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Single-Photon Atomic Cooling - Raizen Lab - The University of ...

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to other existing cooling techniques. <strong>The</strong> prospects <strong>of</strong> such a demonstration<br />

are particularly promising in light <strong>of</strong> recent work with supersonic beams which<br />

produced trapped samples <strong>of</strong> paramagnetic atoms [97, 98] and molecules [99–<br />

102] at tens <strong>of</strong> millikelvins in a simple room-temperature apparatus. <strong>The</strong><br />

general nature <strong>of</strong> the single-photon cooling technique means that it can po-<br />

tentially be adapted to cool and trap a large portion <strong>of</strong> these species, many <strong>of</strong><br />

which cannot be laser cooled with existing techniques. <strong>The</strong>re has even been<br />

a proposal to use this technique to cool molecules [103], which existing laser<br />

cooling techniques have failed to cool due to their complicated energy level<br />

structures.<br />

<strong>The</strong> main focus in our lab however will be the application <strong>of</strong> single-<br />

photon atomic cooling to hydrogenic isotopes. <strong>The</strong> methods described in this<br />

dissertation, with appropriate modifications, are well suited to cooling and<br />

trapping all three isotopes. In short, the proposed technique begins by seed-<br />

ing a supersonic beam <strong>of</strong> neon with the hydrogenic isotope under study. After<br />

entrainment, the hydrogenic beam will be brought to rest and trapped mag-<br />

netically using an “atomic coilgun.” In fact, atomic hydrogen has already been<br />

trapped in this manner [98]. Once trapped, the single-photon cooling process<br />

will proceed in a manner similar to that discussed in this dissertation. <strong>The</strong><br />

species will initially be in the |F = 1,mF = 1〉 state. <strong>The</strong>se atoms will be<br />

depopulated near their classical turning points by driving them into the 2s<br />

manifold via a two-photon transition at 243 nm. This long lived metastable<br />

state will be quenched by application <strong>of</strong> a DC electric field mixing it with<br />

180

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