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Thesis (pdf) - Swinburne University of Technology

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lost—making any meaningful interferometry impossible after this point when<br />

the atoms are localised in the left or right well. This collapse into separate<br />

BECs with undefined relative phase was experimentally seen not only for two<br />

wells [Shi05] but also for an array <strong>of</strong> traps [Gre02a, Gre02b]. These results<br />

seem to indicate that the splitting <strong>of</strong> the BEC has to stay in the so-called<br />

Josephson regime to be useful for interferometry [Jav86, Sme97, Sak02], or<br />

that the whole process <strong>of</strong> splitting, phase evolution and recombining for the<br />

measurement has to be done on short timescales to maintain the coherence<br />

between the wells. The coherence between the wells will only survive as long<br />

as the atom numbers are undefined. One way to achieve this is to split only<br />

so far that some tunnelling is still allowed, so that the atom numbers <strong>of</strong> the<br />

wells fluctuate and are not defined, like in the the above-mentioned Josephson<br />

regime. Another way to keep the coherence is to split the single atoms between<br />

the wells. As long as localisation can be prevented, the atoms in the two wells<br />

then are coherent. However, a BEC consists <strong>of</strong> interacting particles, and these<br />

interactions can be interpreted as measurements <strong>of</strong> the location <strong>of</strong> the atoms.<br />

This limits the coherence time, but there are ways to reduce the interaction<br />

strength by so-called Feshbach resonances [Mar02, Web03, Shi04].<br />

Theoretical work is continuing on this topic, examining the splitting pro-<br />

cess more closely [Bor04] for weakly interacting atoms and ways are being re-<br />

searched on how to increase the sensitivity <strong>of</strong> such an interferometer [Neg04].<br />

Other proposals use the BEC only as a means to create atoms in the ground<br />

state <strong>of</strong> the potential well. Atoms that do not interact with each other, because<br />

they have a scattering length <strong>of</strong> zero, will overcome some <strong>of</strong> the problems <strong>of</strong><br />

the interferometers proposed with interacting BECs. These then in principle<br />

work like multiple single atom interferometers [Dud03], where the single atom<br />

interferometers are the ones proposed for atom chips [Hin01, H¨01c]. Other<br />

6

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