论文标题
Z = 5.7-6.4的X射线光度函数的限制与外层次偶然的Swift调查有关
Constraints on the X-ray Luminosity Function of AGN at z=5.7-6.4 with the Extragalactic Serendipitous Swift Survey
论文作者
论文摘要
活性银河核(AGN)的X射线光度函数(XLF)追踪了跨宇宙时间的超质量黑洞种群的生长和演变,但是,在这些高弹药处缺乏光谱约束时,当前的XLF模型在Z> 6的红移时受到了很大的限制。在这项工作中,我们使用在静脉外串行的Swift Survey(EXSESS)目录中鉴定出的高红移AGN,在z = 5.7-6.4处重新递减{place limits}。在Exess中,我们发现一个偶然的X射线检测到Z> 6 agn,Atlas J025.6821-33.4627,X射线光度为 $L_\mathrm{X}=8.47^{+3.40}_{-3.13}\times10^{44}\mathrm{erg.s^{-1}}$ and $z=6.31\pm0.03$ making it the highest redshift, spectroscopically confirmed, serendipitously X-ray detected quasar known to date.我们还计算了未发现其他来源的较高灯具下空间密度的上限,从而使我们能够在XLF的形状上放置约束。我们的结果与XLF现有参数模型的推断所预测的高光度AGN的空间密度迅速下降是一致的。我们还发现,基于X射线的测量值与基于$ z \ gtrsim6 $的紫外测量值的降压测量值函数的估计是一致的,尽管它们在这些高亮度下需要大的X射线才能进行X射线测量。
X-ray luminosity functions (XLFs) of Active Galactic Nuclei (AGN) trace the growth and evolution of supermassive black hole populations across cosmic time, however, current XLF models are poorly constrained at redshifts of z>6, with a lack of spectroscopic constraints at these high redshifts. In this work we \redit{place limits} on the bright-end of the XLF at z=5.7-6.4 using high-redshift AGN identified within the Extragalactic Serendipitous Swift Survey (ExSeSS) catalogue. Within ExSeSS we find one serendipitously X-ray detected z>6 AGN, ATLAS J025.6821-33.4627, with an X-ray luminosity of $L_\mathrm{X}=8.47^{+3.40}_{-3.13}\times10^{44}\mathrm{erg.s^{-1}}$ and $z=6.31\pm0.03$ making it the highest redshift, spectroscopically confirmed, serendipitously X-ray detected quasar known to date. We also calculate an upper limit on the space density at higher luminosities where no additional sources are found, enabling us to place constraints on the shape of the XLF. Our results are consistent with the rapid decline in the space densities of high-luminosity AGN toward high redshift as predicted by extrapolations of existing parametric models of the XLF. We also find that our X-ray based measurements are consistent with estimates of the bolometric quasar luminosity function based on UV measurements at $z\gtrsim6$, although they require a large X-ray to bolometric correction factor at these high luminosities.