<?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>2026-04-13T03:59:13Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2445/131838" metadataPrefix="marc">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><record xmlns="http://www.loc.gov/MARC21/slim" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.loc.gov/MARC21/slim http://www.loc.gov/standards/marcxml/schema/MARC21slim.xsd">
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      <subfield code="a">Graugés Pous, Eugeni</subfield>
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      <subfield code="a">BABAR Collaboration</subfield>
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      <subfield code="c">2019-04-08T13:50:37Z</subfield>
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      <subfield code="c">2019-04-08T13:50:37Z</subfield>
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      <subfield code="c">2013-06-01</subfield>
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      <subfield code="c">2019-04-08T13:50:37Z</subfield>
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      <subfield code="a">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.</subfield>
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      <subfield code="a">Física de partícules</subfield>
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      <subfield code="a">Particle physics</subfield>
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      <subfield code="a">Search for B→K(*)νν¯ and invisible quarkonium decays</subfield>
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