1,250 research outputs found

    A model independent determination of ∣Vub∣|V_{ub}| using the global q2q^2 dependence of the dispersive bounds on the B→πlνB\to\pi l\nu form factors

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    We propose a method to determine the CKM matrix element ∣Vub∣|V_{ub}| using the global q2q^2 dependence of the dispersive bound on the form factors for B→πlνB\to \pi l\nu decay. Since the lattice calculation of the B→πlνB\to \pi l\nu form factor is limited to the large q2q^2 regime, only the experimental data in a limited kinematic range can be used in a conventional method. In our new method which exploits the statistical distributions of the dispersive bound proposed by Lellouch, we can utilize the information of the global q2q^2 dependence for all kinematic range. As a feasibility study we determine ∣Vub∣|V_{ub}| by combining the form factors from quenched lattice QCD, the dispersive bounds, and the experimental data by CLEO. We show that the accuracy of ∣Vub∣|V_{ub}| can be improved by our method.Comment: 12 pages, 13 figure

    Charmonium spectroscopy with heavy Kogut-Susskind quarks

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    Charmonium spectroscopy with Kogut-Susskind valence quarks are carried out for quenched QCD at β=6.0\beta=6.0 and for two-flavor full QCD at β=5.7\beta=5.7. Results for 1P--1S mass splitting and estimates of αMS‾(5)(mZ)\alpha^{(5)}_{\overline{MS}}(m_Z) are reported. Problems associated with flavor breaking effects and finite size effects of 1P1P states are discussed.Comment: 3 pages, contribution to the Lattice '94 conference, uuencoded compressed ps-fil

    Dual-camera system for high-speed imaging in particle image velocimetry

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    Particle image velocimetry is an important technique in experimental fluid mechanics, for which it has been essential to use a specialized high-speed camera. However, the high speed is at the expense of other performances of the camera, i.e., sensitivity and image resolution. Here, we demonstrate that the high-speed imaging is also possible with a pair of still cameras.Comment: 4 pages, accepted by Journal of Visualization (see http://www.springerlink.com

    Charmed hadron physics in quenched anisotropic lattice QCD

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    We investigate the anisotropic lattice with O(a)O(a) improved quark action as a candidate of framework in which we can treat both the heavy and light quark region in the same manner and systematically reduce the systematic uncertainties. To examine applicability of anisotropic lattice, we calculate the charmed meson spectrum and decay constants in quenched approximation. We find consistent result with most advanced results on isotropic lattices.Comment: 3 pages, 1 figure, contribution to Fifth KEK Topical Conference - Frontiers in Flavor Physics -, Tsukuba, Japan, November 20-22, 200

    Sea Quark Effects on the Strong Coupling Constant

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    We present results showing that the strong coupling constant measured in two-flavor full QCD with dynamical Kogut-Susskind quarks at β=5.7\beta=5.7 exhibit a 15\% increase due to sea quarks over that for quenched QCD at the scale μ≈7\mu\approx 7GeV . (talk at lattice93)Comment: 3 pages, compressed, uuencoded PostScript file(name:lat93ch.ps.Z

    Heavy-Light Semileptonic Decays in Staggered Chiral Perturbation Theory

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    We calculate the form factors for the semileptonic decays of heavy-light pseudoscalar mesons in partially quenched staggered chiral perturbation theory (\schpt), working to leading order in 1/mQ1/m_Q, where mQm_Q is the heavy quark mass. We take the light meson in the final state to be a pseudoscalar corresponding to the exact chiral symmetry of staggered quarks. The treatment assumes the validity of the standard prescription for representing the staggered ``fourth root trick'' within \schpt by insertions of factors of 1/4 for each sea quark loop. Our calculation is based on an existing partially quenched continuum chiral perturbation theory calculation with degenerate sea quarks by Becirevic, Prelovsek and Zupan, which we generalize to the staggered (and non-degenerate) case. As a by-product, we obtain the continuum partially quenched results with non-degenerate sea quarks. We analyze the effects of non-leading chiral terms, and find a relation among the coefficients governing the analytic valence mass dependence at this order. Our results are useful in analyzing lattice computations of form factors B→πB\to\pi and D→KD\to K when the light quarks are simulated with the staggered action.Comment: 53 pages, 8 figures, v2: Minor correction to the section on finite volume effects, and typos fixed. Version to be published in Phys. Rev.

    Nucleon sigma term and strange quark content from lattice QCD with exact chiral symmetry

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    We calculate the nucleon sigma term in two-flavor lattice QCD utilizing the Feynman-Hellman theorem. Both sea and valence quarks are described by the overlap fermion formulation, which preserves exact chiral and flavor symmetries on the lattice. We analyse the lattice data for the nucleon mass using the analytical formulae derived from the baryon chiral perturbation theory. From the data at valence quark mass set different from sea quark mass, we may extract the sea quark contribution to the sigma term, which corresponds to the strange quark content. We find that the strange quark content is much smaller than the previous lattice calculations and phenomenological estimates.Comment: 27 page

    Ferromagnetism in a Hubbard model for an atomic quantum wire: a realization of flat-band magnetism from even-membered rings

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    We have examined a Hubbard model on a chain of squares, which was proposed by Yajima et al as a model of an atomic quantum wire As/Si(100), to show that the flat-band ferromagnetism according to a kind of Mielke-Tasaki mechanism should be realized for an appropriate band filling in such a non-frustrated lattice. Reflecting the fact that the flat band is not a bottom one, the ferromagnetism vanishes, rather than intensified, as the Hubbard U is increased. The exact diagonalization method is used to show that the critical value of U is in a realistic range. We also discussed the robustness of the magnetism against the degradation of the flatness of the band.Comment: misleading terms and expressions are corrected, 4 pages, RevTex, 5 figures in Postscript, to be published in Phys. Rev. B (rapid communication
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