Weak ferromagnetic component on the bulk ZnFe sub(2)O sub(4) compound

Magnetization data on the bulk ZnFe sub(2)O sub(4) antiferromagnetic compound (T sub()N[approx =] 10 K) obtained via solid state reaction at different synthesis temperatures show one weak ferromagnetic component at room temperature. We have related it with the cationic disorder effect present on spi...

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Bibliographic Details
Published in:Journal of magnetism and magnetic materials 2014-01, Vol.350, p.47-49
Main Authors: Jesus, C BR, Mendonca, E C, Silva, L S, Folly, W SD, Meneses, C T, Duque, J GS
Format: Article
Language:English
Subjects:
Antiferromagnetism
Cationic
Curie-Weiss law
Disorders
Ferromagnetism
Iron
Magnetization
Synthesis
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Summary:Magnetization data on the bulk ZnFe sub(2)O sub(4) antiferromagnetic compound (T sub()N[approx =] 10 K) obtained via solid state reaction at different synthesis temperatures show one weak ferromagnetic component at room temperature. We have related it with the cationic disorder effect present on spinel structure of our bulk samples which comes from the magnetic interaction between iron ions sit on both octahedral and tetrahedral sites. The magnetization measurements show to all samples a clear peak around 10 K consistent with the antiferromagnetic phase transition. On the other hand, after extracted the para-magnetic component, the hysteresis loops measured at room temperature display one weak ferromagnetic component. Once the T-dependence of magnetization does not fit to a Curie-Weiss law to temperatures well above the magnetic transition we have used a combination of the Curie-Weiss law (paramagnetic spins) and a typical temperature dependence of M sub(0), M sub(0)(T)=M sub(0)(O)[1 -(T/T sub()c super(2)] super(0.5) (ordered ferromagnetic spins). We note an increase of the M sub(0)(O) as function of the synthesis temperature. This reinforce our supposition of a cationic disorder effect driving the system to present two kinds of magnetic interactions between iron ions on A and B sites.
ISSN:0304-8853
DOI:10.1016/j.jmmm.2013.09.025