Electronically steerable plasma mirror for radar applications

J. Mathew, R.A. Meger, J. Gregor, R.E. Pechacek, R. Fernsler, W. Manheimer
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引用次数: 12

Abstract

An alternative to using a phased array to steer a high frequency microwave beam is to electronically control the orientation of an inertialess broadband microwave reflector. Such a system could steer one or more high power beams for search or tracking radars, and the system could possess wide instantaneous bandwidth. Experiments have demonstrated that a planar plasma mirror can be formed with electron densities high enough to reflect X-band microwaves. Estimates of microwave beam power handling capabilities of such a plasma Sheet exceed 3 kW/cm/sup 2/ for microsecond duration pulses at kilohertz repetition rates. The plasma minor is formed by driving a glow discharge between a hollow cathode and a flat plate anode which are immersed in an axial magnetic field of 150-300 Gauss. The plasma sheet could in principle be steered in one plane using the magnetic field, and in another by designation of the cathode. A 50 cm wide, 1 cm thick, 60 cm long plasma sheet is formed between the cathode and the anode 10 /spl mu/s after the voltage is applied. The discharge also extinguishes within 10 /spl mu/s of the voltage being turned off. For a 4 kV voltage pulse, plasma densities /spl les/10/sup 13/ cm/sup -3/ are achieved within the plasma sheet. The discharge gas is air at 130 mTorr. Single mirrors have been formed with pulse widths of 20-1000 /spl mu/s, and burst mode operation at 10 kHz has been achieved with 30-70 /spl mu/s long pulses. Measurements of the phase using a heterodyned microwave interferometer show that the critical surface is stationary during most of the pulse. A 30 cm diameter Cutler-feed antenna is being used to illuminate the mirror at 10 GHz. The H-plane radiation pattern (for a 90/spl deg/ reflection) measured 4.3 m from the plasma mirror, is very similar to that obtained from a metal mirror of comparable dimensions.
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用于雷达的电子操纵等离子体反射镜
一种替代使用相控阵来引导高频微波束的方法是电子控制无惯性宽带微波反射器的方向。这样的系统可以引导一个或多个高功率波束用于搜索或跟踪雷达,并且系统可以拥有宽的瞬时带宽。实验证明,一个平面等离子体镜面可以形成足够高的电子密度,以反射x波段的微波。估计这种等离子体片的微波光束处理能力超过3千瓦/厘米/sup 2/微秒持续脉冲在千赫兹重复率。在浸入150 ~ 300高斯的轴向磁场中,在中空阴极和平板阳极之间驱动辉光放电形成等离子体。原则上,等离子体片可以利用磁场在一个平面上操纵,而通过阴极的指定在另一个平面上操纵。施加电压10 /spl mu/s后,阴极和阳极之间形成50 cm宽、1 cm厚、60 cm长的等离子体片。放电也在电压关断后10 /spl μ s内熄灭。对于4 kV电压脉冲,等离子体密度/spl / les/10/sup / 13/ cm/sup -3/在等离子体片内实现。排出气体为130 mTorr的空气。形成了脉冲宽度为20-1000 /spl μ s的单镜,并在30-70 /spl μ s的长脉冲下实现了10 kHz的突发模式工作。用外差微波干涉仪测量的相位表明,在脉冲的大部分时间里,临界表面是静止的。一个直径30厘米的卡特勒馈电天线被用来在10千兆赫的频率上照亮镜子。在距离等离子体反射镜4.3 m处测量到的h面辐射图(90/spl度/反射)与同等尺寸的金属反射镜得到的结果非常相似。
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