Search for C-parity violation in J/ψ→γγJ/ ψ\to γγ and γϕ γϕ

preprint2014arXivOpen access
BESIII CollaborationM. 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. BogerO. BondarenkoI. BoykoS. BraunR. A. BriereH. CaiX. CaiO. CakirA. CalcaterraG. F. CaoS. A. CetinJ. F. ChangG. ChelkovG. ChenH. S. ChenJ. C. ChenM. L. ChenS. J. ChenX. ChenX. R. ChenY. B. ChenH. P. ChengX. K. ChuY. P. ChuG. CibinettoD. Cronin-HennessyH. L. DaiJ. P. DaiD. DedovichZ. Y. DengA. DenigI. DenysenkoM. DestefanisF. De MoriY. DingC. DongJ. DongL. Y. DongM. Y. DongS. X. DuJ. Z. FanJ. FangS. S. FangY. FangL. FavaF. FeldbauerG. FeliciC. Q. FengE. FioravantiC. D. FuQ. GaoY. GaoI. GarziaC. GengK. GoetzenW. X. GongW. GradlM. GrecoM. H. GuY. T. GuY. H. GuanA. Q. GuoL. B. GuoT. GuoY. P. GuoZ. HaddadiS. HanY. L. HanF. A. HarrisK. L. HeZ. Y. HeT. HeldY. K. HengZ. L. HouC. HuH. M. HuJ. F. HuT. 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. JiangJ. B. JiaoZ. JiaoD. P. JinS. JinT. JohanssonA. JulinN. Kalantar-NayestanakiX. L. KangX. S. KangM. KavatsyukB. C. KeB. KlossO. B. KolcuB. KopfM. KornicerW. KuehnA. KupscW. LaiJ. S. LangeM. LaraP. LarinM. LeyheCheng LiCui LiD. M. LiF. LiG. LiH. B. LiJ. C. LiJin LiK. LiQ. J. LiT. LiW. D. LiW. G. LiX. H. LiX. L. LiX. N. LiX. Q. LiZ. B. LiH. LiangY. F. LiangY. T. LiangD. X. LinB. J. LiuC. L. LiuC. X. LiuF. H. LiuFang LiuFeng LiuH. B. LiuH. H. LiuH. M. LiuJ. LiuJ. P. LiuK. LiuK. Y. 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. MaQ. M. MaS. MaT. MaX. Y. MaF. E. MaasM. MaggioraQ. A. MalikY. J. MaoZ. P. MaoS. MarcelloJ. G. MesschendorpJ. MinT. J. MinR. E. MitchellX. H. MoY. J. MoH. MoeiniC. 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. L. PingR. G. PingR. PolingY. N. PuM. QiS. QianC. F. QiaoL. Q. QinN. QinX. S. QinY. QinZ. H. QinJ. F. QiuK. H. RashidC. F. RedmerH. L. RenM. RipkaG. RongX. D. RuanV. SantoroA. SarantsevM. SavriéK. SchoenningS. SchumannW. ShanM. ShaoC. P. ShenX. Y. ShenH. Y. ShengM. R. ShepherdW. M. SongX. Y. SongS. SosioS. SpataroB. SpruckG. X. SunJ. F. SunS. S. SunY. J. SunY. Z. SunZ. J. SunZ. T. SunC. J. TangX. TangI. TapanE. H. ThorndikeM. TiemensD. TothM. UllrichI. UmanG. S. VarnerB. WangB. L. WangD. WangD. Y. WangK. WangL. L. WangL. S. WangM. WangP. WangP. L. WangQ. J. WangS. G. WangW. WangX. F. WangY. D. WangY. F. WangY. Q. WangZ. WangZ. G. WangZ. H. WangZ. Y. WangD. H. WeiJ. B. WeiP. WeidenkaffS. P. WenM. WernerU. WiednerM. WolkeL. H. WuZ. WuL. G. XiaY. XiaD. XiaoZ. J. XiaoY. G. XieQ. L. XiuG. F. XuL. XuQ. J. XuQ. N. XuX. P. XuZ. XueL. YanW. B. YanW. C. YanY. H. YanH. X. YangL. YangY. YangY. X. YangH. YeM. YeM. H. YeB. X. YuC. X. YuH. W. YuJ. S. YuC. Z. YuanW. L. YuanY. YuanA. YuncuA. A. ZafarA. ZalloS. L. ZangY. ZengB. X. ZhangB. Y. ZhangC. ZhangC. C. ZhangD. H. ZhangH. H. ZhangH. Y. ZhangJ. J. ZhangJ. Q. ZhangJ. W. ZhangJ. Y. ZhangJ. Z. ZhangL. ZhangS. H. ZhangX. J. ZhangX. Y. ZhangY. ZhangY. H. ZhangZ. H. ZhangZ. P. ZhangZ. Y. ZhangG. ZhaoJ. W. ZhaoJ. Z. ZhaoLei ZhaoLing ZhaoM. G. ZhaoQ. ZhaoQ. W. ZhaoS. J. ZhaoT. C. ZhaoY. B. ZhaoZ. G. ZhaoA. ZhemchugovB. ZhengJ. P. ZhengY. H. ZhengB. ZhongL. ZhouLi ZhouX. ZhouX. R. ZhouX. Y. ZhouK. ZhuK. J. ZhuX. L. ZhuY. C. ZhuY. S. ZhuZ. A. ZhuJ. ZhuangB. S. ZouJ. H. Zou

Abstract

Using 1.06×1081.06\times10^8 ψ(3686)ψ(3686) events recorded in e+e−e^{+}e^{-} collisions at s=\sqrt{s}= 3.686 GeV with the BESIII at the BEPCII collider, we present searches for C-parity violation in J/ψ→γγJ/ψ\to γγ and γϕ γϕ decays via ψ(3686)→J/ψπ+π−ψ(3686) \to J/ψπ^+π^-. No significant signals are observed in either channel. Upper limits on the branching fractions are set to be B(J/ψ→γγ)<2.7×10−7\mathcal{B}(J/ψ\to γγ) < 2.7 \times 10^{-7} and B(J/ψ→γϕ)<1.4×10−6\mathcal{B}(J/ψ\to γϕ) < 1.4 \times 10^{-6} at the 90\% confidence level. The former is one order of magnitude more stringent than the previous upper limit, and the latter represents the first limit on this decay channel.

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