首页 | 官方网站   微博 | 高级检索  
     

场致爆炸发射阴极有效发射面积研究
引用本文:刘国治,孙钧,邵浩,杨占峰.场致爆炸发射阴极有效发射面积研究[J].强激光与粒子束,2005,17(2):249-252.
作者姓名:刘国治  孙钧  邵浩  杨占峰
作者单位:西北核技术研究所,陕西,西安,710024;西北核技术研究所,陕西,西安,710024;西北核技术研究所,陕西,西安,710024;西北核技术研究所,陕西,西安,710024
基金项目:国家863计划项目资助课题
摘    要:通过改变阴阳极间隙,得到在不同外加电场情况下,场致爆炸发射石墨阴极有效发射面积随时间变化的实验结果。结果表明,在起始的一定时间内,阴极有效发射面积随时间的增加而增大。阴极有效发射面积达到1.0的时间随阴阳极间隙内电场的增加而减小;当二极管阴阳极之间的平均电场约为100 kV/cm时,阴极有效发射面积达到1.0的时间约为20 ns;阴极有效发射面积相对电压波形的延迟时间随电场的变化近似呈指数衰减曲线。

关 键 词:强流相对论电子束  阴极  二极管  有效面积
文章编号:1001-4322(2005)02-0249-04
收稿时间:2004/9/3
修稿时间:2004年9月3日

Experimental study on effective emitting area of explosive emitting cathode
LIU Guo-zhi,SUN Jun,Shao Hao,YANG Zhan-feng.Experimental study on effective emitting area of explosive emitting cathode[J].High Power Laser and Particle Beams,2005,17(2):249-252.
Authors:LIU Guo-zhi  SUN Jun  Shao Hao  YANG Zhan-feng
Affiliation:1.Northwest Institute of Nuclear Technology,P.O.Box 69,Xi'an 710024,China
Abstract:Variation relation between the effective emitting area of field induced explosive ementting graphite cathode and time has been acquired experimentally under different externally applied electric field corresponding to different anode cathode gaps. It is illustrated that the effective emitting area increase over time at the beginning of emission.The time for the effective emitting area to reach 1.0 decreases with increasing mean electric field in the gap. Under approximate 100 kV/cm mean electric field between anode and cathode, about 20 ns is needed for the effective emitting area to reach 1.0. The relative delay time of effective emitting area reaching 0.5 to 50 % voltage pulse with the electric field behaves as a decaying exponential curve.
Keywords:Intense relativistic electron beams  Cathode  Diode  Effective emitting area
本文献已被 CNKI 维普 万方数据 等数据库收录!
点击此处可从《强激光与粒子束》浏览原始摘要信息
点击此处可从《强激光与粒子束》下载全文
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司    京ICP备09084417号-23

京公网安备 11010802026262号