2001
DOI: 10.1002/mop.1079
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The CGFFT method with a discontinuous FFT algorithm

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Cited by 19 publications
(10 citation statements)
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“…Again, this change in a variable produces a set of quadrature point in τ that do not coincide with the computational grid on the integration patch P k requiring an interpolation strategy for which we utilize the FFT refined polynomial interpolation [29]. The final step in high-order approximation of K sing k [u](x) relates to the the computation of t 2integral in (17). The main difficulty, here, is encountered in the form of a jump discontinuity in the t-derivative of J k (t; x) at t = t x 2 [13].…”
Section: Singular Integrationmentioning
confidence: 99%
See 1 more Smart Citation
“…Again, this change in a variable produces a set of quadrature point in τ that do not coincide with the computational grid on the integration patch P k requiring an interpolation strategy for which we utilize the FFT refined polynomial interpolation [29]. The final step in high-order approximation of K sing k [u](x) relates to the the computation of t 2integral in (17). The main difficulty, here, is encountered in the form of a jump discontinuity in the t-derivative of J k (t; x) at t = t x 2 [13].…”
Section: Singular Integrationmentioning
confidence: 99%
“…In contrast, the integral equation approach, where the mathematical formulation directly ensures that the solution satisfies condition (3) by suitably employing the radiating fundamental solution, is free from considerations mentioned above, and consequently, does not require solution strategies to discretize outside the inhomogeneity. We, therefore, base our numerical treatment of the scattering problem on an equivalent integral equation formulation which is given by the Lippmann-Schwinger equation [1,11], (4) u(x) + κ 2 In recent years, a lot of progress has been made toward numerical solution of the Lippmann-Schwinger equation; for example, see [12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27]. Most fast numerical schemes among these, though high order accurate for smooth scattering media, exhibit only linear convergence in the presence of material discontinuity [12,15,17,22,26,27].…”
Section: Introductionmentioning
confidence: 99%
“…( ) Figure 1. Arbitrary dielectric object embedded in a cuboid [7]. Journal of Applied Mathematics and Physics where d n is unknown, and q n φ is defined as the rooftop basic function on x,y,z directions respectively, and the superscript q = x,y,z.…”
Section: Theorymentioning
confidence: 99%
“…er, for the simulation of radome, FEM and FDTD usually consume a lot of memory because of its discretization of whole region including the volume which is vacuum [5]. MoM only requires the discretization of dielectric object rather than the whole region, but has to solve the linear equation, which means Journal of Applied Mathematics and Physics that it consumes computational complexity O(N 2 ) if solved iteratively [6] [7].…”
Section: Introductionmentioning
confidence: 99%
“…Again here, this solution procedure leads to very efficient numerics and is highly accurate for smoothly varying media, but its convergence degrades significantly in the presence of material discontinuities. 17,23 In fact, to our knowledge, only limited attempts have been made toward the development of efficient higher-order integral-equation solvers for volumetric scattering applications. A notable exception is the work of Zhu and Gedney, 24,25 based on the "discontinuous FFT" of Fan and Liu. 23 This latter scheme is based on the accurate evaluation of Fourier coefficients of discontinuous functions ͑through Gaussian quadratures and careful interpolation from and to equispaced grids͒ and, while it can be shown that this improves on the convergence of the CGFFT ͑from first-to second-order accurate, in fact͒, it fails to address the Gibbs phenomenon which arises as the Fourier series is summed.…”
Section: Introductionmentioning
confidence: 99%