Abstract

The topological invariants of a time-reversal-invariant band structure in two dimensions are multiple copies of the $\mathbb{Z}_2$ invariant found by Kane and Mele. Such invariants protect the topological insulator and give rise to a spin Hall effect carried by edge states. Each pair of bands related by time reversal is described by a single $\mathbb{Z}_2$ invariant, up to one less than half the dimension of the Bloch Hamiltonians. In three dimensions, there are four such invariants per band. The $\mathbb{Z}_2$ invariants of a crystal determine the transitions between ordinary and topological insulators as its bands are occupied by electrons. We derive these invariants using maps from the Brillouin zone to the space of Bloch Hamiltonians and clarify the connections between $\mathbb{Z}_2$ invariants, the integer invariants that underlie the integer quantum Hall effect, and previous invariants of ${\cal T}$-invariant Fermi systems.

Keywords

Brillouin zoneInvariant (physics)Topological insulatorPhysicsWinding numberQuantum Hall effectTopology (electrical circuits)Quantum mechanicsElectronMathematicsCombinatoricsMathematical analysis

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2006 Physical Review B 559 citations

Publication Info

Year
2007
Type
article
Volume
75
Issue
12
Citations
2307
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Closed

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Cite This

Joel E. Moore, Leon Balents (2007). Topological invariants of time-reversal-invariant band structures. Physical Review B , 75 (12) . https://doi.org/10.1103/physrevb.75.121306

Identifiers

DOI
10.1103/physrevb.75.121306
arXiv
cond-mat/0607314

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Data completeness: 84%