2508.21748v1
A direct black hole mass measurement in a Little Red Dot at the Epoch of Reionization
First listed 2025-08-29 | Last updated 2025-09-01
Abstract
Recent discoveries of faint active galactic nuclei (AGN) at the redshift frontier have revealed a plethora of broad \Halpha emitters with optically red continua, named Little Red Dots (LRDs), which comprise 15-30\% of the high redshift broad line AGN population. Due to their peculiar spectral properties and X-ray weakness, modeling LRDs with standard AGN templates has proven challenging. In particular, the validity of single-epoch virial mass estimates in determining the black hole (BH) masses of LRDs has been called into question, with some models claiming that masses might be overestimated by up to 2 orders of magnitude, and other models claiming that LRDs may be entirely stellar in nature. We report the direct, dynamical BH mass measurement in a strongly lensed LRD at $z = 7.04$. 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 BH mass estimates from the Balmer lines. The Keplerian rotation leaves little room for any stellar component in a host galaxy, as we conservatively infer $M_{\rm BH}/M_{*}>2$. Such a ''naked'' black hole, together with its near-pristine environment, indicates that this LRD is a massive black hole seed caught in its earliest accretion phase.
Short digest
Strong lensing plus JWST/NIRSpec IFS resolves narrow Hα kinematics and spectroastrometric shifts in the lensed Little Red Dot Abell2744‑QSO1 at z=7.04, enabling a direct rotation curve from ~10–200 pc. The curve is Keplerian and rules out compact extended mass profiles (e.g., MW‑like nuclear star cluster, Plummer, or a DM cusp), implying a central point mass of order 5×10^7 M⊙ consistent with Balmer‑line virial estimates. The inferred stellar content is minimal, with MBH/M* > 2, pointing to a near‑“naked” black hole in a pristine environment. This result validates virial BH masses for LRDs at the EoR and captures a massive BH seed in its earliest growth phase.
Key figures to inspect
- Fig. 1 (narrow Hα maps): Inspect the flux, velocity, and dispersion maps to see the ~200 pc spatial extent, the ~10 km s−1 velocity gradient, and the offset between the broad‑line centroid and the dynamical center—evidence the gradient is real (not slicer PA artefacts).
- Fig. 2 (top, rotation curve): Compare binned narrow‑Hα node velocities with the spectroastrometric points; note the strong preference for a point‑mass fit (χR^2≈0.8) over an MW‑like nuclear star cluster (χR^2≈3.8), yielding log MBH/M⊙≈6.94 as a lower limit due to unknown inclination.
- Fig. 2 (bottom, residuals): The full 2D MOKA3D fits show far smaller residuals for Keplerian rotation than for extended‑mass models—key visual proof that an NSC/Plummer profile cannot reproduce the field.
- Extended Data Fig. 1 (spectroastrometry): The +/−50 km s−1 Hα centroids are separated by 24.9±9.4 pc, implying rspec≈12.5 pc; with FWHM≈52±14 km s−1 this encloses log M/M⊙≈6.90—anchoring the inner mass scale.
- Extended Data Fig. 2 (cluster concentration limits): Upper limit Rc≲0.2 pc places any putative NSC >1 dex more concentrated than known NSCs or early star clusters, reinforcing that the mass must be a BH.
Discussion
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