{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"以SF_6为光敏剂,用CW CO_2激光诱导气相<span style=\"color:red\">Fe</span>(CO)_5热解反应,在室温下高效率地制备出了γ-<span style=\"color:red\">Fe</span> 纳米粒子(20—40nm),并对其进行了分析和表征研究。","authors":[{"authorName":"梁勇","id":"c9869fed-f504-4079-8a8d-c43cdff76298","originalAuthorName":"梁勇"},{"authorName":"赵新清","id":"62f55e68-0827-4b04-858d-a8afc6b30885","originalAuthorName":"赵新清"},{"authorName":"郑丰","id":"e1d5798c-b85d-48c2-91e6-106837ca94d3","originalAuthorName":"郑丰"},{"authorName":"肖克沈","id":"d40b7d9c-91ef-4d8f-9823-dc402798ea28","originalAuthorName":"肖克沈"},{"authorName":"胡壮麒","id":"db7cddd8-9138-4da1-80ca-e1b65b785eb8","originalAuthorName":"胡壮麒"}],"categoryName":"|","doi":"","fpage":"412","id":"a3fe0582-5cd8-4ec7-b13d-fdb75383a3b0","issue":"5","journal":{"abbrevTitle":"CLYJXB","coverImgSrc":"journal/img/cover/CLYJXB.jpg","id":"16","issnPpub":"1005-3093","publisherId":"CLYJXB","title":"材料研究学报"},"keywords":[{"id":"990e1a5a-9023-4ba6-8cd8-39df8adf703d","keyword":"γ-<span style=\"color:red\">Fe</span>","originalKeyword":"γ-Fe"},{"id":"d4baf75d-a3a5-4ecc-8935-1eef58a79003","keyword":"laser pyrolysis","originalKeyword":"laser pyrolysis"},{"id":"98e334e8-3229-4a83-874c-b296fc0b8f00","keyword":"<span style=\"color:red\">Fe</span>(CO)_5","originalKeyword":"Fe(CO)_5"},{"id":"41823318-28aa-4ba7-b4ca-6ba3cfa07920","keyword":"nanopowders","originalKeyword":"nanopowders"}],"language":"zh","publisherId":"1005-3093_1993_5_3","title":"激光气相合成γ-<span style=\"color:red\">Fe</span>纳米粒子","volume":"7","year":"1993"},{"abstractinfo":"利用分子静力学计算了γ-<span style=\"color:red\">Fe</span>中的空位(V)、自间隙原子(SIA)、间隙氦原子(HeI)和氦-空位(He-V)团簇的形成能.<span style=\"color:red\">Fe-Fe</span>,<span style=\"color:red\">Fe</span>-He和He-He原子间相互作用分别用修正嵌入原子法(MEAM)、Wilson-Johnson势和Beck势来描述.计算结果表明,SIA<100>形成能远小于α-<span style=\"color:red\">Fe</span>中的SIA<110>形成能,HeI在γ-<span style=\"color:red\">Fe</span>中的四面体间隙位最稳定.团簇HenV0,HenV1,HenV2和HenV3中的He原子数n分别达到2,5,9和11时即可形成Frenkel对来实现自捕陷,实现自捕陷时的He/V个数比不是定值,且随空位数的增加有逐渐下降趋势.","authors":[{"authorName":"余勇","id":"93304e62-8450-46c4-8877-b1bea5780265","originalAuthorName":"余勇"},{"authorName":"潘晓霞","id":"7bf6c1a7-e53c-48ed-9643-f2ab64eac451","originalAuthorName":"潘晓霞"},{"authorName":"戎咏华","id":"d5338212-86b8-4264-a3cf-db94f4c44265","originalAuthorName":"戎咏华"}],"doi":"10.3321/j.issn:0412-1961.2007.01.001","fpage":"1","id":"7e6fe5d1-03e2-4dae-b950-1210346aa19d","issue":"1","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"89c47ca9-d7be-4b4b-a3ba-28003e9426e7","keyword":"γ-<span style=\"color:red\">Fe</span>","originalKeyword":"γ-Fe"},{"id":"409ed938-77a9-4f9b-baba-ef40634b25d8","keyword":"点缺陷","originalKeyword":"点缺陷"},{"id":"9d849bee-4bfd-4c7b-b6f4-0903d19cdf74","keyword":"形成能","originalKeyword":"形成能"},{"id":"510166f5-f538-4741-b96f-ca79a7fcef02","keyword":"氦-空位团簇","originalKeyword":"氦-空位团簇"},{"id":"6238dd91-060d-45fd-952d-311f46c606af","keyword":"自捕陷","originalKeyword":"自捕陷"}],"language":"zh","publisherId":"jsxb200701001","title":"γ-<span style=\"color:red\">Fe</span>中点缺陷与氦-空位团簇的形成能","volume":"43","year":"2007"},{"abstractinfo":"用激光气相热解法制备了α-<span style=\"color:red\">Fe</span>(bcc)和γ-<span style=\"color:red\">Fe</span>(fcc)纳米微粒利用高分辨透射电子显微镜、X射线衍射和磁测量研究了纳米微粒表面氧化物的结构、形貌及磁性能.