<?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>2026-04-17T19:18:58Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:20.500.14342/3192" metadataPrefix="oai_dc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:20.500.14342/3192</identifier><datestamp>2025-03-11T04:12:30Z</datestamp><setSpec>com_2072_482405</setSpec><setSpec>com_2072_183628</setSpec><setSpec>col_2072_482415</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>Precision measurement of D meson mass differences</dc:title>
   <dc:creator>Calvo Gómez, Míriam</dc:creator>
   <dc:creator>Camboni, Alessandro</dc:creator>
   <dc:creator>Vilasís Cardona, Xavier</dc:creator>
   <dc:creator>LHCb Collaboration - CERN</dc:creator>
   <dc:contributor>Universitat Ramon Llull. La Salle</dc:contributor>
   <dc:contributor>CERN</dc:contributor>
   <dc:subject>Gran col·lisionador d'hadrons (França i Suïssa)</dc:subject>
   <dc:subject>Partícules (Física nuclear)</dc:subject>
   <dc:subject>Col·lisions (Física nuclear)</dc:subject>
   <dc:subject>Mesons</dc:subject>
   <dc:subject>539</dc:subject>
   <dc:description>Using three- and four-body decays of D mesons produced in semileptonic b-hadron decays, precision measurements of D meson mass differences are made together with a measurement of the D 0 mass. The measurements are based on a dataset corresponding to an integrated luminosity of 1.0 fb−1 collected in pp collisions at 7 TeV. Using the decay D 0 → K + K − K − π +, the D 0 mass is measured to be
$ M\left( {{D^0}} \right)={{{1864.75\pm 0.15\left( {\mathrm{stat}} \right)\pm 0.11\left( {\mathrm{syst}} \right)\mathrm{MeV}}} \left/ {{{c^2}}} \right.}. $

The mass differences

M(D+)−M(D0)=4.76±0.12(stat)±0.07(syst)MeV/c2,M(Ds)−M(D+)=98.68±0.03(stat)±0.04(syst)MeV/c2

are measured using the D 0 → K + K − π + π − and D+(s)→K+K−π+
modes.</dc:description>
   <dc:date>2013-06-17</dc:date>
   <dc:type>info:eu-repo/semantics/article</dc:type>
   <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
   <dc:identifier>http://hdl.handle.net/20.500.14342/3192</dc:identifier>
   <dc:identifier>https://doi.org/10.1007/JHEP06(2013)065</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:relation>Journal of High Energy Physics, 2013, Vol. 2013, No.6 (Juny)</dc:relation>
   <dc:rights>Attribution 4.0 International</dc:rights>
   <dc:rights>© CERN</dc:rights>
   <dc:rights>http://creativecommons.org/licenses/by/4.0/</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:format>17 p.</dc:format>
   <dc:publisher>Springer</dc:publisher>
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