{ "id": "0901.2686", "version": "v2", "published": "2009-01-18T08:46:17.000Z", "updated": "2009-01-20T07:33:13.000Z", "title": "Periodic table for topological insulators and superconductors", "authors": [ "Alexei Kitaev" ], "comment": "To appear in the Proceedings of the L.D.Landau Memorial Conference \"Advances in Theoretical Physics\", June 22-26, 2008, Chernogolovka, Moscow region, Russia (v2: arXiv hyperlinks fixed)", "categories": [ "cond-mat.mes-hall", "cond-mat.supr-con", "hep-th", "math-ph", "math.MP" ], "abstract": "Gapped phases of noninteracting fermions, with and without charge conservation and time-reversal symmetry, are classified using Bott periodicity. The symmetry and spatial dimension determines a general universality class, which corresponds to one of the 2 types of complex and 8 types of real Clifford algebras. The phases within a given class are further characterized by a topological invariant, an element of some Abelian group that can be 0, Z, or Z_2. The interface between two infinite phases with different topological numbers must carry some gapless mode. Topological properties of finite systems are described in terms of K-homology. This classification is robust with respect to disorder, provided electron states near the Fermi energy are absent or localized. In some cases (e.g., integer quantum Hall systems) the K-theoretic classification is stable to interactions, but a counterexample is also given.", "revisions": [ { "version": "v2", "updated": "2009-01-20T07:33:13.000Z" } ], "analyses": { "subjects": [ "03.65.Pm", "73.43.Nq", "02.10.Yn", "71.10.Pm", "74.70.-b", "72.15.Rn" ], "keywords": [ "topological insulators", "periodic table", "superconductors", "integer quantum hall systems", "general universality class" ], "tags": [ "conference paper", "journal article", "famous paper" ], "publication": { "doi": "10.1063/1.3149495" }, "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "inspire": 811262, "adsabs": "2009AIPC.1134...22K" } } }