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 ...
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<strong>and</strong> thus <strong>to</strong> coat the viewports.<br />
Figure 7.29: Spectroscopy cell.<br />
lithium reservoir<br />
The spectroscopy cell is heated near the lithium reservoir with high-temperature<br />
heater tape. It is <strong>in</strong>sulated us<strong>in</strong>g fiber glass. To avoid frequency shifts due <strong>to</strong> the presence<br />
of magnetic fields, the heater tape is wound around the cell <strong>in</strong> such a way as <strong>to</strong> m<strong>in</strong>imize<br />
the result<strong>in</strong>g magnetic fields due <strong>to</strong> currents flow<strong>in</strong>g through the tape. Except near the<br />
lithium reservoir the spectroscopy cell is kept near room temperature. Lithium a<strong>to</strong>ms<br />
therefore stick <strong>to</strong> the walls of the cell, which reduces the risk of coat<strong>in</strong>g the viewports<br />
with lithium. The first time the lithium reservoir is heated <strong>to</strong> a temperature of about<br />
450 ◦ C. This breaks any oxide layer that might have been formed on the surface of the<br />
lithium metal dur<strong>in</strong>g the preparation <strong>and</strong> load<strong>in</strong>g <strong>in</strong><strong>to</strong> the cell.<br />
7.3.1.3 Frequency-Offset Lock Setups<br />
Frequency-offset lock<strong>in</strong>g has many applications <strong>in</strong> a<strong>to</strong>mic physics experiments.<br />
Most importantly for the lithium setup, it is an easy method <strong>to</strong> lock the imag<strong>in</strong>g diode<br />
laser <strong>and</strong> the master laser, used <strong>to</strong> seed the tapered amplifier, relative <strong>to</strong> the spectroscopy<br />
laser with a frequency offset ∆f. Us<strong>in</strong>g a tunable scheme, it is possible <strong>to</strong> dynamically<br />
change the laser frequency dur<strong>in</strong>g the course of the experimental sequence. This is<br />
important especially for the master laser, where the frequency offset ∆f controls the<br />
MOT detun<strong>in</strong>g. ∆f can then be changed <strong>to</strong> compress the MOT prior <strong>to</strong> load<strong>in</strong>g a<strong>to</strong>ms<br />
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