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Observation of ${\chi }_{cJ}\to \Lambda \overline{\Lambda }\eta $

CERN İşbirliği


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  <identifier identifierType="URL">https://aperta.ulakbim.gov.tr/record/262531</identifier>
  <creators>
    <creator>
      <creatorName>CERN İşbirliği</creatorName>
      <affiliation>CERN</affiliation>
    </creator>
  </creators>
  <titles>
    <title>Observation Of ${\Chi }_{Cj}\To \Lambda \Overline{\Lambda }\Eta $</title>
  </titles>
  <publisher>Aperta</publisher>
  <publicationYear>2022</publicationYear>
  <dates>
    <date dateType="Issued">2022-01-01</date>
  </dates>
  <resourceType resourceTypeGeneral="Text">Journal article</resourceType>
  <alternateIdentifiers>
    <alternateIdentifier alternateIdentifierType="url">https://aperta.ulakbim.gov.tr/record/262531</alternateIdentifier>
  </alternateIdentifiers>
  <relatedIdentifiers>
    <relatedIdentifier relatedIdentifierType="DOI" relationType="IsIdenticalTo">10.1103/PhysRevD.106.072004</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;By analyzing $\left(448.1±2.9\right)×{10}^{6}\text{}\text{}\psi \left(3686\right)$ events collected with the BESIII detector operating at the BEPCII collider, the decays of ${\chi }_{cJ}\to \Lambda \overline{\Lambda }\eta $ ($J=0$, 1, and 2) are observed for the first time with statistical significances of $13.9\sigma $, $6.7\sigma $, and $8.2\sigma $, respectively. The product branching fractions of $\psi \left(3686\right)\to \gamma {\chi }_{cJ}$ and ${\chi }_{cJ}\to \Lambda \overline{\Lambda }\eta $ are measured. Dividing by the world averages of the branching fractions of $\psi \left(3686\right)\to \phantom{\rule{0ex}{0ex}}\gamma {\chi }_{cJ}$, the branching fractions of ${\chi }_{cJ}\to \Lambda \overline{\Lambda }\eta $ decays are determined to be $\left(2.31±0.30±0.21\right)×{10}^{-4}$, $\left(5.86±1.38±0.68\right)×{10}^{-5}$, and $\left(1.05±0.21±0.15\right)×{10}^{-4}$ for $J=0$, 1 and 2, respectively, where the first uncertainties are statistical and the second systematic.&lt;/p&gt;</description>
  </descriptions>
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