Abstract

We reconsider complex scalar singlet dark matter stabilised by a ℤ3 symmetry. We refine the stability bounds on the potential and use constraints from unitarity on scattering at finite energy to place a stronger lower limit on the direct detection cross section. In addition, we improve the treatment of the thermal freeze-out by including the evolution of the dark matter temperature and its feedback onto relic abundance. In the regions where the freeze-out is dominated by resonant or semi-annihilation, the dark matter decouples kinetically from the plasma very early, around the onset of the chemical decoupling. This results in a modification of the required coupling to the Higgs, which turns out to be at most few per cent in the semi-annihilation region, thus giving credence to the standard approach to the relic density calculation in this regime. In contrast, for dark matter mass just below the Higgs resonance, the modification of the Higgs invisible width and direct and indirect detection signals can be up to a factor 6.7. The model is then currently allowed at 56.8 GeV to 58.4 GeV (depending on the details of early kinetic decoupling) ≲ MS ≲ 62.8 GeV and at MS ≳ 122 GeV if the freeze-out is dominated by semi-annihilation. We show that the whole large semi-annihilation region will be probed by the near-future measurements at the XENONnT experiment.

Highlights

  • Z3 singlet scalar is the simplest dark matter candidate to undergo semi-annihilation [48,49,50,51], which breaks the one-to-one correspondence between annihilation and direct detection cross section present in Z2-symmetric dark matter models

  • We improve the treatment of the thermal freeze-out by including the evolution of the dark matter temperature and its feedback onto relic abundance

  • The concrete example that is given in [76] is the case of Z2 scalar singlet dark matter around the Higgs resonance, which finds its clear analogue in the Higgs resonance region of the Z3 singlet DM

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Summary

The model

The most general renormalisable scalar potential of the Higgs doublet H and the complex singlet S, invariant under the Z3 transformation H → H, S → ei2π/3S, is given by. This is the only possible potential with this field content and symmetry. The mass of the Higgs boson is Mh = 125.09 GeV [87] and the Higgs vacuum expectation value (VEV) v = 246.22 GeV. Dark matter mass MS, the Higgs portal λSH , the singlet cubic coupling μ3 and the singlet quartic self-coupling λS are left as free parameters

Vacuum stability
Unitarity
Stability of the electroweak vacuum
Higgs invisible width The decay width of the Higgs boson to singlets is
Combination of constraints
Relic density
Direct and indirect detection
Conclusions
Findings
A Field dependent masses and counter-terms
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