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软铁磁锰氧化物在室温下的大磁热熵变

Large magnetocaloric entropy change at room temperature in soft ferromagnetic manganites.

作者信息

Bouzidi Souhir, Gdaiem Mohamed Amara, Dhahri J, Hlil E K

机构信息

Laboratoire de la Matière Condensée et des Nanosciences, Département de Physique, Faculté des Sciences de Monastir Avenue de l'Environnement Monastir- 5019 Tunisia

Institut Néel, CNRS et Université Joseph Fourier BP 166 F-38042 Grenoble Cedex 9 France.

出版信息

RSC Adv. 2018 Dec 20;9(1):65-76. doi: 10.1039/c8ra09166h. eCollection 2018 Dec 19.

DOI:10.1039/c8ra09166h
PMID:35521566
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9059358/
Abstract

In this paper, LaCa Na MnO ( = 0.15 and 0.20) samples were prepared by the flux method. Crystallographic study revealed that the = 0.15 sample is characterized by the coexistence of a mixture of orthorhombic and rhombohedral structures with and 3̄ space groups, respectively. While, the = 0.20 sample crystallized in the rhombohedral structure with a 3̄ space group. Magnetic data, under a magnetic field of 0.05 T, indicated that our samples undergo a ferromagnetic (FM)-paramagnetic (PM) phase transition, on increasing the temperature. The magnetic field dependence of the magnetocaloric properties of LaCa Na MnO ( = 0.15 and 0.20) samples, with the second phase transition, was investigated. Near room temperature, the = 0.20 sample exhibited a large magnetic entropy change with maxima of 6.01 and 3.12 J kg K, respectively, under applied magnetic fields of 5 and 2 T. Also, the relative cooling power (RCP) was calculated. According to hysteresis cycles, for our studied samples, at 10 K a typical soft FM behavior with a low coercive field was observed. These results make our samples promising candidates for magnetic refrigerators, magnetic recording, and memory devices.

摘要

在本文中,采用助熔剂法制备了LaCaNaMnO(= 0.15和0.20)样品。晶体学研究表明,= 0.15的样品分别以正交晶系和菱面体结构的混合物共存为特征,其空间群分别为和3̄。而= 0.20的样品以具有3̄空间群的菱面体结构结晶。在0.05 T的磁场下,磁性数据表明,随着温度升高,我们的样品经历了铁磁(FM)-顺磁(PM)相变。研究了具有二级相变的LaCaNaMnO(= 0.15和0.20)样品磁热性能的磁场依赖性。在室温附近,= 0.20的样品在5 T和2 T的外加磁场下分别表现出6.01和3.12 J kg K的最大磁熵变化。此外,还计算了相对制冷量(RCP)。根据磁滞回线,对于我们研究的样品,在10 K时观察到具有低矫顽场的典型软铁磁行为。这些结果使我们的样品有望成为磁制冷机、磁记录和存储设备的候选材料。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/1ab256e692b9/c8ra09166h-f12.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/2a715905b152/c8ra09166h-f11.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/1ab256e692b9/c8ra09166h-f12.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/3e372c362500/c8ra09166h-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/af272f2022dc/c8ra09166h-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/50494f1f74b4/c8ra09166h-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/28136d01ca30/c8ra09166h-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/a4640c80e4f1/c8ra09166h-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/6b73dae7c952/c8ra09166h-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/220cb0a3bdf1/c8ra09166h-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/345749eebf20/c8ra09166h-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/4f2dd86eeec9/c8ra09166h-f9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/a803492fd529/c8ra09166h-f10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/2a715905b152/c8ra09166h-f11.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cfeb/9059358/1ab256e692b9/c8ra09166h-f12.jpg

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