학술논문

Observation of e + e − → π 0 π 0 ψ 2(3823)
Document Type
article
Author
The BESIII collaborationM. AblikimM. N. AchasovP. AdlarsonM. AlbrechtR. AlibertiA. AmorosoM. R. AnQ. AnX. H. BaiY. BaiO. BakinaR. Baldini FerroliI. BalossinoY. BanV. BatozskayaD. BeckerK. BegzsurenN. BergerM. BertaniD. BettoniF. BianchiJ. BlomsA. BortoneI. BoykoR. A. BriereA. BrueggemannH. CaiX. CaiA. CalcaterraG. F. CaoN. CaoS. A. CetinJ. F. ChangW. L. ChangG. R. CheG. ChelkovC. ChenChao ChenG. ChenH. S. ChenM. L. ChenS. J. ChenS. M. ChenT. ChenX. R. ChenX. T. ChenY. B. ChenZ. J. ChenW. S. ChengS. K. ChoiX. ChuG. CibinettoF. CossioJ. J. CuiH. L. DaiJ. P. DaiA. DbeyssiR. E. de BoerD. DedovichZ. Y. DengA. DenigI. DenysenkoM. DestefanisF. De MoriY. DingJ. DongL. Y. DongM. Y. DongX. DongS. X. DuP. EgorovY. L. FanJ. FangS. S. FangW. X. FangY. FangR. FarinelliL. FavaF. FeldbauerG. FeliciC. Q. FengJ. H. FengK FischerM. FritschC. FritzschC. D. FuH. GaoY. N. GaoYang GaoS. GarbolinoI. GarziaP. T. GeZ. W. GeC. GengE. M. GersabeckA GilmanK. GoetzenL. GongW. X. GongW. GradlM. GrecoL. M. GuM. H. GuY. T. GuC. Y GuanA. Q. GuoL. B. GuoR. P. GuoY. P. GuoA. GuskovT. T. HanW. Y. HanX. Q. HaoF. A. HarrisK. K. HeK. L. HeF. H. HeinsiusC. H. HeinzY. K. HengC. HeroldG. Y. HouY. R. HouZ. L. HouH. M. HuJ. F. HuT. HuY. HuG. S. HuangK. X. HuangL. Q. HuangX. T. HuangY. P. HuangZ. HuangT. HussainN HüskenW. ImoehlM. IrshadJ. JacksonS. JaegerS. JanchivE. JangJ. H. JeongQ. JiQ. P. JiX. B. JiX. L. JiY. Y. JiZ. K. JiaH. B. JiangS. S. JiangX. S. JiangY. JiangJ. B. JiaoZ. JiaoS. JinY. JinM. Q. JingT. JohanssonN. Kalantar-NayestanakiX. S. KangR. KappertM. KavatsyukB. C. KeI. K. KeshkA. KhoukazR. KiuchiR. KliemtL. KochO. B. KolcuB. KopfM. KuemmelM. KuessnerA. KupscW. KühnJ. J. LaneJ. S. LangeP. LarinA. LavaniaL. LavezziZ. H. LeiH. LeithoffM. LellmannT. LenzC. LiC. H. LiCheng LiD. M. LiF. LiG. LiH. LiH. B. LiH. J. LiH. N. LiJ. Q. LiJ. S. LiJ. W. LiKe LiL. J LiL. K. LiLei LiM. H. LiP. R. LiS. X. LiS. Y. LiT. LiW. D. LiW. G. LiX. H. LiX. L. LiXiaoyu LiY. G. LiZ. X. LiZ. Y. LiH. LiangY. F. LiangY. T. LiangG. R. LiaoL. Z. LiaoJ. LibbyA. LimphiratC. X. LinD. X. LinT. LinB. J. LiuC. X. LiuD. LiuF. H. LiuFang LiuFeng LiuG. M. LiuH. LiuH. B. LiuH. M. LiuHuanhuan LiuHuihui LiuJ. B. LiuJ. L. LiuJ. Y. LiuK. LiuK. Y. LiuKe LiuL. LiuLu LiuM. H. LiuP. L. LiuQ. LiuS. B. LiuT. LiuW. K. LiuW. M. LiuX. LiuY. LiuY. B. LiuZ. A. LiuZ. Q. LiuX. C. LouF. X. LuH. J. LuJ. G. LuX. L. LuY. LuY. P. LuZ. H. LuC. L. LuoM. X. LuoT. LuoX. L. LuoX. R. LyuY. F. LyuF. C. MaH. L. MaL. L. MaM. M. MaQ. M. MaR. Q. MaR. T. MaX. Y. MaY. MaF. E. MaasM. MaggioraS. MaldanerS. MaldeQ. A. MalikA. MangoniY. J. MaoZ. P. MaoS. MarcelloZ. X. MengJ. MesschendorpG. MezzadriH. MiaoT. J. MinR. E. MitchellX. H. MoN. Yu. MuchnoiY. NefedovF. NerlingI. B. NikolaevZ. NingS. NisarY. NiuS. L. OlsenQ. OuyangS. PacettiX. PanY. PanA. PathakM. PelizaeusH. P. PengK. PetersJ. L. PingR. G. PingS. PluraS. PogodinV. PrasadF. Z. QiH. QiH. R. QiM. QiT. Y. QiS. QianW. B. QianZ. QianC. F. QiaoJ. J. QinL. Q. QinX. P. QinX. S. QinZ. H. QinJ. F. QiuS. Q. QuK. H. RashidC. F. RedmerK. J. RenA. RivettiV. RodinM. RoloG. RongCh. RosnerS. N. RuanH. S. SangA. SarantsevY. SchelhaasC. SchnierK. SchoenningM. ScodeggioK. Y. ShanW. ShanX. Y. ShanJ. F. ShangguanL. G. ShaoM. ShaoC. P. ShenH. F. ShenX. Y. ShenB. A. ShiH. C. ShiJ. Y. Shiq. q. ShiR. S. ShiX. ShiX. D