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City of Light: The Story of Fiber Optics

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244 CITY OF LIGHT<br />

sent signals at four separate wavelengths through a series <strong>of</strong> six erbium amplifiers<br />

and 459 kilometers <strong>of</strong> fiber. 23 Each channel carried 2.4 billion bits per<br />

second.<br />

Other groups encoded their signals in fancy ways to try to make them<br />

resistant to degradation. <strong>The</strong> KDD team didn’t bother. <strong>The</strong>y just turned the<br />

light from each transmitter <strong>of</strong>f for zero bits and on for one bit, a coding called<br />

NRZ that was used throughout the digital telephone network. It was far from<br />

clear that they were blazing a trail for a revolution.<br />

Despite all their attractions, optical amplifiers have a serious inherent limitation.<br />

<strong>The</strong>y depend on stimulated emission, which from an engineer’s viewpoint<br />

is an analog process. At its best, an analog amplifier merely multiplies<br />

the strength <strong>of</strong> the signal it receives. If the input contains noise, it multiplies<br />

the noise along with the signal. If dispersion has stretched the input pulses,<br />

it multiplies the stretched-out pulses. In short, an optical amplifier turns up<br />

the power but does nothing to clean up the signal.<br />

In contrast, sophisticated digital electro-optic repeaters do more than amplify<br />

the signal they receive. <strong>The</strong>y regenerate the original series <strong>of</strong> digital<br />

pulses. Discrimination circuits decide if the input power represents a zero or<br />

a one. Timing circuits fit the pulses into their proper time slots. After figuring<br />

out what the received signal should be, the electronics regenerate a nice clean<br />

series <strong>of</strong> pulses. TAT-8 used such regenerators to send sharp digital signals<br />

across the Atlantic.<br />

Optical amplifiers produce some noise, but in practice the main concern<br />

was the dispersion <strong>of</strong> pulses as they traveled long distances through the fiber.<br />

Dispersion wasn’t a problem as long as single-mode fibers were transmitting<br />

near their zero-dispersion wavelength <strong>of</strong> 1.31 micrometers, with repeaters<br />

about every 50 kilometers. However, erbium amplifies at 1.55 micrometers,<br />

where single-mode fibers have higher dispersion. Realizing the promise <strong>of</strong><br />

erbium amplifiers required a way to control that dispersion.<br />

One approach is to transmit signals in a form not affected by dispersion.<br />

Linn Mollenauer <strong>of</strong> Bell Labs had already shown that special pulses called<br />

solitons could overcome dispersion by delicately balancing it against another<br />

effect called self-phase modulation that can distort light pulses in an optical<br />

fiber. While dispersion tries to stretch the duration <strong>of</strong> the pulse, self-phase<br />

modulation tries to stretch out the range <strong>of</strong> wavelengths it contains. As long<br />

as the power is high enough to trigger the distortion, and the pulse has the<br />

right shape, the tug <strong>of</strong> war between the two effects lets the pulse pass unaltered.<br />

24 Solitons needed optical amplification to keep the pulses powerful<br />

enough. Mollenauer had earlier tried an exotic amplification process, but erbium<br />

amplifiers worked better. A series <strong>of</strong> experiments made the future look<br />

bright for solitons and erbium amplifiers.<br />

A different approach is to control dispersion <strong>of</strong> the fiber itself without doing<br />

special tricks with the transmitted signals. In the early 1980s, both Corning<br />

and British Telecom had designed special single-mode fibers with complex core<br />

structures which shifted their zero-dispersion wavelengths to 1.55 micrometers.<br />

25 <strong>The</strong> emergence <strong>of</strong> erbium amplifiers renewed interest in dispersion-

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