{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"首先合成了甲基丙烯酸甲酯（MMA）与甲基丙烯酸-N,N-二甲胺乙酯的共聚物P（MMA-co-DMAE-MA）,与聚偏氟乙烯（PVDF）共混经溶液相转化法制备了PVDF/P（MMA-co-DMAEMA）隔膜。研究发现,相对于纯PVDF隔膜,共混隔膜的孔隙率增加,结晶度降低,电解液吸收稳定性显著提高。共混隔膜具有＂活性＂隔膜的性质,隔膜-电解液组成的电解质体系表现出凝胶电解质特征,隔膜中PVDF/P（MMA-co-DMAE-MA）质量比为10/1时,隔膜吸液率在420%以上,活化后凝胶电解质膜离子电导率可达到1.8×10-3S/cm。研究结果表明,采用溶液相转化法制备PVDF/P（MMA-co-DMAEMA）共混隔膜,是一种制备凝胶锂离子电池用高性能活性隔膜的有效方法。","authors":[{"authorName":"刘卫东","id":"3f75e195-121d-4273-a0c8-e9fb6782919c","originalAuthorName":"刘卫东"},{"authorName":"李浩","id":"ce6904b2-762a-4700-ae9b-eff69ae9f93c","originalAuthorName":"李浩"},{"authorName":"<span style=\"color:red\">姚</span><span style=\"color:red\">之</span><span style=\"color:red\">侃</span>","id":"808bcbff-2cbc-463b-9d0a-bfce52e68dbc","originalAuthorName":"姚之侃"},{"authorName":"王婷","id":"493b6261-528f-48dc-b2ed-2af46ce5d07d","originalAuthorName":"王婷"},{"authorName":"朱宝库","id":"cf9daec9-e288-42a4-a412-5796910bd402","originalAuthorName":"朱宝库"},{"authorName":"朱利平","id":"d2a0e6ec-05af-4a7f-9d30-fec9eaf5d538","originalAuthorName":"朱利平"}],"doi":"","fpage":"1364","id":"9ea08b6c-5b3f-4e79-adb6-26a5b4fbda78","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":"b4e1325f-b607-4ffd-9895-734283372597","keyword":"锂离子电池","originalKeyword":"锂离子电池"},{"id":"6c335341-bc89-4f47-a434-992cf98444b0","keyword":"隔膜","originalKeyword":"隔膜"},{"id":"884b1c49-985b-41d8-be73-0e773f4b8779","keyword":"聚偏氟乙烯","originalKeyword":"聚偏氟乙烯"},{"id":"7c009b8d-1c92-4324-a1b9-05df7be80016","keyword":"共混","originalKeyword":"共混"},{"id":"76f14636-0ad9-4871-b720-d36c49f1ea8f","keyword":"电导率","originalKeyword":"电导率"}],"language":"zh","publisherId":"gncl201211002","title":"锂离子电池用PVDF/P（MMA-co-DMAEMA）共混隔膜的制备与性能","volume":"43","year":"2012"},{"abstractinfo":"以<span style=\"color:red\">姚</span>冲大型钼多金属矿床为例，阐明了大别山北麓地区区域和矿床地质特征。通过在该地区开展岩矿石物性标本测试、综合物探剖面性研究（可控源音频大地电磁方法和频谱激电方法试验），试验及测试结果表明，<span style=\"color:red\">姚</span>冲钼矿床中含矿岩体为中低阻，高极化特征，<span style=\"color:red\">姚</span>冲钼矿床为斑岩体外接触带成矿，在深部高阻岩体的外侧存在一个低阻异常体，经钻孔验证，该低阻异常体为花岗斑岩体（脉）外接触带含辉钼矿的中元古界片麻岩。频谱激电法反演结果更进一步印证了物性测试结果和可控源音频大地电磁测深结果的准确性。