{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"","authors":[{"authorName":"王小风","id":"4889e5ca-2c30-45ae-bd67-f2c7be2269ad","originalAuthorName":"王小风"},{"authorName":"秦宏伟","id":"3a2fdd11-da09-43ae-abe7-0edcfe23c281","originalAuthorName":"秦宏伟"},{"authorName":"裴金亮","id":"52e592e7-5fac-4a9d-a3b8-41b3755acda3","originalAuthorName":"裴金亮"},{"authorName":"陈艳平","id":"ee1e84bd-733a-46dc-84e7-8149fae85855","originalAuthorName":"陈艳平"},{"authorName":"李玲","id":"e48ccdc8-6aef-42c3-bad8-83501a10d0b8","originalAuthorName":"李玲"},{"authorName":"谢继浩","id":"ebceee80-df38-4a10-9553-9f35919fe41f","originalAuthorName":"谢继浩"},{"authorName":"胡季帆","id":"934cc1ac-2808-4cdc-8007-6e90af68348f","originalAuthorName":"胡季帆"}],"doi":"10.1016/S1002-0721(16)60082-0","fpage":"704","id":"d08e9f63-b814-4d52-9072-3fcb12093e5e","issue":"7","journal":{"abbrevTitle":"XTXBYWB","coverImgSrc":"journal/img/cover/XTXBEN.jpg","id":"66","issnPpub":"1002-0721","publisherId":"XTXBYWB","title":"稀土学报(英文版)"},"keywords":[{"id":"cdfb5850-4824-4abe-9bf4-d64f129f733b","keyword":"","originalKeyword":""}],"language":"zh","publisherId":"zgxtxb-e201607008","title":"","volume":"34","year":"2016"},{"abstractinfo":"用第一性原理密度泛函理论研究了CO在Pt(111)、Pt(100)面上的吸附行为,并对吸附体系的吸附热、C-O键和C-Pt键的键长、布居数分析、电子态密度进行了研究.经比较吸附能、化学键参数和CO布居数,发现在CO主要以C朝下的方式吸附在Pt位,C原子与Pt原子间发生了强烈的杂化作用.为防止铂CO中毒,一般可采用在燃料气中充入一定量的氧气,这些氧气与CO反应生成CO2.计算表明,CO2不会在Pt(111)与(100)上面吸附,从而表明生成的CO2不会阻挡CO与Pt的作用,不会降低Pt的催化效应.","authors":[{"authorName":"陈艳平","id":"14029ff8-e95a-424d-bd7e-76fb2f9bee11","originalAuthorName":"陈艳平"},{"authorName":"秦宏伟","id":"3ace197a-f3b9-466a-8b65-1d37bb4a0a3a","originalAuthorName":"秦宏伟"},{"authorName":"李玲","id":"da50f8e9-6216-4037-87f6-a8f38e1f9a87","originalAuthorName":"李玲"},{"authorName":"胡季帆","id":"cf5e897f-f485-4d4d-bc7b-0605034b36fe","originalAuthorName":"胡季帆"}],"doi":"10.13228/j.boyuan.issn1005-8192.2015061","fpage":"1","id":"242a03f9-b93e-4976-afae-85be8400f018","issue":"5","journal":{"abbrevTitle":"JSGNCL","coverImgSrc":"journal/img/cover/JSGNCL.jpg","id":"46","issnPpub":"1005-8192","publisherId":"JSGNCL","title":"金属功能材料"},"keywords":[{"id":"a0871b1b-81b5-41a9-8974-153a306b3b1f","keyword":"第一性原理","originalKeyword":"第一性原理"},{"id":"3c75259b-f1a0-4fc1-aa1b-f10a4c872028","keyword":"CO","originalKeyword":"CO"},{"id":"9422d355-f288-42dd-a827-167a1245acd2","keyword":"CO2","originalKeyword":"CO2"},{"id":"8e593655-63b3-473b-8d18-968b5da1d177","keyword":"Pt","originalKeyword":"Pt"},{"id":"b298287b-d401-4922-8ace-e1c14b5cff44","keyword":"态密度","originalKeyword":"态密度"}],"language":"zh","publisherId":"jsgncl201505001","title":"CO与CO2在铂表面吸附模式或可能性研究","volume":"22","year":"2015"},{"abstractinfo":"研究了不同退火温度对热等静压(HIP)纯钒组织和力学性能的影响.