The most luminous H α emitters atz∼ 0.8–2.23 from HiZELS: evolution of AGN and star-forming galaxies

observations. [Cosmology] Cosmology and Nongalactic Astrophysics (astro-ph.CO) Cosmology: observations Galaxies: high-redshift Galaxies: evolution FOS: Physical sciences evolution [Galaxies] 530 Astrophysics - Astrophysics of Galaxies 01 natural sciences 520 high-redshift [Galaxies] Astrophysics of Galaxies (astro-ph.GA) 0103 physical sciences Astrophysics - Cosmology and Nongalactic Astrophysics
DOI: 10.1093/mnras/stw022 Publication Date: 2016-02-05T01:43:24Z
ABSTRACT
16 pages, 10 figures. Accepted for publication in MNRAS<br/>We use new near-infrared spectroscopic observations to investigate the nature and evolution of the most luminous H��(Ha) emitters at z~0.8-2.23, which evolve strongly in number density over this period, and compare them to more typical Ha emitters. We study 59 luminous Ha emitters with $L_{H��}>L_{H��}^*$, roughly equally split per redshift slice at z~0.8, 1.47 and 2.23 from the HiZELS and CF-HiZELS surveys. We find that, overall, 30$\pm$8% are AGN (80$\pm$30% of these AGN are broad-line AGN, BL-AGN), and we find little to no evolution in the AGN fraction with redshift, within the errors. However, the AGN fraction increases strongly with Ha luminosity and correlates best with $L_{H��}/L_{H��}^*(z)$. While $L_{H��}80%), the most luminous Ha emitters ($L_{H��}>10L_{H��}^*(z)$) at any cosmic time are essentially all BL-AGN. Using our AGN-decontaminated sample of luminous star-forming galaxies, and integrating down to a fixed Ha luminosity, we find a factor of ~1300x evolution in the star formation rate density from z=0 to z=2.23. This is much stronger than the evolution from typical Ha star-forming galaxies and in line with the evolution seen for constant luminosity cuts used to select "Ultra-Luminous" Infrared Galaxies and/or sub-millimetre galaxies. By taking into account the evolution in the typical Ha luminosity, we show that the most strongly star-forming Ha-selected galaxies at any epoch ($L_{H��}>L^*_{H��}(z)$) contribute the same fractional amount of ~15% to the total star-formation rate density, at least up to z=2.23.<br/>
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