Abstract

We present a detailed study of a combined singlet-doublet scalar and singlet-doublet fermion model for dark matter. These models have only been studied separately in the past. We show that their combination allows for the radiative generation of neutrino masses, but that it also implies the existence of lepton-flavour violating (LFV) processes. We first analyse the dark matter, neutrino mass and LFV aspects separately. We then perform two random scans for scalar dark matter imposing Higgs mass, relic density and neutrino mass constraints, one over the full parameter space, the other over regions where scalar-fermion coannihilations become important. In the first case, a large part of the new parameter space is excluded by LFV, and the remaining models will be probed by XENONnT. In the second case, direct detection cross sections are generally too small, but a substantial part of the viable models will be tested by future LFV experiments. Possible constraints from the LHC are also discussed.

Highlights

  • Ν φ ν ν matter with at most four additional fields have been classified [21] following the notation of a systematic study of the d = 5 Weinberg operator at one-loop order [22]

  • These models have only been studied separately in the past. We show that their combination allows for the radiative generation of neutrino masses, but that it implies the existence of lepton-flavour violating (LFV) processes

  • We investigate the influence of the Yukawa couplings y1 and y2 on the sum of neutrino masses for singlet scalar dark matter of mass MS,S = 1 TeV, which does not mix with the doublet scalar (A = 0), but couples to the doublet fermion with fixed strength g1i = 0.1

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Summary

Particle content and interactions in the model

In our model T1-2-A, the SM is extended by two scalars, a real singlet φS and a complex doublet φD, and two fermions, a Weyl singlet ψS and a vector-like doublet ψD, which can be decomposed into two chiral Weyl fermions ψD1, ψD2. Involves in general five different couplings of the new scalars with the complex SM Higgs doublet H, which acquires a vacuum expectation value v = 246 GeV and breaks the electroweak symmetry. One of these couplings (A) links the singlet and doublet scalars with the SM Higgs in a Yukawa-like form. The presence of scalar and fermion singlets and doublets allows to define couplings of the new particles to the SM leptons,. Is the SM lepton doublet of generation i These new Yukawa couplings gij, together with the interactions of eqs.

Dark matter relic density
Neutrino masses
Lepton flavour violation
Numerical results
Random scan
Coannihilation region
LHC constraints
Conclusion
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