论文标题
Z = 6.003 Quasar SDSS J2310+1855中的离子化和原子星际介质
Ionized and atomic interstellar medium in the z = 6.003 quasar SDSS J2310+1855
论文作者
论文摘要
在$ z \ gtrsim 6 $ quasars宿主星系中观察星际培养基(ISM)对于了解超质量黑洞及其宿主之间的共同发展至关重要。为了探测ISM上活性银河核(AGN)的烙印的物理条件,我们报告了$ \ rm [n \ ii] _ {122μm} $和$ \ rm [o \ \ \ i \ \ i] _ {146μmmm} $ lines和conterue conterums conteruim conteruim conterum s $ z = $ z = $ z = $ z = 6.003 J231038.88+185519.7。与先前的$ \ rm [C \ ii] _ {158μm} $和$ \ rm [o \ iii] _ {88μm} $观测值一起,我们使用这些精细结构线的比率来探测ISM属性。与其他高$ z $系统类似,该对象显示出$ \ rm [c \ ii] _ {158μm} $/$ \ rm [o \ i \ i] _ {146μm} $比例可与本地(Ultra)发光的高级星系中最低值相当,表明了一个“温暖的”和“温暖的” dissonenty dissongonent componcent and''deSornect。 $ \ rm [o \ iii] _ {88μm} $/$ \ rm [o \ i] _ {146μm} $比率低于其他本地和高$ z $系统的比率,这表明该Quasar中的较小的电离气体分数。 $ \ rm [o \ iii] _ {88μm} $/$ \ rm [n \ ii] _ {122μm} $比率与本地系统的比率相当,并建议将$ z/z _ {\ odot} $ = 1.5 $ = 1.5 $ - $ - $ 2.2.1的金属金属性。根据$ \ rm [n \ ii] _ {122μm} $检测,我们估计$ \ rm的$ 17 \%$ [C \ ii] _ {158μm} $发射与电离气体相关。 $ \ rm [n \ ii] _ {122μm} $ line显示了与本地系统相当的“通量赤字”。 $ \ rm [o \ i] _ {146μm} $ line,带有$ \ rm [o \ i] _ {146μm} $/fir比率$ \ ge 2 \ ge 2 \ ge 2 \ ge 2 \ times $比本地关系中的预期,表示没有$ \ rm [o \ i \ i] _ {o \ i] _ {o \ i \ rm rm 146 $} $ 146 $}。 The low $\rm [C\ II]_{158 μm}$/$\rm [O\ I]_{146 μm}$ ratio, together with the high $\rm [O\ I]_{146 μm}$/FIR ratio in J2310+1855, reveals that the warm and dense gas is likely a result of AGN heating to the ISM.
Observing the interstellar medium (ISM) in $z \gtrsim 6$ quasars host galaxies is essential for understanding the co-evolution between the supermassive black holes and their hosts. To probe the gas physical conditions and search for imprints of Active Galactic Nuclei (AGN) on the ISM, we report ALMA observations of the $\rm [N\ II]_{122 μm}$ and $\rm [O\ I]_{146 μm}$ lines and the underlying continuum from the $z=6.003$ quasar SDSS J231038.88+185519.7. Together with previous $\rm [C\ II]_{158 μm}$ and $\rm [O\ III]_{88 μm}$ observations, we use the ratios of these fine-structure lines to probe the ISM properties. Similar to other high-$z$ systems, this object exhibits a $\rm [C\ II]_{158 μm}$/$\rm [O\ I]_{146 μm}$ ratio comparable to the lowest values found in local (Ultra) luminous infrared galaxies, suggesting a "warmer" and "denser" gas component compared to typical local systems. The $\rm [O\ III]_{88 μm}$/$\rm [O\ I]_{146 μm}$ ratio is lower than that of other local and high-$z$ systems, indicating a smaller ionized gas fraction in this quasar. The $\rm [O\ III]_{88 μm}$/$\rm [N\ II]_{122 μm}$ ratio is comparable to that of local systems, and suggests a metallicity of $Z/Z_{\odot}$=1.5$-$2.1. Based on the $\rm [N\ II]_{122 μm}$ detection, we estimate that $17\%$ of the $\rm [C\ II]_{158 μm}$ emission is associated with ionized gas. The $\rm [N\ II]_{122 μm}$ line shows a "flux deficit" comparable to local systems. The $\rm [O\ I]_{146 μm}$ line, with a $\rm [O\ I]_{146 μm}$/FIR ratio $\ge 2\times$ than expected from the local relation, indicates no $\rm [O\ I]_{\rm 146 μm}$ deficit. The low $\rm [C\ II]_{158 μm}$/$\rm [O\ I]_{146 μm}$ ratio, together with the high $\rm [O\ I]_{146 μm}$/FIR ratio in J2310+1855, reveals that the warm and dense gas is likely a result of AGN heating to the ISM.