FIR Luminous Quasars at z ~ 6

There are ~400 quasars at z > 5.7 are published. These high-redshift quasars provide unique labs to investigate the co-evolution of the first SMBHs and their host galaxies at the end of the re-ionization epoch. To study the co-evolution of the SMBHs and their host galaxies, there are two aspects, one is to find ways to improve the estimation of the mass of the central BHs, and the other is to investigate the host galaxy properties though the ISM such as the dust, molecular and ionized gas. There still some open questions in this field: Do these luminous quasars at the earliest epoch form through major galaxy mergers? What are the typical physical conditions and dynamics of the ISM in the nuclear region that is powered by both the luminous AGN and the intense star formation? How is the SMBH-bulge relationship established via host galaxy star formation and AGN feedback at early stage of evolution? We are trying to solve these problems from the aspact of quasar host galaxies.

◈ Resolved Interstellar Medium at z ~ 6 (Shao et al. 2022)

Notes - Resolved ISM at z ~ 6.

◈ Gas Outflow in Early Universe (Shao et al. 2022)

Notes - OH+ P-Cygni profile indicates outflow at z ~ 6.

◈ Quasar-starburst System Dynamics in the Reionization Epoch (Shao et al. 2022)

Notes - Dynamical modelling. The black hole mass can be estimated in case that the angular resolution can zoom in the black hole sphere of influence.

◈ Gas Kinematics of FIR Luminous z ~ 6 Quasars Revealed by ALMA High Resolution Observations (Shao et al. 2017; Shao et al. 2022)

Notes - Gas kinematic modelling.

◈ The Star Formation in the Host Galaxy of the FIR Luminous Quasar J2310+1855 at z = 6.00 with Herschel and ALMA FIR photometries (Shao et al. 2019)

Notes - SED decomposition toward quasar J2310+1855 at z = 6.00.

◈ The Molecular CO in FIR Luminous Quasars at z ~ 6 Revealed by the VLA (Shao et al. 2019)

Notes - CO (2-1) line of three FIR luminouse quasars at z ~ 6.

◈ Deep HST Near-infrared Imaging of the Luminous Quasar - ULAS J1319+0950 at z = 6.13 (Shao et al. 2022 in prep.)