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City of Light: The Story of Fiber Optics

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EPILOGUE: THE BOOM, THE BUBBLE, AND THE BUST 241<br />

<strong>The</strong>y noted that a fiber with a doped core could be used as an optical<br />

amplifier. All they needed was to remove the mirrors and fire a weak pulse<br />

<strong>of</strong> light at the right wavelength down the fiber. That input would stimulate<br />

excited neodymium atoms to emit light at exactly the same wavelength, amplifying<br />

the signal. Initially the idea didn’t seem promising. Neodymium atoms<br />

emitted at 1.06 micrometers, far from the best transmission windows <strong>of</strong> glass<br />

fibers. Stimulated emission from neodymium also didn’t seem strong enough.<br />

To be useful for communications, an optical amplifier had to multiply the<br />

power <strong>of</strong> an input signal by a factor <strong>of</strong> 1000, or 30 decibels, which Payne<br />

didn’t think was possible in a few meters <strong>of</strong> fiber. Instead, he played with<br />

lasers, where power built up as light bounced back and forth between the<br />

mirrors at the opposite ends <strong>of</strong> the fiber.<br />

Other rare earth elements also had useful optical properties, so the Southampton<br />

group also added them to the cores <strong>of</strong> fibers. 7 <strong>The</strong>y soon made lasers<br />

from fibers containing another rare earth called erbium, which emits strongly<br />

at 1.53 micrometers. <strong>The</strong> wavelength was interesting because it is very close<br />

to where silica fibers are most transparent. Experiments showed the erbium<br />

laser wavelength could be varied across a range <strong>of</strong> 25 nanometers. 8<br />

<strong>The</strong> physics <strong>of</strong> erbium didn’t look promising, but the Southampton group<br />

studied it closely. Only slowly did they realize that the nature <strong>of</strong> their fiber<br />

laser experiments was changing the rules. <strong>The</strong>y excited the erbium atoms by<br />

focusing the blue-green beam from an argon gas laser into the core <strong>of</strong> a singlemode<br />

fiber. <strong>The</strong> power from the argon laser aimed into the fiber was modest,<br />

but concentrating it in the tiny core excited most <strong>of</strong> the erbium atoms, eliminating<br />

the loss they had expected from unexcited erbium. ‘‘It took us 26<br />

publications on fiber lasers before we realized that, if we took the mirrors <strong>of</strong>f<br />

and looked at what the gain was, we’d have a huge gain <strong>of</strong> 30 decibels’’<br />

needed for an amplifier, Payne recalled. 9<br />

<strong>The</strong>ir first experiments in late 1986 lived up to expectations. <strong>The</strong>y recorded<br />

peak amplification <strong>of</strong> 26 decibels during pulses from the argon laser. Critically,<br />

they also saw low noise, which is essential for practical optical amplification. 10<br />

Later they boosted the peak gain to 28 decibels by exciting the erbium atoms<br />

with red light from a different laser. <strong>The</strong>y also made another critical discovery:<br />

erbium atoms could amplify light by a factor <strong>of</strong> ten (10 decibels) across a 25nanometer<br />

range <strong>of</strong> wavelengths. 11<br />

<strong>The</strong> first experiment suggested that optical amplifiers could extend the<br />

reach <strong>of</strong> systems transmitting one signal per optical fiber. <strong>The</strong> second experiment<br />

held out another hope—that erbium could multiply the bandwidth <strong>of</strong><br />

a single fiber by amplifying signals at two or more different wavelengths.<br />

<strong>The</strong> idea is called wavelength-division multiplexing, and the old Bell System<br />

had tried it in its ill-fated Northeast Corridor system. <strong>The</strong> idea <strong>of</strong> sending<br />

signals simultaneously at two different wavelengths wasn’t bad; the problem<br />

had been the technology Bell used. Every seven kilometers the optical signals<br />

had to be converted to electrical form and amplified, then used to drive a new<br />

laser transmitter. That required separating the two signals by wavelength and<br />

directing each one to a separate receiver and transmitter.

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