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Metamaterial

From Biocrawler, the free encyclopedia.

In electromagnetism (covering areas like optics and photonics), a meta material (or metamaterial) is an object that gains its (electromagnetic) material properties from its structure rather than inheriting them directly from the materials it is composed of. This term is particularly used when the resulting material has properties not found in naturally formed substances.

In order for its structure to affect electromagnetic waves, a metamaterial must have features with size comparable to the wavelength of the electromagnetic radiation it interacts with. For visible light, this is on the order of one micron; for microwave radiation, this is on the order of one decimetre. An example of a visible light metamaterial is opal, which is composed of tiny quartz spheres. Photonic bandgap materials are an example of an artificial visible light metamaterial. Microwave frequency metamaterials are almost always artificial, constructed as arrays of current-conducting elements (such as loops of wire) that have suitable inductive and capacitive characteristics.

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Negative refractive index

Very nearly all materials encountered in optics, such as glass or water, have positive values for both permittivity $ε$ and permeability $μ$ . However, many metals (such as silver and gold) have negative $ε$ at visible wavelengths. A material having either (but not both) $ε$ or $μ$ negative is opaque to electromagnetic radiation (see surface plasmon for more details).

Although the optical properties of a transparent material are fully specified by the parameters $ε$ and $μ$ , in practice the refractive index $N$ is often used. $N$ may be determined from $N=\sqrt{\epsilon\mu}$ . All known transparent materials possess a positive index because $ε$ and $μ$ are both positive.

However, some engineered metamaterials have $ε < 0$ and $μ < 0$ ; because the product $εμ$ is positive, $N$ is real. Under such circumstances, it is necessary to take the negative square root for $N$ . Physicist Victor Veselago proved that such substances are transparent to light.

Metamaterials with negative $N$ have numerous startling properties:

Snell's law ( $N 1 sinθ 1 = N 2 sinθ 2$ ) still applies; but rays are refracted away from the normal on entering the material
The Doppler shift is reversed (that is, a light source moving toward an observer appears to reduce its frequency)
Cerenkov radiation points the other way
group velocity is antiparallel to phase velocity (as opposed to parallel for normal materials)

One common metamaterial is the Swiss roll.

Such metamaterials follow a "left-hand rule".

The first Superlens (an optical lens employing negative refraction with vastly improved microscopic resolution) was created and demonstrated in 2005 by Xiang Zhang et al of UC Berkeley, as reported in the April 22 issue of the journal Science [1] (http://www.eurekalert.org/pub_releases/2005-04/uoc--nso041805.php)

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