4.6 Article

Electron dynamics in radio frequency magnetron sputtering argon discharges with a dielectric target

期刊

出版社

IOP Publishing Ltd
DOI: 10.1088/1361-6595/abe9f9

关键词

radio frequency magnetron sputtering; electron dynamics; particle-in-cell; magnetized plasma; capacitively coupled plasmas; electron power absorption; moments of Boltzmann equation

资金

  1. National Science Foundation [1917577, 1724941, 1700787]
  2. Air Force Office of Scientific Research [FA9550-18-1-0062]
  3. U.S. Department of Energy Plasma Science Center [DE-SC0001939]
  4. Directorate For Engineering
  5. Div Of Civil, Mechanical, & Manufact Inn [1724941] Funding Source: National Science Foundation
  6. Directorate For Engineering
  7. Div Of Industrial Innovation & Partnersh [1917577] Funding Source: National Science Foundation

向作者/读者索取更多资源

An analysis of electron dynamics in RFMS argon discharge reveals that Ohmic power absorption is the dominant mechanism, while the contribution of secondary electrons to power absorption can be neglected under typical RFMS discharge conditions.
We demonstrate a self-consistent and complete description of electron dynamics in a typical electropositive radio frequency magnetron sputtering (RFMS) argon discharge with a dielectric target. The electron dynamics, including the electron power absorption dynamics in one radio frequency (RF) period, is studied via a fully kinetic 2d3v particle-in-cell/Monte Carlo collision (PIC/MCC) electrostatic simulation. The interplay between the fundamental plasma parameters is analyzed through their spatiotemporal dynamics. Due to the influence of magnetic trap on the electron transport, a spatially dependent charging that perturbs the electric potential is observed on the dielectric target surface, resulting in a spatially dependent ion energy distribution along the target surface. The ExB drift-to-discharge current ratio is in approximate agreement with Bohm diffusion. The electron power absorption can be primarily decoupled into the positive Ohmic power absorption in the bulk plasma region and the negative pressure-induced power absorption near the target surface. Ohmic power absorption is the dominant electron power absorption mechanism, mostly contributed by the azimuthal electron current. The power absorption due to electron inertial effects is negligible on time-average. Both the maximum power absorption and dissipation of electrons appear in the bulk plasma region during the second half of the RF period, implying a strong electron trapping in magnetron discharges. The contribution of secondary electrons is negligible under typical RFMS discharge conditions.

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