[论文解读] First results from the JWST Early Release Science Program Q3D: Ionization cone, clumpy star formation and shocks in a $z=3$ extremely red quasar host
利用詹姆斯·韦布空间望远镜/NIRSpec积分场单元(IFU)观测,本研究绘制了红移z=2.94的极红类星体宿主星系中的电离机制图谱,揭示了类星体驱动的外流在电离锥之外产生广角激波,星暴区域呈团块状且恒星形成速率达200 M⊙ yr⁻¹,以及极端的星际介质(ISM)条件(ne ≈ 3,000 cm⁻³,AV ≤ 3 mag)。在电离锥外检测到激波,证实了大张角风的存在,表明类星体反馈在宇宙正午时期具有广泛影响。
Massive galaxies formed most actively at redshifts $z=1-3$ during the period known as `cosmic noon.' Here we present an emission-line study of an extremely red quasar SDSSJ165202.64+172852.3 host galaxy at $z=2.94$, based on observations with the Near Infrared Spectrograph (NIRSpec) integral field unit (IFU) on board JWST. We use standard emission-line diagnostic ratios to map the sources of gas ionization across the host and a swarm of companion galaxies. The quasar dominates the photoionization, but we also discover shock-excited regions orthogonal to the ionization cone and the quasar-driven outflow. These shocks could be merger-induced or -- more likely, given the presence of a powerful galactic-scale quasar outflow -- these are signatures of wide-angle outflows that can reach parts of the galaxy that are not directly illuminated by the quasar. Finally, the kinematically narrow emission associated with the host galaxy presents as a collection of 1 kpc-scale clumps forming stars at a rate of at least 200 $M_{\odot}$ yr$^{-1}$. The ISM within these clumps shows high electron densities, reaching up to 3,000 cm$^{-3}$ with metallicities ranging from half to a third solar with a positive metallicity gradient and V band extinctions up to 3 magnitudes. The star formation conditions are far more extreme in these regions than in local star-forming galaxies but consistent with that of massive galaxies at cosmic noon. JWST observations reveal an archetypical rapidly forming massive galaxy undergoing a merger, a clumpy starburst, an episode of obscured near-Eddington quasar activity, and an extremely powerful quasar outflow simultaneously.
研究动机与目标
- 理解在宇宙正午(z ≈ 3)时期,大质量、高尘埃消光的类星体宿主星系中的电离机制。
- 研究类星体驱动外流在加热和电离宿主星系星际介质(ISM)中的作用。
- 表征团块状星暴区域的物理条件,包括电子密度、金属丰度和消光程度。
- 确定激波电离是否可在电离锥之外被探测到,从而揭示广角外流的几何结构。
- 评估类星体光致电离对延伸的Lyα亮斑及邻近星系的贡献程度。
提出的方法
- 利用JWST/NIRSpec积分场单元(IFU)光谱学技术,获取类星体宿主星系及其伴星的空间分辨发射线数据。
- 应用标准发射线诊断图(如[O III]/Hβ、[S II]/Hα)以区分光致电离、激波电离与星暴活动。
- 使用q3dfit软件对IFU数据立方体中的流体动力学与电离结构进行建模。
- 通过巴尔末减量(Hα/Hβ)校正Hα光度的尘埃消光,并推导恒星形成速率。
- 利用[O II]与[O III]线比值绘制金属丰度梯度,假设处于光致电离平衡状态。
- 将空间分辨的线比与模拟结果对比,推断外流几何结构与激波特性的特征。
![Figure 1: On the left, we present line-integrated [O III ] 5007 Å flux in units of $\times 10^{-17}$ erg s -1 cm -2 Å -1 arcsec -2 , in the middle, we present the radial velocity centroid ( $v_{50}$ ) map in units of km s -1 and on the right the velocity dispersion maps for each detected kinematic c](https://ar5iv.labs.arxiv.org/html/2303.06970/assets/figures/OIII_5007_emlin_map.png)
实验结果
研究问题
- RQ1类星体宿主星系及其伴星不同区域的主导电离机制是什么?
- RQ2电离锥之外是否可探测到激波电离区域?这些区域揭示了怎样的外流几何结构?
- RQ3宿主星系中团块状星暴区域的物理条件(密度、金属丰度、消光)如何?
- RQ4类星体光致电离对邻近星系与潮汐结构的延伸影响有多大?
- RQ5类星体驱动外流如何影响宿主星系的ISM与恒星形成活动?
主要发现
- 在电离锥垂直方向检测到外锥区域的激波电离区域,表明类星体外流具有大张角,其影响显著超出直接视线方向。
- 宿主星系至少包含九个尺度为1 kpc的星暴团块,总恒星形成速率不低于200 M⊙ yr⁻¹,符合宇宙正午时期的极端条件特征。
- 星暴团块中的电子密度高达3,000 cm⁻³,显著高于本地星暴星系,V波段消光程度可达3个星等。
- 东北方向星暴区域的氧丰度为太阳值的二分之一至三分之一,且从中心向外呈现正向金属丰度梯度。
- 大多数区域以光致电离为主导,但在电离锥外检测到激波电离,证实类星体风可影响未被类星体直接照亮的气体。
- 类星体光致电离的影响延伸至邻近星系与潮汐尾,支持其在驱动类似类星体周围延伸Lyα亮斑中的关键作用。
![Figure 2: A color composite of ionized gas emission in the J1652 quasar host galaxy and the immediate environment. [O III ] is assigned to blue, H $\alpha$ is assigned to green, [N II ] is assigned to red and [S II ] is assigned to orange. Bar on the left represents 1 arcsecond, and the quasar is lo](https://ar5iv.labs.arxiv.org/html/2303.06970/assets/figures/figure_1b.png)
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