{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":4,"startPagecode":1},"records":[{"abstractinfo":"采用DSC测定<span style=\"color:red\">FeSiB</span>非晶粉末的玻璃态转变点(Tg)、初始晶化点(Tx)和过冷液相区(△Tx),以此为基础,利用放电等离子烧结技术制备出了φ10mm×7mm、致密度为92.3%的块体非晶合金.采用XRD、SEM、VSM、万能试验机分析了烧结块体样品的相组成、微观形貌、磁性能和抗压强度.研究表明,当烧结条件为压力500 MPa、温度360℃时,得到的块体非晶合金致密度最高,其饱和磁化强度为1.44 T,抗压强度为1200 MPa.400℃晶化后块体样品的饱和磁化强度为1.54 T,抗压强度为2039 MPa.","authors":[{"authorName":"庾正伟","id":"c59bf739-b5a7-43a7-93fc-75dee34ad6a6","originalAuthorName":"庾正伟"},{"authorName":"刘颖","id":"90716080-fd9b-44f4-b90c-cc56063b9dfd","originalAuthorName":"刘颖"},{"authorName":"李军","id":"7ee5bd53-ea35-4924-8c81-b4b651ed72ca","originalAuthorName":"李军"},{"authorName":"连利仙","id":"307d0169-b666-4c45-852a-e5282a2c9a33","originalAuthorName":"连利仙"},{"authorName":"孙文泽","id":"5eec9027-1166-43be-a25a-efbac3a07754","originalAuthorName":"孙文泽"},{"authorName":"刘海","id":"0fd62a6c-dd58-40f6-9243-6b7d17f1106f","originalAuthorName":"刘海"}],"doi":"","fpage":"44","id":"7525603b-f0fa-49c3-b350-caebe2a53289","issue":"z1","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":"c2552210-46e7-42e3-a5d6-fa2eedfe9548","keyword":"放电等离子烧结","originalKeyword":"放电等离子烧结"},{"id":"07c99806-58b0-4bd6-8264-02904667bd52","keyword":"<span style=\"color:red\">FeSiB</span>","originalKeyword":"FeSiB"},{"id":"90fbc261-38ae-410d-89a2-d18b68206932","keyword":"块体非晶合金","originalKeyword":"块体非晶合金"}],"language":"zh","publisherId":"xyjsclygc2009z1010","title":"放电等离子烧结制备<span style=\"color:red\">FeSiB</span>块体非晶合金","volume":"38","year":"2009"},{"abstractinfo":"","authors":[{"authorName":"","id":"2955b60e-91ac-4a07-ac4d-4620b2cecbdb","originalAuthorName":""}],"doi":"","fpage":"303","id":"cf8ad37c-d101-410a-a47d-1381b6b239c1","issue":"4","journal":{"abbrevTitle":"CLKXJSY","coverImgSrc":"journal/img/cover/JMST.jpg","id":"11","issnPpub":"1005-0302 ","publisherId":"CLKXJSY","title":"材料科学技术（英文）"},"keywords":[{"id":"72dba76f-db77-4c92-93ba-91690c135a8c","keyword":"<span style=\"color:red\">FeSiB</span>","originalKeyword":"FeSiB"},{"id":"fc4aca62-ba9a-4502-a75b-fc52172d0ac9","keyword":"纳米晶","originalKeyword":"纳米晶"},{"id":"8f2c25ae-d49c-406a-9aa2-de5d1f1d0ac7","keyword":"磁学性质","originalKeyword":"磁学性质"},{"id":"3b8d80d6-a7ce-47cd-88f7-8346ca588301","keyword":"微结构","originalKeyword":"微结构"},{"id":"a8888d08-935a-421f-8b7a-a08f8b3e770b","keyword":"纳米薄片","originalKeyword":"纳米薄片"},{"id":"106da2d8-ac30-43b4-b359-bbbd58953a0e","keyword":"基础","originalKeyword":"基础"},{"id":"73214424-01f5-4562-87a1-8af6d83738a4","keyword":"饱和磁化强度","originalKeyword":"饱和磁化强度"},{"id":"27b5a601-45c0-4fda-a85e-a352626dcad9","keyword":"晶粒尺寸","originalKeyword":"晶粒尺寸"}],"language":"zh","publisherId":"clkxjsxb-e201204003","title":"Microforging