2012
DOI: 10.1137/110831568
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Transverse Electric Scattering on Inhomogeneous Objects: Spectrum of Integral Operator and Preconditioning

Abstract: Abstract. The domain integral equation method with its FFT-based matrix-vector products is a viable alternative to local methods in free-space scattering problems. However, it often suffers from the extremely slow convergence of iterative methods, especially in the transverse electric (TE) case with large or negative permittivity. We identify the nontrivial essential spectrum of the pertaining integral operator as partly responsible for this behavior, and the main reason why a normally efficient deflating prec… Show more

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Cited by 16 publications
(5 citation statements)
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References 32 publications
(66 reference statements)
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“…Note that in the quasistatic limit, i.e., when 1/k b is much larger than the size of the scatterer, the term with G 1 cancels this out and only the principal value that contains G 0 contributes. Equation (3) defines a linear operator whose properties have been studied both in 2D [25] and 3D [24].…”
Section: Backgrounds and Purposementioning
confidence: 99%
See 1 more Smart Citation
“…Note that in the quasistatic limit, i.e., when 1/k b is much larger than the size of the scatterer, the term with G 1 cancels this out and only the principal value that contains G 0 contributes. Equation (3) defines a linear operator whose properties have been studied both in 2D [25] and 3D [24].…”
Section: Backgrounds and Purposementioning
confidence: 99%
“…Budko and co-authors [24,25] made the first move towards a Fourier Transform of the Lippman Schwinger Equation (LSE) for 3D geometries. This work was limited, however, to a scatterer described by Hölder continuous functions, and dealt with the singular part of the LSE only.…”
Section: Introductionmentioning
confidence: 99%
“…which derives from the definitions of the complex permittivity and the dielectric contrast. Then, using the definitions of G , Z A , Z Φ,11 , and Z Φ,1 in ( 7), ( 8), ( 2), (16), and ( 17), we can deduce the frequency scalings of these matrices from ( 23), ( 24), (25), and (26). We finally obtain the following lowfrequency behavior for the real and imaginary parts of G , Z A , Z Φ,11 , and Z Φ,1…”
Section: A Low-frequency Analysis Of the D-viementioning
confidence: 99%
“…These projectors have been adapted to the J-VIE and used for curing the HC limitations of this equation for isotropic inhomogeneous scatterers [33]. Another approach to solve the HC problem is presented in [25], where the E-VIE is regularized using symbol calculus and the Calderón identities. Its application to the J-VIE is discussed in [34].…”
Section: Introductionmentioning
confidence: 99%
“…with τ e χ e / r , where the identity operator is now left alone. In this way, the integral equation is regularized and this regularization can be thought as a natural preconditioning for solving the linear system of the discretized current-based VIE, as it has been suggested in [55], [56]. Motivated from these observations, we use a preconditioner of the form P = M r G. From a numerical perspective, when using this preconditioner, the iterative solver converges much faster especially in the case of highly inhomogeneous scatterers.…”
Section: B On Preconditioningmentioning
confidence: 99%