Lecture 8: Laser amplifiers
Lecture 8: Laser amplifiers
Lecture 8: Laser amplifiers
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Neodymium-doped glass<br />
<br />
Level 1 is 0.24 eV above the ground state. This is substantially<br />
larger than the thermal energy 0.026 eV at room temperature, so<br />
that the thermal population of the lower laser is negligible.<br />
Level 3 is a collection of four absorption bands, centered at 805,<br />
745, 585, and 520 nm.<br />
<br />
<br />
The excited ions decay rapidly from level 3 to level 2 and then<br />
remain in level 2 for a substantial time sp = 330 s. 1 is very<br />
short (~ 300 ps)<br />
The 2→1 transition is inhomogeneously broadened because of the<br />
amorphous nature of the glass, which presents a different<br />
environment at each ionic location. This material therefore has a<br />
large spontaneous linewidth (gain bandwidth) ≈ 6 THz<br />
66<br />
66