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Magnetocaloric and Giant Magnetoresistance Effects in La-Ba-Mn-Ti-O Epitaxial Thin Films: Influence of Phase Transition and Magnetic Anisotropy

Magnetic perovskite films have promising properties for use in energy-efficient spintronic devices and magnetic refrigeration. Here, an epitaxial ferromagnetic La(0.67)Ba(0.33)Mn(0.95)Ti(0.05)O(3) (LBMTO-5) thin film was grown on SrTiO(3)(001) single crystal substrate by pulsed laser deposition. Hig...

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Detalles Bibliográficos
Autores principales: Oumezzine, Marwène, Chirila, Cristina Florentina, Pasuk, Iuliana, Galca, Aurelian Catalin, Leca, Aurel, Borca, Bogdana, Kuncser, Victor
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9699288/
https://www.ncbi.nlm.nih.gov/pubmed/36431489
http://dx.doi.org/10.3390/ma15228003
Descripción
Sumario:Magnetic perovskite films have promising properties for use in energy-efficient spintronic devices and magnetic refrigeration. Here, an epitaxial ferromagnetic La(0.67)Ba(0.33)Mn(0.95)Ti(0.05)O(3) (LBMTO-5) thin film was grown on SrTiO(3)(001) single crystal substrate by pulsed laser deposition. High-resolution X-ray diffraction proved the high crystallinity of the film with tetragonal symmetry. The magnetic, magnetocaloric and magnetoresistance properties at different directions of the applied magnetic field with respect to the ab plane of the film were investigated. An in-plane uni-axial magnetic anisotropy was evidenced. The LBMTO-5 epilayer exhibits a second-order ferromagnetic-paramagnetic phase transition around 234 K together with a metal–semiconductor transition close to this Curie temperature (T(C)). The magnetic entropy variation under 5 T induction of a magnetic field applied parallel to the film surface reaches a maximum of 17.27 mJ/cm(3) K. The relative cooling power is 1400 mJ/cm(3) K (53% of the reference value reported for bulk Gd) for the same applied magnetic field. Giant magnetoresistance of about 82% under 5 T is obtained at a temperature close to T(C). Defined as the difference between specific resistivity obtained under 5 T with the current flowing along the magnetic easy axis and the magnetic field oriented transversally to the current, parallel and perpendicular to the sample plane, respectively, the in-plane magneto-resistance anisotropy in 5 T is about 9% near the T(C).