{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"本文采用<span style=\"color:red\">水平</span><span style=\"color:red\">沉积</span>方法,制作出各种胶体晶体薄膜.以聚苯乙烯微球为构建单元,制作了多种二元胶体晶体和非单一平面的胶体晶体.为实现太赫兹光子晶体波导,还采用这一方法将线缺陷植入胶体晶体.结果显示通过该方法可以获得很好的有序结构,说明<span style=\"color:red\">水平</span><span style=\"color:red\">沉积</span>方法可以广泛于各种胶体晶体制作.","authors":[{"authorName":"万勇","id":"9b637b2c-1129-496e-8b3d-aa6288e17b7f","originalAuthorName":"万勇"},{"authorName":"赵修松","id":"74e61f7f-4786-4e38-bfae-0c7bd0bc7f9e","originalAuthorName":"赵修松"},{"authorName":"蔡仲雨","id":"da8334b9-37d1-4e02-a41b-594ce4bf4bfb","originalAuthorName":"蔡仲雨"},{"authorName":"李洪亮","id":"ae4a450f-3add-4563-867d-b47857ba7eca","originalAuthorName":"李洪亮"},{"authorName":"夏临华","id":"ea49d2e3-4efd-4b3d-a7bd-3806bbc23071","originalAuthorName":"夏临华"}],"doi":"","fpage":"1295","id":"b3748ccc-0ffc-408c-bf45-cc774f87b8c8","issue":"5","journal":{"abbrevTitle":"RGJTXB","coverImgSrc":"journal/img/cover/RGJTXB.jpg","id":"57","issnPpub":"1000-985X","publisherId":"RGJTXB","title":"人工晶体学报"},"keywords":[{"id":"7134116f-44f4-4487-8337-826829a52c00","keyword":"光子晶体","originalKeyword":"光子晶体"},{"id":"57de501a-a0aa-4fb1-b501-55789d6f220d","keyword":"微球","originalKeyword":"微球"},{"id":"31d15dd8-92ff-40c5-af93-f01e934252f3","keyword":"<span style=\"color:red\">水平</span><span style=\"color:red\">沉积</span>","originalKeyword":"水平沉积"}],"language":"zh","publisherId":"rgjtxb98201105041","title":"利用<span style=\"color:red\">水平</span><span style=\"color:red\">沉积</span>法制作PS微球二元胶体薄膜及其它复杂结构","volume":"40","year":"2011"},{"abstractinfo":"采用<span style=\"color:red\">水平</span><span style=\"color:red\">沉积</span>方法,制作了多种FCC结构的聚苯乙烯(PS)胶体晶体,并实现了直径在2-10 μm一类大球的自组装.以PS胶体晶体为模板,采用垂直<span style=\"color:red\">沉积</span>方法得到了二氧化硅(SiO2)胶体晶体的反相结构.文中还对两种<span style=\"color:red\">沉积</span>方法进行了比较.","authors":[{"authorName":"万勇","id":"887599c6-a9b8-487f-bbca-eab601df1fea","originalAuthorName":"万勇"},{"authorName":"蔡仲雨","id":"655e3a23-acf5-48ba-a9a8-5232c38363e7","originalAuthorName":"蔡仲雨"},{"authorName":"赵修松","id":"bfda3034-85b0-46b8-9624-0be6cd016a5f","originalAuthorName":"赵修松"},{"authorName":"李洪亮","id":"88470895-4fd6-4fc3-8ac3-07a60067c4d1","originalAuthorName":"李洪亮"},{"authorName":"夏临华","id":"16165db9-2dbd-415e-836c-aa4b288ee241","originalAuthorName":"夏临华"}],"doi":"","fpage":"150","id":"0cfd6683-c720-40b3-ba93-79da2e7d3066","issue":"1","journal":{"abbrevTitle":"RGJTXB","coverImgSrc":"journal/img/cover/RGJTXB.jpg","id":"57","issnPpub":"1000-985X","publisherId":"RGJTXB","title":"人工晶体学报"},"keywords":[{"id":"3f5137b0-a876-4fe5-817b-4f0d16f0c2e8","keyword":"聚苯乙烯","originalKeyword":"聚苯乙烯"},{"id":"ac65466e-1546-4d0c-8a0e-7cc781239f99","keyword":"微球","originalKeyword":"微球"},{"id":"f9ec7a81-896a-4e5b-bab8-aca179880661","keyword":"<span