Lecture 8: Laser amplifiers
Lecture 8: Laser amplifiers
Lecture 8: Laser amplifiers
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Gain and bandwidth<br />
<br />
<br />
The wave is amplified with a gain coefficient () (per unit<br />
length) and undergoes a phase shift () (per unit length).<br />
() > 0 corresponds to amplification, () < 0 corresponds<br />
to attenuation.<br />
Recall that the probability density (s -1 ) that an unexcited<br />
atom absorbs a single photon is<br />
<br />
W i<br />
( )<br />
where the transition cross section at the frequency <br />
2<br />
c<br />
( ) <br />
2 2<br />
8n<br />
<br />
gˆ(<br />
)<br />
Here we assume the probability density for stimulated<br />
emission is the same as that for absorption. ( a () = e () =<br />
())<br />
sp<br />
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