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Lecture 8: Laser amplifiers

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Population inversion<br />

<br />

Population inversion in a medium is generally defined as<br />

N 2 > (g 2 /g 1 ) N 1<br />

(N 2 > N 1 for g 1 = g 2 )<br />

<br />

<br />

However, this condition does not guarantee an optical gain at a particular<br />

optical frequency when the population in each level, |1> or |2>, is<br />

distributed unevenly among its sublevels.<br />

A better condition for population inversion to guarantee an optical gain at<br />

a given frequency <br />

N 2 e () – N 1 a () > 0<br />

<br />

The pumping requirement for the condition to be satisfied depends on the<br />

properties of a medium. For atomic and molecular media, there are three<br />

different basic systems. Each has a different pumping requirement to<br />

reach effective population inversion for an optical gain. The pumping<br />

requirement can be found by solving the coupled rate equations.<br />

49

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