结果表明,纳米铁微粒表面的氧化铁厚度约5 nm,由细小微晶(2-5 nm)组成该氧化铁层呈非铁磁或超顺磁性.室温下微粒表面形成的氧化铁为<span style=\"color:red\">Fe</span>3O4,而非<span style=\"color:red\">Fe</span>3O4和α-<span style=\"color:red\">Fe</span>2O3的混合物","authors":[{"authorName":"赵新清","id":"64e586ba-ea06-488d-a434-e3ddf153c6f3","originalAuthorName":"赵新清"},{"authorName":"梁勇","id":"1fc5e72a-5af6-413e-8b51-d3f8f0f63e38","originalAuthorName":"梁勇"},{"authorName":"胡壮麒","id":"2aee65fb-7410-432a-be91-40875e8a42ce","originalAuthorName":"胡壮麒"}],"doi":"10.3321/j.issn:0412-1961.2001.06.014","fpage":"633","id":"80a250b3-3eb8-4b4e-a852-01f2677efe5c","issue":"6","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"f0b0e51c-aeb3-46a0-a277-1ddae8eb59dd","keyword":"α-<span style=\"color:red\">Fe</span>","originalKeyword":"α-Fe"},{"id":"53880000-8f06-4e02-af5f-98273d5cc69a","keyword":"γ-<span style=\"color:red\">Fe</span>","originalKeyword":"γ-Fe"},{"id":"e1b476c4-1301-40fb-9480-b51c96bd7577","keyword":"纳米微粒","originalKeyword":"纳米微粒"},{"id":"0a872940-3423-4556-b602-7d84d6657944","keyword":"氧化铁","originalKeyword":"氧化铁"},{"id":"1e649cad-c17d-471c-9241-7036c593061c","keyword":"磁性能","originalKeyword":"磁性能"}],"language":"zh","publisherId":"jsxb200106014","title":"纳米铁微粒表面氧化物的结构及磁性","volume":"37","year":"2001"},{"abstractinfo":"用磁控溅射技术制备了系列Ｆｅ／Ｔｉ纳米多层膜，周期调制在２２—２４０ｎｍ：用透射电镜和小角、高角Ｘ射线衍射分别研究了样品的结构；用振动样品磁强计和Ｍｏｓｓｂａｕｅｒ谱研究了样品的磁性．发现铁层厚度在２ｎｍ附近时存在铁磁性面心立方γ－Ｆｅ，样品的易磁化方向平行于膜面；随调制周期增大，样品的饱和磁化强度增加，矫顽力下降且与结晶状态有关．","authors":[{"authorName":"王振军","id":"aae65c96-f8d0-4044-a324-963817885617","originalAuthorName":"王振军"},{"authorName":"常香荣","id":"3a0a7ab5-94f1-4f30-8bb0-788353e13073","originalAuthorName":"常香荣"},{"authorName":"平爵云","id":"8f4cebc5-138b-410b-b411-a89f98f054a2","originalAuthorName":"平爵云"},{"authorName":"田中卓","id":"10384054-2c83-4709-833d-a6cb8a0dd65e","originalAuthorName":"田中卓"},{"authorName":"肖纪美","id":"f354c84d-c4e1-4f5b-8072-6991bf97d07c","originalAuthorName":"肖纪美"},{"authorName":"闻立时","id":"e1b42fb9-d373-4037-9faf-44a6b981414a","originalAuthorName":"闻立时"}],"categoryName":"|","doi":"","fpage":"85","id":"17c6f9f3-b64d-4964-b01a-547529142934","issue":"1","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"322f4b79-747b-4efe-85a8-ec95d4dcc4a7","keyword":"Ｆｅ／Ｔｉ多层膜","originalKeyword":"Ｆｅ／Ｔｉ多层膜"},{"id":"028d84c9-d30b-4495-8102-6f1d120f9a37","keyword":"γ-<span style=\"color:red\">Fe</span>","originalKeyword":"γ-Fe"},{"id":"4d093075-b53f-4cbc-aa52-f18d14f17e5e","keyword":" DC-magnetron sputtering","originalKeyword":" DC-magnetron