{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"采用射频等离子体增强化学气相沉积法(RF-PECVD)在<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>上沉积氮化硅薄膜.用台阶仪、X射线光电子能谱(XPS)、透射电镜(TEM)和扫描电镜(SEM)等手段对薄膜的厚度、成分、结构及形貌进行表征,并探讨了各工艺参数对薄膜沉积速率的影响.","authors":[{"authorName":"杜平凡","id":"40c0a942-e048-452d-a050-ccf2235846aa","originalAuthorName":"杜平凡"},{"authorName":"席珍强","id":"1ad6e3a8-9107-4f12-96f6-789b82973e27","originalAuthorName":"席珍强"},{"authorName":"汪新颜","id":"9547fefa-c6bc-40e9-9563-993a844eeee6","originalAuthorName":"汪新颜"},{"authorName":"金达莱","id":"20d0f32d-4785-4249-9be8-60c146d3bf01","originalAuthorName":"金达莱"},{"authorName":"王勇","id":"8c6476e5-2546-4052-a0dd-aee14d183f24","originalAuthorName":"王勇"}],"doi":"","fpage":"417","id":"d1e81da9-6082-4e2a-80c6-fe5501dda802","issue":"3","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"36f65f00-6ae3-42d2-8d19-2fe4fdca7d21","keyword":"氮化硅薄膜","originalKeyword":"氮化硅薄膜"},{"id":"66162630-b497-48b4-98fb-603c4be47e58","keyword":"<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>","originalKeyword":"钢衬底"},{"id":"d2e67be9-c2ea-41dd-9fc9-32831506d641","keyword":"RF-PECVD","originalKeyword":"RF-PECVD"},{"id":"2ccb700f-90d6-4df8-b7fe-67a13a890b1b","keyword":"沉积速率","originalKeyword":"沉积速率"}],"language":"zh","publisherId":"gncl200803021","title":"RF-PECVD法在<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>上沉积氮化硅薄膜的研究","volume":"39","year":"2008"},{"abstractinfo":"我们用混合物理化学气相沉积法(hybrid physical-chernical vapor deposition简称为HPCVD)以氩气为背景气体,在不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>上于不同条件下制备了一批MgB2超导薄膜样品.用扫描电子显微镜获取了相关的SEM图像,并对膜的成分进行了能谱分析(EDX)的.当把不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>MgB2超导薄膜弯曲不同角度之后,膜面上均出现了裂纹.裂纹的数量和宽度随弯曲的角度的增大而增加,但是膜始终紧紧地覆着在<span style=\"color:red\">衬底</span>上不脱落.因此我们可以说覆着在不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>上的MgB2超导薄膜具有了很好的韧性.在膜中我们也发现有大量的数十纳米大小的晶粒.这个尺寸的纳米粒子的作用可以用来平衡MgB2膜内结构和表面晶粒的活性之间的相互作用.MgB2纳米粒子的存在是MgB2超导膜表现出韧性的关键角色.","authors":[{"authorName":"王银博","id":"81c4980e-062c-43e0-a3f0-efe90c1ec42a","originalAuthorName":"王银博"},{"authorName":"易声宇","id":"91c4bc61-3a10-4451-91a7-eee9a40170c5","originalAuthorName":"易声宇"},{"authorName":"冯庆荣","id":"c3643799-7698-495f-a6f7-3bda7bdc9ef5","originalAuthorName":"冯庆荣"}],"doi":"10.3969/j.issn.1000-3258.2008.02.002","fpage":"101","id":"891013c2-1202-4b39-a7b2-1e17f59c24b5","issue":"2","journal":{"abbrevTitle":"DWWLXB","coverImgSrc":"journal/img/cover/DWWLXB.jpg","id":"19","issnPpub":"1000-3258","publisherId":"DWWLXB","title":"低温物理学报   "},"keywords":[{"id":"10a16aa3-5708-486f-894d-a2aa8511ba5f","keyword":"混合物理化学气相沉积法(HPCVD)","originalKeyword":"混合物理化学气相沉积法(HPCVD)"},{"id":"2db3f8b6-9712-4789-b61d-98989718910b","keyword":"MgB2超导薄膜","originalKeyword":"MgB2超导薄膜"},{"id":"d2013e05-5f42-4386-a344-6347f53e2d36","keyword":"不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>","originalKeyword":"不锈钢衬底"},{"id":"37ba950d-02f7-4547-86a1-0934ef904d27","keyword":"韧性","originalKeyword":"韧性"},{"id":"2124db5f-59f2-405a-af52-457ca77e79d1","keyword":"纳米粒子","originalKeyword":"纳米粒子"}],"language":"zh","publisherId":"dwwlxb200802002","title":"纳米粒子在不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>MgB2超导膜中的作用","volume":"30","year":"2008"},{"abstractinfo":"以改性二氧化锆的过渡层,用溶胶—凝胶法在不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>上成功制备了锆钛比为52/48的锆钛酸铅膜.扫描电镜分析表明,膜的表面平整,无裂纹.X射线分析结果说明,经650℃退火30min,后膜为纯的钙钛矿相.以<span style=\"color:red\">衬底</span>为下电极、直径为0.32mm的金上电极,测量了0.8μm膜的电滞回线及其它性能,膜的乘余极化为18μC/cm2.","authors":[{"authorName":"李坤","id":"c8ef8a31-46ee-4c9c-8835-cb23844e775d","originalAuthorName":"李坤"},{"authorName":"陈王丽华","id":"af7a5dd6-bf1f-4842-a2bd-33e0f24402f8","originalAuthorName":"陈王丽华"},{"authorName":"蔡忠龙","id":"12f21114-e943-4e30-826c-d750b87c0821","originalAuthorName":"蔡忠龙"}],"doi":"","fpage":"308","id":"a24f8d92-f955-4af1-9d1e-66a8cae20497","issue":"3","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"c8ea53af-de26-421b-b638-e35f4e5182fe","keyword":"锆钛酸铅","originalKeyword":"锆钛酸铅"},{"id":"d9ba7ba4-d943-4326-829f-a5179ba121db","keyword":"陶瓷","originalKeyword":"陶瓷"},{"id":"f4294fe6-fdf6-4d5c-9927-7011fcc2863a","keyword":"薄膜","originalKeyword":"薄膜"},{"id":"e905522a-87c8-4310-9094-d14ba920a3e8","keyword":"不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>","originalKeyword":"不锈钢衬底"},{"id":"11bb6cea-5bde-44f8-b950-d8ec6f1b2659","keyword":"阻挡层","originalKeyword":"阻挡层"}],"language":"zh","publisherId":"gncl200103033","title":"不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>上锆钛酸铅膜的制备","volume":"32","year":"2001"},{"abstractinfo":"我们用混和物理化学气相沉积法(HPCVD)在不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>上原位制备了以MgB2厚膜(约10微米厚)为过渡层的MgB2超导厚膜(约20微米厚)样品,两层膜总厚约30微米.X光衍射实验表明过渡层为(101)取向的织构膜,表层MgB2超导厚膜接近多晶膜,但有较强(101)取向,两者均含有少量的Mg和MgO杂相.此超导厚膜样品的Tc(onset)=37.8K,Tc(zero)=36.6K,ΔT=1.2K.对此样品的弯曲实验表明,以曲率半径500微米弯曲到180°后,样品仍具有Tc(onset)=37.8K,Tc(zero)=36.4K的超导电性.样品剖面SEM观测表明该膜结构致密,表面厚膜层和过渡层之间连接紧密.样品表面的SEM观测表明虽然样品弯曲导致表面MgB2超导厚膜面出现了裂缝,甚至有小部分膜面的脱落,但过渡层始终紧紧附着在不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>上.