24.07.2013 Views

Experiments to Control Atom Number and Phase-Space Density in ...

Experiments to Control Atom Number and Phase-Space Density in ...

Experiments to Control Atom Number and Phase-Space Density in ...

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.

FM<br />

λ<br />

Figure 4.9: MOT master laser saturated absorption spectroscopy setup. Figure courtesy<br />

of Gabriel Price.<br />

Error Signal<br />

a b c d e f<br />

MOT Master Laser Frequency<br />

Figure 4.10: Error signal of the MOT master laser. The marked transitions are due <strong>to</strong> the<br />

follow<strong>in</strong>g real <strong>and</strong> crossover transitions: (a) |F = 2〉 → |F ′ = 1〉, (b) |F = 2〉 → |F ′ =<br />

1/2〉, (c) |F = 2〉 → |F ′ = 2〉, (d) |F = 2〉 → |F ′ = 2/3〉, (e) |F = 2〉 → |F ′ = 2/3〉, (f)<br />

|F = 2〉 → |F ′ = 3〉<br />

This setup locks the laser 280 MHz <strong>to</strong> the red of the |F = 2〉 → |F ′ = 3〉<br />

transition. The 280 MHz detun<strong>in</strong>g from the transition is due <strong>to</strong> a number of frequency<br />

55

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

Saved successfully!

Ooh no, something went wrong!