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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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producing a cold sample. Alternatively, by changing the conditions under which the<br />

beam is created, a supersonic beam can be produced. <strong>Supersonic</strong> beams are signif-<br />

icantly colder and more directional than effusive beams, and temperatures <strong>as</strong> cold<br />

<strong>as</strong> a few tens <strong>of</strong> millikelvin have been achieved in the co-moving frame. <strong>Supersonic</strong><br />

beams are also very general sources <strong>of</strong> atoms, <strong>as</strong> most species can be entrained into<br />

the beam. Since the supersonic beam provides a significant degree <strong>of</strong> cooling, the<br />

development <strong>of</strong> methods to control the atoms in the beam is an exciting field which<br />

holds the promise <strong>of</strong> fulfilling the goal <strong>of</strong> general control <strong>of</strong> atomic motion.<br />

1.1 Cooling an Effusive Beam<br />

Starting <strong>with</strong> a hot beam and using interactions <strong>with</strong> external fields or col-<br />

lisions <strong>with</strong> other atoms is the typical method <strong>of</strong> producing cold samples <strong>of</strong> atoms.<br />

The methods described here are some <strong>of</strong> the techniques used for cooling and trapping<br />

the atomic beams created by effusive sources.<br />

1.1.1 L<strong>as</strong>er Cooling<br />

The use <strong>of</strong> l<strong>as</strong>er induced transitions to cool atomic samples h<strong>as</strong> developed<br />

into a mature and widely used technique [1]. This cooling method uses momentum<br />

transfer from photons to atoms to create a dissipative force that is cools the sample.<br />

While this method h<strong>as</strong> found great success, and is used in many labs in the form <strong>of</strong> the<br />

Zeeman slower [2], and the Magneto-Optical Trap (MOT) [3], there are fundamental<br />

limits to its applicability. Because the momentum <strong>of</strong> a photon is typically less than<br />

that <strong>of</strong> an atom, many scattering events are required to cool each atom, usually on<br />

the order <strong>of</strong> a few thousand. Each scattering event consists <strong>of</strong> an atom absorbing a<br />

photon and transitioning from a lower state into an excited state, and then undergoing<br />

spontaneous decay back to the original lower state.<br />

2

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