style=\"color:red\">水平</span><span style=\"color:red\">沉积</span>","originalKeyword":"水平沉积"},{"id":"7c2e835d-4516-4468-a612-b33d5918e560","keyword":"垂直<span style=\"color:red\">沉积</span>","originalKeyword":"垂直沉积"}],"language":"zh","publisherId":"rgjtxb98201101029","title":"PS微球胶体晶体及其反相SiO2结构的制备和表征","volume":"40","year":"2011"},{"abstractinfo":"在MOCVD反应器中,针对GaN生长中的TMGa分子,推导出热泳力、热泳速度以及扩散速度的计算公式.在低温区,热泳速度大于扩散速度；在高温区则相反.影响热泳力的主要因素为温度梯度和分子直径.<span style=\"color:red\">水平</span>式反应器内,粒子同时受到热泳速度和扩散速度的影响.在只考虑组分输运以及包括化学反应等两种情况下,通过改变反应器上壁面温度,模拟得到<span style=\"color:red\">水平</span>式反应器中热泳力对<span style=\"color:red\">沉积</span>速率以及反应物粒子浓度分布的影响.并与文献中的实验数据对比,验证了模拟结果的正确性.结果显示,由于热泳力的影响,在相同操作条件下高温区H2等小直径粒子的质量分数增大、TMGa和NH3等大分子粒子的质量分数减小.从提高生长速率的角度,需减小上下壁面温度梯度；从<span style=\"color:red\">沉积</span>均匀性的角度,应使到达下游的反应粒子数增多,故需增大上下壁面温度梯度.","authors":[{"authorName":"于海群","id":"63182833-7f50-4ebe-81c6-117a17b625fd","originalAuthorName":"于海群"},{"authorName":"左然","id":"a657868f-fcab-4b2b-b458-fda39afbd5c1","originalAuthorName":"左然"},{"authorName":"陈景升","id":"b749798b-630e-4d62-b6d3-6f1e5ae62d47","originalAuthorName":"陈景升"},{"authorName":"彭鑫鑫","id":"0b3d2b5a-7619-4f59-a633-b32dc2d1030c","originalAuthorName":"彭鑫鑫"}],"doi":"","fpage":"1033","id":"78eab9d8-2728-4f89-b0f6-68bc754957f5","issue":"4","journal":{"abbrevTitle":"RGJTXB","coverImgSrc":"journal/img/cover/RGJTXB.jpg","id":"57","issnPpub":"1000-985X","publisherId":"RGJTXB","title":"人工晶体学报"},"keywords":[{"id":"4bdc661b-de21-40dc-a013-97b916e1deba","keyword":"MOCVD","originalKeyword":"MOCVD"},{"id":"bc09f5eb-2cf5-4e79-b4dc-d25cea619935","keyword":"热泳力","originalKeyword":"热泳力"},{"id":"60f843e0-2add-4603-964b-193d538b5564","keyword":"温度梯度","originalKeyword":"温度梯度"},{"id":"e6125166-9f36-4083-b602-19cef2b2748d","keyword":"生长速率","originalKeyword":"生长速率"},{"id":"73da7b49-21b8-4ef9-bfc2-7b70624d55c2","keyword":"数值模拟","originalKeyword":"数值模拟"}],"language":"zh","publisherId":"rgjtxb98201104042","title":"MOCVD<span style=\"color:red\">水平</span>式反应器中热泳力对<span style=\"color:red\">沉积</span>过程中反应前体浓度分布的影响分析及数值模拟","volume":"40","year":"2011"},{"abstractinfo":"<span style=\"color:red\">水平</span>定向凝固法是制备低位错单晶体的重要方法,论述了<span style=\"color:red\">水平</span>定向凝固法的优点和缺点,并报道了<span style=\"color:red\">水平</span>定向凝固法的特点,温度分布,以及<span