TY - JOUR
T1 - The Faint End of the Quasar Luminosity Function at z ∼ 5 from the Subaru Hyper Suprime-Cam Survey
AU - Niida, Mana
AU - Nagao, Tohru
AU - Ikeda, Hiroyuki
AU - Akiyama, Masayuki
AU - Matsuoka, Yoshiki
AU - He, Wanqiu
AU - Matsuoka, Kenta
AU - Toba, Yoshiki
AU - Onoue, Masafusa
AU - Kobayashi, Masakazu A.R.
AU - Taniguchi, Yoshiaki
AU - Furusawa, Hisanori
AU - Harikane, Yuichi
AU - Imanishi, Masatoshi
AU - Kashikawa, Nobunari
AU - Kawaguchi, Toshihiro
AU - Komiyama, Yutaka
AU - Shirakata, Hikari
AU - Terashima, Yuichi
AU - Ueda, Yoshihiro
N1 - Publisher Copyright:
© 2020. The American Astronomical Society. All rights reserved..
PY - 2020/12/1
Y1 - 2020/12/1
N2 - 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 mag. The inferred number density of low-luminosity quasars is lower, and the derived faint-end slope, 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.
AB - 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 mag. The inferred number density of low-luminosity quasars is lower, and the derived faint-end slope, 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.
KW - Active galaxies (17)
KW - Luminosity function (942)
KW - Quasars (1319)
KW - Supermassive black holes (1663)
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U2 - 10.3847/1538-4357/abbe11
DO - 10.3847/1538-4357/abbe11
M3 - Article
AN - SCOPUS:85097479361
SN - 0004-637X
VL - 904
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 2
M1 - 89
ER -