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Solid C36: Crystal structures, formation, and effects of doping

Jeffrey C. Grossman, Steven G. Louie, and Marvin L. Cohen
Phys. Rev. B 60, R6941(R) – Published 1 September 1999
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Abstract

We employ plane-wave pseudopotential density functional calculations to show that the lowest energy D6hC36 crystal is a highly bonded network of hexagonal planes of C36 units with AB stacking. This crystal is significantly more dense and lower in energy than previously proposed structures. We demonstrate that Na is the largest alkali atom that can be intercalated into the crystal structure without causing severe structural distortion. Further, we predict the reaction pathway to form a neutral C36 dimer to be barrierless, while negatively charged C36 molecules are less likely to bond due to a substantial barrier of formation.

  • Received 26 January 1999

DOI:https://doi.org/10.1103/PhysRevB.60.R6941

©1999 American Physical Society

Authors & Affiliations

Jeffrey C. Grossman, Steven G. Louie, and Marvin L. Cohen

  • Department of Physics, University of California at Berkeley and Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720

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Vol. 60, Iss. 10 — 1 September 1999

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