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dc.contributor.authorWang, Shu
dc.contributor.authorShen, Yue
dc.contributor.authorJiang, Linhua
dc.contributor.authorGrier, C. J.
dc.contributor.authorHorne, Keith
dc.contributor.authorHomayouni, Y.
dc.contributor.authorPeterson, B. M.
dc.contributor.authorTrump, Jonathan R.
dc.contributor.authorBrandt, W. N.
dc.contributor.authorHall, P. B.
dc.contributor.authorHo, Luis C.
dc.contributor.authorI-Hsiu Li, Jennifer
dc.contributor.authorHernández Santisteban, J. V.
dc.contributor.authorKinemuchi, K.
dc.contributor.authorMcGreer, Ian D.
dc.contributor.authorSchneider, D. P.
dc.date.accessioned2021-03-24T00:33:12Z
dc.date.available2021-03-24T00:33:12Z
dc.date.issued2020-10-30
dc.identifier.citationWang, S., Shen, Y., Jiang, L., Grier, C. J., Horne, K., Homayouni, Y., ... & Schneider, D. P. (2020). The Sloan Digital Sky Survey Reverberation Mapping Project: How Broad Emission Line Widths Change When Luminosity Changes. The Astrophysical Journal, 903(1), 51.en_US
dc.identifier.issn0004-637X
dc.identifier.doi10.3847/1538-4357/abb36d
dc.identifier.urihttp://hdl.handle.net/10150/657178
dc.description.abstractQuasar broad emission lines are largely powered by photoionization from the accretion continuum. Increased central luminosity will enhance line emissivity in more distant clouds, leading to increased average distance of the broad-line-emitting clouds and decreased averaged line width, which is known as the "breathing" broad-line region. However, different lines breathe differently, and some high-ionization lines, such as C IV, can even show "anti-breathing" where the line broadens when luminosity increases. Using multi-year photometric and spectroscopic monitoring data from the Sloan Digital Sky Survey Reverberation Mapping project, we quantify the breathing effect (Delta logW = alpha Delta log L) of broad H alpha, H beta, Mg II, C IV, and C III] for statistical quasar samples over z. approximate to 0.1-2.5. We find that H beta displays the most consistent normal breathing expected from the virial relation (alpha similar to -0.25), Mg II and Ha on average show no breathing (alpha similar to 0), and C IV (and similarly C III] and Si IV) mostly shows anti-breathing (alpha > 0). The anti-breathing of C IV can be well understood by the presence of a non-varying core component in addition to a reverberating broad-base component, which is consistent with earlier findings. The deviation from canonical breathing introduces extra scatter (a luminosity-dependent bias) in single-epoch virial BH mass estimates due to intrinsic quasar variability, which underlies the long-argued caveats of C IV single-epoch masses. Using the line dispersion instead of FWHM leads to fewer, albeit still substantial, deviations from canonical breathing in most cases. Our results strengthen the need for reverberation mapping to provide reliable quasar BH masses and to quantify the level of variability-induced bias in single-epoch BH masses based on various lines.en_US
dc.description.sponsorshipNational Natural Science Foundation of Chinaen_US
dc.language.isoenen_US
dc.publisherIOP PUBLISHING LTDen_US
dc.rights© 2020. The American Astronomical Society. All rights reserved.en_US
dc.rights.urihttp://rightsstatements.org/vocab/InC/1.0/
dc.subjectReverberation mappingen_US
dc.subjectQuasarsen_US
dc.subjectSupermassive black holesen_US
dc.titleThe Sloan Digital Sky Survey Reverberation Mapping Project: How Broad Emission Line Widths Change When Luminosity Changesen_US
dc.typeArticleen_US
dc.identifier.eissn1538-4357
dc.contributor.departmentUniv Arizona, Steward Observen_US
dc.identifier.journalASTROPHYSICAL JOURNALen_US
dc.description.collectioninformationThis item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.en_US
dc.eprint.versionFinal published versionen_US
dc.source.journaltitleThe Astrophysical Journal
dc.source.volume903
dc.source.issue1
dc.source.beginpage51
refterms.dateFOA2021-03-24T00:33:25Z


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