{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"简要介绍、 反液晶的发现、 发展、 显示应用中遇到的问题以及近来发展起来的无阈值液晶的研究结果。 最后讨论无阈值液晶应用前景。","authors":[{"authorName":"黄锡珉","id":"95b0ddb3-bc67-4b25-9ad3-e9d01299472b","originalAuthorName":"黄锡珉"}],"doi":"10.3969/j.issn.1007-2780.2001.02.001","fpage":"81","id":"97d7aa1d-e6df-4c63-9100-df5ee8159d4c","issue":"2","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"8ad1d6ba-3bf4-4ff7-a7cc-aef93e19f54e","keyword":"无阈值","originalKeyword":"无阈值"},{"id":"81c31550-af11-4ebf-9a56-e34e4e7b8221","keyword":"液晶","originalKeyword":"铁电液晶"},{"id":"33c36f4f-3168-4c4b-a90c-405f2351c0fa","keyword":"聚合物网络","originalKeyword":"聚合物网络"}],"language":"zh","publisherId":"yjyxs200102001","title":"无阈值液晶","volume":"16","year":"2001"},{"abstractinfo":"建立了液晶SmC*相介特性的分子理论,求出在外加交变电场作用下液晶系统的自由能密度,得到极化强度〈P-〉和复介电常数ε*的近似表达式.结果表明ε*是外加交变电场的角频率、幅值、温度以及液晶的分子结构参数的函数.","authors":[{"authorName":"钱祥忠","id":"9b159688-0d37-4870-8dd3-102a0581264a","originalAuthorName":"钱祥忠"}],"doi":"10.3969/j.issn.1007-2780.2000.02.002","fpage":"85","id":"2f817e68-0a39-4a32-93ba-2695f6c4142a","issue":"2","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"a5acaba3-aa36-40fc-a505-8a8608b8238a","keyword":"复介电常数","originalKeyword":"复介电常数"},{"id":"b5848b1e-7a49-44ed-b942-8299b78bc9a0","keyword":"角频率","originalKeyword":"角频率"},{"id":"cc6b9f13-4aed-45b5-b53c-87dbbd1ed6b9","keyword":"液晶","originalKeyword":"铁电液晶"},{"id":"1e4bb51f-13f4-48fe-b512-3ec6ca313337","keyword":"极化强度","originalKeyword":"极化强度"}],"language":"zh","publisherId":"yjyxs200002002","title":"液晶SmC*相介特性的研究","volume":"15","year":"2000"},{"abstractinfo":"将液晶分子的结构分为分子核、非手性尾和手性尾来讨论这些结构的变化对液晶的相行为和铁电性能的影响,以期对液晶的分子结构和其性能的关系有更深的认识.文章首先讨论分子核结构对液晶性能的影响.","authors":[{"authorName":"郑远洋","id":"d80ea060-9082-43d3-b4a2-eae1887f6e46","originalAuthorName":"郑远洋"},{"authorName":"唐岳","id":"0220dde9-4b3d-4147-a0ef-7c30a47801ca","originalAuthorName":"唐岳"},{"authorName":"侯君","id":"9a716060-1a13-449b-921e-0c7fe60f9c31","originalAuthorName":"侯君"},{"authorName":"宋晓凤","id":"105f37f7-0f3f-4543-b26f-512ce78ec766","originalAuthorName":"宋晓凤"}],"doi":"10.3969/j.issn.1007-2780.2005.06.011","fpage":"516","id":"546b0569-ec1f-4228-a891-4020abbac5b5","issue":"6","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"b3aeab63-29bf-4f4b-81f8-315819241688","keyword":"液晶","originalKeyword":"铁电液晶"},{"id":"570d2327-3d55-4424-adfa-512d5c746694","keyword":"分子核","originalKeyword":"分子核"},{"id":"bdedfb14-b7a7-4dec-8391-bff72f3a9502","keyword":"铁电性能","originalKeyword":"铁电性能"},{"id":"b87b28e7-3482-436d-a60d-80f32f918c43","keyword":"相行为","originalKeyword":"相行为"}],"language":"zh","publisherId":"yjyxs200506011","title":"液晶的分子结构与性能评述:(Ⅰ)分子核对液晶性能的影响","volume":"20","year":"2005"},{"abstractinfo":"将分子自组装单层膜技术应用于液晶取向,结合传统摩擦技术制备了非对称取向的液晶器件.