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dc.contributor.authorChiu, Y. H.en_US
dc.contributor.authorLai, Y. H.en_US
dc.contributor.authorHo, J. H.en_US
dc.contributor.authorChuu, D. S.en_US
dc.contributor.authorLin, M. F.en_US
dc.date.accessioned2019-04-03T06:40:46Z-
dc.date.available2019-04-03T06:40:46Z-
dc.date.issued2008-01-01en_US
dc.identifier.issn1098-0121en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.77.045407en_US
dc.identifier.urihttp://hdl.handle.net/11536/9796-
dc.description.abstractMagnetoelectronic properties of a two-dimensional (2D) monolayer graphene are investigated by the Peierls tight-binding model. They are dominated by the period, strength, and direction of a spatially modulated magnetic field. Such a field could induce the reduction in dimensionality, change of energy dispersions, anisotropy at low energy, composite behavior in state degeneracy, extra band-edge states, and asymmetry of energy bands. There are partial flatbands at the Fermi level and one-dimensional parabolic bands at others. These make density of states exhibit delta-function-like structure and asymmetric prominent peaks, respectively. Energies of the extra band-edge states strongly depend on the period, while those of the original band-edge states exhibit little dependence. Both of them grow as the strength increases. The modulated and uniform magnetic fields differ from each other in energy dispersion, state degeneracy, and dimensionality. Important differences between a monolayer graphene and a 2D electron gas also exist.en_US
dc.language.isoen_USen_US
dc.titleElectronic structure of a two-dimensional graphene monolayer in a spatially modulated magnetic field: Peierls tight-binding modelen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.77.045407en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume77en_US
dc.citation.issue4en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000252863100109en_US
dc.citation.woscount19en_US
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