{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"以硝酸银为活化剂、葡萄糖为还原剂,对玻璃纤维化学镀银工艺进行正交优化,并研究了施镀时间对镀层电阻率的影响,得到最佳化学镀银工艺为:AgNO3 6 g/L,C6H12O6 8 g/L,NH3·H2O 100 mL/L,C2H5OH 100 mL/L,NaOH 4 g/L,KI 0.5～1.0 mg/L,温度30℃,时间25 min.结果表明,随施镀时间延长,镀银玻璃纤维的电阻率先减小后增大.在最佳工艺下制得的镀银玻璃纤维表面均匀、有光泽,结合力及导电性良好,厚度可达12 μm.","authors":[{"authorName":"司倩倩","id":"5ccdb114-3123-47f5-bdc5-d9433aec727b","originalAuthorName":"司倩倩"},{"authorName":"陈厚和","id":"ad4e6f5a-192c-4649-bad5-1f5b8b4b1f48","originalAuthorName":"陈厚和"},{"authorName":"张幺玄","id":"4f3c7eb5-8617-415a-9b22-b7264b8965be","originalAuthorName":"张幺玄"},{"authorName":"王雄彪","id":"5682970b-5e37-44ac-9e7b-5bdaa3a630fd","originalAuthorName":"王雄彪"},{"authorName":"<span style=\"color:red\">刘</span><span style=\"color:red\">艳</span><span style=\"color:red\">君</span>","id":"a7c95576-58ec-41c0-b535-ebbc1781bdf2","originalAuthorName":"刘艳君"},{"authorName":"江金金","id":"17e7d817-4c2d-4cd2-a814-2d9c6c6d1b58","originalAuthorName":"江金金"}],"doi":"","fpage":"25","id":"1f076f7f-06fb-4f69-9faa-4cc89ca3c207","issue":"12","journal":{"abbrevTitle":"DDYTS","coverImgSrc":"journal/img/cover/DDYTS.jpg","id":"21","issnPpub":"1004-227X","publisherId":"DDYTS","title":"电镀与涂饰   "},"keywords":[{"id":"20fca4fc-6a59-407c-9c70-7b70e8f00f21","keyword":"玻璃纤维","originalKeyword":"玻璃纤维"},{"id":"944997dc-c625-4664-b50b-145e95eca714","keyword":"化学银镀","originalKeyword":"化学银镀"},{"id":"e2b558aa-1c7b-4925-a5f5-39c74c4b7051","keyword":"导电性","originalKeyword":"导电性"},{"id":"0a9b9b9f-170b-4a2b-97d5-4d540a443580","keyword":"正交试验","originalKeyword":"正交试验"}],"language":"zh","publisherId":"ddyts201212008","title":"玻璃纤维化学镀银工艺的优化","volume":"31","year":"2012"},{"abstractinfo":"在常规晶化退火工艺条件下纳米双相永磁合金快淬非晶薄带的晶化过程中,a-Fe相通常在低温优先析出,这导致了a-Fe晶粒过于粗大并严重损害了材料磁性能.针对这一问题,近期有一些学者对极端晶化条件下非晶快淬薄带的晶化行为和机制进行了仔细的研究.本文对这些研究进行了综述和分析.","authors":[{"authorName":"张文旺","id":"a7081a01-39e5-4f14-8aaf-066c8328a1ff","originalAuthorName":"张文旺"},{"authorName":"潘晶","id":"c3a50303-310b-40cc-9414-e7489a8a0f17","originalAuthorName":"潘晶"},{"authorName":"<span style=\"color:red\">刘</span>新才","id":"bc147430-dfc3-4c23-a791-e75932fa3f01","originalAuthorName":"刘新才"},{"authorName":"李柱柏","id":"83eefbf5-fc40-42f1-a0dd-e9b02090c7d1","originalAuthorName":"李柱柏"},{"authorName":"戴浩","id":"cc43d01d-3a7d-4e38-9c18-052e5882bfc1","originalAuthorName":"戴浩"},{"authorName":"<span