Experiments with Supersonic Beams as a Source of Cold Atoms
Experiments with Supersonic Beams as a Source of Cold Atoms
Experiments with Supersonic Beams as a Source of Cold Atoms
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Ionizer<br />
500 l/s Turbo Pump<br />
Ion Optics<br />
Quadrupole<br />
Figure 5.17: A CAD image <strong>of</strong> the hydrogen detection chamber <strong>with</strong> a mockup <strong>of</strong> the<br />
Ardara Technologies ionizer and quadrupole. The front <strong>of</strong> the ionizer sits 6.04 cm<br />
from the center <strong>of</strong> the trapping volume.<br />
The trapping chamber is a 6-way 1.33 inch conflat cross <strong>with</strong> tubes made <strong>of</strong><br />
the same dimensions <strong>as</strong> the coilgun chamber’s tube. This chamber is made from 304<br />
stainless steel, since it would be difficult to construct this chamber from titanium.<br />
The center <strong>of</strong> the trapping volume is 6.30 cm from the start <strong>of</strong> the chamber. The<br />
final three coilgun coils are wound around this chamber, and the junction between<br />
the coilgun and trapping chambers leads to a center-to-center distance <strong>of</strong> 28.65 mm<br />
between coils 15 and 16, instead <strong>of</strong> the 12.45 mm between the other coilgun coils.<br />
The cross arms <strong>of</strong> the chamber allow for optical access to the trapped atoms, which<br />
will be important for l<strong>as</strong>er detection and spectroscopy (see section 5.4.1). Finally, the<br />
chamber extends p<strong>as</strong>t the trap to another 1.33 inch conflat 5.03 cm from the center<br />
<strong>of</strong> the trapping volume, which connects to the detection chamber.<br />
The detection chamber serves two purposes in the experiment. First, it houses<br />
the Ardara Technologies ionizer and quadrupole m<strong>as</strong>s spectrometer used to for detec-<br />
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