Polar optical modes play an important role in electron-phonon processe
s such as scattering rates, polaron effects and resonant Raman scatter
ing in quantum wells and superlattices, Because of this there has been
in recent years a strong interest in the development of a long-wave t
heory for optical modes in semiconductor nanostructures. This theory w
ould be the equivalent of the effective mass theory for electrons. Bes
ides microscopic calculations it should provide a satisfactory theoret
ical model to study the long-wave limit, to which most experimental ev
idence is circumscribed. Important elements in this type of theory are
the inclusion of the bulk spatial dispersion of the optical modes tog
ether with the fact that, at an interface between two media, mechanica
l and electromagnetic boundary conditions must be satisfied, In some c
ases, like InAs/GaSb and related superlattices, the details of the int
erface structure are also important. We discuss here the different app
roaches employed to study the long-wave limit in these systems, includ
ing other approaches in which the envelope function model is derived d
irectly from microscopic lattice dynamics.