A theory of self-localized states of free carriers near polarization f
luctuations (fluctuons) in disordered ferroelectrics is developed. Cal
culations are carried out for the model disordered ferroelectric K1-xL
ixTaO3 (x much less than 0.05). The basic characteristics of the fluct
uon the energy and radius of the fluctuon state - are calculated as fu
nctions of the impurity dipole concentration and temperature. The theo
ry predicts the appearence of stable fluctuon states in both the mixed
ferroelectric-dipole-glass phase (a dipole glass is the electric anal
og of a spin glass) and the dipole-glass state of disordered ferroelec
trics. The possible role of fluctuons in kinetic phenomena such as con
ductivity in these substances is discussed. (C) 1997 American Institut
e of Physics.