Cold Accretion Disks and Lineless Quasars
Ari Laor, Shane W. Davis

TL;DR
This paper proposes that very high-velocity quasars may have accretion disks too cold to produce ionizing photons, explaining the rarity of line-emitting quasars with v>10,000 km/s and predicting a population of weak emission line quasars with specific spectral features.
Contribution
It introduces a model linking accretion disk temperature to quasar velocity, suggesting lineless quasars result from cold disks, and predicts observable spectral signatures for these objects.
Findings
Quasars with v>10,000 km/s likely have non-ionizing, cold accretion disks.
Weak emission line quasars may be explained by cold disk SEDs.
Observed SEDs of some WLQ match cold accretion disk models.
Abstract
The optical-UV continuum of quasars is broadly consistent with the emission from a geometrically thin optically thick accretion disk (AD). The AD produces the ionizing continuum which powers the broad and narrow emission lines. The maximum AD effective temperature is given by Teff=fmax(Mdot/M^2)^1/4, where M is the black hole mass, Mdot the accretion rate, and fmax is set by the black hole spin a_*. For a low enough value of Mdot/M^2 the AD may become too cold to produce ionizing photons. Such an object will form a lineless quasar. This occurs for a local blackbody (BB) AD with a luminosity Lopt=10^46 erg/s for M>3.6E9 Msun, when a_*=0, and for M>1.4E10 Msun, when a_*=0.998. Using the AD based Mdot, derived from M and Lopt, and the reverberation based M, derived from Lopt and the Hbeta FWHM, v, gives Teff \propto Lopt^-0.13v^-1.45. Thus, Teff is mostly set by v. Quasars with a local BB…
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