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Ion Energy and Plasma Potential Measurements in HIPIMS Discharges

机译:HIPIMS放电中的离子能量和等离子体潜在测量

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Using a fast electrostatic gating technique the ion energy distribution functions (IEDF's) at the substrate in a High Power Impulse Magnetron Sputtering (HIPIMS) discharge have been determined with a 2μs time-resolution. The discharge was operated with a repetition rate of 100Hz, a pulse width of 100μs, a pressure of 0.26Pa and a peak power density of 2.5kW cm~(-2). The results show that Ar~+ ions appear 8μs after initiation of the discharge voltage pulse and have a narrow distribution of energies, consistent with being created locally to the substrate; as seen by plasma potential measurements. The time-evolution of the plasma potential (1μs time-resolution) was obtained using a Langmuir probe close to the mass spectrometer extraction orifice. In contrast to the Ar~+ ions, sputtered post-ionised atoms in the form of Ti~+ ions were detected 14μs after the pulse initiation, showing a distinct high-energy tail extending up to about 100eV. The form of the IEDF's for these ions is believed to be determined by both the energy distribution of the sputtered atoms from the target and the space potential in the bulk plasma at which they were ionized.
机译:使用快速静电选通技术,在高功率脉冲磁控管溅射(HIPIMS)放电中的基板处的离子能量分布功能(IEDF)已经用2μs的时间分辨来确定。排出的重复率为100Hz,脉冲宽度为100μs,压力为0.26A,峰值功率密度为2.5kw cm〜(-2)。结果表明,在引发放电电压脉冲后,Ar〜+离子出现了8μs,并且具有窄的能量分布,与局部地在基板上产生一致;如等离子体潜在测量所见。使用靠近质谱仪提取孔口的Langmuir探针获得等离子体电位(1μs时间分辨率)的时间 - 进化。与Ar〜+离子相比,在脉冲开始后14μs检测Ti〜+离子形式的溅射后的原子,显示出直至约100ev的不同高能量尾。所述IEDF的形式是为这些离子被认为是由从靶溅射原子两者的能量分布,并在它们被离子化的等离子体中的空间电势来确定。

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