We discuss several aspects of the dielectric response theory applicati
on to the density functional theory. This field has been an unceasing
source of confusion during several decades. The most frequent reasons
for this confusion are (a) uncritical transfer of the results, especia
lly regarding so-called local field corrections, obtained in many-body
perturbation theory onto density functional theory, and (b) mixing up
the statements true for the exact density functional theory with thos
e applicable to the local density approximation only. In these notes w
e try to draw an appropriate lines between those theories. We also dis
cuss a newly introduced (X. Gonze, Ph. Ghosez and R. W. Godby, Phys. R
et,. Lett., 74, 4035, 1995) ''polarization + density functional'' and
show that within a given (e.g., local density) approximation to the e
xchange-correlation energy the Gonze et al. approach is exactly equiva
lent to the conventional one.