3,653 research outputs found

    Branching ratio and CP asymmetry of Bs→π+π−B_s \to \pi^+ \pi^- decays in the perturbative QCD approach

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    In this paper, we calculate the decay rate and CP asymmetry of the Bs→π+π−B_s \to \pi^+\pi^- decay in perturbative QCD approach with Sudakov resummation. Since none of the quarks in final states is the same as those of the initial BsB_s meson, this decay can occur only via annihilation diagrams in the standard model. Besides the current-current operators, the contributions from the QCD and electroweak penguin operators are also taken into account. We find that (a) the branching ratio is about 4×10−74 \times 10^{-7}; (b) the penguin diagrams dominate the total contribution; and (c) the direct CP asymmetry is small in size: no more than 33% ; but the mixing-induced CP asymmetry can be as large as ten percent testable in the near future LHC-b experiments.Comment: 12 pages, 4 figures included, RevTe

    Study of color suppressed modes B0→Dˉ(∗)0η(′)B^0 \to \bar D^{(*)0} \eta^{(\prime)}

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    The color suppressed modes B0→Dˉ(∗)0η(′)B^0 \to \bar D^{(*)0} \eta^{(\prime)} are analyzed in perturbative QCD approach. We find that the dominant contribution is from the non-factorizable diagrams. The branching ratios calculated in our approach for B0→Dˉ(∗)0ηB^0 \to \bar D^{(*)0} \eta agree with current experiments. By neglecting the gluonic contribution, we predict the branching ratios of B0→Dˉ(∗)0η′B^0 \to \bar D^{(*)0} \eta' are at the comparable size of B0→Dˉ(∗)0π0B^0 \to \bar D^{(*)0} \pi^0, but smaller than that of B0→Dˉ(∗)0ηB^0 \to \bar D^{(*)0} \eta .Comment: revtex, 5 pages, axodraw.st

    Branching ratios of B+→D(∗)+K(∗)0B^+ \to D^{(*)+}K^{(*)0} decays in perturbative QCD approach

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    We study the rare decays B+→D(∗)+K(∗)0B^+ \to D^{(*)+}K^{(*)0}, which can occur only via annihilation type diagrams in the standard model. We calculate all of the four modes, B→PP,VP,PV,VVB \to PP, VP, PV, VV, in the framework of perturbative QCD approach and give the branching ratios of the order about 10−610^{-6}.Comment: 18 pages, 1 figure, Revte

    Nonleptonic two-body charmless B decays involving a tensor meson in the Perturbative QCD Approach

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    Two-body charmless hadronic B decays involving a light tensor meson in the final states are studied in the perturbative QCD approach based on kTk_T factorization. From our calculations, we find that the decay branching ratios for color allowed tree-dominated decays B→a20π+B\to a_{2}^{0}\pi^{+} and B→a2−π+B\to a_{2}^{-}\pi^{+} modes are of order 10−610^{-6} and 10−510^{-5}, respectively. While other color suppressed tree-dominated decays have very small branching ratios. In general, the branching ratios of most decays are in the range of 10−510^{-5} to 10−810^{-8}, which are bigger by one or two orders of magnitude than those predictions obtained in Isgur-Scora-Grinstein-Wise II model and in the covariant light-front approach, but consistent with the recent experimental measurements and the QCD factorization calculations. Since the decays with a tensor meson emitted from vacuum are prohibited in naive factorization, the contributions of nonfactorizable and annihilation diagrams are very important to these decays, which are calculable in our perturbative QCD approach. We also give predictions to the direct CP asymmetries, some of which are large enough for the future experiments to measure. Because we considered the mixing between f2f_{2} and f2′f_{2}', the decay rates are enhanced significantly for some decays involving f2′f_{2}^{\prime} meson, even with a small mixing angle.Comment: 26 pages, 2 figure

    Study of pure annihilation type decays B→Ds∗KB \to D_s^{*} K

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    In this work, we calculate the rare decays B0→Ds∗−K+B^0 \to D_s^{*-} K^+ and B+→Ds∗+Kˉ0B^+ \to D_s^{*+} \bar{K}^0 in perturbative QCD approach with Sudakov resummation. We give the branching ratio of 10−510^{-5} for B0→Ds∗−K+B^0 \to D_s^{*-}K^+, which will be tested soon in BB factories. The decay B+→Ds∗+Kˉ0B^+ \to D_s^{*+} \bar{K}^0 has a very small branching ratio at O(10−8){\cal O}(10^{-8}), due to the suppression from CKM matrix elements ∣Vub∗Vcd∣|V_{ub}^* V_{cd}|. It may be sensitive to new physics contributions.Comment: 14 pages, 1 figur
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