Lecture 8: Laser amplifiers
Lecture 8: Laser amplifiers
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 />
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