Fig. 1.

Sketch of the geometry (not to scale) assumed for the model. Seed electrons are accelerated in the gap and multiplied in and behind the gap through ADAF photons. For simplicity of drawing, photons are not shown in the in-gap and post-gap multiplication. After propagating away from the gap, the electron beam meets an emission-line photon field, driving a cascade, whose steady-state gamma-ray photon density is nγ and whose escaping flux is Fcasc. To convert nγ into Fcasc, cf. Eq. (3).
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