Bulk topological invariants in noninteracting point group symmetric insulators
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 sub(n)-invariant insulator...
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Veröffentlicht in: | Physical review. B, Condensed matter and materials physics Condensed matter and materials physics, 2012-09, Vol.86 (11), Article 115112 |
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Sprache: | eng |
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Zusammenfassung: | 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 sub(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 sub(n)-invariant insulator is also determined, up to a multiple of n, by the C sub(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 sub(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 sub(n), C sub(nh), and S sub(n) PGS can have nonzero 3D quantum Hall coefficient and (ii) only insulators with improper rotation symmetries can have quantized magnetoelectric polarization P sub(3) in the term P sub(3)E times B, the axion term in the electrodynamics of the insulator (medium). |
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ISSN: | 1098-0121 1550-235X |
DOI: | 10.1103/PhysRevB.86.115112 |