4.7 Article

Celestial-body focused dark matter annihilation throughout the Galaxy

Journal

PHYSICAL REVIEW D
Volume 103, Issue 7, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.103.075030

Keywords

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Funding

  1. U.S. Department of Energy [DE-AC02-76SF00515]
  2. Swedish Research Council [2019-05135]
  3. Swedish National Space Agency [117/19]
  4. European Research Council [742104]
  5. Vinnova [2019-05135] Funding Source: Vinnova
  6. Swedish Research Council [2019-05135] Funding Source: Swedish Research Council

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This passage discusses a new scenario in which celestial bodies can enhance the efficiency of dark matter annihilation events, leading to distinctive annihilation signals. By analyzing data from Fermi and H.E.S.S., new constraints on the dark matter-nucleon scattering cross section for different mass scales of dark matter can be set.
Indirect detection experiments typically measure the flux of annihilating dark matter (DM) particles propagating freely through galactic halos. We consider a new scenario where celestial bodies focus DM annihilation events, increasing the efficiency of halo annihilation. In this setup, DM is first captured by celestial bodies, such as neutron stars or brown dwarfs, and then annihilates within them. If DM annihilates to sufficiently long-lived particles, they can escape and subsequently decay into detectable radiation. This produces a distinctive annihilation morphology, which scales as the product of the DM and celestial body densities, rather than as DM density squared. We show that this signal can dominate over the halo annihilation rate in gamma-ray observations in both the Milky Way Galactic center and globular clusters. We use Fermi and H.E.S.S. data to constrain the DM-nucleon scattering cross section, setting powerful new limits down to similar to 10(-39) cm(2) for sub-GeV DM using brown dwarfs, which is up to 9 orders of magnitude stronger than existing limits. We demonstrate that neutron stars can set limits for TeV-scale DM down to about 10(-47) cm(2).

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