A United Model for the cosmic ray energy spectra and anisotropy in the energy range 100 - 100 000 GeV
arXiv:1203.6458 · doi:10.1088/1742-6596/409/1/012028
Abstract
We propose a model where a supernova explodes in some vicinity of our solar system (some tens of parsecs) in the recent past (some tens of thousands years) with the energy release in cosmic rays of order of erg. The flux from this supernova is added to an isotropic flux from other sources. We consider the case where the Sun's location is not in some typical for Our Galaxy average environment, but in the Local Superbubble about 100 pc across, in which the diffusion coefficient , with the value of . We describe the energy dependence of the anisotropy of cosmic rays in the TeV region, together with the observed features of the energy spectrum of protons found in direct measurements. Our model provides a natural explanation to the hardening of the proton spectrum at 200 GeV, together with the observed steepening of the spectrum above 50 TeV.
arXiv comment5 pages, 3 figures, accepted for publication in Journal of Physics:Conference Series, 23rd ECRS, Moscow, 2012. We have added the discussion of Geminga as a possible local source
References in corpus (11)
- PAMELA Measurements of Cosmic-ray Proton and Helium Spectra
- Observation of the Anisotropy of 10 TeV Primary Cosmic Ray Nuclei Flux with the Super-Kamiokande-I Detector
- Diffusive propagation of cosmic rays from supernova remnants in the Galaxy. II: anisotropy
- Three component model of cosmic ray spectra from 10 GeV to 100 PeV
- Large-Scale Sidereal Anisotropy of Galactic Cosmic-Ray Intensity Observed by the Tibet Air Shower Array
- The Tunka-133 EAS Cherenkov light array: status of 2011
- Nearby supernova remnants and the cosmic-ray spectral hardening at high energies
- Energy dependence of Ti/Fe ratio in the Galactic cosmic rays measured by the ATIC-2 experiment
- Keynote Lecture: Galactic and Extragalactic Bubbles
- Supernova remnants as cosmic ray factories
- To the interpretation of the upturn observed by ATIC in heavy nuclei to iron ratios