Study of ψ(3686)→π0hc,hc→γηcψ(3686)\toπ^0 h_c, h_c\toγη_c via ηcη_c exclusive decays

preprint2015arXivOpen access
The BESIII CollaborationM. AblikimM. N. AchasovO. AlbayrakD. J. AmbroseF. F. AnQ. AnJ. Z. BaiY. BanJ. BeckerJ. V. BennettM. 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. ChenX. 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. HuT. HuG. M. HuangG. S. HuangJ. S. HuangX. T. HuangY. P. HuangT. HussainC. S. JiQ. JiQ. P. 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. H. LiuH. M. LiuH. W. LiuJ. P. LiuK. Y. LiuKai LiuP. L. LiuQ. LiuS. B. LiuX. 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. WangD. WangD. Y. 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. WeiJ. B. 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. YuH. W. YuJ. S. YuS. P. YuC. Z. YuanY. YuanA. A. ZafarA. ZalloY. ZengB. X. ZhangB. Y. ZhangC. 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. ZhaoQ. Z. ZhaoS. J. ZhaoT. C. ZhaoX. H. ZhaoY. B. ZhaoZ. G. ZhaoA. ZhemchugovB. ZhengJ. P. ZhengY. H. ZhengB. ZhongJ. ZhongZ. ZhongL. ZhouX. K. ZhouX. R. ZhouC. ZhuK. ZhuK. J. ZhuS. H. ZhuX. L. ZhuY. C. ZhuY. M. ZhuY. S. ZhuZ. A. ZhuJ. ZhuangB. S. ZouJ. H. Zou

Abstract

The process ψ(3686)→π0hc,hc→γηcψ(3686) \to π^0 h_c, h_c \to γη_c has been studied with a data sample of 106±4106 \pm 4 million ψ(3686)ψ(3686) events collected with the BESIII detector at the BEPCII storage ring. The mass and width of the PP-wave charmonium spin-singlet state hc(1P1)h_c(^1P_1) are determined by simultaneously fitting distributions of the π0π^0 recoil mass for 16 exclusive ηcη_c decay modes. The results, $M(\hc) = 3525.31 \pm 0.11 {\rm (stat.)} \pm 0.14 {\rm (syst.)}$\,MeV/c2c^2 and $Γ(\hc) = 0.70 \pm 0.28 \pm 0.22$\,MeV, are consistent with and more precise than previous measurements. We also determine the branching ratios for the 16 exclusive ηcη_c decay modes, five of which have not been measured previously. New measurements of the ηcη_c line-shape parameters in the E1E1 transition hc→γηch_c\toγη_c are made by selecting candidates in the hch_c signal sample and simultaneously fitting the hadronic mass spectra for the 16 ηcη_c decay channels. The resulting ηcη_c mass and width values are M(ηc)=2984.49±1.16±0.52M(η_c) = 2984.49 \pm 1.16 \pm 0.52\,MeV/c2c^2 and Γ(ηc)=36.4±3.2±1.7Γ(η_c) = 36.4 \pm 3.2 \pm 1.7\,MeV.

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