因此，此次综合物探方法试验结果表明，可控源音频大地电磁测深和频谱激电法在该地区寻找斑岩型钼矿床是有效的，可为今后在该区域寻找斑岩型矿床提供技术参考。","authors":[{"authorName":"李冰","id":"dc65a649-28dc-47d8-8db1-024312fc7661","originalAuthorName":"李冰"},{"authorName":"尚建阁","id":"e954eef9-d05f-408d-803f-97fed70d75fe","originalAuthorName":"尚建阁"},{"authorName":"刘清泉","id":"75897a79-3e77-4a84-80f5-09a97fb9c23a","originalAuthorName":"刘清泉"},{"authorName":"张智慧","id":"719cd997-9746-4138-b915-4a97127e02ee","originalAuthorName":"张智慧"},{"authorName":"丁云河","id":"7a366c93-fb58-43c3-b4e6-d4bc8c2136c2","originalAuthorName":"丁云河"},{"authorName":"魏明君","id":"bd762cc1-2563-4e53-b048-019c2e67f404","originalAuthorName":"魏明君"},{"authorName":"王蒙","id":"749d2edf-03af-4586-815c-096d984d0f12","originalAuthorName":"王蒙"}],"doi":"10.11792/hj20150106","fpage":"21","id":"b4817cdb-b4dd-4360-829e-8de7f5bc0efe","issue":"1","journal":{"abbrevTitle":"HJ","coverImgSrc":"journal/img/cover/HJ.jpg","id":"44","issnPpub":"1001-1277","publisherId":"HJ","title":"黄金"},"keywords":[{"id":"d499d377-380d-4b7a-a3b8-4cdf4d28c530","keyword":"可控源音频大地电磁测深","originalKeyword":"可控源音频大地电磁测深"},{"id":"caea6518-fc2a-4427-b346-39df7c03d3c1","keyword":"频谱激电法","originalKeyword":"频谱激电法"},{"id":"0b1253cc-6352-4895-b452-6c6a5719c227","keyword":"斑岩型钼矿床","originalKeyword":"斑岩型钼矿床"},{"id":"164d2631-4e52-4d0a-9df6-1eb451f2e78b","keyword":"<span style=\"color:red\">姚</span>冲钼多金属矿床","originalKeyword":"姚冲钼多金属矿床"}],"language":"zh","publisherId":"huangj201501007","title":"综合物探方法寻找斑岩型钼矿床的应用试验研究---以<span style=\"color:red\">姚</span>冲钼多金属矿床为例","volume":"","year":"2015"},{"abstractinfo":"通过改变胶体添加剂和热处理参数,提高纤维化器的转速,达到了稳定胶体粘度、改善成纤性能、降低纤维直径、稳定并提高氧化铝纤维质量、降低生产成本<span style=\"color:red\">之</span>目的.","authors":[{"authorName":"王孝瑞","id":"2c4e5f8b-8f27-4e14-87b3-4ee74f6fdda1","originalAuthorName":"王孝瑞"},{"authorName":"付顺德","id":"bbaaeed5-00a8-40f2-af7f-ddf09d6d08bc","originalAuthorName":"付顺德"},{"authorName":"夏超","id":"fc6dd8a5-bc6b-4b2c-969b-d35a45315ba9","originalAuthorName":"夏超"},{"authorName":"申超伟","id":"428c4eea-261e-470a-8416-9f2dfa2ab188","originalAuthorName":"申超伟"},{"authorName":"梁献雷","id":"6a92d557-9f73-462a-843c-e0bf969825d2","originalAuthorName":"梁献雷"},{"authorName":"阴怀亮","id":"c2b4724b-b2c2-43b9-a636-2fd51760dcd5","originalAuthorName":"阴怀亮"}],"doi":"10.3969/j.issn.1001-1935.2000.04.006","fpage":"203","id":"5192906a-b709-46f0-a3f7-6a6a9bcab462","issue":"4","journal":{"abbrevTitle":"NHCL","coverImgSrc":"journal/img/cover/NHCL.jpg","id":"55","issnPpub":"1001-1935","publisherId":"NHCL","title":"耐火材料   "},"keywords":[{"id":"cc28957a-075c-441d-abb5-2ce58ea165c2","keyword":"多晶纤维","originalKeyword":"多晶纤维"},{"id":"690e67ef-e03d-4983-aae0-d7ca0ec62a8a","keyword":"氧化铝纤维","originalKeyword":"氧化铝纤维"}],"language":"zh","publisherId":"nhcl200004006","title":"稳定多晶氧化铝纤维质量<span