Near the zone centre, . The tight-binding model becomes
Only appears at quadratic order, so the band effective mass tensor is isotropic. Higher-order lattice terms need not be isotropic.
For the conduction band, , so the curvature is positive and
Here m and both beta parameters must be converted from eV to joules. The band edges at the zone centre are
so the model has a direct gap . The mass values describe curvature at these extrema; they are not constant masses throughout the full tight-binding bands.

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