The adaptive optics modes for HARMONI: from Classical to Laser Assisted Tomographic AO

Proceedings of SPIE--the International Society for Optical Engineering SPIE, the international society for optics and photonics 9909 (2016) 990909-990909-15

Authors:

B Neichel, T Fusco, J-F Sauvage, C Correia, K Dohlen, K El-Hadi, L Blanco, N Schwartz, F Clarke, NA Thatte, M Tecza, J Paufique, J Vernet, M Le Louarn, P Hammersley, J-L Gach, S Pascale, P Vola, C Petit, J-M Conan, A Carlotti, C Vérinaud, H Schnetler, I Bryson, T Morris, R Myers, E Hugot, AM Gallie, David M Henry

GAMA/WiggleZ: The 1.4GHz radio luminosity functions of high- and low-excitation radio galaxies and their redshift evolution to z=0.75

Monthly Notices of the Royal Astronomical Society Oxford University Press 460:1 (2016) 2-17

Authors:

Michael B Pracy, John HY Ching, Elaine M Sadler, Scott M Croom, IK Baldry, Joss Bland-Hawthorn, S Brough, MJI Brown, Warwick Couch, Tamara M Davis, Michael J Drinkwater, Matthew Jarvis, Ben Jelliffe, Russell J Jurek, J Loveday, KA Pimbblet, M Prescott, Emily Wisnioski, David Woods

Abstract:

We present radio active galactic nuclei (AGN) luminosity functions over the redshift range 0.005 < z < 0.75. The sample from which the luminosity functions are constructed is an optical spectroscopic survey of radio galaxies, identified from matched Faint Images of the Radio Sky at Twenty-cm survey (FIRST) sources and Sloan Digital Sky Survey images. The radio AGN are separated into low-excitation radio galaxies (LERGs) and high-excitation radio galaxies (HERGs) using the optical spectra. We derive radio luminosity functions for LERGs and HERGs separately in the three redshift bins (0.005 < z < 0.3, 0.3 < z < 0.5 and 0.5 < z < 0.75). The radio luminosity functions can be well described by a double power law. Assuming this double power-law shape the LERG population displays little or no evolution over this redshift range evolving as ∼(1+z)0.06+0.17−0.18 assuming pure density evolution or ∼(1+z)0.46+0.22−0.24 assuming pure luminosity evolution. In contrast, the HERG population evolves more rapidly, best fitted by ∼(1+z)2.93+0.46−0.47 assuming a double power-law shape and pure density evolution. If a pure luminosity model is assumed, the best-fitting HERG evolution is parametrized by ∼(1+z)7.41+0.79−1.33 . The characteristic break in the radio luminosity function occurs at a significantly higher power (≳1 dex) for the HERG population in comparison to the LERGs. This is consistent with the two populations representing fundamentally different accretion modes.

The KMOS Redshift One Spectroscopic Survey (KROSS): the Tully-Fisher relation at z similar to 1

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY 460:1 (2016) 103-129

Authors:

AL Tiley, JP Stott, AM Swinbank, M Bureau, CM Harrison, R Bower, HL Johnson, AJ Bunker, MJ Jarvis, G Magdis, R Sharples, I Smail, D Sobral, P Best

The SLUGGS survey: a new mask design to reconstruct the stellar populations and kinematics of both inner and outer galaxy regions

(2016)

Authors:

Nicola Pastorello, Duncan A Forbes, Adriano Poci, Aaron J Romanowsky, Richard McDermid, Adebusola B Alabi, Jean P Brodie, Michele Cappellari, Vincenzo Pota, Caroline Foster

Bursty star formation feedback and cooling outflows

(2016)

Authors:

Teresita Suarez, Andrew Pontzen, Hiranya V Peiris, Adrianne Slyz, Julien Devriendt