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      Shape function effects in B -> X_s gamma and B -> X_u l nu decays

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          Abstract

          We calculate the decay distributions for inclusive B -> X_s gamma and B -> X_u l nu decays in the endpoint region, where radiative corrections are large. The computation is done using effective field theory methods. The matching coefficients are computed to O(alpha_s), and the anomalous dimensions to next-to-leading order. The final expressions for the differential decay spectra include the complete O(alpha_s) corrections, and sum the leading and next-to-leading Sudakov series. We present results for regions of phase space where the shape function can be expanded in local operators, and give the matching coefficients of the resulting enhanced non-perturbative effects to order alpha_s. We show that moments of the shape function {\it are not} given by moments of local operators once perturbative effects are included, explain why the shape function and its moments satisfy different renormalization group equations, and contrast this with the situation for deep inelastic scattering. We show that there are large perturbative corrections in the usual definition of the shape function. This renders incorrect previous prescriptions for combining radiative corrections with the shape function.

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          An effective field theory for collinear and soft gluons: heavy to light decays

          We construct the Lagrangian for an effective theory of highly energetic quarks with energy Q, interacting with collinear and soft gluons. This theory has two low energy scales, the transverse momentum of the collinear particles, p_perp, and the scale p_perp^2/Q. The heavy to light currents are matched onto operators in the effective theory at one-loop and the renormalization group equations for the corresponding Wilson coefficients are solved. This running is used to sum Sudakov logarithms in inclusive B -> X_s gamma and B -> X_u \ell nu decays. We also show that the interactions with collinear gluons preserve the relations for the soft part of the form factor for heavy to light decays found by Charles et al., establishing these relations in the large energy limit of QCD.
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            Inclusive Semileptonic B and Polarized Lambda_b Decays from QCD

            The differential decay spectrum \(d\Gamma/dE_e dq^2\) for the semileptonic decay of an unpolarized hadron containing a b-quark, and the decay spectrum \(d\Gamma/dE_e dq^2 d\!\cos\theta\) for polarized \(\Lambda_b\) decay are computed to second order in the \(1/m_b\) expansion. Most of the \(1/m_b^2\) corrections have a simple physical interpretation, which is discussed in detail. The implications of the results for the determination of \(V_{ub}\) are discussed. The decay spectra for semileptonic decay of hadrons containing a c-quark are also given. There is a subtlety in the use of the equations of motion at order \(1/m_b^2\) in the heavy quark expansion which is explained.
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              Soft-Collinear Factorization in Effective Field Theory

              The factorization of soft and ultrasoft gluons from collinear particles is shown at the level of operators in an effective field theory. Exclusive hadronic factorization and inclusive partonic factorization follow as special cases. The leading order Lagrangian is derived using power counting and gauge invariance in the effective theory. Several species of gluons are required, and softer gluons appear as background fields to gluons with harder momenta. Two examples are given: the factorization of soft gluons in B->D pi, and the soft-collinear convolution for the B->Xs gamma spectrum.
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                Author and article information

                Journal
                09 December 2003
                Article
                10.1103/PhysRevD.70.034024
                hep-ph/0312109
                9567c3b0-839e-4bda-afc4-2a55016e0f5c
                History
                Custom metadata
                CALT-68-2465
                Phys.Rev.D70:034024,2004
                20 pages
                hep-ph

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