학술논문

Measurement of the e+e−→π+π− cross section between 600 and 900 MeV using initial state radiation
Document Type
article
Author
M. AblikimM.N. AchasovX.C. AiO. AlbayrakM. AlbrechtD.J. AmbroseA. AmorosoF.F. AnQ. AnJ.Z. BaiR. Baldini FerroliY. BanD.W. BennettJ.V. BennettM. BertaniD. BettoniJ.M. BianF. BianchiE. BogerI. BoykoR.A. BriereH. CaiX. CaiO. CakirA. CalcaterraG.F. CaoS.A. CetinJ.F. ChangG. ChelkovG. ChenH.S. ChenH.Y. ChenJ.C. ChenM.L. ChenS.J. ChenX. ChenX.R. ChenY.B. ChenH.P. ChengX.K. ChuG. CibinettoH.L. DaiJ.P. DaiA. DbeyssiD. DedovichZ.Y. DengA. DenigI. DenysenkoM. DestefanisF. De MoriY. DingC. DongJ. DongL.Y. DongM.Y. DongS.X. DuP.F. DuanE.E. ErenJ.Z. FanJ. FangS.S. FangX. FangY. FangL. FavaF. FeldbauerG. FeliciC.Q. FengE. FioravantiM. FritschC.D. FuQ. GaoX.Y. GaoY. GaoZ. GaoI. GarziaK. GoetzenW.X. GongW. GradlM. GrecoM.H. GuY.T. GuY.H. GuanA.Q. GuoL.B. GuoY. GuoY.P. GuoZ. HaddadiA. HafnerS. HanX.Q. HaoF.A. HarrisK.L. HeX.Q. HeT. HeldY.K. HengZ.L. HouC. HuH.M. HuJ.F. HuT. HuY. HuG.M. HuangG.S. HuangJ.S. HuangX.T. HuangY. HuangT. HussainQ. JiQ.P. JiX.B. JiX.L. JiL.W. JiangX.S. JiangX.Y. JiangJ.B. JiaoZ. JiaoD.P. JinS. JinT. JohanssonA. JulinN. Kalantar-NayestanakiX.L. KangX.S. KangM. KavatsyukB.C. KeP. KieseR. KliemtB. KlossO.B. KolcuB. KopfM. KornicerW. KühnA. KupscJ.S. LangeM. LaraP. LarinC. LengC. LiCheng LiD.M. LiF. LiF.Y. LiG. LiH.B. LiJ.C. LiJin LiK. LiLei LiP.R. LiT. LiW.D. LiW.G. LiX.L. LiX.M. LiX.N. LiX.Q. LiZ.B. LiH. LiangY.F. LiangY.T. LiangG.R. LiaoD.X. LinB.J. LiuC.X. LiuF.H. LiuFang LiuFeng LiuH.B. LiuH.H. LiuH.M. LiuJ. LiuJ.B. LiuJ.P. LiuJ.Y. LiuK. LiuK.Y. LiuL.D. LiuP.L. LiuQ. LiuS.B. LiuX. LiuY.B. LiuZ.A. LiuZhiqing LiuH. LoehnerX.C. LouH.J. LuJ.G. LuY. LuY.P. LuC.L. LuoM.X. LuoT. LuoX.L. LuoX.R. LyuF.C. MaH.L. MaL.L. MaQ.M. MaT. MaX.N. MaX.Y. MaF.E. MaasM. MaggioraY.J. MaoZ.P. MaoS. MarcelloJ.G. MesschendorpJ. MinR.E. MitchellX.H. MoY.J. MoC. Morales