{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"介绍一种测量液晶表面极向锚定强度的方法,通过同步测量线性偏振光经过混合排列的楔形液晶盒的相位及外加电压值,经过数值处理,得到表面极向锚定强度.使用混合排列液晶盒,简化了计算及测量步骤;使用楔形盒并用不同点的厚度差值代替厚度值计算,减小了由于厚度测量误差引起的干扰,提高了测量精度.","authors":[{"authorName":"刘绍锦","id":"70430e57-a9da-4786-8bee-c4d5e51deaec","originalAuthorName":"刘绍锦"},{"authorName":"宋玉龙","id":"9cd14809-393a-4e6c-b5e3-034d81c3faf6","originalAuthorName":"宋玉龙"},{"authorName":"张俊瑞","id":"c3e8d87d-dd3e-493c-9144-b92f5cccd299","originalAuthorName":"张俊瑞"},{"authorName":"崔宏青","id":"0ab5244e-5246-4c0d-9139-2743304c8add","originalAuthorName":"崔宏青"},{"authorName":"凌志华","id":"b2563656-2ff6-40b2-9f3a-676f0883a187","originalAuthorName":"凌志华"},{"authorName":"冯亚云","id":"e9ad56eb-8be4-4457-8f4c-feea10c4a315","originalAuthorName":"冯亚云"}],"doi":"10.3969/j.issn.1007-2780.2006.01.004","fpage":"15","id":"264be8db-6102-41be-9b1e-aa160fbfadcd","issue":"1","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"1bc043eb-71c4-47a6-b52e-8645544d9d36","keyword":"液晶","originalKeyword":"液晶"},{"id":"ec6f42ab-d398-4c9b-86f5-c4cc185d6fbd","keyword":"锚定强度","originalKeyword":"锚定强度"},{"id":"12ff78c1-a630-4fb3-ad76-204752809464","keyword":"混合排列盒","originalKeyword":"混合排列盒"}],"language":"zh","publisherId":"yjyxs200601004","title":"改进的极向锚定强度测量方法","volume":"21","year":"2006"},{"abstractinfo":"为了减小液晶波前校正器的响应时间,本文结合光控取向技术,研究了取向层预倾角及锚定强度特性对器件响应性能的影响.以液晶动力学方程为依据,分析预倾角效应对液晶器件响应时间的影响;利用预倾角及锚定强度与响应时间的定量关系,推导出锚定强度与预倾角的关系,从而简化了锚定强度的测量方法.采用光谱法监测了光控取向膜的取向度;以此为依据,利用4种不同曝光方式获得了不同的预倾角.理论模拟及实验结果一致表明:偶氮染料分子(SD1)获得一定的锚定强度后,通过降低其预倾角角度,其所制器件的响应性能实现了优化.","authors":[{"authorName":"陈云昌","id":"b33e8e65-b764-48a2-8cc2-45eeb9c6878d","originalAuthorName":"陈云昌"},{"authorName":"宣丽","id":"c071b10c-767b-4600-946e-996356da62b4","originalAuthorName":"宣丽"},{"authorName":"姚丽双","id":"bb309506-9d23-49d5-be50-2bd6582deef5","originalAuthorName":"姚丽双"},{"authorName":"彭增辉","id":"b1549338-7301-4453-a5e0-7f7f0502a8f4","originalAuthorName":"彭增辉"}],"doi":"10.3788/YJYXS20163101.0062","fpage":"62","id":"7a072adf-c1ea-4652-a363-9f02e1a93254","issue":"1","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"b7c465f1-23b7-43c0-8118-9f6f4ce76d75","keyword":"预倾角","originalKeyword":"预倾角"},{"id":"0d2a1c33-676c-4bce-ac79-3d00fa8a7633","keyword":"锚定强度","originalKeyword":"锚定强度"},{"id":"f490fc73-7bc7-48a6-8c40-8142bf48e5d1","keyword":"响应时间","originalKeyword":"响应时间"},{"id":"eaafcb2e-f514-4202-a151-8322d1b3287a","keyword":"光致取向液晶盒","originalKeyword":"光致取向液晶盒"}],"language":"zh","publisherId":"yjyxs201601006","title":"取向层参数对响应时间的影响","volume":"31","year":"2016"},{"abstractinfo":"通过测量高分子膜聚酰亚胺由排列记忆效应产生的锚定强度,对锚定强度随记忆时间的变化进行定量描述.