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style=\"color:red\">排列</span>的SWNTs构建的场效应晶体管(FET)的电学性质,所制的p型FET的开关比达到106.此方法适用于在大范围内构建高灵敏度、宽温度范围、快速响应的SWNTs的微电子元器件.","authors":[{"authorName":"王林","id":"48987f02-1f6e-4ce9-8a17-4afe54138ea0","originalAuthorName":"王林"},{"authorName":"谌志强","id":"b9aa0eb6-1cb4-45ff-bdc6-d66145030096","originalAuthorName":"谌志强"},{"authorName":"杨丹娜","id":"abde18db-bdd8-42bc-9e24-a4294cb6d067","originalAuthorName":"杨丹娜"},{"authorName":"张潇娴","id":"ecfc6eb0-68a8-40b1-9cb1-83942550e159","originalAuthorName":"张潇娴"},{"authorName":"王东卫","id":"f1cc4a62-c6bf-46e1-ab32-329730aefdde","originalAuthorName":"王东卫"},{"authorName":"李赛","id":"caeaf323-1cf5-49ba-bf06-f6d67b3a582c","originalAuthorName":"李赛"}],"doi":"","fpage":"85","id":"b58fe109-2d4a-4a73-bdc4-e83b55d64df9","issue":"18","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"fbdf0557-ae5f-4be1-9c00-8bc8fb7aa85f","keyword":"碳纳米管","originalKeyword":"碳纳米管"},{"id":"f17c77f0-35be-416b-88fa-7b6b0cbc7e4e","keyword":"<span style=\"color:red\">流体</span><span style=\"color:red\">排列</span>","originalKeyword":"流体排列"},{"id":"c1e9957a-7d69-48da-9e59-cf74c1d44763","keyword":"模板","originalKeyword":"模板"},{"id":"f2998dbf-0235-47c6-97bc-131b9823e7f4","keyword":"微流道","originalKeyword":"微流道"}],"language":"zh","publisherId":"cldb201118023","title":"基于微流道模板的<span style=\"color:red\">流体</span>法<span style=\"color:red\">排列</span>单壁碳纳米管的研究","volume":"25","year":"2011"},{"abstractinfo":"综述了近几年来碳纳米管(CNTs)在水平方向上的定向生长以及后合成<span style=\"color:red\">排列</span>CNTs的各种方法,如机械拉伸法、磁场法、Langmuir-Blodgett(LB)法、电场法、<span style=\"color:red\">流体</span>法等,系统分析和比较了各种方法的优缺点,同时展望了该领域的研究和应用前景.","authors":[{"authorName":"王林","id":"1182b8eb-16bf-4621-80f1-23a0984c7ac9","originalAuthorName":"王林"},{"authorName":"杨丹娜","id":"f3b85b26-94f8-4627-8849-5b7140eb1f4d","originalAuthorName":"杨丹娜"},{"authorName":"李赛","id":"17530288-d0b8-4904-b4d2-af35ab4a2e9b","originalAuthorName":"李赛"}],"doi":"","fpage":"119","id":"49f84d5c-8b88-4838-9061-2526bd9d5dcd","issue":"5","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"d15ae532-1f95-4e09-9dcd-ae7fce938c1e","keyword":"碳纳米管(CNTs)","originalKeyword":"碳纳米管(CNTs)"},{"id":"e7809dcb-bed4-42ee-a697-5b88061cf38d","keyword":"水平<span style=\"color:red\">排列</span>","originalKeyword":"水平排列"},{"id":"c90eb1b8-5520-48d6-a07e-771a27d97397","keyword":"集成电路","originalKeyword":"集成电路"}],"language":"zh","publisherId":"cldb201105027","title":"碳纳米管在水平方向上<span style=\"color:red\">排列</span>的研究进展","volume":"25","year":"2011"},{"abstractinfo":"综述了近几年来碳纳米管(CNTs)在水平方向上的定向生长以及后合成<span