{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"利用Monte Carlo方法模拟平行基板间<span style=\"color:red\">液晶</span>薄层的指向矢分布.在基板表面处,<span style=\"color:red\">液晶</span>薄层受到表面作用势的作用使<span style=\"color:red\">液晶</span>分子沿面平行排列,采用Lebwohl-Lasher模型,将分子质心固定在简单立方晶格的格点上,并对此格点模型赋以周期性边界条件,然后将简立方格点模型分为平行于基板的20个分子薄层,得到各薄层的指向矢分布的数值结果.计算中同时考虑了基板作用引起的双轴对称性.","authors":[{"authorName":"崔建坡","id":"69c55bc1-4e7f-40c4-bb3b-ec48a57dd64c","originalAuthorName":"崔建坡"},{"authorName":"张志东","id":"b41b5a79-7416-4bd8-a803-6c59f0bbd921","originalAuthorName":"张志东"},{"authorName":"张艳君","id":"5a07adf7-0aad-4c75-b6d4-28161e0a67d2","originalAuthorName":"张艳君"}],"doi":"10.3969/j.issn.1007-2780.2005.02.009","fpage":"123","id":"4257e26a-2dbe-4775-8c01-58d8b34a5577","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":"33ae65f9-5879-4178-a55e-e562145a2753","keyword":"<span style=\"color:red\">液晶</span><span style=\"color:red\">层</span>","originalKeyword":"液晶层"},{"id":"13eb398b-a738-4c17-9262-be98c3642b52","keyword":"表面作用势","originalKeyword":"表面作用势"},{"id":"0cd5f45f-e6a0-416a-9967-dffcfa086d41","keyword":"摩擦基板","originalKeyword":"摩擦基板"},{"id":"21e13be1-480e-471e-9f36-c23eadcbbeaf","keyword":"Monte Carlo模拟","originalKeyword":"Monte Carlo模拟"}],"language":"zh","publisherId":"yjyxs200502009","title":"摩擦基板间<span style=\"color:red\">液晶</span>薄层的Monte Carlo模拟","volume":"20","year":"2005"},{"abstractinfo":"在<span style=\"color:red\">液晶</span>显示器或硅基<span style=\"color:red\">液晶</span>显示器中,取向<span style=\"color:red\">层</span>或彩色滤色膜对驱动电压的分压效应是不能忽视的.文章应用电容模型,理论上给出了<span style=\"color:red\">液晶</span><span style=\"color:red\">层</span>的分压公式和<span style=\"color:red\">液晶</span><span style=\"color:red\">层</span>的等效介电常数公式,并通过模拟计算了取向<span style=\"color:red\">层</span>厚度、<span style=\"color:red\">液晶</span><span style=\"color:red\">层</span>厚度对<span style=\"color:red\">液晶</span><span style=\"color:red\">层</span>分压的影响.研究结果对<span style=\"color:red\">液晶</span>显示器的结构设计有一定的参考意义.","authors":[{"authorName":"田园","id":"0c1d6982-4e70-4d29-96cc-81a838037616","originalAuthorName":"田园"},{"authorName":"张亚星","id":"2eced632-40cd-422c-af47-60628fedde57","originalAuthorName":"张亚星"},{"authorName":"孙玉宝","id":"2c27eb51-c59c-436f-a33e-abfc68b54d9c","originalAuthorName":"孙玉宝"}],"doi":"10.3969/j.issn.1007-2780.2010.04.030","fpage":"588","id":"fdb20a23-5f9f-4895-881c-1635da738a02","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":"da7f2d07-3f6d-4cd5-b57e-b3cd8b4e922b","keyword":"取向<span style=\"color:red\">层</span>","originalKeyword":"取向层"},{"id":"38964b19-8518-4db7-92ea-042ddc720675","keyword":"<span style=\"color:red\">液晶</span>显示器","originalKeyword":"液晶显示器"},{"id":"2c0d72c2-546e-47ab-8a34-ffd517c8d8ff","keyword":"分压","originalKeyword":"分压"}],"language":"zh","publisherId":"yjyxs201004030","title":"取向<span style=\"color:red\">层</span>厚度对<span style=\"color:red\">液晶</span><span style=\"color:red\">层</span>分压的影响","volume":"25","year":"2010"},{"abstractinfo":"从铁电<span style=\"color:red\">液晶</span>(FLC)的物性出发,描述了表面双稳铁电<span style=\"color:red\">液晶</span>(SSFLC)显示结构原理和相应特点;系统地介绍了SSFLC中的<span style=\"color:red\">液晶</span><span style=\"color:red\">层</span>结构分类及相关特征.