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Limits to Gauge Coupling in the Dark Sector Set by the Nonobservation of Instanton-Induced Decay of Super-Heavy Dark Matter in the Pierre Auger Observatory Data

P. Abreu et al. (Pierre Auger Collaboration)
Phys. Rev. Lett. 130, 061001 – Published 7 February 2023

Abstract

Instantons, which are nonperturbative solutions to Yang-Mills equations, provide a signal for the occurrence of quantum tunneling between distinct classes of vacua. They can give rise to decays of particles otherwise forbidden. Using data collected at the Pierre Auger Observatory, we search for signatures of such instanton-induced processes that would be suggestive of super-heavy particles decaying in the Galactic halo. These particles could have been produced during the post-inflationary epoch and match the relic abundance of dark matter inferred today. The nonobservation of the signatures searched for allows us to derive a bound on the reduced coupling constant of gauge interactions in the dark sector: αX0.09, for 109MX/GeV<1019. Conversely, we obtain that, for instance, a reduced coupling constant αX=0.09 excludes masses MX3×1013GeV. In the context of dark matter production from gravitational interactions alone, we illustrate how these bounds are complementary to those obtained on the Hubble rate at the end of inflation from the nonobservation of tensor modes in the cosmological microwave background.

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  • Received 9 August 2022
  • Revised 30 November 2022
  • Accepted 14 December 2022

DOI:https://doi.org/10.1103/PhysRevLett.130.061001

© 2023 American Physical Society

Physics Subject Headings (PhySH)

Gravitation, Cosmology & Astrophysics

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Vol. 130, Iss. 6 — 10 February 2023

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  • Figure 1
    Figure 1

    Upper limits at 95% C.L. (Confidence Level) on the coupling constant αX of a hidden gauge interaction as a function of the mass MX of a dark matter particle decaying into a dozen qq¯ pairs. For reference, the unification of the three SM gauge couplings is shown as the blue dashed line in the framework of supersymmetric grand unified theory [17].

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  • Figure 2
    Figure 2

    Flux upper limits of UHE photons, neutrinos, and cosmic rays as a function of energy thresholds.

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  • Figure 3
    Figure 3

    Constraints in the (Hinf,MX) plane. The red region is excluded by the nonobservation of tensor modes in the cosmic microwave background [9, 16]. The regions of viable (Hinf,MX) values needed to set the right abundance of DM are delineated by the blue lines for different values of reheating efficiency ϵ [54]. Additional constraints from the nonobservation of instanton-induced decay of SHDM particles allow for excluding the mass ranges in the regions to the right of the vertical lines, for the specified values of the dark-sector gauge coupling.

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