The universal power spectrum of Quasars in optical wavelengths: Break timescale scales directly with both black hole mass and accretion rate
arXiv:2306.11099
Abstract
Aims: Establish the dependence of variability properties, such as characteristic timescales and variability amplitude, on basic quasar parameters such as black hole mass and accretion rate, controlling for the rest-frame wavelength of emission. Methods: Using large catalogs of quasars, we selected the g-band light curves for 4770 objects from the Zwicky Transient Facility archive. All selected objects fall into a narrow redshift bin, , but cover a wide range of accretion rates in Eddington units (REdd) and black hole masses (). We grouped these objects into 26 independent bins according to these parameters, calculated low-resolution -band variability power spectra for each of these bins, and approximated the power spectra with a simple analytic model that features a break at a timescale . Results: We found a clear dependence of the break timescale on REdd, on top of the known dependence of on the black hole mass . In our fits, REdd , where the ranges in the exponents correspond to the best-fitting parameters of different power spectrum models. Scaling to the orbital timescale of the innermost stable circular orbit (ISCO), , results approximately in REdd. The observed values of are longer than the orbital timescale at the light-weighted average radius of the disc region emitting in the (observer frame) -band. The different scaling of the break frequency with and REdd shows that the shape of the variability power spectrum cannot be solely a function of the quasar luminosity, even for a single rest-frame wavelength. Finally, the best-fitting models have slopes above the break in the range -2.5 and -3. A slope of -2, as in the damped random walk models, fits the data significantly worse.
Accepted for publication in A&A