{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>是<span style=\"color:red\">等离子体</span>学科和<span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>学科交叉的产物,它不仅具有一般<span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>的性质,而且还体现<span style=\"color:red\">等离子体</span>的特性,通过改变<span style=\"color:red\">等离子体</span>参数或外加磁场可有效控制其带隙.若在可调带隙的<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>中构造适当缺陷,则可形成可调滤波器和波导等器件,在工程方面具有重要应用.结合本课题组工作,综述了<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>的研究进展,在此基础上,展望了<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>的发展前景,为人们进一步研究<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>的特性和应用提供参考.","authors":[{"authorName":"亓丽梅","id":"f45f9590-a91e-4157-a617-3a1a635cc66d","originalAuthorName":"亓丽梅"},{"authorName":"傅涛","id":"c129df3f-2d8e-4c8d-93c2-751cdfa20955","originalAuthorName":"傅涛"},{"authorName":"杨梓强","id":"3c84a1a7-0d31-4046-812f-680b027fa56a","originalAuthorName":"杨梓强"},{"authorName":"殷淑容","id":"0de65e21-98a4-4e17-9524-b61c65899aaa","originalAuthorName":"殷淑容"}],"doi":"10.3969/j.issn.1007-5461.2012.05.001","fpage":"513","id":"0a2f31bb-558e-484a-aa9a-00daa4367ed4","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":"5a2a8779-ab1f-4dbf-ac51-1b8d618fef54","keyword":"量子光学","originalKeyword":"量子光学"},{"id":"cf9ff8e4-3585-4130-ae5a-a37223a221b8","keyword":"可调带隙","originalKeyword":"可调带隙"},{"id":"ec7777b5-373a-4772-b473-0cdbc490647f","keyword":"<span style=\"color:red\">等离子体</span>参数","originalKeyword":"等离子体参数"},{"id":"423ca3ba-59f5-4a8b-a47e-095a5426f36d","keyword":"<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>","originalKeyword":"等离子体光子晶体"}],"language":"zh","publisherId":"lzdzxb201205001","title":"<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>研究进展","volume":"29","year":"2012"},{"abstractinfo":"利用双水电极介质阻挡放电装置,在空气和氩气组成的混合气体气体放电中,观察到了一种由放电丝自组织而形成的<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>.该<span style=\"color:red\">晶体</span>的结构由多个四边形的晶胞构成.每个晶胞由中心点、交叉点及连线组成,分别对应细<span style=\"color:red\">等离子体</span>柱、粗<span style=\"color:red\">等离子体</span>柱和片状<span style=\"color:red\">等离子体</span>.利用发射光谱法,研究了处于不同位置的<span style=\"color:red\">等离子体</span>状态,以及<span style=\"color:red\">等离子体</span>参量随着氩气含量的变化趋势.通过采集氮分子(N2)第二正带系(C3Πu→B3Πg)发射谱线,分别计算出了不同位置的<span style=\"color:red\">等离子体</span>的分子振动温度.通过氩原子696.57 nm(2P2→1S5)谱线的展宽,研究了不同位置的电子密度.实验结果表明:不同位置的<span style=\"color:red\">等离子体</span>具有不同的分子振动温度和电子密度.即他们所处的<span style=\"color:red\">等离子体</span>状态是不同的.在相同的氩气含量下,粗<span style=\"color:red\">等离子体</span>柱、细<span style=\"color:red\">等离子体</span>柱和片状<span style=\"color:red\">等离子体</span>的分子振动温度依次增高,且均随着氩气含量的增加而下降.在相同的氩气含量下,粗<span style=\"color:red\">等离子体</span>柱、细<span style=\"color:red\">等离子体</span>柱,片状<span style=\"color:red\">等离子体</span>的电子密度依次减小,且随着氩气含量的增加而下降.