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Anisotropic magnetic entropy change in RFeO(3) single crystals(R = Tb, Tm, or Y)
Compared with traditional gas-compression/expansion refrigeration, magnetic refrigeration based on magnetocaloric effect (MCE) exhibits the advantages of high energy efficiency and environment friendliness. Here, we created large MCE in RFeO(3) (R = Tb or Tm) single crystals by the magnetization vec...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2016
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4726382/ https://www.ncbi.nlm.nih.gov/pubmed/26806069 http://dx.doi.org/10.1038/srep19775 |
Sumario: | Compared with traditional gas-compression/expansion refrigeration, magnetic refrigeration based on magnetocaloric effect (MCE) exhibits the advantages of high energy efficiency and environment friendliness. Here, we created large MCE in RFeO(3) (R = Tb or Tm) single crystals by the magnetization vector rotation of single crystal with strong magnetocrystalline anisotropy (MCA), rather than merely via the order-disorder magnetic phase transition or magnetic structural transition. Owing to the difference in charge distribution of 4f-electrons between Tb(3+ ) and Tm(3+) ions, the rotating field entropy with different signs, −ΔS(M)(R) = 17.42 J/kg K, and –ΔS(M)(R) = −9.01 J/kg K are achieved at 9 K and 17 K for TbFeO(3 )and TmFeO(3) single crystals from b axis to c axis, at 50 kOe, respectively. The finding of the large anisotropic MCE not only advances our understanding of the anisotropy of MCE, but also extends the application for single crystals to magnetic refrigeration. |
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