style=\"color:red\">之</span>研究","volume":"34","year":"2000"},{"abstractinfo":"以往成信氧化鋯基陶瓷材料<span style=\"color:red\">之</span>韌化機制主要爲正方相轉變爲單斜相<span style=\"color:red\">之</span>相變化及正方晶<span style=\"color:red\">之</span>鐵彈性域轉移,惟其主要應用在發生塑性變形範圍,而在承受循環負荷<span style=\"color:red\">之</span>彈性變形範圍則鮮少論及.本研究發現該材料系統在承受彈性<span style=\"color:red\">之</span>循環負荷作用下,表現出奇特之能量吸收特性,亦即,因應力誘發而使立方相轉换爲具有類橡膠特性<span style=\"color:red\">之</span>斜方相,或是立方相轉换爲不會發生相變<span style=\"color:red\">之</span>正方相,此應爲氧化鋯基材料系統在彈性變形範圍<span style=\"color:red\">之</span>韌化機制,爲一國際上創新<span style=\"color:red\">之</span>發現.","authors":[],"doi":"","fpage":"52","id":"8b1e51c4-d094-444a-be42-6fa00b377d25","issue":"z3","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"9d7532ab-0859-4cc5-8a2a-1ebdcb6ac1d2","keyword":"氧化鋯","originalKeyword":"氧化鋯"},{"id":"e15f608a-ab46-4954-9ed4-7d26b9d5aeef","keyword":"相變化","originalKeyword":"相變化"},{"id":"1a4fa773-69a0-4f12-8549-a2c1c31da57e","keyword":"同步輻射","originalKeyword":"同步輻射"},{"id":"eb51b92d-51fd-483e-b812-348a9f668756","keyword":"X-光繞射","originalKeyword":"X-光繞射"},{"id":"1837c1d2-c848-43d4-b37d-5fe617fdb629","keyword":"拉曼光譜","originalKeyword":"拉曼光譜"},{"id":"94dcd381-b5bd-4a62-a174-248f41ac5bbd","keyword":"應力-應變曲綫","originalKeyword":"應力-應變曲綫"}],"language":"zh","publisherId":"cldb2004z3015","title":"氧化鋯基陶瓷承受循環負荷<span style=\"color:red\">之</span>奇特式能量吸收機制","volume":"18","year":"2004"},{"abstractinfo":"以往咸信氧化鋯基陶瓷材料<span style=\"color:red\">之</span>韌化機制主要爲正方相轉變爲單斜相<span style=\"color:red\">之</span>相變化及正方晶<span style=\"color:red\">之</span>鐵彈性域轉移,惟其主要應用在發生塑性變形範圍,而在承受循環負荷<span style=\"color:red\">之</span>彈性變形範圍則鮮少論及.本研究發現該材料系統在承受彈性<span style=\"color:red\">之</span>循環負荷作用下,表現出奇特之能量吸收特性,亦即,因應力诱發而使立方相轉换爲具有類橡膠特性<span style=\"color:red\">之</span>斜方相,或是立方相轉换爲不會發生相變<span style=\"color:red\">之</span>正方相,此應爲氧化锆基材料系統在彈性變形範圍<span style=\"color:red\">之</span>韌化機制,爲一國際上創新<span style=\"color:red\">之</span>發現.","authors":[{"authorName":"喻盛地","id":"347aaf66-ae2f-43bd-ab06-75cbe5e93b0a","originalAuthorName":"喻盛地"}],"doi":"","fpage":"102","id":"b4e3c640-c8dd-4369-a018-df860fa412b8","issue":"8","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"b12000ce-9a1e-4c0c-98c3-6d470626cdd1","keyword":"氧化鋯","originalKeyword":"氧化鋯"},{"id":"8ecf0186-e33b-4624-941c-89c851b2d940","keyword":"相變化","originalKeyword":"相變化"},{"