6533b820fe1ef96bd1279d0f

RESEARCH PRODUCT

Study of e+e−→γωJ/ψ and Observation of X(3872)→ωJ/ψ

J. LibbyYaquan FangA. GuskovA. GuskovX. D. ShiLu F. X.Lu F. X.W. B. YanJohn Jake LaneTao LuoXiao-rui LyuC. H. HeinzGuoqiang YuSu K. X.Li S. Y.K. SchoenningMa R. T.B. S. ZouGu L. M.Y. G. GaoW. H. WangS. PacettiNiklaus BergerY. BanP. WeidenkaffF. H. HeinsiusG. WilkinsonA. Q. GuoWen-zhao LiuG. LiJ. L. LiuS. P. WenY. H. TanD. Y. LiuH. S. ChenX. WuA. GilmanJ. B. JiaoC. Q. FengX. R. ChenX. R. ZhouF. E. MaasT. HuT. HuX. WangF. De MoriIgor BoykoJ. BlomsZ. Y. DengHai-tian WangLi C. H.N. HüskenS. NisarS. NisarA. CalcaterraZ. G. ZhaoWu L. J.Xu Q. J.M. AlbrechtHe K. L.O. BakinaHao LiangI. DenysenkoI. B. NikolaevI. B. NikolaevL. Z. LiaoXingguo LiGuangshun HuangS. Y. XiaoR. KliemtM. KuessnerL. YanLi J. Q.W. J. ZhuL. KochA. KhoukazY. Y. WangXu Y. C.M. FritschFu C. D.J. TangX D ShiK. BegzsurenR. Baldini FerroliJi X. B.Tao SunX. DongS. NakhoulS. NakhoulJ. Z. ZhaoQ. P. JiLi J. S.Mo X. H.C. LiS. MaldeGuangyi ZhangP. X. ShenXiao CaiXiangcheng PanY. J. MaoM. Q. JingHu H. M.M. Z. WangH. Y. ZhangJianhao ZhangJianhao ZhangY. K. HengY. K. HengH. K. SunYunlong ZhangM. H. LiuF. BianchiH. H. ZhangXu X. P.Ye M. H.K. PetersK. PetersK. J. ZhuJi Q. P.H. X. YangQ. AnJialun PingX. Y. ShenL. Y. DongJ. X. TengLu Y. P.D. BettoniLiangbin LiPeilian LiuX. Y. ZhangSu P. P.Xujin YuanX. L. WangY. H. ZhengY. X. ZhaoY. H. XieS. B. LiuZhiqing ZhangY. X. TanT. LiuJ. F. QiuCong-feng QiaoG. CibinettoMa R. Q.G. A. ChelkovG. A. ChelkovHaiping PengYu C. X.J. B. LiuR. PolingB. KopfW. Y. HanLi D. M.Zhiyong ZhangQ. A. MalikM. Y. DongM. Y. DongR. FarinelliA. MangoniDu S. X.Ma F. C.L. YangA. LavaniaH. B. LiuY. YuanM. LellmannY. J. SunM. MaggioraW. X. GongY. NefedovM. RoloLei ZhaoZ. L. HouZhi YangY. DingXu G. F.P. W. LuoX. S. KangY. C. ZhuJ. L. ZhangF. F. SuiQ. LiuGu Y. T.Stephen Lars OlsenJ. G. MesschendorpA. RivettiM. N. AchasovM. N. AchasovJ. H. ZouT. LenzMo Y. J.Gu M. H.Z. WuR. E. De BoerZ. P. MaoH. J. WangT. J. MinK. Y. LiuI. GarziaX. S. QinJian FangR. KiuchiB. J. LiuA. YuncuA. YuncuT. Y. XingD. Y. ChenZ. H. LeiLi YuanLi P. R.Li H. J.T. HeldZ. J. ChenM. G. ZhaoJ. ZhuLibo ZhangH. MuramatsuX. F. WangZ. Y. YuanJi Y. Y.Li ZhouS. S. SunW. M. SongMa H. L.F. WeidnerW. Y. SunJ. J. ZhangF. CossioC. Z. YuanN. CaoY. SchelhaasM. DestefanisV. RodinQ. OuyangQ. OuyangW. KühnS. MaldanerZ. Y. YouZ. A. ZhuW. C. YanA. G. DenigM. Z. WangLu J. D.Lu J. D.C. L. LuoQ. ZhouMa L. L.W. H. TianA. AmorosoS. S. FangC. Y. GuanB. ZhengR. G. PingM. PelizaeusS. QianT. HoltmannC. W. WangG. RongZ. Y. WangYi ChenLi H. B.A. DbeyssiKe B. C.J. F. ChangX. P. QinQi K. H.X. LiuHaiwen LiuLu J. G.G. Y. HouZengY. B. LiuC. P. ShenC. DongJiajun ZhengL. LavezziJ. Y. LiuLi L. K.R. E. MitchellG. F. ChenW. ImoehlS. SosioW. S. ChengB. ZhongL. B. GuoZ. H. QinMa X. X.F. LiL. L. WangH. CaiJ. Y. ZhangM. L. ChenG. FeliciQi T. Y.A. N. ZhuUlrich WiednerJoachim PetterssonSerkant Ali CetinH. F. ShenJ. F. ShangguanMuhammad IrshadY. D. WangN. Y. MuchnoiL. Q. HuangLi J. L.K. WangFeng YanQu S. Q.Jacek BiernatYanping HuangHu J. F.Y. L. FanJ. H. YinXu ShanLei ZhangLu H. J.Li W. D.Yu B. X.M. QiS. AhmedY. X. YangMa X. Y.F. FeldbauerM. ShaoC. X. YueM. X. LuoDylan Jaide WhiteW. L. ChangW. P. WangH. LeithoffAn M. R.H. J. YangH. J. YangT. T. HanL. WollenbergD. V. DedovichM. ScodeggioMa M. M.S. J. ZhaoM. AblikimXingchao DaiQi H. R.Q. ZhaoY. Z. SunY. P. GuoK. J. ZhuK. J. ZhuZ. QianG. MezzadriX. D. ZhangXiang ZhouI. K. KeshkH. B. LiuA. BortoneXuanhong LouXuanhong LouViktor ThorénH. Y. ZhangH. QiJ. J. ZhangC. X. LinNasser Kalantar-nayestanakiB. WangM. RumpGang ZhaoYue PanA. SarantsevA. SarantsevJ. ZhangM. KavatsyukI. BalossinoD. H. WeiJ. S. LangeH. C. ShiB. X. ZhangY. K. SunZ. HuangS. SpataroGe P. T.Wu L. H.Y. ZhangG. F. CaoS. B. LiuD. C. ShanM. BertaniZ. NingH. B. JiangW. GradlY. H. ZhengY. X. SongD. Y. WangS. L. YangX. SunG. R. LiaoJ. F. SunF. LiuS. MarcelloY. ZengZhe SunS. LussoX. H. XieJ. Z. ZhangH. S. SangJ. J. SongL. SunM. KuemmelMatthew Glenn KurthP. KieseW. ShanYuan HouR. A. BriereX. S. JiangX. S. JiangWei XuP. AdlarsonX. F. CuiY. F. WangY. F. WangJ. ZhaoT. HussainEvelina GersabeckA. PathakK. RavindranM. GrecoJie FengTong ZhuK. Y. LiuR. P. GuoW. Ikegami AnderssonShan JinK. GoetzenA. Q. ZhangS. ZhangR. KappertS. GuX. L. LuoL. D. LiuC. X. LiuG. Y. TangLi X. L.Jie ZhaoZ. X. MengYongke ZhaoX. H. BaiA. A. ZafarChristoph HeroldK. H. RashidHui LiY. T. LiangR. AlibertiS. J. ChenK. J. LiL. FavaV. PrasadF. NerlingF. NerlingJ. DongC. J. TangY. HuY. P. LuP. PatteriZ. A. LiuZ. A. LiuL. Q. QinYi JinL. XiaXu YanLi Z. Y.H. L. DaiS. F. ZhangF. A. HarrisS. JanchivM. HimmelreichM. HimmelreichZhiqing LiuT. JohanssonC. ZhongY. F. WangO. B. KolcuO. B. KolcuYu-xiao LiuZ. H. WangWu J. F.X. Q. HaoW. H. WangC. F. RedmerS. H. ZhuC. SchnierY. Q. WangT. YuLi X. H.A. ZhemchugovA. ZhemchugovX. T. HuangX. K. ZhouLu X. L.Yu J. S.Y. ZhangG. X. SunH. XiaoJi X. L.Z. JiaoFu-hu LiuYang YangC.-h. RosnerWenbin QianC. GengY. G. GaoI. UmanR. S. ShiY. BaiS. JaegerP. LarinMa Q. M.L. GongZ. J. XiaoYuguang XieAndrzej KupscM. YeMagnus WolkeY. F. LiangLi W. G.

