4.7 Article

Dust inflated accretion disc as the origin of the broad line region in active galactic nuclei

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 474, Issue 2, Pages 1970-1994

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stx2850

Keywords

galaxies: active; quasars: emission lines; quasars: general

Funding

  1. Israel Science Foundation [1561/13]

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The broad line region (BLR) in active galactic nuclei (AGNs) is composed of dense gas (similar to 10(11) cm(-3)) on sub-pc scale, which absorbs about 30 per cent of the ionizing continuum. The outer size of the BLR is likely set by dust sublimation, and its density by the incident radiation pressure compression (RPC). But, what is the origin of this gas, and what sets its covering factor (CF)? Czerny & Hryniewicz (2011) suggested that the BLR is a failed dusty wind from the outer accretion disc. We explore the expected dust properties, and the implied BLR structure. We find that graphite grains sublimate only at T similar or equal to 2000K at the predicted density of similar to 10(11) cm(-3), and therefore large graphite grains (>= 0.3 mu m) survive down to the observed size of the BLR, R-BLR. The dust opacity in the accretion disc atmosphere is similar to 50 times larger than previously assumed, and leads to an inflated torus-like structure, with a predicted peak height at R-BLR. The illuminated surface of this torus-like structure is a natural place for the BLR. The BLR CF is mostly set by the gas metallicity, the radiative accretion efficiency, a dynamic configuration and ablation by the incident optical-UV continuum. This model predicts that the BLR should extend inwards of RBLR to the disc radius where the surface temperature is similar or equal to 2000 K, which occurs at R-in similar or equal to 0.18R(BLR). The value of R-in can be tested by reverberation mapping of the higher ionization lines, predicted by RPC to peak well inside R-BLR. The dust inflated disc scenario can also be tested based on the predicted response of R-BLR and the CF to changes in the AGN luminosity and accretion rate.

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