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      Semileptonic form factors D to pi, K and B to pi, K from a fine lattice

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          Abstract

          We extract the form factors relevant for semileptonic decays of D and B mesons from a relativistic computation on a fine lattice in the quenched approximation. The lattice spacing is a=0.04 fm (corresponding to a^{-1}=4.97 GeV), which allows us to run very close to the physical B meson mass, and to reduce the systematic errors associated with the extrapolation in terms of a heavy quark expansion. For decays of D and D_s mesons, our results for the physical form factors at q^2=0 are as follows: f_+^{D to pi}(0)= 0.74(6)(4), f_+^{D to K}(0)= 0.78(5)(4) and f_+^{D_s to K}(0)=0.68(4)(3). Similarly, for B and B_s we find: f_+^{B to pi}(0)=0.27(7)(5), f_+^{B to K}(0)=0.32(6)(6) and f_+^{B_s to K}(0)=0.23(5)(4). We compare our results with other quenched and unquenched lattice calculations, as well as with light-cone sum rule predictions, finding good agreement.

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          Massive Fermions in Lattice Gauge Theory

          This paper presents a formulation of lattice fermions applicable to all quark masses, large and small. We incorporate interactions from previous light-fermion and heavy-fermion methods, and thus ensure a smooth connection to these limiting cases. The couplings in improved actions are evaluated for arbitrary fermion mass~mq, without expansions around small- or large-mass limits. We treat both the action and external currents. By interpreting on-shell improvement criteria through the lattice theory's Hamiltonian, one finds that cutoff artifacts factorize into the form bn(mqa)[\vekpa]sn, where \vekp is a momentum characteristic of the system under study, sn is related to the dimension of the nth interaction, and bn(mqa) is a bounded function, numerically always~\order(1) or less. In heavy-quark systems \vekp is typically rather smaller than the fermion mass~mq. Therefore, artifacts of order (mqa)s do not arise, even when mqa\gsim1. An important by-product of our analysis is an interpretation of the Wilson and Sheikholeslami-Wohlert actions applied to nonrelativistic fermions.
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            Improved Nonrelativistic QCD for Heavy Quark Physics

            We construct an improved version of nonrelativistic QCD for use in lattice simulations of heavy quark physics, with the goal of reducing systematic errors from all sources to below 10\%. We develop power counting rules to assess the importance of the various operators in the action and compute all leading order corrections required by relativity and finite lattice spacing. We discuss radiative corrections to tree level coupling constants, presenting a procedure that effectively resums the largest such corrections to all orders in perturbation theory. Finally, we comment on the size of nonperturbative contributions to the coupling constants.
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              Influence of theB*resonance onB¯→πeν¯e

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                Author and article information

                Journal
                10 March 2009
                2009-11-09
                Article
                10.1140/epja/i2009-10893-3
                0903.1664
                7004a79c-575d-4f76-b37e-9d65a2afa9c4

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                DESY 09-029
                Eur.Phys.J.A43:107-120,2010
                1+18 pages, 19 eps figures; v2: 1+22 pages, discussion extended, references added, version accepted for publication in EPJ A
                hep-lat hep-ex hep-ph

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