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

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

n(x, t)/n(x, t =0)<br />

φ ℓ+1/2<br />

0.01<br />

0.005<br />

0<br />

−0.005<br />

−0.01<br />

−250 −200 −150 −100 −50 0 50 100 150 200 250<br />

6<br />

4<br />

2<br />

0<br />

−2<br />

−4<br />

−6<br />

x 10 −3<br />

−250 −200 −150 −100 −50 0 50 100 150 200 250<br />

Figure 11.5: Sound propagation <strong>in</strong> the l<strong>in</strong>ear regime without lattice for gn =0.5ER. Upper<br />

panel: Relative density n(x, t)/n(x, t =0)at t = 480¯h/ER of the GP-simulation. Lower<br />

panel: Relative phase as def<strong>in</strong>ed <strong>in</strong> (11.12) at t = 480¯h/ER of the GP-simulation<br />

n(x, t)/n(x, t =0)<br />

φ ℓ+1/2<br />

0.04<br />

0.02<br />

0<br />

−0.02<br />

−0.04<br />

0.04<br />

0.02<br />

−0.02<br />

x/d<br />

−250 −200 −150 −100 −50 0 50 100 150 200 250<br />

0<br />

−0.04<br />

−250 −200 −150 −100 −50 0 50 100 150 200 250<br />

Figure 11.6: Sound propagation <strong>in</strong> the l<strong>in</strong>ear regime with a lattice of depth s = 10 for<br />

gn =0.5ER. Upper panel: Relative density n(x, t)/n(x, t =0)at t = 480¯h/ER of the<br />

GP-simulation. Lower panel: Relative phase as def<strong>in</strong>ed <strong>in</strong> (11.12) at t = 480¯h/ER of the<br />

GP-simulation<br />

x/d

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