Astronomy and Astrophysics – Astrophysics
Scientific paper
Sep 1996
adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=1996a%26a...313..457w&link_type=abstract
Astronomy and Astrophysics, v.313, p.457-464
Astronomy and Astrophysics
Astrophysics
1
Galaxy: Center, Gamma-Rays: Theory, Radiation Mechanisms: Non-Thermal, Scattering
Scientific paper
Guided by the HEXAGONE gamma-ray observations of the Galactic Center region we performed a series of Monte Carlo calculations to describe the gamma-ray spectrum between 100 and 500keV by a simple model with as few parameters as possible. This energy range is governed by the continuum spectrum of orthopositronium decay, by Compton scattered annihilation radiation (511keV line + orthopositronium continuum), and by the high energy part of an inverse power law X-ray spectrum. The excess flux above the extrapolated power law spectrum is often ascribed to a orthopositronium continuum. We find that a clear distinction between the interpretations as a "3γ" continuum or as Compton scattered annihilation radiation cannot be achieved for a wide range of the parameters f_ps_ and τ_st_. But the observation of a 170keV backscattering feature strongly requires the presence of Compton scattering. From our models we conclude that the observed spectrum can be best modeled with a small positronium fraction f_ps_~0.2, an optical thin (back)scattering medium (τ_tot_<1), and the gamma-ray source lying in front of the scattering medium, i.e. τ_st_~0. The small positronium fraction is contradictory to the generally assumed value of f_ps_~0.9 for positron annihilation in the interstellar medium. In order to explain the redshift of the 170keV feature we propose a plausible alternative scenario for the Compton scattering region near the Galactic Center containing a jet which has an inhomogeneous structure. A single clump or blob which is moving away from us serves as the backscattering medium while the annihilation region is confinded to a relatively small, not directly observable area, nearly at rest, at the bottom of the jet acceleration region.
Duschl Wolfgang J.
Hof Michael
Tscharnuter Werner M.
Wehrse Rainer
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