Mathematical analysis of the Anderson localization has been facilitate
d by the use of suitable fractional moments of the Green function. Rel
ated methods permit now a readily accessible derivation of a number of
physical manifestations of localization, in regimes of strong disorde
r, extreme energies, or weak disorder away from the unperturbed spectr
um. This work establishes on this basis exponential decay for the modu
lus of the two-point function, at all temperatures as well as in the g
round state, for a Fermi gas within the one-particle approximation. Di
fferent implications, in particular for the integral quantum Hall effe
ct, are reviewed.