2011/07/31 by Patrick deNiverville, Maxim Pospelov, Adam Ritz · 7 citations
Physics and Astronomy · #Astrophysics #Beam (structure) #Beam dump #Cosmology #Dark Matter and Cosmic Phenomena #Dark energy #Dark matter #Dark photon #Hot dark matter #Light dark matter #Luminosity #MiniBooNE #Neutrino #Neutrino Physics Research #Neutrino oscillation #Nuclear physics #Optics #Parameter space #Particle physics #Particle physics theoretical and experimental studies #Physics #Scalar field dark matter #Sterile neutrino #hep-ph
paper · pdf · doi:10.1103/physrevd.84.075020
19 pages, 5 figures; v2: typos corrected, to appear in Phys. Rev. D; v3: note added clarifying the parameter range excluded by LSND
openalex publication_date 2011/10/21 · arxiv created 2013/08/14 · arxiv updated 2015/03/19 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We consider the sensitivity of fixed-target neutrino experiments at the luminosity frontier to light stable states, such as those present in models of MeV-scale dark matter. To ensure the correct thermal relic abundance, such states must annihilate via light mediators, which in turn provide an access portal for direct production in colliders or fixed targets. Indeed, this framework endows the neutrino beams produced at fixed-target facilities with a companion ``dark matter beam,'' which may be detected via an excess of elastic scattering events off electrons or nuclei in the (near-)detector. We study the high-luminosity proton fixed-target experiments at LSND and MiniBooNE, and determine that the ensuing sensitivity to light dark matter generally surpasses that of other direct probes. For scenarios with a kinetically-mixed U(1)^\ensuremath' vector mediator of mass mV, we find that a large volume of parameter space is excluded for mDM\ensuremath∼1--5 MeV, covering vector masses 2mDM\ensuremath\lesssimmV\ensuremath\lesssimm_\ensuremathη and a range of kinetic mixing parameters reaching as low as \ensuremathκ\ensuremath∼10^\ensuremath-5. The corresponding MeV-scale dark matter scenarios motivated by an explanation of the galactic 511 keV line are thus strongly constrained.