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Study of the K+π+π- final state in B+→J/ψK+π+π- and B+→ψK+π+π -

  • H. Guler
  • , H. Aihara
  • , K. Arinstein
  • , V. Aulchenko
  • , T. Aushev
  • , A. M. Bakich
  • , V. Balagura
  • , E. Barberio
  • , K. Belous
  • , V. Bhardwaj
  • , M. Bischofberger
  • , A. Bozek
  • , M. Bračko
  • , T. E. Browder
  • , P. Chang
  • , Y. Chao
  • , A. Chen
  • , P. Chen
  • , B. G. Cheon
  • , K. Cho
  • S. K. Choi, Y. Choi, J. Dalseno, Z. Doležal, Z. Drásal, A. Drutskoy, W. Dungel, S. Eidelman, S. Esen, H. Ha, H. Hayashii, Y. Horii, Y. Hoshi, W. S. Hou, H. J. Hyun, K. Inami, R. Itoh, M. Iwabuchi, N. J. Joshi, T. Julius, J. H. Kang, N. Katayama, T. Kawasaki, H. J. Kim, H. O. Kim, J. H. Kim, M. J. Kim, Y. J. Kim, K. Kinoshita, B. R. Ko, P. Kodyš, P. Krokovny, T. Kumita, A. Kuzmin, Y. J. Kwon, S. H. Kyeong, M. J. Lee, S. H. Lee, J. Li, C. Liu, D. Liventsev, R. Louvot, J. MacNaughton, D. Marlow, A. Matyja, S. McOnie, K. Miyabayashi, H. Miyata, Y. Miyazaki, R. Mizuk, G. B. Mohanty, T. Mori, M. Nakao, Z. Natkaniec, S. Nishida, K. Nishimura, O. Nitoh, S. Ogawa, S. Okuno, S. L. Olsen, P. Pakhlov, C. W. Park, H. Park, H. K. Park, R. Pestotnik, M. Petrič, L. E. Piilonen, A. Poluektov, S. Ryu, H. Sahoo, Y. Sakai, O. Schneider, K. Senyo, M. E. Sevior, M. Shapkin, C. P. Shen, J. G. Shiu, P. Smerkol, S. Stanič, M. Starič, K. Sumisawa, T. Sumiyoshi, Y. Teramoto, K. Trabelsi, S. Uehara, Y. Unno, S. Uno, G. Varner, C. H. Wang, M. Z. Wang, M. Watanabe, Y. Watanabe, K. M. Williams, E. Won, Y. Yamashita, Z. P. Zhang, V. Zhilich, P. Zhou, V. Zhulanov, T. Zivko, A. Zupanc
  • University of Hawai'i at Mānoa
  • McGill University
  • University of Montreal
  • The University of Tokyo
  • RAS - Budker Institute of Nuclear Physics
  • Novosibirsk State University
  • Alikhanov Institute for Theoretical and Experimental Physics
  • Swiss Federal Institute of Technology Lausanne
  • The University of Sydney
  • University of Melbourne
  • Institute for High Energy Physics
  • Panjab University
  • Nara Women's University
  • H. Niewodniczanski Institute of Nuclear Physics
  • Jožef Stefan Institute
  • University of Maribor
  • National Taiwan University
  • National Central University
  • Hanyang 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
  • University of Cincinnati
  • Austrian Academy of Sciences
  • Korea University
  • Tohoku University
  • Tohoku Gakuin University
  • Kyungpook National University
  • Nagoya University
  • High Energy Accelerator Research Organization, Tsukuba
  • Yonsei University
  • Tata Institute of Fundamental Research
  • Niigata University
  • The Graduate University for Advanced Studies
  • Tokyo Metropolitan University
  • Seoul National University
  • University of Science and Technology of China
  • Princeton University
  • Tokyo University of Agriculture and Technology
  • Toho University
  • Kanagawa University
  • Virginia Polytechnic Institute and State University
  • University of Nova Gorica
  • Osaka Metropolitan University
  • National United University Taiwan
  • Nippon Dental University
  • Wayne State University
  • Karlsruhe Institute of Technology

Research output: Contribution to journalArticlepeer-review

32 Scopus citations

Abstract

Using 535×106 B-meson pairs collected by the Belle detector at the KEKB e+e- collider, we measure branching fractions of (7.16±0.10(stat)±0.60(syst)×10-4 for B +→J/ψK+π+π- and (4.31±0.20(stat)±0.50(syst))×10-4 for B +→ψK+π+π -. We perform amplitude analyses to determine the resonant structure of the K+π+π- final state in B +→J/ψK+π+π- and B+→ψK+π+π - and find that the K1(1270) is a prominent component of both decay modes. There is significant interference among the different intermediate states, which leads, in particular, to a striking distortion of the ρ line shape due to the ω. Based on the results of the fit to the B+→J/ψK+π+π- data, the relative decay fractions of the K1(1270) to Kρ, Kω, and K*(892)π are consistent with previous measurements, but the decay fraction to K0*(1430) is significantly smaller. Finally, by floating the mass and width of the K1(1270) in an additional fit of the B+→J/ψK+π+π- data, we measure a mass of (1248.1±3.3(stat)±1.4(syst))MeV/c2 and a width of (119.5±5.2(stat)±6.7(syst))MeV/c2 for the K 1(1270).

Original languageEnglish
Article number032005
JournalPhysical Review D - Particles, Fields, Gravitation and Cosmology
Volume83
Issue number3
DOIs
StatePublished - 3 Feb 2011

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