4.7 Article

The 2dF-SDSS LRG and QSO survey: the QSO luminosity function at 0.4 < z < 2.6

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 399, Issue 4, Pages 1755-1772

Publisher

OXFORD UNIV PRESS
DOI: 10.1111/j.1365-2966.2009.15398.x

Keywords

galaxies: active; quasars: general; galaxies: Seyfert

Funding

  1. Alfred P. Sloan Foundation
  2. National Science Foundation
  3. US Department of Energy
  4. National Aeronautics and Space Administration
  5. Japanese Monbukagakusho
  6. Max Planck Society
  7. Higher Education Funding Council for England
  8. Australian Research Council
  9. Australian Academy of Science
  10. National Science Foundation [AST06-07634, AST-0707266]
  11. Science and Technology Facilities Council [ST/F002963/1, ST/F007817/1] Funding Source: researchfish
  12. STFC [ST/F007817/1, ST/F002963/1] Funding Source: UKRI

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We present the quasi-stellar object (QSO) luminosity function (LF) of the completed 2dF-SDSS LRG and QSO (2SLAQ) survey, based on QSOs photometrically selected from Sloan Digital Sky Survey (SDSS) imaging data and then observed spectroscopically using the 2dF instrument on the Anglo-Australian Telescope. We analyse 10 637 QSOs in the redshift range 0.4 < z < 2.6 to a g-band flux limit of 21.85 (extinction-corrected) and an absolute continuum magnitude of M-g(z = 2) < -21.5. This sample covers an area of 191.9 deg(2). The binned QSO LF agrees with that of the brighter SDSS main QSO sample, but extends similar to 2.5 mag fainter, clearly showing the flattening of the LF towards faint absolute magnitudes. 2SLAQ finds an excess of QSOs compared to the 2dF QSO Redshift Survey at g > 20.0, as found previously by Richards et al. The LF is consistent with other previous, much smaller, samples produced to the depth of 2SLAQ. By combining the 2SLAQ and SDSS QSO samples, we produce a QSO LF with an unprecedented combination of precision and dynamic range. With this we are able to accurately constrain both the bright and faint ends of the QSO LF. While the overall trends seen in the evolution of the QSO LF appear similar to pure luminosity evolution, the data show very significant departures from such a model. Most notably we see clear evidence that the number ensity of faint QSOs peaks at lower redshift than bright QSOs: QSOs with M-g > -23 have space densities which peak at z < 1, while QSOs at M-g < -26 peak at z > 2. By fitting simple LF models in narrow M-g intervals, we find that this downsizing is significant at the 99.98 per cent level. We show that LF models which follow the pure luminosity evolution form [i.e. M-g* equivalent to M-g*(z)], but with a redshift-dependent bright-end slope and an additional density evolution term, Phi* = Phi*(z), provide a much improved fit to the data. The bright-end slope, alpha, steepens from alpha similar or equal to -3.0 at z similar or equal to 0.5 to alpha = -3.5 at z similar or equal to 2.5. This steepening is significant at the 99.9 per cent level. We find a decline in Phi* from z similar or equal to 0.5 to 2.5 which is significant at the 94 per cent level.

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