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Investigation of effect of excitation frequency on electron energy distribution functions in low pressure radio frequency bounded plasmas

机译:激发频率对低压射频有界等离子体中电子能量分布函数的影响

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Particle in cell (PIC) simulations are employed to investigate the effect of excitation frequency on electron energy distribution functions (EEDFs) in a low pressure radio frequency (rf) discharge. The discharge is maintained over a length of 0.10 m, bounded by two infinite parallel plates, with the coherent heating field localized at the center of the discharge over a distance of 0.05 m and applied perpendicularly along the y and z directions. On varying the excitation frequency f (=ω/2) in the range 0.01-50 MHz, it is observed that for f ≤ 5 MHz the EEDF shows a trend toward a convex (Druyvesteyn-like) distribution. For f > 5 MHz, the distribution resembles more like a Maxwellian with the familiar break energy visible in most of the distributions. A prominent hot tail is observed at f ≥ 20 MHz and the temperature of the tail is seen to decrease with further increase in frequency (e.g., at 30 MHz and 50 MHz). The mechanism for the generation of the hot tail is considered to be due to preferential transit time heating of energetic electrons as a function of ω, in the antenna heating field. There exists an optimum frequency for which high energy electrons are maximally heated. The occurrence of the Druyvesteyn-like distributions at lower ω may be explained by a balance between the heating of the electrons in the effective electric field and elastic cooling due to electron neutral collision frequency ν_(en); the transition being dictated by ω ~ 2πν_(en).
机译:单元中粒子(PIC)模拟用于研究低压射频(rf)放电中激发频率对电子能量分布函数(EEDF)的影响。放电保持在0.10 m的长度上,由两个无限的平行板界定,相干的加热场位于放电中心,距离为0.05 m,并沿y和z方向垂直施加。在0.01-50 MHz范围内改变激励频率f(=ω/ 2)时,可以观察到,对于f≤5 MHz,EEDF呈现出趋向于凸形(类似于Druyvesteyn)分布的趋势。对于f> 5 MHz,分布更像是麦克斯韦,具有在大多数分布中可见的熟悉的断裂能。在f≥20 MHz处观察到明显的热尾巴,并且尾巴的温度随着频率的进一步升高而降低(例如在30 MHz和50 MHz处)。产生热尾的机理被认为是由于天线加热场中高能电子的优先渡越时间加热,它是ω的函数。有一个最佳频率,高能电子为此被最大程度地加热。可以通过有效电场中电子的加热与由于电子中性碰撞频率ν_(en)引起的弹性冷却之间的平衡来解释在较低的ω处出现Druyvesteyn状分布的现象。跃迁由ω〜2πν_(en)决定。

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