阐述了不同<span style=\"color:red\">层</span>结构对<span style=\"color:red\">液晶</span>器件双稳态的获得及电光特性的影响.","authors":[{"authorName":"李建军","id":"e5783d7d-1a71-4ef6-8aa8-576fcda81862","originalAuthorName":"李建军"},{"authorName":"宣丽","id":"09c1e13e-0215-4c8d-a300-49e5067e94a4","originalAuthorName":"宣丽"},{"authorName":"黄锡珉","id":"cf526c16-23af-4066-b98d-56ef78d1b2eb","originalAuthorName":"黄锡珉"}],"doi":"10.3969/j.issn.1007-2780.1999.03.012","fpage":"220","id":"cf9acff0-29ae-4cb7-9f2c-9e9a7765646a","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":"4b717b14-2221-42b2-a4d6-25e0aeec08a4","keyword":"表面双稳铁电<span style=\"color:red\">液晶</span>(SSFLC)","originalKeyword":"表面双稳铁电液晶(SSFLC)"},{"id":"eeb179a4-2220-46e3-99c7-9a5b5309891d","keyword":"<span style=\"color:red\">层</span>结构","originalKeyword":"层结构"},{"id":"30bbfe40-862b-407b-9694-a7220ed116e3","keyword":"书架式结构","originalKeyword":"书架式结构"},{"id":"d2103191-7f91-483f-af1b-8b10a007b24b","keyword":"Chevron式结构","originalKeyword":"Chevron式结构"},{"id":"35a1ef76-3b5c-40b5-95d1-5567d185be01","keyword":"Zig-Zag缺陷","originalKeyword":"Zig-Zag缺陷"}],"language":"zh","publisherId":"yjyxs199903012","title":"表面双稳铁电<span style=\"color:red\">液晶</span>中的<span style=\"color:red\">层</span>结构","volume":"14","year":"1999"},{"abstractinfo":"介绍了一种具有柱状结构的a-Si:H/nc-Si复合光导<span style=\"color:red\">层</span>的<span style=\"color:red\">液晶</span>光阀,复合光导<span style=\"color:red\">层</span>是通过热蒸发和等离子体辉光放电沉积方法,采用Al诱导a-Si:H制成的.经过测试,这种柱状结构薄膜具有电导各向异性,其横向电导率小于纵向电导率.用这种薄膜制成的<span style=\"color:red\">液晶</span>光阀其分辨率达到500lp/inch.","authors":[{"authorName":"于永红","id":"2c17a9ed-eefe-428e-a8e2-c59b83b73c47","originalAuthorName":"于永红"},{"authorName":"杜丕一","id":"5b192318-604d-44d8-984b-6f3ed9a2ce8d","originalAuthorName":"杜丕一"},{"authorName":"王瑞春","id":"f5fd1b35-223a-46dd-8d6d-9b0245c265cc","originalAuthorName":"王瑞春"},{"authorName":"韩高荣","id":"e70ba73a-292b-42e2-87e5-09416c77963f","originalAuthorName":"韩高荣"},{"authorName":"翁文剑","id":"727f4d34-3228-4acc-9e5b-2b2443b0808e","originalAuthorName":"翁文剑"}],"doi":"10.3969/j.issn.1007-4252.2003.03.014","fpage":"305","id":"6c0af39e-5807-4762-a2d4-f90226c1de28","issue":"3","journal":{"abbrevTitle":"GNCLYQJXB","coverImgSrc":"journal/img/cover/GNCLYQJXB.jpg","id":"34","issnPpub":"1007-4252","publisherId":"GNCLYQJXB","title":"功能材料与器件学报   "},"keywords":[{"id":"1202efff-a73a-4cbc-8c13-97aabfef6e41","keyword":"<span style=\"color:red\">液晶</span>光阀","originalKeyword":"液晶光阀"},{"id":"1d3b48f4-917b-4a0b-96fa-3cfa9f5b7ce2","keyword":"柱状结构","originalKeyword":"柱状结构"},{"id":"1eb587da-e641-42e0-b9f6-ec4edba2aa1a","keyword":"a-Si:H/nc-Si复合薄膜","originalKeyword":"a-Si:H/nc-Si复合薄膜"},{"id":"ed513f98-8119-4cae-9dc0-47a0e0fd7e00","keyword":"光导<span