Continuum Schroedinger Operators for Sharply Terminated Graphene-Like Structures

We study the single electron model of a semi-infinite graphene sheet interfaced with the vacuum and terminated along a zigzag edge. The model is a Schroedinger operator acting on L 2 ( R 2 ) : H edge λ = - Δ + λ 2 V ♯ , with a potential V ♯ given by a sum of translates an atomic potential well, V 0...

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Bibliographic Details
Published in:Communications in mathematical physics Vol. 380; no. 2; pp. 853 - 945
Main Authors: Fefferman, C. L., Weinstein, M. I.
Format: Journal Article
Language:English
Published: Berlin/Heidelberg Springer Berlin Heidelberg 01-12-2020
Springer Nature B.V
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Summary:We study the single electron model of a semi-infinite graphene sheet interfaced with the vacuum and terminated along a zigzag edge. The model is a Schroedinger operator acting on L 2 ( R 2 ) : H edge λ = - Δ + λ 2 V ♯ , with a potential V ♯ given by a sum of translates an atomic potential well, V 0 , of depth λ 2 , centered on a subset of the vertices of a discrete honeycomb structure with a zigzag edge. We give a complete analysis of the low-lying energy spectrum of H edge λ in the strong binding regime ( λ large). In particular, we prove scaled resolvent convergence of H edge λ acting on L 2 ( R 2 ) , to the (appropriately conjugated) resolvent of a limiting discrete tight-binding Hamiltonian acting in l 2 ( N 0 ; C 2 ) . We also prove the existence of edge states : solutions of the eigenvalue problem for H edge λ which are localized transverse to the edge and pseudo-periodic plane-wave like parallel to the edge. These edge states arise from a “flat-band” of eigenstates of the tight-binding model.
ISSN:0010-3616
1432-0916
DOI:10.1007/s00220-020-03868-0