Effects of cavity resonance and antenna resonance on mode transitions in helicon plasma

Tianliang Zhang, Ying Cui, Zhangyu Xia, Bocong Zheng, Feng He, J. Ouyang
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Abstract

Mechanisms of cavity resonance and antenna resonance and their coupling effect on mode transition in argon helicon plasma excited by a half-helical antenna (14 cm in length) were investigated in this paper. Cavity length was changed to distinguish the effects of cavity and antenna resonances. Plasma parameters in various conditions such as input power (0-2500 W), magnetic field (0-1000 G) and cavity length (10-42 cm) were measured. Characteristics of helicon discharges and mode transitions in cases of fixed and continuously changed cavity lengths were compared. The results show that multiple axial eigenmodes (at least five in the present work) were observed in both cases. In fixed-length cavity, helicon discharge changes abruptly during mode transitions, while in changeable-length cavity, discharge features can change continuously (e.g. in large range of density from 1.7×1012 to 1.3×1013 cm-3) without mode transition. Mode transitions also occur as the cavity length increasing at fixed input power and magnetic field with periodical variations of plasma parameters. Cavity resonance plays a dominant role in formation of standing helicon wave of eigenmodes and mode transition, while antenna resonance affects significantly the transition from inductively coupled mode to helicon wave mode. Enhanced inter-coupling of cavity resonance and antenna resonance appears at specific axial wavelengths of eigenmodes. Threshold conditions for mode transitions were deduced and the overall transition path and the corresponding density were predicted quantitatively, which shows that cavity resonance determines the transition path, while antenna resonance gives the lower limit of the path. Axial wavenumber is closely related to the helicon discharge characteristics. Cavity and antenna resonances influence the helicon discharge and mode transition by determining the axial wavenumber of eigenmodes.
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空腔共振和天线共振对螺旋子等离子体模式转换的影响
本文研究了由半螺旋天线(长 14 厘米)激发的氩氦等离子体中空腔共振和天线共振的机制及其对模式转换的耦合效应。为了区分空腔共振和天线共振的影响,改变了空腔长度。测量了输入功率(0-2500 W)、磁场(0-1000 G)和空腔长度(10-42 cm)等不同条件下的等离子体参数。比较了固定腔长和连续变化腔长情况下的螺旋子放电和模式转换特征。结果表明,在这两种情况下都观察到了多个轴向特征模(在本研究中至少有五个)。在固定长度的空腔中,螺旋子放电在模式转换时会突然发生变化,而在可变长度的空腔中,放电特征可以连续变化(例如在 1.7×1012 至 1.3×1013 cm-3 的大密度范围内),而不会发生模式转换。在固定输入功率和磁场条件下,随着等离子体参数的周期性变化,空腔长度增加,也会发生模式转换。空腔共振在形成驻留螺旋波特征模式和模式转换中起主导作用,而天线共振则对从电感耦合模式到螺旋波模式的转换产生重大影响。在特征模的特定轴向波长处,空腔共振和天线共振的相互耦合增强。推导出了模式转换的阈值条件,并定量预测了整体转换路径和相应密度,这表明空腔共振决定了转换路径,而天线共振给出了路径的下限。轴向波数与螺旋子放电特性密切相关。腔共振和天线共振通过决定特征模的轴向波数来影响螺旋子放电和模式转换。
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