Home | Research | Publications | Members | Contact
Graphene nanoribbons (GNRs) are thin strips of graphene that can have different nanoscale widths and edge symmetries (for more introductory material on GNRs look here). One of the most exciting developments in the study of GNRs has been the discovery of topological phases in armchair GNRs. Topological behavior in GNRs was first predicted by Steven Louie’s group.1 One year later the predictions were confirmed by the Crommie group and collaborators.2 Topology in GNRs is classified by a Z2 index such that when Z2 = 0 GNRs are topologically trivial and when Z2 = 1 GNRs are are topologically nontrivial. What makes this important is that if a trivial GNR (Z2 = 0) is fused to a “topologically nontrivial” GNR (Z2 = 1) then a topologically-protected interface state holding a single unpaired electron forms at the boundary between the two GNR segments (Fig. 1). This is analogous to the 2D metallic surface states that form at the surface of 3D topological insulators and the 1D metallic edge-states that form at the edges of 2D quantum spin Hall insulators.3,4 Since GNRs are 1D topological insulators the protected states at their interfaces can be thought of as 0D metals (i.e., localized states occupied by a single, unpaired electron).