1 Ocak 2020 Dergi makalesi Açık Erişim

CERN İşbirliği

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  <identifier identifierType="URL">https://aperta.ulakbim.gov.tr/record/105101</identifier>
  <creators>
    <creator>
      <creatorName>CERN İşbirliği</creatorName>
      <affiliation>CERN</affiliation>
    </creator>
  </creators>
  <titles>
    <title>Precise Measurements Of Branching Fractions For   ${D}_{S}^{+}$     Meson Decays To Two Pseudoscalar Mesons</title>
  </titles>
  <publisher>Aperta</publisher>
  <publicationYear>2020</publicationYear>
  <dates>
    <date dateType="Issued">2020-01-01</date>
  </dates>
  <resourceType resourceTypeGeneral="Text">Journal article</resourceType>
  <alternateIdentifiers>
    <alternateIdentifier alternateIdentifierType="url">https://aperta.ulakbim.gov.tr/record/105101</alternateIdentifier>
  </alternateIdentifiers>
  <relatedIdentifiers>
    <relatedIdentifier relatedIdentifierType="DOI" relationType="IsIdenticalTo">10.1007/JHEP08(2020)146</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 measure the branching fractions for seven   ${D}_{s}^{+}$     two-body decays to pseudo-scalar mesons, by analyzing data collected at   $\sqrt{s}$     = 4.178 ∼ 4.226 GeV with the BESIII detector at the BEPCII collider. The branching fractions are determined to be  $\begin{array}{c}B\left({D}_{s}^{+}\to {K}^{+}\eta \text{'}\right)=\left(2.68±0.17±0.17±0.08\right)×{10}^{-3},\\ B\left({D}_{s}^{+}\to \eta \text{'}{\pi }^{+}\right)=\left(37.8±0.4±2.1±1.2\right)×{10}^{-3},\\ B\left({D}_{s}^{+}\to {K}^{+}\eta \right)=\left(1.62±0.10±0.03±0.05\right)×{10}^{-3},\\ B\left({D}_{s}^{+}\to \eta {\pi }^{+}\right)=\left(17.41±0.18±0.27±0.54\right)×{10}^{-3},\\ B\left({D}_{s}^{+}\to {K}^{+}{K}_{S}^{0}\right)=\left(15.02±0.10±0.27±0.47\right)×{10}^{-3},\\ B\left({D}_{s}^{+}\to {K}_{S}^{0}{\pi }^{+}\right)=\left(1.109±0.034±0.023±0.035\right)×{10}^{-3},\\ B\left({D}_{s}^{+}\to {K}^{+}{\pi }^{0}\right)=\left(0.748±0.049±0.018±0.035\right)×{10}^{-3},\end{array}$   &lt;/p&gt;</description>
  </descriptions>
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