5,914 research outputs found

    Radiative, actively cooled panel tests results

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    The radiative, actively cooled panel designed to withstand a uniform incident heat flux of 136 kW/sq m to a 444 K surface temperature was evaluated. The test program consisted of preliminary static thermal mechanical loading and aerothermal flow tests. Test results are briefly discussed

    Quantization of Fayet-Iliopoulos Parameters in Supergravity

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    In this short note we discuss quantization of the Fayet-Iliopoulos parameter in supergravity theories. We argue that in supergravity, the Fayet-Iliopoulos parameter determines a lift of the group action to a line bundle, and such lifts are quantized. Just as D-terms in rigid N=1 supersymmetry are interpreted in terms of moment maps and symplectic reductions, we argue that in supergravity the quantization of the Fayet-Iliopoulos parameter has a natural understanding in terms of linearizations in geometric invariant theory (GIT) quotients, the algebro-geometric version of symplectic quotients.Comment: 21 pages, utarticle class; v2: typos and tex issue fixe

    High Precision determination of the pi, K, D and D_s decay constants from lattice QCD

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    We determine DD and DsD_s decay constants from lattice QCD with 2% errors, 4 times better than experiment and previous theory: fDsf_{D_s} = 241(3) MeV, fDf_D = 207(4) MeV and fDs/fDf_{D_s}/f_D = 1.164(11). We also obtain fK/fπf_K/f_{\pi} = 1.189(7) and (fDs/fD)/(fK/fπ)(f_{D_s}/f_D)/(f_K/f_{\pi}) = 0.979(11). Combining with experiment gives VusV_{us}=0.2262(14) and Vcs/VcdV_{cs}/V_{cd} of 4.43(41). We use a highly improved quark discretization on MILC gluon fields that include realistic sea quarks fixing the u/d,su/d, s and cc masses from the π\pi, KK, and ηc\eta_c meson masses. This allows a stringent test against experiment for DD and DsD_s masses for the first time (to within 7 MeV).Comment: 4 pages, 2 figures. Published version - changes from original include a more extensive discussion of errors and an error budget table covering more quantities. There are very small changes in some of the values reporte

    The Kaon BB-parameter with Wilson Fermions

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    We calculate the kaon BB-parameter in quenched lattice QCD at β=6.0\beta=6.0 using Wilson fermions at κ=0.154\kappa=0.154 and 0.1550.155. We use two kinds of non-local (``smeared'') sources for quark propagators to calculate the matrix elements between states of definite momentum. The use of smeared sources yields results with much smaller errors than obtained in previous calculations with Wilson fermions. By combining results for p=(0,0,0)\vec p =(0,0,0) and p=(0,0,1)\vec p =(0,0,1), we show that one can carry out the non-perturbative subtraction necessary to remove the dominant lattice artifacts induced by the chiral symmetry breaking term in the Wilson action. Our final results are in good agreement with those obtained using staggered fermions. We also present results for BB-parameters of the ΔI=3/2\Delta I = 3/2 part of the electromagnetic penguin operators, and preliminary results for \bk\ in the presence of two flavors of dynamical quarks.Comment: 39 pages, including 9 PS figures (LA UR-91-3522

    Non-birational twisted derived equivalences in abelian GLSMs

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    In this paper we discuss some examples of abelian gauged linear sigma models realizing twisted derived equivalences between non-birational spaces, and realizing geometries in novel fashions. Examples of gauged linear sigma models with non-birational Kahler phases are a relatively new phenomenon. Most of our examples involve gauged linear sigma models for complete intersections of quadric hypersurfaces, though we also discuss some more general cases and their interpretation. We also propose a more general understanding of the relationship between Kahler phases of gauged linear sigma models, namely that they are related by (and realize) Kuznetsov's `homological projective duality.' Along the way, we shall see how `noncommutative spaces' (in Kontsevich's sense) are realized physically in gauged linear sigma models, providing examples of new types of conformal field theories. Throughout, the physical realization of stacks plays a key role in interpreting physical structures appearing in GLSMs, and we find that stacks are implicitly much more common in GLSMs than previously realized.Comment: 54 pages, LaTeX; v2: typo fixe

    Hadron Spectrum with Wilson fermions

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    We present results of a high statistics study of the quenched spectrum using Wilson fermions at β=6.0\beta=6.0 on 323×6432^3 \times 64 lattices. We calculate the masses of mesons and baryons composed of both degenerate and non-degenerate quarks. Using non-degenerate quark combinations allows us to study baryon mass splittings in detail. We find significant deviations from the lowest order chiral expansion, deviations that are consistent with the expectations of quenched chiral perturbation theory. We find that there is a 20\sim 20% systematic error in the extracted value of msm_s, depending on the meson mass ratio used to set its value. Using the largest estimate of msm_s we find that the extrapolated octet mass-splittings are in agreement with the experimental values, as is MΔMNM_\Delta - M_N, while the decuplet splittings are 30% smaller than experiment. Combining our results with data from the GF11 collaboration we find considerable ambiguity in the extrapolation to the continuum limit. Our preferred values are MN/Mρ=1.38(7)M_N / M_\rho = 1.38(7) and MΔ/Mρ=1.73(10)M_\Delta / M_\rho = 1.73(10), suggesting that the quenched approximation is good to only 1015\sim 10-15%. We also analyze the O(ma)O(ma) discretization errors in heavy quark masses.Comment: 52 pages. Tex. Modified "axis" source for figures also included. Needs macro packages lanlmac and epsf. Uses hyperbasics if available. Significant number of typographical errors correcte

    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 BπB\to\pi and DKD\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.

    Update: Accurate Determinations of alpha_s from Realistic Lattice QCD

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    We use lattice QCD simulations, with MILC configurations (including vacuum polarization from u, d, and s quarks), to update our previous determinations of the QCD coupling constant. Our new analysis uses results from 6 different lattice spacings and 12 different combinations of sea-quark masses to significantly reduce our previous errors. We also correct for finite-lattice-spacing errors in the scale setting, and for nonperturbative chiral corrections to the 22 short-distance quantities from which we extract the coupling. Our final result is alpha_V(7.5GeV,nf=3) = 0.2120(28), which is equivalent to alpha_msbar(M_Z,n_f=5)= 0.1183(8). We compare this with our previous result, which differs by one standard deviation.Comment: 12 pages, 2 figures, 4 table

    Kaon B parameter from quenched Lattice QCD

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    We present results of a large-scale simulation for the Kaon B parameter BKB_K in quenched lattice QCD with the Kogut-Susskind quark action. Calculating BKB_K at 1% statistical accuracy for seven values of lattice spacing in the range a0.240.04a\approx 0.24-0.04 fm on lattices up to 563×9656^3\times 96, we verify a quadratic aa dependence of BKB_K theoretically predicted. Strong indications are found that, with our level of accuracy, αMSˉ(1/a)2\alpha_{\bar{MS}}(1/a)^2 terms arising from our one-loop matching procedure have to be included in the continuum extrapolation. We present BKB_K(NDR, 2 GeV)=0.628(42) as our final value, as obtained by a fit including the αMSˉ(1/a)2\alpha_{\bar{MS}}(1/a)^2 term.Comment: 8 pages, Latex(revtex, epsf), 2 epsf figure
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