We present room-temperature Raman measurements of pressure-polymerized
C-60 and compare them with the spectra of RbC60 in the orthorhombic p
hase. Although both materials were prepared according to two completel
y different routes the spectra show a surprising similarity with respe
ct to mode positions and line splitting. We concluded from this that b
oth materials, the uncharged pressure-polymerized C-60 and the rubidiu
m-doped orthorhombic compound, have the same overall structure and the
AC(60) compounds can be considered as the doped species of the C-60,
polymerized using moderate low pressure and high temperatures. From a
detailed comparison between both spectra mode shifting and line broade
ning as a consequence of the charge transfer was determined and electr
on-phonon coupling constants were estimated for the high-frequency H-g
(7) and H-g(8) modes. The low values for the coupling constants compar
ed to the ones in the K3C60 can explain the lack of superconductivity
in the AC(60) compounds.