Helium Incorporation into Scandium Fluoride, a Model Negative Thermal Expansion Material

Scandium trifluoride is a model negative thermal expansion (NTE) material. Its simple structure can be described as an A-site vacant perovskite, and it shows isotropic NTE over a very wide temperature range (up to ∼1100 K), due to transverse vibrational motion of the fluoride. Like many framework NTE materials, it undergoes a phase transition at low pressures, adopting a rhombohedral (<i>R</i>3̅<i>c</i>) structure at >0.7 GPa and 300 K in commonly used nonpenetrating pressure media, such as silicone oil. High pressure X-ray diffraction data and gas uptake/release measurements indicate that, on compression in helium above ∼200 K, helium is inserted into ScF<sub>3</sub> to form the defect perovskite He <sub><i>x</i></sub> ScF<sub>3</sub>. The incorporation of helium stiffens the structure and changes its phase behavior. At room temperature, complete filling of the structure with helium does not occur until >1.5 GPa. On compression, a cubic perovskite structure is maintained until ∼5 GPa. As the pressure was increased to ∼9.5 GPa, a further transition occurred at ∼7 GPa. The first transition at ∼5 GPa is likely to a tetragonal (<i>P</i>4/<i>mbm</i>) perovskite, but the detailed structure of the perovskite phase formed on compression above ∼7 GPa is unclear. Cooling down from 300 to 100 K in helium at ∼0.4 GPa leads to an approximate composition of He<sub>0.1</sub>ScF<sub>3</sub>. High pressure neutron diffraction measurements, in the temperature range 15-150 K show that the incorporation of helium increases the pressure at which the cubic (<i>Pm</i>3̅<i>m</i>) to rhombohedral (<i>R</i>3̅<i>c</i>) putative quantum structural phase transition occurs from close to 0 GPa to ∼0.2 GPa at 0 K.

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Publication Details

Journal
Chemistry of Materials
Published
2025-02-04
DOI
https://doi.org/10.1021/acs.chemmater.4c03329
Citations
1
Primary Topic
Thermal Expansion and Ionic Conductivity
Type
article
Field-Weighted Citation Impact
0.52

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article

Helium Incorporation into Scandium Fluoride, a Model Negative Thermal Expansion Material

A. M. dos Santos, Jamie J. Molaison, Shangye Ma, Stella Chariton et al.
1 citations
Chemistry of Materials
Thermal Expansion and Ionic Conductivity
0.52
article

Helium Incorporation into Scandium Fluoride, a Model Negative Thermal Expansion Material

A. M. dos Santos, Jamie J. Molaison, Shangye Ma, Stella Chariton, Changyong Park, Samuel J. Baxter, Angus P. Wilkinson
article en
1 citations

Abstract

Scandium trifluoride is a model negative thermal expansion (NTE) material. Its simple structure can be described as an A-site vacant perovskite, and it shows isotropic NTE over a very wide temperature range (up to ∼1100 K), due to transverse vibrational motion of the fluoride. Like many framework NTE materials, it undergoes a phase transition at low pressures, adopting a rhombohedral (<i>R</i>3̅<i>c</i>) structure at >0.7 GPa and 300 K in commonly used nonpenetrating pressure media, such as silicone oil. High pressure X-ray diffraction data and gas uptake/release measurements indicate that, on compression in helium above ∼200 K, helium is inserted into ScF<sub>3</sub> to form the defect perovskite He <sub><i>x</i></sub> ScF<sub>3</sub>. The incorporation of helium stiffens the structure and changes its phase behavior. At room temperature, complete filling of the structure with helium does not occur until >1.5 GPa. On compression, a cubic perovskite structure is maintained until ∼5 GPa. As the pressure was increased to ∼9.5 GPa, a further transition occurred at ∼7 GPa. The first transition at ∼5 GPa is likely to a tetragonal (<i>P</i>4/<i>mbm</i>) perovskite, but the detailed structure of the perovskite phase formed on compression above ∼7 GPa is unclear. Cooling down from 300 to 100 K in helium at ∼0.4 GPa leads to an approximate composition of He<sub>0.1</sub>ScF<sub>3</sub>. High pressure neutron diffraction measurements, in the temperature range 15-150 K show that the incorporation of helium increases the pressure at which the cubic (<i>Pm</i>3̅<i>m</i>) to rhombohedral (<i>R</i>3̅<i>c</i>) putative quantum structural phase transition occurs from close to 0 GPa to ∼0.2 GPa at 0 K.

Chemistry of MaterialsVol. 37(4)
Argonne National Laboratory (US), Oak Ridge National Laboratory (US), Georgia Institute of Technology (US), University of Chicago (US), X-ray Instrumentation Associates (United States) (US)
National Science Foundation, U.S. Department of Energy, National Nuclear Security Administration, Division of Materials Research, Division of Earth Sciences
Affordable and clean energy
Openalex Percentile: Top 42%
Thermal Expansion and Ionic Conductivity
0.52
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