Orbital magnetization in crystalline solids: Multi-band insulators, Chern insulators, and metals
Davide Ceresoli, T. Thonhauser, David Vanderbilt, R. Resta

TL;DR
This paper develops a multi-band formulation for calculating orbital magnetization in crystalline solids, including insulators, Chern insulators, and metals, with practical expressions and empirical validation.
Contribution
It introduces a gauge-invariant, bulk property expression for orbital magnetization applicable to multi-band systems and extends the formalism heuristically to Chern insulators and metals.
Findings
The reciprocal-space expression matches finite sample calculations.
The formalism is validated for 2D model systems.
Heuristic extension to Chern insulators and metals shows strong agreement.
Abstract
We derive a multi-band formulation of the orbital magnetization in a normal periodic insulator (i.e., one in which the Chern invariant, or in 2d the Chern number, vanishes). Following the approach used recently to develop the single-band formalism [T. Thonhauser, D. Ceresoli, D. Vanderbilt, and R. Resta, Phys. Rev. Lett. {\bf 95}, 137205 (2005)], we work in the Wannier representation and find that the magnetization is comprised of two contributions, an obvious one associated with the internal circulation of bulk-like Wannier functions in the interior and an unexpected one arising from net currents carried by Wannier functions near the surface. Unlike the single-band case, where each of these contributions is separately gauge-invariant, in the multi-band formulation only the \emph{sum} of both terms is gauge-invariant. Our final expression for the orbital magnetization can be rewritten…
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