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Influence of collisional broadening on resonance photoplasma parameters in a sodium-argon mixture. / Асташкевич, Сергей Анатольевич; Мандур, Мохамед Махсуб Махсуб Махсуб; Кудрявцев, Анатолий Анатольевич.

In: Journal of Quantitative Spectroscopy and Radiative Transfer, Vol. 288, No. Sept, 108256, 01.09.2022.

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Асташкевич, Сергей Анатольевич ; Мандур, Мохамед Махсуб Махсуб Махсуб ; Кудрявцев, Анатолий Анатольевич. / Influence of collisional broadening on resonance photoplasma parameters in a sodium-argon mixture. In: Journal of Quantitative Spectroscopy and Radiative Transfer. 2022 ; Vol. 288, No. Sept.

BibTeX

@article{b02c9b3f66b749f3bb6c9131e754bf4b,
title = "Influence of collisional broadening on resonance photoplasma parameters in a sodium-argon mixture",
abstract = "A study of photoplasma parameters in a Na–Ar mixture was carried out in a wide range of Ar pressures, considering the Voigt profile of the D1 and D2 resonance lines of Na in the Biberman-Holstein approximation. The effect of collisional broadening on the full width at half maximum (FWHM) of these lines is analyzed in detail, using the constants of the resonance (Na–Na collision) and van der Waals (Na–Ar collision) line shape broadening. 2D simulations of the main parameters (density of resonance (3p) levels of Na; electron density and temperature; photo-EMF) of the resonance photoplasma in a two-chamber cell at the Na pressure 0.02 Torr and Ar pressure 0.1-100 Torr have been carried out. It has been established that the difference between these parameters and previously obtained data for the case of the Doppler contour of the resonant line for the exact geometry of the gas cell and gas pressures is significant. Numerically, it reaches one-two orders of magnitude for the electron density and two times for the electron temperature. Also, a noticeable difference in the electron flux spatial picture in the cell for these two cases has been found. Therefore, it is shown that it is necessary to consider the collisional broadening of the resonance line of Na to determine plasma parameters even for relatively small pressures of Na and Ar. The developed approach and obtained data open up an opportunity to make a quantitative design of a photoelectric converter in a mixture of Na–Ar.",
keywords = "Photoplasma, Collision processes, Line broadening, Voigt profile, Photovoltaic effects, Simulation, Sodium, Collision processes, Line broadening, Photoplasma, Photovoltaic effects, Simulation, Sodium, Voigt profile",
author = "Асташкевич, {Сергей Анатольевич} and Мандур, {Мохамед Махсуб Махсуб Махсуб} and Кудрявцев, {Анатолий Анатольевич}",
year = "2022",
month = sep,
day = "1",
doi = "10.1016/j.jqsrt.2022.108256",
language = "English",
volume = "288",
journal = "Journal of Quantitative Spectroscopy and Radiative Transfer",
issn = "0022-4073",
publisher = "Elsevier",
number = "Sept",

}

RIS

TY - JOUR

T1 - Influence of collisional broadening on resonance photoplasma parameters in a sodium-argon mixture

AU - Асташкевич, Сергей Анатольевич

AU - Мандур, Мохамед Махсуб Махсуб Махсуб

AU - Кудрявцев, Анатолий Анатольевич

PY - 2022/9/1

Y1 - 2022/9/1

N2 - A study of photoplasma parameters in a Na–Ar mixture was carried out in a wide range of Ar pressures, considering the Voigt profile of the D1 and D2 resonance lines of Na in the Biberman-Holstein approximation. The effect of collisional broadening on the full width at half maximum (FWHM) of these lines is analyzed in detail, using the constants of the resonance (Na–Na collision) and van der Waals (Na–Ar collision) line shape broadening. 2D simulations of the main parameters (density of resonance (3p) levels of Na; electron density and temperature; photo-EMF) of the resonance photoplasma in a two-chamber cell at the Na pressure 0.02 Torr and Ar pressure 0.1-100 Torr have been carried out. It has been established that the difference between these parameters and previously obtained data for the case of the Doppler contour of the resonant line for the exact geometry of the gas cell and gas pressures is significant. Numerically, it reaches one-two orders of magnitude for the electron density and two times for the electron temperature. Also, a noticeable difference in the electron flux spatial picture in the cell for these two cases has been found. Therefore, it is shown that it is necessary to consider the collisional broadening of the resonance line of Na to determine plasma parameters even for relatively small pressures of Na and Ar. The developed approach and obtained data open up an opportunity to make a quantitative design of a photoelectric converter in a mixture of Na–Ar.

AB - A study of photoplasma parameters in a Na–Ar mixture was carried out in a wide range of Ar pressures, considering the Voigt profile of the D1 and D2 resonance lines of Na in the Biberman-Holstein approximation. The effect of collisional broadening on the full width at half maximum (FWHM) of these lines is analyzed in detail, using the constants of the resonance (Na–Na collision) and van der Waals (Na–Ar collision) line shape broadening. 2D simulations of the main parameters (density of resonance (3p) levels of Na; electron density and temperature; photo-EMF) of the resonance photoplasma in a two-chamber cell at the Na pressure 0.02 Torr and Ar pressure 0.1-100 Torr have been carried out. It has been established that the difference between these parameters and previously obtained data for the case of the Doppler contour of the resonant line for the exact geometry of the gas cell and gas pressures is significant. Numerically, it reaches one-two orders of magnitude for the electron density and two times for the electron temperature. Also, a noticeable difference in the electron flux spatial picture in the cell for these two cases has been found. Therefore, it is shown that it is necessary to consider the collisional broadening of the resonance line of Na to determine plasma parameters even for relatively small pressures of Na and Ar. The developed approach and obtained data open up an opportunity to make a quantitative design of a photoelectric converter in a mixture of Na–Ar.

KW - Photoplasma

KW - Collision processes

KW - Line broadening

KW - Voigt profile

KW - Photovoltaic effects

KW - Simulation

KW - Sodium

KW - Collision processes

KW - Line broadening

KW - Photoplasma

KW - Photovoltaic effects

KW - Simulation

KW - Sodium

KW - Voigt profile

UR - http://www.scopus.com/inward/record.url?scp=85130140010&partnerID=8YFLogxK

UR - https://www.mendeley.com/catalogue/5c84b297-847b-3fe9-82f7-ac0f5b9412c7/

U2 - 10.1016/j.jqsrt.2022.108256

DO - 10.1016/j.jqsrt.2022.108256

M3 - Article

VL - 288

JO - Journal of Quantitative Spectroscopy and Radiative Transfer

JF - Journal of Quantitative Spectroscopy and Radiative Transfer

SN - 0022-4073

IS - Sept

M1 - 108256

ER -

ID: 94857951