自定义电压波形驱动氩气和CF4电容放电的电子功率吸收动力学和离子能量分布

B. Berger, S. Brandt, J. Franek, E. Schuengel, M. Koepke, J. Schulze, T. Mussenbrock, B. Bruneau, E. Johnson, T. Lafleur, J. Booth, D. O’Connell, T. Gans, I. Korolov, A. Derzsi, Z. Donkó
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引用次数: 0

摘要

只提供摘要形式。通过实验和PIC模拟研究了Ar和CF4中定制电压波形驱动的电容耦合射频放电的时空电子冲击激发动力学。在实验中,基于一种新颖的射频供电系统,在3pa到200pa的压力下,放电由多达三个连续的13.56 MHz谐波驱动,谐波的幅度和相位可单独调节。采用相位分辨发射光谱法研究了固定总电压幅值下不同形状的驱动电压波形(峰/谷/锯齿)的激发动力学。测量了电极处的直流自偏置和离子能量分布函数。iedf的形成是基于确定护套电压波形的模型来理解的。结果表明,可以通过调整谐波的相位来控制离子的平均能量和激发动态。在CF4中,与高压下的Ar相比,观察到强烈不同的激发动力学,并且根据模拟结果可以理解。对于特定的驱动电压波形,等离子体在空间上被分为电负性强烈不同的两个不同的部分。这种不对称可以通过反转驱动波形来扭转。对于锯齿形波形,由于电子加热模式从α-到漂移-双极加热模式的转变,放电不对称性和直流自偏置的符号随着压力的增加而逆转。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Electron power absorption dynamics and ion energy distributions in capacitive discharges driven by customized voltage waveforms in argon and CF4
Summary form only given. The spatio-temporal electron impact excitation dynamics in a capacitively coupled RF discharge driven by tailored voltage waveforms in Ar and CF4 are investigated experimentally and by PIC simulations. In the experiment, the discharge is driven by up to three consecutive harmonics of 13.56 MHz with individually adjustable harmonics' amplitudes and phases based on a novel RF supply system at pressures between 3 Pa and 200 Pa. The excitation dynamics are investigated by Phase-Resolved Optical Emission Spectroscopy for different shapes of the driving voltage waveform (peaks/valleys/ sawtooth) at fixed total voltage amplitudes. The DC self bias and the ion energy distribution function (IEDF) at the electrodes are also measured. The formation of the IEDFs is understood based on a model that determines sheath voltage waveforms. It is demonstrated that the mean ion energy and the excitation dynamic can be controlled by adjusting the harmonics' phases. In CF4, strongly different excitation dynamics are observed compared to Ar at high pressures and are understood based on the simulation results. The plasma is divided spatially into two different halves of strongly different electronegativity for specific driving voltage waveforms. This asymmetry can be reversed by inverting the driving waveform. For Sawtooth waveforms, the discharge asymmetry and the sign of the DC self bias are found to reverse as the pressure is increased, due to a transition of the electron heating mode from the α-to the Drift-Ambipolar heating mode.
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