Effect on the Microstructure and Magnetic Properties of <span style=\"color:red\">FeSiB</span>-based Nanoflakes","volume":"28","year":"2012"},{"abstractinfo":"分别以FeCuNbSiB和<span style=\"color:red\">FeSiB</span>非晶粉为粉体与硅橡胶复合,制成具有压磁效应的复合薄膜。利用4284A阻抗分析仪对两种薄膜的压磁特性进行了研究。研究表明,非晶FeCuNbSiB粉体/硅橡胶和<span style=\"color:red\">FeSiB</span>粉体/硅橡胶复合薄膜均具有良好的压磁性能,对于FeCuNbSiB粉体/硅橡胶复合薄膜,在压应力〈0.6MPa,频率低于200kHz的条件下,压磁效应敏感;对于<span style=\"color:red\">FeSiB</span>粉体/硅橡胶复合薄膜在0～1.45MPa内,薄膜的压磁效应变化幅度比较均匀;薄膜中粉体含量越高,复合薄膜的压磁效应越大,当含量为83.3%（质量分数）时,压磁性能最好;相同条件下,以FeCuNb-SiB为粉体制成的复合薄膜的压磁性能优于以<span style=\"color:red\">FeSiB</span>为粉体制成的薄膜的压磁性能。","authors":[{"authorName":"周佳","id":"8c98f82d-342d-4f13-8088-ce8946b8c0f8","originalAuthorName":"周佳"},{"authorName":"朱正吼","id":"80afe8b9-02c5-40f6-b6c2-4107a97deb52","originalAuthorName":"朱正吼"},{"authorName":"李晓敏","id":"1b0e2e0a-45d7-49cb-a0eb-3b34275bca2d","originalAuthorName":"李晓敏"},{"authorName":"黄渝鸿","id":"42815db3-db91-4054-a75e-1879c29bcd47","originalAuthorName":"黄渝鸿"},{"authorName":"乔宝英","id":"e5f23c81-af6b-44a7-bbe3-1b6a5e6b487d","originalAuthorName":"乔宝英"}],"doi":"","fpage":"2519","id":"261ab128-1cd0-41c2-958f-814b251bf964","issue":"18","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"2ac3ca28-13f3-4436-bb40-c9286e9b76f7","keyword":"压磁效应","originalKeyword":"压磁效应"},{"id":"ead73256-4672-4a0f-9866-bf2f432dacc0","keyword":"FeCuNbSiB","originalKeyword":"FeCuNbSiB"},{"id":"59606da4-168f-4940-a8f8-efde562be6e0","keyword":"<span style=\"color:red\">FeSiB</span>","originalKeyword":"FeSiB"},{"id":"f869b027-2f6e-4bc4-82a3-8e4978db4b9f","keyword":"硅橡胶","originalKeyword":"硅橡胶"},{"id":"9444a070-6749-48f0-8075-a31b6b3f650b","keyword":"复合薄膜","originalKeyword":"复合薄膜"}],"language":"zh","publisherId":"gncl201218021","title":"多角形非晶粉/硅橡胶复合薄膜压磁性能研究","volume":"43","year":"2012"},{"abstractinfo":"采用磁控溅射法在玻璃基底上制备了曲折状<span style=\"color:red\">FeSiB</span>/Cu/<span style=\"color:red\">FeSiB</span>三层膜结构,在1～40MHz范围内研究了<span style=\"color:red\">FeSiB</span>膜和Cu膜厚度对三层膜结构应力阻抗效应的影响.