{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"压的发动机系统的全功率高度特性的基本规律和物理特征,并随之提供出飞行控制中的增压器子系统和活塞发动机的调节计划数据.","authors":[{"authorName":"<span style=\"color:red\">单</span><span style=\"color:red\">鹏</span>","id":"465bfe82-457f-4326-962c-fb8d1ac3f6a8","originalAuthorName":"单鹏"},{"authorName":"朱德轩","id":"d7754ac8-93fc-4521-9b33-a925ee72f7cd","originalAuthorName":"朱德轩"},{"authorName":"陈小龙","id":"b9be7430-19f9-4c0b-a320-01a58cce9d50","originalAuthorName":"陈小龙"},{"authorName":"李新民","id":"331729bf-8433-4c39-a265-82cf9cfb4a1d","originalAuthorName":"李新民"}],"doi":"","fpage":"1119","id":"d7744944-0dc8-4c16-94a8-48f842fed652","issue":"7","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":"8a451051-4cd1-4774-93bc-b4d7a7167199","keyword":"航空航天推进系统","originalKeyword":"航空航天推进系统"},{"id":"ae2f8d17-d821-4934-8187-e5419d4b434d","keyword":"总体设计","originalKeyword":"总体设计"},{"id":"e1baedff-5513-4f67-8a63-7f53d8a11409","keyword":"活塞式汽油机","originalKeyword":"活塞式汽油机"},{"id":"6b4d246a-7245-44e8-a322-849226200e62","keyword":"涡轮增压器","originalKeyword":"涡轮增压器"},{"id":"abdb1629-3fc0-4cc0-bf7d-f54e67d7f7fa","keyword":"高度特性","originalKeyword":"高度特性"}],"language":"zh","publisherId":"gcrwlxb200907011","title":"航空汽油机双级涡轮增压器系统的基本模型","volume":"30","year":"2009"},{"abstractinfo":"<正> <span style=\"color:red\">单</span>泡(或无泡沫)浮选法是一种在浮选研究领域内广为采用的研究方法。这种方法适用于研究各种浮选药剂(捕收剂、起泡剂和調整剂)对矿物的作用、研究药剂与矿物作用的动力学以及研究各种矿物的可浮性。在研究矿石的可选性时,它也可以用来研究矿物分选的条件。<span style=\"color:red\">单</span>泡浮选法对于研究具有起泡能力的捕收剂的性貭尤为适用,它可以避","authors":[{"authorName":"李明德","id":"03986947-c55b-4717-a7a8-6f13246b8572","originalAuthorName":"李明德"},{"authorName":"沈根生","id":"ef26744e-b7dd-4b85-a2f1-b7128608c776","originalAuthorName":"沈根生"}],"categoryName":"|","doi":"","fpage":"322","id":"e47499a1-46f5-497f-b9db-e14fef569ea5","issue":"3","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[],"language":"zh","publisherId":"0412-1961_1964_3_12","title":"Л型<span style=\"color:red\">单</span>泡浮选装置","volume":"7","year":"1964"},{"abstractinfo":"以甲苯、乙苯、异丙苯、叔丁基苯、氟苯等为硝化底物,通过混酸硝化得到这些<span style=\"color:red\">单</span>取代芳烃转化率最大时的混酸硝化强度φ. 运用密度泛涵理论,在B3LYP/6-311G* *水平上优化了9种单元芳烃的几何构型,计算苯环上C原子电荷分布. 讨论了9种取代基的定位效应,以苯环取代基以外环上C原子总净电荷QRΣC(2～6)表示<span style=\"color:red\">单</span>取代苯的硝化反应活性与硝化强度φ之间的关系. 