Showing 41–60 of 134 results
/ Date/ Name
Nov 13, 2023First Measurement of $R(X_{τ/\ell})$ as an Inclusive Test of the $b \to c τν$ AnomalySep 8, 2023Search for the semileptonic decays $D^+_s \to K_1(1270)^0 e^+ν_e$ and $D^+_s \to b_1(1235)^0 e^+ν_e$Aug 9, 2023Measurement of branching-fraction ratios and $CP$ asymmetries in $B^{\pm} \to D_{CP\pm}K^{\pm}$ decays at Belle and Belle IIJul 18, 2023Measurement of the branching fractions of the singly Cabibbo-suppressed decays $Λ_{c}^{+}\to pη$ and $Λ_{c}^{+}\to pω$Jun 1, 2023Precise measurement of the $D^+_s$ lifetime at Belle IIMay 30, 2023Measurement of the $τ$-lepton mass with the Belle~II experimentMay 24, 2023Determination of spin and parity of $D^{*}_{(s)}$ mesonsMar 15, 2023Measurement of the Branching Fraction for the Decay $ψ(3686) \rightarrow φK_{S}^{0} K_{S}^{0}$Feb 27, 2023Precision Measurement of the Decay $Σ^{+} \rightarrow pγ$ in the Process $J/ψ\rightarrow Σ^{+}\barΣ^{-}$Jan 20, 2023Search for the decay $B^0_s \rightarrow π^0 π^0$ at BelleDec 10, 2022First Direct Measurement of the Absolute Branching Fraction of $Σ^+ \to Λe^+ ν_{e}$Dec 7, 2022Improved measurement of the absolute branching fraction of inclusive semileptonic $Λ_c^+$ decayOct 19, 2022Measurement of the photon-energy spectrum in inclusive $B\rightarrow X_{s}γ$ decays identified using hadronic decays of the recoil $B$ meson in 2019-2021 Belle II dataOct 9, 2022Determination of $|V_{ub}|$ from untagged $B^0\toπ^- \ell^+ ν_{\ell}$ decays using 2019-2021 Belle II dataAug 18, 2022Measurement of the $Ω_c^0$ lifetime at Belle IIAug 9, 2022Search for a massless dark photon in $Λ^{+}_{c}\to p γ^{\prime}$ decayJun 22, 2022Observation of $Ξ^{-}$ Hyperon Transverse Polarization in $ψ(3686)\rightarrowΞ^{-}\barΞ^{+}$Jun 17, 2022Observation of $η_c(2S) \to 3(π^+π^-)$ and measurements of $χ_{cJ} \to 3(π^+π^-)$ in $ψ(3686)$ radiative transitionsApr 16, 2022Observation of the $Y(4230)$ and a new structure in $e^+e^- \rightarrow K^+K^-J/ψ$Mar 23, 2022Observation of the double Dalitz decay $η'\to e^+e^-e^+e^-$