Exchange bias and structural disorder in the nanogranular Ni/NiO system produced by ball milling and hydrogen reduction

被引:73
作者
Del Bianco, L. [1 ,2 ]
Boscherini, F. [1 ,2 ]
Fiorini, A. L. [1 ,2 ]
Tamisari, M. [3 ,4 ]
Spizzo, F. [3 ,4 ]
Antisari, M. Vittori [5 ]
Piscopiello, E. [6 ]
机构
[1] Univ Bologna, Dipartmento Fis, I-40127 Bologna, Italy
[2] CNISM, I-40127 Bologna, Italy
[3] Univ Ferrara, Dipartmento Fis, I-44100 Ferrara, Italy
[4] CNISM, I-44100 Ferrara, Italy
[5] Dipartimento FIM, ENEA, I-00123 Rome, Italy
[6] Dipartimento FIM, ENEA, I-72100 Brindisi, Italy
来源
PHYSICAL REVIEW B | 2008年 / 77卷 / 09期
关键词
D O I
10.1103/PhysRevB.77.094408
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The exchange bias effect has been studied in Ni/NiO nanogranular samples prepared by mechanical milling and partial hydrogen reduction of NiO; the Ni weight fraction varied between 4% and 69%. In this procedure, coarse-grained NiO powder has been ball milled in air for 20 h and subsequently subjected to annealing in H(2) (at a temperature ranging between 200 and 300 degrees C) to induce the formation of metallic Ni. The structural properties of the samples have been studied by x-ray diffraction, electron microscopy, and extended x-ray absorption fine structure. The magnetic properties have been extensively investigated by carrying out hysteresis loops and magnetization measurements in the 5 - 300 K temperature range, in zero-field-cooling and field-cooling conditions. The results indicate that both in the as-milled NiO powder and in the hydrogenated samples, the NiO phase is composed of nanocrystallites (having a mean size of similar to 20 nm, structurally and magnetically ordered) and of highly disordered regions. The samples with low Ni content (up to 15%) can be modeled as a collection of Ni nanoparticles (mean size of similar to 10 nm) dispersed in the NiO phase; with increasing Ni content, the Ni nanoparticles slightly increase in size and tend to arrange in agglomerates. In the Ni/NiO samples, the exchange field depends on the Ni amount, being maximum (similar to 600 Oe), at T=5 K, in the sample with 15% Ni. However, exchange bias is observed also in the as- milled NiO powder, despite the absence of metallic Ni. In all the samples, the exchange bias effect vanishes at similar to 200 K. We propose a mechanism for the phenomenon based on the key role of the disordered NiO component, showing a glassy magnetic character. The exchange bias effect is originated by the exchange interaction between the Ni ferromagnetic moments and the spins of the disordered NiO component (in the as- milled NiO powder, the existence of ferromagnetic moments has been connected to chemical inhomogeneities of the NiO phase). The thermal dependence of the exchange bias effect reflects the variation of the anisotropy of the NiO disordered component with temperature.
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页数:12
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