Bifurcation of the edge-state width in a two-dimensional topological insulator
We examine the properties of edge states in a two-dimensional topological insulator. Based on the Kane-Mele model, we derive coupled equations for the energy and the effective width of the edge states at a given crystal momentum in a semi-infinite honeycomb lattice with a zigzag boundary. It is reve...
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Published in: | Physical review. B, Condensed matter and materials physics Vol. 88; no. 24 |
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Main Authors: | , |
Format: | Journal Article |
Language: | English |
Published: |
11-12-2013
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Subjects: | |
Online Access: | Get full text |
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Summary: | We examine the properties of edge states in a two-dimensional topological insulator. Based on the Kane-Mele model, we derive coupled equations for the energy and the effective width of the edge states at a given crystal momentum in a semi-infinite honeycomb lattice with a zigzag boundary. It is revealed that, in a one-dimensional Brillouin zone, the edge states merge into continuous bands of the bulk states through a bifurcation of the edge-state width. We discuss the implications of the results for experiments in monolayer or thin-film topological insulators. |
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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 1098-0121 1550-235X |
DOI: | 10.1103/PhysRevB.88.245115 |