Abstract

We propose an electroweakly interacting spin-1 dark matter (DM) model. The electroweak gauge symmetry, SU(2)L×U(1)Y , is extended into SU(2)0×SU(2)1×SU(2)2×U(1)Y . A discrete symmetry exchanging SU(2)0 and SU(2)2 is imposed. This discrete symmetry stabilizes the DM candidate. The spin-1 DM particle (V0) and its SU(2)L partners (V±) interact with the Standard Model (SM) electroweak gauge bosons without any suppression factors. Consequently, pairs of DM particles efficiently annihilate into the SM particles in the early universe, and the measured value of the DM energy density is easily realized by the thermal freeze-out mechanism. The model also predicts a heavy vector triplet (W′± and Z′) in the visible sector. They contribute to the DM annihilation processes. The mass ratio of Z′ and V0 determines values of various couplings, and constraints on W′ and Z′ restrict regions of the parameter space that are viable for DM physics. We investigate the constraints from perturbative unitarity of scalar and gauge couplings, the Higgs signal strength, W′ search at the LHC, and DM direct detection experiments. It is found that the relic abundance of V0 explains the right amount of the DM energy density for 3 TeV underset{sim }{<}{m}_Vounderset{sim }{<} 19 TeV.

Highlights

  • Pairs of dark matter (DM) particles efficiently annihilate into the Standard Model (SM) particles in the early universe, and the measured value of the DM energy density is realized by the thermal freeze-out mechanism

  • We propose a renormalizable model of spin-1 DM that does not require Z and Higgs couplings to a DM particle to obtain the correct amount of the DM density by the freeze-out mechanism

  • The electroweak gauge symmetry is extended into SU(2)0×SU(2)1×SU(2)2×U(1)Y, and the discrete symmetry under the exchanging of SU(2)0 and SU(2)2 is imposed

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Summary

Bosonic sector

We briefly describe the electroweak sector and the related scalar sector. More details are discussed in appendices.

Gauge sector
Physical scalars
Model parameters
Perturbative unitarity
The mass ratio of Z and V
W and Z searches at the LHC
Electroweak precision measurements
Higgs signal strength
Mass difference and its implication for collider physics
Direct detection
Relic abundance
Conclusions
B Would-be NG bosons
C Fermi constant
Full Text
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