Solution combustion synthesis and magnetic property of rock-salt (Co0.2Cu0.2Mg0.2Ni0.2Zn0.2)O high-entropy oxide nanocrystalline powder
•The (Co0.2Cu0.2Mg0.2Ni0.2Zn0.2)O nanocrystalline powder was synthesizes by SCS method.•Synthesis temperature of single-phase rock-salt structure was above 1123 K.•The material exhibits long-range antiferromagnetic behavior below TN.•The material shows lower TN. A facile solution combustion synthesi...
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Published in | Journal of magnetism and magnetic materials Vol. 484; pp. 245 - 252 |
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Main Authors | , , , , , |
Format | Journal Article |
Language | English |
Published |
Amsterdam
Elsevier B.V
15.08.2019
Elsevier BV |
Subjects | |
Online Access | Get full text |
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Summary: | •The (Co0.2Cu0.2Mg0.2Ni0.2Zn0.2)O nanocrystalline powder was synthesizes by SCS method.•Synthesis temperature of single-phase rock-salt structure was above 1123 K.•The material exhibits long-range antiferromagnetic behavior below TN.•The material shows lower TN.
A facile solution combustion synthesis method was successfully applied to synthesize single rock-salt structural (Co0.2Cu0.2Mg0.2Ni0.2Zn0.2)O high-entropy oxide (HEO) nanocrystalline powder with chemical homogeneity. The XRD patterns with Rietveld refinement reveal the formation of single-phase rock-salt structure occurs only at the synthesis temperatures ≥ 1123 K, and the average nanocrystalline size is about 43 nm. Moreover, two series of experiments confirm the effect of configurational entropy on phase stabilization. Furthermore, the as-synthesized single-phase (Co0.2Cu0.2Mg0.2Ni0.2Zn0.2)O nanocrystalline powder exhibits long-range antiferromagnetic behavior below Néel temperature (TN = 106 K), which can be well understood by the super-exchange interactions in the rock-salt HEO. The powder also shows lower TN due to the significant amount of nonmagnetic ions suppressing the antiferromagnetic order. |
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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 14 |
ISSN: | 0304-8853 1873-4766 |
DOI: | 10.1016/j.jmmm.2019.04.023 |