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Observation of psi(4040) and psi(4160) decay into eta J/psi

Authors
Wang, X. L.Han, Y. L.Yuan, C. Z.Shen, C. P.Wang, P.Adachi, I.Aihara, H.Asner, D. M.Aulchenko, V.Aushev, T.Aziz, T.Bakich, A. M.Ban, Y.Bhuyan, B.Bonvicini, G.Bozek, A.Bracko, M.Brodzicka, J.Brovchenko, O.Browder, T. E.Chen, P.Cheon, B. G.Cho, K.Choi, S. -K.Choi, Y.Dalseno, J.Dolezal, Z.Drasal, Z.Eidelman, S.Esen, S.Farhat, H.Fast, J. E.Gaur, V.Gillard, R.Goh, Y. M.Golob, B.Hayashii, H.Hoshi, Y.Hou, W. -S.Hyun, H. J.Inami, K.Ishikawa, A.Iwabuchi, M.Kang, J. H.Kapusta, P.Kim, H. J.Kim, H. O.Kim, J. B.Kim, J. H.Kim, M. J.Kim, Y. J.Kinoshita, K.Klucar, J.Ko, B. R.Kodys, P.Kouzes, R. T.Krizan, P.Krokovny, P.Kumita, T.Lange, J. S.Lee, S. -H.Li, J.Libby, J.Liu, C.Liu, Z. Q.Lukin, P.McOnie, S.Miyata, H.Mizuk, R.Mohanty, G. B.Moll, A.Muramatsu, N.Mussa, R.Nakao, M.Nishida, S.Nitoh, O.Ogawa, S.Ohshima, T.Okuno, S.Olsen, S. L.Pakhlova, G.Park, H.Pedlar, T. K.Pestotnik, R.Petric, M.Piilonen, L. E.Prothmann, K.Sahoo, H.Sakai, Y.Sandilya, S.Santel, D.Sanuki, T.Schneider, O.Schwanda, C.Senyo, K.Sevior, M. E.Shapkin, M.Shibata, T. -A.Shiu, J. -G.Sibidanov, A.Simon, F.Smerkol, P.Sohn, Y. -S.Solovieva, E.Stanic, S.Staric, M.Sumiyoshi, T.Tanida, K.Tatishvili, G.Teramoto, Y.Trabelsi, K.Uchida, M.Uehara, S.Unno, Y.Uno, S.Usov, Y.Vanhoefer, P.Varner, G.Wang, C. H.Wang, J.Wang, M. -Z.Williams, K. M.Won, E.Yamashita, Y.Zhang, C. C.Zhang, Z. P.Zhilich, V.Zupanc, A.
Issue Date
20-3월-2013
Publisher
AMER PHYSICAL SOC
Citation
PHYSICAL REVIEW D, v.87, no.5
Indexed
SCIE
SCOPUS
Journal Title
PHYSICAL REVIEW D
Volume
87
Number
5
URI
https://scholar.korea.ac.kr/handle/2021.sw.korea/103725
DOI
10.1103/PhysRevD.87.051101
ISSN
1550-7998
Abstract
The cross section for e(+)e(-) -> eta J=psi between root s=3.8 GeV and 5.3 GeV is measured via initial state radiation using 980 fb(-1) of data on and around the Upsilon(nS)(n=1, 2, 3, 4, 5) resonances collected with the Belle detector at KEKB. Two resonant structures at the psi(4040) and psi(4160) are observed in the (eta)J/psi invariant mass distribution. Fitting the mass spectrum with the coherent sum of two Breit-Wigner functions, one obtains B(psi(4040) -> (eta)J/psi)(.)Gamma(psi(4040))(e+e-) = (4.8 +/- 0.9 +/- 1.5) eV and B(psi(4160) -> (eta)J/psi(.)Gamma(psi(4160))(e+e-) = 4.0 +/- 0.8 +/- 1.4) eV for one solution and B(psi(4040) -> (eta)J/psi)(.)Gamma(psi(4040))(e+e-) = (11.2 +/- 1.3 +/- 2.1) eV and B(psi(4160) -> (eta)J/psi)(.)Gamma(psi(4160))(e+e-) = 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 (eta)J/psi are found to be about 1 MeV. There is no evidence for the Y(4260), Y(4360), psi(4415), or Y(4660) in the (eta)J/psi final state, and upper limits of their production rates in e(+)e(-) annihilation are determined. DOI: 10.1103/PhysRevD.87.051101
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