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Floqeut topological phases in PT symmetric quantum walks with gain and loss

机译:Pt对称量子中的Floquet拓扑阶段随着增益和损失而行走

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A quantum walk, that is, a synthetic quantum system mainly impremented by photonic systems, whose dynamics is described by a time-evolution operator, provides potential applications for quantum computing and information. It is further interesting that the quantum walk possesses novel topological phases akin to those of Floquet topological insulators, which are topological insulators driven by a time-periodic field[1,2]. Recently, a one-dimensional quantum walk dynamics associated with gain and loss is experimentally implemented by optical fiber loops [3]. The experiment shows that the energy of the system is kept to be real as a manifestation of PT symmetry (combined parity and time-reversal symmetry) in spite of the open quantum system.In this work, we theoretically study Floquet topological phases driven by the PT symmetric non-unitary time evolution. We have found the presence of combined parity and chiral symmetry, in addition to PT symmetry[4]. The presence of these symmetries allows us to study Floquet topological phases in open quantum systems by using a procedure for ordinal quantum walks belonging to class BDI[5]. We have confirmed that the number of edge states originating from Floquet topological phases and topological numbers satisfy the bulk-edge correspondence, while a modification due to the imaginary energy is required due to breaking of PT symmetry. We have also found that the probability corresponding to edge states exponentially increases due to the imaginary energy with increasing time as shown in Fig.1. This provides a way to observe huge probabilities originating from edge states in actual experimental setups. We also mention the experimental setup and result confirming the above theoretical predictions.
机译:量子步行,即主要由光子系统压出的合成量子系统,其动态由时换运算符描述了普通计算和信息的潜在应用。它进一步有趣的是,量子步道具有类似于浮子拓扑绝缘体的新型拓扑阶段,这是由时间周期性领域驱动的拓扑绝缘体[1,2]。最近,通过光纤回路实验地实现了与增益和损耗相关的一维量子行走动态[3]。实验表明,尽管打开量子系统,但是系统的能量将是PT对称性(组合奇偶校验和时间反转对称性)的表现形式。在这项工作中,我们理论上研究了由此驱动的浮子拓扑阶段PT对称的非酉时间进化。除了PT对称性之外,我们还发现存在组合奇偶校验和手性对称性[4]。这些对称性的存在使我们能够通过使用属于BDI类的序数量子行程的程序研究开放量子系统中的浮子拓扑阶段[5]。我们已经证实,源自浮子拓扑阶段和拓扑数字的边缘状态满足散装边缘对应关系,而由于PT对称性,需要由于假想的能量而导致的修改。我们还发现,与边缘状态相对应的概率由于具有升高时间的虚线而导致的,如图1所示。这提供了一种方法来观察源自实际实验设置中的巨大概率。我们还提到了实验设置和结果证实了上述理论预测。

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