期刊
JOURNAL OF MATERIALS SCIENCE & TECHNOLOGY
卷 98, 期 -, 页码 258-267出版社
JOURNAL MATER SCI TECHNOL
DOI: 10.1016/j.jmst.2021.04.067
关键词
Exchange bias; Ferromagnetic occupation fraction; Cooling field; Monte Carlo simulation
资金
- National Natural Science Foundation of China [11774045]
- Joint Research Fund Liaoning-Shenyang National Laboratory for Materials Science [20180510008]
- Fundamental Research Funds for Central Universities [N2102006]
This study investigates the influences of Co distribution in a CoFe2O4 matrix on magnetization behavior through a modified Monte Carlo method. Key findings include the temperature-dependent magnetization curves, the relationship between exchange bias field and Co/CFO interfacial coupling, and the control of exchange bias in nanosystems through interfacial randomization.
We conceive a model of nanosystems where Co is uniformly, randomly distributed into a CoFe2O4 (CFO) matrix, and study the influences of composition and CFO antiferromagnetic exchange coupling (J(CFO)) on zero-field-cooled/field-cooled magnetization behavior and the dependencies of exchange bias field (H-E) and coercivity (H-C) on Co/CFO interfacial coupling (J(Co/CFO)), composition and cooling field (H-FC), based on a modified Monte Carlo method. With decreasing temperature, the zero-field-cooled and field-cooled magnetization curves are overlapped and increasing initially, and then splitting at a critical temperature (T-P), below which the field-cooled magnetization continues increasing while the zero-field-cooled magnetization exhibits a peak and drops, indicating a magnetically frozen state. A larger J(CFO) induces an elevated T-P and a reduced magnetization, while the opposite results are obtained by a higher Co occupation fraction (P-Co). On the other hand, H-E is nonmonotonic with J(Co/CFO) and the peak decreases and shifts to a lower J(Co/CFO) value for a larger P-Co. H-C increases monotonically with increasing J(Co/CFO). Moreover, H-E is inversely proportional to P-Co when P-Co varies from 0.11 to 0.30, indicating the exchange bias is still an interfacial effect. Finally, for a nonzero J(CFO), H-E may be suppressed and accompanied by the recovery of H-C with increasing HFC. Otherwise, H-C for zero J(CFO) becomes high and insensitive to HFC. It is ascribed to the uniform contact between Co and CFO, leading to the Co magnetization reversal and the CFO magnetization precisely controlled by HFC. This work opens a new avenue to control the exchange bias in nanosystems through interfacial randomization. (C) 2022 Published by Elsevier Ltd on behalf of The editorial office of Journal of Materials Science & Technology.
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