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Plasma instabilities in electronegative inductive discharges.

机译:负电感应放电中的等离子体不稳定性。

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Plasma instabilities have been observed in low-pressure inductive discharges, in the transition between low density capacitive mode and high density inductive mode of the discharge when attaching gases such as SF6 and Ar/SF 6 mixtures are used. Oscillations of charged particles, plasma potential and light emitted from the plasma with the frequencies from a few hertz to tens of kilohertz are seen for gas pressures between 1 and 100 mTorr and the discharge power in the range of 75–1200 W. The region of instability increases as the plasma becomes more electronegative and the frequency of plasma oscillations increases as the power, pressure, and gas flow rate increase. The instability frequencies may also depend on the settings of a matching network.; A volume-averaged (global) model of the instability has been developed, for a discharge containing time varying densities of electrons, positive ions, and negative ions, and time invariant excited states and neutral densities. The particle and energy balance equations are integrated to produce the dynamical behavior. As pressure or power is varied to cross a threshold, the instability goes through a series of oscillatory states to large scale relaxation oscillations between higher and lower density states. The model qualitatively agrees with experimental observations, and also shows a significant influence of the matching network. A stability analysis of an electronegative discharge has been performed, using a Hurwitz criterion, for a system of linearized particle and power balance differential equations.; Capacitive coupling plays a crucial role in the instability process. A variable electrostatic (Faraday) shield has been used to control the capacitive coupling from the excitation coil to the plasma. The plasma instability disappears when the shielded area exceeds 65% of the total area of the coil. The global model of instability gives a slightly higher value of 85% for instability suppression with the same discharge conditions (Ar/SF6 1:1, 5 mTorr).; A quadrupole mass spectrometer has been used to measure the degree of dissociation and chemical composition of the SF6 and Ar/SF 6 plasmas. These measurements allowed improvements in the instability model, by identifying the most important ionic species.
机译:在低压感应放电中,当附着气体如SF 6 和Ar / SF 6时,在放电的低密度电容模式和高密度感应模式之间的过渡中观察到等离子体不稳定性混合物。在1至100 mTorr的气压和75-1200 W的放电功率范围内,可以看到带电粒子,等离子体电势和从等离子体发出的频率在几赫兹到几十千赫兹之间的振荡。随着等离子体变得更具负电性,不稳定性会增加,并且随着功率,压力和气体流速的增加,等离子体振荡的频率也会增加。不稳定性频率也可能取决于匹配网络的设置。对于包含电子,正离子和负离子随时间变化的密度以及随时间变化的激发态和中性密度的放电,已经开发了不稳定性的体积平均(全局)模型。粒子和能量平衡方程被积分以产生动力学行为。当压力或功率变化超过阈值时,不稳定性会经历一系列振荡状态,从而在较高和较低密度状态之间发生大规模的松弛振荡。该模型在质量上与实验观察一致,并且还显示了匹配网络的重要影响。已经使用Hurwitz准则对线性化粒子和功率平衡微分方程组进行了负电稳定性分析。电容耦合在不稳定过程中起着至关重要的作用。可变静电(法拉第)屏蔽已用于控制从激励线圈到等离子体的电容耦合。当屏蔽面积超过线圈总面积的65%时,等离子体不稳定性消失。全局失稳模型在相同的放电条件下(Ar / SF 6 1:1,5 mTorr)为抑制失稳提供了稍高的值,为85%。使用四极质谱仪测量SF 6 和Ar / SF 6 等离子体的解离度和化学成分。通过确定最重要的离子种类,这些测量可以改进不稳定性模型。

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