2015
DOI: 10.1103/physrevd.91.094026
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Testing GeV-scale dark matter with fixed-target missing momentum experiments

Abstract: We describe an approach to detect dark matter and other invisible particles with mass below a GeV, exploiting missing energy-momentum measurements and other kinematic features of fixedtarget production. In the case of an invisibly decaying MeV-GeV-scale dark photon, this approach can improve on present constraints by 2-6 orders of magnitude over the entire mass range, reaching sensitivity as low as 2 ∼ 10 −14 . Moreover, the approach can explore essentially all of the viable parameter space for thermal or asym… Show more

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Cited by 98 publications
(144 citation statements)
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References 118 publications
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“…We find that the proposed LDMX electron beam dump [158] can probe the entire allowed region of the left panel of figure 13. In our model the LDMX signal will be missing energy events, from the production of an A , followed by its decay to n 2 n 3 (surviving past the detector calorimeters).…”
Section: Jhep08(2018)079mentioning
confidence: 93%
See 1 more Smart Citation
“…We find that the proposed LDMX electron beam dump [158] can probe the entire allowed region of the left panel of figure 13. In our model the LDMX signal will be missing energy events, from the production of an A , followed by its decay to n 2 n 3 (surviving past the detector calorimeters).…”
Section: Jhep08(2018)079mentioning
confidence: 93%
“…The reach for BDX and MiniBooNe adapted from [61], and PIXIE [154][155][156][157] (corresponding to µ < 5 × 10 −8 ) are shown. LDMX [158] can probe the entire allowed region of the left panel, but is not sensitive to the heavier dark photon mass on the right panel. In every point of the plot ∆ is fixed to reproduce the observed relic density.…”
Section: ×10mentioning
confidence: 99%
“…Most generic searches typically focus on a dark photon and either assume that it decays invisibly and search for missing-energy signatures [58,59] -the strongest bounds using this strategy are currently from BaBar [60] and NA64 [61]. Alternatively, one can also try to observe its decay as bumps in a dilepton invariant spectrum such as in NA-48/2 [62], BaBar [63] and LHCb [64].…”
Section: Dark Higgs Boson At Accelerator Experimentsmentioning
confidence: 99%
“…where α D = e 2 D /4π and the parameter f depends on m A ' and m χ [22]. For m A ' mχ = 3, f 10 for a scalar [18], and f 1 for a fermion [19]. This prediction provides an important target for the ( , m A ) parameter space which can be probed at the CERN SPS energies.…”
mentioning
confidence: 99%