Showing 41–60 of 302 results
/ Date/ Name
Jul 17, 2024Interim report for the International Muon Collider Collaboration (IMCC)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 $χ_{c1}(3872)\toγψ_2(3823)$Apr 22, 2024Study of $e^+e^-\toωX(3872)$ and $γX(3872)$ from 4.66 to 4.95 GeVApr 15, 2024First search for light fermionic dark matter absorption on electrons using germanium detector in CDEX-10 experimentApr 2, 2024Search for $C$-even states decaying to $D_{s}^{\pm}D_{s}^{*\mp}$ with masses between $4.08$ and $4.32~\mathrm{GeV}/c^{2}$Mar 29, 2024Probing Dark Matter Particles from Evaporating Primordial Black Holes via Electron Scattering in the CDEX-10 ExperimentMar 22, 2024Precise measurement of the $e^+e^-\to D_s^+D_s^-$ cross sections at center-of-mass energies from threshold to 4.95 GeVMar 6, 2024Observation of the decay $h_{c}\to3(π^{+}π^{-})π^{0}$Feb 6, 2024Precise Measurement of Born Cross Sections for $e^+e^-\to D\bar{D}$ at $\sqrt{s} = 3.80-4.95$ GeVJan 31, 2024Measurements of Normalized Differential Cross Sections of Inclusive $η$ Production in $e^{+}e^{-}$ Annihilation at Energy from 2.0000 to 3.6710 GeVJan 26, 2024Study of $e^{+}e^{-}\rightarrowπ^{+}π^{-}π^{0}$ at $\sqrt{s}$ from 2.00 to 3.08 GeV at BESIIIJan 20, 2024Prompt and nonprompt $ψ(2S)$ production in $p$Pb collisions at $\sqrt{s_{NN}}=8.16$ TeVDec 27, 2023Observation of $χ_{cJ}\to 3(K^+K^-)$Dec 14, 2023Amplitude analysis of the $B^{0}\to K^{*0}μ^+μ^-$ decayNov 17, 2023A model-independent measurement of the CKM angle $γ$ in partially reconstructed $B^{\pm} \to D^{*} h^{\pm}$ decays with $D \to K_{S}^{0} h^{+}h^{-}$ $(h=π, K)$Oct 6, 2023Measurement of the CKM angle $γ$ using the $B^{\pm}\rightarrow D^{*} h^{\pm}$ channels