Abstract

ABSTRACT We examine the distribution of radio emission from ∼42 000 quasars from the Sloan Digital Sky Survey, as measured in the LOFAR Two-metre Sky Survey (LoTSS). We present a model of the radio luminosity distribution of the quasars that assumes that every quasar displays a superposition of two sources of radio emission: active galactic nuclei (jets) and star formation. Our two-component model provides an excellent match to the observed radio flux density distributions across a wide range of redshifts and quasar optical luminosities; this suggests that the jet-launching mechanism operates in all quasars but with different powering efficiency. The wide distribution of jet powers allows for a smooth transition between the ‘radio-quiet’ and ‘radio-loud’ quasar regimes, without need for any explicit bimodality. The best-fitting model parameters indicate that the star formation rate of quasar host galaxies correlates strongly with quasar luminosity and also increases with redshift at least out to z ∼ 2. For a model where star formation rate scales as $L_{\rm bol}^{\alpha } (1+z)^{\beta }$, we find α = 0.47 ± 0.01 and β = 1.61 ± 0.05, in agreement with far-infrared studies. Quasars contribute ≈0.15 per cent of the cosmic star formation rate density at z = 0.5, rising to 0.4 per cent by z ∼ 2. The typical radio jet power is seen to increase with both increasing optical luminosity and black hole mass independently, but does not vary with redshift, suggesting intrinsic properties govern the production of the radio jets. We discuss the implications of these results for the triggering of quasar activity and the launching of jets.

Highlights

  • The fundamental physical mechanism that powers and defines active galactic nuclei (AGN) is the transfer of energy from the relativistically-deep potential well of a central supermassive black hole (SMBH) in a galaxy (Salpeter 1964; Zel’dovich 1964; LyndenBell 1969)

  • We examine the distribution of radio emission from ∼ 42, 000 quasars from the Sloan Digital Sky Survey, as measured in the LOw Frequency ARray (LOFAR) Two-Metre Sky Survey (LoTSS)

  • That the scatter in the relationship between star-formation rate (SFR) and quasar luminosity does not change much with quasar luminosity has been seen before in literature plots (e.g. Lanzuisi et al 2017), and as this ratio is driven by gas distributions within the host galaxies it is not surprising that there is no strong redshift dependence either

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Summary

Introduction

The fundamental physical mechanism that powers and defines active galactic nuclei (AGN) is the transfer of energy from the relativistically-deep potential well of a central supermassive black hole (SMBH) in a galaxy (Salpeter 1964; Zel’dovich 1964; LyndenBell 1969). Lacking the answer to such a fundamental question about the nature of RL and RQ quasars means we cannot obtain a complete understanding of the physical mechanisms at play. This gap in our knowledge has significant consequences for theories of galaxy formation and evolution given the strong evidence for a close relationship between the growth of the central SMBH and the evolution of its surrounding host galaxy (e.g. see reviews by Fabian 2012; Heckman & Best 2014), such as the correlations observed between the mass of the central SMBH and properties of the host galaxy’s bulge This gap in our knowledge has significant consequences for theories of galaxy formation and evolution given the strong evidence for a close relationship between the growth of the central SMBH and the evolution of its surrounding host galaxy (e.g. see reviews by Fabian 2012; Heckman & Best 2014), such as the correlations observed between the mass of the central SMBH and properties of the host galaxy’s bulge (e.g. Ferrarese & Merritt 2000; Gebhardt et al 2000; Marconi & Hunt 2003; Häring & Rix 2004)

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