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Comparison of photo-EMF in cesium- and sodium-containing infinite slab cells one-sided irradiated by a resonance radiation. / Асташкевич, Сергей Анатольевич.

в: Journal of Quantitative Spectroscopy and Radiative Transfer, Том 361, 109985, 08.05.2026.

Результаты исследований: Научные публикации в периодических изданияхстатьяРецензирование

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@article{52af0f2ffa404e59a4e19be026aebc85,
title = "Comparison of photo-EMF in cesium- and sodium-containing infinite slab cells one-sided irradiated by a resonance radiation.",
abstract = "Our model study shows that a spatial non-homogeneous, in particular one-sided, irradiation of a cesium-containing cell can generate a photo-electromotive force (EMF), similar to the well-known Dember{\textquoteright}s effect in semiconductors. Data on the photo-EMF in an infinite slab cell with a width of L = 10^–2 m containing a pure cesium vapor and Cs–Ar mixtures were self-consistently determined at a gas temperature of Tg = 480 K. Cesium vapor pressure ranged from 0.007 to 0.11 torr, the argon to cesium vapor pressure ratio was from 0 to 103, and spectral flux density was F = 10?^2–3.7·10^3 W/(m2·nm) in a wavelength range of the D1 and D2 lines. A model for cesium photoplasma and an approach for determining the photo-EMF in the one-sided irradiated slab cell developed by us previously were used. An error was corrected in the formula for the electric potential in the plasma volume in the approach previously applied to the Na–Ar slab cell. Significant differences were found between data for the cesium- and sodium-containing cells for electron density and temperature and atomic and diatomic alkali ion densities. It was found that photo-EMF can be created in the cesium-containing cell at lower (by a factor of ten) alkali vapor pressure and resonance irradiation spectral flux density than in the sodium-containing cell. Non-monotonic dependencies of the potential change in the plasma volume, the potential drop near the cell walls, and, as a result, photo-EMF on gas component pressures and F were found and discussed. Maximum obtained photo-EMFs in the Cs–Ar and Na–Ar cells were about 0.65 V and 1 V, respectively. These results are of great interest for the application of alkali-containing gas plasmas, particularly in the development of photoelectric gas converters.",
keywords = "Radiation transfer, Electron density and temperature, Wall sheath, Electromotive force, Slab cell, Alkali vapor, Alkali vapor, Electromotive force, Electron density and temperature, Radiation transfer, Slab cell, Wall sheath",
author = "Асташкевич, {Сергей Анатольевич}",
year = "2026",
month = may,
day = "8",
doi = "10.1016/j.jqsrt.2026.109985",
language = "English",
volume = "361",
journal = "Journal of Quantitative Spectroscopy and Radiative Transfer",
issn = "0022-4073",
publisher = "Elsevier",

}

RIS

TY - JOUR

T1 - Comparison of photo-EMF in cesium- and sodium-containing infinite slab cells one-sided irradiated by a resonance radiation.

AU - Асташкевич, Сергей Анатольевич

PY - 2026/5/8

Y1 - 2026/5/8

N2 - Our model study shows that a spatial non-homogeneous, in particular one-sided, irradiation of a cesium-containing cell can generate a photo-electromotive force (EMF), similar to the well-known Dember’s effect in semiconductors. Data on the photo-EMF in an infinite slab cell with a width of L = 10^–2 m containing a pure cesium vapor and Cs–Ar mixtures were self-consistently determined at a gas temperature of Tg = 480 K. Cesium vapor pressure ranged from 0.007 to 0.11 torr, the argon to cesium vapor pressure ratio was from 0 to 103, and spectral flux density was F = 10?^2–3.7·10^3 W/(m2·nm) in a wavelength range of the D1 and D2 lines. A model for cesium photoplasma and an approach for determining the photo-EMF in the one-sided irradiated slab cell developed by us previously were used. An error was corrected in the formula for the electric potential in the plasma volume in the approach previously applied to the Na–Ar slab cell. Significant differences were found between data for the cesium- and sodium-containing cells for electron density and temperature and atomic and diatomic alkali ion densities. It was found that photo-EMF can be created in the cesium-containing cell at lower (by a factor of ten) alkali vapor pressure and resonance irradiation spectral flux density than in the sodium-containing cell. Non-monotonic dependencies of the potential change in the plasma volume, the potential drop near the cell walls, and, as a result, photo-EMF on gas component pressures and F were found and discussed. Maximum obtained photo-EMFs in the Cs–Ar and Na–Ar cells were about 0.65 V and 1 V, respectively. These results are of great interest for the application of alkali-containing gas plasmas, particularly in the development of photoelectric gas converters.

AB - Our model study shows that a spatial non-homogeneous, in particular one-sided, irradiation of a cesium-containing cell can generate a photo-electromotive force (EMF), similar to the well-known Dember’s effect in semiconductors. Data on the photo-EMF in an infinite slab cell with a width of L = 10^–2 m containing a pure cesium vapor and Cs–Ar mixtures were self-consistently determined at a gas temperature of Tg = 480 K. Cesium vapor pressure ranged from 0.007 to 0.11 torr, the argon to cesium vapor pressure ratio was from 0 to 103, and spectral flux density was F = 10?^2–3.7·10^3 W/(m2·nm) in a wavelength range of the D1 and D2 lines. A model for cesium photoplasma and an approach for determining the photo-EMF in the one-sided irradiated slab cell developed by us previously were used. An error was corrected in the formula for the electric potential in the plasma volume in the approach previously applied to the Na–Ar slab cell. Significant differences were found between data for the cesium- and sodium-containing cells for electron density and temperature and atomic and diatomic alkali ion densities. It was found that photo-EMF can be created in the cesium-containing cell at lower (by a factor of ten) alkali vapor pressure and resonance irradiation spectral flux density than in the sodium-containing cell. Non-monotonic dependencies of the potential change in the plasma volume, the potential drop near the cell walls, and, as a result, photo-EMF on gas component pressures and F were found and discussed. Maximum obtained photo-EMFs in the Cs–Ar and Na–Ar cells were about 0.65 V and 1 V, respectively. These results are of great interest for the application of alkali-containing gas plasmas, particularly in the development of photoelectric gas converters.

KW - Radiation transfer

KW - Electron density and temperature

KW - Wall sheath

KW - Electromotive force

KW - Slab cell

KW - Alkali vapor

KW - Alkali vapor

KW - Electromotive force

KW - Electron density and temperature

KW - Radiation transfer

KW - Slab cell

KW - Wall sheath

UR - https://www.mendeley.com/catalogue/f67228f4-1c42-365f-8eab-7bd3d4371527/

U2 - 10.1016/j.jqsrt.2026.109985

DO - 10.1016/j.jqsrt.2026.109985

M3 - Article

VL - 361

JO - Journal of Quantitative Spectroscopy and Radiative Transfer

JF - Journal of Quantitative Spectroscopy and Radiative Transfer

SN - 0022-4073

M1 - 109985

ER -

ID: 154088942