Quasar Luminosity Function at z = 7

dc.contributor.authorMatsuoka, Y.
dc.contributor.authorOnoue, M.
dc.contributor.authorIwasawa, Kazushi
dc.contributor.authorStrauss, M.A.
dc.contributor.authorKashikawa, N.
dc.contributor.authorIzumi, T.
dc.contributor.authorNagao, T.
dc.contributor.authorImanishi, M.
dc.contributor.authorAkiyama, M.
dc.contributor.authorSilverman, J.D.
dc.contributor.authorAsami, N.
dc.contributor.authorBosch, J.
dc.contributor.authorFurusawa, H.
dc.contributor.authorGoto, T.
dc.contributor.authorGunn, J.E.
dc.contributor.authorHarikane, Y.
dc.contributor.authorIkeda, H.
dc.contributor.authorInayoshi, K.
dc.contributor.authorIshimoto, R.
dc.contributor.authorKawaguchi, T.
dc.contributor.authorKikuta, S.
dc.contributor.authorKohno, K.
dc.contributor.authorKomiyama, Y.
dc.contributor.authorLee C.-H.
dc.contributor.authorLupton, R.H.
dc.contributor.authorMinezaki, T.
dc.contributor.authorMiyazaki, S.
dc.contributor.authorMurayama, H.
dc.contributor.authorNishizawa, A.J.
dc.contributor.authorOguri, M.
dc.contributor.authorOno, Y.
dc.contributor.authorOogi, T.
dc.contributor.authorOuchi, M.
dc.contributor.authorPrice, P.A.
dc.contributor.authorSameshima, H.
dc.contributor.authorSugiyama, N.
dc.contributor.authorTait, P.J.
dc.contributor.authorTakada, M.
dc.contributor.authorTakahashi, A.
dc.contributor.authorTakata, T.
dc.contributor.authorTanaka, M.
dc.contributor.authorToba, Y.
dc.contributor.authorWang, S.-Y.
dc.contributor.authorYamashita, T.
dc.date.accessioned2025-01-31T19:19:26Z
dc.date.available2025-01-31T19:19:26Z
dc.date.issued2023
dc.date.updated2025-01-31T19:19:27Z
dc.description.abstractWe present the quasar luminosity function (LF) at z = 7, measured with 35 spectroscopically confirmed quasars at 6.55 < z < 7.15. The sample of 22 quasars from the Subaru High-z Exploration of Low-Luminosity Quasars (SHELLQs) project, combined with 13 brighter quasars in the literature, covers an unprecedentedly wide range of rest-frame ultraviolet magnitudes over −28 < M1450 < −23. We found that the binned LF flattens significantly toward the faint end populated by the SHELLQs quasars. A maximum likelihood fit to a double power-law model has a break magnitude, a characteristic density Gpc−3 mag−1, and a bright-end slope, when the faint-end slope is fixed to α = −1.2 as observed at z ≤ 6. The overall LF shape remains remarkably similar from z = 4 to 7, while the amplitude decreases substantially toward higher redshifts, with a clear indication of an accelerating decline at z ≥ 6. The estimated ionizing photon density, 1048.2±0.1 s−1 Mpc−3, is less than 1% of the critical rate to keep the intergalactic medium ionized at z = 7, and thus indicates that quasars are not a major contributor to cosmic reionization.
dc.format.extent1 p.
dc.format.mimetypeapplication/pdf
dc.identifier.idgrec753898
dc.identifier.issn2041-8205
dc.identifier.urihttps://hdl.handle.net/2445/218392
dc.language.isoeng
dc.publisherInstitute of Physics (IOP)
dc.relation.isformatofReproducció del document publicat a: https://doi.org/10.3847/2041-8213/acd69f
dc.relation.ispartofAstrophysical Journal Letters, 2023
dc.relation.urihttps://doi.org/10.3847/2041-8213/acd69f
dc.rights(c) American Astronomical Society, 2023
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess
dc.sourceArticles publicats en revistes (Institut de Ciències del Cosmos (ICCUB))
dc.subject.classificationGalàxies
dc.subject.classificationQuàsars
dc.subject.otherGalaxies
dc.subject.otherQuasars
dc.titleQuasar Luminosity Function at z = 7
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:eu-repo/semantics/publishedVersion

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