Measurements of Baryon Pair Decays of χcJχ_{cJ} Mesons

preprint2013arXivOpen access
M. AblikimM. N. AchasovO. AlbayrakD. J. AmbroseF. F. AnQ. AnJ. Z. BaiY. BanJ. BeckerJ. V. BennettM. BertaniJ. M. BianE. BogerO. BondarenkoI. BoykoR. A. BriereV. BytevX. CaiO. CakirA. CalcaterraG. F. CaoS. A. CetinJ. F. ChangG. ChelkovG. ChenH. S. ChenJ. C. ChenM. L. ChenS. J. ChenX. 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. FavaC. Q. FengR. B. FerroliP. FriedelC. D. FuY. GaoC. GengK. GoetzenW. X. GongW. GradlM. GrecoM. H. GuY. T. GuY. H. GuanA. Q. GuoL. B. GuoT. GuoY. P. GuoY. L. HanF. A. HarrisK. L. HeM. HeZ. Y. HeT. HeldY. K. HengZ. L. HouC. HuH. M. HuJ. F. HuT. HuG. M. HuangG. S. HuangJ. S. HuangL. HuangX. T. HuangY. HuangY. P. HuangT. HussainC. S. JiQ. JiQ. P. JiX. B. JiX. L. JiL. L. JiangX. S. JiangJ. B. JiaoZ. JiaoD. P. JinS. JinF. F. JingN. Kalantar-NayestanakiM. KavatsyukB. KopfM. KornicerW. KuehnW. LaiJ. S. LangeM. LeyheC. H. LiCheng LiCui LiD. M. LiF. LiG. LiH. B. LiJ. C. LiK. LiLei 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. LiaoD. LinB. J. LiuC. L. LiuC. X. LiuF. H. LiuFang LiuFeng LiuH. LiuH. B. LiuH. H. LiuH. M. LiuH. W. LiuJ. P. LiuK. LiuK. Y. LiuKai LiuP. L. LiuQ. LiuS. B. LiuX. LiuY. B. 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. MaF. E. MaasM. MaggioraQ. A. MalikY. J. MaoZ. P. MaoJ. G. MesschendorpJ. MinT. J. MinR. E. MitchellX. H. MoC. Morales MoralesN. Yu. MuchnoiH. MuramatsuY. NefedovC. NicholsonI. B. NikolaevZ. NingS. L. OlsenQ. OuyangS. PacettiJ. W. ParkM. PelizaeusH. P. PengK. PetersJ. L. PingR. G. PingR. PolingE. PrencipeM. QiS. QianC. F. QiaoL. Q. QinX. S. QinY. QinZ. H. QinJ. F. QiuK. H. RashidG. RongX. D. RuanA. SarantsevB. D. SchaeferM. ShaoC. P. ShenX. Y. ShenH. Y. ShengM. R. ShepherdX. Y. SongS. SpataroB. SpruckD. H. SunG. X. SunJ. F. SunS. S. SunY. J. SunY. Z. SunZ. J. SunZ. T. SunC. J. TangX. TangI. TapanE. H. ThorndikeD. TothM. UllrichG. S. VarnerB. Q. WangD. WangD. Y. WangK. WangL. L. WangL. S. WangM. WangP. WangP. L. WangQ. J. WangS. G. WangX. F. WangX. L. WangY. F. WangZ. WangZ. G. WangZ. Y. WangD. H. WeiJ. B. WeiP. WeidenkaffQ. G. WenS. P. WenM. WernerU. WiednerL. H. WuN. WuS. X. WuW. WuZ. WuL. G. XiaZ. J. XiaoY. G. XieQ. L. XiuG. F. XuG. M. XuQ. J. XuQ. N. XuX. P. XuZ. R. XuF. XueZ. XueL. YanW. B. YanY. H. YanH. X. YangY. YangY. X. YangH. YeM. YeM. H. YeB. X. YuC. X. YuH. W. YuJ. S. YuS. P. YuC. Z. YuanY. YuanA. A. ZafarA. ZalloY. ZengB. X. ZhangB. Y. ZhangC. ZhangC. C. ZhangD. H. ZhangH. H. ZhangH. Y. ZhangJ. Q. ZhangJ. W. ZhangJ. Y. ZhangJ. Z. ZhangR. ZhangS. H. ZhangX. J. ZhangX. Y. ZhangY. ZhangY. H. ZhangZ. P. ZhangZ. Y. ZhangZhenghao ZhangG. ZhaoH. S. ZhaoJ. W. ZhaoK. X. ZhaoLei ZhaoLing ZhaoM. G. ZhaoQ. ZhaoQ. Z. ZhaoS. J. ZhaoT. C. ZhaoY. B. ZhaoZ. G. ZhaoA. ZhemchugovB. ZhengJ. P. ZhengY. H. ZhengB. ZhongZ. ZhongL. ZhouX. K. ZhouX. R. ZhouC. ZhuK. ZhuK. J. ZhuS. H. ZhuX. L. ZhuY. C. ZhuY. M. ZhuY. S. ZhuZ. A. ZhuJ. ZhuangB. S. ZouJ. H. Zou