聚酰亚胺膜表面的锚定强度随着记忆时间的增加逐渐增大,大约经过20h后达到饱和,其归一化饱和值大约为30μm-1.","authors":[{"authorName":"乌日娜","id":"16010824-4a99-46be-afb1-6823b40d2d7f","originalAuthorName":"乌日娜"},{"authorName":"于涛","id":"d5e157ea-4023-4d9c-978e-a09a6b5b8ea0","originalAuthorName":"于涛"},{"authorName":"彭增辉","id":"0c5776d8-5c37-4ade-a09e-c5837029a569","originalAuthorName":"彭增辉"},{"authorName":"张力","id":"02726614-ac5b-4c83-b634-5b1628b22cd5","originalAuthorName":"张力"},{"authorName":"阮圣平","id":"e60dae0a-0e22-4418-ace6-de7c7667ddfe","originalAuthorName":"阮圣平"},{"authorName":"宣丽","id":"63e2df76-229d-4f91-922f-c087797550a1","originalAuthorName":"宣丽"}],"doi":"10.3969/j.issn.1007-2780.2003.05.004","fpage":"338","id":"2dd2c928-396c-4ed7-8fef-721c45082c75","issue":"5","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"d7f9587b-ae58-40c2-b811-678007852451","keyword":"液晶","originalKeyword":"液晶"},{"id":"dfa145fe-26f2-4657-a8b0-897c4d1e4aa7","keyword":"排列记忆效应","originalKeyword":"排列记忆效应"},{"id":"1cbeb0c9-4d84-4e96-b69a-7bead412a9ee","keyword":"锚定强度","originalKeyword":"锚定强度"}],"language":"zh","publisherId":"yjyxs200305004","title":"液晶分子在高分子膜上的排列记忆效应","volume":"18","year":"2003"},{"abstractinfo":"根据液晶动力学理论研究了π型液晶盒中从展曲到弯曲的转变过程和转变所需的最小电压.在低电压驱动情况下,具有非对称预倾角度的展曲结构转变为非对称状态;在高于转变电压的脉冲作用下,再转变成为弯曲结构.结果表明,转变电压随着锚定强度的增加而增加,随着表面黏滞系数的增加而增加,随着预倾角度的增加而减小.使用本文提出的方法得到的转变时间比其他方法要快得多,可以小于50 ms.","authors":[{"authorName":"姜丽","id":"e9e8672d-6c28-422b-b5b2-fe941bb19ad8","originalAuthorName":"姜丽"},{"authorName":"孙玉宝","id":"2bb900c2-a6f4-4545-87e7-38a803cdaf85","originalAuthorName":"孙玉宝"},{"authorName":"马红梅","id":"274310a5-ab86-4a11-b94b-1b11c4ae63a8","originalAuthorName":"马红梅"},{"authorName":"张志东","id":"94b3fd31-b63d-4e77-ab7b-2f4581b2eed9","originalAuthorName":"张志东"}],"doi":"10.3969/j.issn.1007-2780.2007.05.016","fpage":"583","id":"3eadd396-9f6a-43dc-9192-e715ef0ad22c","issue":"5","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"38b13514-9d0f-4c67-86c7-f4435d5152d3","keyword":"液晶","originalKeyword":"液晶"},{"id":"70986272-8e4e-4117-8aed-e489fc3d7a28","keyword":"π型盒","originalKeyword":"π型盒"},{"id":"e3dd8ec9-4c19-4c42-9b9b-82949fbbfccd","keyword":"转变电压","originalKeyword":"转变电压"},{"id":"f07d5083-7402-4c36-aa21-44191ed9c31e","keyword":"锚定强度","originalKeyword":"锚定强度"},{"id":"f3a4a916-6268-41b5-99bb-75da1a6e2cf8","keyword":"表面黏滞系数","originalKeyword":"表面黏滞系数"},{"id":"e8d8ec8c-4956-4322-b18b-626429b75851","keyword":"预倾角度","originalKeyword":"预倾角度"}],"language":"zh","publisherId":"yjyxs200705016","title":"π盒的展曲到弯曲形变","volume":"22","year":"2007"},{"abstractinfo":"向列液晶界面锚定能被认为是液晶分子与固体界面上分子相互作用势之和,据此导出了锚定能的新公式,它包含两项,因而有两个强度参量,其中第二项是由于界面诱导双轴性而引起的,倾角锚定强度Aθ和方位角锚定强度定Aφ的差别可归因于此.