Abstract

(ABRIDGED) We present a model in which the seeds of supermassive black holes form from the lowest angular momentum gas in proto-galaxies at high redshift. We show that this leads to a correlation between black hole masses and spheroid properties, as observed today. We assume that gas in early-forming, rare halos has a distribution of specific angular momentum similar to that expected for dark matter halos. This distribution has a significant low angular momentum tail which implies that every proto-galaxy should contain gas that ends up in a high-density disc. In halos more massive than a critical threshold of \~10^8Msun, the discs are gravitationally unstable, and experience an efficient Lin-Pringle viscosity that allows mass inflow. This process continues until the first massive stars disrupt the disc. Black holes are created with a characteristic mass of ~10^5 Msun, independent of the redshift of formation. This serves as a lower bound for black-hole masses in galaxies today. The comoving mass density of black hole seeds grows with time, and saturates when cosmic reionization stops gas cooling in these low-mass systems. By z~15, the comoving mass density becomes comparable to that inferred from observations, with room for appropriate additional luminous growth during a later quasar accretion phase. Hierarchical merging after z~15 naturally leads to a linear correlation between black-hole mass and stellar spheroid mass, with negligible black hole masses in disc-dominated galaxies.

Highlights

  • Detailed studies of gas and stellar kinematics near the centers of present-day galaxies have revealed that almost all galaxy spheroids host super-massive black holes, with masses Mbh = (106 − 109)M⊙, or ∼ 10−4 of the total stellar mass of their parent galaxies (e.g. Kormendy & Gebhardt 2001; Ferrarese & Merritt 2000; Magorrian et al 1998)

  • We presented a physical model for the production of massive seed black holes at high redshifts, with a characteristic mass ∼ 105M⊙

  • Massive seeds may help explain the existence of the supermassive black holes associated with luminous Active Galactic Nuclei (AGN) at z>∼ 6

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Summary

INTRODUCTION

The situation may get even worse at earlier times because the typical collapsing mass M⋆(a) is smaller in proportion to a high power of the expansion factor a ≡ (1 + z)−1 This implies that the ratio of the centrifugally supported size (∝ aM⋆(a)1/3) to the Schwarzschild radius (∝ M⋆(a) if the black hole mass is a constant fraction of the halo mass) increases dramatically at early times, unless the sites of black hole formation are rare haloes much more massive than M⋆(a). This line of argument indicates that the seed black holes originate from material at the very lowest end of the angular-momentum distribution within rare, massive haloes at high redshift.

SPIN DISTRIBUTION AND DISC PROFILE
ANGULAR MOMENTUM LOSS
Critical halo mass for viscous transport
Viscous inflow
MASS FUNCTION OF SEED BLACK HOLES
TOTAL MASS IN SEED BLACK HOLES
BLACK HOLES AND SPHEROIDS
Findings
CONCLUSION
Full Text
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