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MOTION MOUNTAIN

LIGHT, CHARGES AND BRAINS - Motion Mountain

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images – transporting light 161<br />

F I G U R E 110 An example of an isotropic metamaterial<br />

(M. Zedler et al., © 2007 IEEE).<br />

Ref. 123<br />

Ref. 122<br />

Ref. 124<br />

Ref. 125<br />

effect. However, these predictions have not been verified yet.<br />

Most intriguing, negative index materials are predicted to allow constructing lenses<br />

that are completely flat. In addition, in the year 2000, John Pendry gained the attention<br />

of the whole physics community world-wide by predicting that lenses made with such<br />

materials, in particular for a refractive indexn=−1, would be perfect, thus beating the<br />

usual diffraction limit.This would happen because such a perfect lens would also image<br />

theevanescent parts of the waves – i.e., the exponentially decaying ones – by amplifying<br />

them accordingly. First experiments claim to confirm the prediction. Exploration of the<br />

topic is still in full swing.<br />

So far,left-handedmaterialshave been realized only for microwave and terahertz frequencies.<br />

First claims in the visible domain have been published, but have to be taken<br />

with care. It should be mentioned that one type of negative refraction systems have been<br />

known since a long time: diffraction gratings. We could argue thatleft-handedmaterials<br />

are gratings that attempt to work in all spatial directions. And indeed, all left-handed<br />

materialsrealizedsofarareperiodicarrangementsofelectromagneticcircuits.<br />

Metamaterials<br />

Thesimplestrealizationofleft-handedsystemsaremetamaterials.Metamaterialsareengineered<br />

metal-insulator structures with a periodicity below the wavelength of the radiation<br />

for which they are designed, so that the structure behaves like a homogeneous<br />

material. Metamaterials have negative or otherwise unusual permittivity or permeability<br />

properties in a certain wavelength range, usually in the microwave domain; some<br />

metamaterials areleft-handed.<br />

Currently,therearetwobasicapproachestorealizemetamaterials.Thefirstistobuild<br />

a metamaterial fromalarge array ofcompactresonantsubstructures,suchas inductorcapacitor(LC-)circuitsordielectricspheres.Thesecondapproachistobuildametamaterial<br />

fromtransmissionlines. Thelatter approachhaslowerlossesandawiderspectral<br />

range;anexampleforthistypeisshowninFigure110.Comparingandexploringdifferent<br />

realizationsissubjectofintenseresearch.<br />

Most metamaterials are conceived for microwaves or terahertz waves. Industrial applications<br />

of metamaterials are expected for antenna design; for example, an antenna<br />

dipole could be located just above a metamaterial and thus allowing to build flat direc-<br />

Motion Mountain – The Adventure of Physics copyright © Christoph Schiller June 1990–November 2015 free pdf file available at www.motionmountain.net

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