id":"fd690a2d-a385-496e-bd69-cf31bf7579b3","keyword":"同步輻射","originalKeyword":"同步輻射"},{"id":"cf553bdc-6864-4879-8810-7c3438a761e5","keyword":"X-光繞射","originalKeyword":"X-光繞射"},{"id":"8ae4ee89-321f-4700-b0da-4227344c97df","keyword":"拉曼光譜","originalKeyword":"拉曼光譜"},{"id":"ef1fb342-a8ed-4477-b4c3-8ac2f8892b2b","keyword":"應力-應變曲綫","originalKeyword":"應力-應變曲綫"}],"language":"zh","publisherId":"cldb200408028","title":"氧化鋯基陶瓷承受循環負荷<span style=\"color:red\">之</span>奇特式能量吸收機制","volume":"18","year":"2004"},{"abstractinfo":"本文系探討一種具高玻璃形成能力<span style=\"color:red\">之</span>鋯基(Zr-Cu-Al-Ni)的非晶合金薄膜,以减鍍沉積成達10μm以上厚度<span style=\"color:red\">之</span>薄膜,再經由退火過程而誘發廣泛遍布整個薄膜的部份或全部非晶相.此種可控制<span style=\"color:red\">之</span>整佃薄膜的內泛非晶相反應能明顯影響薄膜性質(如硬度與電阻值等),方便建立組成結構和薄膜性質<span style=\"color:red\">之</span>間的關系,退而設計出具有特定性質的薄膜,文章將進一步探討固態非晶化的機制.","authors":[],"doi":"","fpage":"85","id":"49879886-2605-4131-8ebb-c51dd865ed7f","issue":"z3","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"ee2cb0c3-60cb-496e-8a6c-1f18811f85b3","keyword":"固熊非晶質化","originalKeyword":"固熊非晶質化"},{"id":"fdedc034-99f9-4af2-bb3a-419926e39742","keyword":"濺鍍薄膜","originalKeyword":"濺鍍薄膜"},{"id":"1fca48cb-e49c-4410-a60a-dc0a24b4a1ad","keyword":"大塊非晶","originalKeyword":"大塊非晶"}],"language":"zh","publisherId":"cldb2004z3025","title":"金屬薄膜<span style=\"color:red\">之</span>退火非晶質化現象","volume":"18","year":"2004"},{"abstractinfo":"熔融還原煉鐵法爲直接以煤及鐵礦粉取代焦碳和燒結礦爲原料的一替代性有發展潜力的制程.而熔融還原爐法中鐵礦還原速率<span style=\"color:red\">之</span>好壞與泡沫渣<span style=\"color:red\">之</span>控制,亦即溶渣的黏度、表面張力及密度和温度等有極重要的關系.本文主要希望介绍熔融還原煉鐵法爐渣黏度與爐渣成份及温度等變數<span style=\"color:red\">之</span>關系.研究的爐渣成份主要分成兩大類,分别是①四元系列的SiO2-CaO-MgO-Al2O3,鹽基度變化爲0.9～1.3;②氧化鐵範圍爲FeO 1%～7%,氧化镁MgO,鹽基度固定爲1.08的五元渣系SiO2-CaO-MgOsat-Al2O3-FeO爐渣.實難以高温轉鉅黏度計,量測不同成份及温度的黏度值.實難結果發現黏度與温度基本上呈反比的趨勢,可以Arrhenius equation或Eyring′s expression式子說明黏度與温度的關系.有關黏度與成份的關系,分别以熱力學綱状結構黏度模式、氧橋鍵結矽離子黏度模式與光學鹽基度黏度模式計算其黏度值,其結果爲利用氧橋鍵矽離子黏度模式與本實難的黏度量測值及文獻黏度量測值最接近.基本上黏度值随基鹽度的上升及随FeO量增加而下降,但黏度随著SiO2量增加而增加.至於黏度與温度則呈現反比的趨勢.","authors":[{"authorName":"連雙喜","id":"4ab0ac11-5e9d-481b-991f-fea11c087da5","originalAuthorName":"連雙喜"},{"authorName":"陳柏楊","id":"324571ff-37ae-468f-8c8a-7e559ad917f7","originalAuthorName":"陳柏楊"},{"authorName":"劉世賢","id":"685757c4-8fdb-4567-a3e3-1bd7573a3bb1","originalAuthorName":"劉世賢"},{"authorName":"蔡辛慈","id":"1c50d3a5-9707-4eaf-8919-0bbf9c55fe94","originalAuthorName":"蔡辛慈"}],"doi":"","fpage":