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The Low‐Temperature Three‐Dimensional Structures of the Second‐Stage Caesium Graphitide
Author(s) -
Duclaux L.,
Rannou I.,
Lelaurain M.,
Béguin F.
Publication year - 1998
Publication title -
journal of applied crystallography
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.429
H-Index - 162
ISSN - 1600-5767
DOI - 10.1107/s0021889897009151
Subject(s) - stacking , crystallography , lattice (music) , crystal structure , caesium , atmospheric temperature range , condensed matter physics , chemistry , graphite , materials science , physics , thermodynamics , organic chemistry , acoustics
The three‐dimensional (3D) structure of the second‐stage CSC 24 graphitide was investigated by recording hk . l monochromatic rotating‐crystal diffractograms. At low temperature, the two‐dimensional (2D) structure is formed of an incommensurate (2.53 x 2.53 R 14.5°) and a commensurate (2 x 2 R 0°) lattice. Below 140 K, whereas the Cs incommensurate layers become 3D ordered, the 2 x 2 R 0° commensurate layers are randomly distributed in the structure. The commensurate structure, with composition CsC 16 (stage two), probably equilibrates the lack of Cs induced by the incommensurate structure (composition CSC 26 ), in order to reach the global composition CSC 24 of the compound. Depending on the temperature, two kinds of stackings appear. Below 140 K, the incommensurate Cs layers are arranged in a 2D‐modulated initial stacking, transformed at a lower temperature into a rhombohedral stacking in which Cs atoms are modulated along the c axis. Simulation of the selection rules allowed the determination of models of the incommensurate layers stacking along the c axis, with translations from one Cs layer to another layer commensurate with the graphite lattice. The initial stacking is described by a pseudo‐two‐layer model with successive random translations and a short‐range order. The structure appearing at a lower temperature is described by a pseudorhombohedral stacking with definite translations. The transition from the initial stacking with a first‐neighbour interaction to the pseudorhombohedral stacking with a second‐neighbour interaction could be a result of the change in interactions between the Cs atoms and the graphitic host, due to the dominating influence of the graphite periodic potential at low temperature.