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超导处理器上的拓扑预热强零模

Topological prethermal strong zero modes on superconducting processors.

作者信息

Jin Feitong, Jiang Si, Zhu Xuhao, Bao Zehang, Shen Fanhao, Wang Ke, Zhu Zitian, Xu Shibo, Song Zixuan, Chen Jiachen, Tan Ziqi, Wu Yaozu, Zhang Chuanyu, Gao Yu, Wang Ning, Zou Yiren, Zhang Aosai, Li Tingting, Zhong Jiarun, Cui Zhengyi, Han Yihang, He Yiyang, Wang Han, Yang Jia-Nan, Wang Yanzhe, Shen Jiayuan, Liu Gongyu, Deng Jinfeng, Dong Hang, Zhang Pengfei, Li Weikang, Yuan Dong, Lu Zhide, Sun Zheng-Zhi, Li Hekang, Zhang Junxiang, Song Chao, Wang Zhen, Guo Qiujiang, Machado Francisco, Kemp Jack, Iadecola Thomas, Yao Norman Y, Wang H, Deng Dong-Ling

机构信息

School of Physics, ZJU-Hangzhou Global Scientific and Technological Innovation Center, and Zhejiang Key Laboratory of Micro-nano Quantum Chips and Quantum Control, Zhejiang University, Hangzhou, China.

Center for Quantum Information, IIIS, Tsinghua University, Beijing, China.

出版信息

Nature. 2025 Aug 27. doi: 10.1038/s41586-025-09476-z.

Abstract

Symmetry-protected topological phases cannot be described by any local order parameter and are beyond the conventional symmetry-breaking model. They are characterized by topological boundary modes that remain stable under symmetry respecting perturbations. In clean, gapped systems without disorder, the stability of these edge modes is restricted to the zero-temperature manifold; at finite temperatures, interactions with mobile thermal excitations lead to their decay. Here we report the observation of a distinct type of topological edge mode, which is protected by emergent symmetries and persists across the entire spectrum, in an array of 100 programmable superconducting qubits. Through digital quantum simulation of a one-dimensional disorder-free stabilizer Hamiltonian, we observe robust long-lived topological edge modes over up to 30 cycles for a wide range of initial states. We show that the interaction between these edge modes and bulk excitations can be suppressed by dimerizing the stabilizer strength, leading to an emergent U(1) × U(1) symmetry in the prethermal regime of the system. Furthermore, we exploit these topological edge modes as logical qubits and prepare a logical Bell state, which exhibits persistent coherence, despite the system being disorder-free and at finite temperature. Our results establish a viable digital simulation approach to experimentally study topological matter at finite temperature and demonstrate a potential route to construct long-lived, robust boundary qubits in disorder-free systems.

摘要

对称保护的拓扑相无法用任何局域序参量来描述,且超出了传统的对称破缺模型。它们的特征是拓扑边界模式,在尊重对称性的微扰下保持稳定。在没有无序的干净能隙系统中,这些边缘模式的稳定性仅限于零温流形;在有限温度下,与移动热激发的相互作用会导致它们衰减。在此,我们报告在由100个可编程超导量子比特组成的阵列中观察到一种独特类型的拓扑边缘模式,它由涌现对称性保护且在整个能谱中持续存在。通过对一维无无序稳定器哈密顿量进行数字量子模拟,我们在广泛的初始态下观察到长达30个周期的稳健长寿拓扑边缘模式。我们表明,通过使稳定器强度二聚化,可以抑制这些边缘模式与体激发之间的相互作用,从而在系统的预热阶段产生一种涌现的U(1)×U(1)对称性。此外,我们将这些拓扑边缘模式用作逻辑量子比特并制备了一个逻辑贝尔态,尽管系统无无序且处于有限温度,但该态仍表现出持续的相干性。我们的结果建立了一种可行的数字模拟方法,用于在有限温度下通过实验研究拓扑物质,并展示了在无无序系统中构建长寿、稳健边界量子比特的潜在途径。

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