Revealing the Accretion Physics of Supermassive Black Holes at z ∼ 7 with Chandra

Context

Quasars, the most luminous type of active galactic nuclei (AGN), are believed to be powered by accreting supermassive black holes (SMBHs). The continuum and line emissions from luminous quasars, over a large wavelength range, from optical-infrared to X-ray, carry crucial insights into the accrection and growth of the central SMBHs. We are performing a Chandra X-ray survey of the first uniform and complete sample of luminous quasars at z>6.5. Together with quasar luminosity function and black hole mass function that we are measuring from deep optical-to-infrared observations, the Chandra X-ray observations will provide key constraints to the formation and growth history of the earliest SMBHs. Our Chandra programs, combined with the infrared spectroscopy of a larger sample will allow us to carry out the first statistical measurement of X-ray properties of z>6.5 quasars, to probe the evolution of X-ray slope, spectral energy distribution and accretion rate of early quasars. See Wang+2021 for more details about our Cycle 19 observations.

Science Goals

  • Evolution of quasar X-ray spectral shape, broad-band SED, and accretion rate.
  • X-ray properties of a diverse quasar population.
  • The environment of the most overdense structure traced by quasars.
  • Legacy deep fields with multi-wavelegnth coverage (X-ray, optical, infrared, sub-mm and radio).

Observations

  • In cycle 19, we were awared 130ks (ID:19700283) for observing five brightest z > 6.5 quasars
  • In cycle 22, we were awared 710ks (ID:22700552) for observing seven z ~ 7 quasars
  • In cycle 23, we were awared 900ks (ID:23700397) for obtaining a deep exposure for a protocluster anchored by a z~6.6 quasar
  • All the targets will be observed with JWST, ALMA and other ground-based telesccopes

Targets

The following table lists all the z>6.5 quasars observed (or will be observed) by Chandra observatory. More details will come soon.

Chandra Observed z>6.5 Quasars
Name Redshift M1450 MBH(109M⊙) texp(ks) Obs. Cycle L2-10kev(1044erg/s) Reference
J002429.77+391319.0 6.6210 −25.62 0.27 19.70 19 <15.74 Wang+2021
J022426.54−471129.4 6.5223 −26.67 1.30 17.72 19 35.26 Wang+2021
J022601.87+030259.3 6.5412 −27.26 2.20 25.90 19 6.73 Wang+2021; Vito+2019
J030516.92−315056.0 6.6145 −26.11 0.70 49.88 19 <4.18 Wang+2021; Vito+2019
J104819.09−010940.2 6.6759 −26.03 0.79 34.76 19 <5.02 Wang+2021
J111033.96−132945.6 6.5148 −25.35 0.38 59.33 19 <4.86 Wang+2021; Vito+2019
J112001.48+064124.3 7.0842 −26.45 1.40 15.84 12 8.52 Wang+2021; Page+2014
J134208.11+092838.6 7.5413 −26.65 0.86 45.11 18 12.80 Wang+2021; Banados+2018
J213233.19+121755.3 6.5850 −27.08 0.62 17.82 19 31.32 Wang+2021
J223255.15+293032.0 6.6580 −26.34 2.91 54.21 19 4.68 Wang+2021; Vito+2019
J234833.34−305410.0 6.9018 −25.84 1.60 42.50 19 <7.96 Wang+2021
J003836.10−152723.6 7.0340 −27.13 1.36 100 22 TBD In prep
J025216.60−050331.8 7.0006 −26.63 1.28 120 22 TBD In prep
J041128.60−090749.7 6.8260 −26.58 0.95 120 22 TBD In prep
J070626.40+292105.5 6.6037 −27.44 2.11 50 22 TBD In prep
J091054.50−041406.8 6.6363 −26.61 3.59 900 23 TBD In prep
J092347.10+040254.6 6.6330 −26.68 1.77 100 22 TBD In prep
J100758.26+211529.2 7.5149 −26.73 1.43 120 22 TBD In prep
J110421.50+213428.8 6.7662 −26.63 1.69 100 22 TBD In prep