电泳法是制作碳纳米管冷阴极的重要方法.电泳电压是电泳过程中的重要参数,不同电压会影响阴极沉积的厚度和效率、形貌结构及场发射特性.实验对比研究和机理分析认为,电压在20~30 V区间内较易获得良好的碳纳米管场发射冷阴极.针对电泳边缘增厚效应,提出减小电场强度边缘效应方法.
参考文献
[1] | Iijima S.Helical microtubules of graphitic carbon[J].Narture,1991,354(7):56-8. |
[2] | Frank S,Poncharal P,Wang Z L,et al.Carbon nanotube quantum resistors[J].Science,1998,280(5370):1741-1744. |
[3] | 曹章轶,王红光,孙卓.钯膜上CVD法制备碳纳米管薄膜的研究[J].液晶与显示,2007,22(4):387-392. |
[4] | Wang Lili,Chen Yiwei,Sun Zhuo,et al.Optimization of field emission properties of carbon nanotubes cathodes by electrophoretic deposition[J].Materials Lett.,2007,61(4):1265-1269. |
[5] | 李艳楠,孙卓,陈岳.利用流动催化法在减压化学气相沉积系统中制备碳纳米管粉末[J].液晶与显示,2007,22(3):288-293. |
[6] | Shoushan Fan,Chapline Michael G,Franklin Nathan R.et al.Self-oriented regular arrays of carbon nanotubes and their field emission properties[J].Science,1999,283(5401):512-514. |
[7] | Li Juntao,Lei Wei,Zhang Xiaobing.et al.Field emission characteristic of screen-printed carbon nanotube cathode[J].Appl.Surface Science,2003,220(1):96-104. |
[8] | Zhao Haifeng,Song Hang,Li Zhiming,et al.Electrophoretic deposition and field emission properties of patterned carbon nanotubes[J].Appl.Surface Science,2005,251(1):242-244. |
[9] | Rao A M,Richter E,Bandow S,et al.Diameter-selective raman scattering f rom vibrational modes in carbon nanotubes[J].Science,1997,275(5297):187-191. |
[10] | Negishi H,Yanagishita H,Yokokawa H.Electrophoretic deposition of solid oxide fuel cell material powders[C]//Proceedings of Electrochemical Society on Electrophoretic Deposition:fundamentals and applications,Pennington,NewJersey,USA:The Electrochemical Society Inc.,2002:214-215. |
[11] | 周雪东,张宇宁,雷威.等.最佳碳纳米管场发射阴极阵列密度的研究[J].电子器件,2003,26(4):379-382. |
[12] | 朱亚波,王万录,廖克俊.对碳纳米管阵列的场发射电场增强因子以及最佳阵列密度的研究[J].物理学报,2002,51(10):2335-2339. |
[13] | 谷长寿,张颖,曹力生.平行板电容器边缘效应的研究[J].辽宁工学院学报(自然科学版),1994,14(3):80-82. |
上一张
下一张
上一张
下一张
计量
- 下载量()
- 访问量()
文章评分
- 您的评分:
-
10%
-
20%
-
30%
-
40%
-
50%