We present experimental and theoretical results for the dispersion of
the 0.5 eV charge-carrier plasmon in A(3)C(60) (A = K, Rb) compounds.
The experimental dispersion in K3C60 is zero within the experimental a
ccuracy, and the theoretical dispersion is slightly negative. We show
that the small dispersion results from two large, opposing effects. Lo
cal-field effects tend to lead to a large negative dispersion, while i
nterband transitions largely cancel this effect. The interband effects
can be thought of in terms of the dielectric function due to classica
l, polarizable spheres describing the C-60 molecules. This dielectric
function reduces the plasmon energy, and the reduction of the dielectr
ic function with increasing q tends to lead to a large, positive dispe
rsion.