The concept of a disordered Fermi-liquid fixed point is introduced and used
to understand various properties of disordered metals within a unifying fr
amework. Corrections to scaling near this fixed point give what are commonl
y called weak-localization effects. Various instabilities of the disordered
Fermi-liquid phase are discussed. These include two distinct types of supe
rconducting-to-normal-metal quantum phase transitions. First, the quantum p
hase transition from a disordered metal to a conventional superconductor in
bulk materials is considered. Second, a quantum phase transition in two di
mensions from metallic-like behavior to a novel type of disorder induced, s
pin-triplet, even-parity, superconductivity is treated. The paper is conclu
ded with a discussion of the nature of the ground state of two-dimensional,
disordered electron systems.