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<ri:Resource created="2017-04-07T12:20:43Z" status="active" updated="2025-06-13T15:25:00Z" 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 frequencies of TiO isotopologues</title><shortName>J/ApJ/833/9</shortName><identifier>ivo://CDS.VizieR/J/ApJ/833/9</identifier><altIdentifier>doi:10.26093/cds/vizier.18330009</altIdentifier><curation><publisher ivo-id="ivo://CDS">CDS</publisher><creator><name>Lincowski A.P.</name></creator><creator><name>Halfen D.T.</name></creator><creator><name>Ziurys L.M.</name></creator><date role="Updated">2017-05-22T15:34:09Z</date><date role="Created">2017-04-07T12:20:43Z</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>atomic-physics</subject><subject>radio-spectroscopy</subject><description>Pure rotational spectra of the rare isotopologues of titanium oxide, ^46^TiO, ^47^TiO, ^49^TiO, and ^50^TiO, have been recorded using a combination of Fourier transform millimeter-wave (FTmmW) and millimeter/submillimeter direct absorption techniques in the frequency range 62-538GHz. This study is the first complete spectroscopic characterization of these species in their X^3^{Delta}_r_ ground electronic states. The isotopologues were created by the reaction of N_2_O or O_2_ and titanium vapor, produced either by laser ablation or in a Broida-type oven, and observed in the natural Ti isotopic abundances. Between 10 and 11 rotational transitions J+1&lt;-&gt;J were measured for each species, typically in all 3 spin-orbit ladders {Omega}=1, 2, and 3. For ^47^TiO and ^49^TiO, hyperfine structure was resolved, originating from the titanium-47 and titanium-49 nuclear spins of I=5/2 and 7/2, respectively. For the {Omega}=1 and 3 components, the hyperfine structure was found to follow a classic Lande pattern, while that for {Omega}=2 appeared to be perturbed, likely a result of mixing with the nearby isoconfigurational a^1^{Delta} state. The spectra were analyzed with a case (a) Hamiltonian, and rotational, spin-orbit, and spin-spin parameters were determined for each species, as well as magnetic hyperfine and electric quadrupole constants for the two molecules with nuclear spins. The most abundant species, ^48^TiO, has been detected in circumstellar envelopes. These measurements will enable other titanium isotopologues to be studied at millimeter wavelengths, providing Ti isotope ratios that can test models of nucleosynthesis.</description><source format="bibcode">2016ApJ...833....9L</source><referenceURL>https://cdsarc.cds.unistra.fr/viz-bin/cat/J/ApJ/833/9</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/551/A113">J/A+A/551/A113 : Spectrum of VY CMa in 220.65-224.25GHz range (Kaminski+, 2013)</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/ApJ/833/9</accessURL><mirrorURL title="VizieR at IUCAA: Pune, India">https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/ApJ/833/9</mirrorURL><mirrorURL title="VizieR at SAAO: SAAO, South Africa">http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/ApJ/833/9</mirrorURL></interface></capability><capability><interface xsi:type="vs:ParamHTTP"><accessURL use="base">https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/ApJ/833/9</accessURL><mirrorURL title="VizieR at IUCAA: Pune, India">https://vizier.iucaa.in/viz-bin/votable?-source=J/ApJ/833/9</mirrorURL><mirrorURL title="VizieR at SAAO: SAAO, South Africa">http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/ApJ/833/9</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>Radio</waveband></coverage><tableset><schema><name>default</name><table><name>J/ApJ/833/9/table1</name><description>Observed rotational transitions of titanium oxide (TiO) isotopologues (X^3^{Delta}_r_)</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>Species</name><description>TiO Isotopologue Species</description><ucd>meta.note</ucd><dataType xsi:type="vs:VOTableType" arraysize="5*">char</dataType></column><column><name>J1</name><description>[2/17] Upper J quantum number</description><ucd>instr.det.qe;stat.max</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>J0</name><description>[1/16] Lower J quantum number</description><ucd>instr.det.qe;stat.min</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>F1</name><description>[0.5/19.5]? Upper F quantum number</description><ucd>phys.atmol.qn</ucd><dataType xsi:type="vs:VOTableType">float</dataType><flag>nullable</flag></column><column><name>F0</name><description>[1.5/18.5]? Lower F quantum number</description><ucd>phys.atmol.qn</ucd><dataType xsi:type="vs:VOTableType">float</dataType><flag>nullable</flag></column><column><name>Freq1</name><description>[62687/532616] Frequency of the transition for {Omega}=1</description><unit>MHz</unit><ucd>em.freq;phys.atmol.transition</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>(O-C)1</name><description>[-0.3/0.2]? Observed minus calculated value for Freq1</description><unit>MHz</unit><ucd>stat.fit.residual</ucd><dataType xsi:type="vs:VOTableType">float</dataType><flag>nullable</flag></column><column><name>f_(O-C)1</name><description>[a] Flag on (O-C)1 (1)</description><ucd>meta.code</ucd><dataType xsi:type="vs:VOTableType" arraysize="1*">char</dataType></column><column><name>Freq2</name><description>[221900/538598]? Frequency of the transition for {Omega}=2</description><unit>MHz</unit><ucd>em.freq;phys.atmol.transition</ucd><dataType xsi:type="vs:VOTableType">double</dataType><flag>nullable</flag></column><column><name>(O-C)2</name><description>[-0.3/0.3]? Observed minus calculated value for Freq2</description><unit>MHz</unit><ucd>stat.fit.residual</ucd><dataType xsi:type="vs:VOTableType">float</dataType><flag>nullable</flag></column><column><name>f_(O-C)2</name><description>[a] Flag on (O-C)2 (1)</description><ucd>meta.code</ucd><dataType xsi:type="vs:VOTableType" arraysize="1*">char</dataType></column><column><name>Freq3</name><description>[224069/522730]? Frequency of the transition for {Omega}=3</description><unit>MHz</unit><ucd>em.freq;phys.atmol.transition</ucd><dataType xsi:type="vs:VOTableType">double</dataType><flag>nullable</flag></column><column><name>(O-C)3</name><description>[-0.3/0.3]? 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