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Controlled generation of pulse-modulated RF plasmas for materials processing

机译:用于材料加工的脉冲调制RF等离子体的受控生成

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Pulse-modulated radio frequency (RF) inductively coupled plasmas for materials processing applications were generated using a voltage-control-type power source, and the operating ranges for controlled generation were extended to sufficiently low shimmer power levels. When the plasma was generated at atmospheric pressure and a high power level of 17 kW, the low power level typically went down to about 4 kW for an Ar-H-2 plasma and 3 kW for an Ar-N-2 plasma, levels too low to sustain the continuous plasmas. The overshoot and undershoot at the beginnings of power change were reduced considerably by using an exponential voltage control signal. Spectroscopic measurements of the radiation intensity of the Ar atomic spectral line (751.5 nm) showed that the plasma temperatures varied with time and that the characteristic times of the plasmas depended on the operating conditions and the position in the plasma generator. The characteristic times in the discharge zone may be largely determined by the competition among ionization, recombination and convection in the pulsed plasmas. The characteristic times estimated using an electron transportation model are reasonably in line with those determined from measured emission intensities. The difference between the plasma properties at the higher and lower power levels was large enough to give rise to the nonequilibrium states at the instances of pulse-on and pulse-off, and to the increase in the concentration of chemically active radical species. This offers a unique physico-chemical condition for materials processing. The ranges of controlled generation were determined for the Ar-H-2 and Ar-N-2 plasmas at pressures from 27 to 101 kPa.
机译:使用电压控制型电源生成了用于材料加工应用的脉冲调制射频(RF)感应耦合等离子体,并将用于受控生成的工作范围扩展到足够低的微光功率水平。当在大气压力和17 kW的高功率水平下生成等离子体时,对于Ar-H-2等离子体,低功率水平通常下降至约4 kW,对于Ar-N-2等离子体,低功率水平通常降至3 kW,低以维持连续的等离子体。通过使用指数电压控制信号,可以大大减少功率变化开始时的过冲和下冲。 Ar原子光谱线(751.5 nm)的辐射强度的光谱测量表明,等离子体温度随时间变化,并且等离子体的特征时间取决于操作条件和等离子体发生器中的位置。放电区中的特征时间很大程度上取决于脉冲等离子体中电离,复合和对流之间的竞争。使用电子传输模型估算的特征时间与根据测得的发射强度确定的特征时间基本一致。在较高和较低功率水平下,等离子体特性之间的差异足够大,足以在脉冲接通和脉冲断开时引起非平衡态,并增加化学活性自由基的浓度。这为材料加工提供了独特的物理化学条件。在27至101 kPa的压力下,确定了Ar-H-2和Ar-N-2等离子体的受控生成范围。

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