用新的锚定能公式详细研究了弱锚定扭曲(超扭曲)向列液晶盒,假定Aθ/Aφ=k11/k12,计算了阈值场强和饱和场强的大小,与以前我们认为的Aθ/Aφ=1情况做了比较.结果表明,倾角锚定强度Aθ与方位角锚定强度Aφ的关系对扭曲(超扭曲)向列液晶盒的阈值场强和饱和场强都有影响.","authors":[{"authorName":"张书敬","id":"fb088e6c-88fe-4494-9d80-ff8578191270","originalAuthorName":"张书敬"},{"authorName":"包超恩","id":"ed5b2bcb-8456-4825-a462-96c829f71e71","originalAuthorName":"包超恩"},{"authorName":"杨国琛","id":"447c6738-444a-4268-b3f5-9cddb1f1364d","originalAuthorName":"杨国琛"}],"doi":"10.3969/j.issn.1007-2780.2004.05.007","fpage":"353","id":"99addb5d-bcb3-482c-91ab-3b46686721e3","issue":"5","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"922a2ff6-1bf6-40be-98d7-9187b9a45ee8","keyword":"液晶","originalKeyword":"液晶"},{"id":"51a856d2-9cc2-4ef4-a893-a1238ebab50a","keyword":"弱锚定","originalKeyword":"弱锚定"},{"id":"5449699f-163e-4842-b668-40b5b6176864","keyword":"两参数锚定能公式","originalKeyword":"两参数锚定能公式"},{"id":"aa2efbcb-d6e5-49af-b6f6-7ddeb01d26dd","keyword":"极角锚定能","originalKeyword":"极角锚定能"},{"id":"b40f8bde-a40a-4366-a77b-4516000ab0fc","keyword":"方位角锚定能","originalKeyword":"方位角锚定能"}],"language":"zh","publisherId":"yjyxs200405007","title":"界面锚定能和扭曲向列液晶盒","volume":"19","year":"2004"},{"abstractinfo":"利用摩擦和光控取向技术在基板上分别做成聚酰亚胺(PI)取向膜.由Cano盒测试方位锚定能的原理,测试了在不同温度下摩擦处理的膜和光控取向膜方位锚定能的变化,发现光控取向膜的方位锚定能随温度变化较为敏感,但主要问题还是锚定强度弱,讨论了改善光控取向膜锚定强度的方法.","authors":[{"authorName":"于涛","id":"44344ff0-4b0c-46e6-b1d6-c3024f713da2","originalAuthorName":"于涛"},{"authorName":"彭增辉","id":"b252dbeb-af33-4636-b584-e41ef5b53feb","originalAuthorName":"彭增辉"},{"authorName":"乌日娜","id":"c94a4422-5b39-4c9a-9d41-1fd3cfa76ea0","originalAuthorName":"乌日娜"},{"authorName":"胡明","id":"460cd7e9-a094-4856-9299-847626116d08","originalAuthorName":"胡明"},{"authorName":"鲁兴海","id":"ade3ac9f-8046-4edf-a20c-e98d6ed14e3d","originalAuthorName":"鲁兴海"},{"authorName":"阮圣平","id":"2f587fe9-e03b-461d-8d90-b4bcf0501aaf","originalAuthorName":"阮圣平"},{"authorName":"宣丽","id":"0acbcef8-9663-4896-ace0-cac31b4a5cc1","originalAuthorName":"宣丽"}],"doi":"10.3969/j.issn.1007-2780.2003.01.002","fpage":"7","id":"c19f0392-6169-462b-ba27-1702a12774db","issue":"1","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"2f29ce99-37b8-4a58-812d-a02c1f7a3aa1","keyword":"液晶","originalKeyword":"液晶"},{"id":"986d6f6a-f53e-429a-90ba-475706685a6f","keyword":"光控取向","originalKeyword":"光控取向"},{"id":"14796dfe-f69e-434d-adbc-b81a755f679a","keyword":"方位锚定能","originalKeyword":"方位锚定能"}],"language":"zh","publisherId":"yjyxs200301002","title":"光控PI取向膜方位锚定能的温度特性","volume":"18","year":"2003"},{"abstractinfo":"提出了纳米结构聚合物表面的一个简化模型:由具有交替的沿面和垂面锚定的一维周期性条纹表面表征.