Hubbard Model for Asymmetric Ultracold Fermionic ... - KOMET 337
Hubbard Model for Asymmetric Ultracold Fermionic ... - KOMET 337
Hubbard Model for Asymmetric Ultracold Fermionic ... - KOMET 337
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Chapter 3Unbalanced Fermi-mixturesIn this chapter we will discuss a Fermi-mixture with unequal occupation numbers <strong>for</strong> thedifferent spin species. We will assume that the system is in the ground state T = 0 andthat the hopping amplitudes are the same <strong>for</strong> both spin-species. The parabolic potentialcaused by the magneto-optical trap will be introduced and treated within the local densityapproximation (LDA). We will discuss the phases which can occur in such a system and shownumerical results <strong>for</strong> given trap parameters.3.1 Broken translational invariance and the LDAIn this section we will introduce the concept of the LDA <strong>for</strong> treating the trapping potential.<strong>Ultracold</strong> quantum gases are usually trapped in a magneto-optical trap, which can be describedby a quadratic potential <strong>for</strong> the atoms. The trapping potential and the superimposedoptical lattice <strong>for</strong>m the effective potential in space which the atoms feel [5]. We illustrate thepotential here in one dimension (arbitrary units):2121-2 -1 1 2-1-2 -1 1 2-1-2-2Figure 3.1: Potentials felt by the atomsRed curve: Lattice potentialGreen curve: Trapping potentialFigure 3.2: Sum of the lattice and trapping potentialsIn our one-band tight-binding approximation we assumed that the atoms can be describedas Wannier-states, which are localized around specific lattice sites. Here the position of alattice site is defined, e.g., by a minimum of the translationally invariant lattice potential.We will now assume that the trapping potential varies slowly enough in space, so that thedescription via the Wannier-states is still acceptable and the hopping of atoms from one site19