Radiative neutrino mass model from a mass dimension-11 ∆L = 2 effective operator

A bstract We present the first detailed phenomenological analysis of a radiative Majorana neutrino mass model constructed from opening up a ∆ L = 2 mass-dimension-11 effective operator constructed out of standard model fields. While three such operators are generated, only one dominates neutrino mas...

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Veröffentlicht in:The journal of high energy physics 2020-03, Vol.2020 (3), p.1-51, Article 150
Hauptverfasser: Gargalionis, John, Popa-Mateiu, Iulia, Volkas, Raymond R.
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Sprache:eng
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Zusammenfassung:A bstract We present the first detailed phenomenological analysis of a radiative Majorana neutrino mass model constructed from opening up a ∆ L = 2 mass-dimension-11 effective operator constructed out of standard model fields. While three such operators are generated, only one dominates neutrino mass generation, namely O 47 = L C ¯ L Q C ¯ L Q ¯ Q C HH , where L denotes lepton doublet, Q quark doublet and H Higgs doublet. The under- lying renormalisable theory contains the scalars S 1 ∼ 3 ¯ 1 1 / 3 coupling as a diquark, S 3 ∼ 3 ¯ 3 1 / 3 coupling as a leptoquark, and Φ 3  ∼ (3, 3, 2/3), which has no Yukawa couplings but does couple to S 1 and S 3 in addition to the gauge fields. Neutrino masses and mixings are generated at two-loop order. A feature of this model that is different from many other radiative models is the lack of proportionality to any quark and charged- lepton masses of the neutrino mass matrix. One consequence is that the scale of new physics can be as high as 10 7 TeV, despite the operator having a high mass dimension. This raises the prospect that ∆ L = 2 effective operators at even higher mass dimensions may, when opened up, produce phenomenologically-viable radiative neutrino mass models. The parameter space of the model is explored through benchmark slices that are subject to experimental constraints from charged lepton flavour-violating decays, rare meson de- cays and neutral-meson mixing. The acceptable parameter space can accommodate the anomalies in R K ( ∗ ) and the anomalous magnetic moment of the muon.
ISSN:1029-8479
1029-8479
DOI:10.1007/JHEP03(2020)150