IEEE Antennas and Propagation Society International Symposium. 1995 Digest
DOI: 10.1109/aps.1995.530194
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Comparative study of acceleration techniques for integrals and series in electromagnetic problems

Abstract: Most electromagnetic problems can be reduced to either integrating oscillatory integrals or summing up complex series. However, limits of the integrals and the series usually extend to infinity, and, in addition, they may be slowly convergent. Therefore numerically efficient techniques for evaluating the integrals or for calculating the sum of an infinite series have to be used to make the numerical solution feasible and attractive. In the literature there are a wide range of applications of such methods to va… Show more

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Cited by 18 publications
(24 citation statements)
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“…This expression has a poor [O(1/n)] convergence, hence some acceleration techniques must be exploited to ensure a proper convergence [15]- [17].…”
Section: A Green Function Calculation For Periodic Structuresmentioning
confidence: 99%
“…This expression has a poor [O(1/n)] convergence, hence some acceleration techniques must be exploited to ensure a proper convergence [15]- [17].…”
Section: A Green Function Calculation For Periodic Structuresmentioning
confidence: 99%
“…A more sophisticated approach is based on a Kummer's decomposition before applying the Poisson's formula (6) where (7) and in the third member of (6) we applied Poisson's formula to the last series. The function corresponds to a function , where is the same as in (5).…”
Section: B Kummer's Decompositionsmentioning
confidence: 99%
“…A similar method illustrated in [5], [34], the so-called algorithm, can be applied to non-oscillating series. Other numerical techniques are reported in [6].…”
Section: E Shanks' Transformsmentioning
confidence: 99%
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“…Among different techniques used to speed up the computation of Green's functions [3], the Ewald transform [4] has clearly demonstrated its suitability for periodic problems. It has been advantageously used in the efficient evaluation of GFs of infinite periodic phased arrays of line sources (2-D structures with 1-D periodicity) [5,6], 2-D structures with 2-D periodicity [7], in 3-D problems with 2-D orthogonal [8,9] and skewed [10] lattices as well as for rectangular cavities (3-D problems with 3-D orthogonal lattices) [11,12].…”
Section: Introductionmentioning
confidence: 99%