Further experimental studies of two-body radiativeΥdecays

G. Masek, H. P. Paar,R. Mahapatra,R. A. Briere, G. P. Chen,T. Ferguson, G. Tatishvili,H. Vogel, N. E. Adam, J. P. Alexander, C. Bebek, K. Berkelman,F. Blanc, V. Boisvert,D. G. Cassel, P. S. Drell,J. E. Duboscq,K. M. Ecklund, R. Ehrlich, R. S. Galik, L. Gibbons, B. Gittelman,S. W. Gray, D. L. Hartill, B. K. Heltsley, L. Hsu,C. D. Jones, J. Kandaswamy, D. L. Kreinick, A. Magerkurth, H. Mahlke-Krüger, T. O. Meyer, N. B. Mistry, E. Nordberg, M. Palmer,J. R. Patterson, D. Peterson, J. Pivarski, D. Riley, A. J. Sadoff, H. Schwarthoff, M. R. Shepherd, J. G. Thayer, D. Urner, B. Valant-Spaight, G. Viehhauser,A. Warburton, M. Weinberger, S. B. Athar, P. Avery, H. Stoeck, J. Yelton, G. Brandenburg, A. Ershov, D. Y.-J. Kim,R. Wilson, K. Benslama, B. I. Eisenstein, J. Ernst, G. D. Gollin, R. M. Hans,I. Karliner, N. Lowrey, M. A. Marsh, C. Plager, C. Sedlack, M. Selen, J. J. Thaler, J. Williams, K. W. Edwards, R. Ammar, D. Besson,X. Zhao, S. Anderson, V. V. Frolov,Y. Kubota,S. J. Lee, S. Z. Li,R. Poling,A. Smith, C. J. Stepaniak, J. Urheim,S. Ahmed,M. S. Alam, L. Jian,M. Saleem, F. Wappler, E. Eckhart,K. K. Gan, C. Gwon, T. Hart, K. Honscheid, D. Hufnagel,H. Kagan, R. Kass, T. K. Pedlar, J. B. Thayer, E. von Toerne,T. Wilksen, M. M. Zoeller,S. J. Richichi, H. Severini, P. Skubic, S. A. Dytman, S. Nam, V. Savinov, S. Chen, J. W. Hinson,J. Lee, D. H. Miller, V. Pavlunin, E. I. Shibata, I. P. J. Shipsey, D. Cronin-Hennessy,A. L. Lyon, C. S. Park, W. Park,E. H. Thorndike,T. E. Coan,Y. S. Gao, F. Liu, Y. Maravin, I. Narsky, R. Stroynowski,J. Ye,M. Artuso, C. Boulahouache, K. Bukin, E. Dambasuren, R. Mountain,T. Skwarnicki,S. Stone, J. C. Wang,A. H. Mahmood,S. E. Csorna, I. Danko,Z. Xu, G. Bonvicini,D. Cinabro, M. Dubrovin, S. McGee, N. E. Powell,A. Bornheim, E. Lipeles,S. P. Pappas, A. Shapiro,W. M. Sun,A. J. Weinstein

Physical Review D(2002)

引用 4|浏览0
暂无评分
摘要
Continuing our studies of radiative $\ensuremath{\Upsilon}$ decays, we report on a search for $\stackrel{\ensuremath{\rightarrow}}{\ensuremath{\Upsilon}}\ensuremath{\gamma}\ensuremath{\eta}$ and $\stackrel{\ensuremath{\rightarrow}}{\ensuremath{\Upsilon}}\ensuremath{\gamma}{f}_{J}(2220)$ in $61.3$ ${\mathrm{pb}}^{\ensuremath{-}1}$ of ${e}^{+}{e}^{\ensuremath{-}}$ data taken with the CLEO II detector at the Cornell Electron Storage Ring. For the $\ensuremath{\gamma}\ensuremath{\eta}$ search the three decays of the $\ensuremath{\eta}$ meson to ${\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{0},$ ${\ensuremath{\pi}}^{0}{\ensuremath{\pi}}^{0}{\ensuremath{\pi}}^{0}$, and $\ensuremath{\gamma}\ensuremath{\gamma}$ were investigated. We found no candidate events in the $(3\ensuremath{\pi}{)}^{0}$ modes and no significant excess over expected backgrounds in the $\ensuremath{\gamma}\ensuremath{\gamma}$ mode to set a limit on the branching fraction of $\mathcal{B}(\stackrel{\ensuremath{\rightarrow}}{\ensuremath{\Upsilon}}\ensuremath{\gamma}\ensuremath{\eta})l2.1\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}5}$ at $90%$ C.L. The three charged two-body final states $h\overline{h}(h={\ensuremath{\pi}}^{+}{,K}^{+},p)$ were investigated for ${f}_{J}(2220)$ production, with one, one, and two events found, respectively. Limits at $90%$ C.L. of $\mathcal{B}(\stackrel{\ensuremath{\rightarrow}}{\ensuremath{\Upsilon}}\ensuremath{\gamma}{f}_{J})\ifmmode\times\else\texttimes\fi{}\mathcal{B}{(f}_{J}\ensuremath{\rightarrow}h\overline{h})\ensuremath{\sim}1.5\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}5}$ have been set for each of these modes. We compare our results to measurements of other radiative $\ensuremath{\Upsilon}$ decays, to measurements of radiative $J/\ensuremath{\psi}$ decays, and to theoretical predictions.
更多
查看译文
关键词
further experimental studies,experimental studies,two-body
AI 理解论文
溯源树
样例
生成溯源树,研究论文发展脉络
Chat Paper
正在生成论文摘要