6533b839fe1ef96bd12a591b
RESEARCH PRODUCT
Measurement ofη′→π+π−e+e−andη′→π+π−μ+μ−
Miao HeS. MaD. TothL. P. ZhouZ. G. WangH. Y. ZhangY. H. GuanZ. P. MaoSanfeng WuJ. S. HuangC. X. LiuH. P. ChengJ. FangG. F. ChenM. QiP. FriedelY. NefedovJ. B. JiaoY. X. YangShan WangM. R. ShepherdQ. ZhaoY. Z. SunK. GoetzenGang ZhaoJ. Z. BaiY. N. GaoW. KuehnY. ZhangWei WuM. Y. DongYang QinS. L. ZangM. H. YeXiao-tong LuL. H. WuH. L. MaD. M. LiY. X. XiaH. MuramatsuY. H. ZhengM. PelizaeusY. K. HengX. K. ZhouJ. H. ZouO. FuksH. J. LuY. P. ChuJ. G. LuCong-feng QiaoO. AlbayrakN. Yu. MuchnoiHeng-yun YeH. LiangQ. P. JiX. P. XuX. B. JiYao WangQ. LiuG. S. VarnerHang LiuY. H. ZhangG. F. XuS. S. SunS. JinY. J. MaoH. X. YangJürgen BeckerF. E. MaasS. L. OlsenQ. G. WenZ. Y. WangTao LuoJ. V. BennettB. X. YuT. HuA. CalcaterraZ. G. ZhaoM. BertaniZhiqiang LiuL. HuangR. E. MitchellHao LiuM. G. ZhaoY. H. YangL. G. XiaI. UmanC. NicholsonD. X. LinXichao RuanX. L. LiAlexey ZhemchugovH. M. HuMichael WernerH. H. ZhangB. SpruckX. Y. SongF. H. LiuL. Y. DongZ. J. SunM. H. GuJie YuY. DingW. B. YanP. L. WangX. L. JiS. QianGuangming HuangH. LoehnerB. J. LiuX. H. LiuL. Q. QinFeng LiuQ. AnJialun PingM. N. AchasovLing ZhaoH. S. ChenJ. W. ZhangS. P. YuA. A. ZafarM. AblikimQi-wen LüH. Y. ShengZ. WuL. YanS. PacettiM. UllrichZ. J. XiaoT. J. MinK. J. ZhuH. B. LiM. KornicerM. GrecoShou-hua ZhuB. D. SchaeferZ. Y. ZhangJ. P. DaiH. L. DaiIgor BoykoC. X. YuX. K. ZhouX. K. ZhouW. GradlA. G. DenigC. L. LuoJ. P. LiuJ. M. BianC. L. MaG. R. LuD. Y. WangFang LiuX. Y. ZhangA. ZalloB. WangG. LiX. R. LiC. C. ZhangB. ZhongL. B. GuoS. J. ZhaoG. A. ChelkovU. WiednerI. DenysenkoW. LaiP. LarinY. G. XieLei LiZ. A. ZhuM. KavatsyukC. D. FuC. Q. FengKe WangJ. G. MesschendorpY. M. ZhuR. G. PingC. GengZ. Y. DengB. Y. ZhangS. X. DuCen ZhangB. X. ZhangJ. Q. ZhangJ. F. HuD. H. SunC. P. ShenY. J. SunK. H. RashidT. MaYanping HuangQ. J. XuW. M. DingR. PolingV. V. BytevH. H. LiuFenfen AnJ. ZhuangE. BogerE. BogerH. W. YuT. C. ZhaoRui ZhangJian WeiYucheng HuangZhenghao ZhangPeilian LiuX. F. WangQiunan XuX. L. WangD. V. DedovichM. MaggioraQ. M. MaF. A. HarrisJ. C. ChenX. T. LiaoY. T. LiangQ. P. JiY. YuanY. S. ZhuLili ZhangS. J. ChenNasser Kalantar-nayestanakiZ. P. ZhangZhenli XuS. H. ZhangX. Y. ShenLei ZhaoZ. Y. HeR. Baldini FerroliZ. L. HouO. BondarenkoF. LiZ. A. LiuF. C. MaXi ChenK. J. LiKrisztian PetersM. Z. WangC. Morales MoralesY. BanP. WeidenkaffX. TangX. N. LiEd ThorndikeS. P. WenHaiping PengX. S. QinW. G. LiX. R. ZhouM. L. ChenJ. L. FuCheng LiC. Z. YuanJ. F. QiuL. FavaY. Q. WangS. SpataroX. T. HuangG. RongC. ZhuB. S. ZouX. S. JiangJoong-won