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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Figure 5.3: Photograph <strong>of</strong> the hydrogen coilgun coil wound around the slowing chamber.<br />
The coils are held in place by Delrin clamps, which are clamped onto the chamber<br />
before the coil is wound.<br />
is 19.5 mm. The overall length <strong>of</strong> the coil is 7.26 mm. When the coil is pulsed, a peak<br />
current <strong>of</strong> approximately 825 A flows through the coil, producing peak on axis fields<br />
<strong>of</strong> 1.4 T. The finite element numerical calculation <strong>of</strong> the field pr<strong>of</strong>ile can be seen in<br />
figure 5.2.<br />
The coils are wound around the vacuum chamber and held in place by Delrin<br />
spacers that are clamped to the chamber, <strong>as</strong> shown in figure 5.3. This allows the<br />
coils to be <strong>as</strong> close <strong>as</strong> possible to the atoms <strong>with</strong>out being in vacuum. The Delrin<br />
spacers place the coils 12.45 mm apart center-to-center. This spacing is set by the<br />
wire thickness, <strong>as</strong> the wire from the inner layer <strong>of</strong> a coil needs a path to the outside<br />
<strong>of</strong> the coils. Making the coils much closer together would make it difficult to insert<br />
the inner winding if the adjacent coil is already wound.<br />
5.2.1.2 Slowing Coil Electronics and Switching<br />
Due to the incre<strong>as</strong>ed size <strong>of</strong> the coils, the inductance <strong>of</strong> the hydrogen coilgun<br />
coils is larger than the coils used in the previous coilgun iterations (10 μH instead<br />
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