2008/05/31 by Hideaki Obuse, Akira Furusaki, Shinsei Ryu +1 · 47 citations
Mathematics · Physics and Astronomy · #Condensed matter physics #Critical exponent #Electrical resistivity and conductivity #Electron #Fractal #Geometry #Mathematics #Metal–insulator transition #Multifractal system #Phase transition #Physics #Quantum Hall effect #Quantum and electron transport phenomena #Quantum many-body systems #Quantum mechanics #Quantum spin Hall effect #Scaling #Topological Materials and Phenomena #Topological insulator #cond-mat.dis-nn #cond-mat.mes-hall
paper · pdf · doi:10.1103/physrevb.78.115301
published in Physical Review B 78(11) (American Physical Society) · 12 pages, 13 figures, selected for an Editors' Suggestion in PRB
openalex publication_date 2008/09/02 · arxiv created 2008/09/03 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
Static disorder in a noninteracting gas of electrons confined to two dimensions can drive a continuous quantum (Anderson) transition between a metallic and an insulating state when time-reversal symmetry is preserved but spin-rotation symmetry is broken. The critical exponent \ensuremathν that characterizes the diverging localization length and the bulk multifractal scaling exponents that characterize the amplitudes of the critical wave functions at the metal-insulator transition do not depend on the topological nature of the insulating state, i.e., whether it is topologically trivial (ordinary insulator) or nontrivial (a ℤ2 insulator supporting a quantum spin Hall effect). This is not true of the boundary multifractal scaling exponents, which we show (numerically) to depend on whether the insulating state is topologically trivial or not.