用于低抖动脉冲功率应用的光激活开关

F. Zutavern, J. C. Armijo, S. M. Cameron, G. J. Denison, J. Lehr, T. Luk, A. Mar, M. O’Malley, L. D. Roose, J. V. Rudd
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引用次数: 20

摘要

光激活高压开关通常用于脉冲电力系统中可靠的低抖动,多通道和多开关(低电感)应用。除了低抖动开关外,光激活在触发和开关电源系统之间提供了高度的电气隔离,简化了脉冲电源设计。大间隙气体开关光触发的缺点是光能、视距光学和获得可靠运行所需的系统维护。本文介绍了两种可以减少或消除这些缺点并为脉冲电源系统提供更灵活的光激活开关的技术。一种方法是降低气隙开关的光触发能量需求。较短的光脉冲需要较少的能量来启动等离子体放电。用120秒宽的光脉冲触发50-100千伏气隙开关的实验正在组装中。通过将金属气溶胶引入气隙也证明了较低的触发能量W. Frey(1997)。该装置将被添加到该实验中,以重现这些结果,并确定在一定波长和脉冲宽度范围内的光能和功率密度要求。本文将讨论本实验的现状。第二种方法在两种配置中使用固态开关:(1)作为主开关,(2)作为触发器。高增益光导半导体开关(PCSS)在一些直接脉冲功率开关应用中是实用的。我们已经演示了高达220 kV和8 kA的开关。结合固态和气隙开关技术可以获得更高功率的光激活开关。多兆伏特(MMV)开关可以通过光纤触发,远程定位的PCSS触发。通过将紧凑型PCSS触发器放置在非常靠近触发点的位置,可以使用低能量光纤触发系统实现可靠,低抖动,高功率的开关,可以轻松地从远程控制中心进行控制和调整。触发系统的电力可以来自触发器附近的电场,因此所有连接到触发系统的电缆都被取消,取而代之的是直径100微米的光纤,用于触发和监控系统的运行。本文将报道PCSS触发气隙开关的实验结果和PCSS触发多兆伏特开关的设计。还将介绍PCSS开关特性,包括新的皮秒脉冲结果和提高寿命的制造过程。采用120 fs宽的780 nm激光脉冲,用工作在线性模式下的GaAs PCSS辐射太赫兹带宽脉冲。PCSS触点制造的新方法正在开发和测试,以简化生长过程,增加每灯丝容量的电流,并提高器件寿命。不断的进步使PCSS成为脉冲功率应用中更有用的组件。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Optically activated switches for low jitter pulsed power applications
Optically activated high voltage switches are commonly used in pulsed power systems for reliable low jitter, multichannel and multiswitch (low inductance) applications. In addition to low jitter switching, optical activation provides a high degree of electrical isolation between the triggering and switching power systems simplifying pulsed power design. The disadvantages of optical triggering for large-gap gas switches are the optical energy, line-of-sight optics, and system maintenance required to obtain reliable operation. This paper describes two technologies which can reduce or eliminate these disadvantages and provide more flexible optically activated switches for pulsed power systems. One approach is to reduce the optical trigger energy requirement for gas gap switches. Shorter optical pulses require less energy to initiate a plasma discharge. An experiment is being assembled to trigger a 50-100 kV gas gap switch with 120 fs wide optical pulses. Lower trigger energy has also been demonstrated by the introduction of metallic aerosols into a gas gap W. Frey (1997). The apparatus will be added to this experiment to reproduce these results and determine the optical energy and power density requirements over a range of wavelengths and pulse widths. The status of this experiment will be discussed. A second approach uses solid state switching in two configurations: (1) as the main switch and (2) as a trigger. High-gain photoconductive semiconductor switches (PCSS) are practical for some direct pulsed power switching applications. We have demonstrated switching up to 220 kV and 8 kA. Higher power optically activated switching can be obtained by combining solid state and gas gap switching technologies. Multimegavolt (MMV) switches can be triggered with fiber-optically triggered, remotely located PCSS. By placing the compact PCSS trigger extremely close to the trigger point, reliable, low-jitter, high power switching is achieved with low energy fiber-optic trigger systems that can easily be controlled and adjusted from a remote control center. Power for the trigger system can be derived from the electrical fields near the trigger, so all electrical cables to the trigger system are eliminated and replaced with 100 micron diameter fibers that trigger and monitor the operation of the system. Results from experiments with PCSS triggered gas gap switches and the design for a PCSS triggered multimegavolt switch will be reported. PCSS switching properties including new picosecond pulse results and fabrication procedures for improved longevity will also be described. A 120 fs wide 780 nm laser pulse was used to radiate THz bandwidth pulses with a GaAs PCSS operating in the linear mode. New approaches for PCSS contact fabrication are being developed and tested to simplify the growth procedure, increase the current per filament capability, and improve device longevity. Progress continues to make PCSS a more useful component for pulsed power applications.
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