Enhancing He 2 <sup>3</sup>S<sub>1</sub> state production in the burst regime of a nanosecond discharge

Abstract Atmospheric repetitive He discharge with 10 ns current peak width working in the burst pulse regime was studied. The production of He 3 S 1 and 1 S 0 metastable states was examined using laser- collisions- induced fluorescence and atomic absorption spectroscopy. Both methods independently reveal a significant increase of 3 S 1 population in the burst regime, depending on the plasma pulse separation time in the burst. Up to a seven-fold increase in the 3 S 1 population was detected after the third pulse in a 3-pulse burst sequence (as compared to the value obtained after the first pulse or in a single pulse regime), not requiring additional applied power. The observed effect is explained by recombination between the electrons and the ground state ions (He + , He <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msubsup> <mml:mrow/> <mml:mn>2</mml:mn> <mml:mo>+</mml:mo> </mml:msubsup> </mml:mrow> </mml:math> ) produced in the previous plasma pulse and refilling the volume of interest in few hundred µ s.

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Publication Details

Journal
Plasma Sources Science and Technology
Published
2024-12-06
DOI
https://doi.org/10.1088/1361-6595/ad9b4d
Citations
1
Primary Topic
Plasma Applications and Diagnostics
Type
article
Field-Weighted Citation Impact
0.40

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article

Enhancing He 2 3S1 state production in the burst regime of a nanosecond discharge

Nikolay Britun, Masaru Hori
1 citations
Plasma Sources Science and Technology
Plasma Applications and Diagnostics
0.40
article

Enhancing He 2 3S1 state production in the burst regime of a nanosecond discharge

Nikolay Britun, Masaru Hori
article en
1 citations

Abstract

Abstract Atmospheric repetitive He discharge with 10 ns current peak width working in the burst pulse regime was studied. The production of He 3 S 1 and 1 S 0 metastable states was examined using laser- collisions- induced fluorescence and atomic absorption spectroscopy. Both methods independently reveal a significant increase of 3 S 1 population in the burst regime, depending on the plasma pulse separation time in the burst. Up to a seven-fold increase in the 3 S 1 population was detected after the third pulse in a 3-pulse burst sequence (as compared to the value obtained after the first pulse or in a single pulse regime), not requiring additional applied power. The observed effect is explained by recombination between the electrons and the ground state ions (He + , He <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msubsup> <mml:mrow/> <mml:mn>2</mml:mn> <mml:mo>+</mml:mo> </mml:msubsup> </mml:mrow> </mml:math> ) produced in the previous plasma pulse and refilling the volume of interest in few hundred µ s.

Plasma Sources Science and TechnologyVol. 34(1)
Nagoya University (JP)
Japan Society for the Promotion of Science
Openalex Percentile: Top 32%
Plasma Applications and Diagnostics
0.40
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