ar X iv : h ep - e x / 04 11 00 1 v 1 2 9 O ct 2 00 4 Resonances in J / ψ → φπ + π − and φK + K −

نویسندگان

  • J. G. Bian
  • D. V. Bugg
  • X. Cai
  • J. F. Chang
  • H. F. Chen
  • H. S. Chen
  • H. X. Chen
  • J. C. Chen
  • Jin Chen
  • Jun Chen
  • M. L. Chen
  • Y. B. Chen
  • S. P. Chi
  • Y. P. Chu
  • X. Z. Cui
  • H. L. Dai
  • Y. S. Dai
  • Z. Y. Deng
  • L. Y. Dong
  • Q. F. Dong
  • S. X. Du
  • Z. Z. Du
  • Y. N. Gao
  • M. Y. Gong
  • W. X. Gong
  • S. D. Gu
  • Y. N. Guo
  • Y. Q. Guo
  • Z. J. Guo
  • F. A. Harris
  • Y. K. Heng
  • H. M. Hu
  • T. Hu
  • G. S. Huang
  • X. P. Huang
  • X. T. Huang
  • X. B. Ji
  • C. H. Jiang
  • X. S. Jiang
  • D. P. Jin
  • S. M. Li
  • W. D. Li
  • W. G. Li
  • X. L. Li
  • X. Q. Li
  • Y. L. Li
  • Y. F. Liang
  • H. B. Liao
  • C. X. Liu
  • F. Liu
  • Fang Liu
  • H. H. Liu
  • H. M. Liu
  • J. Liu
  • J. B. Liu
  • J. P. Liu
  • R. G. Liu
  • Z. A. Liu
  • Z. X. Liu
  • F. Lu
  • G. R. Lu
  • H. J. Lu
  • J. G. Lu
  • C. L. Luo
  • L. X. Luo
  • X. L. Luo
  • F. C. Ma
  • H. L. Ma
  • J. M. Ma
  • L. L. Ma
  • Q. M. Ma
  • X. B. Ma
  • X. Y. Ma
  • Z. P. Mao
  • X. H. Mo
  • J. Nie
  • Z. D. Nie
  • S. L. Olsen
  • H. P. Peng
  • P. L. Wang
  • S. Z. Wang
  • W. F. Wang
  • Y. F. Wang
  • Z. Wang
  • Z. Y. Wang
  • Zhe Wang
  • Zheng Wang
  • C. L. Wei
  • D. H. Wei
  • N. Wu
  • Y. M. Wu
  • X. M. Xia
  • X. X. Xie
  • S. L. Zang
  • Y. Zeng
  • Yu Zeng
  • B. X. Zhang
  • B. Y. Zhang
  • C. C. Zhang
  • D. H. Zhang
  • H. Y. Zhang
چکیده

A partial wave analysis is presented of J/ψ → φππ and φKK from a sample of 58M J/ψ events in the BES II detector. The f0(980) is observed clearly in both sets of data, and parameters of the Flatté formula are determined accurately:M = 965± 8 (stat) ±6 (syst) MeV/c, g1 = 165± 10± 15 MeV/c, g2/g1 = 4.21± 0.25± 0.21. The φππ data also exhibit a strong ππ peak centred at M = 1335 MeV/c. It may be fitted with f2(1270) and a dominant 0 + signal made from f0(1370) interfering with a smaller f0(1500) component. There is evidence that the f0(1370) signal is resonant, from interference with f2(1270). There is also a state in ππ with M = 1790 −30 MeV/c 2 and Γ = 270 −30 MeV/c ; spin 0 is preferred over spin 2. This state, f0(1790), is distinct from f0(1710). The φKK̄ data contain a strong peak due to f ′ 2(1525). A shoulder on its upper side may be fitted by interference between f0(1500) and f0(1710). PACS: 13.25.Gv, 14.40.Gx, 13.40.Hq

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تاریخ انتشار 2004