因为<span style=\"color:red\">等离子体</span>电子密度不同,对光的折射率是不同的,因此在该<span style=\"color:red\">晶体</span>结构中,粗<span style=\"color:red\">等离子体</span>柱、细<span style=\"color:red\">等离子体</span>柱,片状<span style=\"color:red\">等离子体</span>具有的折射率是不同的,他们与周围未放电的区域自组织形成了结构比较复杂的<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>.","authors":[{"authorName":"冯建宇","id":"2d8a24f6-80ed-4978-8550-6dfc0c043204","originalAuthorName":"冯建宇"},{"authorName":"董丽芳","id":"870d8abc-67cc-4183-afe7-b87d001e6b51","originalAuthorName":"董丽芳"},{"authorName":"魏领燕","id":"aab70ef7-6443-42fe-a736-2a63222eaa0f","originalAuthorName":"魏领燕"}],"doi":"","fpage":"328","id":"fdbc37a3-18c6-40d4-8844-be76b6a3231c","issue":"2","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":"b27f43be-20e7-49d5-9d1e-43a221dd4b3b","keyword":"<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>","originalKeyword":"等离子体光子晶体"},{"id":"c6ca33bd-ffdd-4661-9220-1eafe350137c","keyword":"介质阻挡放电","originalKeyword":"介质阻挡放电"},{"id":"c6e18dbd-7cca-4a69-ad16-3ebcf3cbc955","keyword":"发射光谱","originalKeyword":"发射光谱"},{"id":"b4a9ab3c-a039-4d8b-8fac-7164576528d7","keyword":"<span style=\"color:red\">等离子体</span>参量","originalKeyword":"等离子体参量"}],"language":"zh","publisherId":"rgjtxb98201602006","title":"自组织<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>的光谱研究","volume":"45","year":"2016"},{"abstractinfo":"采用平板双水电极介质阻挡放电装置,通过放电丝的非线性自组织,在空气放电中获得不同对称性二维<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>.随外加电压升高,<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>经历了从等边三角晶格到四方晶格结构的转化.在实验测量数据的基础上,采用平面波展开方法计算了<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>转化过程中的带隙结构变化.提出了一种在空气放电中实现的新型可调<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>.","authors":[{"authorName":"范伟丽","id":"39977968-d9c2-469e-a273-3139d098870e","originalAuthorName":"范伟丽"},{"authorName":"董丽芳","id":"7b469a10-8d30-45ed-a61f-f25bda8d9080","originalAuthorName":"董丽芳"}],"doi":"","fpage":"1290","id":"3467a1fa-debb-4942-b97d-9fc564d6ece5","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":"e50672f3-be03-47b3-80c9-c4887a7293a5","keyword":"<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>","originalKeyword":"等离子体光子晶体"},{"id":"f38bee1e-acfc-4782-a892-d4f80f072764","keyword":"平面波展开方法","originalKeyword":"平面波展开方法"},{"id":"6f4eeb9a-8663-4b33-b453-efbcff5bbb3c","keyword":"带隙结构","originalKeyword":"带隙结构"}],"language":"zh","publisherId":"rgjtxb98201105040","title":"空气放电中自组织<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>研究","volume":"40","year":"2011"},{"abstractinfo":"利用基于有限元法的COMSOL软件仿真研究了在微波波段下二维点缺陷<span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>缺陷模的特性.主要讨论了在TM模式下,点缺陷对透射系数的影响以及<span style=\"color:red\">等离子体</span>密度对二维点缺陷<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>透射系数的影响.重点研究了缺陷模与<span style=\"color:red\">等离子体</span>密度之间的关系,以及<span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>的层数对缺陷模特性的影响.