style=\"color:red\">排列</span>CNTs的各种方法,如机械拉伸法、磁场法、Langmuir-Blodgett(LB)法、电场法、<span style=\"color:red\">流体</span>法等,系统分析和比较了各种方法的优缺点,同时展望了该领域的研究和应用前景.","authors":[{"authorName":"王林","id":"edcfc597-8904-4620-a8ae-cd16d202e20c","originalAuthorName":"王林"},{"authorName":"杨丹娜","id":"57200bd9-17e7-4bbb-9c69-d95c23e6d822","originalAuthorName":"杨丹娜"},{"authorName":"李赛","id":"a75c5086-44b4-413c-bce7-c3abc77f33bf","originalAuthorName":"李赛"}],"doi":"","fpage":"119","id":"cb13e8aa-ff62-456d-a9e7-80791d639820","issue":"3","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"f6b61ae5-5371-409d-b5dc-2f730392a334","keyword":"纳米管(CNTs)","originalKeyword":"纳米管(CNTs)"},{"id":"c0ef9658-0420-4264-9589-ec5e54b962bc","keyword":"水平<span style=\"color:red\">排列</span>","originalKeyword":"水平排列"},{"id":"3eca0474-91d4-4fb9-8960-33d8646627ed","keyword":"集成电路","originalKeyword":"集成电路"}],"language":"zh","publisherId":"cldb201103027","title":"碳纳米管在水平方向上<span style=\"color:red\">排列</span>的研究进展","volume":"25","year":"2011"},{"abstractinfo":"纳米<span style=\"color:red\">流体</span>的导热系数相对于基础<span style=\"color:red\">流体</span>而言有了显著提高,然而这种现象却无法用现有理论进行解释.应用平衡分子动力学方法对纳米<span style=\"color:red\">流体</span>的导热系数进行了模拟,并研究了纳米颗粒表面类似于固体的液体吸附层的存在和特性以及其对纳米<span style=\"color:red\">流体</span>导热能力的影响,在此基础上进一步对纳米<span style=\"color:red\">流体</span>导热性能显著提高的微观机理进行了探讨.模拟结果表明由于固体分子较强的吸引力,一部分液体分子被吸附在固体颗粒表面形成一个薄层,薄层内分子的<span style=\"color:red\">排列</span>结构不同于纯液体的分子<span style=\"color:red\">排列</span>结构,导热性能也优于基础<span style=\"color:red\">流体</span>,从而使得纳米<span style=\"color:red\">流体</span>的导热系数有了显著提高.最后对纳米颗粒表面液体薄层的厚度进行了定量计算.","authors":[{"authorName":"李凌","id":"6cb4041a-0ba8-401f-881f-9f3217751bfa","originalAuthorName":"李凌"},{"authorName":"郭丽","id":"80d01277-9cdf-4011-910b-7097367271bf","originalAuthorName":"郭丽"},{"authorName":"杨茉","id":"bd450392-53ff-4255-8d76-58f0d898c05e","originalAuthorName":"杨茉"},{"authorName":"卢玫","id":"baa6c5e1-6747-4572-8c7b-4932ab5fbcb3","originalAuthorName":"卢玫"},{"authorName":"余敏","id":"78e30665-d363-4ec8-9fa9-723c024f7629","originalAuthorName":"余敏"}],"doi":"","fpage":"1933","id":"0b8339e9-5dca-4d02-8b34-a86b75790cee","issue":"11","journal":{"abbrevTitle":"GCRWLXB","coverImgSrc":"journal/img/cover/GCRWLXB.jpg","id":"32","issnPpub":"0253-231X","publisherId":"GCRWLXB","title":"工程热物理学报   "},"keywords":[{"id":"527759e3-ae63-4629-a002-f66bcf4ce069","keyword":"纳米<span