Measurement of the branching fraction for ψ(3686)→ωK+K−ψ(3686)\toωK^+ K^-

preprint2014arXivOpen access
BESIII CollaborationM. AblikimM. N. AchasovX. C. AiO. AlbayrakM. AlbrechtD. J. AmbroseF. F. AnQ. AnJ. Z. BaiR. Baldini FerroliY. BanD. W. BennettJ. V. BennettM. BertaniJ. M. BianE. BogerO. BondarenkoI. BoykoS. BraunR. A. BriereH. CaiX. CaiO. CakirA. CalcaterraG. F. CaoS. A. CetinJ. F. ChangG. ChelkovG. ChenH. S. ChenJ. C. ChenM. L. ChenS. J. ChenX. ChenX. R. ChenY. B. ChenH. P. ChengX. K. ChuY. P. ChuD. Cronin-HennessyH. L. DaiJ. P. DaiD. DedovichZ. Y. DengA. DenigI. DenysenkoM. DestefanisW. M. DingY. DingC. DongJ. DongL. Y. DongM. Y. DongS. X. DuJ. Z. FanJ. FangS. S. FangY. FangL. FavaC. Q. FengC. D. FuO. FuksQ. GaoY. GaoC. GengK. GoetzenW. X. GongW. GradlM. GrecoM. H. GuY. T. GuY. H. GuanL. B. GuoT. GuoY. P. GuoZ. HaddadiS. HanY. L. HanF. A. HarrisK. L. HeM. HeZ. Y. HeT. HeldY. K. HengZ. L. HouC. HuH. M. HuJ. F. HuT. HuG. M. HuangG. S. HuangH. P. HuangJ. S. HuangL. HuangX. T. HuangY. HuangT. HussainC. S. JiQ. JiQ. P. JiX. B. JiX. L. JiL. L. JiangL. W. JiangX. S. JiangJ. B. JiaoZ. JiaoD. P. JinS. JinT. JohanssonA. JulinN. Kalantar-NayestanakiX. L. KangX. S. KangM. KavatsyukB. KlossB. KopfM. KornicerW. KuehnA. KupscW. LaiJ. S. LangeM. LaraP. LarinM. LeyheC. H. LiCheng LiCui LiD. LiD. M. LiF. LiG. LiH. B. LiJ. C. LiJin LiK. LiP. R. LiQ. J. LiT. LiW. D. LiW. G. LiX. L. LiX. N. LiX. Q. LiZ. B. LiH. LiangY. F. LiangY. T. LiangD. X. LinB. J. LiuC. L. LiuC. X. LiuF. H. LiuFang LiuFeng LiuH. B. LiuH. H. LiuH. M. LiuJ. LiuJ. P. LiuK. LiuK. Y. LiuP. L. LiuQ. LiuS. B. LiuX. LiuY. B. LiuZ. A. LiuZhiqiang LiuZhiqing LiuH. LoehnerX. C. LouG. R. LuH. J. LuH. L. LuJ. G. LuY. LuY. P. LuC. L. LuoM. X. LuoT. LuoX. L. LuoM. LvX. R. LyuF. C. MaH. L. MaQ. M. MaS. MaT. MaX. Y. MaF. E. MaasM. MaggioraQ. A. MalikY. J. MaoZ. P. MaoJ. G. MesschendorpJ. MinT. J. MinR. E. MitchellX. H. MoY. J. MoH. MoeiniC. Morales MoralesK. MoriyaN. Yu. MuchnoiH. MuramatsuY. NefedovF. NerlingI. B. NikolaevZ. NingS. NisarX. Y. NiuS. L. OlsenQ. OuyangS. PacettiM. PelizaeusH. P. PengK. PetersJ. L. PingR. G. PingR. PolingM. QiS. QianC. F. QiaoL. Q. QinN. QinX. S. QinY. QinZ. H. QinJ. F. QiuK. H. RashidC. F. RedmerM. RipkaG. RongX. D. RuanA. SarantsevK. SchoenningS. SchumannW. ShanM. ShaoC. P. ShenX. Y. ShenH. Y. ShengM. R. ShepherdW. M. SongX. Y. SongS. SpataroB. SpruckG. X. SunJ. F. SunS. S. SunY. J. SunY. Z. SunZ. J. SunZ. T. SunC. J. TangX. TangI. TapanE. H. ThorndikeM. TiemensD. TothM. UllrichI. UmanG. S. VarnerB. WangD. WangD. Y. WangK. WangL. L. WangL. S. WangM. WangP. WangP. L. WangQ. J. WangS. G. WangW. WangX. F. WangY. D. WangY. F. WangY. Q. WangZ. WangZ. G. WangZ. H. WangZ. Y. WangD. H. WeiJ. B. WeiP. WeidenkaffS. P. WenM. WernerU. WiednerM. WolkeL. H. WuN. WuZ. WuL. G. XiaY. XiaD. XiaoZ. J. XiaoY. G. XieQ. L. XiuG. F. XuL. XuQ. J. XuQ. N. XuX. P. XuZ. XueL. YanW. B. YanW. C. YanY. H. YanH. X. YangL. YangY. YangY. X. YangH. YeM. YeM. H. YeB. X. YuC. X. YuH. W. YuJ. S. YuS. P. YuC. Z. YuanW. L. YuanY. YuanA. YuncuA. A. ZafarA. ZalloS. L. ZangY. ZengB. X. ZhangB. Y. ZhangC. ZhangC. B. ZhangC. C. ZhangD. H. ZhangH. H. ZhangH. Y. ZhangJ. J. ZhangJ. Q. ZhangJ. W. ZhangJ. Y. ZhangJ. Z. ZhangS. H. ZhangX. J. ZhangX. Y. ZhangY. ZhangY. H. ZhangZ. H. ZhangZ. P. ZhangZ. Y. ZhangG. ZhaoJ. W. ZhaoLei ZhaoLing ZhaoM. G. ZhaoQ. ZhaoQ. W. ZhaoS. J. ZhaoT. C. ZhaoX. H. ZhaoY. B. ZhaoZ. G. ZhaoA. ZhemchugovB. ZhengJ. P. ZhengY. H. ZhengB. ZhongL. ZhouLi ZhouX. ZhouX. K. ZhouX. R. ZhouX. Y. ZhouK. ZhuK. J. ZhuX. L. ZhuY. C. ZhuY. S. ZhuZ. A. ZhuJ. ZhuangB. S. ZouJ. H. Zou

Abstract

With 1.06×1081.06\times 10^8 ψ(3686)ψ(3686) events collected with the BESIII detector, the branching fraction of ψ(3686)→ωK+K−ψ(3686) \to ωK^+ K^- is measured to be (1.54±0.04±0.11)×10−4(1.54 \pm 0.04 \pm 0.11) \times 10^{-4}. This is the most precise result to date, due to the largest ψ(3686)ψ(3686) sample, improved signal reconstruction efficiency, good simulation of the detector performance, and a more accurate knowledge of the continuum contribution. Using the branching fraction of J/ψ→ωK+K−J/ψ\to ωK^+ K^-, the ratio B(ψ(3868)→K+K−)/B(J/ψ→K+K−)\mathcal{B}(ψ(3868) \to K^+K^-) / \mathcal{B}(J/ψ\to K^+K^-) is determined to be (18.4±3.7) %(18.4 \pm 3.7)\,\%. This constitutes a significantly improved test of the 12 %12\,\% rule, with the uncertainty now dominated by the J/ψJ/ψ branching fraction.

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