Issue |
A&A
Volume 526, February 2011
|
|
---|---|---|
Article Number | A13 | |
Number of page(s) | 6 | |
Section | Cosmology (including clusters of galaxies) | |
DOI | https://doi.org/10.1051/0004-6361/200913649 | |
Published online | 14 December 2010 |
Black holes and galactic density cusps
From black hole to bulge
1
Instituto de Física Teórica UAM/CSIC, Facultad de Ciencias, C-XI,
Universidad Autónoma de Madrid Cantoblanco,
28049
Madrid,
Spain
e-mail: Morgan.LeDelliou@uam.es
2
Queen’s University, Kingston, Ontario, Canada
e-mail: henriksn@astro.queensu.ca
3
Faculty of Science, University of Ontario Institute of Technology,
Oshawa, L1H 7K4
Ontario,
Canada
e-mail: joseph.macmillan@gmail.com
Received:
11
November
2009
Accepted:
26
October
2010
Aims. In this paper we continue our study of density cusps that may contain central black holes.
Methods. Our previous thus attempts to use distribution functions with a memory of self-similar relaxation apply mainly in restricted regions of the global system. We are forced to consider related distribution functions that are steady but not self-similar.
Results. One remarkably simple distribution function that has a filled loss cone describes a bulge that transits from a near black hole domain to an outer “zero flux” regime where ρ ∝ r−7/4. The transition passes from an initial inverse square profile through a region having a 1/r density profile. The structure is likely to be developed at an early stage in the growth of a galaxy. A central black hole is shown to grow exponentially in this background with an e-folding time of a few million years.
Conclusions. We derive our results from first principles, using only the angular momentum integral in spherical symmetry. The initial relaxation probably requires bar instabilities and clump-clump interactions.
Key words: cosmology: theory / dark matter / galaxies: halos / galaxies: nuclei / black hole physics / gravitation
© ESO, 2010
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