{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"系统分析了热喷涂技术的发展历程与最新动态,提出了\"三阶段<span style=\"color:red\">演化</span>规律\"(热能的较量、动能的较量、创新理念的较量),并就工艺特性与潜在应用两方面较详细地探讨了几种新颖的喷涂工艺:低压等离子喷涂-薄涂层技术(LPPS-TF)、冷喷涂(CS)和液料等离子喷涂(SPS/SPPS).结合国内外热喷涂产业发展现状,尝试提出了几点亟待国内热喷涂界同仁共同努力的方向,最后展望了热喷涂工艺与产业的未来发展.","authors":[{"authorName":"尹志坚","id":"f8c7f209-55d4-419a-9c10-fba52aac1229","originalAuthorName":"尹志坚"},{"authorName":"王树保","id":"a04a1928-5b02-43ef-8aa7-e434d60e54c0","originalAuthorName":"王树保"},{"authorName":"傅卫","id":"f038d199-7f46-4632-8718-00002b57cfaf","originalAuthorName":"傅卫"},{"authorName":"谭兴海","id":"7c6a8469-4a82-4cff-8032-6da432b845cb","originalAuthorName":"谭兴海"},{"authorName":"陶顺衍","id":"9e28c80b-c73b-4946-b19e-4e47fdff866f","originalAuthorName":"陶顺衍"},{"authorName":"丁传贤","id":"94bcc870-ff73-41fc-91fa-a6fc97acb1a3","originalAuthorName":"丁传贤"}],"doi":"10.3724/SP.J.1077.2011.00225","fpage":"225","id":"2092402a-0f43-4336-a6e0-511bcf0b65f8","issue":"3","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":"8c28d767-0d99-4929-bc8a-931e5e6d505e","keyword":"热喷涂","originalKeyword":"热喷涂"},{"id":"6a9c7d6c-f3c0-4985-9625-9addee5ec4c6","keyword":"<span style=\"color:red\">演化</span>","originalKeyword":"演化"},{"id":"c68a564a-7dd7-4935-aac8-842ddb7e2199","keyword":"应用","originalKeyword":"应用"},{"id":"e5f52b1d-906d-4c0e-aff7-14d5457154a9","keyword":"展望","originalKeyword":"展望"},{"id":"55f77ec0-3852-4d7a-bc05-fd68fb41c99f","keyword":"综述","originalKeyword":"综述"}],"language":"zh","publisherId":"wjclxb201103001","title":"热喷涂技术的<span style=\"color:red\">演化</span>与展望","volume":"26","year":"2011"},{"abstractinfo":"研究了色散光纤混沌传输理论及混沌信号与色散光纤相互作用的物理机制;通过耦合激光混沌系统和色散光纤传输信道,提出了色散光纤混沌信号传输<span style=\"color:red\">演化</span>物理模型;提出混沌信号在色散光纤传输中的非线性<span style=\"color:red\">演化</span>频率啁啾和公式;着重分析光纤色散对激光混沌信号传输与<span style=\"color:red\">演化</span>的作用,色散能够展宽混沌信号脉冲,但不影响混沌信号的形状;色散能够改变混沌信号每个频谱分量相位,但不影响混沌信号频谱形状;色散能够改变混沌信号光场慢变场分量的变化,但不改变混沌信号包络时变特性,也不影响混沌信号脉冲的功率分布和场强分布;色散能够改变混沌吸引子在相空间整体旋转角度并使其旋转角度随光纤传输长度而发生改变,但不改变混沌吸引子在相空间中的内部结构.最后数值模拟了混沌信号在光纤传输过程中的相位、场慢变部分分量以及混沌吸引子等<span style=\"color:red\">演化</span>形式等.","authors":[{"authorName":"颜森林","id":"646c77b0-282e-49b5-9f93-3552187b9fbc","originalAuthorName":"颜森林"}],"doi":"10.3969/j.issn.1007-5461.2007.05.021","fpage":"640","id":"5491287a-9d73-41e8-a447-f70cc01e5123","issue":"5","journal":{"abbrevTitle":"LZDZXB","coverImgSrc":"journal/img/cover/LZDZXB.jpg","id":"53","issnPpub":"1007-5461","publisherId":"LZDZXB","title":"量子电子学报   "},"keywords":[{"id":"2150d99f-3542-46db-84f6-384b5794409c","keyword":"非线性光学","originalKeyword":"非线性光学"},{"id":"efeeb392-1d48-4a84-8687-55cd243f17c3","keyword":"<span style=\"color:red\">演化</span>","originalKeyword":"演化"},{"id":"06fad616-e4af-415e-9ef0-7df0e3b09969","keyword":"混沌","originalKeyword":"混沌"},{"id":"22404fe8-493c-417e-bc5f-8aa0a9623e29","keyword":"光纤","originalKeyword":"光纤"},{"id":"24f1c7c7-2f7b-4b04-a667-f5d6c2ff5492","keyword":"传输","originalKeyword":"传输"},{"id":"ad1d2316-1ff5-46c6-aedb-d6376ed6eb1e","keyword":"色散","originalKeyword":"色散"}],"language":"zh","publisherId":"lzdzxb200705021","title":"混沌信号在色散光纤传输过程中的<span style=\"color:red\">演化</span>","volume":"24","year":"2007"},{"abstractinfo":"基于一维平板鞘层模型,建立了脉冲偏压电弧离子镀(PBAIP)鞘层随时间<span style=\"color:red\">演化</span>的动力学模型,给出了其解析表达式,并结合PBAIP工艺中等离子体参数的测量结果,模拟分析了PBAIP鞘层的厚度和鞘层中的离子流密度随时间的<span style=\"color:red\">演化</span>规律及其受脉冲偏压幅度等参数的影响.结果表明:在PBAIP工艺中,稳态鞘层的厚度及形成稳态鞘层的时间均远小于已报道的等离子体源注入(PSⅡ)等鞘层对应的值;PBAIP鞘层的扩展几乎是实时跟随脉冲偏压的变化,脉冲偏压下每一时刻的鞘层厚度与对应直流偏压下的鞘层厚度几乎相等.","authors":[{"authorName":"戚栋","id":"b6e22e30-7772-4ce1-9bea-e8490736db19","originalAuthorName":"戚栋"},{"authorName":"王宁会","id":"a1cf6181-33af-4db0-8ae8-8c93f891b8d6","originalAuthorName":"王宁会"},{"authorName":"林国强","id":"3cb15550-4f92-43f9-b03e-d23e32d49457","originalAuthorName":"林国强"},{"authorName":"董闯","id":"429bcf56-9125-428b-93ae-53ca6c657f7b","originalAuthorName":"董闯"}],"doi":"10.3321/j.issn:0412-1961.2006.08.015","fpage":"861","id":"427f1885-3c03-48e1-afc8-75a5d3eb4187","issue":"8","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"1b7df728-da49-4897-b0c1-e1f934893320","keyword":"脉冲偏压电弧离子镀(PBAIP)","originalKeyword":"脉冲偏压电弧离子镀(PBAIP)"},{"id":"187eb37d-e896-494f-b5bf-0812b4f8ea0e","keyword":"鞘层","originalKeyword":"鞘层"},{"id":"79591e96-1055-47e3-8332-8a7f853afdb6","keyword":"<span style=\"color:red\">演化</span>","originalKeyword":"演化"},{"id":"8f7038f0-4225-40ba-b863-372a64c6757f","keyword":"数值模拟","originalKeyword":"数值模拟"}],"language":"zh","publisherId":"jsxb200608015","title":"脉冲偏压电弧离子镀鞘层尺度<span style=\"color:red\">演化</span>的特性与分析","volume":"42","year":"2006"},{"abstractinfo":"裂纹愈合是一个不可逆的热力学过程.笔者在连续介质热力学框架内,由热力学第二定律推导出裂纹愈合耗散不等式,定义了描述金属材料内部裂纹愈合过程的热力学内变量H.