实验结果表明,烷基苯、卤苯、硝基苯的硝化反应活性与其混酸硝化转化率达最大时的混酸硝化强度φ呈良好的线性关系.","authors":[{"authorName":"王鹏程","id":"adfd5211-5cb5-49ca-b056-0fea1413c0a9","originalAuthorName":"王鹏程"},{"authorName":"陈晶","id":"2b38f5b5-f93d-43a8-b595-5e47b491f078","originalAuthorName":"陈晶"},{"authorName":"陆明","id":"bb3df14f-3fc5-48f7-afb4-95ceef3d2a48","originalAuthorName":"陆明"}],"doi":"10.3724/SP.J.1095.2010.90575","fpage":"783","id":"7dd276f2-bd53-441f-bc20-df3cbfee9938","issue":"7","journal":{"abbrevTitle":"YYHX","coverImgSrc":"journal/img/cover/YYHX.jpg","id":"73","issnPpub":"1000-0518","publisherId":"YYHX","title":"应用化学"},"keywords":[{"id":"123da3bb-f481-4358-bca3-62a2dcd7ea35","keyword":"芳烃","originalKeyword":"芳烃"},{"id":"8771f4af-b966-4a2e-a361-456133bc1e5d","keyword":"混酸硝化","originalKeyword":"混酸硝化"},{"id":"a54cf61d-6114-4921-a6cf-8680e69737b6","keyword":"量子化学计算","originalKeyword":"量子化学计算"},{"id":"a7afbc9c-58b6-49a7-82e1-8e986e7ab226","keyword":"定位效应","originalKeyword":"定位效应"}],"language":"zh","publisherId":"yyhx201007008","title":"<span style=\"color:red\">单</span>取代芳烃的硝化","volume":"27","year":"2010"},{"abstractinfo":"本文提出一种基于<span style=\"color:red\">单</span>帧<span style=\"color:red\">单</span>曝光图像的气固两相流固相颗粒的速度场测量方法。通过控制相机的<span style=\"color:red\">单</span>次曝光时间获得流场中颗粒的<span style=\"color:red\">单</span>帧运动模糊图像，运用分水岭算法分割图像，提取颗粒，由自相关函数获得各颗粒的速度大小和方向，重建二维速度场。利用该方法对玻璃珠在空气中重力沉降的速度测量结果与理论值基本一致，矢量场与颗粒运动轨迹相符，说明该方法可以用于气固两相流速度场的测量。研究发现使用片光源比背光源能够获得更加准确的速度值。","authors":[{"authorName":"张晶晶","id":"7e76f0de-0437-437f-be88-a17d0848ace0","originalAuthorName":"张晶晶"},{"authorName":"范学良","id":"128afb6c-e2b1-4fe8-b201-3d87d906be98","originalAuthorName":"范学良"},{"authorName":"蔡小舒","id":"b5708db0-c007-44f7-9cd5-493558c69839","originalAuthorName":"蔡小舒"}],"doi":"","fpage":"79","id":"b5031825-aed1-4cc2-8320-fc76b5fe8729","issue":"1","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":"90230588-ada1-4ca3-a05d-cf82288dd6f4","keyword":"气固两相流","originalKeyword":"气固两相流"},{"id":"b892504a-dfa7-4576-884e-adb8fc828a9e","keyword":"速度场","originalKeyword":"速度场"},{"id":"f522a96d-bc31-49ff-bc28-d9b0f84a18d2","keyword":"运动模糊","originalKeyword":"运动模糊"},{"id":"352b8d9d-4814-410d-911d-0e55456ab067","keyword":"<span style=\"color:red\">单</span>帧<span style=\"color:red\">单</span>曝光","originalKeyword":"单帧单曝光"}],"language":"zh","publisherId":"gcrwlxb201201020","title":"<span style=\"color:red\">单</span>帧<span style=\"color:red\">单</span>曝光图像法测量气固两相流速度场","volume":"33","year":"2012"},{"abstractinfo":"以氨水为催化剂、正硅酸乙酯为硅源、醇为溶剂,采用改进的溶胶-凝胶工艺制备<span style=\"color:red\">单</span>分散SiO2微球,通过扫描电镜、激光粒度分析仪着重研究了正硅酸乙酯添加方式、反应温度、溶剂类型等<span style=\"color:red\">单</span>因素对SiO2的颗粒大小和形貌的影响.结果表明,正硅酸水解对醇溶剂是有选择性的,乙醇作为溶剂合成SiO2的<span style=\"color:red\">单</span>分散性和球形度最好.连续滴定和分步滴定更有利于<span style=\"color:red\">单</span>分散SiO2微球的形成.