By Filippo Capolino
This booklet makes use of the 1st volume’s exploration of thought, simple houses, and modeling themes to improve readers’ realizing of purposes and units which are in line with man made fabrics. It explores a variety of functions in fields together with electronics, telecommunications, sensing, clinical instrumentation, and information garage. The textual content additionally features a sensible user’s consultant and explores key components within which synthetic fabrics have built. It contains specialists’ views on present and destiny functions of metamaterials, to provide a well-rounded view on state of the art technologies.
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Additional info for Applications of Metamaterials
Rev. E, , , . ) In the above equation, q x is the x-component of wave vector q k = ω/c is the wave number of the host medium c is the speed of light k p = ω p /c is the wave number corresponding to the plasma frequency ω p The plasma frequency depends on the lattice period a and on the radius of wires r . For an array of metallic wires arranged in a square lattice, we have that: k p = π/a . ). Suppose that a plane wave with transverse magnetic (TM) polarization (magnetic field is parallel to the interface) illuminates the wire medium slab.
Pendry, Subwavelength imaging in photonic crystals, Phys. Rev. B, : , . . P. V. Parimi, W. T. Lu, P. Vodo, and S. Sridhar, Imaging by flat lens using negative refraction, Nature, : , . . X. Wang, Z. Ren, and K. Kempa, Unrestricted superlensing in a triangular two-dimensional photonic crystals, Opt. Express, (): –, . . E. Cubukcu, K. Aydin, E. Ozbay, S. Foteinopolou, and C. Soukoulis, Subwavelength resolution in a two-dimensional photonic-crystal-based superlens, Phys.
Transmission and Reflection Characteristics of Wire Medium Slabs . . . . . . . . . . . . . . . . . Magnifying and Demagnifying Lenses with Super-Resolution . . . . . . . . . . . . . . . . . . . Imaging at Terahertz Frequencies and Beyond . . . . References . . . . . . . . . . . . . . . . . . . . . . . . . - - - Introduction Lens-based imaging devices such as conventional microscopes cannot provide resolution better than λ/, where λ is the wavelength of radiation.