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西安交通大学 电子物理与器件教育部重点实验室, 陕西 西安 710049
收稿日期:2014-04-08,
修回日期:2014-04-29,
网络出版日期:2014-05-01,
纸质出版日期:2014-12-05
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杨小艳, 沈志华, 吴胜利. 纳米裂缝位置可控的表面传导电子发射薄膜[J]. 液晶与显示, 2014,29(6): 911-915
YANG Xiao-yan, SHEN Zhi-hua, WU Sheng-li. Controllable nano-scale gap formation in surface conduction-electron emitter[J]. , 2014,29(6): 911-915
杨小艳, 沈志华, 吴胜利. 纳米裂缝位置可控的表面传导电子发射薄膜[J]. 液晶与显示, 2014,29(6): 911-915 DOI: 10.3788/YJYXS20142906.0911.
YANG Xiao-yan, SHEN Zhi-hua, WU Sheng-li. Controllable nano-scale gap formation in surface conduction-electron emitter[J]. , 2014,29(6): 911-915 DOI: 10.3788/YJYXS20142906.0911.
提出一种新型结构的表面传导电子发射导电薄膜,该导电薄膜在中间位置向内有凹陷,基于电形成过程中焦耳热引起薄膜龟裂的原理,会在凹陷附近诱导纳米级裂缝形成,控制纳米裂缝形成位置。分析了此结构导电薄膜对裂缝产生位置的影响及2种不同电形成方法对裂缝形貌的影响,测试了电子发射性能,得到了发射电流特性曲线和发光图像。实验结果表明,这种新型导电薄膜能一定程度上控制纳米裂缝的形成位置,有利于改进表面传导电子发射的均匀性,在阳极高压2.0 kV、阴极板电子发射单元施加的器件电压14 V时,新型结构导电薄膜实现了均匀发光,发射电流最大为18 A。
A conductive film with new structure for surface conduction electron emitter is proposed in this paper. Since the specific conductive film structure is narrower in the middle part
the joule heat in this region can be larger than that in the other region. This may lead to a thermal stress concentration in the middle region
and finally cause the nano-scale fissure to be generated easily from this position. With this new conductive film structure
the formation position of the nano-scale fissure can be controlled easily. The results indicate that the nano-scale gap position formed in the conductive film can be controlled to some extent. SCEs with the specific conductive film have better uniformity compared with the SCEs with the conventional conductive film structure. For an anode voltage of 2.0 kV and a device voltage of 14 V
the emission current of the SCEs with the specific conductive film can reach 18 A.
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