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Topology and edge states survive quantum criticality between topological insulators
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abstract
It is often thought that emergent phenomena in topological phases of matter are destroyed when tuning to a critical point. In particular, topologically protected edge states supposedly delocalize when the bulk correlation length diverges. We show that this is not true in general. Edge states of topological insulators or superconductors remain exponentially localized---despite a vanishing band gap---if the transition increases the topological index. This applies to all classes where the topological classification is larger than $Z_2$, notably including Chern insulators. Moreover, these edge states are stable to disorder, unlike in topological semi-metals. This new phenomenon is explained by generalizing band (or mass) inversion---a unifying perspective on topological insulators---to kinetic inversion. In the spirit of the bulk-boundary correspondence, we also identify topological invariants at criticality, which take half-integer values and separate topologically-distinct universality classes by a multi-critical point. This work enlarges the scope of topological protection and stability by showing that bulk energy gaps can be unnecessary. Experimental probes and stability to interactions are discussed.
Forward citations
Cited by 2 Pith papers
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Gapless higher-order topology and corner states in Floquet systems
Corner modes at zero and π quasienergy survive topological transitions in a driven Creutz ladder plus SSH chain, with a generalized winding number that counts them even when the bulk is gapless.
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Topologically nontrivial multicritical points
Under a parameter condition (Γ0 ≤ Γ2/3), multicritical points in a third-neighbor SSH/Kitaev chain retain one localized zero-energy edge mode per end, giving a topological invariant w_mc = 1.
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