style=\"color:red\">刘</span><span style=\"color:red\">艳</span><span style=\"color:red\">君</span>","id":"7f0cd070-0f1e-498e-8c55-c0db7aa9726e","originalAuthorName":"刘艳君"}],"doi":"","fpage":"1876","id":"c44dbd7e-207d-4a27-a529-d65ff675d3ba","issue":"10","journal":{"abbrevTitle":"XYJSCLYGC","coverImgSrc":"journal/img/cover/XYJSCLYGC.jpg","id":"69","issnPpub":"1002-185X","publisherId":"XYJSCLYGC","title":"稀有金属材料与工程"},"keywords":[{"id":"06d20f7f-6c98-4915-a841-5792c3e329d2","keyword":"纳米双相永磁合金","originalKeyword":"纳米双相永磁合金"},{"id":"75edea43-0e80-4685-9524-f821eb7b98d9","keyword":"非晶快淬薄带","originalKeyword":"非晶快淬薄带"},{"id":"28da2329-945b-4c12-88fa-2bb280ce96da","keyword":"晶化工艺","originalKeyword":"晶化工艺"}],"language":"zh","publisherId":"xyjsclygc201110041","title":"极端晶化条件下纳米双相永磁合金快淬薄带的晶化研究","volume":"40","year":"2011"},{"abstractinfo":"以Nd9Fe85.5-xCoxB5.5(x=0,1,3,5)合金快淬薄带(钼辊表面速度V=35 m/s)为原料采用热压/热变形工艺制各了各向同性磁体.微观组织研究表明,含Co合金快淬薄带由大量非晶和少量a-(Fe,Co)和Nd2(Fe,Co)14B相组成,含Co量达到5at%的合金薄带中出现了亚稳相Nd3(Fe,Co)62B14,它在随后的热压/热变形过程中分解为a-(Fe,Co)和Nd2(Fe,Co)14B:添加Co元素显著减小了热变形磁体的晶粒尺寸,软磁性相与硬磁性相的平均晶粒尺寸分别从无Co合金磁体的61,168nm减小为含1at%Co合金磁体的24,50 nm.磁性能研究表明,与晶粒尺寸变化相对应,无Co合金以晶间静磁耦合作用为主,含Co合金以晶间交换耦合作用为主,并且随着Co含量的升高,交换耦合作用有所减弱,导致热变形磁体的矫顽力从无Co磁体的151 kA/m单调增大为含5at%Co磁体的218 kA/m.","authors":[{"authorName":"张文旺","id":"c9f866e9-15a5-4c7c-93c4-fa532359023e","originalAuthorName":"张文旺"},{"authorName":"潘晶","id":"5e6659a9-03ab-4d23-be74-b2a88582985e","originalAuthorName":"潘晶"},{"authorName":"<span style=\"color:red\">刘</span>新才","id":"b542d585-7351-4b84-a68b-0b9ee03f3084","originalAuthorName":"刘新才"},{"authorName":"郭鹏举","id":"40c91728-7db4-4e7f-8259-88af6d244ca9","originalAuthorName":"郭鹏举"},{"authorName":"<span style=\"color:red\">刘</span><span style=\"color:red\">艳</span><span style=\"color:red\">君</span>","id":"e4e64d52-ba6d-4f04-957d-f3288e9c29e4","originalAuthorName":"刘艳君"},{"authorName":"李柱柏","id":"7e13c0a6-30d0-426b-ad48-a9b0abb6aefb","originalAuthorName":"李柱柏"}],"doi":"","fpage":"600","id":"e91c1108-a011-4172-8d91-859d0390fa19","issue":"4","journal":{"abbrevTitle":"XYJSCLYGC","coverImgSrc":"journal/img/cover/XYJSCLYGC.jpg","id":"69","issnPpub":"1002-185X","publisherId":"XYJSCLYGC","title":"稀有金属材料与工程"},"keywords":[{"id":"37702e35-0388-