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The Structures of C60 Films on Different Single-Crystal Substrates

โœ Scribed by Wei Zhao; Wei-Lie Zhou; Li-Quan Chen; Yu-Zhen Huang; Ze-Bo Zhang; K.K. Fung; Zhong-Xian Zhao


Publisher
Elsevier Science
Year
1994
Tongue
English
Weight
660 KB
Volume
112
Category
Article
ISSN
0022-4596

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โœฆ Synopsis


The structures of (\mathrm{C}{60}) films sublimated on the ( 001 ) surface of five substrates, (\mathrm{LaAlO}{3}, \mathrm{SrTiO}{3}, \mathrm{ZrO}{2}, \mathrm{NaCl}), and (\mathrm{KBr}), and an amorphous quartz substrate were studied by XRD and TEM. All films are of fcc structure with corresponding lattice parameters (a=14.10,14.10,14.17,14.16,14.25), and (14.12 \AA), respectively. Various factors influencing the lattice constant are discussed. TEM was used to investigate two (\mathrm{C}{60}) films prepared on (\mathrm{NaCl}(001)) substrates with different temperatures and showed that in the initial growth stage of the film, it mainly contains microparticles with fcc structure; a few particles of hep structure with (a=1.02) and (b=1.64 \mathrm{~nm}) coexist in the film. With higher substrate temperature and growth of the film, the number of hcp phase particles was reduced. These results indicate that planar defects and hcp phase particles may contribute to the low-angle sawtooth feature on the (111) peak in the XRD patterns. The existence of an abnormal defect in fcc stacking with a sequence (A B C A A A A B C \ldots) in the ใ€ˆ111) direction, which is normally impossible in fcc spherical packings, suggests that the adhesion forces between (\mathrm{C}{60}) molecules are strong to some extent. 1994 Academic Press. Inc.


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Structures of C60 thin films fabricated
โœ Toshinari Ichihashi; Katsumi Tanigaki; Thomas W. Ebbesen; Sadanori Kuroshima; Su ๐Ÿ“‚ Article ๐Ÿ“… 1992 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 489 KB

C6o thin film crystals have been fabricated on the (001) surface of alkali halide substrates, KC1, KBr, and NaC1, and their structures have been studied. TEM observations show that the hexagonal close packing (hcp) with lattice parameters a = 10.0 A and c = 16.3 A and the face-centered cubic ( fcc )