Coupled spheroid and black-hole formation, and the multifrequency detectability of active galactic nuclei and submillimetre sources

Details Coupled spheroid and black-hole formation, and the multifrequency detectability of active galactic nuclei and submillimetre sources Coupled spheroid and black-hole formation, and the multifrequency detectability of active galactic nuclei and submillimetre sources

2001-08-07

arxiv.org/abs/astro-ph/0108122v2

Mon.Not.Roy.Astron.Soc. 336 (2002) 353

Astronomy and Astrophysics

Astrophysics

Revised version accepted for publication in MNRAS. 10 pages with 8 figures

Scientific paper

10.1046/j.1365-8711.2002.05725.x

We use a simple model of spheroid formation to explore the relationship between the creation of stars and dust in a massive proto galaxy and the growth of its central black hole. This model predicts that sub-mm luminosity peaks after only ~ 0.2 Gyr. However, without a very massive seed black hole, Eddington-limited growth means that a black hole mass of 10^9 solar masses, and hence very luminous AGN activity, cannot be produced until > 0.5 Gyr after the formation of the first massive stars in the halo. The model thus predicts a time-lag between the peak of sub-mm luminosity and AGN luminosity in a massive proto-elliptical of a few times 10^8 years. For a formation redshift z = 5, this means that powerful AGN activity is delayed until z = 3.5, by which time star formation in the host is 90% complete, and sub-mm luminosity has declined to ~ 25% of its peak value. This provides a natural explanation for why successful sub-mm detections of luminous radio galaxies are largely confined to z > 2.5. Conversely the model also predicts that while all high-redshift luminous sub-mm-selected sources should contain an active (and growing) black hole, the typical luminosity of the AGN in such objects is ~1000 times smaller than that of the most powerful AGN. This is consistent with the almost complete failure to detect sub-mm selected galaxies with existing X-ray surveys. Finally the model yields a black-hole:spheroid mass ratio which evolves rapidly in the first Gyr, but asymptotes to ~ 0.001-0.003 in agreement with results at low redshift. This ratio arises not because the AGN terminates star formation, but because fueling of the massive black hole is linked to the total mass of gas available for star formation in the host.

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