Topological band insulators are bulk insulating states of matter, which in the presence of time-reversal symmetry feature metallic states at their edge or surface. This state of quantum matter has been experimentally realized in the HgTe/CdTe quantum wells and various (mostly) Bismuth-based compounds.
I will first introduce the concept of topological band insulators and then discuss the role of crystal symmetries in the physics of these states of quantum matter. I will derive the classification of topological band-insulators protected not only by time-reversal, but also by space group symmetries [1]. As a result, there are three broad classes of topological states: (a) Gamma-states robust against general time-reversal invariant perturbations; (b) Translationally-active states protected from elastic scattering, but susceptible to topological crystalline disorder; (c) Valley (crystalline) topological insulators sensitive to both elastic and crystalline disorder. I will also discuss probing of the topological states in the bulk by magnetic pi-fluxes and lattice dislocations both in two [2] and three dimensions [3].
Finally, some experimental implications of our classification scheme will be considered.