Showing 1–20 of 180 results
/ Date/ Name
Mar 12, 2020Search for the decay $J/ψ\toγ+ \rm {invisible}$Feb 28, 2020Model-independent determination of the relative strong-phase difference between $D^0$ and $\bar{D}^0\rightarrow K^0_{S,L}π^+π^-$ and its impact on the measurement of the CKM angle $γ/φ_3$Jul 15, 2020Improved model-independent determination of the strong-phase difference between $D^{0}$ and $\bar{D}^{0}\to K^{0}_{\mathrm{S,L}}K^{+}K^{-}$ decaysJun 4, 2020Analysis of the decay $D^0\rightarrow K_{S}^{0} K^{+} K^{-}$Sep 19, 2020Observation of the decays $χ_{cJ}\toΣ^{0}\bar{p}K^{+}+{\rm c.c.}~(J=0, 1, 2)$May 22, 2020Measurement of the absolute branching fraction of the inclusive decay $Λ_c^+ \to K_S^0X$Apr 16, 2020$Σ^{+}$ and $\barΣ^-$ polarization in the $J/ψ$ and $ψ(3686)$ decaysMar 31, 2021Measurements of the branching fractions of $ψ(3686)\rightarrow\barΣ^{0}Λ+c.c.$ and $χ_{cJ (J = 0,1,2)} \rightarrow Λ\barΛ$Feb 1, 2021Study of $e^+e^- \rightarrow π^{0}X(3872)γ$ and search for $Z_c(4020)^{0}\rightarrow X(3872)γ$Feb 22, 2021Search for new decay modes of the $ψ_2(3823)$ and the process $e^+e^-\rightarrowπ^0π^0ψ_2(3823)$May 28, 2021Cross section measurement of $e^{+}e^{-} \to K_{S}^{0}K_{L}^{0}$ at $\sqrt{s}=2.00-3.08~{\rm GeV}$May 15, 2021Measurement of the branching fraction of leptonic decay $D_s^+\toτ^+ν_τ$ via $τ^+\toπ^+π^0\bar ν_τ$Sep 3, 2020Measurements of Sigma+ and Sigma- Time-like Electromagnetic Form Factors for center-of-mass energies from 2.3864 to 3.0200 GeVOct 7, 2018Study of the Dalitz decay $J/ψ\to e^+e^- η$Aug 23, 2021Amplitude analysis of $D_s^{+} \rightarrow π^{+} π^{-} π^{+}$Aug 23, 2021Search for the hyperon semileptonic decay $Ξ^{-} \rightarrow Ξ^{0} e^{-} \bar{ν_{e}}$Sep 26, 2021Amplitude analysis and branching fraction measurement of the decay $D_{s}^{+} \to π^{+}π^{0}π^{0}$Dec 8, 2020Observation of $η^\prime\rightarrowπ^+π^-μ^+μ^-$Feb 1, 2022Partial wave analysis of $J/ψ\rightarrowγηη'$Feb 28, 2022Measurements of Absolute Branching Fractions of $D^0\to K_L^0φ$, $K_L^0η$, $K_L^0ω$, and $K_L^0η^{\prime}$