微秒脉冲产生管

W. Cornetet, J. Josenhans
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引用次数: 1

摘要

本文介绍了一种利用速调管聚束的100毫微秒重复脉冲产生管的原理和测试。漂管通过角Θ0of约为150°时,获得了发电机的最佳运行状态;调制深度\alpha = {V_1}/{V_0} = 1;还原等离子体角\Phi _q0{ < 20°。观察和数据是用Edgerton, Germeshausen和Grier行波示波器和比较测量技术确定的。发生器的测量脉冲上升时间为130µµs(0- 100%),在半电压点的脉冲持续时间为300µµs。在50欧姆的同轴线上,20伏的脉冲高度是可能的。应用于脉冲形状预测的分析是基于大信号弹道聚束理论和量子化集电极间隙理论。分析和测量之间的比较表明误差约为20%。理论预测,脉冲持续时间几乎没有改进,但脉冲上升时间可能随着电路复杂性的增加而改善。}
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A millimicrosecond pulse-generator tube
This paper describes the theory and testing of a 100- Mc repetition-rate millimicrosecond pulse-generator tube utilizing klystron bunching. The optimum operation of the generator was obtained with a drift-tube transit angle Θ0of approximately 150°; depth of modulation\alpha = V_{1}/V_{0} = 1; and the reduced plasma-angle\Phi_{q}was less than 20°. Observations and data were determined with an Edgerton, Germeshausen and Grier traveling-wave oscilloscope and a comparison measurement technique. The generator has a measured pulse rise time of 130 µµsec (0-100 per cent), and a pulse duration of 300 µµsec at the half-voltage point. A pulse height of 20 volts on a 50-ohm coaxial line is possible. The analysis applied in predicting the shape of the pulse was based on large signal ballistic bunching theory and a quantized collector gap theory. A comparison between analysis and measurement indicates an error of about 20 per cent. Theory predicts that little improvement can be made in the pulse duration, but the pulse rise time may be improved with increased circuit complexity.
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