EIGER. VI. The Correlation Function, Host Halo Mass, and Duty Cycle of Luminous Quasars at z ≳ 6
We expect luminous ( M _1450 ≲ −26.5) high-redshift quasars to trace the highest-density peaks in the early Universe. Here, we present observations of four z ≳ 6 quasar fields using JWST/NIRCam in the imaging and wide-field slitless spectroscopy mode and report a wide range in the number of detected...
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| Main Authors: | , , , , , , , , , , , , , , , |
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| Format: | Article |
| Language: | English |
| Published: |
IOP Publishing
2024-01-01
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| Series: | The Astrophysical Journal |
| Subjects: | |
| Online Access: | https://doi.org/10.3847/1538-4357/ad778b |
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| Summary: | We expect luminous ( M _1450 ≲ −26.5) high-redshift quasars to trace the highest-density peaks in the early Universe. Here, we present observations of four z ≳ 6 quasar fields using JWST/NIRCam in the imaging and wide-field slitless spectroscopy mode and report a wide range in the number of detected [O iii ]-emitting galaxies in the quasars’ environments, ranging between a density enhancement of δ ≈ 65 within a 2 cMpc radius—one of the largest protoclusters during the Epoch of Reionization discovered to date—to a density contrast consistent with zero, indicating the presence of a UV-luminous quasar in a region comparable to the average density of the Universe. By measuring the two-point cross-correlation function of quasars and their surrounding galaxies, as well as the galaxy autocorrelation function, we infer a correlation length of quasars at 〈 z 〉 = 6.25 of ${r}_{0}^{\mathrm{QQ}}={22.0}_{-2.9}^{+3.0}\,\mathrm{cMpc}\,{h}^{-1}$ , while we obtain a correlation length of the [O iii ]-emitting galaxies of ${r}_{0}^{\mathrm{GG}}=4.1\,\pm 0.3\,\mathrm{cMpc}\,{h}^{-1}$ . By comparing the correlation functions to dark-matter-only simulations we estimate the minimum mass of the quasars’ host dark matter halos to be ${\mathrm{log}}_{10}({M}_{\mathrm{halo},\min }/{M}_{\odot })={12.43}_{-0.15}^{+0.13}$ (and ${\mathrm{log}}_{10}({M}_{\mathrm{halo},\min }^{[\mathrm{OIII}]}/{M}_{\odot })\,={10.56}_{-0.03}^{+0.05}$ for the [O iii ] emitters), indicating that (a) luminous quasars do not necessarily reside within the most overdense regions in the early Universe, and that (b) the UV-luminous duty cycle of quasar activity at these redshifts is f _duty ≪ 1. Such short quasar activity timescales challenge our understanding of early supermassive black hole growth and provide evidence for highly dust-obscured growth phases or episodic, radiatively inefficient accretion rates. |
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| ISSN: | 1538-4357 |