Help Privacy Policy Disclaimer
  Advanced SearchBrowse




Journal Article

Supermassive black holes in cosmological simulations I: MBH − M relation and black hole mass function


Nelson,  Dylan
Galaxy Formation, MPI for Astrophysics, Max Planck Society;

External Resource
No external resources are shared
Fulltext (public)
There are no public fulltexts stored in PuRe
Supplementary Material (public)
There is no public supplementary material available

Habouzit, M., Li, Y., Somerville, R. S., Genel, S., Pillepich, A., Volonteri, M., et al. (2021). Supermassive black holes in cosmological simulations I: MBH − M relation and black hole mass function. Monthly Notices of the Royal Astronomical Society, 503(2), 1940-1975. doi:10.1093/mnras/stab496.

Cite as: http://hdl.handle.net/21.11116/0000-0008-F424-C
The past decade has seen significant progress in understanding galaxy formation and evolution using large-scale cosmological simulations. While these simulations produce galaxies in overall good agreement with observations, they employ different sub-grid models for galaxies and supermassive black holes (BHs). We investigate the impact of the sub-grid models on the BH mass properties of the Illustris, TNG100, TNG300, Horizon-AGN, EAGLE, and SIMBA simulations, focusing on the MBH − M relation and the BH mass function. All simulations predict tight MBH − M relations, and struggle to produce BHs of MBH⩽107.5M in galaxies of M∼1010.5−1011.5M⁠. While the time evolution of the mean MBH − M relation is mild (⁠ΔMBH⩽1dex for 0 ⩽z⩽ 5) for all the simulations, its linearity (shape) and normalization varies from simulation to simulation. The strength of SN feedback has a large impact on the linearity and time evolution for M⩽1010.5M⁠. We find that the low-mass end is a good discriminant of the simulation models, and highlights the need for new observational constraints. At the high-mass end, strong AGN feedback can suppress the time evolution of the relation normalization. Compared with observations of the local Universe, we find an excess of BHs with MBH⩾109M in most of the simulations. The BH mass function is dominated by efficiently accreting BHs (⁠log10fEdd⩾−2⁠) at high redshifts, and transitions progressively from the high-mass to the low-mass end to be governed by inactive BHs. The transition time and the contribution of active BHs are different among the simulations, and can be used to evaluate models against observations.