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对称破缺相中拓扑保护的长边缘相干时间

Topologically Protected Long Edge Coherence Times in Symmetry-Broken Phases.

作者信息

Parker Daniel E, Vasseur Romain, Scaffidi Thomas

机构信息

Department of Physics, University of California, Berkeley, California 94720, USA.

Department of Physics, University of Massachusetts, Amherst, Massachusetts 01003, USA.

出版信息

Phys Rev Lett. 2019 Jun 21;122(24):240605. doi: 10.1103/PhysRevLett.122.240605.

Abstract

We argue that symmetry-broken phases proximate in phase space to symmetry-protected topological phases can exhibit dynamical signatures of topological physics. This dynamical, symmetry-protected "topological" regime is characterized by anomalously long edge coherence times due to the topological decoration of quasiparticle excitations, even if the underlying zero-temperature ground state is in a nontopological, symmetry-broken state. The dramatic enhancement of coherence can even persist at infinite temperature due to prethermalization. We find exponentially long edge coherence times that are stable to symmetry-preserving perturbations and not the result of integrability.

摘要

我们认为,在相空间中与对称保护拓扑相接近的对称破缺相可以展现出拓扑物理的动力学特征。这种动力学的、对称保护的“拓扑” regime 的特征是,由于准粒子激发的拓扑修饰,边缘相干时间异常长,即使潜在的零温基态处于非拓扑的对称破缺态。由于预热化,相干性的显著增强甚至可以在无限温度下持续存在。我们发现指数级长的边缘相干时间对于保持对称性的微扰是稳定的,且不是可积性的结果。

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