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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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a method by which beams <strong>of</strong> helium may be controlled. In the experiment described<br />

here, specular reflection from receding single crystal surfaces is used to control the<br />

velocity <strong>of</strong> a supersonic beam <strong>of</strong> helium atoms. The crystal is mounted on the tip<br />

<strong>of</strong> a spinning rotor that provides the necessary crystal velocity to effectively slow the<br />

beam. The original concept for this experiment w<strong>as</strong> first proposed by Doak [41], but<br />

the design studied had an expected slow beam flux that is significantly lower than in<br />

the experiment described here. The work presented in this chapter is also described<br />

in [33, 42, 43].<br />

The slower itself is similar to the beam paddle that w<strong>as</strong> developed for neutrons<br />

[44]. For helium atoms reflecting from a linearly moving single crystal surface, the<br />

velocity <strong>of</strong> the atoms after hitting the mirror will be<br />

vf = −vi +2vm, (3.2)<br />

where vf is the final velocity <strong>of</strong> the atoms, vi is the initial velocity <strong>of</strong> the incoming<br />

beam, and vm is the velocity <strong>of</strong> the mirror. The mirror is <strong>as</strong>sumed to be perpendicular<br />

to the incoming beam. Since the typical velocity <strong>of</strong> a supersonic beam is 500 m/s,<br />

reducing the velocity <strong>of</strong> the beam by a factor <strong>of</strong> two requires a crystal velocity <strong>of</strong><br />

125 m/s. While it is possible to create a device to repeatably move a mirror linearly<br />

at these speeds (perhaps by mounting the mirror on a projectile and launching and<br />

catching it using electromagnetic coils), it is simpler to let rotary motion approximate<br />

linear motion and mount the crystal on the tip <strong>of</strong> a spinning rotor arm. This facilitates<br />

the high mirror velocities required to significantly slow the beam. The introduction<br />

<strong>of</strong> rotary motion complicates equation 3.2, and the full description <strong>of</strong> the velocity<br />

change due to an atom reflecting from the rotor is shown in appendix A.<br />

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