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Search for Light Dark Matter in Rare Meson Decays

Ze-Kun Liu, Ying Li, Biao-Feng Hou, Qin Chang

TL;DR

This work probes sub-GeV dark matter through rare meson decays mediated by a $Z^{\prime}$ portal. By mapping a UV $Z^{\prime}$-DM-quark interaction onto a dark low-energy EFT (DLEFT) and computing differential decay widths for $B\to P(V)\chi\bar{\chi}$ and $K\to \pi\chi\bar{\chi}$, it derives upper bounds on the couplings $g_f^{V,A}$ and $g_{\chi}^{V,A}$ from current data. The resulting constraints are translated into DM-nucleon cross sections for both spin-independent and spin-dependent interactions, revealing that rare meson decays provide competitive and background-free probes of sub-GeV DM, with sensitivity approaching or surpassing some direct-detection limits and offering strong complementarity to neutrino-floor-limited searches. The findings underscore the potential of flavor-changing neutral current processes as powerful tools for light DM model building and motivate future experimental and theoretical refinements to enhance sensitivity in the sub-GeV regime.

Abstract

Current dark matter direct detection experiments have low sensitivity to sub-GeV dark matter. In this work, we demonstrate that rare $B$ and $K$ meson decays with missing energy in the final state can serve as efficient probes in this mass range. We analyze a generic $Z^{\prime}$ portal dark matter model and derive upper limits on its parameters from experimental bounds on the rare $B$ and $K$ meson decays. Our results show that such meson decay processes provide complementary constraints to current direct detection experiments for sub-GeV dark matter, particularly for interaction forms mediated by dark matter momentum-dependent operators.

Search for Light Dark Matter in Rare Meson Decays

TL;DR

This work probes sub-GeV dark matter through rare meson decays mediated by a portal. By mapping a UV -DM-quark interaction onto a dark low-energy EFT (DLEFT) and computing differential decay widths for and , it derives upper bounds on the couplings and from current data. The resulting constraints are translated into DM-nucleon cross sections for both spin-independent and spin-dependent interactions, revealing that rare meson decays provide competitive and background-free probes of sub-GeV DM, with sensitivity approaching or surpassing some direct-detection limits and offering strong complementarity to neutrino-floor-limited searches. The findings underscore the potential of flavor-changing neutral current processes as powerful tools for light DM model building and motivate future experimental and theoretical refinements to enhance sensitivity in the sub-GeV regime.

Abstract

Current dark matter direct detection experiments have low sensitivity to sub-GeV dark matter. In this work, we demonstrate that rare and meson decays with missing energy in the final state can serve as efficient probes in this mass range. We analyze a generic portal dark matter model and derive upper limits on its parameters from experimental bounds on the rare and meson decays. Our results show that such meson decay processes provide complementary constraints to current direct detection experiments for sub-GeV dark matter, particularly for interaction forms mediated by dark matter momentum-dependent operators.
Paper Structure (8 sections, 11 equations, 5 figures, 2 tables)

This paper contains 8 sections, 11 equations, 5 figures, 2 tables.

Figures (5)

  • Figure 1: Leading-order Feynman diagrams for the $B$ and $K$ meson decays into a pair of DM, with $q=u,c,t$.
  • Figure 2: Constraints on the effective couplings $g_f^{V(A)} g_{\chi}^{V(A)}$ versus DM mass $m_\chi$ from rare $B$ meson decays. The colored curves represent upper limits from different $b\to s(d)\chi\bar{\chi}$ transition channels, with the regions above each curve experimentally excluded at $90\%$ confidence level.
  • Figure 3: Same as Figure \ref{['fig:Bs']}, but for rare $K$ meson decays.
  • Figure 4: Upper limits on spin-independent DM-nucleon cross section as a function of the DM mass. Also shown are the CRESST(2019) CRESST:2019jnq, DAMIC(2020) DAMIC:2020cut, CDMSlite(2018) SuperCDMS:2018gro, DarkSide-50(2023) DarkSide-50:2022qzh, SuperCDMS(2017) SuperCDMS:2017mbc, DEAP-3600(2019) DEAP:2019yzn, LZ(2025) LZ:2024zvo, PandaX-4T(2024) PandaX:2024qfu and XENONnT(2025) XENON:2025vwd limits.
  • Figure 5: Upper limits on spin-dependent DM-neutron(left) and DM-proton(right) cross sections as a function of the DM mass. Also shown are the PICO-60 PICO:2019vsc, PandaX-II PandaX-II:2018woa, LUX LUX:2017ree, XENONnT XENON:2023cxc, XENON1T XENON:2019rxp and LZ LZ:2024zvo limits.