利用Spark3D软件分析实验多因素观测信号

T. Sugai, Z. Shaw, J. Dickens, A. Neuber
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引用次数: 0

摘要

多因子是一种共振非线性电子倍增效应,可能发生在极低压力下的高功率微波器件中,例如粒子加速器和卫星子系统。其影响范围从信号退化到微波元件的损坏和破坏。因此,通过理论分析、数值模拟和实验对多因子物理进行了研究。在此之前,我们开发了一种使用电子倍增管(EMT)的直接电子观测系统,并成功地直接检测到矩形波导宽壁中心的多封装电子1,2。在此,我们提供了一种评估波导中电荷密度和二次发射产率的方法。利用Spark3D数值模拟软件对实验得到的EMT信号进行了分析。利用该软件分析了波导结构中多因子的起始,采用高频求解器对无多因子的电场分布进行了仔细模拟。在与实验相同的条件下,模拟了EMT信号和电荷密度。得到了一条表示EMT电压与电荷密度之间的比例关系的校准线,该校准线不受输入功率和间隙大小等条件的影响。进一步,对导入Spark3D的SEY曲线进行调整后,实验EMT信号脉冲的上升形状与仿真EMT信号脉冲的上升形状拟合,EMT信号生成的实验阈值功率与仿真多因子阈值功率一致。由于模拟结果在阈值功率和信号形状上与实验结果相吻合,因此可以预期从模拟中得到的电荷密度和SEY曲线是准确的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Analysis Of Experimental Multipactor Observation Signals Using Spark3D Software
Multipactor is a resonant nonlinear electron multiplication effect that may occur in high power microwave devices at very low pressures, such as those operating in particle accelerators and satellite subsystems. Its effects range from signal degradation to the damage and destruction of microwave components. Thus, multipactor physics has been studied through theoretical analysis, numerical simulation, and experiment. Previously, we developed a direct electron observation system using an Electron Multiplier Tube (EMT) and succeeded to directly detect multipactoring electrons in the center of the broadwall of rectangular waveguides 1, 2. Here, we provide a method for evaluating the electric charge density and secondary emission yield (SEY) in waveguides. The experimentally obtained EMT signal is analyzed with the extensive usage of the numerical simulation software Spark3D. The software was utilized to analyze multipactor onset in waveguide structures, where the electric field distribution without multipactor was carefully simulated, employing high-frequency solvers. The EMT signal and the charge density were simulated for the same conditions as the experiment. As a result, a calibration line indicating the proportional relation between the EMT voltage and the charge density, which is independent of some conditions, i.e., input power and gap size, was obtained. Further, after adjusting the SEY curve imported to Spark3D, the rising shape of the experimental EMT signal pulses fit with the simulated one, and the experimental threshold power for the EMT signal generation was consistent with the simulated multipactor threshold power. Since the simulation matches the experiment in threshold power and signal shape, one expects that the charge density and SEY curve deduced from the simulation are accurate.
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