6533b82ffe1ef96bd1295c68
RESEARCH PRODUCT
Partial wave analysis ofJ/ψ→γηη
Y. J. MaoCheng LiC. HuK. J. ZhuZ. ZhongJ. MinYong-feng HuangH. B. LiuY. H. GuanJ. C. LiP. WangTao LuoHongsheng ZhaoQ. J. WangR. PolingQ ZhaoJ. V. BennettJianping ZhengD. J. AmbroseXiangdong RuanQ. LiuLei ZhaoM. LvC. ZhuM. DestefanisM. DestefanisJ. ZhuangB. KopfG. LiH. X. YangJ. F. SunP. FriedelM. X. LuoY. F. WangH. B. LiShou-hua ZhuW. B. YanKai ZhuL. H. WuFeng LiuD. V. DedovichC. D. FuA. ZalloE. PrencipeM. G. ZhaoLei HuangZ. Y. DengL. G. XiaY. ZengYang QinJ. B. JiaoJing ZhaoWei WuA. ZhemchugovT. HussainYuekun HengX. Y. MaW. X. GongT. J. MinL. L. WangH. CaiXingguo LiY.n. GaoS. P. WenJianguo ZhangF. Y. LiQ. L. XiuH. S. ChenShujun ZhaoY. X. XiaJ. M. BianW. LaiX.l. ZhuY. NefedovChangjin ZhangZheng WangH. L. DaiIgor BoykoHuihui LiuS. P. YuG. A. ChelkovG. A. ChelkovJ. P. LiuX. H. MoP. L. WangJie YuF. C. MaX. L. LuoY. B. ChenJ. Z. ZhangM. WernerFeng XueCui LiX. K. ZhouM. ShaoY. X. YangM. H. GuNiklaus BergerQ. A. MalikO. BondarenkoC. H. LiX. L. JiZhiqiang LiuMiao HeB. S. ZouY. T. GuKe WangChun LiuB. D. SchaeferZ. NingQ. J. LiQ. AnI. TapanS. L. LiJ. C. ChenM. BertaniM. R. ShepherdJ. G. MesschendorpZ. G. ZhaoY. H. YanC. X. YuX. Y. ShenJifeng HuNasser Kalantar-nayestanakiZ. T. SunYubin ZhaoM. MaggioraD. Cronin-hennessyY. Z. SunC. Morales MoralesYongmei HuangX. Q. LiXuejun WangB. ZhengR. G. PingM. N. AchasovZ. J. SunH. LoehnerShaodan MaA. SarantsevD. H. WeiJ. S. LangeS. X. WuQiunan XuX. T. HuangM. AblikimY. T. LiangZhanwen ZhuW. GradlX. LiuZ. B. LiGang ZhaoA. G. DenigC. L. LuoCunming LiuT. HeldMario GrecoB. X. YuM. H. YeY. D. WangQ. M. MaY. S. ZhuJ. Z. BaiW. D. LiY. P. ChuWei LiK. PetersKe HeV. V. BytevT. C. ZhaoRui ZhangY. J. SunK. Y. LiuZ. J. XiaoY. P. GuoA. A. ZafarS. B. LiuM. KavatsyukT. GuoM. QiH. Y. ZhangG. R. LiaoS. PacettiXu ZhangSerkant Ali CetinYun-zhi ZhangK. X. ZhaoHaiwen LiuG. X. SunG. F. ChenX. W. TangZhenghao ZhangC. C. ZhangA. Q. GuoG. RongB. ZhongL. B. GuoChen YuanLei LiH. P. PengL. Y. DongH. P. ChengJ. FangJ. B. WeiXiao-tong LuZ. WuJ. F. QiuN. WuK. H. RashidH. J. LuS. QianJialun PingF. F. JingJ. G. LuLili ZhangHailong MaUlrich WiednerB. X. ZhangM. KornicerD. M. LiA. CalcaterraC. S. JiI. B. NikolaevDing-xiong WangH. MuramatsuQ. P. JiX. Y. ZhangM. YeBingxin ZhangS. J. ChenE. BogerE. BogerT. MaX. T. LiaoQ. OuyangY. M. ZhuL. FavaF. E. MaasHao-ran YuX. B. JiM. PelizaeusShi-lun JinG. S. HuangS. L. OlsenRoy A. BriereJ. F. ChangK. LiY. P. LuT. HuB. Q. WangS. S. FangY. BanP. WeidenkaffJun DaiW. M. DingX. Z. CaiR. Baldini FerroliFang LiuS. SpataroY. B. LiuX. S. QinZ. L. HouLi ZhouJianhao ZhangQ. J. XuS. X. DuJ. L. FuI. DenysenkoX. S. JiangD. X. LinM. LeyheZ. H. QinH. M. HuZhihao XuY. G. XieGuangming HuangJun-yi ZhangZhiqing ZhangX. N. LiZhen WangY. C. ZhuX. P. XuQi-wen LüShan WangYe-fei YuanO. CakirM. Y. DongF. A. HarrisK. LiuH. B. LiuG. S. VarnerHang LiuS. S. SunJürgen BeckerG. F. CaoR. E. MitchellL. L. JiangZujian WangB. SpruckX. H. ZhaoE. H. ThorndikeX. K. ZhouL. Q. QinC. L. MaC. GengK. GoetzenW. KuehnLi YanZhiqing LiuY. H. ZhengZ. JiaoFu-hu LiuC. Q. FengCong-feng QiaoO. AlbayrakD. TothD. H. ZhangQ. P. JiMeng WangN. Yu. MuchnoiHeng-yun YeJ. S. HuangS. H. ZhangY. H. ZhangY. DingB. J. LiuG. R. LuZ. XueG. F. XuJ. H. ZouQ. G. WenD. H. SunY. Q. WangC. P. ShenX. R. ZhouYulei HanLi-feng WangQiang ZhaoC. J. TangX. Y. SongKai LiuX. R. LiZ. A. LiuM. L. ChenY. F. LiangD. P. JinJ.w. ParkXian ChenDayong WangP. L. LiuI. UmanC. NicholsonZ. P. MaoH. LiangM. UllrichH. H. ZhangX. L. WangF. F. AnLing ZhaoZhenyu ZhangZ. Y. HeYang YangH. Y. ShengG. M. Xusubject
PhysicsNuclear and High Energy PhysicsAmplitudeClassical mechanicsMesonBranching fractionElectron–positron annihilationPartial wave analysisAnalytical chemistryddc:530High Energy Physics::Experimentdescription
Based on a sample of 2.25 x 10(8) J/psi events collected with the BESIII detector at BEPCII, a full partial wave analysis on J/psi -> gamma eta eta was performed using the relativistic covariant tensor amplitude method. The results show that the dominant 0(++) and 2(++) components are from the f(0)(1710), f(0)(2100), f(0)(1500), f(2)'(1525), f(2)(1810) and f(2)(2340). The resonance parameters and branching fractions are also presented.
year | journal | country | edition | language |
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2013-05-21 | Physical Review D |