这表明过渡层MgB2厚膜的存在大大地提高样品整体的柔韧性,展现了不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>上的MgB2厚膜超导带(线)巨大的开发潜力和诱人的广阔应用前景.","authors":[{"authorName":"陈莉萍","id":"7aef581f-0634-49cf-8a99-92ccdf4c8957","originalAuthorName":"陈莉萍"},{"authorName":"丁莉莉","id":"3c3ba80d-cb57-41b3-bde8-fdf0599f7f89","originalAuthorName":"丁莉莉"},{"authorName":"庄承<span style=\"color:red\">钢</span>","id":"3dd0b851-3c74-46df-8136-cf41417d8673","originalAuthorName":"庄承钢"},{"authorName":"张开诚","id":"1c4de28d-e28a-453f-9d3e-0123b15a56f2","originalAuthorName":"张开诚"},{"authorName":"陈晋平","id":"0855719a-7613-4607-b0c3-14bf24952514","originalAuthorName":"陈晋平"},{"authorName":"徐军","id":"1e70335b-aa83-41fe-aff4-d3f2482ea5b9","originalAuthorName":"徐军"},{"authorName":"安玲","id":"5f7cb2ee-c99b-4b44-9015-cd52c64a7566","originalAuthorName":"安玲"},{"authorName":"闫昌硕","id":"8ca90423-31c1-4e8e-ae42-f8373d638847","originalAuthorName":"闫昌硕"},{"authorName":"熊光成","id":"b03a6dbf-db53-4860-984e-ba66cea76c40","originalAuthorName":"熊光成"},{"authorName":"冯庆荣","id":"0226ab05-a05f-427f-84e1-c7db00641c5d","originalAuthorName":"冯庆荣"}],"doi":"10.3969/j.issn.1000-3258.2006.01.007","fpage":"31","id":"9f2b3d04-7109-4397-b308-30463e14bf1e","issue":"1","journal":{"abbrevTitle":"DWWLXB","coverImgSrc":"journal/img/cover/DWWLXB.jpg","id":"19","issnPpub":"1000-3258","publisherId":"DWWLXB","title":"低温物理学报   "},"keywords":[{"id":"f271f93e-10db-4f19-8836-a401861184d2","keyword":"混合物理化学气相沉积(HPCVD)","originalKeyword":"混合物理化学气相沉积(HPCVD)"},{"id":"a7133a16-3ab7-4569-a2db-5a5530836146","keyword":"MgB2超导厚膜","originalKeyword":"MgB2超导厚膜"},{"id":"8181790e-e2ba-4e95-9f6b-7f82ed12b100","keyword":"过渡层","originalKeyword":"过渡层"},{"id":"5070c89f-0e47-4238-9337-b27a795229b0","keyword":"不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>","originalKeyword":"不锈钢衬底"},{"id":"bc3550b2-d6b5-4a49-be3b-2064db4c71e0","keyword":"韧度","originalKeyword":"韧度"}],"language":"zh","publisherId":"dwwlxb200601007","title":"不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>MgB2厚膜韧性的研究","volume":"28","year":"2006"},{"abstractinfo":"在抛光的和未抛光的不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>上,利用微波等离子体化学气相沉积(MPCVD)方法从甲烷和氢气的混合气体中沉积碳纳米管薄膜,并对其场发射性能进行了研究.实验发现,不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>的机械抛光能降低碳纳米管膜的开启场强,增大它的发射电流密度.在同一场强7.5 V/μm下,<span style=\"color:red\">衬底</span>未抛光样品的电流密度为2.9 mA/cm2,而<span style=\"color:red\">衬底</span>抛光样品的电流密度达到5.5 mA/cm2.