10,833 research outputs found

    Charming Penguins in B decays

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    Full expressions of the Bd0→π+π−B^0_d \to \pi^+ \pi^- and Bd0→π0π0B^0_d \to \pi^0 \pi^0 amplitudes, given in terms of matrix elements of operators of the effective weak Hamiltonian, are used to study the dependence of the relevant branching ratios on the different contributions. The uncertainty in the extraction of the weak phase α\alpha from the measurement of the time-dependent asymmetry in Bd0→π+π−B^0_d \to \pi^+ \pi^- decays is also analyzed. We find that, among several effects which may enhance the Bd0→π0π0B^0_d \to \pi^0 \pi^0 branching ratio, the most important is due to ``charming penguin" diagrams that have never been studied before. These diagrams easily increase BR(Bd0→π0π0)BR(B^0_d \to \pi^0 \pi^0) up to a value of 1−3×10−61-3 \times 10^{-6}. The same effect produces, however, a large error in the extraction of α\alpha from the measurement of the Bd0→π+π−B^0_d \to \pi^+ \pi^- time-dependent asymmetry. We show that it is possible to determine charming-penguin amplitudes from the experimental measurement of many decay rates. Their effect is impressive in B+→π+K0B^+ \to \pi^+ K^0 and Bd0→K+π−B^0_d \to K^+ \pi^- decays, where charming-penguin contributions easily give values of BR(B+→π+K0)BR(B^+ \to \pi^+ K^0) and BR(Bd0→K+π−)BR(B^0_d \to K^+ \pi^-) of about 1×10−51 \times 10^{-5}. Among other possibilities, we also suggest to use Bd0→K0Kˉ0B^0_d \to K^0 \bar K^0, the BR of which can be as large as 2−3×10−62-3 \times 10^{-6}, to determine the size of charming-penguin amplitudes.Comment: LaTeX, 28 pages, 8 figure

    Scheme Independence of the Effective Hamiltonian for b→s γb \rightarrow s \, \gamma and b→s gb \rightarrow s \, g Decays

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    We present a calculation of the effective weak Hamiltonian which governs b→s γb \rightarrow s\, \gamma and b→s gb \rightarrow s \, g transitions in two different renormalization schemes (NDR and HV). In the leading logarithmic approximation, we show that the coefficients of the effective Hamiltonian are scheme independent only when one takes correctly into account the scheme dependence of one- and two- loop diagrams. We demonstrate that in NDR there are contributions which were missed in previous calculations. These contributions are necessary to obtain scheme independent coefficients in the final results.Comment: 16 pp + 5 figures not included (available by anonymous ftp at amisan.iss.infn.it (141.108.15.215), directory /ftp/bsgamma), LaTeX, LPTENS 93/28, ROME 93/958, ULB-TH 93/0

    Penguin Contractions and Factorization in B -> K pi Decays

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    We study Lambda_{QCD}/m_B corrections to factorization in B -> K pi decays. First, we analyze these decay channels within factorization, showing that, irrespectively of the value of gamma, it is not possible to reproduce the experimental data. Then, we discuss Lambda_{QCD}/m_B corrections to these processes, and argue that there is a class of doubly Cabibbo enhanced non-factorizable contributions, usually called charming penguins, that cannot be neglected. Including these corrections, we obtain an excellent agreement with experimental data. Furthermore, contrary to what is obtained with factorization, we predict sizable rate asymmetries in B^\pm -> K^\pm \pi^0 and B -> K^\pm pi^\mp.Comment: 4 pages, 3 figures. Talk given by L. Silvestrini at BCP4, Ise-Shima, Japan, 18-23 Feb 200

    Charming Penguins Saga

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    We briefly recall the main formulae for computing the B -> K pi branching ratios within the "charming penguin" approach, present an updated fit to the data, and explain why we believe that, in general, these fits can hardly be used to extract gamma.Comment: Invited talk at FPCP '02 given by M. Ciuchini, uses econfmacros.tex. Final version with minor changes to appear in the proceeding

    Two Body B Decays, Factorization and LambdaQCD/mb Corrections

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    By using the recent experimental measurements of B -> pi pi and B -> K pi branching ratios, we find that the amplitudes computed at the leading order of the LambdaQCD/mb expansion disagree with the observed BRs, even taking into account the uncertainties of the input parameters. Beyond the leading order, Charming and GIM penguins allow to reconcile the theoretical predictions with the data. Because of these large effects, we conclude, however, that it is not possible, with the present theoretical and experimental accuracy, to determine the CP violation angle gamma from these decays. We compare our results with those obtained with the parametrization of the chirally enhanced non-perturbative contributions by BBNS. We also predict large asymmetries for several of the particle--antiparticle BRs, in particular BR(B+ -> K+ pi0), BR(Bd -> K+ pi-) and BR(Bd -> pi+ pi-).Comment: 14 pages 3 figures uses aippro

    Two-body nonleptonic B decays in the Standard Model and beyond

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    We briefly discuss the phenomenology of B to pi pi, B to K pi and B to phi K decays in the Standard Model and in Supersymmetry.Comment: 7 pages, 2 figures, uses moriond.sty. Talk given by L. Silvestrini at the XXXIXth Rencontres de Moriond on ElectroWeak Interactions and Unified Theories, La Thuile, Aosta Valley, Italy, March 21st-28th 200

    Factorization, charming penguins, and all that

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    We discuss few selected topics related to the calculation of hadronic amplitudes relevant for two-body non-leptonic B decays.Comment: LaTeX, 9 pages, 1 eps figure included, uses psfig.sty. Talk given by M.C. at Beauty '97, UCLA, USA, October 13-17, 199
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