结果表明:高频下三层膜的应力阻抗效应随着其形变的增加近似线性增加,在自由端弯曲变形1mm、外加电场频率为25MHz时,应力阻抗效应达到-18.3%,在力敏传感器方面具有广阔的应用前景.","authors":[{"authorName":"陈吉安","id":"70c66b3f-2b87-4230-b988-4379648511be","originalAuthorName":"陈吉安"},{"authorName":"茅昕辉","id":"02fd83d2-88ab-4c11-a64f-d7efcc6db0dd","originalAuthorName":"茅昕辉"},{"authorName":"赵晓昱","id":"8d692d30-068b-4d4f-90ab-5b277b00edc9","originalAuthorName":"赵晓昱"},{"authorName":"丁文","id":"85d97168-97e7-4b6b-8218-84cb4eea3215","originalAuthorName":"丁文"},{"authorName":"曹莹","id":"9257d255-423b-46dd-85ea-db61ec77e864","originalAuthorName":"曹莹"},{"authorName":"周勇","id":"831d75fd-7b9c-4487-8706-840d4775b15b","originalAuthorName":"周勇"}],"doi":"10.3969/j.issn.1007-4252.2005.04.005","fpage":"419","id":"9c97c387-c207-4267-88b4-cf0b102a31a5","issue":"4","journal":{"abbrevTitle":"GNCLYQJXB","coverImgSrc":"journal/img/cover/GNCLYQJXB.jpg","id":"34","issnPpub":"1007-4252","publisherId":"GNCLYQJXB","title":"功能材料与器件学报   "},"keywords":[{"id":"d84bbd02-7adb-40e5-8a6b-daffb96aff58","keyword":"应力阻抗","originalKeyword":"应力阻抗"},{"id":"97d868b3-b75d-4b6c-b104-a7b4c589233f","keyword":"<span style=\"color:red\">FeSiB</span>/Cu/<span style=\"color:red\">FeSiB</span>三层膜","originalKeyword":"FeSiB/Cu/FeSiB三层膜"},{"id":"e86b6098-396d-4a7b-adbf-8c2527502a05","keyword":"磁控溅射","originalKeyword":"磁控溅射"},{"id":"108e21a0-16ee-4e30-ba1e-d075ca25d159","keyword":"曲折状","originalKeyword":"曲折状"}],"language":"zh","publisherId":"gnclyqjxb200504005","title":"曲折状<span style=\"color:red\">FeSiB</span>/Cu/<span style=\"color:red\">FeSiB</span>三层膜结构应力阻抗效应研究","volume":"11","year":"2005"},{"abstractinfo":"Sensitive magnetic field sensor with good performances can be fabricated utilizing the giant magneto-impedance (GMI) effect of soft magnetic multi-layer thin films. The transverse and longitudinal GMI effect in patterned <span style=\"color:red\">FeSiB</span>/Cu/<span style=\"color:red\">FeSiB</span> tri-layer films with the change of external magnetic field and frequency were studied at the same time. The change of the impedance of the films with the external magnetic fieldand frequency was shown. Comparing the longitudinal and transverse effect, the transverseeffect has a larger linear range from zero magnetic field to a quite large magnetic field at all frequencies, and the change still were not saturated until the external magnetic field reached 1.2×10^4A/m, which illustrated that the films can be utilized to detect laraer maanetic fields than now presented GMI sensors.","authors":[{"authorName":"X.H.Mao","id":"16053e45-1d18-43c6-b864-14cfa5b39aea","originalAuthorName":"X.H.Mao"},{"authorName":" Y.Zhou","id":"ad37ccab-b415-45ee-8c00-6a109f62b854","originalAuthorName":" Y.Zhou"},{"authorName":" M.S.Wu","id":"6b494a1e-3b8a-4958-95a1-3ee390ea14c4","originalAuthorName":" M.S.Wu"},{"authorName":" B.C.Cai","id":"eee0b6aa-e7f4-462c-b854-b929216948c4","originalAuthorName":" B.C.Cai"}],"categoryName":"|","doi":"","fpage":"327","id":"59f1c375-abbb-482c-8146-3dd1be436334","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":"0f6b0fd8-cb46-4e53-996e-6087ac977c76","keyword":"giant