2006
DOI: 10.1051/0004-6361:20065108
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Three component model of cosmic ray spectra from 10 GeV to 100 PeV

Abstract: Aims. A model to describe cosmic ray spectra in the energy region from 10 10 to 10 17 eV is suggested based on the assumption that Galactic cosmic ray flux is a mixture of fluxes accelerated by shocks from nova and supernova of different types. Methods. We analyze recent experimental data on cosmic ray spectra obtained in direct measurements above the atmosphere and data obtained with ground extensive air shower (EAS) arrays. Results. The model of the three classes of cosmic ray sources is consistent with dire… Show more

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Cited by 152 publications
(143 citation statements)
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References 17 publications
(15 reference statements)
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“…Consequently, the magnitude of the prompt component strongly depends on the primary model. Except for the proposal by Zatsepin and Sokolskaya [35], each of the flux assumptions can be reconciled with the data without a major spectral adjustement.…”
Section: Energy Spectrummentioning
confidence: 98%
See 1 more Smart Citation
“…Consequently, the magnitude of the prompt component strongly depends on the primary model. Except for the proposal by Zatsepin and Sokolskaya [35], each of the flux assumptions can be reconciled with the data without a major spectral adjustement.…”
Section: Energy Spectrummentioning
confidence: 98%
“…A well-known proposal by Hillas postulates two galactic sources, one accounting for the knee, the other for the presumptive knee-like feature at 300 PeV [34]. Another model, by Zatsepin and Sokolskaya, identifies three distinct types of galactic sources to account for the flux up to 100 PeV [35]. The hardening of the spectrum around the "ankle" at several EeV can be described elegantly by a pure protonic flux and its interaction with CMB radiation [36] or, more in line with recent experimental results, in terms of separate light and heavy components [37].…”
Section: Cosmic Rays In the Icecube Energy Rangementioning
confidence: 99%
“…Additional flux variants are calculated using the analytic air shower evolution code of [46][47][48]. The cosmic spectrum variants considered are the Gaisser-Hillas [45], Zatsepin-Sokolskaya [49], and Poly-gonato models [50]. The hadronic models considered are QGSJET-II-4 [51] and SIBYILL2.3 [52].…”
Section: Prl 117 071801 (2016) P H Y S I C a L R E V I E W L E T T Ementioning
confidence: 99%
“…To begin with, a break in α could arise from a modification of the conventional diffusive shock acceleration (DSA) scheme, as suggested by Malkov et al (2012) and Ohira & Ioka (2011). In the same vein, the possibility of different classes of CR sources has been proposed some time ago by Stanev et al (1993) and Zatsepin & Sokolskaya (2006); for instance, cosmic rays accelerated in the magnetized winds of exploding Wolf-Rayet and red supergiant stars could have a double spectrum, with a hard component produced in the polar cap regions of these objects. According to Biermann et al (2010), this hard component would take over the smooth one above a few hundred GeV, hence the observed break in the proton and helium spectra.…”
Section: Introductionmentioning
confidence: 99%