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{
"@context": "https://schema.org/",
"@id": 275155,
"@type": "ScholarlyArticle",
"creator": [
{
"@type": "Person",
"affiliation": "CERN",
"name": "CERN \u0130\u015fbirli\u011fi"
}
],
"datePublished": "2024-04-08",
"description": "<p>Using a data sample corresponding to an integrated luminosity of $10.9\\text{}\\text{}{\\mathrm{fb}}^{-1}$ collected at center-of-mass energies from 4.16 to 4.34 GeV with the BESIII detector, we search for the decay ${\\chi }_{c1}\\left(3872\\right)\\to {\\pi }^{+}{\\pi }^{-}{\\chi }_{c1}$ in the radiative production ${e}^{+}{e}^{-}\\to \\gamma {\\chi }_{c1}\\left(3872\\right)$. No significant signal is observed, and the ratio for the branching fraction of ${\\chi }_{c1}\\left(3872\\right)\\to {\\pi }^{+}{\\pi }^{-}{\\chi }_{c1}$ to ${\\chi }_{c1}\\left(3872\\right)\\to {\\pi }^{+}{\\pi }^{-}J/\\psi $ is measured as $R\\equiv \\frac{B\\left[{\\chi }_{c1}\\left(3872\\right)\\to {\\pi }^{+}{\\pi }^{-}{\\chi }_{c1}\\right]}{B\\left[{\\chi }_{c1}\\left(3872\\right)\\to {\\pi }^{+}{\\pi }^{-}J/\\psi \\right]}<0.18$ at 90% confidence level. An upper limit on the product of the cross section $\\sigma \\left[{e}^{+}{e}^{-}\\to \\gamma {\\chi }_{c1}\\left(3872\\right)\\right]$ and the branching fraction $B\\left[{\\chi }_{c1}\\left(3872\\right)\\to {\\pi }^{+}{\\pi }^{-}{\\chi }_{c1}\\right]$ at each center-of-mass energy is also given. These measurements favor the nonconventional charmonium nature of the ${\\chi }_{c1}\\left(3872\\right)$ state.</p>",
"headline": "Search for the decay ${\\chi }_{c1}\\left(3872\\right)\\to {\\pi }^{+}{\\pi }^{-}{\\chi }_{c1}$",
"identifier": 275155,
"image": "https://aperta.ulakbim.gov.tr/static/img/logo/aperta_logo_with_icon.svg",
"license": "http://www.opendefinition.org/licenses/cc-by",
"name": "Search for the decay ${\\chi }_{c1}\\left(3872\\right)\\to {\\pi }^{+}{\\pi }^{-}{\\chi }_{c1}$",
"url": "https://aperta.ulakbim.gov.tr/record/275155"
}
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