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City of Light: The Story of Fiber Optics

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RECIPES FOR GRAINS OF SALT 149<br />

negative carrier) semiconductor. An impurity with one less outer electron<br />

creates a hole, forming a semiconductor <strong>of</strong> the p-type (for positive carrier,<br />

because the absence <strong>of</strong> an electron leaves a positive charge on the atomic<br />

nucleus). Adding such dopants releases more carriers in the crystal, making<br />

better electronic devices. Put layers <strong>of</strong> n-and p-type semiconductor together,<br />

and you have a simple two-terminal device called a diode. 2<br />

Things get interesting when you apply a voltage across a diode. A positive<br />

electrical voltage attracts the negative electrons, while a negative voltage<br />

attracts the positive holes. Apply a positive voltage to the n-type material<br />

and a negative voltage to the p-type material, and the electrons and holes<br />

move to the terminals and stay there, so no current flows through the junction<br />

between the two materials. However, a current will flow if you switch<br />

the voltages, because electrons in the n material move toward the positive<br />

terminal on the p material, and holes move in the opposite direction. Thus,<br />

a semiconductor diode conducts electricity in only one direction 3 (figure<br />

12-1).<br />

<strong>The</strong> real action happens at the junction between n and p material, where<br />

electrons from the n material combine with holes from the p material. As<br />

the electron drops into the hole, it releases its extra energy by a process called<br />

recombination. In silicon, the energy typically is released as heat. However,<br />

in gallium arsenide, indium phosphide, and certain other semiconductor<br />

crystals, some energy is released as light. This is the basis <strong>of</strong> a light-emitting<br />

diode or LED. Initially, the process was quite inefficient. <strong>The</strong> first LEDs turned<br />

only about 0.01 percent <strong>of</strong> the input electrical energy into visible or infrared<br />

light. 4<br />

Birth <strong>of</strong> the Semiconductor Laser<br />

When the laser hit the headlines, a few physicists thought <strong>of</strong> making lasers<br />

from light-emitting semiconductors. However, nobody took the idea too<br />

seriously until 1962, when Robert Rediker, Tom Quist, and Robert Keyes<br />

changed the way they were processing gallium arsenide at the MIT Lincoln<br />

Laboratory. LEDs made from the new material generated light surprisingly<br />

efficiently. When Keyes announced their results at a July 1962 meeting in<br />

New Hampshire, an astounded member <strong>of</strong> the audience stood up to say that<br />

Keyes’s statement violated the second law <strong>of</strong> thermodynamics—a cardinal<br />

principle <strong>of</strong> modern physics which holds that the degree <strong>of</strong> disorder or ‘‘entropy’’<br />

always increases. Keyes returned to the microphone and deadpanned,<br />

‘‘I’m sorry.’’ 5<br />

Bob Hall, a semiconductor expert from the General Electric Research Laboratory,<br />

immediately figured out what the MIT group had done. After everyone<br />

stopped laughing, he stood up and explained why the results were possible.<br />

He also realized that high efficiency opened the door to making a<br />

semiconductor laser. He worked through the numbers on the train ride home,

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