Answers are grounded in this paper and cite their sources.
The Waxman-Bahcall bound converts the energy budget of ultra-high-energy cosmic rays into a ceiling on the diffuse neutrino flux. This paper recomputes the bound with the source-evolution factor evaluated as an explicit integral rather than inserted as a canonical constant. For star-formation-like evolution the integral gives an evolution factor of 9.71, against the canonical value near 3 often quoted, and the corresponding per-flavour bound is 3.569e-08 in E-squared flux units — a factor 1.43 above the measured contained-event level of 2.500e-08. Truncating the source history at redshift 8, as a bounced thermal history would, lowers the evolution factor to 9.2 and the bound by only 5.18 per cent, to 3.384e-08. With the canonical evolution factor of 3 the bound evaluates to 1.103e-08, below the measurement. The bound's verdict on the data therefore depends entirely on which evolution factor is defended — a dependence the integral makes impossible to hide. The study is computed from stated assumptions, not measured.
No takes yet. Share an insight, caveat, or question.
William Alexander Aldred (2026) studied this question.
Synapse has enriched 8 closely related papers on similar clinical questions. Consider them for comparative context: