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Shape Derivatives of Boundary Integral Operators in Electromagnetic Scattering. Part II: Application to Scattering by a Homogeneous Dielectric Obstacle

机译:电磁散射中边界积分算子的形状导数。第二部分:均质介质障碍物在散射中的应用

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摘要

We develop the shape derivative analysis of solutions to the problem of scattering of time-harmonic electromagnetic waves by a penetrable bounded obstacle. Since boundary integral equations are a classical tool to solve electromagnetic scattering problems, we study the shape differentiability properties of the standard electromagnetic boundary integral operators. The latter are typically bounded on the space of tangential vector fields of mixed regularity ${mathsf T mathsf H^{-frac{1}{2}}({rm div}_{Gamma},Gamma)}$ . Using Helmholtz decomposition, we can base their analysis on the study of pseudo-differential integral operators in standard Sobolev spaces, but we then have to study the Gâteaux differentiability of surface differential operators. We prove that the electromagnetic boundary integral operators are infinitely differentiable without loss of regularity. We also give a characterization of the first shape derivative of the solution of the dielectric scattering problem as a solution of a new electromagnetic scattering problem.
机译:我们开发了一种可穿透有界障碍物对时谐波电磁波散射问题的解的形状导数分析。由于边界积分方程是解决电磁散射问题的经典工具,因此我们研究了标准电磁边界积分算子的形状微分性质。后者通常在混合规则性$ {mathsf T mathsf H ^ {-frac {1} {2}}({rm div} _ {Gamma},Gamma)} $的切向矢量场的空间上有界。使用Helmholtz分解,我们可以基于标准Sobolev空间中伪微分积分算子的研究来进行分析,但随后我们必须研究表面微分算子的Géteaux可微性。我们证明了电磁边界积分算子是无限可微的而不会损失规则性。我们还将介电散射问题的解的一阶导数表征为新电磁散射问题的解。

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