18,716 research outputs found

    Semi-Leptonic B Decay

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    The definitions and properties of elastic and inelastic Isgur-Wise form factors are reviewed. The nature of the "missing" exclusive semi-leptonic decay fraction is identified. The role that completeness sum rules play in relating form factors, spectroscopy, and model building is outlined.Comment: Latex2.09, uses sprocl.sty and epsf.sty. 10 pages with 3 postscript files included. Talk presented at the Conference on B Physics and CP Violation, March 24-27, 1997, Honolulu, Hawai

    Semi-leptonic B decays into higher charmed resonances

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    We apply HQET to semi-leptonic BB meson decays into a variety of excited charm states. Using three realistic meson models with fermionic light degrees of freedom, we examine the extent that the sum of exclusive single charmed states account for the inclusive semi-leptonic BB decay rate. The consistency of form factors with the Bjorken and Voloshin sum rules is also investigated.Comment: Latex, 27 pages. A few references and errors corrected, to appear in Phys. Rev.

    Instantaneous Bethe-Salpeter Equation: Analytic Approach for Nonvanishing Masses of the Bound-State Constituents

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    The instantaneous Bethe-Salpeter equation, derived from the general Bethe-Salpeter formalism by assuming that the involved interaction kernel is instantaneous, represents the most promising framework for the description of hadrons as bound states of quarks from first quantum-field-theoretic principles, that is, quantum chromodynamics. Here, by extending a previous analysis confined to the case of bound-state constituents with vanishing masses, we demonstrate that the instantaneous Bethe-Salpeter equation for bound-state constituents with (definitely) nonvanishing masses may be converted into an eigenvalue problem for an explicitly - more precisely, algebraically - known matrix, at least, for a rather wide class of interactions between these bound-state constituents. The advantages of the explicit knowledge of this matrix representation are self-evident.Comment: 12 Pages, LaTeX, 1 figur

    Bethe--Salpeter equation in QCD

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    We extend to regular QCD the derivation of a confining qqˉ q \bar{q} Bethe--Salpeter equation previously given for the simplest model of scalar QCD in which quarks are treated as spinless particles. We start from the same assumptions on the Wilson loop integral already adopted in the derivation of a semirelativistic heavy quark potential. We show that, by standard approximations, an effective meson squared mass operator can be obtained from our BS kernel and that, from this, by 1m2{1\over m^2} expansion the corresponding Wilson loop potential can be reobtained, spin--dependent and velocity--dependent terms included. We also show that, on the contrary, neglecting spin--dependent terms, relativistic flux tube model is reproduced.Comment: 23 pages, revte

    Two phase transitions in the fully frustrated XYXY model

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    The fully frustrated XYXY model on a square lattice is studied by means of Monte Carlo simulations. A Kosterlitz-Thouless transition is found at TKT0.446T_{\rm KT} \approx 0.446, followed by an ordinary Ising transition at a slightly higher temperature, Tc0.452T_c \approx 0.452. The non-Ising exponents reported by others, are explained as a failure of finite size scaling due to the screening length associated with the nearby Kosterlitz-Thouless transition.Comment: REVTEX file, 8 pages, 5 figures in uuencoded postscrip

    The Impact of NLO-Corrections on the Determination of the $\bar{u},\bar{d} Content of Nucleons from Drell-Yan Production

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    The interpretation of Drell-Yan production in terms of the antiquark densities depends on NLO corrections. Besides the NLO corrections to the familiar annihilation qqˉγl+lq\bar{q}\to \gamma^* \to l^+ l^-, there is a substantial contribution from the QCD Compton subprocesses gqqγql+lgq \to q\gamma^* \to q l^+ l^- and gqˉqγql+lg\bar{q} \to q\gamma^* \to q l^+ l^-. The beam and target dependence of the two classes of corrections is different. We discuss the impact of this difference on the determination of the dˉuˉ\bar{d}-\bar{u} asymmetry in the proton from the comparison of the pppp and pnpn Drell-Yan production.Comment: 4 pages, 1 eps-figure. To be published in Proceedings of DIS'9
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