sputtering"}],"language":"zh","publisherId":"0412-1961_1996_1_4","title":"磁控溅射制备<span style=\"color:red\">Fe</span>/Ti多层膜的结构和磁性","volume":"32","year":"1996"},{"abstractinfo":"Mechanism for diffusion of B in γ-<span style=\"color:red\">Fe</span> is believed to be mainly by means of boron-vacancy complexes other than as interstitial atoms previously.This was made of calculation on the ba- sis of theoretical model proposed by the authors.The calculated diffusion coefficient of B in γ-<span style=\"color:red\">Fe</span> after this mechanism is consistent with the experimental values.In addition,this is also supported by the non-equilibrium segregation phenomenon of B at grain boundaries of γ-<span style=\"color:red\">Fe</span> and the lattice constant measurement of <span style=\"color:red\">Fe</span>-B alloy.","authors":[{"authorName":"YU Zongsen CHEN Ning University of Science and Technology Beijing","id":"30600f20-8490-4841-9604-469f70a601cc","originalAuthorName":"YU Zongsen CHEN Ning University of Science and Technology Beijing"},{"authorName":"Beijing","id":"1eef510c-6b9e-401b-b98a-8239971e2ccb","originalAuthorName":"Beijing"},{"authorName":"China","id":"503e394b-03d8-4d01-916d-0d231265139e","originalAuthorName":"China"}],"categoryName":"|","doi":"","fpage":"318","id":"2ab3e993-3f86-402f-b5d8-8b57276770dc","issue":"5","journal":{"abbrevTitle":"JSXBYWB","coverImgSrc":"journal/img/cover/amse.jpg","id":"49","issnPpub":"1006-7191","publisherId":"JSXBYWB","title":"金属学报(英文版)"},"keywords":[{"id":"642bb779-2d0f-4af5-9767-2ce08744ed91","keyword":"boron","originalKeyword":"boron"},{"id":"a40ec025-efd2-40b3-b830-7394b16f7c52","keyword":"null","originalKeyword":"null"},{"id":"a0546955-e81b-43f5-ac86-3111b9bc16de","keyword":"null","originalKeyword":"null"},{"id":"2c6e7720-4530-4fd7-97be-f570cb7cd7c5","keyword":"null","originalKeyword":"null"},{"id":"e3cecefc-a421-420e-a94a-f10b76c6744d","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_1992_5_3","title":"MECHANISM FOR DIFFUSION OF BORON IN γ-<span style=\"color:red\">Fe</span>","volume":"5","year":"1992"},{"abstractinfo":"Pr-<span style=\"color:red\">Fe</span>-B/<span style=\"color:red\">Fe</span>/Pr-<span style=\"color:red\">Fe</span>-B films with different <span style=\"color:red\">Fe</span> layer thicknesses were deposited by magnetron sputtering on Si (100) substrate heated at 650 degrees C. Structural and magnetic properties of the Pr-<span style=\"color:red\">Fe</span>-B/<span style=\"color:red\">Fe</span>/Pr-<span style=\"color:red\">Fe</span>-B films were investigated. X-ray diffraction and magnetic measurement results reveal that the Pr-<span style=\"color:red\">Fe</span>-B/<span style=\"color:red\">Fe</span>/Pr-<span style=\"color:red\">Fe</span>-B films are anisotropic when the thickness of <span style=\"color:red\">Fe</span> layer is