<?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>2026-04-14T02:07:54Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:20.500.14342/3139" metadataPrefix="qdc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:20.500.14342/3139</identifier><datestamp>2026-03-05T23:39:57Z</datestamp><setSpec>com_2072_482405</setSpec><setSpec>com_2072_183628</setSpec><setSpec>col_2072_482415</setSpec></header><metadata><qdc:qualifieddc xmlns:qdc="http://dspace.org/qualifieddc/" xmlns:dc="http://purl.org/dc/elements/1.1/" 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://purl.org/dc/elements/1.1/ http://dublincore.org/schemas/xmls/qdc/2006/01/06/dc.xsd http://purl.org/dc/terms/ http://dublincore.org/schemas/xmls/qdc/2006/01/06/dcterms.xsd http://dspace.org/qualifieddc/ http://www.ukoln.ac.uk/metadata/dcmi/xmlschema/qualifieddc.xsd">
   <dc:title>First evidence for the annihilation decay mode B+→D+sφ</dc:title>
   <dc:creator>Calvo Gomez, Miriam</dc:creator>
   <dc:creator>Camboni, Alessandro</dc:creator>
   <dc:creator>Vilasis-Cardona, Xavier</dc:creator>
   <dc:creator>LHCb Collaboration - CERN</dc:creator>
   <dc:subject>Gran col·lisionador d'hadrons (França i Suïssa)</dc:subject>
   <dc:subject>Partícules (Física nuclear)</dc:subject>
   <dcterms:abstract>Evidence for the hadronic annihilation decay mode B+→D+sϕ&#xd;
&#xd;
is found with greater than 3σ significance. The branching fraction and CP asymmetry are measured to be&#xd;
$&#xd;
B(B+→D+sϕ)=(1.87+1.25−0.73(stat)±0.19(syst)±0.32(norm))×10−6,ACP(B+→D+sϕ)=−0.01±0.41(stat)±0.03(syst).&#xd;
$&#xd;
&#xd;
The last uncertainty on B(B+→D+sϕ)&#xd;
is from the branching fractions of the B+→D+sD¯¯¯¯0 normalization mode and intermediate resonance decays. Upper limits are also set for the branching fractions of the related decay modes B+(c)→D+(s)K∗0,B+(c)→D+(s)K¯¯¯¯¯∗0 and B+c→D+sϕ, including the result B(B+→D+K∗0)&lt;1.8×10−6 at the 90% credibility level.</dcterms:abstract>
   <dcterms:issued>2013-02-07</dcterms:issued>
   <dc:type>info:eu-repo/semantics/article</dc:type>
   <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
   <dc:identifier>http://hdl.handle.net/20.500.14342/3139</dc:identifier>
   <dc:identifier>https://doi.org/10.1007/JHEP02(2013)043</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:relation>Journal of High Energy Physics, 2013, Vol. 2013, No.2 (Febrer)</dc:relation>
   <dc:rights>http://creativecommons.org/licenses/by/4.0/</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:rights>Attribution 4.0 International</dc:rights>
   <dc:rights>© CERN</dc:rights>
   <dc:publisher>Springer</dc:publisher>
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