周期势中玻色-爱因斯坦凝聚体的非线性诱导效应

O. Morsch
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引用次数: 0

摘要

在BECs中,凝聚原子之间的碰撞对动力学产生非线性贡献,通常作为薛定谔方程中的平均场项。这种非线性导致了周期势中与物质波相关的众所周知的效应的修正,并增加了线性问题中不存在的一些现象。我们关注加速光学晶格中BEC的动力学。在线性情况下,这会引起布洛赫振荡,并在超过临界加速度时引起朗道-齐纳隧穿。在非线性情况下,朗道-齐纳隧穿的概率根据其发生在两个带之间的方向进行修正。通过改变光学晶格的加速度和测量干涉对比度的时间依赖性,我们能够确定不稳定状态和动态不稳定破坏干涉图案的特征时间。此外,我们观察到,当到达不稳定区域时,垂直于晶格方向的凝聚尺寸增加。这表明了纵向不稳定性导致横向释放能量增加的机制
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Nonlinearity-induced effects of Bose-Einstein condensates in periodic potentials
In BECs, collisions between condensate atoms give rise to a nonlinear contribution to the dynamics which is typically included as a mean-field term in the Schrodinger equation. This nonlinearity leads to a modification of well-known effects associated with matter waves in periodic potentials and adds a number of phenomena that are absent in the linear problem. We focused on the dynamics of a BEC in an accelerated optical lattice. In the linear case, this gives rise to Bloch oscillations and, above a critical acceleration, to Landau-Zener tunneling. In the nonlinear case, the probability for Landau-Zener tunneling is modified depending on the direction in which it occurs between two bands. By varying the acceleration of the optical lattice and measuring the time-dependence of the interference contrast, we were able to identify the instability regime and the characteristic time in which the dynamical instability destroys the interference pattern. Furthermore, we observed an increase in the condensate dimensions perpendicular to the lattice direction when the unstable region was reached. This indicates a mechanism whereby the longitudinal instability leads to an increase in the transverse release energy
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