A cobalt-copper top spin valve was prepared by thermal evaporation of a stack of ferromagnetic thin films separated by thin layers of the diamagnetic metal, with a cap layer containing an antiferromagnetic AFM exchange-biasing material. A nonconventional top AFM layer was used, in order to optimize the multilayer roughness and to avoid electrical interference with metallic layers; it consists of a composite material easily processed by means of optical lithography, basically a polymeric matrix composite with a dispersion of nickel oxide microparticles. Magnetization and magnetoresistance measurements were performed from 4 to 300 K. The measurements of both quantities indicate random pinning action of the top AFM layer, resulting in a small exchange-bias field and in asymmetric magnetization and magnetoresistance curves. A simple model explains the observed physical effects.
Thermally evaporated Cu-Co top spin valve with random exchange bias / Chiolerio, Alessandro; Allia, PAOLO MARIA EUGENIO ICILIO; A., Chiodoni; Pirri, Candido; F., Celegato; M., Coisson. - In: JOURNAL OF APPLIED PHYSICS. - ISSN 0021-8979. - 101:12(2007). [10.1063/1.2749289]
Thermally evaporated Cu-Co top spin valve with random exchange bias
CHIOLERIO, ALESSANDRO;ALLIA, PAOLO MARIA EUGENIO ICILIO;PIRRI, Candido;
2007
Abstract
A cobalt-copper top spin valve was prepared by thermal evaporation of a stack of ferromagnetic thin films separated by thin layers of the diamagnetic metal, with a cap layer containing an antiferromagnetic AFM exchange-biasing material. A nonconventional top AFM layer was used, in order to optimize the multilayer roughness and to avoid electrical interference with metallic layers; it consists of a composite material easily processed by means of optical lithography, basically a polymeric matrix composite with a dispersion of nickel oxide microparticles. Magnetization and magnetoresistance measurements were performed from 4 to 300 K. The measurements of both quantities indicate random pinning action of the top AFM layer, resulting in a small exchange-bias field and in asymmetric magnetization and magnetoresistance curves. A simple model explains the observed physical effects.File | Dimensione | Formato | |
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https://hdl.handle.net/11583/1648845
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