We employ a quantitative microscopic theory of nonuniform quantum liqu
ids to explore the excitations in thin films of He-4 adsorbed onto a s
ubstrate. These liquid films studied undergo a series of structural ph
ase transitions coinciding with the completion of individual atomic la
yers. A generalized Feynman ansatz is used for the wave function of th
e excited states; multiphonon effects are included by generalizing the
Feynman theory to allow for time-dependent pair correlations. We stud
y the dispersion relation, excitation mechanisms, transition densities
, and particle currents, as a function of the surface coverage, includ
ing coverages near the phase transitions. Because of the film's layere
d growth, the sound velocity exhibits a series of minima and maxima. A
pronounced long-wavelength softening of the lowest-energy mode is obs
erved near the transitions. In the monolayer, the nature of the excita
tions undergoes a noticeable change at the coverage where the velocity
of sound starts to decrease. This is a crossover from ''essentially t
wo-dimensional'' to ''essentially three-dimensional'' behavior. At lon
g wavelengths, below and above the crossover coverage, the lowest-ener
gy excitation is a longitudinal phonon (propagating within the monolay
er) and a surface excitation, respectively. At shorter wavelengths, a
layer-phonon propagating within the liquid layers, level crosses with
a surface excitation to become the lowest-energy mode. For double- and
higher-layer films the excitations are complicated by multiple (layer
phonon with layer phonon and layer phonon with surface excitation) le
vel crossings. At higher coverages, a mode is identifiable that will e
volve into the bulk phonon-maxon roton. Our results agree qualitativel
y with the available spectra obtained by neutron-scattering experiment
s.