2012 International Conference on Electromagnetics in Advanced Applications 2012
DOI: 10.1109/iceaa.2012.6328809
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Computation of the one-dimensional free-space periodic Green's function for leaky waves using the Ewald method

Abstract: − This paper examines an extension of the Ewald method for evaluating the periodic free-space Green's function due to an array of point sources, when the wavenumber of the phased sources is allowed to be complex. This makes the Ewald method useful for treating leaky modes on periodic structures.

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Cited by 2 publications
(9 citation statements)
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“…Note that the proper or improper nature of the terms is determined by the choice of the logarithmic branch cut of the exponential integral E q (·) [57]. The Green's function g E,p spectral can then be evaluated even if a finite number of harmonics is improper.…”
Section: Appendixmentioning
confidence: 99%
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“…Note that the proper or improper nature of the terms is determined by the choice of the logarithmic branch cut of the exponential integral E q (·) [57]. The Green's function g E,p spectral can then be evaluated even if a finite number of harmonics is improper.…”
Section: Appendixmentioning
confidence: 99%
“…Accordingly, the correct determination for the homogeneousmedium term G p ∞ , when added back in (3), has to be improper in both cases. The computation of the improper determination of G p ∞ can be performed as explained in [57].…”
Section: E Integration Pathsmentioning
confidence: 99%
“…4is slowly convergent, and it is even divergent for complex values of the wavenumber z k , and some technique must be adopted to allow analytic continuation of the GF into the complex z k plane. The GF representation adopted in this work makes use of Ewald's method for linear arrays, which, besides providing analytic continuation, it also provides series with Gaussian convergence and only a handful of terms are needed [32][33][34]. The dyadic form of the Ewald representation of the periodic GF evaluation used in this paper is provided in Appendix B.…”
Section: Simulation Modelmentioning
confidence: 99%
“…Modes 'Proper 1', 'Proper 2', 'Improper 1' and 'Improper 2' in Figs. 3 and 4 are computed using the method described in [33], where only m = 0 and −1 are considered, and adapted to the present case as in Appendix B. When the wavenumber dispersion curves change complex quadrant, they can be continued with dispersion curves computed with different m-values (see appendix B).…”
Section: Mode Analysismentioning
confidence: 99%
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