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<ri:Resource created="2014-02-17T09:45:55Z" 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>Ti and Fe lines in red supergiants</title><shortName>J/ApJ/751/156</shortName><identifier>ivo://CDS.VizieR/J/ApJ/751/156</identifier><altIdentifier>doi:10.26093/cds/vizier.17510156</altIdentifier><curation><publisher ivo-id="ivo://CDS">CDS</publisher><creator><name>Bergemann M.</name></creator><creator><name>Kudritzki R.-P.</name></creator><creator><name>Plez B.</name></creator><creator><name>Davies B.</name></creator><creator><name>Lind K.</name></creator><creator><name>Gazak Z.</name></creator><date role="Updated">2017-06-20T13:17:03Z</date><date role="Created">2014-02-17T09:45:55Z</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>supergiant-stars</subject><subject>astronomical-models</subject><subject>stellar-atmospheres</subject><subject>chemical-abundances</subject><subject>line-intensities</subject><description>Detailed non-LTE (NLTE) calculations for red supergiant (RSG) stars are presented to investigate the influence of NLTE on the formation of atomic iron and titanium lines in the J band. With their enormous brightness at J band RSG stars are ideal probes of cosmic abundances. Recent LTE studies have found that metallicities accurate to 0.15 dex can be determined from medium-resolution spectroscopy of individual RSGs in galaxies as distant as 10 Mpc. The NLTE results obtained in this investigation support these findings. NLTE abundance corrections for iron are smaller than 0.05 dex for effective temperatures between 3400 K and 4200 K and 0.1 dex at 4400 K. For titanium the NLTE abundance corrections vary smoothly between -0.4 dex and +0.2 dex as a function of effective temperature. For both elements, the corrections also depend on stellar gravity and metallicity. The physical reasons behind the NLTE corrections and the consequences for extragalactic J-band abundance studies are discussed.</description><source format="bibcode">2012ApJ...751..156B</source><referenceURL>https://cdsarc.cds.unistra.fr/viz-bin/cat/J/ApJ/751/156</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/MNRAS/418/863">J/MNRAS/418/863 : NLTE corrections for Mg and Ca lines (Merle+ 2011)</relatedResource><relatedResource ivo-id="ivo://CDS.VizieR/J/A+A/503/541">J/A+A/503/541 : Neutral Li in late-type stars non-LTE calc. (Lind+, 2009)</relatedResource><relatedResource ivo-id="ivo://CDS.VizieR/J/A+A/350/955">J/A+A/350/955 : Atmosph. parameters in metal-poor stars. II (Gratton+, 1999)</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/751/156</accessURL><mirrorURL title="VizieR at IUCAA: Pune, India">https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/ApJ/751/156</mirrorURL><mirrorURL title="VizieR at SAAO: SAAO, South Africa">http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/ApJ/751/156</mirrorURL></interface></capability><capability><interface xsi:type="vs:ParamHTTP"><accessURL use="base">https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/ApJ/751/156</accessURL><mirrorURL title="VizieR at IUCAA: Pune, India">https://vizier.iucaa.in/viz-bin/votable?-source=J/ApJ/751/156</mirrorURL><mirrorURL title="VizieR at SAAO: SAAO, South Africa">http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/ApJ/751/156</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"/></coverage><tableset><schema><name>default</name><table><name>J/ApJ/751/156/NLTE</name><description>Non-LTE abundance corrections and equivalent widths of the TiI and FeI lines in red supergiants</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>Vt</name><description>Microturbulence velocity {xi} (2 or 5)</description><unit>km/s</unit><ucd>phys.veloc.microTurb</ucd><dataType xsi:type="vs:VOTableType">int</dataType><flag>nullable</flag></column><column><name>Teff</name><description>[3400/4400] Effective temperature</description><unit>K</unit><ucd>phys.temperature.effective</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>log(g)</name><description>[-0.5/1] Log surface gravity</description><unit>log(cm.s**-2)</unit><ucd>phys.gravity</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>[Z]</name><description>[-0.5/0.5] Metallicity</description><unit>log(Sun)</unit><ucd>phys.abund.Z</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>dA(TiI)1</name><description>TiI(11892.85) NLTE log(abundance) correction</description><ucd>arith.factor</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>dA(TiI)2</name><description>TiI(11949.58) NLTE log(abundance) correction</description><ucd>arith.factor</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>dA(FeI)1</name><description>FeI(11593.55) NLTE log(abundance) correction</description><ucd>arith.factor</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>dA(FeI)2</name><description>FeI(11638.25) NLTE log(abundance) correction</description><ucd>arith.factor</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>dA(FeI)3</name><description>FeI(11882.80) NLTE log(abundance) correction</description><ucd>arith.factor</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>dA(FeI)4</name><description>FeI(11973.01) NLTE log(abundance) correction</description><ucd>arith.factor</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>W(TiI)1L</name><description>TiI(11892) LTE equivalent width (m{AA})</description><unit>1e-13m</unit><ucd>spect.line.eqWidth</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>W(TiI)1N</name><description>TiI(11892) NLTE equivalent width (m{AA})</description><unit>1e-13m</unit><ucd>spect.line.eqWidth</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>W(TiI)2L</name><description>TiI(11949) LTE equivalent width (m{AA})</description><unit>1e-13m</unit><ucd>spect.line.eqWidth</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>W(TiI)2N</name><description>TiI(11949) NLTE equivalent width (m{AA})</description><unit>1e-13m</unit><ucd>spect.line.eqWidth</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>W(FeI)1L</name><description>FeI(11593) LTE equivalent width (m{AA})</description><unit>1e-13m</unit><ucd>spect.line.eqWidth</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>W(FeI)1N</name><description>FeI(11593) NLTE equivalent width (m{AA})</description><unit>1e-13m</unit><ucd>spect.line.eqWidth</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>W(FeI)2L</name><description>FeI(11638) LTE equivalent width (m{AA})</description><unit>1e-13m</unit><ucd>spect.line.eqWidth</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>W(FeI)2N</name><description>FeI(11638) NLTE equivalent width (m{AA})</description><unit>1e-13m</unit><ucd>spect.line.eqWidth</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>W(FeI)3L</name><description>FeI(11882) LTE equivalent width (m{AA})</description><unit>1e-13m</unit><ucd>spect.line.eqWidth</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>W(FeI)3N</name><description>FeI(11882) NLTE equivalent width (m{AA})</description><unit>1e-13m</unit><ucd>spect.line.eqWidth</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>W(FeI)4L</name><description>FeI(11973) LTE equivalent width (m{AA})</description><unit>1e-13m</unit><ucd>spect.line.eqWidth</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>W(FeI)4N</name><description>FeI(11973) NLTE equivalent width (m{AA})</description><unit>1e-13m</unit><ucd>spect.line.eqWidth</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column></table></schema></tableset></ri:Resource>