ShiJ. J. SongW. M. SongY. X. SongS. SosioS. SpataroF. StielerK. X. SuP. P. SuY. J. SuG. X. SunH. SunH. K. SunJ. F. SunL. SunS. S. SunT. SunW. Y. SunX SunY. J. SunY. Z. SunZ. T. SunY. H. TanY. X. TanC. J. TangG. Y. TangJ. TangL. Y TaoQ. T. TaoM. TatJ. X. TengV. ThorenW. H. TianY. TianI. UmanB. WangB. L. WangC. W. WangD. Y. WangF. WangH. J. WangH. P. WangK. WangL. L. WangM. WangM. Z. WangMeng WangS. WangT. WangT. J. WangW. WangW. H. WangW. P. WangX. WangX. F. WangX. L. WangY. WangY. D. WangY. F. WangY. H. WangY. Q. WangYaqian WangZ. WangZ. Y. WangZiyi WangD. H. WeiF. WeidnerS. P. WenD. J. WhiteU. WiednerG. WilkinsonM. WolkeL. WollenbergJ. F. WuL. H. WuL. J. WuX. WuX. H. WuY. WuY. J WuZ. WuL. XiaT. XiangD. XiaoG. Y. XiaoH. XiaoS. Y. XiaoY. L. XiaoZ. J. XiaoC. XieX. H. XieY. XieY. G. XieY. H. XieZ. P. XieT. Y. XingC. F. XuC. J. XuG. F. XuH. Y. XuQ. J. XuX. P. XuY. C. XuZ. P. XuF. YanL. YanW. B. YanW. C. YanH. J. YangH. L. YangH. X. YangL. YangS. L. YangTao YangY. F. YangY. X. YangYifan YangM. YeM. H. YeJ. H. YinZ. Y. YouB. X. YuC. X. YuG. YuT. YuX. D. YuC. Z. YuanL. YuanS. C. YuanX. Q. YuanY. YuanZ. Y. YuanC. X. YueA. A. ZafarF. R. ZengX. ZengY. ZengY. H. ZhanA. Q. ZhangB. L. ZhangB. X. ZhangD. H. ZhangG. Y. ZhangH. ZhangH. H. ZhangH. Y. ZhangJ. L. ZhangJ. Q. ZhangJ. W. ZhangJ. X. ZhangJ. Y. ZhangJ. Z. ZhangJianyu ZhangJiawei ZhangL. M. ZhangL. Q. ZhangLei ZhangP. ZhangQ. Y. ZhangShuihan ZhangShulei ZhangX. D. ZhangX. M. ZhangX. Y. ZhangY. ZhangY. T. ZhangY. H. ZhangYan ZhangYao ZhangZ. H. ZhangZ. Y. ZhangG. ZhaoJ. ZhaoJ. Y. ZhaoJ. Z. ZhaoLei ZhaoLing ZhaoM. G. ZhaoS. J. ZhaoY. B. ZhaoY. X. ZhaoZ. G. ZhaoA. ZhemchugovB. ZhengJ. P. ZhengY. H. ZhengB. ZhongC. ZhongX. ZhongH. ZhouL. P. ZhouX. ZhouX. K. ZhouX. R. ZhouX. Y. ZhouY. Z. ZhouJ. ZhuK. ZhuK. J. ZhuL. X. ZhuS. H. ZhuS. Q. ZhuT. J. ZhuW. J. ZhuY. C. ZhuZ. A. ZhuJ. H. Zou
Source
Journal of High Energy Physics, Vol 2023, Iss 2, Pp 1-17 (2023)
Subject
Exotics
Spectroscopy
e +-e − Experiments
Particle and Resonance Production
Nuclear and particle physics. Atomic energy. Radioactivity
QC770-798
Language
English
ISSN
1029-8479
Abstract
Abstract Using a data sample corresponding to an integrated luminosity of 11.3 fb −1 collected at center-of-mass energies from 4.23 to 4.70 GeV with the BESIII detector, we observe the process e + e − → π 0 π 0 ψ 2(3823) for the first time with a statistical significance of 6.0 standard deviations. The ratio of average cross sections for e + e − → π 0 π 0 ψ 2(3823) and π + π − ψ 2(3823) is determined to be R = σ e + e − → π 0 π 0 ψ 2 3823 σ e + e − → π + π − ψ 2 3823 = 0.57 ± 0.14 ± 0.05 $$ \mathcal{R}=\frac{\sigma \left[{e}^{+}{e}^{-}\to {\pi}^0{\pi}^0{\psi}_2(3823)\right]}{\sigma \left[{e}^{+}{e}^{-}\to {\pi}^{+}{\pi}^{-}{\psi}_2(3823)\right]}=0.57\pm 0.14\pm 0.05 $$ , which is consistent with expectations from isospin symmetry. Here and below, the first uncertainties are statistical and the second are systematic. The mass of the ψ 2(3823) is measured to be M[ψ 2(3823)] = 3824.5 ± 2.4 ± 1.0 MeV/c 2. Due to the limited data sample, an upper limit of 18.8 MeV at 90% confidence level is set on the intrinsic width of ψ 2(3823).