Exchange bias training effect in IrMn-layer/ferromagnetic-ribbon heterostructures probed with magnetoimpedance
The exchange-bias training effect in IrMn-layer/ferromagnetic-ribbon heterostructure is studied by performing magnetoimpedance (MI) measurements. Asymmetric, hysteretic and single peak behavior of the MI response and a shift in the MI peak to zero fields accompanied by 52% increase in MI has been de...
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Published in | arXiv.org |
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Main Authors | , , , |
Format | Paper Journal Article |
Language | English |
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Cornell University Library, arXiv.org
20.12.2019
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ISSN | 2331-8422 |
DOI | 10.48550/arxiv.1912.10032 |
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Abstract | The exchange-bias training effect in IrMn-layer/ferromagnetic-ribbon heterostructure is studied by performing magnetoimpedance (MI) measurements. Asymmetric, hysteretic and single peak behavior of the MI response and a shift in the MI peak to zero fields accompanied by 52% increase in MI has been detected as the signature of the exchange bias (EB) and training effect (TE), respectively. Also, during the consecutive filed sweep of MI response, both EB field and the degree of asymmetry of MI decrease that is another reason for existence of TE in our sample. The analysis of the magneto-optical Kerr effect (MOKE) and MI behavior establish that Hoffmann s model (Phys. Rev. Lett. 93, 097203 (2004)) is a good description of our experimental data, due to the existence of a strong single cycle TE in our IrMn-layer/ferromagnetic-ribbon system. |
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AbstractList | The exchange-bias training effect in IrMn-layer/ferromagnetic-ribbon
heterostructure is studied by performing magnetoimpedance (MI) measurements.
Asymmetric, hysteretic and single peak behavior of the MI response and a shift
in the MI peak to zero fields accompanied by 52% increase in MI has been
detected as the signature of the exchange bias (EB) and training effect (TE),
respectively. Also, during the consecutive filed sweep of MI response, both EB
field and the degree of asymmetry of MI decrease that is another reason for
existence of TE in our sample. The analysis of the magneto-optical Kerr effect
(MOKE) and MI behavior establish that Hoffmann s model (Phys. Rev. Lett. 93,
097203 (2004)) is a good description of our experimental data, due to the
existence of a strong single cycle TE in our IrMn-layer/ferromagnetic-ribbon
system. The exchange-bias training effect in IrMn-layer/ferromagnetic-ribbon heterostructure is studied by performing magnetoimpedance (MI) measurements. Asymmetric, hysteretic and single peak behavior of the MI response and a shift in the MI peak to zero fields accompanied by 52% increase in MI has been detected as the signature of the exchange bias (EB) and training effect (TE), respectively. Also, during the consecutive filed sweep of MI response, both EB field and the degree of asymmetry of MI decrease that is another reason for existence of TE in our sample. The analysis of the magneto-optical Kerr effect (MOKE) and MI behavior establish that Hoffmann s model (Phys. Rev. Lett. 93, 097203 (2004)) is a good description of our experimental data, due to the existence of a strong single cycle TE in our IrMn-layer/ferromagnetic-ribbon system. |
Author | Mohseni, Majid Hajiali, Mohammadreza Mohammad Javad Kamali Ashtiani Jamilpanah, Loghman |
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BackLink | https://doi.org/10.48550/arXiv.1912.10032$$DView paper in arXiv https://doi.org/10.1016/j.spmi.2020.106710$$DView published paper (Access to full text may be restricted) |
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Snippet | The exchange-bias training effect in IrMn-layer/ferromagnetic-ribbon heterostructure is studied by performing magnetoimpedance (MI) measurements. Asymmetric,... The exchange-bias training effect in IrMn-layer/ferromagnetic-ribbon heterostructure is studied by performing magnetoimpedance (MI) measurements. Asymmetric,... |
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SubjectTerms | Asymmetry Bias Exchanging Ferromagnetism Heterostructures Kerr magnetooptical effect Magnetoimpedance Physics - Applied Physics Physics - Mesoscale and Nanoscale Physics Training |
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Title | Exchange bias training effect in IrMn-layer/ferromagnetic-ribbon heterostructures probed with magnetoimpedance |
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