549 research outputs found

    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

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

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    The color suppressed modes B0→Dˉ(∗)0η(â€Č)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(∗)0ηâ€ČB^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

    B -> J/psi K^* Decays in QCD Factorization

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    The hadronic decay B -> J K^* is analyzed within the framework of QCD factorization. The spin amplitudes A_0, A_\parallel and A_\perp in the transversity basis and their relative phases are studied using various different form-factor models for B-K^* transition. The effective parameters a_2^h for helicity h=0,+,- states receive different nonfactorizable contributions and hence they are helicity dependent, contrary to naive factorization where a_2^h are universal and polarization independent. QCD factorization breaks down even at the twist-2 level for transverse hard spectator interactions. Although a nontrivial strong phase for the A_\parallel amplitude can be achieved by adjusting the phase of an infrared divergent contribution, the present QCD factorization calculation cannot say anything definite about the phase phi_\parallel. Unlike B -> J/psi K decays, the longitudinal parameter a_2^0 for B -> J/psi K^* does not receive twist-3 corrections and is not large enough to account for the observed branching ratio and the fraction of longitudinal polarization. Possible enhancement mechanisms for a_2^0 are discussed.Comment: 21 pages, 1 figure, a table and a reference added, some typos correcte

    Testing QCD factorisation and charming penguins in charmless B→PV{\boldsymbol{B\to PV}}

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    We try a global fit of the experimental branching ratios and CP-asymmetries of the charmless B→PVB\to PV decays according to QCD factorisation. We find it impossible to reach a satisfactory agreement, the confidence level (CL) of the best fit is smaller than .1 %. The main reason for this failure is the difficulty to accomodate several large experimental branching ratios of the strange channels. Furthermore, experiment was not able to exclude a large direct CP asymmetry in B0ˉ→ρ+π−\bar {B^0}\to\rho^+ \pi^-, which is predicted very small by QCD factorisation. Trying a fit with QCD factorisation complemented by a charming-penguin inspired model we reach a best fit which is not excluded by experiment (CL of about 8 %) but is not fully convincing. These negative results must be tempered by the remark that some of the experimental data used are recent and might still evolve significantly.Comment: 21 pages, 4 figures; several typos corrected, added one footnote and two references, comments added about PQCD. To appear in Phys.Rev.

    A Detailed Analysis of One-loop Neutrino Masses from the Generic Supersymmetric Standard Model

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    In the generic supersymmetric standard model which had no global symmetry enforced by hand, lepton number violation is a natural consequence. Supersymmetry, hence, can be considered the source of experimentally demanded beyond standard model properties for the neutrinos. With an efficient formulation of the model, we perform a comprehensive detailed analysis of all one-loop contributions to neutrino masses.Comment: 27 pages Revtex, no figur

    One-loop Neutron Electric Dipole Moment from Supersymmetry without R-parity

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    We present a detailed analysis together with exact numerical calculations on one-loop contributions to neutron electric dipole moment from supersymmetry without R-parity, focusing on the gluino, chargino, and neutralino contributions. Apart from the neglected family mixing among quarks, complete formulae are given for the various contributions, through the quark dipole operators, to which the present study is restricted. We discuss the structure and main features of the R-parity violating contributions and the interplay between the R-parity conserving and violating parameters. In particular, the parameter combination ÎŒi∗λi11â€Č\mu_i^*\lambda^{\prime}_{i11}, under the optimal parametrization adopted, is shown to be solely responsible for the R-parity violating contributions in the supersymmetric loop diagrams. While ÎŒi∗λi11â€Č\mu_i^*\lambda^{\prime}_{i11} could bear a complex phase, the latter is not necessary to have a R-parity violating contribution.Comment: 43 pages Revtex with 15 eps- and 4 ps- figure files incoporated; proofread version to be published in Phys. Rev.

    Newly observed two-body decays of B mesons in a hybrid perspective

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    In consistency with the b --> c type of (quasi) two body decays, recently observed two body decays of B mesons are studied in a hybrid perspective in which their amplitude is given by a sum of factorizable and non-factorizable ones, and a role of the latter in these decays are discussed.Comment: 7 page

    Charmless two-body B decays: A global analysis with QCD factorization

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    In this paper, we perform a global analysis of B→PPB \to PP and PVPV decays with the QCD factorization approach. It is encouraging to observe that the predictions of QCD factorization are in good agreement with experiment. The best fit Îł\gamma is around 79∘79^\circ. The penguin-to-tree ratio ∣Pππ/TÏ€Ï€âˆŁ|P_{\pi \pi}/T_{\pi \pi}| of π+π−\pi^+ \pi^- decays is preferred to be larger than 0.3. We also show the confidence levels for some interesting channels: B0→π0π0B^0 \to \pi^0 \pi^0, K+K−K^+ K^- and B+→ωπ+B^+ \to \omega \pi^+, ωK+\omega K^+. For B→πK∗B \to \pi K^\ast decays, they are expected to have smaller branching ratios with more precise measurements.Comment: 20 pages, 4 figures, version to appear in Phys. Rev.

    Possible Large Direct CP Violations in Charmless B-Decays

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    We discuss the perturbative QCD approach for the exclusive two body B-meson decays to light mesons. We briefly review its ingredients and some important theoretical issues on factorization approach. We show numerical results which are compatible with present experimantal data for the charmless B-meson decays. Specailly we predict the possibility of large direct CP violation effects in B0→π+π−B^0 \to \pi^{+}\pi^{-} (23±7(23\pm7 %) and B0→K+π−B^0\to K^{+}\pi^{-} (−17±5(-17\pm5%). In the last section we investigate two methods to determine the weak phases ϕ2\phi_2 and ϕ3\phi_3 from B→ππ,KπB \to \pi\pi,K\pi processes. We obtain bounds on ϕ2\phi_2 and ϕ3\phi_3 from present experimental measurements.Comment: 18 pages, latex, 8 figures and 8 tables, typos corrected and added more tables and references. Presented at the 3rd workshop on Higher Luminosity B Factory, 6-7 August 2002, Kanagawa, Japan; Submitted to Phys. Rev.

    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
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