26.09.2014 Views

Lecture 8: Laser amplifiers

Lecture 8: Laser amplifiers

Lecture 8: Laser amplifiers

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

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 />

75

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!