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Observation of Two Charged Bottomoniumlike Resonances inΥ(5S)Decays

Authors
A. Bondar,A. Garmash
R. Mizuk,D. Santel,K. Kinoshita,I. Adachi,H. Aihara,K. Arinstein,D. Asner,T. Aushev,T. Aziz,E. Banaś,E. Barberio,K. Belous,V. Bhardwaj,M. Bischofberger,T. Browder,M. Bračko,P. Chang,A Chen,K. Chilikin,R. Chistov,I-S Cho,K Cho,S. Choi,Y. Choi,J. Dalseno,M. Danilov,Z. Doležal,L. Dong,D. Epifanov,J. Fast,V. Gaur,N. Gabyshev,Y. Goh,B. Golob,J. Haba,M. Różańska,K. Hayasaka,Y. Hoshi,H. Hyun,T. Iijima,K. Inami,A. Ishikawa,M. Iwabuchi,M. Yamauchi,T. Iwashita,T. Julius,P. Kapusta,T. Kawasaki,H. Kichimi,C. Kiesling,J Kim,J. Kim,K Kim,M Kim,Younghun Kim,T. Kobayashi,S. Yang,B. Grube,P. Kodyš,S. Korpar,P. Krokovny,T. Kuhr,R. Kumar,T. Kumita,A. Kuzmin,J. Lange,Soohyung Lee,J Li,Y. Li,J. Libby,C Liu,Z Liu,D. Liventsev,R. Louvot,D. Matvienko,S. McOnie,K. Miyabayashi,G. Mitselmakher,S. Nishida,A. Moll,N. Muramatsu,R. Mussa,J. Nielsen,M. Niiyama,K. Nishimura,O. Nitoh,T. Nozaki,S. Olsen,Y. Onuki,P. Pakhlov,H. Park,H Park,T. Pedlar,M. Petrič,L. Piilonen,A. Poluektov,M. Prim,M. Ritter,M. Röhrken,H. Russell,H. Sahoo,Y. Sakai,T. Sanuki,O. Schneider,C. Schwanda,K. Senyo,M. Sevior,M. Shapkin,T. Peitzmann,J.-G. Shiu,B. Shwartz,F. Simon,P. Smerkol,Y-S Sohn,A. Sokolov,E. Solovieva,M. Starič,M. Sumihama,T. Sumiyoshi,S. Tanaka,Y. Teramoto,M. Uchida,S. Uehara,T. Uglov,P. Urquijo,G. Varner,A. Vinokurova,C Wang,M.-Z. Wang,P Wang,X Wang,B. Yabsley,K. Williams,E. Won,Y. Yamashita,C. Yuan,Y. Yusa,Z Zhang,J. Zhong,K. Sumisawa,A. Zupanc,O. Zyukova,Zdeněk Doležal,S. Eidelman,Naomi Kolk,B. Ko,Peter Kodyš
+147 authors
,Guenakh Mitselmakher
Published
Mar 20, 2012
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Abstract

We report the observation of two narrow structures in the mass spectra of the ${\ensuremath{\pi}}^{\ifmmode\pm\else\textpm\fi{}}\ensuremath{\Upsilon}(nS)$ ($n=1$, 2, 3) and ${\ensuremath{\pi}}^{\ifmmode\pm\else\textpm\fi{}}{h}_{b}(mP)$ ($m=1$, 2) pairs that are produced in association with a single charged pion in $\ensuremath{\Upsilon}(5S)$ decays. The measured masses and widths of the two structures averaged over the five final states are ${M}_{1}=(10\text{ }607.2\ifmmode\pm\else\textpm\fi{}2.0)\text{ }\text{ }\mathrm{MeV}/{c}^{2}$, ${\ensuremath{\Gamma}}_{1}=(18.4\ifmmode\pm\else\textpm\fi{}2.4)\text{ }\text{ }\mathrm{MeV}$, and ${M}_{2}=(10\text{ }652.2\ifmmode\pm\else\textpm\fi{}1.5)\text{ }\text{ }\mathrm{MeV}/{c}^{2}$, ${\ensuremath{\Gamma}}_{2}=(11.5\ifmmode\pm\else\textpm\fi{}2.2)\text{ }\text{ }\mathrm{MeV}$. The results are obtained with a $121.4\text{ }\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ data sample collected with the Belle detector in the vicinity of the $\ensuremath{\Upsilon}(5S)$ resonance at the KEKB asymmetric-energy ${e}^{+}{e}^{\ensuremath{-}}$ collider.

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