中压下双极直流脉冲微等离子体的特性

Peng Tian, Sanghun Song, M. Kushner, S. Macheret
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引用次数: 2

摘要

只提供摘要形式。在空间受限腔中产生的微等离子体具有广泛的应用,从电气开关和自由基生产到照明。在这些应用中,通常需要在获得较短的等离子体响应时间和最大化等离子体密度之间进行权衡,两者都需要更高的压力才能优化;并获得均匀的等离子体,在较低的压力下达到最佳状态。这些尺度推动了在中等压力下的操作,从几十托到100托,通过pd尺度对应于数百微米的微腔尺寸。在许多情况下,由于易于制造或最大化寿命,微等离子体腔的内表面大部分是介电的。这些条件激发了某种形式的双极激发。本文讨论了以时间平均电子密度最大化为目标的脉冲直流双极波激发的微等离子体尺度计算研究的结果。计算平台是混合等离子体设备模型,这是一个二维流体动力学模型,其中辐射输运、电子和离子分布使用蒙特卡罗技术进行处理。我们研究了由短直流双极脉冲(几ns)激发的10s-100s Torr等离子体,脉冲重复周期从几十到几百ns,使用稀有气体混合物。空腔尺寸为几百微米。预测了Penning混合物的准稳态、时间平均电子密度超过1015 cm-3。虽然本体电子的电离是主要来源,但由于鞘层加速的次级电子,等离子体的均匀性对电离很敏感。等离子体的行为与电压脉冲的极性是不对称的,在循环的阳极部分发生了更多的电离,这在很大程度上是由于电漂浮的介电边界。
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Properties of bipolar DC-pulsed microplasmas at intermediate pressures
Summary form only given. Microplasmas generated in spatially confined cavities have applications ranging from electrical switching and radical production to lighting. In these applications, there is often a tradeoff between obtaining a short response time of the plasma and maximizing plasma density, both of which optimize with higher pressure; and obtaining a uniform plasma, which optimizes with lower pressure. These scalings motivate operation at intermediate pressures, tens of Torr to 100 Torr, which by pd scaling corresponds to sizes of the micro-cavity of hundreds of microns. In many cases, the inner surfaces of the microplasma cavities are largely dielectric due to ease of fabrication or to maximize lifetime. These conditions then motivate use of some form of bipolar excitation.In this paper, we discuss results from a computational investigation of scaling of microplasmas excited by pulsed dc-bipolar waveforms with the goal of maximizing the time averaged electron density. The computational platform is the Hybrid Plasma Equipment Model, a 2-dimensional hydrodynamics model in which radiation transport, and electron and ion distributions are addressed using Monte Carlo techniques. We investigated plasmas of 10s-100s Torr excited by short DC bipolar pulses (a few ns) with pulse repetition periods ranging from tens to hundreds of ns using mixtures of rare gases. Cavity sizes are a few hundred microns. Quasi-steady state, time averaged electron densities in excess of 1015 cm-3 in Penning mixtures are predicted. Although ionization by bulk electrons is the major source, the uniformity of the plasma is sensitive to ionization due to sheath accelerated secondary electrons. The behavior of the plasma was asymmetric with respect to the polarity of the voltage pulses, with more ionization occurring on the anodic portion of the cycle, in large part due to the electrically floating dielectric boundaries.
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