style=\"color:red\">水平</span>定向凝固法的数字模拟的方面的工作.","authors":[{"authorName":"韩杰才","id":"59631062-fd87-4203-ba0e-51679b545f4a","originalAuthorName":"韩杰才"},{"authorName":"李长青","id":"435c483d-7d73-457c-bc60-26bfcf880245","originalAuthorName":"李长青"},{"authorName":"张明福","id":"ee95895c-af81-4f3d-ad65-30e5a48e9bad","originalAuthorName":"张明福"},{"authorName":"左洪波","id":"30f3da00-876a-4ffa-99be-52aaac68e82d","originalAuthorName":"左洪波"},{"authorName":"孟松鹤","id":"9a9ae843-7649-4051-befc-a43bd48e44b4","originalAuthorName":"孟松鹤"},{"authorName":"姚泰","id":"77a579f9-05e4-4078-9817-6a993f3cb411","originalAuthorName":"姚泰"}],"doi":"","fpage":"10","id":"445bf5d8-c514-4c80-a72f-9b637845db9b","issue":"7","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"58ac4e4d-621a-421b-bd18-b642dee9e462","keyword":"<span style=\"color:red\">水平</span>定向凝固法单","originalKeyword":"水平定向凝固法单"},{"id":"6808b7fe-5b0b-4f45-a4bf-2495f983fa16","keyword":"晶生长","originalKeyword":"晶生长"},{"id":"ca5365b9-5d86-4e45-a0f6-b75c19b89b33","keyword":"数字模拟","originalKeyword":"数字模拟"}],"language":"zh","publisherId":"cldb200607003","title":"单晶<span style=\"color:red\">水平</span>定向凝固法","volume":"20","year":"2006"},{"abstractinfo":"为了研究轧机振动特性并找到振源,根据轧制界面非线性粘滑摩擦特性,建立了轧辊<span style=\"color:red\">水平</span>方向摩擦颤振模型、接轴不平衡力引起的工作辊<span style=\"color:red\">水平</span>方向\"跳振\"模型.模型仿真表明,当外扰力幅较小时系统呈现概周期运动,外扰力幅较大时系统呈混沌状态;当机座有间隙时轧辊<span style=\"color:red\">水平</span>振动波形有削顶现象,系统动力学变差;当采取消除间隙、消除接轴不平衡力措施后,系统的动力学性能得到改善.实测表明,当采取相应措施后振动强度减弱.","authors":[{"authorName":"范小彬","id":"d4f34ee3-1a5b-4e9e-b9ce-ef62a6203bf9","originalAuthorName":"范小彬"},{"authorName":"臧勇","id":"a166352a-6484-403d-819e-f01922df3577","originalAuthorName":"臧勇"},{"authorName":"王会刚","id":"2fe480b0-93dd-4ff5-b83a-0be9146e99e8","originalAuthorName":"王会刚"}],"doi":"","fpage":"62","id":"1bb9eee4-4659-4509-a6b7-3d47cad8edf7","issue":"9","journal":{"abbrevTitle":"GT","coverImgSrc":"journal/img/cover/GT.jpg","id":"27","issnPpub":"0449-749X","publisherId":"GT","title":"钢铁"},"keywords":[{"id":"f268605b-1dd8-4a5f-abde-959eaf4cb2d2","keyword":"轧机","originalKeyword":"轧机"},{"id":"d747722b-f3c9-4a85-85d4-5c77fc9d06b5","keyword":"颤振","originalKeyword":"颤振"},{"id":"880fabad-6539-4b97-8636-560790da7c10","keyword":"碰撞","originalKeyword":"碰撞"},{"id":"db548b00-9536-4ec4-b8f5-02cac209c9ff","keyword":"时频分析","originalKeyword":"时频分析"}],"language":"zh","publisherId":"gt201009013","title":"热连轧机<span style=\"color:red\">水平</span>振动特性研究","volume":"45","year":"2010"},{"abstractinfo":"根据轧制界面非线性粘滑摩擦特性，建立了轧辊<span style=\"color:red\">水平</span>方向摩擦颤振模型、接轴不平衡力引起的工作辊<span style=\"color:red\">水平</span>方向“跳振”模型。数值仿真表明，当外扰力幅较小时系统呈现概周期运动，外扰力幅较大时系统呈混沌状态；当机座有间隙时轧辊<span style=\"color:red\">水平</span>振动波形有削顶现象，系统动力学变差；当采取消除间隙、消除接轴不平衡力措施后，系统的动力学性能得到改善。