研究结果对微波段的多通道滤波器、波分复用器的设计和制作提供了理论参考.","authors":[{"authorName":"杨东瑾","id":"d2662cba-b1eb-407d-8922-0827b1d187b1","originalAuthorName":"杨东瑾"},{"authorName":"谭海云","id":"d1764e1c-279f-40c2-b6d0-2f885365f768","originalAuthorName":"谭海云"},{"authorName":"金成刚","id":"b01c7989-e6cf-414c-8e7c-8acf34408d87","originalAuthorName":"金成刚"},{"authorName":"诸葛兰剑","id":"dc5ef29e-4434-4fbb-9905-c25829920a7f","originalAuthorName":"诸葛兰剑"},{"authorName":"吴雪梅","id":"c6168d07-e2cd-4b2e-b58f-b046776f4acc","originalAuthorName":"吴雪梅"}],"doi":"10.3969/j.issn.1001-9731.2017.05.007","fpage":"5037","id":"b8ee3367-34ad-4a46-88fb-9164164ec78c","issue":"5","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"14264cce-069a-4ee3-9fb7-3b97a742616e","keyword":"微波","originalKeyword":"微波"},{"id":"528fd42d-9e08-4a3f-94bd-7a48170fbbb6","keyword":"<span style=\"color:red\">等离子体</span>","originalKeyword":"等离子体"},{"id":"dd32d2d6-5e8f-46c5-94e3-829e57025e76","keyword":"点缺陷","originalKeyword":"点缺陷"},{"id":"26e261bb-4fb9-4028-ba64-58bf3e9a8493","keyword":"<span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>","originalKeyword":"光子晶体"},{"id":"c15a69b6-14f2-4d86-85af-14434a400e97","keyword":"缺陷模","originalKeyword":"缺陷模"}],"language":"zh","publisherId":"gncl201705007","title":"二维点缺陷<span style=\"color:red\">等离子体</span><span style=\"color:red\">光子</span><span style=\"color:red\">晶体</span>缺陷模特性研究","volume":"48","year":"2017"},{"abstractinfo":"提出了一种夸克-胶子<span style=\"color:red\">等离子体</span>中的喷注-<span style=\"color:red\">光子</span>转换机制.对于热<span style=\"color:red\">光子</span>而言,在热夸克-胶子媒介中的喷注-<span style=\"color:red\">光子</span>转换是一个非常重要的热<span style=\"color:red\">光子</span>来源.喷注可以通过次级康普顿散射和湮灭过程来实现喷注-<span style=\"color:red\">光子</span>转换.此外,还考虑了在快<span style=\"color:red\">光子</span>产生过程中起重要修正作用的胶子-<span style=\"color:red\">光子</span>贡献,其中,核遮蔽效应和同位旋效应也被引入到了部分子模型中.","authors":[{"authorName":"傅永平","id":"73c5a3d6-022d-4aa8-a825-2bb8b891c774","originalAuthorName":"傅永平"},{"authorName":"李云德","id":"1a8c42d6-c88c-48ab-8a97-5028964f8da2","originalAuthorName":"李云德"}],"doi":"","fpage":"16","id":"f22a7f19-76b6-44a2-884d-aa6871acb555","issue":"1","journal":{"abbrevTitle":"YZHWLPL","coverImgSrc":"journal/img/cover/YZHWLPL.jpg","id":"78","issnPpub":"1007-4627","publisherId":"YZHWLPL","title":"原子核物理评论   "},"keywords":[{"id":"e348f93a-cc17-4867-88f6-7e9ba58aa53e","keyword":"夸克-胶子<span style=\"color:red\">等离子体</span>","originalKeyword":"夸克-胶子等离子体"},{"id":"4902ee2e-c602-4044-a0f4-2f5be46590eb","keyword":"喷注-<span style=\"color:red\">光子</span>转换","originalKeyword":"喷注-光子转换"},{"id":"f7d381be-f141-4657-9be2-49118462eb89","keyword":"<span style=\"color:red\">光子</span>产生","originalKeyword":"光子产生"}],"language":"zh","publisherId":"yzhwlpl201001002","title":"夸克-胶子<span style=\"color:red\">等离子体</span>中的喷注-<span style=\"color:red\">光子</span>转换机制","volume":"27","year":"2010"},{"abstractinfo":"本文研究了金纳米棒的局域表面<span style=\"color:red\">等离子体</span>共振效应在双<span style=\"color:red\">光子</span>聚合过程中的作用,即当激发光与金纳米棒表面<span style=\"color:red\">等离子体</span>共振波长相匹配时,会在金纳米棒表面产生很强的局域电磁场,从而引发双<span style=\"color:red\">光子</span>聚合.