Two-dimensional topological phases are characterized by Thouless-Kohmoto-Nightingale--den Nijs integers, which classify Bloch energy bands or groups of Bloch bands. However, quantization does not survive thermal averaging or dephasing to mixed states. We show that using Uhlmann's parallel transport for density matrices [Rep. Math. Phys. 24, 229 (1986)], an integer classification of topological phases can be defined for a finite generalized temperature T or dephasing Lindbladian. This scheme reduces to the familiar Thouless-Kohmoto-Nightingale--den Nijs classification for T<Tc,1, becomes trivial for T>Tc,2, and exhibits a ``gapless'' intermediate regime where topological indices are not well defined. We demonstrate these ideas in detail, applying them to Haldane's honeycomb lattice model and the Bernevig-Hughes-Zhang model, and we comment on their generalization to multiband Chern insulators.
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Huang et al. (2014) studied this question.
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