Fermilab E791 Collaboration

نویسندگان

  • J. C. Anjos
  • D. Ashery
  • S. B. Bracker
  • H. S. Carvalho
  • N. J. Copty
  • L. M. Cremaldi
  • K. Denisenko
  • A. M. Halling
  • D. C. Langs
  • K. C. Peng
  • L. P. Perera
  • M. V. Purohit
  • B. Quinn
  • J. J. Reidy
  • H. A. Rubin
  • D. A. Sanders
  • A. K. S. Santha
  • A. F. S. Santoro
  • R. A. Sidwell
  • M. D. Sokoloff
  • K. Stenson
  • A. K. Tripathi
چکیده

Using the large hadroproduced charm sample collected in experiment E791 at Fermilab, we have measured ratios of branching fractions for the two-body singlyCabibbo-suppressed charged decays of the D: Γ(D → KK) Γ(D → Kπ) = 0.109± 0.003± 0.003, Γ(D → ππ) Γ(D → Kπ) = 0.040 ± 0.002 ± 0.003, and Γ(D → KK) Γ(D → ππ) = 2.75 ± 0.15±0.16. We have looked for differences in the decay rates of D andD to the CP eigenstates KK and ππ, and have measured the CP asymmetry parameters ACP (K K) = −0.010± 0.049± 0.012 and ACP (π π) = −0.049± 0.078± 0.030, both consistent with zero. PACS: 11.30.Er; 13.25.Ft; 14.40.Lb The measured world average for the ratio of the branching fractions of the two-body singly-Cabibbo-suppressed (SCS) charged decays of the D meson is Γ(D → KK) Γ(D → ππ) = 2.86±0.28 [1]. Models including final state interactions [2,3], penguin diagrams [4], QCD sum rules [5], and non-perturbative algebraic approaches [6] have been proposed to explain the experimental value observed for this ratio. Precise measurements of this ratio can help to differentiate among models, and can also aid in our understanding of the Standard Model predictions forD–D mixing via long-range mechanisms, which require SU(3) symmetry-breaking to be non-zero [7,8]. ⋆ Submitted to Physics Letters B.

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تاریخ انتشار 1997