
The radio luminosity function of radio‐loud quasars from the 7C Redshift Survey
Author(s) -
Willott Chris J.,
Rawlings Steve,
Blundell Katherine M.,
Lacy Mark
Publication year - 1998
Publication title -
monthly notices of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.058
H-Index - 383
eISSN - 1365-2966
pISSN - 0035-8711
DOI - 10.1046/j.1365-8711.1998.t01-1-01946.x
Subject(s) - physics , quasar , redshift , astrophysics , luminosity function , astronomy , redshift survey , luminosity , galaxy
We present a complete sample of 24 radio‐loud quasars (RLQs) from the new 7C Redshift Survey. Every quasar with a low‐frequency (151 MHz) radio flux density S 151 > 0.5 Jy in two regions of the sky covering 0.013 sr is included; 23 of these have sufficient extended flux to meet the selection criteria, 18 of these have steep radio spectra (hereafter denoted as SSQs). The key advantage of this sample over most samples of RLQs is the lack of an optical magnitude limit. By combining the 7C and 3CRR samples, we have investigated the properties of RLQs as a function of redshift x and radio luminosity L 151 . We derive the radio luminosity function (RLF) of RLQs and find that the data are well fitted by a single power law with slope α 1 = 1.9 ± 0.1 (for H 0 = 50 km s −1 Mpc −1 , Ω M = 1, Ω λ = 0). We find that there must be a break in the RLQ RLF at log 10 L 151 /W Hz −1 sr −1 ) ≲ 27, in order for the models to be consistent with the 7C and 6C source counts. The z ‐dependence of the RLF follows a one‐tailed Gaussian which peaks at z = 1.7 ± 0.2. We find no evidence for a decline in the comoving space density of RLQs at higher redshifts. A positive correlation between the radio and optical luminosities of SSQs is observed, confirming a result of Serjeant et al. We are able to rule out this correlation being the result of selection effects or biases in our combined sample. The radio–optical correlation and best‐fitting model RLF enable us to estimate the distribution of optical magnitudes of quasars in samples selected at low radio frequencies. We conclude that for samples with S 151 ≲ 1 Jy, one must use optical data significantly deeper than the POSS‐I limit ( R ≈ 20), in order to avoid severe incompleteness.