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Infrared to x-ray spectral energy distributions of high redshift quasars

dash.depositing.authorWilkes, Belinda Jane
dash.licenseLAA
dc.contributor.authorBechtold, Jill
dc.contributor.authorElvis, Martin
dc.contributor.authorFiore, Fabrizio
dc.contributor.authorKuhn, Olga
dc.contributor.authorCutri, Roc M.
dc.contributor.authorMcDowell, Jonathan
dc.contributor.authorRieke, Marcia
dc.contributor.authorSiemiginowska, Aneta
dc.contributor.authorWilkes, Belinda
dc.date.accessioned2017-02-13T16:45:36Z
dc.date.available2017-02-13T16:45:36Z
dc.date.issued1994
dc.description.abstractWe have observed 14 quasars with z greater than 2.8 with the ROSAT-PSPC, and detected 12 of them, including the z=4.11 quasar 0000-263. We present the first x-ray spectrum of a radio quiet quasar with z greater than 3, 1946+768. Its x-ray spectrum is consistent with a power law with spectral index alphaE=1.8+2.1,-1.4 and no evidence for absorption in excess of the galactic column (alphaE=1.00+0.28,-0.32 assuming NH=NH(Gal)). A Position Sensitive Proportional Counter (PSPC) hardness ratio is used to constrain the x-ray spectral properties of the quasars for which there were less than 100 photons detected. For the radio quiet quasars, (alphaE) approximately equals 1.2, if one assumes that there is no absorption in excess of the galactic column. We combine the x-ray data with new ground based optical and near-IR spectrophotometry obtained at the Steward 2.3 m and Multiple Mirror Telescope, and data from the literature. The spectral energy distributions are compared to those of low redshift objects. For the radio quiet quasars with z greater than 2.5, the mean (alphaox) is approximately 1.8. This is larger than the mean for quasars with z less than 2.5, but consistent with the expected value for quasars with the high optical luminosities of the objects in this sample. For the radio-loud quasars, (alphaox) is approximately 1.4, independent of redshift. This is smaller than the expected value for the optically luminous, high redshift objects in this sample, if they are mostly GHz peaked radio sources and hence comparable to steep-spectrum, compact radio sources at lower redshift. Finally, we compare the spectral energy distributions of two representative objects to the predicted spectrum of a thin accretion disk in the Kerr geometry, and discuss the uncertainties in deriving black hole masses and mass accretion rates.en_US
dc.description.sponsorshipAstronomyen_US
dc.description.versionVersion of Recorden_US
dc.identifier.citationBechtold, Jill, Martin Elvis, Fabrizio Fiore, Olga Kuhn, Roc M. Cutri, Jonathan C. McDowell, Marcia Rieke, Aneta Siemiginowska, and Belinda J. Wilkes. 1994. “Infrared to x-Ray Spectral Energy Distributions of High Redshift Quasars.” The Astronomical Journal 108 (August): 374. doi:10.1086/117076.en_US
dc.identifier.doi10.1086/117076*
dc.identifier.issn0004-6256en_US
dc.identifier.urihttp://nrs.harvard.edu/urn-3:HUL.InstRepos:30212176
dc.language.isoen_USen_US
dc.publisherIOP Publishingen_US
dc.relation.hasversionhttp://adsabs.harvard.edu/abs/1994AJ....108..374Ben_US
dc.relation.isversionofdoi:10.1086/117076en_US
dc.relation.journalThe Astronomical Journalen_US
dc.subjectAstronomical Spectroscopyen_US
dc.subjectInfrared Astronomyen_US
dc.subjectQuasarsen_US
dc.subjectRed Shiften_US
dc.subjectSpectral Energy Distributionen_US
dc.subjectX Ray Spectroscopyen_US
dc.subjectAccretion Disksen_US
dc.subjectGalaxiesen_US
dc.subjectInfrared Photometryen_US
dc.subjectRadio Astronomyen_US
dc.subjectSpectrophotometryen_US
dc.subjectX Ray Astronomyen_US
dc.titleInfrared to x-ray spectral energy distributions of high redshift quasarsen_US
dc.typeJournal Articleen_US
dspace.entity.typePublication
oaire.licenseConditionLAA
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relation.isAuthorOfPublication418c40d0-f0e6-4aea-9108-c787a285d531
relation.isAuthorOfPublication1210250a-02a8-4ce1-946a-c0e3d15f8944
relation.isAuthorOfPublicationeb7326ba-9419-4ab4-bdb2-c8f1c62d2a0c
relation.isAuthorOfPublication.latestForDiscovery7bf32413-a418-4a77-a6b6-f2505b45dbd7

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