Table A.1.
Parameters of the model.
Symbol | Value | Units | Parameter |
---|---|---|---|
β | 0.5 a | – | 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 |
![]() |
Radius of the outflow at its base |
γ0 c | 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 |
![]() |
Outer radius of the accretion disk |
cos θ e | –1 to 1 | – | θ is the viewing angle |
m | 10 | M⊙ | Mass of the black hole |
Nphot | 107 − 108 | – | Number of simulated photon beams |
p f | 3 | – | Index of the Lorentz factor power-law distribution |
![]() |
1 | – | Lower limit of the Lorentz factor power-law distribution |
![]() |
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: 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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