结果表明,纯钒的退火过程呈明显的回复、再结晶、晶粒长大3个阶段;随退火温度升高,板条状马氏体含量减少,温度高于950℃退火时板条状马氏体消失;随着退火温度的升高,纯钒的拉伸强度降低,塑性先增加后降低;塑性在950℃退火时达最大值,延伸率、断面收缩率分别为35.2%、64%.","authors":[{"authorName":"谢东华","id":"58cd5df7-c31c-4bbd-9942-0e8172d53b40","originalAuthorName":"谢东华"},{"authorName":"刘柯钊","id":"f345e614-ba2c-4f80-a649-984d0dfb3f4c","originalAuthorName":"刘柯钊"},{"authorName":"鲜晓斌","id":"86eec81a-b4fc-4712-9bcb-de91486212b4","originalAuthorName":"鲜晓斌"},{"authorName":"叶林森","id":"a78ad917-6e24-4c3e-a968-9beacb87c2d3","originalAuthorName":"叶林森"},{"authorName":"陈艳平","id":"89689adf-718e-4478-bb83-6b87a7760d71","originalAuthorName":"陈艳平"}],"doi":"","fpage":"1566","id":"4869e6c5-89f5-4e12-ac37-97e69e46cf61","issue":"9","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":"7b89d40b-e672-4668-9a6b-09a6e49408e5","keyword":"钒","originalKeyword":"钒"},{"id":"5976df1e-55e1-43ab-b74b-a206498e407e","keyword":"热等静压","originalKeyword":"热等静压"},{"id":"42d9701f-3ba8-436e-8247-f2cef4b0d753","keyword":"退火","originalKeyword":"退火"},{"id":"96829d55-f186-4124-8185-fb27467b140c","keyword":"组织","originalKeyword":"组织"},{"id":"ec8d2e8d-faf3-4e1b-a912-c5b8eba5e0bb","keyword":"力学性能","originalKeyword":"力学性能"}],"language":"zh","publisherId":"xyjsclygc200809013","title":"退火温度对纯钒组织和性能的影响","volume":"37","year":"2008"},{"abstractinfo":"自上世纪50年代第一代玻璃闪烁材料开发以来, 玻璃闪烁材料在核物理、高能物理、工业探测(中子能谱测量、中子射线照相术及极端环境下α、β与γ射线的探测等)等领域发挥着越来越难以替代的作用. 中子探测用玻璃闪烁材料的研究集中于镧系离子(Ce³⁺、Tb³⁺、Pr³⁺等)掺杂含6Li、10B等中子吸收截面较大核素的硅酸盐、磷酸盐、铝酸盐上. 本文由中子探测用玻璃闪烁材料的性能特点、发展历程与发光机理出发, 重点关注了含⁶Li硅酸盐玻璃、磷酸盐玻璃、氟氧玻璃及其它玻璃闪烁材料的制备方法、光学性能、荧光衰减时间及中子探测效率等性能研究, 并对玻璃闪烁材料的发展趋势及未来应用方向作出了展望.","authors":[{"authorName":"陈艳平","id":"ba1e361b-4dcd-4b6c-b75a-1ad673ebf608","originalAuthorName":"陈艳平"},{"authorName":"罗德礼","id":"c3fc7a29-d32d-40d8-9130-0d45faa7f94f","originalAuthorName":"罗德礼"}],"categoryName":"|","doi":"10.3724/SP.J.1077.2012.12098","fpage":"1121","id":"5d368d17-fdf9-4589-9b5c-ab3ba4fc0c9d","issue":"11","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"3afaaa76-0bef-4495-a2db-45a500a9c38f","keyword":"中子探测; 玻璃闪烁材料; 性能; 综述","originalKeyword":"中子探测; 玻璃闪烁材料; 性能; 综述"}],"language":"zh","publisherId":"1000-324X_2012_11_6","title":"中子探测用含⁶Li玻璃闪烁材料最新进展","volume":"27","year":"2012"},{"abstractinfo":"用化学气相沉积法制备的聚氯代对二甲苯膜具有优异的耐溶剂腐蚀及气体阻隔性能.文中采用X射线衍射(XRD)、扫描电镜(SEM)表征了不同基体温度下制备聚氯代对二甲苯膜的微观组织结构;采用MOCON透湿仪测试了其水汽渗透率.结果表明,随基体温度升高,膜内聚合物分子链取向度先升高、后降低,且在较高温度下聚合物苯环基团更倾向于垂直基体表面.