论文标题
准膜冷冷原子链中的拓扑量子光态
Topological quantum optical states in quasiperiodic cold atomic chains
论文作者
论文摘要
在这项工作中,研究了一维(1D)准碘冷原子链中的拓扑量子光学态。我们提出,通过对1D周期性原子链的原子间距离进行不兑换的调制,可以模仿非对抗的Abry-André-Harper(AAH)模型,尽管至关重要的差异是长距离偶极 - 偶极相互作用的存在。相对于调制阶段的离散带结构,该阶段的作用是尺寸扩展参数的作用,是针对最近邻近近似值以外的有限链计算的。发现目前的系统确实支持在边界上定位的非平凡拓扑状态。尽管存在导致不对称带结构的远距离偶极 - 偶极相互作用,但证明该系统继承了二维整数量子Hall系统的拓扑特性。对于真实和假想的频率,光谱位置以及这些受拓扑保护的边缘状态的数量仍由差距标记的定理控制,并以拓扑不变的特征,即(第一个)Chern数字,表明散装信函的有效性。由于在大量的系统参数范围内由准二拟合产生的分形光谱,因此我们的系统提供了大量的拓扑间隙和光学状态,易于实用。还发现,很大一部分拓扑边缘状态是高度次级的,衰减率极低,因此为控制外部量子发射器的排放提供了一种吸引人的途径,并实现了高保真的量子状态存储。
Topological quantum optical states in one-dimensional (1D) quasiperiodic cold atomic chains are studied in this work. We propose that by introducing incommensurate modulations on the interatomic distances of 1D periodic atomic chains, the off-diagonal Aubry-André-Harper (AAH) model can be mimicked, although the crucial difference is the existence of long-range dipole-dipole interactions. The discrete band structures with respect to the modulation phase, which plays the role of a dimension extension parameter, are calculated for finite chains beyond the nearest-neighbor approximation. It is found that the present system indeed supports nontrivial topological states localized over the boundaries. Despite the presence of long-range dipole-dipole interactions that leads to an asymmetric band structure, it is demonstrated that this system inherits the topological properties of two-dimensional integer quantum Hall systems. The spectral position, for both real and imaginary frequencies, and number of these topologically protected edge states are still governed by the gap-labeling theorem and characterized by the topological invariant, namely, the (first) Chern number, indicating the validity of bulk-boundary correspondence. Due to the fractal spectrum arising from the quasiperiodicity in a substantially wide range of system parameters, our system provides a large number of topological gaps and optical states readily for practical use. It is also revealed that a substantial proportion of the topological edge states are highly subradiant with extremely low decay rates, which therefore offer an appealing route for controlling the emission of external quantum emitters and achieving high-fidelity quantum state storage.