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Influence of Crystallite Size on the Magnetic Order in Semiconducting ZnCr(2)Se(4) Nanoparticles

Structural, electrical, magnetic, and specific heat measurements were carried out on ZnCr(2)Se(4) single crystal and on nanocrystals obtained from the milling of this single crystal after 1, 3, and 5 h, whose crystallite sizes were 25.2, 2.5, and 2 nm, respectively. For this purpose, the high-energy...

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Detalles Bibliográficos
Autores principales: Malicka, Ewa, Karolus, Małgorzata, Groń, Tadeusz, Gudwański, Adrian, Ślebarski, Andrzej, Goraus, Jerzy, Oboz, Monika, Sawicki, Bogdan, Panek, Joanna
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6926978/
https://www.ncbi.nlm.nih.gov/pubmed/31795184
http://dx.doi.org/10.3390/ma12233947
Descripción
Sumario:Structural, electrical, magnetic, and specific heat measurements were carried out on ZnCr(2)Se(4) single crystal and on nanocrystals obtained from the milling of this single crystal after 1, 3, and 5 h, whose crystallite sizes were 25.2, 2.5, and 2 nm, respectively. For this purpose, the high-energy ball-milling method was used. The above studies showed that all samples have a spinel structure, and are p-type semiconductors with less milling time and n-type with a higher one. In turn, the decrease in crystallite size caused a change in the magnetic order, from antiferromagnetic for bulk material and nanocrystals after 1 and 3 h of milling to spin-glass with the freezing temperature T(f) = 20 K for the sample after 5 h of milling. The spin-glass behavior for this sample was derived from a broad peak of dc magnetic susceptibility, a splitting of the zero-field-cooling and field-cooling susceptibilities, and from the shift of T(f) towards the higher frequency of the ac susceptibility curves. A spectacular result for this sample is also the lack of a peak on the specific heat curve, suggesting a disappearance of the structural transition that is observed for the bulk single crystal.