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An, Kwangjin
Advanced Nanocatalysis Lab.
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Antiferromagnetic MnO nanoparticles with ferrimagnetic Mn3O4 shells: Doubly inverted core-shell system

Author(s)
Berkowiz, AERodiguez, GFHong, JIAn, KwangjinHyeon, TAgarwal, NSmith, DJFullerton, EE
Issued Date
2008-01
DOI
10.1103/PhysRevB.77.024403
URI
https://scholarworks.unist.ac.kr/handle/201301/12888
Fulltext
http://journals.aps.org/prb/abstract/10.1103/PhysRevB.77.024403
Citation
PHYSICAL REVIEW B, v.77, no.2, pp.024403-1 - 024403-6
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.
Publisher
AMER PHYSICAL SOC
ISSN
1098-0121

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