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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 |
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author | Ke, Ya-Jiao Zhang, Xiang-Qun Ma, Yue Cheng, Zhao-Hua |
author_facet | Ke, Ya-Jiao Zhang, Xiang-Qun Ma, Yue Cheng, Zhao-Hua |
author_sort | Ke, Ya-Jiao |
collection | PubMed |
description | 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. |
format | Online Article Text |
id | pubmed-4726382 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2016 |
publisher | Nature Publishing Group |
record_format | MEDLINE/PubMed |
spelling | pubmed-47263822016-01-27 Anisotropic magnetic entropy change in RFeO(3) single crystals(R = Tb, Tm, or Y) Ke, Ya-Jiao Zhang, Xiang-Qun Ma, Yue Cheng, Zhao-Hua Sci Rep Article 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. Nature Publishing Group 2016-01-25 /pmc/articles/PMC4726382/ /pubmed/26806069 http://dx.doi.org/10.1038/srep19775 Text en Copyright © 2016, Macmillan Publishers Limited http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ |
spellingShingle | Article Ke, Ya-Jiao Zhang, Xiang-Qun Ma, Yue Cheng, Zhao-Hua Anisotropic magnetic entropy change in RFeO(3) single crystals(R = Tb, Tm, or Y) |
title | Anisotropic magnetic entropy change in RFeO(3) single crystals(R = Tb, Tm, or Y) |
title_full | Anisotropic magnetic entropy change in RFeO(3) single crystals(R = Tb, Tm, or Y) |
title_fullStr | Anisotropic magnetic entropy change in RFeO(3) single crystals(R = Tb, Tm, or Y) |
title_full_unstemmed | Anisotropic magnetic entropy change in RFeO(3) single crystals(R = Tb, Tm, or Y) |
title_short | Anisotropic magnetic entropy change in RFeO(3) single crystals(R = Tb, Tm, or Y) |
title_sort | anisotropic magnetic entropy change in rfeo(3) single crystals(r = tb, tm, or y) |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4726382/ https://www.ncbi.nlm.nih.gov/pubmed/26806069 http://dx.doi.org/10.1038/srep19775 |
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