实测表明，当采取相应措施后振动强度减弱。","authors":[{"authorName":"范小彬\t臧勇\t王会刚","id":"9131a00e-638e-41d3-b42f-8a03dd2d27b1","originalAuthorName":"范小彬\t臧勇\t王会刚"}],"categoryName":"|","doi":"","fpage":"62","id":"2a1a298a-36e8-4e16-92cd-268e731fb379","issue":"9","journal":{"abbrevTitle":"GT","coverImgSrc":"journal/img/cover/GT.jpg","id":"27","issnPpub":"0449-749X","publisherId":"GT","title":"钢铁"},"keywords":[{"id":"febe1e5d-28b0-4587-98dc-bdd48b522267","keyword":"轧机;颤振;碰撞;时频分析","originalKeyword":"轧机;颤振;碰撞;时频分析"}],"language":"zh","publisherId":"0449-749X_2010_9_8","title":"热连轧机<span style=\"color:red\">水平</span>振动特性研究","volume":"45","year":"2010"},{"abstractinfo":"介绍了<span style=\"color:red\">水平</span>连铸工艺参数--反推的各种型式,分析了反推在<span style=\"color:red\">水平</span>连铸生产中的作用,讨论了影响反推大小的各种因素以及反推大小对铸坯质量的影响.","authors":[{"authorName":"周维汉","id":"b73c5d79-216a-4ceb-984a-bc94e3bb4408","originalAuthorName":"周维汉"},{"authorName":"杨扬","id":"f23534b9-9014-47c1-813d-b196228f5874","originalAuthorName":"杨扬"},{"authorName":"钟春生","id":"7aafb553-198a-4d7a-92e9-183a46bc6381","originalAuthorName":"钟春生"}],"doi":"10.3969/j.issn.1001-1447.2005.03.010","fpage":"35","id":"da6bcb55-e5c1-4a90-a18b-c7d23fec32b3","issue":"3","journal":{"abbrevTitle":"GTYJ","coverImgSrc":"journal/img/cover/GTYJ.jpg","id":"29","issnPpub":"1001-1447","publisherId":"GTYJ","title":"钢铁研究"},"keywords":[{"id":"44c266b6-bcd5-4df4-8db5-71381756398f","keyword":"<span style=\"color:red\">水平</span>连铸","originalKeyword":"水平连铸"},{"id":"8c7e4a3c-04b4-4a0c-9590-2e73a4e755dc","keyword":"反推","originalKeyword":"反推"},{"id":"36b65c66-fde2-4368-a4ff-3d731612c493","keyword":"拉坯曲线","originalKeyword":"拉坯曲线"},{"id":"3604d6f9-f6fe-4666-b808-cf57f9a426a2","keyword":"拉坯阻力","originalKeyword":"拉坯阻力"}],"language":"zh","publisherId":"gtyj200503010","title":"对<span style=\"color:red\">水平</span>连铸工艺参数--反推的研究","volume":"33","year":"2005"},{"abstractinfo":"为了提高UR、UF<span style=\"color:red\">水平</span>轧辊利用率,分析了轧辊的装配结构与各类参数,对立辊R值、辊环二楞台直径、轧辊标定参数等进行了优化.结果表明:通过轧辊参数的优化,UR、UF<span style=\"color:red\">水平</span>轧辊的最小使用直径不但可达到设计值1 040 mm,还可减小至1 020mm,增加了轧辊的使用次数,UR、UF<span style=\"color:red\">水平</span>轧辊的利用率提高了3.5％.","authors":[{"authorName":"王彬","id":"ddbbc5c5-3d66-437c-8381-a67d932f629e","originalAuthorName":"王彬"},{"authorName":"石春有","id":"239fb6bd-4170-40e5-9070-f73b257ed419","originalAuthorName":"石春有"}],"doi":"","fpage":"50","id":"9a72e6bb-44cf-4615-9498-9c000826c821","issue":"6","journal":{"abbrevTitle":"GTYJ","coverImgSrc":"journal/img/cover/GTYJ.jpg","id":"29","issnPpub":"1001-1447","publisherId":"GTYJ","title":"钢铁研究"},"keywords":[{"id":"42aaf231-2abb-46e2-9ee2-33e8e716c496","keyword":"<span style=\"color:red\">水平</span>轧辊","originalKeyword":"水平轧辊"},{"id":"f374c360-f84f-41ae-b236-0d18ad2f50ae","keyword":"辊环","originalKeyword":"辊环"},{"id":"0840ab16-c0d6-4c74-bb10-b487194ff03d","keyword":"芯轴","originalKeyword":"芯轴"},{"id":"048c7e08-5739-4812-9b03-040ce0243297","keyword":"立辊","originalKeyword":"立辊"}],"language":"zh","publisherId":"gtyj201306014","title":"提高UR、UF<span