4.7 Article

Search for b → u transitions in B- → DK- and D*K- decays

Journal

PHYSICAL REVIEW D
Volume 82, Issue 7, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.82.072006

Keywords

-

Funding

  1. US Department of Energy and National Science Foundation
  2. Natural Sciences and Engineering Research Council (Canada)
  3. Commissariat a l'Energie Atomique and Institut National de Physique Nucleaire et de Physique des Particules (France)
  4. Bundesministerium fur Bildung und Forschung and Deutsche Forschungsgemeinschaft (Germany)
  5. Istituto Nazionale di Fisica Nucleare (Italy)
  6. Foundation for Fundamental Research on Matter (The Netherlands)
  7. Research Council of Norway
  8. Ministry of Education and Science of the Russian Federation
  9. Ministerio de Ciencia e Innovacion (Spain)
  10. Science and Technology Facilities Council (United Kingdom)
  11. European Union
  12. A.P. Sloan Foundation (USA)
  13. Binational Science Foundation (USA-Israel)
  14. Science and Technology Facilities Council [ST/H001166/1, PP/E000444/1] Funding Source: researchfish
  15. STFC [ST/H001166/1] Funding Source: UKRI

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We report results from an updated study of the suppressed decays We report results from an updated study of the suppressed decays B- -> DK- and B- -> D*K- followed by D -> K+ pi(-), where D-(*()0) indicates a D-(*()0)or a (D) over bar (()*()0) meson, and D* -> D pi(0) or D* -> D gamma. These decays are sensitive to the Cabibbo-Kobayashi-Maskawa unitarity triangle angle gamma due to interference between the b -> c transition B- -> D-(*K-)0(-) followed by the doubly Cabibbo-suppressed decay D-0 -> K+ pi(-), and the b -> u transition B- -> (D) over bar (()*()0) K- followed by the Cabibbo-favored decay (D) over bar (0) -> K+ pi(-). We also report an analysis of the decay B- -> D-(*())pi(-) with the D decaying into the doubly Cabibbo-suppressed mode D -> K+ pi(-). Our results are based on 467 x 10(6) Gamma(4S) -> BB- decays collected with the BABAR detector at SLAC. We measure the ratios R-(*()) of the suppressed ([K+ pi(-)](D)K- / pi(-)) to favored ([K+ pi(-)](D)K- / pi(-)) branching fractions as well as the CP asymmetries A(()*()) of those modes. We see indications of signals for the B- -> DK- and B- -> D-D pi 0(()*()) K- suppressed modes, with statistical significances of 2.1 and 2.2 sigma, respectively, and we measure: R-DK = (1.1 +/- 0: 6 +/- 0.2) x 10(-2); A(DK) = -0.86 +/- 0: 47(-0.16)(+0.12), R-(D pi 0)K* = (1.8 +/- 0: 9 +/- 0: 4) x 10(-2); A ((D pi 0)K)* = +0.77 +/- 0: 35 +/- 0.12; R-(D gamma)K* = (1.3 +/- 1.4 +/- 0.8) x 10(-2); A((D gamma)K)* = +0.36 +/- 0: 94(-0.41)(+0.25), where the first uncertainty is statistical and the second is systematic. We use a frequentist approach to obtain the magnitude of the ratio r(B) equivalent to vertical bar A(B- -> (D) over bar 0K(-))/A(B- -> (DK-)-K-0)vertical bar = (9.5(-4.1)(+5.1))%, with r(B) < 16: 7% at 90% confidence level. In the case of B- -> D*K- we find r(B) equivalent to vertical bar A(B- -> <(D)over bar>0K(-))/A(B- -> (DK-)-K-0)vertical bar = (9.6(-5.1)(+3.5))%, with r(B)* < 15.0% at 90% confidence level.

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