以铜单晶为例,依据分子动力学模拟结果对铜单晶内部微裂纹愈合过程中愈合内变量的<span style=\"color:red\">演化</span>趋势进行了定量分析.","authors":[{"authorName":"张永军","id":"d92f4d8c-fb82-4a41-b799-31c2a7a22ca5","originalAuthorName":"张永军"},{"authorName":"韩静涛","id":"6d72c3c9-c089-4e64-81ca-a4bdf12d9e48","originalAuthorName":"韩静涛"},{"authorName":"韦东滨","id":"23023741-d757-4906-a952-d1d788fa597b","originalAuthorName":"韦东滨"}],"doi":"","fpage":"59","id":"c0ed9702-32a5-4596-ac0d-f6d029f428c4","issue":"2","journal":{"abbrevTitle":"GTYJXB","coverImgSrc":"journal/img/cover/GTYJXB.jpg","id":"30","issnPpub":"1001-0963","publisherId":"GTYJXB","title":"钢铁研究学报"},"keywords":[{"id":"c5deffbc-3025-41ba-901a-0d44af16e81d","keyword":"微裂纹","originalKeyword":"微裂纹"},{"id":"6228627d-e35e-4b7f-ad4f-c6b0aec1342b","keyword":"愈合","originalKeyword":"愈合"},{"id":"440df5a1-0bd3-4932-9781-030883fda5c9","keyword":"内变量","originalKeyword":"内变量"},{"id":"07f4f947-e66e-419c-bf07-4ada0f48de91","keyword":"<span style=\"color:red\">演化</span>","originalKeyword":"演化"},{"id":"e89835ba-eda2-439c-8cfd-6ccb8ec7c0b7","keyword":"金属","originalKeyword":"金属"}],"language":"zh","publisherId":"gtyjxb200402015","title":"金属内部微裂纹愈合内变量及其<span style=\"color:red\">演化</span>分析","volume":"16","year":"2004"},{"abstractinfo":"采用射频等离子体化学气相沉积(RF-PECVD)方法制备了沉积时间系列的微晶硅薄膜.采用椭圆偏振光谱仪(SE)和原子力显微镜(AFM)表征薄膜表面粗糙度,分析了表面粗糙度随沉积时间的<span style=\"color:red\">演化</span>行为.讨论了这两种测量手段在分析薄膜表面粗糙度时的差异.结果表明,采用SE拟合得到的表面粗糙度数值要大于采用AFM直接测量得到的结果.产生差异的原因,一是由于两种测量手段的测量机制不同;二是由于薄膜的结构不均匀导致薄膜表面形貌差异.另外,还发现这两种测量手段得到的表面粗糙度数值之间存在线性关系.","authors":[{"authorName":"李新利","id":"29f6321b-872d-4186-834f-d9df18431313","originalAuthorName":"李新利"},{"authorName":"马战红","id":"5ded0e09-1fbc-45f2-b057-5e259e811669","originalAuthorName":"马战红"},{"authorName":"任凤章","id":"0b7d76ef-dfc4-48fd-8da6-0d3da9d881aa","originalAuthorName":"任凤章"},{"authorName":"许荣辉","id":"fac7eb6c-0254-4af6-b73b-3f703b6563ff","originalAuthorName":"许荣辉"},{"authorName":"柳勇","id":"79286706-b067-45bb-b6b0-572542a0787a","originalAuthorName":"柳勇"}],"doi":"","fpage":"2384","id":"2b6891e4-1990-48d5-ac33-c53b916be832","issue":"9","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":"9150f8cd-5398-429d-96a1-2694fae1bcd1","keyword":"射频等离子体化学气相沉积","originalKeyword":"射频等离子体化学气相沉积"},{"id":"4aaf829a-70e1-45a3-93f9-86779c3841d5","keyword":"微晶硅薄膜","originalKeyword":"微晶硅薄膜"},{"id":"011df7df-1ec4-4727-8d0b-bc37f7765fc6","keyword":"表面粗糙度","originalKeyword":"表面粗糙度"},{"id":"72e12919-38a8-4b72-ad4d-52870003f8b6","keyword":"<span style=\"color:red\">演化</span>","originalKeyword":"演化"}],"language":"zh","publisherId":"rgjtxb98201409036","title":"微晶硅薄膜表面粗糙度的<span style=\"color:red\">演化</span>过程分析","volume":"43","year":"2014"},{"abstractinfo":"借助X射线衍射仪、透射电镜及显微硬度仪等先进仪器,研究经超音速微粒轰击(SFPB)处理TC17合金表面自身纳米化晶粒尺寸<span style=\"color:red\">演化</span>及纳米化机理.