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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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successful. Any water that remains on the crystal can be removed by blowing it <strong>of</strong>f<br />

<strong>with</strong> argon. Storing the crystal in an argon environment until it can be inserted into<br />

vacuum preserves the pristine state <strong>of</strong> the surface.<br />

3.2.3 Crystal Characterization<br />

To characterize the p<strong>as</strong>sivated surfaces, they are examined using an atomic<br />

force microscope (AFM). The AFM is operated in tapping mode, and scanning 2μmby<br />

2μm regions <strong>of</strong> the wafer w<strong>as</strong> found to provide a good compromise between examining<br />

a large area and scan speed. Figure 3.2 shows AFM images <strong>of</strong> a wafer that w<strong>as</strong> wet<br />

etched. Image (a) shows a clean surface, <strong>with</strong> large atomically flat regions. The steps<br />

seen in the image are bilayer steps from one crystal plane to another, and are 3.8 ˚A<br />

high. The image is <strong>of</strong> the wafer 15 minutes after removing it from the etching solution.<br />

Image (b) shows the same wafer after waiting an additional 28 minutes. The apparent<br />

incre<strong>as</strong>e in surface roughness is likely due to the oxidation <strong>of</strong> the crystal. The height<br />

pr<strong>of</strong>iles shown in images (c) and (d) are taken along the white lines shown in (a) and<br />

(b) respectively. The surface roughness shown in (c) is less than an ˚A in magnitude,<br />

and is probably noise in the AFM rather than real artifacts on the crystal surface.<br />

However, the incre<strong>as</strong>ed surface roughness shown in (d) shows grains approximately 2˚A<br />

in height, and is likely showing real contamination <strong>of</strong> the surface. This indicates the<br />

importance <strong>of</strong> minimizing the time the crystals spend in atmosphere before inserting<br />

them into the vacuum chamber.<br />

3.3 The Experimental Apparatus<br />

This section describes the apparatus constructed to create, slow, and detect<br />

a beam <strong>of</strong> supersonic helium. The description <strong>of</strong> the apparatus follows the path <strong>of</strong><br />

the beam, starting <strong>with</strong> the vacuum system, followed by the slowing apparatus, and<br />

28

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