Abstract

We propose a new extension of the Standard Model by a $U(1)_{B-L}$ gauge symmetry in which the anomalies are canceled by two right-handed neutrinos plus four chiral fermions with fractional B-L charges. Two scalar fields that break the B-L symmetry and give masses to the new fermions are also required. After symmetry breaking, two neutrinos acquire Majorana masses via the seesaw mechanism leaving a massless neutrino in the spectrum. Additionally, the other new fermions arrange themselves into two Dirac particles, both of which are automatically stable and contribute to the observed dark matter density. This model thus realizes in a natural way, without ad hoc discrete symmetries, a two-component dark matter scenario. We analyze in some detail the dark matter phenomenology of this model. The dependence of the relic densities with the parameters of the model is illustrated and the regions consistent with the observed dark matter abundance are identified. Finally, we impose the current limits from LHC and direct detection experiments, and show that the high mass region of this model remains unconstrained.

Highlights

  • One of the main problems in particle physics today is to find out what is the New Physics that lies beyond the Standard Model (SM)

  • As we have seen in the previous section, the relic density can be obtained via gauge or scalar interactions, and agreement with the observed dark matter (DM) density is achieved typically close to the resonance regions

  • The experimental evidence in favor of dark matter and neutrino masses compel us to look for physics beyond the Standard Model

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Summary

INTRODUCTION

One of the main problems in particle physics today is to find out what is the New Physics that lies beyond the Standard Model (SM). This model realizes, a two-component DM scenario All in all, this model introduces 17 additional parameters: four masses for the new fermions (MR1, MR2, M1, M2), three scalar masses (MH1, MH2, MA), one mixing angle in the scalar sector (sin θ), six neutrino Yukawa couplings (yij), the ratio of the two vevs (tan β), the gauge coupling constant (gBL) of the Uð1ÞB−L group, and the mass of the new gauge boson MZ0. This model introduces 17 additional parameters: four masses for the new fermions (MR1, MR2, M1, M2), three scalar masses (MH1, MH2, MA), one mixing angle in the scalar sector (sin θ), six neutrino Yukawa couplings (yij), the ratio of the two vevs (tan β), the gauge coupling constant (gBL) of the Uð1ÞB−L group, and the mass of the new gauge boson MZ0 These parameters are constrained by a combination of collider, neutrino, and DM experiments

NEUTRINO MASSES
DARK MATTER PHENOMENOLOGY
VIABLE PARAMETER SPACE
CONCLUSIONS

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