Search for XYZ states in Upsilon(1S) inclusive decays

Belle Collaboration: C. P. Shen , C. Z. Yuan , Y. Ban , H. Aihara , D. M. Asner , I. Badhrees , A. M. Bakich , E. Barberio

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P. Behera V. Bhardwaj B. Bhuyan J. Biswal A. Bondar G. Bonvicini A. Bozek M. Bra\v{c}ko T. E. Browder D. \v{C}ervenkov V. Chekelian A. Chen K. Chilikin R. Chistov K. Cho V. Chobanova S.-K. Choi Y. Choi D. Cinabro J. Dalseno M. Danilov N. Dash S. Di Carlo Z. Dole\v{z}al Z. Dr\'asal D. Dutta S. Eidelman H. Farhat J. E. Fast T. Ferber B. G. Fulsom V. Gaur N. Gabyshev A. Garmash P. Goldenzweig J. Haba K. Hayasaka H. Hayashii W.-S. Hou T. Iijima G. Inguglia A. Ishikawa R. Itoh W. W. Jacobs H. B. Jeon K. K. Joo T. Julius K. H. Kang D. Y. Kim J. B. Kim K. T. Kim S. H. Kim Y. J. Kim K. Kinoshita P. Kody\v{s} S. Korpar D. Kotchetkov P. Kri\v{z}an P. Krokovny T. Kuhr A. Kuzmin Y.-J. Kwon J. S. Lange C. H. Li H. Li L. Li Y. Li L. Li Gioi J. Libby D. Liventsev T. Luo M. Masuda T. Matsuda D. Matvienko A. Moll H. K. Moon R. Mussa M. Nakao T. Nanut K. J. Nath Z. Natkaniec M. Nayak K. Negishi S. Nishida S. Ogawa S. Okuno S. L. Olsen P. Pakhlov G. Pakhlova B. Pal R. Pestotnik M. Petri\v{c} L. E. Piilonen C. Pulvermacher M. Ritter A. Rostomyan Y. Sakai S. Sandilya L. Santelj T. Sanuki V. Savinov T. Schl\"uter O. Schneider G. Schnell C. Schwanda Y. Seino K. Senyo O. Seon I. S. Seong M. E. Sevior T.-A. Shibata J.-G. Shiu F. Simon A. Sokolov E. Solovieva M. Stari\v{c} T. Sumiyoshi M. Takizawa K. Tanida F. Tenchini K. Trabelsi M. Uchida T. Uglov Y. Unno S. Uno G. Varner A. Vinokurova V. Vorobyev C. H. Wang M.-Z. Wang P. Wang X. L. Wang M. Watanabe Y. Watanabe K. M. Williams E. Won J. Yamaoka S. D. Yang S. Yashchenko Y. Yook Y. Yusa Z. P. Zhang V. Zhilich V. Zhukova V. Zhulanov A. Zupanc

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classification ✦ hep-ex hep-ph

keywords upsilondecaysmathrmstatesinclusiveanythingdecaysearch

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The branching fractions of the $\Upsilon(1S)$ inclusive decays into final states with a $J/\psi$ or a $\psi(2S)$ are measured with improved precision to be $\BR(\Upsilon(1S)\to J/\psi + {\rm anything})=(5.25\pm 0.13(\mathrm{stat.})\pm 0.25(\mathrm{syst.}))\times 10^{-4}$ and $\BR(\Upsilon(1S)\to \psi(2S) + {\rm anything})=(1.23\pm 0.17(\mathrm{stat.})\pm 0.11(\mathrm{syst.}))\times 10^{-4}$. The first search for $\Upsilon(1S)$ decays into $XYZ$ states that decay into a $J/\psi$ or a $\psi(2S)$ plus one or two charged tracks yields no significant signals for $XYZ$ states in any of the examined decay modes, and upper limits on their production rates in $\Upsilon(1S)$ inclusive decays are determined.

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Search for XYZ states in Upsilon(1S) inclusive decays

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