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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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