Academic Journal
Magnetic properties and magnetocaloric effects of RNiSi2 (R= Gd, Dy, Ho, Er, Tm) compounds
العنوان: | Magnetic properties and magnetocaloric effects of RNiSi2 (R= Gd, Dy, Ho, Er, Tm) compounds |
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المؤلفون: | Zhang, B., Zheng, X. Q., Zhang, Y., Zhao, X., Xiong, J. F., Zuo, S. L., Liu, D., Zhao, T. Y., Hu, F. X., Shen, B. G. |
المساهمون: | Knowledge Innovation Project of the Chinese Academy of Sciences, National Key Research Program of China, National Natural Science Foundation of China |
المصدر: | AIP Advances ; volume 8, issue 5 ; ISSN 2158-3226 |
بيانات النشر: | AIP Publishing |
سنة النشر: | 2018 |
الوصف: | Orthorhombic CeNiSi2-type polycrystalline RNiSi2 (R=Gd, Dy, Ho, Er, Tm) compounds were synthesized and the magnetic and magnetocaloric properties were investigated in detail. The transition temperatures of RNiSi2 compounds are all in a very low temperature range (<30 K). As temperature increases, all of the compounds undergo an AFM to PM transition (GdNiSi2 at 18 K, DyNiSi2 at 25 K, HoNiSi2 at 10.5 K, ErNiSi2 at 3 K and TmNiSi2 at 3.5 K, respectively). ErNiSi2 compound shows the largest (ΔSM)max (maximal magnetic entropy change) among these compounds. The value of (ΔSM)max is 27.9 J/kgK under a field change of 0-5 T, which indicates that ErNiSi2 compound is very competitive for practical applications in low-temperature magnetic refrigeration in the future. DyNiSi2 compound shows large inverse MCE (almost equals to the normal MCE) below the TN which results from metamagenitic transition under magnetic field. Considering of the normal and inverse MCE, DyNiSi2 compound also has potential applications in low-temperature multistage refrigeration. |
نوع الوثيقة: | article in journal/newspaper |
اللغة: | English |
DOI: | 10.1063/1.5007018 |
DOI: | 10.1063/1.5007018/12983650/056423_1_online.pdf |
الاتاحة: | http://dx.doi.org/10.1063/1.5007018 https://pubs.aip.org/aip/adv/article-pdf/doi/10.1063/1.5007018/12983650/056423_1_online.pdf |
رقم الانضمام: | edsbas.E38D4311 |
قاعدة البيانات: | BASE |
DOI: | 10.1063/1.5007018 |
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