Spectral approach to homogenization of an elliptic operator periodic in some directions

preprint2009arXivOpen access

Abstract

The operator Aε=D1g1(x1/ε,x2)D1+D2g2(x1/ε,x2)D2 A_{\varepsilon}= D_{1} g_{1}(x_{1}/\varepsilon, x_{2}) D_{1} + D_{2} g_{2}(x_{1}/\varepsilon, x_{2}) D_{2} is considered in L2(R2)L_{2}({\mathbb{R}}^{2}), where gj(x1,x2)g_{j}(x_{1},x_{2}), j=1,2,j=1,2, are periodic in x1x_{1} with period 1, bounded and positive definite. Let function Q(x1,x2)Q(x_{1},x_{2}) be bounded, positive definite and periodic in x1x_{1} with period 1. Let Qε(x1,x2)=Q(x1/ε,x2)Q^{\varepsilon}(x_{1},x_{2})= Q(x_{1}/\varepsilon, x_{2}). The behavior of the operator (Aε+Qε(A_{\varepsilon}+ Q^{\varepsilon}%)^{-1} as ε→0\varepsilon\to0 is studied. It is proved that the operator (Aε+Qε)−1(A_{\varepsilon}+ Q^{\varepsilon})^{-1} tends to (A0+Q0)−1(A^{0} + Q^{0})^{-1} in the operator norm in L2(R2)L_{2}(\mathbb{R}^{2}). Here A0A^{0} is the effective operator whose coefficients depend only on x2x_{2}, Q0Q^{0} is the mean value of QQ in x1x_{1}. A sharp order estimate for the norm of the difference (Aε+Qε)−1−(A0+Q0)−1(A_{\varepsilon}+ Q^{\varepsilon})^{-1}- (A^{0} + Q^{0})^{-1} is obtained. The result is applied to homogenization of the Schrödinger operator with a singular potential periodic in one direction.

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