Abstract

In this paper, we study the viability of having a fermion Dark Matter particle below the TeV mass scale in connection to the neutrino mass generation mechanism. The simplest realisation is achieved within the scotogenic model where neutrino masses are generated at the 1-loop level. Hence, we consider the case where the dark matter particle is the lightest -odd Majorana fermion running in the neutrino mass loop. We assume that lepton number is broken dynamically due to a lepton number carrier scalar singlet which acquires a non-zero vacuum expectation value. In the present scenario the Dark Matter particles can annihilate via t- and s-channels. The latter arises from the mixing between the new scalar singlet and the Higgs doublet. We identify three different Dark Matter mass regions below 1 TeV that can account for the right amount of dark matter abundance in agreement with current experimental constraints. We compute the Dark Matter-nucleon spin-independent scattering cross-section and find that the model predicts spin-independent cross-sections ‘naturally’ dwelling below the current limit on direct detection searches of Dark Matter particles reported by XENON1T.

Highlights

  • The observed fundamental particles as well as their interactions via the strong and electroweak forces are well described under the Standard Model (SM) picture

  • In this work we have studied the scotogenic model with spontaneous breaking of lepton number

  • We have shown that it is possible to account for the whole amount of dark matter (DM) relic density thanks to the scalar singlet used to break lepton number which mixes with the CP-even part of the SM Higgs doublet

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Summary

INTRODUCTION

The observed fundamental particles as well as their interactions via the strong and electroweak forces are well described under the Standard Model (SM) picture. The simplest idea in this regard is the so-called Scotogenic model [14], where the neutrino masses are generated at the 1-loop level In this model, the DM candidate happens to be the lightest particle running inside the loop with an odd charge under a Z2 discrete symmetry. One is mediated by Z2-odd particles (t-channel) [24] and the other one (s-channel) [18, 25] coming from the mixing between the scalar singlet and the SM model Higgs after the spontaneous breaking of lepton number and electroweak symmetries. The latter helps to explain DM relic abundance in the Universe for DM masses below the TeV region.

THE MODEL
Mass spectrum
Boundedness conditions
Searches of new physics
Dark matter searches
Neutrino oscillation parameters
NUMERICAL ANALYSIS
Findings
CONCLUSIONS
Full Text
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