By Ricardo Marqués
The first basic textbook to provide a whole assessment of metamaterial thought and its microwave applications
Metamaterials with unfavourable Parameters represents the single unified remedy of metamaterials to be had in a single handy ebook. dedicated quite often to metamaterials that may be characterised by way of a detrimental powerful permittivity and/or permeability, the booklet features a vast evaluate of crucial subject matters, clinical basics, and technical functions of metamaterials.
Chapter assurance comprises: the electrodynamics of left-handed media, synthesis of bulk metamaterials, synthesis of metamaterials in planar know-how, microwave purposes of metamaterial ideas, and complex and similar subject matters, together with SRR- and CSRR-based admittance surfaces, magneto- and electro-inductive waves, and sub-diffraction imaging units. a listing of difficulties and references is integrated on the finish of every bankruptcy, and a bibliography deals a whole, up-to-daterepresentation of the present cutting-edge in metamaterials.
Geared towards scholars and pros alike, Metamaterials with adverse Parameters is a perfect textbook for postgraduate classes and likewise serves as a helpful introductory reference for scientists and RF/microwave engineers.
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Extra info for Metamaterials with Negative Parameters: Theory, Design and Microwave Applications
Quasistatic surface plasmons. Show that Laplace’s equation at the interface between two media, 1 and 2, has bounded propagative solutions along such interface provided 11 ¼ À 12 . These solutions are usually called quasistatic surface plasmons . 3. Full-wave surface plasmons – polaritons. Find the dispersion relation for TM surface waves at the interface between two media with 11 . 0 and 12 , 0. 2) in the limit k ! 1. For small values of k, these waves have a different dispersion relation and are sometimes called surface polaritons.
1097–1099, 2002. 9. I. V. Lindell, S. A. Tretyakov, K. I. Nikoskinen, and S. ” Microwave Opt. Tech. , vol. 31, pp. 129– 133, 2001. 10. R. W. Ziolkowski and E. ” Phys. Rev. E, vol. 64, paper 056625, 2001. 11. A.
This characteristic of the perfect lens (and similar devices) imposes severe limitations to its applicability for subsurface heating or burning devices. It also imposes restrictions on its usefulness 4 Such three-dimensional superfocusing will be contrary to the well-known uncertainty principle, as has already been noted in  and . 10). 21 29 in imaging devices, at least if the distance between the source and the lens is unknown. In fact, because the electromagnetic ﬁeld intensity has a monotonic decay at the back side of the lens, the location of an unknown source can hardly be recovered from the analysis of the ﬁeld distribution at the back side of the lens (see  for a complete discussion, with examples, of this point).