Majorana phases beyond neutrinoless double beta decay

A bstract The ν M SM is defined as the SM extended to include dimension-5 operators. In this model neutrino masses violate lepton number, and two parameters of the lepton mixing matrix, the Majorana phases, are yet to be constrained. One combination of these phases and the neutrino masses, often denoted by m ee , is probed by neutrinoless double beta decays (0 νββ ). We explore what information may be obtained beyond 0 νββ , and how it depends on the lightest neutrino mass. We point out that with current central values of the mixing parameters, ∆ L e = 2 and ∆ L e = ∆ L μ = 1 (or ∆ L e = 2 and ∆ L μ = 2) processes cannot simultaneously vanish, providing a no-lose theorem, in principle, for excluding the ν M SM, even in the case of normal mass ordering.

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Publication Details

Journal
Journal of High Energy Physics
Published
2024-10-11
DOI
https://doi.org/10.1007/jhep10(2024)100
Citations
2
Primary Topic
Neutrino Physics Research
Type
article
Field-Weighted Citation Impact
1.32

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article

Majorana phases beyond neutrinoless double beta decay

Avital Dery, Zoltan Ligeti, Stefania Gori, Yuval Grossman
2 citations
Journal of High Energy Physics
Neutrino Physics Research
1.32
article

Majorana phases beyond neutrinoless double beta decay

Avital Dery, Zoltan Ligeti, Stefania Gori, Yuval Grossman
article en
2 citations

Abstract

A bstract The ν M SM is defined as the SM extended to include dimension-5 operators. In this model neutrino masses violate lepton number, and two parameters of the lepton mixing matrix, the Majorana phases, are yet to be constrained. One combination of these phases and the neutrino masses, often denoted by m ee , is probed by neutrinoless double beta decays (0 νββ ). We explore what information may be obtained beyond 0 νββ , and how it depends on the lightest neutrino mass. We point out that with current central values of the mixing parameters, ∆ L e = 2 and ∆ L e = ∆ L μ = 1 (or ∆ L e = 2 and ∆ L μ = 2) processes cannot simultaneously vanish, providing a no-lose theorem, in principle, for excluding the ν M SM, even in the case of normal mass ordering.

Journal of High Energy PhysicsVol. 2024(10)
Lawrence Berkeley National Laboratory (US), University of California, Santa Cruz (US), Cornell University (US), University of California System (US), University of California, Berkeley (US)
National Science Foundation, U.S. Department of Energy, Weizmann Institute of Science, High Energy Physics
Openalex Percentile: Top 11%
Neutrino Physics Research
1.32
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Majorana phases beyond neutrinoless double beta decay — Avital Dery, Zoltan Ligeti, et al. · Journal of High Energy Physics (2024) | TGRS Research Map | TGRS