Thickness Dependent Magnetic Anisotropy of Ultrathin LCMO Epitaxial Thin Films

The magnetic properties of La_0.7Ca_0.3Mn_O3 (LCMO) manganite thin films were studied with magnetometry and ferromagnetic resonance as a function of film thickness. They maintain the colossal magnetoresistance behavior with a pronounced metal-insulator transition around 150-200 K, except for the ver...

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Detalles Bibliográficos
Autores: Nemes, Norbert Marcel, García Hernández, Mar, Szatmári, Zsolt, Fehér, Titusz, Simon, Ferenc, Visani, Cristina, Peña, Vanessa, Miller, Christian, Garcia Barriocanal, Javier, Bruno, Flavio Yair, Sefrioui, Zouhair, León Yebra, Carlos, Santamaría Sánchez-Barriga, Jacobo
Tipo de recurso: artículo
Fecha de publicación:2009
País:España
Institución:Universidad Complutense de Madrid (UCM)
Repositorio:Docta Complutense
Idioma:inglés
OAI Identifier:oai:docta.ucm.es:20.500.14352/44762
Acceso en línea:https://hdl.handle.net/20.500.14352/44762
Access Level:acceso abierto
Palabra clave:537
Epitaxial layers
Magnetic anisotropy
Magnetic resonance
Manganites
Thin films
Electricidad
Electrónica (Física)
2202.03 Electricidad
Descripción
Sumario:The magnetic properties of La_0.7Ca_0.3Mn_O3 (LCMO) manganite thin films were studied with magnetometry and ferromagnetic resonance as a function of film thickness. They maintain the colossal magnetoresistance behavior with a pronounced metal-insulator transition around 150-200 K, except for the very thinnest films studied (3 nm). Nevertheless, LCMO films as thin as 3 nm remain ferromagnetic, without a decrease in saturation magnetization, indicating an absence of dead-layers, although below approximately 6 nm the films remain insulating at low temperature. Magnetization hysteresis loops reveal that the magnetic easy axes lie in the plane of the film for thicknesses in the range of 4-15 nm. Ferromagnetic resonance studies confirm that the easy axes are in-plane, and find a biaxial symmetry in-plane with two, perpendicular easy axes. The directions of the easy axes with respect to the crystallographic directions of the cubic SrTiO_3 substrate differ by 45 deg in 4- and 15-nm-thick LCMO films.