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PECVD by hollow cathodes

机译:空心阴极的PECVD

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摘要

Hollow cathodes produce about 2-3 order of magnitude higher plasma density as compared with the conventional electrode systemsat the s ame generation power. High ionization and gas activation efficiency in the hollow cathodes are reflected by very high rates of plasma processing, particularly in Plasma Enhanced CHemical Vapor Deposition (PECVD) of films. Growth rates of Si-N andf a-Si:H films up to even 100 #mu# m/min ewere observed in the PECVD by the radio frequency )RF) hollw cathode. At constant power the growth rate de-pends non-linearly on the mxing ratio of gases in the cathode. Both the mixing ratio and the dilution of the ractive gas in an intert carrier, as well as the type of the carrier gas, the gas flow rate, and the generator power are the parameters which affect distribution of ions and active radicals in the Highly Activated Near Afterglow (HANA) region around the substrate. Possibilities to optimize these parameters for selected PECVD of films are discussed.
机译:与传统电极系统垫相比,中空阴极产生约2-3级级较高的等离子体密度。 中空阴极中的高电离和气体活化效率通过非常高的等离子体处理来反映,特别是在膜的等离子体增强的化学气相沉积(PECVD)中。 Si-n Andf A-Si的生长速率:H射门在射频射频中观察到甚至100#mu#m / min Ewere的射频)rf)HOLLW阴极。 在恒定的功率下,生长速率在阴极中的气体的MXING比率上非线性地脱模。 混合比和载体中的载体稀释气体的稀释气体以及载气的类型,以及载气,气流速率和发电机功率是影响离子分布和高度激活的主动自由基的参数 靠近底部的余辉(HANA)区域。 讨论了优化这些参数的选定薄膜的选定PECVD的可能性。

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