archive</source><creator>Murai, Hideya ; Gotoh, Tomohisa ; Nakata, Taisaku ; Hasegawa, Etsuo</creator><creatorcontrib>Murai, Hideya ; Gotoh, Tomohisa ; Nakata, Taisaku ; Hasegawa, Etsuo</creatorcontrib><description>We have proposed a new type of reverse-mode polymer-liquid crystal device: homeotropic reverse-mode polymer-liquid crystal (HRPLC). This device consists of a liquid crystal with a dielectric constant having negative anisotropy and a pair of glass plates covered with a homeotropic alignment layer. The HRPLC’s operation is the reverse of the usual; i.e., it is clear when no voltage is applied and opaque under applied voltage. We have confirmed that the HRPLC operates well in reverse mode and have studied the dependence of its properties on liquid crystal material, curing process, and cell thickness. Experimental results indicate the HRPLC has a 30:1 contrast ratio over an operating voltage range of 0–11 V. In special fabrication conditions, the transmittance–voltage curve of the HRPLC drops to a minimum at a certain voltage level and begins to increase at that point. We have proposed a model to explain this result.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.364052</identifier><language>eng</language><ispartof>Journal of applied physics, 1997-02, Vol.81 (4), p.1962-1965</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c291t-7c315d63c696dd2b847dd69621e909378f94fa43545c565c18ceb9bfb7b6084a3</citedby><cites>FETCH-LOGICAL-c291t-7c315d63c696dd2b847dd69621e909378f94fa43545c565c18ceb9bfb7b6084a3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,778,782,27907,27908</link.rule.ids></links><search><creatorcontrib>Murai, Hideya</creatorcontrib><creatorcontrib>Gotoh, Tomohisa</creatorcontrib><creatorcontrib>Nakata, Taisaku</creatorcontrib><creatorcontrib>Hasegawa, Etsuo</creatorcontrib><title>Homeotropic reverse-mode polymer-liquid crystal device</title><title>Journal of applied physics</title><description>We have proposed a new type of reverse-mode polymer-liquid crystal device: homeotropic reverse-mode polymer-liquid crystal (HRPLC). This device consists of a liquid crystal with a dielectric constant having negative anisotropy and a pair of glass plates covered with a homeotropic alignment layer. The HRPLC’s operation is the reverse of the usual; i.e., it is clear when no voltage is applied and opaque under applied voltage. We have confirmed that the HRPLC operates well in reverse mode and have studied the dependence of its properties on liquid crystal material, curing process, and cell thickness. Experimental results indicate the HRPLC has a 30:1 contrast ratio over an operating voltage range of 0–11 V. In special fabrication conditions, the transmittance–voltage curve of the HRPLC drops to a minimum at a certain voltage level and begins to increase at that point. We have proposed a model to explain this result.</description><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1997</creationdate><recordtype>article</recordtype><recordid>eNotj01LxDAUAIMoWFfBn9Cjl6zv5TtHWdRdWPCi59Imr1BpSU3qQv-9ynqaOQ0MY_cIWwQjH3ErjQItLliF4Dy3WsMlqwAEcuetv2Y3pXwCIDrpK2b2aaK05DQPoc50olyITylSPadxnSjzcfj6HmId8lqWdqwjnYZAt-yqb8dCd__csI-X5_fdnh_fXg-7pyMPwuPCbZCoo5HBeBOj6JyyMf66QPLgpXW9V32rpFY6aKMDukCd7_rOdgacauWGPZy7IadSMvXNnIepzWuD0Pz9Nticf-UPfC9HNw</recordid><startdate>19970215</startdate><enddate>19970215</enddate><creator>Murai, Hideya</creator><creator>Gotoh, Tomohisa</creator><creator>Nakata, Taisaku</creator><creator>Hasegawa, Etsuo</creator><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19970215</creationdate><title>Homeotropic reverse-mode polymer-liquid crystal device</title><author>Murai, Hideya ; Gotoh, Tomohisa ; Nakata, Taisaku ; Hasegawa, Etsuo</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c291t-7c315d63c696dd2b847dd69621e909378f94fa43545c565c18ceb9bfb7b6084a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1997</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Murai, Hideya</creatorcontrib><creatorcontrib>Gotoh, Tomohisa</creatorcontrib><creatorcontrib>Nakata, Taisaku</creatorcontrib><creatorcontrib>Hasegawa, Etsuo</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Murai, Hideya</au><au>Gotoh, Tomohisa</au><au>Nakata, Taisaku</au><au>Hasegawa, Etsuo</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Homeotropic reverse-mode polymer-liquid crystal device</atitle><jtitle>Journal of applied physics</jtitle><date>1997-02-15</date><risdate>1997</risdate><volume>81</volume><issue>4</issue><spage>1962</spage><epage>1965</epage><pages>1962-1965</pages><issn>0021-8979</issn><eissn>1089-7550</eissn><abstract>We have proposed a new type of reverse-mode polymer-liquid crystal device: homeotropic reverse-mode polymer-liquid crystal (HRPLC). This device consists of a liquid crystal with a dielectric constant having negative anisotropy and a pair of glass plates covered with a homeotropic alignment layer. The HRPLC’s operation is the reverse of the usual; i.e., it is clear when no voltage is applied and opaque under applied voltage. We have confirmed that the HRPLC operates well in reverse mode and have studied the dependence of its properties on liquid crystal material, curing process, and cell thickness. Experimental results indicate the HRPLC has a 30:1 contrast ratio over an operating voltage range of 0–11 V. In special fabrication conditions, the transmittance–voltage curve of the HRPLC drops to a minimum at a certain voltage level and begins to increase at that point. We have proposed a model to explain this result.</abstract><doi>10.1063/1.364052</doi><tpages>4</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0021-8979 |
ispartof | Journal of applied physics, 1997-02, Vol.81 (4), p.1962-1965 |
issn | 0021-8979 1089-7550 |
language | eng |
recordid | cdi_crossref_primary_10_1063_1_364052 |
source | AIP Digital Archive |
title | Homeotropic reverse-mode polymer-liquid crystal device |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-16T20%3A44%3A55IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-crossref&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Homeotropic%20reverse-mode%20polymer-liquid%20crystal%20device&rft.jtitle=Journal%20of%20applied%20physics&rft.au=Murai,%20Hideya&rft.date=1997-02-15&rft.volume=81&rft.issue=4&rft.spage=1962&rft.epage=1965&rft.pages=1962-1965&rft.issn=0021-8979&rft.eissn=1089-7550&rft_id=info:doi/10.1063/1.364052&rft_dat=%3Ccrossref%3E10_1063_1_364052%3C/crossref%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true |