magneto-impedance effect","originalKeyword":"giant magneto-impedance effect"},{"id":"0647e1b9-66cb-4fd0-828b-9c6e16f41684","keyword":"null","originalKeyword":"null"},{"id":"4849902f-0469-4862-b1d1-338cadafc483","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_2003_5_7","title":"GIANT MAGNETO-IMPEDANCE OF PATTERNED <span style=\"color:red\">FeSiB</span>／Cu／<span style=\"color:red\">FeSiB</span> TRI-LAYER FILMS","volume":"16","year":"2003"},{"abstractinfo":"The effect of microforging on the processing of nanocrystalline <span style=\"color:red\">FeSiB</span> alloy flakes was studied in terms of microstructure and magnetic properties. The flakes microforged from amorphous precursor showed submicron thicknesses with the crystal size of about 15 nm. The crystallite size during microforging was primarily determined by plastic deformation rather than fracturing and agglomeration. Unlike the general trend of coercivity reduction with annealing, the coercivity of the nanocrystalline flakes was slightly increased with increasing annealing temperature, which can be explained with the diffusion anisotropy of the magnetic moments resulting from the formation of Fe-atoms pairs. The magnetic remanence (<em>M</em><sub>r</sub>) of the planar nanocrystalline flakes was</br>\nmeasured to be about 26% of the saturation magnetization (<em>M</em><sub>s</sub>), a significant increase from 2% of the initial amorphous precursor.","authors":[{"authorName":"Wooseung Kang","id":"9c7a7c31-a827-4b42-87ef-44868479c0a9","originalAuthorName":"Wooseung Kang"}],"categoryName":"|","doi":"","fpage":"303","id":"7ee17c49-adf2-4189-b74e-a2b5af40e8d9","issue":"4","journal":{"abbrevTitle":"CLKXJSY","coverImgSrc":"journal/img/cover/JMST.jpg","id":"11","issnPpub":"1005-0302 ","publisherId":"CLKXJSY","title":"材料科学技术（英文）"},"keywords":[{"id":"f2867140-1728-4c73-9b3f-4eb02be2a2e4","keyword":"Microforging","originalKeyword":"Microforging"}],"language":"en","publisherId":"1005-0302_2012_4_12","title":"Microforging Effect on the Microstructure and Magnetic Properties of <span style=\"color:red\">FeSiB</span>-based Nanoflakes","volume":"28","year":"2012"},{"abstractinfo":"由于快淬材料的特殊组织结构和制品形式,不仅具有特殊的功能特性,还具有特殊的机械特性.以常规<span style=\"color:red\">FeSiB</span>磁性材料为研究对象,采用快淬方法制备连续快淬纤维,并测试机械性能.