717 research outputs found
LISA double black holes: Dynamics in gaseous nuclear discs
We study the inspiral of double black holes, with masses in the LISA window
of detectability, orbiting inside a massive circum-nuclear disc. Using
high-resolution SPH simulations, we follow the black hole dynamics in the early
phase when gas-dynamical friction acts on the black holes individually, and
continue our simulation until they form a close binary. We find that in the
early sinking the black holes lose memory of their initial orbital eccentricity
if they co-rotate with the gaseous disc, forming a binary with a low
eccentricity, consistent with zero within our numerical resolution limit. The
cause of circularization resides in the rotation present in the gaseous
background where dynamical friction operates. Circularization may hinder
gravitational waves from taking over and leading the binary to coalescence. In
the case of counter-rotating orbits the initial eccentricity does not decrease,
and the black holes may bind forming an eccentric binary. When dynamical
friction has subsided, for equal mass black holes and regardless their initial
eccentricity, angular momentum loss, driven by the gravitational torque exerted
on the binary by surrounding gas, is nevertheless observable down to the
smallest scale probed. In the case of unequal masses, dynamical friction
remains efficient down to our resolution limit, and there is no sign of
formation of any ellipsoidal gas distribution that may further harden the
binary. During inspiral, gravitational capture of gas by the black holes occurs
mainly along circular orbits: eccentric orbits imply high relative velocities
and weak gravitational focusing. Thus, AGN activity may be excited during the
black hole pairing process and double active nuclei may form when
circularization is completed, on distance-scales of tens of pcs.Comment: Minor changes, accepted to MNRAS (11 pags, 14 figs). Movies (.avi)
are available at http://pitto.mib.infn.it/~haardt/MOVIES
Unresolved X-ray background: clues on galactic nuclear activity at z>6
We study, by means of dedicated simulations of massive black hole build-up,
the possibility to constraint the existence and nature of the AGN population at
z>6 with available and planned X-ray and near infrared space telescopes. We
find that X-ray deep-field observations can set important constraints to the
faint-end of the AGN luminosity function at very high redshift. Planned X-ray
telescopes should be able to detect AGN hosting black holes with masses down to
>10^5 Msun (i.e., X-ray luminosities in excess of 10^42 erg s^-1), and can
constrain the evolution of the population of massive black hole at early times
(6<z<10). We find that this population of AGN should contribute substantially
(~25%) to the unresolved fraction of the cosmic X-ray background in the 0.5-10
keV range, and that a significant fraction (~3-4%) of the total background
intensity would remain unaccounted even after future X-ray observations. As
byproduct, we compute the expected UV background from AGN at z>6 and we discuss
the possible role of AGN in the reionization of the Universe at these early
epochs, showing that AGN alone can provide enough ionizing photons only in the
(improbable) case of an almost completely homogeneous inter-galactic medium.
Finally, we show that super-Eddington accretion, suggested by the observed QSOs
at z>6, must be a very rare event, confined to black holes living in the
highest density peaks.Comment: 9 pages, 7 figures, MNRAS in pres
Hypervelocity stars and the environment of Sgr A*
Hypervelocity stars (HVSs) are a natural consequence of the presence of a
massive nuclear black hole (Sgr A*) in the Galactic Center. Here we use the
Brown et al. sample of unbound and bound HVSs together with numerical
simulations of the propagation of HVSs in the Milky Way halo to constrain three
plausible ejection mechanisms: 1) the scattering of stars bound to Sgr A* by an
inspiraling intermediate-mass black hole (IMBH); 2) the disruption of stellar
binaries in the tidal field of Sgr A*; and 3) the two-body scattering of stars
off a cluster of stellar-mass black holes orbiting Sgr A*. We compare the
predicted radial and velocity distributions of HVSs with the limited-statistics
dataset currently available, and show that the IMBH model appears to produce a
spectrum of ejection velocities that is too flat. Future astrometric and deep
wide-field surveys of HVSs should shed unambiguous light on the stellar
ejection mechanism and probe the Milky Way potential on scales as large as 200
kpc.Comment: 5 pages, 5 figures, accepted for publication in MNRAS letter
Growing massive black holes through super-critical accretion of stellar-mass seeds
The rapid assembly of the massive black holes that power the luminous quasars
observed at remains a puzzle. Various direct collapse models have
been proposed to head-start black hole growth from initial seeds with masses
, which can then reach a billion solar mass while
accreting at the Eddington limit. Here we propose an alternative scenario based
on radiatively inefficient super-critical accretion of stellar-mass holes
embedded in the gaseous circum-nuclear discs (CNDs) expected to exist in the
cores of high redshift galaxies. Our sub-pc resolution hydrodynamical
simulations show that stellar-mass holes orbiting within the central 100 pc of
the CND bind to very high density gas clumps that arise from the fragmentation
of the surrounding gas. Owing to the large reservoir of dense cold gas
available, a stellar-mass black hole allowed to grow at super-Eddington rates
according to the "slim disc" solution can increase its mass by 3 orders of
magnitudes within a few million years. These findings are supported by
simulations run with two different hydro codes, RAMSES based on the Adaptive
Mesh Refinement technique and GIZMO based on a new Lagrangian Godunov-type
method, and with similar, but not identical, sub-grid recipes for star
formation, supernova feedback, black hole accretion and feedback. The low
radiative efficiency of super-critical accretion flows are instrumental to the
rapid mass growth of our black holes, as they imply modest radiative heating of
the surrounding nuclear environment.Comment: 12 pages, 8 figures, 2 tables. Accepted for publication in MNRA
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