Abstract

We investigate whether right-handed neutrinos can play the role of the dark matter of the Universe and be generated by the freeze-out production mechanism. In the standard picture, the requirement of a long lifetime of the right-handed neutrinos implies a small neutrino Yukawa coupling. As a consequence, they never reach thermal equilibrium, thus prohibiting production by freeze-out. We note that this limitation is alleviated if the neutrino Yukawa coupling is large enough in the early Universe to thermalize the sterile neutrinos, and then becomes tiny at a certain moment, which makes them drop out of equilibrium. As a concrete example realization of this framework, we consider a Froggatt-Nielsen model supplemented by an additional scalar field which obeys a global symmetry (not the flavour symmetry). Initially, the vacuum expectation value of the flavon is such, that the effective neutrino Yukawa coupling is large and unsuppressed, keeping them in thermal equilibrium. At some point the new scalar also gets a vacuum expectation value that breaks the symmetry. This may occur in such a way that the vev of the flavon is shifted to a new (smaller) value. In that case, the Yukawa coupling is reduced such that the sterile neutrinos are rendered stable on cosmological time scales. We show that this mechanism works for a wide range of sterile neutrino masses.

Highlights

  • The identity and the character of the Dark Matter (DM) of the Universe and the origin of the minute mass of neutrinos in the Standard Model of particle physics (SM) are two of the most prominent problems in fundamental physics

  • Assuming that the type I seesaw mechanism is responsible for the masses of SM neutrinos, one immediately wonders whether one of the new sterile neutrinos might play the role of the dark matter particle

  • Our goal is to show that dark matter sterile neutrinos can be produced in the early Universe by decoupling from thermal equilibrium

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Summary

Introduction

The identity and the character of the Dark Matter (DM) of the Universe and the origin of the minute mass of neutrinos in the Standard Model of particle physics (SM) are two of the most prominent problems in fundamental physics. The question would be whether the observed DM density can be generated by thermal freeze-out, i.e. whether, after entering thermal equilibrium, its rate with the SM plasma at some stage can no longer compete with the expansion of the Universe. This production mechanism is well known and. If it is able to decay, the lifetime of the decay must be comparable or larger than the age of the Universe

Constraints
Seesaw mechanism and sterile neutrinos as a dark matter candidate
Seesaw-Froggatt-Nielsen models for sterile neutrino dark matter
The longevity of DM
Dark matter genesis
Findings
Conclusions
Full Text
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