On the population density of the argon excited levels in a high power impulse magnetron sputtering discharge

被引:1
作者
Rudolph, M. [1 ]
Revel, A. [2 ]
Lundin, D. [2 ,3 ]
Brenning, N. [3 ,4 ]
Raadu, M. A. [4 ]
Anders, A. [1 ,5 ]
Minea, T. M. [2 ]
Gudmundsson, J. T. [4 ,6 ]
机构
[1] Leibniz Inst Surface Engn IOM, Permoserstr 15, D-04318 Leipzig, Germany
[2] Univ Paris Saclay, Lab Phys Gaz Plasmas LPGP, UMR 8578, CNRS, F-91405 Orsay, France
[3] Linkoping Univ, IFM Mat Phys, Plasma & Coatings Phys Div, SE-58183 Linkoping, Sweden
[4] KTH Royal Inst Technol, Sch Elect Engn & Comp Sci, Space & Plasma Phys, SE-10044 Stockholm, Sweden
[5] Univ Leipzig, Felix Bloch Inst Solid State Phys, Linnestr 5, D-04103 Leipzig, Germany
[6] Univ Iceland, Sci Inst, IS-S107 Reykjavik, Iceland
基金
瑞典研究理事会;
关键词
COLLISIONAL-RADIATIVE MODEL; ENERGY ELECTRON-DISTRIBUTION; BEAM-PRODUCED PLASMAS; ATOM-ATOM COLLISIONS; RESONANCE RADIATION; WIDE-RANGE; IONIZATION; RECOMBINATION; IMPRISONMENT; EXCITATION;
D O I
10.1063/5.0071887
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
Population densities of excited states of argon atoms in a high power impulse magnetron sputtering (HiPIMS) discharge are examined using a global discharge model and a collisional-radiative model. Here, the ionization region model (IRM) and the Orsay Boltzmann equation for electrons coupled with ionization and excited states kinetics (OBELIX) model are combined to obtain the population densities of the excited levels of the argon atom in a HiPIMS discharge. The IRM is a global plasma chemistry model based on particle and energy conservation of HiPIMS discharges. OBELIX is a collisional-radiative model where the electron energy distribution is calculated self-consistently from an isotropic Boltzmann equation. The collisional model constitutes 65 individual and effective excited levels of the argon atom. We demonstrate that the reduced population density of high-lying excited argon states scales with (p*)(-6), where p * is the effective quantum number, indicating the presence of a multistep ladder-like excitation scheme, also called an excitation saturation. The reason for this is the dominance of electron impact processes in the population and de-population of high-lying argon states in combination with a negligible electron-ion recombination. (C) 2022 Author(s). All article content, except where otherwise noted, is licensed under a Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).
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页数:12
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