论文标题
冷原子的随机单线阶段,耦合到光子晶体波导
Random singlet phase of cold atoms coupled to a photonic crystal waveguide
论文作者
论文摘要
最近出现了由光子晶体波导附近的冷原子组成的系统,已成为量子原子界面的令人兴奋的平台。这样的系统可以实现由指导光子介导的原子内部状态(旋转)之间的可调远程相互作用。当前,实验平台仍然受到低填充分数的限制,其中原子的数量比可能被捕获的原子的位点数量要小得多。在这里,我们表明,这种制度实际上可以实现有趣的多体量子现象,这些现象通常与短距离无序系统有关。例如,我们展示了系统如何实现所谓的“随机单重阶段”,其中所有原子将所有原子对纠缠单重,但是配对发生在范围的分布中,而不是最近的邻居。我们使用重新归一化的组方法在随机单重阶段中获得自旋纠缠的分布,并显示如何通过绝热的进化从非相互作用的哈密顿量的基础状态达到该状态。我们还讨论如何观察到这个随机的单线阶段。我们预计,这项工作将通过避免填充完美填充的晶格的要求来加速原子 - 纳米光子界面中强相关物质的途径。
Systems consisting of cold atoms trapped near photonic crystal waveguides have recently emerged as an exciting platform for quantum atom-light interfaces. Such a system enables realization of tunable long-range interactions between internal states of atoms (spins), mediated by guided photons. Currently, experimental platforms are still limited by low filling fractions, where the atom number is much smaller than the number of sites at which atoms can potentially be trapped. Here, we show that this regime in fact enables interesting many-body quantum phenomena, which are typically associated with short-range disordered systems. As an example, we show how the system can realize the so-called "random singlet phase", in which all atoms pair into entangled singlets, but the pairing occurs over a distribution of ranges as opposed to nearest neighbors. We use a renormalization group method to obtain the distribution of spin entanglement in the random singlet phase, and show how this state can be approximately reached via adiabatic evolution from the ground state of a non-interacting Hamiltonian. We also discuss how experimentally this random singlet phase can be observed. We anticipate that this work will accelerate the route toward the exploration of strongly correlated matter in atom-nanophotonics interfaces, by avoiding the requirement of perfectly filled lattices.