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dc.contributor.authorElvis, Martin S.
dc.contributor.authorWilkes, Belinda Jane
dc.contributor.authorMcDowell, Jonathan Christopher
dc.contributor.authorGreen, Richard F.
dc.contributor.authorBechtold, Jill
dc.contributor.authorWillner, Steven P.
dc.contributor.authorOey, M. S.
dc.contributor.authorPolomski, Elisha
dc.contributor.authorCutri, Roc
dc.date.accessioned2017-02-14T17:44:45Z
dc.date.issued1994
dc.identifier.citationElvis, Martin, Belinda J. Wilkes, Jonathan C. McDowell, Richard F. Green, Jill Bechtold, S. P. Willner, M. S. Oey, Elisha Polomski, and Roc Cutri. 1994. “Atlas of Quasar Energy Distributions.” The Astrophysical Journal Supplement Series 95 (November): 1. doi:10.1086/192093.en_US
dc.identifier.issn0067-0049en_US
dc.identifier.urihttp://nrs.harvard.edu/urn-3:HUL.InstRepos:30248667
dc.description.abstractWe present an atlas of the spectral energy distributions (SEDs) of normal, nonblazar, quasars over the whole available range (radio to 10 keV X-rays) of the electromagnetic spectrum. The primary (UVSX) sample includes 47 quasars for which the spectral energy distributions include X-ray spectral indices and UV data. Of these, 29 are radio quiet, and 18 are radio loud. The SEDs are presented both in figures and in tabular form, with additional tabular material published on CD-ROM. Previously unpublished observational data for a second set of quasars excluded from the primary sample are also tabulated. The effects of host galaxy starlight contamination and foreground extinction on the UVSX sample are considered and the sample is used to investigate the range of SED properties. Of course, the properties we derive are influenced strongly by the selection effects induced by quasar discovery techniques. We derive the mean energy distribution (MED) for radio-loud and radio-quiet objects and present the bolometric corrections derived from it. We note, however, that the dispersion about this mean is large (approximately one decade for both the infrared and ultraviolet components when the MED is normalized at the near-infrared inflection). At least part of the dispersion in the ultraviolet may be due to time variability, but this is unlikely to be important in the infrared. The existence of such a large dispersion indicates that the MED reflects only some of the properties of quasars and so should be used only with caution.en_US
dc.description.sponsorshipAstronomyen_US
dc.language.isoen_USen_US
dc.publisherIOP Publishingen_US
dc.relation.isversionofdoi:10.1086/312966en_US
dash.licenseLAA
dc.subjectAstronomical Catalogsen_US
dc.subjectInfrared Photometryen_US
dc.subjectQuasarsen_US
dc.subjectRadio Astronomyen_US
dc.subjectSpectral Energy Distributionen_US
dc.subjectStellar Luminosityen_US
dc.subjectStellar Spectrophotometryen_US
dc.subjectUltraviolet Astronomyen_US
dc.subjectX Ray Spectraen_US
dc.subjectGalactic Radiationen_US
dc.subjectHeao 2en_US
dc.subjectInfrared Astronomy Satelliteen_US
dc.subjectIueen_US
dc.subjectSignal To Noise Ratiosen_US
dc.titleAtlas of quasar energy distributionsen_US
dc.typeJournal Articleen_US
dc.description.versionVersion of Recorden_US
dc.relation.journalThe Astrophysical Journal Supplement Seriesen_US
dash.depositing.authorWilkes, Belinda Jane
dc.date.available2017-02-14T17:44:45Z
dc.identifier.doi10.1086/312966*
dash.contributor.affiliatedMcDowell, Jonathan
dash.contributor.affiliatedWillner, Steven
dash.contributor.affiliatedWilkes, Belinda
dash.contributor.affiliatedElvis, Martin


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