被动等离子体光子晶体器件太赫兹击穿的三种等离子体中性模型

W. Thomas, E. Meier, U. Shumlak
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引用次数: 0

摘要

等离子体光子晶体(PPCs)通过在GHz到低太赫兹范围内提供对能量带隙/通特性的高速(μs)控制,有可能显著扩展当前毫米波滤波和开关技术的能力。此外,介质光子晶体可以用共振缺陷中的自激发等离子体功能化,以提供无源功率调制。在低太赫兹范围内构建实验装置是具有挑战性的,要求等离子体密度为10 - 22 m -3,器件特征长度为亚毫米。通常用于低温和过程等离子体模拟的漂移扩散模型依赖于反应速率和输运系数,该模型由玻尔兹曼解算器计算,假设低电离分数(<10 -5),以及稳态电场和电子密度。必须对时间和空间变化的字段进行特别扩展。因此,探索计算上易于处理的高密度和高电离分数反应等离子体中性混合物的替代方法是强烈的动机。在这项工作中,Meier和Shumlak[等离子体物理学,19,7,(2012)]开发的现有三种(电子-离子中性原子)5矩模型被扩展到包括反应速率中的电子中性相对速度,以捕获静电和交流击穿。给出了太赫兹氩等离子体的初步实验结果和模型验证。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Three-Species Plasma-Neutral Modeling of THz Breakdown for Passive Plasma-Based Photonic Crystal Devices
Plasma photonic crystals (PPCs) have the potential to significantly expand the capabilities of current millimeter wave filtering and switching technologies by providing high speed (μs) control of energy band-gap/pass characteristics in the GHz through low THz range. Furthermore, dielectric photonic crystals can be functionalized with self-initiated plasmas in resonant defects to provide passive power modulation. Constructing experimental devices in the low THz range is challenging, requiring plasma densities on the order of 10 22 m -3 , and sub-millimeter device characteristic lengths. Drift-diffusion models typically used in low temperature and process plasma simulations rely on reaction rate and transport coefficients calculated by Boltzmann solvers that assume low ionization fractions (<10 -5 ), and steady-state electric fields and electron densities. Ad hoc extensions to temporally and spatially varying fields must be made. Exploring computationally tractable alternative methods for high-density and high-ionization-fraction reacting plasma-neutral mixtures is therefore strongly motivated. In this work, an existing three-species (electron-ion-neutral atom) 5-moment model developed by Meier and Shumlak [ Physics of Plasmas , 19, 7, (2012)] is extended to include electron-neutral relative velocity in reaction rates in order to capture electrostatic and AC breakdown. Initial results and model validation for a THz argon plasma are presented.
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