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First Observation of a Three-Resonance Structure in e
Ablikim, M; Achasov, M N; Adlarson, P; Ai, X C; Aliberti, R; Amoroso, A; An, M R; An, Q; Bai, Y; Bakina, O; Balossino, I; Ban, Y; Batozskaya, V; Begzsuren, K; Berger, N; Berlowski, M; Bertani, M; Bettoni, D; Bianchi, F; Bianco, E; Bortone, A; Boyko, I; Briere, R A; Brueggemann, A; Cai, H; Cai, X; Calcaterra, A; Cao, G F; Cao, N; Cetin, S A; Chang, J F; Chang, T T; Chang, W L; Che, G R; Chelkov, G; Chen, C; Chen, Chao; Chen, G; Chen, H S; Chen, M L; Chen, S J; Chen, S M; Chen, T; Chen, X R; Chen, X T; Chen, Y B; Chen, Y Q; Chen, Z J; Cheng, W S; Choi, S K.
Affiliation
  • Ablikim M; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Achasov MN; Budker Institute of Nuclear Physics SB RAS (BINP), Novosibirsk 630090, Russia.
  • Adlarson P; Uppsala University, Box 516, SE-75120 Uppsala, Sweden.
  • Ai XC; Zhengzhou University, Zhengzhou 450001, People's Republic of China.
  • Aliberti R; Johannes Gutenberg University of Mainz, Johann-Joachim-Becher-Weg 45, D-55099 Mainz, Germany.
  • Amoroso A; University of Turin and INFN, University of Turin, I-10125 Turin, Italy.
  • An MR; INFN, I-10125 Turin, Italy.
  • An Q; Liaoning Normal University, Dalian 116029, People's Republic of China.
  • Bai Y; State Key Laboratory of Particle Detection and Electronics, Beijing 100049, Hefei 230026, People's Republic of China.
  • Bakina O; University of Science and Technology of China, Hefei 230026, People's Republic of China.
  • Balossino I; Southeast University, Nanjing 211100, People's Republic of China.
  • Ban Y; Joint Institute for Nuclear Research, 141980 Dubna, Moscow region, Russia.
  • Batozskaya V; INFN Sezione di Ferrara, INFN Sezione di Ferrara, I-44122 Ferrara, Italy.
  • Begzsuren K; Peking University, Beijing 100871, People's Republic of China.
  • Berger N; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Berlowski M; National Centre for Nuclear Research, Warsaw 02-093, Poland.
  • Bertani M; Institute of Physics and Technology, Peace Avenue 54B, Ulaanbaatar 13330, Mongolia.
  • Bettoni D; Johannes Gutenberg University of Mainz, Johann-Joachim-Becher-Weg 45, D-55099 Mainz, Germany.
  • Bianchi F; National Centre for Nuclear Research, Warsaw 02-093, Poland.
  • Bianco E; INFN Laboratori Nazionali di Frascati, INFN Laboratori Nazionali di Frascati, I-00044 Frascati, Italy.
  • Bortone A; INFN Sezione di Ferrara, INFN Sezione di Ferrara, I-44122 Ferrara, Italy.
  • Boyko I; University of Turin and INFN, University of Turin, I-10125 Turin, Italy.
  • Briere RA; INFN, I-10125 Turin, Italy.
  • Brueggemann A; University of Turin and INFN, University of Turin, I-10125 Turin, Italy.
  • Cai H; INFN, I-10125 Turin, Italy.
  • Cai X; University of Turin and INFN, University of Turin, I-10125 Turin, Italy.
  • Calcaterra A; INFN, I-10125 Turin, Italy.
  • Cao GF; Joint Institute for Nuclear Research, 141980 Dubna, Moscow region, Russia.
  • Cao N; Carnegie Mellon University, Pittsburgh, Pennsylvania 15213, USA.
  • Cetin SA; University of Muenster, Wilhelm-Klemm-Strasse 9, 48149 Muenster, Germany.
  • Chang JF; Wuhan University, Wuhan 430072, People's Republic of China.
  • Chang TT; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Chang WL; State Key Laboratory of Particle Detection and Electronics, Beijing 100049, Hefei 230026, People's Republic of China.
  • Che GR; INFN Laboratori Nazionali di Frascati, INFN Laboratori Nazionali di Frascati, I-00044 Frascati, Italy.
  • Chelkov G; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Chen C; University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China.
  • Chen C; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Chen G; University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China.
  • Chen HS; Turkish Accelerator Center Particle Factory Group, Istinye University, 34010, Istanbul, Turkey.
  • Chen ML; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Chen SJ; State Key Laboratory of Particle Detection and Electronics, Beijing 100049, Hefei 230026, People's Republic of China.
  • Chen SM; Xinyang Normal University, Xinyang 464000, People's Republic of China.
  • Chen T; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Chen XR; University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China.
  • Chen XT; Nankai University, Tianjin 300071, People's Republic of China.
  • Chen YB; Joint Institute for Nuclear Research, 141980 Dubna, Moscow region, Russia.
  • Chen YQ; Nankai University, Tianjin 300071, People's Republic of China.
  • Chen ZJ; Soochow University, Suzhou 215006, People's Republic of China.
  • Cheng WS; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Choi SK; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
Phys Rev Lett ; 132(19): 191902, 2024 May 10.
Article in En | MEDLINE | ID: mdl-38804946
ABSTRACT
We report the measurement of the inclusive cross sections for e^{+}e^{-}→nOCH (where nOCH denotes non-open charm hadrons) with improved precision at center-of-mass (c.m.) energies from 3.645 to 3.871 GeV. We observe three resonances R(3760), R(3780), and R(3810) with significances of 8.1σ, 13.7σ, and 8.8σ, respectively. The R(3810) state is observed for the first time, while the R(3760) and R(3780) states are observed for the first time in the nOCH cross sections. Two sets of resonance parameters describe the energy-dependent line shape of the cross sections well. In set I [set II], the R(3810) state has mass (3805.7±1.1±2.7) [(3805.7±1.1±2.7)] MeV/c^{2}, total width (11.6±2.9±1.9) [(11.5±2.8±1.9)] MeV, and an electronic width multiplied by the nOCH decay branching fraction of (10.9±3.8±2.5) [(11.0±3.4±2.5)] eV. In addition, we measure the branching fractions B[R(3760)→nOCH]=(25.2±16.1±30.4)%[(6.4±4.8±7.7)%] and B[R(3780)→nOCH]=(12.3±6.6±8.3)%[(10.4±4.8±7.0)%] for the first time. The R(3760) state can be interpreted as an open-charm (OC) molecular state, but containing a simple four-quark state component. The R(3810) state can be interpreted as a hadrocharmonium state.

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev Lett Year: 2024 Document type: Article

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev Lett Year: 2024 Document type: Article
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