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Effective Mass

Current status: READY

Near a parabolic extremum,

E(k)≈E0+ℏ22(k−k0)T(m∗)−1(k−k0),E(\mathbf k) \approx E_0 + \frac{\hbar^2}{2} (\mathbf k-\mathbf k_0)^T (m^*)^{-1} (\mathbf k-\mathbf k_0),

so

(m∗−1)ij=1ℏ2∂2E∂ki∂kj.(m^{*-1})_{ij} = \frac{1}{\hbar^2} \frac{\partial^2E}{\partial k_i\partial k_j}.

The user chooses electron/hole and CBM/VBM behavior. Analyze shows the source data and fitted parabola.

Insufficient sampling returns an explicit diagnostic rather than a zero or NaN mass.