학술논문

Measurement of e + e − → ωπ + π − cross section at s $$ \sqrt{s} $$ = 2.000 to 3.080 GeV
Document Type
article
Author
The BESIII collaborationM. AblikimM. N. AchasovP. AdlarsonS. AhmedM. 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. ChelkovC. ChenG. ChenH. S. ChenM. L. ChenS. J. ChenT. ChenX. R. ChenX. T. ChenY. B. ChenZ. J. ChenW. S. ChengG. CibinettoF. CossioJ. J. CuiH. L. DaiJ. P. DaiX. C. 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. FangY. FangR. FarinelliL. FavaF. FeldbauerG. FeliciC. Q. FengJ. H. FengK FischerM. FritschC. D. FuY. N. GaoYang GaoI. GarziaP. T. GeC. GengE. M. GersabeckA GilmanK. GoetzenL. GongW. X. GongW. GradlM. GrecoM. H. 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. HeroldM. HimmelreichT. HoltmannG. 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. IrshadS. JaegerS. JanchivQ. JiQ. P. JiX. B. JiX. L. JiY. Y. JiH. B. JiangS. S. JiangX. S. JiangJ. B. JiaoZ. JiaoS. JinY. JinM. Q. JingT. 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. B. LiH. J. LiH. N. LiJ. L. LiJ. Q. LiJ. S. LiKe LiL. J LiL. K. LiLei LiM. H. LiP. R. LiS. X. LiS. Y. LiT. LiW. D. LiW. G. LiX. H. LiX. L. LiXiaoyu 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. M. LiuHuanhuan LiuHuihui LiuJ. B. LiuJ. L. LiuJ. Y. LiuK. LiuK. Y. LiuKe LiuL. LiuM. H. LiuP. L. LiuQ. LiuS. B. LiuT. LiuW. M. LiuX. LiuY. LiuY. B. LiuZ. A. LiuZ. Q. LiuX. C. LouF. X. LuH. J. LuJ. D. 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. X. MaX. Y. MaY. MaF. E. MaasM. MaggioraS. MaldanerS. MaldeQ. A. MalikA. MangoniY. J. MaoZ. P. MaoS. MarcelloZ. X. MengJ. G. MesschendorpG. MezzadriH. MiaoT. J. MinR. E. MitchellX. H. MoN. Yu. MuchnoiH. MuramatsuS. NakhoulY. NefedovF. NerlingI. B. NikolaevZ. NingS. NisarS. L. OlsenQ. OuyangS. PacettiX. PanY. PanA. PathakM. PelizaeusH. P. PengK. PetersJ. PetterssonJ. L. PingR. G. PingS. PluraS. PogodinR. PolingV. PrasadH. 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. RashidK. RavindranC. F. RedmerK. J. RenA. RivettiV. RodinM. RoloG. RongCh. RosnerM. RumpH. 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. ShiR. S. ShiX. ShiX. D ShiJ. J. SongW. M. SongY. X. SongS. SosioS. SpataroF. StielerK. X. SuP. P. SuY.-J. SuG. X. 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. TaoJ. X. TengV. ThorenW. H. TianY. T. TianI. UmanB. WangD. Y. WangF. WangH. J. WangH. P. WangK. WangL. L. WangM. WangM. Z. WangMeng WangS. WangT. J. WangW. WangW. H. WangW. P. WangX. WangX. F. WangX. L. WangY. D. WangY. F. WangY. Q. WangY. Y. WangYing WangZ. WangZ. Y. WangZiyi WangZongyuan WangD. H. WeiF. WeidnerS. P. WenD. J. WhiteU. WiednerG. WilkinsonM. WolkeL. WollenbergJ. F. WuL. H. WuL. J. WuX. WuX. H. WuY. WuZ. WuL. XiaT. XiangH. XiaoS. Y. XiaoY. L. XiaoZ. J. XiaoX. H. XieY. G. XieY. H. XieZ. P. XieT. Y. XingC. F. XuC. J. XuG. F. XuQ. J. XuS. Y. XuW. XuX. P. XuY. C. XuF. YanL. YanW. B. YanW. C. 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. YuanS. C. YuanX. Q. YuanY. YuanZ. Y. YuanC. X. YueA. A. ZafarX. ZengY. ZengY. H. ZhanA. Q. ZhangB. L. ZhangB. X. ZhangG. Y. ZhangH. ZhangH. H. ZhangH. Y. ZhangJ. L. ZhangJ. Q. ZhangJ. W. ZhangJ. Y. ZhangJ. Z. ZhangJianyu ZhangJiawei ZhangL. M. ZhangL. Q. ZhangLei ZhangP. 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. ZhaoQ. ZhaoS. J. ZhaoY. B. ZhaoY. X. ZhaoZ. G. ZhaoA. ZhemchugovB. ZhengJ. P. ZhengY. H. ZhengB. ZhongC. ZhongX. ZhongL. P. ZhouQ. ZhouX. ZhouX. K. ZhouX. R. ZhouX. Y. ZhouY. Z. ZhouA. N. ZhuJ. ZhuK. ZhuK. J. ZhuS. H. ZhuT. J. ZhuW. J. ZhuY. C. ZhuZ. A. ZhuB. S. ZouJ. H. Zou
Source
Journal of High Energy Physics, Vol 2023, Iss 1, Pp 1-34 (2023)
Subject
e +-e − Experiments
Particle and Resonance Production
Vector Boson Production
Nuclear and particle physics. Atomic energy. Radioactivity
QC770-798
Language
English
ISSN
1029-8479
Abstract
Abstract A partial wave analysis on the process e + e − → ωπ + π − is performed using 647 pb −1 of data sample collected by using the BESIII detector operating at the BEPCII storage ring at center-of-mass (c.m.) energies from 2.000 GeV to 3.080 GeV. The Born cross section of the e + e − → ωπ + π − process is measured, with precision improved by a factor of 3 compared to that of previous studies. A structure near 2.25 GeV is observed in the energy-dependent cross sections of e + e − → ωπ + π − and ωπ 0 π 0 with a statistical significance of 7.6σ, and its determined mass and width are 2232 ± 19 ± 27 MeV/c 2 and 93 ± 53 ± 20 MeV, respectively, where the first and second uncertainties are statistical and systematic, respectively. By analyzing the cross sections of subprocesses e + e − → ωf 0(500), ωf 0(980), ωf 0(1370), ωf 2(1270), and b 1(1235)π, a structure, with mass M = 2200 ± 11 ± 17 MeV/c 2 and width Γ = 74 ± 20 ± 24 MeV, is observed with a combined statistical significance of 7.9σ. The measured resonance parameters will help to reveal the nature of vector states around 2.25 GeV.