4.5 Article

Refining perovskite structures to pair distribution function data using collective Glazer modes as a basis

Journal

IUCRJ
Volume 9, Issue -, Pages 705-712

Publisher

INT UNION CRYSTALLOGRAPHY
DOI: 10.1107/S2052252522007680

Keywords

inorganic materials; materials modelling; perovskites; structure refinement; pair distribution functions; octahedral rotations; geometric modelling

Funding

  1. US National Science Foundation, Directorate for Mathematical and Physical Sciences [DMREF-1922234]
  2. Carlsberg Foundation [CF17-0823]
  3. US Department of Energy, Office of Science, Office of Basic Energy Sciences [DE-SC0012704]

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This paper discusses the development of constraints for modelling pure octahedral tilts in perovskites, which helps disentangle the tilts from other structural distortions and provides stable refinements of the tilt components in real materials. The model in the program allows features in the PDF to be separated based on rigid tilts and non-rigid relaxations, giving researchers an intuitive picture of the tilting.
Structural modelling of octahedral tilts in perovskites is typically carried out using the symmetry constraints of the resulting space group. In most cases, this introduces more degrees of freedom than those strictly necessary to describe only the octahedral tilts. It can therefore be a challenge to disentangle the octahedral tilts from other structural distortions such as cation displacements and octahedral distortions. This paper reports the development of constraints for modelling pure octahedral tilts and implementation of the constraints in diffpy-CMI, a powerful package to analyse pair distribution function (PDF) data. The model in the program allows features in the PDF that come from rigid tilts to be separated from non-rigid relaxations, providing an intuitive picture of the tilting. The model has many fewer refinable variables than the unconstrained space group fits and provides robust and stable refinements of the tilt components. It further demonstrates the use of the model on the canonical tilted perovskite CaTiO3 which has the known Glazer tilt system alpha(+)beta(-)beta(-). The Glazer model fits comparably to the corresponding space-group model Pnma below r = 14 angstrom and becomes progressively worse than the space-group model at higher r due to non-rigid distortions in the real material.

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