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Observation of exclusive Υ(1S) and Υ(2S) decays into light hadrons

  • C. P. Shen
  • , C. Z. Yuan
  • , T. Iijima
  • , I. Adachi
  • , H. Aihara
  • , D. M. Asner
  • , T. Aushev
  • , A. M. Bakich
  • , A. Bay
  • , K. Belous
  • , B. Bhuyan
  • , M. Bischofberger
  • , G. Bonvicini
  • , A. Bozek
  • , M. Bračko
  • , T. E. Browder
  • , M. C. Chang
  • , P. Chang
  • , A. Chen
  • , P. Chen
  • B. G. Cheon, K. Chilikin, R. Chistov, I. S. Cho, K. Cho, S. K. Choi, Y. Choi, J. Dalseno, Z. Doleåal, Z. Drásal, S. Eidelman, J. E. Fast, V. Gaur, N. Gabyshev, Y. M. Goh, B. Golob, J. Haba, H. Hayashii, Y. Horii, Y. Hoshi, W. S. Hou, Y. B. Hsiung, H. J. Hyun, K. Inami, A. Ishikawa, R. Itoh, M. Iwabuchi, Y. Iwasaki, T. Iwashita, T. Julius, J. H. Kang, T. Kawasaki, C. Kiesling, B. H. Kim, H. O. Kim, J. B. Kim, J. H. Kim, M. J. Kim, Y. J. Kim, K. Kinoshita, B. R. Ko, S. Koblitz, P. Kodyå, S. Korpar, R. T. Kouzes, P. Kriåan, P. Krokovny, R. Kumar, T. Kumita, A. Kuzmin, Y. J. Kwon, S. H. Lee, J. Li, Y. Li, J. Libby, C. Liu, Y. Liu, Z. Q. Liu, R. Louvot, S. McOnie, K. Miyabayashi, H. Miyata, G. B. Mohanty, D. Mohapatra, A. Moll, N. Muramatsu, E. Nakano, M. Nakao, Z. Natkaniec, S. Nishida, K. Nishimura, O. Nitoh, S. Ogawa, T. Ohshima, S. Okuno, S. L. Olsen, P. Pakhlov, G. Pakhlova, C. W. Park, H. Park, H. K. Park, T. K. Pedlar, R. Pestotnik, M. Petrič, L. E. Piilonen, M. Ritter, H. Sahoo, Y. Sakai, D. Santel, T. Sanuki, Y. Sato, O. Schneider, C. Schwanda, K. Senyo, O. Seon, M. E. Sevior, M. Shapkin, V. Shebalin, T. A. Shibata, J. G. Shiu, B. Shwartz, A. Sibidanov, F. Simon, P. Smerkol, Y. S. Sohn, A. Sokolov, E. Solovieva, M. Starič, M. Sumihama, T. Sumiyoshi, G. Tatishvili, Y. Teramoto, M. Uchida, S. Uehara, T. Uglov, Y. Unno, S. Uno, P. Urquijo, Y. Usov, P. Vanhoefer, G. Varner, C. H. Wang, P. Wang, X. L. Wang, M. Watanabe, Y. Watanabe, K. M. Williams, E. Won, B. D. Yabsley, Y. Yamashita, C. C. Zhang, Z. P. Zhang, V. Zhilich, V. Zhulanov, A. Zupanc
  • Nagoya University
  • CAS - Institute of High Energy Physics
  • High Energy Accelerator Research Organization, Tsukuba
  • The University of Tokyo
  • Pacific Northwest National Laboratory
  • Alikhanov Institute for Theoretical and Experimental Physics
  • The University of Sydney
  • Swiss Federal Institute of Technology Lausanne
  • Institute for High Energy Physics
  • Indian Institute of Technology Guwahati
  • Nara Women's University
  • Wayne State University
  • H. Niewodniczanski Institute of Nuclear Physics
  • Jožef Stefan Institute
  • University of Maribor
  • University of Hawai'i at Mānoa
  • Fu Jen Catholic University
  • National Taiwan University
  • National Central University
  • Hanyang University
  • Yonsei University
  • Korea Institute of Science and Technology Information
  • Gyeongsang National University
  • Sungkyunkwan University
  • Max Planck Institute for Physics (Werner Heisenberg Institute)
  • Technische Universität München
  • Charles University
  • Novosibirsk State University
  • Tata Institute of Fundamental Research
  • University of Ljubljana
  • Tohoku Gakuin University
  • Kyungpook National University
  • Tohoku University
  • University of Melbourne
  • Niigata University
  • Seoul National University
  • Korea University
  • University of Cincinnati
  • Panjab University
  • Tokyo Metropolitan University
  • Virginia Polytechnic Institute and State University
  • Indian Institute of Technology Madras
  • University of Science and Technology of China
  • Osaka Metropolitan University
  • Tokyo University of Agriculture and Technology
  • Toho University
  • Kanagawa University
  • Luther College, Decorah
  • Austrian Academy of Sciences
  • Yamagata University
  • Institute of Science Tokyo
  • Gifu University
  • University of Bonn
  • National United University Taiwan
  • Nippon Dental University
  • Karlsruhe Institute of Technology

Research output: Contribution to journalArticlepeer-review

14 Scopus citations

Abstract

Using samples of 102×106 Υ(1S) and 158×106 Υ(2S) events collected with the Belle detector, we study exclusive hadronic decays of these two bottomonium resonances to the three-body final states Ï•K +K -, ωπ +π - and K *0(892)K -π +, and to the two-body Vector-Tensor states (Ï•f2′(1525), ωf 2(1270), ρa 2(1320) and K *0(892)K̄2*0(1430)) and Axial-vector-Pseudoscalar (K 1(1270) +K -, K 1(1400) +K - and b 1(1235) +π -) states. Signals are observed for the first time in the Υ(1S)→Ï•K +K -, ωπ +π -, K *0K -π +, K *0K2*0 and Υ(2S)→Ï•K +K -, K *0K -π + decay modes. Branching fractions are determined for all the processes, while 90% confidence level upper limits are established on the branching fractions for the modes with a statistical significance less than 3σ. The ratios of the branching fractions of Υ(2S) and Υ(1S) decays into the same final state are used to test a perturbative QCD prediction for OZI-suppressed bottomonium decays.

Original languageEnglish
Article number031102
JournalPhysical Review D - Particles, Fields, Gravitation and Cosmology
Volume86
Issue number3
DOIs
StatePublished - 15 Aug 2012

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