A deep/wide 1-2 GHz snapshot survey of SDSS Stripe 82 using the Karl G. Jansky Very Large Array in a compact hybrid configuration

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY 460:4 (2016) 4433-4452

Authors:

I Heywood, MJ Jarvis, AJ Baker, KW Bannister, CS Carvalho, M Hardcastle, M Hilton, K Moodley, OM Smirnov, DJB Smith, SV White, EJ Wollack

Sizes, colour gradients and resolved stellar mass distributions for the massive cluster galaxies in XMMUJ2235-2557 at z = 1.39

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 458:3 (2016) 3181-3209

Authors:

Jeffrey CC Chan, Alessandra Beifiori, J Trevor Mendel, Roberto P Saglia, Ralf Bender, Matteo Fossati, Audrey Galametz, Michael Wegner, David J Wilman, Michele Cappellari, Roger L Davies, Ryan CW Houghton, Laura J Prichard, Ian J Lewis, Ray Sharples, John P Stott

The cosmic evolution of massive black holes in the Horizon-AGN simulation

Monthly Notices of the Royal Astronomical Society Oxford University Press 460:3 (2016) 2979-2996

Authors:

Marta Volonteri, Yohan Dubois, Christophe Pichon, Julien Devriendt

Abstract:

We analyse the demographics of black holes (BHs) in the large-volume cosmological hydrodynamical simulation Horizon-AGN. This simulation statistically models how much gas is accreted on to BHs, traces the energy deposited into their environment and, consequently, the back-reaction of the ambient medium on BH growth. The synthetic BHs reproduce a variety of observational constraints such as the redshift evolution of the BH mass density and the mass function. Strong self-regulation via AGN feedback, weak supernova feedback, and unresolved internal processes result in a tight BH–galaxy mass correlation. Starting at z ∼ 2, tidal stripping creates a small population of BHs over-massive with respect to the halo. The fraction of galaxies hosting a central BH or an AGN increases with stellar mass. The AGN fraction agrees better with multi-wavelength studies, than single-wavelength ones, unless obscuration is taken into account. The most massive haloes present BH multiplicity, with additional BHs gained by ongoing or past mergers. In some cases, both a central and an off-centre AGN shine concurrently, producing a dual AGN. This dual AGN population dwindles with decreasing redshift, as found in observations. Specific accretion rate and Eddington ratio distributions are in good agreement with observational estimates. The BH population is dominated in turn by fast, slow, and very slow accretors, with transitions occurring at z = 3 and z = 2, respectively.

Comparing Simulations of AGN Feedback

(2016)

Authors:

Mark LA Richardson, Evan Scannapieco, Julien Devriendt, Adrianne Slyz, Robert J Thacker, Yohan Dubois, James Wurster, Joseph Silk

Radio continuum surveys and galaxy evolution: modelling and simulations

Proceedings of Science Sissa Medialab 267 (2016) 1-12

Authors:

Adrianne Slyz, Julien Devriendt, Matthew Jarvis, Y Dubois, C Pichon

Abstract:

We predict the evolution of the radio continuum sky at 1.4 GHz from the Horizon-AGN Adaptive Mesh Refinement (AMR) cosmological hydrodynamical simulation of a cubic volume of the Universe 100h−1 Mpc on a side. With empirically motivated models for the radio continuum emission due to both star formation and Active Galactic Nuclei (AGN), we estimate the contribution of each of these processes to the local radio continuum luminosity function (LF) and describe its evolution up to redshift 4. Despite the simplicity of these models, we find that our predictions for the local luminosity function are fairly consistent with Mauch & Sadler (2007) observations, with the faint end of the luminosity function dominated by star forming galaxies and the bright end by radio loud AGNs. At redshift one, a decent match to Smolcic et al. (2009) VLA data in the COSMOS field can only be achieved when we account for radio continuum emission from AGNs. We predict that the strongest evolution across the peak epoch of cosmic activity happens for low luminosity star forming galaxies L1.4GHz < 1022 W Hz−1 , whose contribution rises until z ∼ 2 and declines at higher redshifts. The contribution of low luminosity AGNs L1.4GHz < 1022 W Hz−1 steadily declines from z = 0 throughout the redshift range, whilst that of radio loud objects with luminosities in the range 1022 W Hz−1 < L1.4GHz < 1024 W Hz−1 rises dramatically until z = 4. Finally, high-luminosity radio loud AGNs, with L1.4GHz > 1024 W Hz−1 show surprisingly little evolution from z = 0 to z = 4.