<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-04-14T05:39:32Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2445/131838" metadataPrefix="oai_dc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2445/131838</identifier><datestamp>2025-12-05T16:39:04Z</datestamp><setSpec>com_2072_1057</setSpec><setSpec>col_2072_478823</setSpec><setSpec>col_2072_478917</setSpec></header><metadata><oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
   <dc:title>Search for B→K(*)νν¯ and invisible quarkonium decays</dc:title>
   <dc:creator>Graugés Pous, Eugeni</dc:creator>
   <dc:creator>BABAR Collaboration</dc:creator>
   <dc:subject>Física de partícules</dc:subject>
   <dc:subject>Experiments</dc:subject>
   <dc:subject>Particle physics</dc:subject>
   <dc:subject>Experiments</dc:subject>
   <dc:description>We search for the flavor-changing neutral-current decays B → K ( * ) ν ¯ ν , and the invisible decays J / ψ → ν ¯ ν and ψ ( 2 S ) → ν ¯ ν via B → K ( * ) J / ψ and B → K ( * ) ψ ( 2 S ) , respectively, using a data sample of 471 × 10 6 B ¯¯¯ B pairs collected by the BABAR experiment. We fully reconstruct the hadronic decay of one of the B mesons in the Υ ( 4 S ) → B ¯¯¯ B decay, and search for the B → K ( * ) ν ¯ ν decay in the rest of the event. We observe no significant excess of signal decays over background and report branching fraction upper limits of B ( B + → K + ν ¯ ν ) &lt; 3.7 × 10 − 5 , B ( B 0 → K 0 ν ¯ ν ) &lt; 8.1 × 10 − 5 , B ( B + → K * + ν ¯ ν ) &lt; 11.6 × 10 − 5 , B ( B 0 → K * 0 ν ¯ ν ) &lt; 9.3 × 10 − 5 , and combined upper limits of B ( B → K ν ¯ ν ) &lt; 3.2 × 10 − 5 and B ( B → K ∗ ν ¯ ν ) &lt; 7.9 × 10 − 5 , all at the 90% confidence level. For the invisible quarkonium decays, we report branching fraction upper limits of B ( J / ψ → ν ¯ ν ) &lt; 3.9 × 10 − 3 and B ( ψ ( 2 S ) → ν ¯ ν ) &lt; 15.5 × 10 − 3 at the 90% confidence level. Using the improved kinematic resolution achieved from hadronic reconstruction, we also provide partial branching fraction limits for the B → K ( * ) ν ¯ ν decays over the full kinematic spectrum.</dc:description>
   <dc:date>2019-04-08T13:50:37Z</dc:date>
   <dc:date>2019-04-08T13:50:37Z</dc:date>
   <dc:date>2013-06-01</dc:date>
   <dc:date>2019-04-08T13:50:37Z</dc:date>
   <dc:type>info:eu-repo/semantics/article</dc:type>
   <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
   <dc:identifier>1550-7998</dc:identifier>
   <dc:identifier>https://hdl.handle.net/2445/131838</dc:identifier>
   <dc:identifier>628996</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:relation>Reproducció del document publicat a: https://doi.org/10.1103/PhysRevD.87.112005</dc:relation>
   <dc:relation>Physical Review D, 2013, vol. 87, num. 11, p. 112005</dc:relation>
   <dc:relation>https://doi.org/10.1103/PhysRevD.87.112005</dc:relation>
   <dc:rights>(c) American Physical Society, 2013</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:format>13 p.</dc:format>
   <dc:format>application/pdf</dc:format>
   <dc:publisher>American Physical Society</dc:publisher>
   <dc:source>Articles publicats en revistes (Física Quàntica i Astrofísica)</dc:source>
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