The study was published the week of February 10-14 in the online
edition of the Proceedings of the National Academy of Sciences. The work
is the result of a five-year effort by researchers in the laboratory of
Amnon Yariv, Martin and Eileen Summerfield Professor of Applied Physics
and professor of electrical engineering; the project was led by
postdoctoral scholar Christos Santis (PhD '13) and graduate student
Scott Steger.
Light is capable of carrying vast amounts of information—approximately
10,000 times more bandwidth than microwaves, the earlier carrier of
long-distance communications. But to utilize this potential, the laser
light needs to be as spectrally pure—as close to a single frequency—as
possible. The purer the tone, the more information it can carry, and for
decades researchers have been trying to develop a laser that comes as
close as possible to emitting just one frequency.
Today's worldwide optical-fiber network is still powered by a laser
known as the distributed-feedback semiconductor (S-DFB) laser, developed
in the mid 1970s in Yariv's research group. The S-DFB laser's unusual
longevity in optical communications stemmed from its, at the time,
unparalleled spectral purity—the degree to which the light emitted
matched a single frequency. The laser's increased spectral purity
directly translated into a larger information bandwidth of the laser
beam and longer possible transmission distances in the optical
fiber—with the result that more information could be carried farther and
faster than ever before.
At the time, this unprecedented spectral purity was a direct consequence
of the incorporation of a nanoscale corrugation within the multilayered
structure of the laser. The washboard-like surface acted as a sort of
internal filter, discriminating against spurious "noisy" waves
contaminating the ideal wave frequency. Although the old S-DFB laser had
a successful 40-year run in optical communications—and was cited as the
main reason for Yariv receiving the 2010 National Medal of Science—the
spectral purity, or coherence, of the laser no longer satisfies the
ever-increasing demand for bandwidth.
"What became the prime motivator for our project was that the
present-day laser designs—even our S-DFB laser—have an internal
architecture which is unfavorable for high spectral-purity operation.
This is because they allow a large and theoretically unavoidable optical
noise to comingle with the coherent laser and thus degrade its spectral
purity," he says.
The old S-DFB laser consists of continuous crystalline layers of
materials called III-V semiconductors—typically gallium arsenide and
indium phosphide—that convert into light the applied electrical current
flowing through the structure. Once generated, the light is stored
within the same material. Since III-V semiconductors are also strong
light absorbers—and this absorption leads to a degradation of spectral
purity—the researchers sought a different solution for the new laser.
The high-coherence new laser still converts current to light using the
III-V material, but in a fundamental departure from the S-DFB laser, it
stores the light in a layer of silicon, which does not absorb light.
Spatial patterning of this silicon layer—a variant of the corrugated
surface of the S-DFB laser—causes the silicon to act as a light
concentrator, pulling the newly generated light away from the
light-absorbing III-V material and into the near absorption-free
silicon.
This newly achieved high spectral purity—a 20 times narrower range of
frequencies than possible with the S-DFB laser—could be especially
important for the future of fiber-optic communications. Originally,
laser beams in optic fibers carried information in pulses of light; data
signals were impressed on the beam by rapidly turning the laser on and
off, and the resulting light pulses were carried through the optic
fibers. However, to meet the increasing demand for bandwidth,
communications system engineers are now adopting a new method of
impressing the data on laser beams that no longer requires this "on-off"
technique. This method is called coherent phase communication.
In coherent phase communications, the data resides in small delays in
the arrival time of the waves; the delays—a tiny fraction (10-16) of a
second in duration—can then accurately relay the information even over
thousands of miles. The digital electronic bits carrying video, data, or
other information are converted at the laser into these small delays in
the otherwise rock-steady light wave. But the number of possible delays,
and thus the data-carrying capacity of the channel, is fundamentally
limited by the degree of spectral purity of the laser beam. This purity
can never be absolute—a limitation of the laws of physics—but with the
new laser, Yariv and his team have tried to come as close to absolute
purity as is possible.
Caltech;
Feb. 19, 2014
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