6533b859fe1ef96bd12b7361
RESEARCH PRODUCT
Search for new decay modes of the $\psi_2(3823)$ and the process $e^+e^-\rightarrow\pi^0\pi^0\psi_2(3823)$
M. AblikimM. N. AchasovP. AdlarsonS. AhmedM. AlbrechtR. AlibertiA. AmorosoM. R. AnQ. AnX. H. BaiY. BaiO. BakinaR. Baldini FerroliI. BalossinoY. BanK. BegzsurenN. BergerM. BertaniD. BettoniF. BianchiJ. BlomsA. BortoneI. BoykoR. A. BriereH. CaiX. CaiA. CalcaterraG. F. CaoN. CaoS. A. CetinJ. F. ChangW. L. ChangG. ChelkovD. Y. ChenG. ChenH. S. ChenM. L. ChenS. J. ChenX. R. ChenY. B. ChenZ. J ChenW. S. ChengG. CibinettoF. CossioX. F. CuiH. L. DaiX. C. DaiA. DbeyssiR. E. De BoerD. DedovichZ. Y. DengA. DenigI. DenysenkoM. DestefanisF. De MoriY. DingC. DongJ. DongL. Y. DongM. Y. DongX. DongS. X. DuY. L. FanJ. FangS. S. FangY. FangR. FarinelliL. FavaF. FeldbauerG. FeliciC. Q. FengJ. H. FengM. FritschC. D. FuY. GaoY. GaoY. GaoY. G. GaoI. GarziaP. T. GeC. GengE. M. GersabeckA GilmanK. GoetzenL. GongW. X. GongW. GradlM. GrecoL. M. GuM. H. GuS. GuY. T. GuC. Y GuanA. Q. GuoL. B. GuoR. P. GuoY. P. GuoA. GuskovT. T. HanW. Y. HanX. Q. HaoF. A. HarrisN HüskenK. L. HeF. H. HeinsiusC. H. HeinzT. HeldY. K. HengC. HeroldM. HimmelreichT. HoltmannY. R. HouZ. L. HouH. M. HuJ. F. HuT. HuY. HuG. S. HuangL. Q. HuangX. T. HuangY. P. HuangZ. HuangT. HussainW. Ikegami AnderssonW. ImoehlM. IrshadS. JaegerS. JanchivQ. JiQ. P. JiX. B. JiX. L. JiY. Y. JiH. B. JiangX. S. JiangJ. B. JiaoZ. JiaoS. JinY. JinT. JohanssonN. Kalantar-nayestanakiX. S. KangR. KappertM. KavatsyukB. C. KeI. K. KeshkA. KhoukazP. KieseR. KiuchiR. KliemtL. KochO. B. KolcuB. KopfM. KuemmelM. KuessnerA. KupscM. G. KurthW. KühnJ. J. LaneJ. S. LangeP. LarinA. LavaniaL. LavezziZ. H. LeiH. LeithoffM. LellmannT. LenzC. LiC. H. LiCheng LiD. M. LiF. LiG. LiH. LiH. LiH. B. LiH. J. LiH. J. LiJ. L. LiJ. Q. LiJ. S. LiKe LiL. K. LiLei LiP. R. LiS. Y. LiW. D. LiW. G. LiX. H. LiX. L. LiXiaoyu LiZ. Y. LiH. LiangH. LiangH. LiangY. F. LiangY. T. LiangG. R. LiaoL. Z. LiaoJ. LibbyC. X. LinB. J. LiuC. X. LiuD. LiuF. H. LiuFang LiuFeng LiuH. B. LiuH. M. LiuHuanhuan LiuHuihui LiuJ. B. LiuJ. L. LiuJ. Y. LiuK. LiuK. Y. LiuKe LiuL. LiuM. H. LiuP. L. LiuQ. LiuQ. LiuS. B. LiuShuai LiuT. LiuW. M. LiuX. LiuY. LiuY. B. LiuZ. A. LiuZ. Q. LiuX. C. LouF. X. LuF. X. LuH. J. LuJ. D. LuJ. G. LuX. L. LuY. LuY. P. LuC. L. LuoM. X. LuoP. W. LuoT. LuoX. L. LuoS. LussoX. R. LyuF. C. MaH. L. MaL. L. MaM. M. MaQ. M. MaR. Q. MaR. T. MaX. X. MaX. Y. MaF. E. MaasM. MaggioraS. MaldanerS. MaldeQ. A. MalikA. MangoniY. J. MaoZ. P. MaoS. MarcelloZ. X. MengJ. G. MesschendorpG. MezzadriT. J. MinR. E. MitchellX. H. MoY. J. MoN. Yu. MuchnoiH. MuramatsuS. NakhoulY. NefedovF. NerlingI. B. NikolaevZ. NingS. NisarS. L. OlsenQ. OuyangS. PacettiX. PanY. PanA. PathakP. PatteriM. PelizaeusH. P. PengK. PetersJ. PetterssonJ. L. PingR. G. PingR. PolingV. PrasadH. QiH. R. QiK. H. QiM. QiT. Y. QiT. Y. QiS. QianW. B. QianZ. QianC. F. QiaoL. Q. QinX. P. QinX. S. QinZ. H. QinJ. F. QiuS. Q. QuK. H. RashidK. RavindranC. F. RedmerA. RivettiV. RodinM. RoloG. RongCh. RosnerM. RumpH. S. SangA. SarantsevY. SchelhaasC. SchnierK. SchoenningM. ScodeggioD. C. ShanW. ShanX. Y. ShanJ. F. ShangguanM. ShaoC. P. ShenP. X. ShenX. Y. ShenH. C. ShiR. S. ShiX. ShiX. D