<?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>2026-04-17T00:42:25Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2445/131414" metadataPrefix="marc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2445/131414</identifier><datestamp>2025-12-05T16:43:50Z</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">2019-04-04T13:02:44Z</subfield>
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      <subfield code="c">2019-04-04T13:02:44Z</subfield>
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      <subfield code="c">2006-09-01</subfield>
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      <subfield code="c">2019-04-04T13:02:44Z</subfield>
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      <subfield code="a">We present measurements of branching fractions of B 0 decays to multibody final states containing protons, based on 232 × 10 6 Υ ( 4 S ) → B ¯¯¯ B decays collected with the BABAR detector at the SLAC PEP-II asymmetric-energy B factory. We measure the branching fractions B ( B 0 → ¯¯¯ D 0 p ¯ p ) = ( 1.13 ± 0.06 ± 0.08 ) × 10 − 4 , B ( B 0 → ¯¯¯ D * 0 p ¯ p ) = ( 1.01 ± 0.10 ± 0.09 ) × 10 − 4 , B ( B 0 → D − p ¯ p π + ) = ( 3.38 ± 0.14 ± 0.29 ) × 10 − 4 , and B ( B 0 → D * − p ¯ p π + ) = ( 4.81 ± 0.22 ± 0.44 ) × 10 − 4 where the first error is statistical and the second systematic. We present a search for the charmed pentaquark state, Θ c ( 3100 ) observed by H1 and put limits on the branching fraction B ( B 0 → Θ c ¯ p π + ) × B ( Θ c → D * − p ) &lt; 14 × 10 − 6 and B ( B 0 → Θ c ¯ p π + ) × B ( Θ c → D − p ) &lt; 9 × 10 − 6 . Upon investigation of the decay structure of the above four B 0 decay modes, we see an enhancement at low p ¯ p mass and deviations from phase-space in the ¯¯¯ D ¯ p and ¯¯¯ D p invariant mass spectra.</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">Experiments</subfield>
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      <subfield code="a">Measurements of the decays B0 → ¯D0p¯p, B0 → ¯D*0p¯p, B0 → D−p¯pπ+, and B0 → D*−p¯p+</subfield>
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