style=\"color:red\">流体</span>","originalKeyword":"纳米流体"},{"id":"e472defa-7162-4567-a7ef-7d1f1958a808","keyword":"导热系数","originalKeyword":"导热系数"},{"id":"f63b899b-0d6b-4f69-a890-76c72b1fd0b0","keyword":"分子动力学模拟","originalKeyword":"分子动力学模拟"}],"language":"zh","publisherId":"gcrwlxb201011034","title":"纳米<span style=\"color:red\">流体</span>导热系数的分子动力学模拟","volume":"31","year":"2010"},{"abstractinfo":"微观组织定向<span style=\"color:red\">排列</span>能明显提高无机非金属材料的韧性,并产生力学和其它物理性能的各向异性,因此受到人们的广泛重视.主要介绍了当前实现玻璃陶瓷微观组织定向<span style=\"color:red\">排列</span>的3种不同方法的工艺过程及其理论基础,并展望了其应用前景.","authors":[{"authorName":"单小宏","id":"effbaebf-a6b1-4bfb-8b81-82ebb2b695d1","originalAuthorName":"单小宏"},{"authorName":"刘咏","id":"bb11c07d-37a1-4cb6-a3b3-59912a72e3e7","originalAuthorName":"刘咏"}],"doi":"","fpage":"69","id":"8dfd6ed4-6313-487e-a9ec-ea23874ca378","issue":"6","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"b3079fda-da14-466b-aae2-b7f242fdce5c","keyword":"定向<span style=\"color:red\">排列</span>","originalKeyword":"定向排列"},{"id":"7abba895-fea4-4bb1-8498-3c1b4e84d60a","keyword":"玻璃陶瓷","originalKeyword":"玻璃陶瓷"},{"id":"9effa694-c47f-4746-b4e3-4b38ce44ff62","keyword":"工艺过程","originalKeyword":"工艺过程"},{"id":"8f43ca8a-1cc9-4811-a44c-5713e6388033","keyword":"理论基础","originalKeyword":"理论基础"},{"id":"97f4402a-fed9-4225-b0ea-44224fb1e8f7","keyword":"应用","originalKeyword":"应用"}],"language":"zh","publisherId":"cldb200406021","title":"定向<span style=\"color:red\">排列</span>玻璃陶瓷的研究进展","volume":"18","year":"2004"},{"abstractinfo":"N*-Sc*铁电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相铁电液晶的均匀<span style=\"color:red\">排列</span>.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<span style=\"color:red\">排列</span>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":"铁电液晶","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*相变铁电液晶的<span style=\"color:red\">排列</span>","volume":"19","year":"2004"},{"abstractinfo":"模拟了手性垂直<span style=\"color:red\">排列</span>液晶盒的指向矢分布和电光特性,并在大视角内研究了其关态透过率、开态透过率和对比度.研究发现该常黑型显示模式具有很高的对比度、几乎无色散、高亮度、较低工作电压和在水平和垂直方向具有宽视角等特点.文章最后模拟了具有更宽视角的膜补偿手性垂直<span style=\"color:red\">排列</span>液晶盒.","authors":[{"authorName":"任芝","id":"0829a95f-6f7a-4e10-bc60-60652e953e0a","originalAuthorName":"任芝"},{"authorName":"张志东","id":"89b2c310-854e-42ba-ace4-f05788e358a8","originalAuthorName":"张志东"}],"doi":"10.3969/j.issn.1007-2780.2005.01.006","fpage":"32","id":"2792e37c-4d7b-472c-8c45-1cc4b38afbe2","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":"03fb2fa8-a5b5-4ca9-bd3a-ad2958756b54","keyword":"手性垂直<span