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      Weak Radiative B-Meson Decay Beyond Leading Logarithms

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          Abstract

          We present our results for three-loop anomalous dimensions necessary in analyzing \(B{\to}X_s\gamma\) decay at the next-to-leading order in QCD. We combine them with other recently calculated contributions, obtaining a practically complete next-to-leading order prediction for the branching ratio \({\cal B}(B{\to}X_s\gamma) = (3.28 \pm 0.33) \times 10^{-4}\). The uncertainty is more than twice smaller than in the previously available leading order theoretical result. The Standard Model prediction remains in agreement with the CLEO measurement at the \(2 \sigma\) level.

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          Effective Hamiltonian forΔS=1weak nonleptonic decays in the six-quark model

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            Nonperturbative Contributions to the Inclusive Rare Decays \(B\to X_s\gamma\) and \(B\to X_s\ell^+\ell^-\)

            We discuss nonperturbative contributions to the inclusive rare \(B\) decays \(B\to X_s\gamma\) and \(B\to X_s\ell^+\ell^-\). We employ an operator product expansion and the heavy quark effective theory to compute the leading corrections to the decay rate found in the free quark decay model, which is exact in the limit \(m_b\to\infty\). These corrections are of relative order \(1/m_b^2\), and may be parameterised in terms of two low-energy parameters. We also discuss the corrections to other observables, such as the average photon energy in \(B\to X_s\gamma\) and the lepton invariant mass spectrum in \(B\to X_s\ell^+\ell^-\).
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              Analysis of the Photon Spectrum in Inclusive \(B\to X_s\,\gamma\) Decays

              Using a combination of the operator product and heavy quark expansions, we resum the leading nonperturbative contributions to the inclusive photon spectrum in \(B\to X_s\,\gamma\) decays. The shape of the spectrum is determined by a universal structure function, which describes the distribution of the light-cone momentum of the \(b\)-quark inside the \(B\)-meson. The moments of this function are proportional to forward matrix elements of higher-dimension operators. As a by-product, we obtain the bound \(\lambda_1<0\) for one of the parameters of the heavy quark effective theory. The integral over the \(B\to X_s\,\gamma\) structure function is related to the shape function that governs the fall-off of the lepton spectrum close to the endpoint in \(B\to X_u\,\ell\,\bar\nu\) decays. A measurement of the photon spectrum in rare \(B\)-decays can therefore help to obtain a model-independent determination of \(V_{ub}\).
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                Author and article information

                Journal
                10 December 1996
                1998-02-20
                Article
                10.1016/S0370-2693(97)00324-9
                hep-ph/9612313
                53c4781b-1457-4909-a7c9-4f508aa7eaa1
                History
                Custom metadata
                Phys.Lett.B400:206-219,1997; Erratum-ibid.B425:414,1998
                Formulae for f_88(delta), f_78(delta), f_12(delta) and the first equation in Appendix B corrected
                hep-ph

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