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Search for the η_c(2S)/h_cto pbar{p} decays and measurements of the chi_(cJ)to pbar{p} branching fractions

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arxiv 1310.6099 v2 pith:CRJBMJBV submitted 2013-10-23 hep-ex

Search for the η_c(2S)/h_cto pbar{p} decays and measurements of the chi_(cJ)to pbar{p} branching fractions

BESlll Collaboration: M.Ablikim , M.N.Achasov , X.C.Ai , O.Albayrak , D.J.Ambrose , F.F.An , Q.An , J.Z.Bai
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R.Baldini Ferroli Y.Ban J.V.Bennett M.Bertani J.M.Bian E.Boger O.Bondarenko I.Boyko S.Braun R.A.Briere H.Cai X.Cai O. Cakir A.Calcaterra G.F.Cao S.A.Cetin J.F.Chang G.Chelkov G.Chen H.S.Chen J.C.Chen M.L.Chen S.J.Chen X.Chen X.R.Chen Y.B.Chen H.P.Cheng X.K.Chu Y.P.Chu D.Cronin-Hennessy H.L.Dai J.P.Dai D.Dedovich Z.Y.Deng A.Denig I.Denysenko M.Destefanis W.M.Ding Y.Ding C.Dong J.Dong L.Y.Dong M.Y.Dong S.X.Du J.Z.Fan J.Fang S.S.Fang Y.Fang L.Fava C.Q.Feng C.D.Fu J.L.Fu O.Fuks Q.Gao Y.Gao C.Geng K.Goetzen W.X.Gong W.Gradl M.Greco M.H.Gu Y.T.Gu Y.H.Guan A.Q.Guo L.B.Guo T.Guo Y.P.Guo Y.L.Han F.A.Harris K.L.He M.He Z.Y.He T.Held Y.K.Heng Z.L.Hou C.Hu H.M.Hu J.F.Hu T.Hu G.M.Huang G.S.Huang J.S.Huang L.Huang X.T.Huang Y.Huang T.Hussain C.S.Ji Q.Ji Q.P.Ji X.B.Ji X.L.Ji L.L.Jiang X.S.Jiang J.B.Jiao Z.Jiao D.P.Jin S.Jin T.Johansson N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.Kloss B.Kopf M.Kornicer W.Kuehn A.Kupsc W.Lai J.S.Lange M.Lara P. Larin M.Leyhe C.H.Li Cheng Li Cui Li D.Li D.M.Li F.Li G.Li H.B.Li J.C.LI K.Li Lei Li P.R.Li Q.J.Li T. Li W.D.Li W.G.Li X.L.Li X.N.Li X.Q.Li X.R.Li Z.B.Li H.Liang Y.F.Liang Y.T.Liang D.X.Lin B.J.Liu C.L.Liu C.X.Liu F.H.Liu Fang Liu Feng Liu H.B.Liu H.H.Liu H.M.Liu J.Liu J.P.Liu K.Liu K.Y.Liu P.L.Liu Q.Liu S.B.Liu X.Liu Y.B.Liu Z.A.Liu Zhiqiang Liu Zhiqing Liu H.Loehner X.C.Lou G.R.Lu H.J.Lu H.L.Lu J.G.Lu X.R.Lu Y.LU Y.P.Lu C.L.Luo M.X.Luo T.Luo X.L.Luo M.Lv F.C.Ma H.L.Ma Q.M.Ma S.Ma T.Ma X.Y.Ma F.E.Maas M.Maggiora Q.A.Malik Y.J.Mao Z.P.Mao J.G.Messchendorp J.Min T.J.Min R.E.Mitchell X.H.Mo Y.J.Mo H.Moeini C.Morales Morales K.Moriya N.Yu.Muchnoi Y.Nefedov I.B.Nikolaev Z.Ning S.Nisar X.Y.Niu S.L.Olsen Q.Ouyang S.Pacetti M.Pelizaeus H.P.Peng K.Peters J.L.Ping R.G.Ping R.Poling E.Prencipe M.Qi S.Qian C.F.Qiao L.Q.Qin X.S.Qin Y.Qin Z.H.Qin J.F.Qiu