水汽在膜内渗透速率随基体温度升高先降低、后升高,且在约30℃～45℃处达到最低值.","authors":[{"authorName":"陈艳平","id":"62c3e127-5536-465b-9489-470b388aa425","originalAuthorName":"陈艳平"},{"authorName":"帅茂兵","id":"a513f2ac-90d1-45d8-a484-4ee5e33441a4","originalAuthorName":"帅茂兵"},{"authorName":"鲜晓斌","id":"b2f51606-4fe9-41a0-b075-d7b1811006c3","originalAuthorName":"鲜晓斌"},{"authorName":"吉祥波","id":"a9f11d6b-97f6-4493-b919-5629e55abe30","originalAuthorName":"吉祥波"},{"authorName":"唐贤臣","id":"05b9547b-ca4c-433b-8a42-bd5f9b74a4e7","originalAuthorName":"唐贤臣"}],"doi":"","fpage":"40","id":"615d7668-5eba-4c65-87b9-75cb2eec25cb","issue":"8","journal":{"abbrevTitle":"GFZCLKXYGC","coverImgSrc":"journal/img/cover/GFZCLKXYGC.jpg","id":"31","issnPpub":"1000-7555","publisherId":"GFZCLKXYGC","title":"高分子材料科学与工程"},"keywords":[{"id":"51fc41cd-494b-43d7-8133-4ff29e9281b8","keyword":"聚氯代对二甲苯膜","originalKeyword":"聚氯代对二甲苯膜"},{"id":"32b95be0-98a0-429e-9392-f6f135932931","keyword":"基体温度","originalKeyword":"基体温度"},{"id":"9871fe69-e31a-4354-9134-9013523e4aaa","keyword":"微观结构","originalKeyword":"微观结构"},{"id":"4f5bebe0-b633-4dd4-a2fd-846811196dd5","keyword":"渗透性","originalKeyword":"渗透性"}],"language":"zh","publisherId":"gfzclkxygc200908012","title":"基体温度对气相沉积聚氯代对二甲苯膜结构与性能的影响","volume":"25","year":"2009"},{"abstractinfo":"以高纯Ti箔作中间过渡层材料.在QIH16型热等静压机内扩散连接W-Fe-Ni合金与紫铜材料.采用SEM对连接界面的元素分布进行了分析,测试了不同温度下连接件的拉伸强度,并分析了连接过程中元素的扩散特点.结果表明,采用145MPa/1050℃/120min热等静压工艺可成功实现W-Fe-Ni合金与铜的冶金结合,随HIP温度升高,界面元素扩散越充分,结合强度更高.","authors":[{"authorName":"陈艳平","id":"12b48255-7cf1-4346-aab6-823cdda16950","originalAuthorName":"陈艳平"},{"authorName":"王锡胜","id":"855a4f1f-9ab7-4c4a-87e3-d5b45a91799f","originalAuthorName":"王锡胜"},{"authorName":"叶林森","id":"0c2e679f-60f7-40c6-ac24-6d5caddd3cf6","originalAuthorName":"叶林森"},{"authorName":"谢金华","id":"b0677cd5-4fb3-4906-b49d-6c4d736a5a8c","originalAuthorName":"谢金华"},{"authorName":"颜宏伟","id":"1601692b-19ce-407d-9766-69e81d5bb4e6","originalAuthorName":"颜宏伟"}],"doi":"","fpage":"240","id":"9d5c1003-c224-418e-a665-1332940b5212","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":"2c042a8a-6b7a-4329-ab8a-36799f72f57e","keyword":"W-Fe-Ni合金","originalKeyword":"W-Fe-Ni合金"},{"id":"6949ab05-e14c-4023-a2ea-0b7eddd740ce","keyword":"铜","originalKeyword":"铜"},{"id":"c131a7fe-ea0e-4739-84f3-fdefa2609f8f","keyword":"热等静压","originalKeyword":"热等静压"},{"id":"711b6381-c38b-41ff-b05e-168c3984eb12","keyword":"扩散连接","originalKeyword":"扩散连接"}],"language":"zh","publisherId":"cldb2010z2066","title":"W-Fe-Ni合金与铜HIP扩散连接技术研究","volume":"24","year":"2010"},{"abstractinfo":"考察了NaY分子筛负载高碘酸的条件,介绍了负载型H5IO6/NaY分子筛氧化纤维素的反应,H5IO6/NaY分子筛氧化纤维素的产物用红外光谱和X射线衍射表征,结果表明,H5IO6/NaY分子筛有效降低了纤维素的结晶度,而且可以将纤维素氧化成双醛纤维素.H5IO6/NaY分子筛与高碘酸氧化纤维素的实验对比表明,H5IO6/NaY分子筛能在40℃氧化纤维素8 