620 research outputs found

    Analyticity of layer potentials and L2L^{2} solvability of boundary value problems for divergence form elliptic equations with complex L∞L^{\infty} coefficients

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    We consider divergence form elliptic operators of the form L=-\dv A(x)\nabla, defined in Rn+1={(x,t)∈Rn×R}R^{n+1} = \{(x,t)\in R^n \times R \}, n≥2n \geq 2, where the L∞L^{\infty} coefficient matrix AA is (n+1)×(n+1)(n+1)\times(n+1), uniformly elliptic, complex and tt-independent. We show that for such operators, boundedness and invertibility of the corresponding layer potential operators on L2(Rn)=L2(∂R+n+1)L^2(\mathbb{R}^{n})=L^2(\partial\mathbb{R}_{+}^{n+1}), is stable under complex, L∞L^{\infty} perturbations of the coefficient matrix. Using a variant of the TbTb Theorem, we also prove that the layer potentials are bounded and invertible on L2(Rn)L^2(\mathbb{R}^n) whenever A(x)A(x) is real and symmetric (and thus, by our stability result, also when AA is complex, ∥A−A0∥∞\Vert A-A^0\Vert_{\infty} is small enough and A0A^0 is real, symmetric, L∞L^{\infty} and elliptic). In particular, we establish solvability of the Dirichlet and Neumann (and Regularity) problems, with L2L^2 (resp. L˙12)\dot{L}^2_1) data, for small complex perturbations of a real symmetric matrix. Previously, L2L^2 solvability results for complex (or even real but non-symmetric) coefficients were known to hold only for perturbations of constant matrices (and then only for the Dirichlet problem), or in the special case that the coefficients Aj,n+1=0=An+1,jA_{j,n+1}=0=A_{n+1,j}, 1≤j≤n1\leq j\leq n, which corresponds to the Kato square root problem

    Weighted norm inequalities, off-diagonal estimates and elliptic operators. Part I: General operator theory and weights

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    This is the first part of a series of four articles. In this work, we are interested in weighted norm estimates. We put the emphasis on two results of different nature: one is based on a good-λ\lambda inequality with two-parameters and the other uses Calder\'on-Zygmund decomposition. These results apply well to singular 'non-integral' operators and their commutators with bounded mean oscillation functions. Singular means that they are of order 0, 'non-integral' that they do not have an integral representation by a kernel with size estimates, even rough, so that they may not be bounded on all LpL^p spaces for 1<p<∞1 < p < \infty. Pointwise estimates are then replaced by appropriate localized Lp−LqL^p-L^q estimates. We obtain weighted LpL^p estimates for a range of pp that is different from (1,∞)(1,\infty) and isolate the right class of weights. In particular, we prove an extrapolation theorem ' \`a la Rubio de Francia' for such a class and thus vector-valued estimates.Comment: 43 pages. Series of 4 paper

    Remarks on functional calculus for perturbed first order Dirac operators

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    We make some remarks on earlier works on R−R-bisectoriality in LpL^p of perturbed first order differential operators by Hyt\"onen, McIntosh and Portal. They have shown that this is equivalent to bounded holomorphic functional calculus in LpL^p for pp in any open interval when suitable hypotheses are made. Hyt\"onen and McIntosh then showed that RR-bisectoriality in LpL^p at one value of pp can be extrapolated in a neighborhood of pp. We give a different proof of this extrapolation and observe that the first proof has impact on the splitting of the space by the kernel and range.Comment: 11 page

    Hardy spaces and divergence operators on strongly Lipschitz domains in RnR^n

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    Let Ω\Omega be a strongly Lipschitz domain of \reel^n. Consider an elliptic second order divergence operator LL (including a boundary condition on ∂Ω\partial\Omega) and define a Hardy space by imposing the non-tangential maximal function of the extension of a function ff via the Poisson semigroup for LL to be inL1L^1. Under suitable assumptions on LL, we identify this maximal Hardy space with atomic Hardy spaces, namely with H^1(\reel^n) if \Omega=\reel^n, Hr1(Ω)H^{1}_{r}(\Omega) under the Dirichlet boundary condition, and Hz1(Ω)H^{1}_{z}(\Omega) under the Neumann boundary condition. In particular, we obtain a new proof of the atomic decomposition for Hz1(Ω)H^{1}_{z}(\Omega). A version for local Hardy spaces is also given. We also present an overview of the theory of Hardy spaces and BMO spaces on Lipschitz domains with proofs.Comment: submitte

    Orthonormal bases of regular wavelets in spaces of homogeneous type

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    Adapting the recently developed randomized dyadic structures, we introduce the notion of spline function in geometrically doubling quasi-metric spaces. Such functions have interpolation and reproducing properties as the linear splines in Euclidean spaces. They also have H\"older regularity. This is used to build an orthonormal basis of H\"older-continuous wavelets with exponential decay in any space of homogeneous type. As in the classical theory, wavelet bases provide a universal Calder\'on reproducing formula to study and develop function space theory and singular integrals. We discuss the examples of LpL^p spaces, BMO and apply this to a proof of the T(1) theorem. As no extra condition {(like 'reverse doubling', 'small boundary' of balls, etc.)} on the space of homogeneous type is required, our results extend a long line of works on the subject.Comment: We have made improvements to section 2 following the referees suggestions. In particular, it now contains full proof of formerly Theorem 2.7 instead of sending back to earlier works, which makes the construction of splines self-contained. One reference adde
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