Magnetic anisotropy and layer-selective magnetometry of Cu/Co/Ni/Cu/Si (001)
Perpendicular magnetic anisotropy (PMA) up to 6.15±1.25 angstroms Co thickness is found for ferromagnetically coupled epitaxial Co/60 angstroms Ni/Cu/Si(0 0 1) structures. Polarized neutron reflection measurements on a Cu/9 angstroms Co/Ni/Cu(0 0 1) structure yield almost bulk like magnetic moments...
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Elsevier
1999
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_version_ | 1797067947490934784 |
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author | Lauhoff, G Lee, J Bland, J Langridge, S Penfold, J |
author_facet | Lauhoff, G Lee, J Bland, J Langridge, S Penfold, J |
author_sort | Lauhoff, G |
collection | OXFORD |
description | Perpendicular magnetic anisotropy (PMA) up to 6.15±1.25 angstroms Co thickness is found for ferromagnetically coupled epitaxial Co/60 angstroms Ni/Cu/Si(0 0 1) structures. Polarized neutron reflection measurements on a Cu/9 angstroms Co/Ni/Cu(0 0 1) structure yield almost bulk like magnetic moments at room-temperature of 1.70±0.20 μB and 0.57±0.05 μB for Co and Ni, respectively. Magneto-optic Kerr effect measurements show that the uniaxial Co volume anisotropy is entirely attributed to the Co shape anisotropy due to an absence of strain in the Co film. |
first_indexed | 2024-03-06T22:03:42Z |
format | Conference item |
id | oxford-uuid:4f70b521-7794-41d0-930b-e81db63dd419 |
institution | University of Oxford |
last_indexed | 2024-03-06T22:03:42Z |
publishDate | 1999 |
publisher | Elsevier |
record_format | dspace |
spelling | oxford-uuid:4f70b521-7794-41d0-930b-e81db63dd4192022-03-26T16:07:14ZMagnetic anisotropy and layer-selective magnetometry of Cu/Co/Ni/Cu/Si (001)Conference itemhttp://purl.org/coar/resource_type/c_5794uuid:4f70b521-7794-41d0-930b-e81db63dd419Symplectic Elements at OxfordElsevier1999Lauhoff, GLee, JBland, JLangridge, SPenfold, JPerpendicular magnetic anisotropy (PMA) up to 6.15±1.25 angstroms Co thickness is found for ferromagnetically coupled epitaxial Co/60 angstroms Ni/Cu/Si(0 0 1) structures. Polarized neutron reflection measurements on a Cu/9 angstroms Co/Ni/Cu(0 0 1) structure yield almost bulk like magnetic moments at room-temperature of 1.70±0.20 μB and 0.57±0.05 μB for Co and Ni, respectively. Magneto-optic Kerr effect measurements show that the uniaxial Co volume anisotropy is entirely attributed to the Co shape anisotropy due to an absence of strain in the Co film. |
spellingShingle | Lauhoff, G Lee, J Bland, J Langridge, S Penfold, J Magnetic anisotropy and layer-selective magnetometry of Cu/Co/Ni/Cu/Si (001) |
title | Magnetic anisotropy and layer-selective magnetometry of Cu/Co/Ni/Cu/Si (001) |
title_full | Magnetic anisotropy and layer-selective magnetometry of Cu/Co/Ni/Cu/Si (001) |
title_fullStr | Magnetic anisotropy and layer-selective magnetometry of Cu/Co/Ni/Cu/Si (001) |
title_full_unstemmed | Magnetic anisotropy and layer-selective magnetometry of Cu/Co/Ni/Cu/Si (001) |
title_short | Magnetic anisotropy and layer-selective magnetometry of Cu/Co/Ni/Cu/Si (001) |
title_sort | magnetic anisotropy and layer selective magnetometry of cu co ni cu si 001 |
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