Pj. Benning et al., ELECTRON-DIFFRACTION AND PHOTOELECTRON-SPECTROSCOPY STUDIES OF FULLERENE AND ALKALI-METAL FULLERIDE FILMS, Physical review. B, Condensed matter, 48(12), 1993, pp. 9086-9096
Photoelectron spectroscopy and low-energy electron diffraction (LEED)
have been used to examine the electronic structure and crystallinity o
f thin films of A(X)C60 where A = Na, K, Rb, and Cs and 0 less-than-or
-equal-to x less-than-or-equal-to 6. For undoped C60 films, temperatur
e-dependent LEED studies show changes that correspond to the lattice t
ransformation from the simple-cubic to the face-centered-cubic structu
re. For doped C60 films, the LEED results show a decrease in the quali
ty of the LEED pattern upon the nucleation of the body-centered A-C60
phases. Spectroscopic studies of these fullerides indicate that the ef
fects of electron correlation are always important. In particular, the
A1C60 phases of Rb and Cs are characterized by an occupied-valence-ba
nd feature approximately 0.5 eV wide centered approximately 0.25 eV be
low E(F) that is derived from the lowest unoccupied molecular orbitals
(LUMO) of C60. The much greater width relative to band calculations i
s attributed to electron correlation. For these phases, there is also
emission at the Fermi level, despite the fact that transport studies i
ndicate insulating character. This implies that the electronic states
at E(F) are localized. The A3C60 phase of K and Rb exhibit a metallic
Fermi-level cutoff. Spectroscopic features 0.3 and 0.7 eV below EF are
also observed that are not reproduced in one-electron band-structure
calculations. The A4C60 phases of K, Rb, and Cs all exhibit insulating
character with a split LUMO band. All of the A6C60 phases are insulat
ors with a filled LUMO band. For Na-C60, the valence-band spectra show
no emission at E(F) for any Na concentration. Finally, photoemission
results showed partial occupation of the (LUMO+1)-derived levels, corr
esponding to C60(8-) for isolated C60 molecules deposited onto multila
yers of Na, K, and Rb at 40 K.