Showing 1–20 of 31 results
/ Date/ Name
Jul 9, 2025Search for the lepton number violating process $J/ψ\to K^+K^+e^-e^- +c.c.$Jun 12, 2025Search for sub-GeV invisible particles in inclusive decays of $J/ψ$ to $φ$Jun 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 27, 2025Measurements of branching fractions of $D^0\to K^- 3π^+2π^-$, $D^0\to K^- 2π^+π^-2π^0$ and $D^+\to K^- 3π^+π^-π^0$Apr 18, 2025Search for $1^{-+}$ charmonium-like hybrid via $e^{+}e^{-}\rightarrow γη^{(\prime)} η_{c}$ at center-of-mass energies between 4.258 and 4.681 GeVApr 10, 2025Search for the baryon and lepton number violating decay $J/ψ\to pe^-$ + c.cFeb 27, 2025Precision measurement of the branching fraction for the decay $ψ(2S)\rightarrowτ^{+}τ^{-}$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 $χ_{c1}(3872)\toγψ_2(3823)$