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Photomeson-threshold origin of the TeV break in astrophysical neutrinos: Spectrum, flavor, resolved sources, and the ultrahigh-energy landscape

Vernon Barger*

  • *Contact author: barger@pheno.wisc.edu

APS Open Sci. 1, 000175 – Published 19 October, 2026

DOI: https://doi.org/10.1103/l9sf-3yht

Abstract

IceCube observes a break near 30 TeV in the diffuse astrophysical neutrino spectrum. We interpret it as the photomeson (pγ) threshold. Accelerated protons interact with the soft x rays of accreting black holes through the Δ(1232) resonance. One kinematic relation sets the break energy from the target field’s lowest photon energy, the seed scale ɛ0. The measured break fixes ɛ0≃0.13keV and supplies the low-energy suppression no sum of falling power laws can produce. Building on the Δ(1232) identification of Khatee Zathul, Fang, Halzen, and Hooper and the single-source-class photo-pion fit of Winter, Fiorillo, and Buson, we give closed-form relations that invert the four broken-power-law fit parameters to the source physics with no remaining freedom, namely, γ2=s and γ1=s−(αx−1) (s, αx the proton and target photon indices), and Ebr∝[(1+z¯)ɛ0]−1. The break width then measures the population’s uniformity. The total smearing is bounded to σs≤0.235dex (68% confidence level), no broader than redshift alone must make it, and the seed scale is the same across the sources to within a factor ≲1.5, a constraint mean-spectrum fits do not provide. The model also predicts that below-break neutrinos come on average from higher redshifts than those above. The threshold also fixes the flavor and neutrino-antineutrino composition, including the energy-dependent ν¯e fraction and the Glashow-resonance discriminator computed in detail by Winter et al., matching current flavor data. Inverted source by source, the relation gives each resolved IceCube source its target photon scale, from the keV coronae of NGC 1068 and PKS 1424+240 to the ∼20eV jet of TXS 0506+056. That two-decade spread means they cannot supply the homogeneous break. It requires a separate, fainter population. KM3-230213A points to a warm-dust target, ɛ0≃0.02eV, unless cosmogenic.

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