In the
quantum mechanical framework, this scattering is most noticeable in
confined systems, in which the energies for charge carriers are determined by the locations of interfaces. An example of such a system is a
quantum well, which may be constructed from a sandwich of different layers of semiconductor. Variations in the thickness of these layers therefore causes the energy of particles to be dependent on their in-plane location in the layer. Classification of the roughness at a given position, \Delta_z(\mathbf{r}), is complex, but as in the classical models, it has been modeled as a
Gaussian distribution by some researchers This assumption may be formulated in terms of the
ensemble average for some given characteristic height, \Delta, and correlation length, \Lambda, such that :\langle\Delta_z(\mathbf{r})\Delta_z(\mathbf{r'})\rangle = \Delta^2\exp\left(-\frac{|\mathbf{r}-\mathbf{r'}|^2}{\Lambda^2}\right) == Types of Scattering ==