style=\"color:red\">排列</span>液晶盒","originalKeyword":"手性垂直排列液晶盒"},{"id":"b35e7389-a95b-4648-8070-fc2cdc1fd5a7","keyword":"宽视角","originalKeyword":"宽视角"},{"id":"fe60c3db-ec8d-4c2c-a487-678b2d5792d9","keyword":"计算机模拟","originalKeyword":"计算机模拟"},{"id":"94a68cd4-0a3d-4dda-b29b-54ca02fe4a3c","keyword":"膜补偿","originalKeyword":"膜补偿"}],"language":"zh","publisherId":"yjyxs200501006","title":"手性垂直<span style=\"color:red\">排列</span>液晶盒的视角特性","volume":"20","year":"2005"},{"abstractinfo":"基于透镜扩束系统,应用棱镜耦合技术对液晶层的全漏导模特性进行了研究.采用盒厚为4.6 μm的平行<span style=\"color:red\">排列</span>向列相液晶盒,其内灌注E7液晶,通过实验给出了平行<span style=\"color:red\">排列</span>向列相液晶薄层的导波图,进而将实验结果与理论模拟结果进行了比较,理论所预言的液晶波导的导模在实验的导波图上得到了很好的验证.","authors":[{"authorName":"李志广","id":"a4bcdf6f-e05d-4974-b904-88db7a13afb1","originalAuthorName":"李志广"},{"authorName":"叶文江","id":"b94ec05e-0216-4910-a104-3c5eb2e76306","originalAuthorName":"叶文江"},{"authorName":"郭婷婷","id":"a1c0f3f8-28f7-4f15-8d53-e179a185c79d","originalAuthorName":"郭婷婷"},{"authorName":"张志东","id":"45c3ef92-8398-486e-b957-a66d06334442","originalAuthorName":"张志东"},{"authorName":"檀润华","id":"3fad2230-29ba-4078-934b-f8eacdf0a36d","originalAuthorName":"檀润华"}],"doi":"10.3969/j.issn.1007-2780.2009.06.009","fpage":"818","id":"3742a0da-db02-4105-ab36-3aaf0cf15546","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":"0f48ed83-2eed-4b3c-bf8b-e33ba3eb1806","keyword":"向列相液晶","originalKeyword":"向列相液晶"},{"id":"c572b933-0f29-4fb3-a22a-42651fb3bba6","keyword":"透镜扩束系统","originalKeyword":"透镜扩束系统"},{"id":"82333305-e8ba-432a-a31d-07d75796a1f3","keyword":"导波","originalKeyword":"导波"},{"id":"be54e218-c0b2-4618-b408-330f1d4567ef","keyword":"导模","originalKeyword":"导模"},{"id":"d9a0a513-d320-4f59-9cac-0ea6ed6a9b1e","keyword":"波导","originalKeyword":"波导"}],"language":"zh","publisherId":"yjyxs200906009","title":"平行<span style=\"color:red\">排列</span>向列相液晶的导波研究","volume":"24","year":"2009"},{"abstractinfo":"提出了一种采用垂直<span style=\"color:red\">排列</span>模式与混合<span style=\"color:red\">排列</span>模式相搭配的单倍盒间距的半透半反式液晶显示模式,液晶材料为负性.基于液晶分子的初始取向,反射区为混合<span style=\"color:red\">排列</span>模式,其关态和开态有效相位延迟在x/2和,x之间变化;透射区为平行<span style=\"color:red\">排列</span>模式,其关态和开态有效相位延迟在0和π之间变化.采用半波延迟膜补偿的方法可以使器件工作于常黑模式.对于透射区下层偏振片吸收轴和上层偏振片吸收轴分别平行和垂直放置时,下层的半波延迟膜光轴的方位角不同,导致光谱响应曲线和视角锥对比度分布不同.