结果表明:超音速微粒轰击使TC17合金表面获得了纳米组织,并发生显著的加工硬化,表面显微硬度比基体硬度提高了1倍左右;随着SFPB处理时间的延长,纳米结构层厚度不断增加,晶粒逐步细化,当SFPB处理30 min后晶粒尺寸趋于稳定,在最表层形成了晶粒尺寸约为16.3 nm具有随机取向的等轴纳米晶粒.TC17合金表面自身纳米化主要是位错滑移、位错分割的结果;由于外界多方向载荷的重复作用而产生大量的位错,位错的滑移、积累、交互作用而产生位错墙和位错纠结,位错继续运动进而产生亚晶界、亚晶;随着应变的增加,更多的位错在亚晶界处产生和湮灭,从而使亚晶界、亚晶转变为晶界、晶粒;当位错的产生和湮灭速率达到平衡时,晶粒达到纳米量级.","authors":[{"authorName":"赵坤","id":"3ac324ce-9a6c-4c98-92e5-24ed631f8099","originalAuthorName":"赵坤"},{"authorName":"王敏","id":"6646b9b9-2aa7-4a68-83d3-b094685fcdd0","originalAuthorName":"王敏"},{"authorName":"蔺成效","id":"062d5483-8448-43e8-8758-376629ec61c7","originalAuthorName":"蔺成效"},{"authorName":"拓川","id":"4d6ae80e-8ae4-4d69-9f87-c731ae21a53c","originalAuthorName":"拓川"}],"doi":"","fpage":"2048","id":"357eb4f5-8559-405b-85be-dc9ef1f8d72a","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":"d90e8d8c-723f-4544-b784-74d05bfd9f41","keyword":"TC17合金","originalKeyword":"TC17合金"},{"id":"23fee64c-1ab4-4664-af04-f41b8cfe8168","keyword":"表面自身纳米化","originalKeyword":"表面自身纳米化"},{"id":"386db0a9-2fdf-4345-83d3-e2017c7f73c1","keyword":"机制","originalKeyword":"机制"},{"id":"28153491-6177-40a2-830b-2cae1db8bdf3","keyword":"<span style=\"color:red\">演化</span>","originalKeyword":"演化"},{"id":"4f9956c5-af23-429d-bf74-ccb2bb8a8130","keyword":"位错","originalKeyword":"位错"}],"language":"zh","publisherId":"xyjsclygc201310014","title":"TC17钛合金自表面纳米化机制及组织<span style=\"color:red\">演化</span>","volume":"42","year":"2013"},{"abstractinfo":"微裂纹的生长与<span style=\"color:red\">演化</span>是导致准脆性材料损伤及破坏的本质,本工作对承载过程中准脆性材料内部的椭圆形微裂纹的生长与<span style=\"color:red\">演化</span>规律进行研究.采用复势函数求解受远场载荷作用下代表性单元中椭圆形微裂纹的变形,讨论了椭圆形微裂纹初始取向的变化对微裂纹尺寸增长的影响,并结合微裂纹扩展准则推导出损伤开始时的临界应力条件.基于翼型裂纹扩展过程的能量守恒关系,建立了损伤阶段的本构关系.","authors":[{"authorName":"方敏杰","id":"f5698de3-e02a-4fc3-9c3e-64706f15a9e4","originalAuthorName":"方敏杰"},{"authorName":"任会兰","id":"d5b442d7-290e-403b-a713-d38e9e4d8b00","originalAuthorName":"任会兰"},{"authorName":"宁建国","id":"91780fe1-084d-478e-9e5d-09b059695a26","originalAuthorName":"宁建国"}],"doi":"10.3969/j.issn.1001-4381.2013.02.007","fpage":"35","id":"d707ad98-bab9-4b12-a540-67492e5f86df","issue":"2","journal":{"abbrevTitle":"CLGC","coverImgSrc":"journal/img/cover/CLGC.jpg","id":"9","issnPpub":"1001-4381","publisherId":"CLGC","title":"材料工程"},"keywords":[{"id":"2c4a46ad-aa04-486b-ad2d-b495e5b19f28","keyword":"微裂纹","originalKeyword":"微裂纹"},{"id":"cd16a83d-2e78-43a4-93f2-42c5b3d86196","keyword":"损伤","originalKeyword":"损伤"},{"id":"6aa28b8d-0676-43b1-bb82-b8dd25e91def","keyword":"<span style=\"color:red\">演化</span>","originalKeyword":"演化"}],"language":"zh","publisherId":"clgc201302007","title":"准脆性材料中椭圆形微裂纹的生长与<span style=\"color:red\">演化</span>","volume":"","year":"2013"},{"abstractinfo":"对12根锈蚀钢筋混凝土梁进行了地震损伤分析,得到锈蚀梁地震损伤指数随加载循环水平的变化曲线,即D-N曲线,分析了锈蚀钢筋混凝土梁地震损伤<span style=\"color:red\">演化</span>规律以及钢筋锈蚀率、试件破坏形式对地震损伤指数的影响.