Abstract

We consider a semi-periodic two-dimensional Schr\"odinger operator which is cut at an angle. When the cut is commensurate with the periodic lattice, the spectrum of the operator has the band-gap Bloch structure. We prove that in the incommensurable case, there are no gaps: the gaps of the bulk operator are filled with edge spectrum.

Highlights

  • We study the spectral properties of a half-periodic material, when this one is cut along any line

  • One can apply partial Bloch theory in this direction, and obtain that its spectrum has again the band-gap structure. This spectrum usually differs from σbulk due to the presence of edge modes. This is described by the edge spectrum σedge[θ] := σ H D [θ] \ σbulk

  • We focus on a dislocated version of the bulk operator

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Summary

Introduction

We study the spectral properties of a half-periodic material, when this one is cut along any line. Its spectrum σbulk is independent of θ, and has a band-gap structure by Bloch theory. One can apply partial Bloch theory in this direction, and obtain that its spectrum has again the band-gap structure. This spectrum usually differs from σbulk due to the presence of edge modes. In the incommensurable case, all gaps of σbulk are filled with edge spectrum This extends the previous work by Hempel and Kohlmann [7, 9], where the authors proved this filling gap phenomenon in the limit θ → 0. In the special case of Dirichlet boundary conditions, the Σ appearing in Theorem 1 is independent of θ, and equals the infimum of the bulk spectrum Σ = inf σbulk.

Bulk Hamiltonian
Dislocated Hamiltonians
Dirichlet Hamiltonian
Spectrum for rational angles
The spectrum for irrational angles
Domain wall Hamiltonians

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