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ANNUAL REPORT 2006

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Annual report <strong>2006</strong> 24<br />

we have constructed the effective actions that incorporate the one-loop effects in the<br />

presence of an NS five-brane and membrane respectively. We have restricted ourselves<br />

to the study of these nonperturbative effects in the case of the universal hypermultiplet.<br />

In the case of the NS five-brane we have performed an instanton calculation by<br />

constructing the one-loop measure in the presence of the NS five-brane. This measure<br />

can then be used to compute correlation functions and thereby construct the effective<br />

action. The effects of the membrane have been computed by making use of knowledge<br />

of the isometries that are preserved and/or broken by this object. Gauging the unbroken<br />

isometry of the universal hypermultiplet produces a potential. We have shown<br />

that the nonperturbative membrane effects to the effective action make it possible for<br />

this potential to have a (meta-)stable de Sitter vacuum.<br />

Dickerscheid, D.B.M. (UU)<br />

thesis title: Quantum phases in optical lattices<br />

advisors: prof. dr. ir. H.T.C. Stoof<br />

co-advisor: dr. P.J.H. Denteneer<br />

date: 6 February <strong>2006</strong><br />

present position: postdoctoral fellow, Tokyo Institute of Technology, Japan<br />

An important new development in the field of ultracold atomic gases is the study<br />

of the properties of these gases in a so-called optical lattice. An optical lattice is a<br />

periodic trapping potential for the atoms that is formed by the interference pattern<br />

of a few laser beams. A reason for the interest in these systems is that the effects of<br />

the interatomic interactions can be strongly enhanced. More specifically, it has been<br />

shown in a beautiful experiment by Greiner et al. in 2002 that by loading a Bose-<br />

Einstein condensate into an optical lattice it is possible for the system to undergo a<br />

quantum phase transition to a new quantum phase of matter, the so-called Mott insulator<br />

phase. Within this Mott insulator phase each lattice site is occupied by exactly<br />

one atom. This makes the Mott insulator phase especially well suited for applications<br />

in the field of quantum computation and quantum information processing. We have<br />

theoretically investigated the above mentioned quantum phase transition and our formalism<br />

allows for a description of the Mott insulator phase at nonzero temperatures.<br />

Another important experimental development in the field of ultracold atomic gases is<br />

the use of Feshbach resonances to control the interatomic interactions. Such a resonance<br />

occurs whenever two colliding atoms form a long-lived molecule for some time.<br />

The crucial point of a Feshbach resonance is that the above mentioned molecule has a<br />

magnetic moment that is not equal to twice the magnetic moment of the atom. As a<br />

consequence the energy difference between the two atoms and the molecule and hence<br />

the interactions between the atoms can be controlled by using an external magnetic<br />

field. By combining these two techniques, i.e, by trapping ultracold atomic gases in<br />

an optical lattice and by tuning a magnetic field near a Feshbach resonance there can<br />

be a new quantum phase transition between two superfluid phases.<br />

We gave derived the the theory for the description of these Feshbach Resonances in<br />

optical lattices and applied it to various systems. To be a bit more precise, if we tune<br />

the external magnetic field such that the energy difference between a molecule and<br />

two atoms is sufficiently negative, then the gas consists of a Bose-Einstein condensate

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