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arxiv: 1003.4959 · v1 · pith:XOCJGZVQnew · submitted 2010-03-25 · 🌌 astro-ph.HE · astro-ph.CO· hep-ph· nucl-th

Neutrino Background Flux from Sources of Ultrahigh-Energy Cosmic-Ray Nuclei

classification 🌌 astro-ph.HE astro-ph.COhep-phnucl-th
keywords sourcesbackgroundneutrinonucleifluxinteractionscosmicicecube
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Motivated by Pierre Auger Observatory results favoring a heavy nuclear composition for ultrahigh-energy (UHE) cosmic rays, we investigate implications for the cumulative neutrino background. The requirement that nuclei not be photodisintegrated constrains their interactions in sources, therefore limiting neutrino production via photomeson interactions. Assuming a $dN_{\rm CR}/dE_{\rm CR} \propto E_{\rm CR}^{-2}$ injection spectrum and photodisintegration via the giant dipole resonance, the background flux of neutrinos is lower than $E_\nu^2 \Phi_\nu \sim {10}^{-9} {\rm GeV} {\rm cm}^{-2} {\rm s}^{-1} {\rm sr}^{-1}$ if UHE nuclei ubiquitously survive in their sources. This is smaller than the analogous Waxman-Bahcall flux for UHE protons by about one order of magnitude, and is below the projected IceCube sensitivity. If IceCube detects a neutrino background, it could be due to other sources, e.g., hadronuclear interactions of lower-energy cosmic rays; if it does not, this supports our strong restrictions on the properties of sources of UHE nuclei.

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  1. Ultraheavy Ultrahigh-Energy Cosmic Rays

    astro-ph.HE 2024-05 unverdicted novelty 7.0

    Ultraheavy nuclei have longer energy loss lengths at ≲300 EeV than lighter nuclei, allowing them to explain UHECRs above 100 EeV from sources like collapsars and neutron star mergers while predicting distinct shower maxima.