SIMBAD references

The most massive black holes observed in the universe weigh up to ∼10¹⁰ M_☉, nearly independent of redshift. Reaching these final masses likely required copious accretion and several major mergers. Employing a dynamical approach that rests on the role played by a new, relevant physical scale-the transition radius-we provide a theoretical calculation of the maximum mass achievable by a black hole seed that forms in an isolated halo, one that scarcely merged. Incorporating effects at the transition radius and their impact on the evolution of accretion in isolated halos, we are able to obtain new limits for permitted growth. We find that large black hole seeds (M_* >= 10⁴ M_☉) hosted in small isolated halos (M_h <= 10⁹ M_☉) accreting with relatively small radiative efficiencies (ε <= 0.1) grow optimally in these circumstances. Moreover, we show that the standard M_*-σ relation observed at z ∼ 0 cannot be established in isolated halos at high-z, but requires the occurrence of mergers. Since the average limiting mass of black holes formed at z >= 10 is in the range 10^4–6 M_☉, we expect to observe them in local galaxies as intermediate-mass black holes, when hosted in the rare halos that experienced only minor or no merging events. Such ancient black holes, formed in isolation with subsequent scant growth, could survive, almost unchanged, until present.