style=\"color:red\">层</span>","originalKeyword":"光导层"}],"language":"zh","publisherId":"gnclyqjxb200303014","title":"复合光导<span style=\"color:red\">层</span><span style=\"color:red\">液晶</span>光阀的研究","volume":"9","year":"2003"},{"abstractinfo":"<span style=\"color:red\">液晶</span>显示器的聚酰亚胺配向<span style=\"color:red\">层</span>(Polyimide,PI)电荷累积过程属于凝聚态物理的电介质理论范畴,由于电介质物理理论还不够完整,造成<span style=\"color:red\">液晶</span>显示器PI<span style=\"color:red\">层</span>电荷累积和释放过程机理不甚清晰.文章应用麦克斯韦方程组分析<span style=\"color:red\">液晶</span>PI<span style=\"color:red\">层</span>表面电荷累积过程,应用可将快慢效应分开的时域谱学理论分析慢电荷的释放过程,得出<span style=\"color:red\">液晶</span>面板PI<span style=\"color:red\">层</span>和<span style=\"color:red\">液晶</span><span style=\"color:red\">层</span>接触面电荷累积与两者的介电常数和电导率的关系,以及累积慢电荷的释放时间常数与PI<span style=\"color:red\">层</span>厚度的关系.","authors":[{"authorName":"张武勤","id":"134a7631-c3c8-4934-9cdd-e7b57865c2b1","originalAuthorName":"张武勤"}],"doi":"10.3969/j.issn.1007-2780.2010.03.011","fpage":"351","id":"3e9f5a71-1b1e-4220-91de-2bf68a7c9e1c","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":"2039ccca-7a00-43f9-b3c6-fa310b8b6d8f","keyword":"电荷极化","originalKeyword":"电荷极化"},{"id":"435b8497-bfc0-434c-b859-5fc7f0da6880","keyword":"快电荷","originalKeyword":"快电荷"},{"id":"b6723e79-05b7-4955-a416-1341e528247e","keyword":"慢电荷","originalKeyword":"慢电荷"}],"language":"zh","publisherId":"yjyxs201003011","title":"<span style=\"color:red\">液晶</span>面板PI<span style=\"color:red\">层</span>电荷累积和释放过程分析","volume":"25","year":"2010"},{"abstractinfo":"基于手性<span style=\"color:red\">液晶</span>的布拉格反射特性,设计了旋向相反的手性<span style=\"color:red\">液晶</span>所构成的红、绿、蓝三基色叠层级联结构,以达到增强单元反射率的目的.采用Berreman 4×4矩阵对其单元反射率进行了分析,比较了手性<span style=\"color:red\">液晶</span>的单旋向三基色叠<span style=\"color:red\">层</span>(三叠<span style=\"color:red\">层</span>结构)与双旋向三基色叠<span style=\"color:red\">层</span>(六叠<span style=\"color:red\">层</span>结构)单元的反射谱,给出了改变<span style=\"color:red\">液晶</span>材料参数和级联顺序进一步提高单元反射率的计算结果.在最佳参数与级联顺序下,六叠<span style=\"color:red\">层</span>单元的最大反射率达到98.91%,三叠<span style=\"color:red\">层</span>单元的最大反射率为64.95%.叠<span style=\"color:red\">层</span>结构单元的色度分析结果表明,三<span style=\"color:red\">层</span>单元的色温依级联<span style=\"color:red\">液晶</span>旋向而改变,范围为5 240.9～7 029.8 K,在反射率最优的条件下,六叠<span style=\"color:red\">层</span>单元的色温为6 285.7 K.","authors":[{"authorName":"秦臻","id":"face23fc-d479-4103-b0dd-f24c35f811f0","originalAuthorName":"秦臻"},{"authorName":"方旭","id":"044771b4-4fe3-47b5-b297-cf4bcb9806df","originalAuthorName":"方旭"},{"authorName":"毛鑫","id":"a0fe29aa-b6a1-4769-aeea-3e46c4756f72","originalAuthorName":"毛鑫"},{"authorName":"黄子强","id":"3e840a65-5998-4dcd-8b65-4dcf236d39da","originalAuthorName":"黄子强"}],"doi":"10.3788/YJYXS20112605.0592","fpage":"592","id":"e33684f9-3445-4b35-948d-0d81fa071c0c","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":"b8e4636c-b509-4c8a-b378-f046fa3cf9a4","keyword":"手性<span