Abstract:This note addresses the homogenization error for linear elliptic equations in divergenceform with random stationary coefficients. The homogenization error is measured by comparing the quenched Green's function to the Green's function belonging to the homogenized coefficients, more precisely, by the (relative) spatial decay rate of the difference of their second mixed derivatives. The contribution of this note is purely deterministic: It uses the expanded notion of corrector, namely the couple of scalar and vec… Show more
“…One interesting feature we emphasize in the present contribution is that the results of [1,24] of the periodic setting indeed carry over not only to the perturbed periodic setting, but also to a quite general abstract setting, which we make precise in Section 1.2 below. The latter observation about the generalization of the results of [1] and related works to non periodic setting is corroborated by the recent works [5,17]. Some of the necessary assumptions presented there (in the context of random homogenization) are quite close in spirit to our own formalization.…”
We consider homogenization problems for linear elliptic equations in divergence form. The coefficients are assumed to be a local perturbation of some periodic background. We prove W 1,p and Lipschitz convergence of the two-scale expansion, with explicit rates. For this purpose, we use a corrector adapted to this particular setting, and defined in [10,11], and apply the same strategy of proof as Avellaneda and Lin in [1]. We also propose an abstract setting generalizing our particular assumptions for which the same estimates hold.
“…One interesting feature we emphasize in the present contribution is that the results of [1,24] of the periodic setting indeed carry over not only to the perturbed periodic setting, but also to a quite general abstract setting, which we make precise in Section 1.2 below. The latter observation about the generalization of the results of [1] and related works to non periodic setting is corroborated by the recent works [5,17]. Some of the necessary assumptions presented there (in the context of random homogenization) are quite close in spirit to our own formalization.…”
We consider homogenization problems for linear elliptic equations in divergence form. The coefficients are assumed to be a local perturbation of some periodic background. We prove W 1,p and Lipschitz convergence of the two-scale expansion, with explicit rates. For this purpose, we use a corrector adapted to this particular setting, and defined in [10,11], and apply the same strategy of proof as Avellaneda and Lin in [1]. We also propose an abstract setting generalizing our particular assumptions for which the same estimates hold.
“…when d > 2, is an L 2 -off-diagonal bound for ∇∇G D and ∇G D , in both space variables x and y and depending only on the dimension and the ellipticity ratio. It is mainly obtained through a duality argument à la Avellaneda-Lin ( [3], Theorem 13) on standard energy estimates for solutions of −∇ · a∇u = ∇ · g, combined with an inner-regularity estimate for a-harmonic functions in the spirit of Lemma 4 of [5]. We stress here that this result is inspired by Lemma 2 of [5] and provides the new and pivotal ingredient for the first fundamental estimate for G D .…”
Section: Main Results and Remarksmentioning
confidence: 97%
“…We start with two variants of Lemma 4 of [5]; while this last one is a statement for ensembles of locally a-harmonic functions, the following Lemma 2 takes into account the new perturbation term L n and the more general domain D. If d > 2, then Lemma 3 is a further generalisation to the case of functions solving −∇ · a∇u + εL n u = 0 on outer domains. We postpone the proofs of Lemma 2 and Lemma 3 to the Appendix.…”
Section: Proof Of Theoremmentioning
confidence: 99%
“…Roughly speaking, Lemma 2 and Lemma 3 state that the previous inequalities remain true also if we exchange in the r.h.s. the order of the integration in μ and the supremum over the functionals F. We may refer to the result of Lemma 4 of [5], which corresponds to Lemma 2 with D = R d and ε = 0, as a compactness statement for ensembles of locally a-harmonic functions. Indeed, as we show in the appendix, inequality (35) actually follows by an inner regularity estimate which allows to control the energy of an a-harmonic function u in an interior domain by the L 2 -norm on {|x| < 2R} of (− N ) − l 2 u for any even l ∈ N. Here, − N denotes the Laplacian with Neumann boundary conditions.…”
Section: Analogously To Theorem 1 Means ≤ C With a Generic C = C(d λ)mentioning
This paper is divided into two parts: In the main deterministic part, we prove that for an open domain D ⊂ R d with d ≥ 2, for every (measurable) uniformly elliptic tensor field a and for almost every point y ∈ D, there exists a unique Green's function centred in y associated to the vectorial operator −∇ · a∇ in D. This result implies the existence of the fundamental solution for elliptic systems when d > 2, i.e. the Green function for −∇ · a∇ in R d . In the second part, we introduce a shift-invariant ensemble · over the set of uniformly elliptic tensor fields, and infer for the fundamental solution G some pointwise bounds for |G(·; x, y)| , |∇ x G(·; x, y)| and |∇ x ∇ y G(·; x, y)| . These estimates scale optimally in space and provide a generalisation to systems of the bounds obtained by Delmotte and Deuschel for the scalar case.
Mathematics Subject Classification
“…Loosely speaking, it can be seen as relating the quenched Green's function to the homogenized Green's function, on the level of gradients. In this sense, this work takes up the analysis started by the three authors in [15]. Going beyond [15], this paper provides a second-order error analysis.…”
In a homogeneous medium, the far-field generated by a localized source can be expanded in terms of multipoles; the coefficients are determined by the moments of the localized charge distribution. We show that this structure survives to some extent for a random medium in the sense of quantitative stochastic homogenization: In three space dimensions, the effective dipole and quadrupole -but not the octupole -can be inferred without knowing the realization of the random medium far away from the (overall neutral) source and the point of interest.Mathematically, this is achieved by using the two-scale expansion to higher order to construct isomorphisms between the hetero-and homogeneous versions of spaces of harmonic functions that grow at a certain rate, or decay at a certain rate away from the singularity (near the origin); these isomorphisms crucially respect the natural pairing between growing and decaying harmonic functions given by the second Green's formula. This not only yields effective multipoles (the quotient of the spaces of decaying functions) but also intrinsic moments (taken with respect to the elements of the spaces of growing functions). The construction of these rigid isomorphisms relies on a good (and dimension-dependent) control on the higher-order correctors and their flux potentials.
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