J/MNRAS/467/4220ivo://CDS.VizieR/J/MNRAS/467/4220doi:10.26093/cds/vizier.74674220CDSRusu C.E.Fassnacht C.D.Sluse D.Hilbert S.Wong K.C.Huang K.-H.,Suyu S.H.Collett T.E.Marshall P.J.Treu T.Koopmans L.V.E.2024-08-17T20:18:19Z2019-12-16T10:18:37ZCDS support team

CDS, Observatoire de Strasbourg, 11 rue de l'Universite, F-67000 Strasbourg, France

cds-question@unistra.frgravitational-lensinggalaxiesphotometryredshiftedvisible-astronomysloan-photometryinfrared-photometryBased on spectroscopy and multiband wide-field observations of the gravitationally lensed quasar HE 0435-1223, we determine the probability distribution function of the external convergence {kappa}_ext_ for this system. We measure the under/overdensity of the line of sight towards the lens system and compare it to the average line of sight throughout the Universe, determined by using the CFHTLenS (The Canada France Hawaii Lensing Survey) as a control field. Aiming to constrain {kappa}_ext_ as tightly as possible, we determine under/overdensities using various combinations of relevant informative weighting schemes for the galaxy counts, such as projected distance to the lens, redshift and stellar mass. We then convert the measured under/overdensities into a {kappa}_ext_ distribution, using ray-tracing through the Millennium Simulation. We explore several limiting magnitudes and apertures, and account for systematic and statistical uncertainties relevant to the quality of the observational data, which we further test through simulations. Our most robust estimate of {kappa}_ext_ has a median value {kappa}^med^_ext_=0.004 and a standard deviation {sigma}_{kappa}_=0.025. The measured {sigma}_{kappa}_ corresponds to 2.5 per cent relative uncertainty on the time delay distance, and hence the Hubble constant H_0_ inferred from this system. The median {kappa}^med^_ext_ value varies by ~0.005 with the adopted aperture radius, limiting magnitude and weighting scheme, as long as the latter incorporates galaxy number counts, the projected distance to the main lens and a prior on the external shear obtained from mass modelling. This corresponds to just ~0.5 per cent systematic impact on H_0_. The availability of a well-constrained {kappa}_ext_ makes HE 0435-1223 a valuable system for measuring cosmological parameters using strong gravitational lens time delays.2017MNRAS.467.4220Rhttps://cdsarc.cds.unistra.fr/viz-bin/cat/J/MNRAS/467/4220CatalogResearchIsServedByTAP VizieR generic serviceIsServedByConesearch servicehttps://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/MNRAS/467/4220https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/MNRAS/467/4220http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/MNRAS/467/4220https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/MNRAS/467/4220https://vizier.iucaa.in/viz-bin/votable?-source=J/MNRAS/467/4220http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/MNRAS/467/4220GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapCone search capability for table J/MNRAS/467/4220/catalog (Catalogue of i<=24 galaxies inside 120 arcsec of HE 0435-1223 (Tables A1 and A2 from the paper))https://vizier.cds.unistra.fr/viz-bin/conesearch/J/MNRAS/467/4220/catalog?https://vizier.iucaa.in/viz-bin/conesearch/J/MNRAS/467/4220/catalog?http://vizieridia.saao.ac.za/viz-bin/conesearch/J/MNRAS/467/4220/catalog?GETtext/xml+votable180.050000true69.578359161-12.2693666280.0055555555555555566/225812.5144872812864278e-20 1.7003137259100215e-19https://cdsarc.cds.unistra.fr/viz-bin/moc/J/MNRAS/467/4220?format=asciiOpticalInfrareddefaultJ/MNRAS/467/4220/catalogCatalogue of i<=24 galaxies inside 120 arcsec of HE 0435-1223 (Tables A1 and A2 from the paper)SimbadNameSimbad column added by the CDSmeta.idcharnullablerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintRAJ2000Right ascension (J2000)degpos.eq.ra;meta.mainDEJ2000Declination (J2000)degpos.eq.dec;meta.mainimagtotTotal i magnitude (SExractor magAuto) (1)magphot.mag;em.opt.Ifloatumag? Subaru/Suprime-Cam u magnitude (1)magphot.mag;em.opt.Ufloatnullablee_umagrms uncertainty on umagmagstat.error;phot.magfloatgmagSubaru/Suprime-Cam g magnitude (1)magphot.mag;em.opt.Bfloate_gmagrms uncertainty on gmagmagstat.error;phot.magfloatrmagSubaru/Suprime-Cam r magnitude (1)magphot.mag;em.opt.Rfloate_rmagrms uncertainty on rmagmagstat.error;phot.magfloatimagSubaru/Suprime-Cam i magnitude (1)magphot.mag;em.opt.Ifloate_imagrms uncertainty on imagmagstat.error;phot.magfloatJmag? Gemini North/NIRI J magnitude, calibrated on 2MASS systemmagphot.mag;em.IR.Jfloatnullablee_Jmagrms uncertainty on Jmagmagstat.error;phot.magfloatHmag? Subaru/MOIRCS 2MASS H magnitude, calibrated on 2MASS systemmagphot.mag;em.IR.Hfloatnullablee_Hmag? rms uncertainty on Hmagmagstat.error;phot.magfloatnullableKsmag? Gemini North/NIRI Ks magnitude,magphot.mag;em.IR.Kfloatnullablee_Ksmag? rms uncertainty on Ksmag calibrated on 2MASS systemmagstat.error;phot.magfloatnullablezRedshiftsrc.redshiftdoublee_z? Error on z, lower value 16 percentile (z16)stat.error;src.redshiftfloatnullableE_z? Error on z, upper value 84 percentile (z84)stat.error;stat.maxfloatnullableIRAC1? IRAC1 (3.6um) magnitudemagphot.mag;em.IR.3-4umfloatnullablee_IRAC1? rms uncertainty on IRAC1magstat.errorfloatnullableIRAC2? IRAC2 (4.5um) magnitudemagphot.mag;em.IR.4-8umfloatnullablee_IRAC2? rms uncertainty on IRAC2magstat.errorfloatnullableIRAC3? IRAC3 (5.7um) magnitudemagphot.flux.density;em.IR.4-8umfloatnullablee_IRAC3? rms uncertainty on IRAC3magstat.errorfloatnullableIRAC4? IRAC4 (7.9um) magnitudemagphot.flux.density;em.IR.8-15umfloatnullablee_IRAC4? rms uncertainty on IRAC4magstat.errorfloatnullablelogMstarStellar masslog(solMass)phys.massfloatlogMhaloHalo masslog(solMass)phys.massfloatSepSeparation of HE 0435-1223arcsecpos.angDistancefloat