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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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