Abstract

Some of the phenomena related to the prompt gamma-ray burst emission could be interpreted as the presence of a consistent amount of material (Thomson optical depth ∼1) at rest and close to the source at a typical distance of ∼10 15 cm. The material optical depth τ=σ ΔR, where (n) is the average particle density over the distance ΔR, will attenuate the prompt gamma-ray flux by an amount e -τ , while producing a secondary flux proportional to 1-e -τ of scattered photons with a partly modified energy spectrum. This emission should be delayed with respect to the prompt gamma-ray emission by a time-scale which is directly related to the burst opening angle (θ j ) and to the scattering material space distribution (ΔR).

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