Classification of Topological Insulators and Superconductors

Details Classification of Topological Insulators and Superconductors Classification of Topological Insulators and Superconductors

2009-05-13

arxiv.org/abs/0905.2029v1

AIP Conf. Proc. 1134, 10 (2009)

Physics

Condensed Matter

Mesoscale and Nanoscale Physics

12 pages, 5 figures; Proceedings of the L.D. Landau Memorial Conference, 2008

Scientific paper

An exhaustive classification scheme of topological insulators and superconductors is presented. The key property of topological insulators (superconductors) is the appearance of gapless degrees of freedom at the interface/boundary between a topologically trivial and a topologically non-trivial state. Our approach consists in reducing the problem of classifying topological insulators (superconductors) in d spatial dimensions to the problem of Anderson localization at a (d-1) dimensional boundary of the system. We find that in each spatial dimension there are precisely five distinct classes of topological insulators (superconductors). The different topological sectors within a given topological insulator (superconductor) can be labeled by an integer winding number or a Z_2 quantity. One of the five topological insulators is the 'quantum spin Hall' (or: Z_2 topological) insulator in d=2, and its generalization in d=3 dimensions. For each dimension d, the five topological insulators correspond to a certain subset of five of the ten generic symmetry classes of Hamiltonians introduced more than a decade ago by Altland and Zirnbauer in the context of disordered systems (which generalizes the three well known "Wigner-Dyson'' symmetry classes).

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