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BASS XXXVII: The role of radiative feedback in the growth and obscuration properties of nearby supermassive black holes

Authors :
Ricci, C.
Ananna, T. T.
Temple, M. J.
Urry, C. M.
Koss, M. J.
Trakhtenbrot, B.
Ueda, Y.
Stern, D.
Bauer, F. E.
Treister, E.
Privon, G. C.
Oh, K.
Paltani, S.
Stalevski, M.
Ho, L. C.
Fabian, A. C.
Mushotzky, R.
Chang, C. S.
Ricci, F.
Kakkad, D.
Sartori, L.
Baer, R.
Caglar, T.
Powell, M.
Harrison, F.
Ricci, C.
Ananna, T. T.
Temple, M. J.
Urry, C. M.
Koss, M. J.
Trakhtenbrot, B.
Ueda, Y.
Stern, D.
Bauer, F. E.
Treister, E.
Privon, G. C.
Oh, K.
Paltani, S.
Stalevski, M.
Ho, L. C.
Fabian, A. C.
Mushotzky, R.
Chang, C. S.
Ricci, F.
Kakkad, D.
Sartori, L.
Baer, R.
Caglar, T.
Powell, M.
Harrison, F.
Publication Year :
2022

Abstract

We study the relation between obscuration and supermassive black hole (SMBH) growth using a large sample of hard X-ray selected Active Galactic Nuclei (AGN). We find a strong decrease in the fraction of obscured sources above the Eddington limit for dusty gas ($\log \lambda_{\rm Edd}\gtrsim -2$) confirming earlier results, and consistent with the radiation-regulated unification model. This also explains the difference in the Eddington ratio distribution functions (ERDFs) of type 1 and type 2 AGN obtained by a recent study. The break in the ERDF of nearby AGN is at $\log \lambda_{\rm Edd}^{*}=-1.34\pm0.07$. This corresponds to the $\lambda_{\rm Edd}$ where AGN transition from having most of their sky covered by obscuring material to being mostly devoid of absorbing material. A similar trend is observed for the luminosity function, which implies that most of the SMBH growth in the local Universe happens when the AGN is covered by a large reservoir of gas and dust. These results could be explained with a radiation-regulated growth model, in which AGN move in the $N_{\rm H}-\lambda_{\rm Edd}$ plane during their life cycle. The growth episode starts with the AGN mostly unobscured and accreting at low $\lambda_{\rm Edd}$. As the SMBH is further fueled, $\lambda_{\rm Edd}$, $N_{\rm H}$ and covering factor increase, leading AGN to be preferentially observed as obscured. Once $\lambda_{\rm Edd}$ reaches the Eddington limit for dusty gas, the covering factor and $N_{\rm H}$ rapidly decrease, leading the AGN to be typically observed as unobscured. As the remaining fuel is depleted, the SMBH goes back into a quiescent phase.<br />Comment: Accepted for publication in ApJ

Details

Database :
OAIster
Publication Type :
Electronic Resource
Accession number :
edsoai.on1363569533
Document Type :
Electronic Resource
Full Text :
https://doi.org/10.3847.1538-4357.ac8e67