低开启场强和大发射电流密度意味着β增大,说明机械抛光能使碳纳米管膜的β增大.","authors":[{"authorName":"樊志琴","id":"dabb698b-e6d5-4824-b6f7-c033249df2d6","originalAuthorName":"樊志琴"},{"authorName":"朱庆芳","id":"794a5e81-f5f5-40ea-893b-4d06714dc8a1","originalAuthorName":"朱庆芳"},{"authorName":"杨仕娥","id":"d999c52d-90e1-4518-b8c1-6f90d0c8504a","originalAuthorName":"杨仕娥"},{"authorName":"姚宁","id":"cf8096b4-ed2c-4d20-9e5f-a20d2a5dd4aa","originalAuthorName":"姚宁"},{"authorName":"鲁占灵","id":"45f108c3-36e4-4e08-bffd-5e5af86e9255","originalAuthorName":"鲁占灵"},{"authorName":"张兵临","id":"26cc3fda-9ff8-42c6-9424-fc6941b85788","originalAuthorName":"张兵临"}],"doi":"10.3969/j.issn.1000-985X.2005.05.040","fpage":"954","id":"0f76a20a-a507-496a-b7f4-7ffc07019431","issue":"5","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":"fcedec94-44c9-4b1e-b8fa-639a202d136e","keyword":"碳纳米管膜","originalKeyword":"碳纳米管膜"},{"id":"c7a3ff9c-a35e-4d72-8d41-c934132a0803","keyword":"场发射","originalKeyword":"场发射"},{"id":"2081bdbd-74fa-4175-b5c0-3c0da8fcdebf","keyword":"MPCVD","originalKeyword":"MPCVD"},{"id":"a14bf9bf-ffe9-424b-a417-846aa28c7674","keyword":"拉曼光谱","originalKeyword":"拉曼光谱"}],"language":"zh","publisherId":"rgjtxb98200505040","title":"不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>的抛光处理对碳纳米管薄膜场发射性能的影响","volume":"34","year":"2005"},{"abstractinfo":"为了利用液相电沉积技术实现在金属<span style=\"color:red\">衬底</span>表面全方位电沉积类金刚石(DLC)薄膜,采用不同尺度的不锈钢片作为<span style=\"color:red\">衬底</span>,在表面电沉积了DLC薄膜,利用X射线光电子能谱、Raman光谱和扫描电子显微镜分别对<span style=\"color:red\">衬底</span>两面薄膜的化学成分、微观结构和表面形貌进行了分析.结果显示:对于尺度大于石墨阳极的不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>,仅在<span style=\"color:red\">衬底</span>正对着阳极的一面实现了DLC薄膜的沉积;而对于尺度小于阳极的不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>,在<span style=\"color:red\">衬底</span>两面都有DLC薄膜沉积,且两面薄膜结构相似,形貌相近.利用准静态电场理论对实验结果进行了解释,提出在金属<span style=\"color:red\">衬底</span>表面实现液相电沉积DLC薄膜的前提条件是存在垂直于<span style=\"color:red\">衬底</span>表面的电场分量,为进一步实现在复杂形状的导电性<span style=\"color:red\">衬底</span>表面沉积DLC薄膜提供了理论依据.","authors":[{"authorName":"李瑞山","id":"0cd7b5fb-47e3-4f34-ada3-f09b53aa947c","originalAuthorName":"李瑞山"},{"authorName":"冯有才","id":"17785087-fb42-4cdb-8560-d9064faf311b","originalAuthorName":"冯有才"},{"authorName":"王璇","id":"5d927523-b67e-43b8-a114-c169aeac6331","originalAuthorName":"王璇"},{"authorName":"张培增","id":"6ad0c5ab-006a-4d3d-bbec-4435a0a49828","originalAuthorName":"张培增"},{"authorName":"谢二庆","id":"c2de5e9c-dab1-40e9-a411-270c08c96573","originalAuthorName":"谢二庆"},{"authorName":"杨华","id":"41fe6094-a2d1-4638-bf4e-c4ab44e4b35a","originalAuthorName":"