论文标题

来自Subaru Hyper Soprime-Cam调查的$ z \ sim 5 $的类星体光度函数的微弱末端

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

论文作者

Niida, Mana, Nagao, Tohru, Ikeda, Hiroyuki, Akiyama, Masayuki, Matsuoka, Yoshiki, He, Wanqiu, Matsuoka, Kenta, Toba, Yoshiki, Onoue, Masafusa, Kobayashi, Masakazu A. R., Taniguchi, Yoshiaki, Furusawa, Hisanori, Harikane, Yuichi, Imanishi, Masatoshi, Kashikawa, Nobunari, Kawaguchi, Toshihiro, Komiyama, Yutaka, Shirakata, Hikari, Terashima, Yuichi, Ueda, Yoshihiro

论文摘要

我们以$ z \ sim 5 $的形式介绍了从$ z \ sim 5 $衍生出的,该数据是从Subaru Strategic Program(SSP)的一部分获得的,具有超级Suprime-CAM(HSC)。从$ \ sim $ 81.8度$^2 $区域的HSC-SSP调查层中,我们通过采用Lyman-break方法降低到$ i = 24.1 $ mag,从而选择了224个低亮度类星体的候选候选者。基于我们的候选人和光谱确认的类星体,来自Sloan Digital Sky Survey(SDSS),我们以$ Z \ SIM \ SIM 5 $得出了类星体发光功能,覆盖$ -28.76 <m _ {\ rm 1450} <-22.32 <-22.32 <-22.32 $ mag。我们发现,类星体光度函数由双重幂律模型拟合,其断裂幅度为$ m^{*} _ {1450} = -25.05^{+0.10} _ { - 0.24} $ mag。低亮度类星体的推断数量密度较低,而派生的微弱斜率,$ -1.22^{+0.03} _ { - 0.10} $比以前在$ z \ sim 5 $上的研究更平坦。从HSC-SSP的$ 4 \ leq Z \ leq 6 $中的类星体发光函数的汇编表明,在此红移范围内的断裂幅度和微弱的斜率中,红移的演变很小,尽管先前的研究表明,在较高的红移处,微弱的端斜率变得更陡峭。低亮度类星体的数量密度从$ z \ sim 5 $降低到$ z \ sim 6 $,而不是$ z \ sim 4 $到$ z \ sim \ sim 5 $。

We present the quasar luminosity function at $z \sim 5$ derived from the optical wide-field survey data obtained as a part of the Subaru strategic program (SSP) with Hyper Suprime-Cam (HSC). From $\sim$81.8 deg$^2$ area in the Wide layer of the HSC-SSP survey, we selected 224 candidates of low-luminosity quasars at $z \sim 5$ 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 $z \sim 5$ covering a wide luminosity range of $-28.76 < M_{\rm 1450} < -22.32$ mag. We found that the quasar luminosity function is fitted by a double power-law model with a break magnitude of $M^{*}_{1450} = -25.05^{+0.10}_{-0.24}$ mag. The inferred number density of low-luminosity quasars is lower, and the derived faint-end slope, $-1.22^{+0.03}_{-0.10}$, is flatter than those of previous studies at $z \sim 5$. A compilation of the quasar luminosity function at $4 \leq z \leq 6$ 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 $z \sim 5$ to $z \sim 6$ than from $z \sim 4$ to $z \sim 5$.

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