# Stability Analysis of a Simple Discretization Method for a Class of Strongly Singular Integral Equations

**Authors:** Martin Costabel, Monique Dauge, Khadijeh Nedaiasl

arXiv: 2302.13159 · 2025-08-01

## TL;DR

This paper analyzes the stability of a simple discretization method for strongly singular integral equations, including applications to electromagnetic scattering, revealing conditions under which the method is stable or unstable.

## Contribution

It introduces a novel analysis of a discretization method for singular integral equations, connecting it to finite section methods and spectral properties using Ewald's technique.

## Key findings

- The method can be viewed as a finite section of an infinite Toeplitz matrix.
- The spectrum and numerical range of the discretization are characterized.
- The method is stable for many parameters but can be unstable even when the continuous problem is well-posed.

## Abstract

Motivated by the discrete dipole approximation (DDA) for the scattering of electromagnetic waves by a dielectric obstacle that can be considered as a simple discretization of a Lippmann-Schwinger style volume integral equation for time-harmonic Maxwell equations, we analyze an analogous discretization of convolution operators with strongly singular kernels.   For a class of kernel functions that includes the finite Hilbert transformation in 1D and the principal part of the Maxwell volume integral operator used for DDA in dimensions 2 and 3, we show that the method, which does not fit into known frameworks of projection methods, can nevertheless be considered as a finite section method for an infinite block Toeplitz matrix. The symbol of this matrix is given by a Fourier series that does not converge absolutely. We use Ewald's method to obtain an exponentially fast convergent series representation of this symbol and show that it is a bounded function, thereby allowing to describe the spectrum and the numerical range of the matrix.   It turns out that this numerical range includes the numerical range of the integral operator, but that it is in some cases strictly larger. In these cases the discretization method does not provide a spectrally correct approximation, and while it is stable for a large range of the spectral parameter $\lambda$, there are values of $\lambda$ for which the singular integral equation is well posed, but the discretization method is unstable.

## Full text

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## Figures

7 figures with captions in the complete paper: https://tomesphere.com/paper/2302.13159/full.md

## References

21 references — full list in the complete paper: https://tomesphere.com/paper/2302.13159/full.md

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Source: https://tomesphere.com/paper/2302.13159