A. I. Allagulov, V. Chigrinov, S. Pikin, D. Wester
{"title":"铁电液晶在电场中的双稳性","authors":"A. I. Allagulov, V. Chigrinov, S. Pikin, D. Wester","doi":"10.1080/00150199308223446","DOIUrl":null,"url":null,"abstract":"Bistability in a ferroelectric smectic-C # liquid crystal (C #LC) is attained in an electric field exceeding a certain threshold value that pedents on the adhesion energy of the C #LC to the surface. The case of bistability where the equilibrium orientation angles do not coincide for the polar and dispersed components of the C #LC adhesion energy is examined separately. In this case the bistability is achieved with a twisted directrix for the C #LC","PeriodicalId":21932,"journal":{"name":"Soviet physics. Crystallography","volume":"40 1","pages":"870-872"},"PeriodicalIF":0.0000,"publicationDate":"1993-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":"{\"title\":\"Bistability of a ferroelectric liquid crystal in an electric field\",\"authors\":\"A. I. Allagulov, V. Chigrinov, S. Pikin, D. Wester\",\"doi\":\"10.1080/00150199308223446\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Bistability in a ferroelectric smectic-C # liquid crystal (C #LC) is attained in an electric field exceeding a certain threshold value that pedents on the adhesion energy of the C #LC to the surface. The case of bistability where the equilibrium orientation angles do not coincide for the polar and dispersed components of the C #LC adhesion energy is examined separately. In this case the bistability is achieved with a twisted directrix for the C #LC\",\"PeriodicalId\":21932,\"journal\":{\"name\":\"Soviet physics. Crystallography\",\"volume\":\"40 1\",\"pages\":\"870-872\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1993-03-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Soviet physics. Crystallography\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1080/00150199308223446\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Soviet physics. Crystallography","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1080/00150199308223446","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Bistability of a ferroelectric liquid crystal in an electric field
Bistability in a ferroelectric smectic-C # liquid crystal (C #LC) is attained in an electric field exceeding a certain threshold value that pedents on the adhesion energy of the C #LC to the surface. The case of bistability where the equilibrium orientation angles do not coincide for the polar and dispersed components of the C #LC adhesion energy is examined separately. In this case the bistability is achieved with a twisted directrix for the C #LC
京公网安备 11010802042870号
京ICP备2023020795号-1
分享
求助内容：
应助结果提醒方式：
扫码关注我们
