학술논문

Measurement of branching fractions for D meson decaying into ϕ meson and a pseudoscalar meson
Document Type
article
Author
M. AblikimM.N. AchasovP. AdlarsonS. AhmedM. AlbrechtM. AlekseevA. AmorosoF.F. AnQ. AnY. BaiO. BakinaR. Baldini FerroliI. BalossinoY. BanK. BegzsurenJ.V. BennettN. BergerM. BertaniD. BettoniF. BianchiJ. BiernatJ. BlomsI. BoykoR.A. BriereH. CaiX. CaiA. CalcaterraG.F. CaoN. CaoS.A. CetinJ. ChaiJ.F. ChangW.L. ChangG. ChelkovD.Y. ChenG. ChenH.S. ChenJ.C. ChenM.L. ChenS.J. ChenY.B. ChenW. ChengG. CibinettoF. CossioX.F. CuiH.L. DaiJ.P. DaiX.C. DaiA. DbeyssiD. DedovichZ.Y. DengA. DenigI. DenysenkoM. DestefanisF. De MoriY. DingC. DongJ. DongL.Y. DongM.Y. DongZ.L. DouS.X. DuJ.Z. FanJ. FangS.S. FangY. FangR. FarinelliL. FavaF. FeldbauerG. FeliciC.Q. FengM. FritschC.D. FuY. FuQ. GaoX.L. GaoY. GaoY.G. GaoZ. GaoB. GarillonI. GarziaE.M. GersabeckA. GilmanK. GoetzenL. GongW.X. GongW. GradlM. GrecoL.M. GuM.H. GuS. GuY.T. GuA.Q. GuoL.B. GuoR.P. GuoY.P. GuoA. GuskovS. HanX.Q. HaoF.A. HarrisK.L. HeF.H. HeinsiusT. HeldY.K. HengM. HimmelreichY.R. HouZ.L. HouH.M. HuJ.F. HuT. HuY. HuG.S. HuangJ.S. HuangX.T. HuangX.Z. HuangN. HueskenT. HussainW. Ikegami AnderssonW. ImoehlM. IrshadQ. JiQ.P. JiX.B. JiX.L. JiH.L. JiangX.S. JiangX.Y. JiangJ.B. JiaoZ. JiaoD.P. JinS. JinY. JinT. JohanssonN. Kalantar-NayestanakiX.S. KangR. KappertM. KavatsyukB.C. KeI.K. KeshkA. KhoukazP. KieseR. KiuchiR. KliemtL. KochO.B. KolcuB. KopfM. KuemmelM. KuessnerA. KupscM. KurthM.G. KurthW. KühnJ.S. LangeP. LarinL. LavezziH. LeithoffT. LenzC. LiCheng LiD.M. LiF. LiF.Y. LiG. LiH.B. LiH.J. LiJ.C. LiJ.W. LiKe LiL.K. LiLei LiP.L. LiP.R. LiQ.Y. LiW.D. LiW.G. LiX.H. LiX.L. LiX.N. LiZ.B. LiZ.Y. LiH. LiangY.F. LiangY.T. LiangG.R. LiaoL.Z. LiaoJ. LibbyC.X. LinD.X. LinY.J. LinB. LiuB.J. LiuC.X. LiuD. LiuD.Y. LiuF.H. LiuFang LiuFeng LiuH.B. LiuH.M. LiuHuanhuan LiuHuihui LiuJ.B. LiuJ.Y. LiuK. LiuK.Y. LiuKe LiuL.Y. LiuQ. LiuS.B. LiuT. LiuX. LiuX.Y. LiuY.B. LiuZ.A. LiuZhiqing LiuY.F. LongX.C. LouH.J. LuJ.D. LuJ.G. LuY. LuY.P. LuC.L. LuoM.X. LuoP.W. LuoT. LuoX.L. LuoS. LussoX.R. LyuF.C. MaH.L. MaL.L. MaM.M. MaQ.M. MaX.N. MaX.X. MaX.Y. MaY.M. MaF.E. MaasM. MaggioraS. MaldanerS. MaldeQ.A. MalikA. MangoniY.J. MaoZ.P. MaoS. MarcelloZ.X. MengJ.G. MesschendorpG. MezzadriJ. MinT.J. MinR.E. MitchellX.H. MoY.J. MoC. Morales MoralesN.Yu. MuchnoiH. MuramatsuA. MustafaS. NakhoulY. NefedovF. NerlingI.B. NikolaevZ. NingS. NisarS.L. NiuS.L. OlsenQ. OuyangS. PacettiY. PanM. PapenbrockP. PatteriM. PelizaeusH.P. PengK. PetersJ. PetterssonJ.L. PingR.G. PingA. PitkaR. PolingV. PrasadH.R. QiM. QiT.Y. QiS. QianC.F. QiaoN. QinX.P. QinX.S. QinZ.H. QinJ.F. QiuS.Q. QuK.H. RashidK. RavindranC.F. RedmerM. RichterA. RivettiV. RodinM. RoloG. RongCh. RosnerM. RumpA. SarantsevM. SavriéY. SchelhaasK. SchoenningW. ShanX.Y. ShanM. ShaoC.P. ShenP.X. ShenX.Y. ShenH.Y. ShengX. ShiX.D