J/A+A/639/A129ivo://CDS.VizieR/J/A+A/639/A129doi:10.26093/cds/vizier.36390129CDSCabezas C.Bermudez C.Tercero B.Cernicharo J.2020-10-06T09:01:11Z2020-07-21T10:56:51ZCDS support team

CDS, Observatoire de Strasbourg, 11 rue de l'Universite, F-67000 Strasbourg, France

cds-question@unistra.fratomic-physicsSulfur-containing molecules constitute only 8% of the molecules observed in the interstellar medium (ISM) in spite that sulfur has been shown to be an abundant element in the ISM. In order to understand the chemical behaviour of the ISM and specific cases like the missing sulfur reservoir, a detailed chemical molecular composition in the ISM must be mapped out. Our goal is the investigation of the rotational spectrum of ethyl methyl sulfide, CH_3_CH_2_SCH_3_, which seems to be a potential candidate to be observed in the ISM since the simpler analogs, CH_3_SH and CH_3_CH_2_SH, have been already detected. Rotational spectrum of ethyl methyl sulfide has been observed before, but its experimental rotational parameters are not precise enough to allow its detection in the ISM. The rotational spectrum of ethyl methyl sulfide in the frequency range 72-116.5GHz was measured using a broadband millimeter-wave spectrometer based on radio astronomy receivers with fast Fourier transform backends. The spectral searches and identification of the vibrational excited states of ethyl methyl sulfide was supported by high-level ab initio calculations on the harmonic and anharmonic force fields. The rotational spectra for the trans and gauche conformers of ethyl methyl sulfide was analyzed and a total of 172 and 259 rotational transitions were observed for each one, respectively. The observation of A-E internal rotation splittings allowed the experimental determination of the V3 hindered internal rotation barrier height for both trans and gauche species. In addition, the vibrational excited states, resulting from the lowest frequency vibrational mode nu30 were identified for both conformers. The new experimental rotational parameters were employed to search for ethyl methyl sulfide in the cold and warm molecular clouds Orion KL, Sgr B2(N), B1-b and TMC-1, using the spectral surveys captured by IRAM 30m at 3mm and 2mm.2020A&A...639A.129Chttps://cdsarc.cds.unistra.fr/viz-bin/cat/J/A+A/639/A129CatalogResearchIsServedByTAP VizieR generic servicehttps://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/A+A/639/A129https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/A+A/639/A129http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/A+A/639/A129https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/A+A/639/A129https://vizier.iucaa.in/viz-bin/votable?-source=J/A+A/639/A129http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/A+A/639/A129GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapdefaultJ/A+A/639/A129/tablea1Measured transitions for trans ethyl methyl sulfiderecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintJ'Quantum number J for upper levelinstr.det.qeintKa'Quantum number Ka for upper levelphys.atmol.qnintKc'Quantum number Kc for upper levelphys.atmol.qnintJ"Quantum number J for lower levelinstr.det.qeintKa"Quantum number Ka for lower levelphys.atmol.qnintKc"Quantum number Kc for lower levelphys.atmol.qnintA-EInternal rotation sub-state (only in tables A1-A3)phys.atmolcharFreqMeasMeasured frequencyMHzem.freqdoubleO-CDifference between observed & calculated frequencyMHzstat.fit.residualfloatUncertUncertainty associated to frequencyMHzstat.errorfloatJ/A+A/639/A129/tablea2Measured transitions for gauche ethyl methyl sulfiderecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintJ'Quantum number J for upper levelinstr.det.qeintKa'Quantum number Ka for upper levelphys.atmol.qnintKc'Quantum number Kc for upper levelphys.atmol.qnintJ"Quantum number J for lower levelinstr.det.qeintKa"Quantum number Ka for lower levelphys.atmol.qnintKc"Quantum number Kc for lower levelphys.atmol.qnintA-EInternal rotation sub-state (only in tables A1-A3)phys.atmolcharFreqMeasMeasured frequencyMHzem.freqdoubleO-CDifference between observed & calculated frequencyMHzstat.fit.residualfloatUncertUncertainty associated to frequencyMHzstat.errorfloatJ/A+A/639/A129/tablea3Measured transitions for n30 trans ethyl methyl sulfiderecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintJ'Quantum number J for upper levelinstr.det.qeintKa'Quantum number Ka for upper levelphys.atmol.qnintKc'Quantum number Kc for upper levelphys.atmol.qnintJ"Quantum number J for lower levelinstr.det.qeintKa"Quantum number Ka for lower levelphys.atmol.qnintKc"Quantum number Kc for lower levelphys.atmol.qnintA-EInternal rotation sub-state (only in tables A1-A3)phys.atmolcharFreqMeasMeasured frequencyMHzem.freqdoubleO-CDifference between observed & calculated frequencyMHzstat.fit.residualfloatUncertUncertainty associated to frequencyMHzstat.errorfloatJ/A+A/639/A129/tablea4Measured transitions for 2n30 trans ethyl methyl sulfiderecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintJ'Quantum number J for upper levelinstr.det.qeintKa'Quantum number Ka for upper levelphys.atmol.qnintKc'Quantum number Kc for upper levelphys.atmol.qnintJ"Quantum number J for lower levelinstr.det.qeintKa"Quantum number Ka for lower levelphys.atmol.qnintKc"Quantum number Kc for lower levelphys.atmol.qnintFreqMeasMeasured frequencyMHzem.freqdoubleO-CDifference between observed & calculated frequencyMHzstat.fit.residualfloatUncertUncertainty associated to frequencyMHzstat.errorfloatJ/A+A/639/A129/tablea5Measured transitions for n30 gauche ethyl methyl sulfiderecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintJ'Quantum number J for upper levelinstr.det.qeintKa'Quantum number Ka for upper levelphys.atmol.qnintKc'Quantum number Kc for upper levelphys.atmol.qnintJ"Quantum number J for lower levelinstr.det.qeintKa"Quantum number Ka for lower levelphys.atmol.qnintKc"Quantum number Kc for lower levelphys.atmol.qnintFreqMeasMeasured frequencyMHzem.freqdoubleO-CDifference between observed & calculated frequencyMHzstat.fit.residualfloatUncertUncertainty associated to frequencyMHzstat.errorfloatJ/A+A/639/A129/tablea6Predicted frequencies for trans ethyl methyl sulfide up to 200GHzSymInternal rotation sub-statephys.atmolintrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintJ'Quantum number J for upper levelinstr.det.qeintKa'Quantum number Ka for upper levelphys.atmol.qnintKc'Quantum number Kc for upper levelphys.atmol.qnintJ"Quantum number J for lower levelinstr.det.qeintKa"Quantum number Ka for lower levelphys.atmol.qnintKc"Quantum number Kc for lower levelphys.atmol.qnintFreqFrequencyMHzem.freqdoublelogIntBase 10 logarithm of the integrated intensitylog(nm**2.MHz**-1)spect.line.intensityfloatJ/A+A/639/A129/tablea7Predicted frequencies for gauche ethyl methyl sulfide up to 200GHzrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintJ'Quantum number J for upper levelinstr.det.qeintKa'Quantum number Ka for upper levelphys.atmol.qnintKc'Quantum number Kc for upper levelphys.atmol.qnintJ"Quantum number J for lower levelinstr.det.qeintKa"Quantum number Ka for lower levelphys.atmol.qnintKc"Quantum number Kc for lower levelphys.atmol.qnintSymInternal rotation sub-statephys.atmolintFreqFrequencyMHzem.freqdoublelogIntBase 10 logarithm of the integrated intensitylog(nm**2.MHz**-1)spect.line.intensityfloat