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Tuning the relaxation dynamics of ultracold atoms in a lattice with an optical cavity

机译:用光学腔在晶格中调整超级原子的放松动态

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摘要

We investigate the out-of-equilibrium dynamics of ultracold atoms trapped in an optical lattice and loaded into an optical resonator that is driven transversely.We derive an effective quantum master equation for weak atom-light coupling that can be brought into Lindblad form in both the bad- and good-cavity limits. In the so-called bad-cavity regime, we find that the steady state is always that of infinite temperature, but that the relaxation dynamics can be highly nontrivial. For small hopping, the interplay between dissipation and strong interactions generally leads to anomalous diffusion in the space of atomic configurations. However, for a fine-tuned ratio of cavity-mediated and on-site interactions, we discover a limit featuring normal diffusion. In contrast, for large hopping and vanishing on-site interactions, the system can be described by a linear rate equation leading to an exponential approach of the infinite-temperature steady state. Finally, in the good-cavity regime, we show that for vanishing on-site interactions, the system allows for optical pumping between momentum mode pairs enabling cavity cooling.
机译:我们研究了捕获在光学晶格中的超容易静脉的动态,并加载到横向驱动的光学谐振器中。我们导出了用于弱原子光耦合的有效量子母部方程,可以在两者中进入Lindblad形式坏和洞穴的限制。在所谓的坏腔制度中,我们发现稳定状态始终是无限温度的,而是松弛动态可以高度不动。对于小跳跃,耗散和强相互作用之间的相互作用通常导致原子配置空间中的异常扩散。然而,对于腔介导和现场相互作用的微调比率,我们发现具有正常扩散的极限。相反,对于大跳跃和消失的现场相互作用,可以通过线性速率方程描述系统,导致无限温度稳态的指数方法。最后,在良好的腔内制度中,我们表明,为了消失现场相互作用,系统允许在动量模式对之间进行光学泵送,使能腔冷却。

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