Abstract

The Fourier expansion technique for coupled bands is applied to the electronic dispersion relations of solids which crystallize into structures with ${D}_{3}^{4}$ (or ${D}_{3}^{6}$) symmetries. In this treatment, the spin-orbit interaction is included. A magnetic Hamiltonian is developed which is valid throughout the Brillouin zone. When $H$ is parallel to the $c$ axis, the Landau-level energy eigenvalues can be obtained as a one-dimensional Fourier expansion in ${k}_{z}$. Selection rules for optical transitions in a magnetic field are presented.

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