采用在液晶相变过程中不施加电场的简易制备方法,获得了液晶的均一排列.且对比实验表明,自组装膜末端基团极性越大,器件对比度越高.通过分子模拟和排列机理分析认为自组装膜极性端基的引入,基板附近处液晶分子偶极和自组装膜端基基团相互作用,导致自组装取向层和摩擦取向层表面处液晶分子的偶极指向一致性,通过器件表面-内部液晶分子排列的诱导作用,从而实现了液晶器件的单畴无缺陷排列.","authors":[{"authorName":"姚丽双","id":"98469ff1-9101-4819-92f6-f3028db5c1f8","originalAuthorName":"姚丽双"},{"authorName":"彭增辉","id":"f1c8b708-a90b-4b69-9c80-61f63f22226c","originalAuthorName":"彭增辉"},{"authorName":"刘永刚","id":"e0a59e43-33e6-461c-b14c-990da5b4a023","originalAuthorName":"刘永刚"},{"authorName":"宣丽","id":"f8e0eb86-13aa-4fd3-bcaf-bdc44271edf6","originalAuthorName":"宣丽"}],"doi":"10.3788/YJYXS20132802.0162","fpage":"162","id":"08cd3df8-f149-49e0-851a-28afe7fed25d","issue":"2","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"89ec05d1-0f6f-4184-abe5-62626e5b7db4","keyword":"液晶","originalKeyword":"铁电液晶"},{"id":"c213a64d-066c-4803-b5fa-8e299d776bb1","keyword":"自组装单层膜","originalKeyword":"自组装单层膜"},{"id":"8da30bdc-3e51-4f1b-9541-b97b323ba3b7","keyword":"非对称","originalKeyword":"非对称"},{"id":"b93f398b-f2f3-4cb4-b2f2-4bdb38a73d1f","keyword":"单畴","originalKeyword":"单畴"}],"language":"zh","publisherId":"yjyxs201302002","title":"液晶摩擦-自组装非对称取向","volume":"28","year":"2013"},{"abstractinfo":"在改变外加电场实现液晶调谐滤波中,由于液晶的螺距和自发极化强度对温度变化很敏感,从而为液晶调谐滤波器的应用和准确度的提高带来了困难.从液晶的螺距和自发极化强度与温度的关系出发,讨论了温度对液晶双折射的影响,给出了液晶调谐滤波器的透射率随温度变化的关系式,并进行了数值计算.结果表明,温度升高时,透射率和带宽增大,透射峰波长向短波长方向移动,温度变化对液晶调滤波特性的影响远小于电场变化的影响.","authors":[{"authorName":"钱祥忠","id":"17fde2b1-611d-4e16-9012-cf8149426c08","originalAuthorName":"钱祥忠"}],"doi":"10.3969/j.issn.1007-5461.2007.04.024","fpage":"519","id":"8e93b99a-111f-44ca-aa05-49cc8a6243fb","issue":"4","journal":{"abbrevTitle":"LZDZXB","coverImgSrc":"journal/img/cover/LZDZXB.jpg","id":"53","issnPpub":"1007-5461","publisherId":"LZDZXB","title":"量子电子学报 "},"keywords":[{"id":"8f4e1253-6a74-4067-a574-8176fb65ceb6","keyword":"光电子学","originalKeyword":"光电子学"},{"id":"10881f78-3819-405f-b416-71b8d3b8af5d","keyword":"滤波特性","originalKeyword":"滤波特性"},{"id":"51962bea-f33f-41d8-a610-076f63a9181a","keyword":"数值计算","originalKeyword":"数值计算"},{"id":"3a080bf6-3c90-434a-aa57-417c759dc4c5","keyword":"光子晶体","originalKeyword":"光子晶体"},{"id":"8f9d2bb0-5f41-4231-a126-87779d446316","keyword":"温度","originalKeyword":"温度"},{"id":"b486bf96-31d4-4572-b08a-f6d19225da73","keyword":"液晶","originalKeyword":"铁电液晶"}],"language":"zh","publisherId":"lzdzxb200704024","title":"温度对液晶调谐滤波特性影响的研究","volume":"24","year":"2007"},{"abstractinfo":"描述了矩阵寻址液晶(FLC)多信道透射型空间光调制器(SLM)的结构和运转特性,测量了器件的二进制相位调制的空间和时间特性.","authors":[{"authorName":"史永基","id":"ca366d0d-dd5a-4cd2-8f21-758911a098fe","originalAuthorName":"史永基"},{"authorName":"史建军","id":"0b992819-c5be-4a59-9ca4-a146320611d1","originalAuthorName":"史建军"},{"authorName":"史红军","id":"ee6bd13f-fed5-4110-b327-91a14a517955","