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Black Hole

Lensing of space time around a black hole. At Oxford we study black holes observationally and theoretically on all size and time scales - it is some of our core work.

Credit: ALAIN RIAZUELO, IAP/UPMC/CNRS. CLICK HERE TO VIEW MORE IMAGES.

Julien Devriendt

Professor of Astrophysics

Research theme

  • Astronomy and astrophysics
  • Particle astrophysics & cosmology

Sub department

  • Astrophysics

Research groups

  • Beecroft Institute for Particle Astrophysics and Cosmology
  • Cosmology
  • Galaxy formation and evolution
julien.devriendt@physics.ox.ac.uk
Telephone: 01865 (2)73307
Denys Wilkinson Building, room 555D
  • About
  • Teaching
  • Publications

Active Galactic Nuclei In Cosmological Simulations - I. Formation of black holes and spheroids through mergers

ArXiv astro-ph/0509116 (2005)

Authors:

A Cattaneo, J Blaizot, J Devriendt, B Guiderdoni

Abstract:

The Active Galactic Nuclei In Cosmological Simulations (AGNICS) project includes AGN into the GalICS hybrid (N-body + semi-analytic) model to explore the quasar-galaxy link in a cosmological perspective. The key problems are the quasar fuelling mechanism, the origin of the BH to bulge mass relation, the causal and chronological link between BH growth and galaxy formation, the properties of quasar hosts and the role of AGN feedback in galaxy formation. This first paper has two goals: to describe the general structure and the assumptions of the method, and to apply AGNICS to studying the joint formation of BHs and spheroids in galaxy mergers. We investigate under what conditions this scenario can reproduce the local BH distribution and the evolution of the quasar population. AGNICS contains two star formation modes: a quiescent one in discs and a starburst one in protospheroids, the latter triggered by mergers and disc instabilities. We assume that BH growth is linked to the starburst mode. The simplest version of this scenario, in which the BH accretion rate and the star formation rate in the starburst component are simply related by a constant of proportionality, does not to reproduce the cosmic evolution of the quasar population. A model in which this relation is modulated by a scaling with the square root of the starburst gas density can explain the evolution of the quasar luminosity function in B-band and X-rays (accounting for the obscuration inferred from X-ray studies). The scatter and the tilt that this model introduces in the BH-to-bulge mass relation are within the observational constraints. The quasar contribution grows with bolometric luminosity and for a given bulge mass the most massive BHs are in the bulges with the oldest stars.

Active Galactic Nuclei In Cosmological Simulations - I. Formation of black holes and spheroids through mergers

(2005)

Authors:

A Cattaneo, J Blaizot, J Devriendt, B Guiderdoni

Formation of Structure in Molecular Clouds: A Case 51猎奇入口

(2005)

Authors:

F Heitsch, A Burkert, L Hartmann, AD Slyz, JEG Devriendt

Non-linear evolution of suppressed dark matter primordial power spectra

Monthly Notices of the Royal Astronomical Society 360:1 (2005) 282-287

Authors:

C Boehm, H Mathis, J Devriendt, J Silk

Abstract:

We address the degree and rapidity of generation of small-scale power over the course of structure formation in cosmologies where the primordial power spectrum is strongly suppressed beyond a given wavenumber. We first summarize the situations where one expects such suppressed power spectra and point out their diversity. We then employ an exponential cut-off, which characterizes warm dark matter (WDM) models, as a template for the shape of the cut-off and focus on damping scales ranging from 106 to 109 h -1 M鈯�. Using high-resolution simulations, we show that the suppressed part of the power spectrum is quickly (re)generated and catches up with both the linear and the non-linear evolution of the unsuppressed power spectrum. From z = 2 onwards, a power spectrum with a primordial cut-off at 109 h-1 M艁贸d藕, becomes virtually indistinguishable from an evolved cold dark matter (CDM) power spectrum. An attractor such as that described in Zaldarriaga, Scoccimarro & Hui for power spectra with different spectral indices also emerges in the case of truncated power spectra. Measurements of z 鈭� 0 non-linear power spectra at 鈭�100 h-1 kpc cannot rule out the possibility of linear power spectra damped below 鈭�109 h-1 M 鈯�. Therefore, WDM or scenarios with similar features should be difficult to exclude in this way. 漏 2005 RAS.

A simple model for the evolution of supermassive black holes and the quasar population

Monthly Notices of the Royal Astronomical Society 359:4 (2005) 1363-1378

Authors:

JEG Devriendt, Mahmood, A., Silk, J.

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