6533b7d6fe1ef96bd1265cd6
RESEARCH PRODUCT
Measurement of cross sections of the interactions e+e−→ ϕϕω and e+e−→ ϕϕϕ at center-of-mass energies from 4.008 to 4.600 GeV
M. AblikimM.n. AchasovS. AhmedX.c. AiO. AlbayrakM. AlbrechtD.j. AmbroseA. AmorosoF.f. AnQ. AnJ.z. BaiO. BakinaR. Baldini FerroliY. BanD.w. BennettJ.v. BennettN. BergerM. BertaniD. BettoniJ.m. BianF. BianchiE. BogerI. BoykoR.a. BriereH. CaiX. CaiO. CakirA. CalcaterraG.f. CaoS.a. CetinJ. ChaiJ.f. ChangG. ChelkovG. ChenH.s. ChenJ.c. ChenM.l. ChenS. ChenS.j. ChenX. ChenX.r. ChenY.b. ChenX.k. ChuG. CibinettoH.l. DaiJ.p. DaiA. DbeyssiD. DedovichZ.y. DengA. DenigI. DenysenkoM. DestefanisF. De MoriY. DingC. DongJ. DongL.y. DongM.y. DongZ.l. DouS.x. DuP.f. DuanJ.z. FanJ. FangS.s. FangX. FangY. FangR. FarinelliL. FavaF. FeldbauerG. FeliciC.q. FengE. FioravantiM. FritschC.d. FuQ. GaoX.l. GaoY. GaoZ. GaoI. GarziaK. GoetzenL. GongW.x. GongW. GradlM. GrecoM.h. GuY.t. GuY.h. GuanA.q. GuoL.b. GuoR.p. GuoY. GuoY.p. GuoZ. HaddadiA. HafnerS. HanX.q. HaoF.a. HarrisK.l. HeF.h. HeinsiusT. HeldY.k. HengT. HoltmannZ.l. HouC. HuH.m. HuT. HuY. HuG.s. HuangJ.s. HuangX.t. HuangX.z. HuangZ.l. HuangT. HussainW. Ikegami AnderssonQ. 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. KornicerA. KupscW. KühnJ.s. LangeM. LaraP. LarinH. LeithoffC. LengC. LiCheng LiD.m. LiF. LiF.y. LiG. LiH.b. LiH.j. LiJ.c. LiJin LiK. LiK. LiLei LiP.r. LiQ.y. LiT. LiW.d. LiW.g. LiX.l. LiX.n. LiX.q. LiY.b. LiZ.b. LiH. LiangY.f. LiangY.t. LiangG.r. LiaoD.x. LinB. LiuB.j. LiuC.x. LiuD. LiuF.h. LiuFang LiuFeng LiuH.b. LiuH.h. LiuH.h. LiuH.m. LiuJ. LiuJ.b. LiuJ.p. LiuJ.y. LiuK. LiuK.y. LiuL.d. LiuP.l. LiuQ. LiuS.b. LiuX. LiuY.b. LiuY.y. LiuZ.a. LiuZhiqing LiuH. LoehnerY.f. LongX.c. LouH.j. LuJ.g. LuY. LuY.p. LuC.l. LuoM.x. LuoT. LuoX.l. LuoX.r. LyuF.c. MaH.l. MaL.l. MaM.m. MaQ.m. MaT. MaX.n. MaX.y. MaY.m. MaF.e. MaasM. MaggioraQ.a. MalikY.j. MaoZ.p. MaoS. MarcelloJ.g. MesschendorpG. MezzadriJ. MinT.j. MinR.e. MitchellX.h. MoY.j. MoC. Morales MoralesG. MorelloN.yu. MuchnoiH. MuramatsuP. MusiolY. NefedovF. NerlingI.b. NikolaevZ. NingS. NisarS.l. NiuX.y. NiuS.l. OlsenQ. OuyangS. PacettiY. PanP. PatteriM. PelizaeusH.p. PengK. PetersJ. PetterssonJ.l. PingR.g. PingR. PolingV. PrasadH.r. QiM. QiS. QianC.f. QiaoL.q. QinN. QinX.s. QinZ.h. QinJ.f. QiuK.h. RashidC.f. RedmerM. RipkaG. RongCh. RosnerX.d. RuanA. SarantsevM. SavriéC. SchnierK. SchoenningW. ShanM. ShaoC.p. ShenP.x. ShenX.y. ShenH.y. ShengW.m. SongX.y. SongS. SosioS. SpataroG.x. SunJ.f. SunS.s. SunX.h. SunY.j. SunY.z. SunZ.j. SunZ.t. SunC.j. TangX. TangI. TapanE.h. ThorndikeM. TiemensI. UmanG.s. VarnerB. WangB.l. WangD. WangD.y. WangK. WangL.l. WangL.s. WangM. WangP. WangP.l. WangW. WangW.p. WangX.f. WangY. WangY.d. WangY.f. WangY.q. WangZ. WangZ.g. WangZ.h. WangZ.y. WangZongyuan WangT. WeberD.h. WeiP. WeidenkaffS.p. WenU. WiednerM. WolkeL.h. WuL.j. WuZ. WuL. XiaL.g. XiaY. XiaD. XiaoH. XiaoZ.j. XiaoY.g. XieY.h. XieQ.l. XiuG.f. XuJ.j. XuL. XuQ.j. XuQ.n. XuX.p. XuL. YanW.b. YanW.c. YanY.h. YanH.j. YangH.x. YangL. YangY.x. YangM. YeM.h. YeJ.h. YinZ.y. YouB.x. YuC.x. YuJ.s. YuC.z. YuanY. YuanA. YuncuA.a. ZafarY. ZengZ. ZengB.x. ZhangB.y. ZhangC.c. ZhangD.h. ZhangH.h. ZhangH.y. ZhangJ. ZhangJ.j. ZhangJ.l. ZhangJ.q. ZhangJ.w. ZhangJ.y. ZhangJ.z. ZhangK. ZhangL. ZhangS.q. ZhangX.y. ZhangY. ZhangY. ZhangY.h. ZhangY.n. 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. Zousubject
Nuclear and High Energy PhysicsBESIII детекторe+e- annihilationElectron–positron annihilation01 natural sciencesNOlaw.inventionNuclear physicsCross section (physics)law0103 physical sciencesCross section; e+e−annihilation; Triple quarkonia; Nuclear and High Energy Physics010306 general physicsColliderTriple quarkoniaPhysicsAnnihilationCross section010308 nuclear & particles physicse+e−annihilatione+e− annihilationlcsh:QC1-999BEPCII коллайдерe+e? annihilationCenter of massCross section; e+e- annihilation; Triple quarkonia; Nuclear and High Energy Physicslcsh:Physicsdescription
Abstract Using data samples collected with the BESIII detector at the BEPCII collider at six center-of-mass energies between 4.008 and 4.600 GeV, we observe the processes e + e − → ϕ ϕ ω and e + e − → ϕ ϕ ϕ . The Born cross sections are measured and the ratio of the cross sections σ ( e + e − → ϕ ϕ ω ) / σ ( e + e − → ϕ ϕ ϕ ) is estimated to be 1.75 ± 0.22 ± 0.19 averaged over six energy points, where the first uncertainty is statistical and the second is systematic. The results represent first measurements of these interactions.
year | journal | country | edition | language |
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2017-11-01 |