Density profile of dark matter haloes and galaxies in the Horizon-AGN simulation: the impact of AGN feedback

Monthly Notices of the Royal Astronomical Society Oxford University Press 472:2 (2017) 2153-2169

Authors:

Sébastien Peirani, Yohan Dubois, Marta Volonteri, Julien Devriendt, Kevin Bundy, Joe Silk, Christophe Pichon, Sugata Kaviraj, Raphaël Gavazzi, Mélanie Habouzit

Abstract:

Using a suite of three large cosmological hydrodynamical simulations, HORIZON-AGN, HORIZON-NOAGN (no AGN feedback) and HORIZON-DM (no baryons), we investigate how a typical sub-grid model for AGN feedback affects the evolution of the inner density profiles of massive dark matter haloes and galaxies. Based on direct object-to-object comparisons, we find that the integrated inner mass and density slope differences between objects formed in these three simulations (hereafter, HAGN, HnoAGN and HDM) significantly evolve with time. More specifically, at high redshift (z ~ 5), the mean central density profiles of HAGN and HnoAGN dark matter haloes tend to be much steeper than their HDM counterparts owing to the rapidly growing baryonic component and ensuing adiabatic contraction. By z ~ 1.5, these mean halo density profiles in HAGN have flattened, pummelled by powerful AGN activity (“quasarmode”): the integrated innermass difference gapswith HnoAGN haloes have widened, and those with HDM haloes have narrowed. Fast forward 9.5 billion years, down to z = 0, and the trend reverses: HAGN halo mean density profiles drift back to a more cusped shape as AGN feedback efficiency dwindles (“radio mode”), and the gaps in integrated central mass difference with HnoAGN and HDM close and broaden respectively.On the galaxy side, the story differs noticeably.Averaged stellar profile central densities and inner slopes are monotonically reduced by AGN activity as a function of cosmic time, resulting in better agreement with local observations. As both dark matter and stellar inner density profiles respond quite sensitively to the presence of a central AGN, there is hope that future observational determinations of these quantities can be used constrain AGN feedback models.

On the time lags of the LIGO signals

Journal of Cosmology and Astroparticle Physics IOP Publishing 2017:08 (2017) 013-013

Authors:

James Creswell, Sebastian von Hausegger, Andrew D Jackson, Hao Liu, Pavel Naselsky

The Low Frequency Receivers for SKA1-Low: Design and Verification

Institute of Electrical and Electronics Engineers (IEEE) (2017) 1-4

Authors:

Pieter Benthem, Marchel Gerbers, Jan Geralt Bij de Vaate, Stefan Wijnholds, Jeanette Bast, Tom Booler, Tim Colgate, Brian Crosse, David Emrich, Peter Hall, Budi Juswardy, David Kenney, Franz Schlazenhaufer, Marcin Sokolowski, Adrian Sutinjo, Daniel Ung, Randall Wayth, Andrew Williams, Monica Alderighi, Pietro Bolli, Gianni Comoretto, Andrea Mattana, Jader Monari, Giovanni Naldi, Frederico Perini, Giuseppe Pupillo, Simone Rusticelli, Marco Schiaffino, Francesco Schilliro, Amin Aminei, Riccardo Chiello, Mike Jones, Jeremy Baker, Richard Bennett, Rob Halsall, Georgina Kaligeridou, Matthew Roberts, Hermine Schnetler, Jens Abraham, Eloy De Lera Accdo, Andrew Faulkner, Nima Razavi Ghods, Denis Cutajar, Andrea DeMarco, Alessio Magro, Kristian Zarb Adami

The third data release of the Kilo-Degree Survey and associated data products

Astronomy & Astrophysics EDP Sciences 604 (2017) A134

Authors:

JTAD Jong, GAV Kleijn, T Erben, H Hildebrandt, K Kuijken, G Sikkema, M Brescia, M Bilicki, NR Napolitano, V Amaro, KG Begeman, H Buddelmeijer, S Cavuoti, F Getman, A Grado, E Helmich, Z Huang, N Irisarri, FL Barbera, G Longo, JP McFarland, R Nakajima, M Paolillo, E Puddu, M Radovich, A Rifatto, C Tortora, EA Valentijn, C Vellucci, W-J Vriend, A Amon, C Blake, A Choi, IF Conti, R Herbonnet, C Heymans, H Hoekstra, D Klaes, Julian Merten, Lance Miller, P Schneider, M Viola

