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Eu_(0.9)M_(0.1)TiO_3(M=Ca,Sr,Ba,La,Ce,Sm)的磁性和磁热效应
引用本文:郝志红,王海英,张荃,莫兆军.Eu_(0.9)M_(0.1)TiO_3(M=Ca,Sr,Ba,La,Ce,Sm)的磁性和磁热效应[J].物理学报,2018,67(24):247502-247502.
作者姓名:郝志红  王海英  张荃  莫兆军
作者单位:1. 天津职业大学眼视光工程学院, 天津 300410;2. 天津理工大学材料科学与工程学院, 材料物理研究所, 天津 300384
基金项目:天津职业大学科学研究基金(批准号:20161102)和天津市教委自然科学基金(批准号:2017KJ247)资助的课题.
摘    要:EuTi0_3是直接带隙半导体材料,在液氦温度附近呈现反铁磁性,且具有较大的磁熵变,但是当其转变为铁磁性时,可以有效提高低磁场下的磁熵变.本文通过元素替代,研究晶格常数的变化和电子掺杂对磁性和磁热效应的影响.实验采用溶胶凝胶法制备EuTiO_3和Eu_(0.9)M_(0.1)TiO_3 (M=Ca, Sr, Ba, La, Ce, Sm)系列样品.结果表明:大离子半径的碱土金属离子替代提高了铁磁性耦合,有利于提高低磁场下的磁热效应.电子掺杂可以抑制其反铁磁性耦合从而使其表现为铁磁性.当大离子半径的稀土La和Ce离子替代Eu离子时,既增大了晶格常数也实现了电子掺杂,表现出较强的铁磁性.在1 T的磁场变化下,Eu_(0.9)La_(0.1)TiO_3和Eu_(0.9)Ce_(0.1)TiO_3的最大磁熵变分别为10.8和11 J/(kg·K),均大于EuTi0_3的9.8 J/(kg·K);制冷能力分别为39.3和51.8 J/kg,相对于EuTi0_3也有所提高.

关 键 词:磁热效应  磁熵变  磁相变
收稿时间:2018-09-21

Magnetic and magnetocaloric effects of Eu0.9M0.1TiO3 (M=Ca,Sr, Ba,La, Ce,Sm) compounds
Hao Zhi-Hong,Wang Hai-Ying,Zhang Quan,Mo Zhao-Jun.Magnetic and magnetocaloric effects of Eu0.9M0.1TiO3 (M=Ca,Sr, Ba,La, Ce,Sm) compounds[J].Acta Physica Sinica,2018,67(24):247502-247502.
Authors:Hao Zhi-Hong  Wang Hai-Ying  Zhang Quan  Mo Zhao-Jun
Institution:1. School of Optometry, Tianjin Vocational Institute, Tianjin 300410, China;2. School of Material Science and Engineering, Institute of Material Physics, Tianjin University of Technology, Tianjin 300384, China
Abstract:EuTiO3 is a direct band-gap semiconductor material and exhibits antiferromagnetism with large magnetic entropy change around the liquid helium temperature. The ferromagnetic state can be changed into antiferromagnetic state through lattice constant change and electron doping by element substitution due to strong spin-lattice coupling coexistence of ferromagnetic coupling, and antiferromagnetic coupling. The values of magnetic entropy change can be effectively improved under low magnetic field change after changing into ferromagnetism. Samples of EuTiO3 and Eu0.9M0.1TiO3 (M=Ca, Sr, Ba, La, Ce, Sm) are prepared by the sol gel method. The Eu0.9Ca0.1TiO3 exhibits the antiferromagnetism due to similar ion radius. The ferromagnetic coupling between Eu0.9Sr0.1TiO3 and Eu0.9Ba0.1TiO3 is enhanced, for alkaline earth metal (Sr and Ba) has larger ion radius, which is beneficial to improving the magnetocaloric effect under low magnetic field. Electron doping can inhibit the antiferromagnetic coupling because the extra carrier may occupy the Ti 3d and reduce the hybridization of Eu 4f-Ti 3d-Eu 4f. When the electron doping concentration is greater than 10%, the spin polarization rate of Ti 3d state on the Fermi surface is negative, resulting in the transition from antiferromagnetic to ferromagnetic state. When the Eu ions are replaced with the Sm ions (Sm ion radius is similar to Eu ion radius), the ferromagnetic coupling is enhanced. However, when the Eu ions are replaced with the La or Ce ions, the samples show strong ferromagnetism, for the lattice constant and electron doping are increased. A giant reversible magnetocaloric effect and large refrigerant capacity for each of Eu0.9M0.1TiO3 (M=Sr, Ba, La, Ce) compounds are observed. Under the magnetic field change of 1 T, the values of maximum magnetic entropy change and refrigeration capacity are 9.8 J/(kg·K) and 36.6 J/kg for Eu0.9Sr0.1TiO3, and 10 J/(kg·K) and 45.1 J/kg for Eu0.9Ba0.1TiO3. The values of maximum magnetic entropy change of Eu0.9La0.1TiO3 and Eu0.9Ce0.1TiO3 are 10.8 J/(kg·K) and 11 J/(kg·K), respectively, which are larger than that of EuTiO3 (9.8 J/(kg·K)). The values of refrigeration capacity are 39.3 J/kg and 51.8 J/kg, which are also improved compared with those of EuTiO3. In a word, the results suggest that these compounds could be considered as good candidates for low-temperature and low-field magnetic refrigerant.
Keywords:magnetocaloric effect  magnetic entropy change  magnetic phase transition
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