性能测试结果展示该类型材料快淬纤维在其他领域的应用前景.","authors":[{"authorName":"郭万林","id":"8f68f124-48ef-4d85-93a2-94405ddf235e","originalAuthorName":"郭万林"},{"authorName":"李天文","id":"22607994-0190-447e-b6f3-74831a35e901","originalAuthorName":"李天文"},{"authorName":"淮军锋","id":"30552e2f-80e2-469a-8004-71a5d562140a","originalAuthorName":"淮军锋"}],"doi":"10.3969/j.issn.1005-5053.2006.03.071","fpage":"315","id":"9a7187f1-3ec7-4dbe-b222-afdeddd7ec7c","issue":"3","journal":{"abbrevTitle":"HKCLXB","coverImgSrc":"journal/img/cover/HKCLXB.jpg","id":"41","issnPpub":"1005-5053","publisherId":"HKCLXB","title":"航空材料学报"},"keywords":[{"id":"ab9f3583-f43d-433b-9156-2495c9dfdd04","keyword":"快淬","originalKeyword":"快淬"},{"id":"e1cf3a35-d9d0-4388-ba02-38cb6444abc5","keyword":"磁性材料","originalKeyword":"磁性材料"},{"id":"38c3a7ae-9f8e-4b89-ad3e-668ff2732f18","keyword":"纤维","originalKeyword":"纤维"}],"language":"zh","publisherId":"hkclxb200603071","title":"<span style=\"color:red\">FeSiB</span>纤维的快淬制备及其性能","volume":"26","year":"2006"},{"abstractinfo":"采用模压成型制备<span style=\"color:red\">FeSiB</span>非晶磁粉芯.并讨论了退火温度和时间、非晶粉体的粒径、不同粒径混合及Fe粉复合量等对磁粉芯磁性能的影响.结果表明,在200～500℃范围内退火,随着退火温度的升高,磁粉芯的μe先增大后减小,375℃时达到最佳,其最佳退火时间为2h.在100kHz～1MHz内,频率稳定性良好,其中心频率在500kHz附近;非晶粉体的粒径越大,磁粉芯的磁性能越好;粉体粒径为60～100目时,其μe达到最大;当粒径为60～100目与100～200目复合时,60～100目的<span style=\"color:red\">FeSiB</span>非晶粉体含量为60%时最佳.当复合Fe粉后,发现其软磁性能得到了明显改善, Fe粉量为30%时,μe达到32,Q值达到33.","authors":[{"authorName":"黄伟兵","id":"f3cd8edc-3160-4e69-a77a-02e8e6bd464e","originalAuthorName":"黄伟兵"},{"authorName":"朱正吼","id":"61b4f754-16f6-446b-ad74-2014a4316dd8","originalAuthorName":"朱正吼"},{"authorName":"杨操兵","id":"f294fdf5-7301-4234-a153-5317518d3512","originalAuthorName":"杨操兵"},{"authorName":"刘志宾","id":"9e92d31f-183d-44a9-9048-e451d9cf8dba","originalAuthorName":"刘志宾"},{"authorName":"付远","id":"f556d5de-d3c3-4eb2-811a-fbc5cf727275","originalAuthorName":"付远"}],"doi":"","fpage":"2010","id":"f0242e07-140b-4f77-a5bf-90a35ee62205","issue":"11","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"2f74cf67-8bd4-42f2-b319-85b4071b573f","keyword":"非晶","originalKeyword":"非晶"},{"id":"3bf265a4-0078-446f-803e-7ea5b17e3812","keyword":"磁粉芯","originalKeyword":"磁粉芯"},{"id":"ed056235-3590-4bfd-b975-5160bc505227","keyword":"软磁性能","originalKeyword":"软磁性能"}],"language":"zh","publisherId":"gncl201011041","title":"Fe/<span style=\"color:red\">FeSiB</span>磁粉芯软磁性能研究","volume":"41","year":"2010"},{"abstractinfo":"本文采用自行研制的微分热分析仪测定了<span style=\"color:red\">FeSiB</span>合金熔体在凝固过程中的温度-时间曲线,并利用扫描电子显微镜(SEM)和能谱仪(EDS)分析了试样的夹杂物形貌及成分,研究了所测曲线特征参数与夹杂物之间的关系.