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Scattering of Dark Particles with Light Mediators

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arxiv 1407.2623 v1 pith:BZ2SIACB submitted 2014-07-09 hep-ph

classification hep-ph
keywords scatteringdarkdescribeddeeplydescriptiondetectorfermionsinelastic
verification ladder T0 review T1 audit T2 compute T3 formal

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abstract

We present a treatment of the high energy scattering of dark Dirac fermions from nuclei, mediated by the exchange of a light vector boson. The dark fermions are produced by proton-nucleus interactions in a fixed target and, after traversing shielding that screens out strongly interacting products, appear similarly to neutrino neutral current scattering in a detector. Using the Fermilab experiment E613 as an example, we place limits on a secluded dark matter scenario. Visible scattering in the detector includes both the familiar regime of large momentum transfer to the nucleus ($Q^2$) described by deeply inelastic scattering, as well as small $Q^2$ kinematics described by the exchanged vector mediator fluctuating into a quark-antiquark pair whose interaction with the nucleus is described by a saturation model. We find that the improved description of the low $Q^2$ scattering leads to important corrections, resulting in more robust constraints in a regime where a description entirely in terms of deeply inelastic scattering cannot be trusted.

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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. Inelastic Scattering Effects on Attenuation of Boosted Dark Matter

    hep-ph 2026-07 conditional novelty 6.0 of 10

    Resonant excitation of nucleons into Δ(1232) during Earth passage is a non-negligible attenuation channel for boosted dark matter at E_χ ≈ 1–2 GeV, lowering the PandaX-4T upper bound on σ̄_n in the heavy-mediator regime.

  2. Underground Production of Electromagnetic Dark States by MeV-scale Electron Beams and Detection with CCDs

    hep-ph 2025-11 unverdicted novelty 4.0 of 10

    Proposes underground MeV-scale electron-beam production of millicharged or dipole fermions followed by CCD detection to access unconstrained parameter space.

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