利用Alexe-Ionescu等提出的扩展各向异性表面能形式,研究了向列相和取向层聚合物之间的锚定以及聚合物和基板表面之间的锚定对向列相液晶表面锚定的影响.在理论处理中,假设两不同锚定区域的锚定强度相等.结果表明:聚合物和基板表面之间的锚定会影响向列相的指向矢分布,降低松弛距离以及系统的总自由能.","authors":[{"authorName":"周璇","id":"e062b09a-c387-4f00-aba3-5cfab1776b64","originalAuthorName":"周璇"},{"authorName":"宋静静","id":"b3d56c11-b9a4-46c9-a5f6-461d7fb7cb7c","originalAuthorName":"宋静静"},{"authorName":"张志东","id":"c56e5305-536f-4df4-b614-4dea58e1486d","originalAuthorName":"张志东"}],"doi":"10.3788/YJYXS20122704.0425","fpage":"425","id":"bbf60bd5-e0dd-41dd-9897-bd74c5462828","issue":"4","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"3037252f-e148-43a7-9a2b-80737ba3dd32","keyword":"纳米结构表面","originalKeyword":"纳米结构表面"},{"id":"b3ea8881-ff35-46a4-89df-b0568c15042a","keyword":"表面锚定","originalKeyword":"表面锚定"},{"id":"d2dc3e1e-c1f5-472c-b876-224a1e06a49e","keyword":"指向矢分布","originalKeyword":"指向矢分布"},{"id":"ed6b51c2-15bf-4797-8f8a-b9ee2d7f5666","keyword":"预倾角","originalKeyword":"预倾角"}],"language":"zh","publisherId":"yjyxs201204001","title":"纳米结构表面向列相液晶的聚合物锚定效应","volume":"27","year":"2012"},{"abstractinfo":"研究了弱锚定条件下混合排列向列液晶显示的动态响应.具体研究沿面排列处为弱锚定,垂面排列处为强锚定的HAN盒.通过计算液晶盒中的瞬时指向矢分布,得到了透射光强随时间的变化.讨论了响应速度与锚定强度系数之间的关系.","authors":[{"authorName":"张志东","id":"4e5fbc27-1ba4-4c72-aea7-3f13af3cb836","originalAuthorName":"张志东"},{"authorName":"于广","id":"10447ecc-1533-4ae1-88c3-cdb13291e426","originalAuthorName":"于广"},{"authorName":"张德贤","id":"e59e93af-4ce7-4913-8cfc-c9ee1481c482","originalAuthorName":"张德贤"}],"doi":"10.3969/j.issn.1007-2780.1999.01.002","fpage":"6","id":"51345a1c-c47d-492c-abbe-e9231095f01f","issue":"1","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"063882b8-6447-4bd8-b332-d08b76f02ac0","keyword":"混合排列","originalKeyword":"混合排列"},{"id":"fba28c85-2aeb-440e-a00c-8f1b3efd14eb","keyword":"液晶显示","originalKeyword":"液晶显示"},{"id":"3b895eed-8132-434f-9624-a7f35b54694f","keyword":"弱锚定","originalKeyword":"弱锚定"},{"id":"b8bba474-8873-4eb7-a2fd-d9b4ccf86794","keyword":"动态响应","originalKeyword":"动态响应"}],"language":"zh","publisherId":"yjyxs199901002","title":"弱锚定条件下混合排列向列液晶显示的动态响应","volume":"14","year":"1999"},{"abstractinfo":"用解析方法研究了上、下基板锚定强度不同的弱锚定沿面排列向列液晶盒(不对称液晶盒),给出了指向矢倾角θ满足的方程和边界条件,讨论了它的解,导出Freedericksz转变的阈值场强和饱和场强.