style=\"color:red\">水平</span>轧辊利用率的探讨","volume":"41","year":"2013"},{"abstractinfo":"本文对影响<span style=\"color:red\">水平</span>连铸结晶器使用寿命的因素进行叙述和分析,并提出相应的改进措施.","authors":[{"authorName":"吕士忠","id":"cf1c4fbf-e869-4123-986f-8ffef106a666","originalAuthorName":"吕士忠"}],"doi":"10.3969/j.issn.1005-4006.2002.02.011","fpage":"27","id":"3996adcd-4e8f-4d97-bfed-8e5968c10b5d","issue":"2","journal":{"abbrevTitle":"LZ","coverImgSrc":"journal/img/cover/LZ.jpg","id":"52","issnPpub":"1005-4006","publisherId":"LZ","title":"连铸"},"keywords":[{"id":"63b2272b-15d5-47b3-b613-0a86651c3add","keyword":"","originalKeyword":""}],"language":"zh","publisherId":"lz200202011","title":"<span style=\"color:red\">水平</span>连铸高效结晶器研究","volume":"","year":"2002"},{"abstractinfo":"在传统酸性镀铜液中加入玻璃球,利用SEM和XRD考察了玻璃球数量与震荡频率对机械研磨电镀工艺的影响,并探讨了<span style=\"color:red\">水平</span>震荡频率和玻璃球数量对镀层微观结构的影响机理.实验结果表明:固定玻璃球数量为80个,震荡频率为2.5～4.2 Hz时,所得镀层的晶粒尺寸随着震荡频率的增加而显著降低;固定<span style=\"color:red\">水平</span>震荡频率为4.2 Hz,玻璃球数量为40～120个时,随着玻璃球数量的增加,所得镀层的晶粒尺寸先降低后略有增大,但仍明显小于传统镀层;<span style=\"color:red\">水平</span>震荡机械研磨电镀铜层具有(111)择优取向,但择优取向程度受<span style=\"color:red\">水平</span>震荡条件影响.","authors":[{"authorName":"吕小莉","id":"699d6495-5f98-414f-8936-48675a42077f","originalAuthorName":"吕小莉"},{"authorName":"冯长杰","id":"cebcf31d-e833-43f1-bd17-ffe2953aaa03","originalAuthorName":"冯长杰"},{"authorName":"钟小荣","id":"20163fae-4787-4302-8139-08a27280c145","originalAuthorName":"钟小荣"},{"authorName":"万小欢","id":"f731d929-7c95-49e7-b84d-d33aab0a74f2","originalAuthorName":"万小欢"},{"authorName":"杜楠","id":"e7d1f45a-0c69-450a-abe2-14dae80c96a7","originalAuthorName":"杜楠"}],"doi":"10.3969/j.issn.1001-3660.2010.03.021","fpage":"74","id":"621dbe54-82a9-46b9-9444-d08611e6f79d","issue":"3","journal":{"abbrevTitle":"BMJS","coverImgSrc":"journal/img/cover/BMJS.jpg","id":"3","issnPpub":"1001-3660","publisherId":"BMJS","title":"表面技术   "},"keywords":[{"id":"701ae846-a2f8-41e7-a213-6ad5c842a93b","keyword":"<span style=\"color:red\">水平</span>震荡","originalKeyword":"水平震荡"},{"id":"88e6c713-6efe-4f00-bb53-e1e2dcc0de9b","keyword":"机械研磨","originalKeyword":"机械研磨"},{"id":"35003f89-650a-44c3-be9c-b81b3f194f9e","keyword":"电<span style=\"color:red\">沉积</span>","originalKeyword":"电沉积"},{"id":"d8efcc07-207c-4c25-b101-732c604899e5","keyword":"镀铜","originalKeyword":"镀铜"},{"id":"27385772-292b-4a31-b9d5-4b5a80b0070c","keyword":"镀层结构","originalKeyword":"镀层结构"}],"language":"zh","publisherId":"bmjs201003021","title":"<span style=\"color:red\">水平</span>震荡机械研磨电镀铜工艺研究","volume":"39","year":"2010"}],"totalpage":1515,"totalrecord":15143}