研究结果表明:锈蚀钢筋混凝土梁地震损伤指数随循环水平的增加而增大,且地震损伤指数增长速率逐渐加大;同一循环水平下锈蚀梁地震损伤指数随锈蚀率的增加而增大,而对于锈蚀率低于5％的锈蚀混凝土梁试件,由于锈蚀改善了钢筋与混凝土间的粘结性能,其损伤指数略低于未锈蚀梁的损伤指数;纵筋与箍筋同时锈蚀的混凝土梁地震损伤<span style=\"color:red\">演化</span>规律与仅箍筋锈蚀的混凝土梁损伤<span style=\"color:red\">演化</span>类似;随着锈蚀率增大,锈蚀钢筋混凝土梁将由弯曲破坏演变为剪切破坏,与发生弯曲破坏的锈蚀梁相比,锈蚀梁发生剪切破坏时地震损伤指数较小,但绝大多数损伤指数均大于0.6;锈蚀钢筋混凝土梁地震损伤模型中试件经历的循环加载位移幅值对损伤指数起主控作用.","authors":[{"authorName":"邢国华","id":"ef1420d0-67ad-49b2-b136-6d0233f6b161","originalAuthorName":"邢国华"},{"authorName":"孙诚","id":"b87f61ce-c967-458f-9f9d-eb41e1f9b5c0","originalAuthorName":"孙诚"},{"authorName":"项荣晨","id":"89b79de0-7695-4191-8fbe-920de0af7258","originalAuthorName":"项荣晨"},{"authorName":"刘伯权","id":"26159c1f-7e3b-4b24-b407-9e4b4917301a","originalAuthorName":"刘伯权"}],"doi":"","fpage":"3330","id":"40f703de-08ae-4eac-91c8-d71e7d82d27c","issue":"10","journal":{"abbrevTitle":"GSYTB","coverImgSrc":"journal/img/cover/GSYTB.jpg","id":"36","issnPpub":"1001-1625","publisherId":"GSYTB","title":"硅酸盐通报   "},"keywords":[{"id":"3d683c35-e14f-48ab-814e-2fcb53ddb149","keyword":"钢筋混凝土梁","originalKeyword":"钢筋混凝土梁"},{"id":"b0a3f0f6-c7d5-4f8a-b7c2-954ddc348609","keyword":"箍筋","originalKeyword":"箍筋"},{"id":"7a3e8a4d-0675-4c1c-91cf-c64f7cfe8548","keyword":"锈蚀率","originalKeyword":"锈蚀率"},{"id":"d07698fb-311d-40e8-bed2-e86b9b1588ec","keyword":"地震损伤指数","originalKeyword":"地震损伤指数"},{"id":"8a6c6105-6a0f-4603-9dce-d017e27c8b60","keyword":"<span style=\"color:red\">演化</span>","originalKeyword":"演化"}],"language":"zh","publisherId":"gsytb201610042","title":"锈蚀钢筋混凝土梁地震损伤分析","volume":"35","year":"2016"},{"abstractinfo":"山西繁峙县义兴寨金矿田位于晋东北地区NW向中生代构造岩浆活动带中.以义兴寨、辛庄金矿床为研究对象,分析本区关键控矿因素、成矿物质来源、成矿流体来源及其<span style=\"color:red\">演化</span>,进而开展矿田成矿机理的研究.结果表明:本区构造具有多期活动的特征,规模较大的NW向区域性张性大断裂为本区的控岩、导矿及配矿构造,次级NNW向压-张扭性断裂裂隙为容矿构造,不同形式、不同级别的构造是成矿最重要的控制因素.S、Pb、H、O同位素组成及微量元素地球化学特征表明,岩浆活动为本区提供了成矿物质及成矿流体.流体包裹体特征及宏观地质特征表明,成矿过程中成矿流体发生了沸腾作用,引起CO2、H2S等的逸失,含金络合物稳定性遭受破坏,导致Au的大规模沉淀,流体的沸腾是矿质沉淀的主要机制.","authors":[{"authorName":"彭南海","id":"194ede2b-f6d8-4529-bd62-d230147a549d","originalAuthorName":"彭南海"},{"authorName":"邵拥军","id":"b4936921-479e-4018-9807-802c4dcce4e1","originalAuthorName":"邵拥军"},{"authorName":"刘忠法","id":"d497a788-a669-4751-8393-6f8eb48279b2","originalAuthorName":"刘忠法"},{"authorName":"汪程","id":"1abb40d1-