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BlackTHUNDER strikes twice: rest-frame Balmer-line absorption and high Eddington accretion rate in a Little Red Dot at $z=7.04$

Francesco D'Eugenio, Roberto Maiolino, Michele Perna, Hannah Uebler, Xihan Ji, William McClymont, Sophie Koudmani, Debora Sijacki, Ignas Juodžbalis, Jan Scholtz, Jake Bennett, Andrew J. Bunker, Stefano Carniani, Stéphane Charlot, Giovanni Cresci, Emma Curtis-Lake, Elena Dalla Bontà, Gareth C. Jones, Jianwei Lyu, Alessandro Marconi, Giovanni Mazzolari, Erica J. Nelson, Eleonora Parlanti, Brant E. Robertson, Raffaella Schneider, Charlotte Simmonds, Sandro Tacchella, Giacomo Venturi, Chris Willott, Joris Witstok, Callum Witten

Abstract

JWST spectroscopy has revealed a population of compact objects at redshifts $z=2$-9 with `v'-shaped spectral energy distributions, broad permitted lines, and, often, hydrogen Balmer absorption. Among these `Little Red Dots' (LRDs), Abell2744-QSO1 at $z=7.04$ has been confirmed to have time-variable equivalent width (EW) in its broad emission lines, confirming its AGN nature. We extend the analysis of NIRSpec/IFS data from the BlackTHUNDER survey to the H$α$ line. The broad-line profile in Abell2744-QSO1 is manifestly non-Gaussian, requiring at least two Gaussian components with full width at half maximum FWHM=$450\pm50$ and $1800\pm100$ km s$^{-1}$. Crucially, we also detect a narrow-line Gaussian component, and strong H$α$ absorption (EW relative to the continuum $\approx 30^{+15}_{-9}$ A), confirming a connection between the strong Balmer break and line absorption. The absorber is at rest with respect to broad H$α$, suggesting that the gas cannot be interpreted as an inflow or outflow, forming instead a long-lived structure. Its velocity dispersion is $σ_{abs} = 100\pm10$ km s$^{-1}$, consistent with the value inferred from the analysis of the Balmer break. Based on H$α$, we infer a black hole mass of log(M$_{BH}$/M$_\odot$)=6.3-6.7, 0.9-1.3 dex smaller than previous estimates based on H$β$. The Eddington ratio is 0.7-1.6. Combining the high signal-to-noise ratio of the narrow H$α$ line with the spectral resolution R=3,700 of the G395H grating, we infer a narrow-line dispersion $σ_n = 22^{+5}_{-6}$ km s$^{-1}$, which places a stringent constraint on the black-hole-to-dynamical-mass ratio of this system to be M$_{BH}$/M$_{dyn}$>0.02-0.4. If M$_{BH}$ is near the low-mass end of our estimates, the SMBH would be accreting at a super-Eddington rate. Alternatively, at the high-M$_{BH}$ end, there would be minimal room for a host galaxy.

BlackTHUNDER strikes twice: rest-frame Balmer-line absorption and high Eddington accretion rate in a Little Red Dot at $z=7.04$

Abstract

JWST spectroscopy has revealed a population of compact objects at redshifts -9 with `v'-shaped spectral energy distributions, broad permitted lines, and, often, hydrogen Balmer absorption. Among these `Little Red Dots' (LRDs), Abell2744-QSO1 at has been confirmed to have time-variable equivalent width (EW) in its broad emission lines, confirming its AGN nature. We extend the analysis of NIRSpec/IFS data from the BlackTHUNDER survey to the H line. The broad-line profile in Abell2744-QSO1 is manifestly non-Gaussian, requiring at least two Gaussian components with full width at half maximum FWHM= and km s. Crucially, we also detect a narrow-line Gaussian component, and strong H absorption (EW relative to the continuum A), confirming a connection between the strong Balmer break and line absorption. The absorber is at rest with respect to broad H, suggesting that the gas cannot be interpreted as an inflow or outflow, forming instead a long-lived structure. Its velocity dispersion is km s, consistent with the value inferred from the analysis of the Balmer break. Based on H, we infer a black hole mass of log(M/M)=6.3-6.7, 0.9-1.3 dex smaller than previous estimates based on H. The Eddington ratio is 0.7-1.6. Combining the high signal-to-noise ratio of the narrow H line with the spectral resolution R=3,700 of the G395H grating, we infer a narrow-line dispersion km s, which places a stringent constraint on the black-hole-to-dynamical-mass ratio of this system to be M/M>0.02-0.4. If M is near the low-mass end of our estimates, the SMBH would be accreting at a super-Eddington rate. Alternatively, at the high-M end, there would be minimal room for a host galaxy.

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