论文标题
红外中学调查。 viii。 $ z \ sim5 $的类星体光度功能
The Infrared Medium-deep Survey. VIII. Quasar Luminosity Function at $z\sim5$
论文作者
论文摘要
众所周知,微弱的$ z \ sim5 $ quasars具有$ M_ {1450} \ sim-23 $ mag是紫外线电离背景的潜在重要贡献者。但是,它们的数量密度尚未得到很好的确定,因此很难评估它们在播层间培养基(IGM)早期电离中的作用。在这项工作中,我们使用红外中学调查(IMS)介绍了$ z \ sim5 $ quasar调查的更新结果,这是一项近红外成像调查,覆盖了85度$^{2} $的面积。从双子座多对象光谱仪(GMOS)的光谱观察到双子座8 m望远镜上的GMOS(GMOS),我们发现了$ -26.1 \ -26.1 \ leq m_ {1450} \ leq-leq -23.3 $的$ z \ sim5 $的八个新类似物。将我们的IMS微弱的类星体($ M_ {1450}> -27 $ mag)与更明亮的斯隆数字天空调查(SDSS)类品牌($ M_ {1450} <-27 $ mag),我们得出$ z \ sim5 $ quasar ullusity(qlf),而没有任何固定参数,而没有任何固定参数,而没有任何固定的参数。我们发现QLF的微弱斜率非常平坦($α= -1.2^{+1.4} _ { - 0.6} $),具有$ M^{*} _ {1450} = -25.8^{+1.4} {+1.4} _ { - 1.4} _ { - 1.1} _ { - 1.1} $的特征光度。 QLF的$ z \ sim5 $ quasars的数量密度在912 $ \ unicode {x212b} $ $ε_{912} =(3.7 $ - $ 7.1)\ times10^{23} $ erg s $^$^$^$^$} $} $} $} $} $} $} $} $} $} $} - 1 $ \ dot {n} _ {\ rm ion} =(3.0 $ - $ 5.7)\ times10^{49} $ mpc $^{ - 3} $ s $ s $^{ - 1} $的电离光子密度{这些结果表明,类星体仅造成10-20%(即使在极端情况下甚至最高50%)的光子完全将IGM完全离子化为$ z \ sim5 $所需的光子,这不利于仅仅以$ z \ sim5 $将IGM电离的IGM将IGM电离化的想法。
Faint $z\sim5$ quasars with $M_{1450}\sim-23$ mag are known to be the potentially important contributors to the ultraviolet ionizing background in the post-reionization era. However, their number density has not been well determined, making it difficult to assess their role in the early ionization of the intergalactic medium (IGM). In this work, we present the updated results of our $z\sim5$ quasar survey using the Infrared Medium-deep Survey (IMS), a near-infrared imaging survey covering an area of 85 deg$^{2}$. From our spectroscopic observations with the Gemini Multi-Object Spectrograph (GMOS) on the Gemini-South 8 m Telescope, we discovered eight new quasars at $z\sim5$ with $-26.1\leq M_{1450} \leq -23.3$. Combining our IMS faint quasars ($M_{1450}>-27$ mag) with the brighter Sloan Digital Sky Survey (SDSS) quasars ($M_{1450}<-27$ mag), we derive the $z\sim5$ quasar luminosity function (QLF) without any fixed parameters down to the magnitude limit of $M_{1450}=-23$ mag. We find that the faint-end slope of the QLF is very flat ($α=-1.2^{+1.4}_{-0.6}$), with a characteristic luminosity of $M^{*}_{1450}=-25.8^{+1.4}_{-1.1}$ mag. The number density of $z\sim5$ quasars from the QLF gives an ionizing emissivity at 912 $\unicode{x212B}$ of $ε_{912}=(3.7$--$7.1)\times10^{23}$ erg s$^{-1}$ Hz$^{-1}$ Mpc$^{-3}$ and an ionizing photon density of $\dot{n}_{\rm ion}=(3.0$--$5.7)\times10^{49}$ Mpc$^{-3}$ s$^{-1}$. These results imply that quasars are responsible for only 10-20% (up to 50% even in the extreme case) of the photons required to completely ionize the IGM at $z\sim5$, disfavoring the idea that quasars alone could have ionized the IGM at $z\sim5$.