TY - JOUR
T1 - The bolometric quasar luminosity function at z = 0-7
AU - Shen, Xuejian
AU - Hopkins, Philip F.
AU - Faucher-Giguère, Claude André
AU - Alexander, D. M.
AU - Richards, Gordon T.
AU - Ross, Nicholas P.
AU - Hickox, R. C.
N1 - Funding Information:
Support for PFH was provided by an Alfred P. Sloan Research Fellowship, National Science Foundation (NSF) Collaborative Research grant #1715847 and CAREER grant #1455342. CAFG was supported by NSF through grants AST-1517491, AST-1715216, and CAREER award AST-1652522; by National Aeronautics and Space Administration (NASA) through grant 17-ATP17-0067; and by a Cottrell Scholar Award and Scialog Award #26968 from the Research Corporation for Science Advancement. NPR acknowledges support from the Science and Technology Facilities Council (STFC) and the Ernest Rutherford Fellowship scheme. GTR was supported in part by NASA Astrophysics Data Analysis Program (ADAP) grant NNX17AF04G. DMA thanks the STFC for support through grant code ST/P000541/1. Numerical calculations were run on the Caltech computer cluster ‘Wheeler’.
Publisher Copyright:
© 2020 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society.
PY - 2020/5/14
Y1 - 2020/5/14
N2 - In this paper, we provide updated constraints on the bolometric quasar luminosity function (QLF) from z = 0 to z = 7. The constraints are based on an observational compilation that includes observations in the rest-frame IR, B band, UV, soft, and hard X-ray in past decades. Our method follows Hopkins et al. with an updated quasar SED model and bolometric and extinction corrections. The new best-fitting bolometric quasar luminosity function behaves qualitatively different from the old Hopkins model at high redshift. Compared with the old model, the number density normalization decreases towards higher redshift and the bright-end slope is steeper at z â 2. Due to the paucity of measurements at the faint end, the faint end slope at z â 5 is quite uncertain. We present two models, one featuring a progressively steeper faint-end slope at higher redshift and the other featuring a shallow faint-end slope at z â 5. Further multiband observations of the faint-end QLF are needed to distinguish between these models. The evolutionary pattern of the bolometric QLF can be interpreted as an early phase likely dominated by the hierarchical assembly of structures and a late phase likely dominated by the quenching of galaxies. We explore the implications of this model on the ionizing photon production by quasars, the CXB spectrum, the SMBH mass density, and mass functions. The predicted hydrogen photoionization rate contributed by quasars is subdominant during the epoch of reionization and only becomes important at z â 3. The predicted CXB spectrum, cosmic SMBH mass density, and SMBH mass function are generally consistent with existing observations.
AB - In this paper, we provide updated constraints on the bolometric quasar luminosity function (QLF) from z = 0 to z = 7. The constraints are based on an observational compilation that includes observations in the rest-frame IR, B band, UV, soft, and hard X-ray in past decades. Our method follows Hopkins et al. with an updated quasar SED model and bolometric and extinction corrections. The new best-fitting bolometric quasar luminosity function behaves qualitatively different from the old Hopkins model at high redshift. Compared with the old model, the number density normalization decreases towards higher redshift and the bright-end slope is steeper at z â 2. Due to the paucity of measurements at the faint end, the faint end slope at z â 5 is quite uncertain. We present two models, one featuring a progressively steeper faint-end slope at higher redshift and the other featuring a shallow faint-end slope at z â 5. Further multiband observations of the faint-end QLF are needed to distinguish between these models. The evolutionary pattern of the bolometric QLF can be interpreted as an early phase likely dominated by the hierarchical assembly of structures and a late phase likely dominated by the quenching of galaxies. We explore the implications of this model on the ionizing photon production by quasars, the CXB spectrum, the SMBH mass density, and mass functions. The predicted hydrogen photoionization rate contributed by quasars is subdominant during the epoch of reionization and only becomes important at z â 3. The predicted CXB spectrum, cosmic SMBH mass density, and SMBH mass function are generally consistent with existing observations.
KW - cosmology: observations
KW - galaxies: Active
KW - galaxies: nuclei
KW - infrared: galaxies
KW - quasars: general
KW - ultraviolet: galaxies
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U2 - 10.1093/mnras/staa1381
DO - 10.1093/mnras/staa1381
M3 - Article
AN - SCOPUS:85088039959
SN - 0035-8711
VL - 495
SP - 3252
EP - 3275
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 3
ER -