Heating mode transitions in capacitively coupled CF4 plasmas at low pressure

Hui Wen, Julian Schulze, Quan-Zhi Zhang
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Abstract

Capacitively coupled plasmas operated in CF4 at low pressure are frequently used for dielectric plasma etching. For such applications the generation of different ion and neutral radical species by energy dependent electron impact ionization and dissociation of the neutral background gas is important. These processes are largely determined by the space and time dependent electron energy distribution function and, thus, by the electron power absorption dynamics. In this work and based on a particle-in-cell/Monte Carlo collision model, we show that the electron heating mode in such plasmas is sensitive to changes of the gap at a constant pressure of 3 Pa. At a gap of 1.5 cm, the dominant mode is found to be a hybrid combination of the Drift-Ambipolar (DA) and the α-mode. As the gap is increased to 2 cm and 2.5 cm, the bulk power absorption and ambipolar power absorption decreases, and the DA mode decays. When the gap reaches 3 cm, the α-mode becomes more prominent, and at a gap of 3.75 cm the α-mode is dominant. These mode transitions are caused by a change of the electronegativity and are found to affect the discharge characteristics. The presence of the DA-mode leads to significant positive electron power absorption inside the bulk region and negative power absorption within the sheaths on time average, as electrons are accelerated from the bulk towards the collapsed sheath. The heating mode transitions result in a change from negative to positive total electron power absorption within the sheaths as the gap increases. When accounting for secondary electron emission, the transition of the heating mode can occur at shorter gaps due to the enhanced plasma density and decreased electronegativity.
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低压下电容耦合 CF4 等离子体的加热模式转换
在 CF4 中低压运行的电容耦合等离子体经常用于电介质等离子体蚀刻。在此类应用中,与能量相关的电子撞击电离和中性背景气体解离产生不同的离子和中性自由基是非常重要的。这些过程在很大程度上取决于与空间和时间相关的电子能量分布函数,因此也取决于电子功率吸收动力学。在这项工作中,我们基于粒子池/蒙特卡洛碰撞模型,证明了在 3 Pa 的恒定压力下,此类等离子体中的电子加热模式对间隙的变化非常敏感。当间隙增大到 2 厘米和 2.5 厘米时,体功率吸收和伏极功率吸收减小,DA 模式衰减。当间隙达到 3 厘米时,α 模式变得更加突出,而当间隙达到 3.75 厘米时,α 模式占据主导地位。这些模式转换是由电负性的变化引起的,并会影响放电特性。DA 模式的存在会导致电子从主体向坍塌的鞘加速,从而在时间平均上在主体区域内产生显著的正电子功率吸收,而在鞘内产生负电子功率吸收。随着间隙的增大,加热模式转换导致鞘内的电子总功率吸收由负转正。当考虑到二次电子发射时,由于等离子体密度增大和电负性降低,加热模式的转变可能发生在更短的间隙处。
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