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Modeling the spectrum and composition of ultrahigh-energy cosmic rays with two populations of extragalactic sources
We fit the ultrahigh-energy cosmic-ray (UHECR, E ≳ 0.1 EeV) spectrum and composition data from the Pierre Auger Observatory at energies E ≳ 5 · 10 18 eV, i.e., beyond the ankle using two populations of astrophysical sources. One population, accelerating dominantly protons ( 1 H), extends up to the h...
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Published in: | The European physical journal. C, Particles and fields Particles and fields, 2021, Vol.81 (1), p.1-15, Article 59 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We fit the ultrahigh-energy cosmic-ray (UHECR,
E
≳
0.1
EeV) spectrum and composition data from the Pierre Auger Observatory at energies
E
≳
5
·
10
18
eV, i.e., beyond the ankle using two populations of astrophysical sources. One population, accelerating dominantly protons (
1
H), extends up to the highest observed energies with maximum energy close to the GZK cutoff and injection spectral index near the Fermi acceleration model; while another population accelerates light-to-heavy nuclei (
4
He,
14
N,
28
Si,
56
Fe) with a relatively low rigidity cutoff and hard injection spectrum. A significant improvement in the combined fit is noted as we go from a one-population to two-population model. For the latter, we constrain the maximum allowed proton fraction at the highest-energy bin within 3.5
σ
statistical significance. In the single-population model, low-luminosity gamma-ray bursts turn out to match the best-fit evolution parameter. In the two-population model, the active galactic nuclei is consistent with the best-fit redshift evolution parameter of the pure proton-emitting sources, while the tidal disruption events could be responsible for emitting heavier nuclei. We also compute expected cosmogenic neutrino flux in such a hybrid source population scenario and discuss possibilities to detect these neutrinos by upcoming detectors to shed light on the sources of UHECRs. |
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ISSN: | 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-021-08885-4 |