Fig. 2.1Recommended energy gaps of wurtzite nitride semiconductor alloys (lines) and binaries (points) vs. lattice constant.
Band Structure Models 15The spin-degenerate conduction band is described by the anisotropic, parabolic form with wavefunctions comprised of the s-orbital (angular momentum l = 0) states:where k * , k * z are the wavevectors and m * , m * ⊥ are the effective masses along the in-plane and c-axis ([0001]) directions, respectively, a c1 and a c2 are the conduction-band deformation potentials, and ε ij are the strain tensor components. In the following, we cite the interband deformation potentials a 1 and a 2 , from which a c1 and a c2 may be obtained by subtracting the hydrostatic shift in the valence band, as determined by the D parameters in Eq. (2.5). The anisotropy is a distinguishing feature of the hexagonal crystal structure. Since the crystal-field and spin-orbit splittings in wurtzite nitride materials are rather small, the momentum matrix element E P and the F parameter are related to the effective mass and energy gap via: