Non-Hermitian Dirac cones with valley-dependent lifetimes

被引:0
|
作者
Xinrong Xie [1 ]
Fei Ma [2 ]
W. B. Rui [3 ]
Zhaozhen Dong [4 ]
Yulin Du [1 ]
Wentao Xie [2 ]
Y. X. Zhao [3 ]
Hongsheng Chen [4 ]
Fei Gao [5 ]
Haoran Xue [6 ]
机构
[1] Zhejiang University,State Key Laboratory of Extreme Photonics and Instrumentation, International Joint Innovation Center, The Electromagnetics Academy at Zhejiang University
[2] Zhejiang University,ZJU
[3] Zhejiang University,Hangzhou Global Scientific and Technological Innovation Center
[4] Zhejiang University,Key Lab. of Advanced Micro/Nano Electronic Devices & Smart Systems of Zhejiang, Jinhua Institute of Zhejiang University
[5] The University of Hong Kong,Shaoxing Institute of Zhejiang University
[6] The University of Hong Kong,Department of Physics and HKU
[7] The Chinese University of Hong Kong,UCAS Joint Institute for Theoretical and Computational Physics at Hong Kong
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D O I
10.1038/s41467-025-56882-y
中图分类号
学科分类号
摘要
Relativistic quasiparticles emerging from band degeneracies in crystals play crucial roles in the transport and topological properties of materials and metamaterials. Quasiparticles are commonly described by Hermitian Hamiltonians, with non-Hermiticity usually considered detrimental. In this work, we show that such an assumption of Hermiticity can be lifted to bring quasiparticles into non-Hermitian regime. We propose a concrete lattice model containing two Dirac cones with valley-dependent lifetimes. The lifetime contrast enables an ultra-strong valley selection rule: only one valley can survive in the long-time limit regardless of the excitation, lattice shape and other details. This property leads to an effective parity anomaly with a single Dirac cone and offers a simple way to generate vortex states. Additionally, extending non-Hermitian features to boundaries generates valley kink states with valley-locked lifetimes, making them effectively unidirectional and more resistant against inter-valley scattering. All these phenomena are experimentally demonstrated in a non-Hermitian electric circuit lattice.
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