The ring-shaped spatial distribution of the argon excimer, $$\hbox {Ar}_2^{*}$$, in the effluent of the kINPen-sci

Spatially resolved measurements of the argon excimer, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>Ar</mml:mtext> <mml:mn>2</mml:mn> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> , were performed in the effluent of a cold atmospheric plasma jet (CAPJ), the so called kINPen-sci, using cavity ringdown spectroscopy. The spatial distribution of the density of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>Ar</mml:mtext> <mml:mrow><mml:mn>2</mml:mn></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> could be distinguished into two distinct populations: a Gaussian and a toroidally shaped distribution. The production mechanisms of these populations seem to differ. On the one hand, a strong correlation was found between the Gaussian <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>Ar</mml:mtext> <mml:mrow><mml:mn>2</mml:mn></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> population and the spatial distribution of the filaments produced in the effluent of the kINPen-sci. On the other hand, measurements performed while varying the experimental conditions under which the kINPen-sci was operated indicate that the gas flow velocity must play a major role in the formation of the toroidal <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>Ar</mml:mtext> <mml:mn>2</mml:mn> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> population. However, the mechanism of formation of the toroid <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>Ar</mml:mtext> <mml:mrow><mml:mn>2</mml:mn></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> population remains unclear.

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Journal
Scientific Reports
Published
2024-09-19
DOI
https://doi.org/10.1038/s41598-024-70966-7
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2
Primary Topic
Mass Spectrometry Techniques and Applications
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article
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article

The ring-shaped spatial distribution of the argon excimer, $$\hbox {Ar}_2^{*}$$, in the effluent of the kINPen-sci

J. H. van Helden, Philipp Mattern, A S C Nave
2 citations
Scientific Reports
Mass Spectrometry Techniques and Applications
0.48
article

The ring-shaped spatial distribution of the argon excimer, $$\hbox {Ar}_2^{*}$$, in the effluent of the kINPen-sci

J. H. van Helden, Philipp Mattern, A S C Nave
article en
2 citations

Abstract

Spatially resolved measurements of the argon excimer, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>Ar</mml:mtext> <mml:mn>2</mml:mn> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> , were performed in the effluent of a cold atmospheric plasma jet (CAPJ), the so called kINPen-sci, using cavity ringdown spectroscopy. The spatial distribution of the density of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>Ar</mml:mtext> <mml:mrow><mml:mn>2</mml:mn></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> could be distinguished into two distinct populations: a Gaussian and a toroidally shaped distribution. The production mechanisms of these populations seem to differ. On the one hand, a strong correlation was found between the Gaussian <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>Ar</mml:mtext> <mml:mrow><mml:mn>2</mml:mn></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> population and the spatial distribution of the filaments produced in the effluent of the kINPen-sci. On the other hand, measurements performed while varying the experimental conditions under which the kINPen-sci was operated indicate that the gas flow velocity must play a major role in the formation of the toroidal <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>Ar</mml:mtext> <mml:mn>2</mml:mn> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> population. However, the mechanism of formation of the toroid <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>Ar</mml:mtext> <mml:mrow><mml:mn>2</mml:mn></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> population remains unclear.

Scientific ReportsVol. 14(1)
Leibniz Institute for Plasma Science and Technology (DE), Silicon Austria Labs (Austria) (AT)
Clean water and sanitation
Openalex Percentile: Top 40%
Mass Spectrometry Techniques and Applications
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