The in-plane profiles of the electron density and potential energy in
modulation delta-doped quantum wells with thin spacer layers are studi
ed as a function of the average sheet electron density. With depleting
the electron gas, the impurity induced density and potential fluctuat
ions become more and more pronounced, until the lateral electron densi
ty profile desintegrates into a set of spatially insulated clusters. T
his strongly disordered phase of an interacting 2D electron system is
analysed by applying and comparing four different theoretical approach
es. In the limit of high average electron density, excellent agreement
is found between the selfconsistent potential profiles calculated wit
h the random phase approximation (RPA), with a non-linearized version
of the semiclassical Thomas-Fermi approximation (NLTF) and with a full
-scale 2D Hartree calculation. For the strongly depleted case the RPA
is invalid, while a modified version of the classical theory of weakly
doped impurity bands (BEGS) becomes effective. The NLTF model is foun
d to be applicable for all electron densities, thus providing a comput
ationally efficient simulation method for both the linear and non-line
ar regime of impurity screening. (C) 1997 Academic Press Limited