A brief review is given of the current understanding of the electronic stru
cture, transport properties and the nature of the electronic states in diso
rdered systems. A simple explanation for the observed exponential behaviour
in the density of states (Urbach tails) based on short-range Gaussian fluc
tuations is presented. The theory of Anderson localization in a disordered
system is reviewed. Basic concepts, and the physics underlying the effects
of weak localization, are discussed. The scaling as well as the self-consis
tent theory of localization are briefly reviewed. It is then argued that th
e problem of localization in a random potential within the so-called ladder
approximation is formally equivalent to the problem of finding a bound sta
te in a shallow potential well. Therefore all states are exponentially loca
lized in d = 1 and d = 2. The fractal nature of the states is also discusse
d. Scaling properties in highly anisotropic systems are also discussed. A b
rief presentation of the recently observed metal-to-insulator transition in
d = 2 is given and, finally, a few remarks about interaction effects in di
sordered systems are presented.