1999
DOI: 10.1002/(sici)1098-2760(19991105)23:3<177::aid-mop14>3.0.co;2-i
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The scattering of electromagnetic waves by rectangular-cell double-periodic magnetodielectric gratings

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Cited by 19 publications
(8 citation statements)
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“…This was the motivation to develop different techniques for studying different configurations of periodic structures. However, only a few published works have discussed the properties of magneto-dielectric periodic structures [1,2]. Recently, it has been shown that such magneto-dielectric periodic structures can also be used to design double negative (DNG) metamaterial where both the relative permittivity and the relative permeability are negative values [3].…”
Section: Introductionmentioning
confidence: 99%
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“…This was the motivation to develop different techniques for studying different configurations of periodic structures. However, only a few published works have discussed the properties of magneto-dielectric periodic structures [1,2]. Recently, it has been shown that such magneto-dielectric periodic structures can also be used to design double negative (DNG) metamaterial where both the relative permittivity and the relative permeability are negative values [3].…”
Section: Introductionmentioning
confidence: 99%
“…In addition, including the relative permeability as a design parameter represents another degree of freedom for designing grating structures. From the analytical point of view, the problem of a magnetodielectric grating slab can be solved by using different techniques; such as MoM, FDTD, FDFD, FEM, and modal analysis [1,2,[6][7][8][9][10][11][12]. This problem has been discussed previously by using MoM [1,2].…”
Section: Introductionmentioning
confidence: 99%
“…Following the algorithm given in [2] we present the field in each period segment as an expansion in terms of the spatial harmonics numbered (r,s) and act on the equation for these fields by the linear operator…”
Section: (R)(= I (R)mentioning
confidence: 99%
“…where Next we solve the equation set for the field functionals and thus for the field components (the procedure in paper [2]). Using the extinction theorem at the last stage we express the internal fields of the structure (region 1 and 3) through the incident wave field.…”
Section: (R)(= I (R)mentioning
confidence: 99%
“…For beginning we suppose that the periods are partitioned into segments with constant material parameters. For each period segment numbered (kJ) we can write the notations bi,-' < v;, < b i , Following the algorithm given in [2] we present the field in each period segment as an expansion in terms of the spatial harmonics numbered (r,s) and act on the equation for these fields by the linear operator biil < Vi, < 9 6l (ri, = &k/ and PI (ri/) = P&/ .…”
mentioning
confidence: 99%