Showing 1–20 of 83 results
/ Date/ Name
Apr 12, 2026First Observation of \boldmath{$D^+ \to a_0(980)ρ$ and $D^+ \to a_0(980)^+ f_0(500)$} in \boldmath{$D^+ \to π^+π^+π^-η$ and $D^+ \to π^+π^0π^0η$} DecaysOct 8, 2025A Giant Peanut-shaped Ultra-High-Energy Gamma-Ray Emitter Off the Galactic PlaneJun 4, 2025Simulation of MAPS and a MAPS-based Inner Tracker for the Super Tau-Charm FacilityJun 3, 2025Measurement of the branching fractions of the Cabibbo-favored decays $Λ_{c}^{+}\toΛK_{S}^{0}K^{+}$ and $Λ_{c}^{+}\toΞ^{0}K_{S}^{0}π^{+}$ and search for $Λ_{c}^{+}\toΣ^{0} K_{S}^{0}K^{+}$Apr 10, 2025Search for the baryon and lepton number violating decay $J/ψ\to pe^-$ + c.cMar 24, 2025Observation of the decay $ψ(3686)\rightarrow Σ^{0}\barΣ^{0}ω$Feb 28, 2025Improved measurement of absolute branching fraction of the inclusive decay $Λ_{c}^{+} \to K_{S}^{0} X$Jan 26, 2025Observation of Charmonium $h_{c}$ Radiative Decays to Multiple Light Hadrons and the Tensor State $f_2(1270)$Jan 5, 2025Observation of $ψ(3686) \to K^{-}Λ(1520)\barΞ^{+} + c.c.$Oct 24, 2024Search for $η_c(2S)\to p\bar{p}$ and branching fraction measurements of $χ_{cJ} \to p\bar{p}$ via $ψ(2S)$ radiative decaysOct 17, 2024Observation of $χ_{c0}\toΣ^{+}\barΣ^{-}η$ and evidence for $χ_{c1,2}\toΣ^{+}\barΣ^{-}η$Oct 17, 2024Observation of the Singly Cabibbo-Suppressed Decay $Λ_c^{+}\to pπ^0$Oct 11, 2024Observation of $D^+\toη^\primeμ^+ν_μ$ and First Study of $D^+\to η^\prime \ell^+ν_\ell$ Decay DynamicsOct 3, 2024Search for lepton number violating decays of $D_s^+\to h^-h^0e^+e^+$Sep 6, 2024Study of the decay $D^0\rightarrow ρ(770)^-e^+ν_e$Jul 17, 2024Observation of $Λ_c^+ \to Λa_0(980)^+$ and Evidence for $Σ(1380)^+$ in $Λ_c^+ \to Λπ^+ η$Jul 3, 2024Measurement of the branching fraction of the decay $J/ψ\to p \bar{p} η$Jun 10, 2024Strong and weak $CP$ tests in sequential decays of polarized $Σ^0$ hyperonsJun 3, 2024Measurements of the branching fractions of semileptonic $D^{+}_s$ decays via $e^+e^-\to D_s^{*+}D_s^{*-}$May 13, 2024Search for the radiative transition $χ_{c1}(3872)\toγψ_2(3823)$