Complex perovskite oxides exhibit a rich spectrum of properties, including magnetism,
ferroelectricity, strongly correlated electron behaviour, superconductivity and
magnetoresistance, which have been research areas of great interest among the scientific
and technological community for decades. There exist very few materials which exhibit
multiple functional properties; one such class of materials is called the multiferroics.
Multiferroics are interesting because they exhibit simultaneously ferromagnetic and
ferroelectric polarizations and a coupling between them. Due to the nontrivial lattice
coupling between the magnetic and electronic domains (the magnetoelectric effect),
the magnetic polarization can be switched by applying an electric field; likewise
the ferroelectric polarization can be switched by applying a magnetic field. As a
consequence, multiferroics offer rich physics and novel devices concepts, which have
recently become of great interest to researchers. In this review article the recent
experimental status, for both the bulk single phase and the thin film form, has been
presented. Current studies on the ceramic compounds in the bulk form including
Bi(Fe,Mn)O3,
REMnO3 andthe series
of REMn2O5 single
crystals (RE = rare earth) are discussed in the first section and a detailed overview on multiferroic thin
films grown artificially (multilayers and nanocomposites) is presented in the second section.
Thin films of the charge-ordered (CO) compound Pr 0.5 Ca 0.5 MnO 3 have been deposited onto (100)-oriented SrTiO 3 substrates using the Pulsed Laser Deposition technique. Magnetization and transport properties are measured when the thickness of the film is varied. While the thinner films do not exhibit any temperature induced insulator-metal transition under an applied magnetic field up to 9T, for thickness larger than 1100Å a 5T magnetic field is sufficient to melt the CO state. For this latest film, we have measured the temperature-field phase diagram. Compared to the bulk material, it indicates that the robustness of the CO state in thin films is strongly depending on the strains and the thickness. We proposed an explanation based on the distortion of the cell of the film.
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