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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500 l/s Turbo<br />
Pump<br />
<strong>Cold</strong> Cathode<br />
Vacuum Gauge<br />
Helium<br />
Beam<br />
Figure 3.4: A CAD image <strong>of</strong> the rotor chamber. The chamber is pumped by a 500 l/s<br />
turbo pump (indicated). The chamber walls are 1 inch thick 304 stainless steel, and<br />
the chamber disc is 112cm in diameter and 12.7cm high.<br />
<strong>of</strong> 5 Hz (10 −8 torr when the nozzle is not operating). This is monitored by a cold<br />
cathode vacuum gauge (not shown). The nozzle hangs from a pool type cryostat into<br />
the center <strong>of</strong> the 6-way cross. The beam propagates 30cm to the 5cm skimmer, which<br />
h<strong>as</strong> a 5 mm aperture. From the skimmer, the beam p<strong>as</strong>ses into the rotor chamber,<br />
which is connected to the nozzle chamber by a flexible bellows, allowing the helium<br />
beam to be aligned to the rest <strong>of</strong> the experiment.<br />
The rotor chamber h<strong>as</strong> to accommodate the rotor, which is the key element<br />
in the design <strong>of</strong> the chamber <strong>as</strong> a whole. As described in section 3.3.2, the rotor is<br />
100.8 cm in diameter, and so the chamber needs to be large enough to allow it to spin<br />
freely. In addition, the beam needs to enter the interaction region and be detected.<br />
This led to a custom chamber design, <strong>as</strong> seen in figure 3.4. The chamber is pumped<br />
by a 500 l/s Varian turbo pump that keeps the chamber at a pressure <strong>of</strong> 2 · 10 −8 torr<br />
while the nozzle is firing (10 −9 torr when the nozzle is not operating). The chamber<br />
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