The standard theory of the Frenkel exciton (a small radius exciton) is
applied to a fullerene 2D solid. It is the dipole collective electron
excitation of a single cluster which forms the delocalized plasmon-Fr
enkel-exciton (PFE) in a crystal. The PFE retarded interaction is take
n into account. We present transverse PFE-polariton dispersion curves
along with the Coulomb problem solution for longitudinal excitation in
the 2D plane. (C) 1998 Elsevier Science B.V.