6533b85efe1ef96bd12bfaab
RESEARCH PRODUCT
Measurement of the branching fractions of Ds+→η′X and Ds+→η′ρ+ in e+e−→Ds+Ds−
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. BoykoRoy 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. GarziaC. GengK. GoetzenW.x. GongW. GradlM. GrecoM.h. GuY.t. GuY.h. GuanA.q. GuoL.b. GuoY. GuoY.p. GuoZ. HaddadiA. HafnerS. HanY.l. HanX.q. HaoF.a. HarrisK.l. HeZ.y. HeT. HeldY.k. HengZ.l. HouC. HuH.m. HuJ.f. HuT. HuY. HuG.m. HuangG.s. HuangH.p. HuangJ.s. HuangX.t. HuangY. HuangT. HussainQ. JiQ.p. JiX.b. JiX.l. JiL.l. JiangL.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. LiC.h. LiCheng LiD.m. LiF. LiG. LiH.b. LiJ.c. LiJin LiK. 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.h. LiuH.m. LiuJ. LiuJ.b. LiuJ.p. LiuJ.y. LiuK. LiuK.y. LiuL.d. LiuP.l. LiuQ. LiuS.b. LiuX. LiuX.x. LiuY.b. LiuZ.a. LiuZhiqiang LiuZhiqing LiuH. LoehnerX.c. LouH.j. LuJ.g. LuR.q. LuY. LuY.p. LuC.l. LuoM.x. LuoT. LuoX.l. LuoM. LvX.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. MinT.j. 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. PrasadY.n. PuM. QiS. QianC.f. QiaoL.q. QinN. QinX.s. QinY. QinZ.h. QinJ.f. QiuK.h. RashidC.f. RedmerH.l. RenM. RipkaG. RongCh. RosnerX.d. RuanV. SantoroA. SarantsevM. SavriéK. SchoenningS. SchumannW. ShanM. ShaoC.p. ShenP.x. ShenX.y. ShenH.y. ShengW.m. SongX.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. WangB.l. 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. XiaoZ.j. XiaoY.g. XieQ.l. XiuG.f. XuL. XuQ.j. XuQ.n. XuX.p. XuL. YanW.b. YanW.c. YanY.h. YanH.j. YangH.x. YangL. YangY. YangY.x. YangH. YeM. YeM.h. YeJ.h. YinB.x. YuC.x. YuH.w. 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. ZhangS.h. 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. ZhouLi ZhouX. ZhouX.k. ZhouX.r. ZhouX.y. ZhouK. ZhuK.j. ZhuS. ZhuX.l. ZhuY.c. ZhuY.s. ZhuZ.a. ZhuJ. ZhuangL. ZottiB.s. ZouJ.h. Zousubject
PhysicsNuclear and High Energy PhysicsMeson010308 nuclear & particles physicsBranching fractionElectron–positron annihilationAnalytical chemistryBranching (polymer chemistry)01 natural sciencesNuclear physics0103 physical sciencesPiHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsdescription
We study D-s(+) decays to final states involving the eta' with a 482 pb(-1) data sample collected at root s = 4.009 GeV with the BESIII detector at the BEPCII collider. We measure the branching fractions B(D-s(+) -> eta'X) = (8.8 +/- 1.8 +/- 0.5)% and B(D-s(+) > eta'rho(+)) = (5.8 +/- 1.4 +/- 0.4)% where the first uncertainty is statistical and the second is systematic. In addition, we estimate an upper limit on the non-resonant branching ratio B(D-s(+) -> eta'pi(+)pi(0)) eta'rho(+)). (C) 2015 The Authors. Published by Elsevier B.V.
year | journal | country | edition | language |
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2015-11-01 | Physics Letters B |