4906-be70-89b196f43613","keyword":"Nd2Fe14B/α-Fe","originalKeyword":"Nd2Fe14B/α-Fe"},{"id":"2e7b0acb-40bd-4767-afe2-1438827b9da6","keyword":"热变形磁体","originalKeyword":"热变形磁体"},{"id":"5e3810ee-2d0e-4e8c-aa12-51253990bfba","keyword":"添加Co","originalKeyword":"添加Co"},{"id":"1ac7a05d-441b-4e71-b81e-d5c72b3459ba","keyword":"晶间相互作用","originalKeyword":"晶间相互作用"},{"id":"629f5f1f-a1a1-4bd4-a0ac-928147f3c6d3","keyword":"矫顽力","originalKeyword":"矫顽力"}],"language":"zh","publisherId":"xyjsclygc201104008","title":"Nd9Fe85.5-xCoxB5.5(x=0,1,3,5)合金快淬薄带及其热变形磁体的微观组织与矫顽力","volume":"40","year":"2011"},{"abstractinfo":"采用热压/热变形工艺制备纳米复合Nd9Fe84.5Co1B5.5永磁体,研究了热变形过程中的变形量对磁体平均晶粒尺寸的影响以及由此带来的晶间相互作用和矫顽力的变化。结果表明变形量54%的磁体中的硬、软磁性相的平均晶粒尺寸分别为61.0和51.8nm,与其热压状态时的两相平均晶粒尺寸（52.1和54.0nm）接近;而变形量74%的磁体中的硬、软磁性相的平均晶粒尺寸则分别显著减小至19.2和22.4nm。随着两相晶粒尺寸的显著细化,磁体中的晶间相互作用由以静磁耦合作用为主转变为以晶间交换耦合作用为主,这导致其矫顽力提高了64%。","authors":[{"authorName":"<span style=\"color:red\">刘</span><span style=\"color:red\">艳</span><span style=\"color:red\">君</span>","id":"430930c6-c1fb-45e4-ad6b-46d4438c9835","originalAuthorName":"刘艳君"},{"authorName":"潘晶","id":"c3fec0d5-f23b-47bc-8261-cfa1eb07482b","originalAuthorName":"潘晶"},{"authorName":"张文旺","id":"c5105c07-07a3-4f8c-bb89-51bb9fc446b8","originalAuthorName":"张文旺"},{"authorName":"林金荣","id":"60b5e003-ccb6-45ed-8dbd-249ff7459cac","originalAuthorName":"林金荣"},{"authorName":"<span style=\"color:red\">刘</span>新才","id":"1015762c-9a25-4336-ab2d-6022f6714cc6","originalAuthorName":"刘新才"}],"doi":"","fpage":"1727","id":"fce8c717-d84c-440e-8e80-c3a9d5cdaf79","issue":"9","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"5032f247-5e27-4fa6-9e90-fec817eeb5d9","keyword":"热压/热变形纳米复合磁体","originalKeyword":"热压/热变形纳米复合磁体"},{"id":"fe89b438-803f-48ea-a198-75fdabc2e099","keyword":"变形量","originalKeyword":"变形量"},{"id":"5e00229c-cf89-439a-949c-50ca0d36a549","keyword":"晶粒尺寸","originalKeyword":"晶粒尺寸"},{"id":"25cebaa7-e492-4267-babc-c11283e5f3e7","keyword":"晶间相互作用","originalKeyword":"晶间相互作用"},{"id":"c1a1a502-a849-463f-8ee5-93563346375e","keyword":"矫顽力","originalKeyword":"矫顽力"}],"language":"zh","publisherId":"gncl201109048","title":"变形量对热压/热变形纳米复合Nd_9Fe_（84.5）Co_1B_（5.5）永磁体晶粒尺寸和矫顽力的影响","volume":"42","year":"2011"},{"abstractinfo":"以活性<span style=\"color:red\">艳</span>橙溶液为模拟废水,通过H2O2/TiO2超声(US)协同作用光降解活性<span style=\"color:red\">艳</span>橙溶液,探讨了TiO2催化剂用量、H2O2用量、活性<span style=\"color:red\">艳</span>橙溶液的初始浓度、pH值、TiO2催化剂锻烧温度等对活性<span style=\"color:red\">艳</span>橙溶液降解率的影响,并比较了几种不同作用方式对活性<span style=\"color:red\">艳</span>橙溶液的降解效果.