Showing 1–20 of 46 results
/ Date/ Name
Sep 6, 2024ZTF SN Ia DR2: Simulations and volume limited sampleSep 6, 2024ZTF SN Ia DR2: The diversity and relative rates of the thermonuclear SN populationJun 4, 2020Search for $CP$ violation in $Ξ_c^+\rightarrow pK^-π^+$ decays using model-independent techniquesFeb 19, 2020Measurement of the branching fraction of the decay $B_s^0\to K_S^0 K_S^0$Feb 5, 2020Observational constraints on the optical and near-infrared emission from the neutron star-black hole binary merger S190814bvNov 8, 2019Measurement of the $η_c(1S)$ production cross-section in $pp$ collisions at $\sqrt{s} = 13$ TeVJul 1, 2019Observation of the $Λ_b^0\rightarrow χ_{c1}(3872)pK^-$ decayJun 19, 2019Precision measurement of the $Λ_c^+$, $Ξ_c^+$ and $Ξ_c^0$ baryon lifetimesMay 16, 2019Amplitude analysis of the $B_{(s)} \to K^{*0} \overline{K}^{*0}$ decays and measurement of the branching fraction of the $B \to K^{*0} \overline{K}^{*0}$ decayMar 29, 2019Observation of an excited $B_c^+$ stateMar 21, 2019Search for lepton-universality violation in $B^+\to K^+\ell^+\ell^-$ decaysFeb 14, 2019Observation of $B^0_{(s)} \to J/ψp \overline{p}$ decays and precision measurements of the $B^0_{(s)}$ massesJan 21, 2019Measurement of the mass and production rate of $Ξ_b^-$ baryonsJan 17, 2019Model-independent observation of exotic contributions to $B^0\to J/ψK^+π^-$ decaysDec 14, 2018Search for the rare decay $B^{+} \rightarrow μ^{+}μ^{-}μ^{+}ν_{μ}$Dec 10, 2018Target of Opportunity Observations of Gravitational Wave Events with LSSTDec 6, 2018Delayed Circumstellar Interaction for Type Ia SN 2015cp Revealed by an HST Ultraviolet Imaging SurveyAug 18, 2018Measurement of antiproton production in ${\rm p He}$ collisions at $\sqrt{s_{NN}}=110$ GeVJul 27, 2018Measurement of the relative $B^{-} \!\rightarrow D^{0} / D^{*0} / D^{**0} μ^{-} \overlineν_μ$ branching fractions using $B^{-}$ mesons from $\overline{B}{}_{s2}^{*0}$ decaysJul 5, 2018First observation of the doubly charmed baryon decay $Ξ_{cc}^{++}\rightarrow Ξ_{c}^{+}π^{+}$