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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Chapter 4<br />
Rubidium Apparatus<br />
A modern a<strong>to</strong>mic physics experiment, even the table-<strong>to</strong>p experiment, requires a<br />
large number of different technological equipment, electronics, optics <strong>and</strong> vacuum. All<br />
of these elements have <strong>to</strong> work simultaneously. It is therefore a challenge <strong>to</strong> design<br />
a system <strong>in</strong> such a way that it runs reproducibly <strong>and</strong> reliably. This chapter gives an<br />
overview of the experimental apparatus used <strong>in</strong> the s<strong>in</strong>gle-pho<strong>to</strong>n cool<strong>in</strong>g experiment.<br />
Details about the construnction of the setup can be found <strong>in</strong> [67–70].<br />
4.1 Vacuum System<br />
The vacuum system is designed for the experiment <strong>to</strong> operate <strong>in</strong> the double MOT<br />
configuration [71]. In this configuration a low background pressure is ma<strong>in</strong>ta<strong>in</strong>ed <strong>in</strong> the<br />
science chamber (where the experiments are performed, <strong>in</strong> this setup the lower chamber),<br />
while rubidium a<strong>to</strong>ms can quickly be accumulated <strong>in</strong> the MOT <strong>in</strong> an upper chamber,<br />
where the background pressure is higher. These two chambers are <strong>in</strong>terconnected by a<br />
differential pump<strong>in</strong>g tube that ma<strong>in</strong>ta<strong>in</strong>s the pressure differential while at the same time<br />
allow<strong>in</strong>g for the accumulated a<strong>to</strong>ms <strong>to</strong> be passed from one chamber <strong>in</strong><strong>to</strong> the other. A<br />
pho<strong>to</strong>graph of the rubidium vacuum chamber is shown <strong>in</strong> figure 4.1.<br />
4.1.1 Upper Chamber<br />
The upper chamber consists of a Pyrex glass cell with outer dimensions 4 <strong>in</strong> ×<br />
1.25 <strong>in</strong>×1.25 <strong>in</strong> connected <strong>to</strong> a 2-3/4 CF sta<strong>in</strong>less steel flange through a graded glas-<br />
<strong>to</strong>-metal seal (Larson Electronics Glass Inc, SQ-150-F2). A 6.75 <strong>in</strong> long sta<strong>in</strong>less steel<br />
tube with a tapered hole (diameter between 1/8 <strong>in</strong> at the <strong>to</strong>p <strong>and</strong> 3/8 <strong>in</strong> at the bot<strong>to</strong>m)<br />
serves as differential pump<strong>in</strong>g tube <strong>and</strong> allows the a<strong>to</strong>ms <strong>to</strong> be transferred from the<br />
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