"74","id":"262494e3-15ca-418d-b7b8-98ef61b69c3f","issue":"8","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"2f5e2dce-f6ee-4018-b698-eb784b679e39","keyword":"熔融還原","originalKeyword":"熔融還原"},{"id":"1cb2394a-72a4-4a4d-a92e-b6ca89f1f845","keyword":"鐵渣","originalKeyword":"鐵渣"},{"id":"98b60e1c-719a-496c-8cdf-68bdd5c49a7e","keyword":"黏度","originalKeyword":"黏度"},{"id":"521809a7-f7e0-4a0d-8728-84758770878d","keyword":"計算模式","originalKeyword":"計算模式"}],"language":"zh","publisherId":"cldb200408022","title":"熔融還原煉鐵渣黏度<span style=\"color:red\">之</span>計算模式","volume":"18","year":"2004"},{"abstractinfo":"熔融還原煉鐵法爲直接以煤及鐵礦粉取代焦碳和燒結礦爲原料的一替代性有發展潜力的制程.而熔融還原爐法中鐵礦還原速率<span style=\"color:red\">之</span>好壞與泡沫渣<span style=\"color:red\">之</span>控制,亦即溶渣的黏度、表面張力及密度和温度等有極重要的關系.本文主要希望介紹熔融還原煉鐵法爐渣黏度與爐渣成份及温度等變數<span style=\"color:red\">之</span>關系.研究的爐渣成份主要分成雨大類,分别是①四元系列的SiO2-CaO-MgO-Al2O3,鹽基度變化爲0.9～1.3;②氧化鐵範圍爲FeO 1%～7%,氧化鎂MgO,鹽基度固定爲1.08的五元渣系SiO2-CaO-MgOsat-Al2O3-FeO爐渣.實驗以高温轉鉅黏度計,量測不同成份及温度的黏度值.實驗結果發現黏度與温度基本上呈反比的趨势,可以Arrhenius equation或Eyring's expression式子說明黏度與温度的關系.有關黏度與成份的關系,分别以熱力學網状結構黏度模式、氧橋鍵結矽離子黏度模式與光學鹽基度黏度模式計算其黏度值,其結果爲利用氧橋鍵矽離子黏度模式與本實驗的黏度量測值及文獻黏度量測值最接近.基本上黏度值随基鹽度的上升及随FeO量增加而下降,但黏度随著SiO2量增加而增加.至於黏度與温度則呈現反比的趋势.","authors":[],"doi":"","fpage":"123","id":"7ea8648d-4292-4adb-b5f4-afc3b35e5c0d","issue":"z3","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"d8bcbd13-74f2-4e2c-91a9-2bf026adb052","keyword":"熔融還原","originalKeyword":"熔融還原"},{"id":"b234ab5f-9895-4a37-98ad-4d482a45fba7","keyword":"鐵渣","originalKeyword":"鐵渣"},{"id":"c5af6015-e1fd-4226-8ed5-db4de3ac2000","keyword":"黏度","originalKeyword":"黏度"},{"id":"b0dfd73c-4cb5-4d25-81a1-277c1c5fcb3b","keyword":"計算模式","originalKeyword":"計算模式"}],"language":"zh","publisherId":"cldb2004z3038","title":"熔融還原煉鐵渣黏度<span style=\"color:red\">之</span>計算模式","volume":"18","year":"2004"},{"abstractinfo":"济钢三炼钢厂1号板坯连铸机,从投产到目前已经开浇1200多次,通过某些具体措施的实施,开浇成功率达到了百分<span style=\"color:red\">之</span>百,创造了较好的经济效益.","authors":[{"authorName":"赵登报","id":"ee406ebb-996b-4ad1-b1e1-881faef54eb2","originalAuthorName":"赵登报"},{"authorName":"贾延利","id":"339d8132-e627-4b64-9c0a-b2cc5c3be720","originalAuthorName":"贾延利"},{"authorName":"赵丽","id":"6502b5b2-1485-46e7-8878-0ace931b5415","originalAuthorName":"赵丽"},{"authorName":"叶勇","id":"c2cdaf59-d1a0-47a2-bd3d-7cf5fc6a5b3e","originalAuthorName":"叶勇"},{"authorName":"李士波","id":"464fab8a-556f-45d5-8af4-b30c82f2cd16","