研究了由于上、下基板锚定强度不同而引起的对称性破缺,以及对称破缺和磁场强度之间的关系,发现了不对称液晶盒一些特殊的现象.作为应用的例子,讨论了一种测定基板锚定强度的新方法.","authors":[{"authorName":"张志国","id":"71580125-f419-4352-a944-165f530916ac","originalAuthorName":"张志国"},{"authorName":"李丽","id":"c6995c82-530a-406c-b929-9413b72b925a","originalAuthorName":"李丽"},{"authorName":"杨国琛","id":"867564f3-6b95-4cce-b22d-8679315792d9","originalAuthorName":"杨国琛"}],"doi":"10.3969/j.issn.1007-2780.2003.03.012","fpage":"205","id":"e76babbd-ecf8-4ffb-992c-57a370db5c4b","issue":"3","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"02544907-7eae-44ce-b072-73670e22cd86","keyword":"液晶盒","originalKeyword":"液晶盒"},{"id":"ea56b3b8-8260-4421-b038-1c256a7e90a4","keyword":"弱锚定","originalKeyword":"弱锚定"},{"id":"fe1a3613-ce27-48af-abd6-119b19fa4470","keyword":"阈值磁场","originalKeyword":"阈值磁场"},{"id":"efbee0e6-8b9c-477b-8e9c-b81b0e68bc81","keyword":"饱和磁场","originalKeyword":"饱和磁场"},{"id":"00a0e0d3-af07-481a-b82f-bc42668cca83","keyword":"对称破缺","originalKeyword":"对称破缺"}],"language":"zh","publisherId":"yjyxs200303012","title":"不对称弱锚定沿面排列向列液晶盒的研究","volume":"18","year":"2003"},{"abstractinfo":"基板的锚定特性,包括锚定能大小和锚定易取方向,影响液晶指向矢的分布,直接导致液晶盒电容的改变,因此可以通过液晶盒电容的测量确定基板表面的锚定特性.基于液晶弹性理论和变分原理,理论推导弱锚定平行排列向列相和混合排列向列相液晶盒系统的平衡态方程和边界条件,采用差分迭代方法数值模拟得到了液晶盒约化电容随电压、锚定能系数及锚定易取方向变化的曲线.结果表明:液晶盒电容随基板锚定能系数的增加而减小;随预倾角的增加,液晶盒电容随锚定能系数的变化缩小;同一电压和基板锚定能系数下,平行排列向列相液晶盒电容不会大于混合排列向列相液晶的电容.","authors":[{"authorName":"叶文江","id":"c5524643-f35a-4240-a3c8-2a6fca012579","originalAuthorName":"叶文江"},{"authorName":"刘小松","id":"483f31c0-4205-4847-b2ae-a70f1a941b3b","originalAuthorName":"刘小松"},{"authorName":"宋晓龙","id":"1a4a3baf-50a5-4c3f-8235-eee482071107","originalAuthorName":"宋晓龙"},{"authorName":"郑桂丽","id":"e9800f9e-f6c6-4cd8-b739-a7ad2dfabb8d","originalAuthorName":"郑桂丽"}],"doi":"10.3788/YJYXS20142905.0686","fpage":"686","id":"cb464748-1935-4a6d-90f2-378683729dcc","issue":"5","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"b03ec6ef-82ac-467e-b8a7-d448237eead7","keyword":"液晶盒电容","originalKeyword":"液晶盒电容"},{"id":"d5c7a180-ec1b-4d30-a696-80c60ae1251a","keyword":"锚定能","originalKeyword":"锚定能"},{"id":"4dda8094-b1a6-4267-b1be-122dcede80d3","keyword":"易取方向","originalKeyword":"易取方向"},{"id":"0639fa16-e6b0-4da7-8879-733861b79e67","keyword":"弱锚定","originalKeyword":"弱锚定"},{"id":"6c137b59-e428-42bd-948f-649c8df9dad0","keyword":"差分迭代方法","originalKeyword":"差分迭代方法"}],"language":"zh","publisherId":"yjyxs201405007","title":"基板锚定特性对液晶盒电容的影响","volume":"29","year":"2014"}],"totalpage":3098,"totalrecord":30979}