6533b862fe1ef96bd12c7583

RESEARCH PRODUCT

Observation of a Resonant Structure in e+e−→K+K−π0π0

Q. A. MalikG. MezzadriM. H. YeX. WangF. De MoriC. SowaM. BertaniL. M. GuZ. X. MengYao WangY. B. ZhaoL. P. ZhouP. R. LiY. M. MaZ. P. MaoM. RichterZ. NingS. Y. XiaoX. A. XiongL. YangMeng WangJinfei WuJ. FangCh. RosnerZhiqing LiuL. Y. DongHuanhuan LiuA. A. ZafarZ. G. WangG. FeliciH. Y. ZhangW. G. LiY. K. SunJ. LibbyJ. DongX. N. MaG. Y. TangKe WangW. Y. SunHaiwen LiuT. JohanssonJ. F. ChangY. F. WangO. B. KolcuX. CaiL. LavezziX. Q. HaoYan ZhangH. B. JiangXu YanR. T. MaJiawei ZhangQ. P. JiS. SpataroX. P. XuShiqun LiShan JinS. F. ZhangF. LiK. H. RashidYaquan FangA. PitkaK. GoetzenS. NisarX. TangG. F. ChenC. J. TangY. T. LiangW. ImoehlH. B. LiY. HuS. J. ChenF. C. MaW. GradlY. H. ZhengM. Y. DongJohn Jake LaneGuoqiang YuD. Y. LiuJ. B. JiaoGuangshun HuangL. YanM. KuessnerY. X. SongY. P. LuZ. A. LiuQ. M. MaV. PrasadJ. Y. ZhangLei LiD. Y. WangM. AlbrechtK. SchoenningB. S. ZouJ. L. LiA. YuncuM. RoloY. DingB. J. LiuX. H. LiL. WollenbergXiao-rui LyuS. ZhangJie ZhaoD. X. LinB. WangM. KavatsyukS. HanXingchao DaiAlexey ZhemchugovH. M. HuA. G. DenigC. L. LuoQ. ZhouH. C. ShiY. YuanY. S. ZhuG. F. CaoW. D. LiB. T. TsedneeKrisztian PetersS. L. YangB. L. WangT. HoltmannNiklaus BergerJ. MinT. LiuJ. F. QiuL. H. WuC. C. ZhangX. Y. JiangM. M. MaTao SunJ. L. ZhangB. ZhongL. B. GuoH. W. WenM. SavrieY. FuG. A. ChelkovL. FavaZhi YangB. KopfT. C. ZhaoY. F. WangJ. ZhaoX D ShiF. CossioF. F. SuiM. H. GuR. KiuchiH. Y. ShengT. HussainJ. Y. LiuT. Y. XingZongyuan WangD. Y. ChenW. KühnYi JinL. XiaRuiting MaH. B. LiuK. J. ZhuM. FritschY. G. GaoB. X. ZhangK. L. HeH. MuramatsuZiyi WangA. N. ZhuUlrich WiednerI. UmanY. J. MaoX. Y. MaH. X. YangT. T. HanQ. LiuL. L. MaL. GongW. YuanL. KochJ. W. ZhaoW. X. GongR. KappertS. J. ZhaoTao ZhangZ. Y. YouHongrong QiJ. H. ZouF. WeidnerC. H. LiM. Z. WangY. J. XiaoY. ZhangZ. A. ZhuW. C. YanG. X. SunJ. V. BennettH. XiaoJimin ZhaoA. KhoukazY. H. XieZiyuan LiC. X. YuY. C. ZhuA. AmorosoS. NakhoulA. Q. GuoQ. OuyangJianhao ZhangP. L. LiZ. JiaoFu-hu LiuS. S. SunD. H. ZhangR. X. YangS. JanchivX. L. GaoR. Baldini FerroliB. ZhengR. G. PingT. Z. HanM. MaggioraLing ZhaoA. PathakS. S. FangC. Y. GuanS. JaegerKe LiuT. WeberF. FeldbauerC. LiS. QianQ. AnJialun PingH. J. LuJ. G. LuAndrzej KupscP. LarinM. QiH. J. YangHuihui LiuLei ZhaoZ. L. HouT. HeldM. KuemmelMatthew Glenn KurthXu ShanA. DbeyssiX. S. QinC. ZhongY. B. LiuS. MaldeG. F. XuC. X. YueQ. J. XuFeng LiuF. E. MaasW. ShanC. DongS. SosioM. HimmelreichY. BanP. WeidenkaffM. Z. WangF. H. HeinsiusAnitaJ. G. MesschendorpY. P. GuoS. GuT. HuX. Y. ZhangX. L. WangC. P. ShenL. J. WuJ. BlomsR. S. ShiS. P. WenXuanhong LouJ. P. DaiM. AblikimX. R. ZhouX. F. CuiJianyu ZhangX. WuX. L. LuViktor ThorénJ. B. LiuO. BakinaA. CalcaterraZ. G. ZhaoX. N. LiL. Z. LiaoP. L. WangCheng LiR. E. MitchellC. Z. YuanN. CaoNasser Kalantar-nayestanakiY. J. SunYifan YangZujian WangAngelo RivettiHaiping PengJoachim PetterssonP. KieseY. J. MoMuhammad IrshadL. Q. QinYuan HouC. Morales MoralesHao LiangX. L. LuoX. L. JiY. P. LuY. BaiP. X. ShenTao LuoYue PanR. A. BriereI. BalossinoC. F. RedmerD. C. ShanT. Y. QiJ. D. LuC. W. WangG. RongJ. TangH. H. ZhangY. K. HengX. Y. SongY. H. ZhengCong-feng QiaoZ. WuEvelina GersabeckC. SchnierY. Q. WangL. D. LiuS. AhmedK. BegzsurenY. X. YangZ. J. SunN. Yu. MuchnoiX. S. JiangY. SchelhaasYunlong ZhangF. BianchiB. X. YuZhiqing ZhangD. BettoniW. J. ZhuF. A. HarrisJ. F. HuY. H. ZhangX. D. ShiM. LellmannLingxuan ZhangY. X. TanW. B. YanS. MaldanerW. L. ChangHuimin WangXiang-gan LiuM. L. ChenZhiyong ZhangL Y LiuX. S. KangX. T. HuangR. PolingS. H. ZhuT. YuH. LeithoffM. N. AchasovJ. F. SunX. P. QinQ. P. JiZ. Y. WangX. LiuQ. Q. SongJianping ZhengW. P. WangZ. H. QinQ. ZhaoX. K. ZhouM. G. ZhaoY. H. YangX. X. MaS. PacettiH. S. ChenH. QiC. X. LiuD. Y. LiuS. MarcelloY. Z. SunX. Y. ShenY. G. XieLi ZhouY. ZengT. J. MinJ. ZhuX. F. WangWei XuK. Y. LiuI. GarziaH. L. DaiIgor BoykoJ. C. LiZhe SunS. LussoP. AdlarsonXiang ZhouI. K. KeshkN. HueskenSerkant Ali CetinS. X. DuC. X. LinY. G. GaoKe LiM. DestefanisJ. ZhuangM. RumpGang ZhaoY. B. ChenXiaofeng ZhuJ. Z. ZhangJ. J. SongL. SunFang LiuM. X. LuoDylan Jaide WhiteR. FarinelliH. J. LiI. DenysenkoStephen Lars OlsenJ. Q. ZhangH. L. MaT. LenzD. M. LiMichael PapenbrockD. V. DedovichShuai LiuB. Y. ZhangJ. J. XuGuangyi ZhangM. PelizaeusY. F. LongB. C. KeZ. J. XiaoK. RavindranM. GrecoMagnus WolkeY. F. LiangD. P. JinX. PanYi ZhangK. Y. LiuXujin YuanR. P. GuoS. Q. QuS. B. LiuZ. B. LiW. Ikegami AnderssonY. NefedovF. NerlingX. H. MoL. S. WangM. H. YeL. L. WangH. CaiL. Q. HuangJacek BiernatI. B. NikolaevJ. H. YinLei ZhangM. ShaoY. T. GuA. SarantsevD. H. WeiJ. S. LangeBingxuan LiuG. WilkinsonW. S. ChengYao ZhangG. LiA. GilmanC. D. FuC. Q. FengX. R. ChenZ. Y. DengXingguo LiR. KliemtA. MangoniA. GuskovJie YuK. J. ZhuG. CibinettoP. W. LuoL. K. LiV. RodinX. B. JiP. Patteri