Abstract:

Context

The Kilo-Degree Survey (KiDS) is an ongoing optical wide-field imaging survey with the OmegaCAM camera at the VLT Survey Telescope. It aims to image 1500 square degrees in four filters (ugri). The core science driver is mapping the large-scale matter distribution in the Universe, using weak lensing shear and photometric redshift measurements. Further science cases include galaxy evolution, Milky Way structure, detection of high-redshift clusters, and finding rare sources such as strong lenses and quasars.

Aims

Here we present the third public data release and several associated data products, adding further area, homogenized photometric calibration, photometric redshifts and weak lensing shear measurements to the first two releases.

Methods

A dedicated pipeline embedded in the Astro-WISE information system is used for the production of the main release. Modifications with respect to earlier releases are described in detail. Photometric redshifts have been derived using both Bayesian template fitting, and machine-learning techniques. For the weak lensing measurements, optimized procedures based on the THELI data reduction and lensfit shear measurement packages are used.

Results

In this third data release an additional 292 new survey tiles (≈ 300 deg2) stacked ugri images are made available, accompanied by weight maps, masks, and source lists. The multi-band catalogue, including homogenized photometry and photometric redshifts, covers the combined DR1, DR2 and DR3 footprint of 440 survey tiles (447 deg2). Limiting magnitudes are typically 24.3, 25.1, 24.9, 23.8 (5σ in a 200aperture) in ugri, respectively, and the typical r-band PSF size is less than 0.700. The photometric homogenization scheme ensures accurate colors and an absolute calibration stable to ≈ 2% for gri and ≈ 3% in u. Separately released for the combined area of all KiDS releases to date are a weak lensing shear catalogue and photometric redshifts based on two different machine-learning techniques.

Cosmic evolution of stellar quenching by AGN feedback: clues from the Horizon-AGN simulation

Monthly Notices of the Royal Astronomical Society Oxford University Press 472:1 (2017) 949-965

Authors:

Ricarda S Beckmann, Julien Devriendt, Adrianne D Slyz, S Peirani, Mark LA Richardson, Y Dubois, C Pichon, Nora E Chisari, S Kaviraj, Clotilde MC Laigle, M Volonteri

Abstract:

The observed massive end of the local galaxy stellar mass function is steeper than its predicted dark matter (DM) halo counterpart in the standard $\Lambda $CDM paradigm. We investigate how active galactic nuclei (AGN) feedback can account for such a reduction in the stellar content of massive galaxies, through an influence on the gas content of their interstellar (ISM) and circum-galactic medium (CGM). We isolate the impact of AGNs by comparing two simulations from the HORIZON suite, which are identical except that one includes super massive black holes (SMBH) and related feedback. This allows us to cross-identify individual galaxies between these simulations and quantify the effect of AGN feedback on their properties, such as stellar mass and gas outflows. We find that the most massive galaxies ($ \rm M_{*} \geq 3 \times 10^{11} M_\odot $) are quenched to the extent that their stellar masses decrease by about 80% at $z=0$. More generally, SMBHs affect their host halo through a combination of outflows that reduce their baryonic mass, particularly for galaxies in the mass range $ \rm 10^9 M_\odot \leq M_{*} \leq 10^{11} M_\odot $, and a disruption of central gas inflows, which limits in-situ star formation, particularly massive galaxies with $ \rm M_{*} \approx10^{11} M_\odot $. As a result of these processes, net gas inflows onto massive galaxies drop by up to 70%. Finally, we measure a redshift evolution in the stellar mass ratio of twin galaxies with and without AGN feedback, with galaxies of a given stellar mass showing stronger signs of quenching earlier on. This evolution is driven by a progressive flattening of the $\rm M_{SMBH}-M_* $ relation for galaxies with $\rm M_{*} \leq 10^{10} M_\odot $ as redshift decreases, which translates into smaller SBMHs being harboured by galaxies of any fixed stellar mass, and indicates stronger AGN feedback at higher redshift.