Investigating different carbon-based target materials: Can we improve ionization in HiPIMS for the deposition of diamondlike carbon films?

M. Fenker, Martin Balzer, Holger Kaßner
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Abstract

Diamondlike carbon (DLC) thin films have attracted growing interest due to their extraordinary properties, which occur if the fraction of sp3 C-bonds in the amorphous carbon films is high. This high fraction of sp3 C-bonds requires a high ionization rate of the sputtered carbon and a high kinetic energy of the carbon species. The first part of this article provides a detailed overview of the possibilities to increase the ionized fraction of the sputtered carbon and a brief description of the DLC growth models. The overview will include previously unpublished calculations by our group that include the ionization rate of carbon compared to some metals, the mean ionization path length of carbon, and the carbon ion flux at the substrate. In addition, the problem of simultaneous deposition of sp2- and sp3-bonded carbon during a HiPIMS pulse is explained for the first time. In the second part, we will present the influence of different carbon-based target materials on ionization, arcing, and deposition rates. Therefore, three different carbon-based target materials were investigated for high-power impulse magnetron sputtering (HiPIMS) depositions of a-C films: (a) graphite target, (b) fine-grained graphite target, and (c) glassy carbon target. The acquired data were compared to dc magnetron sputtering (dcMS). For HiPIMS, the pulse parameters and the total argon gas pressure were varied. The deposition process was characterized by the acquisition of the target currents and voltages, the arcing rate, optical emission spectroscopy (OES), and monitoring the deposition rate using a quartz crystal microbalance. The studies revealed that with HiPIMS, arcing was increased strongly with the peak current density for the graphite target. With the glassy carbon target, arcing was low at the beginning but increased with the duration of the tests. This target had a polished surface in the as-delivered state, which became rougher during sputtering. Similar deposition rates have been measured for dcMS and HiPIMS. With OES, only a low ionization of carbon was identified. The deposition of a-C coatings produced films with a low hardness of about 1200 HV (about 12 GPa) for both sputtering methods (dcMS and HiPIMS), as no substrate bias was applied. It can be concluded that arcing was lowest with the glassy carbon target and that the ionization rate was not significantly influenced by the change in the target material.
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研究不同的碳基目标材料:我们能否改进 HiPIMS 中的电离,以沉积类金刚石碳薄膜?
如果无定形碳薄膜中 sp3 C 键的比例较高,就会产生非凡的特性,因此类金刚石碳(DLC)薄膜越来越受到人们的关注。这种高比例的 sp3 C 键需要溅射碳的高电离率和碳物种的高动能。本文第一部分详细概述了提高溅射碳电离部分的可能性,并简要介绍了 DLC 生长模型。概述将包括我们小组之前未发表的计算结果,其中包括与某些金属相比碳的电离率、碳的平均电离路径长度以及基底的碳离子通量。此外,我们还首次解释了在 HiPIMS 脉冲期间同时沉积 sp2 和 sp3 键碳的问题。在第二部分,我们将介绍不同碳基靶材料对电离、电弧和沉积速率的影响。因此,我们研究了用于高功率脉冲磁控溅射(HiPIMS)沉积 a-C 薄膜的三种不同碳基靶材:(a) 石墨靶材、(b) 细粒度石墨靶材和 (c) 玻璃碳靶材。获得的数据与直流磁控溅射(dcMS)进行了比较。对于 HiPIMS,改变了脉冲参数和氩气总压。通过采集靶电流和电压、电弧速率、光学发射光谱(OES)以及使用石英晶体微天平监测沉积速率,对沉积过程进行了表征。研究表明,使用 HiPIMS 时,石墨靶的电弧随峰值电流密度的增加而剧增。对于玻璃碳靶材,起初电弧较低,但随着测试时间的延长,电弧逐渐增加。这种靶材在交货时表面抛光,在溅射过程中变得更加粗糙。dcMS 和 HiPIMS 也测得了类似的沉积率。通过 OES,只发现碳的电离程度较低。在两种溅射方法(dcMS 和 HiPIMS)中,由于没有施加基底偏压,a-C 涂层沉积产生的薄膜硬度较低,约为 1200 HV(约 12 GPa)。可以得出的结论是,玻璃碳靶材的电弧最低,电离率不受靶材变化的显著影响。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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