Phys. Rev. D
45,
2196–2211
(1992)
Resonant substructure in K̅ πππ decays of D mesons
D. Coffman et al. (Mark III Collaboration)
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D. Coffman*, F. DeJongh†, G. P. Dubois, G. Eigen, D. G. Hitlin, C. G. Matthews, A. Mincer‡, J. Richman§, A. J. Weinstein, W. J. Wisniewski, and Y. Zhu**
California Institute of Technology, Pasadena, California 91125
T. Bolton††, K. O. Bunnell, R. E. Cassell, D. H. Coward, P. C. Kim*, J. Labs, A. Odian, D. Pitman‡‡, R. H. Schindler, W. Toki, and S. Wasserbaecha
Stanford Linear Acclerator Center, Stanford, California 94305
J. J. Drinkardb, C. Gattoc, C. A. Heusch, W. S. Lockman, M. Scarlatella, H. F. W. Sadrozinski, T. L. Schalk, A. Seiden, and S. Weselerd
University of California at Santa Cruz, Santa Cruz, California 95064
B. I. Eisenstein, T. Freesee, G. Gladding, J. M. Izen, I. E. Stockdalef, and B. Tripsasg
University of Illinois at Urbana-Champaign, Urbana, Illinois 61801
U. Mallik and M. Z. Wang
University of Iowa, Iowa City, Iowa 52242
J. Brown, T. H. Burnett, A. D. Li, R. Mirh, P. M. Mockett, B. Nematii, L. Parrish, and H. Willutzkij (Mark III Collaboration)
University of Washington, Seattle, Washington 98195
Received 23 September 1991; published in the issue dated 1 April 1992
We determine the resonant substructure of D→K̅ πππ decays, extracting the relative fractions and phases of the amplitudes contributing to the K-π+π+π-, K̅ 0π+π+π-, K-π+π+π0, and K̅ 0π+π-π0 final states. We find that two-body decay modes account for at least 75% of these decays. We obtain branching ratios for D→K̅ a1(1260), D→K̅ *ρ, D→K̅ 1(1270)π, D→K̅ 1(1400)π, and D0→K̅ 0ω decay modes, as well as for several three- and four-body decay modes. In the case of D→K̅ a1(1260) and D→K̅ *ρ, we obtain the branching ratios for all three possible isospin combinations, enabling us to extract the isospin-½ and -3/2 amplitudes, and their relative phases. We find that the isospin-3/2 amplitudes are suppressed relative to the isospin-½ amplitudes. This implies that the widths of the D+ modes are suppressed relative to those of the D0, confirming that an understanding of the lifetime difference of the D0 and D+ depends on an understanding of two-body hadronic decays. For the D→K̅ *ρ decay modes, we obtain detailed information on the polarization of the K̅ * and ρ. This enables us to place constraints on the form factors for D→K̅ * and D→ρ transitions. A comparison of our results on D→K̅ *ρ decays with recent results on semileptonic decays allows us to test the factorization hypothesis.
© 1992 The American Physical Society
URL:
http://link.aps.org/doi/10.1103/PhysRevD.45.2196
DOI:
10.1103/PhysRevD.45.2196
*Present address: Wilson Laboratory, Cornell University, Ithaca, NY 14853. †Present address: Fermilab, P. O. Box 500, Batavia, IL 60510. ‡Present address: New York University, New York, NY 10003. §Present address: University of California at Santa Barbara, Santa Barbara, CA 93106. **Present address: International Telephone and Teledata, Inc., P. O. Box 80160, Goleta, CA 93118. ††Present address: Columbia University, P. O. Box 137, Irvington, NY 10533. ‡‡Present address: University of Victoria, Victoria, BC V8W 3P6 Canada. aPresent address: EP Division, CERN, 1211 Geneva 23, Switzerland. bPresent address: Centre de Physique des Particules de Marseille, F-13288 Marseille, CEDEX 9, France. cPresent address: INFN, 80125 Napoli, Italy. dPresent address: University of Karlsruhe, Postfach 6980, D-7500 Karlsruhe, Germany. ePresent address: Systems Control Technology, 2300 Geng Road, Palo Alto, CA 94303. fPresent address: NASA Ames Research Center, MS 258-6, Moffett Field, CA 94035. gPresent address: Center for Naval Analyses, 4401 Ford Avenue, Alexandria, VA 22302. hPresent address: Indiana University, Bloomington, IN 47405. iPresent address: State University of New York at Albany, Albany, NY 12222. jPresent address: Brookhaven National Laboratory, Upton. NY 11973.
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