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Experiments with Supersonic Beams as a Source of Cold Atoms

Experiments with Supersonic Beams as a Source of Cold Atoms

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8 Ω<br />

LN2<br />

Liquid<br />

Nitrogen<br />

Dewar<br />

Nozzle<br />

Figure 4.32: A schematic summary <strong>of</strong> the system used to cool the nozzle to 150 K.<br />

A 50 W 8Ω resistor provides a variable heat source in a liquid nitrogen dewar, which<br />

controls the rate <strong>of</strong> the boil<strong>of</strong>f. The cold g<strong>as</strong>eous nitrogen is forced to flow through<br />

the cryostat <strong>of</strong> the nozzle, cooling it. Incre<strong>as</strong>ing the current in the resistor incre<strong>as</strong>es<br />

the boil <strong>of</strong>f rate, and cools the nozzle more.<br />

advantageous to cool the nozzle significantly below room temperature to reduce the<br />

initial velocity <strong>of</strong> the beam. With a lower temperature limit <strong>of</strong> 120K from the krypton<br />

carrier g<strong>as</strong>, and due to a desire to avoid excessive clustering and heating <strong>of</strong> the beam,<br />

the nozzle is run at a temperature <strong>of</strong> 150 K. To run the nozzle at this temperature, a<br />

g<strong>as</strong> line is run from a tank <strong>of</strong> liquid nitrogen to the pool type cryostat <strong>of</strong> the nozzle.<br />

This directs the cold boil <strong>of</strong>f g<strong>as</strong> from the liquid nitrogen dewar into the cryostat,<br />

cooling the nozzle. The flow rate <strong>of</strong> the boil <strong>of</strong>f is controlled by inserting a 50 W<br />

8 Ω resistor into the nitrogen dewar, <strong>with</strong> greater current leading to more power in<br />

the resistor and f<strong>as</strong>ter boil <strong>of</strong>f. Currents <strong>of</strong> up to 3 A are run through the resistor,<br />

which exceeds the power rating and is only fe<strong>as</strong>ible because the resistor is immersed<br />

in liquid nitrogen. A schematic illustration <strong>of</strong> this method <strong>of</strong> cooling the nozzle is<br />

shown in figure 4.32.<br />

The final change in the apparatus concerns the detection method. Since the<br />

oxygen is not met<strong>as</strong>table, it will not create a free electron when it hits the surface<br />

112

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