Zak phase and the existence of edge states in graphene
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We develop a method to predict the existence of edge states in graphene ribbons for a large class of boundaries. This approach is based on the bulk-edge correspondence between the quantized value of the Zak phase $\mathcal{Z}({k}_{\ensuremath{\parallel}})$, which is a Berry phase across an appropriately chosen one-dimensional Brillouin zone, and the existence of a localized state of momentum ${k}_{\ensuremath{\parallel}}$ at the boundary of the ribbon. This bulk-edge correspondence is rigorously demonstrated for a one-dimensional toy model as well as for graphene ribbons with zigzag edges. The range of ${k}_{\ensuremath{\parallel}}$ for which edge states exist in a graphene ribbon is then calculated for arbitrary orientations of the edges. Finally, we show that the introduction of an anisotropy leads to a topological transition in terms of the Zak phase, which modifies the localization properties at the edges. Our approach gives a new geometrical understanding of edge states, and it confirms and generalizes the results of several previous works.
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Introducing anisotropy along the vertical and diagonal directions into graphene leads to broken six-fold symmetry and level crossing with deformation of the bandstructure.
“In contrast, introducing the anisotropy along the vertical direction and diagonal direction into the graphene leads to the broken six-fold symmetry and level crossing with the deformation of the bandstructure [29-31].”
From Observing movement of Dirac cones from single-photon dynamics (2021) · cites this paper as [30]
Section IV.A says that changing the hopping ratios moves the Dirac points, and Section IV.B says that increasing anisotropy can merge them and then open a band gap. The copy does not specifically describe anisotropy along vertical and diagonal directions or state that it breaks six-fold symmetry; the reported band touching and merging also do not establish a general level-crossing claim. Page numbers are unavailable in our copy. (LLM, conf=0.83)
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“In contrast, introducing the anisotropy along the vertical direction and diagonal direction into the graphene leads to the broken six-fold symmetry and level crossing with the deformation of the bandstructure [29–31].”
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- Authors
- Delplace, P., Ullmo, D., & Montambaux, G.
- Affiliations
- University of Geneva (CH)
- Université Paris-Sud (FR)
- Venue
- Physical Review B
- Publisher
- American Physical Society (APS)
- Published
- 2011-11-23
- Volume
- 84
- Issue
- 19
- Pages
- 195452
- ISSN
- 1098-0121 (ISSN-L)
- 1550-235X
- OpenAlex
- W1979276597
- Cited by
- 541
- References
- 3
- Citations by year
- 2026: 25 · 2025: 37 · 2024: 58 · 2023: 50 · 2022: 38 · 2021: 62 · 2020: 41 · 2019: 47 · 2018: 55 · 2017: 44 · 2016: 37 · 2015: 17 · 2014: 11 · 2013: 16 · 2012: 2
- FWCI
- 5.04
- Type
- journal article
- Language
- en
- Open access
- green
- hal.science
- Locations
- Physical Review B (publishedVersion)
- HAL (submittedVersion)
- arXiv (Cornell University) (submittedVersion)
- arXiv (Cornell University)
- Funders
- Agence Nationale de la Recherche (ANR-09-NANO-0016, ANR-09-NANO-016-01)
- Topics
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Topological Materials and Phenomena
- Physical Sciences › Materials Science › Materials Chemistry › Graphene research and applications
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum and electron transport phenomena
- Keywords
- Zak phase, edge states, graphene nanoribbons, bulk-boundary correspondence, Berry phase, zigzag edge, anisotropy, topological phase transition, edge localization
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