Terahertz spectroscopy of hydrogen sulfide

被引:36
作者
Azzam, Ala'a A. A. [1 ]
Yurchenko, Sergei N. [1 ]
Tennyson, Jonathan [1 ]
Martin-Drumel, Marie-Aline [2 ,3 ]
Pirali, Olivier [2 ,3 ]
机构
[1] UCL, Dept Phys & Astron, London WC1E 6BT, England
[2] Univ Paris 11, Inst Sci Mol Orsay, CNRS, UMR 8214, F-91405 Orsay, France
[3] Synchrotron SOLEIL, AILES Beamline, F-91192 Gif Sur Yvette, France
基金
欧洲研究理事会;
关键词
Hydrogen sulfide; Line assignments; Atmospheric physics; Planetary atmospheres; ROTATIONAL SPECTRUM; MOLECULAR-SPECTROSCOPY; HYPERFINE-STRUCTURE; MICROWAVE-SPECTRUM; COLOGNE DATABASE; MILLIMETER-WAVE; H2S; TRANSITIONS; SULFUR; REGION;
D O I
10.1016/j.jqsrt.2013.05.035
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
Pure rotational transitions of hydrogen sulfide (H2S) in its ground and first excited vibrational states have been recorded at room temperature. The spectrum comprises an average of 1020 scans at 0.005 cm(-1) resolution recorded in the region 45-360 cm(-1) (1.4 to 10.5 THz) with a globar continuum source using a Fourier transform spectrometer located at the AILES beamline of the SOLEIL synchrotron. Over 2400 rotational lines have been detected belonging to ground vibrational state transitions of the four isotopologues (H2S)-S-32, (H2S)-S-33, (H2S)-S-34, and (H2S)-S-36 observed in natural abundance. 65% of these lines are recorded and assigned for the first time, sampling levels as high as J=26 and K-a=17 for (H2S)-S-32. 320 pure rotational transitions of (H2S)-S-32 in its first excited bending vibrational state are recorded and analysed for the first time and 86 transitions for (H2S)-S-34, where some of these transitions belong to new experimental energy levels. Rotational constants have been fitted for all the isotopologues in both vibrational states using a standard effective Hamiltonian approach. Comprehensive comparisons are made with previously available data as well as the data available in HITRAN, CDMS, and JPL databases. The 91 transitions assigned to (H2S)-S-36 give the first proper characterization of its pure rotational spectrum. (C) 2013 Published by Elsevier Ltd.
引用
收藏
页码:341 / 351
页数:11
相关论文
共 40 条
[1]   A λ=1.3 mm and 2 mm molecular line survey towards M 82 [J].
Aladro, R. ;
Martin, S. ;
Martin-Pintado, J. ;
Mauersberger, R. ;
Henkel, C. ;
Ocana Flaquer, B. ;
Amo-Baladron, M. A. .
ASTRONOMY & ASTROPHYSICS, 2011, 535
[2]  
Azzam AAA, 2013, MON NOT R ASTR UNPUB
[3]   TERAHERTZ ROTATIONAL SPECTRUM OF H2S [J].
BELOV, SP ;
YAMADA, KMT ;
WINNEWISSER, G ;
POTEAU, L ;
BOCQUET, R ;
DEMAISON, J ;
POLYANSKY, OL ;
TRETYAKOV, MY .
JOURNAL OF MOLECULAR SPECTROSCOPY, 1995, 173 (02) :380-390
[4]   Performance of the AILES THz-Infrared beamline at SOLEIL for High resolution spectroscopy [J].
Brubach, Jean-Blaise ;
Manceron, Laurent ;
Rouzieres, Mathieu ;
Pirali, Olivier ;
Balcon, Didier ;
Tchana, Fridolin Kwabia ;
Boudon, Vincent ;
Tudorie, M. ;
Huet, Therese ;
Cuisset, Arnaud ;
Roy, Pascale .
WIRMS 2009: 5TH INTERNATIONAL WORKSHOP ON INFRARED MICROSCOPY AND SPECTROSCOPY WITH ACCELERATOR BASED SOURCES, 2010, 1214 :81-+
[5]   MICROWAVE-SPECTRUM OF THE HYDROGEN-SULFIDE MOLECULE H-2S-32 IN THE GROUND-STATE [J].
BURENIN, AV ;
FEVRALSKIKH, TM ;
MELNIKOV, AA ;
SHAPIN, SM .
JOURNAL OF MOLECULAR SPECTROSCOPY, 1985, 109 (01) :1-7
[6]   ONE-TO-2 MILLIMETER WAVE SPECTROSCOPY .2. H2S [J].
BURRUS, CA ;
GORDY, W .
PHYSICAL REVIEW, 1953, 92 (02) :274-277
[7]   HYPERFINE STRUCTURE IN MILLIMETER SPECTRUM OF HYDROGEN SULFIDE - ELECTRIC RESONANCE SPECTROSCOPY ON ASYMMETRIC-TOP MOLECULES [J].
CUPP, RE ;
KEMPF, RA ;
GALLAGHER, JJ .
PHYSICAL REVIEW, 1968, 171 (01) :60-+
[8]   THE FAR-INFRARED SPECTRUM OF HYDROGEN-SULFIDE - THE (000) ROTATIONAL-CONSTANTS OF (H2S)-S-32, (H2S)-S-33 AND (H2S)-S-34 [J].
FLAUD, JM ;
CAMYPEYRET, C ;
JOHNS, JWC .
CANADIAN JOURNAL OF PHYSICS, 1983, 61 (10) :1462-1473
[9]   MICROWAVE-SPECTRUM AND CENTRIFUGAL DISTORTION EFFECTS OF H2S [J].
HELMINGER, P ;
DELUCIA, FC ;
COOK, RL .
JOURNAL OF CHEMICAL PHYSICS, 1972, 56 (09) :4581-+
[10]  
Helminger P., 1973, Journal of Physical and Chemical Reference Data, V2, P215, DOI 10.1063/1.3253117