subject

Particle physicsElectron–positron annihilationGeneral Physics and Astronomy01 natural sciencesSpectral linelaw.inventionLuminosityNuclear physicsCross section (physics)law0103 physical sciencesInvariant massCollider010306 general physicsPhysicsAnnihilationMass distribution010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyOrder (ring theory)ResonanceBaryonPhase spaceHigh Energy Physics::ExperimentCenter of massAtomic physicsEnergy (signal processing)Storage ringBar (unit)X(3872)

description

We study the e^{+}e^{-}→γωJ/ψ process using 11.6  fb^{-1} e^{+}e^{-} annihilation data taken at center-of-mass energies from sqrt[s]=4.008  GeV to 4.600 GeV with the BESIII detector at the BEPCII storage ring. The X(3872) resonance is observed for the first time in the ωJ/ψ system with a significance of more than 5σ. The relative decay ratio of X(3872)→ωJ/ψ and π^{+}π^{-}J/ψ is measured to be R=1.6_{-0.3}^{+0.4}±0.2, where the first uncertainty is statistical and the second systematic (the same hereafter). The sqrt[s]-dependent cross section of e^{+}e^{-}→γX(3872) is also measured and investigated, and it can be described by a single Breit-Wigner resonance, referred to as the Y(4200), with a mass of 4200.6_{-13.3}^{+7.9}±3.0  MeV/c^{2} and a width of 115_{-26}^{+38}±12  MeV. In addition, to describe the ωJ/ψ mass distribution above 3.9  GeV/c^{2}, we need at least one additional Breit-Wigner resonance, labeled as X(3915), in the fit. The mass and width of the X(3915) are determined. The resonant parameters of the X(3915) agree with those of the Y(3940) in B→KωJ/ψ and of the X(3915) in γγ→ωJ/ψ observed by the Belle and BABAR experiments within errors.

https://doi.org/10.1103/physrevlett.122.232002