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Well-conditioned boundary integral equation formulations for the solution of high-frequency electromagnetic scattering problems

机译:条件良好的边界积分方程公式,用于解决高频电磁散射问题

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We present several versions of Regularized Combined Field Integral Equation (CFIER) formulations for the solution of three dimensional frequency domain electromagnetic scattering problems with Perfectly Electric Conducting (PEC) boundary conditions. Just as in the Combined Field Integral Equations (CFIE), we seek the scattered fields in the form of a combined magnetic and electric dipole layer potentials that involves a composition of the latter type of boundary layers with regularizing operators. The regularizing operators are of two types: (1) modified versions of electric field integral operators with complex wavenum-bers, and (2) principal symbols of those operators in the sense of pseudodifferential operators. We show that the boundary integral operators that enter these CFIER formulations are Fredholm of the second kind, and invertible with bounded inverses in the classical trace spaces of electromagnetic scattering problems. We present a spectral analysis of CFIER operators with regularizing operators that have purely imaginary wavenumbers for spherical geometries-we refer to these operators as Calderon-Ikawa CFIER. Under certain assumptions on the coupling constants and the absolute values of the imaginary wavenumbers of the regularizing operators, we show that the ensuing Calderon-Ikawa CFIER operators are coercive for spherical geometries. These properties allow us to derive wavenumber explicit bounds on the condition numbers of Calderon-Ikawa CFIER operators. When regularizing operators with complex wavenumbers with non-zero real parts are used-we refer to these operators as Calderon-Complex CFIER, we show numerical evidence that those complex wavenumbers can be selected in a manner that leads to CFIER formulations whose condition numbers can be bounded independently of frequency for spherical geometries. In addition, the Calderon-Complex CFIER operators possess excellent spectral properties in the high-frequency regime for both convex and non-convex scatterers. We provide numerical evidence that our solvers based on fast, high-order Nystrom discretization of these equations converge in very small numbers of GMRES iterations, and the iteration counts are virtually independent of frequency for several smooth scatterers with slowly varying curvatures.
机译:我们提出了多种版本的正则化组合场积分方程(CFIER)公式,用于求解具有完美导电(PEC)边界条件的三维频域电磁散射问题。就像在组合场积分方程(CFIE)中一样,我们以电磁偶极层电势组合的形式寻找散射场,该电势涉及具有规则化算符的后一种边界层的组成。正则化算子有两种类型:(1)具有复数波数的电场积分算子的修改版本,以及(2)在伪微分算子意义上的那些算子的主要符号。我们证明,输入这些CFIER公式的边界积分算符是第二类Fredholm,并且在电磁散射问题的经典迹线空间中具有界逆可逆。我们用正则化算子对CFIER算子进行频谱分析,这些算子对球形几何图形具有纯虚波数-我们将这些算子称为Calderon-Ikawa CFIER。在正则化算子的耦合常数和虚波数的绝对值的某些假设下,我们证明了随后的Calderon-Ikawa CFIER算子对于球面几何具有强制性。这些属性使我们能够得出Calderon-Ikawa CFIER算子的条件数的波数显式边界。当使用具有非零实部的复杂波数的正则化运算符时-我们将这些运算符称为Calderon-Complex CFIER,我们显示了数值证据,可以以导致条件值可以为CFIER公式的方式选择那些复杂波数球形几何图形不受频率限制。此外,Calderon-Complex CFIER算子在凸型和非凸型散射体的高频状态下均具有出色的光谱特性。我们提供了数值证据,表明基于这些方程式的快速,高阶Nystrom离散化的求解器收敛于极少数的GMRES迭代中,并且对于具有缓慢变化的曲率的多个平滑散射体,迭代次数实际上与频率无关。

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