Determination of Plasma Current on the Electrode Biased a High Negative Potential

H. Hwang, Jae-Myeong Choe, Kyung-Jae Jung, Kwang-Chul Ko, Y. Hwang, Gon-Ho Kim
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Abstract

In the case of highly negative biased target immersed in the plasma, the current on the target is composed of the incident ion current and the emission electron current. The virtual area of collecting current on the target is proportional to the sheath area formed over the target electrode which is considerable increased with applied high bias. The spatially distributed plasma also affects on the sheath formation, resulting in the target current. Consideration of the dimensional sheath formation and spatial plasma distribution with the secondary electron emission coefficient is conducted for analyzing the target current. Experiments were carried out with the planar stainless steel and aluminum targets having a diameter 100mm, negatively bias ranging in 2kV~11kV. Sheath size and spatial plasma distributions are measured by electrical probes. The current model including the dimensional sheath, spatial plasma distribution and secondary electron emission coefficient will be presented
高负电位偏置电极上等离子体电流的测定
当高负偏靶浸入等离子体中时,靶上的电流由入射离子电流和发射电子电流组成。目标上收集电流的虚拟面积与目标电极上形成的护套面积成正比,该护套面积随着施加高偏压而大大增加。空间分布的等离子体也影响鞘层的形成,从而产生目标电流。在分析目标电流时,考虑了尺寸鞘层形成和空间等离子体分布与二次电子发射系数的关系。实验采用直径为100mm,负偏压在2kV~11kV范围内的平面不锈钢和铝靶。电探针测量鞘层尺寸和空间等离子体分布。目前的模型包括尺寸鞘层、空间等离子体分布和二次电子发射系数
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