{ "id": "1710.06584", "version": "v1", "published": "2017-10-18T04:48:31.000Z", "updated": "2017-10-18T04:48:31.000Z", "title": "Collective resonances near zero energy induced by a point defect in bilayer graphene", "authors": [ "Jhih-Shih You", "Jian-Ming Tang", "Wen-Min Huang" ], "comment": "6 figures", "categories": [ "cond-mat.mes-hall" ], "abstract": "Intrinsic defects give rise to scattering processes governing the transport properties of mesoscopic systems. We investigate analytically and numerically the local density of states in Bernal stacking bilayer graphene with a point defect. From this theoretical study, a picture emerges in which the pronounced zero-energy peak in the local density of states does not attribute to zero-energy impurity states associated to two different types of defects, but to a collective phenomenon of the low-energy resonant states induced by the defect. To corroborate this description, we numerically show that at small system size $N$, the zero-energy peak near the defect scales as $1/\\ln N$ for the quasi-localized zero-energy state and as $1/N$ for the delocalized state. As the system size approaches to the thermodynamic limit, the former zero-energy peak becomes a power-law singularity $1/|E|$ in low energies, while the latter is broadened into a Lorentzian shape. A striking point is that both types of zero-energy peaks decay as $1/r^2$ away from the defect, manifesting the quasi-localized character. Based on our results, we propose a general formula for the local density of states in low-energy and in real space. Our study sheds light on this fundamental problem of defects.", "revisions": [ { "version": "v1", "updated": "2017-10-18T04:48:31.000Z" } ], "analyses": { "keywords": [ "point defect", "zero energy", "collective resonances", "local density", "zero-energy impurity states" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }