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Dark Matter interpretations of the e± excesses after FERMI

2009/05/31 by Patrick Meade, Michele Papucci, Alessandro Strumia +2 · 211 citations
Physics and Astronomy · #Annihilation #Astrophysics #Astrophysics and Cosmic Phenomena #Atomic physics #Compton scattering #Cosmic ray #Dark Matter and Cosmic Phenomena #Dark matter #Electron #Fermi Gamma-ray Space Telescope #Nuclear physics #Particle physics #Particle physics theoretical and experimental studies #Photon #Physics #Positron #Quantum mechanics #hep-ph

paper · pdf · doi:10.1016/j.nuclphysb.2010.01.012

published in Nuclear Physics B 831(1-2), 178-203 (Elsevier BV) · 30 pages, 13 figures. Final and updated version

openalex publication_date 2010/01/19 · arxiv created 2010/02/24 · arxiv updated 2010/02/26 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05

Abstract

The cosmic-ray excess observed by PAMELA in the positron fraction and by FERMI and HESS in the electron + positron flux can be interpreted in terms of DM annihilations or decays into leptonic final states. Final states into tau's or 4mu give the best fit to the excess. However, in the annihilation scenario, they are incompatible with photon and neutrino constraints, unless DM has a quasi-constant density profile. Final states involving electrons are less constrained but poorly fit the excess, unless hidden sector radiation makes their energy spectrum smoother, allowing a fit to all the data with a combination of leptonic modes. In general, DM lighter than about a TeV cannot fit the excesses, so PAMELA should find a greater positron fraction at higher energies. The DM interpretation can be tested by FERMI gamma observations above 10 GeV: if the electronic excess is everywhere in the DM halo, inverse Compton scattering on ambient light produces a well-predicted gamma excess that FERMI should soon detect.

Citations