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Table A.1.

Parameters of the model.

Symbol Value Units Parameter
β 0.5a Index of the radial dependence with height of the outflow
τ 1 − 6 Optical depth to electron scattering along the axis of the outflow
R0 50 − 1500 R g b $ R_{\mathit{g}}^{\,b} $ Radius of the outflow at its base
γ0c 1.10–1.15 Lorentz factor of the electrons, when the flow is coasting
kTBB 0.2 keV Characteristic energy of the input soft photons
z0 5 Rg Distance of the bottom of the outflow from the black hole
H 105 Rg Height of the outflow
z1 50 Rg Height of the acceleration zone
a 0.5 Exponent of the velocity profile in the acceleration zone
Rdisk 103 R ISCO d $ R_{\mathrm{ISCO}}^{\,d} $ Outer radius of the accretion disk
cos θe –1 to 1 θ is the viewing angle
m 10 M Mass of the black hole
Nphot 107 − 108 Number of simulated photon beams
pf 3 Index of the Lorentz factor power-law distribution
γ min f $ \gamma_{\mathrm{min}}^{\,f} $ 1 Lower limit of the Lorentz factor power-law distribution
γ max f $ \gamma_{\mathrm{max}}^{\,f} $ 500 Upper limit of the Lorentz factor power-law distribution

Notes. a: β = 0.5 assumes a parabolic outflowb: Gravitational radius Rg = Gm/c2. Rg ≈ 1.48 × 106 cm for a m = 10 M black holec: γ 0 = 1 / 1 ( v 0 2 + v 2 ) / c 2 $ \gamma_0 = 1/\sqrt{1-(\mathit{v}_0^2+\mathit{v}_\perp^2)/c^2} $d: Radius of the inner-most stable circular orbit.e: θ is the angle between the observer and the outflow axis. The code records the escaping direction of the photon in bins of 0.1 in w = cos θ, from w = −1 to w = 1. Negative values indicate back scattering.f: For the computation of the radio emission.

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