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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Main Authors: Yoshihisa Kosugi, Masato Goto, Zhenhong Tan, Daisuke Kan, Masahiko Isobe, Kenji Yoshii, Masaichiro Mizumaki, Asaya Fujita, Hidenori Takagi, Yuichi Shimakawa
Format: Article
Language:English
Published: Nature Publishing Group 2021-06-01
Series:Scientific Reports
Online Access:https://doi.org/10.1038/s41598-021-91888-8
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spelling 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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