Theoretical and Experimental Studies of the Structural Chameleon EuYCuTe3

Layered orthorhombic single crystals of EuYCuTe<sub>3</sub> are synthesized using the ampoule method from the elemental precursors taken in the ratio of 1 Eu:1 Y:1 Cu:3 Te by heating up to 1120 K with an excess of CsI as flux. The orthorhombic structure of EuYCuTe<sub>3</sub> is established, and structural parameters are obtained using X-ray diffraction. At ambient conditions, the sample crystallizes in the space group <i>Pnma</i> with the unit cell parameters <i>a</i> = 11.2730(7) Å, <i>b</i> = 4.3214(3) Å, <i>c</i> = 14.3271(9) Å. The structure is composed of vertex-connected [CuTe<sub>4</sub>]<sup>7-</sup> tetrahedra, which form chains along the [010] direction, and of edge-connected [YTe<sub>6</sub>]<sup>9-</sup> octahedra, which form layers parallel to the (010) plane. The Eu<sup>2+</sup> cations are found in a capped trigonal prismatic coordination of Te<sup>2-</sup> anions. The structural phase transition from the <i>α</i> to the <i>β</i> phase is discovered upon heating the sample to 323 K, which comes accompanied with a decrease of [CuTe<sub>4</sub>]<sup>7-</sup> tetrahedral distortion. The symmetry of the high-temperature phase is established as ordered in the space group <i>Cmcm</i> (<i>a</i> = 4.3231(3) Å, <i>b</i> = 14.3328(9) Å, <i>c</i> = 11.2843(7) Å). The nature and microscopic mechanism of the phase transition is discussed. By cooling it down below 3 K, the soft ferromagnetic properties of EuYCuTe<sub>3</sub> are discovered. The correlation of the ferromagnetic transition temperature in the series of chalcogenides EuYCu<i>Ch</i><sub>3</sub> (<i>Ch</i> = S, Se, Te) with the ionic radius of the chalcogenide anion is established. The structural dynamical elastic properties of <i>α</i>- and <i>β</i>-EuYCuTe<sub>3</sub> were calculated within the ab initio approach. The vibrational mode frequencies and decomposition on irreducible representations, as well as the degree of ion involvement in each mode, were determined. The calculations reveal an imaginary mode in the Y-point of the <i>Brillouin</i> zone in the high symmetry <i>β</i>-EuYCuTe<sub>3</sub> phase. This finding explains the nature of structural reconstruction in EuYCuTe<sub>3</sub> crystal as a second-order phase transition induced by soft mode condensation at the edge of the <i>Brillouin</i> zone. The exfoliation of a single layer is simulated theoretically. The exfoliation energy is estimated, and the dynamical properties of EuYCuTe<sub>3</sub> single layers are studied.

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Journal
Materials
Published
2025-02-13
DOI
https://doi.org/10.3390/ma18040820
Citations
3
Primary Topic
Advanced Thermoelectric Materials and Devices
Type
article
Field-Weighted Citation Impact
1.55

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article

Theoretical and Experimental Studies of the Structural Chameleon EuYCuTe3

Maxim V. Grigoriev, Alexander A. Garmonov, Аnna V. Ruseikina, V. A. Chernyshev et al.
3 citations
Materials
Advanced Thermoelectric Materials and Devices
1.55
article

Theoretical and Experimental Studies of the Structural Chameleon EuYCuTe3

Maxim V. Grigoriev, Alexander A. Garmonov, Аnna V. Ruseikina, V. A. Chernyshev, Thomas Schleid, E. M. Roginskiĭ, Ralf J. C. Locke
article en
3 citations

Abstract

Layered orthorhombic single crystals of EuYCuTe<sub>3</sub> are synthesized using the ampoule method from the elemental precursors taken in the ratio of 1 Eu:1 Y:1 Cu:3 Te by heating up to 1120 K with an excess of CsI as flux. The orthorhombic structure of EuYCuTe<sub>3</sub> is established, and structural parameters are obtained using X-ray diffraction. At ambient conditions, the sample crystallizes in the space group <i>Pnma</i> with the unit cell parameters <i>a</i> = 11.2730(7) Å, <i>b</i> = 4.3214(3) Å, <i>c</i> = 14.3271(9) Å. The structure is composed of vertex-connected [CuTe<sub>4</sub>]<sup>7-</sup> tetrahedra, which form chains along the [010] direction, and of edge-connected [YTe<sub>6</sub>]<sup>9-</sup> octahedra, which form layers parallel to the (010) plane. The Eu<sup>2+</sup> cations are found in a capped trigonal prismatic coordination of Te<sup>2-</sup> anions. The structural phase transition from the <i>α</i> to the <i>β</i> phase is discovered upon heating the sample to 323 K, which comes accompanied with a decrease of [CuTe<sub>4</sub>]<sup>7-</sup> tetrahedral distortion. The symmetry of the high-temperature phase is established as ordered in the space group <i>Cmcm</i> (<i>a</i> = 4.3231(3) Å, <i>b</i> = 14.3328(9) Å, <i>c</i> = 11.2843(7) Å). The nature and microscopic mechanism of the phase transition is discussed. By cooling it down below 3 K, the soft ferromagnetic properties of EuYCuTe<sub>3</sub> are discovered. The correlation of the ferromagnetic transition temperature in the series of chalcogenides EuYCu<i>Ch</i><sub>3</sub> (<i>Ch</i> = S, Se, Te) with the ionic radius of the chalcogenide anion is established. The structural dynamical elastic properties of <i>α</i>- and <i>β</i>-EuYCuTe<sub>3</sub> were calculated within the ab initio approach. The vibrational mode frequencies and decomposition on irreducible representations, as well as the degree of ion involvement in each mode, were determined. The calculations reveal an imaginary mode in the Y-point of the <i>Brillouin</i> zone in the high symmetry <i>β</i>-EuYCuTe<sub>3</sub> phase. This finding explains the nature of structural reconstruction in EuYCuTe<sub>3</sub> crystal as a second-order phase transition induced by soft mode condensation at the edge of the <i>Brillouin</i> zone. The exfoliation of a single layer is simulated theoretically. The exfoliation energy is estimated, and the dynamical properties of EuYCuTe<sub>3</sub> single layers are studied.

MaterialsVol. 18(4)
University of Stuttgart (DE), Ural Federal University (RU), University of Tyumen (RU), Ioffe Institute (RU)
Russian Science Foundation
Openalex Percentile: Top 20%
Advanced Thermoelectric Materials and Devices
1.55
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