Incommensurately modulated structures of the <i>M</i> <sub>1/8</sub> Pr <sub>5/8</sub> MoO <sub>4</sub> ( <i>M</i> = Li, Na, K) scheelites

The effect of cation substitutions in the scheelite-type framework is investigated to understand the ordering of M<sup>+</sup>/Pr<sup>3+</sup> cations and vacancies in the structure. The cation deficient M<sub>1/8</sub>Pr<sub>5/8</sub>□<sub>1/4</sub>MoO<sub>4</sub> (M = Li, Na, K) phases were synthesized using solid state reactions. The K:Pr ratio in the K<sub>1/8</sub>Pr<sub>5/8</sub>MoO<sub>4</sub> sample was determined by inductively coupled plasma mass spectroscopy, inductively coupled plasma optical emission spectrometry and total reflection X-ray fluorescence spectroscopy. The local element distributions in K<sub>1/8</sub>Pr<sub>5/8</sub>□<sub>1/4</sub>MoO<sub>4</sub> were determined by energy-dispersive X-ray spectrometry. The incommensurately modulated crystal structures of the scheelite-based M<sub>1/8</sub>Pr<sub>5/8</sub>MoO<sub>4</sub> (M = Li, Na, K) phases were refined from synchrotron powder X-ray diffraction data. The analysis revealed that cation ordering in the M<sub>1/8</sub>Pr<sub>5/8</sub>MoO<sub>4</sub> (M = Li, Na) structures is incomplete and is more accurately described by continuous, rather than discontinuous (step-like), occupational modulation functions. The occupancy modulation waves for Li/Na and Pr atoms demonstrate an antiphase relation. Compared with M = Li, Na, the order of K and Pr cations in the A position in the K<sub>1/8</sub>Pr<sub>5/8</sub>MoO<sub>4</sub> structure is best approximated by crenel functions. Refining the coordinates and lengths of three atomic domains yields the composition of K<sub>0.145</sub>Pr<sub>0.618</sub>MoO<sub>4</sub>. In all cases, the modulation arises from ordering of M/Pr cations and cation vacancies at the A-sublattice of the parent scheelite ABO<sub>4</sub> structure. The distortion of PrO<sub>8</sub> and MO<sub>8</sub> polyhedra is practically independent of the radius of the M<sup>+</sup> cations. The refinements of the M<sub>1/8</sub>Pr<sub>5/8</sub>MoO<sub>4</sub> (M = Li, Na, K) structures reveal that MoO<sub>4</sub><sup>2-</sup> tetrahedra in these scheelite-type compounds demonstrate a flexible geometry. Both Mo-O bond distances and O-Mo-O bond angles vary significantly with changing the population of the A site by cations with different sizes.

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Journal
Acta Crystallographica Section B Structural Science Crystal Engineering and Materials
Published
2026-02-16
DOI
https://doi.org/10.1107/s2052520626000375
Primary Topic
Nuclear materials and radiation effects
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article
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article

Incommensurately modulated structures of the M 1/8 Pr 5/8 MoO 4 ( M = Li, Na, K) scheelites

Elena G. Khaikina, Olga M. Basovich, Darya G. Filatova, Bogdan I. Lazoryak et al.
Acta Crystallographica Section B Structural Science Crystal Engineering and Materials
Nuclear materials and radiation effects
article

Incommensurately modulated structures of the M 1/8 Pr 5/8 MoO 4 ( M = Li, Na, K) scheelites

Elena G. Khaikina, Olga M. Basovich, Darya G. Filatova, Bogdan I. Lazoryak, Alexei A. Belik, Dina V. Deyneko, Vladimir A. Morozov
article en

Abstract

The effect of cation substitutions in the scheelite-type framework is investigated to understand the ordering of M<sup>+</sup>/Pr<sup>3+</sup> cations and vacancies in the structure. The cation deficient M<sub>1/8</sub>Pr<sub>5/8</sub>□<sub>1/4</sub>MoO<sub>4</sub> (M = Li, Na, K) phases were synthesized using solid state reactions. The K:Pr ratio in the K<sub>1/8</sub>Pr<sub>5/8</sub>MoO<sub>4</sub> sample was determined by inductively coupled plasma mass spectroscopy, inductively coupled plasma optical emission spectrometry and total reflection X-ray fluorescence spectroscopy. The local element distributions in K<sub>1/8</sub>Pr<sub>5/8</sub>□<sub>1/4</sub>MoO<sub>4</sub> were determined by energy-dispersive X-ray spectrometry. The incommensurately modulated crystal structures of the scheelite-based M<sub>1/8</sub>Pr<sub>5/8</sub>MoO<sub>4</sub> (M = Li, Na, K) phases were refined from synchrotron powder X-ray diffraction data. The analysis revealed that cation ordering in the M<sub>1/8</sub>Pr<sub>5/8</sub>MoO<sub>4</sub> (M = Li, Na) structures is incomplete and is more accurately described by continuous, rather than discontinuous (step-like), occupational modulation functions. The occupancy modulation waves for Li/Na and Pr atoms demonstrate an antiphase relation. Compared with M = Li, Na, the order of K and Pr cations in the A position in the K<sub>1/8</sub>Pr<sub>5/8</sub>MoO<sub>4</sub> structure is best approximated by crenel functions. Refining the coordinates and lengths of three atomic domains yields the composition of K<sub>0.145</sub>Pr<sub>0.618</sub>MoO<sub>4</sub>. In all cases, the modulation arises from ordering of M/Pr cations and cation vacancies at the A-sublattice of the parent scheelite ABO<sub>4</sub> structure. The distortion of PrO<sub>8</sub> and MO<sub>8</sub> polyhedra is practically independent of the radius of the M<sup>+</sup> cations. The refinements of the M<sub>1/8</sub>Pr<sub>5/8</sub>MoO<sub>4</sub> (M = Li, Na, K) structures reveal that MoO<sub>4</sub><sup>2-</sup> tetrahedra in these scheelite-type compounds demonstrate a flexible geometry. Both Mo-O bond distances and O-Mo-O bond angles vary significantly with changing the population of the A site by cations with different sizes.

Acta Crystallographica Section B Structural Science Crystal Engineering and MaterialsVol. 82(2)
State University of Management (RU), National Institute for Materials Science (JP), Baikal Institute of Nature Management (RU)
Openalex Percentile: Top 44%
Nuclear materials and radiation effects
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