Phys. Rev. D
68,
032002
(2003)
[10 pages]
Observation of a narrow resonance of mass 2.46 GeV/c2 decaying to Ds*+π0 and confirmation of the DsJ*(2317) state
D. Besson et al.
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D. Besson
University of Kansas, Lawrence, Kansas 66045, USA
S. Anderson, V. V. Frolov, D. T. Gong, Y. Kubota, S. Z. Li, R. Poling, A. Smith, C. J. Stepaniak, and J. Urheim
University of Minnesota, Minneapolis, Minnesota 55455, USA
Z. Metreveli, K. K. Seth, A. Tomaradze, and P. Zweber
Northwestern University, Evanston, Illinois 60208, USA
K. Arms, E. Eckhart, K. K. Gan, C. Gwon, T. K. Pedlar, and E. von Toerne
Ohio State University, Columbus, Ohio 43210, USA
H. Severini and P. Skubic
University of Oklahoma, Norman, Oklahoma 73019, USA
S. A. Dytman, J. A. Mueller, S. Nam, and V. Savinov
University of Pittsburgh, Pittsburgh, Pennsylvania 15260, USA
J. W. Hinson, G. S. Huang, J. Lee, D. H. Miller, V. Pavlunin, B. Sanghi, E. I. Shibata, and I. P. J. Shipsey
Purdue University, West Lafayette, Indiana 47907, USA
D. Cronin-Hennessy, C. S. Park, W. Park, J. B. Thayer, and E. H. Thorndike
University of Rochester, Rochester, New York 14627, USA
T. E. Coan, Y. S. Gao, F. Liu, and R. Stroynowski
Southern Methodist University, Dallas, Texas 75275, USA
M. Artuso, C. Boulahouache, S. Blusk, E. Dambasuren, O. Dorjkhaidav, R. Mountain, H. Muramatsu, R. Nandakumar, T. Skwarnicki, S. Stone, and J. C. Wang
Syracuse University, Syracuse, New York 13244, USA
A. H. Mahmood
University of Texas–Pan American, Edinburg, Texas 78539, USA
S. E. Csorna and I. Danko
Vanderbilt University, Nashville, Tennessee 37235, USA
G. Bonvicini, D. Cinabro, M. Dubrovin, and S. McGee
Wayne State University, Detroit, Michigan 48202, USA
A. Bornheim, E. Lipeles, S. P. Pappas, A. Shapiro, W. M. Sun, and A. J. Weinstein
California Institute of Technology, Pasadena, California 91125, USA
R. A. Briere, G. P. Chen, T. Ferguson, G. Tatishvili, H. Vogel, and M. E. Watkins
Carnegie Mellon University, Pittsburgh, Pennsylvania 15213, USA
N. E. Adam, J. P. Alexander, K. Berkelman, V. Boisvert, D. G. Cassel, 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, J. R. Patterson, D. Peterson, J. Pivarski, S. J. Richichi, D. Riley, A. J. Sadoff, H. Schwarthoff, M. R. Shepherd, J. G. Thayer, D. Urner, T. Wilksen, A. Warburton, and M. Weinberger
Cornell University, Ithaca, New York 14853, USA
S. B. Athar, P. Avery, L. Breva-Newell, V. Potlia, H. Stoeck, and J. Yelton
University of Florida, Gainesville, Florida 32611, USA
B. I. Eisenstein, G. D. Gollin, I. Karliner, N. Lowrey, C. Plager, C. Sedlack, M. Selen, J. J. Thaler, and J. Williams
University of Illinois, Urbana-Champaign, Illinois 61801, USA
K. W. Edwards
Carleton University, Ottawa, Ontario, Canada K1S 5B6 the Institute of Particle Physics, Canada M5S 1A7
(CLEO Collaboration)
See Also:
Publisher's Note
Received 28 May 2003; published 28 August 2003; corrected 6 June 2007
Using 13.5 fb-1 of e+e- annihilation data collected with the CLEO II detector, we have observed a narrow resonance decaying to Ds*+π0 with a mass near 2.46GeV/c2. The search for such a state was motivated by the recent discovery by the BaBar Collaboration of a narrow state at 2.32GeV/c2, the DsJ*(2317)+, that decays to Ds+π0. Reconstructing the Ds+π0 and Ds*+π0 final states in CLEO data, we observe peaks in both of the corresponding reconstructed mass difference distributions, ΔM(Dsπ0)=M(Dsπ0)-M(Ds) and ΔM(Ds*π0)=M(Ds*π0)-M(Ds*), both of them at values near 350MeV/c2. We interpret these peaks as signatures of two distinct states, the DsJ*(2317)+ plus a new state, designated as the DsJ(2463)+. Because of the similar ΔM values, each of these states represents a source of background for the other if photons are lost, ignored or added. A quantitative accounting of these reflections confirms that both states exist. We have measured the mean mass differences 〈ΔM(Dsπ0)〉=350.0±1.2(stat)±1.0(syst)MeV/c2 for the DsJ*(2317)+ state, and 〈ΔM(Ds*π0)〉=351.2±1.7(stat)±1.0(syst)MeV/c2 for the new DsJ(2463)+ state. We have also searched, but find no evidence, for decays of the two states via the channels Ds*+γ,Ds+γ, and Ds+π+π-. The observations of the two states at 2.32 and 2.46GeV/c2, in the Ds+π0 and Ds*+π0 decay channels, respectively, are consistent with their interpretations as cs̅ mesons with an orbital angular momentum L=1 and spin and parity JP=0+ and 1+.
© 2003 The American Physical Society
URL:
http://link.aps.org/doi/10.1103/PhysRevD.68.032002
DOI:
10.1103/PhysRevD.68.032002
PACS:
14.40.Lb, 12.40.Yx, 13.25.Ft
See Also
Publisher's Note:
D. Besson et al. CLEO Collaboration,
Publisher’s Note: Observation of a narrow resonance of mass 2.46 GeV/c2 decaying to Ds*+π0 and confirmation of the DsJ*(2317) state [Phys. Rev. D 68, 032002 (2003)],
Phys. Rev. D 75, 119908 (2007).
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