{ "id": "1303.3488", "version": "v3", "published": "2013-03-14T15:57:08.000Z", "updated": "2014-02-20T07:51:42.000Z", "title": "Edge states versus diffusion in disordered graphene flakes", "authors": [ "Ioannis Kleftogiannis", "Ilias Amanatidis" ], "comment": "9 pages, 14 figures, updated the journal reference", "journal": "Eur. Phys. J. B (2014) 87: 16", "doi": "10.1140/epjb/e2013-40756-0", "categories": [ "cond-mat.mes-hall" ], "abstract": "We study the localization properties of the wavefunctions in graphene flakes with short range disorder, via the numerical calculation of the Inverse Participation Ratio($IPR$) and it scaling which provides the fractal dimension $D_{2}$. We show that the edge states which exist at the Dirac point of ballistic graphene (no disorder) with zig-zag edges survive in the presence of weak disorder with wavefunctions localized at the boundaries of the flakes. We argue, that there is a strong interplay between the underlying destructive interference mechanism of the honeycomb lattice of graphene leading to edge states and the diffusive interference mechanism introduced by the short-range disorder. This interplay results in a highly abnormal behavior, wavefunctions are becoming progressively less localized as the disorder is increased, indicated by the decrease of the average $\\langle IPR\\rangle$ and the increase of $D_{2}$. We verify, that this abnormal behavior is absent for graphene flakes with armchair edges which do not provide edge states.", "revisions": [ { "version": "v3", "updated": "2014-02-20T07:51:42.000Z" } ], "analyses": { "keywords": [ "edge states", "disordered graphene flakes", "short range disorder", "inverse participation ratio", "wavefunctions" ], "tags": [ "journal article" ], "publication": { "journal": "European Physical Journal B", "year": 2014, "month": "Jan", "volume": 87, "number": 1, "pages": 16 }, "note": { "typesetting": "TeX", "pages": 9, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2014EPJB...87...16K" } } }