Bogoliubov Excitations of Inhomogeneous Bose-Einstein ...
Bogoliubov Excitations of Inhomogeneous Bose-Einstein ...
Bogoliubov Excitations of Inhomogeneous Bose-Einstein ...
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3. Disorder<br />
In the previous chapter, we have set up the general formalism for describing<br />
<strong>Bogoliubov</strong> excitations in a weak external potential, and, as a first application,<br />
we have applied it to the scattering <strong>of</strong> <strong>Bogoliubov</strong> waves at a single<br />
impurity. Now it is time to enter the disordered world by specifying the<br />
potential V (r) as a disordered potential with certain statistical properties.<br />
The disorder potential causes an imprint in the condensate density, which<br />
forms an inhomogeneous background for the excitations (figure 3.1).<br />
In section 3.1, the experimentally relevant optical speckle potential is<br />
presented, and its statistical properties are derived. The speckle disorder will<br />
be used throughout this work. In the final results, the two-point correlation<br />
function <strong>of</strong> the speckle disorder can be replaced with the correlation function<br />
<strong>of</strong> any other kind <strong>of</strong> disorder.<br />
The goal <strong>of</strong> this chapter is to give a useful characterization <strong>of</strong> the dynamics<br />
<strong>of</strong> <strong>Bogoliubov</strong> excitations in presence <strong>of</strong> disorder. Of course, the results<br />
should not depend on the particular realization <strong>of</strong> disorder, so suitable disorder<br />
averages are necessary. Before doing so, some considerations about<br />
the choice <strong>of</strong> the basis for the excitations have to be made. Until now, the<br />
free <strong>Bogoliubov</strong> basis in terms <strong>of</strong> density and phase fluctuations has been<br />
used rather intuitively. In section 3.2, it is discussed in detail, why this<br />
basis actually is the only reasonable choice for the disordered <strong>Bogoliubov</strong><br />
problem.<br />
All considerations made so far meet in section 3.3, the essential <strong>of</strong> this<br />
chapter. The propagation <strong>of</strong> <strong>Bogoliubov</strong> excitations in the disorder averaged<br />
effective medium is described by the average Green function, which<br />
reveals the disorder-broadened dispersion relation, with a finite lifetime and<br />
a renormalized propagation speed <strong>of</strong> the excitations. The optical analog <strong>of</strong><br />
this is the index <strong>of</strong> refraction and the absorption coefficient in a medium<br />
like glass or water.<br />
Figure 3.1: Schematic representation <strong>of</strong> the<br />
disordered <strong>Bogoliubov</strong> setting. The disorder<br />
potential (red) leaves an imprint in<br />
the condensate (blue). On top <strong>of</strong> that,<br />
wave excitations (green) are considered.<br />
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