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dc.contributor.authorAmanatidis, I.en
dc.contributor.authorEvangelou, S. N.en
dc.date.accessioned2015-11-24T18:38:16Z-
dc.date.available2015-11-24T18:38:16Z-
dc.identifier.issn1098-0121-
dc.identifier.urihttps://olympias.lib.uoi.gr/jspui/handle/123456789/17307-
dc.rightsDefault Licence-
dc.subjectcarbon nanotubesen
dc.subjectchaosen
dc.subjectgrapheneen
dc.subjecttight-binding calculationsen
dc.subjectwigner crystalen
dc.subjectcarbon nanotubesen
dc.subjectsystemsen
dc.subjectstatisticsen
dc.subjecttransporten
dc.subjectbilliardsen
dc.subjectphaseen
dc.subjectgasen
dc.titleQuantum chaos in weakly disordered grapheneen
heal.typejournalArticle-
heal.type.enJournal articleen
heal.type.elΆρθρο Περιοδικούel
heal.identifier.primaryDoi 10.1103/Physrevb.79.205420-
heal.identifier.secondary<Go to ISI>://000266501500101-
heal.identifier.secondaryhttp://prb.aps.org/abstract/PRB/v79/i20/e205420-
heal.languageen-
heal.accesscampus-
heal.recordProviderΠανεπιστήμιο Ιωαννίνων. Σχολή Επιστημών και Τεχνολογιών. Τμήμα Βιολογικών Εφαρμογών και Τεχνολογιώνel
heal.publicationDate2009-
heal.abstractWe have studied numerically the statistics for electronic states (level spacings and participation ratios) from disordered graphene dots of finite size, described by the aspect ratio W/L and various geometries, corresponding to finite chiral or achiral carbon nanotubes. Quantum chaotic Wigner energy level-spacing distribution is found for weak disorder, even infinitesimally small disorder for wide and short tight-binding samples (W/L > 1), while for strong disorder, Anderson localization with Poisson level-statistics always sets in. Although pure graphene near the Dirac point corresponds to integrable ballistic statistics diffusive chaotic behavior seems more common for realistic (weakly disordered) finite samples.en
heal.journalNamePhysical Review Ben
heal.journalTypepeer reviewed-
heal.fullTextAvailabilityTRUE-
Appears in Collections:Άρθρα σε επιστημονικά περιοδικά ( Ανοικτά)

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