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arXiv 1707.04055cond-mat.quant-gas
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玻色-爱因斯坦凝聚体的参量激发:从法拉第波到粒化

Parametric Excitation of a Bose-Einstein Condensate: From Faraday Waves to Granulation

J. H. V. Nguyen, M. C. Tsatsos, D. Luo, A. U. J. Lode, G. D. Telles, V. S. Bagnato, R. G. Hulet

摘要:

我们从实验和理论两方面探讨了拉长的玻色-爱因斯坦凝聚体对调制相互作用的响应。我们确定了两个不同的制度在调制频率和调制强度。纵向表面波产生共振或参数附近的径向陷阱频率或两倍的陷阱频率的调制频率,分别。这些波的色散,后者是一个法拉第波,是很好地再现了平均场论,占的3D性质的拉长凝聚。相比之下,在较低的调制频率的制度,我们发现,没有明确的共振发生,但随着调制强度的增加,冷凝物形成不规则的粒状分布的范围外的平均场方法。我们发现颗粒凝聚体具有很大的量子涨落和关联,这可以用零温下超平均场论计算的波函数,多组态含时Hartree玻色子方法进行单次模拟来描述.

英文摘要:

We explore, both experimentally and theoretically, the response of an elongated Bose-Einstein condensate to modulated interactions. We identify two distinct regimes differing in modulation frequency and modulation strength. Longitudinal surface waves are generated either resonantly or parametrically for modulation frequencies near the radial trap frequency or twice the trap frequency, respectively. The dispersion of these waves, the latter being a Faraday wave, is well-reproduced by a mean-field theory that accounts for the 3D nature of the elongated condensate. In contrast, in the regime of lower modulation frequencies we find that no clear resonances occur, but with increased modulation strength, the condensate forms an irregular granulated distribution that is outside the scope of a mean-field approach. We find that the granulated condensate is characterized by large quantum fluctuations and correlations, which are well-described with single-shot simulations obtained from wavefunctions computed by a beyond mean-field theory at zero temperature, the multiconfigurational time-dependent Hartree for bosons method.

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