smaller than 50 nm. The enhancement of the saturation magnetization in nanocomposite films is attributed to the exchange coupling between the soft and hard phases. The highest coercivity of about 13.9 kOe is achieved in the Mo(50 nm)/Pr-<span style=\"color:red\">Fe</span>-B(50 nm)/Mo(2 nm)/<span style=\"color:red\">Fe</span>(2 nm)/Mo(2 nm)/Pr-<span style=\"color:red\">Fe</span>-B(50 nm)/Mo(50 nm) film and increasing the thickness of soft-magnetic layer results in a continuous decreasing of the coercivity.","authors":[],"categoryName":"|","doi":"","fpage":"2059","id":"33fb8ad7-44f6-449e-82d2-3dd9a1be97ba","issue":"6","journal":{"abbrevTitle":"JOSANM","id":"057212ff-7198-4baa-a71b-12159747586f","issnPpub":"1557-1939","publisherId":"JOSANM","title":"Journal of Superconductivity and Novel Magnetism"},"keywords":[{"id":"d48b2ed1-f54a-4804-8294-7a4f4c70a242","keyword":"Magnetic films and multilayers;Anisotropy;Atomic force microscopy;Nanocomposites;remanence enhancement;multilayer magnets;exchange","originalKeyword":"Magnetic films and multilayers;Anisotropy;Atomic force microscopy;Nanocomposites;remanence enhancement;multilayer magnets;exchange"}],"language":"en","publisherId":"1557-1939_2012_6_1","title":"Magnetic Properties of Anisotropic Pr-<span style=\"color:red\">Fe</span>-B/<span style=\"color:red\">Fe</span>/Pr-<span style=\"color:red\">Fe</span>-B Films","volume":"25","year":"2012"},{"abstractinfo":"The formation kinetics of epsilon-<span style=\"color:red\">Fe</span>3-2N phase in a nanocrystalline alpha-<span style=\"color:red\">Fe</span>, which was processed by surface mechanical attrition treatment, is found to be obviously increased with respect to that in the coarse-grained form. This can be attributed to the much enhanced heterogeneous nucleation rate at numerous grain boundaries in the nanocrystalline alpha-<span style=\"color:red\">Fe</span>. (C) 2003 Acta Materialia Inc. Published by Elsevier Ltd. All rights reserved.","authors":[],"categoryName":"|","doi":"","fpage":"647","id":"5d41232e-d57c-4122-b56d-5f834b429eb0","issue":"5","journal":{"abbrevTitle":"SM","id":"37a994ff-74c6-4c39-a38b-4d9dcf2c8354","issnPpub":"1359-6462","publisherId":"SM","title":"Scripta Materialia"},"keywords":[{"id":"08a954ef-d8b4-4080-99cf-7a8f9d1c6dde","keyword":"nanocrystalline materials;iron;nitriding;surface mechanical attrition;treatment (SMAT);surface nanocrystallization;iron","originalKeyword":"nanocrystalline materials;iron;nitriding;surface mechanical attrition;treatment (SMAT);surface nanocrystallization;iron"}],"language":"en","publisherId":"1359-6462_2004_5_1","title":"The formation of epsilon-<span style=\"color:red\">Fe</span>-3-N-2 phase in a nanocrystalline <span style=\"color:red\">Fe</span>","volume":"50","year":"2004"},{"abstractinfo":"采用所构建的长程F-S势函数,对连续升温过程中γ-<span style=\"color:red\">Fe</span>→δ-<span style=\"color:red\">Fe</span>→液态<span style=\"color:red\">Fe</span>的相变过程进行了分子动力学(MD)模拟.