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

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Appendix A<br />

Magic Wavelength of Hydrogen<br />

The concept of a magic wavelength is important for precision frequency mea-<br />

surements of optically trapped a<strong>to</strong>ms. In general, an optical potential will <strong>in</strong>troduce an<br />

AC-Stark shift of the energy levels, lead<strong>in</strong>g <strong>to</strong> a spatial dependence of the transition<br />

frequency with<strong>in</strong> the trapped cloud, <strong>and</strong> limit<strong>in</strong>g the precision achievable. Many new<br />

technologies rely on precision time; the Global Position<strong>in</strong>g System (GPS) is just one<br />

important example.<br />

This section <strong>in</strong>troduces the idea of a magic wavelength trap, <strong>and</strong> how this provides<br />

a unique environment for precision spectroscopy. Subsequently, the magic wavelength<br />

for hydrogen is determ<strong>in</strong>ed theoretically.<br />

A.1 Magic Wavelength<br />

An optical clock us<strong>in</strong>g trapped neutral a<strong>to</strong>ms is desirable for two ma<strong>in</strong> reasons:<br />

long <strong>in</strong>teraction times <strong>and</strong> high short-term stability [127, 128]. Because trapped neutral<br />

a<strong>to</strong>ms exhibit both qualities, they can potentiall provide a frequency st<strong>and</strong>ard superior<br />

<strong>to</strong> s<strong>in</strong>gle-ion <strong>and</strong> a<strong>to</strong>mic founta<strong>in</strong> clocks. This would be an important step <strong>to</strong>wards new<br />

tests of fundamental physics <strong>and</strong> improved measurements of fundamental constants.<br />

Chapter 2.6.2 showed that the shift of a<strong>to</strong>mic energy levels of an a<strong>to</strong>m <strong>in</strong> the<br />

presence of an external light field due <strong>to</strong> the AC-Stark effect is given by (compare<br />

equation 2.26)<br />

∆EAC = − 1<br />

Re(α)I (A.1)<br />

2ǫ0c<br />

= − 1 <br />

|〈k|µ|j〉|<br />

4ǫ0c<br />

2<br />

<br />

1<br />

ωkg +ω +<br />

<br />

1<br />

I. (A.2)<br />

ωkg −ω<br />

k<br />

174

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