4.7 Article

Measurements of branching fractions and direct CP asymmetries for B → Kπ, B → ππ and B → KK decays

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PHYSICAL REVIEW D
卷 87, 期 3, 页码 -

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AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.87.031103

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资金

  1. MEXT (Japan)
  2. JSPS (Japan)
  3. Nagoya's TLPRC (Japan)
  4. ARC (Australia)
  5. DIISR (Australia)
  6. NSFC (China)
  7. MSMT (Czechia)
  8. DST (India)
  9. INFN (Italy)
  10. MEST (Korea)
  11. NRF (Korea)
  12. GSDC of KISTI (Korea)
  13. WCU (Korea)
  14. MNiSW (Poland)
  15. MES (Russia)
  16. RFAAE (Russia)
  17. ARRS (Slovenia)
  18. SNSF (Switzerland)
  19. NSC (Taiwan)
  20. MOE (Taiwan)
  21. DOE (USA)
  22. NSF (USA)

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We report measurements of the branching fractions and direct CP asymmetries (A(CP)) for B -> K pi, pi pi and KK decays (but not pi(0) pi(0)) based on the final data sample of 772 x 10(6) B (B) over bar pairs collected at the Y(4S) resonance with the Belle detector at the KEKB asymmetric-energy e(+)e(-) collider. We set a 90% confidence-level upper limit for K+K- at 2.0 x 10(-7); all other decays are observed with branching fractions ranging from 10(-6) to 10(-5). In the B-0/(B) over bar (0) -> K-+/-pi(-/+) mode, we confirm Belle's previously reported large A(CP) with a value of -0.069 +/- 0.014 +/- 0.007 and a significance of 4.4 sigma. For all other flavor-specific modes, we find A(CP) values consistent with zero, including A(CP)(K+pi(0)) = +0.043 +/- 0.024 +/- 0.007 with 1.8 sigma significance. The difference of CP asymmetry between B-+/- -> K-+/- pi(0) and B-0/(B) over bar (0) K-+/-pi(-/+) is found to be Delta A(K pi) equivalent to A(CP)(K+pi(0)) - A(CP)(K+pi(-)) = +0.112 +/- 0.027 +/- 0.007 with 4.0 sigma significance. We also calculate the ratios of partial widths for the B -> K pi decays. Using our results, we test the validity of the sum rule A(CP)(K+pi(-)) + A(CP)(K-0 pi(+)) Gamma(K-0 pi(+))/Gamma(K+pi(-)) - A(CP)(K+pi(0))2 Gamma(K+pi(0))/Gamma(K+pi(-)) - A(CP)(K-0 pi(0))2 Gamma(K-0 pi(0))/Gamma(K+pi(-)) =0 and obtain a sum of -0.270 +/- 0.132 +/- 0.060 with 1:9 sigma significance. DOI: 10.1103/PhysRevD.87.031103

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