Lecture 8: Laser amplifiers
Lecture 8: Laser amplifiers
Lecture 8: Laser amplifiers
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Two-level systems<br />
Take the upward pumping rate W 12p = W p and the downward<br />
pumping rate to be W 21P = p W p , where p is a constant that depends<br />
on the detailed characteristics of the two-level atomic system and<br />
the pump source.<br />
In the steady state when dN 2 /dt = dN 1 /dt = 0,<br />
N 2 e –N 1 a = [W p 2 ( e -p a )- a ]N t [1+(1+p)W p 2 + (I 2 /h)( e + a )] -1<br />
<br />
For optical pumping<br />
p = ep / ap = e ( p )/ a ( p ),<br />
where ap and ep are the absorption and emission cross sections at<br />
the pump wavelength.<br />
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