Lecture 8: Laser amplifiers
Lecture 8: Laser amplifiers
Lecture 8: Laser amplifiers
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Four-level pumping<br />
<br />
This is not always the case because the population densities<br />
of the ground state and level 3, N g and N 3 , are related to N 1<br />
and N 2 by<br />
N g<br />
N 1<br />
N 2<br />
N 3<br />
N a<br />
<br />
where the total atomic density in the system, N a , is a constant.<br />
If the pumping involves a transition between the ground state<br />
and level 3 with transition probability W, then<br />
R (N g<br />
N 3<br />
)W<br />
<br />
If levels 1 and 3 are short-lived, then N 1 ≈ N 3 ≈ 0, N g + N 2 ≈<br />
N a s.t. N g ≈ N a -N 2 ≈ N a - N<br />
94<br />
94