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迈向亚铁磁性理论:II.

Towards the theory of ferrimagnetism: II.

作者信息

Karchev Naoum

机构信息

Department of Physics, University of Sofia, 1126 Sofia, Bulgaria.

出版信息

J Phys Condens Matter. 2009 May 27;21(21):216003. doi: 10.1088/0953-8984/21/21/216003. Epub 2009 Apr 29.

Abstract

The present paper is a sequel to the paper by Karchev (2008 J. Phys.: Condens. Matter 20 325219). A two-sublattice ferrimagnet, with spin- s(1) operators S(1i) at the sublattice A site and spin-s(2) operators S(2i) at the sublattice B site, is considered. Renormalized spin-wave theory, which accounts for the magnon-magnon interaction, and its extension are developed to describe the two ferrimagnetic phases (0,T()) and (T(),T(N)) in the system, and to calculate the magnetization as a function of temperature. The influence of the parameters in the theory on the characteristic temperatures T(N) and T() is studied. It is shown that, increasing the inter-sublattice exchange interaction, the ratio T(N)/T()>1 decreases approaching one, and above some critical value of the exchange constant there is only one phase T(N) = T(), and the magnetization-temperature curve has the typical Curie-Weiss profile. When the intra-exchange constant of the sublattice with stronger intra-exchange interaction increases the Néel temperature increases while T() remains unchanged. Finally, when the magnetic order of the sublattice with smaller magnetic order decreases, T(*) decreases. The theoretical predictions are utilized to interpret the experimentally measured magnetization-temperature curves.

摘要

本文是卡尔切夫(2008年,《物理学杂志:凝聚态》20 325219)论文的续篇。考虑一个双亚晶格亚铁磁体,在亚晶格A位具有自旋 - s(1) 算符S(1i),在亚晶格B位具有自旋 - s(2) 算符S(2i)。发展了考虑磁振子 - 磁振子相互作用的重整化自旋波理论及其扩展,以描述系统中的两个亚铁磁相(0,T())和(T(),T(N)),并计算磁化强度随温度的变化。研究了该理论中的参数对特征温度T(N)和T()的影响。结果表明,增加亚晶格间交换相互作用时,T(N)/T()>1的比值减小并趋近于1,并且在交换常数的某个临界值以上,只有一个相T(N) = T(),且磁化强度 - 温度曲线具有典型的居里 - 外斯分布。当具有较强内部交换相互作用的亚晶格的内部交换常数增加时,奈尔温度升高而T()保持不变。最后,当磁有序较小的亚晶格的磁有序降低时,T(*)减小。理论预测被用于解释实验测量的磁化强度 - 温度曲线。

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