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Direct observation of growth and collapse of a Bose-Einstein condensate with attractive interactions.

机译:直接观察具有相互作用的玻色-爱因斯坦冷凝物的生长和坍塌。

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摘要

Quantum theory predicts that Bose-Einstein condensation of a spatially homogeneous gas with attractive interactions is precluded by a conventional phase transition into either a liquid or solid. When confined to a trap, however, such a condensate can form, provided that its occupation number does not exceed a limiting value. The stability limit is determined by a balance between the self-attractive forces and a repulsion that arises from position-momentum uncertainty under conditions of spatial confinement. Near the stability limit, self-attraction can overwhelm the repulsion, causing the condensate to collapse. Growth of the condensate is therefore punctuated by intermittent collapses that are triggered by either macroscopic quantum tunnelling or thermal fluctuation. Previous observations of growth and collapse dynamics have been hampered by the stochastic nature of these mechanisms. Here we report direct observations of the growth and subsequent collapse of a 7Li condensate with attractive interactions, using phase-contrast imaging. The success of the measurement lies in our ability to reduce the stochasticity in the dynamics by controlling the initial number of condensate atoms using a two-photon transition to a diatomic molecular state.
机译:量子理论预测,具有吸引力相互作用的空间均匀气体的玻色-爱因斯坦凝聚可通过常规的相变转变为液体或固体来排除。但是,当冷凝水被限制在疏水阀中时,只要其占用数量不超过限制值,就可以形成这种冷凝水。稳定性极限由自吸引力与在空间限制条件下位置动量不确定性引起的排斥之间的平衡确定。在稳定极限附近,自吸力会使压斥力不堪重负,从而导致冷凝水坍塌。因此,冷凝物的生长因宏观量子隧穿或热波动触发的间歇性崩塌而中断。这些机制的随机性阻碍了先前对生长和坍塌动力学的观察。在这里,我们使用相衬成像技术对7Li冷凝物的生长和随后的坍塌进行了直接观察,这些冷凝物具有吸引作用。测量的成功在于我们能够通过使用双光子跃迁至双原子分子态来控制缩合原子的初始数量,从而降低动力学的随机性。

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  • 来源
    《Nature》 |2000年第6813期|P.692-695|共4页
  • 作者单位

    Physics and Astronomy Department and Rice Quantum Institute, Rice University, Houston, Texas 77251, USA.;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);美国《化学文摘》(CA);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 自然科学总论;
  • 关键词

  • 入库时间 2022-08-18 02:57:37

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