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

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9.5 Small amplitude collective oscillations <strong>in</strong> the presence of harmonic trapp<strong>in</strong>g 127<br />

ω/2πHz<br />

10<br />

9<br />

8<br />

7<br />

6<br />

5<br />

4<br />

3<br />

2<br />

1<br />

0<br />

0 1 2 3 4 5 6 7 8 9 10<br />

Figure 9.1: Frequency of the small amplitude center-of-mass oscillation as a function of lattice<br />

depth s for the experimental sett<strong>in</strong>g [73]. The circles display the experimental data reported<br />

<strong>in</strong> [73]. The solid l<strong>in</strong>e refers to the theoretical prediction (9.51).<br />

quadrupole (Hz)<br />

14<br />

13<br />

12<br />

11<br />

10<br />

s<br />

6.5 7.0 7.5 8.0 8.5 9.0<br />

dipole (Hz)<br />

Figure 9.2: Frequency of the axial quadrupole mode of an elongated condensate trapped <strong>in</strong> the<br />

comb<strong>in</strong>ed potential of harmonic magnetic trap <strong>and</strong> 1D optical lattice as a function of the axial<br />

dipole mode frequency measured for different values of the optical lattice depth from 0ER to<br />

4.1ER <strong>in</strong> the experiment [75]. The l<strong>in</strong>e represents a l<strong>in</strong>ear fit with a slope of 1.57 ± 0.01.<br />

Figure taken from [75].

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