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Room temperature ferromagnetism and ferroelectricity in strained multiferroic BiFeO3 thin films on La0.7Sr0.3MnO3/SiO2/Si substrates

dc.contributor.authorRamírez Camacho, Mayra Cecilia
dc.contributor.authorSánchez Valdés, Cesar Fidel
dc.contributor.authorGervacio Arciniega, José Juan
dc.contributor.authorOstos, Carlos
dc.contributor.authorBueno Baques, D.
dc.contributor.authorCuriel Álvarez, Mario
dc.contributor.authorSánchez Llamazares, José Luis
dc.contributor.authorRaymond Herrera, Oscar
dc.date.accessioned2018-08-29T23:12:30Z
dc.date.available2018-08-29T23:12:30Z
dc.date.issued2017-04
dc.identifier.citationM.C. Ramírez-Camacho, C.F. Sánchez-Valdés, J.J. Gervacio-Arciniega, R. Font, C. Ostos, D. Bueno-Baques, M. Curiel, J.L. Sánchez-Llamazares, J.M. Siqueiros, O. Raymond-Herrera, Room temperature ferromagnetism and ferroelectricity in strained multiferroic BiFeO3 thin films on La0.7Sr0.3MnO3/SiO2/Si substrates, Acta Materialia, Volume 128, 2017, Pages 451-464.es_MX
dc.identifier.urihttp://hdl.handle.net/11627/4098
dc.description.abstract"A novel ferromagnetic state coexisting with ferroelectric ordering at room temperature in strained BiFeO3 (BFO) thin films grown using a sputtering technique on La0.7Sr0.3MnO3/SiO2/Si(100) (LSMO/SOS) substrates is reported. The properties of BFO films with different thicknesses (tBFO = 15, 50, 70, 120, and 140 nm) on 40 nm LSMO layers are explored. [012] out-of-plane highly textured BFO/LSMO stacks grew with rhombohedral structures. LSMO layers are nanostructured in nature, constituted by ferromagnetic single-domain nanoregions induced by the constrain of the SiO2 surface, with TC ∼200 K and high coercive field (HC) of ∼1100 Oe at 2.5 K. BFO films grew epitaxially nanostructured on LSMO, exhibiting ∼4 nm spherical nanoregions. The BFO layers show typical antiferromagnetic behavior (in a greater volume fraction) when made thicker (tBFO > 70 nm). The thinner films (tBFO < 50 nm) display ferromagnetic behavior with TC > 400 K, HC ∼ 1600 Oe for 15 nm and ∼1830 Oe for 50 nm. We propose that such ferromagnetic behavior is originated by the establishment of a new magnetic configuration in the Fe3+OFe3+ sublattice of the BFO structure, induced by strong hybridization at the interface as consequence of superexchange coupling interactions with the ferromagnetic Mn3+OMn3+/Mn4+ sublattice of LSMO. All BFO layers show excellent ferroelectric and piezoelectric properties (coercive field ∼ 740 kV/cm, and d33 = 23 p.m./V for 50 nm; ∼200 kV/cm and 55 p.m./V for 140 nm), exhibiting 180° and 109° DWs structures depending on the thickness. Such multiferroic properties predict the potential realization of new magneto-electronic devices integrated with Si technology."es_MX
dc.language.isoenges_MX
dc.publisherElsevier B.Ves_MX
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/*
dc.subjectMultiferroices_MX
dc.subjectBFO/LSMO thin filmes_MX
dc.subjectRf sputteringes_MX
dc.subjectInterlayer exchange couplinges_MX
dc.subjectSuperexchangees_MX
dc.subject.classificationArea::CIENCIAS FÍSICO MATEMÁTICAS Y CIENCIAS DE LA TIERRA::FÍSICAes_MX
dc.titleRoom temperature ferromagnetism and ferroelectricity in strained multiferroic BiFeO3 thin films on La0.7Sr0.3MnO3/SiO2/Si substrateses_MX
dc.typearticlees_MX
dc.identifier.doihttps://doi.org/10.1016/j.actamat.2017.02.030


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Attribution-NonCommercial-NoDerivatives 4.0 Internacional
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