h获得较高氧化度,比高碘酸氧化效率有所提高.","authors":[{"authorName":"陈艳平","id":"47a30922-b3cb-4b5f-9bc7-a1845b1f8546","originalAuthorName":"陈艳平"},{"authorName":"黎钢","id":"234111c5-be5d-479e-bd9a-e724c5a2e08c","originalAuthorName":"黎钢"},{"authorName":"杨芳","id":"b1cb3029-b388-424c-86a4-b49d8528d53b","originalAuthorName":"杨芳"},{"authorName":"张松梅","id":"81464469-a81b-4f59-9889-44fe1f43a94e","originalAuthorName":"张松梅"},{"authorName":"祁健","id":"d45b1c90-ed1d-4dd4-9673-0b8b7e6b1eb4","originalAuthorName":"祁健"},{"authorName":"陈雨露","id":"fe89d3d2-d243-4f78-aef6-5140ac16f0ba","originalAuthorName":"陈雨露"}],"doi":"","fpage":"142","id":"e7a3d677-a920-4886-8de3-19fe8cfd3157","issue":"6","journal":{"abbrevTitle":"GFZCLKXYGC","coverImgSrc":"journal/img/cover/GFZCLKXYGC.jpg","id":"31","issnPpub":"1000-7555","publisherId":"GFZCLKXYGC","title":"高分子材料科学与工程"},"keywords":[{"id":"633033f2-3852-4254-a15b-348d1e575372","keyword":"NaY分子筛","originalKeyword":"NaY分子筛"},{"id":"3549c2a9-9cfa-4b21-b587-eb78f70c0981","keyword":"高碘酸","originalKeyword":"高碘酸"},{"id":"384c8dd6-6d37-4689-9962-d22230ab78ec","keyword":"负载","originalKeyword":"负载"},{"id":"ce88c39e-76df-4a88-974f-ed0339bf8504","keyword":"双醛纤维素","originalKeyword":"双醛纤维素"}],"language":"zh","publisherId":"gfzclkxygc201106038","title":"NaY分子筛负载高碘酸氧化纤维素","volume":"27","year":"2011"},{"abstractinfo":"自上世纪50年代第一代玻璃闪烁材料开发以来,玻璃闪烁材料在核物理、高能物理、工业探测(中子能谱测量、中子射线照相术及极端环境下α、β与γ射线的探测等)等领域发挥着越来越难以替代的作用.中子探测用玻璃闪烁材料的研究集中于镧系离子(Ce3+、Tb3+、Pr3+等)掺杂含6Li、10B等中子吸收截面较大核素的硅酸盐、磷酸盐、铝酸盐上.本文由中子探测用玻璃闪烁材料的性能特点、发展历程与发光机理出发,重点关注了含6Li硅酸盐玻璃、磷酸盐玻璃、氟氧玻璃及其它玻璃闪烁材料的制备方法、光学性能、荧光衰减时间及中子探测效率等性能研究,并对玻璃闪烁材料的发展趋势及未来应用方向作出了展望.","authors":[{"authorName":"陈艳平","id":"841ccdab-976d-40f1-8d8d-89c609b9bc41","originalAuthorName":"陈艳平"},{"authorName":"罗德礼","id":"10d1b1c9-810c-43bb-ab23-7e5d9d934fb5","originalAuthorName":"罗德礼"}],"doi":"10.3724/SP.J.1077.2012.12098","fpage":"1121","id":"eae069b0-d650-4877-9740-7eb09936e048","issue":"11","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"44fa2a9d-151a-4d35-befb-731f0f8fa862","keyword":"中子探测","originalKeyword":"中子探测"},{"id":"b53ea690-53f4-4628-9b6b-f3ed9a966570","keyword":"玻璃闪烁材料","originalKeyword":"玻璃闪烁材料"},{"id":"f801e089-a7eb-44b5-9582-00ae6b5e324e","keyword":"性能","originalKeyword":"性能"},{"id":"1e9fc576-fc60-4f5b-a97a-e7e484c43d55","keyword":"综述","originalKeyword":"综述"}],"language":"zh","publisherId":"wjclxb201211001","title":"中子探测用含6Li玻璃闪烁材料最新进展","volume":"27","year":"2012"},{"abstractinfo":"采用熔融淬冷法制备了不同浓度 Ce3+离子掺杂的20Li2O-5MgO-20Al2O3-55SiO2玻璃闪烁材料。采用 X 射线衍射(XRD)、高分辨透射电镜(HRTEM)技术、密度检测等方法研究了玻璃的微观结构随 Ce3+离子掺杂浓度的变化规律，采用荧光分光技术检测了玻璃的紫外光致激发光谱(PLE)、发射光谱(PE)。