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Determination of Spin-Parity Quantum Numbers of $X\left(2370\right)$ as ${0}^{-+}$ from $J/\psi \to \gamma {K}_{S}^{0}{K}_{S}^{0}{\eta }^{\prime }$

CERN İşbirliği


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  <identifier identifierType="URL">https://aperta.ulakbim.gov.tr/record/275097</identifier>
  <creators>
    <creator>
      <creatorName>CERN İşbirliği</creatorName>
      <affiliation>CERN</affiliation>
    </creator>
  </creators>
  <titles>
    <title>Determination Of Spin-Parity Quantum Numbers Of $X\Left(2370\Right)$ As ${0}^{-+}$ From $J/\Psi \To \Gamma {K}_{S}^{0}{K}_{S}^{0}{\Eta }^{\Prime }$</title>
  </titles>
  <publisher>Aperta</publisher>
  <publicationYear>2024</publicationYear>
  <dates>
    <date dateType="Issued">2024-05-02</date>
  </dates>
  <resourceType resourceTypeGeneral="Text">Journal article</resourceType>
  <alternateIdentifiers>
    <alternateIdentifier alternateIdentifierType="url">https://aperta.ulakbim.gov.tr/record/275097</alternateIdentifier>
  </alternateIdentifiers>
  <relatedIdentifiers>
    <relatedIdentifier relatedIdentifierType="DOI" relationType="IsIdenticalTo">10.1103/PhysRevLett.132.181901</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;Based on $\left(10087±44\right)×{10}^{6}\text{}\text{}J/\psi $ events collected with the BESIII detector, a partial wave analysis of the decay $J/\psi \to \gamma {K}_{S}^{0}{K}_{S}^{0}{\eta }^{\prime }$ is performed. The mass and width of the $X\left(2370\right)$ are measured to be $2395±11\left(\mathrm{stat}{\right)}_{-94}^{+26}\left(\mathrm{syst}\right)\text{}\text{}\mathrm{MeV}/{c}^{2}$ and ${188}_{-17}^{+18}\left(\mathrm{stat}{\right)}_{-33}^{+124}\left(\mathrm{syst}\right)\text{}\text{}\mathrm{MeV}$, respectively. The corresponding product branching fraction is $B\left[J/\psi \to \gamma X\left(2370\right)\right]×B\left[X\left(2370\right)\to {f}_{0}\left(980\right){\eta }^{\prime }\right]×B\left[{f}_{0}\left(980\right)\to {K}_{S}^{0}{K}_{S}^{0}\right]=\phantom{\rule{0ex}{0ex}}\left(1.31±0.22\left(\mathrm{stat}{\right)}_{-0.84}^{+2.85}\left(\mathrm{syst}\right)\right)×{10}^{-5}$. The statistical significance of the $X\left(2370\right)$ is greater than $11.7\sigma $ and the spin parity is determined to be ${0}^{-+}$ for the first time. The measured mass and spin parity of the $X\left(2370\right)$ are consistent with the predictions of the lightest pseudoscalar glueball.&lt;/p&gt;</description>
  </descriptions>
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