通过采用与金纳米棒表面<span style=\"color:red\">等离子体</span>共振波长相同的飞秒激光,在低于光刻胶聚合阈值的功率下照射含有金纳米棒的光刻胶,制备聚合物包覆金纳米棒的纳米复合材料.透射电子显微镜结果表明,当飞秒激光功率为0.6W、光斑直径为1.6 cm、照射时间为0.3s时,金纳米棒表面成功聚合上厚度为5 nm左右的聚合物.本研究在制备聚合物/金属纳米粒子方面提供了一种简单可行的方法,有望在纳米<span style=\"color:red\">光子</span>学、纳米传感器等新兴领域得到应用.","authors":[{"authorName":"张金龙","id":"2e409426-0b67-4378-8d03-6b36cf8b5664","originalAuthorName":"张金龙"},{"authorName":"郑美玲","id":"f318da2e-a724-42a4-b25f-19c928a7913d","originalAuthorName":"郑美玲"},{"authorName":"金峰","id":"3c576466-8435-4167-b549-15fe1fa0bb83","originalAuthorName":"金峰"},{"authorName":"董贤子","id":"0571f439-9a01-4c6d-a0db-0504b3ddeb3a","originalAuthorName":"董贤子"},{"authorName":"陈述","id":"199366a7-c08a-4280-a311-390ddbb24ed5","originalAuthorName":"陈述"},{"authorName":"赵震声","id":"2badc914-368b-42cb-831b-1bb1fb3b93b0","originalAuthorName":"赵震声"},{"authorName":"段宣明","id":"4739bce0-187d-4113-b0d8-82909a093733","originalAuthorName":"段宣明"}],"doi":"10.7517/j.issn.1674-0475.2014.03.267","fpage":"267","id":"7ec8f5a2-98df-4631-8683-8c9e3dea957e","issue":"3","journal":{"abbrevTitle":"YXKXYGHX","coverImgSrc":"journal/img/cover/YXKXYGHX.jpg","id":"74","issnPpub":"1674-0475","publisherId":"YXKXYGHX","title":"影像科学与光化学   "},"keywords":[{"id":"f1eb22d5-823a-4f69-830c-d085d396557d","keyword":"金纳米棒","originalKeyword":"金纳米棒"},{"id":"bbf82f3d-bd47-441b-8924-5c6ca21fcc46","keyword":"飞秒激光","originalKeyword":"飞秒激光"},{"id":"e5b26258-228b-4f64-b5da-446d3c14e01b","keyword":"双<span style=\"color:red\">光子</span>聚合","originalKeyword":"双光子聚合"},{"id":"fea2ea9b-c53c-4906-b129-03c5182f8d06","keyword":"金属/聚合物纳米复合材料","originalKeyword":"金属/聚合物纳米复合材料"}],"language":"zh","publisherId":"ggkxyghx201403005","title":"局域表面<span style=\"color:red\">等离子体</span>共振辅助的金纳米棒/聚合物纳米复合材料的双<span style=\"color:red\">光子</span>聚合","volume":"32","year":"2014"},{"abstractinfo":"在微波<span style=\"color:red\">等离子体</span>化学气相沉积系统中,利用脉冲氮<span style=\"color:red\">离子</span>束溅射二氰二氨靶产生的碳氮粒子作为合成前驱物,在石英玻璃基片上研究了SiCN<span style=\"color:red\">晶体</span>的合成.用扫描电子显微镜(SEM)、X射线能谱(EDX)、X射线衍射(XRD)和X射线光电子能谱(XPS)研究了基片温度对薄膜的形貌、成分和结构的影响.结果表明:随着基片温度的降低,沉积物由截面为六方形的结晶良好的SiCN<span style=\"color:red\">晶体</span>(800℃)变成发育不完全的聚片状<span style=\"color:red\">晶体</span>(700℃),直到变成颗粒细小的无定形碳氮薄膜(550℃).衍射峰的强度以及晶胞参数a和c的值随温度的降低而减小.薄膜为C原子部分取代Si_3N_4中的Si原子位置而形成的SiCN<span style=\"color:red\">晶体</span>,其中N原子主要与Si原子结合,C原子以sp~3C-N、sp~2C=N和sp~2C=C键的形式存在.