TY - JOUR
T1 - Electronic structure of KxC60 studied by high-energy resolved photoemission spectroscopy
AU - Morikawa, Takashi
AU - Takahashi, Takashi
N1 - Funding Information:
C6o powders. They also thank H. Katayama-Yoshida at Tohoku University and A. Fujimori at Tokyo University for useful discussions. This work was supported by grants from the Ministry of Education, Culture and Science of Japan and from the Foundation for Promotion of Material Science and Technology of Japan.
PY - 1993/9
Y1 - 1993/9
N2 - High-energy resolved low-temperature ultraviolet photoemission spectroscopy has been performed on KxC60 (x=0 - 6) to study the detailed electronic structure near the Fermi level (EF). The experimental result shows that a very narrow peak and a broad distribution of density of states coexist near EF in K3C60. While the narrow peak at EF is correlated to a part of the occupied LUMO (lowest unoccupied molecular orbital) band of C60 as predicted from the band structure calculation, the observed broad distribution of density of states near EF has no counterpart in the calculation. It was also found that K4C60 is a semiconductor with an energy gap of more than 0.2 eV. This shows a sharp contrast with the prediction from the band calculation that K4C60 should be a metal with four electrons in the three-fold degenerate LUMO band. Some possible origins to give these discrepancies have been discussed.
AB - High-energy resolved low-temperature ultraviolet photoemission spectroscopy has been performed on KxC60 (x=0 - 6) to study the detailed electronic structure near the Fermi level (EF). The experimental result shows that a very narrow peak and a broad distribution of density of states coexist near EF in K3C60. While the narrow peak at EF is correlated to a part of the occupied LUMO (lowest unoccupied molecular orbital) band of C60 as predicted from the band structure calculation, the observed broad distribution of density of states near EF has no counterpart in the calculation. It was also found that K4C60 is a semiconductor with an energy gap of more than 0.2 eV. This shows a sharp contrast with the prediction from the band calculation that K4C60 should be a metal with four electrons in the three-fold degenerate LUMO band. Some possible origins to give these discrepancies have been discussed.
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U2 - 10.1016/0038-1098(93)90552-X
DO - 10.1016/0038-1098(93)90552-X
M3 - Article
AN - SCOPUS:0027658912
SN - 0038-1098
VL - 87
SP - 1017
EP - 1021
JO - Solid State Communications
JF - Solid State Communications
IS - 11
ER -