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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

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