Magnetization reversal in weak ferrimagnets and canted antiferromagnets

被引:18
作者
Kageyama, H
Khomskii, DI
Levitin, RZ
Markina, MM
Okuyama, T
Uchimoto, T
Vasil'ev, AN [2 ]
机构
[1] Univ Groningen, Ctr Mat Sci, Solid State Phys Lab, NL-9747 AG Groningen, Netherlands
[2] Moscow MV Lomonosov State Univ, Fac Phys, Moscow 119899, Russia
[3] Univ Tokyo, Inst Solid State Phys, Mat Design & Characterizat Lab, Kashiwa, Chiba 2778581, Japan
[4] Tohoku Univ, Inst Fluid Sci, Aoba Ku, Sendai, Miyagi 9808577, Japan
关键词
weak ferrimagnetism; compensation point; magnetization reversal; Ni(HCOO)(2)center dot 2H(2)O;
D O I
10.1016/S0304-8853(03)00076-3
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
In some ferrimagnets the total magnetization vanishes at a certain compensation temperature T*. In weak magnetic fields, the magnetization can change sign at T* (the magnetization reversal). Much rarer is observation of ferrimagnetic-like response in canted anti ferromagnets, where the weak ferromagnetic moment is due to the tilting of the sublattice magnetizations. The latter phenomenon was observed in nickel (II) formate dihydrate Ni(HCOO)(2). 2H(2)O. The observed weak magnetic moment increases initially below T-N = 15.5 K, equals zero at T* = 8.5 K and increases again at lowering temperature. The sign of the low-field magnetization at any given temperature is determined by the sample's magnetic prehistory and the signs are opposite to each other at T < T* and T* < T < T-N. (C) 2003 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:445 / 451
页数:7
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