originalAuthorName":"李士波"}],"doi":"10.3969/j.issn.1005-4006.2006.02.004","fpage":"9","id":"27a6c3ed-6ba9-4599-b635-46636dd87874","issue":"2","journal":{"abbrevTitle":"LZ","coverImgSrc":"journal/img/cover/LZ.jpg","id":"52","issnPpub":"1005-4006","publisherId":"LZ","title":"连铸"},"keywords":[{"id":"896da863-04d2-429c-a04b-80453ac89312","keyword":"","originalKeyword":""}],"language":"zh","publisherId":"lz200602004","title":"开浇成功率百分<span style=\"color:red\">之</span>百的生产实践","volume":"","year":"2006"},{"abstractinfo":"本研究計()<span style=\"color:red\">之</span>目的,系探討沃斯田鐵面心立方結構<span style=\"color:red\">之</span>鐵-9鋁-30 錳-1碳-0.5矽合金,兩種試樣時效熱處理后内部微析出物顯微結構與超順磁性質<span style=\"color:red\">之</span>關系,兩種試樣分别爲固溶油冷與固溶油冷鍛應變20%～50%,再同時於823K持温140天時效處理.本研究結果顯示:此種合金固溶油冷經冷鍛應變再時效析出處理,可以顯著地改善此種合金内部微結構磁性相析出物<span style=\"color:red\">之</span>導磁率與饱和磁化强度,其原因系歸因於沃斯田鐵相面心立方結構<span style=\"color:red\">之</span>鐵鋁錳碳合金,固溶處理,再經20%～50%<span style=\"color:red\">之</span>冷鍛加工應變(變形)后,則在{111}八面體原子最密集結晶面<span style=\"color:red\">之</span><110>原子最密集向量上,會引生叠差與可動差排密度量<span style=\"color:red\">之</span>增加,進而在沃斯田鐵基地内部,增加叠差能與差排<span style=\"color:red\">之</span>相互作用,并促成差排核心鐵/錳-碳偶合(Fe/Mn-C couples)的碳原子重新取向,所以應變與時效析出處理,能提升此種材料内部差排和其相關溶質原子<span style=\"color:red\">之</span>擴散與物理化學反應,進而提升時效處理后,合金内部<span style=\"color:red\">之</span>微結構磁性相析出物在非磁性基地的時效析出效果,并改善時效處理后,試樣内部<span style=\"color:red\">之</span>微結構磁性相析出物<span style=\"color:red\">之</span>導磁率與饱和磁化强度.X-ray繞射實難與穿透式電子顯微鏡(TEM)研究證實:微結構磁性相析出物系源自於層狀κ-相的相變能反應所産生<span style=\"color:red\">之</span>産物,而微結構磁性相析出物(B2+D03)與κ-相<span style=\"color:red\">之</span>結晶方向關系爲[1￣12](B2+D03)∥[￣133]k;[￣300](B2+D03)∥[￣400](B2+D03)∥[011]κ,及微結構磁性相析出物α′-Mn與B2<span style=\"color:red\">之</span>結晶方向關系爲[001]α′-Mn∥[123]B2.","authors":[{"authorName":"林英志","id":"40075310-929f-4f81-a9d4-78b4150b07c3","originalAuthorName":"林英志"}],"doi":"","fpage":"114","id":"0e11c104-c8ae-4faa-8e56-7bb6704739df","issue":"8","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"2c860452-4dc3-476f-9573-bc4768ae7f02","keyword":"應變時效","originalKeyword":"應變時效"},{"id":"4fce3573-ce80-46d7-ac1f-540533c24e63","keyword":"微細析出物","originalKeyword":"微細析出物"},{"id":"e46eb927-b799-488e-88f2-9a83a4498d9e","keyword":"磁性","originalKeyword":"磁性"}],"language":"zh","publisherId":"cldb200408031","title":"應變時效處理鐵鋁錳碳合金的相變態與超順磁微結構<span style=\"color:red\">之</span>研究","volume":"18","year":"2004"}],"totalpage":89,"totalrecord":890}