Electronic states of graphene nanoribbons and analytical solutions

Graphene is a one-atom-thick layer of graphite, where low-energy electronic states are described by the massless Dirac fermion. The orientation of the graphene edge determines the energy spectrum of π-electrons. For example, zigzag edges possess localized edge states with energies close to the Fermi...

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Main Author: Katsunori Wakabayashi, Ken-ichi Sasaki, Takeshi Nakanishi and Toshiaki Enoki
Format: Article
Language:English
Published: Taylor & Francis Group 2010-01-01
Series:Science and Technology of Advanced Materials
Online Access:http://iopscience.iop.org/1468-6996/11/5/054504
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spelling doaj-526dec8f02d147feb3e6f8e8c5c3f7402020-11-25T00:22:44ZengTaylor & Francis GroupScience and Technology of Advanced Materials1468-69961878-55142010-01-01115054504Electronic states of graphene nanoribbons and analytical solutions Katsunori Wakabayashi, Ken-ichi Sasaki, Takeshi Nakanishi and Toshiaki EnokiGraphene is a one-atom-thick layer of graphite, where low-energy electronic states are described by the massless Dirac fermion. The orientation of the graphene edge determines the energy spectrum of π-electrons. For example, zigzag edges possess localized edge states with energies close to the Fermi level. In this review, we investigate nanoscale effects on the physical properties of graphene nanoribbons and clarify the role of edge boundaries. We also provide analytical solutions for electronic dispersion and the corresponding wavefunction in graphene nanoribbons with their detailed derivation using wave mechanics based on the tight-binding model. The energy band structures of armchair nanoribbons can be obtained by making the transverse wavenumber discrete, in accordance with the edge boundary condition, as in the case of carbon nanotubes. However, zigzag nanoribbons are not analogous to carbon nanotubes, because in zigzag nanoribbons the transverse wavenumber depends not only on the ribbon width but also on the longitudinal wavenumber. The quantization rule of electronic conductance as well as the magnetic instability of edge states due to the electron–electron interaction are briefly discussed.http://iopscience.iop.org/1468-6996/11/5/054504
collection DOAJ
language English
format Article
sources DOAJ
author Katsunori Wakabayashi, Ken-ichi Sasaki, Takeshi Nakanishi and Toshiaki Enoki
spellingShingle Katsunori Wakabayashi, Ken-ichi Sasaki, Takeshi Nakanishi and Toshiaki Enoki
Electronic states of graphene nanoribbons and analytical solutions
Science and Technology of Advanced Materials
author_facet Katsunori Wakabayashi, Ken-ichi Sasaki, Takeshi Nakanishi and Toshiaki Enoki
author_sort Katsunori Wakabayashi, Ken-ichi Sasaki, Takeshi Nakanishi and Toshiaki Enoki
title Electronic states of graphene nanoribbons and analytical solutions
title_short Electronic states of graphene nanoribbons and analytical solutions
title_full Electronic states of graphene nanoribbons and analytical solutions
title_fullStr Electronic states of graphene nanoribbons and analytical solutions
title_full_unstemmed Electronic states of graphene nanoribbons and analytical solutions
title_sort electronic states of graphene nanoribbons and analytical solutions
publisher Taylor & Francis Group
series Science and Technology of Advanced Materials
issn 1468-6996
1878-5514
publishDate 2010-01-01
description Graphene is a one-atom-thick layer of graphite, where low-energy electronic states are described by the massless Dirac fermion. The orientation of the graphene edge determines the energy spectrum of π-electrons. For example, zigzag edges possess localized edge states with energies close to the Fermi level. In this review, we investigate nanoscale effects on the physical properties of graphene nanoribbons and clarify the role of edge boundaries. We also provide analytical solutions for electronic dispersion and the corresponding wavefunction in graphene nanoribbons with their detailed derivation using wave mechanics based on the tight-binding model. The energy band structures of armchair nanoribbons can be obtained by making the transverse wavenumber discrete, in accordance with the edge boundary condition, as in the case of carbon nanotubes. However, zigzag nanoribbons are not analogous to carbon nanotubes, because in zigzag nanoribbons the transverse wavenumber depends not only on the ribbon width but also on the longitudinal wavenumber. The quantization rule of electronic conductance as well as the magnetic instability of edge states due to the electron–electron interaction are briefly discussed.
url http://iopscience.iop.org/1468-6996/11/5/054504
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