高功率微波管磁压缩光束相对论Mlg的计算机模拟

J. E. Beers
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引用次数: 0

摘要

高功率微波管需要高度聚焦的高能电子束。高频率使与电子束的r-f相互作用集中在电子束的外缘,使中心相对不重要。磁控管注射枪(MIG)用一个截锥作为阴极,用一个轴向磁场将电子流集中在一个环隙中,消除了电子束中心的电流。对于需要这些大电流相对论光束的加速器,已经使用pbgun进行了相对论MIG的理论研究,数字程序的泊松模拟粒子束模拟显示,有两种类型的枪支,需要考虑阴极相比,短轴向轴的平均半径和那些长度相当于或超过平均半径短阴极是由轴向端条件需要接近皮尔斯角(67 5度),但小影响加速电极的形状了阴极对末端条件和加速电极都至关重要,需要一个或两个过渡区,一个用于将光束传输到其最终直径,另一个用于将光束轴向旋转,使其在到达阴极前不会产生过多的波纹。更长的阴极也可以用更大的锥角来稳定,锥角小于15度的半角往往更不稳定,阴极越长,电流越高,形成可移动的压缩光束的难度就越大
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Computer Simulations Of Relativistic Mlg's With Magnetically Compressed Beams For High Power Microwave Tubes
High power microwave tubes require well focussed high energy electron beams High frequencies cause the r-f interaction with the beam to concentrate in the outer edge of the beam making the center relatively unimportant The Magnetron Injection Gun (MIG) uses a truncated cone for a cathode and an axial magnetic field to concentrate the electron current in an annulus eliminating the current in the center of the beam High power microwave tubes used for r f plasma generation, and for accelerators require these high current relativistic beams A theoretical study of Relativistic MIG's has been carried out using PBGUNS', a digital program for the Poisson simulation of particle beams The simulations show that there are two types of guns that need to be considered those with cathodes that are short axially compared with their mean radius from the axis and those whose length are comparable to or longer than the mean radius Short cathodes are dominated by the axial end conditions which need to be close to the Pierce angle (67 5 degrees) but are little effected by the shape of the accelerating electrode The longer cathodes are critically dependent on both the end conditions and the accelerating electrode One or two transition regions are needed, one to transporl the beam to its final diameter and a second to turn it axially in such a way that it does not ripple excessively before it reaches the front of the cathode, but can be relieved by reducing the magnetic field so that the electrons rise well above the cathode Longer cathodes can also be stabilized by using larger cone angles Cone half angles of less than 15 degrees tend to be more unstable The longer the cathode and the higher the current the greater the difficulty in forming a transportable, compressed beam Several examples will be presented
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