6533b827fe1ef96bd12863bf
RESEARCH PRODUCT
Search for baryonic decays ofψ(3770)andψ(4040)
M. BertaniY. L. HanG. R. LiaoHongsheng ZhaoS. L. OlsenRoy A. BriereQ. P. JiK. GoetzenW. KuehnR. PolingF. F. JingW. GradlJianping ZhengP. L. WangX. S. JiangQi-wen LüM. LvM. QiS. H. ZhangX. Y. ShenZ. XueY. X. YangD. J. AmbroseA. ZalloH. X. YangQ. OuyangO. CakirYang QinFeng LiuX. L. WangQ. M. MaF. LiF. C. MaY. X. XiaE. PrencipeZ. P. ZhangS. S. FangShan WangY. DingTao LuoJ. V. BennettM. G. ZhaoS. B. LiuB. J. LiuM. R. ShepherdZujian WangHuihui LiuJ. P. LiuY. T. LiangY. YuanY. S. ZhuG. R. LuM. L. ChenC. S. JiW. D. LiX. Q. LiJ. F. QiuQ. ZhaoM. GrecoX. H. MoL. S. WangL. FavaZ. G. ZhaoJ. G. MesschendorpZ. B. LiZ. A. ZhuB. X. YuX. H. ZhaoXiangdong RuanChi ZhangH. LiangM. H. YeFeng XueCui LiY. Z. SunQ. LiuY. B. LiuGuangshun HuangQiunan XuQ. P. JiM. KavatsyukK. LiY. D. WangD. H. SunG. S. VarnerL. HuangHang LiuW. G. LiX. T. HuangXiang ZhouKai LiuK. Y. LiuY. B. ZhaoI. TapanS. L. LiY. H. YanFang LiuJ. W. ZhaoK. X. ZhaoL. G. XiaX. P. XuX. P. XuH. S. ChenShujun ZhaoJ. M. BianJ. Q. ZhangL. L. JiangL. L. WangP. LarinH. CaiM. AblikimA. A. ZafarG. RongZ. J. SunB. X. ZhangJ. Z. BaiD. Cronin-hennessyY. C. ZhuS. SpataroC. ZhuGang ZhaoY. J. MaoH. L. DaiIgor BoykoZhenyu ZhangY. Q. WangN. WuW. LaiI. DenysenkoH. LoehnerY. F. WangY. NefedovKrisztian PetersC. J. TangM. KornicerY. M. ZhuY. P. LuF. A. HarrisI. B. NikolaevX. L. JiS. P. YuK. H. RashidX. T. LiaoE. BogerH. B. LiA. G. DenigC. L. LuoH. M. LiuH. J. LuJ. G. LuH. H. ZhangG. A. ChelkovZhiqing LiuTalib HussainT. HeldX. Y. MaH. MoeiniZhiqiang LiuMiao HeY. F. LiangW. X. GongD. P. JinR. Baldini FerroliM. ShaoY. T. GuD. X. LinP. FriedelC. C. ZhangJifeng HuB. ZhongL. B. GuoAlexey ZhemchugovH. M. HuQ. J. XuB. Q. WangC. P. ShenQ. L. XiuF. E. MaasB. Y. ZhangJ. F. ChangT. HuQ. J. LiG. F. CaoL. P. ZhouLei LiY. G. XieJ. C. ChenXuanhong LouUlrich WiednerY. N. GaoY. ZhangQ. AnZ. P. MaoS. L. ZangP. L. WangMichael WernerA. Q. GuoJ. W. ZhangJ. F. SunX. CaiX. N. LiX. R. LiC. H. LiS. X. DuNasser Kalantar-nayestanakiH. P. ChengJ. FangT. MaYanping HuangX. L. LuoDayong WangP. L. LiuHaiping PengHai YuG. X. SunLi YanQun-yao WangS. J. ChenWei WuY. ZengGuangming HuangO. BondarenkoA. SarantsevD. H. WeiJ. S. LangeZ. NingA. CalcaterraA. CalcaterraZ. WuM. H. YeM. MaggioraLing ZhaoJ. C. LiZ. JiaoFu-hu LiuD. H. ZhangKe WangZhe SunW. M. SongC. Morales MoralesI. UmanC. NicholsonY. H. GuanX. K. ZhouJ. ZhuangM. X. LuoLei ZhaoLili ZhangZ. Y. HeZ. L. HouXiao-tong LuShou-hua ZhuYang YangY. B. ChenD. Y. WangXiaofeng ZhuJ. Z. ZhangY. P. ChuL. Y. DongJian WeiV. V. BytevL. H. WuYucheng HuangD. V. DedovichFenfen AnM. LeyheZ. H. QinM. UllrichB. S. ZouX. B. JiChuan LiuW. M. DingZ. G. WangT. C. ZhaoH. Y. ZhangH. L. MaD. M. LiZhenli XuH. MuramatsuRui ZhangM. PelizaeusZhenghao ZhangW. B. YanG. F. ChenM. H. GuJ. Y. ZhangM. N. AchasovH. Y. ShengG. LiS. PacettiC. D. FuC. Q. FengC. X. YuZ. Y. DengXingguo LiXiao Dong ChenJie YuB. ZhengT. J. MinK. J. ZhuB. D. SchaeferB. SpruckE. H. ThorndikeR. G. PingL. Q. QinM. Y. DongZ. A. LiuJ. P. DaiH. B. LiuC. L. MaY. BanP. WeidenkaffJ. H. ZouO. FuksS. S. SunS. P. WenJürgen BeckerX. S. QinX. R. ZhouR. E. MitchellJ. L. FuCheng LiC. GengG. F. XuY. H. ZhengCong-feng QiaoS. JinO. AlbayrakX. Y. SongS. MaD. TothN. Yu. MuchnoiSanfeng WuJ. S. HuangC. X. LiuHeng-yun YeY. H. ZhangG. M. XuC. Z. YuanQ. G. WenZ. Y. WangX. LiuZ. J. XiaoY. P. GuoT. GuoSerkant Ali CetinS. QianJialun PingX. Y. ZhangY. J. SunJ. B. JiaoM. DestefanisQ. A. MalikY. K. HengXuejun WangC. HuX. TangJ. MinH. B. LiuB. KopfK. J. ZhuK. L. HeM. Z. WangXuantong ZhangK. Moriyasubject
PhysicsNuclear physicsBaryonNuclear and High Energy PhysicsParticle physicsBranching fractionElectron–positron annihilationSigmaHigh Energy Physics::ExperimentLambdaBar (unit)description
By analyzing data samples of 2.9 fb(-1) collected at root s = 3.773 GeV, 482 pb(-1) collected at root s = 4.009 GeV and 67 pb(-1) collected at root s = 3.542, 3.554, 3.561, 3.600 and 3.650 GeV with the BESIII detector at the BEPCII storage ring, we search for psi(3770) and psi(4040) decay to baryonic final states, including Lambda(Lambda) over bar pi(+)pi(-), Lambda(Lambda) over bar pi(0), Lambda(Lambda) over bar eta , Sigma(0)(Sigma) over bar (0) and Xi(0) (Xi) over bar (0) decays. None are observed, and upper limits are set at the 90% confidence level.
year | journal | country | edition | language |
---|---|---|---|---|
2013-06-21 | Physical Review D |