Modeling the spectrum and composition of ultrahigh-energy cosmic rays with two populations of extragalactic sources
Abstract We fit the ultrahigh-energy cosmic-ray (UHECR, $$E\gtrsim 0.1$$ E ≳ 0.1 EeV) spectrum and composition data from the Pierre Auger Observatory at energies $$E\gtrsim 5\cdot 10^{18}$$ E ≳ 5 · 10 18 eV, i.e., beyond the ankle using two populations of astrophysical sources. One population, accel...
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doaj-dc2eeca0130049cf85f6f5cf11905ad32021-01-24T12:40:54ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522021-01-0181111510.1140/epjc/s10052-021-08885-4Modeling the spectrum and composition of ultrahigh-energy cosmic rays with two populations of extragalactic sourcesSaikat Das0Soebur Razzaque1Nayantara Gupta2Astronomy and Astrophysics Group, Raman Research InstituteCentre for Astro-Particle Physics (CAPP) and Department of Physics, University of JohannesburgAstronomy and Astrophysics Group, Raman Research InstituteAbstract We fit the ultrahigh-energy cosmic-ray (UHECR, $$E\gtrsim 0.1$$ E ≳ 0.1 EeV) spectrum and composition data from the Pierre Auger Observatory at energies $$E\gtrsim 5\cdot 10^{18}$$ E ≳ 5 · 10 18 eV, i.e., beyond the ankle using two populations of astrophysical sources. One population, accelerating dominantly protons ( $$^1$$ 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 ( $$^4$$ 4 He, $$^{14}$$ 14 N, $$^{28}$$ 28 Si, $$^{56}$$ 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 $$\sigma $$ 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.https://doi.org/10.1140/epjc/s10052-021-08885-4 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Saikat Das Soebur Razzaque Nayantara Gupta |
spellingShingle |
Saikat Das Soebur Razzaque Nayantara Gupta Modeling the spectrum and composition of ultrahigh-energy cosmic rays with two populations of extragalactic sources European Physical Journal C: Particles and Fields |
author_facet |
Saikat Das Soebur Razzaque Nayantara Gupta |
author_sort |
Saikat Das |
title |
Modeling the spectrum and composition of ultrahigh-energy cosmic rays with two populations of extragalactic sources |
title_short |
Modeling the spectrum and composition of ultrahigh-energy cosmic rays with two populations of extragalactic sources |
title_full |
Modeling the spectrum and composition of ultrahigh-energy cosmic rays with two populations of extragalactic sources |
title_fullStr |
Modeling the spectrum and composition of ultrahigh-energy cosmic rays with two populations of extragalactic sources |
title_full_unstemmed |
Modeling the spectrum and composition of ultrahigh-energy cosmic rays with two populations of extragalactic sources |
title_sort |
modeling the spectrum and composition of ultrahigh-energy cosmic rays with two populations of extragalactic sources |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2021-01-01 |
description |
Abstract We fit the ultrahigh-energy cosmic-ray (UHECR, $$E\gtrsim 0.1$$ E ≳ 0.1 EeV) spectrum and composition data from the Pierre Auger Observatory at energies $$E\gtrsim 5\cdot 10^{18}$$ E ≳ 5 · 10 18 eV, i.e., beyond the ankle using two populations of astrophysical sources. One population, accelerating dominantly protons ( $$^1$$ 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 ( $$^4$$ 4 He, $$^{14}$$ 14 N, $$^{28}$$ 28 Si, $$^{56}$$ 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 $$\sigma $$ 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. |
url |
https://doi.org/10.1140/epjc/s10052-021-08885-4 |
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