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Download Advances in Electromagnetics of Complex Media and by A. Sihvola (auth.), Saïd Zouhdi, Ari Sihvola, Mohamed PDF

By A. Sihvola (auth.), Saïd Zouhdi, Ari Sihvola, Mohamed Arsalane (eds.)

The NATO complex examine Workshop Bianisotropics 2002 used to be held in th Marrakesh, Morocco, in the course of 8-11 may possibly 2002. This was once the nine overseas convention on Electromagnetics of complicated Media, belonging to a sequence of conferences the place the point of interest is on electromagnetics of chiral, bianisotropic, and different fabrics that could reply to electrical and magnetic box excitations in detailed demeanour. the 1st of those conferences used to be held in Espoo, Finland (1993), and the subsequent venues have been Gomel, Belarus (1993), Perigueux, France (1994), country collage, Pennsylvania, united states (1995), the rivers and channels among St. Petersburg and Moscow in Russia (1996), Glasgow, Scotland (1997), Brunswick, Germany (1998), and Lisbon, Portugal (2000). the current booklet includes complete articles of a number of of the displays that got within the Marrakesh convention. In Bianisotropics 2002, eight re­ view lectures, 14 invited lectures and sixty eight contributed talks and posters have been offered. of those shows, after a double evaluation method, 28 contributions have completed their ultimate shape at the pages to stick to. From the contributions ofthe assembly, additionally one other e-book is being deliberate: a distinct factor of the magazine Electromagnetics could be dedicated to advanced fabrics. visitor editors for this factor are Keith W. Whites and acknowledged Zouhdi. The chairmen of Bianisotropics 2002conference have been stated Zouhdi (Pierre et Marie Curie college - Paris) and Mohamed Arsalane (Cadi Ayyad college - Marrakesh), who have been assisted via Scientists from Moroccan Universities and the overseas Bianisotropics convention Committee.

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Extra resources for Advances in Electromagnetics of Complex Media and Metamaterials

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In fact, different approaches lead to incompatible values of effective parameters when skin effect is not negligible [13], because they rely on different definitions . As permeability and permittivity values are obtained through reflection - transmission measurements, it was found necessary to establish a definition of the effective quantities, so that the conventional expressions of the Fresnel coefficients using the effective quantities are valid. Using this approach, it has been shown that [33] : ~composile=lHinsuJalor (5) Bcomposile=Dinsulalo/ (6) where the brackets correspond to the spatial average over the whole volume of a periodical cell in the composite , and HinsuJalo" DinsuJalor are the fields in a plane containing no conductive element, and normal to the electric field.

37 21. 22. 23. 24. 25. 26. Notomi, M. (2000) Theory of light propagation in strongly modulated photonic crystals: Refractionlike behavior in the vicinity of the photonic bandgap, Physical Review E, 62(16), 10696. , and Kawakami, S. (1999) Self-coIlimating phenomena in photonic crystals, Applied Physics Letters, 74(9), 1212-1214. , and Kawakami, S. (1998) Superprism phenomena in photonic crystals, Physical Review E, 58(16), 10096. Engheta, N. (2002) Guided waves in paired dielectric-metamaterials with negative permittivity and permeability layers, a talk presented at the National Radio Science Meeting (USNC-URSI), Boulder, Colorado, January 9-12, 2002, p.

1/0 , although this assumption is not necessary. :#; no. We now consider a monochromatic uniform plane wave normally incident on this slab. , and exits from the other face of the slab. , where k, == (J)~&oPo • Now let us put another layer of width d, made of a lossless DNG metamaterial, in which &2 < 0 and P2 < 0 at certain frequencies, next to this DPS slab. (See Fig. ) The index of refraction for this DNG layer is a real quantity denoted by n2 == ~( &2P2) / (&oPo). We emphasize here that we do not need to specify any sign for the operation of the square root appearing in the expression of n2 • We merely state that n2 is a real quantity for the lossless DNG metamaterial here.

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