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Copyright by Kirsten Viering 2006 - Raizen Lab - The University of ...

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Chapter 3<br />

Magic Wavelength<br />

<strong>The</strong> concept <strong>of</strong> a magic wavelength is mostly discussed in connection with time and<br />

frequency measurements. Today time and frequency standards are determined <strong>by</strong><br />

Cesium fountain clocks as NIST-F1, where transitions are induced in a microwave-<br />

cavity [14]. Although frequency is already the most precisely measurable quantity,<br />

frequency measurements would be greatly improved <strong>by</strong> exploiting optical instead <strong>of</strong><br />

microwave transitions.<br />

For an optical clock, ultracold neutral atoms have to be trapped in order to<br />

minimize Doppler-Shifts. Optical traps have the disadvantage <strong>of</strong> shifting the energy<br />

levels, where the magnitude <strong>of</strong> the shift is proportional to the intensity <strong>of</strong> the beam<br />

used to create the trap, as we have shown in the previous chapter. In general, these<br />

shifts are different for different atomic levels, and the resonance frequency therefore<br />

depends on the trapping potential, i.e. the exact position <strong>of</strong> the atom inside the trap.<br />

Nevertheless, if the energy shifts are equal for the ground and the respective excited<br />

state the resonance frequency gets insensitive to the intensity <strong>of</strong> the laser beam and<br />

hence to the trapping potential. <strong>The</strong> wavelength with the above characteristics is called<br />

the magic wavelength [15].<br />

An attractive trap at the magic wavelength provides the same potential for the<br />

ground and excited state. Hence the atoms held in this trap are not heated when a<br />

resonant transition is induced. <strong>The</strong> fluorescence signal contains information not only<br />

13

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