结果表明:UV/H2O2/TiO2/US协同作用降解活性<span style=\"color:red\">艳</span>橙溶液的效果最好;当活性<span style=\"color:red\">艳</span>橙溶液的初始浓度为20 mg·L-1,pH＝5,TiO2用量为0.4 g·L-1,H2O2用量为0.4 ml·L-1时,降解率可达92.06%.","authors":[{"authorName":"陈芳","id":"c018b667-4b1a-4338-b385-2d4c125d64b8","originalAuthorName":"陈芳"},{"authorName":"易回阳","id":"7008f390-2bc9-4a87-b6ed-71777a8de22a","originalAuthorName":"易回阳"},{"authorName":"吴一鸣","id":"bf3d8c22-2232-46d8-8102-d586676d01f0","originalAuthorName":"吴一鸣"}],"doi":"","fpage":"230","id":"b15922b8-beeb-4a39-9990-eeb51b375572","issue":"3","journal":{"abbrevTitle":"YXKXYGHX","coverImgSrc":"journal/img/cover/YXKXYGHX.jpg","id":"74","issnPpub":"1674-0475","publisherId":"YXKXYGHX","title":"影像科学与光化学   "},"keywords":[{"id":"88a482ad-2c4f-4805-8a02-a613239277fb","keyword":"超声波","originalKeyword":"超声波"},{"id":"dc948252-a79c-4d4a-9236-5ae4192b8f72","keyword":"TiO2","originalKeyword":"TiO2"},{"id":"d7b25bb4-ef3f-4423-a23b-6a3ab0c3ac88","keyword":"协同作用","originalKeyword":"协同作用"},{"id":"b41f2468-584b-4018-ac2c-90b0366a1c28","keyword":"活性<span style=\"color:red\">艳</span>橙","originalKeyword":"活性艳橙"},{"id":"510604c2-b4ac-4dd0-9b95-2ca3d2b4fc0b","keyword":"降解","originalKeyword":"降解"}],"language":"zh","publisherId":"ggkxyghx201003008","title":"H2O2/TiO2超声协同光降解活性<span style=\"color:red\">艳</span>橙的研究","volume":"28","year":"2010"},{"abstractinfo":"通过静态吸附实验方法,研究了有机改性凹凸棒石吸附活性<span style=\"color:red\">艳</span>蓝KN-R的动力学行为.研究结果表明:准二级动力学模型能很好地描述活性<span style=\"color:red\">艳</span>蓝KN-R在有机改性凹凸棒石上的动力学行为,平衡吸附量q2随着KN-R初始浓度、振荡速度、温度的增加而增加.有机改性凹凸棒石吸附活性<span style=\"color:red\">艳</span>蓝KN-R主要是外表面吸附,吸附活化能为39.2 kJ/mol,说明其为物理吸附、化学吸附综合作用的过程,其速率由化学过程与外扩散共同控制.","authors":[{"authorName":"张波","id":"f9714a14-4182-4326-b828-5048e81c1590","originalAuthorName":"张波"},{"authorName":"彭书传","id":"ee74e18c-2c8d-444d-b77e-7d7cc30a323f","originalAuthorName":"彭书传"},{"authorName":"王世亮","id":"2081aac6-56de-48dc-afb0-2a3156bf3ad2","originalAuthorName":"王世亮"},{"authorName":"张泽滨","id":"93899ca6-0450-415a-ace0-d2cad41cd09c","originalAuthorName":"张泽滨"},{"authorName":"吴敏