Novel Cosmic-Ray Electron and Positron Constraints on MeV Dark Matter Particles

Mathieu Boudaud, Julien Lavalle, Pierre Salati

Physical Review Letters · 2017 · 114 citations · 48 references

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TL;DR

MeV dark matter annihilating or decaying to electron‑positron pairs cannot be detected by local cosmic‑ray measurements due to solar magnetic shielding. We exploit Voyager 1’s interstellar cosmic‑ray data, acquired after its heliopause crossing in 2012, to probe sub‑GeV dark matter for the first time. By modeling low‑energy electron and positron transport, we predict astrophysical backgrounds and dark‑matter pair production, then combine Voyager and AMS‑02 observations to derive limits spanning MeV to TeV masses. Reacceleration can raise positrons above the dark‑matter mass, and the resulting Voyager/AMS‑02 constraints limit MeV‑scale annihilation cross sections to ∼10⁻²⁸ cm³ s⁻¹, are largely insensitive to propagation assumptions, and are comparable to or tighter than cosmic‑microwave‑background bounds, especially for p‑wave annihilation.

Abstract

MeV dark matter (DM) particles annihilating or decaying to electron-positron pairs cannot, in principle, be observed via local cosmic-ray (CR) measurements because of the shielding solar magnetic field. In this letter, we take advantage of spacecraft Voyager 1's capacity for detecting interstellar CRs since it crossed the heliopause in 2012. This opens up a new avenue to probe DM in the sub-GeV energy/mass range that we exploit here for the first time. From a complete description of the transport of electrons and positrons at low energy, we derive predictions for both the secondary astrophysical background and the pair production mechanisms relevant to DM annihilation or decay down to the MeV mass range. Interestingly, we show that reacceleration may push positrons up to energies larger than the DM particle mass. We combine the constraints from the Voyager and AMS-02 data to get novel limits covering a very extended DM particle mass range, from MeV to TeV. In the MeV mass range, our limits reach annihilation cross sections of order $\langle \sigma v\rangle \sim 10^{-28}{\rm cm^3/s}$. An interesting aspect is that these limits barely depend on the details of cosmic-ray propagation in the weak reacceleration case, a configuration which seems to be favored by the most recent boron-to-carbon ($B/C$) data. Though extracted from a completely different and new probe, these bounds have a strength similar to those obtained with the cosmic microwave background --- they are even more stringent for $p$-wave annihilation.

References

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