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Anderson localization of a non-interactingBose-Einstein condensate

机译:非相互作用的玻色-爱因斯坦凝聚物的安德森局部化

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Anderson localization of waves in disordered media was originally predicted fifty years ago, in the context of transport of electrons in crystals. The phenomenon is much more general and has been observed in a variety of systems, including light waves. However, Anderson localization has not been observed directly for matter waves. Owing to the high degree of control over most of the system parameters (in particular the interaction strength), ultracold atoms offer opportunities for the study of disorder-induced localization, Here we use a non-interacting Bose-Einstein condensate to study Anderson localization. The experiment is performed with a one-dimensional quasi-periodic lattice-a system that features a crossover between extended and exponentially localized states, as in the case of purely random disorder in higher dimensions. Localization is clearly demonstrated through investigations of the transport properties and spatial and momentum distributions. We characterize the crossover, finding that the critical disorder strength scales with the tunnelling energy of the atoms in the lattice. This controllable system may be used to investigate the interplay of disorder and interaction (ref. 7 and references therein), and to explore exotic quantum phases.
机译:最初是在50年前在晶体中电子传输的背景下预测了安德森在无序介质中的电波定位。这种现象更为普遍,并且已经在包括光波在内的各种系统中被观察到。但是,尚未直接观察到物质波的安德森定位。由于对大多数系统参数(特别是相互作用强度)的高度控制,超冷原子为无序诱导的局域化研究提供了机会。在这里,我们使用非相互作用的玻色-爱因斯坦凝聚物研究安德森局域化。该实验是使用一维准周期晶格进行的,该系统具有扩展状态和指数局部状态之间的交叉特征,就像在更高维度上的纯随机无序情况一样。通过研究运输特性以及空间和动量分布可以清楚地证明本地化。我们表征了交叉,发现临界无序强度与晶格中原子的隧穿能成比例。该可控系统可用于研究无序和相互作用的相互作用(参考文献7及其中的参考文献),并探索奇异的量子相。

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