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dc.contributor.author
Wakabayashi, Katsunori
dc.contributor.author
Takane, Yositake
dc.contributor.author
Yamamoto, Masayuki
dc.contributor.author
Sigrist, Manfred
dc.date.accessioned
2019-03-20T17:48:25Z
dc.date.available
2017-06-08T23:38:54Z
dc.date.available
2019-03-20T17:48:25Z
dc.date.issued
2009-09-30
dc.identifier.issn
1367-2630
dc.identifier.other
10.1088/1367-2630/11/9/095016
en_US
dc.identifier.uri
http://hdl.handle.net/20.500.11850/19616
dc.identifier.doi
10.3929/ethz-b-000019616
dc.description.abstract
We will present a brief overview of the electronic and transport properties of graphene nanoribbons focusing on the effect of edge shapes and impurity scattering. The low-energy electronic states of graphene have two non-equivalent massless Dirac spectra. The relative distance between these two Dirac points in the momentum space and edge states due to the existence of zigzag-type graphene edges is a deciding factor in the electronic and transport properties of graphene nanoribbons. In graphene nanoribbons with zigzag edges (zigzag nanoribbons), two valleys related to each Dirac spectrum are well separated in momentum space. The propagating modes in each valley contain a single chiral mode originating from a partially flat band at the band center. This feature gives rise to a perfectly conducting channel in the disordered system, if impurity scattering does not connect the two valleys, i.e. for long-range impurity (LRI) potentials. Ribbons with short-range impurity potentials, however, display ordinary localization behavior through inter-valley scattering. On the other hand, the low-energy spectrum of graphene nanoribbons with armchair edges (armchair nanoribbons) is described as the superposition of two non-equivalent Dirac points of graphene. In spite of the lack of two well separated valley structures, the single-channel transport subjected to LRIs is nearly perfectly conducting, where the backward scattering matrix elements in the lowest order vanish as a manifestation of internal phase structures of the wave function. For the multi-channel energy regime, however, conventional exponential decay of the averaged conductance occurs. Symmetry considerations lead to the classification of disordered zigzag ribbons into the unitary class for LRIs, and the orthogonal class for short-range impurities. Since inter-valley scattering is not completely absent, armchair nanoribbons can be classified into the orthogonal universality class irrespective of the range of impurities.
en_US
dc.format
application/pdf
en_US
dc.language.iso
en
en_US
dc.publisher
IOP Publishing
dc.rights.uri
http://creativecommons.org/licenses/by/3.0/
dc.title
Electronic transport properties of graphene nanoribbons
en_US
dc.type
Journal Article
dc.rights.license
Creative Commons Attribution 3.0 Unported
ethz.journal.title
New Journal of Physics
ethz.journal.volume
11
en_US
ethz.journal.abbreviated
New J. Phys.
ethz.pages.start
95016
en_US
ethz.size
21 p.
en_US
ethz.version.deposit
publishedVersion
en_US
ethz.identifier.wos
ethz.identifier.nebis
001997538
ethz.publication.place
London
ethz.publication.status
published
en_US
ethz.leitzahl
ETH Zürich::00002 - ETH Zürich::00012 - Lehre und Forschung::00007 - Departemente::02010 - Dep. Physik / Dep. of Physics::02511 - Institut für Theoretische Physik / Institute for Theoretical Physics::03571 - Sigrist, Manfred / Sigrist, Manfred
en_US
ethz.leitzahl.certified
ETH Zürich::00002 - ETH Zürich::00012 - Lehre und Forschung::00007 - Departemente::02010 - Dep. Physik / Dep. of Physics::02511 - Institut für Theoretische Physik / Institute for Theoretical Physics::03571 - Sigrist, Manfred / Sigrist, Manfred
ethz.date.deposited
2017-06-08T23:39:16Z
ethz.source
ECIT
ethz.identifier.importid
imp59364ca8ed78e90293
ethz.ecitpid
pub:32010
ethz.eth
yes
en_US
ethz.availability
Open access
en_US
ethz.rosetta.installDate
2017-07-12T10:50:55Z
ethz.rosetta.lastUpdated
2024-02-02T07:22:15Z
ethz.rosetta.versionExported
true
ethz.COinS
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