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Study of hc→3 (π+π-)π0, hc→2 (π+π-)ω, hc→2 (π+π-)π0η, hc→2 (π+π-)η, and hc→p p ̄

  • BESIII Collaboration
  • CAS - Institute of High Energy Physics
  • Budker Institute of Nuclear Physics of the Siberian Branch of the RAS
  • Novosibirsk State University
  • Uppsala University
  • Ruhr University Bochum
  • Chinese Academy of Sciences
  • Zhengzhou University
  • Johannes Gutenberg University Mainz
  • University of Turin
  • National Institute for Nuclear Physics
  • University of Science and Technology of China
  • Helmholtz Institute Mainz
  • Southeast University, Nanjing
  • Joint Institute for Nuclear Research
  • Peking University
  • University of Chinese Academy of Sciences
  • National Centre for Nuclear Research
  • Mongolian Academy of Sciences
  • Carnegie Mellon University
  • University of Münster
  • Wuhan University
  • Istinye University
  • Nankai University
  • Moscow Institute of Physics and Technology
  • China University of Geosciences, Wuhan
  • Soochow University
  • Henan University
  • Nanjing University
  • North China Electric Power University
  • Tsinghua University
  • CAS - Institute of Modern Physics
  • Jilin University
  • Hunan University
  • Chung-Ang University
  • Shandong University
  • Yunnan University
  • University of South China
  • University of Jinan
  • Liaoning University
  • Sun Yat-Sen University
  • University of Eastern Piedmont
  • Nanjing Normal University
  • University of Ferrara
  • University of Manchester
  • University of Oxford
  • GSI Helmholtz Centre for Heavy Ion Research
  • Guangxi University
  • Henan University of Technology
  • Shandong Normal University
  • Fudan University
  • Indiana University Bloomington
  • Henan Normal University
  • University of Hawai'i at Mānoa
  • Suranaree University of Technology
  • South China Normal University
  • University of the Punjab
  • Liaoning Normal University
  • Hangzhou Normal University
  • Huangshan College
  • University of Groningen
  • Indian Institute of Technology Madras
  • Justus Liebig University Giessen
  • Qufu Normal University
  • Renmin University of China
  • Lanzhou University
  • Hebei University
  • Sichuan University
  • Guangxi Normal University
  • Shanxi University
  • Central China Normal University
  • Henan University of Science and Technology
  • Central South University
  • Zhejiang University
  • Goethe University Frankfurt
  • COMSATS University Islamabad
  • University of Perugia
  • Universidad de Tarapacá
  • Petersburg Nuclear Physics Institute (PNPI)
  • Hunan Normal University
  • China Center of Advanced Science and Technology World Laboratory
  • The Department of Mathematical Sciences
  • Shanghai Jiao Tong University
  • Ministry of Education of the People's Republic of China
  • Near East University
  • Swiss Federal Institute of Technology Lausanne
  • Inner Mongolia University
  • Yantai University
  • Beihang University
  • Shanxi Normal University
  • University of Science and Technology Liaoning

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2 Citas (Scopus)

Resumen

Based on (2712.4±14.1)×106 ψ(3686) events collected with the BESIII detector, we study the decays hc→3(π+π-)π0, hc→2(π+π-)ω, hc→2(π+π-)π0η, hc→2(π+π-)η, and hc→pp¯ via ψ(3686)→π0hc. The decay channel hc→3(π+π-)π0 is observed for the first time, and its branching fraction is determined to be (9.28±1.14±0.77)×10-3, where the first uncertainty is statistical and the second is systematic. In addition, first evidence is found for the modes hc→2(π+π-)π0η and hc→2(π+π-)ω with significances of 4.8σ and 4.7σ, and their branching fractions are determined to be (7.55±1.51±0.77)×10-3 and (4.00±0.86±0.35)×10-3, respectively. No significant signals of hc→2(π+π-)η and hc→pp¯ are observed, and the upper limits of the branching fractions of these decays are determined to be <6.19×10-4 and <4.40×10-5 at the 90% confidence level, respectively.

Idioma originalInglés
Número de artículo072018
PublicaciónPhysical Review D
Volumen109
N.º7
DOI
EstadoPublicada - 1 abr 2024

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Profundice en los temas de investigación de 'Study of hc→3 (π+π-)π0, hc→2 (π+π-)ω, hc→2 (π+π-)π0η, hc→2 (π+π-)η, and hc→p p ̄'. En conjunto forman una huella única.

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