Abstract

Using 106 ×106\times 10^{6} ψ′ψ^{\prime} decays collected with the BESIII detector at the BEPCII, three decays of χcJχ_{cJ} (J=0,1,2J=0,1,2) with baryon pairs ($\llb$, $\ssb$, $\SSB$) in the final state have been studied. The branching fractions are measured to be B\cal{B}(χc0,1,2→ΛΛˉ)=(33.3±2.0±2.6)×10−5(χ_{c0,1,2}\rightarrowΛ\barΛ) =(33.3 \pm 2.0 \pm 2.6)\times 10^{-5}, (12.2±1.1±1.1)×10−5(12.2 \pm 1.1 \pm 1.1)\times 10^{-5}, (20.8±1.6±2.3)×10−5(20.8 \pm 1.6 \pm 2.3)\times 10^{-5}; B\cal{B}(χc0,1,2→Σ0Σˉ0)(χ_{c0,1,2}\rightarrowΣ^{0}\barΣ^{0}) = (47.8±3.4±3.9)×10−5(47.8 \pm 3.4 \pm 3.9)\times 10^{-5}, (3.8±1.0±0.5)×10−5(3.8 \pm 1.0 \pm 0.5)\times 10^{-5}, (4.0±1.1±0.5)×10−5(4.0 \pm 1.1 \pm 0.5) \times 10^{-5}; and B\cal{B}(χc0,1,2→Σ+Σˉ−)(χ_{c0,1,2}\rightarrowΣ^{+}\barΣ^{-}) = (45.4±4.2±3.0)×10−5(45.4 \pm 4.2 \pm 3.0)\times 10^{-5}, (5.4±1.5±0.5)×10−5(5.4 \pm 1.5 \pm 0.5)\times 10^{-5}, (4.9±1.9±0.7)×10−5(4.9 \pm 1.9 \pm 0.7)\times 10^{-5}, where the first error is statistical and the second is systematic. Upper limits on the branching fractions for the decays of χc1,2→Σ0Σˉ0χ_{c1,2}\rightarrowΣ^{0}\barΣ^{0}, Σ+Σˉ−Σ^{+}\barΣ^{-}, are estimated to be B\cal{B}(χc1→Σ0Σˉ0)<6.2×10−5(χ_{c1}\rightarrowΣ^{0}\barΣ^{0}) < 6.2\times 10^{-5}, B\cal{B}(χc2→Σ0Σˉ0)<6.5×10−5(χ_{c2}\rightarrowΣ^{0}\barΣ^{0}) < 6.5\times 10^{-5}, B\cal{B}(χc1→Σ+Σˉ−)<8.7×10−5(χ_{c1}\rightarrowΣ^{+}\barΣ^{-}) < 8.7\times 10^{-5} and B\cal{B}(χc2→Σ+Σˉ−)<8.8×10−5(χ_{c2}\rightarrowΣ^{+}\barΣ^{-}) < 8.8\times 10^{-5} at the 90% confidence level.

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