Showing 1–20 of 442 results
/ Date/ Name
Jun 28, 2022Absolute Measurements of Branching Fractions of Cabibbo-Suppressed Hadronic $D^{0(+)}$ Decays Involving Multiple PionsSep 22, 2022Study of $η(1405)/η(1475)$ in $J/ψ\toγK^{0}_{S} K^{0}_{S}π^{0}$ decayAug 19, 2022Search for hyperon $ΔS=ΔQ$ violating decay $Ξ^{0}\toΣ^{-}e^{+}ν_{e}$Aug 22, 2022Measurement of the $C\!P$-even fraction of $D^{0}\toπ^{+}π^{-}π^{+}π^{-}$Sep 13, 2022Search for baryon and lepton number violation decay $D^{\pm}\to n(\bar{n})e^{\pm}$Dec 18, 2022Determination of U-spin breaking parameters with an amplitude analysis of the decay $D^0 \to K_{\rm L}^0π^+π^-$Dec 14, 2022Measurements of the electric and magnetic form factors of the neutron for time-like momentum transferNov 23, 2022Search for an axion-like particle in radiative $J/ψ$ decaysOct 18, 2022Measurement of the absolute branching fraction of the inclusive decay $\barΛ_{c}^{-} \to \bar{n} + X$Jan 24, 2022Partial wave analysis of $J/ψ\to γη^{\prime} η^{\prime}$Jan 26, 2022Observation of a state $X(2600)$ in the $π^{+}π^{-}η'$ system in the process $J/ψ\rightarrowγπ^{+}π^{-}η'$Feb 14, 2022Measurement of $e^{+}e^{-} \to K^{+}K^{-}π^{0}$ cross section and observation of a resonant structureMar 7, 2022Measurement of integrated luminosities at BESIII for data samples at center-of-mass energies between 4.0 and 4.6 GeVMay 18, 2022Amplitude analysis and branching fraction measurement of the decay $D_{s}^{+} \to K^+π^+π^-$Aug 9, 2022Search for a massless dark photon in $Λ^{+}_{c}\to p γ^{\prime}$ decayJun 28, 2022Measurement of the total and leptonic decay widths of the $J/ψ$ resonance with an energy scan method at BESIIIJul 3, 2022Evidence for the Cusp Effect in $η'$ Decays into $ηπ^0π^0$Jul 29, 2022Measurement of $e^{+}e^{-}\rightarrowπ^{+}π^{-}D^{+}D^{-}$ cross sections at center-of-mass energies from 4.190 to 4.946 GeVAug 16, 2023Study of $e^+e^-\toηφ$ at center-of-mass energies from 3.773 to 4.600 GeVDec 10, 2022First Direct Measurement of the Absolute Branching Fraction of $Σ^+ \to Λe^+ ν_{e}$