{ "id": "1109.6137", "version": "v2", "published": "2011-09-28T09:18:35.000Z", "updated": "2012-02-27T14:35:59.000Z", "title": "Time-reversal invariant realization of the Weyl semimetal phase", "authors": [ "Gábor B. Halász", "Leon Balents" ], "comment": "9 pages, 5 figures, published version with infinitesimal changes", "journal": "Phys. Rev. B 85, 035103 (2012)", "doi": "10.1103/PhysRevB.85.035103", "categories": [ "cond-mat.mes-hall" ], "abstract": "We propose a realization of the Weyl semimetal phase that is invariant under time reversal and occurs due to broken inversion symmetry. We consider both a simple superlattice model and a more realistic tight-binding model describing an experimentally reasonable HgTe/CdTe multilayer structure. The two models have the same underlying symmetry, therefore their low-energy features are equivalent. We find a Weyl semimetal phase between the normal insulator and the topological insulator phases that exists for a finite range of the system parameters and exhibits a finite number of Weyl points with robust band touching at the Fermi level. This phase is experimentally characterized by a strong conductivity anisotropy and topological surface states. The principal conductivities change in a complementary fashion as the system parameters are varied, and the surface states only exist in a region of momentum space that is determined by the positions of the Weyl points.", "revisions": [ { "version": "v2", "updated": "2012-02-27T14:35:59.000Z" } ], "analyses": { "subjects": [ "03.65.Vf", "73.21.Cd", "73.20.-r" ], "keywords": [ "weyl semimetal phase", "time-reversal invariant realization", "surface states", "weyl points", "system parameters" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review B", "year": 2012, "month": "Jan", "volume": 85, "number": 3, "pages": "035103" }, "note": { "typesetting": "TeX", "pages": 9, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2012PhRvB..85c5103H" } } }