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)

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Abstract
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)%.
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Key words
Belle experiment,Branching fraction,KEKB,Electron–positron annihilation,Hadron,Hyperfine structure,Analytical chemistry,Physics
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