Abstract

The effect of a magnetic field on a two-dimensional Chern band insulator is discussed. It is shown that, unlike the trivial insulator, an anomalous Hall insulator with Chern number CC becomes a metal when a magnetic field is applied at constant particle density, for any C>0C>0. For a time reversal invariant topological insulator with a spin Chern resolved number, C↑=−C↓=CC_\uparrow= - C_\downarrow=C, the magnetic field induces a spin polarized spin Hall insulator. We consider also the effect of a superlattice potential and extend previous results for the quantization of the Hall conductance of filled Hofstadter bands to this problem.

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