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

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∆ n ( U / δ ) 1/2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

11.3 Nonl<strong>in</strong>ear propagation of sound signals 155<br />

0<br />

0 3 6 9 12 15<br />

T p b / w<br />

∆ φ / π<br />

0.25<br />

0<br />

0 3 6 9 12 15<br />

T p b / w<br />

Figure 11.10: Results for the density <strong>and</strong> relative signal amplitudes ∆n <strong>and</strong> ∆φ obta<strong>in</strong>ed from<br />

DNLS simulations for vary<strong>in</strong>g barrier parameters TP ,b,w(see Eq.(11.1)), tunnel coupl<strong>in</strong>g δ<br />

<strong>and</strong> on-site <strong>in</strong>teraction U (see Eq.(11.8)) with δ ≪ U/3.<br />

This is <strong>in</strong> agreement with the behavior we f<strong>in</strong>d for ∆n <strong>in</strong> the first (l<strong>in</strong>ear) <strong>and</strong> even <strong>in</strong> the<br />

second (shockwave) regime as summarized <strong>in</strong> Fig. 11.10. The first order approximation to<br />

s<strong>in</strong>(φℓ±1/2) <strong>in</strong> φℓ±1/2 is valid for ∆φ

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