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Crosstalk-Free Excitation Scheme for Quantitative OH Laser-Induced Fluorescence in Environments Containing Excited CO

Spectral overlap in the single-photon laser-induced fluorescence between the 3064 Å system of OH and the third positive system of CO is detected in a highly-excited environment, namely, a CO(2)-H(2)O plasma. The overlap is distorting excitation and fluorescence spectra as well as fluorescence time d...

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Autores principales: Budde, Maik, Engeln, Richard
Formato: Online Artículo Texto
Lenguaje:English
Publicado: SAGE Publications 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9289968/
https://www.ncbi.nlm.nih.gov/pubmed/35311380
http://dx.doi.org/10.1177/00037028221088591
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author Budde, Maik
Engeln, Richard
author_facet Budde, Maik
Engeln, Richard
author_sort Budde, Maik
collection PubMed
description Spectral overlap in the single-photon laser-induced fluorescence between the 3064 Å system of OH and the third positive system of CO is detected in a highly-excited environment, namely, a CO(2)-H(2)O plasma. The overlap is distorting excitation and fluorescence spectra as well as fluorescence time decays of commonly used excitation transitions of OH. As a consequence, systematic errors are introduced into the determination of temperatures, gas compositions, and absolute number densities. The P(1)(2) transition is proposed to circumvent the distortion while still allowing for quantitative measurements due to the availability of non-radiative rate coefficients.
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spelling pubmed-92899682022-07-19 Crosstalk-Free Excitation Scheme for Quantitative OH Laser-Induced Fluorescence in Environments Containing Excited CO Budde, Maik Engeln, Richard Appl Spectrosc Rapid Communication Spectral overlap in the single-photon laser-induced fluorescence between the 3064 Å system of OH and the third positive system of CO is detected in a highly-excited environment, namely, a CO(2)-H(2)O plasma. The overlap is distorting excitation and fluorescence spectra as well as fluorescence time decays of commonly used excitation transitions of OH. As a consequence, systematic errors are introduced into the determination of temperatures, gas compositions, and absolute number densities. The P(1)(2) transition is proposed to circumvent the distortion while still allowing for quantitative measurements due to the availability of non-radiative rate coefficients. SAGE Publications 2022-04-25 2022-07 /pmc/articles/PMC9289968/ /pubmed/35311380 http://dx.doi.org/10.1177/00037028221088591 Text en © The Author(s) 2022 https://creativecommons.org/licenses/by/4.0/This article is distributed under the terms of the Creative Commons Attribution 4.0 License (https://creativecommons.org/licenses/by/4.0/) which permits any use, reproduction and distribution of the work without further permission provided the original work is attributed as specified on the SAGE and Open Access page (https://us.sagepub.com/en-us/nam/open-access-at-sage).
spellingShingle Rapid Communication
Budde, Maik
Engeln, Richard
Crosstalk-Free Excitation Scheme for Quantitative OH Laser-Induced Fluorescence in Environments Containing Excited CO
title Crosstalk-Free Excitation Scheme for Quantitative OH Laser-Induced Fluorescence in Environments Containing Excited CO
title_full Crosstalk-Free Excitation Scheme for Quantitative OH Laser-Induced Fluorescence in Environments Containing Excited CO
title_fullStr Crosstalk-Free Excitation Scheme for Quantitative OH Laser-Induced Fluorescence in Environments Containing Excited CO
title_full_unstemmed Crosstalk-Free Excitation Scheme for Quantitative OH Laser-Induced Fluorescence in Environments Containing Excited CO
title_short Crosstalk-Free Excitation Scheme for Quantitative OH Laser-Induced Fluorescence in Environments Containing Excited CO
title_sort crosstalk-free excitation scheme for quantitative oh laser-induced fluorescence in environments containing excited co
topic Rapid Communication
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9289968/
https://www.ncbi.nlm.nih.gov/pubmed/35311380
http://dx.doi.org/10.1177/00037028221088591
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