First observation of the hadronic transition $ \Upsilon(4S) \to \eta h_{b}(1P)$ and new measurement of the $h_b(1P)$ and $\eta_b(1S)$ parameters

U. Tamponi, M. Staric, Z.P. Zhang,D. Epifanov,H. Kichimi, C.P. Shen, R. Pestotnik,S.L. Olsen, K. Hayasaka,P. Lukin,T. Uglov, E. Won,D. Matvienko,Y. Choi, S.H. Kim,I. Jaegle,H. Park,M.N. Wagner,S. Okuno,M. Ritter,G.B. Mohanty,K. Cho,B.G. Cheon,B. Golob,K. Arinstein,T. Iijima, A. Ishikawa,J.S. Lange,A. Bozek, S. Yashchenko,J. Biswal,J. Libby,Y. Watanabe,K. Inami,J.E. Fast, L. Santelj, G. Varner, P. Vanhoefer,V. Zhilich,H. Hayashii,S. Uno,X.H. He, Y. Sakai,J. Haba,S. Korpar, M. Petric,N.K. Nisar,S. Ogawa,P. Katrenko,T. Julius,T. Aushev, A. Rostomyan,G. Bonvicini,R. Mizuk, L.E. Piilonen,D.Y. Kim, T.K. Pedlar,B.G. Fulsom,W. Ostrowicz,P. Krizan, O. Schneider,M. Bracko,H. Farhat,Z. Natkaniec,A. Moll,K. Kinoshita,M.T. Hedges, M.Z. Wang,H. Atmacan, M.E. Sevior,V. Bhardwaj,T.A. Shibata,H. Miyata, M. Shapkin,P. Lewis, Y. Unno, Y.S. Sohn,T. Mori, K.M. Williams,D. Getzkow,C. Oswald,D. Cinabro,T. Ferber,E. Barberio,M. Nayak, M. Steder,R. Gillard,S. Eidelman,P. Kodys,A. Abdesselam, V. Zhulanov,R. Mussa,R. Ayad,M. Nakao, C. Schwanda,H. Aihara, H.J. Kim,X.L. Wang, T. Sanuki,Y. Teramoto, A. Vinokurova,A. Chen,V. Chobanova,T.E. Browder, K. Tanida,N. Gabyshev,W.S. Hou,A. Drutskoy,P. Krokovny,D.M. Asner, J. Stypula, J.H. Kim,J. Yamaoka, Y. Sato,D. Cervenkov,L. Pesantez,F. Simon, K. Senyo, D. Semmler,Y.M. Goh, V. Shebalin,S. Ryu,V. Gaur,A. Bondar,S.K. Choi,A. Vossen,K.T. Kim,C. Van Hulse, A. Sibidanov,K. Miyabayashi,B. Bhuyan,Z. Dolezal, J.G. Shiu, A. Zupanc, G. Schnell,M. Danilov,A. Sokolov, K. Trabelsi,I. Badhrees, E. Ribezl, V. Savinov, P. Urquijo,A. Kuzmin,Z. Drasal,E. Kato,D. Joffe,T. Kumita,E. Nakano,G. Pakhlova,S. Nishida, S. Sandilya, B. Shwartz,T. Nanut,A. Garmash,A.M. Bakich,C. Kiesling,B. Pal,M. Uchida

user-5f8411ab4c775e9685ff56d3(2015)

引用 21|浏览5
暂无评分
摘要
Using a sample of 771.6×106 ϒϒ(4S) decays collected by the Belle experiment at the KEKB e+e- collider, we observe, for the first time, the transition ϒ(4S)→ηhb(1P) with the branching fraction B[ϒ(4S)→ηhb(1P)]=(2.18±0.11±0.18)×10-3 and we measure the hb(1P) mass Mhb(1P)=(9899.3±0.4±1.0)  MeV/c2, corresponding to the hyperfine (HF) splitting ΔMHF(1P)=(0.6±0.4±1.0)  MeV/c2. Using the transition hb(1P)→γηb(1S), we measure the ηb(1S) mass Mηb(1S)=(9400.7±1.7±1.6)  MeV/c2, corresponding to ΔMHF(1S)=(59.6±1.7±1.6)  MeV/c2, the ηb(1S) width Γηb(1S)=(8-5+6±5)  MeV/c2 and the branching fraction B[hb(1P)→γηb(1S)]=(56±8±4)%.
更多
查看译文
关键词
Belle experiment,Branching fraction,KEKB,Electron–positron annihilation,Hadron,Hyperfine structure,Analytical chemistry,Physics
AI 理解论文
溯源树
样例
生成溯源树,研究论文发展脉络
Chat Paper
正在生成论文摘要