Radiative neutrino mass model from a mass dimension-11 $\Delta L =2 $ effective operator

TL;DR

This paper introduces a novel radiative Majorana neutrino mass model based on a high-dimension $ ext{dim-11}$ effective operator, analyzing its phenomenology and potential to explain experimental anomalies.

Contribution

It presents the first detailed phenomenological analysis of a neutrino mass model derived from a $ ext{dim-11}$ operator, highlighting its unique features and experimental viability.

Findings

Neutrino masses generated at two-loop order without proportionality to quark or lepton masses.

The model allows a high new physics scale up to $10^7$ TeV.

Parameter space can explain $R_{K^{(*)}}$ anomalies and muon g-2.

Abstract

We present the first detailed phenomenological analysis of a radiative Majorana neutrino mass model constructed from opening up a $\Delta L = 2$ mass-dimension-11 effective operator constructed out of standard model fields. While three such operators are generated, only one dominates neutrino mass generation, namely $O_{47} = \overline{L^C} L \overline{Q^C} Q \overline{Q} Q^C H H$, where $L$ denotes lepton doublet, $Q$ quark doublet and $H$ Higgs doublet. The underlying renormalisable theory contains the scalars $S_1 \sim (\bar{3},1,1/3)$ coupling as a diquark, $S_3 \sim (\bar{3},3,1/3)$ coupling as a leptoquark, and $\Phi_3 \sim (3,3,2/3)$, 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 $\Delta L = 2$ 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 decays and neutral-meson mixing. The acceptable parameter space can accommodate the anomalies in $R_{K^{(*)}}$ and the anomalous magnetic moment of the muon.