2018
DOI: 10.1103/physreva.97.042118
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Edge states at the interface of non-Hermitian systems

Abstract: Topological edge states appear at the interface of topologically distinct two Hermitian insulators. We study the extension of this idea to non-Hermitian systems. We consider PT symmetric and topologically distinct non-Hermitian insulators with real spectra and study topological edge states at the interface of them. We show that PT symmetry is spontaneously broken at the interface during the topological phase transition. Therefore topological edge states with complex energy eigenvalues appear at the interface. … Show more

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Cited by 104 publications
(60 citation statements)
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“…Our gain/loss-dressed photonic graphene always preserves P (as well as M x ) symmetry even when γ a = γ b and it is known that spatial symmetry is crucial for stabilizing higher-order corner modes [41,43]. In previous works, the topological properties of the PT -symmetric systems usually originate from the Hermitian parts of Hamiltoinians [57][58][59][60], but in our work non-Hermitian parts (patterned gain and loss) are crucial to induce the nontrival phase. Moreover, current PT -symmetric topological systems concern mainly 1D systems and the discussion of PT symmetry is limited to conventional topolog- ical phases [7,23,55,60,61], but our model presents a 2D higher-order counterpart.…”
Section: Discussionmentioning
confidence: 62%
“…Our gain/loss-dressed photonic graphene always preserves P (as well as M x ) symmetry even when γ a = γ b and it is known that spatial symmetry is crucial for stabilizing higher-order corner modes [41,43]. In previous works, the topological properties of the PT -symmetric systems usually originate from the Hermitian parts of Hamiltoinians [57][58][59][60], but in our work non-Hermitian parts (patterned gain and loss) are crucial to induce the nontrival phase. Moreover, current PT -symmetric topological systems concern mainly 1D systems and the discussion of PT symmetry is limited to conventional topolog- ical phases [7,23,55,60,61], but our model presents a 2D higher-order counterpart.…”
Section: Discussionmentioning
confidence: 62%
“…First, the topological edge and defect states have finite imaginary eigenvalues [ Fig. 9 (b)], namely net gain or loss in their dynamics [95,96]. Second, the conventional Zak phase [97] becomes continuous then fails to be a good topological number of this non-Hermitian system [98,99].…”
Section: The Complex Ssh Modelmentioning
confidence: 99%
“…The nontrivial bulk topology in Hermitian systems can * wuyajie@xatu.edu.cn † Junpeng.Hou@utdallas.edu be detected by defects, such as edges, π-flux, dislocations and vortices [48][49][50][51][52][53]. When it comes to non-Hermitian systems, stable edge states could also exist at the interface between topological and trivial phases [54][55][56][57][58][59][60][61][62]. These topological states, originated from bulk topologies, are immune to local symmetry-preserved perturbations.…”
Section: Non-hermitian Hamiltonian Captures Essentials Of Open Systemmentioning
confidence: 99%