Magnetic compensation, field-dependent magnetization reversal, and complex magnetic ordering in Co2TiO4

被引:53
作者
Nayak, S. [1 ]
Thota, S. [1 ]
Joshi, D. C. [1 ]
Krautz, M. [2 ]
Waske, A. [2 ]
Behler, A. [2 ]
Eckert, J. [3 ,4 ]
Sarkar, T. [5 ]
Andersson, M. S. [5 ]
Mathieu, R. [5 ]
Narang, V. [6 ]
Seehra, M. S. [6 ]
机构
[1] Indian Inst Technol, Dept Phys, Gauhati 781039, Assam, India
[2] IFW Dresden, Inst Complex Mat, D-01171 Dresden, Germany
[3] Austrian Acad Sci, Erich Schmid Inst Mat Sci, A-8700 Leoben, Austria
[4] Univ Leoben, Dept Mat Phys, A-8700 Leoben, Austria
[5] Uppsala Univ, Dept Engn Sci, SE-75121 Uppsala, Sweden
[6] W Virginia Univ, Dept Phys & Astron, Morgantown, WV 26506 USA
来源
PHYSICAL REVIEW B | 2015年 / 92卷 / 21期
基金
瑞典研究理事会;
关键词
SPIN-GLASS BEHAVIOR; EXCHANGE CONSTANTS; SURFACE; FERRITES; SPECTROSCOPY; COMPOUND; OXIDES; OXYGEN; FILMS;
D O I
10.1103/PhysRevB.92.214434
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The complex nature of magnetic ordering in the spinel Co2TiO4 is investigated by analyzing the temperature and magnetic field dependence of its magnetization (M), specific heat (C-p), and ac magnetic susceptibilities chi' and chi ''. X-ray diffraction of the sample synthesized by the solid-state reaction route confirmed the spinel structure whereas x-ray photoelectron spectroscopy shows its electronic structure to be Co2TiO4 = [Co2+][Co3+ Ti3+]O-4. From analysis of the temperature dependence of the dc paramagnetic susceptibility, the magnetic moments mu(A) = 3.87 mu(B) and mu(B) = 5.19 mu B on the A and B sites are determined with mu(B) in turn yielding mu(Ti3+) = 1.73 mu(B) and mu(Co3+) = 4.89 mu(B). Analysis of the dc and ac susceptibilities combined with the weak anomalies observed in the C-p vs T data shows the existence of a quasi-long-range ferrimagnetic state below T-N similar to 47.8K and a compensation temperature T-comp similar to 32 K, the latter characterized by sign reversal of magnetization with its magnitude depending on the applied magnetic field and the cooling protocol. Analysis of the temperature dependence of M (field cooled) and M (zero field cooled) data and the hysteresis loop parameters is interpreted in terms of large spin clusters. These results in Co2TiO4, significantly different from those reported recently in isostructural Co2SnO4 = [Co2+][Co2+ Sn4+]O-4, warrant further investigations of its magnetic structure using neutron diffraction.
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页数:10
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