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The Radio-Loud Fraction of Quasars is a Strong Function of Redshift and Optical Luminosity
Journal article   Open access

The Radio-Loud Fraction of Quasars is a Strong Function of Redshift and Optical Luminosity

Linhua Jiang, Xiaohui Fan, Zeljko Ivezic, Gordon T Richards, Donald P Schneider, Michael A Strauss and Brandon C Kelly
The Astrophysical journal, v 656(2 I), pp 680-690
14 Nov 2006
url
https://doi.org/10.1086/510831View

Abstract

Physics - Astrophysics of Galaxies Physics - Cosmology and Nongalactic Astrophysics Physics - Earth and Planetary Astrophysics Physics - High Energy Astrophysical Phenomena Physics - Instrumentation and Methods for Astrophysics Physics - Solar and Stellar Astrophysics
Astrophys.J.656:680-690,2007 Using a sample of optically-selected quasars from the Sloan Digital Sky Survey, we have determined the radio-loud fraction (RLF) of quasars as a function of redshift and optical luminosity. The sample contains more than 30,000 objects and spans a redshift range of 0<z<5 and a luminosity range of -30<M_i<-22. We use both the radio-to-optical flux ratio (R parameter) and radio luminosity to define radio-loud quasars. After breaking the correlation between redshift and luminosity due to the flux-limited nature of the sample, we find that the RLF of quasars decreases with increasing redshift and decreasing luminosity. The relation can be described in the form of log(RLF/(1-RLF)) = b_0 + b_z log(1+z) + b_M (M_{2500}+26), where M_{2500} is the absolute magnitude at rest-frame 2500A, and b_z, b_M<0. When using R>10 to define radio-loud quasars, we find that b_0=-0.132+/-0.116, b_z=-2.052+/-0.261, and b_M=-0.183+/-0.025. The RLF at z=0.5 declines from 24.3% to 5.6% as luminosity decreases from M_{2500}=-26 to M_{2500}=-22, and the RLF at M_{2500}=-26 declines from 24.3% to 4.1% as redshift increases from 0.5 to 3, suggesting that the RLF is a strong function of both redshift and luminosity. We also examine the impact of flux-related selection effects on the RLF determination using a series of tests, and find that the dependence of the RLF on redshift and luminosity is highly likely to be physical, and the selection effects we considered are not responsible for the dependence.

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Astronomy & Astrophysics
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