水解温度升高,生成的颗粒粒径将运渐增大,最佳反应温度为常温25℃或恒温水浴25～35℃.","authors":[{"authorName":"李朝毅","id":"f2209023-b6cb-47f4-8c5a-b2060f54443f","originalAuthorName":"李朝毅"},{"authorName":"段涛","id":"75b930bc-c382-4ccd-95c2-6718d174488e","originalAuthorName":"段涛"},{"authorName":"杨玉山","id":"9497f431-e0c3-43d8-afac-328b45a8cf73","originalAuthorName":"杨玉山"}],"doi":"","fpage":"151","id":"c0876092-dd59-4fd7-910b-a8003099ecc6","issue":"z2","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"ec696ee0-1a9f-4223-8009-9e5487ba524e","keyword":"SiO2","originalKeyword":"SiO2"},{"id":"21b65524-8787-400a-86c6-50d95e47e2c6","keyword":"<span style=\"color:red\">单</span>分散","originalKeyword":"单分散"},{"id":"ec3770df-6bb5-41e8-91bf-444c73cf5394","keyword":"微球","originalKeyword":"微球"},{"id":"993bd799-19a6-4bb5-862f-a60a1da2fbdc","keyword":"<span style=\"color:red\">单</span>因素","originalKeyword":"单因素"}],"language":"zh","publisherId":"cldb2009z2047","title":"<span style=\"color:red\">单</span>因素对<span style=\"color:red\">单</span>分散二氧化硅微球制备的影响","volume":"23","year":"2009"},{"abstractinfo":"在众多的量子信息方案中,光学方法是独特的,因为它们允许长距离的通信且提供量子计算新的方法.在光量子信息处理过程中,<span style=\"color:red\">单</span>光子源和探测器是很重要的一个方面.本文回顾了测量和产生<span style=\"color:red\">单</span>光子的方法,且讨论了它们在量子信息处理中的应用.","authors":[{"authorName":"李健军","id":"ad41dc37-2396-419c-9082-23264665272c","originalAuthorName":"李健军"},{"authorName":"郑小兵","id":"348ee814-258d-411d-8cc0-ebd209b2ddf1","originalAuthorName":"郑小兵"},{"authorName":"冯渝","id":"541e756e-f576-4640-9539-d56346b1e515","originalAuthorName":"冯渝"}],"doi":"10.3969/j.issn.1007-5461.2006.06.003","fpage":"766","id":"79f9fc4c-b9d8-4497-8cca-b26b2f6b7eaa","issue":"6","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":"84d0f353-8df1-4591-b4f6-13280eef5a35","keyword":"量子光学","originalKeyword":"量子光学"},{"id":"9252161e-93b0-44b2-a4f9-b5f5e9482bbd","keyword":"量子信息","originalKeyword":"量子信息"},{"id":"77bd9868-d9d9-480c-889e-0fd7727c081f","keyword":"<span style=\"color:red\">单</span>光子源","originalKeyword":"单光子源"},{"id":"098e8d0c-5310-46c9-810b-f20eaeb7637c","keyword":"<span style=\"color:red\">单</span>光子探测器","originalKeyword":"单光子探测器"}],"language":"zh","publisherId":"lzdzxb200606003","title":"<span style=\"color:red\">单</span>光子源和<span style=\"color:red\">单</span>光子探测器研究进展","volume":"23","year":"2006"},{"abstractinfo":"本文在<span style=\"color:red\">单</span>颗粒脱硫缩核模型的基础上分析了晶粒模型,并指出了原有晶粒模型中的不足之处,分析了晶粒初始孔隙率非均匀的原因,建立了一个初始孔隙率沿半径变化的改进晶粒模型.改进后的非均匀模型考虑到颗粒内部初始孔隙率的非均匀性,分析了非均匀初始孔隙率对脱硫效率和脱硫剂利用率的影响,并给出了初始非均匀孔隙率模型的完整的数学描述.","authors":[{"authorName":"陈兵","id":"eb31f83c-8d37-4557-bb14-9662c0ddbc81","originalAuthorName":"陈兵"},{"authorName":"张学学","id":"72bde4e5-fd45-4ee8-a6a6-20b57b504406","originalAuthorName":"张学学"}],"doi":"","fpage":"852","id":"a8db9f80-d60a-4ded-b8dd-4a3b6c1e1d5b","issue":"5","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