{"title":"Heavy flavor spectroscopy studies at CMS","authors":"Feng Zhu, Kai Yi","doi":"arxiv-2408.04557","DOIUrl":null,"url":null,"abstract":"The CMS Collaboration has performed many studies in the field of heavy flavor\nspectroscopy. In this report, recent studies on exotic resonances in\nproton-proton collisions at $\\sqrt{s} = 13$ TeV at CMS are presented. For the\nexotic hadrons, these results include the first evidence for X(3872) in\nheavy-ion collisions and three new structures in $J/\\psi J/\\psi$ mass spectrum.\nBeside the exotic hadrons, we also found new decay channels in conventional\nbeauty hadrons, including $B^{0}_{s}\\rightarrow\\psi(2S)K^{0}_{S}$,\n$\\Lambda_{b}^{0}\\rightarrow J/\\psi\\Xi^{-}K^{+} $, $B^{0} \\rightarrow\n\\psi(2S)K^{0}_{S}\\pi^{+} \\pi^{-}$, and $\\Xi_{b}^{-} \\rightarrow\n\\psi(2S)\\Xi^{-}$.","PeriodicalId":501181,"journal":{"name":"arXiv - PHYS - High Energy Physics - Experiment","volume":"84 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Physics - Experiment","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.04557","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The CMS Collaboration has performed many studies in the field of heavy flavor
spectroscopy. In this report, recent studies on exotic resonances in
proton-proton collisions at $\sqrt{s} = 13$ TeV at CMS are presented. For the
exotic hadrons, these results include the first evidence for X(3872) in
heavy-ion collisions and three new structures in $J/\psi J/\psi$ mass spectrum.
Beside the exotic hadrons, we also found new decay channels in conventional
beauty hadrons, including $B^{0}_{s}\rightarrow\psi(2S)K^{0}_{S}$,
$\Lambda_{b}^{0}\rightarrow J/\psi\Xi^{-}K^{+} $, $B^{0} \rightarrow
\psi(2S)K^{0}_{S}\pi^{+} \pi^{-}$, and $\Xi_{b}^{-} \rightarrow
\psi(2S)\Xi^{-}$.