<?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>2026-04-13T07:01:37Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2445/131406" metadataPrefix="marc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2445/131406</identifier><datestamp>2025-12-05T16:41:35Z</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">2019-04-04T12:50:29Z</subfield>
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      <subfield code="c">2019-04-04T12:50:29Z</subfield>
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      <subfield code="c">2006-09-05</subfield>
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      <subfield code="c">2019-04-04T12:50:29Z</subfield>
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      <subfield code="a">We describe searches for B meson decays to the charmless vector-vector final states ω K ∗ , ω ρ , ω ω , and ω ϕ with 233 × 10 6 B ¯¯¯ B pairs produced in e + e − B ¯¯¯ B annihilation at √ s = 10.58     GeV . We also search for the vector-scalar B decay to ω f 0 . We measure the following branching fractions in units of 10 − 6 : B ( B 0 → ω K * 0 ) = 2.4 ± 1.1 ± 0.7     ( &lt; 4.2 ) , B ( B + → ω K * + ) = 0.6 + 1.4 + 1.1 − 1.2 − 0.9     ( &lt; 3.4 ) , B ( B 0 → ω ρ 0 ) = − 0.6 ± 0.7 + 0.8 − 0.3     ( &lt; 1.5 ) , B ( B + → ω ρ + ) = 10.6 ± 2.1 + 1.6 − 1.0 , B ( B 0 → ω ω ) = 1.8 + 1.3 − 0.9 ± 0.4     ( &lt; 4.0 ) , B ( B 0 → ω ϕ ) = 0.1 ± 0.5 ± 0.1     ( &lt; 1.2 ) , and B ( B 0 → ω f 0 ) = 0.9 ± 0.4 + 0.2 − 0.1     ( &lt; 1.5 ) . In each case the first error quoted is statistical, the second systematic, and the upper limits are defined at the 90% confidence level. For B + → ω ρ + decays we also measure the longitudinal spin component f L = 0.82 ± 0.11 ± 0.02 and the charge asymmetry A C P = 0.04 ± 0.18 ± 0.02 .</subfield>
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      <subfield code="a">Física de partícules</subfield>
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      <subfield code="a">Experiments</subfield>
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      <subfield code="a">Mesons (Física nuclear)</subfield>
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      <subfield code="a">Particle physics</subfield>
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      <subfield code="a">Experiments</subfield>
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      <subfield code="a">Mesons (Nuclear physics)</subfield>
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      <subfield code="a">B meson decays to ωK*, ωρ, ωω, ωϕ, and ωf0</subfield>
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