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<ri:Resource created="2019-02-07T14:43:40Z" 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>Yields of Fe and Zn for different types of SNe</title><shortName>J/ApJ/855/63</shortName><identifier>ivo://CDS.VizieR/J/ApJ/855/63</identifier><altIdentifier>doi:10.26093/cds/vizier.18550063</altIdentifier><curation><publisher ivo-id="ivo://CDS">CDS</publisher><creator><name>Hirai Y.</name></creator><creator><name>Saitoh T.R.</name></creator><creator><name>Ishimaru Y.</name></creator><creator><name>Wanajo S.</name></creator><date role="Updated">2019-02-25T13:36:00Z</date><date role="Created">2019-02-07T14:43:40Z</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>stellar-evolutionary-models</subject><subject>supernovae</subject><subject>chemical-abundances</subject><description>The heaviest iron-peak element Zinc (Zn) has been used as an important tracer of cosmic chemical evolution. Spectroscopic observations of the metal-poor stars in Local Group galaxies show an increasing trend of [Zn/Fe] ratios toward lower metallicity. However, the enrichment of Zn in galaxies is not well understood due to poor knowledge of astrophysical sites of Zn, as well as metal mixing in galaxies. Here we show possible explanations for the observed trend by taking into account electron-capture supernovae (ECSNe) as one of the sources of Zn in our chemodynamical simulations of dwarf galaxies. We find that the ejecta from ECSNe contribute to stars with [Zn/Fe]&gt;~0.5. We also find that scatters of [Zn/Fe] in higher metallicities originate from the ejecta of type Ia supernovae. On the other hand, it appears difficult to explain the observed trends if we do not consider ECSNe as a source of Zn. These results come from an inhomogeneous spatial metallicity distribution due to the inefficiency of the metal mixing. We find that the optimal value of the scaling factor for the metal diffusion coefficient is ~0.01 in the shear- based metal mixing model in smoothed particle hydrodynamics simulations. These results suggest that ECSNe could be one of the contributors of the enrichment of Zn in galaxies.</description><source format="bibcode">2018ApJ...855...63H</source><referenceURL>https://cdsarc.cds.unistra.fr/viz-bin/cat/J/ApJ/855/63</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/416/1117">J/A+A/416/1117 : Abundances in the early Galaxy (Cayrel+, 2004)</relatedResource><relatedResource ivo-id="ivo://CDS.VizieR/J/ApJ/608/405">J/ApJ/608/405 : Explosive yields of massive star (Chieffi+, 2004)</relatedResource><relatedResource ivo-id="ivo://CDS.VizieR/J/A+A/415/993">J/A+A/415/993 : FeII, ZNI and SI abundances on halo stars (Nissen+, 2004)</relatedResource><relatedResource 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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>Metal</name><description>[1e-05/0.02] Metallicity</description><ucd>phys.abund.Z</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>D15L</name><description>[8.2/9.8] Lower Mass of ECSN progenitors in Doherty+(2015MNRAS.446.2599D)</description><unit>solMass</unit><ucd>phys.mass</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>D15U</name><description>[8.4/9.9] Upper Mass of ECSN progenitors in Doherty+ (2015MNRAS.446.2599D)</description><unit>solMass</unit><ucd>phys.mass</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>P07L</name><description>[6.4/9] Lower Mass of ECSN progenitors in Poelarends (2007PhDT.......212P)</description><unit>solMass</unit><ucd>phys.mass</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>P07U</name><description>[8.2/9.3] Upper Mass of ECSN progenitors in Poelarends (2007PhDT.......212P)</description><unit>solMass</unit><ucd>phys.mass</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>CL</name><description>[8.5] Lower Mass of ECSN progenitors in the constant mass model (1)</description><unit>solMass</unit><ucd>phys.mass</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>CU</name><description>[9] Upper Mass of ECSN progenitors in the constant mass model (1)</description><unit>solMass</unit><ucd>phys.mass</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column></table><table><name>J/ApJ/855/63/table2</name><description>*Yields of Fe and Zn of each type of SN</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>El</name><description>Names of elements</description><ucd>meta.id;meta.main</ucd><dataType xsi:type="vs:VOTableType" arraysize="2*">char</dataType></column><column><name>Metal</name><description>[0/0.02] Metallicity</description><ucd>phys.abund.Z</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>e8.8</name><description>[0.001/0.0031] Yields of electron-capture SNe (1)</description><unit>solMass</unit><ucd>phys.composition.yield</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>SN15</name><description>[/0.073] Yields of core-collapse SNe of 15Msun (2)</description><unit>solMass</unit><ucd>phys.composition.yield</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>SN20</name><description>[/0.073] Yields of core-collapse SNe of 20Msun (2)</description><unit>solMass</unit><ucd>phys.composition.yield</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>SN25</name><description>[/0.074] Yields of core-collapse SNe of 25Msun (2)</description><unit>solMass</unit><ucd>phys.composition.yield</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>SN30</name><description>[/0.075] Yields of core-collapse SNe of 30Msun (2)</description><unit>solMass</unit><ucd>phys.composition.yield</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>SN40</name><description>[/0.081] Yields of core-collapse SNe of 40Msun (2)</description><unit>solMass</unit><ucd>phys.composition.yield</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>HN20</name><description>[/0.085] Yields of hypernovae of 20Msun (2)</description><unit>solMass</unit><ucd>phys.composition.yield</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>HN25</name><description>[0.00026/0.16] Yields of hypernovae of 25Msun (2)</description><unit>solMass</unit><ucd>phys.composition.yield</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>HN30</name><description>[0.00013/0.21] Yields of hypernovae of 30Msun (2)</description><unit>solMass</unit><ucd>phys.composition.yield</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>HN40</name><description>[0.00069/0.28] Yields of hypernovae of 40Msun (2)</description><unit>solMass</unit><ucd>phys.composition.yield</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column></table></schema></tableset></ri:Resource>