均匀磁场和会聚磁场中的射频线性等离子体装置的特性分析

Kazunori Takahashi, Yume Teranishi
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引用次数: 0

摘要

我们建造了一个线性射频等离子体装置,将一个频率为 13.56 MHz、最大功率为几千瓦的源连接到一个长约 1 米的圆柱形真空室上。源和真空室周围有七个螺线管,通过改变螺线管电流提供各种磁场配置。射频线性等离子体装置的等离子体密度最初以均匀和会聚磁场配置为特征。在这两种配置下,都能在源下游的腔室中观察到蓝模氩等离子体,这是螺旋放电或高密度放电所固有的,而天线附近的等离子体密度低于腔室中的等离子体密度。此外,收敛磁场配置的密度大于均匀配置的密度,最大密度约为 2×1019 m-3。离子饱和电流的时空测量结果表明,在放电初期,密度峰值在射频天线附近形成,随后在天线下游出现外围高密度区,这意味着一旦形成初始等离子体,射频功率就会与天线下游的电子有效耦合。开启射频功率几毫秒后,整个区域的密度降低,这似乎是由于中性耗竭造成的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Characterization of a radiofrequency linear plasma device in uniform and convergent magnetic fields
A linear radiofrequency plasma device is constructed, where a source operating at a frequency of 13.56 MHz and a maximum power of several kW is attached to a cylindrical vacuum chamber about 1 m in length. Seven solenoids are located around the source and the chamber, providing various magnetic field configurations by changing the solenoid currents. The plasma density of the radiofrequency linear plasma device is initially characterized in uniform and convergent magnetic field configurations. A blue mode argon plasma, being inherent to the helicon or high-density discharge, is observed in the chamber downstream of the source for both configurations, while the density near the antenna is lower than that in the chamber. Furthermore, the density for the convergent magnetic field configuration is found to be larger than that for the uniform case, providing a maximum density of about 2×1019m3 . Spatiotemporal measurements of the ion saturation current reveal that the density peak is formed near the rf antenna at the initial time of the discharge and the peripheral high-density region subsequently appears downstream of the antenna, implying that the rf power is efficiently coupled with the electrons downstream of the antenna once the initial plasma is created. A few ms after turning on the rf power, the density over the whole region reduces, which seems to be due to a neutral depletion.
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