The radio loudness of SDSS quasars from the LOFAR Two-metre Sky Survey: ubiquitous jet activity and constraints on star formation

Author:

Macfarlane C1,Best P N1,Sabater J12,Gürkan G34ORCID,Jarvis M J56ORCID,Röttgering H J A7,Baldi R D89ORCID,Calistro Rivera G10ORCID,Duncan K J17ORCID,Morabito L K11ORCID,Prandoni I8ORCID,Retana-Montenegro E12

Affiliation:

1. Institute for Astronomy, University of Edinburgh, Royal Observatory, Blackford Hill, Edinburgh EH9 3HJ, UK

2. UK Astronomy Technology Centre, Royal Observatory, Blackford Hill, Edinburgh EH9 3HJ, UK

3. Thüringer Landessternwarte, Sternwarte 5, D-07778 Tautenburg, Germany

4. CSIRO Astronomy and Space Science, PO Box 1130, Bentley, WA 6102, Australia

5. Astrophysics, Department of Physics,University of Oxford, Keble Road, Oxford OX1 3RH, UK

6. Department of Physics & Astronomy, University of the Western Cape, Private Bag X17, Bellville, Cape Town 7535, South Africa

7. Leiden Observatory, Leiden University, PO Box 9513, NL-2300 RA Leiden, the Netherlands

8. INAF – Istituto di Radioastronomia, Via Piero Gobetti 101, I-40129 Bologna, Italy

9. Department of Physics & Astronomy, University of Southampton, Hampshire, Southampton SO17 1BJ, UK

10. European Southern Observatory, Karl-Schwarzschild-Straße 2, D-85748 Garching bei München, Germany

11. Centre for Extragalactic Astronomy, Department of Physics, Durham University, Durham DH1 3LE, UK

12. Astrophysics & Cosmology Research Unit, School of Mathematics, Statistics & Computer Science, University of KwaZulu-Natal, Durban 4041, South Africa

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.

Funder

Science and Technology Facilities Council

INAF

CTA

Gruber Foundation

IAU

CNRS

BMBF

MIWF-NRW

MPG

Science Foundation Ireland

NWO

Ministry of Science and Higher Education

National Science Foundation

U.S. Department of Energy

National Aeronautics and Space Administration

Max Planck Society

Higher Education Funding Council for England

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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