Your browser doesn't support javascript.
loading
Observation of Resonance Structures in e
Ablikim, M; Achasov, M N; Adlarson, P; Albrecht, M; Aliberti, R; Amoroso, A; An, M R; An, Q; Bai, X H; Bai, Y; Bakina, O; Baldini Ferroli, R; Balossino, I; Ban, Y; Batozskaya, V; Becker, D; Begzsuren, K; Berger, N; Bertani, M; Bettoni, D; Bianchi, F; Bloms, J; 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, W L; Chelkov, G; Chen, C; Chen, G; Chen, H S; Chen, M L; Chen, S J; Chen, T; Chen, X R; Chen, X T; Chen, Y B; Chen, Z J; Cheng, W S; Cibinetto, G; Cossio, F; Cui, J J; Dai, H L.
Afiliación
  • Ablikim M; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Achasov MN; G. I. Budker Institute of Nuclear Physics SB RAS (BINP), Novosibirsk 630090, Russia.
  • Adlarson P; Uppsala University, Box 516, SE-75120 Uppsala, Sweden.
  • Albrecht M; Bochum Ruhr-University, D-44780 Bochum, Germany.
  • 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 XH; State Key Laboratory of Particle Detection and Electronics, Beijing 100049, Hefei 230026, People's Republic of China.
  • Bai Y; University of Science and Technology of China, Hefei 230026, People's Republic of China.
  • Bakina O; University of Jinan, Jinan 250022, People's Republic of China.
  • Baldini Ferroli R; Southeast University, Nanjing 211100, People's Republic of China.
  • Balossino I; Joint Institute for Nuclear Research, 141980 Dubna, Moscow region, Russia.
  • Ban Y; INFN Laboratori Nazionali di Frascati, INFN Laboratori Nazionali di Frascati, I-00044 Frascati, Italy.
  • Batozskaya V; INFN Sezione di Ferrara, INFN Sezione di Ferrara, I-44122 Ferrara, Italy.
  • Becker D; Peking University, Beijing 100871, People's Republic of China.
  • Begzsuren K; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Berger N; National Centre for Nuclear Research, Warsaw 02-093, Poland.
  • Bertani M; Johannes Gutenberg University of Mainz, Johann-Joachim-Becher-Weg 45, D-55099 Mainz, Germany.
  • Bettoni D; Institute of Physics and Technology, Peace Avenue 54B, Ulaanbaatar 13330, Mongolia.
  • Bianchi F; Johannes Gutenberg University of Mainz, Johann-Joachim-Becher-Weg 45, D-55099 Mainz, Germany.
  • Bloms J; 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 Muenster, Wilhelm-Klemm-Strasse 9, 48149 Muenster, Germany.
  • Cai H; University of Turin and INFN, University of Turin, I-10125 Turin, Italy.
  • Cai X; INFN, I-10125 Turin, Italy.
  • Calcaterra A; Joint Institute for Nuclear Research, 141980 Dubna, Moscow region, Russia.
  • Cao GF; Carnegie Mellon University, Pittsburgh, Pennsylvania 15213, USA.
  • Cao N; University of Muenster, Wilhelm-Klemm-Strasse 9, 48149 Muenster, Germany.
  • Cetin SA; Wuhan University, Wuhan 430072, People's Republic of China.
  • Chang JF; 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.
  • Chelkov G; INFN Laboratori Nazionali di Frascati, INFN Laboratori Nazionali di Frascati, I-00044 Frascati, Italy.
  • 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; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Chen ML; University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China.
  • Chen SJ; Turkish Accelerator Center Particle Factory Group, Istinye University, 34010 Istanbul, Turkey.
  • Chen T; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Chen XR; State Key Laboratory of Particle Detection and Electronics, Beijing 100049, Hefei 230026, People's Republic of China.
  • Chen XT; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Chen YB; University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China.
  • Chen ZJ; Joint Institute for Nuclear Research, 141980 Dubna, Moscow region, Russia.
  • Cheng WS; Nankai University, Tianjin 300071, People's Republic of China.
  • Cibinetto G; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Cossio F; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
  • Cui JJ; University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China.
  • Dai HL; Institute of High Energy Physics, Beijing 100049, People's Republic of China.
Phys Rev Lett ; 129(10): 102003, 2022 Sep 02.
Article en En | MEDLINE | ID: mdl-36112441
Using a data sample corresponding to an integrated luminosity of 11.3 fb^{-1} collected at center-of-mass energies from 4.23 to 4.70 GeV with the BESIII detector, we measure the product of the e^{+}e^{-}→π^{+}π^{-}ψ_{2}(3823) cross section and the branching fraction B[ψ_{2}(3823)→γχ_{c1}]. For the first time, resonance structure is observed in the cross section line shape of e^{+}e^{-}→π^{+}π^{-}ψ_{2}(3823) with significances exceeding 5σ. A fit to data with two coherent Breit-Wigner resonances modeling the sqrt[s]-dependent cross section yields M(R_{1})=4406.9±17.2±4.5 MeV/c^{2}, Γ(R_{1})=128.1±37.2±2.3 MeV, and M(R_{2})=4647.9±8.6±0.8 MeV/c^{2}, Γ(R_{2})=33.1±18.6±4.1 MeV. Though weakly disfavored by the data, a single resonance with M(R)=4417.5±26.2±3.5 MeV/c^{2}, Γ(R)=245±48±13 MeV is also possible to interpret data. This observation deepens our understanding of the nature of the vector charmoniumlike states. The mass of the ψ_{2}(3823) state is measured as (3823.12±0.43±0.13) MeV/c^{2}, which is the most precise measurement to date.

Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Idioma: En Revista: Phys Rev Lett Año: 2022 Tipo del documento: Article

Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Idioma: En Revista: Phys Rev Lett Año: 2022 Tipo del documento: Article
...