<p>Recent discoveries of faint active galactic nuclei (AGN) at the redshift frontier have revealed a plethora of broad Hα emitters with optically red continua, named little red dots (LRDs)<sup><CitationRef CitationID="CR1">1</CitationRef></sup>, which comprise 15–30% of the high-redshift broad-line AGN population<sup><CitationRef CitationID="CR2">2</CitationRef></sup>. Owing to their peculiar properties<sup><CitationRef AdditionalCitationIDS="CR4 CR5" CitationID="CR3">3</CitationRef>–<CitationRef CitationID="CR6">6</CitationRef></sup>, modelling LRDs with standard AGN scenarios has proven challenging. In particular, the validity of single-epoch virial mass estimates in determining the black-hole masses of LRDs has been called into question, with some models claiming that masses might be overestimated by up to two orders of magnitude<sup><CitationRef AdditionalCitationIDS="CR8 CR9" CitationID="CR7">7</CitationRef>–<CitationRef CitationID="CR10">10</CitationRef></sup>. Here we report a direct, dynamical black-hole mass measurement in a strongly lensed LRD at a&#xa0;redshift&#xa0;of 7.04. The combination of lensing with deep spectroscopic data reveals a rotation curve that is inconsistent with a nuclear star cluster, yet can be well explained by Keplerian rotation around a point mass of 50 million solar masses, consistent with virial black-hole mass estimates. The Keplerian rotation leaves little room for any stellar component in a host galaxy, as we conservatively infer <i>M</i><sub>BH</sub>/<i>M</i><sub>⁎</sub>&#xa0;&gt;&#xa0;2 (where <i>M</i><sub>BH</sub> is the black-hole mass and <i>M</i><sub>⁎</sub> is the stellar mass). Such a ‘naked’ black hole, together with its near-pristine environment<sup><CitationRef CitationID="CR11">11</CitationRef></sup>, indicates that this LRD is a massive black-hole seed caught in its earliest accretion phase.</p>

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A direct black-hole mass measurement in a little red dot at high redshift

  • Ignas Juodžbalis,
  • Cosimo Marconcini,
  • Francesco D’Eugenio,
  • Roberto Maiolino,
  • Alessandro Marconi,
  • Hannah Übler,
  • Jan Scholtz,
  • Xihan Ji,
  • Gareth C. Jones,
  • Michele Perna,
  • Santiago Arribas,
  • Jake S. Bennett,
  • Volker Bromm,
  • Andrew J. Bunker,
  • Stefano Carniani,
  • Stéphane Charlot,
  • Giovanni Cresci,
  • Pratika Dayal,
  • Eiichi Egami,
  • Andrew Fabian,
  • Kohei Inayoshi,
  • Yuki Isobe,
  • Lucy R. Ivey,
  • Sophie Koudmani,
  • Nicolas Laporte,
  • Boyuan Liu,
  • Jianwei Lyu,
  • Giovanni Mazzolari,
  • Stephanie Monty,
  • Eleonora Parlanti,
  • Pablo G. Pérez-González,
  • Brant Robertson,
  • Raffaella Schneider,
  • Debora Sijacki,
  • Sandro Tacchella,
  • Alessandro Trinca,
  • Rosa Valiante,
  • Marta Volonteri,
  • Joris Witstok,
  • Saiyang Zhang

摘要

Recent discoveries of faint active galactic nuclei (AGN) at the redshift frontier have revealed a plethora of broad Hα emitters with optically red continua, named little red dots (LRDs)1, which comprise 15–30% of the high-redshift broad-line AGN population2. Owing to their peculiar properties36, modelling LRDs with standard AGN scenarios has proven challenging. In particular, the validity of single-epoch virial mass estimates in determining the black-hole masses of LRDs has been called into question, with some models claiming that masses might be overestimated by up to two orders of magnitude710. Here we report a direct, dynamical black-hole mass measurement in a strongly lensed LRD at a redshift of 7.04. The combination of lensing with deep spectroscopic data reveals a rotation curve that is inconsistent with a nuclear star cluster, yet can be well explained by Keplerian rotation around a point mass of 50 million solar masses, consistent with virial black-hole mass estimates. The Keplerian rotation leaves little room for any stellar component in a host galaxy, as we conservatively infer MBH/M > 2 (where MBH is the black-hole mass and M is the stellar mass). Such a ‘naked’ black hole, together with its near-pristine environment11, indicates that this LRD is a massive black-hole seed caught in its earliest accretion phase.