Metal/oxide composite films of Ni80Fe20/NixFe1-xO were prepared by dual
ion beam reactive deposition. The ion beam sputtered metal film is
bombarded during growth with an oxygen ion flux from a secondary ion source.
The oxide phase forms by the shallow ion implantation of oxygen followed
by supersaturation and precipitation. The oxide is dispersed in the
metal matrix as 10nm diameter crystallites. Varying the oxygen
ion flux can be used to control the oxide volume fraction. The oxide
has the rock salt structure but after vacuum annealing at 500C for 3 hours
the spinel ferrite, NiFe2O4 is formed. The metal/ferrite composites
show unusually large anisotropic magnetoresistance (AMR) up to 4.5% at
298K and 14% at 77K as compared to about 1% in the metal/rock salt oxide
mixtures. The largest values are observed when the volume fraction
of metal approaches the percolation limit. The latter observation
suggests that the enhanced anisotropic scattering is occurring at the metal/ferrite
interface. The AMR effect is caused by the spin-orbit interaction
that gives rise to a field dependent scattering cross-section. We
suggest that in the metal/ferrite nanocomposites, strongly anisotropic
scattering is associated with spin polarized oxygen p-orbitals in the ferrite
that is exchange coupled to the ferromagnetic metal. The p-orbitals
have a larger scattering cross-section because they have a larger radial
extent compared to the d-orbitals. The oxygen p-orbitals only contribute
to the AMR, however, when they are exchange coupled to the ferromagnetic
conductor.
Richard J. Gambino and Ko-Wei Lin Department of Materials Science
and Engineering Stony Brook University Metal/oxide composite films of Ni80Fe20/NixFe1-xO
were prepared by dual ion beam reactive deposition. The ion beam sputtered
metal film is bombarded during growth with an oxygen ion flux from a secondary
ion source. The oxide phase forms by the shallow ion implantation of oxygen
followed by supersaturation and precipitation. The oxide is dispersed in
the metal matrix as 10nm diameter crystallites. Varying the oxygen ion
flux can be used to control the oxide volume fraction. The oxide has the
rock salt structure but after vacuum annealing at 500C for 3 hours the
spinel ferrite, NiFe2O4 is formed. The metal/ferrite composites show unusually
large anisotropic magnetoresistance (AMR) up to 4.5% at 298K and 14% at
77K as compared to about 1% in the metal/rock salt oxide mixtures. The
largest values are observed when the volume fraction of metal approaches
the percolation limit. The latter observation suggests that the enhanced
anisotropic scattering is occurring at the metal/ferrite interface. The
AMR effect is caused by the spin-orbit interaction that gives rise to a
field dependent scattering cross-section. We suggest that in the metal/ferrite
nanocomposites, strongly anisotropic scattering is associated with spin
polarized oxygen p-orbitals in the ferrite that is exchange coupled to
the ferromagnetic metal. The p-orbitals have a larger scattering cross-section
because they have a larger radial extent compared to the d-orbitals. The
oxygen p-orbitals only contribute to the AMR, however, when they are exchange
coupled to the ferromagnetic conductor.
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