Two-photon widths of the χc0,2χ_{c0, 2} states and helicity analysis for $χ_{c2}\arγγ$}

preprint2012arXivOpen access
BESIII CollaborationM. AblikimM. N. AchasovD. J. AmbroseF. F. AnQ. AnZ. H. AnJ. Z. BaiR. B. FerroliY. BanJ. BeckerN. BergerM. B. BertaniJ. M. BianE. BogerO. BondarenkoI. BoykoR. A. BriereV. BytevX. CaiA. C. CalcaterraG. F. CaoJ. F. ChangG. ChelkovG. ChenH. S. ChenJ. C. ChenM. L. ChenS. J. ChenY. ChenY. B. ChenH. P. ChengY. P. ChuD. Cronin-HennessyH. L. DaiJ. P. DaiD. DedovichZ. Y. DengA. DenigI. DenysenkoM. DestefanisW. M. DingY. DingL. Y. DongM. Y. DongS. X. DuJ. FangS. S. FangL. FavaF. FeldbauerC. Q. FengC. D. FuJ. L. FuY. GaoC. GengK. GoetzenW. X. GongW. GradlM. GrecoM. H. GuY. T. GuY. H. GuanA. Q. GuoL. B. GuoY. P. GuoY. L. HanX. Q. HaoF. A. HarrisK. L. HeM. HeZ. Y. HeT. HeldY. K. HengZ. L. HouH. M. HuJ. F. HuT. HuB. HuangG. M. HuangJ. S. HuangX. T. HuangY. P. HuangT. HussainC. S. JiQ. JiX. B. JiX. L. JiL. K. JiaL. L. JiangX. S. JiangJ. B. JiaoZ. JiaoD. P. JinS. JinF. F. JingN. Kalantar-NayestanakiM. KavatsyukW. KuehnW. LaiJ. S. LangeJ. K. C. LeungC. H. LiCheng LiCui LiD. M. LiF. LiG. LiH. B. LiJ. C. LiK. LiLei LiN. B. LiQ. J. LiS. L. LiW. D. LiW. G. LiX. L. LiX. N. LiX. Q. LiX. R. LiZ. B. LiH. LiangY. F. LiangY. T. LiangG. R. LiaoX. T. LiaoB. J. LiuC. L. LiuC. X. LiuC. Y. LiuF. H. LiuFang LiuFeng LiuH. LiuH. B. LiuH. H. LiuH. M. LiuH. W. LiuJ. P. LiuKun LiuKai LiuK. Y. LiuP. L. LiuS. B. LiuX. LiuX. H. LiuY. B. LiuY. LiuZ. A. LiuZhiqiang LiuZhiqing LiuH. LoehnerG. R. LuH. J. LuJ. G. LuQ. W. LuX. R. LuY. P. LuC. L. LuoM. X. LuoT. LuoX. L. LuoM. LvC. L. MaF. C. MaH. L. MaQ. M. MaS. MaT. MaX. Y. MaY. MaF. E. MaasM. MaggioraQ. A. MalikH. MaoY. J. MaoZ. P. MaoJ. G. MesschendorpJ. MinT. J. MinR. E. MitchellX. H. MoC. Morales MoralesC. MotzkoN. Yu. MuchnoiY. NefedovC. NicholsonI. B. NikolaevZ. NingS. L. OlsenQ. OuyangS. P. PacettiJ. W. ParkM. PelizaeusK. PetersJ. L. PingR. G. PingR. PolingE. PrencipeC. S. J. PunM. QiS. QianC. F. QiaoX. S. QinY. QinZ. H. QinJ. F. QiuK. H. RashidG. RongX. D. RuanA. SarantsevJ. SchulzeM. ShaoC. P. ShenX. Y. ShenH. Y. ShengM. R. ShepherdX. Y. SongS. SpataroB. SpruckD. H. SunG. X. SunJ. F. SunS. S. SunX. D. SunY. J. SunY. Z. SunZ. J. SunZ. T. SunC. J. TangX. TangE. H. ThorndikeH. L. TianD. TothM. U. UlrichG. S. VarnerB. WangB. Q. WangK. WangL. L. WangL. S. WangM. WangP. WangP. L. WangQ. WangQ. J. WangS. G. WangX. F. WangX. L. WangY. D. WangY. F. WangY. Q. WangZ. WangZ. G. WangZ. Y. WangD. H. WeiP. WeidenkaffQ. G. WenS. P. WenM. W. WernerU. WiednerL. H. WuN. WuS. X. WuW. WuZ. WuL. G. XiaZ. J. XiaoY. G. XieQ. L. XiuG. F. XuG. M. XuH. XuQ. J. XuX. P. XuY. XuZ. R. XuF. XueZ. XueL. YanW. B. YanY. H. YanH. X. YangT. YangY. YangY. X. YangH. YeM. YeM. H. YeB. X. YuC. X. YuJ. S. YuS. P. YuC. Z. YuanW. L. YuanY. YuanA. A. ZafarA. Z. ZalloY. ZengB. X. ZhangB. Y. ZhangC. C. ZhangD. H. ZhangH. H. ZhangH. Y. ZhangJ. ZhangJ. G. ZhangJ. Q. ZhangJ. W. ZhangJ. Y. ZhangJ. Z. ZhangL. ZhangS. H. ZhangT. R. ZhangX. J. ZhangX. Y. ZhangY. ZhangY. H. ZhangY. S. ZhangZ. P. ZhangZ. Y. ZhangG. ZhaoH. S. ZhaoJ. W. ZhaoK. X. ZhaoLei ZhaoLing ZhaoM. G. ZhaoQ. ZhaoS. J. ZhaoT. C. ZhaoX. H. ZhaoY. B. ZhaoZ. G. ZhaoA. ZhemchugovB. ZhengJ. P. ZhengY. H. ZhengZ. P. ZhengB. ZhongJ. ZhongL. ZhouX. K. ZhouX. R. ZhouC. ZhuK. ZhuK. J. ZhuS. H. ZhuX. L. ZhuX. W. ZhuY. M. ZhuY. S. ZhuZ. A. ZhuJ. ZhuangB. S. ZouJ. H. ZouJ. X. Zuo

