3 research outputs found

    Constraining the Unitarity Triangle with B -> V gamma

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    We discuss the exclusive radiative decays Bβ†’Kβˆ—Ξ³B\to K^{*}\gamma, B→ργB \to\rho\gamma, and B→ωγB\to\omega\gamma in QCD factorization within the Standard Model. The analysis is based on the heavy-quark limit of QCD. Our results for these decays are complete to next-to-leading order in QCD and to leading order in the heavy-quark limit. Special emphasis is placed on constraining the CKM-unitarity triangle from these observables. We propose a theoretically clean method to determine CKM parameters from the ratio of the B→ρlΞ½B\to\rho l\nu decay spectrum to the branching fraction of B→ργB\to\rho\gamma. The method is based on the cancellation of soft hadronic form factors in the large energy limit, which occurs in a suitable region of phase space. The ratio of the B→ργB\to\rho\gamma and Bβ†’Kβˆ—Ξ³B\to K^{*}\gamma branching fractions determines the side RtR_{t} of the standard unitarity triangle with reduced hadronic uncertainties. The recent Babar bound on B(B0→ρ0Ξ³)B(B^0\to\rho^0\gamma) implies Rt<0.81(ΞΎ/1.3)R_t < 0.81 (\xi/1.3), with the limiting uncertainty coming only from the SU(3) breaking form factor ratio ΞΎ\xi. This constraint is already getting competitive with the constraint from BsB_{s}-BΛ‰s\bar B_{s} mixing. Phenomenological implications from isospin-breaking effects are briefly discussed.Comment: 23 pages, 8 figure

    Exploring the Unitarity Triangle through CP violation observables in Bsβ†’K+Kβˆ’B_s \to K^+ K^-

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    We discuss the determination of the CKM parameters from the forthcoming CPCP violation observables in Bsβ†’K+Kβˆ’B_s \to K^+ K^- decays. Combining the information on mixing induced CP violation in Bsβ†’K+Kβˆ’B_s \to K^+ K^-, with the Bdβ†’J/ψKsB_d \to J/\psi K_s precision observable sin⁑2Ξ²\sin 2\beta and the Bs0B^0_s--Bs0Λ‰\bar{B^0_s} mixing phase Ο•s\phi_s, we propose a determination of the unitarity triangle (ρˉ,Ξ·Λ‰)(\bar\rho, \bar\eta). Computing the penguin parameters (r,ΞΈ)(r, \theta) within QCD factorization yield precise determination of (ρˉ,Ξ·Λ‰)(\bar\rho, \bar\eta), reflected by a weak dependence on the ΞΈ\theta which is shown as a second order effect. The impact of the direct CP violation observable CKKC_{KK} on the penguin parameters are investigated and a lower bound on CKKC_{KK} is extracted. We also discuss the effect of the Bs0B^0_s--Bs0Λ‰\bar{B^0_s} new physics mixing phase on the penguin parameters (r,ΞΈ)(r, \theta) and SKKS_{KK}. Using the SU(3)-flavour symmetry argument and the current BB-factories data provided by the Bdβ†’Ο€+Ο€βˆ’B_d \to \pi^+ \pi^- modes, we complement the Bsβ†’K+Kβˆ’B_s \to K^+ K^- CP-violating observables in a variety of ways, in particular we find that SKK>0S_{KK}>0. Finally we analyze systematically the SU(3)-symmetry breaking factor within QCD factorization.Comment: 22 pages, 6 figures, typos corrected, reference and some remarks adde

    Direct CP Violation, Branching Ratios and Form Factors B→πB \to \pi, B→KB \to K in BB Decays

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    The Bβ†’Ο€B \to \pi and Bβ†’KB \to K transitions involved in hadronic B decays are investigated in a phenomenological way through the framework of QCD factorization. By comparing our results with experimental branching ratios from the BELLE, BABAR and CLEO Collaborations for all the B decays including either a pion or a kaon, we propose boundaries for the transition form factors Bβ†’Ο€B \to \pi and Bβ†’KB \to K depending on the CKM matrix element parameters ρ\rho and Ξ·\eta. From this analysis, the form factors required to reproduce the experimental data for branching ratios are FBβ†’Ο€=0.31Β±0.12F^{B \to \pi}= 0.31 \pm 0.12 and FBβ†’K=0.37Β±0.13F^{B \to K}= 0.37\pm 0.13. We calculate the direct CP violating asymmetry parameter, aCPa_{CP}, for Bβ†’Ο€+Ο€βˆ’Ο€B \to \pi^{+} \pi^{-} \pi and Bβ†’Ο€+Ο€βˆ’KB \to \pi^{+} \pi^{-} K decays, in the case where Οβˆ’Ο‰\rho-\omega mixing effects are taken into account. Based on these results, we find that the direct CP asymmetry for Bβˆ’β†’Ο€+Ο€βˆ’Ο€βˆ’B^{-} \to \pi^{+} \pi^{-} \pi^{-}, BΛ‰0β†’Ο€+Ο€βˆ’Ο€0\bar{B}^{0} \to \pi^{+} \pi^{-} \pi^{0}, Bβˆ’β†’Ο€+Ο€βˆ’Kβˆ’B^{-} \to \pi^{+} \pi^{-} K^{-}, and BΛ‰0β†’Ο€+Ο€βˆ’KΛ‰0\bar{B}^{0} \to \pi^{+} \pi^{-} \bar{K}^{0}, reaches its maximum when the invariant mass Ο€+Ο€βˆ’\pi^{+} \pi^{-} is in the vicinity of the Ο‰\omega meson mass. The inclusion of Οβˆ’Ο‰\rho-\omega mixing provides an opportunity to erase, without ambiguity, the phase uncertainty mod(Ο€)(\pi) in the determination of the CKM angles Ξ±\alpha in case of bβ†’ub\to u and Ξ³\gamma in case of bβ†’sb \to s.Comment: 74 pages, 15 figures, 8 tables. A few misprints corrected, two references adde
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