":"3bb6ae3c-635b-4c35-9ae7-73fd43e4248c","keyword":"干法脱硫","originalKeyword":"干法脱硫"},{"id":"ad593b3b-46a2-4e8f-9b38-d94319d059ea","keyword":"晶粒模型","originalKeyword":"晶粒模型"},{"id":"ca95c9fc-e8f1-4886-ae96-98d9a8343eed","keyword":"孔隙率","originalKeyword":"孔隙率"},{"id":"4b21e7e3-186f-4647-8364-61c720c0699f","keyword":"数学模型","originalKeyword":"数学模型"}],"language":"zh","publisherId":"gcrwlxb200305040","title":"<span style=\"color:red\">单</span>颗粒脱硫反应模型分析","volume":"24","year":"2003"},{"abstractinfo":"介绍了<span style=\"color:red\">单</span>级衍射光栅的应用背景及其基本理论,分析了<span style=\"color:red\">单</span>级衍射光栅与传统黑白透射光栅的不同之处.阐述了<span style=\"color:red\">单</span>级衍射光栅的制作技术,分析了以电子束光刻、X射线光刻和微电镀技术为主的工艺路线的优缺点.综述了X光<span style=\"color:red\">单</span>级衍射光栅的发展历程以及存在的问题,并指出了其未来的研究方向.","authors":[{"authorName":"黄成龙","id":"df6a6102-022f-4f18-9d7a-534e98680b1f","originalAuthorName":"黄成龙"},{"authorName":"张继成","id":"f19a9672-e3f5-45c9-9990-9e580a253c19","originalAuthorName":"张继成"},{"authorName":"易勇","id":"010a2dca-e29c-4355-b506-2a7baa599813","originalAuthorName":"易勇"},{"authorName":"曹磊峰","id":"8d7a24fe-a8d3-4fb0-b077-3adf9cb64e7c","originalAuthorName":"曹磊峰"},{"authorName":"王红斌","id":"10e4a59d-6384-4959-8b5c-3b0d4d0fecf0","originalAuthorName":"王红斌"}],"doi":"","fpage":"164","id":"315b9a2e-0c15-47bd-bc52-c6ce4463a14d","issue":"z2","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"03ff18d1-1a57-4a38-9ce6-a76c5e178719","keyword":"X光<span style=\"color:red\">单</span>级衍射光栅","originalKeyword":"X光单级衍射光栅"},{"id":"5468ed6a-0e9c-45af-a0c0-7122a55c9156","keyword":"黑白透射光栅","originalKeyword":"黑白透射光栅"},{"id":"1100ff42-604e-4a7f-ba26-a657343d9f5d","keyword":"电子束光刻","originalKeyword":"电子束光刻"},{"id":"2ed0a952-1121-4ffc-b805-223fe2bcddde","keyword":"X射线光刻","originalKeyword":"X射线光刻"}],"language":"zh","publisherId":"cldb2013z2044","title":"X光<span style=\"color:red\">单</span>级衍射光栅的研究进展","volume":"27","year":"2013"},{"abstractinfo":"在信息存储和量子计算方面具有广阔应用前景的<span style=\"color:red\">单</span>分子磁体及相关研究中,应用各向异性显著的稀土离子以期提高<span style=\"color:red\">单</span>分子磁体自旋翻转能垒的研究倍受关注. 本文综述了稀土<span style=\"color:red\">单</span>分子磁体的研究进展,并着重介绍了单核、三核及四核镝配合物<span style=\"color:red\">单</span>分子磁体的磁学性质.","authors":[{"authorName":"林双燕","id":"b7b04e83-74b9-4920-aac0-4eb61c8f12cb","originalAuthorName":"林双燕"},{"authorName":"郭云南","id":"c83ec790-52e5-4725-9903-a61d6cd0fd6b","originalAuthorName":"郭云南"},{"authorName":"许公峰","id":"38bc81ba-5c02-48c7-a595-ff142111d265","originalAuthorName":"许公峰"},{"authorName":"唐金魁","id":"ed21c988-a431-4930-a49d-79fc84ff926b","originalAuthorName":"唐金魁"}],"doi":"10.3724/SP.J.1095.2010.00171","fpage":"1365","id":"54f81dd6-498b-4074-9828-cfe5a5a06523","issue":"12","journal":{"abbrevTitle":"YYHX","coverImgSrc":"journal/img/cover/YYHX.jpg","id":"73","issnPpub":"1000-0518","publisherId":"YYHX","title":"应用化学"},"keywords":[{"id":"93ebe5d9-ff17-4d2d-b216-1da25d24cd86","keyword":"<span