Bogoliubov Excitations of Inhomogeneous Bose-Einstein ...
Bogoliubov Excitations of Inhomogeneous Bose-Einstein ...
Bogoliubov Excitations of Inhomogeneous Bose-Einstein ...
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Abstract<br />
In this thesis, different aspects <strong>of</strong> interacting ultracold bosons in presence<br />
<strong>of</strong> inhomogeneous external potentials are studied. The first part deals with<br />
repulsively interacting <strong>Bose</strong>-<strong>Einstein</strong> condensates in speckle disorder potentials.<br />
In the <strong>Bogoliubov</strong> approach, the many-body problem is split into the<br />
Gross-Pitaevskii condensate (mean-field) and the <strong>Bogoliubov</strong> excitations,<br />
which are bosonic quasiparticles. The disorder potential causes an imprint<br />
in the condensate, which makes the Hamiltonian for the <strong>Bogoliubov</strong> excitations<br />
inhomogeneous. The inhomogeneous <strong>Bogoliubov</strong> Hamiltonian is<br />
the starting point for a diagrammatic perturbation theory that leads to the<br />
renormalized <strong>Bogoliubov</strong> dispersion relation. From this effective dispersion<br />
relation, physical quantities are derived, e.g. the mean free path and disorder<br />
corrections to the speed <strong>of</strong> sound and the density <strong>of</strong> states. The analytical<br />
results are supported by a numerical integration <strong>of</strong> the Gross-Pitaevskii<br />
equation and by an exact diagonalization <strong>of</strong> the disordered <strong>Bogoliubov</strong> problem.<br />
In the second part, Bloch oscillations <strong>of</strong> <strong>Bose</strong>-<strong>Einstein</strong> condensates in<br />
presence <strong>of</strong> time-dependent interactions are considered. In general, the interaction<br />
leads to dephasing and destroys the Bloch oscillation. Feshbach<br />
resonances allow the atom-atom interaction to be manipulated as function<br />
<strong>of</strong> time. In particular, modulations around zero are considered. Different<br />
modulations lead to very different behavior: either the wave packet evolves<br />
periodically with time or it decays rapidly. The former is explained by a periodic<br />
time-reversal argument. The decay in the other cases can be described<br />
by a dynamical instability with respect to small perturbations, which are<br />
similar to the <strong>Bogoliubov</strong> excitations in the first part.