Observation of e+e−→ηJ/ψe^{+}e^{-} \to ηJ/ψ at center-of-mass energy sqrts=4.009sqrt{s}=4.009 GeV

preprint2012arXivOpen access
The BESIII CollaborationM. AblikimM. N. AchasovD. J. AmbroseF. F. AnQ. AnZ. H. AnJ. Z. BaiY. BanJ. BeckerM. BertaniJ. M. BianE. BogerO. BondarenkoI. BoykoR. A. BriereV. BytevX. CaiO. CakirA. CalcaterraG. F. CaoS. A. CetinJ. F. ChangG. ChelkovG. ChenH. S. ChenJ. C. ChenM. L. ChenS. J. ChenY. B. ChenH. P. ChengY. P. ChuD. Cronin-HennessyH. L. DaiJ. P. DaiD. DedovichZ. Y. DengA. DenigI. DenysenkoM. DestefanisW. M. DingY. DingL. Y. DongM. Y. DongS. X. DuJ. FangS. S. FangL. FavaF. FeldbauerC. Q. FengR. B. FerroliC. D. FuJ. L. FuY. GaoC. GengK. GoetzenW. X. GongW. GradlM. GrecoM. H. GuY. T. GuY. H. GuanA. Q. GuoL. B. GuoY. P. GuoY. L. HanF. A. HarrisK. L. HeM. HeZ. Y. HeT. HeldY. K. HengZ. L. HouH. M. HuJ. F. HuT. HuG. M. HuangJ. S. HuangX. T. HuangY. P. HuangT. HussainC. S. JiQ. JiX. B. JiX. L. JiL. L. JiangX. S. JiangJ. B. JiaoZ. JiaoD. P. JinS. JinF. F. JingN. Kalantar-NayestanakiM. KavatsyukW. KuehnW. LaiJ. S. LangeC. H. LiCheng LiCui LiD. M. LiF. LiG. LiH. B. LiJ. C. LiK. LiLei LiQ. J. LiS. L. LiW. D. LiW. G. LiX. L. LiX. N. LiX. Q. LiX. R. LiZ. B. LiH. LiangY. F. LiangY. T. LiangG. R. LiaoX. T. LiaoB. J. LiuC. L. LiuC. X. LiuC. Y. LiuF. H. LiuFang LiuFeng LiuH. LiuH. B. LiuH. H. LiuH. M. LiuH. W. LiuJ. P. LiuK. Y. LiuKai LiuP. L. LiuQ. LiuS. B. LiuX. LiuX. H. LiuY. B. LiuZ. A. LiuZhiqiang LiuZhiqing LiuH. LoehnerG. R. LuH. J. LuJ. G. LuQ. W. LuX. R. LuY. P. LuC. L. LuoM. X. LuoT. LuoX. L. LuoM. LvC. L. MaF. C. MaH. L. MaQ. M. MaS. MaT. MaX. Y. MaY. MaF. E. MaasM. MaggioraQ. A. MalikY. J. MaoZ. P. MaoJ. G. MesschendorpJ. MinT. J. MinR. E. MitchellX. H. MoC. Morales MoralesC. MotzkoN. Yu. MuchnoiH. MuramatsuY. NefedovC. NicholsonI. B. NikolaevZ. NingS. L. OlsenQ. OuyangS. PacettiJ. W. ParkM. PelizaeusH. P. PengK. PetersJ. L. PingR. G. PingR. PolingE. PrencipeM. QiS. QianC. F. QiaoX. S. QinY. QinZ. H. QinJ. F. QiuK. H. RashidG. RongX. D. RuanA. SarantsevB. D. SchaeferJ. SchulzeM. ShaoC. P. ShenX. Y. ShenH. Y. ShengM. R. ShepherdX. Y. SongS. SpataroB. SpruckD. H. SunG. X. SunJ. F. SunS. S. SunY. J. SunY. Z. SunZ. J. SunZ. T. SunC. J. TangX. TangI. TapanE. H. ThorndikeD. TothM. UllrichG. S. VarnerB. WangB. Q. WangK. WangL. L. WangL. S. WangM. WangP. WangP. L. WangQ. WangQ. J. WangS. G. WangX. L. WangY. D. WangY. F. WangY. Q. WangZ. WangZ. G. WangZ. Y. WangD. H. WeiP. WeidenkaffQ. G. WenS. P. WenM. WernerU. WiednerL. H. WuN. WuS. X. WuW. WuZ. WuL. G. XiaZ. J. XiaoY. G. XieQ. L. XiuG. F. XuG. M. XuH. XuQ. J. XuX. P. XuZ. R. XuF. XueZ. XueL. YanW. B. YanY. H. YanH. X. YangY. YangY. X. YangH. YeM. YeM. H. YeB. X. YuC. X. YuJ. S. YuS. P. YuC. Z. YuanY. YuanA. A. ZafarA. ZalloY. ZengB. X. ZhangB. Y. ZhangC. C. ZhangD. H. ZhangH. H. ZhangH. Y. ZhangJ. Q. ZhangJ. W. ZhangJ. Y. ZhangJ. Z. ZhangS. H. ZhangX. J. ZhangX. Y. ZhangY. ZhangY. H. ZhangY. S. ZhangZ. P. ZhangZ. Y. ZhangG. ZhaoH. S. ZhaoJ. W. ZhaoK. X. ZhaoLei ZhaoLing ZhaoM. G. ZhaoQ. ZhaoS. J. ZhaoT. C. ZhaoX. H. ZhaoY. B. ZhaoZ. G. ZhaoA. ZhemchugovB. ZhengJ. P. ZhengY. H. ZhengB. ZhongJ. ZhongL. ZhouX. K. ZhouX. R. ZhouC. ZhuK. ZhuK. J. ZhuS. H. ZhuX. L. ZhuX. W. ZhuY. C. ZhuY. M. ZhuY. S. ZhuZ. A. ZhuJ. ZhuangB. S. ZouJ. H. Zou

Abstract

Using a 478 pb−1^{-1} data sample collected with the BESIII detector operating at the BEPCII storage ring at a center-of-mass energy of s=4.009\sqrt{s}=4.009 GeV, the production of e+e−→ηJψe^{+}e^{-}\to ηJψ is observed for the first time with a statistical significance of greater than 10σ10σ. The Born cross section is measured to be (32.1±2.8±1.3)(32.1\pm 2.8 \pm 1.3) pb, where the first error is statistical and the second systematic. Assuming the ηJψηJψ signal is from a hadronic transition of the ψ(4040)ψ(4040), the fractional transition rate is determined to be B(ψ(4040)→ηJψ)=(5.2±0.5±0.2±0.5)×10−3{\cal B}(ψ(4040)\to ηJψ)=(5.2\pm 0.5\pm 0.2\pm 0.5)\times 10^{-3}, where the first, second, and third errors are statistical, systematic, and the uncertainty from the ψ(4040)ψ(4040) resonant parameters, respectively. The production of e+e−→π0Jψe^{+}e^{-} \to π^0 Jψ is searched for, but no significant signal is observed, and B(ψ(4040)→π0Jψ)<2.8×10−4{\cal B}(ψ(4040)\to π^0 Jψ) < 2.8 \times 10^{-4} is obtained at the 90% confidence level.

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