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Effect of Radio-Frequency Electric Power Applied to a Boron Nitride Unbalanced Magnetron Sputter Target on the Deposition of Cubic Boron Nitride Thin Film

机译:氮化硼不平衡磁控溅射靶上施加的射频功率对立方氮化硼薄膜沉积的影响

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摘要

Cubic boron nitride (c-BN) films were deposited by an unbalanced magnetron sputtering method. A (100) Si wafer with a nanocrystalline diamond thin film as a surface coating layer or that without it was used as a substrate. The target power was varied from 100 to 400 W. A boron nitride target was used, which was connected to a radio frequency power supply. High frequency power connected to a substrate holder was used for self-biasing. The deposition pressure was 0.27 MPa with a flow of Ar (18 sccm) - N_2 (2 sccm) mixed gas. The existence of threshold bias voltages for c-BN formation and rcsputtering were observed irrespective of target power. The bias voltage window for c-BN formation broadened with increased target power. The deposition rate decreased with enhanced bias voltage and decreased target power. Residual stresses of the films did not vary noticeably with target power within the target power range of c-BN formation. A parameter space for c-BN formation according to the target power and the bias voltage, as two variables, was suggested.
机译:通过不平衡磁控溅射方法沉积立方氮化硼(c-BN)膜。将具有纳米晶金刚石薄膜作为表面涂层或没有纳米晶金刚石薄膜的(100)Si晶片用作衬底。目标功率从100到400 W不等。使用了氮化硼靶,该靶连接到射频电源上。连接到基板支架的高频电源用于自偏置。在Ar(18sccm)-N_2(2sccm)混合气体的流动下,沉积压力为0.27MPa。无论目标功率如何,观察到存在用于c-BN形成和rc溅射的阈值偏置电压。用于c-BN形成的偏置电压窗口随着目标功率的增加而扩大。沉积速率随着偏置电压的增加和目标功率的降低而降低。在c-BN形成的目标功率范围内,膜的残余应力不会随目标功率而显着变化。提出了根据目标功率和偏置电压作为两个变量的c-BN形成的参数空间。

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