{ "id": "1301.1257", "version": "v1", "published": "2013-01-07T16:45:14.000Z", "updated": "2013-01-07T16:45:14.000Z", "title": "Quantum Hall Effect in Hydrogenated Graphene", "authors": [ "J. Guillemette", "S. S. Sabri", "B. Wu", "K. Bennaceur", "P. E. Gaskell", "M. Savard", "P. L. Lévesque", "F. Mahvash", "A. Guermoune", "M. Siaj", "R. Martel", "T. Szkopek", "G. Gervais" ], "comment": "4 pages, 4 figures + supplemental info", "journal": "Phys. Rev. Lett. 110, 176801 (2013)", "doi": "10.1103/PhysRevLett.110.176801", "categories": [ "cond-mat.mes-hall", "cond-mat.mtrl-sci", "cond-mat.str-el" ], "abstract": "The quantum Hall effect is observed in a two-dimensional electron gas formed in millimeter-scale hydrogenated graphene, with a mobility less than 10 $\\mathrm{cm^{2}/V\\cdot s}$ and corresponding Ioffe-Regel disorder parameter $(k_{F}\\lambda)^{-1}\\gg1$. In zero magnetic field and low temperatures, the hydrogenated graphene is insulating with a two-point resistance of order of $250 h/e^2$. Application of a strong magnetic field generates a negative colossal magnetoresistance, with the two-point resistance saturating within 0.5% of $h/2e^{2}$ at 45T. Our observations are consistent with the opening of an impurity-induced gap in the density of states of graphene. The interplay between electron localization by defect scattering and magnetic confinement in two-dimensional atomic crystals is discussed.", "revisions": [ { "version": "v1", "updated": "2013-01-07T16:45:14.000Z" } ], "analyses": { "subjects": [ "73.22.Pr", "73.20.At", "73.43.-f" ], "keywords": [ "quantum hall effect", "hydrogenated graphene", "strong magnetic field generates", "two-point resistance", "two-dimensional atomic crystals" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review Letters", "year": 2013, "month": "Apr", "volume": 110, "number": 17, "pages": 176801 }, "note": { "typesetting": "TeX", "pages": 4, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2013PhRvL.110q6801G" } } }