伟","id":"7bd933ae-1226-4ef6-b7a1-c107f72d1daf","originalAuthorName":"吴敏伟"}],"doi":"","fpage":"122","id":"2ad6a218-c793-44a4-af6f-213768c81239","issue":"4","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"14b91fae-876a-4a73-aed5-77891101763e","keyword":"有机改性","originalKeyword":"有机改性"},{"id":"1314339a-4fe8-4996-83a2-feff1221503c","keyword":"凹凸棒","originalKeyword":"凹凸棒"},{"id":"35569aab-9a77-4074-b7c3-dbfeb611ffe3","keyword":"吸附","originalKeyword":"吸附"},{"id":"acbdf65e-ed32-4155-a86c-5a7cc298153f","keyword":"活性<span style=\"color:red\">艳</span>蓝KN-R","originalKeyword":"活性艳蓝KN-R"},{"id":"6d9a6b9d-9b2e-48a1-bd3d-bd6a2a787f27","keyword":"动力学","originalKeyword":"动力学"}],"language":"zh","publisherId":"cldb201304031","title":"有机改性凹凸棒石吸附活性<span style=\"color:red\">艳</span>蓝KN-R的动力学研究","volume":"27","year":"2013"},{"abstractinfo":"<span style=\"color:red\">刘</span>文中,关于贝氏体形成机制,包括形核过程的文献很少被引述。作者（<span style=\"color:red\">刘</span>等）的主要论点为贝氏体铁素体以无扩散、非切变机制在奥氏体内贫碳区形核,并未引述形成贫碳区的必要条件。本文作者强调,在钢及铜合金中,不可能由Spinodal分解和位错偏聚形成贫溶质区。<span style=\"color:red\">刘</span>等的理念未得到先进理论观点和精细实验结果的支持。在<span style=\"color:red\">刘</span>文中,据此对临界核心大小和形核能的计算并无显著意义,期望青年学者对贝氏体相变机制作进一步研究。","authors":[{"authorName":"徐祖耀","id":"f5bc6b26-ec4d-45e7-a1da-067daa9d3115","originalAuthorName":"徐祖耀"}],"doi":"","fpage":"158","id":"66a9e9e8-09a0-408c-8c33-bc00aeff35c0","issue":"2","journal":{"abbrevTitle":"CLRCLXB","coverImgSrc":"journal/img/cover/CLRCLXB.jpg","id":"15","issnPpub":"1009-6264","publisherId":"CLRCLXB","title":"材料热处理学报"},"keywords":[{"id":"5224cfe0-dd6d-4ccc-aac3-2bed80f388a5","keyword":"贝氏体形核","originalKeyword":"贝氏体形核"},{"id":"cae16aae-8a2b-43f5-9886-1ca5759c5972","keyword":"扩散机制","originalKeyword":"扩散机制"},{"id":"36bc9f8f-ee13-4c27-8020-c2c5b0dfca8f","keyword":"切变机制","originalKeyword":"切变机制"},{"id":"a3bb808d-ba7a-4c9a-90ff-d5e59a6a0f1a","keyword":"贫碳区","originalKeyword":"贫碳区"}],"language":"zh","publisherId":"jsrclxb201202033","title":"评<span style=\"color:red\">刘</span>宗昌等《贝氏体铁素体的形核》一文","volume":"33","year":"2012"},{"abstractinfo":"利用质子激发X射线荧光分析(PIXE)测试分析汝官瓷、张公巷窑青瓷和<span style=\"color:red\">刘</span>家门窑青瓷样品的主要化学组成,用多元统计判别分析方法对数据进行分析,以确定它们的分类和起源关系.