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<ri:Resource created="2013-04-29T12:21:10Z" status="active" updated="2025-05-19T09:50:00Z" version="1.2" xmlns:ri="http://www.ivoa.net/xml/RegistryInterface/v1.0" xmlns:vr="http://www.ivoa.net/xml/VOResource/v1.0" xmlns:vs="http://www.ivoa.net/xml/VODataService/v1.1" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.ivoa.net/xml/VOResource/v1.0 http://vo.ari.uni-heidelberg.de/docs/schemata/VOResource.xsd http://www.ivoa.net/xml/VODataService/v1.1 http://vo.ari.uni-heidelberg.de/docs/schemata/VODataService.xsd" xsi:type="vs:CatalogService"><title>Rotational transition frequencies of HCOOCH_3_</title><shortName>J/ApJS/205/9</shortName><identifier>ivo://CDS.VizieR/J/ApJS/205/9</identifier><altIdentifier>doi:10.26093/cds/vizier.22050009</altIdentifier><curation><publisher ivo-id="ivo://CDS">CDS</publisher><creator><name>Kobayashi K.</name></creator><creator><name>Takamura K.</name></creator><creator><name>Sakai Y.</name></creator><creator><name>Tsunekawa S.</name></creator><creator><name>Odashima H.</name></creator><creator><name>Ohashi N.</name></creator><date role="Updated">2013-05-18T16:04:52Z</date><date role="Created">2013-04-29T12:21:10Z</date><contact><name>CDS support team</name><address>CDS, Observatoire de Strasbourg, 11 rue de l'Universite, F-67000 Strasbourg, France</address><email>cds-question@unistra.fr</email></contact></curation><content><subject>spectroscopy</subject><subject>interstellar-medium</subject><subject>atomic-physics</subject><description>The cis-methyl formate molecule (HCOOCH_3_) is a well known molecule found in interstellar space. Recently, rotational lines of methyl formate in the first CH_3_ torsional excited state were observed in Orion KL and W51e2. It is quite natural to observe methyl formate in even higher vibrational states considering the temperature estimated in Orion KL and W51e2. Maeda et al. (2008JMoSp.251..293M) reported results on the laboratory spectroscopy of methyl formate including the spectral analysis in its second CH_3_ torsional state. Their assignments were limited to a series of a-type R-branch lines and low K_a_ b-type R-branch transitions, and many assigned lines are excluded in the least-squares analysis. In the present study, we extended the line assignments of both the A- and E-species transitions in the second CH_3_ torsional state especially in the frequency region below the 120GHz region. By combining the present assignments and those made by Maeda et al., 1951 transitions in total for the second CH_3_ torsional state, 1096 A-species transitions up to J=39, and K_a_=15 and 855 E-species transitions up to J=35 and K_a_=13, were least-squares analyzed by using the pseudo-principal-axis-method Hamiltonian with 42 parameters consisting of rotational, centrifugal distortion, and internal rotational constants in the second CH_3_ torsional state. In addition, 1012 transitions out of 1096 A-species transitions could also be least-squares analyzed by using Watson's A-reduced Hamiltonian with 43 parameters, which can serve to calculate the energy levels of the A-species lines of molecules with the CH_3_ internal rotation conveniently.</description><source format="bibcode">2013ApJS..205....9K</source><referenceURL>https://cdsarc.cds.unistra.fr/viz-bin/cat/J/ApJS/205/9</referenceURL><type>Catalog</type><contentLevel>Research</contentLevel><relationship><relationshipType>IsServedBy</relationshipType><relatedResource ivo-id="ivo://CDS.VizieR/TAP">TAP VizieR generic service</relatedResource></relationship><relationship><relationshipType>related-to</relationshipType><relatedResource ivo-id="ivo://CDS.VizieR/J/A+A/538/A119">J/A+A/538/A119 : Spectrum of ^18^O-methyl formate (HCO^18^OCH_3_)</relatedResource><relatedResource ivo-id="ivo://CDS.VizieR/J/ApJS/190/315">J/ApJS/190/315 : Rotational spectrum of H^13^COOCH_3_ (Carvajal+, 2010)</relatedResource><relatedResource ivo-id="ivo://CDS.VizieR/J/A+A/500/1109">J/A+A/500/1109 : Rotational spectrum of HCOO^13^CH_3_ (Carvajal+, 2009)</relatedResource></relationship></content><rights>https://cds.unistra.fr/vizier-org/licences_vizier.html</rights><capability><interface xsi:type="vr:WebBrowser"><accessURL use="full">https://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/ApJS/205/9</accessURL><mirrorURL title="VizieR at IUCAA: Pune, India">https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/ApJS/205/9</mirrorURL><mirrorURL title="VizieR at SAAO: SAAO, South Africa">http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/ApJS/205/9</mirrorURL></interface></capability><capability><interface xsi:type="vs:ParamHTTP"><accessURL use="base">https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/ApJS/205/9</accessURL><mirrorURL title="VizieR at IUCAA: Pune, India">https://vizier.iucaa.in/viz-bin/votable?