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Proton Fixed-Target Scintillation Experiment to Search for Minicharged Particles

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arxiv 1812.03998 v2 pith:TPXVEUKW submitted 2018-12-10 hep-ph hep-ex

classification hep-phhep-ex
keywords detectorminichargedparticlesprotonsearchalternativeexperimentfermini
verification ladder T0 review T1 audit T2 compute T3 formal

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abstract

We propose a low-cost and movable setup to probe minicharged particles (or milli-charged particles) using high-intensity proton fixed-target facilities. This proposal, FerMINI, consists of a milliQan-type detector, requiring multi-coincident (nominally, triple-coincident) scintillation signatures within a small time window, located downstream of the proton target of a neutrino experiment. During the collisions of a large number of protons on the target, intense minicharged particle beams may be produced via meson photo-decays and Drell-Yan production. We take advantage of the high statistics, shielding, and potential neutrino-detector-related background reduction to search for minicharged particles in two potential sites: the MINOS near detector hall and the proposed DUNE near detector hall, both at Fermilab. We also explore several alternative designs, including the modifications of the nominal detector to increase signal yield, and combining this detector technology with existing and planned neutrino detectors to better search for minicharged particles. The CERN SPS beam and associated experimental structure also provide a similar alternative. FerMINI can achieve unprecedented sensitivity for minicharged particles in the MeV to few GeV regime with fractional charge $\varepsilon=Q_{\chi}/e $ between $10^{-4}$ (potentially saturating the detector limitation) and $10^{-1}$.

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Forward citations

Cited by 5 Pith papers

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

  1. Reviving Millicharged Dark Matter for 21-cm Cosmology

    hep-ph 2019-08 conditional novelty 7.0 of 10

    Adding a long-range interaction between a millicharged dark matter subcomponent and the dominant cold dark matter lets the dark sector act as a heat sink, reviving the millicharged explanation of the EDGES 21-cm anomaly.

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    A clockwork chain of U(1) gauge groups naturally generates a dark-matter electric charge of order 10^{-12}e with O(1) inputs, with the relic abundance set by resonant annihilation through TeV-scale Z' bosons.

  3. Constraints on millicharged particles from nuclear gamma-decays

    hep-ph 2025-07 conditional novelty 6.0 of 10

    Nuclear gamma cascades in reactors produce millicharged particle pairs, giving the strongest constraints on millicharge for masses between 0.7 and 2 MeV.

  4. Constraints on Strongly-Interacting Dark Matter from the James Webb Space Telescope

    astro-ph.CO 2024-12 conditional novelty 6.0 of 10

    JWST NIRSpec dark calibration images exclude previously allowed high-cross-section parameter space for sub-GeV dark matter coupled to an ultralight dark photon, for subcomponent fractions as low as about 0.01%.

  5. The High-Energy Frontier of the Intensity Frontier: Closing the Dark Photon, Inelastic Dark Matter, and Muon g-2 Windows

    hep-ph 2019-08 conditional novelty 6.0 of 10

    Reanalysis of CHARM and NuCal beam-dump data nearly excludes inelastic dark matter as a full-abundance thermal relic in the MeV to GeV range for the benchmark splittings considered, and yields updated dark photon constraints.

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