K.H.Rashid C.F.Redmer M.Ripka G.Rong X.D.Ruan A.Sarantsev K.Schoenning S.Schumann W.Shan M.Shao C.P.Shen X.Y.Shen H.Y.Sheng M.R.Shepherd W.M.Song X.Y.Song S.Spataro B.Spruck G.X.Sun J.F.Sun S.S.Sun Y.J.Sun Y.Z.Sun Z.J.Sun Z.T.Sun C.J.Tang X.Tang I.Tapan E.H.Thorndike D.Toth M.Ullrich I.Uman G.S.Varner B.Wang D.Wang D.Y.Wang K.Wang L.L.Wang L.S.Wang M.Wang P.Wang P.L.Wang Q.J.Wang S.G.Wang W.Wang X.F. Wang Y.D.Wang Y.F.Wang Y.Q.Wang Z.Wang Z.G.Wang Z.H.Wang Z.Y.Wang D.H.Wei J.B.Wei P.Weidenkaff S.P.Wen M.Werner U.Wiedner M.Wolke L.H.Wu N.Wu W.Wu Z.Wu L.G.Xia Y.Xia D.Xiao Z.J.Xiao Y.G.Xie Q.L.Xiu G.F.Xu L.Xu Q.J.Xu Q.N.Xu X.P.Xu Z.Xue L.Yan W.B.Yan W.C.Yan Y.H.Yan H.X.Yang Y.Yang Y.X.Yang H.Ye M.Ye M.H.Ye B.X.Yu C.X.Yu H.W.Yu J.S.Yu S.P.Yu C.Z.Yuan W.L.Yuan Y.Yuan A.A.Zafar A.Zallo S.L.Zang Y.Zeng B.X.Zhang B.Y.Zhang C.Zhang C.B.Zhang C.C.Zhang D.H.Zhang H.H.Zhang H.Y.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.W.Zhang J.Y.Zhang J.Z.Zhang S.H.Zhang X.J.Zhang X.Y.Zhang Y.Zhang Y.H.Zhang Z.H.Zhang Z.P.Zhang Z.Y.Zhang G.Zhao J.W.Zhao Lei Zhao Ling Zhao M.G.Zhao Q.Zhao Q.W.Zhao S.J.Zhao T.C.Zhao X.H.Zhao Y.B.Zhao Z.G.Zhao A.Zhemchugov B.Zheng J.P.Zheng Y.H.Zheng B.Zhong L.Zhou Li Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou K.Zhu K.J.Zhu X.L.Zhu Y.C.Zhu Y.S.Zhu Z.A.Zhu J.Zhuang B.S.Zou J.H.Zou
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Using a sample of $1.06\times10^{8}~\psi(3686)$ events collected with the BESIII detector at BEPCII, the decays $\eta_{c}(2S)\to p\bar{p}$ and $h_{c}\to p\bar{p}$ are searched for, where $\eta_c(2S)$ and $h_c$ are reconstructed in the decay chains $\psi(3686)\to\gamma\eta_{c}(2S)$, $\eta_{c}(2S)\to p\bar{p}$ and $\psi(3686)\to\pi^{0}h_{c}$, $h_{c}\to p\bar{p}$, respectively. No significant signals are observed. The upper limits of the product branching fractions are determined to be $\mathcal{B}(\psi(3686)\to\gamma\eta_c(2S))\times\mathcal{B}(\eta_{c}(2S)\to p\bar{p})<1.4\times10^{-6}$ and $\mathcal{B}(\psi(3686)\to\pi^0h_c)\times\mathcal{B}(h_{c}\to p\bar{p})<1.3\times10^{-7}$ at the 90% C.L.. The branching fractions for $\chi_{cJ}\to p\bar{p}$ $(J=0,~1,~2)$ are also measured to be $(24.5\pm0.8\pm1.3,~8.6\pm0.5\pm0.5,~8.4\pm0.5\pm0.5)\times10^{-5}$, which are the world's most precise measurements.

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