Abstract

We construct a self-interacting dark matter model that could simultaneously explain the observed muon anomalous magnetic moment. It is based on a gauged mathrm{U}{(1)}_{L_{mu }-{L}_{tau }} extension of the standard model, where we introduce a vector-like pair of fermions as the dark matter candidate and a new Higgs boson to break the symmetry. The new gauge boson has a sizable contribution to muon (g − 2), while being consistent with other experimental constraints. The mathrm{U}{(1)}_{L_{mu }-{L}_{tau }} Higgs boson acts as a light force carrier, mediating dark matter self-interactions with a velocity-dependent cross section. It is large enough in galaxies to thermalize the inner halo and explain the diverse rotation curves and diminishes towards galaxy clusters. Since the light mediator dominantly decays to the mathrm{U}{(1)}_{L_{mu }-{L}_{tau }} gauge boson and neutrinos, the astrophysical and cosmological constraints are weak. We study the thermal evolution of the model in the early Universe and derive a lower bound on the gauge boson mass.

Highlights

  • The presence of Z could contribute to (g − 2)μ

  • We construct a self-interacting dark matter model that could simultaneously explain the observed muon anomalous magnetic moment. It is based on a gauged U(1)Lμ−Lτ extension of the standard model, where we introduce a vector-like pair of fermions as the dark matter candidate and a new Higgs boson to break the symmetry

  • We study the thermal evolution of the model in the early Universe and derive a lower bound on the gauge boson mass

Read more

Summary

The model

We introduce a vector-like pair of fermions N and Nand a U(1)Lμ−Lτ Higgs Φ in addition to the U(1)Lμ−Lτ gauge boson Zμ. We assume that there is no kinetic mixing between Z and B at some high-energy scale, = 0. This can be achieved by imposing a charge conjugation symmetry CLμ−Lτ : L2 ↔ L3, μ ↔ τ , N ↔ N , Z → −Z , and Φ → Φ∗. Since this symmetry is broken by the Yukawa mass terms of μ and τ , the mixings of Z with the photon A and with the Z boson arise at the 1-loop level at low energy. In the rest of this section, we discuss the observational constraints on Z and φ

Experimental constraints
Dark Matter phenomenology
DM relic abundance
DM self-scattering
Direct and indirect searches
Conclusion
A Neutrino-electron scattering rate
B Temperature evolution around the BBN
Findings
C Decay width of φ
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call