4.6 Article

Dynamics of bipolar HiPIMS discharges by plasma potential probe measurements

Journal

PLASMA SOURCES SCIENCE & TECHNOLOGY
Volume 31, Issue 2, Pages -

Publisher

IOP Publishing Ltd
DOI: 10.1088/1361-6595/ac4b65

Keywords

high-power impulse magnetron sputtering; bipolar HiPIMS; plasma potential; ion acceleration

Funding

  1. Swedish Research Council [VR 2018-04139]
  2. Swedish Government Strategic Research Area in Materials Science on Functional Materials at Linkoping University (Faculty Grant SFOMat-LiU) [2009-00971]
  3. Eurostars program (IonDrive) [E!114277]
  4. Ministry of Education Youth and Sports of Czech Republic [LM2018097]
  5. Czech Science Foundation [GA19-00579S]
  6. National Natural Science Foundation of China [51805102, 52165021]

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The study explores the plasma potential variations during a bipolar HiPIMS discharge with a Cu target, aiming to identify conditions for achieving ion acceleration independent of substrate grounding. By analyzing the characteristics of plasma potential under different discharge conditions, including pressure, peak current, pulse length, and voltage amplitude, suitable conditions for ion acceleration in the target region were identified. Furthermore, a simple theory linking the plasma potential profile to the ratio of target electron current to ion saturation current at the chamber walls was described through investigation of target current and ion saturation current.
The plasma potential at a typical substrate position is studied during the positive pulse of a bipolar high-power impulse magnetron sputtering (bipolar HiPIMS) discharge with a Cu target. The goal of the study is to identify suitable conditions for achieving ion acceleration independent on substrate grounding. We find that the time-evolution of the plasma potential during the positive pulse can be separated into several distinct phases, which are highly dependent on the discharge conditions. This includes exploring the influence of the working gas pressure (0.3-2 Pa), HiPIMS peak current (10-70 A corresponding to 0.5-3.5 A cm(-2)), HiPIMS pulse length (5-60 mu s) and the amplitude of the positive voltage U (+) applied during the positive pulse (0-150 V). At low enough pressure, high enough HiPIMS peak current and long enough HiPIMS pulse length, the plasma potential at a typical substrate position is seen to be close to 0 V for a certain time interval (denoted phase B) during the positive pulse. At the same time, spatial mapping of the plasma potential inside the magnetic trap region revealed an elevated value of the plasma potential during phase B. These two plasma potential characteristics are identified as suitable for achieving ion acceleration in the target region. Moreover, by investigating the target current and ion saturation current at the chamber walls, we describe a simple theory linking the value of the plasma potential profile to the ratio of the available target electron current and ion saturation current at the wall.

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