Abstract

We show that the event excess observed by the IceCube collaboration at TeV--PeV energies, usually interpreted as evidence for astrophysical neutrinos, can be explained alternatively by the scattering of highly boosted dark matter particles. Specifically, we consider a scenario where a $\sim 4$ PeV scalar dark matter particle $\phi$ can decay to a much lighter dark fermion $\chi$, which in turn scatters off nuclei in the IceCube detector. Besides these events, which are exclusively shower-like, the model also predicts a secondary population of events at $\mathcal{O}(100 \text{TeV})$ originating from the 3-body decay $\phi \to \chi \bar\chi a$, where $a$ is a pseudoscalar which mediates dark matter--Standard Model interactions and whose decay products include neutrinos. This secondary population also includes track-like events, and both populations together provide an excellent fit to the IceCube data. We then argue that a relic abundance of light Dark Matter particles $\chi$, which may constitute a subdominant component of the Dark Matter in the Universe, can have exactly the right properties to explain the observed excess in GeV gamma rays from the galactic center region. Our boosted Dark Matter scenario also predicts fluxes of $\mathcal{O}(10)$ TeV positrons and $\mathcal{O}(100 \text{TeV})$ photons from 3-body cascade decays of the heavy Dark Matter particle $\phi$, and we show how these can be used to constrain parts of the viable parameter space of the model. Direct detection limits are weak due to the pseudoscalar couplings of $\chi$. Accelerator constraints on the pseudoscalar mediator $a$ lead to the conclusion that the preferred mass of $a$ is $\gtrsim 10$ GeV and that large coupling to $b$ quarks but suppressed or vanishing coupling to leptons are preferred.

Highlights

  • In [16], is the following: a heavy O(PeV) DM species φ, which makes up a substantial fraction of the dark matter in the Universe, decays to a much lighter species χ

  • We show that the event excess observed by the IceCube collaboration at TeV– PeV energies, usually interpreted as evidence for astrophysical neutrinos, can be explained alternatively by the scattering of highly boosted dark matter particles

  • We argue that a relic abundance of light Dark Matter particles χ, which may constitute a subdominant component of the Dark Matter in the Universe, can have exactly the right properties to explain the observed excess in GeV gamma rays from the galactic center region

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Summary

The framework

While most of the qualitative results of this paper apply to any PeV-scale boosted DM model, we consider as a specific example a toy model featuring a dark sector that contains two DM particles: a heavy real scalar φ with mass mφ ∼ O(PeV) and a light Dirac fermion χ with mass mχ ∼ O(10) GeV. We assume the mass of a to satisfy ma 10 GeV since constraints are weak in this case (see section 6), allowing large couplings gYf to fermions This is important for the model to fit the IceCube data and is interesting because it allows for a detectable indirect signal from the annihilation of non-relativistic relic χ particles. This requires large tan β to lift up the coupling to down-type quarks Already at this stage, we can see that the MSSM-like model will be constrained by experiments sensitive to anomalous couplings of the charged leptons (which are tan β-enhanced) and by searches for an extended Higgs sector. The third model has no extended Higgs sector, and the pseudoscalar mediator a does not directly couple to SM quarks Instead, it couples to new, heavy vector-like quarks, which in turn mix with the SM quarks [57]. The mass of the heavy vector-like quark should be large to avoid LHC limits

Primary signal: scattering of boosted DM particles on nuclei
Secondary signal: neutrino flux from 3-body decays of heavy DM
Fitting procedure
Results
Dark matter relic density
The galactic center gamma ray excess
Constraints
Direct detection
Constraints from flavor physics experiments and from collider searches
1.44 Flipped
Summary and conclusion
A Details on the calculation of effective detector mass
Full Text
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