Skip to main navigation Skip to search Skip to main content

Observation of ψ(4040) and ψ(4160) decay into ηj/ψ

  • X. L. Wang
  • , Y. L. Han
  • , C. Z. Yuan
  • , C. P. Shen
  • , P. Wang
  • , I. Adachi
  • , H. Aihara
  • , D. M. Asner
  • , V. Aulchenko
  • , T. Aushev
  • , T. Aziz
  • , A. M. Bakich
  • , Y. Ban
  • , B. Bhuyan
  • , G. Bonvicini
  • , A. Bozek
  • , M. Bračko
  • , J. Brodzicka
  • , O. Brovchenko
  • , T. E. Browder
  • P. Chen, B. G. Cheon, K. Cho, S. K. Choi, Y. Choi, J. Dalseno, Z. Doležal, Z. Drásal, S. Eidelman, S. Esen, H. Farhat, J. E. Fast, V. Gaur, R. Gillard, Y. M. Goh, B. Golob, H. Hayashii, Y. Hoshi, W. S. Hou, H. J. Hyun, K. Inami, A. Ishikawa, M. Iwabuchi, J. H. Kang, P. Kapusta, H. J. Kim, H. O. Kim, J. B. Kim, J. H. Kim, M. J. Kim, Y. J. Kim, K. Kinoshita, J. Klucar, B. R. Ko, P. Kodyš, R. T. Kouzes, P. Križan, P. Krokovny, T. Kumita, J. S. Lange, S. H. Lee, J. Li, J. Libby, C. Liu, Z. Q. Liu, P. Lukin, S. McOnie, H. Miyata, R. Mizuk, G. B. Mohanty, A. Moll, N. Muramatsu, R. Mussa, M. Nakao, S. Nishida, O. Nitoh, S. Ogawa, T. Ohshima, S. Okuno, S. L. Olsen, G. Pakhlova, H. Park, T. K. Pedlar, R. Pestotnik, M. Petrič, L. E. Piilonen, K. Prothmann, H. Sahoo, Y. Sakai, S. Sandilya, D. Santel, T. Sanuki, O. Schneider, C. Schwanda, K. Senyo, M. E. Sevior, M. Shapkin, T. A. Shibata, J. G. Shiu, A. Sibidanov, F. Simon, P. Smerkol, Y. S. Sohn, E. Solovieva, S. Stanič, M. Starič, T. Sumiyoshi, K. Tanida, G. Tatishvili, Y. Teramoto, K. Trabelsi, M. Uchida, S. Uehara, Y. Unno, S. Uno, Y. Usov, P. Vanhoefer, G. Varner, C. H. Wang, J. Wang, M. Z. Wang, K. M. Williams, E. Won, Y. Yamashita, C. C. Zhang, Z. P. Zhang, V. Zhilich, A. Zupanc
  • CAS - Institute of High Energy Physics
  • Virginia Polytechnic Institute and State University
  • Nagoya University
  • High Energy Accelerator Research Organization, Tsukuba
  • The University of Tokyo
  • Pacific Northwest National Laboratory
  • Novosibirsk State University
  • Alikhanov Institute for Theoretical and Experimental Physics
  • Tata Institute of Fundamental Research
  • The University of Sydney
  • Peking University
  • Indian Institute of Technology Guwahati
  • Wayne State University
  • H. Niewodniczanski Institute of Nuclear Physics
  • Jožef Stefan Institute
  • University of Maribor
  • Karlsruhe Institute of Technology
  • University of Hawai'i at Mānoa
  • National Taiwan 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
  • University of Ljubljana
  • Nara Women's University
  • Tohoku Gakuin University
  • Kyungpook National University
  • Tohoku University
  • Yonsei University
  • Korea University
  • Tokyo Metropolitan University
  • Justus Liebig University Giessen
  • Seoul National University
  • Indian Institute of Technology Madras
  • University of Science and Technology of China
  • Niigata University
  • National Institute for Nuclear Physics
  • Tokyo University of Agriculture and Technology
  • Toho University
  • Kanagawa University
  • Luther College, Decorah
  • Swiss Federal Institute of Technology Lausanne
  • Austrian Academy of Sciences
  • Yamagata University
  • University of Melbourne
  • Institute for High Energy Physics
  • Institute of Science Tokyo
  • University of Nova Gorica
  • Osaka Metropolitan University
  • National United University Taiwan
  • Nippon Dental University

Research output: Contribution to journalArticlepeer-review

67 Scopus citations

Abstract

The cross section for e+e-→ηJ/ψ between √s=3.8 GeV and 5.3 GeV is measured via initial state radiation using 980 fb-1 of data on and around the Υ(nS)(n=1,2,3,4,5) resonances collected with the Belle detector at KEKB. Two resonant structures at the ψ(4040) and ψ(4160) are observed in the ηJ/ψ invariant mass distribution. Fitting the mass spectrum with the coherent sum of two Breit-Wigner functions, one obtains B(ψ(4040)→ηJ/ψ) ·Γe+e-ψ(4040)=(4.8±0.9±1.5) eV and B(ψ(4160)→ηJ/ψ)·Γe+e -ψ(4160)=(4.0±0.8±1.4) eV for one solution and B(ψ(4040)→ηJ/ψ)·Γe+e -ψ(4040)=(11.2±1.3±2.1) eV and B(ψ(4160) →ηJ/ψ)·Γe+e-ψ(4160)=(13. 8±1.3±2.1) eV for the other solution, where the first errors are statistical and the second are systematic. This is the first measurement of this hadronic transition mode of these two states, and the partial widths to ηJ/ψ are found to be about 1 MeV. There is no evidence for the Y(4260), Y(4360), ψ(4415), or Y(4660) in the ηJ/ψ final state, and upper limits of their production rates in e+e- annihilation are determined.

Original languageEnglish
Article number051101
JournalPhysical Review D - Particles, Fields, Gravitation and Cosmology
Volume87
Issue number5
DOIs
StatePublished - 20 Mar 2013

Fingerprint

Dive into the research topics of 'Observation of ψ(4040) and ψ(4160) decay into ηj/ψ'. Together they form a unique fingerprint.

Cite this