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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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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