Multipactor suppression via higher-order modes

S. Rice, J. Verboncoeur
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引用次数: 2

Abstract

Summary form only given. Multipactor is a resonant phenomenon in which an electromagnetic field causes a free electron to impact a surface, resulting in the surface emitting one or more secondary electrons. If the surface geometry and electromagnetic fields are appropriately arranged, the secondary electrons can then be accelerated and again impact a surface in the bounding geometry. If the net number of secondary electrons participating in multipactor is non-decreasing, then the process can repeat indefinitely. This phenomenon is of considerable practical interest in the design and operation of high power resonant structures. When the secondary electron yield (SEY) of a material measured as a function of the incident electron kinetic energy, the curve follows a similar shape for many materials: At low incident kinetic energies, the SEY is low; at intermediate kinetic energies, the SEY is maximized at a material-dependent energy; at high kinetic energies, the SEY tapers down to zero with increasing energy. In order multipactor to be self-sustaining, the average SEY over multipactor path must be at least unity. This means that multipactor can only be sustained within a certain material-dependent range of incident electron kinetic energies. This research investigates the feasibility of suppressing multipactor through the use of higher-order cavity modes which will modify the incident kinetic energy of impacting electrons. Since the SEY is dependent upon kinetic energy of the incident electron, our goal is modify impacting electron velocities to reduce the average SEY less than unity such that multipactor is not sustainable. Preliminary computer simulations are presented which demonstrate this concept in reducing or eliminating multipactor in a 2-dimensional coaxial cavity geometry.
通过高阶模式的多因子抑制
只提供摘要形式。多因素是一种共振现象,其中电磁场导致一个自由电子撞击表面,导致表面发射一个或多个次级电子。如果表面几何形状和电磁场安排得当,那么二次电子就可以被加速并再次撞击边界几何形状中的表面。如果参与多因子的次级电子的净数量不减少,则该过程可以无限重复。这种现象在大功率谐振结构的设计和运行中具有重要的实际意义。当测量材料的二次电子产率(SEY)作为入射电子动能的函数时,许多材料的曲线都遵循类似的形状:在低入射动能时,SEY较低;在中等动能时,SEY在物质依赖能量处最大;在高动能时,随着能量的增加,SEY逐渐减小到零。为了使多因子自维持,多因子路径上的平均SEY必须至少为1。这意味着多因子只能在入射电子动能的一定物质依赖范围内维持。本研究探讨了利用高阶空腔模式来抑制多因子的可行性,该模式将改变撞击电子的入射动能。由于SEY依赖于入射电子的动能,我们的目标是修改冲击电子的速度,使平均SEY小于1,从而使多因子不可持续。初步的计算机模拟证明了这一概念在减少或消除二维同轴腔几何中的多因子。
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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