TY - JOUR
T1 - Scanning tunneling microscopy/spectroscopy studies of two isomers of Ce@C82 on Si(111)-(7 X 7) surfaces
AU - Fujiki, Satoshi
AU - Kubozono, Yoshihiro
AU - Rikiishi, Yoshie
AU - Urisu, Tsuneo
N1 - Funding Information:
This work was supported by CREST of Japan Science and Technology Agency, by a Grant-in-Aid (No. 15350089) from the Ministry of Education, Science, Sports and Culture of Japan, Okayama University COE Project, and by the Mitsubishi Foundation. S.F. thanks the Japan Society of Promotion of Science for financial support.
PY - 2004/12
Y1 - 2004/12
N2 - Scanning tunneling microscopy images for two isomers of Ce@C82 were observed on Si(111)-(7X7) at 295 K. The Ce@C82 molecules in the first layer were bound to the Si surfaces, and the motions were frozen even at 295 K. The multilayer of the Ce@C82 isomer I (Ce@C82-I) produced a close-packed structure in the surface layer by annealing the Si substrate at 473 K. The distance between the nearest-neighboring molecules was 1.15(4) nm whose value was consistent with that, 1.12 nm, estimated from x-ray diffraction of the Ce@C82-I crystals. This implies that the close-packed structure is dominated by van der Waals forces, as in crystals of Ce@C82-I. The internal structure of Ce@C82-I was observed in the first layer due to a freeze of molecular motion caused by strong interactions between the molecule and the Si adatoms in the surface. Scanning tunneling spectroscopy revealed that the energy gaps for Ce@C82-I and -II in the first layer opened to gap energies, Eg of 0.7 and 1.0 eV, respectively. This fact suggests that these molecules are semiconductors with smaller value of Eg than those for C60 and C70.
AB - Scanning tunneling microscopy images for two isomers of Ce@C82 were observed on Si(111)-(7X7) at 295 K. The Ce@C82 molecules in the first layer were bound to the Si surfaces, and the motions were frozen even at 295 K. The multilayer of the Ce@C82 isomer I (Ce@C82-I) produced a close-packed structure in the surface layer by annealing the Si substrate at 473 K. The distance between the nearest-neighboring molecules was 1.15(4) nm whose value was consistent with that, 1.12 nm, estimated from x-ray diffraction of the Ce@C82-I crystals. This implies that the close-packed structure is dominated by van der Waals forces, as in crystals of Ce@C82-I. The internal structure of Ce@C82-I was observed in the first layer due to a freeze of molecular motion caused by strong interactions between the molecule and the Si adatoms in the surface. Scanning tunneling spectroscopy revealed that the energy gaps for Ce@C82-I and -II in the first layer opened to gap energies, Eg of 0.7 and 1.0 eV, respectively. This fact suggests that these molecules are semiconductors with smaller value of Eg than those for C60 and C70.
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U2 - 10.1103/PhysRevB.70.235421
DO - 10.1103/PhysRevB.70.235421
M3 - Article
AN - SCOPUS:13944269435
SN - 1098-0121
VL - 70
SP - 1
EP - 7
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 23
M1 - 235421
ER -