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首页> 外文期刊>Contributions to Plasma Physics >Enhancement of VUV Emission from a Coaxial Xenon Excimer Ultraviolet Lamp Driven by Distorted Bipolar Square Voltages
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Enhancement of VUV Emission from a Coaxial Xenon Excimer Ultraviolet Lamp Driven by Distorted Bipolar Square Voltages

机译:双极性方波畸变驱动同轴氙准分子紫外灯的VUV发射增强

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摘要

Enhancement of vacuum UV emission (172 nm VUV) from a coaxial xenon excimer UV lamp (EUV) driven by distorted 50 kHz bipolar square voltages, as compared to that by sinusoidal voltages, is investigated numerically in this paper. A self-consistent radial one-dimensional fluid model, taking into consideration non-local electron energy balance, is employed to simulate the discharge physics and chemistry. The discharge is divided into two three-period portions; these include: the pre-discharge, the discharge (most intense at 172 nm VUV emission) and the post-discharge periods. The results show that the efficiency of VUV emission using the distorted bipolar square voltages is much greater than when using sinusoidal voltages; this is attributed to two major mechanisms. The first is the much larger rate of change of the voltage in bipolar square voltages, in which only the electrons can efficiently absorb the power in a very short period of time. Energetic electrons then generate a higher concentration of metastable (and also excited dimer) xenon that is distributed more uniformly across the gap, for a longer period of time during the discharge process. The second is the comparably smaller amount of “wasted” power deposition by Xe+2 in the post-discharge period, as driven by distorted bipolar square voltages, because of the nearly vanishing gap voltage caused by the shielding effect resulting from accumulated charges on both dielectric surfaces (© 2011 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)
机译:与正弦电压相比,通过数值研究了失真的50 kHz双极方波电压驱动的同轴氙准分子紫外灯(EUV)的真空紫外发射(172 nm VUV)。考虑非局部电子能量平衡的自洽径向一维流体模型用于模拟放电物理和化学过程。放电分为两个三个周期的部分:这些包括:放电前,放电(在172 nm VUV发射时最强)和放电后时间。结果表明,使用失真的双极性方波电压时,VUV发射效率要比使用正弦波电压时高得多。这归因于两个主要机制。第一个是双极性方电压的电压变化率大得多,其中只有电子才能在非常短的时间内有效吸收功率。然后,高能电子会产生更高浓度的亚稳态氙(以及激发的二聚体)氙气,该氙气在放电过程中会在整个间隙中分布更长的时间。第二个原因是在双放电方波畸变的驱动下,后放电期间Xe + 2 产生的“浪费的”功率沉积量相对较小,这是因为几乎由于在两个介电表面上积累的电荷而产生的屏蔽效应导致的间隙电压消失(©2011 WILEY-VCH Verlag GmbH&Co. KGaA,Weinheim)

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  • 来源
    《Contributions to Plasma Physics》 |2011年第10期|p.906-919|共14页
  • 作者单位

    Department of Mechanical Engineering, National Chiao Tung University, Hsinchu, Taiwan;

    Department of Mechanical Engineering, National Chiao Tung University, Hsinchu, Taiwan;

    Department of Mechanical Engineering, National Chiao Tung University, Hsinchu, Taiwan;

    Department of Mechanical Engineering, National Chiao Tung University, Hsinchu, Taiwan;

    High-Efficiency Gas Discharge Lamps Group, Material and Chemical Research Laboratories, Hsinchu, Taiwan;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    Xenon lamp; fluid modeling; excimer; coaxial;

    机译:氙气灯;流体建模;准分子;同轴;

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