Abstract

We consider a local $U(1)_{B-L}$ extension of Zee-Babu model to explain the recently observed 3.5 keV X-ray line signal. The model has three Standard model (SM)-singlet Dirac fermions with different $U(1)_{B-L}$ charges. A complex scalar field charged under $U(1)_{B-L}$ is introduced to break the $U(1)_{B-L}$ symmetry. After $U(1)_{B-L}$ symmetry breaking a remnant discrete symmetry stabilizes the lightest state of the Dirac fermions, which can be a stable dark matter (DM). The second lightest state, if mass splitting with the stable DM is about 3.5 keV, decays dominantly to the stable DM and 3.5 keV photon through two-loop diagrams, explaining the X-ray line signal. Two-loop suppression of the decay amplitude makes its lifetime much longer than the age of the universe and it can be a decaying DM candidate in large parameter region. We also introduce a real scalar field which is singlet under both the SM and $U(1)_{B-L}$ and can explain the current relic abundance of the Dirac fermionic DMs. If the mixing with the SM Higgs boson is small, it does not contribute to DM direct detection. The main contribution to the scattering of DM off atomic nuclei comes from the exchange of $U(1)_{B-L}$ gauge boson, $Z'$, and is suppressed below current experimental bound when $Z'$ mass is heavy ($\gtrsim 10$ TeV). If the singlet scalar mass is about 0.1-10 MeV, the DM self-interaction can be large enough to solve small scale structure problems in simulations with the cold DM, such as, the core-vs-cusp problem and too-big-to-fail problem.

Highlights

  • We consider a local U(1)B−L extension of Zee-Babu model to explain the recently observed 3.5 keV X-ray line signal

  • We introduce a real scalar field which is singlet under both the Standard model (SM) and U(1)B−L and can explain the current relic abundance of the Dirac fermionic dark matter (DM)

  • The lifetime of ψ2′ is much longer than the age of the universe and it can be a decaying dark matter candidate

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Summary

The model

This proves our argument that the DM carrying only dark charge does not couple to the photon for the massive Z′ case even if there is mixing between γ and Z′. Given that χ [74] and h − φ(n) [66,67,68] mixing are strongly constrained and the Barr-Zee type diagrams are generated even in the limits where those mixings vanish, we can consider the effects of nonvanishing mixings as small perturbations. We note that large Λ (∼ 1015 GeV) is generated mainly from two-loop suppression factor, the typical dimensionless parameters are of order 0.1 − 1 and the involved particle masses are of order 1–10 TeV

Decaying dark matter scenario
Conclusions
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