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The experiments are actually performed in three-dimensions with varying degrees of transverse confinement. Under these conditions, the axially self-trapped condensate is strictly speaking a bright solitary wave; the three-dimensional analog of the bright soliton. In line with the large body of published literature, however, we refer to these states as solitons.
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We consider silicon in order to be able to compare our results with the experimental observations of quantum reflection using a repulsive condensate [12].
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50
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67349204209
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note
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For Δ x < 5 μ m, atom losses occur even before the reflection process begins.
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51
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28844432114
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Simulations and experiments have been performed in which the trap centre was not shifted all the way to the surface
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Simulations and experiments have been performed in which the trap centre was not shifted all the way to the surface,. Günther A., Kraft S., Kemmler M., Koelle D., Kleiner R., Zimmermann C., and Fortágh J. Phys. Rev. Lett. 95 (2005) 170405
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34147125351
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This forced the BEC to rise up the far side of the harmonic trap and hence decelerate before striking the surface. This improves control of the impact speed, but the presence of the harmonic potential remains a complicating factor and can affect the condensate's dynamics
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Günther A., Kraft S., Zimmermann C., and Fortágh J. Phys. Rev. Lett. 98 (2007) 140403 This forced the BEC to rise up the far side of the harmonic trap and hence decelerate before striking the surface. This improves control of the impact speed, but the presence of the harmonic potential remains a complicating factor and can affect the condensate's dynamics
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