style=\"color:red\">液晶</span>","originalKeyword":"手性液晶"},{"id":"31fc2e9d-03bb-438b-8c2f-ae845ffd3b1d","keyword":"级联","originalKeyword":"级联"},{"id":"6010fcf8-c6ae-4a93-983d-69ff44ab8329","keyword":"光谱","originalKeyword":"光谱"},{"id":"32040512-bd88-485d-a0f1-609e7d66bec9","keyword":"4×4矩阵","originalKeyword":"4×4矩阵"}],"language":"zh","publisherId":"yjyxs201105005","title":"叠<span style=\"color:red\">层</span>结构的手性<span style=\"color:red\">液晶</span>单元的反射谱特性","volume":"26","year":"2011"},{"abstractinfo":"建立了基于有限元法的<span style=\"color:red\">液晶</span><span style=\"color:red\">层</span>中指向矢分布的计算方法, 可以方便地考虑非对称取向和表面锚定能及其形式对指向矢分布的影响. 作为应用实例, 给出了非对称弱锚定情形下的<span style=\"color:red\">液晶</span><span style=\"color:red\">层</span>中指向矢分布的计算结果. ","authors":[{"authorName":"邵喜斌","id":"aca726b2-a76f-4fd8-8933-3227772e1879","originalAuthorName":"邵喜斌"},{"authorName":"黄锡珉","id":"98025d2c-c988-4965-9a36-6fc64b1e9123","originalAuthorName":"黄锡珉"}],"doi":"10.3969/j.issn.1007-2780.2001.03.001","fpage":"163","id":"dcf3b5e7-e132-4ee3-a81c-c058c3264b4c","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":"efa4d3bb-6911-43b7-985c-05a3cdab54a4","keyword":"<span style=\"color:red\">液晶</span>","originalKeyword":"液晶"},{"id":"d1ebfcbd-eb5b-447b-8de5-405739452d95","keyword":"有限元法","originalKeyword":"有限元法"},{"id":"fdd49051-12d5-48ea-b2e5-111d6083c9a2","keyword":"指向矢分布","originalKeyword":"指向矢分布"},{"id":"1d1944c9-3bfc-46a5-ad5b-0e68fb74be9a","keyword":"锚定能","originalKeyword":"锚定能"}],"language":"zh","publisherId":"yjyxs200103001","title":"有限元法求解<span style=\"color:red\">液晶</span><span style=\"color:red\">层</span>中的指向矢分布","volume":"16","year":"2001"},{"abstractinfo":"用化学气相沉积法制备了<span style=\"color:red\">液晶</span>光阀中光电导<span style=\"color:red\">层</span>--非晶硅薄膜,从实验中得出最佳制备工艺的参数取值.给出了用包络线法测量非晶硅薄膜光吸收系数的原理,测量了样品的光吸收系数随波长的变化规律.得到样品在最佳工艺条件下的光吸收系数高于1×103 cm-1.","authors":[{"authorName":"钱祥忠","id":"82f89a71-1a14-4b1a-a297-647184ad9c28","originalAuthorName":"钱祥忠"},{"authorName":"黄芳云","id":"ecd7156f-e23e-4a57-8f96-6993d1a0f85d","originalAuthorName":"黄芳云"}],"doi":"10.3969/j.issn.1007-2780.2004.03.013","fpage":"218","id":"609e1b84-e6bc-47e4-82b6-16e5c61a73dc","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":"1172d713-fdbd-449a-be04-4cda03b3652d","keyword":"<span style=\"color:red\">液晶</span>光阀","originalKeyword":"液晶光阀"},{"id":"ff55b015-3a20-4c6c-8c2a-4305a582ff1d","keyword":"光吸收系数","originalKeyword":"光吸收系数"},{"id":"60ffca48-a730-4bc6-b94d-c80a3f8f9b06","keyword":"光电导<span style=\"color:red\">层</span>","originalKeyword":"光电导层"},{"id":"aff1a24a-e44c-454d-b114-b5b0d9104eb8","keyword":"波长","originalKeyword":"波长"},{"id":"597575aa-a8db-4d97-b319-cbcd47614276","keyword":"非晶硅","originalKeyword":"非晶硅"}],"language":"zh","publisherId":"yjyxs200403013","title":"<span style=\"color:red\">液晶</span>光阀光电导<span style=\"color:red\">层</span>光吸收系数的研究","volume":"19","year":"2004"},{"abstractinfo":"利用传输矩阵法研究了含向列相<span style=\"color:red\">液晶</span>缺陷<span style=\"color:red\">层</span>的1维阶梯型双周期第4代准周期结构缺陷模的电场方向调控特性.