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<ri:Resource created="2020-03-27T09:01:43Z" status="active" updated="2025-05-19T09:50:00Z" version="1.2" xmlns:cs="http://www.ivoa.net/xml/ConeSearch/v1.0" 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/ConeSearch/v1.0 http://vo.ari.uni-heidelberg.de/docs/schemata/ConeSearch.xsd 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>CALIFA galaxies stellar angular momentum</title><shortName>J/A+A/632/A59</shortName><identifier>ivo://CDS.VizieR/J/A+A/632/A59</identifier><altIdentifier>doi:10.26093/cds/vizier.36320059</altIdentifier><curation><publisher ivo-id="ivo://CDS">CDS</publisher><creator><name>Falcon-Barroso J.</name></creator><creator><name>Van De Ven G.</name></creator><creator><name>Lyubenova M.</name></creator><creator><name>Mendez-Abreu J.,Aguerri J.A.L.</name></creator><creator><name>Garcia-Lorenzo B.</name></creator><creator><name>Bekeraite S.</name></creator><creator><name>Sanchez S.F.</name></creator><creator><name>Husemann B.,Garcia-Benito R.</name></creator><creator><name>Gonzalez Delgado R.M.</name></creator><creator><name>Mast D.</name></creator><creator><name>Walcher C.J.</name></creator><creator><name>Zibetti S.,Zhu L.</name></creator><creator><name>Barrera-Ballesteros J.K.</name></creator><creator><name>Galbany L.</name></creator><creator><name>Sanchez-Blazquez P.,Singh R.</name></creator><creator><name>van den Bosch R.C.E.</name></creator><creator><name>Wild V.</name></creator><creator><name>Bland-Hawthorn J.,Cid Fernandes R.</name></creator><creator><name>de Lorenzo-Caceres A.</name></creator><creator><name>Gallazzi A.</name></creator><creator><name>Marino R.A.,Marquez I.</name></creator><creator><name>Peletier R.F.</name></creator><creator><name>Perez E.</name></creator><creator><name>Perez I.</name></creator><creator><name>Roth M.M.,Rosales-Ortega F.F.</name></creator><creator><name>Ruiz-Lara T.</name></creator><creator><name>Wisotzki L.</name></creator><creator><name>Ziegler B.</name></creator><date role="Updated">2021-02-05T08:13:24Z</date><date role="Created">2020-03-27T09:01:43Z</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>galaxies</subject><subject>catalogs</subject><subject>galaxy-classification-systems</subject><description>We present the apparent stellar angular momentum over the optical extent of 300 galaxies across the Hubble sequence using integral-field spectroscopic (IFS) data from the CALIFA survey. Adopting the same {lambda}_R_ parameter previously used to distinguish between slow and fast rotating early-type (elliptical and lenticular) galaxies, we show that spiral galaxies are almost all fast rotators, as expected. Given the extent of our data, we provide relations for {lambda}_R_ measured in different apertures (e.g. fractions of the effective radius: 0.5R_e_, R_e_, 2R_e_), including conversions to long-slit 1D apertures. Our sample displays a wide range of {lambda}_Re_ values, consistent with previous IFS studies. The fastest rotators are dominated by relatively massive and highly star-forming Sb galaxies, which preferentially reside in the main star-forming sequence. These galaxies reach {lambda}_Re_ values of ~0.85, and they are the largest galaxies at a given mass, while also displaying some of the strongest stellar population gradients. Compared to the population of S0 galaxies, our findings suggest that fading may not be the dominant mechanism transforming spirals into lenticulars. Interestingly, we find that {lambda}_Re_ decreases for late-type Sc and Sd spiral galaxies, with values that occasionally set them in the slow-rotator regime. While for some of them this can be explained by their irregular morphologies and/or face-on configurations, others are edge-on systems with no signs of significant dust obscuration. The latter are typically at the low-mass end, but this does not explain their location in the classical (V/{sigma}, {epsilon}) and ({lambda}_Re_, {epsilon}) diagrams. Our initial investigations, based on dynamical models, suggest that these are dynamically hot disks, probably influenced by the observed important fraction of dark matter within R_e_.