Measurement and analysis of field emission electrons in the LCLS gun

D. Dowell, E. Jongewaard, C. Limborg-Deprey, J. Schmerge, A. Vlieks
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引用次数: 8

Abstract

The field emission was measured during the high- power testing of the LCLS photocathode RF gun. A careful study and analysis of the field emission electrons, or dark current is important in assessing the gun's internal surface quality in actual operation, especially those surfaces with high fields. The first indication of a good RF gun design and fabrication is short processing time to the required fields and low electron emission at high- fields. The charge per 2 microsecond long RF pulse (the dark charge) was measured as a function of the peak cathode field for the 1.6 cell, 2.856 GHz LCLS RF gun. Faraday cup data was taken for cathode peak RF fields up to 120 MV/m producing a maximum of 0.6 nC/RF pulse for a diamond-turned polycrystalline copper cathode installed in the gun. Digitized images of the dark charge were taken using a 100 micron thick YAG crystal for a range of solenoid fields to determine the location and angular distribution of the field emitters. The FN plots and emitter image analysis will be described in this paper.
LCLS枪场发射电子的测量与分析
在LCLS光电阴极射频枪的高功率测试中测量了场发射。仔细研究和分析场发射电子或暗电流在实际操作中对于评估枪的内部表面质量非常重要,特别是那些具有高场的表面。一个好的射频枪设计和制造的第一个标志是短的加工时间到所需的场和低的电子发射在高场。测量了每2微秒长射频脉冲的电荷(暗电荷)与1.6电池,2.856 GHz LCLS射频枪峰值阴极场的函数关系。法拉第杯采集了高达120 MV/m的阴极峰值射频场数据,为安装在枪中的金刚石转多晶铜阴极产生了最大0.6 nC/RF脉冲。利用100微米厚的YAG晶体在一定范围的电磁场中拍摄暗电荷的数字化图像,以确定场发射体的位置和角分布。本文将描述FN图和发射器图像分析。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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