降低基片温度有利于提高薄膜中的C含量和sp~3C-N键的含量.","authors":[{"authorName":"万军","id":"a78d3812-ec4b-4bea-9095-408952598064","originalAuthorName":"万军"},{"authorName":"马志斌","id":"8b040c2b-7a94-47bd-8266-44a5772a122a","originalAuthorName":"马志斌"},{"authorName":"曹宏","id":"8f92282f-e224-4dab-93fd-b2ae15abb3cf","originalAuthorName":"曹宏"},{"authorName":"吴振辉","id":"217d35e9-fb3e-443f-8706-9b8985fdb5b3","originalAuthorName":"吴振辉"},{"authorName":"汪建华","id":"7a975bc0-9aa1-43ef-828f-15802f0a47da","originalAuthorName":"汪建华"}],"doi":"","fpage":"48","id":"288c670e-0c86-4805-8097-e44857b7a5a4","issue":"1","journal":{"abbrevTitle":"XXTCL","coverImgSrc":"journal/img/cover/XXTCL.jpg","id":"70","issnPpub":"1007-8827","publisherId":"XXTCL","title":"新型炭材料"},"keywords":[{"id":"efa70981-1bf6-4d57-b448-a7350d2246c2","keyword":"SiCN<span style=\"color:red\">晶体</span>","originalKeyword":"SiCN晶体"},{"id":"9d2436ac-9148-40da-a4a2-a68a991b3729","keyword":"微波<span style=\"color:red\">等离子体</span>","originalKeyword":"微波等离子体"},{"id":"dd1da616-244a-4bc1-b289-97a42d73d5aa","keyword":"溅射","originalKeyword":"溅射"},{"id":"25f8683f-8788-4ac9-9403-016638c53851","keyword":"二氰二氨","originalKeyword":"二氰二氨"}],"language":"zh","publisherId":"xxtcl201001008","title":"溅射辅助微波<span style=\"color:red\">等离子体</span>化学气相沉积SiCN<span style=\"color:red\">晶体</span>","volume":"","year":"2010"},{"abstractinfo":"利用微波<span style=\"color:red\">等离子体</span>化学气相沉积系统,以甲烷、氮气和氢气作为气源,在Si(100)衬底上成功地制备出了碳氮<span style=\"color:red\">晶体</span>薄膜,并对两种衬底温度下的薄膜性质进行了比较.用高分辨率场发射扫描电子显微镜观察薄膜,可以看出晶型完整,结构致密,结晶质量较好.X射线能谱证明了碳氮是以C-N和C=N共价键的形式存在,氮碳元素的原子比均为1.3.X射线衍射确定出在衬底温度为900410℃时薄膜样品的主要晶相成份是α-C3N4,β-C3N4,赝立方C3N4,立方C3N4和一个未知相(面间距d=0.4002nm),而在950±10℃时薄膜样品的主要晶相成份是α-C3N4,β-C3N4,赝立方C3N4,类石墨C3N4和一个未知相(面间距d=0.3984nm).喇曼光谱分析也证实了薄膜中主要存在α-C3N4,β-C3N4相.","authors":[{"authorName":"江锦春","id":"dbb43969-11bd-4ec0-81e4-b04648afb305","originalAuthorName":"江锦春"},{"authorName":"程文娟","id":"d3281f97-7e42-4f0f-8886-1bf6957c58c5","originalAuthorName":"程文娟"},{"authorName":"张阳","id":"74d5ac40-9c3e-4b65-9c46-0b1d11fbf219","originalAuthorName":"张阳"},{"authorName":"朱鹤孙","id":"5836749a-ccb1-4055-8633-b1f2e71c0899","originalAuthorName":"朱鹤孙"},{"authorName":"沈德忠","id":"38e1bf66-e349-4211-8e12-83bea02aee67","originalAuthorName":"沈德忠"}],"doi":"10.3969/j.issn.1000-985X.2004.06.012","fpage":"930","id":"14d716c0-a08d-43a4-a001-8329eb685f6f","issue":"6","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":"9e2737f5-d23f-4d92-aba6-936f902de4d5","keyword":"C3N4<span style=\"color:red\">晶体</span>","originalKeyword":"C3N4晶体"},{"id":"51ef6d3b-1922-4a6c-8d13-2b55daf614fd","keyword":"微波<span style=\"color:red\">等离子体</span>化学汽相沉积","originalKeyword":"微波等离子体化学汽相沉积"},{"id":"1444f7cc-b0b2-4ec5-b929-481cc8654a8a","keyword":"薄膜","originalKeyword":"薄膜"}],"language":"zh","publisherId":"rgjtxb98200406012","title":"微波<span style=\"color:red\">等离子体</span>化学气相沉积制备碳氮<span style=\"color:red\">晶体</span>薄膜","volume":"33","year":"2004"},{"abstractinfo":"采用加热的调谐单探针技术,研究了射频辉光放电Ar<span style=\"color:red\">等离子体</span>空间电子能量分布函数,电子平均能量和电子密度,并系统分析了<span style=\"color:red\">等离子体</span>增强化学气相沉积工艺参量对<span