1.5 MW, 110 GHz脉冲回旋管启动方案的实验结果

D. Tax, W. Guss, I. Mastovsky, M. Shapiro, R. Temkin
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引用次数: 1

摘要

我们介绍了在1.5 MW, 110 GHz, TE22,6模式回旋管上运行3µs脉冲的实验结果。最近安装了一种新的内模转换器(IMC),它表现良好,提供了高高斯输出光束1。我们最近的研究集中在电压脉冲上升过程中回旋管的工作。功率和频率作为电压的函数以两种不同的方式测量。首先,外差接收系统可以在脉冲的不同时间间隔内进行门控,允许在电压脉冲上升到96千伏的峰值期间识别频率。或者,可以改变峰值电压,并且可以记录在电压脉冲平顶期间测量的功率和频率。在标称工作电压为96千伏附近,观察到频率与电压的小变化,在较低电压下略高。随着电压的进一步降低,频移变得更加明显,最终腔模式切换到更低的频率模式。当主磁场为4.38 T(回旋管的最高输出功率)时,电压从50到70 kV变化时,这种低频模式从~ 109 - 107.5 GHz变化。模态可以是高阶轴向te21,6 BWO模态。我们还观察到模式切换的例子,没有大的瞬时频率移位,这被怀疑是从一个轴向模态数切换到另一个。在这些情况下,频移的速率突然变化,轴向模态数较高的模态的频移速率较大,尽管频率保持连续。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Experimental results of the start-up scenario for a 1.5 MW, 110 GHz pulsed gyrotron
We present experimental results on our 1.5 MW, 110 GHz, TE22,6 mode gyrotron, operating with 3 µs pulses. A new internal mode converter (IMC) was recently installed, and it performed well, providing a highly Gaussian output beam1. Our latest studies have focused on the operation of the gyrotron during the rise of the voltage pulse. The power and frequency are measured as a function of voltage in two different ways. First, a heterodyne receiver system that can be gated over various time intervals of the pulse allows for frequencies to be identified during the rise of the voltage pulse to its peak value of 96 kV. Alternatively, the peak voltage can be varied and the power and frequency measured during the flat top of the voltage pulse can be recorded. Around the nominal operating voltage of 96 kV, a small shift in frequency vs. voltage was observed, being slightly higher at lower voltages. As the voltage was further decreased, the frequency shift became more pronounced, and eventually the cavity mode switched to a lower frequency mode. This lower frequency mode varied from ∼109 – 107.5 GHz as the voltage varied from 50 to 70 kV at a main magnetic field of 4.38 T (where the gyrotron has its highest output power). The mode may be a higher order axial TE21,6 BWO mode. We also observed examples of mode switching without a large instantaneous shift in frequency, which is suspected to be the switch from one axial mode number to another. In these cases, the rate of the frequency shift changes suddenly, being larger for the modes with higher axial mode numbers, though the frequency remains continuous.
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