The interface between two materials described by spectrally gapped Hamiltonians is expected to host an in-gap interface mode, whenever a certain topological invariant changes across the interface. We provide a precise statement of this bulk-interface correspondence and its rigorous justification. The correspondence applies to continuum and lattice models of interfaces between one-dimensional materials with inversion symmetry, with dislocation models being of particular interest. For continuum models, the analysis of the parity of the 'edge' Bloch modes is the key component in our argument, while for the lattice models, the relative Zak phase and index theory are.
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Stanford Univ, Dept Appl Phys, Stanford, CA 94305 USAStanford Univ, Dept Appl Phys, Stanford, CA 94305 USA
Hong, Seung Sae
Zhang, Yi
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Stanford Univ, Dept Phys, Stanford, CA 94305 USAStanford Univ, Dept Appl Phys, Stanford, CA 94305 USA
Zhang, Yi
Cha, Judy J.
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Stanford Univ, Dept Mat Sci & Engn, Stanford, CA 94305 USAStanford Univ, Dept Appl Phys, Stanford, CA 94305 USA
Cha, Judy J.
Qi, Xiao-Liang
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Stanford Univ, Dept Phys, Stanford, CA 94305 USAStanford Univ, Dept Appl Phys, Stanford, CA 94305 USA
Qi, Xiao-Liang
Cui, Yi
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Stanford Univ, Dept Mat Sci & Engn, Stanford, CA 94305 USA
SLAC Natl Accelerator Lab, Stanford Inst Mat & Energy Sci, Menlo Pk, CA 94025 USAStanford Univ, Dept Appl Phys, Stanford, CA 94305 USA