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Experiments to Control Atom Number and Phase-Space Density in ...

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Optical molasses do not provide a spatial conf<strong>in</strong>ement, <strong>and</strong> are thus a cool<strong>in</strong>g<br />

<strong>and</strong> not a trapp<strong>in</strong>g method.<br />

2.9 Magne<strong>to</strong>-Optical Trap<br />

While optical molasses provides an effective method <strong>to</strong> cool a<strong>to</strong>ms, it cannot<br />

conf<strong>in</strong>e a<strong>to</strong>ms for an extended period of time; optical molasses is not an optical trap for<br />

a<strong>to</strong>ms. The extension of the idea of optical molasses <strong>to</strong> create a trap is called magne<strong>to</strong>-<br />

optical trap (MOT) [37].<br />

Add<strong>in</strong>g a quadrupole magnetic field, created by a pair of anti-Helmholtz coils, <strong>to</strong><br />

the three pairs of counter-propagat<strong>in</strong>g laser beams creates a magne<strong>to</strong>-optical trap. A<br />

schematic of the setup is shown <strong>in</strong> figure 2.15. The res<strong>to</strong>r<strong>in</strong>g force <strong>to</strong>wards the center<br />

of the trap is aga<strong>in</strong> provided by pho<strong>to</strong>ns scattered from the laser beams. Because<br />

the magnetic field def<strong>in</strong>es a quantization axis, the polarization of the laser beams is<br />

important. The beams have <strong>to</strong> be circularly polarized, where oppos<strong>in</strong>g beams have<br />

opposite h<strong>and</strong>edness [22, 35].<br />

σ<br />

σ<br />

Figure 2.15: Schematic of a magne<strong>to</strong>-optical trap setup. A pair of anti-Helmholtz coils<br />

produces a quadrupole magnetic field. Three pairs of counter-propagat<strong>in</strong>g laser beams<br />

with opposite circular polarization cause a res<strong>to</strong>r<strong>in</strong>g force, push<strong>in</strong>g a<strong>to</strong>ms <strong>to</strong>wards the<br />

center of the magnetic quadrupole field. Figure courtesy of Gabriel Price.<br />

σ<br />

σ<br />

22<br />

σ<br />

σ

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