subject

PhysicsParticle physics0103 physical sciencesStructure (category theory)General Physics and Astronomy010306 general physics01 natural sciencesEnergy (signal processing)Luminosity

description

A partial-wave analysis is performed for the process e^{+}e^{-}→K^{+}K^{-}π^{0}π^{0} at the center-of-mass energies ranging from 2.000 to 2.644 GeV. The data samples of e^{+}e^{-} collisions, collected by the BESIII detector at the BEPCII collider with a total integrated luminosity of 300  pb^{-1}, are analyzed. The total Born cross sections for the process e^{+}e^{-}→K^{+}K^{-}π^{0}π^{0}, as well as the Born cross sections for the subprocesses e^{+}e^{-}→ϕπ^{0}π^{0}, K^{+}(1460)K^{-}, K_{1}^{+}(1400)K^{-}, K_{1}^{+}(1270)K^{-}, and K^{*+}(892)K^{*-}(892), are measured versus the center-of-mass energy. The corresponding results for e^{+}e^{-}→K^{+}K^{-}π^{0}π^{0} and ϕπ^{0}π^{0} are consistent with those of BABAR with better precision. By analyzing the cross sections for the four subprocesses, K^{+}(1460)K^{-}, K_{1}^{+}(1400)K^{-}, K_{1}^{+}(1270)K^{-}, and K^{*+}(892)K^{*-}(892), a structure with mass M=(2126.5±16.8±12.4)  MeV/c^{2} and width Γ=(106.9±32.1±28.1)  MeV is observed with an overall statistical significance of 6.3σ, although with very limited significance in the subprocesses e^{+}e^{-}→K_{1}^{+}(1270)K^{-} and K^{*+}(892)K^{*-}(892). The resonant parameters of the observed structure suggest it can be identified with the ϕ(2170), thus the results provide valuable input to the internal nature of the ϕ(2170).

https://doi.org/10.1103/physrevlett.124.112001