Issue |
A&A
Volume 377, Number 3, October III 2001
|
|
---|---|---|
Page(s) | 1056 - 1062 | |
Section | The Sun | |
DOI | https://doi.org/10.1051/0004-6361:20011125 | |
Published online | 15 October 2001 |
Excess GeV radiation and cosmic ray origin
Institut für Theoretische Physik, Lehrstuhl IV: Weltraum- und Astrophysik, Ruhr-Uni ver si tät Bochum, 44780 Bochum, Germany e-mail: mkp@tp4.ruhr-uni-bochum.de; rsch@tp4.ruhr-uni-bochum.de
Corresponding author: I. Büsching, ib@tp4.ruhr-uni-bochum.de
Received:
21
March
2001
Accepted:
8
August
2001
Particle acceleration at supernova remnant (SNR) shock waves is regarded as
the most probable mechanism for providing Galactic cosmic rays at energies
below 1015 eV. The Galactic cosmic ray hadron component would
in this picture result from the injection of relativistic
particles from many SNRs. It is well known
that the superposition of individual power law source spectra with dispersion
in the spectral index value, which behaviour is observed in the
synchrotron radio spectra of shell SNR, displays a positive curvature
in the total
spectrum and in particular shows a hardening at higher energies.
Recent observations
made with the EGRET instrument on the Compton Gamma-Ray Observatory
of the diffuse Galactic γ-ray emission reveal a spectrum which is
incompatible with the assumption that the cosmic ray spectra measured
locally hold throughout the Galaxy: the spectrum above 1 GeV,
where the emission is supposedly dominated by -decay, is harder
than that derived from the local cosmic ray proton spectrum.
We demonstrate that in case of a SNR origin
of cosmic ray nucleons part of this γ-ray excess may be attributed to
the
dispersion of the spectral indices in these objects. In global averages, as
are γ-ray line-of-sight integrals, this dispersion leads to a positive
curvature in the composite spectrum, and hence to modified
-decay
γ-ray spectra.
Key words: ISM: cosmic rays / ISM: supernova remnants / gamma rays: theory
© ESO, 2001
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