MoralesK. MoriyaN.Yu. MuchnoiH. MuramatsuY. NefedovF. NerlingI.B. NikolaevZ. NingS. NisarS.L. NiuX.Y. NiuS.L. OlsenQ. OuyangS. PacettiP. PatteriM. PelizaeusH.P. PengK. PetersJ. PetterssonJ.L. PingR.G. PingR. PolingV. PrasadM. QiS. QianC.F. QiaoL.Q. QinN. QinX.S. QinZ.H. QinJ.F. QiuK.H. RashidC.F. RedmerM. RipkaG. RongCh. RosnerX.D. RuanV. SantoroA. SarantsevM. SavriéK. SchoenningS. SchumannW. ShanM. ShaoC.P. ShenP.X. ShenX.Y. ShenH.Y. ShengW.M. SongM.R. ShepherdX.Y. SongS. SosioS. SpataroG.X. SunJ.F. SunS.S. SunY.J. SunY.Z. SunZ.J. SunZ.T. SunC.J. TangX. TangI. TapanE.H. ThorndikeM. TiemensM. UllrichI. UmanG.S. VarnerB. WangD. WangD.Y. WangK. WangL.L. WangL.S. WangM. WangP. WangP.L. WangS.G. WangW. WangX.F. WangY.D. WangY.F. WangY.Q. WangZ. WangZ.G. WangZ.H. WangZ.Y. WangT. WeberD.H. WeiJ.B. WeiP. WeidenkaffS.P. WenU. WiednerM. WolkeL.H. WuZ. WuL.G. XiaY. XiaD. XiaoH. XiaoZ.J. XiaoY.G. XieQ.L. XiuG.F. XuL. XuQ.J. XuX.P. XuL. YanW.B. YanW.C. YanY.H. YanH.J. YangH.X. YangL. YangY. YangY.X. YangM. YeM.H. YeJ.H. YinB.X. YuC.X. YuJ.S. YuC.Z. YuanW.L. YuanY. YuanA. YuncuA.A. ZafarA. ZalloY. ZengB.X. ZhangB.Y. ZhangC. ZhangC.C. ZhangD.H. ZhangH.H. ZhangH.Y. ZhangJ.J. ZhangJ.L. ZhangJ.Q. ZhangJ.W. ZhangJ.Y. ZhangJ.Z. ZhangK. ZhangL. ZhangX.Y. ZhangY. ZhangY.N. ZhangY.H. ZhangY.T. ZhangYu ZhangZ.H. ZhangZ.P. ZhangZ.Y. ZhangG. ZhaoJ.W. ZhaoJ.Y. ZhaoJ.Z. ZhaoLei ZhaoLing ZhaoM.G. ZhaoQ. ZhaoQ.W. ZhaoS.J. ZhaoT.C. ZhaoY.B. ZhaoZ.G. ZhaoA. ZhemchugovB. ZhengJ.P. ZhengW.J. ZhengY.H. ZhengB. ZhongL. ZhouX. ZhouX.K. ZhouX.R. ZhouX.Y. ZhouK. ZhuK.J. ZhuS. ZhuS.H. ZhuX.L. ZhuY.C. ZhuY.S. ZhuZ.A. ZhuJ. ZhuangL. ZottiB.S. ZouJ.H. Zou
Source
Physics Letters B, Vol 753, Iss C, Pp 629-638 (2016)
Subject
Hadronic cross section
Muon anomaly
Initial state radiation
Pion form factor
BESIII
Physics
QC1-999
Language
English
ISSN
0370-2693
1873-2445
Abstract
We extract the e+e−→π+π− cross section in the energy range between 600 and 900 MeV, exploiting the method of initial state radiation. A data set with an integrated luminosity of 2.93 fb−1 taken at a center-of-mass energy of 3.773 GeV with the BESIII detector at the BEPCII collider is used. The cross section is measured with a systematic uncertainty of 0.9%. We extract the pion form factor |Fπ|2 as well as the contribution of the measured cross section to the leading-order hadronic vacuum polarization contribution to (g−2)μ. We find this value to be aμππ,LO(600–900MeV)=(368.2±2.5stat±3.3sys)⋅10−10, which is between the corresponding values using the BaBar or KLOE data.