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

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154 Sound propagation <strong>in</strong> presence of a one-dimensional optical lattice<br />

n<br />

φ / π<br />

0.8<br />

−200 −100 0 100 200<br />

n<br />

φ / π<br />

1.2<br />

1<br />

1<br />

0.5<br />

0<br />

0.5<br />

−1<br />

−200 −100 0 100 200<br />

1.2<br />

1<br />

1<br />

0.5<br />

0<br />

0.5<br />

x / d<br />

0.8<br />

−200 −100 0 100 200<br />

−1<br />

−200 −100 0 100 200<br />

x / d<br />

Figure 11.9: Sound signals <strong>in</strong> the saturation regime at an early (t = 16¯h/ER; upper two panels)<br />

<strong>and</strong> a late stage (t = 200¯h/ER; lower two panels) for a deep lattice with δ/U ≪ 1/3. First<strong>and</strong><br />

third panel from top: Relative density nℓ(t)/nℓ(t =0)obta<strong>in</strong>ed from the DNLS-simulation.<br />

Second <strong>and</strong> forth panel from top: Relative phase (11.11) obta<strong>in</strong>ed from the DNLS-simulation.

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