originalAuthorName":"史红军"}],"doi":"10.3969/j.issn.1007-2780.2003.02.012","fpage":"130","id":"7224268a-ffad-46ef-bc92-cddafea311d0","issue":"2","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"520ee3c1-bbca-4248-ba64-26ef3e63d23a","keyword":"液晶","originalKeyword":"铁电液晶"},{"id":"91b24cb2-de33-4a23-ad20-b3dffc6af1e8","keyword":"空间光调制器","originalKeyword":"空间光调制器"},{"id":"4dde39cc-134e-44d4-9a52-7a5a180bd139","keyword":"空间特性","originalKeyword":"空间特性"},{"id":"d1c7e6f1-ba64-4828-882b-3e5b03ca4b06","keyword":"时间响应特性","originalKeyword":"时间响应特性"}],"language":"zh","publisherId":"yjyxs200302012","title":"多信道液晶空间光调制器","volume":"18","year":"2003"},{"abstractinfo":"N*-Sc*液晶由于具备自发极化值较小、能够实现灰度、快速响应等特点,能够满足场序全彩色显示的要求,近年来倍受关注.采用传统的摩擦取向的方法,通过在N*-Sc*相变时施加10 V直流电压,得到了没有SA相液晶的均匀排列.并且获得了半\"V\"字型的电光特性.分析了摩擦强度和相变时施加的电压对获得均匀排列的影响.","authors":[{"authorName":"乌日娜","id":"68ea64a9-d865-4948-9cd1-ff859b506a82","originalAuthorName":"乌日娜"},{"authorName":"彭增辉","id":"19b4a1a2-52a5-4313-9fac-dee3c2c14b19","originalAuthorName":"彭增辉"},{"authorName":"鲁兴海","id":"3c241023-45ed-4144-89f6-424ba3ac5632","originalAuthorName":"鲁兴海"},{"authorName":"宣丽","id":"438fab38-e1e4-4531-952b-f1ca044012c5","originalAuthorName":"宣丽"}],"doi":"10.3969/j.issn.1007-2780.2004.06.004","fpage":"427","id":"b2554fe4-ae94-4dff-a8df-d51c7714cfb0","issue":"6","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"31205e99-ac6a-4215-af47-644b47991fe4","keyword":"液晶","originalKeyword":"铁电液晶"},{"id":"67e3365d-7d79-4c61-994e-c6812c945a04","keyword":"N*-Sc*相变","originalKeyword":"N*-Sc*相变"},{"id":"5cb21ef4-a0c3-4b91-a4fa-7c64df811aaf","keyword":"半\"V\"字型","originalKeyword":"半\"V\"字型"},{"id":"94ccf3e6-b430-471e-b554-2e32ecf6d45e","keyword":"摩擦强度","originalKeyword":"摩擦强度"},{"id":"fc958499-b40b-403a-845d-2dcf3071a8e9","keyword":"DC电压","originalKeyword":"DC电压"}],"language":"zh","publisherId":"yjyxs200406004","title":"N*-Sc*相变液晶的排列","volume":"19","year":"2004"},{"abstractinfo":"自从Clark与Lagerwall提出表面双稳液晶显示原理后,液晶材料在显示领域中的应用一直是国内外研究的热点课题.总结了国内近年来液晶材料的合成与研究工作和目前在显示领域应用中遇到的问题,并阐述了在其他领域的应用前景.","authors":[{"authorName":"杭德余","id":"1af3acd7-541c-4370-b413-1df5630e239a","originalAuthorName":"杭德余"},{"authorName":"郑志","id":"e1d9ca87-3705-4480-9ac6-ff197e1a8470","originalAuthorName":"郑志"},{"authorName":"陈闯","id":"54f7d63d-e94f-427a-8ff0-f270e0e3d9a1","originalAuthorName":"陈闯"},{"authorName":"章于川","id":"f42fb07c-08e9-42f9-9399-66037a86ad2d","originalAuthorName":"章于川"}],"doi":"10.3969/j.issn.1007-2780.2002.02.004","fpage":"98","id":"3e6ed553-cadb-43ff-a8ee-a9608d364ef5","issue":"2","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"a4cb840d-f4a6-498f-b963-78101d461260","keyword":"液晶","originalKeyword":"铁电液晶"},{"id":"1c6c2317-8c35-4dfb-b03d-8de3d3af90b6","keyword":"液晶材料","originalKeyword":"铁电液晶材料"},{"id":"d2cb26c8-d97e-4647-b067-b940f7aa8d26","keyword":"应用前景","originalKeyword":"应用前景"}],"language":"zh","publisherId":"yjyxs200202004","title":"我国液晶材料研究进展","volume":"17","year":"2002"},{"abstractinfo":"采用N*-Sc*序列相液晶,通过在N*-Sc*相变时施加直流电压,得到了半\"V\"字型的电光特性曲线,可以实现连续灰度;同时解决了表面稳定液晶中存在的液晶层倾斜方向不惟一的缺陷,获得了无缺陷排列取向的液晶器件.