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Antiferromagnetic MnO nanoparticles with ferrimagnetic Mn3 O4 shells: Doubly inverted core-shell system

Cited 132 time in Web of Science Cited 137 time in Scopus
Authors

Berkowitz, A. E.; Rodriguez, G. F.; Hong, J. I.; An, K.; Hyeon, T.; Agarwal, N.; Smith, D. J.; Fullerton, E. E.

Issue Date
2008-01
Publisher
American Physical Society
Citation
Physical Review B - Condensed Matter and Materials Physics, Vol.77 No.2, p. 024403
Abstract
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.
ISSN
1098-0121
URI
https://hdl.handle.net/10371/165854
DOI
https://doi.org/10.1103/PhysRevB.77.024403
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