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Table 1
Parametrization of the AGN model.
Component | Description |
|
|
Continuum sources | 2 point-like sources of isotropic emission, |
power-law spectrum with a spectral flux F∗ ∝ ν− α, | |
photon index Γ = 1+α = variable, | |
distance from accretion disk mid-plane = ± 1 × 10-3 pc | |
|
|
Accretion disk | cylindrical disk with Rout = 4 × 10-3 pc, |
half-thickness = 3.25 × 10-7 pc, | |
irradiated by two isotropic sources, | |
filled with optically thick cold matter | |
|
|
Equatorial hot flow | wedge structure with Rin = 3 × 10-2 pc and Rout = 5 × 10-2 pc, |
half-opening angle (from the equatorial plane) = 20°, | |
equatorial Thomson optical depth = 1, | |
filled with electrons | |
|
|
Polar outflows | double-cone with Rin = 1 pc and Rout = 400 pc, |
half-opening angle (from the polar axis) = 33°, | |
vertical Thomson optical depth = 0.3, | |
filled with electrons | |
|
|
Dusty torus | elliptical torus with Rin = variable and Rout = 2.0 pc, |
half-opening angle (from the polar axis) = variable, | |
equatorial Mie optical depth ≫ 1, | |
filled with optically-thick cold matter |
Notes. Parametrization of the AGN model used in this paper (references are given in the text). A sketch of the model can be seen in Fig. 1.
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