杨华"}],"doi":"10.11896/j.issn.1005-023X.2016.02.014","fpage":"56","id":"a7a6e922-46ae-47b1-87ae-eb4bd3470ad2","issue":"2","journal":{"abbrevTitle":"CLDB","coverImgSrc":"journal/img/cover/CLDB.jpg","id":"8","issnPpub":"1005-023X","publisherId":"CLDB","title":"材料导报"},"keywords":[{"id":"d4b2d068-414c-42d2-80b0-850912bb6f7f","keyword":"类金刚石薄膜","originalKeyword":"类金刚石薄膜"},{"id":"4a5e76bf-e74e-467e-ae42-b2f12681db48","keyword":"电沉积","originalKeyword":"电沉积"},{"id":"af509521-ec2a-4d9e-a584-794ddd1f96e0","keyword":"全方位沉积","originalKeyword":"全方位沉积"}],"language":"zh","publisherId":"cldb201602014","title":"不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>两面同时液相电沉积类金刚石薄膜及其沉积机理研究","volume":"30","year":"2016"},{"abstractinfo":"研究了通过热丝CVD法在施加了Ni-P/Cu复合中间过渡层的W18Cr4V高速<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>表面进行金刚石涂层的沉积技术以及不同压力条件对沉积出的CVD金刚石涂层质量的影响.最后通过扫描电镜分别对Cu、Ni-P以及不同反应压力下沉积的金刚石涂层的表面形貌进行了检测分析,通过XRD、拉曼光谱仪、洛氏硬度仪对金刚石涂层性能进行检测分析.结果表明:Ni-P/Cu复合中间过渡层可以明显的抑制Fe、Co的催石墨化作用.在此基础上通过沉积参数的优化,在W18Cr4V高速<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>表面成功沉积出高质量的CVD金刚石涂层.压力为4 kPa条件下沉积的CVD金刚石涂层较5 kPa的金刚石颗粒晶型明显、分布致密.","authors":[{"authorName":"马玉平","id":"9d7b212c-8539-4fd3-8626-241dc439278f","originalAuthorName":"马玉平"},{"authorName":"王金龙","id":"993607aa-fc71-48d9-baba-11d8ded48008","originalAuthorName":"王金龙"}],"doi":"","fpage":"1041","id":"8365721a-cba6-46ed-a510-76296454f7e2","issue":"4","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":"aa6ed5fa-14f1-4123-8d1f-3b4e53203b58","keyword":"高速<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>","originalKeyword":"高速钢衬底"},{"id":"d77c04ff-5382-47d0-9321-a8c3eb4e6e48","keyword":"Ni-P/Cu复合中间过渡层","originalKeyword":"Ni-P/Cu复合中间过渡层"},{"id":"33f08bfc-8a59-4847-8286-1ff4b7939758","keyword":"CVD金刚石涂层","originalKeyword":"CVD金刚石涂层"}],"language":"zh","publisherId":"rgjtxb98201504033","title":"W18Cr4V高速<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>CVD金刚石涂层沉积技术研究","volume":"44","year":"2015"},{"abstractinfo":"介绍用混合物理化学气相沉积法(HPCVD)制备的不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>MgB2超导厚膜样品.该样品的Tc(onset)=38K,Tc(0)=27K.X光衍射图形表明它是(101)方向织构的致密厚膜.这种膜具有较强的韧性,同时和<span style=\"color:red\">衬底</span>有高度的结合性.