结果表明,计算得到的γ-<span style=\"color:red\">Fe</span>→δ-<span style=\"color:red\">Fe</span>→以及液态<span style=\"color:red\">Fe</span>的微观结构(径向分布函数、配位数)和宏观物性(密度)都能与实验结果吻合很好,但相变温度点与实验值的偏差较大,推测是由过快升温速度造成的过热度过高所致.从微观结构、瞬态能量及密度的分析出发,讨论了固态相变(γ-<span style=\"color:red\">Fe</span>→δ-<span style=\"color:red\">Fe</span>→)和固-液相变(δ-<span style=\"color:red\">Fe</span>→液态<span style=\"color:red\">Fe</span>)的具体过程.其中,固态相变主要形成于晶格扭曲和滑移,而固-液相变即熔化过程起始于固体岛颗粒的边缘,并逐渐向其中心扩散.在相变演化过程中,通过瞬态能量和密度的起伏观察到明显的孕育过程.","authors":[{"authorName":"刘益虎","id":"c4e8e3f1-20fa-4a10-9a99-89284823151d","originalAuthorName":"刘益虎"},{"authorName":"吴永全","id":"d6a518dc-c9eb-4cf2-882e-49e87e587e75","originalAuthorName":"吴永全"},{"authorName":"沈通","id":"21ef26bd-4ce3-45a1-84e0-6006bf9525c4","originalAuthorName":"沈通"},{"authorName":"王召柯","id":"7efeefa2-7d50-4ed2-b3c7-a93af16bf8f0","originalAuthorName":"王召柯"},{"authorName":"蒋国昌","id":"21cd38c7-dca2-45a8-b7ea-e79b654b961f","originalAuthorName":"蒋国昌"}],"doi":"10.3724/SP.J.1037.2009.00327","fpage":"172","id":"19f869ba-9c12-4bff-b08d-51e2f455860e","issue":"2","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"d919dd41-f361-42f3-b995-ddb5d9c631f4","keyword":"纯<span style=\"color:red\">Fe</span>","originalKeyword":"纯Fe"},{"id":"6cb94979-6e84-45e7-aae2-6c3011f877bb","keyword":"升温相变","originalKeyword":"升温相变"},{"id":"39ff5a83-2707-4a13-afce-0eab218ba530","keyword":"分子动力学","originalKeyword":"分子动力学"},{"id":"b57b47b3-6384-4dab-8f8d-b5c3826ac4cc","keyword":"微观结构","originalKeyword":"微观结构"}],"language":"zh","publisherId":"jsxb201002008","title":"连续升温过程中γ-<span style=\"color:red\">Fe</span>→δ-<span style=\"color:red\">Fe</span>→液态<span style=\"color:red\">Fe</span>相变的分子动力学模拟","volume":"46","year":"2010"},{"abstractinfo":"The saturated solubility of carbon and nitrogen in <span style=\"color:red\">Fe</span>CN and <span style=\"color:red\">Fe</span>CBN melts was measured experimentally at 1 485 ℃ to obtain the activity interaction coefficients between components in these melts. A new method was used to treat experimental results. Using thermodynamic derivation and calculation, some important interaction coefficients between components in these melts were obtained.","authors":[{"authorName":"CHEN Erbao","id":"c8f41f8c-da76-496e-807c-0f49271c765c","originalAuthorName":"CHEN Erbao"},{"authorName":"WANG Shijun","id":"56b04243-a460-464e-95ff-54d6bde63242","originalAuthorName":"WANG Shijun"},{"authorName":"DONG Yuanchi","id":"c5e18623-48ff-4044-a1b9-6266c5c6b0a7","originalAuthorName":"DONG Yuanchi"},{"authorName":"WU Baoguo","id":"58788d36-a548-4117-ad42-985277bb4b64","originalAuthorName":"WU Baoguo"},{"authorName":"ZHOU Yun","id":"6ec16a4b-8c46-47fc-bd77-133dafb23997","originalAuthorName":"ZHOU