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  • Babusci, D; Berlowski, M; Bloise, C; Bossi, F; Branchini, P; Budano, A; Cao, B; Ceradini, F; Ciambrone, P; Curciarello, F; Czerwisnski, E; D'Agostini, G; Danè, E; De Leo, V; De Lucia, E; De Santis, A; De Simone, P; Di Cicco, A; Di Domenico, A; Domenici, D; D'Uffizi, A; Fantini, A; Fermani, P; Fiore, S; Gajos, A; Gauzzi, P; Giovannella, S; Graziani, E; Ivanov, V. L; Johansson, T; Kang, X; Kisielewska-Kamisnska, D; Kozyrev, E. A; Krzemien, W; Kupsc, A; Lukin, P. A; Mandaglio, G; Martini, M; Messi, R; Miscetti, S; Moricciani, D; Moskal, P; Parzych, S; Passeri, A; Patera, V; del Rio, E. Perez; Santangelo, P; Schioppa, M; Selce, A; Silarski, M; Sirghi, F; Solodov, E. P; Tortora, L; Venanzoni, G; Wislicki, W; Wolke, M

    12/2019
    Journal Article

    Based on a sample of 300 million $K_S$ mesons produced in $\phi \to K_L K_S$ decays recorded by the KLOE experiment at the DA$\Phi$NE $e^+e^-$ collider we have measured the branching fraction for the decay $K_S \to \pi \mu \nu$. The $K_S$ mesons are identified by the interaction of $K_L$ mesons in the detector. The $K_S \to \pi \mu \nu$ decays are selected by a boosted decision tree built with kinematic variables and by a time-of-flight measurement. Signal efficiencies are evaluated with data control samples of $K_L \to \pi \mu \nu$ decays. A fit to the reconstructed muon mass distribution finds $7223 \pm 180$ signal events. Normalising to the $K_S \to \pi^+ \pi^-$ decay events the result for the branching fraction is $\mathcal{B}(K_S \to \pi \mu \nu) = (4.56 \pm 0.11_{\rm stat} \pm 0.17_{\rm syst})\times10^{-4}$.