分析了外加电场方向和正入射波方向间夹角θ与缺陷模波长的位置、品质因子、空间位置光场分布的变化关系,探讨了缺陷模的品质因子对光场强度的影响.结果表明:随着夹角θ的逐渐增大,缺陷模的位置向短波方向移动,缺陷模波长的调控量为84 nm;随着夹角θ的逐渐增大,缺陷模的品质因子逐渐增大;缺陷模在空间位置的光场分布呈现出局域现象,随夹角θ的增大,空间位置的光场强度逐渐增强;缺陷模的品质因子与光场强度成正比关系.","authors":[{"authorName":"廖昆","id":"78b96c89-6215-4d4b-abef-e26a94d6085d","originalAuthorName":"廖昆"},{"authorName":"谢应茂","id":"359cc26d-0a94-4cd8-9825-5d5da47ceb1b","originalAuthorName":"谢应茂"}],"doi":"10.3969/j.issn.1007-5461.2016.02.002","fpage":"135","id":"992b03cc-8ab0-4c89-8359-9969eb6510e5","issue":"2","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":"898cc574-e521-40ad-8d94-899412fcce23","keyword":"光的电磁理论","originalKeyword":"光的电磁理论"},{"id":"6fbfb020-19f2-4565-90cb-fd12da97028c","keyword":"阶梯型双周期结构","originalKeyword":"阶梯型双周期结构"},{"id":"b0abe5aa-2dbf-454d-81a6-c4319fa5ae44","keyword":"缺陷模","originalKeyword":"缺陷模"},{"id":"9b06d1df-cd06-42bb-8b9c-b9b140713ff2","keyword":"传输矩阵法","originalKeyword":"传输矩阵法"},{"id":"6c7ba08f-9502-451a-9d70-31dca2ce9003","keyword":"光场分布","originalKeyword":"光场分布"},{"id":"d5195207-d672-425e-9532-30374bf42f8f","keyword":"品质因子","originalKeyword":"品质因子"}],"language":"zh","publisherId":"lzdzxb201602002","title":"含<span style=\"color:red\">液晶</span>缺陷<span style=\"color:red\">层</span>阶梯型双周期结构的电场方向调控特性","volume":"33","year":"2016"},{"abstractinfo":"基于<span style=\"color:red\">液晶</span>折射率对温度和电场的特性,采用传输矩阵法,研究了含一缺陷<span style=\"color:red\">层</span>一维<span style=\"color:red\">液晶</span>填充光子晶体缺陷模电场和温度调控特性.研究结果表明:当温度T在273～330 K内一定时,随着垂直入射光与电场方向间夹角θ在(0,π/2)内增大,缺陷模波长向短波方向漂移,最大调控波长为37.3 nm.当夹角θ在(0,π/2)内一定时,随着外界温度T在273～330 K内升高,缺陷模波长发生改变,变化量先负后正,最大调控波长为21.9 nm.当θ=0.7505时,不管外界温度T在273～330 K内如何变化,缺陷模波长保持不变.温度对缺陷模波长的影响比垂直入射光与电场方向间夹角θ对缺陷模波长的影响更弱.","authors":[{"authorName":"殷新星","id":"830bbd92-9817-4f21-95a7-9be4c8c23dea","originalAuthorName":"殷新星"},{"authorName":"谢应茂","id":"da65053d-f2a4-43ac-a7f8-4bc53dfd64c9","originalAuthorName":"谢应茂"}],"doi":"10.3969/j.issn.1007-5461.2013.03.012","fpage":"318","id":"539785ef-22f2-45ef-b49d-a1bbe7d7be4c","issue":"3","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":"01580f42-d72b-4b67-a1f6-59241fc1c453","keyword":"光电子学","originalKeyword":"光电子学"},{"id":"945ce685-bd07-4f15-934e-fd6468301936","keyword":"缺陷模","originalKeyword":"缺陷模"},{"id":"463834b8-c413-4630-844b-72df6216ed80","keyword":"传输矩阵法","originalKeyword":"传输矩阵法"},{"id":"a6dfa622-5834-436d-92fb-f38d4b79c902","keyword":"可调光子晶体","originalKeyword":"可调光子晶体"},{"id":"76a6cfa5-8441-4b16-ac58-f7394f300fed","keyword":"<span style=\"color:red\">液晶</span>","originalKeyword":"液晶"}],"language":"zh","publisherId":"lzdzxb201303012","title":"含一缺陷<span style=\"color:red\">层</span>的一维<span style=\"color:red\">液晶</span>填充光子晶体缺陷模电场和温度调控特性","volume":"30","year":"2013"}],"totalpage":2416,"totalrecord":24154}