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Overmassive No More: The Case for Little Red Dots Hosting Black Hole Seeds as Massive as Single Supermassive Stars

Published 8 Sep 2026 in astro-ph.GA, astro-ph.CO, astro-ph.HE, and astro-ph.SR | (2609.09274v1)

Abstract: Little Red Dots (LRDs) display singular properties unlike any known class of AGN or galaxies, motivating novel mass estimators for their central engines. Inspired by their similarities to stellar phenomena, here we interpret the LRD continuum as being produced by a pseudo-photosphere. We fit tailored stellar atmosphere models to host-subtracted LRD central engines ("black hole stars," BH*s) represented by stacks of $117$ objects. Typical BH* continuum spectra are well fit by models in a narrow range of temperatures (Teff≈4200−4800T_{\rm eff}\approx4200-4800 K), with bolometric luminosities ≈10<sup>43−45\approx10<sup>{43-45} erg s<sup>−1<sup>{-1}, implying pseudo-photospheric radii ≈700−2000\approx700-2000 au. Based on these parameters, we explore four different approaches to deriving BH* masses: 1) using the surface gravity from atmosphere models; 2) appealing to the resemblance to super-Eddington phenomena; 3) approximating the escape velocity from the outflowing material; and 4) exploiting the lack of variability to bound the dynamical time. For the typical BH*, all of these methods yield remarkably consistent masses of ≈10<sup>4−5 M⊙\approx10<sup>{4-5}\,M_\odot, implying a highly super-Eddington luminosity of Lbol/LEdd∼5−50L_{\rm{bol}}/L_{\rm{Edd}}\sim5-50. These mass estimates place BH*s within the scatter of the local scaling relation between black hole mass and host galaxy stellar mass, providing a self-consistent alternative to "overmassive" black holes that lie $2-3$ dex above it. Crucially, our derived masses are consistent with BH*s arising from single supermassive stars (SMSs), whose masses cannot exceed ≈10<sup>5−6 M⊙\approx10<sup>{5-6}\,M_\odot due to general relativistic instabilities. Furthermore, for our derived Lbol/LEddL_{\rm bol}/L_{\rm Edd}, the sharp cutoff of the LRD luminosity function matches the maximum theoretical mass of an SMS. With LRDs, we may therefore be directly observing the birth of heavy black hole seeds.

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