1. Weaker yet again: mass spectrum-consistent cosmological constraints on the neutrino lifetime.
- Author
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Chen, Joe Zhiyu, Oldengott, Isabel M., Pierobon, Giovanni, and Wong, Yvonne Y. Y.
- Subjects
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NEUTRINOS , *NEUTRINO mass , *COSMIC background radiation , *NEUTRINO detectors , *PHASE space - Abstract
We consider invisible neutrino decay ν H → ν l + ϕ in the ultra-relativistic limit and compute the neutrino anisotropy loss rate relevant for the cosmic microwave background (CMB) anisotropies. Improving on our previous work which assumed massless ν l and ϕ , we reinstate in this work the daughter neutrino mass m ν l in a manner consistent with the experimentally determined neutrino mass splittings. We find that a nonzero m ν l introduces a new phase space factor in the loss rate Γ T proportional to (Δ m ν 2 / m ν H 2) 2 in the limit of a small squared mass gap between the parent and daughter neutrinos, i.e., Γ T ∼ (Δ m ν 2 / m ν H 2) 2 (m ν H / E ν) 5 (1 / τ 0) , where τ 0 is the ν H rest-frame lifetime. Using a general form of this result, we update the limit on τ 0 using the Planck 2018 CMB data. We find that for a parent neutrino of mass m ν H ≲ 0.1 eV, the new phase space factor weakens the constraint on its lifetime by up to a factor of 50 if Δ m ν 2 corresponds to the atmospheric mass gap and up to 10 5 if the solar mass gap, in comparison with naïve estimates that assume m ν l = 0 . The revised constraints are (i) τ 0 ≳ (6 → 10) × 10 5 s and τ 0 ≳ (400 → 500) s if only one neutrino decays to a daughter neutrino separated by, respectively, the atmospheric and the solar mass gap, and (ii) τ 0 ≳ (2 → 6) × 10 7 s in the case of two decay channels with one near-common atmospheric mass gap. In contrast to previous, naïve limits which scale as m ν H 5 , these mass spectrum-consistent τ 0 constraints are remarkably independent of the parent mass and open up a swath of parameter space within the projected reach of IceCube and other neutrino telescopes in the next two decades. [ABSTRACT FROM AUTHOR]
- Published
- 2022
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