Antiferromagnetic MnO nanoparticles with ferrimagnetic Mn3O4 shells:: Doubly inverted core-shell system

被引:135
作者
Berkowitz, A. E. [1 ,2 ]
Rodriguez, G. F. [1 ]
Hong, J. I. [2 ]
An, K. [3 ]
Hyeon, T. [3 ]
Agarwal, N. [4 ,5 ]
Smith, D. J. [4 ,5 ]
Fullerton, E. E. [2 ,6 ]
机构
[1] Univ Calif San Diego, Dept Phys, La Jolla, CA 92093 USA
[2] Univ Calif San Diego, Ctr Magnet Recording Res, La Jolla, CA 92093 USA
[3] Seoul Natl Univ, Natl Creat Res Initiat Ctr Oxide Nanocrystalline, Seoul 151744, South Korea
[4] Arizona State Univ, Sch Mat, Tempe, AZ 85287 USA
[5] Arizona State Univ, Dept Phys, Tempe, AZ 85287 USA
[6] Univ Calif San Diego, Dept Elect & Comp Engn, La Jolla, CA 92093 USA
来源
PHYSICAL REVIEW B | 2008年 / 77卷 / 02期
关键词
D O I
10.1103/PhysRevB.77.024403
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We report the magnetic and microstructural properties of antiferromagnetic MnO nanoparticles with shells of ferrimagnetic Mn(3)O(4), which is opposite the usual arrangement of antiferromagnetically coated ferromagnetic nanoparticles. In addition, the antiferromagnetic MnO cores order at much higher temperature (T(N)=118 K) than the ferrimagnetic Mn(3)O(4) shells (T(C)=43 K)-another reversal of the usual situation. The single crystal MnO cores, with rocksalt structure, are crystallographically aligned with the tetragonal spinel structure of the Mn(3)O(4) shells. Particles field cooled in 50 kOe have large coercive force and exchange bias below T(C), e.g., 5800 and 2950 Oe, respectively, at 5 K. The spontaneous magnetization at T(C)(Mn(3)O(4)) is similar to 20% of its value at 5 K, and remains finite for more than 20 K above T(C)(Mn(3)O(4)). Hysteresis with exchange bias is present in this anomalous region. The MnO cores with their uncompensated spins are responsible for the behavior above T(C)(Mn(3)O(4)). The MnO cores have a blocking temperature of 95 K, and the hysteresis and exchange bias above T(C)(Mn(3)O(4)) results from the switching of the MnO spin lattices by their uncompensated spins. Analysis of the thermoremanent magnetization and field cooling and/or zero field cooling in 50 kOe, and the dependence of exchange bias on the temperature at which the cooling field was applied support this model.
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页数:6
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