Abstract

Based on a data sample of 106 M ψ′ψ^{\prime} events collected with the BESIII detector, the decays $ψ^{\prime}\arγχ_{c0, 2}$,$χ_{c0, 2}\arγγ$ are studied to determine the two-photon widths of the χc0,2χ_{c0, 2} states. The two-photon decay branching fractions are determined to be ${\cal B}(χ_{c0}\arγγ) = (2.24\pm 0.19\pm 0.12\pm 0.08)\times 10^{-4}$ and ${\cal B}(χ_{c2}\arγγ) = (3.21\pm 0.18\pm 0.17\pm 0.13)\times 10^{-4}$. From these, the two-photon widths are determined to be Γγγ(χc0)=(2.33±0.20±0.13±0.17)Γ_{γγ}(χ_{c0}) = (2.33\pm0.20\pm0.13\pm0.17) keV, Γγγ(χc2)=(0.63±0.04±0.04±0.04)Γ_{γγ}(χ_{c2}) = (0.63\pm0.04\pm0.04\pm0.04) keV, and R\cal R =Γγγ(χc2)/Γγγ(χc0)=0.271±0.029±0.013±0.027=Γ_{γγ}(χ_{c2})/Γ_{γγ}(χ_{c0})=0.271\pm 0.029\pm 0.013\pm 0.027, where the uncertainties are statistical, systematic, and those from the PDG ${\cal B}(ψ^{\prime}\arγχ_{c0,2})$ and Γ(χc0,2)Γ(χ_{c0,2}) errors, respectively. The ratio of the two-photon widths for helicity λ=0λ=0 and helicity λ=2λ=2 components in the decay $χ_{c2}\arγγ$ is measured for the first time to be f0/2=Γγγλ=0(χc2)/Γγγλ=2(χc2)=0.00±0.02±0.02f_{0/2} =Γ^{λ=0}_{γγ}(χ_{c2})/Γ^{λ=2}_{γγ}(χ_{c2}) = 0.00\pm0.02\pm0.02.

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