当其被弯曲到约200微米半径的弧度时,膜面会出现条状裂纹,但仍有少部分膜面未被破坏,保持完整,表现出较好的韧性.","authors":[{"authorName":"王新峰","id":"c2bf9db3-362c-4e11-83b4-6c4e61f8f409","originalAuthorName":"王新峰"},{"authorName":"郭荆璞","id":"b41d55e4-2c44-4deb-8521-e59c9af3b145","originalAuthorName":"郭荆璞"},{"authorName":"贾璋","id":"afe42fff-8607-47fe-9bca-4993f3eaef77","originalAuthorName":"贾璋"},{"authorName":"吕莹","id":"ff58c671-7eab-4a69-ac85-3a316064919b","originalAuthorName":"吕莹"},{"authorName":"朱萌","id":"c06e6345-ca1d-4d03-a0eb-2419081b4137","originalAuthorName":"朱萌"},{"authorName":"王晓楠","id":"bdbf2fcf-3e5b-47bf-b862-cb5867396a7f","originalAuthorName":"王晓楠"},{"authorName":"陈晋平","id":"67c58791-84ca-448f-97c9-9e057aad6cd6","originalAuthorName":"陈晋平"},{"authorName":"徐军","id":"0d02b541-2822-4ef3-8af2-69ddd8a8fbf3","originalAuthorName":"徐军"},{"authorName":"冯庆荣","id":"350f623e-a349-450c-a09c-98331c813a46","originalAuthorName":"冯庆荣"}],"doi":"10.3969/j.issn.1000-3258.2004.04.013","fpage":"344","id":"832181b9-8eff-43b0-b421-c74715dd9c81","issue":"4","journal":{"abbrevTitle":"DWWLXB","coverImgSrc":"journal/img/cover/DWWLXB.jpg","id":"19","issnPpub":"1000-3258","publisherId":"DWWLXB","title":"低温物理学报   "},"keywords":[{"id":"aa13d289-8ea6-4d79-89f3-55b71563adfc","keyword":"MgB2","originalKeyword":"MgB2"},{"id":"7e90415c-8e76-46db-b7d5-4282ff5eaf9a","keyword":"厚膜超导体","originalKeyword":"厚膜超导体"},{"id":"fc2f6e2f-0c2b-44e9-9b2a-0c261013d3d7","keyword":"不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>","originalKeyword":"不锈钢衬底"},{"id":"06417da8-6f7a-4903-b975-ce7ca3d93ab1","keyword":"SEM图","originalKeyword":"SEM图"},{"id":"b71f0bbf-eb56-4d7c-a5a7-03dc9801b512","keyword":"X-光衍射","originalKeyword":"X-光衍射"}],"language":"zh","publisherId":"dwwlxb200404013","title":"初探混合物理化学气相沉积法(HPCVD)制备不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>MgB2超导厚膜样品","volume":"26","year":"2004"},{"abstractinfo":"我们用混合物理化学气相沉积法(HPCVD)制备了一批不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>的MgB2超导厚膜样品,厚度在10～30μm间,Tc(onset)是37.8～37.2K,超导转变宽度ΔT在1.2K左右,是(101)方向织构的致密厚膜,并有少许MgO杂相.对样品进行弯折研究,随着弯曲角度的增加,膜面出现不同程度的条状裂纹,但仍能保持膜面的基本完整;虽然样品的超导起始转变温度降低、转变温区变宽,性能有所下降,但超导特性仍能保持在一个很好的水平上.这个结果表明了采用HPCVD方法制备不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>带材将会很好地克服MgB2超导膜由于硬脆的性质而无法绕制磁体的问题,有着十分重要的应用意义.","authors":[{"authorName":"庄承<span style=\"color:red\">钢</span>","id":"510d5c75-e04b-4243-b2bc-fbe2eb4dd172","originalAuthorName":"庄承钢"},{"authorName":"安玲","id":"cfb3f5a4-1f4f-47c4-9d63-75c8eb14e1c1","originalAuthorName":"安玲"},{"authorName":"陈莉萍","id":"e0c47e64-80c8-4454-9c53-30be16f1a334","originalAuthorName":"陈莉萍"},{"authorName":"丁莉莉","id":"3fbe910b-2e42-4b3e-92a8-70b23a3d634f","originalAuthorName":"丁莉莉"},{"authorName":"张开诚","id":"01c05421-642d-4222-9471-8f7c020cfce8","originalAuthorName":"张开诚"},{"authorName":"陈晋平","id":"c5d84b47-