2015/04/19 by Robert-Jan Slager, Louk Rademaker, Jan Zaanen +1 · 226 citations
Materials Science · Mathematics · Physics and Astronomy · #Bound state #Codimension #Combinatorics #Condensed matter physics #Eigenvalues and eigenvectors #Graphene research and applications #Impurity #Mathematical analysis #Mathematics #Physics #Quantum many-body systems #Quantum mechanics #Topological Materials and Phenomena #Topological insulator #Topology (electrical circuits) #cond-mat.mes-hall
paper · pdf · doi:10.1103/physrevb.92.085126
published in Physical Review B 92(8) (American Physical Society) · 11 pages, 8 figures
arxiv created 2015/04/19 · openalex publication_date 2015/08/17 · arxiv updated 2015/08/26 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
We show that the local in-gap Green's function of a band insulator G0(\ensuremathε,k_\ensuremath∥,r_\ensuremath⊥=0), with r_\ensuremath⊥ the position perpendicular to a codimension-1 or codimension-2 impurity, reveals the topological nature of the phase. For a topological insulator, the eigenvalues of this Green's function attain zeros in the gap, whereas for a trivial insulator the eigenvalues remain nonzero. This topological classification is related to the existence of in-gap bound states along codimension-1 and codimension-2 impurities. Whereas codimension-1 impurities can be viewed as soft edges, the result for codimension-2 impurities is nontrivial and allows for a direct experimental measurement of the topological nature of two-dimensional insulators.