Skip to main navigation Skip to search Skip to main content

Measurement of the B¯→Dlv¯ partial width and form factor parameters

  • M. Athanas
  • , P. Avery
  • , C. D. Jones
  • , M. Lohner
  • , C. Prescott
  • , J. Yelton
  • , J. Zheng
  • , G. Brandenburg
  • , R. A. Briere
  • , A. Ershov
  • , Y. S. Gao
  • , D. Y.J. Kim
  • , R. Wilson
  • , H. Yamamoto
  • , T. E. Browder
  • , F. Li
  • , Y. Li
  • , J. L. Rodriguez
  • , T. Bergfeld
  • , B. I. Eisenstein
  • J. Ernst, G. E. Gladding, G. D. Gollin, R. M. Hans, E. Johnson, I. Karliner, M. A. Marsh, M. Palmer, M. Selen, J. J. Thaler, K. W. Edwards, A. Bellerive, R. Janicek, D. B. MacFarlane, P. M. Patel, A. J. Sadoff, R. Ammar, P. Baringer, A. Bean, D. Besson, D. Coppage, C. Darling, R. Davis, N. Hancock, S. Kotov, I. Kravchenko, N. Kwak, Yuichi Kubota, T. Riehle, CLEO Collaboration

Research output: Contribution to journalArticlepeer-review

Abstract

We have studied the decayB¯→Dlν¯ where l = e or μ. From a fit to the differential decay ratedγ/dwwe measure the rate normalizationFD(1) |V cb | and form factor slopeρˆ2D, and, using measured values ofτB, findγ(B¯→Dlv¯) = (12.0 ± 0.9 ± 2.1) ns−1 . The resulting branching fractions areB (B¯0 → D+ lν¯) = (1.87 ± 0.15 ± 0.32)% and B (B → D0lν¯) = (1.94 ± 0.15 ± 0.34)% . The form factor parameters are in agreement with those measured in B¯ → D*lν¯ decays, as predicted by heavy quark effective theory.

Original languageEnglish (US)
Pages (from-to)2208-2212
Number of pages5
JournalPhysical review letters
Volume79
Issue number12
DOIs
StatePublished - 1997

Fingerprint

Dive into the research topics of 'Measurement of the B¯→Dlv¯ partial width and form factor parameters'. Together they form a unique fingerprint.

Cite this