Abstract

We model the spectropolarimetric signature resulting from the radiative coupling between the innermost parts of active galactic nuclei (AGNs). We use a new public version of STOKES, a Monte Carlo radiative transfer code presented in the first paper of this series. The code has been significantly improved for computational speed and polarization imaging has been implemented. We couple continuum sources with equatorial scattering regions, polar outflows, and toroidal obscuring dust and we study the resulting polarization. We compute a grid of thermal AGN models for different half-opening angles of the torus and polar winds. We also consider a range of optical depths for equatorial and polar electron scattering and investigate how the model geometry influences the type-1/type-2 polarization dichotomy for thermal AGNs. We put new constrains on the inflowing medium within the inner walls of the torus. The inflow should be confined to the common equatorial plane of the torus and the accretion disc and have a radial optical depth of 1 < tau < 3. Our modeling of type-1 AGNs also indicates that the torus is more likely to have a large (~ 60{\deg}) half-opening angle. Polarization perpendicular to the axis of the torus may arise at a type-1 viewing angle for a torus half-opening angle of 30{\deg}- 45{\deg} or polar outflows with an optical depth near unity. Our modeling suggests that most Seyfert-2 AGN must have a half-opening angle > 60{\deg} to match the level of perpendicular polarization expected. If outflows are collimated by the torus inner walls, they must not be optically thick (tau < 1) in order to preserve the polarization dichotomy. The wind's optical depth is found not to play a critical role for the degree of polarization of type-2 thermal AGNs but it has a significant impact on the type-1/type-2 polarization dichotomy when the optical depth exceeds tau = 0.3.

Highlights

  • Active galactic nuclei (AGN) are divided observationally into a number ofclasses based on the optical spectrum and radio properties

  • We considered a range of optical depths for equatorial and polar electron scattering and investigated how the model geometry influences the type-1/type-2 polarization dichotomy for thermal AGNs

  • If the broad-line region (BLR) is directly visible in the optical, the AGN is of type-1, while if the BLR is not visible, it is of type-2

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Summary

Introduction

Active galactic nuclei (AGN) are divided observationally into a number of (sub-)classes based on the optical spectrum and radio properties. Keel (1980) discovered that nearby type-1 AGNs are preferentially oriented face-on while nearby type-2 AGNs are randomly oriented. These discoveries showed that the viewing angle of the observer is a key element in AGN classification (Antonucci 1993). The ionizing continuum source and its surrounding BLR sit inside the funnel of the torus In this scenario the half-opening angle of the torus can be estimated from the ratio of type-1 to type-2 AGNs in an isotropically selected sample and from the “infra-red calorimeter” – the relative strength of the mid-IR continuum that arises from dust reprocessing of the higher-energy continuum (see Antonucci 2012). There is evidence that the opening angle is a function of luminosity (Lawrence 1991) or accretion history (Wang & Zhang 2007)

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