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Structure, magnetism and magnetocaloric effect in a new triangular lattice compound Gd(3)Cu(9)(OH)(19)Br(8)
A new triangular lattice compound Gd(3)Cu(9)(OH)(19)Br(8) has been synthesized by the hydrothermal method. The structure, magnetism and magnetocaloric effect of Gd(3)Cu(9)(OH)(19)Br(8) have been studied by X-ray diffraction, magnetic susceptibility, isothermal magnetization and specific heat measure...
Autores principales: | , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9465698/ https://www.ncbi.nlm.nih.gov/pubmed/36199608 http://dx.doi.org/10.1039/d2ra04553b |
Sumario: | A new triangular lattice compound Gd(3)Cu(9)(OH)(19)Br(8) has been synthesized by the hydrothermal method. The structure, magnetism and magnetocaloric effect of Gd(3)Cu(9)(OH)(19)Br(8) have been studied by X-ray diffraction, magnetic susceptibility, isothermal magnetization and specific heat measurements. In Gd(3)Cu(9)(OH)(19)Br(8), the Cu(2+) ions form a Kagome lattice along the ab plane, and Gd(3+) ions are located in the center of hexagonal holes of the Kagome layer. The Cu-sublattice and Gd-sublattice overlap and constitute a magnetic triangular lattice. The temperature dependence of susceptibility and specific heat curves indicate no magnetic transition down to 2 K, suggesting a paramagnetic-like behavior at low temperature. The magnetocaloric effect (MCE) at low temperature has been calculated according to Maxwell's equations. The maximum value of magnetic entropy change −ΔS(M) is 26.04 J kg(−1) K(−1) and adiabatic temperature change ΔT(ad) is 13.79 K, for a field change of 0–7 T, indicating a potential application of this compound in the field of magnetic refrigeration at low temperature. The influence of 4f–3d interaction on magnetism and MCE is also discussed. |
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