一维超导微波腔晶格中逆旋转波项调制的拓扑相变和拓扑量子态

None Zheng Zhi-Yong, None Chen Li-Jie, None Xiang Lü, None Wang He, None Wang Yi-Ping
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摘要

提出了一种基于超导微波腔的一维晶格理论方案,其中包括两种不同类型的微波腔单元胞。利用通量量子比特控制单元胞间的耦合,模拟和研究其拓扑绝缘体特性。具体而言,通过将反旋转波项映射到p波超导配对项,获得了具有p波超导配对项的一维超导微波腔晶格格式。我们发现p波超导配对项可以调制系统的拓扑量子态,允许创建具有四个边缘态的拓扑量子信息传输通道。此外,当p波超导配对项和最近邻相互作用存在时,我们发现能带发生波动,诱导新能带的产生,但边缘态的简并保持稳定,可以实现多个拓扑量子态传输路径。然而,当其调节值超过阈值时,系统的能隙将闭合,导致边缘态在新的能带中湮灭。进一步,在考虑系统中存在缺陷的情况下,我们发现当缺陷的强度较小时,边缘状态产生较小的波动,但可以明显区分,表明其鲁棒性。当缺陷强度超过阈值时,边缘状态和能带产生不规则波动,使边缘状态融入能带。我们的研究成果具有重要的理论价值和实际意义,可以应用于未来的量子光学和量子信息处理。
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Topological phase transitions and topological quantum states modulated by the counter-rotating wave terms in a one-dimensional superconducting microwave cavity lattice
We propose a one-dimensional lattice theory scheme based on superconducting microwave cavities, which includes two different types of microwave cavity unit cells. The coupling between unit cells is controlled by flux qubits to simulate and study their topological insulator characteristics. Specifically, a one-dimensional superconducting microwave cavity lattice scheme with a p-wave superconducting pairing term is achieved by mapping the counter-rotating wave terms to the p-wave superconducting pairing term. We found that the p-wave superconducting pairing term can modulate the topological quantum state of the system, allowing for the creation of topological quantum information transmission channels with four edge states. In addition, when the p-wave superconducting pairing term and the nearest-neighbor interaction exist, we find that the energy band undergoes fluctuations, inducing the generation of new energy bands, but the degeneracy of the edge states remains stable, which can achieve multiple topological quantum state transmission paths. However, when its regulatory value exceeds the threshold, the energy gap of the system will close, causing the edge states to annihilate in new energy bands. Furthermore, when considering the existence of defects in the system, we found that when the strength of the defects are small, the edge state produces small fluctuations, but it can be clearly distinguished, indicating its robustness. When the strength of the defect exceeds the threshold, the edge state and energy band cause irregular fluctuations, allowing the edge state to integrate into the energy band. Our research results have important theoretical value and practical significance, and can be applied in quantum optics and quantum information processing in the future.
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