结果表明:当<span style=\"color:red\">FeSiB</span>合金熔体在凝固过程中的初晶时间间隔和初晶温度间隔都随熔体的夹杂物含量的增加而增大,同时,在薄带制带过程中容易产生水口堵塞等异常现象.","authors":[{"authorName":"王建","id":"2a82669f-49bd-4d1d-979a-a6fc9c96a2ba","originalAuthorName":"王建"},{"authorName":"姚书芳","id":"186713b9-c108-4c83-8b66-6d4905823d8e","originalAuthorName":"姚书芳"},{"authorName":"张淑兰","id":"b3cb5e71-b5cd-4a3e-b38f-1e15876650b5","originalAuthorName":"张淑兰"},{"authorName":"陈文智","id":"30791dea-3a56-402c-a3f4-7c29a3a71e99","originalAuthorName":"陈文智"},{"authorName":"周少雄","id":"b0a6299b-28ce-42bd-af5f-a7f5d0111152","originalAuthorName":"周少雄"}],"doi":"","fpage":"1","id":"3cc9d9ca-d6d1-4ecd-b065-711e4f46b067","issue":"3","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":"2d698f9e-f419-452e-b596-4895b49a9e72","keyword":"<span style=\"color:red\">FeSiB</span>合金","originalKeyword":"FeSiB合金"},{"id":"0228567a-889c-498a-8bbf-a635d39d4deb","keyword":"微分热分析","originalKeyword":"微分热分析"},{"id":"9eea94f9-e87b-480e-89cf-2ca9595ce474","keyword":"夹杂物","originalKeyword":"夹杂物"}],"language":"zh","publisherId":"jsgncl201203001","title":"<span style=\"color:red\">FeSiB</span>合金熔体的微分热分析和夹杂物研究","volume":"19","year":"2012"},{"abstractinfo":"通过高能球磨技术制备了Fe78 Si13B9磁性非晶合金粉体,采用XRD和DSC分析了Fe78Si13B9非晶合金粉体的相组成、玻璃转变温度Tg、开始晶化温度Tx和晶化峰温度Tp;利用放电等离子烧结(SPS)技术在不同烧结温度下制备了块体磁性非晶纳米晶合金试样,利用XRD、SEM、Gleeble3500、VSM等分析了不同烧结温度下烧结块体试样的相转变特性、微观形貌、力学性能和磁学性能.结果表明,在500 MPa的烧结压力下,随着烧结温度的升高,烧结试样中的非晶相开始逐渐晶化,烧结试样的致密度、抗压强度、微观硬度、饱和磁化强度均显著提高;在500 MPa的烧结压力和823.15 K的烧结温度下,获得了密度为6.6 g/cm3,抗压强度为1500 MPa,饱和磁化强度为1.3864 T的非晶纳米晶磁性材料.","authors":[{"authorName":"王兴华","id":"c44cf8f1-919c-4904-8a9d-083b04f7cee2","originalAuthorName":"王兴华"},{"authorName":"王葛","id":"fc827970-709f-4d43-bf91-500961f21d5a","originalAuthorName":"王葛"},{"authorName":"李强","id":"56d6c6d8-21c8-4f3f-aaad-0ea1f27ab15e","originalAuthorName":"李强"}],"doi":"","fpage":"153","id":"885e3657-acc2-402a-b0e8-991c6cb5a59a","issue":"6","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":"72cfb557-186b-43d6-9bf9-aabc5464026e","keyword":"高能球磨","originalKeyword":"高能球磨"},{"id":"f67ca3f9-daa8-4a9d-9598-58712ca415a7","keyword":"非晶纳米晶","originalKeyword":"非晶纳米晶"},{"id":"e877a914-a9a3-4b13-be04-ffd2bd07bd87","keyword":"磁性材料","originalKeyword":"磁性材料"},{"id":"4b8504fc-c512-4fe2-b7d1-d194bc1fd3ae","keyword":"放电等离子烧结","originalKeyword":"放电等离子烧结"},{"id":"996687b7-7248-437f-beb9-469faf38d771","keyword":"<span style=\"color:red\">FeSiB</span>","originalKeyword":"FeSiB"}],"language":"zh","publisherId":"fhclxb201306023","title":"放电等离子烧结技术制备Fe78Si13B9块体非晶纳米晶磁性材料","volume":"30","year":"2013"}],"totalpage":4,"totalrecord":34}