M. Procario, Carnegie Mellon University
S. Yang, Carnegie Mellon University
D. S. Akerib, California Institute of Technology
B. Barish, California Institute of Technology
M. Chadha, California Institute of Technology
S. Chan, California Institute of Technology
D. F. Cowen, California Institute of Technology
G. Eigen, California Institute of Technology
J. S. Miller, California Institute of Technology
J. Urheim, California Institute of Technology
A. J. Weinstein, California Institute of Technology
D. Acosta, University of California, San Diego
M. Athanas, University of California, San Diego
G. Masek, University of California, San Diego
B. Ong, University of California, San Diego
H. Paar, University of California, San Diego
M. Sivertz, University of California, San Diego
A. Bean, University of California, Santa Barbara
J. Gronberg, University of California, Santa Barbara
R. Kutschke, University of California, Santa Barbara
S. Menary, University of California, Santa Barbara
R. J. Morrison, University of California, Santa Barbara
S. Nakanishi, University of California, Santa Barbara
H. N. Nelson, University of California, Santa Barbara
T. K. Nelson, University of California, Santa Barbara
J. D. Richman, University of California, Santa Barbara
H. Tajima, University of California, Santa Barbara
D. Schmidt, University of California, Santa Barbara
D. Sperka, University of California, Santa Barbara
M. S. Witherell, University of California, Santa Barbara
R. Ballest, University of Colorado Boulder

Document Type

Article

Publication Date

1-1-1993

Abstract

Using the CLEO II detector at CESR we have studied D0 decays into final states with a K̄0 or K̄*0, and have measured branching ratios for the decay modes D0→(K̄0K̄*0)π0,η, η′. These results are compared with predictions of various charm decay models, and contributions of final-state interactions are discussed. © 1993 The American Physical Society.

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