用扩展琼斯矩阵方法模拟分析了这两种器件结构的电光响应及光谱响应特性以及视角锥对比度分布特性.","authors":[{"authorName":"崔宏青","id":"dd29b35a-f223-4b72-8a92-8c0e07b8c68c","originalAuthorName":"崔宏青"},{"authorName":"冯亚云","id":"03ba3625-df4e-4a15-9a54-ca9b08125fdf","originalAuthorName":"冯亚云"},{"authorName":"陈冬静","id":"7f8ee655-eb25-44b4-9a8f-c62f2dfe2296","originalAuthorName":"陈冬静"},{"authorName":"任娇燕","id":"51084119-3e49-4be8-bc0d-f6c86484df1e","originalAuthorName":"任娇燕"},{"authorName":"凌志华","id":"4aa0971f-3466-4b7e-908d-aa506931c484","originalAuthorName":"凌志华"}],"doi":"10.3969/j.issn.1007-2780.2008.03.005","fpage":"281","id":"0b189273-3fc7-499a-95be-f3d1f3b010a1","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":"d0966ccd-429b-49e1-b2b7-79bc58911248","keyword":"半透半反式液晶显示","originalKeyword":"半透半反式液晶显示"},{"id":"e29c59a8-037e-4b5b-b8fa-0feaa0325571","keyword":"混合<span style=\"color:red\">排列</span>","originalKeyword":"混合排列"},{"id":"b6095f86-58d9-4a1a-888c-fae121a599a0","keyword":"垂直<span style=\"color:red\">排列</span>","originalKeyword":"垂直排列"}],"language":"zh","publisherId":"yjyxs200803005","title":"单倍盒厚间距垂直<span style=\"color:red\">排列</span>和混合<span style=\"color:red\">排列</span>半透半反式液晶显示模式","volume":"23","year":"2008"},{"abstractinfo":"本文运用Lattice-Boltzmann(LB)方法建立了宏观静止磁<span style=\"color:red\">流体</span>模型,提出磁性聚集体概念,充分考虑了磁性颗粒受到的各种内力与外力包括重力、布朗力、van der Waals相互作用及静磁相互作用,对无外加磁场及外加竖直均匀磁场时磁<span style=\"color:red\">流体</span>的结构进行了模拟,并分析了磁能与热能之比对磁<span style=\"color:red\">流体</span>系统中粒子分布形态的影响.模拟结果表明:无外加磁场时磁<span style=\"color:red\">流体</span>结构易失去稳定性,外加均匀磁场时磁<span style=\"color:red\">流体</span>粒子沿外磁场方向<span style=\"color:red\">排列</span>,随着磁热能比例的增大,外磁场对粒子分布的影响逐渐明显.","authors":[{"authorName":"宣益民","id":"bf5de529-b29c-4d81-870e-7d21e21deed7","originalAuthorName":"宣益民"},{"authorName":"叶萌","id":"2ee6eb38-90fa-40d2-9f4d-31a6d5535d52","originalAuthorName":"叶萌"},{"authorName":"李强","id":"a23ba220-6f0c-40b6-9c44-4e2d590e3b7f","originalAuthorName":"李强"}],"doi":"","fpage":"301","id":"daf0cfd0-97e6-4519-8e17-b33a996e2c7d","issue":"2","journal":{"abbrevTitle":"GCRWLXB","coverImgSrc":"journal/img/cover/GCRWLXB.jpg","id":"32","issnPpub":"0253-231X","publisherId":"GCRWLXB","title":"工程热物理学报   "},"keywords":[{"id":"a4dfd8e7-36cf-4d25-8632-2a19e6bb2669","keyword":"磁<span style=\"color:red\">流体</span>","originalKeyword":"磁流体"},{"id":"cbaf80a9-cede-4b2d-8e6a-d464c7faf582","keyword":"Lattice-Boltzmann","originalKeyword":"Lattice-Boltzmann"},{"id":"acb1742f-ec99-4d17-9d3f-4ab5e3afc6e6","keyword":"磁聚集体","originalKeyword":"磁聚集体"},{"id":"4dc296b9-b672-4c70-a1ae-e734e9f2e173","keyword":"磁相互作用","originalKeyword":"磁相互作用"},{"id":"efa360bd-345a-4422-9ae3-154f182afc52","keyword":"布朗力","originalKeyword":"布朗力"}],"language":"zh","publisherId":"gcrwlxb200502037","title":"磁<span style=\"color:red\">流体</span>结构的Lattice-Boltzmann方法模拟","volume":"26","year":"2005"}],"totalpage":390,"totalrecord":3891}