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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Published in: | Communications in mathematical physics Vol. 380; no. 2; pp. 853 - 945 |
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Main Authors: | , |
Format: | Journal Article |
Language: | English |
Published: |
Berlin/Heidelberg
Springer Berlin Heidelberg
01-12-2020
Springer Nature B.V |
Subjects: | |
Online Access: | Get full text |
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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. |
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ISSN: | 0010-3616 1432-0916 |
DOI: | 10.1007/s00220-020-03868-0 |