The synthesis, crystal structure, phase transformations, and thermal expansion of (Y
1−xEu
x)
2(SO
4)
3*8H
2O (where
x = 0, 0.17, 0.33, 0.50, 0.66, 0.83, and 1) are presented. (Y
1−xEu
x)
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The synthesis, crystal structure, phase transformations, and thermal expansion of (Y
1−xEu
x)
2(SO
4)
3*8H
2O (where
x = 0, 0.17, 0.33, 0.50, 0.66, 0.83, and 1) are presented. (Y
1−xEu
x)
2(SO
4)
3*8H
2O solid solutions were synthesized via crystallization from an aqueous solution. (Y
1−xEu
x)
2(SO
4)
3*8H
2O (
C2/
c) ↔ (Y
1−xEu
x)
2(SO
4)
3 (
Pbcn) → (Y
1−xEu
x)
2O
2SO
4 (
C2/
c) and Eu
2(SO
4)
3*8H
2O (
C2/
c) ↔ Eu
2(SO
4)
3 (
C2/
c) → Eu
2O
2SO
4 (
C2/
c) phase transformations for all samples were investigated by high-temperature powder X-ray diffraction, differential scanning calorimetry and thermogravimetry in the temperature ranges of 25–750 and 25–1350 °C, respectively. The aim of this work is to identify the structural heredity of the phases formed during thermal transformations of (Y
1−xEu
x)
2(SO
4)
3*8H
2O solid solutions, and to study the mechanisms of the thermal deformations of the crystal structure. Structural relations between these phases were found. The crystal structures of YEu(SO
4)
3*8H
2O and (Y
0.83Eu
0.17)
2(SO
4)
3*8H
2O were refined at −173, −123, −73, −23, 27, and 77 °C. Thermal expansion coefficients for (Y
1−xEu
x)
2(SO
4)
3*8H
2O, Eu
2(SO
4)
3, (Y
1−xEu
x)
2O
2SO
4 (where
x = 0, 0.17, 0.33, 0.50, 0.66, 0.83, and 1) compounds and solid solutions were calculated for the first time. The thermal expansion of Eu
2(SO
4)
3 was highest in the direction approximately coinciding with the
c-axis, because the Eu–O chains extended in this direction. As temperature increased, the crystal structure of (Y
1−xEu
x)
2(SO
4)
3*8H
2O expanded significantly in the
ac plane along directions close to the
a and
c axes, while thermal expansion along the
b axis was relatively low. The distance between layers in the (Y
1−xEu
x)
2(SO
4)
3*8H
2O crystal structure increased with increasing temperature, and corrugated layers (parallel to (101) direction) straightened out due to the rotation of the S
2O
4 tetrahedra. At high temperature, thermal expansion of Y
2O
2SO
4 was highest along the longer diagonal of the
ac parallelogram perpendicular to the plane of the oxo-centered
[YO] layers.
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