Measurements of 193 NM laser air breakdown and scaling to the microwave regime

M. Thiyagarajan, J. Scharer, J. Way, J. Hummelt
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Abstract

We report the measurements and analysis of air breakdown process by focusing 193 nm, 200 mJ, 10 MW high power UV laser radiation onto a 20-60 mum spot size that produces a maximum laser intensity of 1012-1013 W/cm2, well above the threshold flux for air ionization. The breakdown threshold is measured and compared with theoretical models including classical (collisional cascade) and quantum (multi-photon) ionization analyses. The air breakdown threshold is measured for a wide range of pressures ranging from 90 torr to 5 atmospheres. Higher pressure enhances the effective electric field due to the increased collisional frequency relative to the high laser frequency (1015 Hz). Multiphoton ionization (MPI) (n = 3) processes play a substantial role at 193 nm due to the high photon energy (6.4 eV). We examine regimes for which substantial MPI is present and analyze the plasma temperature and density evolution. The breakdown threshold data for air at 193 nm is correlated with the microwave breakdown regime using the concept of universal scaling, for which extensive microwave breakdown data is available as well as current microwave and mm wave breakdown experiments at Texas Tech University and MIT. An extensive range of optical and spectroscopic diagnostics with 5 ns time scale gating and 13 mum ICCD resolution has been constructed to characterize the plasma. The spatial and temporal evolution of the laser focused plasma is measured using shadowgraphy and two- color laser interferometry techniques. The plasma temperatures are obtained by measuring the velocity of the shock wave front and also by using optical emission spectroscopy. Optical emission spectroscopy is performed to diagnose the plasma temperature using the emission lines of O II ranging from 372.3 to 470.4 nm and the band of the N2 second positive system N2 (2+) (0,0) at 337.1 nm. Measurements of the core laser plasma density (ne= 8times1017/cc) and electron temperature (25 eV) decay are compared with a dominant two- and three-body recombination model with good correlation.
193nm激光空气击穿的测量及对微波区的缩放
我们报告了空气击穿过程的测量和分析,通过将193 nm, 200 mJ, 10 MW的高功率紫外激光辐射聚焦在20-60 μ m光斑上,产生的最大激光强度为1012-1013 W/cm2,远高于空气电离的阈值通量。测量了击穿阈值,并与经典(碰撞级联)和量子(多光子)电离分析等理论模型进行了比较。空气击穿阈值是在从90托到5个大气压的压力范围内测量的。相对于激光的高频率(1015hz),更高的压力增加了碰撞频率,从而增强了有效电场。多光子电离(MPI) (n = 3)过程在193 nm处由于高光子能量(6.4 eV)而发挥重要作用。我们研究了存在大量MPI的制度,并分析了等离子体温度和密度的演变。空气在193nm处的击穿阈值数据与微波击穿状态使用通用尺度的概念相关联,其中广泛的微波击穿数据可用,以及目前在德克萨斯理工大学和麻省理工学院的微波和毫米波击穿实验。广泛的光学和光谱诊断与5 ns时间尺度门控和13 mum ICCD分辨率已经构建表征等离子体。采用阴影法和双色激光干涉测量技术测量了激光聚焦等离子体的时空演化。等离子体温度是通过测量激波前的速度和利用光学发射光谱得到的。利用oii在372.3 ~ 470.4 nm范围内的发射谱线和N2(2+)(0,0)在337.1 nm范围内的发射谱线对等离子体温度进行了诊断。对核心激光等离子体密度(ne= 8times1017/cc)和电子温度(25ev)衰减的测量结果进行了比较,得到了具有良好相关性的二体和三体复合模型。
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