style=\"color:red\">单</span>分子磁体","originalKeyword":"单分子磁体"},{"id":"3d89acc2-4be1-434c-805c-32dc2b760667","keyword":"稀土离子","originalKeyword":"稀土离子"},{"id":"a3f8e03d-41ea-496f-b877-eea2b10bc0d1","keyword":"弛豫","originalKeyword":"弛豫"},{"id":"78dd4608-6214-449d-b522-e1857ff48eea","keyword":"量子隧穿","originalKeyword":"量子隧穿"},{"id":"08d9bc96-884b-4bdd-aeb4-ec6f94175266","keyword":"磁性表征","originalKeyword":"磁性表征"}],"language":"zh","publisherId":"yyhx201012001","title":"稀土<span style=\"color:red\">单</span>分子磁体的研究进展","volume":"27","year":"2010"},{"abstractinfo":"本文以Maxwell电磁场理论为基础,对金属型<span style=\"color:red\">单</span>壁碳纳米管场发射阴极尖端附近的电场进行了计算,给出了不同结构<span style=\"color:red\">单</span>壁碳纳米管尖端附近的电场分布,发现场强沿管的径向及轴向方向随与管尖端距离的增加而迅速下降,说明了碳纳米管产生的激发场为极强的小范围局域场.通过计算不同几何尺寸<span style=\"color:red\">单</span>壁碳纳米管的场增强因子随其长度、半径的变化曲线,发现<span style=\"color:red\">单</span>壁碳纳米管的场增强因子数值非常大,并且根据曲线的变化规律可知,越细越长的<span style=\"color:red\">单</span>壁碳纳米管具有更大的场增强因子,同时也表明了<span style=\"color:red\">单</span>壁碳纳米管作为场发射阴极具有低的阈值和大的发射电流密度.本文所得结果为<span style=\"color:red\">单</span>壁碳纳米管做场发射材料提供了理论参考.","authors":[{"authorName":"郭连权","id":"f5ec3584-a2cb-47ac-97f9-a6234827c517","originalAuthorName":"郭连权"},{"authorName":"韩东","id":"2f2d1669-e63b-44da-9c37-c87150fd3c99","originalAuthorName":"韩东"},{"authorName":"马贺","id":"ae70f5d1-6de6-478e-9756-7e9ee37e4e04","originalAuthorName":"马贺"},{"authorName":"宋开颜","id":"b7fa1e4f-6dc4-40c4-a0df-5b60b3f7521c","originalAuthorName":"宋开颜"},{"authorName":"武鹤楠","id":"b78b7efc-a01d-4151-ba11-e22e2e824d1f","originalAuthorName":"武鹤楠"},{"authorName":"王帅","id":"4d6c4115-dc15-456a-ac8f-85d4de2ceeaa","originalAuthorName":"王帅"}],"doi":"10.3969/j.issn.1000-985X.2007.04.029","fpage":"847","id":"32d8f9cd-6893-41e3-9e8e-db6dcff7f499","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":"6051c97b-a6eb-45f1-936c-fe7edd0f931a","keyword":"<span style=\"color:red\">单</span>壁碳纳米管","originalKeyword":"单壁碳纳米管"},{"id":"17d37628-7329-4057-9645-0574f88daa36","keyword":"场增强因子","originalKeyword":"场增强因子"},{"id":"09b7ba74-8df1-4f7d-ba5e-aafe625ae853","keyword":"阈值","originalKeyword":"阈值"},{"id":"883132f1-2418-497f-ae73-5c386e9cf841","keyword":"场发射","originalKeyword":"场发射"}],"language":"zh","publisherId":"rgjtxb98200704029","title":"<span style=\"color:red\">单</span>壁碳纳米管场发射计算","volume":"36","year":"2007"}],"totalpage":617,"totalrecord":6168}