该器件具有较低的饱和电压3.2 V,静态对比度达196:1,上升时间和下降时间分别是526靤和424 靤.","authors":[{"authorName":"冯亚云","id":"3a1202ec-f18f-42c9-a942-34374dce8c73","originalAuthorName":"冯亚云"},{"authorName":"任娇燕","id":"e52cc1d5-5f43-4b82-ac4e-30b3bc4e7325","originalAuthorName":"任娇燕"},{"authorName":"凌志华","id":"51f7614f-2073-4d72-b375-1b697b9e1666","originalAuthorName":"凌志华"}],"doi":"10.3969/j.issn.1007-2780.2008.02.014","fpage":"191","id":"0df1e86e-b0ba-4de8-af40-8599f61d91f5","issue":"2","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"6c13ae10-a52b-440d-9f9e-99cbaaf8c2e4","keyword":"液晶","originalKeyword":"铁电液晶"},{"id":"86781f89-e28e-44c2-8673-a0448159f02f","keyword":"N*-Sc*相变点","originalKeyword":"N*-Sc*相变点"},{"id":"c4e37bc7-9c2c-4824-8b69-ee0eb19f0972","keyword":"连续灰度","originalKeyword":"连续灰度"},{"id":"2b06f920-f656-47c6-8943-41515cb039ca","keyword":"表面稳定","originalKeyword":"表面稳定"},{"id":"9c9b663f-0fbd-4bc3-bfbd-c574a35c88e3","keyword":"半\"V\"字型","originalKeyword":"半\"V\"字型"}],"language":"zh","publisherId":"yjyxs200802014","title":"具有半\"V\"字型特性的液晶显示器件制备","volume":"23","year":"2008"},{"abstractinfo":"采用极性自组装单层膜和摩擦的方法制备了非对称的液晶盒.在液晶相变的过程中不施加电场,得到了排列均一的液晶器件.实验表明:极性自组装单层膜极性越大器件的对比度越高.经过分析得出该器件液晶分子取向机理为:基板附近的液晶通过偶极和极性自组装膜的作用,使得靠近自组装膜表面处的偶极和靠近摩擦表面的偶极的指向相同,通过分子的相互作用使得体内分子排列方向一致.","authors":[{"authorName":"邹忠飞","id":"f59d9a15-99c4-407d-a06d-54f19c954d39","originalAuthorName":"邹忠飞"},{"authorName":"唐先柱","id":"b388c116-be33-49cd-a241-46035c04fbbc","originalAuthorName":"唐先柱"},{"authorName":"季新建","id":"01a8370a-9292-455e-ac20-327dab241505","originalAuthorName":"季新建"},{"authorName":"鲁星海","id":"8623afcb-ecce-4725-ad6e-9981e014e66d","originalAuthorName":"鲁星海"},{"authorName":"宣丽","id":"6b53d1cd-b09a-4bf9-bcc3-caa4f0cab78e","originalAuthorName":"宣丽"}],"doi":"10.3969/j.issn.1007-2780.2009.02.005","fpage":"179","id":"3491c175-295b-431d-861b-d0fefae4c71c","issue":"2","journal":{"abbrevTitle":"YJYXS","coverImgSrc":"journal/img/cover/YJYXS.jpg","id":"72","issnPpub":"1007-2780","publisherId":"YJYXS","title":"液晶与显示 "},"keywords":[{"id":"f50ec93c-6788-4bb2-8db4-3b4399869edb","keyword":"液晶","originalKeyword":"铁电液晶"},{"id":"5b659eaf-bd9c-45a2-b7d5-64a967e4d145","keyword":"自组装单层膜","originalKeyword":"自组装单层膜"},{"id":"4078bc7a-ba45-4921-95b8-2677ec982781","keyword":"单畴","originalKeyword":"单畴"}],"language":"zh","publisherId":"yjyxs200902005","title":"极性自组装单层膜取向液晶器件","volume":"24","year":"2009"}],"totalpage":2063,"totalrecord":20627}