Topological invariants of time-reversal-invariant band structures

TLDR

Topological invariants of time‑reversal‑invariant band structures are multiple copies of the Kane–Mele ${\mathbb{Z}}_{2}$ invariant, protecting the topological insulator phase and enabling a spin Hall effect carried by edge states. The authors derive these invariants by mapping the Brillouin zone to the space of Bloch Hamiltonians, linking the ${\mathbb{Z}}_{2}$ invariants to the integer invariants of the quantum Hall effect and to earlier invariants of time‑reversal‑invariant Fermi systems.

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'' phase and give rise to a spin Hall effect carried by edge states. Each pair of bands related by time reversal is described by one ${\mathbb{Z}}_{2}$ invariant, up to one less than half the dimension of the Bloch Hamiltonians. In three dimensions, there are four such invariants per band pair. 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 $\mathcal{T}$-invariant Fermi systems.