Giant multiple caloric effects in charge transition ferrimagnet
Abstract Caloric effects of solids can provide us with innovative refrigeration systems more efficient and environment-friendly than the widely-used conventional vapor-compression cooling systems. Exploring novel caloric materials is challenging but critically important in developing future technolo...
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2021-06-01
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Series: | Scientific Reports |
Online Access: | https://doi.org/10.1038/s41598-021-91888-8 |
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doaj-8f8247d3514448548b25b2e3c52f085e2021-06-27T11:32:25ZengNature Publishing GroupScientific Reports2045-23222021-06-011111810.1038/s41598-021-91888-8Giant multiple caloric effects in charge transition ferrimagnetYoshihisa Kosugi0Masato Goto1Zhenhong Tan2Daisuke Kan3Masahiko Isobe4Kenji Yoshii5Masaichiro Mizumaki6Asaya Fujita7Hidenori Takagi8Yuichi Shimakawa9Institute for Chemical Research, Kyoto UniversityInstitute for Chemical Research, Kyoto UniversityInstitute for Chemical Research, Kyoto UniversityInstitute for Chemical Research, Kyoto UniversityMax Planck Institute for Solid State ResearchJapan Atomic Energy AgencyJapan Synchrotron Radiation Research InstituteMagnetic Powder Metallurgy Research Center, AIST ChubuMax Planck Institute for Solid State ResearchInstitute for Chemical Research, Kyoto UniversityAbstract Caloric effects of solids can provide us with innovative refrigeration systems more efficient and environment-friendly than the widely-used conventional vapor-compression cooling systems. Exploring novel caloric materials is challenging but critically important in developing future technologies. Here we discovered that the quadruple perovskite structure ferrimagnet BiCu3Cr4O12 shows large multiple caloric effects at the first-order charge transition occurring around 190 K. Large latent heat and the corresponding isothermal entropy change, 28.2 J K−1 kg−1, can be utilized by applying both magnetic fields (a magnetocaloric effect) and pressure (a barocaloric effect). Adiabatic temperature changes reach 3.9 K for the 50 kOe magnetic field and 4.8 K for the 4.9 kbar pressure, and thus highly efficient thermal controls are achieved in multiple ways.https://doi.org/10.1038/s41598-021-91888-8 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Yoshihisa Kosugi Masato Goto Zhenhong Tan Daisuke Kan Masahiko Isobe Kenji Yoshii Masaichiro Mizumaki Asaya Fujita Hidenori Takagi Yuichi Shimakawa |
spellingShingle |
Yoshihisa Kosugi Masato Goto Zhenhong Tan Daisuke Kan Masahiko Isobe Kenji Yoshii Masaichiro Mizumaki Asaya Fujita Hidenori Takagi Yuichi Shimakawa Giant multiple caloric effects in charge transition ferrimagnet Scientific Reports |
author_facet |
Yoshihisa Kosugi Masato Goto Zhenhong Tan Daisuke Kan Masahiko Isobe Kenji Yoshii Masaichiro Mizumaki Asaya Fujita Hidenori Takagi Yuichi Shimakawa |
author_sort |
Yoshihisa Kosugi |
title |
Giant multiple caloric effects in charge transition ferrimagnet |
title_short |
Giant multiple caloric effects in charge transition ferrimagnet |
title_full |
Giant multiple caloric effects in charge transition ferrimagnet |
title_fullStr |
Giant multiple caloric effects in charge transition ferrimagnet |
title_full_unstemmed |
Giant multiple caloric effects in charge transition ferrimagnet |
title_sort |
giant multiple caloric effects in charge transition ferrimagnet |
publisher |
Nature Publishing Group |
series |
Scientific Reports |
issn |
2045-2322 |
publishDate |
2021-06-01 |
description |
Abstract Caloric effects of solids can provide us with innovative refrigeration systems more efficient and environment-friendly than the widely-used conventional vapor-compression cooling systems. Exploring novel caloric materials is challenging but critically important in developing future technologies. Here we discovered that the quadruple perovskite structure ferrimagnet BiCu3Cr4O12 shows large multiple caloric effects at the first-order charge transition occurring around 190 K. Large latent heat and the corresponding isothermal entropy change, 28.2 J K−1 kg−1, can be utilized by applying both magnetic fields (a magnetocaloric effect) and pressure (a barocaloric effect). Adiabatic temperature changes reach 3.9 K for the 50 kOe magnetic field and 4.8 K for the 4.9 kbar pressure, and thus highly efficient thermal controls are achieved in multiple ways. |
url |
https://doi.org/10.1038/s41598-021-91888-8 |
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