A small and vigorous black hole in the early Universe
A small and vigorous black hole in the early Universe
Jan 17, 2024·,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,
Roberto Maiolino
Jan Scholtz
Joris Witstok
Stefano Carniani
Francesco D'Eugenio
Anna De Graaff
Hannah Übler
Sandro Tacchella
Emma Curtis-Lake
Santiago Arribas
Andrew Bunker
Stéphane Charlot
Jacopo Chevallard
Mirko Curti
Tobias J. Looser
Michael v. Maseda
Timothy D. Rawle
Bruno Rodrı́guez Del Pino
Chris J. Willott
Eiichi Egami
Daniel J. Eisenstein
Kevin N. Hainline
Brant Robertson
Christina C. Williams
Christopher N. A. Willmer
William M. Baker
Kristan Boyett
Christa DeCoursey
Andrew C. Fabian
Jakob M. Helton
Zhiyuan Ji
Gareth C. Jones
Nimisha Kumari
Nicolas Laporte
Erica J. Nelson
Michele Perna
Lester Sandles
Irene Shivaei
Fengwu Sun
Abstract
Several theories have been proposed to describe the formation of black hole seeds in the early Universe and to explain the emergence of very massive black holes observed in the first thousand million years after the Big Bang. Models consider different seeding and accretion scenarios, which require the detection and characterization of black holes in the first few hundred million years after the Big Bang to be validated. Here we present an extensive analysis of the JWST-NIRSpec spectrum of GN-z11, an exceptionally luminous galaxy at $z = 10.6$
, revealing the detection of the $\mathrm{[NeIV]}\lambda2423$
and $\mathrm{CII}^{\ast}\lambda1335$
transitions (typical of active galactic nuclei), as well as semi-forbidden nebular lines tracing gas densities higher than $10^{9}\ \mathrm{cm}^{-3}$
, typical of the broad line region of active galactic nuclei. These spectral features indicate that GN-z11 hosts an accreting black hole. The spectrum also reveals a deep and blueshifted $\mathrm{CIV}\lambda1549$
absorption trough, tracing an outflow with velocity $800-1,000\ \mathrm{km/s}$
, probably driven by the active galactic nucleus. Assuming local virial relations, we derive a black hole mass of $\mathrm{log}_{10}(M_{\mathrm{BH}}/M_{\odot}) = 6.2 \pm 0.3$
, accreting at about five times the Eddington rate. These properties are consistent with both heavy seeds scenarios and scenarios considering intermediate and light seeds experiencing episodic super-Eddington phases. Our finding explains the high luminosity of GN-z11 and can also provide an explanation for its exceptionally high nitrogen abundance.
Type
Publication
Nature, Volume 627, Issue 8002, pages 59-63
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