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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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The apertures set the transverse temperature, and hotter atoms are removed from the<br />

beam by the apertures, leaving only the colder atoms in the beam. For this re<strong>as</strong>on,<br />

it is appropriate to concentrate on the parallel component <strong>of</strong> the velocity, giving the<br />

Gaussian velocity pr<strong>of</strong>ile<br />

<br />

m<br />

p(v) = e<br />

2πkBT<br />

− m(v<br />

<br />

−w) 2<br />

2kB T<br />

=<br />

σ<br />

1<br />

√ e<br />

2π −(v <br />

−w) 2<br />

2σ 2 , (2.25)<br />

where σ is the standard deviation in the velocity parallel to the beam axis. This<br />

velocity distribution is compared to the Maxwellian velocity distribution for a few<br />

relevant g<strong>as</strong> species and reservoir temperatures in figure 2.1. As can be seen in<br />

the figure, the width <strong>of</strong> the velocity pr<strong>of</strong>ile is significantly narrower for the c<strong>as</strong>e <strong>of</strong><br />

a supersonic beam. Expressed in terms <strong>of</strong> temperature, beams <strong>of</strong> a few tens to a<br />

few hundred milliKelvin are common. This is significantly colder than the reservoir<br />

temperatures, and the supersonic expansion h<strong>as</strong> effectively cooled the beam.<br />

The cooling achieved by supersonic expansion is extremely general and can be<br />

used to cool any desired species. In the above discussion on isotropic expansion, it is<br />

<strong>as</strong>sumed that the g<strong>as</strong>es were truly ideal g<strong>as</strong>es. <strong>Supersonic</strong> beams are generally created<br />

<strong>with</strong> a noble carrier g<strong>as</strong> that generally behaves <strong>as</strong> an ideal g<strong>as</strong> at higher pressures<br />

and lower temperatures than many other g<strong>as</strong> species. Other species <strong>of</strong> interest are<br />

mixed in the reservoir before the expansion, or added just outside the nozzle during<br />

the expansion. If the species <strong>of</strong> interest is a g<strong>as</strong> at the reservoir temperature, it is<br />

typically seeded into the carrier g<strong>as</strong> in the reservoir. A species that is not a g<strong>as</strong> at the<br />

reservoir temperature is typically entrained into the beam at the exit <strong>of</strong> the nozzle.<br />

L<strong>as</strong>er ablation can be used to produce an atomic sample <strong>of</strong> a solid at the exit <strong>of</strong> a<br />

nozzle, or alternatively, an oven can produce an atomic beam that is then entrained in<br />

the supersonic beam. In either c<strong>as</strong>e, the added species is cooled by thermalizing <strong>with</strong><br />

the dominant carrier g<strong>as</strong> and is carried along <strong>with</strong> the supersonic beam, providing a<br />

15

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