posted on 2023-05-12, 16:34authored byYves A. Mantz, Yueh-Lin Lee
The first six cubic LaMnO3 high-index surfaces,
(210),
(211), (221), (310), (311), and (320), are examined for the first
time. The unrelaxed and relaxed surface energies of the surfaces are
computed as a function of surface model thickness using unrelaxed
and relaxed surface models, respectively. The (210), (320), (211),
and (221) surfaces are found to be more stable than the low-index
(011) and (111) surfaces. Helping to explain this result, the surface
terminations of the (210), (320), (211), or (221) surface are seen
to exhibit a rotational relaxation of the MnO6 or oxygen
octahedra extending from the surface into the bulk. By contrast, the
relaxed surface energies of the (310) and (311) surfaces are concluded
to be difficult to determine due to a structural transformation or
phase change in the surface models of the surfaces away from cubic
LaMnO3. The finding of a phase change is important. It
indicates that a phase change in the surface models of a surface for
another material could occur if the surface is relatively open and
a different phase of the material is stable at low temperature. When
modeling such a surface, two steps are suggested to be taken.