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CrNx Films Prepared by DC Magnetron Sputtering and High-Power Pulsed Magnetron Sputtering: A Comparative Study

机译:直流磁控溅射与大功率脉冲磁控溅射制备CrNx薄膜的比较研究

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摘要

CrNx (0 andlt;= x andlt;= 0.91) films synthesized using high-power pulsed magnetron sputtering, also known as high-power impulse magnetron sputtering (HiPIMS), have been compared with those made by conventional direct-current (dc) magnetron sputtering (DCMS) operated at the same average power. The HiPIMS deposition rate relative to the DCMS rate was found to decrease linearly with increasing emission strength from the Cr ions relative to Cr neutrals, in agreement with the predictions of the target-pathway model. The low deposition rate in HiPIMS is thus a direct consequence of the high ionization level (similar to 56%) of the target material and effective capturing of Cr ions by the cathode potential. Although the HiPIMS deposition rate did not exceed 40% of the DCMS rate, the drop in the relative deposition rate upon increasing the N-2-to-Ar flow ratio, f(N2/Ar), was found to be similar for both sputtering techniques. Films prepared by HiPIMS contained similar amounts of atomic nitrogen as the dc-sputtered samples grown at the same f(N2/Ar), indicating that the nitride formation at the substrate takes place mostly during the time period of the high-power pulses, and the N-2 uptake between the pulses is negligible. The microstructure evolution in the two types of CrNx films, however, differed clearly from each other. A combination of a high substrate bias and a high flux of doubly charged Cr ions present during the HiPIMS discharge led to a disruption of the grain growth and renucleation, which resulted in column-free films with nanosized grains not observed in the conventional DCMS-based process. The comparison of nanoindentation hardness as a function of f(N2/Ar) revealed superior properties of HiPIMS-sputtered films in the entire range of gas compositions.
机译:使用高功率脉冲磁控溅射(也称为大功率脉冲磁控溅射(HiPIMS))合成的CrNx(0 = x x = 0.91)薄膜已与传统的直流(dc)磁控管薄膜进行了比较。溅射(DCMS)以相同的平均功率运行。发现HiPIMS沉积速率相对于DCMS速率随Cr离子相对于Cr中性的发射强度的增加而线性降低,这与目标通道模型的预测一致。因此,HiPIMS中的低沉积速率是靶材料的高电离水平(约56%)和阴极电势有效捕获Cr离子的直接结果。尽管HiPIMS沉积速率未超过DCMS速率的40%,但发现两种溅射法在增加N-2-to-Ar流量比f(N2 / Ar)时相对沉积速率的下降是相似的技术。由HiPIMS制备的薄膜包含的原子氮量与在相同f(N2 / Ar)下生长的dc溅射样品的原子量相似,这表明衬底上的氮化物形成主要发生在高功率脉冲的时间段内,并且脉冲之间的N-2吸收可以忽略不计。然而,两种类型的CrNx薄膜的微观结构演变彼此之间明显不同。在HiPIMS放电过程中,高基材偏压和高流量的双电荷Cr离子的结合导致晶粒生长和成核的中断,这导致了无柱膜的纳米尺寸晶粒在传统的基于DCMS的系统中未观察到处理。纳米压痕硬度作为f(N2 / Ar)的函数的比较表明,在整个气体成分范围内,HiPIMS溅射膜的性能优越。

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