结果表明:汝官瓷、张公巷窑青瓷和<span style=\"color:red\">刘</span>家门窑青瓷釉基本能很好的区分；但是胎区分得不是很理想,张公巷窑青瓷的胎可以和汝官瓷、<span style=\"color:red\">刘</span>家门窑青瓷胎很好的区分,汝官瓷胎和<span style=\"color:red\">刘</span>家门窑青瓷胎有个别样品不能分开.","authors":[{"authorName":"蔡敏敏","id":"bf1f4660-208a-4999-ac81-266bf48c5bcb","originalAuthorName":"蔡敏敏"},{"authorName":"李国霞","id":"f8d3a4dc-7472-4dd6-9382-9f4430feef58","originalAuthorName":"李国霞"},{"authorName":"赵维娟","id":"9572b140-eca3-4192-af6e-ab9fdb21502b","originalAuthorName":"赵维娟"},{"authorName":"李融武","id":"e2d1fb82-016c-4ae3-9ee6-0cabbe60a2a0","originalAuthorName":"李融武"},{"authorName":"赵文军","id":"ea875a05-c1f7-4a8f-b405-2005de7db87c","originalAuthorName":"赵文军"},{"authorName":"承焕生","id":"9ff5fa85-a1fb-4cd2-bdc3-3bd240fd6894","originalAuthorName":"承焕生"},{"authorName":"郭敏","id":"d4074d21-787e-429b-8123-a13fcf5ce433","originalAuthorName":"郭敏"}],"doi":"","fpage":"1363","id":"f1ea8842-b3fe-42a2-9557-aa4c186cac5a","issue":"6","journal":{"abbrevTitle":"GSYTB","coverImgSrc":"journal/img/cover/GSYTB.jpg","id":"36","issnPpub":"1001-1625","publisherId":"GSYTB","title":"硅酸盐通报   "},"keywords":[{"id":"d281b6ff-a4b5-41d8-ad69-47236e801de5","keyword":"汝官瓷","originalKeyword":"汝官瓷"},{"id":"adf8b648-9625-4b38-96ff-ec6174d0c5d4","keyword":"张公巷窑青瓷","originalKeyword":"张公巷窑青瓷"},{"id":"3a61e23c-a3f8-43e6-84fc-1b7cd4edef5b","keyword":"<span style=\"color:red\">刘</span>家门窑青瓷","originalKeyword":"刘家门窑青瓷"},{"id":"494e2983-99cd-4c53-a919-4bfad5b7c54a","keyword":"判别分析","originalKeyword":"判别分析"}],"language":"zh","publisherId":"gsytb201206005","title":"汝官瓷、张公巷窑青瓷和<span style=\"color:red\">刘</span>家门窑青瓷的判别分析研究","volume":"31","year":"2012"},{"abstractinfo":"采用湿相转化法制备了以活性<span style=\"color:red\">艳</span>蓝KN-R为印迹分子的醋酸纤维素(CA)-聚偏二氟乙烯(PVDF)分子印迹膜(MIM).实验结果表明在一定的制备条件下可制得具有较大吸附结合率的MIM,此时的铸膜液组成为:活性<span style=\"color:red\">艳</span>蓝KN-R质量浓度硼ω1为0.1%,共混组成比ω(CA):ω(PVDF)=9.5:0.5,聚合物质量浓度ωp,为14%,添加剂LiCl质量浓度ωa为7.5%.所制得的MIM是一种特异分子吸附膜,对印迹分子具有亲和性,其分离机理属于延迟渗透机理.在一定范围(0～0.1%)内,随着印迹分子活性<span style=\"color:red\">艳</span>蓝KN-R质量浓度增大,MIM的吸附选择性提高.由吸附焓△H0及MIM与印迹分子间结合力强弱的测定结果可知,MIM与印迹分子之间的结合作用力以疏水/范德华力与氢键作用为主.","authors":[{"authorName":"李婧娴","id":"adc39f6d-454c-4444-b471-9abaf319eb20","originalAuthorName":"李婧娴"},{"authorName":"董声雄","id":"974c9bac-83ba-4efc-8746-ddffb5b2a98e","originalAuthorName":"董声雄"},{"authorName":"苗晶","id":"40757d46-48bb-449f-a6f5-b995922abdcb","originalAuthorName":"苗晶"}],"doi":"10.3969/j.issn.1007-8924.2009.01.002","fpage":"8","id":"00fd3ec0-448e-4ff2-a4bf-8e3a505411fa","issue":"1","journal":{"abbrevTitle":"MKXYJS","coverImgSrc":"journal/img/cover/MKXYJS.jpg","id":"54","issnPpub":"1007-8924","publisherId":"MKXYJS","title":"膜科学与技术   "},"keywords":[{"id":"ab540a8e-4a22-4c27-9032-8794df61b554","keyword":"湿相转化法","originalKeyword":"湿相转化法"},{"id":"f919dd35-564c-46a0-8918-ae39230d5374","keyword":"活性<span style=\"color:red\">艳</span>蓝KN-R","originalKeyword":"活性艳蓝KN-R"},{"id":"034d028a-41f9-48db-b3e0-c9cfdc9d8c26","keyword":"分子印迹膜(MIM)","originalKeyword":"分子印迹膜(MIM)"},{"id":"f3c4f724-a1ba-4f6c-998c-93cc8914abec","keyword":"共混膜","originalKeyword":"共混膜"}],"language":"zh","publisherId":"mkxyjs200901002","title":"活性<span style=\"color:red\">艳</span>蓝KN-R分子印迹CA/PVDF共混膜的制备及性能表征","volume":"29","year":"2009"},{"abstractinfo":"采用溶胶-凝胶法制备了不掺杂和掺杂铝离子、镧离子以及两种离子共掺杂的ZnO,并用X射线衍射(XRD),高分辨透射电镜(HRTEM),紫外-可见(UV-Vis)吸收光谱对其进行了表征.用紫外灯作为光源,一定浓度的活性<span style=\"color:red\">艳</span>蓝X-BR溶液为光催化反应模型污染物,研究了各种离子掺杂ZnO的光催化性能,考察了掺杂量对降解率的影响.结果表明,镧离子和铝离子掺杂浓度为2 at%和3 at%的共搀杂ZnO的光催化性能最好;在室温下,加入催化剂浓度为0.1 g/L,降解时间为45 min时,对活性<span style=\"color:red\">艳</span>蓝X-BR溶液的降解率达到96.63%.","authors":[{"authorName":"周银","id":"490f2150-e783-47a1-8704-d2f879571574","originalAuthorName":"周银"},{"authorName":"王宇","id":"9889757b-2987-4b5e-83bb-e106ffd7f6a1","originalAuthorName":"王宇"},{"authorName":"卢士香","id":"8f1b321e-def4-42df-9c69-db5772180c51","originalAuthorName":"卢士香"},{"authorName":"徐文国","id":"3d5fd658-3b2e-4813-b421-3c76f27b6af4","originalAuthorName":"徐文国"},{"authorName":"苏苏","id":"a70d8526-7852-4b5e-883c-6555b9987294","originalAuthorName":"苏苏"}],"doi":"","fpage":"998","id":"6ec05008-600c-430c-90c0-d112e4b2ec7d","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":"e960863a-1c4b-48e3-9edd-d7d235e981ea","keyword":"溶胶-凝胶","originalKeyword":"溶胶-凝胶"},{"id":"eac95f4b-6141-422d-bc5f-f6bcf0341d93","keyword":"纳米氧化锌","originalKeyword":"纳米氧化锌"},{"id":"3cc63b6d-1577-4565-bd8c-a1ef019394f0","keyword":"光催化降解","originalKeyword":"光催化降解"},{"id":"7b88e351-38b3-48ee-96b5-d6da24950946","keyword":"镧铝共掺杂","originalKeyword":"镧铝共掺杂"}],"language":"zh","publisherId":"rgjtxb98200904041","title":"La3+,Al3+共掺杂纳米ZnO光催化降解活性<span style=\"color:red\">艳</span>蓝X-BR研究","volume":"38","year":"2009"}],"totalpage":6,"totalrecord":59}