Abstract

We show that a minimal local $B-L$ symmetry extension of the standard model can provide a unified description of both neutrino mass and dark matter. In our model, $B-L$ breaking is responsible for neutrino masses via the seesaw mechanism, whereas the real part of the $B-L$ breaking Higgs field (called $\sigma$ here) plays the role of a freeze-in dark matter candidate for a wide parameter range. Since the $\sigma$-particle is unstable, for it to qualify as dark matter, its lifetime must be longer than $10^{25}$ seconds implying that the $B-L$ gauge coupling must be very small. This in turn implies that the dark matter relic density must arise from the freeze-in mechanism. The dark matter lifetime bound combined with dark matter relic density gives a lower bound on the $B-L$ gauge boson mass in terms of the dark matter mass. We point out parameter domains where the dark matter mass can be both in the keV to MeV range as well as in the PeV range. We discuss ways to test some parameter ranges of this scenario in collider experiments. Finally, we show that if instead of $B-L$, we consider the extra $U(1)$ generator to be $-4I_{3R}+3(B-L)$, the basic phenomenology remains unaltered and for certain gauge coupling ranges, the model can be embedded into a five dimensional $SO(10)$ grand unified theory.

Highlights

  • If small neutrino masses arise via the seesaw mechanism [1,2,3,4,5], the addition of a local B − L symmetry [6,7] to the standard model (SM) provides a minimal scenario for beyond the standard model physics to achieve this goal

  • We show that if we replace the B − L symmetry by I ≡ −4I3R þ 3ðB − LÞ, the dark matter phenomenology remains largely unchanged and the model can be embedded into the SOð10Þ grand unified theory in five space-time dimensions

  • For the case when mσ > mh, on the other hand, the dark matter (DM) particle can decay to a pair of Higgs doublets through the mixing, and we find that the loop induced mixing is not small enough to be consistent with the results shown in the right panels of Figs. 1 and 3

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Summary

INTRODUCTION

If small neutrino masses arise via the seesaw mechanism [1,2,3,4,5], the addition of a local B − L symmetry [6,7] to the standard model (SM) provides a minimal scenario for beyond the standard model physics to achieve this goal. The DM turns out to be the real part (denoted here as σ) of the complex B − L 1⁄4 2 Higgs field, that breaks B − L and gives mass to the right-handed neutrinos in the seesaw formula Even though this particle is not stable, there are certain allowed parameter ranges of the model, where its lifetime can be so long that it can play the role of a decaying dark matter. We isolate this parameter range and show that in this case, the freeze-in mechanism [17] can generate its relic density. VII, we conclude with some comments and other implications of the model

BRIEF OVERVIEW OF THE MODEL
DARK MATTER LIFETIME
GeV MN ð5Þ
Allowed range of gBL from preconditions to freeze-in
Relic density buildup
Lifetime constraint
Relic density constraints
GeV : ð19Þ
CONCLUDING REMARKS
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