2002
DOI: 10.1086/340857
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Dust Emission from Active Galactic Nuclei

Abstract: Unified schemes of active galactic nuclei (AGN) require an obscuring dusty torus around the central source, giving rise to Seyfert 1 line spectrum for pole-on viewing and Seyfert 2 characteristics in edge-on sources. Although the observed IR is in broad agreement with this scheme, the behavior of the 10 micron silicate feature and the width of the far-IR emission peak remained serious problems in all previous modeling efforts. We show that these problems find a natural explanation if the dust is contained in a… Show more

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Cited by 491 publications
(672 citation statements)
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“…When discussing these models, it's important to keep in mind that the accuracy or applicability of these models cannot be tested with data since it simply does not exist in enough detail to disentangle effects of geometry, distribution, optical depth, etc. It's also important to note that many have done work in this area, particularly modeling radiative transfer in local starburst populations to generate SEDs (Efstathiou & Rowan-Robinson, 1995;Efstathiou et al, 2000;Efstathiou & Siebenmorgen, 2009;Nenkova et al, 2002;Dullemond & van Bemmel, 2005;Piovan et al, 2006;Nenkova et al, 2008;Takagi et al, 2003;Fritz et al, 2006;Hönig et al, 2006;Schartmann et al, 2008), but here we try to focus on the techniques which have been most commonly employed for SED fitting of high-z dusty starbursts 11 . Silva et al (1998) developed the Grasil code to model galaxy emission by explicitly accounting for dust absorption and emission from the ultraviolet through to the far-infrared.…”
Section: Employing Dust Radiative Transfer Models and Empirical Templmentioning
confidence: 99%
“…When discussing these models, it's important to keep in mind that the accuracy or applicability of these models cannot be tested with data since it simply does not exist in enough detail to disentangle effects of geometry, distribution, optical depth, etc. It's also important to note that many have done work in this area, particularly modeling radiative transfer in local starburst populations to generate SEDs (Efstathiou & Rowan-Robinson, 1995;Efstathiou et al, 2000;Efstathiou & Siebenmorgen, 2009;Nenkova et al, 2002;Dullemond & van Bemmel, 2005;Piovan et al, 2006;Nenkova et al, 2008;Takagi et al, 2003;Fritz et al, 2006;Hönig et al, 2006;Schartmann et al, 2008), but here we try to focus on the techniques which have been most commonly employed for SED fitting of high-z dusty starbursts 11 . Silva et al (1998) developed the Grasil code to model galaxy emission by explicitly accounting for dust absorption and emission from the ultraviolet through to the far-infrared.…”
Section: Employing Dust Radiative Transfer Models and Empirical Templmentioning
confidence: 99%
“…A power-law extension of the restframe optical disk emission into the NIR is a common assumption for the primary source that is used as input for radiative transfer codes that model the torus emission (e.g. Granato & Danese 1994;Nenkova et al 2002;Fritz et al 2006;Stalevski et al 2012), but it is not universal. In particular, some torus models assume a steep fall of the disk spectrum longwards of 1 µm (e.g.…”
Section: Modelling Of the Continuum Emissionmentioning
confidence: 99%
“…All these models consider radiative transfer in an anisotropic, but homogenous dusty torus. Nenkova et al (2002) considered radiative transfer between several clouds of dust along radial rays through the torus, and overcame some difficulties of the former homogeneous models for the description of the spectral energy distributions. More recently, Schartmann et al (2005) described the three dimensional treatment of radiative transfer through dusty tori at hydrostatic equilibrium and succeed in reproducing both the mean large aperture spectra from UV to far-IR of several Seyfert type 1 galaxies, and the recent MIDI observations of two specified Seyfert type 2: Circinus and NGC 1068, except for the 9.7 µm silicate feature.…”
Section: Introductionmentioning
confidence: 99%