The 2dF QSO Redshift Survey - I. The Optical QSO Luminosity Function
The 2dF QSO Redshift Survey - I. The Optical QSO Luminosity Function
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DOI:
10.1046/j.1365-8711.2000.03730.x
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发表时间:
2000-05
期刊:
影响因子:
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通讯作者:
B.J.Boyle;T.Shanks;S.M.Croom;R.J.Smith;L.Miller;N.Loaring;C.Heymans
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文献类型:
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作者:
B.J.Boyle;T.Shanks;S.M.Croom;R.J.Smith;L.Miller;N.Loaring;C.Heymans
We present a determination of the optical QSO luminosity function and its cosmological evolution with redshift for a sample of over 6000 QSOs identified primarily from the first observations of the 2dF QSO Redshift Survey (2QZ). For QSOs with − 26 < M B < − 23 and 0 . 35 < z < 2 . 3, we find that pure luminosity evolution (PLE) models provide an acceptable fit to the observed redshift dependence of the luminosity function. The luminosity function is best fit by a two-power-law function of the form Φ( L B ) ∝ [( L B /L ∗ B ) α + ( L B /L ∗ B ) β ] − 1 . Exponential luminosity evolution models, both as a function of look-back time, L ∗ B ( z ) = L ∗ B (0)e k 1 τ , and as a general second-order polynomial, L ∗ B ( z ) ∝ 10 k 1 z + k 2 z 2 , were found to provide acceptable fits to the dataset comprising the 2QZ and the Large Bright Quasar Survey. Exponential evolution with look-back time is prefered for q 0 = 0 . 05, while the polynomial evolution model is prefered for q 0 = 0 . 5. The shape and evolution of the LF at low redshifts ( z < 0 . 5) and/or high luminosities, not currently well sampled by the 2dF QSO survey, may show departures from pure luminosity evolution, but the results presented here show that over a significant range of redshift, PLE is a good description of QSO evolution.