Science · 2007 · 1.2K citations · 8 references
Natural SciencesMaterials SciencePhysicsMagnetic MaterialsSurface ScienceThin FilmsFerromagnetic MaterialsFerromagnetismMagnetic CharacterizationMagnetic Properties Of SolidsMagnetism In SolidsThin Film Magnetic PropertiesAnisotropyAnisotropy In FerromagnetsIntermetallic Magnetic CompoundsMagnetic PropertiesMagnetocrystalline AnisotropyThin Film FerromagnetismThin Film FerromagnetsThin Film Magnetism
Large surface electric fields are expected to alter the electron density and thus the intrinsic magnetic properties of ferromagnetic metals, especially in ultrathin films where surface effects dominate. The magnetic changes arise from a field‑induced variation in the number of unpaired d electrons. Reversible electric‑field control of magnetocrystalline anisotropy and coercivity was achieved in 2‑nm FePt and FePd films immersed in electrolyte, with a –0.6 V bias reducing FePt coercivity by 4.5 % and increasing FePd coercivity by 1 %, demonstrating a general device platform for thin‑film magnetic systems.
A large electric field at the surface of a ferromagnetic metal is expected to appreciably change its electron density. In particular, the metal's intrinsic magnetic properties, which are commonly regarded as fixed material constants, will be affected. This requires, however, that the surface has a strong influence on the material's properties, as is the case with ultrathin films. We demonstrated that the magnetocrystalline anisotropy of ordered iron-platinum (FePt) and iron-palladium (FePd) intermetallic compounds can be reversibly modified by an applied electric field when immersed in an electrolyte. A voltage change of -0.6 volts on 2-nanometer-thick films altered the coercivity by -4.5 and +1% in FePt and FePd, respectively. The modification of the magnetic parameters was attributed to a change in the number of unpaired d electrons in response to the applied electric field. Our device structure is general and should be applicable for characterization of other thin-film magnetic systems.
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