氢直流辉光放电中的 H- 生成。

D. Lopaev, Y. Mankelevich, A. Kropotkin, D. Voloshin, T. V. Rakhimova
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引用次数: 0

摘要

在 0.1-3 托的压力和 1-30 毫安的电流范围内,采用激光光致脱附技术研究了 H2 直流辉光放电正柱中的 H- 离子动力学,其 E/N 范围从 ~ 40 Td 到 ~ 170 Td。放电电流的部分调制表明,由于原子的快速脱离反应,H-浓度与 H 原子的动态一致:H 密度越高,H-/ne 比值越低。放电调制时 H 原子密度的动态是通过对 Ar 原子的时间分辨放电测量法来测量的,而 H2 振荡温度则是通过比较测量和模拟的 H2 紫外吸收光谱来估算的。通过分析放电参数对 H- 和 H/H2 的实验依赖性,可以估算出放电中 H- 生成的有效速率常数与还原电场的函数关系。为此,我们建立了放电模型,其中包括自洽的态间振动动力学以及 H2 的高度激发电子态。本文详细讨论了导致 H- 生成和损耗的主要过程。与振动激发的 H2(v)分子发生解离附着是 H- 生成的主要途径,但只有在低 E/N 时才会通过激发 H2-(X2Σu+)著名的低能(εth ≈ 3 eV)形状共振发生。在高 E/N 时,H- 的产生主要是通过激发高能 H2- 态来实现的,如 H2-(B2Σg+、A2Σg+、C2Πu) 和类似于 H2-(2Σg+)雷德贝格态的费什巴赫共振。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
H– production in hydrogen DC glow discharge.
H- ion dynamics in the positive column of H2 dc glow discharge was studied by the laser photodetachment technique in a wide range of pressure, 0.1–3 Torr, and current, 1-30 mA which cover a range of E/N from ~ 40 Td up to ~ 170 Td. Using partial modulation of discharge current it is shown that the H– concentration follows H atom dynamics due to fast detachment reaction with the atoms: the higher H density, the lower H-/ne ratio. Dynamics of H atom density at discharge modulation was measured by the time-resolved actinometry on Ar atoms while H2vibrational temperature was estimated by comparing measured and simulated H2 VUV absorption spectra. The analysis of the experimental dependencies of H– and H/H2 on the discharge parameters allowed estimating the effective rate constant of H– production in the discharge as a function of the reduced electric field. For this the discharge model including self-consistently state-to-state vibrational kinetics as well as H2 highly excited electronic states was developed. The main processes, that contribute to H– production and loss, are discussed in detail. Dissociative attachment to vibrationally excited H2(v) molecules is the main channel of H- production but occurs via the excitation of the well-known low-energy (εth ≈ 3 eV) shape resonance of H2-(X2Σu+) only at low E/N. At high E/N, the H- production mostly occurs via the excitation of the high-energy H2- states, such as H2-(B2Σg+, A2Σg+, C2Πu) and Feshbach resonances similar to H2-(2Σg+) Rydberg state.
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