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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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5.2 The Hydrogen Apparatus<br />

The apparatus constructed to slow and trap a supersonic beam <strong>of</strong> hydrogen is<br />

different from the coilgun used to slow neon and oxygen. The differences are primarily<br />

due to the incre<strong>as</strong>ed magnetic moment to m<strong>as</strong>s ratio <strong>of</strong> hydrogen, which significantly<br />

lowers the magnetic field strength requirements while still permitting slowing in a<br />

short distance. The lower field requirements permit the coils to be incre<strong>as</strong>ed in size.<br />

This incre<strong>as</strong>es number <strong>of</strong> atoms slowed due to the incre<strong>as</strong>ed aperture and allows the<br />

coils to be removed from vacuum, reducing the experimental complexity. The new coil<br />

geometry and electronics are described, along <strong>with</strong> the advantages <strong>of</strong> this change in<br />

geometry. The experiment also integrates a magnetic trap at the end <strong>of</strong> the coilgun,<br />

and the method by which the atoms can be trapped is explained, along <strong>with</strong> the<br />

trap design and electronics. Finally, since the beam consists <strong>of</strong> hydrogen, the beam<br />

creation and detection are changed.<br />

5.2.1 Slowing Coils and Electronics<br />

The greatly incre<strong>as</strong>ed magnetic moment to m<strong>as</strong>s ratio <strong>of</strong> hydrogen ( 1amu ),<br />

3 μB<br />

1.8 μB<br />

compared <strong>with</strong> met<strong>as</strong>table neon ( ) or molecular oxygen ( ), permits smaller<br />

20 amu 32 amu<br />

fields to be used in a convenient laboratory scale coilgun. An incre<strong>as</strong>e in the coil size<br />

is thus fe<strong>as</strong>ible, which results in several advantages. The most significant advantage <strong>of</strong><br />

using larger coils is that the coils can be moved outside <strong>of</strong> the vacuum envelope, greatly<br />

reducing the experimental complexity. Outside <strong>of</strong> vacuum, the need for feedthroughs<br />

is eliminated and the coils can be cooled much more e<strong>as</strong>ily, allowing the repetition rate<br />

<strong>of</strong> the experiment to be incre<strong>as</strong>ed and reducing the time required to take data. The<br />

larger coils require a modification to the switching electronics since the inductance <strong>of</strong><br />

a coil incre<strong>as</strong>es <strong>with</strong> its size.<br />

119<br />

1 μB

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