Spectral line parameters including line shapes in the 2 nu(3) Q branch of (CH4)-C-12

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TitreSpectral line parameters including line shapes in the 2 nu(3) Q branch of (CH4)-C-12
Type de publicationJournal Article
Year of Publication2016
AuteursV. Devi M, D. Benner C, Sung K, Brown LR, Crawford TJ, Yu S, Smith MAnn H, Mantz AW, Boudon V, Ismail S
JournalJOURNAL OF QUANTITATIVE SPECTROSCOPY & RADIATIVE TRANSFER
Volume177
Pagination152-169
Date PublishedJUL
Type of ArticleArticle; Proceedings Paper
ISSN0022-4073
Mots-clés2 nu(3) Q branch, Lorentz broadening, methane, Pressure-induced shifts, Relaxation matrix element coefficients, Temperature dependences
Résumé

In this study, we report the first experimental measurements of spectral line shape parameters (self- and air-broadened Lorentz half-widths, pressure-shifts, and line mixing (via off-diagonal relaxation matrix elements) coefficients and their temperature dependences, where appropriate) for transitions in the 2 nu(3) Q branch manifolds, Q(11)-Q(1) of methane ((CH4)-C-12), in the 5996.5-6007-cm(-1) region. The analysis included 23 high-resolution, high signal-to-noise laboratory absorption spectra recorded with the Bruker IFS-125HR Fourier transform spectrometer (FfS) at JPL The experimental data were obtained using C-12-enriched (CH4)-C-12 and dilute mixtures of (CH4)-C-12 in dry air in the 130-296 K range using a room-temperature long path absorption cell and, two custom-built coolable cells. In the analysis, an interactive multispectrum fitting software was employed where all the 23 spectra (11 self-broadened and 12 air-broadened) were fit simultaneously. By carefully applying reasonable constraints to the parameters for severely blended lines, we were able to determine a self-consistent set of broadening, shift and line mixing (relaxation matrix coefficients) parameters for CH4-CH4 and CH4-air collisions. In the majority of cases, a quadratic speed dependence parameter common for all transitions in each Q(I) manifold was determined. However, temperature dependences of the Q branch line mixing parameter could not be determined from the present data. Since no other experimental line shape measurements have been reported for this Q-branch, the present results are compared to available values in the HITRAN2012 database. (C) 2015 Elsevier Ltd. All rights reserved.

DOI10.1016/j.jqsrt.2015.12.009