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Magnetic and Electrical Properties of CoRE(2)W(2)O(10) Ceramic Materials
[Image: see text] Microcrystalline samples of CoRE(2)W(2)O(10) tungstates (RE = Y, Dy, Ho, Er) were prepared by a high-temperature solid-state reaction and then sintered into a ceramic form for unique properties and potential applications. For this purpose, structural, microscopic, ultraviolet–visib...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2023
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10568695/ https://www.ncbi.nlm.nih.gov/pubmed/37841119 http://dx.doi.org/10.1021/acsomega.3c04645 |
Sumario: | [Image: see text] Microcrystalline samples of CoRE(2)W(2)O(10) tungstates (RE = Y, Dy, Ho, Er) were prepared by a high-temperature solid-state reaction and then sintered into a ceramic form for unique properties and potential applications. For this purpose, structural, microscopic, ultraviolet–visible (UV–vis), magnetic, electrical, and thermoelectric measurements were performed. These studies showed a monoclinic structure, paramagnetism, short-range antiferromagnetic interactions in all samples, long-range ferrimagnetic interactions only in CoY(2)W(2)O(10), poor n-type conductivity of 6.7 × 10(–7) S/m at room temperature, strong thermal activation (E(a1) = 0.7 eV) in the intrinsic region, a strong increase in the power factor (S(2)σ) above 300 K, a Fermi energy (E(F)) of 0.16 eV, and a Fermi temperature (T(F)) of 1800 K. The above studies suggest that anion vacancy levels, which act as doubly charged donors, and to a lesser extent, the mixed valence band of cobalt ions (Co(2+), Co(3+)), which are located below the bottom of the conduction band and below the Fermi level, are responsible for electron transport. |
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