We determine the behavior of the phonon excitations in liquid He-4, co
vering both the normal and superfluid phase, for a range of temperatur
es T (1<T<4.2K), wave numbers q (0.1<q<2.2 Angstrom(-1)) and pressures
p (0<p<25 bars), by means of a numerical fitting procedure based on t
he effective eigenmode description of the density correlation function
. We find that the q,p and T dependence of all inelastic neutron scatt
ering data cona be well described by using only one adjustable paramet
er, the damping rate of the momentum fluctuations. We establish that t
here is a close similarity between classical liquids, normal fluid He-
4 and superfluid He-4. We observe, for all q-values, a marked change i
n the damping rate of the momentum fluctuations as one passes through
the superfluid-transition temperature T-lambda. For the roton excitati
ons, this results in a heavily damped (overdamped at p=20 bars) mode i
n the normal phase, in contrast to the propagating mode observed in th
e superfluid phase. The change in damping rate is found to occur predo
minantly in a small temperature region just below T-lambda, for all q-
values. We don not find any evidence for the sudden appearance of the
predicted ''renormalized single-particle'' excitations as one enters t
he superfluid phase. We argue that the full dispersion curve of the ph
onon-maxon-roton excitations can be understood for all temperature and
pressures in terms of the damping rate of the momentum fluctuations,
whereas the rapid changes in this damping rate near T-lambda can be vi
ewed as a direct consequence of the Bose symmetry requirements on the
He-4-wavefunction.