Materials with the cubic ReO 3 -type structure are, in principle, excellent candidates for negative thermal expansion (NTE). However, many such materials, including TaO 2 F, do not display NTE. It is proposed that local distortions away from the ideal structure, associated with the need to accommodate the different bonding requirements of the disordered O/F, contribute to the occurrence of near zero thermal expansion rather than NTE. The local structure of TaO 2 F is poorly described by an ideal cubic ReO 3 -type model with O and F randomly distributed over the available anion sites. A supercell model featuring −Ta–O–Ta–O–Ta–F– chains along ⟨1 0 0⟩, with different Ta–O and Ta–F distances and O/F off-axis displacements, gives much better agreement with pair distribution functions (PDFs) derived from total X-ray scattering data for small separations (<8 Å). Analyses of PDFs derived from variable temperature measurements (80 to 487 K), over different length scales, indicate an average linear expansion coefficient of close to zero with similar contributions from the geometrically distinct Ta–O—Ta and Ta–F—Ta links in TaO 2 F.
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Morelock et al. (2013) studied this question.
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