25,767 research outputs found

    The Lorentzian distance formula in noncommutative geometry

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    For almost twenty years, a search for a Lorentzian version of the well-known Connes' distance formula has been undertaken. Several authors have contributed to this search, providing important milestones, and the time has now come to put those elements together in order to get a valid and functional formula. This paper presents a historical review of the construction and the proof of a Lorentzian distance formula suitable for noncommutative geometry.Comment: 16 pages, final form, few references adde

    Heavy-heavy form factors and generalized factorization

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    We reanalyze B -> D pi and B -> K J/psi data to extract a set of parameters which give the relevant hadronic matrix elements in terms of factorized amplitudes. Various sources of theoretical uncertainties are studied, in particular those depending on the model adopted for the form factors. We find that the fit to the B -> D pi branching ratios substantially depends on the model describing the Isgur-Wise function and on the value of its slope. This dependence can be reduced by substituting the BR(B -> D pi) with suitable ratios of non-leptonic to differential semileptonic BRs. In this way, we obtain a model-independent determination of these parameters. Using these results, the B -> D form factors at q^2=M_pi^2 can be extracted from a fit of the BR(B -> D pi). The comparison between the form factors obtained in this way and the corresponding measurements in semileptonic decays can be used as a test of (generalized) factorization free from the uncertainties due to heavy-heavy form factor modeling. Finally, we present predictions for yet-unmeasured D pi and D K branching ratios and extract f_{D_s} and f_{D_s^*} from B -> DD_s decays. We find f_{D_s} = 270 +- 45 MeV and f_{D_s^*}=260 +- 40 MeV, in good agreement with recent measurements and lattice calculations.Comment: 20 pages, 16 ps/eps files, uses epsfig.sty; exp. numbers update

    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 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
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