ShiJ. J. SongW. M. SongY. X. SongS. SosioS. SpataroK. X. SuP. P. SuF. F. SuiG. X. SunH. K. SunJ. F. SunL. SunS. S. SunT. SunW. Y. SunW. Y. SunX SunY. J. SunY. K. SunY. Z. SunZ. T. SunY. H. TanY. X. TanC. J. TangG. Y. TangJ. TangJ. X. TengV. ThorenY. T. TianI. UmanB. WangC. W. WangD. Y. WangH. J. WangH. P. WangK. WangL. L. WangM. WangM. Z. WangMeng WangW. WangW. H. WangW. P. WangX. WangX. F. WangX. L. WangY. WangY. WangY. D. WangY. F. WangY. Q. WangY. Y. WangZ. WangZ. Y. WangZiyi WangZongyuan WangD. H. WeiP. WeidenkaffF. WeidnerS. P. WenD. J. WhiteU. WiednerG. WilkinsonM. WolkeL. WollenbergJ. F. WuL. H. WuL. J. WuX. WuZ. WuL. XiaH. XiaoS. Y. XiaoZ. J. XiaoX. H. XieY. G. XieY. H. XieT. Y. XingG. F. XuQ. J. XuW. XuX. P. XuY. C. XuF. YanL. YanW. B. YanW. C. YanXu YanH. J. YangH. X. YangL. YangS. L. YangY. X. YangYifan YangZhi YangM. YeM. H. YeJ. H. YinZ. Y. YouB. X. YuC. X. YuG. YuJ. S. YuT. YuC. Z. YuanL. YuanX. Q. YuanY. YuanZ. Y. YuanC. X. YueA. YuncuA. A. ZafarY. ZengB. X. ZhangGuangyi ZhangH. ZhangH. H. ZhangH. H. ZhangH. Y. ZhangJ. J. ZhangJ. L. ZhangJ. Q. ZhangJ. W. ZhangJ. Y. ZhangJ. Z. ZhangJianyu ZhangJiawei ZhangL. M. ZhangL. Q. ZhangLei ZhangS. ZhangS. F. ZhangShulei ZhangX. D. ZhangX. Y. ZhangY. ZhangY. H. ZhangY. T. ZhangYan ZhangYao ZhangYi ZhangZ. H. ZhangZ. Y. ZhangG. ZhaoJ. ZhaoJ. Y. ZhaoJ. Z. ZhaoLei ZhaoLing ZhaoM. G. ZhaoQ. ZhaoS. J. ZhaoY. B. ZhaoY. X. ZhaoZ. G. ZhaoA. ZhemchugovB. ZhengJ. P. ZhengY. ZhengY. H. ZhengB. ZhongC. ZhongL. P. ZhouQ. ZhouX. ZhouX. K. ZhouX. R. ZhouX. Y. ZhouA. N. ZhuJ. ZhuK. ZhuK. J. ZhuS. H. ZhuT. J. ZhuW. J. ZhuW. J. ZhuY. C. ZhuZ. A. ZhuB. S. ZouJ. H. Zousubject
High Energy Physics::ExperimentHigh Energy Physics - Experimentdescription
The decays $\psi_2(3823)\rightarrow\gamma\chi_{c0,1,2}, \pi^+\pi^-J/\psi, \pi^0\pi^0J/\psi, \eta J/\psi$, and $\pi^0J/\psi$ are searched for using the reaction $e^+e^-\rightarrow\pi^+\pi^-\psi_2(3823)$ in a 19 fb$^{-1}$ data sample collected at center-of-mass energies between 4.1 and 4.7 GeV with the BESIII detector. The process $\psi_2(3823)\rightarrow\gamma\chi_{c1}$ is observed in a 9 fb$^{-1}$ data sample in the center-of-mass energy range 4.3 to 4.7 GeV, which confirms a previous observation but with a higher significance of $11.8\sigma$, and evidence for $\psi_2(3823)\rightarrow\gamma\chi_{c2}$ is found with a significance of $3.2\sigma$ for the first time. The branching-fraction ratio $\frac{\mathcal{B}(\psi_2(3823)\rightarrow\gamma\chi_{c2})}{\mathcal{B}(\psi_2(3823)\rightarrow\gamma\chi_{c1})}$ is determined. No significant $\psi_2(3823)$ signals are observed for any of the other decay channels. Upper limits of branching-fraction ratios for $\psi_2(3823)\rightarrow\pi^+\pi^-J/\psi, \pi^0\pi^0J/\psi, \eta J/\psi, \pi^0J/\psi, \gamma\chi_{c0}$ relative to $\psi_2(3823)\rightarrow\gamma\chi_{c1}$ are reported. The process $e^+e^-\rightarrow\pi^0\pi^0\psi_2(3823)$ is also searched for, and we find evidence for the process with a significance of $4.3\sigma$. The average cross-section ratio $\frac{\sigma(e^+e^-\rightarrow\pi^0\pi^0\psi_2(3823))}{\sigma(e^+e^-\rightarrow\pi^+\pi^-\psi_2(3823))}$ is also determined.
year | journal | country | edition | language |
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2021-02-22 |