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<ri:Resource created="2026-09-03T16:18:36Z" status="active" updated="2026-09-03T15:24:07Z" 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>Masses of galaxy clusters and groups in eFEDS</title><shortName>J/MNRAS/522/1601</shortName><identifier>ivo://CDS.VizieR/J/MNRAS/522/1601</identifier><curation><publisher ivo-id="ivo://CDS">CDS</publisher><creator><name>Chiu I.-N.</name></creator><creator><name>Klein M.</name></creator><creator><name>Mohr J.</name></creator><creator><name>Bocquet S.</name></creator><date role="Updated">2026-09-03T15:24:07Z</date><date role="Created">2026-09-03T16:18:36Z</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>galaxy-clusters</subject><subject>x-ray-sources</subject><subject>active-galactic-nuclei</subject><description>We present the first cosmological study of a sample of eROSITA clusters, which were identified in the eROSITA Final Equatorial Depth Survey (eFEDS). In a joint selection on X-ray and optical observables, the sample contains 455 clusters within a redshift range of 0.1 &lt; z &lt; 1.2, of which 177 systems are covered by the public data from the Hyper Suprime-Cam (HSC) survey that enables uniform weak-lensing cluster mass constraints. With minimal assumptions, at each cluster redshift we empirically model (1) the scaling relations between the cluster halo mass and the observables, which include the X-ray count rate, the optical richness, and the weak-lensing mass, and (2) the X-ray selection in terms of the completeness function C. Using the richness distribution of the clusters, we directly measure the X-ray completeness and adopt those measurements as informative priors for the parameters of C. In a blinded analysis, we obtain the cosmological constraints {omega}_m_=0.245^+0.048^_-0.058_, {sigma}_8_=0.833^+0.075^_-0.063_, and S_8_ = {sigma}_8_({omega}_m_/0.3)^0.3^ = 0.791^+0.028^_-0.031_ in a flat LCDM cosmology. Extending to a flat wCDM cosmology leads to the constraint on the equation of state parameter of the dark energy of w = -1.25 +/- 0.47. The eFEDS constraints are in good agreement with the results from the Planck mission, the galaxy-galaxy lensing and clustering analysis of the Dark Energy Survey, and the cluster abundance analysis of the SPT-SZ survey at a level of &lt;~ 1{sigma}. With the empirical modelling, this work presents the first fully self-consistent cosmological constraints based on a synergy between wide-field X-ray and weak lensing surveys.</description><source format="bibcode">2023MNRAS.522.1601C</source><referenceURL>https://cdsarc.cds.unistra.fr/viz-bin/cat/J/MNRAS/522/1601</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/MNRAS/488/739">J/MNRAS/488/739 : MARD-Y3 catalog (Klein+, 2019)</relatedResource><relatedResource ivo-id="ivo://CDS.VizieR/J/MNRAS/474/3324">J/MNRAS/474/3324 : Multicomponent matched filter test (Klein+, 2018)</relatedResource><relatedResource ivo-id="ivo://CDS.VizieR/J/MNRAS/444/147">J/MNRAS/444/147 : Richness of galaxy clusters (Oguri, 2014)</relatedResource><relatedResource ivo-id="ivo://CDS.VizieR/J/A+A/661/A1">J/A+A/661/A1 : The eFEDS X-ray catalogs (V7.4) (Brunner+, 2022)</relatedResource><relatedResource ivo-id="ivo://CDS.VizieR/J/A+A/661/A10">J/A+A/661/A10 : eFEDS galaxy clusters and groups in disguise (Bulbul+, 2022)</relatedResource><relatedResource ivo-id="ivo://CDS.VizieR/J/A+A/661/A11">J/A+A/661/A11 : eFEDS. 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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>Name</name><description>The cluster name (Name)</description><ucd>meta.id;meta.main</ucd><dataType xsi:type="vs:VOTableType" arraysize="22*">char</dataType></column><column><name>eFEDS</name><description>Display the ancilliary eFEDS catalog data</description><ucd>meta.ref.url</ucd><dataType xsi:type="vs:VOTableType" arraysize="*">char</dataType></column><column><name>zbest</name><description>The cluster redshift the quantity in the official eFEDS catalog (Z_BEST_COMB)</description><ucd>src.redshift;pos.heliocentric</ucd><dataType xsi:type="vs:VOTableType">float</dataType></column><column><name>R500cL</name><description>The cluster radius R500c in the LCDM cosmology (r500c_lcdm)</description><unit>arcmin</unit><ucd>phys.angSize;phys.cosmology</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>log(M500cEL)</name><description>The ensemble mass M500c,ens in the LCDM cosmology (ensemble_500c_lcdm)</description><unit>log(solMass)</unit><ucd>phys.mass;phys.cosmology</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>log(M500cML)</name><description>The median of the mass posterior P(M|{eta},z,p) where are the best-fitting parameters in the LCDM cosmology (median_500c_lcdm)</description><unit>log(solMass)</unit><ucd>phys.mass;phys.cosmology</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>E_log(M500cML)</name><description>Upper uncertainty from distribution of log (M500cML) (m500c_lcdm_hierr)</description><unit>log(solMass)</unit><ucd>stat.error;stat.max</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>e_log(M500cML)</name><description>Lower uncertainty from distribution of log (M500cML) (m500c_lcdm_loerr)</description><unit>log(solMass)</unit><ucd>stat.error</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>R500cw</name><description>The cluster radius R500c in the wCDM cosmology (r500c_wcdm)</description><unit>arcmin</unit><ucd>phys.angSize;phys.cosmology</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>log(M500cEw)</name><description>The ensemble mass M500c,ens in the wCDM cosmology (ensemble_500c_wcdm)</description><unit>log(solMass)</unit><ucd>phys.mass;phys.cosmology</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>log(M500cMw)</name><description>The median of the mass posterior P(M|{eta},z,p) where are the best-fitting parameters in the wCDM cosmology (median_500c_wcdm)</description><unit>log(solMass)</unit><ucd>phys.mass;phys.cosmology</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>E_log(M500cMw)</name><description>Upper uncertainty from distribution of log (M500cMw) (m500c_wcdm_hierr)</description><unit>log(solMass)</unit><ucd>stat.error;stat.max</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>e_log(M500cMw)</name><description>Lower uncertainty from distribution of log (M500cMw) (m500c_wcdm_loerr)</description><unit>log(solMass)</unit><ucd>stat.error</ucd><dataType xsi:type="vs:VOTableType">double</dataType></column><column><name>_RA</name><description>Positions from eFEDS names (right ascension part)</description><unit>deg</unit><ucd>pos.eq.ra;meta.main</ucd></column><column><name>_DE</name><description>Positions from eFEDS names (declination part)</description><unit>deg</unit><ucd>pos.eq.dec;meta.main</ucd></column></table></schema></tableset></ri:Resource>