style=\"color:red\">等离子体</span>空间电子特性的影响.","authors":[{"authorName":"魏俊红","id":"63be274b-007d-437d-91ce-9e6a84df1675","originalAuthorName":"魏俊红"},{"authorName":"林璇英","id":"fcbac941-5661-4ea5-85e2-b03d914a1b25","originalAuthorName":"林璇英"},{"authorName":"赵韦人","id":"5223bc85-a201-4ef7-a6c3-ca6384d5d16d","originalAuthorName":"赵韦人"},{"authorName":"池凌飞","id":"e173d84d-f7d4-4121-8e15-ef463ff57083","originalAuthorName":"池凌飞"},{"authorName":"余云鹏","id":"0f3cd2b3-b718-4a5d-b72f-3a31e3b1c906","originalAuthorName":"余云鹏"},{"authorName":"林揆训","id":"c48337d0-29f7-4a93-bbf6-ee07ef98b05a","originalAuthorName":"林揆训"},{"authorName":"黄锐","id":"344ed0c6-10f4-40d7-89fa-3031698a8765","originalAuthorName":"黄锐"},{"authorName":"王照奎","id":"f63d9f48-82ad-4d14-aa6e-5b5a09ab9c7f","originalAuthorName":"王照奎"},{"authorName":"余楚迎","id":"99520e66-093b-44a9-bfaa-7995c3a0c613","originalAuthorName":"余楚迎"}],"doi":"","fpage":"755","id":"8574b65f-4ad3-4f7c-b96b-daec1c98d7a4","issue":"6","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"5e101bb3-a68b-4226-a323-288fe65d573b","keyword":"调谐单探针","originalKeyword":"调谐单探针"},{"id":"35bf6ab4-b559-4f62-992a-699068bcbe86","keyword":"<span style=\"color:red\">等离子体</span>化学气相沉积","originalKeyword":"等离子体化学气相沉积"},{"id":"20e9dc6b-2ab7-4fb5-9e1c-c3a7a9a78676","keyword":"Ar<span style=\"color:red\">等离子体</span>","originalKeyword":"Ar等离子体"}],"language":"zh","publisherId":"gncl200406032","title":"<span style=\"color:red\">等离子体</span>化学气相沉积参量对Ar<span style=\"color:red\">等离子体</span>电子特性的影响","volume":"35","year":"2004"},{"abstractinfo":"低温<span style=\"color:red\">等离子体</span>是空间主要环境之一,近年来也被广泛应用于能源、航空、环境科学、国防及材料表面改性等方面.详细的分析了<span style=\"color:red\">等离子体</span>诊断的常用方法和适用范围,认为准确进行<span style=\"color:red\">等离子体</span>诊断取决于两大因素,一是测量准确度(灵敏度),二是测试系统不对<span style=\"color:red\">等离子体</span>产生较大扰动.","authors":[{"authorName":"刘晓东","id":"566fd258-8c58-4abe-bd74-bd27646e8d1d","originalAuthorName":"刘晓东"},{"authorName":"郑晓泉","id":"32fadd4c-2dd1-4f97-b79f-3d1579b68ca9","originalAuthorName":"郑晓泉"},{"authorName":"张要强","id":"3ebb117c-d292-453d-89d5-8c2959ca9f4f","originalAuthorName":"张要强"},{"authorName":"曲文波","id":"1f3f1e74-cfdd-4abd-8e68-da1ebce1233f","originalAuthorName":"曲文波"}],"doi":"10.3969/j.issn.1009-9239.2006.02.013","fpage":"43","id":"defd0108-83d6-4ff0-8a4e-81e803f6c2b4","issue":"2","journal":{"abbrevTitle":"JYCL","coverImgSrc":"journal/img/cover/JYCL.jpg","id":"50","issnPpub":"1009-9239","publisherId":"JYCL","title":"绝缘材料"},"keywords":[{"id":"67556934-013c-4856-b308-293ba74cfc90","keyword":"<span style=\"color:red\">等离子体</span>","originalKeyword":"等离子体"},{"id":"5571b7e8-3dec-4e5e-98e6-1ffca7c583bc","keyword":"郎缪尔探针法","originalKeyword":"郎缪尔探针法"},{"id":"0a57fad8-44b3-455e-b479-7f218c92d433","keyword":"微波透射法","originalKeyword":"微波透射法"},{"id":"0775b43b-9b38-46ac-98f9-c791c1bdabea","keyword":"光谱法","originalKeyword":"光谱法"}],"language":"zh","publisherId":"jycltx200602013","title":"低温<span style=\"color:red\">等离子体</span>的诊断方法","volume":"39","year":"2006"}],"totalpage":5019,"totalrecord":50188}