Spatially resolved measurements of electron density of a magnetically confined split-ring resonator source

Laser-collisional induced fluorescence is used to study the plasma generated by a split-ring resonator discharge under an external cusp shaped magnetic field created by permanent magnets. The electron density and electron temperature are measured for a helium plasma at different pressures, powers, and magnet field strengths. It is found that the magnetic fields produce higher electron temperatures with peak temperatures of ∼3 eV, while the no magnet case has peak temperatures of ∼0.8 eV. Conversely, the peak electron density is obtained in the no magnet case at a value of ∼1.9 × 1011 cm−3. This indicates that the cusp-field did magnetize the electrons, but contrary to expectations, it resulted in a decrease in electron density. This is believed to be due to the magnetic field having negative effects on the resonance of the plasma source.

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Publication Details

Journal
Physics of Plasmas
Published
2024-09-01
DOI
https://doi.org/10.1063/5.0215171
Citations
1
Primary Topic
Plasma Diagnostics and Applications
Type
article
Field-Weighted Citation Impact
0.21

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article

Spatially resolved measurements of electron density of a magnetically confined split-ring resonator source

Andrew T. Walsten, Kunning Gabriel Xu, Kevin Youngman, Brian Bentz
1 citations
Physics of Plasmas
Plasma Diagnostics and Applications
0.21
article

Spatially resolved measurements of electron density of a magnetically confined split-ring resonator source

Andrew T. Walsten, Kunning Gabriel Xu, Kevin Youngman, Brian Bentz
article en
1 citations

Abstract

Laser-collisional induced fluorescence is used to study the plasma generated by a split-ring resonator discharge under an external cusp shaped magnetic field created by permanent magnets. The electron density and electron temperature are measured for a helium plasma at different pressures, powers, and magnet field strengths. It is found that the magnetic fields produce higher electron temperatures with peak temperatures of ∼3 eV, while the no magnet case has peak temperatures of ∼0.8 eV. Conversely, the peak electron density is obtained in the no magnet case at a value of ∼1.9 × 1011 cm−3. This indicates that the cusp-field did magnetize the electrons, but contrary to expectations, it resulted in a decrease in electron density. This is believed to be due to the magnetic field having negative effects on the resonance of the plasma source.

Physics of PlasmasVol. 31(9)
Sandia National Laboratories (US), Optica (US), University of Alabama in Huntsville (US)
National Science Foundation, U.S. Department of Energy, Office of Science, National Nuclear Security Administration, Oak Ridge Institute for Science and Education, Fusion Energy Sciences, Workforce Development for Teachers and Scientists, Office of Experimental Program to Stimulate Competitive Research, Sandia National Laboratories
Affordable and clean energy
Openalex Percentile: Top 49%
Plasma Diagnostics and Applications
0.21
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