TY - JOUR
T1 - Bulk topological invariants in noninteracting point group symmetric insulators
AU - Fang, Chen
AU - Gilbert, Matthew J.
AU - Bernevig, B. Andrei
PY - 2012/9/10
Y1 - 2012/9/10
N2 - We survey various quantized bulk physical observables in two- and three-dimensional topological band insulators invariant under translational symmetry and crystallographic point group symmetries (PGS). In two-dimensional insulators, we show that (i) the Chern number of a C n-invariant insulator can be determined, up to a multiple of n, by evaluating the eigenvalues of symmetry operators at high-symmetry points in the Brillouin zone; (ii) the Chern number of a C n-invariant insulator is also determined, up to a multiple of n, by the C n eigenvalue of the Slater determinant of a noninteracting many-body system; and (iii) the Chern number vanishes in insulators with dihedral point groups D n, and the quantized electric polarization is a topological invariant for these insulators. In three-dimensional insulators, we show that (i) only insulators with point groups C n, C nh, and S n PGS can have nonzero 3D quantum Hall coefficient and (ii) only insulators with improper rotation symmetries can have quantized magnetoelectric polarization P 3 in the term P 3E•B, the axion term in the electrodynamics of the insulator (medium).
AB - We survey various quantized bulk physical observables in two- and three-dimensional topological band insulators invariant under translational symmetry and crystallographic point group symmetries (PGS). In two-dimensional insulators, we show that (i) the Chern number of a C n-invariant insulator can be determined, up to a multiple of n, by evaluating the eigenvalues of symmetry operators at high-symmetry points in the Brillouin zone; (ii) the Chern number of a C n-invariant insulator is also determined, up to a multiple of n, by the C n eigenvalue of the Slater determinant of a noninteracting many-body system; and (iii) the Chern number vanishes in insulators with dihedral point groups D n, and the quantized electric polarization is a topological invariant for these insulators. In three-dimensional insulators, we show that (i) only insulators with point groups C n, C nh, and S n PGS can have nonzero 3D quantum Hall coefficient and (ii) only insulators with improper rotation symmetries can have quantized magnetoelectric polarization P 3 in the term P 3E•B, the axion term in the electrodynamics of the insulator (medium).
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U2 - 10.1103/PhysRevB.86.115112
DO - 10.1103/PhysRevB.86.115112
M3 - Article
AN - SCOPUS:84866385973
SN - 1098-0121
VL - 86
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 11
M1 - 115112
ER -