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Search for a Non-Relativistic Component in the Spectrum of Cosmic Rays at Earth

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arxiv 1805.02646 v2 pith:MKXMK6JO submitted 2018-05-07 astro-ph.CO astro-ph.IMhep-exhep-ph

classification astro-ph.COastro-ph.IMhep-exhep-ph
keywords darkearthmatterparticlescosmicnuclearraysrecoils
verification ladder T0 review T1 audit T2 compute T3 formal

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abstract

Dark matter particles gravitationally bound to our galaxy should exhibit a characteristic speed distribution limited by their escape velocity at the position of the Earth ($v_{esc}\simeq$ 550 km/s). An ongoing search for anomalous cosmic rays at Earth, kinematically similar to cold dark matter, is described. The technique can discriminate between these and known slow-moving particles such as neutrons, would be sensitive to telltale signatures from presently unexplored candidates, and offers the possibility of identifying the mediating type of interaction (nuclear vs. electron recoils). Studies of background identification and abatement in a shallow underground site are presented. The expected reach of the method is discussed, and illustrated by obtaining the first limits for dark matter particles lighter than 100 MeV/c$^{2}$ interacting via nuclear recoils.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. On the relation between Migdal effect and dark matter-electron scattering in isolated atoms and semiconductors

    hep-ph 2019-08 conditional novelty 6.0 of 10

    The Migdal ionization rate from dark matter-nucleus scattering equals the dark matter-electron ionization form factor evaluated at momentum q_e = (m_e/m_N) q, enabling the first semiconductor Migdal estimate and new s...

  2. The CRESST experiment: towards the next-generation of sub-GeV direct dark matter detection

    astro-ph.CO 2025-05 conditional novelty 4.0 of 10

    CRESST's projected 288-channel upgrade with gram-scale CaWO4 detectors could reach spin-independent dark matter cross sections near 10^-42 cm^2 at 1 GeV/c^2, if the low-energy excess is reduced by a factor of 10 to 100.

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