Unveiling the different physical origins of magnetic anisotropy and magnetoelasticity in ga-rich fega thin films
The aim of this work is to clarify how in-plane magnetic anisotropy and magnetoelasticity depend on the thickness of Ga-rich FeGa layers. Samples with an Fe72Ga28 composition were grown by sputtering in the ballistic regime in oblique incidence. Although for these growth conditions uniaxial magnetic...
| Autores: | ; ; ; ; |
|---|---|
| Tipo de documento: | Artículo |
| Fecha de publicación: | 2020 |
| País: | España |
| Institución: | Universidad Complutense de Madrid (UCM) |
| Repositorio: | Docta Complutense |
| Lenguaje: | Inglés |
| OAI Identifier: | oai:docta.ucm.es:20.500.14352/6105 |
| Acceso en línea: | https://hdl.handle.net/20.500.14352/6105 |
| Nivel de acceso: | Acceso abierto |
| Palabra clave: | 538.9 Magnetostriction Stress Chemistry Physical Nanoscience Nanotechnology Materials Science Multidisciplinary Física de materiales Física del estado sólido 2211 Física del Estado Sólido |
| _version_ | 1878735021900038144 |
|---|---|
| author | Bartolomé, Pablo |
| author2 | Begué, A Muñoz Noval, Álvaro Ciria, M. Ranchal Sánchez, Rocío |
| author2_role | author author author author |
| author_browse | Bartolomé, Pablo Begué, A Ciria, M. Muñoz Noval, Álvaro Ranchal Sánchez, Rocío |
| author_facet | Bartolomé, Pablo Begué, A Muñoz Noval, Álvaro Ciria, M. Ranchal Sánchez, Rocío |
| author_role | author |
| collection | Docta Complutense |
| description | The aim of this work is to clarify how in-plane magnetic anisotropy and magnetoelasticity depend on the thickness of Ga-rich FeGa layers. Samples with an Fe72Ga28 composition were grown by sputtering in the ballistic regime in oblique incidence. Although for these growth conditions uniaxial magnetic anisotropy could be expected, in-plane anisotropy is only present when the sample thickness is above 100 nm. By means of differential X-ray absorption spectroscopy, we have determined the influence of both Ga pairs and tetragonal cell distortion on the evolution of the magnetic anisotropy with the increase of FeGa thickness. On the other hand, we have used the cantilever beam technique with capacitive detection to also determine the evolution of the magnetoelastic parameters with the thickness increase. In this case, experimental results can be understood considering the grain distribution. Therefore, the different physical origins for anisotropy and magnetoelasticity open up the possibility to independently tune these two characteristics in Ga-rich FeGa films. |
| eu_rights_str_mv | openAccess |
| format | article |
| id | ES_746d0bbc97568c2d6e015d9d54657316 |
| institution | Universidad Complutense de Madrid (UCM) |
| instname_str | Universidad Complutense de Madrid (UCM) |
| language | eng |
| network_acronym_str | ES |
| network_name_str | España |
| oai_identifier_str | oai:docta.ucm.es:20.500.14352/6105 |
| publishDate | 2020 |
| publishDateSort | 2020 |
| publisher | American Chemical Society |
| publisherStr | American Chemical Society |
| reponame_str | Docta Complutense |
| spelling | Unveiling the different physical origins of magnetic anisotropy and magnetoelasticity in ga-rich fega thin films Bartolomé, Pablo Begué, A Muñoz Noval, Álvaro Ciria, M. Ranchal Sánchez, Rocío 538.9 Magnetostriction Stress Chemistry Physical Nanoscience Nanotechnology Materials Science Multidisciplinary Física de materiales Física del estado sólido 2211 Física del Estado Sólido The aim of this work is to clarify how in-plane magnetic anisotropy and magnetoelasticity depend on the thickness of Ga-rich FeGa layers. Samples with an Fe72Ga28 composition were grown by sputtering in the ballistic regime in oblique incidence. Although for these growth conditions uniaxial magnetic anisotropy could be expected, in-plane anisotropy is only present when the sample thickness is above 100 nm. By means of differential X-ray absorption spectroscopy, we have determined the influence of both Ga pairs and tetragonal cell distortion on the evolution of the magnetic anisotropy with the increase of FeGa thickness. On the other hand, we have used the cantilever beam technique with capacitive detection to also determine the evolution of the magnetoelastic parameters with the thickness increase. In this case, experimental results can be understood considering the grain distribution. Therefore, the different physical origins for anisotropy and magnetoelasticity open up the possibility to independently tune these two characteristics in Ga-rich FeGa films. American Chemical Society https://hdl.handle.net/20.500.14352/6105 |
| spellingShingle | Unveiling the different physical origins of magnetic anisotropy and magnetoelasticity in ga-rich fega thin films Bartolomé, Pablo 538.9 Magnetostriction Stress Chemistry Physical Nanoscience Nanotechnology Materials Science Multidisciplinary Física de materiales Física del estado sólido 2211 Física del Estado Sólido |
| title | Unveiling the different physical origins of magnetic anisotropy and magnetoelasticity in ga-rich fega thin films |
| title_full | Unveiling the different physical origins of magnetic anisotropy and magnetoelasticity in ga-rich fega thin films |
| title_fullStr | Unveiling the different physical origins of magnetic anisotropy and magnetoelasticity in ga-rich fega thin films |
| title_full_unstemmed | Unveiling the different physical origins of magnetic anisotropy and magnetoelasticity in ga-rich fega thin films |
| title_short | Unveiling the different physical origins of magnetic anisotropy and magnetoelasticity in ga-rich fega thin films |
| title_sort | Unveiling the different physical origins of magnetic anisotropy and magnetoelasticity in ga-rich fega thin films |
| topic | 538.9 Magnetostriction Stress Chemistry Physical Nanoscience Nanotechnology Materials Science Multidisciplinary Física de materiales Física del estado sólido 2211 Física del Estado Sólido |
| topic_facet | 538.9 Magnetostriction Stress Chemistry Physical Nanoscience Nanotechnology Materials Science Multidisciplinary Física de materiales Física del estado sólido 2211 Física del Estado Sólido |
| url | https://hdl.handle.net/20.500.14352/6105 |