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Measurement of the \(K_S \to \pi e \nu\) branching fraction with the KLOE experiment
The branching fraction for the decay \(K_S \to \pi e \nu\) has been measured with 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. Signal decays are selected by a boosted decision tree built with k...
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Published in: | arXiv.org 2023-01 |
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format: | Article |
Language: | English |
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Online Access: | Get full text |
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Summary: | The branching fraction for the decay \(K_S \to \pi e \nu\) has been measured with 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. Signal decays are selected by a boosted decision tree built with kinematic variables and time-of-flight measurements. Data control samples of \(K_L \to \pi e \nu\) decays are used to evaluate signal selection efficiencies. A fit to the reconstructed electron mass distribution finds 49647\(\pm\)316 signal events. Normalising to the \(K_S \to \pi^+\pi^-\) decay events the result for the branching fraction is \(\mathcal{B}(K_S \to \pi e \nu) = (7.211 \pm 0.046_{\rm stat} \pm 0.052_{\rm syst}) \times10^{-4}\). The combination with our previous measurement gives \(\mathcal{B}(K_S \to \pi e \nu) = (7.153 \pm 0.037_{\rm stat} \pm 0.043_{\rm syst}) \times10^{-4}\). From this value we derive \(f_+(0)|V_{us}| = 0.2170 \pm 0.009\). |
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ISSN: | 2331-8422 |