摘要
采用PIC-MC自洽模型,模拟了氮气电容性耦合射频放电的微观等离子体过程及带电粒子(e,N2+,N+)的行为。结果表明,离子(N2+,N+)的运动状态滞后瞬时射频电场的变化;在两极附近,N2+具较高密度,但能量较低,N+具较低的密度但能量较高,两者的密度差6倍左右。两种离子轰击射频电极的能量分布变化规律类似,随放电参数变化,离子(N2+,N+)能量变化显著,其密度变化不明显。模拟的电子能量几率分布与测量结果一致。
N2 capacitively coupled rf discharge was simulated by PIC/MCC model, in which we computed the rf electric field, the density and mean energy of charged particles (e, N2^+, N+), the energy distribution of ions (N2^+, N^+) bombarding rf electrode and their variation by following different discharge parameter (p, Vrf). The simulated results show that, ions (N2^+, N^+) seem to follow the electric field with a slight delay; the ions N^+ have higher energy near the two electrode, the ions N2^+ have higher density, and the N2^+ density is about six times of the N^+ density. With as the change of discharge parameter, the change of the energy of ions (N2^+, N^+) bombarding rf electrode is obvious, but the change of their density is slightly unconspicuous. The simulated results for electron energy probability distribution function are agreement with the measured results.
出处
《核聚变与等离子体物理》
CAS
CSCD
北大核心
2012年第3期206-212,共7页
Nuclear Fusion and Plasma Physics
基金
河北省自然科学基金资助项目(A2012205072)
河北师范大学自然基金(2010Y02)资助课题