401 research outputs found

    1++1^{++} Nonet Singlet-Octet Mixing Angle, Strange Quark Mass, and Strange Quark Condensate

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    Two strategies are taken into account to determine the f1(1420)f_1(1420)-f1(1285)f_1(1285) mixing angle θ\theta. (i) First, using the Gell-Mann-Okubo mass formula together with the K1(1270)K_1(1270)-K1(1400)K_1(1400) mixing angle θK1=(34±13)\theta_{K_1}=(-34\pm 13)^\circ extracted from the data for B(BK1(1270)γ),B(BK1(1400)γ),B(τK1(1270)ντ){\cal B}(B\to K_1(1270) \gamma), {\cal B}(B\to K_1(1400) \gamma), {\cal B}(\tau\to K_1(1270) \nu_\tau), and B(τK1(1420)ντ){\cal B}(\tau\to K_1(1420) \nu_\tau), gave θ=(2323+17)\theta = (23^{+17}_{-23})^\circ. (ii) Second, from the study of the ratio for f1(1285)ϕγf_1(1285) \to \phi\gamma and f1(1285)ρ0γf_1(1285) \to \rho^0\gamma branching fractions, we have two-fold solution θ=(19.44.6+4.5)\theta=(19.4^{+4.5}_{-4.6})^\circ or (51.14.6+4.5)(51.1^{+4.5}_{-4.6})^\circ. Combining these two analyses, we thus obtain θ=(19.44.6+4.5)\theta=(19.4^{+4.5}_{-4.6})^\circ. We further compute the strange quark mass and strange quark condensate from the analysis of the f1(1420)f1(1285)f_1(1420)-f_1(1285) mass difference QCD sum rule, where the operator-product-expansion series is up to dimension six and to O(αs3,ms2αs2){\cal O}(\alpha_s^3, m_s^2 \alpha_s^2) accuracy. Using the average of the recent lattice results and the θ\theta value that we have obtained as inputs, we get /=0.41±0.09/ =0.41 \pm 0.09.Comment: 10 pages, 1 table, published versio

    GPU-based simulations of fracture in idealized brick and mortar composites

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    Stiff ceramic platelets (or bricks) that are aligned and bonded to a second ductile phase with low volume fraction (mortar) are a promising pathway to produce stiff, high-toughness composites. For certain ranges of constituent properties, including those of some synthetic analogs to nacre, one can demonstrate that the deformation is dominated by relative brick motions. This paper describes simulations of fracture that explicitly track the motions of individual rigid bricks in an idealized microstructure; cohesive tractions acting between the bricks introduce elastic, plastic and rupture behaviors. Results are presented for the stresses and damage near macroscopic cracks with different brick orientations relative to the loading orientation. The anisotropic macroscopic initiation toughness is computed for small-scale yielding conditions and is shown to be independent of specimen geometry and loading configuration. The results are shown to be in agreement with previously published experiments on synthetic nacre

    Impact of Subleading Corrections on Hadronic B Decays

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    We study the subleading corrections originating from the 3-parton (q\bar q g) Fock states of final-state mesons in B decays. The corrections could give significant contributions to decays involving an \omega or \eta^{(\prime)} in the final states. Our results indicate the similarity of \omega K and \omega \pi^- rates, of order 5\times 10^{-6}, consistent with the recent measurements. We obtain a_2(B\to J/\psi K)\approx 0.27+0.05i, in good agreement with data. Without resorting to the unknown singlet annihilation effects, 3-parton Fock state contributions can enhance the branching ratios of K\eta' to the level above 50\times 10^{-6}.Comment: 5 pages, 5 figures, revtex4; some typos corrected, a new figure and a reference added, more explanations for the calculation provided, to appear in Phys. Rev.

    Pd/Cu Site Interchange and Non-Fermi-Liquid Behavior in UCu_4Pd

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    X-ray-absorption fine-structure measurements of the local structure in UCu_4Pd are described which indicate a probable lattice-disorder origin for non-Fermi-liquid behavior in this material. Short Pd-Cu distances are observed, consistent with 24 +/- 3% of the Pd atoms occupying nominally Cu sites. A "Kondo disorder" model, based on the effect on the local Kondo temperature T_K of this interchange and some additional bond-length disorder, agrees quantitatively with previous experimental susceptibility data, and therefore also with specific heat and magnetic resonance experiments.Comment: 4 pages, 3 PostScript figures, to be published in PR

    Local lattice disorder in the geometrically-frustrated spin glass pyrochlore Y2Mo2O7

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    The geometrically-frustrated spin glass Y2Mo2O7 has been considered widely to be crystallographically ordered with a unique nearest neighbor magnetic exchange interaction, J. To test this assertion, we present x-ray-absorption fine-structure results for the Mo and Y K edges as a function of temperature and compare them to results from a well-ordered pyrochlore, Tl2Mn2O7. We find that the Mo-Mo pair distances are significantly disordered at approximately right angles to the Y-Mo pairs. These results strongly suggest that lattice disorder nucleates the spin-glass phase in this material.Comment: 9 pages, 2 Postscript figures, Phys. Rev. B: Rapid, in pres

    Born Effective Charges of Barium Titanate: band by band decomposition and sensitivity to structural features

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    The Born effective charge tensors of Barium Titanate have been calculated for each of its 4 phases. Large effective charges of Ti and O, also predicted by shell model calculations and made plausible by a simplified model, reflect the partial covalent character of the chemical bond. A band by band decomposition confirms that orbital hybridization is not restricted to Ti and O atoms but also involves Ba which appears more covalent than generally assumed. Our calculations reveal a strong dependence of the effective charges on the atomic positions contrasting with a relative insensitivity on isotropic volume changes.Comment: 13 page

    Indications for Factorization and ReVub<0Re V_{ub} < 0 from Rare B Decay Data

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    Surveying known hadronic rare B decays, we find that the factorization approximation can give a coherent account of KπK\pi, ππ\pi\pi and ρ0π+\rho^0\pi^+ data and give predictions for ω0π+\omega^0\pi^+, ρπ\rho\pi and KπK^*\pi modes, {\it if ReVub{Re}V_{ub} is taken as negative} (in standard phase convention) rather than positive. As further confirmation, we expect a lower sin2β\sin2\beta value at B Factories as compared to current fits, and BsB_s mixing close to LEP bounds at SLD and CDF.Comment: 11 pages, revtex, 4 figures (unchanged and eps files included); version (including title and abstract change) to appear in Phys. Rev. Let
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