6533b825fe1ef96bd1282857

RESEARCH PRODUCT

Measurements of baryon pair decays of chi(cJ) mesons

H. J. LuJ. G. LuY. J. MaoX. L. WangM. BertaniA. ZalloB. SpruckE. H. ThorndikeC. NicholsonM. UllrichM. L. ChenL. Q. QinY. DingZhiqiang LiuMiao HeYang QinY. F. LiangY. F. WangD. P. JinM. Y. DongXian ChenDayong WangP. L. LiuZhiqing LiuB. J. LiuY. H. GuanA. CalcaterraZ. G. ZhaoD. J. AmbroseJ. F. ChangF. E. MaasT. HuJ. P. DaiG. R. LuZ. P. ZhangS. QianJialun PingJifeng HuL. P. ZhouF. LiA. Q. GuoX. Y. MaG. R. LiaoF. F. JingC. L. MaW. X. GongL. HuangC. HuH. B. LiuX. CaiX. R. LiP. FriedelJ. H. ZouZ. A. ZhuX. Y. ZhangZ. P. MaoKe WangMichael WernerM. MaggioraLing ZhaoX. TangKai LiuC. GengZ. J. SunZujian WangK. GoetzenH. P. ChengH. LoehnerZ. Y. HeZ. L. HouD. X. LinYang YangQ. OuyangS. S. SunE. PrencipeW. KuehnR. PolingM. LeyheZ. H. QinZ. NingR. B. FerroliD. H. SunY. J. SunF. C. MaJ. FangY. ZhangW. GradlV. V. BytevChuan LiuD. Y. WangAlexey ZhemchugovH. M. HuC. H. LiS. S. FangY. NefedovM. H. GuFenfen AnX. K. ZhouQ. AnW. G. LiQ. M. MaX. H. MoL. S. WangY. B. LiuY. H. ZhengH. B. LiA. G. DenigC. L. LuoH. Y. ShengWei WuJürgen BeckerT. C. ZhaoM. H. YeS. SpataroX. P. XuC. ZhuW. D. LiCong-feng QiaoG. M. XuR. ZhangO. AlbayrakC. Z. YuanMeng WangN. Yu. MuchnoiR. E. MitchellY. B. ZhaoZhenghao ZhangC. C. ZhangGuangming HuangZ. WuP. L. WangC. X. YuC. S. JiK. J. ZhuH. H. LiuY. YuanX. T. LiaoB. ZhongL. B. GuoX. L. LuoFeng XueCui LiHeng-yun YeY. H. ZhangXuantong ZhangQ. G. WenH. M. LiuK. LiLei LiY. S. ZhuFang LiuX. LiuJ. MinL. L. WangH. B. LiuH. LiangZ. Y. WangB. ZhengR. G. PingG. F. CaoJ. F. QiuQ. P. JiZ. J. XiaoY. P. GuoI. DenysenkoL. L. JiangUlrich WiednerG. F. XuJ. W. ZhangChi ZhangXiangdong RuanQ. LiuS. H. ZhangX. Y. ShenT. GuoSerkant Ali CetinX. Q. LiM. GrecoH. X. YangB. KopfQiang ZhaoS. JinI. TapanXiao-tong LuQ. P. JiS. L. LiQ. A. MalikL. FavaLei ZhaoB. Y. ZhangC. J. TangM. H. YeQ. J. XuF. A. HarrisY. H. YanT. MaYanping HuangJ. B. JiaoY. P. LuX. T. HuangM. AblikimA. A. ZafarK. L. HeJ. W. ZhaoKai LiuG. RongX. N. LiHaiping PengHai YuD. Cronin-hennessyH. H. ZhangY. C. ZhuG. A. ChelkovX. Y. SongJ. P. LiuH. L. MaFeng LiuS. MaL. G. XiaD. M. LiTao LuoJ. V. BennettD. TothJ. G. MesschendorpH. MuramatsuL. Y. DongJ. C. LiY. L. HanQun-yao WangG. S. HuangQiunan XuN. WuKrisztian PetersW. B. YanShan WangB. X. YuM. N. AchasovSanfeng WuM. PelizaeusXuejun WangE. BogerT. HeldJ. ZhuangHongsheng ZhaoS. PacettiY. M. ZhuJ. S. HuangZ. A. LiuY. X. YangM. X. LuoJianping ZhengC. X. LiuJian WeiM. KornicerJ. Q. ZhangL. H. WuM. QiYucheng HuangD. V. DedovichK. Y. LiuM. R. ShepherdK. X. ZhaoW. M. DingM. LvZ. XueY. BanP. WeidenkaffQ. ZhaoI. B. NikolaevJoong-won ParkQ. L. XiuM. DestefanisM. DestefanisB. Q. WangY. Z. SunShou-hua ZhuG. S. VarnerY.n. GaoC. P. ShenK. H. RashidS. P. WenG. X. SunLi YanZhenli XuM. ShaoY. T. GuGang ZhaoZ. JiaoFu-hu LiuD. H. ZhangHang LiuJ. F. SunQ. J. LiS. L. OlsenRoy A. BriereB. S. ZouX. S. QinX. R. ZhouCheng LiH. S. ChenShujun ZhaoY. ZengY. T. LiangX. S. JiangZhe SunA. SarantsevD. H. WeiZ. B. LiS. B. LiuY. B. ChenXiaofeng ZhuJ. Z. ZhangJ. S. LangeM. KavatsyukO. CakirB. X. ZhangH. L. DaiIgor BoykoP. L. WangQi-wen LüX. L. JiS. P. YuTalib HussainY. G. XieS. X. DuS. J. ChenO. BondarenkoJ. M. BianZhenyu ZhangW. LaiJ. C. ChenNasser Kalantar-nayestanakiC. Morales MoralesZ. ZhongM. G. ZhaoZ. G. WangH. Y. ZhangG. F. ChenJ. Y. ZhangY. K. HengJie YuT. J. MinK. J. ZhuB. D. SchaeferG. LiC. D. FuC. Q. FengZ. Y. DengXingguo LiJ. Z. BaiY. P. ChuX. B. Ji

subject

BaryonPhysicsNuclear and High Energy PhysicsParticle physicsMesonBranching fractionPhysics - Data Analysis Statistics and ProbabilityAnalytical chemistrySigmaLambdaHigh Energy Physics - Experiment

description

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

10.1103/physrevd.87.032007https://hdl.handle.net/11370/38cc6ec9-58ba-470f-a7ff-13b9e2dc8d1f