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Light's Might Harnessed

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PASADENA, Calif., June 5, 2009 – A new nanoscale device harnesses the power of light on a silicon chip at the smallest scale to date and has potential applications in force detection and optical communication, among others.

Physicists at California Institute of Technology (Caltech) developed the device, which exploits the mechanical properties of light to create an optomechanical cavity in which interactions between light and motion are greatly strengthened and enhanced.

ZipperCavity.jpg
Scanning electron microscope image of an array of “zipper” optomechanical cavities. The highly localized optical field within the nanoscale and picogram mass structure is rendered on top of the structural image to indicate the sensitive interaction of light and mechanics in this nanodevice. (Images: Matt Eichenfield and Jasper Chan)

The fact that photons of light, despite having no mass, nonetheless carry momentum and can interact with mechanical objects is an idea that dates back to Kepler and Newton. The mechanical properties of light are also known to limit the precision with which one can measure an object’s position, since simply by using light to do the measurement, you apply a force and disturb the object.
It was important to consider these so-called back-action effects in the design of devices to measure weak, classical forces. Such considerations were part of the development of gravity-wave detectors like the Laser Interferometer Gravitational-Wave Observatory (LIGO). These sorts of interferometer-based detectors have also been used at much smaller scales, in scanning probe instruments used to detect or image atomic surfaces or even single electron spins.

To get an idea of how these systems work, consider a mirror attached to a floppy cantilever, or spring. The cantilever is designed to respond to a particular force – say, a magnetic field. Light shining down on the mirror will be deflected when the force is detected – i.e., when the cantilever moves – resulting in a variation in the light beam’s intensity that can then be detected and recorded.

“LIGO is a huge multikilometer-scale interferometer,” said Oskar Painter, associate professor of applied physics at Caltech and the principal investigator on the research. “What we did was to take that and scale it all the way down to the size of the wavelength of light itself, creating a nanoscale device.”

They did this, he explains, because as these interferometer-based detectors are scaled down, the mechanical properties of light become more pronounced, and interesting interactions between light and mechanics can be explored.

SEMZipper.jpg
Scanning electron microscope image of an array of “zipper” optomechanical cavities. The scale and sensitivity of the device is set by its physical mass (40 picograms /1 trillionth of a gram) and the nanoscale gap between the two nanobeams (100 nanometers/1 billionth of a meter).

“To this end, we made our cantilevers many, many times smaller, and made the optical interaction many, many times larger,” he said.

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They call this nanoscale device a zipper cavity because of the way its dual cantilevers – or nanobeams, as Painter calls them – move together and apart when the device is in use. “If you look at it, it actually looks like a zipper,” he said.

“Zipper structures break new ground on coupling photonics with micromechanics and can impact the way we measure motion, even into the quantum realm,” said Kerry Vahala, Caltech’s Ted and Ginger Jenkins Professor of Information Science and Technology and professor of applied physics, and one of the authors of a paper on the work that appeared a recent issue of the journal Nature. “The method embodied in the zipper design also suggests new microfabrication design pathways that can speed advances in the subject of cavity optomechanics as a whole.”

To create their zipper cavity device, the researchers made two nanobeams from a silicon chip, poking holes through the beams to form an effective optical mirror. Instead of training a light down onto the nanobeams, the researchers used optical fibers to send the light “in plane down the length of the beams,” said Painter. The holes in the nanobeams intercept some of the photons, circulating them through the cavity between the beams rather than allowing them to travel straight through the device.

Or, to be more precise, the circulating photons actually create the cavity between the beams. As Painter puts it: “The mechanical rigidity of the structure and the changes in its optical response are predominantly governed by the internal light field itself.”

Such an interaction is possible, he adds, because the structure is precisely designed to maximize the transfer of momentum from the input laser’s photons to the mechanical nanobeams. Indeed, a single photon of laser light zipping through this structure produces a force equivalent to 10 times that of Earth’s gravity. With the addition of several thousand photons to the cavity, the nanobeams are effectively suspended by the laser light.

Changes in the intensity and other properties of the light as it moves along the beams to the far end of the chip can be detected and recorded, just as with any large-scale interferometer.

The potential uses for this sort of optomechanical zipper cavity are myriad. It could be used as a sensor in biology by coating it with a solution that would bind to, say, a specific protein molecule that might be found in a sample. The binding of the protein molecule to the device would add mass to the nanobeams and thus change the properties of the light traveling through them, signaling that such a molecule had been detected. Similarly, it could be used to detect other ultrasmall physical forces, Painter adds.

Zipper cavities could also be used in optical communications, where circuits route information via optical beams of different colors, i.e., wavelengths.

“You could control and manipulate what the optical beams of light are doing,” Painter said. “As the optical signals moved around in a circuit, their direction or color could be manipulated via other control light fields.” This would create tunable photonics, “optical circuits that can be tuned with light.”

Additionally, the zipper cavity could lead to applications in RF-over-optical communications and microwave photonics as well, where a laser source is modulated at microwave frequencies, allowing the signals to travel for kilometers along optical fibers. In such systems, the high-frequency mechanical vibrations of the zipper cavity could be used to filter and recover the RF or microwave signal riding on the optical wave.

The research was supported by a DARPA seeding effort, and an Emerging Models and Technologies grant from the National Science Foundation.
 
For more information, visit: www.caltech.edu

Published: June 2009
Glossary
beam
1. A bundle of light rays that may be parallel, converging or diverging. 2. A concentrated, unidirectional stream of particles. 3. A concentrated, unidirectional flow of electromagnetic waves.
cantilever
A projecting beam or other structure supported only at one end.
chip
1. A localized fracture at the end of a cleaved optical fiber or on a glass surface. 2. An integrated circuit.
nano
An SI prefix meaning one billionth (10-9). Nano can also be used to indicate the study of atoms, molecules and other structures and particles on the nanometer scale. Nano-optics (also referred to as nanophotonics), for example, is the study of how light and light-matter interactions behave on the nanometer scale. See nanophotonics.
photonics
The technology of generating and harnessing light and other forms of radiant energy whose quantum unit is the photon. The science includes light emission, transmission, deflection, amplification and detection by optical components and instruments, lasers and other light sources, fiber optics, electro-optical instrumentation, related hardware and electronics, and sophisticated systems. The range of applications of photonics extends from energy generation to detection to communications and...
wavelength
Electromagnetic energy is transmitted in the form of a sinusoidal wave. The wavelength is the physical distance covered by one cycle of this wave; it is inversely proportional to frequency.
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