重复脉冲电子束二极管中的等离子体特性

M. Myers, D. Hinshelwood, F. Hegeler, M. Wolford
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引用次数: 0

摘要

在大功率真空二极管中电子束的产生导致阳极和阴极等离子体的形成。有充分的证据表明,这些等离子体进入A-K间隙的膨胀可能对主电子束脉冲期间二极管的性能产生不利影响。电离气体存在于主脉冲之后,会限制二极管的性能。对于一个给定的重复脉冲驱动器,二极管的物理特性很大程度上取决于阴极中使用的发射极材料、阳极材料、电场E、dE/dt、电流密度(J)、真空泵速度、脉冲宽度和脉冲重复频率(PRF)。在NRL固态脉冲发生器的单次发射和每秒1脉冲(PPS)的PRF下,使用介电纤维天鹅绒和石墨阴极研究了二极管等离子体。利用光纤激光干涉仪测量阴极等离子体的线密度。一个门控相机被用于纳秒分辨率等离子体发射在轴向位置横跨阳极-阴极间隙。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Plasma characterization in a repetitively pulsed electron beam diode
Electron beam (e-beam) generation in high power vacuum diodes results in anode and cathode plasma formation. It is well documented that expansion of these plasmas into the A-K gap may adversely affect diode performance during the main e-beam pulse. Ionized gases exist after the main pulse and can limit diode performance. For a given repetitively pulsed driver, diode physics will depend largely on the emitter material used in the cathode, the anode material, the electric field E, dE/dt, current density (J), vacuum pumping speed, the pulse width, and the pulse repetition frequency (PRF). For single shots and at a PRF of 1 pulse per second (PPS) taken on the NRL Solid State Pulser, diode plasmas are investigated using dielectric fiber velvet and graphite cathodes. A fiber laser interferometer is used to measure the line density of plasma at the cathode. A gated camera is fielded for nanosecond resolution of plasma emissions at axial positions across the anode-cathode gap.
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