</description><source format="bibcode">2019A&amp;A...632A..59F</source><referenceURL>https://cdsarc.cds.unistra.fr/viz-bin/cat/J/A+A/632/A59</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>IsServedBy</relationshipType><relatedResource>Conesearch service</relatedResource></relationship><relationship><relationshipType>related-to</relationshipType><relatedResource ivo-id="ivo://CDS.VizieR/J/A+A/597/A48">J/A+A/597/A48 : Stellar kinematics in CALIFA survey (Falcon-Barroso+, 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Should Not be used for identification.</description><ucd>meta.record</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>eps</name><description>Average ellipticity measured in the outer parts of the galaxy, using SDSS images</description><ucd>src.ellipticity</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>PA</name><description>[] Average position angle measured in the outer parts of the galaxy, using SDSS images</description><unit>deg</unit><ucd>pos.posAng;stat.mean</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>Incl</name><description>Statistical inclination (see Appendix A)</description><unit>deg</unit><ucd>stat.value;src.orbital.inclination</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>Reff</name><description>Effective radius of the galaxy, measured as described in Walcher et al. (2014A&amp;A...569A...1W)</description><unit>arcsec</unit><ucd>phys.angSize</ucd><dataType xsi:type="vs:VOTableType">int</dataType></column><column><name>Type</name><description>Hubble type of the galaxy from Walcher et al. (2014A&amp;A...569A...1W)</description><ucd>meta.note;src.morph.type</ucd><dataType xsi:type="vs:VOTableType" arraysize="3*">char</dataType></column><column><name>M*</name><description>Total stellar mass of the galaxy, measured as described in Walcher et al. (2014A&amp;A...569A...1W)</description><unit>1e+10solMass</unit><ucd>src.class.starGalaxy</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>rMAG</name><description>Total absolute magnitude in r-band from SDSS (Abazajian et al. 2009ApJS..182..543A)</description><unit>mag</unit><ucd>phys.magAbs</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>C90/50</name><description>? Concentration index (ratio of Petrosian radius rad90 and rad50)</description><ucd>meta.code;spect.index</ucd><dataType xsi:type="vs:VOTableType">float</dataType><flag>nullable</flag></column><column><name>u-r</name><description>SDSS Petrosian u-r color index</description><unit>mag</unit><ucd>phot.color;em.opt.U;em.opt.R</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>SFR</name><description>? Star formation rate based on extinction corrected H{alpha} measurements (Sanchez et al. 2017MNRAS.469.2121S)</description><unit>solMass/yr</unit><ucd>phys.SFR</ucd><dataType xsi:type="vs:VOTableType">float</dataType><flag>nullable</flag></column><column><name>l0.5Re</name><description>Apparent stellar angular momentum, {lambda}R measured on an elliptical aperture with semi-major axis 0.5Re</description><ucd>phys.angMomentum</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>lRe</name><description>Apparent stellar angular momentum, {lambda}R measured on an elliptical aperture with semi-major axis Re</description><ucd>phys.angMomentum</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>l2Re</name><description>? Apparent stellar angular momentum, {lambda}R measured on an elliptical aperture with semi-major axis 2Re</description><ucd>phys.angMomentum</ucd><dataType xsi:type="vs:VOTableType">float</dataType><flag>nullable</flag></column><column><name>lRe90</name><description>Deprojected apparent stellar angular momentum, {lambda}Re,90{deg}</description><ucd>phys.angMomentum</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>(V/sig)e</name><description>Ordered-over-random stellar motion (V/{sigma})e measured on an elliptical aperture with semi-major axis Re. We refer the reader to Falcon-Barroso et al. (2017A&amp;A...597A..48F, Cat. J/A+A/597/A48) for further properties of the galaxies not listed here.</description><ucd>pos.cartesian.y</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>_RA</name><description>Positions from Simbad et NED (right ascension part)</description><unit>deg</unit><ucd>pos.eq.ra;meta.main</ucd></column><column><name>_DE</name><description>Positions from Simbad et NED (declination part)</description><unit>deg</unit><ucd>pos.eq.dec;meta.main</ucd></column></table></schema></tableset></ri:Resource>