研究结果表明：在不对称的晶体场作用下， Ce3+离子5d能级被劈裂为5个组分；随着玻璃基质内Ce3+离子掺杂浓度增大，玻璃的非晶化程度加深；5d能级的劈裂宽度随之增大，由此导致激发带向低能量端展宽、发射光谱明显红移； Ce3+离子的荧光发射强度随Ce3+离子掺杂浓度先升高、后降低，浓度猝灭过程成为其荧光发射效率降低的主要原因。","authors":[{"authorName":"陈艳平","id":"addf104b-431b-4f3c-b8ff-4a40bdde91f1","originalAuthorName":"陈艳平"},{"authorName":"罗德礼","id":"bc803c14-93dd-4525-9373-5ff42cfd9c9c","originalAuthorName":"罗德礼"},{"authorName":"徐钦英","id":"7952f610-89a8-4559-a090-cecea0f1a016","originalAuthorName":"徐钦英"},{"authorName":"杨锁龙","id":"4ee4085e-9270-4e1e-8727-d4463c6d3bbb","originalAuthorName":"杨锁龙"},{"authorName":"唐涛","id":"506ccf16-90a8-4b6f-bac3-8cec16f0ba24","originalAuthorName":"唐涛"},{"authorName":"王小英","id":"4f1d77aa-5fb0-4f8b-b125-951ce67c1d48","originalAuthorName":"王小英"}],"doi":"10.15541/jim20130662","fpage":"967","id":"faa25979-7350-4831-ad42-7db2a406d9e3","issue":"9","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"c4774429-b055-46e6-bbf9-b9879d289dd6","keyword":"Ce3+掺杂浓度","originalKeyword":"Ce3+掺杂浓度"},{"id":"7cddd702-e9bd-4678-bd7e-2b7ccbc0de9d","keyword":"Li2O-MgO-Al2O3-SiO2玻璃","originalKeyword":"Li2O-MgO-Al2O3-SiO2玻璃"},{"id":"45a645e0-a6e0-44ff-93c1-8c815dd27dfc","keyword":"5d能级劈裂","originalKeyword":"5d能级劈裂"},{"id":"c31c83c8-24f2-4106-9b8a-abd9b0578e40","keyword":"浓度猝灭","originalKeyword":"浓度猝灭"}],"language":"zh","publisherId":"wjclxb201409012","title":"Ce3+掺杂Li2O-MgO-Al2O3-SiO2玻璃的结构与荧光猝灭现象","volume":"","year":"2014"},{"abstractinfo":"采用熔体-淬冷法制备了Ce3＋离子掺杂锂(硼、磷)硅酸盐闪烁玻璃，采用紫外-可见透射、荧光分光法分别研究了Ce3＋离子掺杂锂硅酸盐、锂硼酸盐、锂硼硅酸盐、锂硼磷硅酸盐玻璃的紫外-可见透射、激发与发射性质。研究结果表明，在Ce3＋离子掺杂锂硅酸盐玻璃内引入一定量的B3＋、P5＋离子，其紫外吸收截止边，紫外激发与发射光谱分别发生一定的红移与蓝移，紫外激发与发射光谱强度明显降低。","authors":[{"authorName":"陈艳平","id":"52e9705a-1380-404d-9d7c-0b00b632ec31","originalAuthorName":"陈艳平"},{"authorName":"程浩","id":"aa89fd15-c1bc-4520-8f5a-591691a867e7","originalAuthorName":"程浩"},{"authorName":"唐贤臣","id":"d48d2c5a-603f-419a-b643-6a7734c8fd04","originalAuthorName":"唐贤臣"},{"authorName":"李强","id":"cbb8ad48-7bda-4744-b087-f3c949fc7f2b","originalAuthorName":"李强"}],"doi":"10.3969/j.issn.1001-9731.2016.10.022","fpage":"10124","id":"14468af2-e562-4109-a84b-26b176d7f32c","issue":"10","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"c4b6ecc0-a4ce-49fc-b1a4-f24daf2891cc","keyword":"Ce3+掺杂","originalKeyword":"Ce3+掺杂"},{"id":"d4b98075-9a2e-4ea2-9e81-c041543dead9","keyword":"锂(硼","originalKeyword":"锂(硼"},{"id":"bbb9fb0b-f143-4e98-8453-63aac58f6eb1","keyword":"磷)硅酸盐玻璃","originalKeyword":"磷)硅酸盐玻璃"},{"id":"0d9eabd1-419b-41ad-aa57-b15c00358dab","keyword":"紫外激发与发射","originalKeyword":"紫外激发与发射"}],"language":"zh","publisherId":"gncl201610022","title":"Ce3＋掺杂锂（硼、磷）硅酸盐玻璃的制备与荧光性质研究?","volume":"47","year":"2016"}],"totalpage":69,"totalrecord":682}