{ "id": "1105.5138", "version": "v2", "published": "2011-05-25T20:00:04.000Z", "updated": "2011-09-16T21:15:11.000Z", "title": "Weyl Semimetal in a Topological Insulator Multilayer", "authors": [ "A. A. Burkov", "Leon Balents" ], "comment": "4 pages, 3 figures, published version", "journal": "Phys. Rev. Lett. 107, 127205 (2011)", "doi": "10.1103/PhysRevLett.107.127205", "categories": [ "cond-mat.mes-hall" ], "abstract": "We propose a simple realization of the three-dimensional (3D) Weyl semimetal phase, utilizing a multilayer structure, composed of identical thin films of a magnetically-doped 3D topological insulator (TI), separated by ordinary-insulator spacer layers. We show that the phase diagram of this system contains a Weyl semimetal phase of the simplest possible kind, with only two Dirac nodes of opposite chirality, separated in momentum space, in its bandstructure. This particular type of Weyl semimetal has a finite anomalous Hall conductivity, chiral edge states, and occurs as an intermediate phase between an ordinary insulator and a 3D quantum anomalous Hall insulator with a quantized Hall conductivity, equal to $e^2/h$ per TI layer. We find that the Weyl semimetal has a nonzero DC conductivity at zero temperature and is thus an unusual metallic phase, characterized by a finite anomalous Hall conductivity and topologically-protected edge states.", "revisions": [ { "version": "v2", "updated": "2011-09-16T21:15:11.000Z" } ], "analyses": { "subjects": [ "75.47.-m", "03.65.Vf", "71.90.+q", "73.43.-f" ], "keywords": [ "topological insulator multilayer", "finite anomalous hall conductivity", "weyl semimetal phase", "3d quantum anomalous hall insulator", "edge states" ], "tags": [ "journal article", "famous paper" ], "publication": { "publisher": "APS", "journal": "Physical Review Letters", "year": 2011, "month": "Sep", "volume": 107, "number": 12, "pages": 127205 }, "note": { "typesetting": "TeX", "pages": 4, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2011PhRvL.107l7205B" } } }