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Tuning the relaxation dynamics of ultracold atoms with an optical cavity

机译:用光学腔调整超冷原子的弛豫动力学

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摘要

We investigate the out-of-equilibrium dynamics of ultracold atoms trapped inan optical lattice and loaded into an optical resonator that is driventransversely. We derive an effective quantum master equation for weakatom-light coupling that can be brought into Lindblad form both in the bad andgood cavity limits. In the so-called bad cavity regime, we find that the steadystate is always that of infinite temperature, but that the relaxation dynamicscan be highly non-trivial. For small hopping, the interplay between dissipationand strong interactions generally leads to anomalous diffusion in the space ofatomic configurations. However, for a fine-tuned ratio of cavity-mediated andon-site interactions, we discover a limit featuring normal diffusion. Incontrast, for large hopping and vanishing on-site interactions, the system canbe described by a linear rate equation leading to an exponential approach ofthe infinite-temperature steady state. Finally, in the good cavity regime, weshow that for vanishing on-site interactions, the system allows for opticalpumping between momentum mode pairs enabling cavity cooling.
机译:我们研究了被困在光学晶格中并装入横向驱动的光学谐振器中的超冷原子的失衡动力学。我们推导了一个有效的弱原子-光耦合的量子主方程,该方程可以在坏腔和好腔范围内都转换为Lindblad形式。在所谓的坏腔状态下,我们发现稳态始终是无限温度下的稳态,但是弛豫动态却非常重要。对于小跳频,耗散与强相互作用之间的相互作用通常会导致在原子构型空间中的异常扩散。但是,对于微调的腔介导的和现场相互作用的比率,我们发现了一个以正态扩散为特征的极限。相反,对于大的跳跃和消失的现场相互作用,可以通过导致无限温度稳态的指数方法的线性速率方程来描述该系统。最后,在良好的腔体状态下,我们表明,为了消除现场相互作用,该系统允许在动量模式对之间进行光学泵浦,从而实现腔体冷却。

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