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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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creator | Babusci, D Berlowski, M Bloise, C Bossi, F Branchini, P Cao, B Ceradini, F Ciambrone, P Curciarello, F Czerwiński, E D'Agostini, G D'Amico, R Danè, E De Leo, V De Lucia, E De Santis, A De Simone, P A Di Cicco A Di Domenico Diociaiuti, E Domenici, D D'Uffizi, A Fantini, G Gajos, A Gamrat, S Gauzzi, P Giovannella, S Graziani, E Kang, X Kupsc, A Mandaglio, G Martini, M Miscetti, S Moskal, P Passeri, A Perez del Rio, E Schioppa, M Selce, A Silarski, M Sirghi, F Solodov, E P Wiślicki, W Wolke, M |
description | 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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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 \(f_+(0)|V_{us}| = 0.2170 \pm 0.009\).</description><identifier>EISSN: 2331-8422</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Decay ; Decision trees ; Electron mass ; Mass distribution ; Mesons</subject><ispartof>arXiv.org, 2023-01</ispartof><rights>2023. This work is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.proquest.com/docview/2700908316?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>780,784,25753,37012,44590</link.rule.ids></links><search><creatorcontrib>Babusci, D</creatorcontrib><creatorcontrib>Berlowski, M</creatorcontrib><creatorcontrib>Bloise, C</creatorcontrib><creatorcontrib>Bossi, F</creatorcontrib><creatorcontrib>Branchini, P</creatorcontrib><creatorcontrib>Cao, B</creatorcontrib><creatorcontrib>Ceradini, F</creatorcontrib><creatorcontrib>Ciambrone, P</creatorcontrib><creatorcontrib>Curciarello, F</creatorcontrib><creatorcontrib>Czerwiński, E</creatorcontrib><creatorcontrib>D'Agostini, G</creatorcontrib><creatorcontrib>D'Amico, R</creatorcontrib><creatorcontrib>Danè, E</creatorcontrib><creatorcontrib>De Leo, V</creatorcontrib><creatorcontrib>De Lucia, E</creatorcontrib><creatorcontrib>De Santis, A</creatorcontrib><creatorcontrib>De Simone, P</creatorcontrib><creatorcontrib>A Di Cicco</creatorcontrib><creatorcontrib>A Di Domenico</creatorcontrib><creatorcontrib>Diociaiuti, E</creatorcontrib><creatorcontrib>Domenici, D</creatorcontrib><creatorcontrib>D'Uffizi, A</creatorcontrib><creatorcontrib>Fantini, G</creatorcontrib><creatorcontrib>Gajos, A</creatorcontrib><creatorcontrib>Gamrat, S</creatorcontrib><creatorcontrib>Gauzzi, P</creatorcontrib><creatorcontrib>Giovannella, S</creatorcontrib><creatorcontrib>Graziani, E</creatorcontrib><creatorcontrib>Kang, X</creatorcontrib><creatorcontrib>Kupsc, A</creatorcontrib><creatorcontrib>Mandaglio, G</creatorcontrib><creatorcontrib>Martini, M</creatorcontrib><creatorcontrib>Miscetti, S</creatorcontrib><creatorcontrib>Moskal, P</creatorcontrib><creatorcontrib>Passeri, A</creatorcontrib><creatorcontrib>Perez del Rio, E</creatorcontrib><creatorcontrib>Schioppa, M</creatorcontrib><creatorcontrib>Selce, A</creatorcontrib><creatorcontrib>Silarski, M</creatorcontrib><creatorcontrib>Sirghi, F</creatorcontrib><creatorcontrib>Solodov, E P</creatorcontrib><creatorcontrib>Wiślicki, W</creatorcontrib><creatorcontrib>Wolke, M</creatorcontrib><title>Measurement of the \(K_S \to \pi e \nu\) branching fraction with the KLOE experiment</title><title>arXiv.org</title><description>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 \(\mathcal{B}(K_S \to \pi e \nu) = (7.153 \pm 0.037_{\rm stat} \pm 0.043_{\rm syst}) \times10^{-4}\). 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; Miscetti, S ; Moskal, P ; Passeri, A ; Perez del Rio, E ; Schioppa, M ; Selce, A ; Silarski, M ; Sirghi, F ; Solodov, E P ; Wiślicki, W ; Wolke, M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_journals_27009083163</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Decay</topic><topic>Decision trees</topic><topic>Electron mass</topic><topic>Mass distribution</topic><topic>Mesons</topic><toplevel>online_resources</toplevel><creatorcontrib>Babusci, D</creatorcontrib><creatorcontrib>Berlowski, M</creatorcontrib><creatorcontrib>Bloise, C</creatorcontrib><creatorcontrib>Bossi, F</creatorcontrib><creatorcontrib>Branchini, P</creatorcontrib><creatorcontrib>Cao, B</creatorcontrib><creatorcontrib>Ceradini, F</creatorcontrib><creatorcontrib>Ciambrone, P</creatorcontrib><creatorcontrib>Curciarello, F</creatorcontrib><creatorcontrib>Czerwiński, 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D</au><au>D'Uffizi, A</au><au>Fantini, G</au><au>Gajos, A</au><au>Gamrat, S</au><au>Gauzzi, P</au><au>Giovannella, S</au><au>Graziani, E</au><au>Kang, X</au><au>Kupsc, A</au><au>Mandaglio, G</au><au>Martini, M</au><au>Miscetti, S</au><au>Moskal, P</au><au>Passeri, A</au><au>Perez del Rio, E</au><au>Schioppa, M</au><au>Selce, A</au><au>Silarski, M</au><au>Sirghi, F</au><au>Solodov, E P</au><au>Wiślicki, W</au><au>Wolke, M</au><format>book</format><genre>document</genre><ristype>GEN</ristype><atitle>Measurement of the \(K_S \to \pi e \nu\) branching fraction with the KLOE experiment</atitle><jtitle>arXiv.org</jtitle><date>2023-01-24</date><risdate>2023</risdate><eissn>2331-8422</eissn><abstract>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 \(f_+(0)|V_{us}| = 0.2170 \pm 0.009\).</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><oa>free_for_read</oa></addata></record> |
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subjects | Decay Decision trees Electron mass Mass distribution Mesons |
title | Measurement of the \(K_S \to \pi e \nu\) branching fraction with the KLOE experiment |
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