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Bose-Einstein Condensates in Rotating Traps and Optical ... - BEC

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8.1 Dynamic structure factor 105<br />

The excitation strength to the lowest Bogoliubov b<strong>and</strong> - Numerical results<br />

The study of the excitation strength to the lowest Bogoliubov b<strong>and</strong> Z1(p) requires the evaluation<br />

of (8.8) with the solutions u1q(z), v1q(z) <strong>and</strong> ϕ(z) for a given lattice depth s <strong>and</strong><br />

<strong>in</strong>teraction parameter gn/ER. Numeric results are depicted <strong>in</strong> Figs.8.3 <strong>and</strong> 8.4 for s =5, 10<br />

<strong>and</strong> gn =0ER, 0.02ER <strong>and</strong> gn =0.5ER.<br />

In general, we f<strong>in</strong>d the follow<strong>in</strong>g characteristics:<br />

• Z1(p) features an overall decay for <strong>in</strong>creas<strong>in</strong>g |p|. This is due to the fact that the<br />

momentum components of the created excitations are smaller at large momenta.<br />

• Provided that gn/ER = 0, Z1(p) exhibits characteristic oscillations: Z1(p) is suppressed<br />

<strong>in</strong> the vic<strong>in</strong>ities of p = l2π/d where the excitations contribut<strong>in</strong>g to the strength have<br />

phonon character <strong>and</strong> is exactly zero at p = l2π/d (l <strong>in</strong>teger) where the energy of the<br />

contribut<strong>in</strong>g excitation vanishes.<br />

• Increas<strong>in</strong>g gn/ER at fixed s or <strong>in</strong>creas<strong>in</strong>g s at fixed gn/ER = 0leads to an overall<br />

decrease of Z1(p).<br />

Z1(p)/Ntot<br />

1<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

−6 −4 −2 0 2 4 6<br />

p/qB<br />

Figure 8.3: Excitation strength to the lowest Bogoliubov b<strong>and</strong> Z1(p) (8.8) at lattice depth<br />

s =5for gn =0.5ER (solid l<strong>in</strong>e), gn =0.02ER (dashed l<strong>in</strong>e) <strong>and</strong> gn =0(dash-dotted l<strong>in</strong>e).

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