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Solid state electronic structure of Ba3C60 — A model approach

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Böhm,  Michael C.
Fritz Haber Institute, Max Planck Society;
Institut für Physikalische Chemie, Physikalische Chemie III, Technische Hochschule Darmstadt;

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Schedel-Niedrig,  Thomas
Inorganic Chemistry, Fritz Haber Institute, Max Planck Society;

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Werner,  Harald
Inorganic Chemistry, Fritz Haber Institute, Max Planck Society;

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Schlögl,  Robert
Inorganic Chemistry, Fritz Haber Institute, Max Planck Society;

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Citation

Böhm, M. C., Schedel-Niedrig, T., Werner, H., Schlögl, R., & Schulte, J. (1996). Solid state electronic structure of Ba3C60 — A model approach. Solid State Communications, 98(5), 463-468. doi:10.1016/0038-1098(95)00752-0.


Cite as: https://hdl.handle.net/21.11116/0000-000A-0FD3-8
Abstract
The band structure of Ba3C60 has been modeled by a crystal orbital (CO) formalism of the intermediate neglect of differential overlap (INDO) type. The fulleride crystallizes in a novel A15 structure with three crystallographically non-equivalent alkaline-earth atoms in the unit cell. The symmetry of the space group is Pm3n. To define the underlying unit cell for the CO calculations, two formula units are necessary. A finite band gap is predicted for the fulleride system, a theoretical result which is in line with the resistivity maximum observed in alkaline-earth fullerides with three donor atoms per C60 soccerball. The alkaline-earth atoms are essentially monovalent and hybridize strongly with the π-type functions of the C60 network. The Ba-to-C60 charge transfer (CT) is responsible for an almost perfect alignment between formal CC “double” and “single” bonds. The nature of the Ba-C interaction is discussed on the basis of covalent and ionic two-center energies.