Published December 1, 2020 | Version v1
Journal article

The Faint End of the Quasar Luminosity Function at z ∼ 5 from the Subaru Hyper Suprime-Cam Survey

  • 1. Graduate School of Science and Engineering, Ehime University, 2-5 Bunkyo-cho, Matsuyama, Ehime 790-8577 (Japan)
  • 2. Research Center for Space and Cosmic Evolution, Ehime University, 2–5 Bunkyo-cho, Matsuyama, Ehime 790-8577 (Japan)
  • 3. National Astronomical Observatory of Japan, Mitaka, Tokyo 181-8588 (Japan)
  • 4. Astronomical Institute, Tohoku University, Aramaki, Aoba-ku, Sendai, 980-8578 (Japan)
  • 5. Max Planck Institut für Astronomie, Königstuhl 17, D-69117, Heidelberg (Germany)
  • 6. Faculty of Natural Sciences, National Institute of Technology, Kure College, 2-2-11, Agaminami, Kure, Hiroshima 737-8506 (Japan)
  • 7. The Open University of Japan, 2-11, Wakaba, Mihama-ku, Chiba 261-8586 (Japan)
  • 8. Institute for Cosmic Ray Research, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8582 (Japan)
  • 9. Department of Economics, Management and Information Science, Onomichi City University, Onomichi, Hiroshima 722-8506 (Japan)
  • 10. Department of Cosmosciences, Graduates School of Science, Hokkaido University, N10 W8, Kitaku, Sapporo 060-0810 (Japan)
  • 11. Department of Astronomy, Kyoto University, Kitashirakawa-Oiwake-cho, Sakyo-ku, Kyoto 606-8502 (Japan)

Description

We present the quasar luminosity function at z ∼ 5 derived from the optical wide-field survey data obtained as a part of the Subaru strategic program (SSP) with the Hyper Suprime-Cam (HSC). From a ∼81.8 deg2 area in the Wide layer of the HSC-SSP survey, we selected 224 candidates of low-luminosity quasars at z ∼ 5 by adopting the Lyman-break method down to i = 24.1 mag. Based on our candidates and spectroscopically confirmed quasars from the Sloan Digital Sky Survey (SDSS), we derived the quasar luminosity function at z ∼ 5, covering a wide luminosity range of −28.76 < M 1450 < −22.32 mag. We found that the quasar luminosity function is fitted by a double power-law model with a break magnitude of M 1450 = 25.05 0.24 + 0.10 mag. The inferred number density of low-luminosity quasars is lower, and the derived faint-end slope, 1.22 0.10 + 0.03 , is flatter than those of previous studies at z ∼ 5. A compilation of the quasar luminosity function at 4 ≤ z ≤ 6 from the HSC-SSP suggests that there is little redshift evolution in the break magnitude and in the faint-end slope within this redshift range, although previous studies suggest that the faint-end slope becomes steeper at higher redshifts. The number density of low-luminosity quasars decreases more rapidly from z ∼ 5 to z ∼ 6 than from z ∼ 4 to z ∼ 5.

Availability note (English)

Available from http://dx.doi.org/10.3847/1538-4357/abbe11

Additional details

Identifiers

Publishing Information

Journal Title
Astrophysical Journal
Journal Volume
904
Journal Issue
2
Journal Page Range
[14 p.]
ISSN
0004-637X
CODEN
ASJOAB

INIS

Country of Publication
United Kingdom
Country of Input or Organization
International Atomic Energy Agency (IAEA)
INIS RN
52073950
Subject category
S79: ASTROPHYSICS, COSMOLOGY AND ASTRONOMY;
Descriptors DEI
DENSITY; LUMINOSITY; LYMAN LINES; QUASARS; RED SHIFT
Descriptors DEC
COSMIC RADIO SOURCES; OPTICAL PROPERTIES; PHYSICAL PROPERTIES