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7
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0037033397
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G. Baym and C. J. Pethick, cond-mat/0308325
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G. Baym and C. J. Pethick, cond-mat/0308325.
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J.R. Anglin and M. Crescimanno, cond-mat/0210063
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J.R. Anglin and M. Crescimanno, cond-mat/0210063.
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13
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0142057418
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In this work, measured Tkachenko frequencies showed deviations from existing TF-limit theory valid at low rotation [9]. These were resolved in subsequent theoretical work [11, 13]
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I. Coddington, P. Engels, V. Schweikhard, and E. A. Cornell, Phys. Rev. Lett. 91, 100402 (2003). In this work, measured Tkachenko frequencies showed deviations from existing TF-limit theory valid at low rotation [9]. These were resolved in subsequent theoretical work [11, 13].
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Coddington, I.1
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1442348548
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private communication
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A. H. MacDonald (private communication).
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MacDonald, A.H.1
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1442324148
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L.O. Baksmaty et al., cond-mat/0307368
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L.O. Baksmaty et al., cond-mat/0307368; T. Mizushima et al., cond-mat/0308010.
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T. Mizushima et al., cond-mat/0308010
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L.O. Baksmaty et al., cond-mat/0307368; T. Mizushima et al., cond-mat/0308010.
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V. Bretin, S. Stock, Y. Seurin, and J. Dalibard, cond-mat/0307464.
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24
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1442348549
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note
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2D we correct for quantum-pressure contributions to axial size.
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26
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1442324153
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note
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2D, the axial density profile is slightly better fitted by a Gaussian. To avoid bias, however, we fit all data assuming a TF profile.
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27
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1442299556
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Melting and loss of contrast are also reported in Ref. [17]
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Melting and loss of contrast are also reported in Ref. [17].
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29
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0035672265
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D. L. Feder and C.W. Clark, Phys. Rev. Lett. 87, 190401 (2001); A. L. Fetter, Phys. Rev. A 64, 063608 (2001).
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Fetter, A.L.1
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30
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1442275073
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note
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peak is density weighted along the rotation axis and is radially averaged over the vortex cores within 1/2 the TF radius, as only in this region we fit the observed vortex cores.
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31
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1442275076
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I. Coddington et al. (to be published)
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I. Coddington et al. (to be published).
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33
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1442275079
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G. Baym, cond-mat/0308342
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G. Baym, cond-mat/0308342.
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