Abstract
We propose a new model with the Majorana neutrino masses generated at two-loop level, in which the lepton number violation (LNV) processes, such as neutrino-less double beta decays, are mainly induced by the dimension-7 LNV effective operator $$ {\mathcal{O}}_7={\overline{l}}_R^c{\gamma}^{\mu }{L}_L\left({D}_{\mu}\varPhi \right)\varPhi \varPhi $$ . Note that it is necessary to impose an Z2 symmetry in order that $$ {\mathcal{O}}_7 $$ dominates over the conventional dimension-5 Weinberg operator, which naturally results in a stable Z2-odd neutral particle to be the cold dark matter candidate. More interestingly, due to the non-trivial dependence of the charged lepton masses, the model predicts the neutrino mass matrix to be in the form of the normal hierarchy. We also focus on a specific parameter region of great phenomenological interests, such as electroweak precision tests, dark matter direct searches along with its relic abundance, and lepton flavor violation processes.
Highlights
The modelIn order to produce O7 at one-loop level, we introduce two scalars: s : (1, 2) and χ : (2, 1/2), and three vector-like fermions D(L,R)i : (2, 1/2) with i = 1, 2 and 3 to the SM under SU(2)L × U(1)Y
Such a connection has been already exemplified by some recent three-loop neutrino mass models [13, 39,40,41], which realize the dimension-9 effective operator O9 = lcRlR[(DμΦ)Φ]2 with the DM embedded in the loop
We propose a new model with the Majorana neutrino masses generated at two-loop level, in which the lepton number violation (LNV) processes, such as neutrinoless double beta decays, are mainly induced by the dimension-7 LNV effective operator O7 = ̄lRc γμLL(DμΦ)ΦΦ
Summary
In order to produce O7 at one-loop level, we introduce two scalars: s : (1, 2) and χ : (2, 1/2), and three vector-like fermions D(L,R)i : (2, 1/2) with i = 1, 2 and 3 to the SM under SU(2)L × U(1)Y. A Z2 symmetry is imposed, in which only the new particles carry odd charges. The relevant new parts of the Lagrangian are given by. As for the new fermions, we have the tree-level relation MDi± = MDi0 for each Di doublet. The mass splittings between the charge and neutral components of the inert fermion doublets can only be induced by loop corrections with values around a few hundred MeV [44].
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