4,676 research outputs found

    MRI and clinical characteristics of suspected cerebrovascular accident in nine cats

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    Pressure-induced phase transitions in AgClO4

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    AgClO4 has been studied under compression by x-ray diffraction and density functional theory calculations. Experimental evidence of a structural phase transition from the tetragonal structure of AgClO4 to an orthorhombic barite-type structure has been found at 5.1 GPa. The transition is supported by total-energy calculations. In addition, a second transition to a monoclinic structure is theoretically proposed to take place beyond 17 GPa. The equation of state of the different phases is reported as well as the calculated Raman-active phonons and their pressure evolution. Finally, we provide a description of all the structures of AgClO4 and discuss their relationships. The structures are also compared with those of AgCl in order to explain the structural sequence determined for AgClO4.Comment: 38 pages, 11 figures, 4 table

    Sparse bounds for pseudodifferential operators

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    We prove sparse bounds for pseudodifferential operators associated to H\"ormander symbol classes. Our sparse bounds are sharp up to the endpoint and rely on a single scale analysis. As a consequence, we deduce a range of weighted estimates for pseudodifferential operators. The results naturally apply to the context of oscillatory Fourier multipliers, with applications to dispersive equations and oscillatory convolution kernels

    Endpoint Sobolev continuity of the fractional maximal function in higher dimensions

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    We establish continuity mapping properties of the non-centered fractional maximal operator MβM_{\beta} in the endpoint input space W1,1(Rd)W^{1,1}(\mathbb{R}^d) for d≥2d \geq 2 in the cases for which its boundedness is known. More precisely, we prove that for q=d/(d−β)q=d/(d-\beta) the map f↦∣∇Mβf∣f \mapsto |\nabla M_\beta f| is continuous from W1,1(Rd)W^{1,1}(\mathbb{R}^d) to Lq(Rd)L^{q}(\mathbb{R}^d) for 0<β<1 0 < \beta < 1 if ff is radial and for 1≤β<d1 \leq \beta < d for general ff. The results for 1≤β<d1\leq \beta < d extend to the centered counterpart MβcM_\beta^c. Moreover, if d=1d=1, we show that the conjectured boundedness of that map for MβcM_\beta^c implies its continuity

    Bilinear identities involving the kk-plane transform and Fourier extension operators

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    We prove certain L2(Rn)L^2(\mathbb{R}^n) bilinear estimates for Fourier extension operators associated to spheres and hyperboloids under the action of the kk-plane transform. As the estimates are L2L^2-based, they follow from bilinear identities: in particular, these are the analogues of a known identity for paraboloids, and may be seen as higher-dimensional versions of the classical L2(R2)L^2(\mathbb{R}^2)-bilinear identity for Fourier extension operators associated to curves in R2\mathbb{R}^2

    Regularity of fractional maximal functions through Fourier multipliers

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    We prove endpoint bounds for derivatives of fractional maximal functions with either smooth convolution kernel or lacunary set of radii in dimensions n≥2n \geq 2. We also show that the spherical fractional maximal function maps LpL^p into a first order Sobolev space in dimensions n≥5n \geq 5

    Sharp local smoothing estimates for Fourier integral operators

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    The theory of Fourier integral operators is surveyed, with an emphasis on local smoothing estimates and their applications. After reviewing the classical background, we describe some recent work of the authors which established sharp local smoothing estimates for a natural class of Fourier integral operators. We also show how local smoothing estimates imply oscillatory integral estimates and obtain a maximal variant of an oscillatory integral estimate of Stein. Together with an oscillatory integral counterexample of Bourgain, this shows that our local smoothing estimates are sharp in odd spatial dimensions. Motivated by related counterexamples, we formulate local smoothing conjectures which take into account natural geometric assumptions arising from the structure of the Fourier integrals
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