ParkX. H. MoL. S. WangY. F. LiangD. P. JinC. S. JiH. M. LiuM. H. YeG. F. CaoA. Q. GuoY. P. GuoT. GuoW. M. SongL. L. WangH. CaiSerkant Ali CetinM. LeyheI. B. NikolaevZ. H. QinChuan LiuG. S. HuangM. ShaoY. T. GuQ. L. XiuDan WangJ. F. SunQ. J. LiY. ZengZhe SunA. SarantsevD. H. WeiJ. S. LangeY. B. ChenXiaofeng ZhuJ. Z. ZhangP. L. WangN. WuX. L. LuoG. R. LiaoRoy A. BriereO. CakirX. Q. LiF. F. JingQ. OuyangS. S. FangK. Y. LiuY. B. LiuK. X. ZhaoZ. B. LiY. F. WangX. Y. MaH. MoeiniW. X. GongC. H. LiJ. Y. ZhangC. HuT. HussainZ. NingB. ZhengQ. J. WangK. J. ZhuXuantong ZhangK. MoriyaY. L. HanJ. MinH. B. LiuB. KopfK. L. HeHongsheng ZhaoD. J. AmbroseJianping ZhengL. L. JiangE. PrencipeW. D. LiM. LvG. M. XuFeng XueCui LiI. TapanS. L. LiY. H. YanK. Y. LiuZ. XueJ. W. ZhaoD. Cronin-hennessyY. C. ZhuM. DestefanisT. HeldZhiqing LiuJ. F. ChangX. CaiG. X. SunZ. JiaoD. H. ZhangY. B. ZhaoM. X. LuoC. J. TangY. P. LuKai LiuJ. C. LiZujian WangS. B. LiuX. H. ZhaoQ. A. Maliksubject
PhysicsNuclear and High Energy PhysicsCrystallographyBranching fractiondescription
Based on a sample of 225.3 million $J/\ensuremath{\psi}$ events accumulated with the BESIII detector at the BEPCII, the decays of ${\ensuremath{\eta}}^{\ensuremath{'}}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{l}^{+}{l}^{\ensuremath{-}}$ are studied via $J/\ensuremath{\psi}\ensuremath{\rightarrow}\ensuremath{\gamma}{\ensuremath{\eta}}^{\ensuremath{'}}$. A clear ${\ensuremath{\eta}}^{\ensuremath{'}}$ signal is observed in the ${\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{e}^{+}{e}^{\ensuremath{-}}$ mass spectrum, and the branching fraction is measured to be $\mathcal{B}({\ensuremath{\eta}}^{\ensuremath{'}}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{e}^{+}{e}^{\ensuremath{-}})=(2.11\ifmmode\pm\else\textpm\fi{}0.12(\mathrm{stat})\ifmmode\pm\else\textpm\fi{}0.14(\mathrm{syst}))\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}3}$, which is in good agreement with theoretical predictions and the previous measurement, but is determined with much higher precision. No ${\ensuremath{\eta}}^{\ensuremath{'}}$ signal is found in the ${\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}}$ mass spectrum, and the upper limit is determined to be $\mathcal{B}({\ensuremath{\eta}}^{\ensuremath{'}}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}})l2.9\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}5}$ at the 90% confidence level.
year | journal | country | edition | language |
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2013-05-28 | Physical Review D |