4.8 Article

Observation of a Charged Charmoniumlike Structure in e+e- → π+π- J/ψ at √s=4.26 GeV

期刊

PHYSICAL REVIEW LETTERS
卷 110, 期 25, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.110.252001

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资金

  1. Ministry of Science and Technology of China [2009CB825200]
  2. National Natural Science Foundation of China (NSFC) [10625524, 10821063, 10825524, 10835001, 10935007, 11125525, 11235011]
  3. Joint Funds of the National Natural Science Foundation of China [11079008, 11179007]
  4. Chinese Academy of Sciences (CAS) Large-Scale Scientific Facility Program
  5. CAS [KJCX2-YW-N29, KJCX2-YW-N45]
  6. 100 Talents Program of CAS
  7. German Research Foundation DFG under Contract No. Collaborative Research Center [CRC-1044]
  8. Istituto Nazionale di Fisica Nucleare, Italy
  9. Ministry of Development of Turkey [DPT2006K-120470]
  10. U.S. Department of Energy [DE-FG02-04ER41291, DE-FG02-05ER41374, DE-FG02-94ER40823]
  11. U.S. National Science Foundation
  12. University of Groningen (RuG)
  13. Helmholtzzentrum fuer Schwerionenforschung GmbH (GSI), Darmstadt
  14. National Research Foundation of Korea [2011-0029457]
  15. WCU Grant [R32-10155]

向作者/读者索取更多资源

We study the process e(+)e(-) -> pi(+)pi(-) J/psi at a center-of-mass energy of 4.260 GeV using a 525 pb(-1) data sample collected with the BESIII detector operating at the Beijing Electron Positron Collider. The Born cross section is measured to be (62.9 +/- 1.9 +/- 3.7) pb, consistent with the production of the Y(4260). We observe a structure at around 3.9 GeV/c(2) in the pi(+/-) J/psi mass spectrum, which we refer to as the Z(c)(3900). If interpreted as a new particle, it is unusual in that it carries an electric charge and couples to charmonium. A fit to the pi(+/-) J/psi invariant mass spectrum, neglecting interference, results in a mass of (3899.0 +/- 3.6 +/- 4.9) MeV/c(2) and a width of (46 +/- 10 +/- 20) MeV. Its production ratio is measured to be R = (sigma(e(+)e(-) -> pi(+/-) Z(c)(3900)(-/+) -> pi(+)pi(-) J/psi)/sigma(e(+)e(-) -> pi(+)pi(-) J/psi)) = (21.5 +/- 3.3 +/- 7.5)%. In all measurements the first errors are statistical and the second are systematic.

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