posted on 2023-05-12, 16:34authored byYves A. Mantz, Yueh-Lin Lee
The first six cubic LaMnO<sub>3</sub> 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 MnO<sub>6</sub> 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
LaMnO<sub>3</sub>. 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.