Interfacial coupling effect of Cr_2O_3 on the magnetic properties of Fe_72Ga_28 thin films
Here it is investigated the effect of the antiferromagnet Cr_2O_3 on the magnetic properties of ferromagnetic Fe_72Ga_28 thin films. Sputtered Fe_72Ga_28 layers have their magnetization in the sample plane with a magnetic fluctuation that gives rise to magnetic ripple. In order to turn its magnetiza...
| Autores: | , , , |
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| Tipo de recurso: | artículo |
| Fecha de publicación: | 2021 |
| País: | España |
| Institución: | Universidad Complutense de Madrid (UCM) |
| Repositorio: | Docta Complutense |
| Idioma: | inglés |
| OAI Identifier: | oai:docta.ucm.es:20.500.14352/8418 |
| Acceso en línea: | https://hdl.handle.net/20.500.14352/8418 |
| Access Level: | acceso abierto |
| Palabra clave: | 538.9 Random-field model Exchange bias Fe-Ga Anisotropy Surface Física de materiales Física del estado sólido 2211 Física del Estado Sólido |
| Sumario: | Here it is investigated the effect of the antiferromagnet Cr_2O_3 on the magnetic properties of ferromagnetic Fe_72Ga_28 thin films. Sputtered Fe_72Ga_28 layers have their magnetization in the sample plane with a magnetic fluctuation that gives rise to magnetic ripple. In order to turn its magnetization into the out of plane (OOP) direction, it has been magnetically coupled with Cr_2O_3 that has magnetic moments along the c-axis, that is the perpendicular direction when properly aligned. Cr2O3 has been obtained from Cr oxidation, whereas Fe_72Ga_28 has been deposited on top of it by sputtering in the ballistic regime. Although a uniaxial in-plane magnetic anisotropy is expected for Fe_72Ga_28 thickness above 100 nm, the interfacial coupling with Cr2O3 prevents this anisotropy. The formation of stripe domains in Fe_72Ga_28 above a critical thickness reveals the enhancement of the out of plane component of the Fe_72Ga_28 magnetization with respect to uncoupled layers. Due to the interface coupling, the Fe72Ga28 magnetization turns into the out-of-plane direction as its thickness is gradually reduced, and a perpendicular magnetic anisotropy of 3.10^6 erg.cm^(-3) is inferred from experimental results. Eventually, the coupling between Cr_2O_3 and Fe_72Ga_28 promotes an exchange-bias effect that has been well fitted by means of the random field model. |
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