Abstract

ABSTRACT We present a study of 9 242 spectroscopically confirmed quasars with multiepoch ugriz photometry from the SDSS Southern Survey. By fitting a separable linear model to each quasar’s spectral variations, we decompose their five-band spectral energy distributions into variable (disc) and non-variable (host galaxy) components. In modelling the disc spectra, we include attenuation by dust on the line of sight through the host galaxy to its nucleus. We consider five commonly used attenuation laws, and find that the best description is by dust similar to that of the Small Magellanic Cloud, inferring a lack of carbonaceous grains from the relatively weak 2175-Å absorption feature. We go on to construct a composite spectrum for the quasar variations spanning 700–8000 Å. By varying the assumed power-law Lν ∝ να spectral slope, we find a best-fitting value α = 0.71 ± 0.02, excluding at high confidence the canonical Lν ∝ ν1/3 prediction for a steady-state accretion disc with a T ∝ r−3/4 temperature profile. The bluer spectral index of the observed quasar variations instead supports the model of Agol & Krolik, and Mummery & Balbus, in which a steeper temperature profile, T ∝ r−7/8, develops as a result of finite magnetically induced stress at the innermost stable circular orbit extracting energy and angular momentum from the black hole spin.

Highlights

  • The optical identification of quasi-stellar objects by Matthews & Sandage (1963) enabled, for the first time, studies of the distant universe at z > 0.1

  • We have separated the variable accretion disc light from their static host galaxies using broad-band photometric lightcurves, de-reddened their spectral energy distributions (SEDs) to account for dust, and leveraged the results to test accretion disc physics

  • We developed a method for decomposing quasar lightcurves by separating the contribution of the variable light from the static, background emission

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Summary

Introduction

The optical identification of quasi-stellar objects (quasars hereafter) by Matthews & Sandage (1963) enabled, for the first time, studies of the distant universe at z > 0.1. Quasars are recognised as highluminosity examples of Active Galactic Nuclei (AGN), powered by accretion onto a super-massive black hole (SMBH) (LyndenBell 1969; Shakura & Sunyaev 1973). The continuum variability of quasars, known soon after their discovery, allows us to peer directly into their central engines. Varying by 10-20% over timescales of months to years, the intrinsic variability of quasar continuum emission has long been theorised to be caused by changes in the environment close to the SMBH. Spanning the full range from gamma rays to radio, quasar SEDs exhibit both thermal (accretion disc, dust) and non-thermal (corona, jet) components. In the rest-frame UV-optical, thermal emission from the accretion disc is thought to manifest as the ‘Big Blue Bump’ (Shields 1978; Malkan & Sargent 1982), described by a sum of blackbody spectra over a range of

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