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Measurement of the production cross section for a W boson in association with a charm quark in proton–proton collisions at $\sqrt{s}=13\phantom{\rule{0.166667em}{0ex}}\text{TeV}$

CERN İşbirliği


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  <identifier identifierType="URL">https://aperta.ulakbim.gov.tr/record/275341</identifier>
  <creators>
    <creator>
      <creatorName>CERN İşbirliği</creatorName>
      <affiliation>CERN</affiliation>
    </creator>
  </creators>
  <titles>
    <title>Measurement Of The Production Cross Section For A W Boson In Association With A Charm Quark In Proton–Proton Collisions At     $\Sqrt{S}=13\Phantom{\Rule{0.166667Em}{0Ex}}\Text{Tev}$</title>
  </titles>
  <publisher>Aperta</publisher>
  <publicationYear>2024</publicationYear>
  <dates>
    <date dateType="Issued">2024-01-10</date>
  </dates>
  <resourceType resourceTypeGeneral="Text">Journal article</resourceType>
  <alternateIdentifiers>
    <alternateIdentifier alternateIdentifierType="url">https://aperta.ulakbim.gov.tr/record/275341</alternateIdentifier>
  </alternateIdentifiers>
  <relatedIdentifiers>
    <relatedIdentifier relatedIdentifierType="DOI" relationType="IsIdenticalTo">10.1140/epjc/s10052-023-12258-4</relatedIdentifier>
  </relatedIdentifiers>
  <rightsList>
    <rights rightsURI="http://www.opendefinition.org/licenses/cc-by">Creative Commons Attribution</rights>
    <rights rightsURI="info:eu-repo/semantics/openAccess">Open Access</rights>
  </rightsList>
  <descriptions>
    <description descriptionType="Abstract">&lt;p&gt;The strange quark content of the proton is probed through the measurement of the production cross section for a W boson and a charm (c) quark in proton–proton collisions at a center-of-mass energy of 13    $\phantom{\rule{0.166667em}{0ex}}\text{Te}\phantom{\rule{-0.80002pt}{0ex}}\text{V}$  . The analysis uses a data sample corresponding to a total integrated luminosity of 138    $\phantom{\rule{0.166667em}{0ex}}{\text{fb}}^{-1}$   collected with the CMS detector at the LHC. The W bosons are identified through their leptonic decays to an electron or a muon, and a neutrino. Charm jets are tagged using the presence of a muon or a secondary vertex inside the jet. The     $\text{W}+\text{c}$   production cross section and the cross section ratio     ${R}_{\text{c}}^{±}=\sigma \left({\text{W}}^{+}+\overline{\text{c}}\right)/\sigma \left({\text{W}}^{-}+\text{c}\right)$   are measured inclusively and differentially as functions of the transverse momentum and the pseudorapidity of the lepton originating from the W boson decay. The precision of the measurements is improved with respect to previous studies, reaching 1% in     ${R}_{\text{c}}^{±}=0.950±0.005\phantom{\rule{0.166667em}{0ex}}\text{(stat)}±0.010\phantom{\rule{0.166667em}{0ex}}\text{(syst)}$  . The measurements are compared with theoretical predictions up to next-to-next-to-leading order in perturbative quantum chromodynamics.&lt;/p&gt;</description>
  </descriptions>
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