-source=J/ApJS/205/9</mirrorURL><mirrorURL title="VizieR at SAAO: SAAO, South Africa">http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/ApJS/205/9</mirrorURL><queryType>GET</queryType><resultType>text/xml+votable</resultType></interface></capability><capability standardID="ivo://ivoa.net/std/TAP#aux"><interface xsi:type="vs:ParamHTTP" role="std"><accessURL use="base">https://tapvizier.cds.unistra.fr/TAPVizieR/tap</accessURL></interface></capability><coverage><footprint ivo-id="ivo://ivoa.net/std/moc"/><waveband>Optical</waveband></coverage><tableset><schema><name>default</name><table><name>J/ApJS/205/9/table1</name><description>Pure rotational transition frequencies of cis-methyl formate in v_t_=2 analyzed by using the pseudo-principal-axis-method-(PAM) Hamiltonian model (Ohashi et al. 2004JMoSp.227...28O)</description><column><name>recno</name><description>Record number assigned by the VizieR team. Should Not be used for identification.</description><ucd>meta.record</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>S</name><description>[AE] Symmetry: the A or E torsional substates</description><ucd>phys.atmol</ucd><dataType xsi:type="vs:VOTableType" arraysize="1*">char</dataType></column><column><name>J'</name><description>[2/40] The upper J quantum number</description><ucd>instr.det.qe;stat.max</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>Ka'</name><description>[0/15] The upper Ka quantum number</description><ucd>phys.atmol.qn;stat.max</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>Kc'</name><description>[0/37] The upper Kc quantum number</description><ucd>phys.atmol.qn;stat.max</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>J"</name><description>[1/39] The lower J quantum number</description><ucd>instr.det.qe;stat.min</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>Ka"</name><description>[0/15] The lower Ka quantum number</description><ucd>phys.atmol.qn;stat.min</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>Kc"</name><description>[0/34] The lower Kc quantum number</description><ucd>phys.atmol.qn;stat.min</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>Freq</name><description>[-168772.5/378357.1] The experimental frequency of the transition</description><unit>MHz</unit><ucd>em.freq;phys.atmol.transition</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>f_Freq</name><description>[*] The * shows the transitions not included</description><ucd>meta.code</ucd><dataType xsi:type="vs:VOTableType" arraysize="1*">char</dataType></column><column><name>O-C</name><description>[-0.23/0.44] The observed minus calculated value</description><unit>MHz</unit><ucd>stat.fit.residual</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>El</name><description>[0.4105/347.948] The lower state energy (G1)</description><unit>cm**-1</unit><ucd>phys.energy;phys.atmol.level</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>Smu2</name><description>[0.07/89.51] The line strength (see equation (6))</description><unit>D**2</unit><ucd>spect.line.intensity</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>Ref</name><description>The source of measurement (G2)</description><ucd>meta.bib</ucd><dataType xsi:type="vs:VOTableType" arraysize="4*">char</dataType></column></table><table><name>J/ApJS/205/9/table3</name><description>Pure rotational A-sublevel transition frequencies of cis-methyl formate in v_t_=2 analyzed by using Watson's A-reduced Hamiltonian (Equation (5))</description><column><name>recno</name><description>Record number assigned by the VizieR team. Should Not be used for identification.</description><ucd>meta.record</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>J'</name><description>[2/35] The upper J quantum number</description><ucd>instr.det.qe;stat.max</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>Ka'</name><description>[0/13] The upper Ka quantum number</description><ucd>phys.atmol.qn;stat.max</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>Kc'</name><description>[0/35] The upper Kc quantum number</description><ucd>phys.atmol.qn;stat.max</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>J"</name><description>[1/34] The lower J quantum number</description><ucd>instr.det.qe;stat.min</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>Ka"</name><description>[0/13] The lower Ka quantum number</description><ucd>phys.atmol.qn;stat.min</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>Kc"</name><description>[0/34] The lower Kc quantum number</description><ucd>phys.atmol.qn;stat.min</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>Freq</name><description>[-108498.4/378357.1] The experimental frequency of the transition</description><unit>MHz</unit><ucd>em.freq;phys.atmol.transition</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>O-C</name><description>[-0.28/0.244] The observed minus calculated value</description><unit>MHz</unit><ucd>stat.fit.residual</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>El</name><description>[0.4105/217.274] The lower state energy (G1)</description><unit>cm**-1</unit><ucd>phys.energy;phys.atmol.level</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>Smu2</name><description>[0.09/90.1] The line strength (see equation (6))</description><unit>D**2</unit><ucd>spect.line.intensity</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>Ref</name><description>The source of measurement (G2)</description><ucd>meta.bib</ucd><dataType xsi:type="vs:VOTableType" arraysize="4*">char</dataType></column><column><name>all</name><description>Frequencies for this transition from the different methods</description><ucd>meta.ref.url</ucd><dataType xsi:type="vs:VOTableType" arraysize="*">char</dataType></column></table></schema></tableset></ri:Resource>