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dc.contributor.authorKao, H. C.en_US
dc.contributor.authorLewkowicz, M.en_US
dc.contributor.authorKorniyenko, Y.en_US
dc.contributor.authorRosenstein, B.en_US
dc.date.accessioned2014-12-08T15:38:09Z-
dc.date.available2014-12-08T15:38:09Z-
dc.date.issued2011-01-01en_US
dc.identifier.issn0010-4655en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.cpc.2010.07.029en_US
dc.identifier.urihttp://hdl.handle.net/11536/26168-
dc.description.abstractThe process of the coherent creation of particle-hole excitations by an electric field in graphene is quantitatively described beyond linear response We calculate the evolution of the current density and the number of pairs in the ballistic regime using the tight binding model While for small electric fields the I-V curve is linear characterized by the universal minimal resistivity sigma = pi/2(e(2)/h) for larger fields after a certain time interval the linear regime crosses over to a quadratic one and finally at larger times Bloch oscillations set in (C) 2010 Elsevier BV All rights reserveden_US
dc.language.isoen_USen_US
dc.subjectGrapheneen_US
dc.subjectBallistic transporten_US
dc.titleDynamical approach to ballistic transport in grapheneen_US
dc.typeArticleen_US
dc.identifier.doi10.1016/j.cpc.2010.07.029en_US
dc.identifier.journalCOMPUTER PHYSICS COMMUNICATIONSen_US
dc.citation.volume182en_US
dc.citation.issue1en_US
dc.citation.spage112en_US
dc.citation.epage114en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000285119900036-
dc.citation.woscount3-
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