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Using a numerical implementation of the truncated Wigner approximation, we simulate the experiment reported by Ramanathan et al.
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We corrected for a missing factor of 1 / 2 1/\sqrt{2} in μ 2 D \mu_{2D} in Ref. Ramanathan et al. 2011
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In Ref. Ramanathan et al. 2011 , the 3D speed of sound for a cylindrical BEC, c 3 D = μ / 2 m c_{3D}=\sqrt{\mu/2m} , was used, which is valid in the limit of a Thomas-Fermi distribution in both y y and z z direction. Here, we have plotted the experimental data in terms of c 2 D = 2 μ 2 D ( x b ) / 3 m c_{2D}=\sqrt{2\mu_{2D}(x_{b})/3m} (see Appendix C
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Private communication with the authors of Ref. Ramanathan et al. 2011
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