2011/04/30 by Nicole F. Bell, James B. Dent, Ahmad J. Galea +5 · 3 citations
Physics and Astronomy · #Annihilation #Bremsstrahlung #Cosmology and Gravitation Theories #Dark Matter and Cosmic Phenomena #Dark matter #Electroweak interaction #Helicity #Lepton #Nuclear physics #Particle physics #Particle physics theoretical and experimental studies #Physics #astro-ph.HE #hep-ph
paper · pdf · doi:10.1016/j.physletb.2011.10.057
published as Phys.Lett. B706 (2011) 6-12 · 8 pages, 6 figures; replaced to match published version
openalex publication_date 2011/10/27 · arxiv created 2012/05/23 · arxiv updated 2015/03/18 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
We revisit the calculation of electroweak bremsstrahlung contributions to dark matter annihilation. Dark matter annihilation to leptons is necessarily accompanied by electroweak radiative corrections, in which a W or Z boson is also radiated. Significantly, while many dark matter models feature a helicity suppressed annihilation rate to fermions, bremsstrahlung process can remove this helicity suppression such that the branching ratios Br(ℓ νW ), Br(ℓ+ℓ-Z), and Br(ννZ) dominate over Br(ℓ+ℓ-) and Br(νν). We find this is most significant in the limit where the dark matter mass is nearly degenerate with the mass of the boson which mediates the annihilation process. Electroweak bremsstrahlung has important phenomenological consequences both for the magnitude of the total dark matter annihilation cross section and for the character of the astrophysical signals for indirect detection. Given that the W and Z gauge bosons decay dominantly via hadronic channels, it is impossible to produce final state leptons without accompanying protons, antiprotons, and gamma rays.