Plasmonics at the bottom: shrinking wavelengths

Plasmonics may be older than you think.  Alchemists and glassmakers spent millennia taking advantage of plasmonic effects when they created stained-glass windows and colorful goblets that incorporated small metallic particles in the glass. By analogy, ignorance of modern biology did not stop Stone-Age humans from genetically engineering wolves and various plants (via selective breeding) to become dogs and farming crops.   Best known example of alchemical plasmonics is the Lycurgus cup, a Roman goblet dating from the 300s A.D.; now held in the British museum.  Thanks to plasmonic excitation of electrons in the metallic particles suspended in the glass, the cup absorbs and scatters blue and green light (relatively short wavelengths in the visible spectrum).  When viewed in reflected light, the plasmonic scattering gives the cup a greenish hue, but if a normal light source (emits white light) is placed inside the goblet, the glass appears red because it transmits only the longer wavelengths (red) and absorbs the shorter ones (green/blue).

Lycurgus Cup: a Roman goblet dating from the 4th century A.D.  It changes color because of the plasmonic excitation of metallic particles within the glass matrix.  When a light source is placed inside the normally green goblet, it looks red.

 Surface plasmon research began with a bang in the 1980s, as chemists studied the phenomenon using Raman spectroscopy: the scattering of laser light off a sample to determine its structure from molecular vibrations.  In 1989, Thomas Ebbesen, then at the NEC Research Institute in Japan, discovered that when he illuminated a thin but opaque gold film imprinted with millions of microscopic holes, the foil somehow transmitted more light than was expected from the number and size of the holes.  This phenomenon, now known as extraordinary optical transmission, was eventually found to be caused by surface plasmons that intensified the transmission of electromagnetic energy.

Then came the discovery of novel "metamaterials": materials in which electron oscillations can result in some weird optical effects.  Their optical effects are so complex (due to plasmons) they require astronomically powerful computers for accurate simulation, but studying them has become less daunting by novel methods for constructing nanoscale structures that allow researchers to build and test ultrasmall plasmonic devices and circuits.

In most circumstances, it would be unwise to use metallic structures to transmit light signals because metals are known for high optical losses (signal weakens after each bounce off the metallic surface until evanescence).  However, when a thin film is combined with an electrical insulator, optical losses decrease due to the electromagnetic (EM) field spreading into the insulating material, where there are no conducting electrons  to oscillate, thus no energy-dissipating collisions.  This property naturally confines plasmons to the metallic surface adjoining the insulator; e.g., in the the top portion of the figure below (PLANAR WAVEGUIDE), the surface plasmons propagate only in the thin plane at the interface.  Note that in this example, the insulator is air. 

With this planar structure acting as a waveguide, shepherding the EM waves along the metal-dielectric boundary, it may be useful in routing signals on a chip.  Most optical signals may attenuate rapidly in metals, but the exception here is a plasmon traveling in a thin-film metal waveguide, whose journey can last for several cm.  The plasmon signal can be made to last longer  if the waveguide employs an asymmetric mode,  meaning the EM energy disperses more intensely in a certain direction than others.  This mode pushes a greater portion of the EM energy away from the guiding metal film and into the surrounding insulator, thus delaying attenuation a little longer.  The EM fields at the top and bottom surfaces of the metal film are known to interact with each other, and this interaction can be manipulated by changing the thickness of the film, which manifests as different frequencies and wavelengths for the plasmons.  In fact, this has already been done in the late '90s by a Danish/Canadian collaboration; they created a planar plasmon waveguide like in the top of the figure, but the EM fields it generated were too large to convey signals through the nanoscale innards of a processor.

Plasmons can propagate through nanoscale wires, but they require more complex waveguide geometries than that of the planar form; plasmons can shrink the wavelength of the optical signal by squeezing it into a narrow space.  This is seen in the middle illustration of the above figure.  This device is called a plasmon slot waveguide; the plasmon wavelength changes with respect to the thickness of the insulator core in the middle.  This is capable of transmitting a signal 10s of microns long (1 micron = 1 µm ≈ diameter of a blood cell).  Now comes the juicy part: a Japanese researcher had managed to squeeze red light (wavelength of 651 nm) into a plasmon slot waveguide that was only 3 nm thick and 55 nm wide.  The wavelength of the surface plasmon propagating through the device was 51 nm, or 8% of the original red light wavelength.  But the frequency remains the same, which means information gets transmitted.  This striking ability to shrink the wavelength opens the floodgates for nanoscale plasmonic structures to perhaps replace purely electronic circuits containing wires and transistors. 

Mass-production of plasmon slot waveguides is another story, but it should be similar to lithography (used to imprint circuit patterns on silicon chips).  This process could mass-produce miniuscule plasmonic devices with arrays of narrow insulating stripes and gaps.  These arrays would guide the waves of positive and negative charges on the metal surface; their behavior is similar to alternating current traveling along an ordinary wire.  However, since the frequency of an optical signal is so much higher than that of an electrical signal (400,000 GHz vs. 60 Hz, respectively),  the plasmonic circuit can carry tons more data.  Additionally, electrons  don't travel from one end of a plasmonic circuit to another; rather, they clump together and spread apart (thus no net directional surface current).  This fact accounts for the device's immunity to resistance and capacitance effects that limit the data-carrying capacity of integrated circuits with electrical interconnects.