d212-4865-a604-6b602727e973","originalAuthorName":"陈晋平"},{"authorName":"徐军","id":"97ec13d7-0f35-4bea-ac8b-2c444791c19c","originalAuthorName":"徐军"},{"authorName":"冯庆荣","id":"01916db3-c838-4a80-a4f4-88e74ffc78a3","originalAuthorName":"冯庆荣"},{"authorName":"甘子钊","id":"9489ccb3-b513-4193-9fd7-528a6381f03b","originalAuthorName":"甘子钊"}],"doi":"10.3969/j.issn.1000-3258.2005.02.002","fpage":"103","id":"d5df8f28-bb84-4c3d-8fc8-b564647f89d0","issue":"2","journal":{"abbrevTitle":"DWWLXB","coverImgSrc":"journal/img/cover/DWWLXB.jpg","id":"19","issnPpub":"1000-3258","publisherId":"DWWLXB","title":"低温物理学报   "},"keywords":[{"id":"8850db86-47db-401b-a65c-8244bdd0943c","keyword":"混合物理化学气相沉积(HPCVD),MgB2超导厚膜,不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>,韧度","originalKeyword":"混合物理化学气相沉积(HPCVD),MgB2超导厚膜,不锈钢衬底,韧度"}],"language":"zh","publisherId":"dwwlxb200502002","title":"混合物理化学气相沉积法制备不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>MgB2超导厚膜样品的韧度研究","volume":"27","year":"2005"},{"abstractinfo":"采用复合络合剂,在2cr12不锈<span style=\"color:red\">钢</span>上直接化学镀Ni-W-P,并对镀层的形貌、成分、组织结构及性能进行了检测和分析.结果表明:不锈<span style=\"color:red\">钢</span>经过合适的前处理后,得到的镀层光亮、均匀,表面呈胞状组织;在400℃热处理后,开始析出Ni3P相;镀态层的硬度HK值由8186 MPa提高至11850 MPa;结合力、耐磨性也有明显增强.","authors":[{"authorName":"耿冰霜","id":"cf5f481e-dbe8-415b-9796-b2e96005958b","originalAuthorName":"耿冰霜"},{"authorName":"卫英慧","id":"6c727669-fa39-47e5-b519-dc9550f1be44","originalAuthorName":"卫英慧"},{"authorName":"侯利锋","id":"d42ccb63-ff23-4ed8-82d0-e9f84b07507f","originalAuthorName":"侯利锋"},{"authorName":"李杉","id":"92c9a1e2-8ce6-46e0-88d8-9c693cb559f9","originalAuthorName":"李杉"},{"authorName":"杨海燕","id":"100c9d0c-c332-4f45-884e-3653eba93dce","originalAuthorName":"杨海燕"},{"authorName":"许并社","id":"8e77b63f-dc47-4dfa-9866-f388c36beaa9","originalAuthorName":"许并社"}],"doi":"","fpage":"71","id":"b610e69f-053f-41a3-8c0f-8ee958b7e855","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":"8b233603-43b1-4e81-b9ed-7ad28594a772","keyword":"化学镀","originalKeyword":"化学镀"},{"id":"80eba730-33fc-443f-9346-4d6e1a986107","keyword":"Ni-W-P合金","originalKeyword":"Ni-W-P合金"},{"id":"a09aa2d5-7cd3-4967-b501-1390ad3215d9","keyword":"组织结构","originalKeyword":"组织结构"},{"id":"65631c91-67d5-4a15-b7d9-395af83b8d0d","keyword":"性能","originalKeyword":"性能"}],"language":"zh","publisherId":"xyjsclygc2009z1016","title":"不锈<span style=\"color:red\">钢</span><span style=\"color:red\">衬底</span>化学镀Ni-W-P三元合金组织及性能研究","volume":"38","year":"2009"}],"totalpage":2545,"totalrecord":25447}