501. First observation ofB¯→D(*)ρ′−,ρ′−→ωπ−
- Author
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D. H. Miller, P. Gaidarev, K. Benslama, D. Riley, S. E. Csorna, G. W. Brandenburg, D. G. Cassel, Y. S. Gao, M. Dubrovin, H. P. Paar, T. O. Meyer, D. E. Jaffe, E. H. Thorndike, J. E. Duboscq, L. K. Gibbons, V. V. Frolov, Yuichi Kubota, H. Schwarthoff, A. H. Mahmood, Shuai Chen, A. Anastassov, P. S. Drell, Karl Berkelman, E. Nordberg, R. Mahapatra, M. M. Zoeller, M. Saleem, I. Karliner, G. Bonvicini, J. P. Alexander, D. Z. Besson, T. E. Coan, J. Urheim, D. Hufnagel, R. Ammar, A. J. Weinstein, C.Y. Prescott, J. J. Thaler, Tomasz Skwarnicki, Thomas Ferguson, S. Ahmed, I. P.J. Shipsey, R. M. Hans, B. I. Eisenstein, D. M. Asner, Hans J. Vogel, C. Gwon, S. J. Richichi, M. Lohner, M. A. Marsh, L. Jian, J. G. Thayer, Jianqiao Ye, J. Ernst, W. M. Sun, Sheldon Stone, G. P. Chen, Ryszard Stroynowski, S.C. Timm, D. Urner, E. I. Shibata, A. Wolf, Paul Avery, H. Stoeck, R. A. Briere, Andreas Warburton, C. J. Stepaniak, K. W. Edwards, D. Cinabro, Richard Wilson, Marina Artuso, M. Kostin, C. D. Jones, D. Y.J. Kim, G. J. Zhou, B. E. Berger, E. Johnson, B. Gittelman, C. Sedlack, K. K. Gan, G. Viehhauser, R. Poling, L. Hsu, T. Bergfeld, S. B. Athar, J. W. Hinson, V. Pavlunin, R. Godang, T. Hart, Z. Xu, P. Skubic, Sacha E Kopp, K. Honscheid, M. S. Alam, I. Danko, C. Boulahouache, N. B. Mistry, T. K. Pedlar, A. I. Rubiera, D. L. Hartill, S. McGee, R. D. Kass, A. Smith, A. Shapiro, J. Williams, C. Plager, S. Anderson, Daniel P Cronin-Hennessy, R. Mountain, A. Undrus, K. Bukin, S. W. Gray, A. Romano, A. Magerkurth, Yurii Maravin, F. R. Wappler, S. P. Pappas, C. Bebek, J. B. Thayer, E. Eckhart, L. Ling, V. Fadeyev, I. Narsky, E. von Toerne, T. Wlodek, T. S. Hill, A. Ershov, R. Ehrlich, G. Masek, Juliet Ritchie Patterson, John Yelton, B. Valant-Spaight, H. Kagan, R. J. Morrison, Mats A Selen, Horst Severini, A. J. Sadoff, J. Kandaswamy, X. Zhao, A. Bornheim, D. Peterson, K. W. McLean, M.A. Palmer, Alice Bean, Jason Sang Hun Lee, V. Boisvert, A. Eppich, B. K. Heltsley, E. Lipeles, S. J. Lee, G. D. Gollin, D. L. Kreinick, V. Savinov, F. Blanc, G. E. Gladding, K. M. Ecklund, A. L. Lyon, E. Dambasuren, Jing Wang, and G. Majumder
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Combinatorics ,Physics ,Nuclear and High Energy Physics ,Central mass ,010308 nuclear & particles physics ,0103 physical sciences ,010306 general physics ,01 natural sciences ,Omega - Abstract
We report on the observation of $\overline{B}\ensuremath{\rightarrow}{D}^{*}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{0}$ decays. The branching ratios for ${D}^{*+}$ and ${D}^{*0}$ are $(1.72\ifmmode\pm\else\textpm\fi{}0.14\ifmmode\pm\else\textpm\fi{}0.24)%$ and $(1.80\ifmmode\pm\else\textpm\fi{}0.24\ifmmode\pm\else\textpm\fi{}0.27)%,$ respectively. Each final state has a ${D}^{*}\ensuremath{\omega}{\ensuremath{\pi}}^{\ensuremath{-}}$ component, with branching ratios $(0.29\ifmmode\pm\else\textpm\fi{}0.03\ifmmode\pm\else\textpm\fi{}0.04)%$ and $(0.45\ifmmode\pm\else\textpm\fi{}0.10\ifmmode\pm\else\textpm\fi{}0.07)%$ for the ${D}^{*+}$ and ${D}^{*0}$ modes, respectively. We also observe $\overline{B}\ensuremath{\rightarrow}D\ensuremath{\omega}{\ensuremath{\pi}}^{\ensuremath{-}}$ decays. The branching ratios for ${D}^{+}$ and ${D}^{0}$ are $(0.28\ifmmode\pm\else\textpm\fi{}0.05\ifmmode\pm\else\textpm\fi{}0.04)%$ and $(0.41\ifmmode\pm\else\textpm\fi{}0.07\ifmmode\pm\else\textpm\fi{}0.06)%,$ respectively. A spin parity analysis of the $\ensuremath{\omega}{\ensuremath{\pi}}^{\ensuremath{-}}$ system in the $D\ensuremath{\omega}{\ensuremath{\pi}}^{\ensuremath{-}}$ final state shows a preference for a wide ${1}^{\ensuremath{-}}$ resonance. A fit to the $\ensuremath{\omega}{\ensuremath{\pi}}^{\ensuremath{-}}$ mass spectrum finds a central mass of $(1349\ifmmode\pm\else\textpm\fi{}{25}_{\ensuremath{-}5}^{+10})$ MeV and width of $(547\ifmmode\pm\else\textpm\fi{}{86}_{\ensuremath{-}45}^{+46})$ MeV. We identify this object as the $\ensuremath{\rho}(1450)$ or the ${\ensuremath{\rho}}^{\ensuremath{'}}.$
- Published
- 2001
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