Yun"}],"categoryName":"|","doi":"","fpage":"21","id":"9d55e59f-d5ae-428a-b998-ef3015f66cdc","issue":"1","journal":{"abbrevTitle":"GTYJXBYWB","coverImgSrc":"journal/img/cover/GTYJXBEN.jpg","id":"1","issnPpub":"1006-706X","publisherId":"GTYJXBYWB","title":"钢铁研究学报(英文版)"},"keywords":[{"id":"b085373b-7d05-4ad2-acee-2e8f6554a0ab","keyword":"<span style=\"color:red\">Fe</span>CN melt;<span style=\"color:red\">Fe</span>CBN melt;<span style=\"color:red\">Fe</span>CB melt;interaction coefficient;thermodynamic property","originalKeyword":"FeCN melt;FeCBN melt;FeCB melt;interaction coefficient;thermodynamic property"}],"language":"en","publisherId":"1006-706X_2007_1_13","title":"Thermodynamic Properties of <span style=\"color:red\">Fe</span>CN and <span style=\"color:red\">Fe</span>CBN Melts","volume":"14","year":"2007"},{"abstractinfo":"采用SHS/QP工艺制备了(TiB2+<span style=\"color:red\">Fe</span>)/<span style=\"color:red\">Fe</span>叠层材料.SEM分析表明TiB2+<span style=\"color:red\">Fe</span>金属陶瓷层结构致密.用EPMA研究了TiB2+<span style=\"color:red\">Fe</span>金属陶瓷层与<span style=\"color:red\">Fe</span>基片之间的界面连接机制,结果表明TiB2从TiB2+<span style=\"color:red\">Fe</span>侧向<span style=\"color:red\">Fe</span>基片侧进行扩散,以及TiB2+<span style=\"color:red\">Fe</span>层中的<span style=\"color:red\">Fe</span>粘结相和<span style=\"color:red\">Fe</span>基片的粘接完成了(TiB2+<span style=\"color:red\">Fe</span>)/<span style=\"color:red\">Fe</span>叠层材料的界面连接.叠层材料接头断裂时,断裂位置发生在TiB2+<span style=\"color:red\">Fe</span>金属陶瓷层,而不是沿着TiB2+<span style=\"color:red\">Fe</span>层与<span style=\"color:red\">Fe</span>基片的界面断裂.","authors":[{"authorName":"刘建平","id":"db7d683b-0cc0-493a-9956-0771645c9ce0","originalAuthorName":"刘建平"},{"authorName":"傅正义","id":"b0457f64-5505-4bbe-8455-4db7765329d2","originalAuthorName":"傅正义"},{"authorName":"王皓","id":"a30ff503-2659-4c00-b52f-995b454270f2","originalAuthorName":"王皓"},{"authorName":"张金咏","id":"aaa94e61-adb3-46a6-b725-6cdec57f9a70","originalAuthorName":"张金咏"},{"authorName":"张清杰","id":"c5695dcf-3d30-4f7d-8f3e-414d17d37926","originalAuthorName":"张清杰"}],"doi":"10.3321/j.issn:1000-3851.2003.01.022","fpage":"116","id":"2c7adf5d-775e-4fc1-8be4-51c60bd73bf4","issue":"1","journal":{"abbrevTitle":"FHCLXB","coverImgSrc":"journal/img/cover/FHCLXB.jpg","id":"26","issnPpub":"1000-3851","publisherId":"FHCLXB","title":"复合材料学报"},"keywords":[{"id":"f02f6c19-f442-4ad3-8c83-016e2b5cbb2e","keyword":"(TiB2+<span style=\"color:red\">Fe</span>)/<span style=\"color:red\">Fe</span>叠层材料","originalKeyword":"(TiB2+Fe)/Fe叠层材料"},{"id":"24086064-622d-4c7c-a03e-215529da9a49","keyword":"SHS/QP","originalKeyword":"SHS/QP"},{"id":"b2216b0f-a676-424f-9a6a-010239ff6b50","keyword":"界面结合","originalKeyword":"界面结合"}],"language":"zh","publisherId":"fhclxb200301022","title":"SHS/QP制备(TiB2+<span style=\"color:red\">Fe</span>)/<span style=\"color:red\">Fe</span>叠层材料的结构与性能分析","volume":"20","year":"2003"}],"totalpage":1435,"totalrecord":14348}