Bulk-Edge Correspondence for Two-Dimensional Topological Insulators

Topological insulators can be characterized alternatively in terms of bulk or edge properties. We prove the equivalence between the two descriptions for two-dimensional solids in the single-particle picture. We give a new formulation of the $${\mathbb{Z}_{2}}$$Z2-invariant, which allows for a bulk index not relying on a (two-dimensional) Brillouin zone. When available though, that index is shown to agree with known formulations. The method also applies to integer quantum Hall systems. We discuss a further variant of the correspondence, based on scattering theory.

[1]  R. Roy On the $Z_2$ classification of Quantum Spin Hall Models , 2006, cond-mat/0604211.

[2]  Walter Kohn Analytic Properties of Bloch Waves and Wannier Functions , 1966 .

[3]  J. Fröhlich,et al.  Gauge invariance and current algebra in nonrelativistic many body theory , 1993 .

[4]  Quantum Theory of Large Systems of Non-Relativistic Matter , 1995, cond-mat/9508062.

[5]  G. M. Graf,et al.  Equivalence of Topological and Scattering Approaches to Quantum Pumping , 2009, 0902.4638.

[6]  Shou-Cheng Zhang,et al.  The Chern-Simons-Landau-Ginzburg theory of the fractional quantum Hall effect , 1992 .

[7]  L. Molenkamp,et al.  Quantum Spin Hall Insulator State in HgTe Quantum Wells , 2007, Science.

[8]  C. Kane,et al.  Topological Insulators , 2019, Electromagnetic Anisotropy and Bianisotropy.

[9]  Y. Hatsugai,et al.  Chern number and edge states in the integer quantum Hall effect. , 1993, Physical review letters.

[10]  K. Kusakabe,et al.  Peculiar Localized State at Zigzag Graphite Edge , 1996 .

[11]  Haldane,et al.  Model for a quantum Hall effect without Landau levels: Condensed-matter realization of the "parity anomaly" , 1988, Physical review letters.

[12]  C. Kane,et al.  Time Reversal Polarization and a Z 2 Adiabatic Spin Pump , 2006, cond-mat/0606336.

[13]  J. Fröhlich,et al.  Universality in quantum Hall systems , 1991 .

[14]  L. Balents,et al.  Topological invariants of time-reversal-invariant band structures , 2007 .

[15]  A. Zee,et al.  Large scale physics of the quantum Hall fluid , 1991 .

[16]  M. Nakahara Geometry, Topology and Physics , 2018 .

[17]  Mark S. C. Reed,et al.  Method of Modern Mathematical Physics , 1972 .

[18]  Shou-Cheng Zhang,et al.  Quantum Spin Hall Effect and Topological Phase Transition in HgTe Quantum Wells , 2006, Science.

[19]  Shinsei Ryu,et al.  Topological origin of zero-energy edge states in particle-hole symmetric systems. , 2001, Physical review letters.

[20]  D. Thouless,et al.  Quantization of particle transport , 1983 .

[21]  Xiao-Liang Qi,et al.  Topological quantization of the spin Hall effect in two-dimensional paramagnetic semiconductors , 2005, cond-mat/0505308.

[22]  V. Gurarie,et al.  Bulk-boundary correspondence of topological insulators from their respective Green’s functions , 2011, 1104.1602.

[23]  Tosio Kato Perturbation theory for linear operators , 1966 .

[24]  Barry Simon,et al.  Methods of modern mathematical physics. III. Scattering theory , 1979 .

[25]  E. Prodan Robustness of the spin-Chern number , 2009, 0904.1894.

[26]  W. F. Pfeffer More on Involutions of a Circle , 1974 .

[27]  Yize Jin,et al.  Topological insulators , 2014, Topology in Condensed Matter.

[28]  L. Sheng,et al.  Quantum spin-Hall effect and topologically invariant Chern numbers. , 2006, Physical review letters.

[29]  C. Villegas-Blas,et al.  Topological Invariants of Edge States for Periodic Two-Dimensional Models , 2012, 1202.0537.

[30]  Wen,et al.  Chiral Luttinger liquid and the edge excitations in the fractional quantum Hall states. , 1990, Physical review. B, Condensed matter.

[31]  E. J. Mele,et al.  Z2 topological order and the quantum spin Hall effect. , 2005, Physical review letters.

[32]  Fujita,et al.  Edge state in graphene ribbons: Nanometer size effect and edge shape dependence. , 1996, Physical review. B, Condensed matter.

[33]  D. Hsieh,et al.  A topological Dirac insulator in a quantum spin Hall phase , 2008, Nature.