ShiJ.J. SongQ.Q. SongX.Y. SongS. SosioC. SowaS. SpataroF.F. SuiG.X. SunJ.F. SunL. SunS.S. SunX.H. SunY.J. SunY.K SunY.Z. SunZ.J. SunZ.T. SunY.T TanC.J. TangG.Y. TangX. TangV. ThorenB. TsedneeI. UmanB. WangB.L. WangC.W. WangD.Y. WangK. WangL.L. WangL.S. WangM. WangM.Z. WangMeng WangP.L. WangR.M. WangW.P. WangX. WangX.F. WangX.L. WangY. WangY.F. WangY.Q. WangZ. WangZ.G. WangZ.Y. WangZongyuan WangT. WeberD.H. WeiP. WeidenkaffF. WeidnerH.W. WenS.P. WenU. WiednerG. WilkinsonM. WolkeL.H. WuL.J. WuZ. WuL. XiaY. XiaS.Y. XiaoY.J. XiaoZ.J. XiaoY.G. XieY.H. XieT.Y. XingX.A. XiongQ.L. XiuG.F. XuJ.J. XuL. XuQ.J. XuW. XuX.P. XuF. YanL. YanW.B. YanW.C. YanY.H. YanH.J. YangH.X. YangL. YangR.X. YangS.L. YangY.H. YangY.X. YangYifan YangZ.Q. YangM. YeM.H. YeJ.H. YinZ.Y. YouB.X. YuC.X. YuJ.S. YuT. YuC.Z. YuanX.Q. YuanY. YuanA. YuncuA.A. ZafarY. ZengB.X. ZhangB.Y. ZhangC.C. ZhangD.H. ZhangH.H. ZhangH.Y. ZhangJ. ZhangJ.L. ZhangJ.Q. ZhangJ.W. ZhangJ.Y. ZhangJ.Z. ZhangK. ZhangL. ZhangS.F. ZhangT.J. ZhangX.Y. ZhangY. ZhangY.H. ZhangY.T. ZhangYang ZhangYao ZhangYi ZhangYu ZhangZ.H. ZhangZ.P. ZhangZ.Y. ZhangG. ZhaoJ.W. ZhaoJ.Y. ZhaoJ.Z. ZhaoLei ZhaoLing ZhaoM.G. ZhaoQ. ZhaoS.J. ZhaoT.C. ZhaoY.B. ZhaoZ.G. ZhaoA. ZhemchugovB. ZhengJ.P. ZhengY. ZhengY.H. ZhengB. ZhongL. ZhouL.P. ZhouQ. ZhouX. ZhouX.K. ZhouX.R. ZhouXiaoyu ZhouXu ZhouA.N. ZhuJ. ZhuK. ZhuK.J. ZhuS.H. ZhuW.J. ZhuX.L. ZhuY.C. ZhuY.S. ZhuZ.A. ZhuJ. ZhuangB.S. ZouJ.H. Zou
Source
Physics Letters B, Vol 798, Iss , Pp - (2019)
Subject
Physics
QC1-999
Language
English
ISSN
0370-2693
Abstract
The four decay modes D0→ϕπ0, D0→ϕη, D+→ϕπ+, and D+→ϕK+ are studied by using a data sample taken at the centre-of-mass energy s=3.773 GeV with the BESIII detector, corresponding to an integrated luminosity of 2.93 fb−1. The branching fractions of the first three decay modes are measured to be B(D0→ϕπ0)=(1.168±0.028±0.028)×10−3, B(D0→ϕη)=(1.81±0.46±0.06)×10−4, and B(D+→ϕπ+)=(5.70±0.05±0.13)×10−3, respectively, where the first uncertainties are statistical and the second are systematic. In addition, the upper limit of the branching fraction for D+→ϕK+ is given to be 2.1×10−5 at the 90% confidence level. The ratio of B(D0→ϕπ0) to B(D+→ϕπ+) is calculated to be (20.49±0.50±0.45)%, which is consistent with the theoretical prediction based on isospin symmetry between these two decay modes. Keywords: BESIII, D meson, Hadronic decays, Branching fractions