Exploring AGN Activity over cosmic time with the SKA

Proceedings of Science 9-13-June-2014 (2014)

Authors:

V Smolcic, P Padovani, J Delhaize, I Prandoni, N Seymour, M Jarvis, J Afonso, M Magliocchett, IM Huynh, M Vaccari, A Karim

Abstract:

In this Chapter we present the motivation for undertaking both a wide and deep survey with the SKA in the context of studying AGN activity across cosmic time. With an rms down to 1 μJy/beam at 1 GHz over 1,000 - 5,000 deg2 in 1 year (wide tier band 1/2) and an rms down to 200 nJy/beam over 10 - 30 deg2 in 2000 hours (deep tier band 1/2), these surveys will directly detect faint radio-loud and radio-quiet AGN (down to a 1 GHz radio luminosity of about 2×1023 W/Hz at z = 6). For the first time, this will enable us to conduct detailed studies of the cosmic evolution of radio AGN activity to the cosmic dawn (z ≳ 6), covering all environmental densities.

Galaxy masses

Reviews of Modern Physics American Physical Society (APS) 86:1 (2014) 47-119

Authors:

Stéphane Courteau, Michele Cappellari, Roelof S de Jong, Aaron A Dutton, Eric Emsellem, Henk Hoekstra, LVE Koopmans, Gary A Mamon, Claudia Maraston, Tommaso Treu, Lawrence M Widrow

HerMES: Candidate high-redshift galaxies discovered with Herschel/Spire

Astrophysical Journal 780:1 (2014)

Authors:

CD Dowell, A Conley, J Glenn, V Arumugam, V Asboth, H Aussel, F Bertoldi, M Béthermin, J Bock, A Boselli, C Bridge, V Buat, D Burgarella, A Cabrera-Lavers, CM Casey, SC Chapman, DL Clements, L Conversi, A Cooray, H Dannerbauer, F De Bernardis, TP Ellsworth-Bowers, D Farrah, A Franceschini, M Griffin, MA Gurwell, M Halpern, E Hatziminaoglou, S Heinis, E Ibar, RJ Ivison, N Laporte, L Marchetti, P Martínez-Navajas, G Marsden, GE Morrison, HT Nguyen, B O'Halloran, SJ Oliver, A Omont, MJ Page, A Papageorgiou, CP Pearson, G Petitpas, I Pérez-Fournon, M Pohlen, D Riechers, D Rigopoulou, IG Roseboom, M Rowan-Robinson, J Sayers, B Schulz, D Scott, N Seymour, DL Shupe, AJ Smith, A Streblyanska, M Symeonidis, M Vaccari, I Valtchanov, JD Vieira, M Viero, L Wang, J Wardlow, CK Xu, M Zemcov

Abstract:

We present a method for selecting z > 4 dusty, star-forming galaxies (DSFGs) using Herschel/Spectral and Photometric Imaging Receiver 250/350/500 μm flux densities to search for red sources. We apply this method to 21 deg2 of data from the HerMES survey to produce a catalog of 38 high-z candidates. Follow-up of the first five of these sources confirms that this method is efficient at selecting high-z DSFGs, with 4/5 at z = 4.3-6.3 (and the remaining source at z = 3.4), and that they are some of the most luminous dusty sources known. Comparison with previous DSFG samples, mostly selected at longer wavelengths (e.g., 850 μm) and in single-band surveys, shows that our method is much more efficient at selecting high-z DSFGs, in the sense that a much larger fraction are at z > 3. Correcting for the selection completeness and purity, we find that the number of bright (S 500 μm ≥ 30 mJy), red Herschel sources is 3.3 ± 0.8 deg-2. This is much higher than the number predicted by current models, suggesting that the DSFG population extends to higher redshifts than previously believed. If the shape of the luminosity function for high-z DSFGs is similar to that at z ∼ 2, rest-frame UV based studies may be missing a significant component of the star formation density at z = 4-6, even after correction for extinction. © 2014. The American Astronomical Society. All rights reserved.

How typical is the Coma cluster?

Monthly Notices of the Royal Astronomical Society 438:4 (2014) 3049-3057

Authors:

KA Pimbblet, SJ Penny, RL Davies

Abstract:

Coma is frequently used as the archetype z ∼ 0 galaxy cluster to compare higher redshift work against. It is not clear, however, how representative the Coma cluster is for galaxy clusters of its mass or X-ray luminosity, and significantly, recent works have suggested that the galaxy population of Coma may be in some ways anomalous. In this work, we present a comparison of Coma to an X-ray-selected control sample of clusters. We show that although Coma is typical against the control sample in terms of its internal kinematics (sub-structure and velocity dispersion profile), it has a significantly high (∼3σ) X-ray temperature set against clusters of comparable mass. By de-redshifting our control sample cluster galaxies star formation rates using a fit to the galaxy main-sequence evolution at z < 0.1, we determine that the typical star formation rate of Coma galaxies as a function of mass is higher than for galaxies in our control sample at a confidence level of >99 per cent. One way to alleviate this discrepancy and bring Coma in line with the control sample would be to have the distance to Coma to be slightly lower, perhaps through a non-negligible peculiar velocity with respect to the Hubble expansion, but we do not regard this as likely given precision measurements using a variety of approaches. Therefore, in summary, we urge caution in using Coma as a z ∼ 0 baseline cluster in galaxy evolution studies. © 2014 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society.

Morphological classification of radio sources for galaxy evolution and cosmology with the SKA

Proceedings of Science 9-13-June-2014 (2014)

Authors:

S Makhathini, OM Smirnov, MJ Jarvis, I Heywood

Abstract:

Morphologically classifying radio sources in continuum images with the SKA has the potential to address some of the key questions in cosmology and galaxy evolution. In particular, we may use different classes of radio sources as independent tracers of the dark-matter density field, and thus overcome cosmic variance in measuring large-scale structure, while on the galaxy evolution side we could measure the mechanical feedback from FRII and FRI jets. This work makes use of a MeqTrees-based simulations framework to forecast the ability of the SKA to recover true source morphologies at high redshifts. A suite of high resolution images containing realistic continuum source distributions with different morphologies (FRI, FRII, starburst galaxies) is fed through an SKA Phase 1 simulator, then analysed to determine the sensitivity limits at which the morphologies can still be distinguished. We also explore how changing the antenna distribution affects these results.