2002-4951-87c6-596299ce06a9","originalAuthorName":"汪程"}],"doi":"","fpage":"305","id":"ace49ae6-e9d7-4d65-8c2e-d6028dc15e9c","issue":"2","journal":{"abbrevTitle":"ZGYSJSXB","coverImgSrc":"journal/img/cover/ZGYSJSXB.jpg","id":"88","issnPpub":"1004-0609","publisherId":"ZGYSJSXB","title":"中国有色金属学报"},"keywords":[{"id":"fc8b05f4-ab22-4c1b-a162-717dd434b3c3","keyword":"义兴寨金矿田","originalKeyword":"义兴寨金矿田"},{"id":"cc5bcb6b-17d2-4ebd-8306-65eaedeaf20d","keyword":"关键控矿因素","originalKeyword":"关键控矿因素"},{"id":"9ffe0fca-935b-4e03-896a-7da2a3cf4ddb","keyword":"成矿物质","originalKeyword":"成矿物质"},{"id":"501342b5-23fc-4496-a7a7-bc1b8c2ce8f8","keyword":"成矿流体","originalKeyword":"成矿流体"},{"id":"6a668834-040a-42e1-b2d4-c7e64889c99a","keyword":"<span style=\"color:red\">演化</span>","originalKeyword":"演化"},{"id":"a421ffc5-9ac0-4df1-a4f0-c3dff3b53563","keyword":"成矿机理","originalKeyword":"成矿机理"}],"language":"zh","publisherId":"zgysjsxb201702011","title":"山西义兴寨金矿田成矿机理研究:来自同位素和流体包裹体的证据","volume":"27","year":"2017"},{"abstractinfo":"利用显微硬度HV测试、光学显微组织技术研究旋压成形紫铜喇叭罩的组织结构和力学特性。结果表明：紫铜药型罩显微硬度沿母线方向线性递增；旋压罩组织呈纤维状且发生细化，350℃保温1 h后发生再结晶，晶粒尺寸为8.5μm，纵横比为1.6，组织取向与变形组织一致。旋压紫铜药型罩可能存在较强织构、具有抗旋性。","authors":[{"authorName":"蒋尧","id":"3fc86b76-3026-4cb2-bc18-299a565b2c9e","originalAuthorName":"蒋尧"},{"authorName":"黄正祥","id":"afd7adaa-5190-4f71-8492-481fe14b2d16","originalAuthorName":"黄正祥"},{"authorName":"陶从高","id":"7df3335e-0a64-4f01-98f0-7266dcaa6783","originalAuthorName":"陶从高"},{"authorName":"郝日光","id":"4301754c-bf8d-4960-a984-874db5decf86","originalAuthorName":"郝日光"},{"authorName":"胡士廉","id":"b6382d8e-3139-4c43-9fb9-7ac36bc07ae3","originalAuthorName":"胡士廉"}],"doi":"","fpage":"81","id":"4a6e2042-de1e-42c8-b9c8-82dbbb0be7bb","issue":"5","journal":{"abbrevTitle":"BQCLKXYGC","coverImgSrc":"journal/img/cover/BQCLKXYGC.jpg","id":"4","issnPpub":"1004-244X","publisherId":"BQCLKXYGC","title":"兵器材料科学与工程   "},"keywords":[{"id":"8700b8cc-e3d2-4fab-b9e7-70fbb7f18c18","keyword":"喇叭罩","originalKeyword":"喇叭罩"},{"id":"9dee099d-bbad-404e-8815-da28356969a7","keyword":"紫铜","originalKeyword":"紫铜"},{"id":"d8646b78-0bef-4d45-bb1a-8c824adf8372","keyword":"显微硬度","originalKeyword":"显微硬度"},{"id":"1b3038ec-bc0f-4743-80a8-0292d3fb5066","keyword":"显微组织","originalKeyword":"显微组织"},{"id":"497e0852-c51f-4bf5-914c-6a833b92f2a9","keyword":"<span style=\"color:red\">演化</span>","originalKeyword":"演化"}],"language":"zh","publisherId":"bqclkxygc201305029","title":"旋压紫铜药型罩组织结构与力学特性试验研究","volume":"","year":"2013"}],"totalpage":175,"totalrecord":1750}