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Direct Energy, 2018a

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158 7.4 Devices Involving Stimulated Emission<br />

a photon by spontaneous or stimulated emission. Alternatively, other excited<br />

electrons decay to a lower energy level while emitting heat or lattice<br />

vibrations instead. The internal quantum eciency is the ratio of the rate<br />

with which excited electrons decay and produce a photon over the rate at<br />

which all excited electrons decay [10, p. 562]. It depends on temperature,<br />

the concentration of impurities or crystalline defects, and other factors [10,<br />

p. 596].<br />

Eciency is also determined by the laser cavity. A laser cavity reects<br />

photons towards the active material. However, the laser cavity must let<br />

some light exit. In many lasers, the cavity is formed by mirrors. While<br />

these mirrors reect most of the light, some light is absorbed and some light<br />

is transmitted through the mirrors as laser output. Many lasers which use<br />

mirrors include lenses, prisms, and other optical components in the cavity<br />

to focus or lter light to the active material. These components may also<br />

reect or absorb some light and thereby decrease the laser eciency. As<br />

mentioned above, the cavity of many semiconductor lasers is formed by<br />

the interface between the active material and the surrounding air. While<br />

external mirrors can reect over 99% of photons [86, p. 159], mirrors formed<br />

by semiconductor air interfaces are much less ecient. The amount of light<br />

reected depends on the indexof refraction of the material. In gallium<br />

arsenide, for example, the index of refraction is 3.52 which corresponds to<br />

only 31% of light reected at each interface [97].<br />

The inuence on eciency of internal absorption and mirror reectivity<br />

can be summarized in a single relationship [98].<br />

( )<br />

1<br />

ln<br />

R<br />

η eff = η eff−other ( ) (7.22)<br />

αl +ln<br />

In this equation, R is the unitless mirror reectivity, α is the absorption<br />

coecient of the active material in units m −1 , and l is the length of the<br />

active material in m. The term η eff−other represents the eciency due to<br />

all other factors besides absorption and mirror reectivity, and η eff is the<br />

overall eciency. Equation 7.22 can be rewritten with some algebra.<br />

⎛<br />

⎞<br />

1<br />

η eff = η eff−other<br />

⎝1 − ( ) ⎠ (7.23)<br />

1+ 1 ln 1<br />

αl R<br />

These eciency concepts generalize to other energy conversion devices<br />

which produce light. Equation 7.20 also describes the overall eciency of<br />

LEDs and lamps in addition to electrically pumped lasers. The concepts<br />

1<br />

R

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