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{
"@context": "https://schema.org/",
"@id": 275327,
"@type": "ScholarlyArticle",
"creator": [
{
"@type": "Person",
"affiliation": "CERN",
"name": "CERN \u0130\u015fbirli\u011fi"
}
],
"datePublished": "2024-01-12",
"description": "<p>The first observation of the decays $J/\\psi \\to \\overline{p}{\\Sigma }^{+}{K}_{S}^{0}$ and $J/\\psi \\to p{\\overline{\\Sigma }}^{-}{K}_{S}^{0}$ is reported using $\\left(10087\u00b144\\right)\u00d7{10}^{6}\\text{}\\text{}J/\\psi $ events recorded by the BESIII detector at the BEPCII storage ring. The branching fractions of each channel are determined to be $B\\left(J/\\psi \\to \\overline{p}{\\Sigma }^{+}{K}_{S}^{0}\\right)=\\left(1.361\u00b10.006\u00b10.025\\right)\u00d7{10}^{-4}$, and $B\\left(J/\\psi \\to p{\\overline{\\Sigma }}^{-}{K}_{S}^{0}\\right)=\\left(1.352\u00b10.006\u00b10.025\\right)\u00d7{10}^{-4}$. The combined result is $B\\left(J/\\psi \\to \\overline{p}{\\Sigma }^{+}{K}_{S}^{0}+\\phantom{\\rule{0ex}{0ex}}c.c.\\right)=\\left(2.725\u00b10.009\u00b10.050\\right)\u00d7{10}^{-4}$, where the first uncertainty is statistical and the second systematic. The results presented are in good agreement with the branching fractions of the isospin partner decay $J/\\psi \\to p{K}^{-}{\\overline{\\Sigma }}^{0}+c.c.$</p>",
"headline": "Observation and branching fraction measurement of the decay $J/\\psi \\to \\overline{p}{\\Sigma }^{+}{K}_{S}^{0}+c.c.$",
"identifier": 275327,
"image": "https://aperta.ulakbim.gov.tr/static/img/logo/aperta_logo_with_icon.svg",
"license": "http://www.opendefinition.org/licenses/cc-by",
"name": "Observation and branching fraction measurement of the decay $J/\\psi \\to \\overline{p}{\\Sigma }^{+}{K}_{S}^{0}+c.c.$",
"url": "https://aperta.ulakbim.gov.tr/record/275327"
}
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