Phase Equilibria in Systems DyCuS2–EuS and Cu2S−Dy2S3−EuS
- Authors: Ruseikina A.V.1, Andreev O.V.1
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Affiliations:
- Tyumen State University
- Issue: Vol 63, No 11 (2018)
- Pages: 1494-1500
- Section: Physicochemical Analysis of Inorganic Systems
- URL: https://journal-vniispk.ru/0036-0236/article/view/169112
- DOI: https://doi.org/10.1134/S0036023618110141
- ID: 169112
Cite item
Abstract
The phase diagram of system DyCuS2–EuS has been first constructed, and the phase equilibria in the Cu2S–Dy2S3–EuS triangle at 970 K have been studied. Compound EuDyCuS3 (1DyCuS2 : 1EuS), space group Pnma, a = 10.1901(3) Å, b = 3.9270(1) Å, c = 12.8468(3) Å, melts incongruently at 1727 ± 7 K according to the reaction: EuDyCuS3solid ↔ 0.17 SS EuS (90 mol % EuS, 10 mol % DyCuS2) + 0.83 liq (42 mol % EuS, 58 mol % DyCuS2), ΔH = 2.9 ± 0.6 kJ/mol; microhardness of the phase is 3080 ± 35 MPa. Compound EuDyCuS3 is transparent in the range 3000–1800 cm–1. In system DyCuS2–EuS, the solid solution (SS) based on EuS extends from 91 to 100 mol % at 1770 K and from 92 to 100 mol % at 1170 K. In γ-DyCuS2, 2 mol % EuS dissolves at 1487 K. The eutectic is formed between compounds DyCuS2 and EuDyCuS3 at 12 mol % EuS, T = 1487 ± 8 K. In system Cu2S−Dy2S3−EuS, 10 secondary systems have been isolated. At 970 K, tie-lines are located between compound EuDyCuS3 and solid solutions based on compounds β-Cu2S, EuS, DyCuS2, β-(DyCu3S3), and EuDy2S4; between DyCuS2 and the solid solution of α-Dy2S3, DyCuS2, and EuDy2S4.
About the authors
A. V. Ruseikina
Tyumen State University
Author for correspondence.
Email: adeschina@mail.ru
Russian Federation, Tyumen, 625003
O. V. Andreev
Tyumen State University
Email: adeschina@mail.ru
Russian Federation, Tyumen, 625003
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