1 Ocak 2022 Dergi makalesi Açık Erişim

Bayar, M.; Oset, E.

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  <identifier identifierType="URL">https://aperta.ulakbim.gov.tr/record/262589</identifier>
  <creators>
    <creator>
      <creatorName>Bayar, M.</creatorName>
      <givenName>M.</givenName>
      <familyName>Bayar</familyName>
      <affiliation>Department of Physics, Kocaeli University, Izmit, Turkey</affiliation>
    </creator>
    <creator>
      <creatorName>Oset, E.</creatorName>
      <givenName>E.</givenName>
      <familyName>Oset</familyName>
      <affiliation>Departamento de Física Teórica, IFIC, Centro Mixto Universidad de Valencia-CSIC Institutos de Investigación de Paterna, Valencia, Spain</affiliation>
    </creator>
  </creators>
  <titles>
    <title>Method To Observe The = 2 Partner Of The (2866) In The → Reaction</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/262589</alternateIdentifier>
  </alternateIdentifiers>
  <relatedIdentifiers>
    <relatedIdentifier relatedIdentifierType="DOI" relationType="IsIdenticalTo">10.1016/j.physletb.2022.137364</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;We propose a method based on the moments of the ${D}^{-}{K}^{+}$ mass distribution in the ${B}^{+}\to {D}^{+}{D}^{-}{K}^{+}$ decay to disentangle the contribution of the ${2}^{+}$ state, partner of ${X}_{0}\left(2900\right)$ in the ${\overline{D}}^{⁎}{K}^{⁎}$ picture for this resonance. Some of these moments show the interference patterns of the ${X}_{1}\left(2900\right)$ and ${X}_{0}\left(2900\right)$ with the ${2}^{+}$ state, which provide a clearer signal of the ${2}^{+}$ resonance than the ${2}^{+}$ signal alone. The construction of these magnitudes from present data is easy to implement, and based on these data we show that clear signals for that resonance should be seen even with the present statistics.&lt;/p&gt;</description>
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